Study of associated $bbH, H \to \tau\tau$ channel Szymocha T Cracow, INP 2005 The analysis presented in this note is a comparative study of the observability potential in the lepton-lepton and lepton-hadron final state of a Higgs boson decay into tau lepton pair. Discussed are mass points mH=120GeV, 150GeV and 200GeV and production in b-quark fussion. It is based on fast simulation of the ATLAS detector. The cross-section enhancement of the MSSM regarding tan beta is not included. It is shown that introducing lepton-lepton mode to the analysis stream may increase significance about 20-40%. INTNOTEATLASPUBL

MSSM Higgs at LHC Vivarelli I Meoni E CERN Gennai S CERN 2003 The ATLAS and CMS discovery potential for the MSSM Higgs bosons is reviewed in this paper. The attention is focused on the direct Higgs production and on the Standard Model decay channels. After a short introduction, the most promising final states are discussed, showing that, if supersymmetry exists, its Higgs sector can be explored at LHC with an integrated luminosity of 10 fb$^{-1}$. INTNOTEATLASPUBL

On the simulation of Zbb and Hbb events at LHC González de la Hoz S Ros E Vos M A 2001 A detailed study of the various possible mechanisms leading to Zbb and Hbb events in the final state is performed in the light of recent work released after the completion of the ATLAS physics TDR. The cross sections are computed using both analytical methods and the latest version 6.1 of the PYTHIA Monte Carlo program. Some conclusions concerning the reliability of the various approaches are presented. INTNOTEATLASPUBL

Combined Analysis of A/H to mu+mu- Events from Direct and Associated bbA Production Cavalli D Bosatelli P 1999 INTNOTEATLASPUBL

Combined Analysis of A->tautau Events from Direct and Associated bbA Production Cavalli D Resconi S 1998 INTNOTEATLASPUBL

Analysis of the process pp->bbh/A->bbmumu in the MSSM with mA < 125 GeV González S Ros E Vos M A 2002 In the Minimal Supersymmetric extension of the Standard Model two nearly degenerate light Higgs bosons (h0, A0) exist when the A0 mass is in the range from 90 to 125 GeV. Decay of these Higgs bosons to muons has a small branching ratio, but can be detected taking advantage of the mass resolution. In this note the possibility to extract the pp -> bb h0/A0 -> bb mu+ mu- signal from the background is investigated. INTNOTEATLASPUBL

MSSM Higgs searches in multi-b-jet final states Froidevaux D Richter-Was Elzbieta 1997 INTNOTEATLASPUBL

ATLAS discovery potential for the Charged Higgs Boson in $H^{+} \to \tau \nu$ decays Mohn Bjarte Flechl Martin Alwall Johan 2006 The ATLAS discovery potential for the hadronic $\tau$ decay of a heavy charged Higgs boson, $H^\pm \rightarrow \tau^\pm \nu_\tau$, is presented. A new matched production algorithm for the processes $gg \rightarrow tbH^\pm$ and $gb \rightarrow tH^\pm$ is used allowing to span the investigated mass range from $m_H^\pm < m_t$ up to $m_H^\pm \gg m_t$ with a consistent treatment of the transition region. For the considered charged Higgs boson masses from $165$ to $600$ GeV, $H^\pm \rightarrow \tau^\pm \nu_\tau$ is the most relevant decay channel together with $H^\pm \rightarrow tb$. Whereas the latter suffers from large irreducible backgrounds, the $\tau$ decay channel offers a decisively cleaner signature. This is the first \textsc{Atlas} Full Simulation study of the $H^\pm \rightarrow \tau^\pm \nu_\tau$ channel. For the background, \textsc{Atlas} Fast Simulation is used for the investigation of a greater variety of channels than in previous studies, emphasizing the need for new selection cuts with additional discriminating power between signal and background. Such cuts are introduced and it is shown that current limits from direct charged Higgs boson searches can be substantially extended already with a few years of LHC data. INTNOTEATLASPUBL

Beyond Standard Model searches with top quark at ATLAS Chevallier F IRFU, SPP, Saclay 2008 At the LHC, the top quark is expected to be a huge and clean signal. With about eight millions of expected top pairs and three millions of single top events produced per year in the low luminosity runs, and with a low level of backgrounds, the LHC will open a new opportunity for precision measurements of the top quark properties and for exotic topology searches involving top quarks. As the ATLAS discovery potential on new physics with top quark is being assessed with many analyses, this article focuses on two particular topics: heavy neutral resonances and charged Higgs boson searches with top quarks. The analyses and the ATLAS expectations are described. INTNOTEATLASPUBL

ATLAS Charged Higgs Boson Searches Assamagan K Behar S Coniavitis E Dufour M -A Ehrich T Flechl M Gross E Lane J Mohn B Mohrdieck-Möck S Potter C Robertson S Rozen Y Sopczak A Talby M Vachon B Vickey T Vitells O Yang U K Zaidan R 2008 The discovery of a charged Higgs boson would be a definite signal for the existence of New Physics beyond the Standard Model, possibly the first experimental evidence to be found. This note presents the ATLAS potential for discovering a charged Higgs boson, utilizing six different final states of the signal arising from the three dominating fermionic decay modes of the charged Higgs boson. The search covers the region below the top quark mass, taking into account the present experimental constraints, the transition region with a charged Higgs boson mass of the order of the top quark mass, and the high mass region with a charged Higgs boson mass up to 600 GeV. All studies are performed with a realistic simulation of the detector response including all three trigger levels and taking into account all dominant systematic uncertainties. Results are given in terms of discovery and exclusion contours for each channel individually and for all channels combined, showing that the ATLAS experiment is capable of detecting the charged Higgs boson in a significant fraction of the ($\tan\beta$, $m_{H^\pm}$) parameter space with its first 10 fb$^{-1}$ of data. The so-called intermediate $\tan\beta$ region (around $\tb=7$) remains experimentally hard to reach but exclusion sensitivity is also given in this area. INTNOTEATLASINT

Searching for New Physics using High-$P_T$ Tau Pairs in ATLAS Czyczula Z Vickey T Dam M Xella S Mellado B Wu S L 2008 A number of non-Standard-Model physics processes can lead to events in ATLAS with tau lepton pairs in the final state. In this note we discuss the potential for ATLAS to observe high-mass resonances which decay into two oppositely-charged taus. All three di-tau final states are considered in the study presented here: lepton-lepton, lepton-hadron and hadron-hadron. Using the official ATLAS offline reconstruction software, we consider a $Z'$ with masses between 600 and 2000 GeV. The application of this study to Graviton and heavy MSSM Higgs boson searches is also discussed. INTNOTEATLASINT

ATLAS Search for the MSSM Charged Higgs Boson Potter C McGill U. 2008 The discovery of a charged Higgs boson would be definitive evidence of new physics beyond the Standard Model. The discovery potential of a MSSM charged Higgs boson with the ATLAS detector at the Large Hadron Collider is presented. The study is based on the analysis of signal and background simulated in detail through the experimental apparatus. research-article

A Data-driven Control Sample for $Z\rightarrow\tau^+\tau^- + \mbox{ jets}$ Backgrounds to Higgs Searches Vickey T Chen X Mellado B Quayle W Wu S L 2008 The $Z\rightarrow\tau\tau$ process is a major contribution to the backgrounds for both Standard Model (SM) $H\rightarrow\tau\tau$ and Minimal Supersymmetric Standard Model (MSSM) $h/A/H\rightarrow\tau\tau$ channels in the lepton-lepton, lepton-hadron and hadron-hadron final states. As the relative contributions from this background in different jet multiplicities are not known, and unknowns related to critical analysis cut-specific variables exist (e.g., the Central Jet Veto and event missing energy), the subtraction of these backgrounds using a data-driven method is ideal. Here we present a background subtraction strategy that is data-driven and uses $Z\rightarrow\mu\mu$ events from experimental data to model the $Z\rightarrow\tau\tau$ backgrounds. By using {\tt TAUOLA} via {\tt ATHENA}, as well as {\tt GEANT} and the ATLAS reconstruction software, we are able to accurately model these backgrounds in each of the lepton-lepton, lepton-hadron and hadron-hadron final states using events from data on which we can easily and efficiently trigger. Excellent agreement with this emulated control sample and the true $Z\rightarrow\tau\tau$ distributions is shown. INTNOTEATLASPRIV

Investigation of the ATLAS Discovery Potential for NMSSM Higgs bosons Rottlaender I Schumacher M 2008 The NMSSM is a powerful extension to the MSSM, solving the so-called mu-problem. To evaluate the discovery potential of NMSSM particles, it is desirable to define benchmark regions. In the following, seven two-dimensional benchmark planes over the Higgs sector of the NMSSM are proposed. Afterwards, we present an evaluation of the discovery potential for NMSSM Higgs bosons in these benchmark planes based on previous ATLAS Monte Carlo studies. INTNOTEATLASPRIV

Search of the Higgs boson decaying into tau-leptons at ATLAS Sarri F Pisa U. INFN, Pisa 2008 The search for the Higgs boson is one of the main goals of the Large Hadron Collider experiments. Both in the Standard Model (SM) and in its minimal supersymmetric extensions (MSSM), one or several new bosons are expected as manifestations of the Higgs fi eld. The tau lepton will be essential for Higgs(es) discovery. In fact, both in SM and in the MSSM, the Higgs boson(s) decaying into tau-pairs is one of the favourite discovery channels, especially at low masses. The discovery potential of the ATLAS experiment for neutral Higgs bosons decaying into tau-pairs is shown both in the SM and the MSSM. For the latter, the results on the charged Higgs boson decaying into tau plus neutrino are also discussed. INTNOTEATLASPUBL

ATLAS MSSM Higgs search in SUSY cascade Gentile S INFN, Rome 2009 The neutral MSSM Higgs boson production and following decay in heavy neutralino/chargino pairs has been studied for the ATLAS experiment. The final state with 4 leptons and missing energy is considered. The study has been performed using a realistic detector simulation of signal and the SM and MSSM backgrounds for four benchmark scenarios. The discovery and exclusion sensitivity in the (MA,tanb)-plane is discussed for different luminosity scenarios. An extension of the searches to the charged Higgs boson sector is given. INTNOTEATLASPUBL

Charged Higgs Prospects with ATLAS Flechl M Uppsala U. 2008 The charged Higgs boson simulation studies for charged Higgs boson searches with ATLAS are presented. The focus is on new developments since c$mathrm{H}^pm$arged06. Since then, the first studies with a realistic detector simulation for the most important charged Higgs boson channels have been carried out, including all trigger levels and taking the dominant systematic uncertainties into account. These studies deal both with low-mass (produced in top quark pair decays) and high-mass $H^+$ (produced in $gg$- and $gb$-fusion), with a consistent treatment of the transition region. Analysis techniques and their largest challenges are discussed. The ATLAS H+ sensitivity is presented in terms of discovery and exclusion contours, and eventually a brief outlook on the LHC data-taking era is given. INTNOTEATLASPUBL

Balkan Phys. Lett. Balkan Phys. Lett. The ATLAS discovery potential for MSSM neutral Higgs bosons decaying into muon, tau, supersymmetric particle pairs Gentile S Rome U. INFN, Rome 2009 16 109 113 The discovery potential for MSSM neutral Higgs bosons in the ATLAS experiment at centre-of-mass energy $\sqrt{s}$ = 14 TeV at the Large Hadron Collider (LHC) is discussed. The discovery and exclusion sensitivity in the (m$_A$, tan$\beta$) plane in different luminosity scenarios is discussed for three processes: h/A/H decaying into $\tau\tau$ or into $\mu\mu$ pairs or in supersymmetric particles (heavy neutralino/chargino pairs). research-article

Higgs Property Measurements at the LHC Assamagan K A 2009 The physics program at the LHC includes precision tests of the Standard Model (SM), the search for the SM Higgs boson up to 1 TeV, the search for the MSSM Higgs bosons in the entire parameter space, the search for Super Symmetry, sensitivity to alternative scenarios such as compositeness, large extra dimensions, etc. This requires general purpose detector with excellent performance. ATLAS and CMS are general purpose detectors under construction for the LHC. The detector performance and the prospects for discoveries are studied in various physics working groups. In this talk, I will discuss the determination of the properties of a Higgs-like particle to establish its nature, once such a particle is discovered at the LHC. PUBLATLASSLIDE

Feasibility of SM Higgs Searches at the LHC Mellado B 2009 Feasibility studies for the discovery of the SM Higgs boson by the CMS and ATLAS collaboration are reviewed. PUBLATLASSLIDE

Searches for the Higgs boson at LHC with the ATLAS Detector Kourkoumelis C Athens U. 2009 The Higgs boson is the only particle missing to complete the successful description of the elementary ingredients of our world. As of yet, it escapes experimental detection despite the enormous worldwide efforts. The new Large Hadron Collider (LHC) at CERN will provide enough collision energy for its formation, if it exists. The large experiments already installed, are equipped with excellent detector capabilities in order to confirm (or exclude) its existence. Discovery examples for each mass region of the Higgs boson are given using the complete - "as built" - detector simulation and the latest theoretical cross-section calculations, as well as, optimized selection criteria and statistical treatment. Furthermore, the sensitivity for discovery of the Higgs bosons in the framework of the extended SM model, the MSSM, is shortly reviewed. Emphasis is given to the expected discovery potentials from the first years of running. INTNOTEATLASPUBL

ATLAS searches for MSSM Higgs bosons decaying into SUSY cascades 2009 The neutral MSSM Higgs boson production and subsequent decay into heavy neutralino/chargino pairs has been studied for the ATLAS experiment. The final state with four leptons and missing energy is considered. The study has been performed using a realistic detector simulation of the signal and the SM and MSSM backgrounds for four benchmark scenarios. The discovery and exclusion sensitivity in the (mA,tanb) plane was discussed for different luminosity scenarios. An extension of the searches to the charged Higgs boson sector was explored. INTNOTEATLASPUBL

Non-SM Higgs searches at the LHC Horvat S Max-Planck-Institut f. Physik Munich 2009 Slides for the DIS 2009 Conference, 26-30.04.2009, Madrid, Spain PUBLATLASSLIDE

Discovery Potential of h/A/H to tau+ tau- to l+l- 4nu 2009 This note describes a study of the discovery potential for the supersymmetric Higgs bosons h/H/A in proton-proton collisions at a center-of-mass energy of 14 TeV in final states with tau lepton pairs with the ATLAS detector at the LHC. The Higgs bosons are produced in association with b quarks and decay into a tautau final state where both tau leptons decay leptonically. The signature of Higgs bosons with masses between 110 and 450 GeV is analyzed and the discovery potential is assessed. The analysis is based on an integrated luminosity of 30 fb−1. All results are obtained using full simulation of the ATLAS detector. No pile-up or cavern background has been considered in this analysis. In addition a procedure for estimating the shape and the normalization of the irreducible Z → tau+ tau- background from data is investigated. The discovery potential as a function of mA and tan beta is shown for the mh-max MSSM benchmark scenario. INTNOTEATLASPUBL

Search for the Neutral MSSM Higgs Bosons in the Decay Channel $A/H/h \to \mu^+ \mu^-$ 2009 Motivated by the high muon momentum resolution and identification efficiency achievable with the ATLAS detector, the observability of A/H/h to mu+ mu- channel is explored. The high experimental resolution in this decay mode compensates to some extent for the suppression of the branching ratio, with respect to the A/H/h to tau+ tau- decays. The analyses are performed in the Higgs mass range from 100 to 500 GeV. Two main analysis strategies are applied - the search for the dimuon final states resulting from the direct A/H/h production is combined with the search for the associated bbA/H/h production mode. The studies are optimized for the early stage of data taking up to an integrated luminosity of 30 fb−1 . All results are obtained combining the fast and the full simulation of the ATLAS detector with the nominal detector layout and the trigger efficiencies included. In addition, dedicated data samples are produced to study the impact of the pile-up and cavern background on the analysis performance. The estimation of the background contribution from the experimental data and the contribution of theoretical and experimental uncertainties are also addressed. The discovery potential is shown in the mA -tan beta plane in the context of the mh-max MSSM benchmark scenario. INTNOTEATLASPUBL

ATLAS Serach for MSSM Higgs bosons decaying into SUSY cascades Gentile S Kuznetsova E 2009 The neutral MSSM Higgs boson production and subsequent decay into heavy neutralino/chargino pairs has been studied for the ATLAS experiment. The final state with four leptons and missing energy is considered. The study has been performed using a realistic detector simulation of the signal and the SM and MSSM backgrounds for four benchmark scenarios. The discovery and exclusion sensitivity in the (mA,tamb) plane was discussed for different luminosity scenarios. An extension of the searches to the charged Higgs boson sector was explored. INTNOTEATLASINT

Beyond the Standard Model Higgs Searches at ATLAS Lampen C University of Arizona 2009 The discovery of a neutral Higgs boson with large decay branching fraction to tau and muon pairs final states, as well as the discovery of a charged Higgs boson would represent a strong evidence of New Physics beyond the Standard Model. The potential discovery of these processes with the ATLAS detector at the Large Hadron Collider is presented. The studies are based on the analysis of Monte Carlo signal and background data simulated in detail through the experimental apparatus. PUBLATLASSLIDE

LHC Higgs Prospects Schaffer A Orsay, LAL 2009 We present an overview of recent results of the ATLAS and CMS collaborations from their studies of the discovery potential of a Standard Model Higgs discovery. This is followed by a discussion of the measurement of the Higgs boson parameters, and by a brief discussion of the discovery potential of a MSSM Higgs. INTNOTEATLASPUBL

The ATLAS Forward Physics Program Pinfold JL 2009 After a brief review of the approved ATLAS forward detector system we describe the main ATLAS forward physics program. This program currently includes such topics as soft and hard diffraction, double pomeron exchange, central exclusive production, rapidity gap survival, two photon physics, the determination of the total cross-section and the determination of the absolute luminosity A possible high luminosity upgrade program involving new forward proton detectors is also briefly reviewed. This program opens up a new vista of forward physics for ATLAS that includes SM/MSSM/NMSSM Higgs boson studies, W pair production, slepton production and gluino pair production, etc. INTNOTEATLASPRIV

Prog. High Energy Phys. Prog. High Energy Phys. Non-SM Higgs Searches at the LHC Horvat S Munich, Max Planck Inst. 2009 3 We review the prospects for the Higgs boson searches in the Minimal Supersymmetric Standard Model (MSSM) with the ATLAS and CMS experiments at the Large Hadron Collider (LHC). In preparation for the approaching start of the LHC operation, the discovery reach accessible in proton-proton collisions at a center-of-mass energy of $sqrt{s}$=14~TeV has been recently updated by both experiments. The results are interpreted within the $m_h^{max}$ benchmark scenario. research-article

Detection of Long-Lived Neutral Particles with ATLAS Policicchio A 2009 A number of extensions of the Standard Model result in particles that are neutral, weakly-coupled and have macroscopic decay lengths comparable with LHC detector dimensions. These long-lived particles occur in many models: gauge-mediated SUSY extensions of the MSSM (addition of one singlet field), MSSM with R-parity violation, split SUSY, inelastic dark matter and Hidden Valley (HV) Scenarios in which a new sector is weakly coupled to the Standard Model. In the HV models long-lived HV particles that decay to heavy quark pairs and tau pairs can be produced in SUSY processes, Z' decays and Higgs boson decays. For the purpose of exploring the challenges to the trigger posed by long-lived neutral particles, the Hidden Valley scenario serves as an excellent setting. Results are presented of a first study of the ATLAS Detector performance for the Higgs decay h0 → π0v π0v , where π0v is neutral and has a displaced decay mainly to bottom quarks. The initial goal of the study is to obtain benchmark triggers for processes with such non-standard signatures in the ATLAS apparatus. INTNOTEATLASPRIV

Search for non-standard-model Higgs at the LHC with ATLAS Fassouliotis D 2009 The discovery prospects of non Standard Model Higgs bosons with the ATLAS detector are presented. Due to the high branching ratio, results on decay channels that include tau leptons are presented both for the search of the neutral and the charged MSSM Higgs bosons. For the neutral Higgs bosons results on the muon pair final state are also reported. Furthermore, decay scenarios that include SUSY particle cascades are investigated. Finally, in the absence of light Higgs bosons, processes of vector boson scattering at high mass are discussed, in the context of studying the mechanism of electroweak symmetry breaking. All the studies presented are based on the analysis of Monte Carlo signal and background data simulated in detail through the experimental apparatus INTNOTEATLASPRIV

Light Charged Higgs Boson Searches for H+ to tau+ nu and H+ to c sbar in Early LHC Data at the ATLAS Experiment Lane J Manchester University, United Kingdom Martyniuk A Manchester University, United Kingdom Miyagawa P Manchester University, United Kingdom Yang U Manchester University, United Kingdom Klemetti M McGill University, Montreal, Canada Potter C McGill University, Montreal, Canada Robertson S McGill University, Montreal, Canada Buszello C Uppsala University, Sweden Ferrari A Uppsala University, Sweden Zimmer S Uppsala University, Sweden Gross E Weizmann Institute of Science, Rehovot, Israel Vitells O Weizmann Institute of Science, Rehovot, Israel 2009 In many particle physics models beyond the Standard Model, the top quark can decay to a bottom quark and a light charged Higgs boson in the reaction top to b H+. In the Minimal Super-Symmetric Model (MSSM) and the Next-to-MSSM (NMSSM), the decays H+ to tau+ nu can dominate other decays, depending on the parameter space, while H+ to c sbar can have a significant branching ratio for low tan(beta). In the early data-taking period, the ATLAS detector at the Large Hadron Collider (LHC) could either discover the light H+ or substantially improve the current Tevatron upper limits on the branching ratio of top to b H+. We assume an integrated luminosity of 200/pb and a center of mass energy 10 TeV, and evaluate expected upper limits for the branching ratio top to b H+ separately assuming the branching ratio of H+ to tau+ nu is 1 and the branching ratio of H+ to c sbar is 1. INTNOTEATLASPRIV

The ATLAS Forward Physics Program 2009 After a brief review of the approved ATLAS forward detector system we describe the main ATLAS forward physics program. This program currently includes such topics as soft and hard diffraction, double pomeron exchange, central exclusive production, rapidity gap survival, two photon physics, the determination of the total cross-section and the determination of the absolute luminosity A possible high luminosity upgrade program involving new forward proton detectors is also briefly reviewed. This program opens up a new vista of forward physics for ATLAS that includes SM/MSSM/NMSSM Higgs boson studies, W pair production, slepton production and gluino pair production, etc. INTNOTEATLASPUBL

Higgs physics with ATLAS Davidek T Charles University, Prague 2009 The ATLAS physics program includes the search for the Higgs boson. The discovery prospects are discussed in various channels both for the Standard Model and the MSSM Higgs boson(s). The measurement of the Higgs boson properties - mass, spin, CP, couplings - are also briefly reviewed. Talk to be presented at Hadron Structure'09 conference. INTNOTEATLASPRIV

Beyond Standard Model Higgs Searches at the LHC Schumacher J IKTP TU Dresden 2009 This is a talk for the conference Weak Interactions and Neutrinos '09. An overview of searches for non Standard Model Higgs Boson searches of ATLAS and CMS is given. In particular, neutral and charged Higgs boson searches in the MSSM are presented. Because of the relatively high branching ratios and the possibility to trigger on and identify tau leptons, decays into a tau lepton pair play an important role in discovery. Muon pairs from Higgs are much rarer but have the advantage of a very clear signal. Alternative approaches via neutralino decays and reinterpretation of Standard Model searches are discussed. Analyses to find charged MSSM Higgs bosons are presented. Two examples of non-supersymmetric searches, invisible Higgs and search for radions are also given. INTNOTEATLASPRIV

Prospects for Higgs boson searches with ATLAS Part II: Neutral Higgs decays to fermions Schumacher M University Freiburg 2009 The prospects for the observation of neutral Higgs bosons decaying to fermions in the Standard Model (SM) and in the Minimal Supersymmetric Standard Model (MSSM) with ATLAS is reviewed. INTNOTEATLASPRIV

b-Tag-Independent Search for the Neutral MSSM Higgs Boson in the Dimuon Decay Channel Ruiz-Martinez A Mellado B Valls J A Wu S L 2009 This note describes the Minimal Supersymmetric Standard Model (MSSM) $h/A/H$ boson search in the dimuon channel at the ATLAS experiment. Since jet flavour tagging is not required in the analysis, it can be performed with low integrated luminosity, even before the b-tagging in the experiment reaches its optimal performance. Discovery significances and exclusion limits for several Higgs masses (110 GeV to 400 GeV) and $\tan\beta$ values (10 to 60) are evaluated using a maximum likelihood fit formalism based on toy Monte Carlo experiments at different integrated luminosities. Our results show that the MSSM parameter space can be significantly constrained with this analysis at 1 fb$^{-1}$ (a 95% C.L. exclusion can be established for $m_A=130$ GeV and $\tan\beta>30$) and discovery is feasible at 10 fb$^{-1}$ ($5\sigma$ significance can be achieved for $m_A=130$ GeV and $\tan\beta>35$). The study is performed assuming that the collisions take place at the 14 TeV center-of-mass energy. INTNOTEATLASINT

Search for non-Standard-Model Higgs at the LHC with ATLAS Fassouliotis D University of Athens 2009 The discovery prospects of non Standard Model Higgs bosons with the ATLAS detector are presented. Due to the high branching ratio, results on decay channels that include tau leptons are presented both for the search of the neutral and the charged MSSM Higgs bosons. For the neutral Higgs bosons results on the muon pair final state are also reported. Furthermore, decay scenarios that include SUSY particle cascades are investigated. Finally, in the absence of light Higgs bosons, processes of vector boson scattering at high mass are discussed, in the context of studying the mechanism of electroweak symmetry breaking. All the studies presented are based on the analysis of Monte Carlo signal and background data simulated in detail through the experimental apparatus INTNOTEATLASPRIV

Search for non-Standard-Model Higgs at the LHC with ATLAS Fassouliotis D Athens U. 2009 The discovery prospects of non Standard Model Higgs bosons with the ATLAS detector are presented. Due to the high branching ratio, results on decay channels that include tau leptons are presented both for the search of the neutral and the charged MSSM Higgs bosons. For the neutral Higgs bosons results on the muon pair final state are also reported. Furthermore, decay scenarios that include SUSY particle cascades are investigated. Finally, in the absence of light Higgs bosons, processes of vector boson scattering at high mass are discussed, in the context of studying the mechanism of electroweak symmetry breaking. All the studies presented are based on the analysis of Monte Carlo signal and background data simulated in detail through the experimental apparatus INTNOTEATLASPUBL

Investigation of the ATLAS Discovery Potential for NMSSM Higgs bosons Rottlaender I Schumacher M 2009 The NMSSM is a powerful extension to the MSSM, solving the so-called mu-problem. To evaluate the discovery potential of NMSSM particles, it is desirable to define benchmark regions. In the following, seven two-dimensional benchmark planes over the Higgs sector of the NMSSM are proposed. Afterwards, we present an evaluation of the discovery potential for NMSSM Higgs bosons in these benchmark planes based on previous ATLAS Monte Carlo studies. INTNOTEATLASINT

Instituto de Física Corpuscular (IFIC) UV-CSIC Valencia Studies with Muons in ATLAS: TileCal Level-2 Trigger and MSSM Higgs Discovery Reach Ruiz Martínez A Valencia U., Valencia U., IFIC 2009 This thesis was carried out in the years previous to the LHC start-up, i.e. during the ATLAS detector commissioning phase. It contains an introductory part about the detector and its expected physics performance and two main parts about the development of a Level-2 trigger for muons and a study of the MSSM Higgs discovery reach with simulated data, which are briefly described below. The first part of the thesis is devoted to TileMuId, the muon identication algorithm based on TileCal whose main goal is to be used as a Level-2 trigger of low-$p_{\text{T}}$ muons. A second version of TileMuId (ROD-based) has been implemented to run in the TileCal ROD DSPs. This involved developments in the DSP firmware and in the Athena framework, described in the document. In addition, studies of the algorithm performance in terms of efficiency and fraction of fakes have been done. Developments and studies to match the TileCal muon candidates with the Inner Detector tracks (provided by ID reconstruction algorithms) have been performed and two new trigger chains combining TileCal and ID have been created. Both TileMuId versions are fully integrated in the Muon Trigger Slice Working Group, have been running in High Level Trigger during cosmics data taking periods and are included in the trigger menu of ${\cal{L}}=10^{31}$ cm$^{-2}$s$^{-1}$. In the second part of the thesis, the ATLAS discovery potential of the MSSM neutral Higgs boson in the dimuon decay channel, $h/A/H \to \mu^{+}\mu^{-}$, for a center-of-mass energy of 14 TeV is explored with simulated data. For this analysis, we used the official event selection cuts agreed by the collaboration with the only exception of not requiring b-tagging for the jets. Since jet flavor tagging is not required in the analysis, it can be performed with low integrated luminosity, even before the b-tagging in the experiment reaches its optimal performance. Discovery significances and exclusion limits for several Higgs masses (110 GeV to 400 GeV) and $\tan\beta$ values (10 to 60) are evaluated using a maximum likelihood fit formalism based on toy Monte Carlo experiments at different integrated luminosities. Our results show that the MSSM parameter space can be significantly constrained with this analysis at 1 fb$^{-1}$ (a 95\% CL exclusion can be established for $m_A=130$ GeV and $\tan\beta>30$) and discovery is feasible at 10 fb$^{-1}$ ($5\sigma$ significance can be achieved for $m_A=130$ GeV and $\tan\beta>35$). technical-report

Light Charged Higgs Boson Searches for H+ to tau+ nu and H+ to c sbar in Early LHC Data at the ATLAS Experiment Lane J Manchester University, United Kingdom Martyniuk A Manchester University, United Kingdom Miyagawa P Manchester University, United Kingdom Yang U Manchester University, United Kingdom Klemetti M McGill University, Montreal, Canada Potter C McGill University, Montreal, Canada Robertson S McGill University, Montreal, Canada Buszello C Uppsala University, Sweden Ferrari A Uppsala University, Sweden Zimmer S Uppsala University, Sweden Gross E Weizmann Institute of Science, Rehovot, Israel Vitells O Weizmann Institute of Science, Rehovot, Israel 2009 In many particle physics models beyond the Standard Model, the top quark can decay to a bottom quark and a light charged Higgs boson in the reaction top to b H+. In the Minimal Super-Symmetric Model (MSSM) and the Next-to-MSSM (NMSSM), the decays H+ to tau+ nu can dominate other decays, depending on the parameter space, while H+ to c sbar can have a significant branching ratio for low tan(beta). In the early data-taking period, the ATLAS detector at the Large Hadron Collider (LHC) could either discover the light H+ or substantially improve the current Tevatron upper limits on the branching ratio of top to b H+. We assume an integrated luminosity of 200/pb and a center of mass energy 10 TeV, and evaluate expected upper limits for the branching ratio top to b H+ separately assuming the branching ratio of H+ to tau+ nu is 1 and the branching ratio of H+ to c sbar is 1. INTNOTEATLASINT

Light Charged Higgs Boson Searches for H+ to tau+ nu and H+ to c sbar in Early LHC Data at the ATLAS Experiment Atlas Coll 2009 In many particle physics models beyond the Standard Model, the top quark can decay to a bottom quark and a light charged Higgs boson in the reaction top to b H+. In the Minimal Super-Symmetric Model (MSSM) and the Next-to-MSSM (NMSSM), the decays H+ to tau+ nu can dominate other decays, depending on the parameter space, while H+ to c sbar can have a significant branching ratio for low tan(beta). In the early data-taking period, the ATLAS detector at the Large Hadron Collider (LHC) could either discover the light H+ or substantially improve the current Tevatron upper limits on the branching ratio of top to b H+. We assume an integrated luminosity of 200/pb and a center of mass energy 10 TeV, and evaluate expected upper limits for the branching ratio top to b H+ separately assuming the branching ratio of H+ to tau+ nu is 1 and the branching ratio of H+ to c sbar is 1. INTNOTEATLASPRIV

Max Planck Inst. Munich Measurement of the mumu Background for Neutral MSSM Higgs Searches with the ATLAS Detector Stern S Munich, Tech. U. 2009 The subject of this work is the development of a data-driven method for the background estimation for neutral MSSM Higgs searches in the decay channel h/H/A -> mumu. The method employs signal-free control samples from the ee and emu final states and is based on the vanishing decay rate h/H/A -> ee. In contrast, for the background processes the decay rates into electrons and muons are equal at particle level. Differences between the electron and muon final states at reconstruction level arising from the detector response and the presence of Bremsstrahlung and final state radiation are studied in detail. The accuracy of the method is evaluated for the dominant background contributions from Z boson and tt decays. Detector-related systematic uncertainties concerning muon, electron and jet reconstruction are taken into account. Finally, the presented method for the background estimation is used to evaluate the exclusion limits at a confidence level of 95%. technical-report

Prospects for data-driven Estimation of the mumu Background for Neutral MSSM Higgs Searches in the Decay Channel h/H/A -> mumu Stern S Horvat S Kortner O Kroha H 2009 This note describes the discovery prospects for the neutral MSSM Higgs bosons in the decay channel h/H/A -> mumu with the ATLAS detector. The analysis is performed for 10 TeV collision data simulated with full and fast simulation assuming Higgs masses of 130, 150 and 200 GeV and a benchmark point of tan beta = 40. A good knowledge of the large Standard Model background, dominated by Z and tt production, is crucial for the exclusion of the signal in early data analyses. Thus, a method is presented which allows to estimate these backgrounds from data by means of signal-free control samples from ee and emu final states. The method is based on the vanishing decay rate h/H/A -> ee. In contrast, the top quarks and Z bosons decay with equal probability into electrons and muons. Differences between the dielectron and dimuon final states arising from detector properties and photon radiation are studied in detail. The expected accuracy of the method is evaluated for different integrated luminosities of 0.2, 1 and 4 fb{-1} by comparing the control samples with the actual mumu background. Finally, the information from the control samples and side band regions in the mumu final state are combined to calculate the exclusion limits at a 95% confidence level. INTNOTEATLASPRIV

Higgs Production Cross Sections and Decay Branching Ratios Assamagan K Bourgaux A Campanelli M Carrillo-Montoya G Escalier M Flechl M Huston J Muanza S Murray B Mellado B Nisati A Qian J Rebuzzi D Schram M Schumacher M Tanaka R Vickey T Warsinsky M Zhang H Andari N 2010 This note summarizes a survey of state-of-art theoretical tools currently available for the calculation of the Higgs production cross sections at the LHC and and their decay branching ratios in both the Standard Model and its minimal supersymmetric extension. All major production processes and decay modes are investigated. Cross sections and their theoretical uncertainties at $sqrt{s}=7, 10$ and 14~TeV are presented for most of the processes studied. The note also discusses unresolved issues and offers suggestions for future improvements. INTNOTEATLASPRIV

Discovery Potential of $A/H\to\tau^+\tau^-\to\ell h$ in ATLAS Anders C Barberio E Cavalli D Davey W Dingfelder J Felzmann U Glatzer J Goussiou A Kobel M Mader W F Mazur M Pashapour S Schaarschmidt J 2010 This note describes a study of the discovery potential for the supersymmetric Higgs bosons $H/A$ in proton-proton collisions at a center-of-mass energy of $14\,\mathrm{TeV}$ in final states with $\tau$-lepton pairs with the ATLAS detector at the LHC. The Higgs bosons are produced in association with $b$-quarks or from gluon-fusion processes and decay into a di-$\tau$ final state where one $\tau$ lepton decays leptonically and the other hadronically. Higgs boson masses between $150$ and $800\,\mathrm{GeV}$ are analysed. All results are obtained using the ATLFAST-II simulation of the ATLAS detector except for the determination of the trigger efficiencies. For the latter, selected signal samples are processed with full simulation. Procedures to estimate the contribution of all relevant backgrounds from control regions in data have been developed. The discovery potential in the $m_A$ vs. $\tan\beta$ plane is assessed for the $m_h^\mathrm{max}$ MSSM benchmark scenario and compared to that obtained previously in the fully-leptonic analysis, published in the CSC book. No pile-up or cavern background has been considered in this analysis. The analysis is based on an integrated luminosity of $30\,\mathrm{fb}^{-1}$. INTNOTEATLASPRIV

An ATLAS Search for the NMSSM Ideal Higgs Scenario Klemetti M Laflamme C Lou HK Potter CT Robertson S 2010 The Next to Minimal Supersymmetric Model (NMSSM) is motivated by $mu$ term problem of the Minimal Supersymmetric Model (MSSM) and may explain anomalous experimental measurements. In the NMSSM, the lightest CP-odd Higgs Boson $a_1$ can be very light ($m_{a_1}<2m_{b}$) and significantly alter the phenomenology of the MSSM Higgs sector. Searches for the light $a_1$ have been carried out by BaBar, ALEPH, DZero and CDF. We present searches for gg to $a_1$, $h_1$ to 2$a_1$ and $H^+$ to $a_1$ $W^+$ in early ATLAS data. We assume integrated luminosities of $10$pb$^{-1}$ and $200$pb$^{-1}$ at 10TeV center of mass energy. INTNOTEATLASPRIV

Higgs Production Cross Sections and Decay Branching Ratios Andari N Assamagan K Bourgaux A Campanelli M Carrillo-Montoya G Escalier M Flechl M Huston J Muanza S Murray B Mellado B Nisati A Qian J Rebuzzi D Schram M Schumacher M Tanaka R Vickey T Warsinsky M Zhang H 2010 This note summarizes a survey of state-of-art theoretical tools currently available for the calculation of the Higgs production cross sections at the LHC and and their decay branching ratios in both the Standard Model and its minimal supersymmetric extension. All major production processes and decay modes are investigated. Cross sections and their theoretical uncertainties at $sqrt{s}=7, 10$ and 14~TeV are presented for most of the processes studied. The note also discusses unresolved issues and offers suggestions for future improvements. INTNOTEATLASINT

Discovery Potential of $A/H\to\tau^+\tau^-\to\ell h$ in ATLAS Anders C Barberio E Cavalli D Davey W Dingfelder J Felzmann U Glatzer J Goussiou A Kobel M Mader W F Mazur M Pashapour S Schaarschmidt J 2010 This note describes a study of the discovery potential for the supersymmetric Higgs bosons $H/A$ in proton-proton collisions at a center-of-mass energy of $14\,\mathrm{TeV}$ in final states with $\tau$-lepton pairs with the ATLAS detector at the LHC. The Higgs bosons are produced in association with $b$-quarks or from gluon-fusion processes and decay into a di-$\tau$ final state where one $\tau$ lepton decays leptonically and the other hadronically. Higgs boson masses between $150$ and $800\,\mathrm{GeV}$ are analysed. All results are obtained using the ATLFAST-II simulation of the ATLAS detector except for the determination of the trigger efficiencies. For the latter, selected signal samples are processed with full simulation. Procedures to estimate the contribution of all relevant backgrounds from control regions in data have been developed. The discovery potential in the $m_A$ vs. $\tan\beta$ plane is assessed for the $m_h^\mathrm{max}$ MSSM benchmark scenario and compared to that obtained previously in the fully-leptonic analysis, published in the CSC book. No pile-up or cavern background has been considered in this analysis. The analysis is based on an integrated luminosity of $30\,\mathrm{fb}^{-1}$. INTNOTEATLASINT

Expected Sensitivity in Light Charged Higgs Boson Searches for H+ to tau+nu and H+ to c+sbar with Early LHC Data at the ATLAS Experiment "ATLAS Coll" 2010 In many particle physics models beyond the Standard Model, the top quark can decay to a bottom quark and a light charged Higgs boson in the reaction top to bH+. In the Minimal Super-Symmetric Model (MSSM), the decays H+ to tau+nu can dominate other decays, depending on the parameter space, while H+ to c sbar can have a significant branching ratio for low tan(beta). In the early data-taking period, the ATLAS detector at the Large Hadron Collider (LHC) could either discover the light H+ or substantially improve the current Tevatron upper limits on the branching ratio of top to b H+. We assume an integrated luminosity of 200/pb and a center of mass energy 10 TeV, and evaluate expected upper limits for the branching ratio top to b H+ separately assuming the branching ratio of H+ to tau+ nu is 1 and the branching ratio of H+ to c sbar is 1. INTNOTEATLASPRIV

Discovery Potential of A/H->&tau;&tau;->lh in ATLAS ATLAS Coll 2010 This note describes a study of the discovery potential for the supersymmetric Higgs bosons $H/A$ in proton-proton collisions at a centre-of-mass energy of 14 TeV in final states with $\tau$-lepton pairs with the ATLAS detector at the LHC. The Higgs bosons are produced in association with $b$-quarks or from gluon-fusion processes and decay into a di-$\tau$ final state. The final state where one $\tau$ lepton decays leptonically and the other hadronically is studied. Higgs boson masses between 150 and 800 GeV are analysed. All results are obtained using the ATLFAST-II simulation of the ATLAS detector except for the determination of the trigger efficiencies. For the latter, selected signal samples are processed with full simulation. Procedures to estimate the contribution of all relevant backgrounds from control regions in data have been developed. The discovery potential in the $m_A$ vs. $\tan\beta$ plane is assessed for the $m_h^\mathrm{max}$ MSSM benchmark scenario and compared to that obtained previously in the fully-leptonic analysis. No pile-up or cavern background has been considered in this analysis. The analysis is based on an integrated luminosity of $30$ fb$^-1$. INTNOTEATLASPRIV

MSSM Higgs searches at the LHC Lenzi B CEA - Saclay 2010 Slides for MCTP Spring Symposium on Higgs Boson Physics (Spring 2010) INTNOTEATLASPRIV

Higgs Searches beyond SM and MSSM at the LHC Rebuzzi D Pavia University and INFN 2010 The present slides discuss the LHC discovery potential for beyond SM and MSSM Higgs searches at LHC. INTNOTEATLASPRIV

Nuovo Cimento C Nuovo Cimento C Search for the MSSM Higgs bosons at the LHC Sarri F Pisa U. INFN, Pisa 2009 32 221 224 research-article

Combined Sensitivity to MSSM $H/A$->&tau;&tau;->lh in 7 TeV Collisions at ATLAS Anders C Barberio E Cavalli D Davey W Dingfelder J Felzmann U Glatzer J Goussiou A Kobel M Mader W Mazur M Pashapour S Schaarschmidt J Thoma S 2010 In this note the sensitivity of the ATLAS experiment at the LHC to neutral MSSM Higgs bosons $H/A$ at a center-of-mass energy of 7TeV and an integrated luminosity of 1fb$^{-1}$ is studied in the final state with two τ leptons, where one τ lepton decays hadronically and one leptonically. The results of this study are based on a similar analysis conducted at a center-of-mass energy of 14TeV. The cross sections, the selection efficiencies and the systematic uncertainties assumed have been extrapolated to a center-of-mass energy of 7TeV and an integrated luminosity of 1fb$^{-1}$. The five-σ discovery potential as well as the exclusion limit at a confidence level of 95% in the $m_h^\mathrm{max}$ scenario are presented. No pile-up or cavern background has been considered in this analysis. INTNOTEATLASPRIV

ATLAS sensitivity prospects for the neutral MSSM Higgs bosons in the $H/A\to \mu^+\mu^-$ decay channel at $\sqrt{s}$ = 7 TeV Horvat S Max-Planck-Institut f. Physik, Munich Kortner O Max-Planck-Institut f. Physik, Munich Kroha H Max-Planck-Institut f. Physik, Munich Stern S Max-Planck-Institut f. Physik, Munich 2010 The ATLAS sensitivity propspects for the neutral MSSM Higgs bosons are studied in the $H/A\to \mu^+\mu^-$ decay channel at a center-of-mass collision energy of $\sqrt{s}$ = 7~TeV. The expected exclusion limits are evaluated at a 95\% confidence level for the Higgs masses of 130, 150 and 200~GeV in the frame of the $m_h^{max}$ MSSM benchmark scenario. The estimation is based on the recently obtained Monte Carlo simulation results at $\sqrt{s}$ = 10~TeV, in which the data-driven background estimation and the systematic uncertainties have been taken into account. These results are extrapolated to $\sqrt{s}$ = 7~TeV by rescaling the signal and background contributions according to their cross sections. Such a procedure is shown to be justified, since the event selection efficiency is rather independent of the center-of-mass energy. INTNOTEATLASPRIV

ATLAS Forward Detectors and Physics Soni N University of Alberta, Canada 2010 The ATLAS has a very strong program to study the forward region of the interacti on point. This contribution describes the current ATLAS forward detectors LUCID, ZDC, ALFA, and the upgrade future project AFP. The current forward detectors ar e dedicated for the luminosity measurements and the forward physics measurements at first low luminosity LHC phase. The measuring ability in the forward region is also crucial for soft QCD, diffractive physics and the determination of absol ute luminosity. The AFP project will significantly extend the ATLAS physics prog ram at high luminosities by tagging the very forward going protons. This program will open up a new vista of forward physics that includes SM/MSSM/NMSSM Higgs b oson studies, W pair production etc. INTNOTEATLASPRIV

ATLAS sensitivity prospects for the neutral MSSM Higgs bosons in the $H/A\to \mu^+\mu^-$ decay channel at $\sqrt{s}$ = 7 TeV Horvat S Max-Planck-Institut f. Physik, Munich Kortner O Max-Planck-Institut f. Physik, Munich Kroha H Max-Planck-Institut f. Physik, Munich Stern S Max-Planck-Institut f. Physik, Munich 2010 The ATLAS sensitivity propspects for the neutral MSSM Higgs bosons are studied in the $H/A\to \mu^+\mu^-$ decay channel at a center-of-mass collision energy of $\sqrt{s}$ = 7~TeV. The expected exclusion limits are evaluated at a 95\% confidence level for the Higgs masses of 130, 150 and 200~GeV in the frame of the $m_h^{max}$ MSSM benchmark scenario. The estimation is based on the recently obtained Monte Carlo simulation results at $\sqrt{s}$ = 10~TeV, in which the data-driven background estimation and the systematic uncertainties have been taken into account. These results are extrapolated to $\sqrt{s}$ = 7~TeV by rescaling the signal and background contributions according to their cross sections. Such a procedure is shown to be justified, since the event selection efficiency is rather independent of the center-of-mass energy. INTNOTEATLASINT

Prospects for data-driven Estimation of the mumu Background for Neutral MSSM Higgs Searches in the Decay Channel h/H/A -> mumu Stern S Horvat S Kortner O Kroha H 2010 This note describes the discovery prospects for the neutral MSSM Higgs bosons in the decay channel h/H/A -> mumu with the ATLAS detector. The analysis is performed for 10 TeV collision data simulated with full and fast simulation assuming Higgs masses of 130, 150 and 200 GeV and a benchmark point of tan beta = 40. A good knowledge of the large Standard Model background, dominated by Z and tt production, is crucial for the exclusion of the signal in early data analyses. Thus, a method is presented which allows to estimate these backgrounds from data by means of signal-free control samples from ee and emu final states. The method is based on the vanishing decay rate h/H/A -> ee. In contrast, the top quarks and Z bosons decay with equal probability into electrons and muons. Differences between the dielectron and dimuon final states arising from detector properties and photon radiation are studied in detail. The expected accuracy of the method is evaluated for different integrated luminosities of 0.2, 1 and 4 fb{-1} by comparing the control samples with the actual mumu background. Finally, the information from the control samples and side band regions in the mumu final state are combined to calculate the exclusion limits at a 95% confidence level. INTNOTEATLASINT

ATLAS Sensitivity Prospects for Higgs Boson Production at the LHC Running at 7 TeV ATLAS Coll 2010 Projections for the ATLAS sensitivity in selected channels to the Standard Model (SM) and Minimal Super-Symmetric Standard Model (MSSM) Higgs boson(s) from the LHC running at 7 TeV are reported. The results are based on re-scaling expectations from detailed analyses at 10 or 14 TeV using cross section ratios or parton distribution function (PDF) reweighting to arrive at the 7 TeV projections. INTNOTEATLASPRIV

Expected Sensitivity in Light Charged Higgs Boson Searches for H+ to tau+nu and H+ to c+sbar with Early LHC Data at the ATLAS Experiment "ATLAS Coll" 2010 In many particle physics models beyond the Standard Model, the top quark can decay to a bottom quark and a light charged Higgs boson in the reaction top to bH+. In the Minimal Super-Symmetric Model (MSSM), the decays H+ to tau+nu can dominate other decays, depending on the parameter space, while H+ to c sbar can have a significant branching ratio for low tan(beta). In the early data-taking period, the ATLAS detector at the Large Hadron Collider (LHC) could either discover the light H+ or substantially improve the current Tevatron upper limits on the branching ratio of top to b H+. We assume an integrated luminosity of 200/pb and a center of mass energy 10 TeV, and evaluate expected upper limits for the branching ratio top to b H+ separately assuming the branching ratio of H+ to tau+ nu is 1 and the branching ratio of H+ to c sbar is 1. INTNOTEATLASPUBL

ATLAS Sensitivity Prospects for Higgs Boson Production at the LHC Running at 7 TeV 2010 Projections for the ATLAS sensitivity in selected channels to the Standard Model (SM) and Minimal Super-Symmetric Standard Model (MSSM) Higgs boson(s) from the LHC running at 7 TeV are reported. The results are based on re-scaling expectations from detailed analyses at 10 or 14 TeV using cross section ratios or parton distribution function (PDF) reweighting to arrive at the 7 TeV projections. INTNOTEATLASPUBL

MSSM Higgs to Tau Tau Searches at the ATLAS Experiment Leney KJC University of Liverpool 2010 Slides for talk at Higgs Hunting, Orsay, 29th-31st July 2010 INTNOTEATLASPRIV

Discovery Potential of A/H->&tau;&tau;->lh in ATLAS 2010 This note describes a study of the discovery potential for the supersymmetric Higgs bosons $H/A$ in proton-proton collisions at a centre-of-mass energy of 14 TeV in final states with $\tau$-lepton pairs with the ATLAS detector at the LHC. The Higgs bosons are produced in association with $b$-quarks or from gluon-fusion processes and decay into a di-$\tau$ final state. The final state where one $\tau$ lepton decays leptonically and the other hadronically is studied. Higgs boson masses between 150 and 800 GeV are analysed. All results are obtained using the ATLFAST-II simulation of the ATLAS detector except for the determination of the trigger efficiencies. For the latter, selected signal samples are processed with full simulation. Procedures to estimate the contribution of all relevant backgrounds from control regions in data have been developed. The discovery potential in the $m_A$ vs. $\tan\beta$ plane is assessed for the $m_h^\mathrm{max}$ MSSM benchmark scenario and compared to that obtained previously in the fully-leptonic analysis. No pile-up or cavern background has been considered in this analysis. The analysis is based on an integrated luminosity of $30$ fb$^-1$. INTNOTEATLASPUBL

BSM Higgs at LHC: prospects end 2011 and before Tanaka R LAL-Orsay 2010 Slide for the talk on BSM Higgs at the Higgs Hunting Workshop, July 29-31, 2010 to be held at Orsay, France. Early Higgs beyond the Standard Model searches are discussed for the centre-of-mass energy at 7TeV with a target luminosity of 1fb^-1 to be accumulated by the end of 2011. INTNOTEATLASPRIV

ATLAS Sensitivity Prospects for Light Charged Higgs Searches at 7 TeV Miyagawa PS The University of Manchester 2010 We present the ATLAS sensitivity for light charged Higgs boson searches at 7 TeV. In some models beyond the Standard Model, including the Minimal Supersymmetric Model (MSSM), charged Higgs bosons can be produced in top quark decays. We study the ATLAS sensitivity to light charged Higgs in the two dominant MSSM decay channels: H+ -&gt; tau-nu, and csbar. With 1 fb-1 of expected data, we find that the ATLAS sensitivity to light charged Higgs improves substantially on current Tevatron upper limits on B(t -&gt; bH+). INTNOTEATLASPRIV

H -&gt; tautau and H+ -&gt; tau nu with the ATLAS detector at the LHC Gonçalo R Royal Holloway, University of London 2010 The H -&gt; tautau channel is important for the observation of a Higgs boson signal. In the Standard Model, the H -&gt; tautau would provide a significant contribution to the Higgs boson search in the low mass region when the Higgs is produced by vector boson fusion. The  H-&gt; tautau channel is also important for the MSSM neutral Higgs boson searches through the associated production of the Higgs bosons with heavy quarks or by gluon fusion. The observation of a charged Higgs boson will constitute an irrefutable evidence of new physics beyond the Standard Model. In many particle physics models beyond the Standard Model, the top quark can decay to a bottom quark and a light charged Higgs boson (m_H+&lt;m_top) in the reaction t to bH+. The decay channel H+-&gt;tau+nu is important in the search for a charged Higgs signal at the LHC. Fake tau-jets from various sources are a major background for Higgs signal final states containing genuine hadronic tau-jets. We report on techniques based on real data to estimate backgrounds from fake taus. Also, sensitivity prospects for early Higgs signal with taus in the final states are presented. INTNOTEATLASPRIV

ATLAS discovery prospects for the charged Higgs in di-lepton ttbar events (H+ to taunu) Klemetti M 2010 We present projections for the ATLAS sensitivity to a light charged Higgs boson in the channel H-&gt;taunu-&gt;lnu, present in models beyond the Standard Model, with an expected dataset corresponding to an integrated luminosity of 1fb-1 gathered at the ATLAS detector with the LHC running at 7 TeV. The results are based on re-scaling expectations from detailed analyses at 10 TeV using cross-section ratios. INTNOTEATLASPRIV

ATLAS discovery prospects for a light charged Higgs, H+ to csbar Yang Un-ki University of Manchester 2010 We present the ATLAS sensitivity for light charged Higgs boson searches at 7 TeV. In some models beyond the Standard Model, including the Minimal Super-symmetric Model (MSSM), charged Higgs bosons can be produced in top quark decays. We study the ATLAS sensitivity to a light charged Higgs in the H+ to csbar decay channel. With 1fb^-1 of expected data, we find that ATLAS sensitivity to the light charged Higgs improves substantially on the current Tevatron upper limits on B(t to bH+). INTNOTEATLASPRIV

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ATLAS discovery prospects for the charged Higgs in the H+ to tau nu final state Klemetti M McGill University 2010 In the Minimal Super-Symmetric model (MSSM), the decay H+ to tau nu can be a dominant decay channel for the light (m(H+) < m(top) ) charged Higgs boson. Through this channel, the ATLAS detector at the Large Hadron Collider (LHC) could either discover the light H+ or improve the current Tevatron upper limits on B(t to bH+). We evaluate the expected ATLAS upper limit for B(t to b H+), assuming B(H+ to tau nu)=1 and an integrated luminosity of 200 pb-1 gathered at sqrt(s)=10 TeV. INTNOTEATLASPRIV

Higgs searches at the LHC Nakamura K 2010 During the operation at the center-of-mass energy of 7~TeV, the LHC is expected to deliver up to 1~fb$^{-1}$ of $pp$ collision data by the end of 2011. Prospect for the Higgs searches at the LHC with 1~fb$^{-1}$ of integrated luminosity of data is discussed. Promising results are expected by two Higgs boson search channels which are Standard Model Higgs boson decaying to two $W$ bosons final state and MSSM Higgs decaying to two $ au$ lepton final state. INTNOTEATLASPRIV

Systematics in charged Higgs search in ATLAS Gentile S Università di Roma La Sapienza,INFN 2010 The charged light MH+ &lt;Mtop MSSM Higgs boson production via t-&gt;bH+ and the subsequent decay into H+-&gt;csbar or H+ -&gt;taunu has been studied for the ATLAS experiment. The first channel, dominating at low tan beta region (&lt;1), is explored in the final state with 4 jets and one lepton and missing energy; the second, at high er tan beta region (&gt;3), is searched in two leptons and two jets and missing ener gy final state. The study has been performed using a realistic detector simulation of the s ignal and the SM backgrounds. The discovery sensitivity and the upper limit on BR(t-&gt;gt;b H+) as function of MH+ , assuming the Br(H-&gt;csbar)=1 or Br(H-&gt;taunu)=1, were discussed for different luminosity and center of mass energy scenarios: at root(s)=10 TeV with integrated luminosity=~200 pb-1 and at root(s) = 7 TeV with integrated luminosity = 1 fb-1, obtained using a rescaling tecnique. The main focus of the present paper is on the impact of systematics on these results. INTNOTEATLASPRIV

University of Liverpool Liverpool Searches for Higgs Bosons in the Di-tau Decay Channels at the ATLAS Experiment Leney Katharine Julie Clementine U. Liverpool 2010 The search for the Higgs boson will be one of the primary tasks of the LHC. One of the most promising channels in the search for a low mass Higgs boson ($M_{H}$ ∼120 GeV) will be the scenario where the Higgs is produced via Vector Boson Fusion and subsequently decays to a pair of tau leptons. One of the dominant (and most complex) backgrounds to this analysis is expected to come from $tar{t}$~decays. Monte Carlo samples with a centre-of-mass energy of 14 TeV are used to investigate the contributions from different $tar{t}$~decay modes and to develop methods to reduce the contribution from this background process and improve the overall sensitivity of the analysis. A technique to estimate contributions from background processes when there are insufficient Monte Carlo samples available to calculate this directly is also presented. A low mass Standard Model Higgs boson will require at least 10 $fb^{−1}$~data before a discovery (or exclusion) can be claimed, but extensions to the Standard Model that realise Supersymmetry predict that there should be three neutral Higgs bosons. The production cross-section is strongly enhanced and it is there- fore expected that competitive limits on an MSSM Higgs boson can be made using data from the 2010-2011 LHC data-taking period (1 $fb^{−1}$~expected with 7 TeV centre-of-mass collisions). A search strategy for an MSSM Higgs boson decaying to two taus is presented, focusing on ensuring ana lysis robustness during this early period. Comparisons with the first ATLAS data are also made. technical-report

Higgs Sensitivity in ATLAS Novakova J 2010 Higgs boson searches are one of the main goals of the LHC physics program. Expected Higgs boson exclusion limits that can be reached with an integrated luminosity 1fb^{-1} at a center of mass energy 7 TeV will be shown. The integrated luminosity 1fb^{-1} should be delivered to the ATLAS experiment by the end of 2011 according to the current LHC plans. The sensitivity for both, the Standard Model Higgs boson and the MSSM Higgs bosons, will be discussed. Results of the ongoing effort to measure the Standard Model background to the H->WW channel will be also shown. INTNOTEATLASPRIV

ATLAS discovery prospects for the charged Higgs in the H+ to tau nu final state Klemetti M McGill U. 2010 In the Minimal Super-Symmetric model (MSSM), the decay H+ to tau nu can be a dominant decay channel for the light (m(H+) < m(top) ) charged Higgs boson. Through this channel, the ATLAS detector at the Large Hadron Collider (LHC) could either discover the light H+ or improve the current Tevatron upper limits on B(t to bH+). We evaluate the expected ATLAS upper limit for B(t to b H+), assuming B(H+ to tau nu)=1 and an integrated luminosity of 200 pb-1 gathered at sqrt(s)=10 TeV. INTNOTEATLASPUBL

Universitat de Valencia Valencia Implementation of the ROD Crate DAQ Software for the ATLAS Tile Calorimeter and a Search for a MSSM Higgs Boson decaying into Tau pairs Solans Sánchez Carlos Antonio Valencia U., IFIC (Universidad de Valencia - CSIC) 2010 The ATLAS experiment of the LHC at CERN started its operation in 2009. The ROD Crate DAQ as a part of the Trigger and Data Acquisition system is responsible for the operation of the sub-detector specific hardware at the level of the back-end electronics crates. In particular, it is the framework that controls the Read-Out Driver of the ATLAS Tile Calorimeter which is responsible for the cell energy and time computation based on the Optimal Filtering algorithm. We describe the implementation of the ROD Crate DAQ for the ATLAS Tile Calorimeter. In first place how the specific Tile hardware and software is described in the configuration database. In second place, the characterization of the various plug-ins for the ROD Crate DAQ, specially the ones for the ROD and TBM motherboards. Results from the transition times of the ROD Crate DAQ measured in real data taking scenario during the year 2010 are presented. In the third place, we present the results from the Optimal Filtering validation in terms of energy resolution and time calibration of the calorimeter. A time based cut may be used to develop algorithms to search for the Higgs boson. One of the most interesting channels for this search is within the MSSM. In this model, the Higgs production cross section is enhanced quadratically by a parameter of the model, the tangent of beta, with respect to the Standard Model. It is possible to search for neutral MSSM Higgs bosons decayin g into Tau pairs by setting an upper exclusion limit to its cross section in case of a non observation or by establishing the discovery significance of an excess in the observation. It has been imported into ATLAS, the Bayesian technique developed at CDF to set upper exclusion limits to the Higgs boson production cross section and significance of a possible observation. This method takes into account systematic uncertainties, like luminosity and background cross section, that modify the normalization of the observables and also the contribution of the energy scale uncertainties, such as jet and electromagnetic, that change the shape of the observables. Expected results to the upper exclusion limits and discovery significances for neutral MSSM Higgs bosons decaying to Tau pairs are presented. These are very promising for ATLAS for the first two years of data taking. technical-report

Dresden University Dresden The Discovery Potential of Neutral Supersymmetric Higgs Bosons with Decay to Tau Pairs at the ATLAS Experiment Schaarschmidt Jana TU, Dresden (main) 2010 This work presents a study of the discovery potential for the neutral supersymmetric Higgs bosons h/A/H decaying to tau pairs with the ATLAS experiment at the LHC. The study is based on Monte Carlo samples which are scaled to state-of-the-art cross sections. The analyses are designed assuming an integrated luminosity of 30 1/fb and a center-of-mass energy of sqrt(s) = 14 TeV. The results are interpreted in the m_h^max benchmark scenario. Two final states are analyzed: The dileptonic channel where the two tau leptons decay to electrons or muons and the lepton-hadron channel where one tau decays to an electron or muon and the other tau decays to hadrons. The study of the dilepton channel is based completely on the detailed ATLAS simulation, the analysis of the lepton-hadron channel is based on the fast simulation. The collinear approximation is used to reconstruct the Higgs boson mass and its performance is studied. Cuts are optimized in order to discriminate the signal from background and to maximize the discovery potential given a certain Higgs boson mass hypotheses. In the lepton-hadron channel the selection is split into two analyses depending on the number of identified b-jets. Procedures to estimate the dominant backgrounds from data are studied. The shape and normalization of the Z-&gt;tautau background are estimated from Z-&gt;ll control regions. The ttbar contributions to the signal regions are estimated from ttbar contr ol regions. The individual analyses are combined and sensitivity predictions are made depending on the Higgs boson mass m_A and the coupling parameter tanb. The light neutral MSSM Higgs bosons with m_A = 150 GeV can be discovered when at least tanb = 11 is realized in nature. The heavy neutral MSSM Higgs bosons with m_A = 800 GeV can be discovered for tanb ≥ 44. However, due to the large width of the reconstructed Higgs boson mass and the mass degeneration, only the sum of at least two of the three Higgs boson signals will be visible. technical-report

TU Dresden Dresden Studien zur Produktion neutraler Higgs-Bosonen des Minimal Supersymmetrischen Standardmodells zusammen mit b-Quarks und deren Zerfall in Myonen am ATLAS Experiment Warsinsky Markus Dresden, Tech. U. 2008 This thesis presents a Monte Carlo study of neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) decaying into muons at the ATLAS experiment at the CERN Large Hadron Collider. Signal and background processes are simulated using novel Monte Carlo generators that incorporate parts of higher order corrections and are expected to give a more accurate prediction than previous programs. The SHERPA Monte Carlo generator is validated for its use in the analysis and compared to results obtained with other programs. Where possible, the Monte Carlo event samples are normalized to higher order calculations. To increase the available Monte Carlo statistics, this study is based on the ATLAS fast detector simulation ATLFAST. Differences between ATLFAST and the detailed detector simulation of ATLAS are examined, and, where possible, correction procedures are devised. A cut based analysis is performed assuming an integrated luminosity of 30 fb-1, and optimized with respect to the discovery potential for MSSM Higgs bosons. The systematic uncertainties of the event selection and the Monte Carlo predictions are estimated. A method that can be used to estimate the background from data is presented and evaluated. Last, the discovery potential of the ATLAS experiment in the CP conserving benchmark scenarios of the MSSM is evaluated. One or more of the neutral Higgs bosons of the MSSM can be discovered in the muonic decay mode usin g 30 fb-1 of data for low masses of the pseudoscalar boson A0, if the model parameter tanb is at least 20. For higher masses of the A0, tanb would need to be signi cantly higher to ensure a discovery in the studied decay channel. The sensitivity of ATLAS to MSSM Higgs bosons is multiple times larger than the one of previous and currently running experiments. technical-report

PoS PoS Systematics in charged Higgs search in ATLAS Gentile S Rome U. INFN, Rome 2010 Charged 2010 The charged light MH+ &lt;Mtop MSSM Higgs boson production via t-&gt;bH+ and the subsequent decay into H+-&gt;csbar or H+ -&gt;taunu has been studied for the ATLAS experiment. The first channel, dominating at low tan beta region (&lt;1), is explored in the final state with 4 jets and one lepton and missing energy; the second, at high er tan beta region (&gt;3), is searched in two leptons and two jets and missing ener gy final state. The study has been performed using a realistic detector simulation of the s ignal and the SM backgrounds. The discovery sensitivity and the upper limit on BR(t-&gt;gt;b H+) as function of MH+ , assuming the Br(H-&gt;csbar)=1 or Br(H-&gt;taunu)=1, were discussed for different luminosity and center of mass energy scenarios: at root(s)=10 TeV with integrated luminosity=~200 pb-1 and at root(s) = 7 TeV with integrated luminosity = 1 fb-1, obtained using a rescaling tecnique. The main focus of the present paper is on the impact of systematics on these results. research-article

Göpfert, Thomas Dresden Studies of Charged Higgs Boson Observability in the $H \to tb$ Decay at the ATLAS Experiment within the Minimal Supersymmetric Standard Model Göpfert Thomas TU, Dresden (main) 2010 This thesis presents a Monte Carlo study of the search for charged Higgs bosons heavier than the mass of the top quark within the Minimal Supersymmetric Standard Model (MSSM) at the ATLAS experiment at the CERN Large Hadron Collider. Charged Higgs bosons are predicted in many non-minimal Higgs extensions of the Standard Model. Their discovery would be a clear signal for the existence of New Physics beyond the Standard Model, possibly the first experimental evidence to be found if the MSSM is realized in nature. The feasibility of detecting the heavy charged Higgs boson with a mass up to 600 GeV is studied in the decay channel $H^{+}\rightarrow \bar{t}b$ for an integrated luminosity of 30 $fb^{−1}$ at a center-of-mass energy of $\sqrt{s}$=10TeV. A major difficulty for charged Higgs boson reconstruction is the combinatorial background in the complex multi-jet final state environment. It is shown that this can be overcome by applying a kinematic fitting procedure and by a subsequent cut-based event and candidate selection. An iterative solution of the developed kinematic fit with non-linear constraints is presented. In addition, the reconstruction of charged Higgs bosons makes high demands on the ability to identify jets containing b-hadrons. A special b-tagging algorithm is introduced and a comparison with first ATLAS data is presented showing good agreement of the expected performance. This study is performed with a realistic simul ation of the ATLAS detector and takes into account all dominant experimental uncertainties and statistical uncertainties arising from limited Monte Carlo statistics. The result is given in terms of discovery and exclusion contours in the $(m_{H^{+}}, tan\beta)$ parameter space in the $m_{h}$-max scenario of the MSSM. This study indicates that the heavy charged Higgs boson can be discovered in this decay channel only for large values of $tan\beta$. It, however, can contribute to a combined $H^{+}$ sensitivity including other decay channels. Compared to previous studies the discovery reach could be improved. technical-report

Searches for a Neutral MSSM Higgs Boson Decaying to $ au_h au_l$ in $sqrt{s} = 7$ TeV Collisions at the ATLAS Experiment Leney KJC University of Liverpool, University of the Witwatersrand Burdin S University of Liverpool Vickey T University of the Witwatersrand, University of Oxford 2010 A low mass Standard Model Higgs boson will require at least 10invfb~data before a discovery (or exclusion) can be claimed, but extensions to the Standard Model that realise Supersymmetry predict that there should be three neutral Higgs bosons. The production cross-section is strongly enhanced and it is therefore expected that competitive limits on an MSSM Higgs boson can be made using data from the 2010-2011 LHC data-taking period (1invfb~expected with 7~TeV~centre-of-mass collisions). A search strategy for an MSSM Higgs boson decaying to two taus is presented, focusing on ensuring analysis robustness during this early period. INTNOTEATLASPRIV

Higgs searches at the LHC Nakamura K Tokyo U., ICEPP 2010 During the operation at the center-of-mass energy of 7~TeV, the LHC is expected to deliver up to 1~fb$^{-1}$ of $pp$ collision data by the end of 2011. Prospect for the Higgs searches at the LHC with 1~fb$^{-1}$ of integrated luminosity of data is discussed. Promising results are expected by two Higgs boson search channels which are Standard Model Higgs boson decaying to two $W$ bosons final state and MSSM Higgs decaying to two $ au$ lepton final state. INTNOTEATLASPUBL

A Search for Light CP-Odd Higgs Bosons Decaying to mu+ mu- in ATLAS Evans H Indiana University Klemetti M McGill University Potter C University of Oregon Yang Y Indiana University 2011 We present a search for a \CP -odd Higgs boson, \aone , with mass less than $2 m_B$, decaying to \mumu , using $\sim$37 \ipb\ of \pp\ collisions at \rts\ = 7 \TeV\ collected by the ATLAS detector at the LHC. Such a light Higgs is predicted in Next-to-Minimal Supersymmetric Models (NMSSM) designed to solve the $\mu$-term problem of the Minimal Supersymmetric Standard Model (MSSM). Its presence can significantly alter the phenomenology of the MSSM Higgs sector. We set new limits on the production cross-section for $gg \to \aone$ in the mass regions 6 -- 9 GeV and 11 -- 12 GeV. INTNOTEATLASPRIV

Search for neutral MSSM Higgs bosons decaying to tau+ tau- pairs in proton-proton collisions at sqrt{s} = 7 TeV with the ATLAS Experiment Anders C Dingfelder J Goussiou A Gross E Keller J Kroseberg J Lai S Leney K Ma L Moeser N Nakamura K Pedraza Morales I Rosati S Schmitz M Schwindt Th Tanaka J Thoma S Vickey T Warsinsky M Wu SL 2011 A search for neutral Higgs bosons $A$, $H$, $h$ in the Minimal Supersymmetric Standard Model with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of $7\tev$, corresponding to an integrated luminosity of $36 \ipb$, and focuses on Higgs decays into two $\tau$ leptons, \Htotautau, where one $\tau$ lepton decays leptonically and the other hadronically. After signal selection, $206$ events are observed in this data sample. The observed number of events is consistent with the total background estimate of $195 \pm 33$ events, where the most important background contributions are obtained from data control samples. A $95\%$ confidence-level exclusion limit for MSSM $A/H/h$ production is derived as a function of the parameters $m_A$ and $\tan\beta$. INTNOTEATLASPRIV

Search for neutral MSSM Higgs bosons decaying to tau+ tau- pairs in proton-proton collisions at sqrt{s} = 7 TeV with the ATLAS Experiment Anders C Dingfelder J Goussiou A Gross E Keller J Kroseberg J Lai S Leney K Ma L Moeser N Nakamura K Pedraza Morales MI Rosati S Schmitz M Schwindt Th Tanaka J Thoma S Vickey T Warsinsky M Wu SL 2011 A search for neutral Higgs bosons $A$, $H$, $h$ in the Minimal Supersymmetric Standard Model with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of $7\tev$, corresponding to an integrated luminosity of $36 \ipb$, and focuses on Higgs decays into two $\tau$ leptons, \Htotautau, where one $\tau$ lepton decays leptonically and the other hadronically. After signal selection, $206$ events are observed in this data sample. The observed number of events is consistent with the total background estimate of $195 \pm 33$ events, where the most important background contributions are obtained from data control samples. A $95\%$ confidence-level exclusion limit for MSSM $A/H/h$ production is derived as a function of the parameters $m_A$ and $\tan\beta$. INTNOTEATLASPRIV

Data-driven estimation of the background to charged Higgs boson searches using hadronically-decaying tau final states in ATLAS Arghir S Behar S Cavaliere V Coadou Y Czodrowski P Flechl M Kopp A McCarn A zur Nedden M Neubauer M Randle-Conde A Rozen Y Sekula S Takahashi Y Tomoto M Vickey T Xella S 2011 The experimental observation of charged Higgs bosons, $H^{\pm}$, which are theoretically predicted by many non-minimal Higgs scenarios, would indicate new physics beyond the Standard Model. In the Minimal Supersymmetric Standard Model, for example, the dominant production mode at the LHC for these Higgs bosons, when $m_{H^+} < m_t$, takes place in $t\overline{t}$ events via the top-quark decay $t\rightarrow H^{+}b$ with $H^{+}\rightarrow\tau \nu$ dominating for most values of $\tan\beta$. Two channels with a hadronically decaying $\tau$ coming from the charged Higgs boson are studied. The delivery of the first 37 pb$^{-1}$ of $\sqrt{s}=7$ TeV collision data allows many significant backgrounds to be estimated with data-driven methods, which represent the primary focus of this note and a crucial step towards ATLAS searches for the charged Higgs boson. INTNOTEATLASPRIV

Higgs Boson Sensitivity in ATLAS Novakova Jana 2011 Higgs boson searches are one of the main goals of the ATLAS physics program. Higgs boson exclusion limits expected, with an integrated luminosity 1 fb-1 in proton-proton collisions at the centre of mass 7 TeV, are shown. This integrated luminosity can be reached by the end of year 2011 according to the LHC plans. The expected sensitivity for both, the Standard Model Higgs boson and the MSSM Higgs bosons, is discussed. The results are based on the Monte Carlo simulations rescaled from 14/10 TeV studies. Extraction of the background to the H -&gt; W +W - channel from real data is also shown. INTNOTEATLASPRIV

Higgs Boson Sensitivity in ATLAS Novakova Jana Charles U. 2011 Higgs boson searches are one of the main goals of the ATLAS physics program. Higgs boson exclusion limits expected, with an integrated luminosity 1 fb-1 in proton-proton collisions at the centre of mass 7 TeV, are shown. This integrated luminosity can be reached by the end of year 2011 according to the LHC plans. The expected sensitivity for both, the Standard Model Higgs boson and the MSSM Higgs bosons, is discussed. The results are based on the Monte Carlo simulations rescaled from 14/10 TeV studies. Extraction of the background to the H -&gt; W +W - channel from real data is also shown. INTNOTEATLASPUBL

Search for the SM and MSSM Higgs boson(s) with ATLAS 2010 data Yuan L IHEP, Beijing and LPNHE, Paris 2011 The ATLAS experiment has searched for the the SM Higgs boson in decays to ZZ, WW and γγ final states and the H/A of the MSSM in ττ states. No significant evidence for a signal is found in any search, and limits are presented either as a multiple of the standard model expected rate or in the mA-tanβ plane. INTNOTEATLASPRIV

A Search for Light CP-Odd Higgs Bosons Decaying to mu+ mu- in ATLAS 2011 We present a search for a very light \CP -odd Higgs boson, \aone , decaying to \mumu , using 36.7 \ipb\ of \pp\ collisions at \rts\ = 7 \TeV\ recorded by the ATLAS detector at the LHC. Such a light Higgs is predicted in Next-to-Minimal Supersymmetric Standard Models (NMSSM) designed to solve the $\mu$-term problem of the Minimal Supersymmetric Standard Model (MSSM). Its presence can significantly alter the phenomenology of the MSSM Higgs sector. We set new limits on the production cross section times branching ratio, \sigggaBamm , for \aone\ masses of 6 -- 9 \GeV\ and 11 -- 12 \GeV , avoiding the region dominated by the \Ups\ resonances. INTNOTEATLASPUBL

Search for neutral MSSM Higgs bosons decaying to tau+ tau- pairs in proton-proton collisions at sqrt{s} = 7 TeV with the ATLAS Experiment 2011 A search for neutral Higgs bosons $A$, $H$, $h$ in the Minimal Supersymmetric Standard Model with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of $7\tev$, corresponding to an integrated luminosity of $36 \ipb$, and focuses on Higgs decays into two $\tau$ leptons, \Htotautau, where one $\tau$ lepton decays leptonically and the other hadronically. After signal selection, $206$ events are observed in this data sample. The observed number of events is consistent with the total background estimate of $195 \pm 33$ events, where the most important background contributions are obtained from data control samples. A $95\%$ confidence-level exclusion limit for MSSM $A/H/h$ production is derived as a function of the parameters $m_A$ and $\tan\beta$. INTNOTEATLASPUBL

Data-driven estimation of the background to H+ searches with hadronic-tau final states Arghir S Behar S Cavaliere V Coadou Y Czodrowski P Flechl M Kopp A McCarn A zur Nedden M Neubauer M Randle-Conde A Rozen Y Sekula S Takahashi Y Tomoto M Vickey T Xella S 2011 Theoretically predicted by many non-minimal Higgs scenarios, the experimental observation of charged Higgs bosons, $H^{\pm}$, would indicate new physics beyond the Standard Model. In the minimal supersymmetric extension to the Standard Model (MSSM), for example, the dominant production mode at the LHC for these Higgs bosons, when $m_{H^+} < m_t$, takes place in $t\overline{t}$ events via the top quark decay $t\rightarrow H^{+}b$ with $H^{+}\rightarrow\tau + \nu$ dominating for most values of $\tan\beta$, the ratio of the vacuum expectation values of the two Higgs doublets. This note considers both the $\tau+$ jets and $\tau+$ lepton channels with hadronically-decaying $\tau$s coming from the charged Higgs. The delivery of the first $\sqrt{s}=7$ TeV collision data allows for the estimation of many significant backgrounds to be done in a data-driven way, the primary focus of this note and a crucial step toward searches for these bosons. INTNOTEATLASINT

Higgs searches with ATLAS Moeser N University of Bonn 2011 Higgs boson searches in the Standard Model, the Minimal Supersymmetric Standard Modell and Next-to-Minimal Supersymmetric Standard Modell are presented. The searches are based on data taken in 2010. Exclusion limits in all channels are established. INTNOTEATLASPRIV

Search for neutral Higgs bosons in the decay mode $H \rightarrow \tau^+\tau^- \rightarrow e\mu + $ 4 neutrinos in proton-proton collisions at $\sqrt{s}=7$~TeV with the ATLAS Experiment Gross E Department of Particle Physics, The Weizmann Institute of Science, Rehovot, Israel Nakamura K Department of Particle Physics, University of Tokyo, Japan Nativ E Department of Particle Physics, The Weizmann Institute of Science, Rehovot, Israel Pitt M Department of Particle Physics, The Weizmann Institute of Science, Rehovot, Israel von Radziewski H Fakult\"at f\"ur Mathematik und Physik, Albert-Ludwigs Universit\"at, Freiburg im Br., Germany Schillo C Fakult\"at f\"ur Mathematik und Physik, Albert-Ludwigs Universit\"at, Freiburg im Br., Germany Silbert O Department of Particle Physics, The Weizmann Institute of Science, Rehovot, Israel Schumacher M Fakult\"at f\"ur Mathematik und Physik, Albert-Ludwigs Universit\"at, Freiburg im Br., Germany Tanaka J Department of Particle Physics, University of Tokyo, Japan Warsinsky M - 2011 A search for neutral Higgs bosons decaying to a pair of tau leptons in the final state $e \mu + 4$ neutrinos is presented based on proton-proton collisions at a center-of-mass energy of $7\tev$, corresponding to an integrated luminosity of \currentlumi. After applying the signal selection, $70$ events are observed in this data sample. The observed number of events is consistent with the total background estimate of $61 \pm 8$ events {\it numbers need to be checked !}. A model independent limit on production of a scalar boson $\phi$ decaying to a pair of tau leptons $\sigma(pp\to\phi)\times BR(\phi\to\tau\tau)$ is derived at $95\%$ confidence-level. The results is also interpreted as a limit on $h/H/A$ production in the context of the Minimal Supersymmetric Standard Model (MSSM), where parameter space in the \tanb-vs.-\MA plane of the $M_\mathrm{h}^\mathrm{max}$ scenario of the MSSM is excluded. INTNOTEATLASPRIV

Search for neutral MSSM Higgs bosons decaying to $ au^+ au^-$ pairs in proton-proton collisions at $sqrt{s}=7$~TeV with the ATLAS Experiment Anders C Dingfelder J Goussiou A Gross E Keller J Kroseberg J Lai S Leney K Ma L Moeser N Nakamura K Pedraza Morales MI Rosati S Schmitz M Schwindt Th Tanaka J Thoma S Vickey T Warsinsky M Wu SL 2011 A search for the neutral Higgs bosons $A$, $H$, and $h$ in the Minimal Supersymmetric Standard Model (MSSM) with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of $7 Tev$, corresponding to an integrated luminosity of $36.5$ pb$^{-1}$, and focuses on Higgs decays Htotautau, where one $ au$ lepton decays leptonically and the other hadronically. After signal selection, $206$ events are observed in this data sample. The observed number of events is consistent with the total background estimate of $195 pm 33$ events, where the most important background contributions are estimated or validated with data control samples. Exclusion limits at the $95%$ confidence level are derived for the Higgs production cross section as a function of the Higgs mass and for MSSM $A/H/h$ production as a function of the parameters $m_A$ and $tan beta$. INTNOTEATLASPRIV

Search for neutral MSSM Higgs bosons decaying to tau+tau- pairs in proton-proton collisions at $sqrt{s}=7$~TeV with the ATLAS Experiment Anders C Dingfelder J Goussiou A Gross E Keller J Kroseberg J Lai S Leney K Ma L Moeser N Nakamura K Nativ E Pedraza Morales I Pitt M Rosati S Schillo C Silbert O Schmitz M Schumacher M Schwindt T Tanaka J Thoma S Vickey T von Radziewski H Warsinsky M Wu SL 2011 A search for the neutral Higgs bosons $A$, $H$, and $h$ in the Minimal Supersymmetric Standard Model (MSSM) with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of $7 Tev$, corresponding to an integrated luminosity of $36.5$ pb$^{-1}$, and focuses on Higgs decays Higgs -> tau+ tau-. After signal selection, $276$ events are observed in this data sample. The observed number of events is consistent with the total background estimate of $257 pm 40$ events, where the most important background contributions are estimated or validated with data control samples. Exclusion limits at the $95%$ confidence level are derived for the Higgs production cross section as a function of the Higgs mass and for MSSM $A/H/h$ production as a function of the parameters $m_A$ and $tan beta$. INTNOTEATLASPRIV

Search for neutral MSSM Higgs bosons decaying to tau+ tau- pairs in proton-proton collisions at sqrt{s} = 7 TeV with the ATLAS Experiment Anders C Dingfelder J Goussiou A Gross E Keller J Kroseberg J Lai S Leney K Ma L Moeser N Nakamura K Pedraza Morales I Rosati S Schmitz M Schwindt Th Tanaka J Thoma S Vickey T Warsinsky M Wu SL 2011 A search for neutral Higgs bosons $A$, $H$, $h$ in the Minimal Supersymmetric Standard Model with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of $7\tev$, corresponding to an integrated luminosity of $36 \ipb$, and focuses on Higgs decays into two $\tau$ leptons, \Htotautau, where one $\tau$ lepton decays leptonically and the other hadronically. After signal selection, $206$ events are observed in this data sample. The observed number of events is consistent with the total background estimate of $195 \pm 33$ events, where the most important background contributions are obtained from data control samples. A $95\%$ confidence-level exclusion limit for MSSM $A/H/h$ production is derived as a function of the parameters $m_A$ and $\tan\beta$. INTNOTEATLASPRIV

First results on Higgs boson searches (SM + MSSM) and prospects from ATLAS Elmsheuser J LMU Munich 2011 First results on Higgs boson searches (SM + MSSM) and prospects from ATLAS INTNOTEATLASPRIV

Tau physics in ATLAS Kuehn S University of Freiburg 2011 Tau Leptons play an important role in Higgs and New Physics searches. In the talk results using data from pp collisions at 7 TeV, collected during 2010, with the ATLAS detector are presented. The observation of Z and W bosons decaying to Tau Leptons is shown. And results of searches for Charged and Neutral Higgs bosons of MSSM decaying in tau final are reported. INTNOTEATLASPRIV

Search for Charged Higgs Bosons in the $\tau$+jets Final State in $t\overline{t}$ Decays with 1.03 fb$^{-1}$ of $pp$ Collision Data Recorded at $\sqrt{s} = 7$ TeV with the ATLAS Experiment---Supporting Note Cavaliere V Czodrowski P Flechl M Isaksson C Kopp A Martyniuk A McCarn A Owen M zur Nedden M Neubauer M Patel N Randle-Conde A Riu I Saavedra A Sekula S Vickey T 2011 This note presents the results of a search for charged Higgs bosons, $H^{\pm}$, in 1.03 fb$^{-1}$ of proton-proton collision data recorded at $\sqrt{s}=7$ TeV with the ATLAS experiment at the LHC using the $\tau$+jets channel in $t\overline{t}$ decays with a hadronically decaying $\tau$ lepton in the final state. The data agree with the SM expectation leading to a limit on the product of branching ratios BR($t \to bH^{\pm}) \times$ BR($H^\pm \to \tau\nu$) of $0.03-0.10$ for $H^\pm$ masses in the range $90 \GeV<m_{H^\pm}<160 \GeV$. In the context of the MSSM values of $\tan \beta$ larger than $22-30$ are excluded in the mass range $90 \GeV< m_{H^\pm}< 140 \GeV$. INTNOTEATLASPRIV

SUSY Higgs results from 2010 ATLAS data Schwindt T Bonn University 2011 This poster presents results on searches for charged and neutral Higgs bosons of the MSSM and NMSSM. Limits are set on cross section times branching ratio for MSSM H/A-&gt;tautau, which in places surpass the Tevatron bounds, and for a light a1-&gt;mumu decay in the NMSSM. Additional studies on discrimination varibles and background estimation for H+ -&gt; tau nu searches in hadronic modes are also shown. INTNOTEATLASPRIV

Higgs Boson Searches with ATLAS based on 2010 Data Schumacher M ALU Freiburg 2011 The results of Higgs Boson searches with the ATLAS detector based on 2010 proton proton collision data corresponding to integrated luminosities of to 39 pb$^{-1}$ are presented. Searches for H to 2 photons, H to W⁺W⁻ to l nu l nu, and H to ZZ to l+ l-/nunu and l+l-, in the context of the Standard Model (SM), for H to tau tau in the context of the Minimal Supersymmetric Extension of the Standard Model (MSSM) and for a generic scalar at low mass in the vicinity of the $Upsilon$ resonance decaying to a pair of muons are discussed. All observations are in agreement with the expectations from the background-only hypothesis. Hence exclusion limits at 95% confidence level are derived. INTNOTEATLASPRIV

Higgs Boson Searches with ATLAS based on 2010 Data Schumacher Markus Freiburg U. 2011 15 21 The results of Higgs Boson searches with the ATLAS detector based on 2010 proton proton collision data corresponding to integrated luminosities of up to 39 pb-1are presented. Searches for H --> 2 photons, H --> W+W- --> l+l- 2 neutrinos and H --> ZZ --> l+l- 2 neutrinos / l+l- qqbar in the context of the Standard Model (SM), for H--> tau+ tau- in the context of the Minimal Supersymmetric Extension of the Standard Model (MSSM) and for a generic scalar at low mass in the vicinity of the Ypsilon resonance decaying to a pair of muons are discussed. All observations are in agreement with the expectations from the background-only hypothesis. Hence exclusion limits at 95% confidence level are derived research-article

Higgs searches with ATLAS "Hoffman J A Southern Methodist University" 2011 In this talk, we discuss search strategies for the Higgs boson with the ATLAS detector at the LHC. A summary of the sensitivity of ATLAS to discover a Standard Model Higgs boson will be presented in various decay channels. Some prospects for Minimal Supersymmetric Standard Model Higgs searches are also included. Furthermore, we present the latest results based on the ATLAS data collected in 2010 and 2011. Limits are given on the production cross section relative to the Standard Model and to the MSSM predictions at the 95% CL. INTNOTEATLASPRIV

Search for neutral Higgs bosons in the decay mode H -> tautau -> ll+ 4 neutrinos in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS Experiment Barberio E Beckingham M Chen X Ferrer A Fiorini L Flechl M Gross E Gumpert C Mellado B Pan Y Pitt M von Radziewski H Schumacher M Schillo C Shao T Silbert O Solans C Tanaka J Torralba G Utecht N Valls J Warsinsky M 2011 A search for neutral Higgs bosons is presented based on proton-proton collisions at a nominal center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 1.06 fb-1. This search focuses on the decay mode Htotautau where the two tau lepton decays leptonically. After applying the signal selection, the observed number of events is consistent with the total background estimate in the inclusive data sample and 1 in the >=1-jet data sample. The results are interpreted in the context of the Standard Model (SM) and Minimal Supersymmetric Standard Model (MSSM) and exclusion limits are derived as a function of m_H and tanb-vs.-M_A plane respectively. INTNOTEATLASPRIV

Search for MSSM Higgs bosons in ATLAS Flechl M Freiburg 2011 Talk for EPS 2011 on the status of ATLAS results on MSSM Higgs boson searches. Presented are results on h/A/H-&gt;tautau, H+-&gt;cs, and H+-&gt;taunu. INTNOTEATLASPRIV

Search for Neutral MSSM Higgs Bosons in inclusive $\mu\mu$ Final States in $\sqrt{s}=7$ TeV p-p Collisions with the ATLAS Detector Grohs J P TU Dresden Kortner S MPI Munich Stern S MPI Munich Vest A TU Dresden 2011 This note presents the search for neutral MSSM Higgs bosons decaying into two muons with the ATLAS detector at the LHC. The analysis is performed on 1067 pb$^{-1}$ of proton-proton collisions at a centre of mass energy of $\sqrt{s}$ = 7 TeV. Exclusion limits are evaluated as a function of $m_A$ and $\tan\beta$ in inclusive dimuon final states for neutral MSSM Higgs boson masses from 110 to 250 GeV. INTNOTEATLASPRIV

Search for neutral MSSM Higgs bosons in the decay mode H->tau tau -> hadhad + 2 neutrinos in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS Experiment Barberio E Davey W Dingfelder J Dhaliwal S Glatzer J Hanninger G N Mader W Morgenstern M Pranko A Rosendahl P Straessner A Stugu B Urquijo P Varouchas D Volpi M Xella S Zanzi D Zinonos Z 2011 A search for neutral MSSM Higgs bosons $A$, $H$, $h$ with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of $7 TeV$, corresponding to an integrated luminosity of 653.3/pb and focuses on Higgs decays into two $\tau$ leptons, $A/H/h \to \tau^+ \tau^-$, where both $\tau$ leptons decay hadronically. After signal selection, 126 events are observed in this data sample. The observed number of events is consistent with the background estimate of 133 $\pm$ 13 (stat) $\pm$ X (syst) events. An exclusion limit for the neutral MSSM CP-odd Higgs boson production is derived as a function of cross section times branching ratio. This limit is also presented as a function of two parameters $m_A$ and $\tan\beta$. INTNOTEATLASPRIV

Search for Neutral Higgs Bosons H → τ+τ− → lτ with the ATLAS Detector in 7 TeV Collisions Anders C Banerjee S Boddy C Bristow T Dingfelder J Farrington S Galea C Hanawa K Heng Y Hsu S-C Keller J Kroseberg J Leney KJC Nakamura K Pedraza-Morales M-I Pranko A Rompotis N Schwindt T Tanaka J Thoma S Varouchas D Vickey T Wang T Wu S-L 2011 A search for neutral Higgs bosons decaying into pairs of τ leptons performed with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of 7 TeV, corresponding to an integrated luminosity of 1063 pb−1, and focuses on final states where one τ lepton decays leptonically and the other hadronically. After signal selection, 1993 events are observed in this data sample. The observed number of events is consistent with the total background estimate of 2100 ± 321 events, which is obtained using a combination of Monte Carlo and data driven techniques. Exclusion limits are derived as a function of production cross section times branching ratio for a generic Higgs boson φ as a function of Higgs boson mass and for the case of the Minimal Supersymmetric Standard Model (MSSM) also expressed as a function of the parameters mA and tan β. INTNOTEATLASPRIV

BSM Higgs Searches Mader W 2011 BSM Higgs Searches INTNOTEATLASPRIV

ATLAS Searches for Higgs Bosons Beyond the Standard Model Vickey T 2011 The search for the neutral and charged Higgs boson(s) beyond the Standard Model is presented, based on the ATLAS data collected in 2010 and 2011. A wide region of the MSSM parameter space is excluded via searches for Higgs boson decays into two tau-leptons, with an additional sensitivity improvement from the di-muon decay channel. The di-muon final state is additionally explored in the region of invariant masses below 12 GeV, motivated by the search for the light CP-odd Higgs boson predicted by the Next-to-Minimal Supersymmetric Models. The experimental observation of charged Higgs bosons would provide a clear signature of the physics beyond the Standard Model. Several final state topologies are explored, with Higgs bosons originating from the top-quark decays in top pair events and subsequently decaying into tau+nu or c bar{s}. INTNOTEATLASPRIV

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Inst. Bunse Moritz Dortmund U. Buran Torleiv Oslo U. Burckhart Helfried CERN Burdin Sergey Liverpool U. Burgess Thomas Bergen U. Burke Stephen Rutherford Busato Emmanuel Clermont-Ferrand U. Bussey Peter Glasgow U. Buszello Claus-Peter Uppsala U., Inst. Theor. Phys. Butin Francois CERN Butler Bart SLAC Butler John Boston U. Buttar Craig Glasgow U. Butterworth Jonathan University Coll. London Buttinger William Cambridge U. Byatt Tom University Coll. London Cabrera Urban Susana Valencia U., IFIC Caforio Davide INFN, Bologna Cakir Orhan Ankara U. Calafiura Paolo LBL, Berkeley Calderini Giovanni Paris U., VI-VII Calfayan Philippe Munich U. Calkins Robert Northern Illinois U. Caloba Luiz Rio de Janeiro Federal U. Caloi Rita INFN, Rome Calvet David Clermont-Ferrand U. Calvet Samuel Clermont-Ferrand U. Camacho Toro Reina Clermont-Ferrand U. Camarri Paolo INFN, Rome Cambiaghi Mario INFN, Pavia Cameron David Oslo U. Campana Simone CERN Campanelli Mario University Coll. London Canale Vincenzo INFN, Naples Canelli Florencia Chicago U., EFI Canepa Anadi TRIUMF Cantero Josu Madrid, Autonoma U. Capasso Luciano INFN, Naples Garrido Maria Del Mar Capeans CERN Caprini Irinel Bucharest, IFIN-HH Caprini Mihai Bucharest, IFIN-HH Capriotti Daniele Munich, Max Planck Inst. Capua Marcella INFN, Cosenza Caputo Regina SUNY, Stony Brook Caramarcu Costin Bucharest, IFIN-HH Cardarelli Roberto INFN, Rome Carli Tancredi CERN Carlino Gianpaolo INFN, Naples Carminati Leonardo INFN, Milan Caron Bryan TRIUMF Caron Sascha Freiburg U. Montoya German D.Carrillo Wisconsin U., Madison Carter Antony Queen Mary, U. of London Carter Janet Cambridge U. Carvalho Joao LIP, Lisbon Casadei Diego New York U. Casado Maria Pilar Barcelona, IFAE Cascella Michele INFN, Pisa Caso Carlo INFN, Genoa Castaneda Hernandez Alfredo Martin Wisconsin U., Madison Castaneda-Miranda Elizabeth Wisconsin U., Madison Castillo Gimenez Victoria Valencia U., IFIC Castro Nuno Filipe LIP, Lisbon Cataldi Gabriella INFN, Lecce Cataneo Fernando CERN Catinaccio Andrea CERN Catmore James Lancaster U. Cattai Ariella CERN Cattani Giordano INFN, Rome Caughron Seth Michigan State U. Cauz Diego INFN, Udine Cavalleri Pietro Paris U., VI-VII Cavalli Donatella INFN, Milan Cavalli-Sforza Matteo Barcelona, IFAE Cavasinni Vincenzo INFN, Pisa Ceradini Filippo INFN, Rome Santiago Cerqueira Augusto Rio de Janeiro Federal U. Cerri Alessandro CERN Cerrito Lucio Queen Mary, U. of London Cerutti Fabio Frascati Cetin Serkant Ali Dogus U., Kadikoy Cevenini Francesco INFN, Naples Chafaq Aziz Casablanca U. Chakraborty Dhiman Northern Illinois U. Chan Kevin Alberta U. Chapleau Bertrand McGill U. Chapman John Derek Cambridge U. Chapman John Wehrley Michigan U. Chareyre Eve Paris U., VI-VII Charlton Dave Birmingham U. Chavda Vikash Manchester U. Chavez Barajas Carlos Alberto CERN Cheatham Susan McGill U. Chekanov Sergei Argonne Chekulaev Sergey TRIUMF Chelkov Gueorgui Dubna, JINR Chelstowska Magda Anna NIKHEF, Amsterdam Chen Chunhui Iowa State U. Chen Hucheng Brookhaven Chen Shenjian Nanjing U. Chen Tingyang Nanjing U. Chen Xin Wisconsin U., Madison Cheng Shaochen Beijing, Inst. High Energy Phys. Cheplakov Alexander Dubna, JINR Chepurnov Vladimir Dubna, JINR Cherkaoui El Moursli Rajaa Mohammed V U., Agdal Chernyatin Valeriy Brookhaven Cheu Elliott Arizona U. Cheung Sing-Leung Toronto U. Chevalier Laurent DAPNIA, Saclay Chiefari Giovanni INFN, Naples Chikovani Leila Tbilisi State U. Tbilisi, Inst. Phys. Childers John Taylor Kirchhoff Inst. Phys. Chilingarov Alexandre Lancaster U. 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Cogan Joshua Godfrey SLAC Coggeshall James Illinois U., Urbana Cogneras Eric CC, Villeurbanne Cojocaru Claudiu Carleton U. Colas Jacques Annecy, LAPP Colijn Auke-Pieter FOM, Amsterdam Collard Caroline Orsay, LAL Collins Neil Birmingham U. Collins-Tooth Christopher Glasgow U. Collot Johann LPSC, Grenoble Colon German Massachusetts U., Amherst Conde Muino Patricia LIP, Lisbon Coniavitis Elias Oxford U. Conidi Maria Chiara Barcelona, IFAE Consonni Michele NIKHEF, Amsterdam Consorti Valerio Freiburg U. Constantinescu Serban Bucharest, IFIN-HH Conta Claudio INFN, Pavia Conventi Francesco INFN, Naples Cook James CERN Cooke Mark LBL, Berkeley Cooper Ben University Coll. London Cooper-Sarkar Amanda Oxford U. Cooper-Smith Neil Royal Holloway, U. of London Copic Katherine Nevis Labs, Columbia U. Cornelissen Thijs INFN, Genoa Corradi Massimo INFN, Bologna Corriveau Francois McGill U. Cortes-Gonzalez Arely Illinois U., Urbana Cortiana Giorgio Munich, Max Planck Inst. 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Demichev Mikhail Dubna, JINR Demirkoz Bilge Barcelona, IFAE Deng Jianrong UC, Irvine Denisov Sergey Serpukhov, IHEP Derendarz Dominik Cracow, INP Derkaoui Jamal Eddine Oujda U. Derue Frederic Paris U., VI-VII Dervan Paul Liverpool U. Desch Klaus Kurt Bonn U. Devetak Erik SUNY, Stony Brook Deviveiros Pier-Olivier Toronto U. Dewhurst Alastair Rutherford DeWilde Burton SUNY, Stony Brook Dhaliwal Saminder Toronto U. Dhullipudi Ramasudhakar Brookhaven Di Ciaccio Anna INFN, Rome Di Ciaccio Lucia Annecy, LAPP Di Girolamo Alessandro CERN Di Girolamo Beniamino CERN Di Luise Silvestro INFN, Rome Di Mattia Alessandro Michigan State U. Di Micco Biagio CERN Di Nardo Roberto INFN, Rome Di Simone Andrea INFN, Rome Di Sipio Riccardo INFN, Bologna Diaz Marco Aurelio Chile U., Catolica Diblen Faruk Gaziantep U. Diehl Edward Michigan U. Dietrich Janet DESY Dietzsch Thorsten Kirchhoff Inst. Phys. Diglio Sara Orsay, LAL Yagci Kamile Dindar Southern Methodist U. Dingfelder Jochen Bonn U. Dionisi Carlo INFN, Rome Dita Petre Bucharest, IFIN-HH Dita Sanda Bucharest, IFIN-HH Dittus Fridolin CERN Djama Fares Marseille, CPPM Djobava Tamar Tbilisi State U. Tbilisi, Inst. Phys. Barros do Vale Maria Aline Rio de Janeiro Federal U. Do Valle Wemans Andre LIP, Lisbon Doan Thi Kieu Oanh Annecy, LAPP Dobbs Matt McGill U. Dobinson Robert CERN Dobos Daniel Dortmund U. Dobson Ellie CERN Dobson Marc UC, Irvine Dodd Jeremy Nevis Labs, Columbia U. Doglioni Caterina Oxford U. Doherty Tom Glasgow U. Doi Yoshikuni KEK, Tsukuba Dolejsi Jiri Charles U. Dolenc Irena Stefan Inst., Ljubljana Dolezal Zdenek Charles U. Dolgoshein Boris Moscow Phys. Eng. Inst. Dohmae Takeshi ICTP, Trieste Donadelli Marisilvia Sao Paulo U. Donega Mauro Pennsylvania U. Donini Julien LPSC, Grenoble Dopke Jens CERN Doria Alessandra INFN, Naples dos Anjos Andre Wisconsin U., Madison Dosil Mireia Barcelona, IFAE Dotti Andrea INFN, Pisa Dova Maria-Teresa La Plata U. Dowell John Birmingham U. Doxiadis Alexander FOM, Amsterdam Doyle Tony Glasgow U. Drasal Zbynek Charles U. Drees Jurgen Wuppertal U. Dressnandt Nandor Pennsylvania U. Drevermann Hans CERN Driouichi Chafik Bohr Inst. Dris Manolis Natl. Tech. U., Athens Dubbert Jorg Munich, Max Planck Inst. Dubbs Tim UC, Santa Cruz Dube Sourabh LBL, Berkeley Duchovni Ehud Weizmann Inst. Duckeck Guenter Munich U. Dudarev Alexey CERN Dudziak Fanny Iowa State U. Duhrssen Michael CERN Duerdoth Ian Manchester U. Duflot Laurent Orsay, LAL Dufour Marc-Andre McGill U. Dunford Monica CERN Duran Yildiz Hatice Dumlupinar U. Duxfield Robert Sheffield U. Dwuznik Michal AGH-UST, Cracow Dydak Friedrich CERN Dzahini Daniel LPSC, Grenoble Duren Michael Giessen U. Ebenstein William Duke U. Ebke Johannes Munich U. Eckert Simon Freiburg U. Eckweiler Sebastian Mainz U. Edmonds Keith Mainz U. Edwards Clive Royal Holloway, U. of London Edwards Nicholas Charles Glasgow U. Ehrenfeld Wolfgang DESY Ehrich Thies Munich, Max Planck Inst. Eifert Till CERN Eigen Gerald Bergen U. Einsweiler Kevin LBL, Berkeley Eisenhandler Eric Queen Mary, U. of London Ekelof Tord Uppsala U., Inst. Theor. Phys. El Kacimi Mohamed Cadi Ayyad U., Marrakech Ellert Mattias Uppsala U., Inst. Theor. Phys. Elles Sabine Annecy, LAPP Ellinghaus Frank Mainz U. Ellis Katherine Queen Mary, U. of London Ellis Nicolas CERN Elmsheuser Johannes Munich U. Elsing Markus CERN Ely Robert LBL, Berkeley Emeliyanov Dmitry Rutherford Engelmann Roderich SUNY, Stony Brook Engl Albert Munich U. Epp Brigitte Innsbruck U. Eppig Andrew Michigan U. Erdmann Johannes Gottingen U., II. Phys. Inst. Ereditato Antonio Bern U., LHEP Eriksson Daniel Stockholm U. Ernst Jesse SUNY, Albany Ernst Michael Brookhaven Ernwein Jean DAPNIA, Saclay Errede Deborah Illinois U., Urbana Errede Steven Illinois U., Urbana Ertel Eugen Mainz U. Escalier Marc Orsay, LAL Escobar Carlos Valencia U., IFIC Espinal Curull Xavier Barcelona, IFAE Esposito Bellisario Frascati Etienne Francois Marseille, CPPM Etienvre Anne-Isabelle DAPNIA, Saclay Etzion Erez Tel Aviv U. Evangelakou Despoina Gottingen U., II. Phys. Inst. Evans Hal Indiana U. Fabbri Laura INFN, Bologna Fabre Caroline CERN Fakhrutdinov Rinat Serpukhov, IHEP Falciano Speranza INFN, Rome Fang Yaquan Wisconsin U., Madison Fanti Marcello INFN, Milan Farbin Amir Texas U., Arlington Farilla Addolorata INFN, Rome Farley Jason SUNY, Stony Brook Farooque Trisha Toronto U. Farrington Sinead Oxford U. Farthouat Philippe CERN Fassnacht Patrick CERN Fassouliotis Dimitrios Athens U. Fatholahzadeh Baharak Toronto U. Favareto Andrea INFN, Milan Fayard Louis Orsay, LAL Fazio Salvatore INFN, Cosenza Febbraro Renato Clermont-Ferrand U. Federic Pavol Comenius U. Fedin Oleg St. Petersburg, INP Fedorko Woiciech Michigan State U. Fehling-Kaschek Mirjam Freiburg U. Feligioni Lorenzo Marseille, CPPM Fellmann Denis Argonne Felzmann Ulrich Melbourne U. Feng Cunfeng Shandong U. Feng Eric Chicago U., EFI Fenyuk Alexander Serpukhov, IHEP Ferencei Jozef Kosice, IEF Ferland Jonathan Montreal U. Fernando Waruna Ohio State U. Ferrag Samir Glasgow U. Ferrando James Glasgow U. Ferrara Valentina DESY Ferrari Arnaud Uppsala U., Inst. Theor. Phys. Ferrari Pamela FOM, Amsterdam Ferrari Roberto INFN, Pavia Ferrer Antonio Valencia U., IFIC Ferrer Maria Lorenza Frascati Ferrere Didier Geneva U. Ferretti Claudio Michigan U. Ferretto Parodi Andrea INFN, Genoa Fiascaris Maria Chicago U., EFI Fiedler Frank Mainz U. Filipcic Andrej Stefan Inst., Ljubljana Filippas Anastasios Natl. Tech. U., Athens Filthaut Frank NIKHEF, Amsterdam Fincke-Keeler Margret Victoria U. Fiolhais Miguel LIP, Lisbon Fiorini Luca Valencia U., IFIC Firan Ana Southern Methodist U. Fischer Gordon DESY Fischer Peter Bonn U. Fisher Matthew Ohio State U. Fisher Steve Rutherford Flechl Martin Freiburg U. Fleck Ivor Siegen U. Fleckner Johanna Mainz U. Fleischmann Philipp Wurzburg U. Fleischmann Sebastian Wuppertal U. Flick Tobias Wuppertal U. Flores Castillo Luis Wisconsin U., Madison Flowerdew Michael Munich, Max Planck Inst. Fohlisch Florian Kirchhoff Inst. Phys. Fokitis Manolis Natl. Tech. U., Athens Fonseca Martin Teresa Bern U., LHEP Forbush David Alan Washington U., Seattle Formica Andrea DAPNIA, Saclay Forti Alessandra Manchester U. Fortin Dominique TRIUMF Foster Joe Manchester U. Fournier Daniel Orsay, LAL Foussat Arnaud CERN Fowler Andrew Duke U. Fowler Ken UC, Santa Cruz Fox Harald Lancaster U. Francavilla Paolo INFN, Pisa Franchino Silvia INFN, Pavia Francis David CERN Frank Tal Weizmann Inst. Franklin Melissa Harvard U., Phys. Dept. Franz Sebastien CERN Fraternali Marco INFN, Pavia Fratina Sasa Pennsylvania U. French Sky Cambridge U. Froeschl Robert CERN Froidevaux Daniel CERN Frost James Cambridge U. Fukunaga Chikara Tokyo Metropolitan U. Fullana Torregrosa Esteban CERN Fuster Juan Valencia U., IFIC Gabaldon Carolina CERN Gabizon Ofir Weizmann Inst. Gadfort Thomas Brookhaven Gadomski Szymon Geneva U. Gagliardi Guido INFN, Genoa Gagnon Pauline Indiana U. Galea Cristina Munich U. Gallas Elizabeth Oxford U. Gallas Manuel CERN Gallo Valentina Santina Bern U., LHEP Gallop Bruce Rutherford Gallus Petr Prague, Inst. Phys. Galyaev Eugene Southern Methodist U. Gan K.K. Ohio State U. Gao Yongsheng SLAC Gapienko Vladimir Serpukhov, IHEP Gaponenko Andrei LBL, Berkeley Garberson Ford Yale U. Garcia-Sciveres Maurice LBL, Berkeley Garcia Carmen Valencia U., IFIC Garcia Navarro Jose Enrique Geneva U. Gardner Robert Chicago U., EFI Garelli Nicoletta CERN Garitaonandia Hegoi FOM, Amsterdam Garonne Vincent CERN Garvey John Birmingham U. Gatti Claudio Frascati Gaudio Gabriella INFN, Pavia Gaumer Olivier Geneva U. Gaur Bakul Siegen U. Gauthier Lea DAPNIA, Saclay Gavrilenko Igor Lebedev Inst. Gay Colin British Columbia U. Gaycken Goetz Bonn U. Gayde Jean-Christophe CERN Gazis Evangelos Natl. Tech. U., Athens Ge Peng Shandong U. Gee Norman Rutherford Geerts Daniel Alphonsus Adrianus FOM, Amsterdam Geich-Gimbel Christoph Bonn U. Gellerstedt Karl Stockholm U. Gemme Claudia INFN, Genoa Gemmell Alistair Glasgow U. Genest Marie-Helene Munich U. Gentile Simonetta INFN, Rome George Matthias Gottingen U., II. Phys. Inst. George Simon Royal Holloway, U. of London Gerlach Peter Wuppertal U. Gershon Avi Tel Aviv U. Geweniger Christoph Kirchhoff Inst. Phys. Ghazlane Hamid CNESTEN, Rabat Ghez Philippe Annecy, LAPP Ghodbane Nabil Clermont-Ferrand U. Giacobbe Benedetto INFN, Bologna Giagu Stefano INFN, Rome Giakoumopoulou Victoria Athens U. Giangiobbe Vincent INFN, Pisa Gianotti Fabiola CERN Gibbard Bruce Brookhaven Gibson Adam Toronto U. Gibson Stephen CERN Gilbert Laura Oxford U. Gilchriese Murdock LBL, Berkeley Gilewsky Valentin Minsk, High Energy Phys. Ctr. Gillberg Dag Carleton U. Gillman Tony Rutherford Gingrich Douglas Alberta U. Ginzburg Jonatan Tel Aviv U. Giokaris Nikos Athens U. Giordano Raffaele INFN, Naples Giorgi Francesco Michelangelo Humboldt U., Berlin Giovannini Paola Munich, Max Planck Inst. Giraud Pierre-Francois DAPNIA, Saclay Giugni Danilo INFN, Milan Giunta Michele INFN, Rome Giusti Paolo INFN, Bologna Gjelsten Borge Kile Oslo U. Gladilin Leonid Moscow State U. Glasman Claudia Madrid, Autonoma U. Glatzer Julian Freiburg U. Glazov Alexandre DESY Glitza Karl-Walter Wuppertal U. Glonti George Dubna, JINR Godfrey Jennifer Simon Fraser U. Godlewski Jan CERN Goebel Martin DESY Gopfert Thomas Dresden, Tech. U. Goeringer Christian Mainz U. Gossling Claus Dortmund U. Gottfert Tobias Munich, Max Planck Inst. Goldfarb Steven Michigan U. Goldin Daniel Southern Methodist U. Golling Tobias Yale U. Golovnia Serguei Serpukhov, IHEP Gomes Agostinho LIP, Lisbon Gomez Fajardo Luz Stella DESY Goncalo Ricardo Royal Holloway, U. of London Goncalves Pinto Firmino Da Costa Joao DESY Gonella Laura Bonn U. Gonidec Allain CERN Gonzalez Saul Wisconsin U., Madison Gonzalez de la Hoz Santiago Valencia U., IFIC Gonzalez Silva Laura Buenos Aires U. Gonzalez-Sevilla Sergio Geneva U. Goodson Jeremiah Jet SUNY, Stony Brook Goossens Luc CERN Gorbounov Petr Andreevich Moscow, ITEP Gordon Howard Brookhaven Gorelov Igor New Mexico U. Gorfine Grant Wuppertal U. Gorini Benedetto CERN Gorini Edoardo INFN, Lecce Gorisek Andrej Stefan Inst., Ljubljana Gornicki Edward Cracow, INP Gorokhov Serguei Serpukhov, IHEP Goryachev Vladimir Serpukhov, IHEP Gosdzik Bjoern DESY Gosselink Martijn FOM, Amsterdam Gostkin Mikhail Ivanovitch Dubna, JINR Gouanere Michel Annecy, LAPP Gough Eschrich Ivo UC, Irvine Gouighri Mohamed Casablanca U. Goujdami Driss Cadi Ayyad U., Marrakech Goulette Marc Phillippe Geneva U. Goussiou Anna Washington U., Seattle Goy Corinne Annecy, LAPP Grabowska-Bold Iwona UC, Irvine Grabski Varlen Yerevan Phys. Inst. Grafstrom Per CERN Grah Christian Wuppertal U. Grahn Karl-Johan DESY Grancagnolo Francesco INFN, Lecce Grancagnolo Sergio Humboldt U., Berlin Grassi Valerio SUNY, Stony Brook Gratchev Vadim St. Petersburg, INP Grau Nathan Nevis Labs, Columbia U. Gray Heather CERN Gray Julia Ann SUNY, Stony Brook Graziani Enrico INFN, Rome Grebenyuk Oleg St. Petersburg, INP Greenfield Debbie Rutherford Greenshaw Timothy Liverpool U. Greenwood Zeno Dixon Brookhaven Gregor Ingrid-Maria DESY Grenier Philippe SLAC Griffiths Justin Washington U., Seattle Grigalashvili Nugzar Dubna, JINR Grillo Alexander UC, Santa Cruz Grinstein Sebastian Barcelona, IFAE Grishkevich Yaroslav Moscow State U. Grivaz Jean-Francois Orsay, LAL Grognuz Joel CERN Groh Manfred Munich, Max Planck Inst. Gross Eilam Weizmann Inst. Grosse-Knetter Joern Gottingen U., II. Phys. Inst. Groth-Jensen Jacob Weizmann Inst. Grybel Kai Siegen U. Guarino Victor Argonne Guest Daniel Yale U. Guicheney Christophe Clermont-Ferrand U. Guida Angelo INFN, Lecce Guillemin Thibault Annecy, LAPP Guindon Stefan Gottingen U., II. Phys. Inst. Guler Hulya McGill U. Gunther Jaroslav Prague, Inst. Phys. Guo Bin Toronto U. Guo Jun Nevis Labs, Columbia U. Gupta Ambreesh Chicago U., EFI Gusakov Yury Dubna, JINR Gushchin Vladimir Serpukhov, IHEP Gutierrez Andrea Montreal U. Gutierrez Phillip Oklahoma U. Guttman Nir Tel Aviv U. Gutzwiller Olivier Wisconsin U., Madison Guyot Claude DAPNIA, Saclay Gwenlan Claire Oxford U. Gwilliam Carl Liverpool U. Haas Andy SLAC Haas Stefan CERN Haber Carl LBL, Berkeley Hackenburg Robert Brookhaven Hadavand Haleh Khani Southern Methodist U. Hadley David Birmingham U. Haefner Petra Munich, Max Planck Inst. Hahn Ferdinand CERN Haider Stefan CERN Hajduk Zbigniew Cracow, INP Hakobyan Hrachya Yerevan Phys. Inst. Haller Johannes Gottingen U., II. Phys. Inst. Hamacher Klaus Wuppertal U. Hamal Petr Palacky U. Hamilton Andrew Geneva U. Hamilton Samuel Tufts U. Han Hongguang Beijing, Inst. High Energy Phys. Han Liang Hefei, CUST Hanagaki Kazunori Osaka U. Hance Michael Pennsylvania U. Handel Carsten Mainz U. Hanke Paul Kirchhoff Inst. Phys. Hansen John Renner Bohr Inst. Hansen Jorgen Beck Bohr Inst. Hansen Jorn Dines Bohr Inst. Hansen Peter Henrik Bohr Inst. Hansson Per SLAC Hara Kazuhiko Tsukuba U. Hare Gabriel UC, Santa Cruz Harenberg Torsten Wuppertal U. Harkusha Siarhei Minsk, Inst. Phys. Harper Devin Michigan U. Harrington Robert Boston U. Harris Orin Washington U., Seattle Harrison Karl Birmingham U. Hartert Jochen Freiburg U. Hartjes Fred FOM, Amsterdam Haruyama Tomiyoshi KEK, Tsukuba Harvey Alex Hampton U. Hasegawa Satoshi Nagoya U. Hasegawa Yoji Shinshu U. Hassani Samira DAPNIA, Saclay Hatch Mark CERN Hauff Dieter Munich, Max Planck Inst. Haug Sigve Bern U., LHEP Hauschild Michael CERN Hauser Reiner Michigan State U. Havranek Miroslav Bonn U. Hawes Brian Oxford U. Hawkes Christopher Birmingham U. Hawkings Richard John CERN Hawkins Donovan UC, Irvine Hayakawa Takashi Kobe U. Hayden Daniel Royal Holloway, U. of London Hayward Helen Liverpool U. Haywood Stephen Rutherford Hazen Eric Boston U. He Mao Shandong U. Head Simon Birmingham U. Hedberg Vincent Lund U. Heelan Louise Texas U., Arlington Heim Sarah Michigan State U. Heinemann Beate LBL, Berkeley Heisterkamp Simon Bohr Inst. Helary Louis Annecy, LAPP Heller Mathieu Orsay, LAL Hellman Sten Stockholm U. Hellmich Dennis Bonn U. Helsens Clement Barcelona, IFAE Henderson Robert Lancaster U. Henke Michael Kirchhoff Inst. Phys. Henrichs Anna Gottingen U., II. Phys. Inst. Henriques Correia Ana Maria CERN Henrot-Versille Sophie Orsay, LAL Henry-Couannier Frederic Marseille, CPPM Hensel Carsten Gottingen U., II. Phys. Inst. Henss Tobias Wuppertal U. Medina Hernandez Carlos Texas U., Arlington Hernandez Jimenez Yesenia Valencia U., IFIC Herrberg Ruth Humboldt U., Berlin Hershenhorn Alon David Technion Herten Gregor Freiburg U. Hertenberger Ralf Munich U. Hervas Luis CERN Hessey Nigel FOM, Amsterdam Hidvegi Attila Stockholm U. Higon-Rodriguez Emilio Valencia U., IFIC Hill Daniel Argonne Hill John Cambridge U. Hill Norman Argonne Hiller Karl Heinz DESY Hillert Sonja Bonn U. Hillier Stephen Birmingham U. Hinchliffe Ian LBL, Berkeley Hines Elizabeth Pennsylvania U. Hirose Minoru Osaka U. Hirsch Florian Dortmund U. Hirschbuehl Dominic Wuppertal U. Hobbs John SUNY, Stony Brook Hod Noam Tel Aviv U. Hodgkinson Mark Sheffield U. Hodgson Paul Sheffield U. Hoecker Andreas CERN Hoeferkamp Martin New Mexico U. Hoffman Julia Southern Methodist U. Hoffmann Dirk Marseille, CPPM Hohlfeld Marc Mainz U. Holder Martin Siegen U. Holmes Alan Oxford U. Holmgren Sven-Olof Stockholm U. Holy Tomas Prague, Tech. U. Holzbauer Jenny Michigan State U. Homma Yasuhiro Kobe U. Hong Tae Min Pennsylvania U. Hooft van Huysduynen Loek New York U. Horazdovsky Tomas Prague, Tech. U. Horn Claus SLAC Horner Stephan Freiburg U. Horton Katherine Oxford U. Hostachy Jean-Yves LPSC, Grenoble Hou Suen Taiwan, Inst. Phys. Houlden Michael Liverpool U. Hoummada Abdeslam Casablanca U. Howarth James Manchester U. Howell David Oxford U. Hristova Ivana Humboldt U., Berlin Hrivnac Julius Orsay, LAL Hruska Ivan Prague, Inst. Phys. Hryn'ova Tetiana Annecy, LAPP Hsu Pai-hsien Jennifer Yale U. Hsu Shih-Chieh LBL, Berkeley Huang Guang Shun Oklahoma U. Hubacek Zdenek Prague, Tech. U. Hubaut Fabrice Marseille, CPPM Huegging Fabian Bonn U. Huffman Todd Brian Oxford U. Hughes Emlyn Nevis Labs, Columbia U. Hughes Gareth Lancaster U. Hughes-Jones Richard Manchester U. Huhtinen Mika CERN Hurst Peter Harvard U., Phys. Dept. Hurwitz Martina LBL, Berkeley Husemann Ulrich DESY Huseynov Nazim Dubna, JINR Huston Joey Michigan State U. Huth John Harvard U., Phys. Dept. Iacobucci Giuseppe Geneva U. Iakovidis Georgios Natl. Tech. U., Athens Ibbotson Michael Manchester U. Ibragimov Iskander Siegen U. Ichimiya Ryo Kobe U. Iconomidou-Fayard Lydia Orsay, LAL Idarraga John Orsay, LAL Idzik Marek AGH-UST, Cracow Iengo Paolo INFN, Naples Igonkina Olga FOM, Amsterdam Ikegami Yoichi KEK, Tsukuba Ikeno Masahiro KEK, Tsukuba Ilchenko Yuri Southern Methodist U. Iliadis Dimitrios Aristotle U., Thessaloniki Imbault Didier Paris U., VI-VII Imhaeuser Martin Wuppertal U. Imori Masatoshi ICTP, Trieste Ince Tayfun Bonn U. Inigo-Golfin Joaquin CERN Ioannou Pavlos Athens U. Iodice Mauro INFN, Rome Ionescu Gelu Annecy, LAPP Irles Quiles Adrian Valencia U., IFIC Ishii Koji KEK, Tsukuba Ishikawa Akimasa Kobe U. Ishino Masaya KEK, Tsukuba Ishmukhametov Renat Southern Methodist U. Issever Cigdem Oxford U. Istin Serhat Bogazici U. Itoh Yuki Nagoya U. Ivashin Anton Serpukhov, IHEP Iwanski Wieslaw Cracow, INP Iwasaki Hiroyuki KEK, Tsukuba Izen Joseph Southern Methodist U. Izzo Vincenzo INFN, Naples Jackson Brett Pennsylvania U. Jackson John Liverpool U. Jackson Paul SLAC Jaekel Martin CERN Jain Vivek Indiana U. Jakobs Karl Freiburg U. Jakobsen Sune Bohr Inst. Jakubek Jan Prague, Tech. U. Jana Dilip Oklahoma U. Jankowski Ernest Toronto U. Jansen Eric University Coll. London Jantsch Andreas Munich, Max Planck Inst. Janus Michel Bonn U. Jarlskog Goran Lund U. Jeanty Laura Harvard U., Phys. Dept. Jelen Kazimierz AGH-UST, Cracow Jen-La Plante Imai Chicago U., EFI Jenni Peter CERN Jeremie Andrea Annecy, LAPP Jez Pavel Bohr Inst. Jezequel Stephane Annecy, LAPP Jha Manoj Kumar INFN, Bologna Ji Haoshuang Wisconsin U., Madison Ji Weina Mainz U. Jia Jiangyong SUNY, Stony Brook Jiang Yi Hefei, CUST Jimenez Belenguer Marcos DESY Jin Ge Hefei, CUST Jin Shan Beijing, Inst. High Energy Phys. Jinnouchi Osamu Tokyo Inst. Tech. Joergensen Morten Dam Bohr Inst. Joffe David Southern Methodist U. Johansen Lars Bergen U. Johansen Marianne Stockholm U. Johansson Erik Stockholm U. Johansson Per Sheffield U. Johnert Sebastian DESY Johns Kenneth Arizona U. Jon-And Kerstin Stockholm U. Jones Graham Manchester U. Jones Roger Lancaster U. Jones Tegid University Coll. London Jones Tim Liverpool U. Jonsson Ove CERN Joram Christian CERN Jorge Pedro LIP, Lisbon Joseph John LBL, Berkeley Jovin Tatjana VINCA Inst. Nucl. Sci., Belgrade Ju Xiangyang Regina U. Juranek Vojtech Prague, Inst. Phys. Jussel Patrick Innsbruck U. Kabachenko Vasily Serpukhov, IHEP Kabana Sonja Bern U., LHEP Kaci Mohammed Valencia U., IFIC Kaczmarska Anna Cracow, INP Kadlecik Peter Bohr Inst. Kado Marumi Orsay, LAL Kagan Harris Ohio State U. Kagan Michael Harvard U., Phys. Dept. Kaiser Steffen Munich, Max Planck Inst. Kajomovitz Enrique Technion Kalinin Sergey Wuppertal U. Kalinovskaya Lidia Dubna, JINR Kama Sami Southern Methodist U. Kanaya Naoko ICTP, Trieste Kaneda Michiru CERN Kanno Takayuki Tokyo Inst. Tech. Kantserov Vadim Moscow Phys. Eng. Inst. Kanzaki Junichi KEK, Tsukuba Kaplan Benjamin Yale U. Kapliy Anton Chicago U., EFI Kaplon Jan CERN Kar Deepak Dresden, Tech. U. Karagoz Muge Oxford U. Karnevskiy Mikhail DESY Karr Kristo Argonne Kartvelishvili Vakhtang Lancaster U. Karyukhin Andrey Serpukhov, IHEP Kashif Lashkar Wisconsin U., Madison Kasmi Azzedine Southern Methodist U. Kass Richard Ohio State U. Kastanas Alex Bergen U. Kataoka Mayuko Annecy, LAPP Kataoka Yousuke ICTP, Trieste Katsoufis Elias Natl. Tech. U., Athens Katzy Judith DESY Kaushik Venkatesh Arizona U. Kawagoe Kiyotomo Kobe U. Kawamoto Tatsuo ICTP, Trieste Kawamura Gen Mainz U. Kayl Manuel FOM, Amsterdam Kazanin Vassili Novosibirsk, IYF Kazarinov Makhail Dubna, JINR Keates James Robert Manchester U. Keeler Richard Victoria U. Kehoe Robert Southern Methodist U. Keil Markus Gottingen U., II. Phys. Inst. Kekelidze George Dubna, JINR Kelly Marc Manchester U. Kennedy John Munich U. Kenney Christopher John SLAC Kenyon Mike Glasgow U. Kepka Oldrich Prague, Inst. Phys. Kerschen Nicolas CERN Kersevan Borut Paul Stefan Inst., Ljubljana Kersten Susanne Wuppertal U. Kessoku Kohei ICTP, Trieste Ketterer Christian Freiburg U. Keung Justin Toronto U. Khakzad Mohsen Carleton U. Khalil-zada Farkhad Baku, Inst. Phys. Khandanyan Hovhannes Illinois U., Urbana Khanov Alexander Oklahoma State U. Kharchenko Dmitri Dubna, JINR Khodinov Alexander Moscow Phys. Eng. Inst. Kholodenko Anatoli Serpukhov, IHEP Khomich Andrei Kirchhoff Inst. Phys. Khoo Teng Jian Cambridge U. Khoriauli Gia Bonn U. Khoroshilov Andrey Wuppertal U. Khovanskiy Nikolai Dubna, JINR Khovanskiy Valery Moscow, ITEP Khramov Evgeniy Dubna, JINR Khubua Jemal Tbilisi State U. Tbilisi, Inst. Phys. Kim Hyeon Jin Texas U., Arlington Kim Min Suk Alberta U. Kim Peter SLAC Kim Shinhong Tsukuba U. Kimura Naoki Waseda U. Kind Oliver Humboldt U., Berlin King Barry Liverpool U. King Matthew Kobe U. King Robert Steven Beaufoy Oxford U. Kirk Julie Rutherford Kirsch Guillaume Oxford U. Kirsch Lawrence Brandeis U. Kiryunin Andrey Munich, Max Planck Inst. Kisielewska Danuta AGH-UST, Cracow Kittelmann Thomas Pittsburgh U. Kiver Andrey Serpukhov, IHEP Kiyamura Hironori Kobe U. Kladiva Eduard Kosice, IEF Klaiber-Lodewigs Jonas Dortmund U. Klein Max Liverpool U. Klein Uta Liverpool U. Kleinknecht Konrad Mainz U. Klemetti Miika McGill U. Klier Amit Weizmann Inst. Klimentov Alexei Brookhaven Klingenberg Reiner Dortmund U. Klinkby Esben Bohr Inst. Klioutchnikova Tatiana CERN Klok Peter NIKHEF, Amsterdam Klous Sander FOM, Amsterdam Kluge Eike-Erik Kirchhoff Inst. Phys. Kluge Thomas Liverpool U. Kluit Peter FOM, Amsterdam Kluth Stefan Munich, Max Planck Inst. Kneringer Emmerich Innsbruck U. Knobloch Juergen CERN Knoops Edith Marseille, CPPM Knue Andrea Gottingen U., II. Phys. Inst. Ko Byeong Rok Duke U. Kobayashi Tomio ICTP, Trieste Kobel Michael Dresden, Tech. U. Kocian Martin SLAC Kocnar Antonin Palacky U. Kodys Peter Charles U. Koneke Karsten CERN Konig Adriaan NIKHEF, Amsterdam Koenig Sebastian Mainz U. Kopke Lutz Mainz U. Koetsveld Folkert NIKHEF, Amsterdam Koevesarki Peter Bonn U. Koffas Thomas CERN Koffeman Els FOM, Amsterdam Kohn Fabian Gottingen U., II. Phys. Inst. Kohout Zdenek Prague, Tech. U. Kohriki Takashi KEK, Tsukuba Koi Tatsumi SLAC Kokott Thomas Bonn U. Kolachev Guennady Novosibirsk, IYF Kolanoski Hermann Humboldt U., Berlin Kolesnikov Vladimir Dubna, JINR Koletsou Iro INFN, Milan Koll James Michigan State U. Kollar Daniel CERN Kollefrath Michael Freiburg U. Kolya Scott Manchester U. Komar Aston Lebedev Inst. Komaragiri Jyothsna Rani Simon Fraser U. Komori Yuto ICTP, Trieste Kondo Takahiko KEK, Tsukuba Kono Takanori DESY Kononov Anatoly Freiburg U. Konoplich Rostislav New York U. Konstantinidis Nikolaos University Coll. London Kootz Andreas Wuppertal U. Koperny Stefan AGH-UST, Cracow Kopikov Sergey Serpukhov, IHEP Korcyl Krzysztof Cracow, INP Kordas Kostantinos Aristotle U., Thessaloniki Koreshev Victor Serpukhov, IHEP Korn Andreas LBL, Berkeley Korol Aleksandr Novosibirsk, IYF Korolkov Ilya Barcelona, IFAE Korolkova Elena Sheffield U. Korotkov Vladislav Serpukhov, IHEP Kortner Oliver Munich, Max Planck Inst. Kortner Sandra Munich, Max Planck Inst. Kostyukhin Vadim Bonn U. Kotamaki Miikka Juhani CERN Kotov Sergey Munich, Max Planck Inst. Kotov Vladislav Dubna, JINR Kotwal Ashutosh Duke U. Kourkoumelis Christine Athens U. Kouskoura Vasiliki Aristotle U., Thessaloniki Koutsman Alex FOM, Amsterdam Kowalewski Robert Victor Victoria U. Kowalski Tadeusz AGH-UST, Cracow Kozanecki Witold DAPNIA, Saclay Kozhin Anatoly Serpukhov, IHEP Kral Vlastimil Prague, Tech. U. Kramarenko Viktor Moscow State U. Kramberger Gregor Stefan Inst., Ljubljana Krasny Mieczyslaw Witold Paris U., VI-VII Krasznahorkay Attila New York U. Kraus James Michigan State U. Kreisel Arik Tel Aviv U. Krejci Frantisek Prague, Tech. U. Kretzschmar Jan Liverpool U. Krieger Nina Gottingen U., II. Phys. Inst. Krieger Peter Toronto U. Kroeninger Kevin Gottingen U., II. Phys. Inst. Kroha Hubert Munich, Max Planck Inst. Kroll Joe Pennsylvania U. Kroseberg Juergen Bonn U. Krstic Jelena Belgrade U. Kruchonak Uladzimir Dubna, JINR Kruger Hans Bonn U. Kruker Tobias Bern U., LHEP Krumshteyn Zinovii Dubna, JINR Kruth Andre Bonn U. Kubota Takashi Melbourne U. Kuehn Susanne Freiburg U. Kugel Andreas Heidelberg U. Kuhl Thorsten DESY Kuhn Dietmar Innsbruck U. Kukhtin Victor Dubna, JINR Kulchitsky Yuri Minsk, Inst. Phys. Kuleshov Sergey Santa Maria U., Valparaiso Kummer Christian Munich U. Kuna Marine Paris U., VI-VII Kundu Nikhil Oxford U. Kunkle Joshua Pennsylvania U. Kupco Alexander Prague, Inst. Phys. Kurashige Hisaya Kobe U. Kurata Masakazu Tsukuba U. Kurochkin Yurii Minsk, Inst. Phys. Kus Vlastimil Prague, Inst. Phys. Kuykendall William Washington U., Seattle Kuze Masahiro Tokyo Inst. Tech. Kuzhir Polina Minsk, High Energy Phys. Ctr. Kvasnicka Ondrej Prague, Inst. Phys. Kvita Jiri CERN Kwee Regina Humboldt U., Berlin La Rosa Alessandro Wisconsin U., Madison La Rotonda Laura INFN, Cosenza Labarga Luis Madrid, Autonoma U. Labbe Julien Annecy, LAPP Lablak Said Casablanca U. Lacasta Carlos Valencia U., IFIC Lacava Francesco INFN, Rome Lacker Heiko Humboldt U., Berlin Lacour Didier Paris U., VI-VII Lacuesta Vicente Ramon Valencia U., IFIC Ladygin Evgueni Dubna, JINR Lafaye Remi Annecy, LAPP Laforge Bertrand Paris U., VI-VII Lagouri Theodota Madrid, Autonoma U. Lai Stanley Freiburg U. Laisne Emmanuel LPSC, Grenoble Lamanna Massimo CERN Lampen Caleb Arizona U. Lampl Walter Arizona U. Lancon Eric DAPNIA, Saclay Landgraf Ulrich Freiburg U. Landon Murrough Queen Mary, U. of London Landsman Hagar Technion Lane Jenna Manchester U. Lange Clemens DESY Lankford Andrew UC, Irvine Lanni Francesco Brookhaven Lantzsch Kerstin CERN Laplace Sandrine Paris U., VI-VII Lapoire Cecile Bonn U. Laporte Jean-Francois DAPNIA, Saclay Lari Tommaso INFN, Milan Larionov Anatoly Serpukhov, IHEP Larner Aimee Oxford U. Lasseur Christian CERN Lassnig Mario CERN Laurelli Paolo Frascati Lavorato Antonia Oxford U. Lavrijsen Wim LBL, Berkeley Laycock Paul Liverpool U. Lazarev Alexandre Dubna, JINR Le Dortz Olivier Paris U., VI-VII Le Guirriec Emmanuel Marseille, CPPM Le Maner Christophe Toronto U. Le Menedeu Eve DAPNIA, Saclay Lebel Celine Montreal U. LeCompte Thomas Argonne Ledroit-Guillon Fabienne Agnes Marie LPSC, Grenoble Lee Hurng-Chun FOM, Amsterdam Lee Jason Sydney U. Lee Shih-Chang Taiwan, Inst. Phys. Lee Lawrence Yale U. Lefebvre Michel Victoria U. Legendre Marie DAPNIA, Saclay Leger Annie Geneva U. LeGeyt Benjamin Pennsylvania U. Legger Federica Munich U. Leggett Charles LBL, Berkeley Lehmacher Marc Bonn U. Lehmann Miotto Giovanna CERN Lei Xiaowen Arizona U. Leite Marco Aurelio Lisboa Sao Paulo U. Leitner Rupert Charles U. Lellouch Daniel Weizmann Inst. Leltchouk Mikhail Nevis Labs, Columbia U. Lendermann Victor Kirchhoff Inst. Phys. Leney Katharine Witwatersrand U. Lenz Tatiana FOM, Amsterdam Lenzen Georg Wuppertal U. Lenzi Bruno CERN Leonhardt Kathrin Dresden, Tech. U. Leontsinis Stefanos Natl. Tech. U., Athens Leroy Claude Montreal U. Lessard Jean-Raphael Victoria U. Lesser Jonas Stockholm U. Lester Christopher Cambridge U. Leung Fook Cheong Annabelle Wisconsin U., Madison Leveque Jessica Annecy, LAPP Levin Daniel Michigan U. Levinson Lorne Weizmann Inst. Levitski Mikhail Serpukhov, IHEP Lewandowska Marta Boston U. Lewis Adrian Oxford U. Lewis George New York U. Leyko Agnieszka Bonn U. Leyton Michael Humboldt U., Berlin Li Bo Marseille, CPPM Li Haifeng Wisconsin U., Madison Li Shu Hefei, CUST Li Xuefei Michigan U. Liang Zhihua Southern Methodist U. Liang Zhijun Oxford U. Liberti Barbara INFN, Rome Lichard Peter CERN Lichtnecker Markus Munich U. Lie Ki Illinois U., Urbana Liebig Wolfgang Bergen U. Lifshitz Ronen Technion Lilley Joseph Birmingham U. Limbach Christian Bonn U. Limosani Antonio Melbourne U. Limper Maaike Iowa U. Lin Simon Taiwan, Inst. Phys. Linde Frank FOM, Amsterdam Linnemann James Michigan State U. Lipeles Elliot Pennsylvania U. Lipinsky Lukas Prague, Inst. Phys. Lipniacka Anna Bergen U. Liss Tony Illinois U., Urbana Lissauer David Brookhaven Lister Alison Geneva U. Litke Alan UC, Santa Cruz Liu Chuanlei Carleton U. Liu Dong Taiwan, Inst. Phys. Liu Hao Michigan U. Liu Jianbei Michigan U. Liu Minghui Hefei, CUST Liu Shengli Alberta U. Liu Yanwen Hefei, CUST Livan Michele INFN, Pavia Livermore Sarah Oxford U. Lleres Annick LPSC, Grenoble Llorente Merino Javier Madrid, Autonoma U. Lloyd Stephen Queen Mary, U. of London Lobodzinska Ewelina DESY Loch Peter Arizona U. Lockman William UC, Santa Cruz Lockwitz Sarah Yale U. Loddenkoetter Thomas Bonn U. Loebinger Fred Manchester U. Loginov Andrey Yale U. Loh Chang Wei British Columbia U. Lohse Thomas Humboldt U., Berlin Lohwasser Kristin Freiburg U. Lokajicek Milos Prague, Inst. Phys. Loken James Oxford U. Lombardo Vincenzo Paolo Annecy, LAPP Long Robin Eamonn Lancaster U. Lopes Lourenco LIP, Lisbon Lopez Mateos David Harvard U., Phys. Dept. Losada Marta Antonio Narino U. Loscutoff Peter LBL, Berkeley Sterzo Francesco Lo INFN, Rome Losty Michael TRIUMF Lou Xinchou Southern Methodist U. Lounis Abdenour Orsay, LAL Loureiro Karina Antonio Narino U. Love Jeremy Boston U. Love Peter Lancaster U. Lowe Andrew SLAC Lu Feng Beijing, Inst. High Energy Phys. Lubatti Henry Washington U., Seattle Luci Claudio INFN, Rome Lucotte Arnaud LPSC, Grenoble Ludwig Andreas Dresden, Tech. U. Ludwig Dorthe DESY Ludwig Inga Freiburg U. Ludwig Jens Freiburg U. Luehring Frederick Indiana U. Luijckx Guy FOM, Amsterdam Lumb Debra Freiburg U. Luminari Lamberto INFN, Rome Lund Esben Oslo U. Lund-Jensen Bengt Royal Inst. Tech., Stockholm Lundberg Bjorn Lund U. Lundberg Johan Stockholm U. Lundquist Johan Bohr Inst. Lungwitz Matthias Mainz U. Lupi Anna INFN, Pisa Lutz Gerhard Munich, Max Planck Inst. Lynn David Brookhaven Lys Jeremy LBL, Berkeley Lytken Else Lund U. Ma Hong Brookhaven Ma Lian Liang Wisconsin U., Madison Macana Goia Jorge Andres Montreal U. Maccarrone Giovanni Frascati Macchiolo Anna Munich, Max Planck Inst. Macek Bostjan Stefan Inst., Ljubljana Machado Miguens Joana LIP, Lisbon Mackeprang Rasmus Bohr Inst. Madaras Ronald LBL, Berkeley Mader Wolfgang Dresden, Tech. U. Maenner Reinhard Heidelberg U. Maeno Tadashi Brookhaven Mattig Peter Wuppertal U. Mattig Stefan DESY Magalhaes Martins Paulo Jorge LIP, Lisbon Magnoni Luca CERN Magradze Erekle Gottingen U., II. Phys. Inst. Mahalalel Yair Tel Aviv U. Mahboubi Kambiz Freiburg U. Mahout Gilles Birmingham U. Maiani Camilla INFN, Rome Maidantchik Carmen Rio de Janeiro Federal U. Maio Amelia LIP, Lisbon Majewski Stephanie Brookhaven Makida Yasuhiro KEK, Tsukuba Makovec Nikola Orsay, LAL Mal Prolay Arizona U. Malecki Pawel Cracow, INP Malecki Piotr Cracow, INP Maleev Victor St. Petersburg, INP Malek Fairouz LPSC, Grenoble Mallik Usha Iowa U. Malon David Argonne Maltezos Stavros Natl. Tech. U., Athens Malyshev Vladimir Novosibirsk, IYF Malyukov Sergei CERN Mameghani Raphael Munich U. Mamuzic Judita VINCA Inst. Nucl. Sci., Belgrade Manabe Atsushi KEK, Tsukuba Mandelli Luciano INFN, Milan Mandic Igor Stefan Inst., Ljubljana Mandrysch Rocco Humboldt U., Berlin Maneira Jose LIP, Lisbon Mangeard Pierre-Simon Michigan State U. Manjavidze Ioseb Dubna, JINR Mann Alexander Gottingen U., II. Phys. Inst. Manning Peter UC, Santa Cruz Manousakis-Katsikakis Arkadios Athens U. Mansoulie Bruno DAPNIA, Saclay Manz Andreas Munich, Max Planck Inst. Mapelli Alessandro CERN Mapelli Livio CERN March Luis Madrid, Autonoma U. Marchand Jean-Francois CERN Marchese Fabrizio INFN, Rome Marchiori Giovanni Paris U., VI-VII Marcisovsky Michal Prague, Inst. Phys. Marin Alexandru Boston U. Marino Christopher Indiana U. Marroquim Fernando Rio de Janeiro Federal U. Marshall Robin Manchester U. Marshall Zach CERN Martens Kalen Toronto U. Marti-Garcia Salvador Valencia U., IFIC Martin Andrew Yale U. Martin Brian CERN Martin Brian Thomas Michigan State U. Martin Franck Francois Pennsylvania U. Martin Jean-Pierre Montreal U. Martin Philippe LPSC, Grenoble Martin Tim Birmingham U. Martin Dit Latour Bertrand Geneva U. Martinez Mario Barcelona, IFAE Martinez Outschoorn Verena Harvard U., Phys. Dept. Martyniuk Alex Manchester U. Marx Marilyn Manchester U. Marzano Francesco INFN, Rome Marzin Antoine Oklahoma U. Masetti Lucia Mainz U. Mashimo Tetsuro ICTP, Trieste Mashinistov Ruslan Lebedev Inst. Masik Jiri Manchester U. Maslennikov Alexey Novosibirsk, IYF Massa Ignazio INFN, Bologna Massaro Graziano FOM, Amsterdam Massol Nicolas Annecy, LAPP Mastrandrea Paolo INFN, Rome Mastroberardino Anna INFN, Cosenza Masubuchi Tatsuya ICTP, Trieste Mathes Markus Bonn U. Matricon Pierre Orsay, LAL Matsumoto Hiroshi ICTP, Trieste Matsunaga Hiroyuki ICTP, Trieste Matsushita Takashi Kobe U. Mattravers Carly Oxford U. Maugain Jean-Marie CERN Maxfield Stephen Liverpool U. Maximov Dmitriy Novosibirsk, IYF May Edward Argonne Mayne Anna Sheffield U. Mazini Rachid Taiwan, Inst. Phys. Mazur Michael Bonn U. Mazzanti Marcello INFN, Milan Mazzoni Enrico INFN, Pisa Mc Kee Shawn Patrick Michigan U. McCarn Allison Illinois U., Urbana McCarthy Robert SUNY, Stony Brook McCarthy Tom Carleton U. McCubbin Norman Rutherford McFarlane Kenneth Hampton U. Mcfayden Josh Sheffield U. McGlone Helen Glasgow U. Mchedlidze Gvantsa Tbilisi State U. Tbilisi, Inst. Phys. McLaren Robert Andrew CERN Mclaughlan Tom Birmingham U. McMahon Steve Rutherford McPherson Robert Victoria U. Meade Andrew Massachusetts U., Amherst Mechnich Joerg FOM, Amsterdam Mechtel Markus Wuppertal U. Medinnis Mike DESY Meera-Lebbai Razzak Oklahoma U. Meguro Tatsuma Osaka U. Mehdiyev Rashid Montreal U. Mehlhase Sascha Bohr Inst. Mehta Andrew Liverpool U. Meier Karlheinz Kirchhoff Inst. Phys. Meinhardt Jens Freiburg U. Meirose Bernhard Lund U. Melachrinos Constantinos Chicago U., EFI Mellado Garcia Bruce Rafael Wisconsin U., Madison Mendoza Navas Luis Antonio Narino U. Meng Zhaoxia Taiwan, Inst. Phys. Mengarelli Alberto INFN, Bologna Menke Sven Munich, Max Planck Inst. Menot Claude CERN Meoni Evelin Barcelona, IFAE Mercurio Kevin Michael Harvard U., Phys. Dept. Mermod Philippe Oxford U. Merola Leonardo INFN, Naples Meroni Chiara INFN, Milan Merritt Frank Chicago U., EFI Messina Andrea CERN Metcalfe Jessica New Mexico U. Mete Alaettin Serhan Iowa State U. Meuser Stefan Bonn U. Meyer Carsten Mainz U. Meyer Jean-Pierre DAPNIA, Saclay Meyer Jochen Wurzburg U. Meyer Joerg Gottingen U., II. Phys. Inst. Meyer Thomas Christian CERN Meyer W.Thomas Iowa State U. Miao Jiayuan Shandong U. Michal Sebastien CERN Micu Liliana Bucharest, IFIN-HH Middleton Robin Rutherford Miele Paola CERN Migas Sylwia Liverpool U. Mijovic Liza DESY Mikenberg Giora Weizmann Inst. Mikestikova Marcela Prague, Inst. Phys. Mikuz Marko Stefan Inst., Ljubljana Miller David SLAC Miller Robert Michigan State U. Mills Bill British Columbia U. Mills Corrinne Harvard U., Phys. Dept. Milov Alexander Weizmann Inst. Milstead David Stockholm U. Milstein Dmitry Weizmann Inst. Minaenko Andrey Serpukhov, IHEP Minano Mercedes Valencia U., IFIC Minashvili Irakli Dubna, JINR Mincer Allen New York U. Mindur Bartosz AGH-UST, Cracow Mineev Mikhail Dubna, JINR Ming Yao Regina U. Mir Lluisa-Maria Barcelona, IFAE Mirabelli Giovanni INFN, Rome Miralles Verge Lluis Barcelona, IFAE Misiejuk Andrzej Royal Holloway, U. of London Mitrevski Jovan UC, Santa Cruz Mitrofanov Gennady Serpukhov, IHEP Mitsou Vasiliki A. Valencia U., IFIC Mitsui Shingo KEK, Tsukuba Miyagawa Paul Manchester U. Miyazaki Kazuki Kobe U. Mjornmark Jan-Ulf Lund U. Moa Torbjoern Stockholm U. Mockett Paul Washington U., Seattle Moed Shulamit Harvard U., Phys. Dept. Moeller Victoria Cambridge U. Monig Klaus DESY Moser Nicolas Bonn U. Mohapatra Soumya SUNY, Stony Brook Mohr Wolfgang Freiburg U. Mohrdieck-Mock Susanne Munich, Max Planck Inst. Moisseev Artemy Serpukhov, IHEP Moles-Valls Regina Valencia U., IFIC Molina-Perez Jorge CERN Monk James University Coll. London Monnier Emmanuel Marseille, CPPM Montesano Simone INFN, Milan Monticelli Fernando La Plata U. Monzani Simone INFN, Bologna Moore Roger Alberta U. Moorhead Gareth Melbourne U. Mora Herrera Clemencia Geneva U. Moraes Arthur Glasgow U. Morais Antonio LIP, Lisbon Morange Nicolas DAPNIA, Saclay Morel Julien Gottingen U., II. Phys. Inst. Morello Gianfranco INFN, Cosenza Moreno Deywis Mainz U. Moreno Llácer María Valencia U., IFIC Morettini Paolo INFN, Genoa Morii Masahiro Harvard U., Phys. Dept. Morin Jerome Queen Mary, U. of London Morita Youhei KEK, Tsukuba Morley Anthony Keith CERN Mornacchi Giuseppe CERN Morone Maria-Christina Geneva U. Morozov Sergey Moscow Phys. Eng. Inst. Morris John Queen Mary, U. of London Morvaj Ljiljana Nagoya U. Moser Hans-Guenther Munich, Max Planck Inst. Mosidze Maia Tbilisi State U. Tbilisi, Inst. Phys. Moss Josh Ohio State U. Mount Richard SLAC Mountricha Eleni DAPNIA, Saclay Mouraviev Sergei Lebedev Inst. Moyse Edward Massachusetts U., Amherst Mudrinic Mihajlo VINCA Inst. Nucl. Sci., Belgrade Mueller Felix Kirchhoff Inst. Phys. Mueller James Pittsburgh U. Mueller Klemens Bonn U. Muller Thomas Munich U. Muenstermann Daniel CERN Muir Alex British Columbia U. Munwes Yonathan Tel Aviv U. Murakami Koichi KEK, Tsukuba Murray Bill Rutherford Mussche Ido FOM, Amsterdam Musto Elisa INFN, Naples Myagkov Alexey Serpukhov, IHEP Myska Miroslav Prague, Inst. Phys. Nadal Jordi Barcelona, IFAE Nagai Koichi Tsukuba U. Nagano Kunihiro KEK, Tsukuba Nagasaka Yasushi Hiroshima Inst. Tech. Nairz Armin Michael CERN Nakahama Yu CERN Nakamura Koji ICTP, Trieste Nakano Itsuo Okayama U. Nanava Gizo Bonn U. Napier Austin Tufts U. Nash Michael University Coll. London Nation Nigel Boston U. Nattermann Till Bonn U. Naumann Thomas DESY Navarro Gabriela Antonio Narino U. Neal Homer Michigan U. Nebot Eduardo Madrid, Autonoma U. Nechaeva Polina Lebedev Inst. Negri Andrea INFN, Pavia Negri Guido CERN Nektarijevic Snezana Geneva U. Nelson Silke SLAC Nelson Timothy Knight SLAC Nemecek Stanislav Prague, Inst. Phys. Nemethy Peter New York U. Nepomuceno Andre Asevedo Rio de Janeiro Federal U. Nessi Marzio CERN Nesterov Stanislav St. Petersburg, INP Neubauer Mark Illinois U., Urbana Neusiedl Andrea Mainz U. Neves Ricardo New York U. Nevski Pavel Brookhaven Newman Paul Birmingham U. Hong Van Nguyen Thi DAPNIA, Saclay Nickerson Richard Oxford U. Nicolaidou Rosy DAPNIA, Saclay Nicolas Ludovic Sheffield U. Nicquevert Bertrand CERN Niedercorn Francois Orsay, LAL Nielsen Jason UC, Santa Cruz Niinikoski Tapio CERN Nikiforov Andriy Humboldt U., Berlin Nikolaenko Vladimir Serpukhov, IHEP Nikolaev Kirill Dubna, JINR Nikolic-Audit Irena Paris U., VI-VII Nikolics Katalin Geneva U. Nikolopoulos Konstantinos Brookhaven Nilsen Henrik Freiburg U. Nilsson Paul Texas U., Arlington Ninomiya Yoichi ICTP, Trieste Nisati Aleandro INFN, Rome Nishiyama Tomonori Kobe U. Nisius Richard Munich, Max Planck Inst. Nodulman Lawrence Argonne Nomachi Masaharu Osaka U. Nomidis Ioannis Aristotle U., Thessaloniki Nordberg Markus CERN Nordkvist Bjoern Stockholm U. Norton Peter Rutherford Novakova Jana Charles U. Nozaki Mitsuaki KEK, Tsukuba Nozicka Miroslav DESY Nozka Libor Palacky U. Nugent Ian Michael TRIUMF Nuncio-Quiroz Adriana-Elizabeth Bonn U. Nunes Hanninger Guilherme Melbourne U. Nunnemann Thomas Munich U. Nurse Emily University Coll. London Nyman Tommi CERN O'Brien Brendan Joseph Edinburgh U. O'Neale Steve Birmingham U. O'Neil Dugan Simon Fraser U. O'Shea Val Glasgow U. Oakham Gerald Carleton U. Oberlack Horst Munich, Max Planck Inst. Ocariz Jose Paris U., VI-VII Ochi Atsuhiko Kobe U. Oda Susumu ICTP, Trieste Odaka Shigeru KEK, Tsukuba Odier Jerome Marseille, CPPM Ogren Harold Indiana U. Oh Alexander Manchester U. Oh Seog Duke U. Ohm Christian Stockholm U. Ohshima Takayoshi Nagoya U. Ohshita Hidetoshi Shinshu U. Ohska Tokio Kenneth KEK, Tsukuba Ohsugi Takashi Hiroshima U. Okada Shogo Kobe U. Okawa Hideki UC, Irvine Okumura Yasuyuki Nagoya U. Okuyama Toyonobu ICTP, Trieste Olcese Marco INFN, Genoa Olchevski Alexander Dubna, JINR Oliveira Miguel Alfonso LIP, Lisbon Oliveira Damazio Denis Brookhaven Oliver Garcia Elena Valencia U., IFIC Olivito Dominick Pennsylvania U. Olszewski Andrzej Cracow, INP Olszowska Jolanta Cracow, INP Omachi Chihiro Kobe U. Onofre Antonio LIP, Lisbon Onyisi Peter Chicago U., EFI Oram Christopher TRIUMF Oreglia Mark Chicago U., EFI Oren Yona Tel Aviv U. Orestano Domizia INFN, Rome Orlov Iliya Novosibirsk, IYF Oropeza Barrera Cristina Glasgow U. Orr Robert Toronto U. Osculati Bianca INFN, Genoa Ospanov Rustem Pennsylvania U. Osuna Carlos Barcelona, IFAE Otero y Garzon Gustavo Buenos Aires U. Ottersbach John FOM, Amsterdam Ouchrif Mohamed Oujda U. Ould-Saada Farid Oslo U. Ouraou Ahmimed DAPNIA, Saclay Ouyang Qun Beijing, Inst. High Energy Phys. Owen Mark Manchester U. Owen Simon Sheffield U. Ozcan Veysi Erkcan Bogazici U. Ozturk Nurcan Texas U., Arlington Pacheco Pages Andres Barcelona, IFAE Padilla Aranda Cristobal Barcelona, IFAE Pagan Griso Simone LBL, Berkeley Paganis Efstathios Sheffield U. Paige Frank Brookhaven Pajchel Katarina Oslo U. Palestini Sandro CERN Pallin Dominique Clermont-Ferrand U. Palma Alberto LIP, Lisbon Palmer Jody Birmingham U. Pan Yibin Wisconsin U., Madison Panagiotopoulou Evgenia Natl. Tech. U., Athens Panes Boris Chile U., Catolica Panikashvili Natalia Michigan U. Panitkin Sergey Brookhaven Pantea Dan Bucharest, IFIN-HH Panuskova Monika Prague, Inst. Phys. Paolone Vittorio Pittsburgh U. Papadelis Aras Stockholm U. Papadopoulou Theodora Natl. Tech. U., Athens Paramonov Alexander Argonne Park Woochun Brookhaven Parker Andy Cambridge U. Parodi Fabrizio INFN, Genoa Parsons John Nevis Labs, Columbia U. Parzefall Ulrich Freiburg U. Pasqualucci Enrico INFN, Rome Passeri Antonio INFN, Rome Pastore Fernanda INFN, Rome Pastore Francesca CERN Pasztor Gabriella Geneva U. Pataraia Sophio Wisconsin U., Madison Patel Nikhul Sydney U. Pater Joleen Manchester U. Patricelli Sergio INFN, Naples Pauly Thilo CERN Pecsy Martin Comenius U. Pedraza Morales Maria Isabel Wisconsin U., Madison Peleganchuk Sergey Novosibirsk, IYF Peng Haiping Hefei, CUST Pengo Ruggero CERN Penson Alexander Nevis Labs, Columbia U. Penwell John Indiana U. Perantoni Marcelo Rio de Janeiro Federal U. Perez Kerstin Nevis Labs, Columbia U. Cavalcanti Tiago Perez DESY Perez Codina Estel Barcelona, IFAE Perez Garcia-Estan Maria Teresa Valencia U., IFIC Perez Reale Valeria Nevis Labs, Columbia U. Perini Laura INFN, Milan Pernegger Heinz CERN Perrino Roberto INFN, Lecce Perrodo Pascal Annecy, LAPP Persembe Seda Ankara U. Peshekhonov Vladimir Dubna, JINR Peters Onne FOM, Amsterdam Petersen Brian CERN Petersen Jorgen CERN Petersen Troels Bohr Inst. Petit Elisabeth Marseille, CPPM Petridis Andreas Aristotle U., Thessaloniki Petridou Chariclia Aristotle U., Thessaloniki Petrolo Emilio INFN, Rome Petrucci Fabrizio INFN, Rome Petschull Dennis DESY Petteni Michele Simon Fraser U. Pezoa Raquel Santa Maria U., Valparaiso Phan Anna Melbourne U. Phillips Alan Cambridge U. Phillips Peter William Rutherford Piacquadio Giacinto CERN Piccaro Elisa Queen Mary, U. of London Piccinini Maurizio INFN, Bologna Pickford Andrew Glasgow U. Piec Sebastian Marcin DESY Piegaia Ricardo Buenos Aires U. Pilcher James Chicago U., EFI Pilkington Andrew Manchester U. Pina Joao Antonio LIP, Lisbon Pinamonti Michele INFN, Udine Pinder Alex Oxford U. Pinfold James Alberta U. Ping Jialun Nanjing U. Pinto Belmiro LIP, Lisbon Pirotte Olivier CERN Pitt Michael Weizmann Inst. Pizio Caterina INFN, Milan Placakyte Ringaile DESY Plamondon Mathieu Victoria U. Plano Will Manchester U. Pleier Marc-Andre Brookhaven Pleskach Anatoly Serpukhov, IHEP Poblaguev Andrei Brookhaven Poddar Sahill Kirchhoff Inst. Phys. Podlyski Fabrice Clermont-Ferrand U. Poggioli Luc Orsay, LAL Poghosyan Tatevik Bonn U. Pohl Martin Geneva U. Polci Francesco LPSC, Grenoble Polesello Giacomo INFN, Pavia Policicchio Antonio Washington U., Seattle Polini Alessandro INFN, Bologna Poll James Queen Mary, U. of London Polychronakos Venetios Brookhaven Pomarede Daniel Marc DAPNIA, Saclay Pomeroy Daniel Brandeis U. Pommes Kathy CERN Pontecorvo Ludovico INFN, Rome Pope Bernard Michigan State U. Popeneciu Gabriel Alexandru Bucharest, IFIN-HH Popovic Dragan Belgrade U. Poppleton Alan CERN Bueso Xavier Portell CERN Porter Robert UC, Irvine Posch Christoph Boston U. Pospelov Guennady Munich, Max Planck Inst. Pospisil Stanislav Prague, Tech. U. Potrap Igor Munich, Max Planck Inst. Potter Christina Sussex U. Potter Christopher Oregon U. Poulard Gilbert CERN Poveda Joaquin Wisconsin U., Madison Prabhu Robindra University Coll. London Pralavorio Pascal Marseille, CPPM Prasad Srivas Harvard U., Phys. Dept. Pravahan Rishiraj Texas U., Arlington Prell Soeren Iowa State U. Pretzl Klaus Peter Bern U., LHEP Pribyl Lukas CERN Price Darren Indiana U. Price Lawrence Argonne Price Michael John CERN Prichard Paul Liverpool U. Prieur Damien Pittsburgh U. Primavera Margherita INFN, Lecce Prokofiev Kirill New York U. Prokoshin Fedor Santa Maria U., Valparaiso Protopopescu Serban Brookhaven Proudfoot James Argonne Prudent Xavier Dresden, Tech. U. Przysiezniak Helenka Annecy, LAPP Psoroulas Serena Bonn U. Ptacek Elizabeth Oregon U. Purdham John Michigan U. Purohit Milind Brookhaven Puzo Patrick Orsay, LAL Pylypchenko Yuriy Oslo U. Qian Jianming Michigan U. Qian Zuxuan Marseille, CPPM Qin Zhonghua DESY Quadt Arnulf Gottingen U., II. Phys. Inst. Quarrie David LBL, Berkeley Quayle William Wisconsin U., Madison Quinonez Fernando Chile U., Catolica Raas Marcel NIKHEF, Amsterdam Radescu Voica Heidelberg U. Radics Balint Bonn U. Rador Tonguc Bogazici U. Ragusa Francesco INFN, Milan Rahal Ghita CC, Villeurbanne Rahimi Amir Ohio State U. Rahm David Brookhaven Rajagopalan Srinivasan Brookhaven Rammensee Michael Freiburg U. Rammes Marcus Siegen U. Ramstedt Magnus Stockholm U. Randrianarivony Koloina Carleton U. Ratoff Peter Lancaster U. Rauscher Felix Munich U. Rauter Emanuel Munich, Max Planck Inst. Raymond Michel CERN Read Alexander Lincoln Oslo U. Rebuzzi Daniela INFN, Pavia Redelbach Andreas Wurzburg U. Redlinger George Brookhaven Reece Ryan Pennsylvania U. Reeves Kendall Southern Methodist U. Reichold Armin FOM, Amsterdam Reinherz-Aronis Erez Tel Aviv U. Reinsch Andreas Oregon U. Reisinger Ingo Dortmund U. Reljic Dusan Belgrade U. Rembser Christoph CERN Ren Zhongliang Taiwan, Inst. Phys. Renaud Adrien Orsay, LAL Renkel Peter Southern Methodist U. Rescigno Marco INFN, Rome Resconi Silvia INFN, Milan Resende Bernardo DAPNIA, Saclay Reznicek Pavel Munich U. Rezvani Reyhaneh Toronto U. Richards Alexander University Coll. London Richter Robert Munich, Max Planck Inst. Richter-Was Elzbieta Cracow, INP Ridel Melissa Paris U., VI-VII Rieke Stefan Mainz U. Rijpstra Manouk FOM, Amsterdam Rijssenbeek Michael SUNY, Stony Brook Rimoldi Adele INFN, Pavia Rinaldi Lorenzo INFN, Bologna Rios Ryan Randy Southern Methodist U. Riu Imma Barcelona, IFAE Rivoltella Giancesare INFN, Milan Rizatdinova Flera Oklahoma State U. Rizvi Eram Queen Mary, U. of London Robertson Steven McGill U. Robichaud-Veronneau Andree Geneva U. Robinson Dave Cambridge U. Robinson James University Coll. London Robinson Mary Oregon U. Robson Aidan Glasgow U. Rocha de Lima Jose Guilherme Northern Illinois U. Roda Chiara INFN, Pisa Roda Dos Santos Denis CERN Rodier Stephane Madrid, Autonoma U. Rodriguez Diego Antonio Narino U. Roe Adam Gottingen U., II. Phys. Inst. Roe Shaun CERN Rohne Ole Oslo U. Rojo Victoria SUNY, Albany Rolli Simona Tufts U. Romaniouk Anatoli Moscow Phys. Eng. Inst. Romanov Victor Dubna, JINR Romeo Gaston Buenos Aires U. Romero Maltrana Diego Chile U., Catolica Roos Lydia Paris U., VI-VII Ros Eduardo Valencia U., IFIC Rosati Stefano INFN, Rome Rosbach Kilian Geneva U. Rose Matthew Royal Holloway, U. of London Rosenbaum Gabriel Toronto U. Rosenberg Eli Iowa State U. Rosendahl Peter Lundgaard Bergen U. Rosselet Laurent Geneva U. Rossetti Valerio Barcelona, IFAE Rossi Elvira INFN, Naples Rossi Leonardo Paolo INFN, Genoa Rossi Lucio INFN, Milan Rotaru Marina Bucharest, IFIN-HH Roth Itamar Weizmann Inst. Rothberg Joseph Washington U., Seattle Rousseau David Orsay, LAL Royon Christophe DAPNIA, Saclay Rozanov Alexander Marseille, CPPM Rozen Yoram Technion Ruan Xifeng Orsay, LAL Rubinskiy Igor DESY Ruckert Benjamin Munich U. Ruckstuhl Nicole FOM, Amsterdam Rud Viacheslav Moscow State U. Rudolph Christian Dresden, Tech. U. Rudolph Gerald Innsbruck U. Ruhr Frederik Arizona U. Ruggieri Federico INFN, Rome Ruiz-Martinez Aranzazu Iowa State U. Rulikowska-Zarebska Elzbieta AGH-UST, Cracow Rumiantsev Viktor Minsk, High Energy Phys. Ctr. Rumyantsev Leonid Dubna, JINR Runge Kay Freiburg U. Runolfsson Ogmundur Bonn U. Rurikova Zuzana Freiburg U. Rusakovich Nikolai Dubna, JINR Rust Dave Indiana U. Rutherfoord John Arizona U. Ruwiedel Christoph LBL, Berkeley Ruzicka Pavel Prague, Inst. Phys. Ryabov Yury St. Petersburg, INP Ryadovikov Vasily Serpukhov, IHEP Ryan Patrick Michigan State U. Rybar Martin Charles U. Rybkin Grigori Orsay, LAL Ryder Nick Oxford U. Rzaeva Sevda Baku, Inst. Phys. Saavedra Aldo Sydney U. Sadeh Iftach Tel Aviv U. Sadrozinski Hartmut UC, Santa Cruz Sadykov Renat Dubna, JINR Safai Tehrani Francesco INFN, Rome Sakamoto Hiroshi ICTP, Trieste Salamanna Giuseppe Queen Mary, U. of London Salamon Andrea INFN, Rome Saleem Muhammad Oklahoma U. Salihagic Denis Munich, Max Planck Inst. Salnikov Andrei SLAC Salt Jose Valencia U., IFIC Salvachua Ferrando Belen Argonne Salvatore Daniela INFN, Cosenza Salvatore Pasquale Fabrizio Sussex U. Salvucci Antonio NIKHEF, Amsterdam Salzburger Andreas CERN Sampsonidis Dimitrios Aristotle U., Thessaloniki Samset Bjorn Hallvard Oslo U. Sanchez Arturo INFN, Naples Sandaker Heidi Bergen U. Sander Heinz Georg Mainz U. Sanders Michiel Munich U. Sandhoff Marisa Wuppertal U. Sandoval Tanya Cambridge U. Sandstroem Rikard Munich, Max Planck Inst. Sandvoss Stephan Wuppertal U. Sankey Dave Rutherford Sansoni Andrea Frascati Santamarina Rios Cibran McGill U. Santoni Claudio Clermont-Ferrand U. Santonico Rinaldo INFN, Rome Santos Helena LIP, Lisbon Saraiva Joao LIP, Lisbon Sarangi Tapas Wisconsin U., Madison Sarkisyan-Grinbaum Edward Texas U., Arlington Sarri Francesca INFN, Pisa Sartisohn Georg Wuppertal U. Sasaki Osamu KEK, Tsukuba Sasaki Takashi KEK, Tsukuba Sasao Noboru Kyoto U. Satsounkevitch Igor Minsk, Inst. Phys. Sauvage Gilles Annecy, LAPP Sauvan Emmanuel Annecy, LAPP Sauvan Jean-Baptiste Orsay, LAL Savard Pierre Toronto U. Savinov Vladimir Pittsburgh U. Savu Dan Octavian CERN Savva Panagiota Natl. Tech. U., Athens Sawyer Lee Brookhaven Saxon David Glasgow U. Says Louis-Pierre Clermont-Ferrand U. Sbarra Carla INFN, Bologna Sbrizzi Antonio INFN, Bologna Scallon Olivia Montreal U. Scannicchio Diana UC, Irvine Schaarschmidt Jana Orsay, LAL Schacht Peter Munich, Max Planck Inst. Schafer Uli Mainz U. Schaepe Steffen Bonn U. Schaetzel Sebastian Heidelberg U. Schaffer Arthur Orsay, LAL Schaile Dorothee Munich U. Schamberger R. Dean SUNY, Stony Brook Schamov Andrey Novosibirsk, IYF Scharf Veit Kirchhoff Inst. Phys. Schegelsky Valery St. Petersburg, INP Scheirich Daniel Michigan U. Schernau Michael UC, Irvine Scherzer Max LBL, Berkeley Schiavi Carlo INFN, Genoa Schieck Jochen Munich U. Schillo Christian Freiburg U. Schioppa Marco INFN, Cosenza Schlenker Stefan CERN Schlereth James Argonne Schmidt Evelyn Freiburg U. Schmieden Kristof Bonn U. Schmitt Christian Mainz U. Schmitt Sebastian Heidelberg U. Schmitz Martin Bonn U. Schoning Andre Heidelberg U. Schott Matthias CERN Schouten Doug Simon Fraser U. Schovancova Jaroslava Prague, Inst. Phys. Schram Malachi McGill U. Schroeder Christian Mainz U. Schroer Nicolai Heidelberg U. Schuh Silvia CERN Schuler Georges CERN Schultes Joachim Wuppertal U. Schultz-Coulon Hans-Christian Kirchhoff Inst. Phys. Schulz Holger Humboldt U., Berlin Schumacher Jan Bonn U. Schumacher Markus Freiburg U. Schumm Bruce UC, Santa Cruz Schune Philippe DAPNIA, Saclay Schwanenberger Christian Manchester U. Schwartzman Ariel SLAC Schwemling Philippe Paris U., VI-VII Schwienhorst Reinhard Michigan State U. Schwierz Rainer Dresden, Tech. U. Schwindling Jerome DAPNIA, Saclay Schwindt Thomas Bonn U. Scott Bill Rutherford Searcy Jacob Oregon U. Sedykh Evgeny St. Petersburg, INP Segura Ester Barcelona, IFAE Seidel Sally New Mexico U. Seiden Abraham UC, Santa Cruz Seifert Frank Dresden, Tech. U. Seixas Jose Rio de Janeiro Federal U. Sekhniaidze Givi INFN, Naples Seliverstov Dmitry St. Petersburg, INP Sellden Bjoern Stockholm U. Sellers Graham Liverpool U. Seman Michal Kosice, IEF Semprini-Cesari Nicola INFN, Bologna Serfon Cedric Munich U. Serin Laurent Orsay, LAL Seuster Rolf Munich, Max Planck Inst. Severini Horst Oklahoma U. Sevior Martin Melbourne U. Sfyrla Anna CERN Shabalina Elizaveta Gottingen U., II. Phys. Inst. Shamim Mansoora Oregon U. Shan Lianyou Beijing, Inst. High Energy Phys. Shank James Boston U. Shao Qi Tao Melbourne U. Shapiro Marjorie LBL, Berkeley Shatalov Pavel Moscow, ITEP Shaver Leif Arizona U. Shaw Christian Glasgow U. Shaw Kate INFN, Udine Sherman Daniel Yale U. Sherwood Peter University Coll. London Shibata Akira New York U. Shichi Hideharu Nagoya U. Shimizu Shima CERN Shimojima Makoto Nagasaki Inst. Appl. Sci. Shin Taeksu Hampton U. Shmeleva Alevtina Lebedev Inst. Shochet Mel Chicago U., EFI Short Daniel Oxford U. Shupe Michael Arizona U. Sicho Petr Prague, Inst. Phys. Sidoti Antonio INFN, Rome Siebel Anca-Mirela Wuppertal U. Siegert Frank Freiburg U. Siegrist James LBL, Berkeley Sijacki Djordje Belgrade U. Silbert Ohad Weizmann Inst. Silva Jose LIP, Lisbon Silver Yiftah Tel Aviv U. Silverstein Daniel SLAC Silverstein Samuel Stockholm U. Simak Vladislav Prague, Tech. U. Simard Olivier DAPNIA, Saclay Simic Ljiljana Belgrade U. Simion Stefan Orsay, LAL Simmons Brinick University Coll. London Simonyan Margar Bohr Inst. Sinervo Pekka Toronto U. Sinev Nikolai Oregon U. Sipica Valentin Siegen U. Siragusa Giovanni Wurzburg U. Sisakyan Alexei Dubna, JINR Sivoklokov Serguei Moscow State U. Sjolin Jorgen Stockholm U. Sjursen Therese Bergen U. Skinnari Louise Anastasia LBL, Berkeley Skovpen Kirill Novosibirsk, IYF Skubic Patrick Oklahoma U. Skvorodnev Nikolai Brandeis U. Slater Mark Birmingham U. Slavicek Tomas Prague, Tech. U. Sliwa Krzysztof Tufts U. Sloan Terrence Lancaster U. Sloper John erik CERN Smakhtin Vladimir Weizmann Inst. Smirnov Sergei Moscow Phys. Eng. Inst. Smirnova Lidia Moscow State U. Smirnova Oxana Lund U. Smith Ben Campbell Harvard U., Phys. Dept. Smith Douglas SLAC Smith Kenway Glasgow U. Smizanska Maria Lancaster U. Smolek Karel Prague, Tech. U. Snesarev Andrei Lebedev Inst. Snow Steve Manchester U. Snow Joel Oklahoma U. Snuverink Jochem FOM, Amsterdam Snyder Scott Brookhaven Soares Mara LIP, Lisbon Sobie Randall Victoria U. Sodomka Jaromir Prague, Tech. U. Soffer Abner Tel Aviv U. Solans Carlos Valencia U., IFIC Solar Michael Prague, Tech. U. Solc Jaroslav Prague, Tech. U. Soldatov Evgeny Moscow Phys. Eng. Inst. Soldevila Urmila Valencia U., IFIC Solfaroli Camillocci Elena INFN, Rome Solodkov Alexander Serpukhov, IHEP Solovyanov Oleg Serpukhov, IHEP Sondericker John Brookhaven Soni Nitesh Alberta U. Sopko Vit Prague, Tech. U. Sopko Bruno Prague, Tech. U. Sorbi Massimo INFN, Milan Sosebee Mark Texas U., Arlington Soukharev Andrey Novosibirsk, IYF Spagnolo Stefania INFN, Lecce Spano Francesco Nevis Labs, Columbia U. Spighi Roberto INFN, Bologna Spigo Giancarlo CERN Spila Federico INFN, Rome Spiriti Eleuterio INFN, Rome Spiwoks Ralf CERN Spousta Martin Charles U. Spreitzer Teresa Toronto U. Spurlock Barry Texas U., Arlington St. Denis Richard Dante Glasgow U. Stahl Thorsten Siegen U. Stahlman Jonathan Pennsylvania U. Stamen Rainer Kirchhoff Inst. Phys. Stanecka Ewa CERN Stanek Robert Argonne Stanescu Cristian INFN, Rome Stapnes Steinar Oslo U. Starchenko Evgeny Serpukhov, IHEP Stark Jan LPSC, Grenoble Staroba Pavel Prague, Inst. Phys. Starovoitov Pavel Minsk, High Energy Phys. Ctr. Staude Arnold Munich U. Stavina Pavel Comenius U. Stavropoulos Georgios LBL, Berkeley Steele Genevieve Glasgow U. Steinbach Peter Dresden, Tech. U. Steinberg Peter Brookhaven Stekl Ivan Prague, Tech. U. Stelzer Bernd Simon Fraser U. Stelzer Harald Joerg Michigan State U. Stelzer-Chilton Oliver TRIUMF Stenzel Hasko Giessen U. Stevenson Kyle Queen Mary, U. of London Stewart Graeme CERN Stillings Jan Andre Bonn U. Stockmanns Tobias Bonn U. Stockton Mark CERN Stoerig Kathrin Freiburg U. Stoicea Gabriel Bucharest, IFIN-HH Stonjek Stefan Munich, Max Planck Inst. Strachota Pavel Charles U. Stradling Alden Texas U., Arlington Straessner Arno Dresden, Tech. U. Strandberg Jonas Royal Inst. Tech., Stockholm Strandberg Sara Stockholm U. Strandlie Are Oslo U. Strang Michael Ohio State U. Strauss Emanuel SLAC Strauss Michael Oklahoma U. Strizenec Pavol Kosice, IEF Strohmer Raimund Wurzburg U. Strom David Oregon U. Strong John Royal Holloway, U. of London Stroynowski Ryszard Southern Methodist U. Strube Jan Rutherford Stugu Bjarne Bergen U. Stumer Iuliu Brookhaven Stupak John SUNY, Stony Brook Sturm Philipp Wuppertal U. Soh Dart-yin Taiwan, Inst. Phys. Su Dong SLAC Subramania Halasya Siva Alberta U. Succurro Antonella Barcelona, IFAE Sugaya Yorihito Osaka U. Sugimoto Takuya Nagoya U. Suhr Chad Northern Illinois U. Suita Koichi Kobe U. Suk Michal Charles U. Sulin Vladimir Lebedev Inst. Sultansoy Saleh TOBB ETU, Ankara Sumida Toshi CERN Sun Xiaohu LPSC, Grenoble Sundermann Jan Erik Freiburg U. Suruliz Kerim Sheffield U. Sushkov Serge Barcelona, IFAE Susinno Giancarlo INFN, Cosenza Sutton Mark Sussex U. Suzuki Yu KEK, Tsukuba Svatos Michal Prague, Inst. Phys. Sviridov Yuri Serpukhov, IHEP Swedish Stephen British Columbia U. Sykora Ivan Comenius U. Sykora Tomas Charles U. Szeless Balazs CERN Sanchez Javier Valencia U., IFIC Ta Duc FOM, Amsterdam Tackmann Kerstin DESY Taffard Anyes UC, Irvine Tafirout Reda TRIUMF Taga Adrian Oslo U. Taiblum Nimrod Tel Aviv U. Takahashi Yuta Nagoya U. Takai Helio Brookhaven Takashima Ryuichi Kyoto U. of Education Takeda Hiroshi Kobe U. Takeshita Tohru Shinshu U. Talby Mossadek Marseille, CPPM Talyshev Alexey Novosibirsk, IYF Tamsett Matthew Brookhaven Tanaka Junichi ICTP, Trieste Tanaka Reisaburo Orsay, LAL Tanaka Satoshi Ritsumeikan U. Tanaka Shuji KEK, Tsukuba Tanaka Yoshito Nagasaki Inst. Appl. Sci. Tani Kazutoshi Kobe U. Tannoury Nancy Marseille, CPPM Tappern Geoffrey CERN Tapprogge Stefan Mainz U. Tardif Dominique Toronto U. Tarem Shlomit Technion Tarrade Fabien Brookhaven Tartarelli Giuseppe Francesco INFN, Milan Tas Petr Charles U. Tasevsky Marek Prague, Inst. Phys. Tassi Enrico INFN, Cosenza Tatarkhanov Mous LBL, Berkeley Taylor Christopher University Coll. London Taylor Frank MIT Taylor Geoffrey Melbourne U. Taylor Wendy York U., Canada Teixeira Dias Castanheira Matilde Queen Mary, U. of London Teixeira-Dias Pedro Royal Holloway, U. of London Temming Kim Katrin Freiburg U. Ten Kate Herman CERN Teng Ping-Kun Taiwan, Inst. Phys. Terada Susumu KEK, Tsukuba Terashi Koji ICTP, Trieste Terron Juan Madrid, Autonoma U. Terwort Mark DESY Testa Marianna Frascati Teuscher Richard Toronto U. Thadome Jocelyn Wuppertal U. Therhaag Jan Bonn U. Theveneaux-Pelzer Timothee Paris U., VI-VII Thioye Moustapha Yale U. Thoma Sascha Freiburg U. Thomas Juergen Birmingham U. Thompson Emily Massachusetts U., Amherst Thompson Paul Birmingham U. Thompson Peter Toronto U. Thompson Stan Glasgow U. Thomson Evelyn Pennsylvania U. Thomson Mark Cambridge U. Thun Rudolf Michigan U. Tic Tomáš Prague, Inst. Phys. Tikhomirov Vladimir Lebedev Inst. Tikhonov Yury Novosibirsk, IYF Timmermans Charles NIKHEF, Amsterdam Tipton Paul Yale U. 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Tremblet Louis CERN Tricoli Alesandro CERN Trigger Isabel Marian TRIUMF Trincaz-Duvoid Sophie Paris U., VI-VII Trinh Thi Nguyet Paris U., VI-VII Tripiana Martin La Plata U. Trischuk William Toronto U. Trivedi Arjun Brookhaven Trocme Benjamin LPSC, Grenoble Troncon Clara INFN, Milan Trottier-McDonald Michel Simon Fraser U. Trzupek Adam Cracow, INP Tsarouchas Charilaos CERN Tseng Jeffrey Oxford U. Tsiakiris Menelaos FOM, Amsterdam Tsiareshka Pavel Minsk, Inst. Phys. Tsionou Dimitra Annecy, LAPP Tsipolitis Georgios Natl. Tech. U., Athens Tsiskaridze Vakhtang Freiburg U. Tskhadadze Edisher Tbilisi State U. Tbilisi, Inst. Phys. Tsukerman Ilya Moscow, ITEP Tsulaia Vakhtang LBL, Berkeley Tsung Jieh-Wen Bonn U. Tsuno Soshi KEK, Tsukuba Tsybychev Dmitri SUNY, Stony Brook Tua Alan Sheffield U. Tuggle Joseph Chicago U., EFI Turala Michal Cracow, INP Turecek Daniel Prague, Tech. U. Turk Cakir Ilkay TAEK, Ankara Turlay Emmanuel FOM, Amsterdam Turra Ruggero INFN, Milan Tuts Michael Nevis Labs, Columbia U. Tykhonov Andrii Stefan Inst., Ljubljana Tylmad Maja Stockholm U. Tyndel Mike Rutherford Tyrvainen Harri CERN Tzanakos George Athens U. Uchida Kirika Bonn U. Ueda Ikuo ICTP, Trieste Ueno Ryuichi Carleton U. Ugland Maren Bergen U. Uhlenbrock Mathias Bonn U. Uhrmacher Michael Gottingen U., II. Phys. Inst. Ukegawa Fumihiko Tsukuba U. Unal Guillaume CERN Underwood David Argonne Undrus Alexander Brookhaven Unel Gokhan UC, Irvine Unno Yoshinobu KEK, Tsukuba Urbaniec Dustin Nevis Labs, Columbia U. Urkovsky Evgeny Tel Aviv U. Urrejola Pedro Chile U., Catolica Usai Giulio Texas U., Arlington Uslenghi Massimiliano INFN, Pavia Vacavant Laurent Marseille, CPPM Vacek Vaclav Prague, Tech. U. Vachon Brigitte McGill U. Vahsen Sven LBL, Berkeley Valenta Jan Prague, Inst. Phys. Valente Paolo INFN, Rome Valentinetti Sara INFN, Bologna Valkar Stefan Charles U. Valladolid Gallego Eva Valencia U., IFIC Vallecorsa Sofia Technion Ferrer Juan Antonio Valls Valencia U., IFIC Van der Graaf Harry FOM, Amsterdam van der Kraaij Erik FOM, Amsterdam van der Leeuw Robin FOM, Amsterdam van der Poel Egge FOM, Amsterdam van der Ster Daniel CERN Van Eijk Bob FOM, Amsterdam van Eldik Niels Massachusetts U., Amherst Van Gemmeren Peter Argonne van Kesteren Zdenko FOM, Amsterdam Van Vulpen Ivo FOM, Amsterdam Vandelli Wainer CERN Vandoni Giovanna CERN Vaniachine Alexandre Argonne Vankov Peter DESY Vannucci Francois Paris U., VI-VII Varela Rodriguez Fernando CERN Vari Riccardo INFN, Rome Varnes Erich Arizona U. Varouchas Dimitris LBL, Berkeley Vartapetian Armen Texas U., Arlington Varvell Kevin Sydney U. Vassilakopoulos Vassilios Hampton U. Vazeille Francois Clermont-Ferrand U. Vegni Guido INFN, Milan Veillet Jean-Jacques Orsay, LAL Vellidis Constantine Athens U. Veloso Filipe LIP, Lisbon Veness Raymond CERN Veneziano Stefano INFN, Rome Ventura Andrea INFN, Lecce Ventura Daniel Washington U., Seattle Venturi Manuela Freiburg U. Venturi Nicola Bern U., LHEP Vercesi Valerio INFN, Pavia Verducci Monica Washington U., Seattle Verkerke Wouter FOM, Amsterdam Vermeulen Jos FOM, Amsterdam Vest Anja Dresden, Tech. U. Vetterli Michel Simon Fraser U. Vichou Irene Illinois U., Urbana Vickey Trevor Witwatersrand U. Viehhauser Georg Oxford U. Viel Simon British Columbia U. Villa Mauro INFN, Bologna Villaplana Perez Miguel Valencia U., IFIC Vilucchi Elisabetta Frascati Vincter Manuella Carleton U. Vinek Elisabeth CERN Vinogradov Vladimir Dubna, JINR Virchaux Marc DAPNIA, Saclay Virzi Joseph LBL, Berkeley Vitells Ofer Weizmann Inst. Viti Michele DESY Vivarelli Iacopo Freiburg U. Vives Vaque Francesc Barcelona, IFAE Vlachos Sotirios Natl. Tech. U., Athens Vlasak Michal Prague, Tech. U. Vlasov Nikolai Bonn U. Vogel Adrian Bonn U. Vokac Petr Prague, Tech. U. Volpi Guido Frascati Volpi Matteo Melbourne U. Volpini Giovanni INFN, Milan von der Schmitt Hans Munich, Max Planck Inst. von Loeben Joerg Munich, Max Planck Inst. von Radziewski Holger Freiburg U. von Toerne Eckhard Bonn U. Vorobel Vit Charles U. Vorobiev Alexander Serpukhov, IHEP Vorwerk Volker Barcelona, IFAE Vos Marcel Valencia U., IFIC Voss Rudiger CERN Voss Thorsten Tobias Wuppertal U. Vossebeld Joost Liverpool U. Vranjes Nenad Belgrade U. Vranjes Milosavljevic Marija FOM, Amsterdam Vrba Vaclav Prague, Inst. Phys. Vreeswijk Marcel FOM, Amsterdam Anh Tuan Vu Mainz U. Vuillermet Raphael CERN Vukotic Ilija Orsay, LAL Wagner Wolfgang Wuppertal U. Wagner Peter Pennsylvania U. Wahlen Helmut Wuppertal U. Wakabayashi Jun Nagoya U. Walbersloh Jorg Dortmund U. Walch Shannon Michigan U. Walder James Lancaster U. Walker Rodney Munich U. Walkowiak Wolfgang Siegen U. Wall Richard Yale U. Waller Peter Liverpool U. Wang Chiho Duke U. Wang Haichen Wisconsin U., Madison Wang Hulin Hefei, CUST Wang Jike Taiwan, Inst. Phys. Wang Jin Shandong U. Wang Joshua C. Washington U., Seattle Wang Rui New Mexico U. Wang Song-Ming Taiwan, Inst. Phys. Warburton Andreas McGill U. Ward Patricia Cambridge U. Warsinsky Markus Freiburg U. Watkins Peter Birmingham U. Watson Alan Birmingham U. Watson Miriam Birmingham U. Watts Gordon Washington U., Seattle Watts Stephen Manchester U. Waugh Anthony Sydney U. Waugh Ben University Coll. London Weber Jens Dortmund U. Weber Marc Rutherford Weber Michele Bern U., LHEP Weber Pavel Gottingen U., II. Phys. Inst. Weidberg Anthony Oxford U. Weigell Philipp Munich, Max Planck Inst. Weingarten Jens Gottingen U., II. Phys. Inst. Weiser Christian Freiburg U. Wellenstein Hermann Brandeis U. Wells Phillippa CERN Wen Mei Frascati Wenaus Torre Brookhaven Wendler Shanti Pittsburgh U. Weng Zhili Taiwan, Inst. Phys. Wengler Thorsten CERN Wenig Siegfried CERN Wermes Norbert Bonn U. Werner Matthias Freiburg U. Werner Per CERN Werth Michael UC, Irvine Wessels Martin Kirchhoff Inst. Phys. Weydert Carole LPSC, Grenoble Whalen Kathleen Carleton U. Wheeler-Ellis Sarah Jane UC, Irvine Whitaker Scott Boston U. White Andrew Texas U., Arlington White Martin Melbourne U. White Sebastian Brookhaven Whitehead Samuel Robert Oxford U. Whiteson Daniel UC, Irvine Whittington Denver Indiana U. Wicek Francois Orsay, LAL Wicke Daniel Wuppertal U. Wickens Fred Rutherford Wiedenmann Werner Wisconsin U., Madison Wielers Monika Rutherford Wienemann Peter Bonn U. Wiglesworth Craig Queen Mary, U. of London Wiik Liv Antje Mari Freiburg U. Wijeratne Peter Alexander University Coll. London Wildauer Andreas Valencia U., IFIC Wildt Martin Andre DESY Wilhelm Ivan Charles U. Wilkens Henric George CERN Will Jonas Zacharias Munich U. Williams Eric Nevis Labs, Columbia U. Williams Hugh Pennsylvania U. Willis William Nevis Labs, Columbia U. Willocq Stephane Massachusetts U., Amherst Wilson John Birmingham U. Wilson Michael Galante SLAC Wilson Alan Michigan U. Wingerter-Seez Isabelle Annecy, LAPP Winkelmann Stefan Freiburg U. Winklmeier Frank CERN Wittgen Matthias SLAC Wolter Marcin Wladyslaw Cracow, INP Wolters Helmut LIP, Lisbon Wooden Gemma Oxford U. Wosiek Barbara Cracow, INP Wotschack Jorg CERN Woudstra Martin Massachusetts U., Amherst Wraight Kenneth Glasgow U. Wright Catherine Glasgow U. Wrona Bozydar Liverpool U. Wu Sau Lan Wisconsin U., Madison Wu Xin Geneva U. Wu Yusheng Hefei, CUST Wulf Evan Nevis Labs, Columbia U. Wunstorf Renate Dortmund U. Wynne Benjamin Edinburgh U. Xaplanteris Leonidas Natl. Tech. U., Athens Xella Stefania Bohr Inst. Xie Song Freiburg U. Xie Yigang Beijing, Inst. High Energy Phys. Xu Chao Hefei, CUST Xu Da Sheffield U. Xu Guofa Beijing, Inst. High Energy Phys. Yabsley Bruce Sydney U. Yacoob Sahal Witwatersrand U. Yamada Miho KEK, Tsukuba Yamamoto Akira KEK, Tsukuba Yamamoto Kyoko Iowa State U. Yamamoto Shimpei ICTP, Trieste Yamamura Taiki ICTP, Trieste Yamaoka Jared Duke U. Yamazaki Takayuki ICTP, Trieste Yamazaki Yuji Kobe U. Yan Zhen Boston U. Yang Haijun Michigan U. Yang Un-Ki Manchester U. Yang Yi Indiana U. Yang Yi Beijing, Inst. High Energy Phys. Yang Zhaoyu Stockholm U. Yanush Serguei Minsk, High Energy Phys. Ctr. Yao Weiming LBL, Berkeley Yao Yushu LBL, Berkeley Yasu Yoshiji KEK, Tsukuba Ybeles Smit Gabriel Valentijn Regina U. Ye Jingbo Southern Methodist U. Ye Shuwei Brookhaven Yilmaz Metin Gazi U. Yoosoofmiya Reza Pittsburgh U. Yorita Kohei Waseda U. Yoshida Riktura Argonne Young Charles SLAC Youssef Saul Boston U. Yu Dantong Brookhaven Yu Jaehoon Texas U., Arlington Yu Jie Nanjing U. Yuan Li Beijing, Inst. High Energy Phys. Yurkewicz Adam SUNY, Stony Brook Zaets Vassilli Serpukhov, IHEP Zaidan Remi Iowa U. Zaitsev Alexander Serpukhov, IHEP Zajacova Zuzana CERN Zalite Youris St. Petersburg, INP Zanello Lucia INFN, Rome Zarzhitsky Pavel Southern Methodist U. Zaytsev Alexander Novosibirsk, IYF Zeitnitz Christian Wuppertal U. Zeller Michael Yale U. Zemla Andrzej Cracow, INP Zendler Carolin Bonn U. Zenin Oleg Serpukhov, IHEP Zenis Tibor Comenius U. Zenonos Zenonas INFN, Pisa Zenz Seth LBL, Berkeley Zerwas Dirk Orsay, LAL Zevi Della Porta Giovanni Harvard U., Phys. Dept. Zhan Zhichao Shandong U. Zhang Dongliang Hefei, CUST Zhang Huaqiao Michigan State U. Zhang Jinlong Argonne Zhang Xueyao Shandong U. Zhang Zhiqing Orsay, LAL Zhao Long New York U. Zhao Tianchi Washington U., Seattle Zhao Zhengguo Hefei, CUST Zhemchugov Alexey Dubna, JINR Zheng Shuchen Beijing, Inst. High Energy Phys. Zhong Jiahang Taiwan, Inst. Phys. Zhou Bing Michigan U. Zhou Ning UC, Irvine Zhou Yue Taiwan, Inst. Phys. Zhu Cheng Guang Shandong U. Zhu Hongbo DESY Zhu Junjie Michigan U. Zhu Yingchun Wisconsin U., Madison Zhuang Xuai Munich U. Zhuravlov Vadym Munich, Max Planck Inst. Zieminska Daria Indiana U. Zimmermann Robert Bonn U. Zimmermann Simone Bonn U. Zimmermann Stephanie Freiburg U. Ziolkowski Michael Siegen U. Zitoun Robert Annecy, LAPP Zivkovic Lidija Nevis Labs, Columbia U. Zmouchko Viatcheslav Serpukhov, IHEP Zobernig Georg Wisconsin U., Madison Zoccoli Antonio INFN, Bologna Zolnierowski Yves Annecy, LAPP Zsenei Andras CERN zur Nedden Martin Humboldt U., Berlin Zutshi Vishnu Northern Illinois U. Zwalinski Lukasz CERN Aad Georges Freiburg U. 2011 705 174 192 A search for neutral Higgs bosons decaying to pairs of tau leptons with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of 7 TeV, recorded in 2010 and corresponding to an integrated luminosity of 36 pb^-1. After signal selection, 276 events are observed in this data sample. The observed number of events is consistent with the total expected background of 269 +/- 36 events. Exclusion limits at the 95% confidence level are derived for the production cross section of a generic Higgs boson phi as a function of the Higgs boson mass and for A/H/h production in the Minimal Supersymmetric Standard Model (MSSM) as a function of the parameters m_A and tan(beta). research-article

Search for neutral MSSM Higgs bosons decaying to tau^+tau^- pairs in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector Anders C Barberio E Banerjee S Beckingham M Boddy C Bristow T Chen X Davey W Dingfelder J Dhaliwal S Farrington S Ferrer A Fiorini L Flechl M Galea C Glatzer J Gross E Gumpert C Hanawa K Hanninger G N Heng Y Hsu S-C Keller J Kroseberg J Leney KJC Mader W Mellado B Morgenstern M Nakamura K Pan Y Pedraza-Morales M-I Pitt M Pranko A von Radziewski H Rompotis N Rosendahl P Rousseau D Schumacher M Schillo C Schwindt T Shao T Silbert O Solans C Straessner A Stugu B Tanaka J Thoma S Torralba G Urquijo P Utecht N Valls J Varouchas D Vickey T Volpi M Wang T Warsinsky M Wu S-L Xella S Zanzi D Zinonos Z 2011 A search for neutral Higgs bosons decaying to pairs of tau leptons with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of 7 TeV, recorded in 2011 and corresponding to an integrated luminosity of 1.06 fb^−1 . After signal selection, 4630 events are observed in this data sample. The observed number of events is consistent with the total expected background of 4947 ± 356 events. Exclusion limits at the 95% confidence level are derived for the production cross section of a generic Higgs boson phi as a function of the Higgs boson mass and for A/H/h production in the Minimal Supersymmetric Standard Model (MSSM) as a function of the parameters mA and tan beta. INTNOTEATLASPRIV

Search for neutral MSSM Higgs bosons decaying to tau+tau- pairs in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector Anders C Barberio E Banerjee S Beckingham M Boddy C Bristow T Chen X Davey W Dingfelder J Dhaliwal S Farrington S Ferrer A Fiorini L Flechl M Galea C Glatzer J Gross E Gumpert C Hanawa K Hanninger G N Heng Y Hsu S-C Keller J Kroseberg J Leney KJC Mader W Mellado B Morgenstern M Nakamura K Pan Y Pedraza-Morales M-I Pitt M Pranko A von Radziewski H Rompotis N Rosendahl P Rousseau D Schumacher M Schillo C Schwindt T Shao T Silbert O Solans C Straessner A Stugu B Tanaka J Thoma S Torralba G Urquijo P Utecht N Valls J Varouchas D Vickey T Volpi M Wang T Warsinsky M Wu S-L Xella S Zanzi D Zinonos Z 2011 A search for neutral Higgs bosons decaying to pairs of tau leptons with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of 7 TeV, recorded in 2011 and corresponding to an integrated luminosity of 1.06 fb^−1 . After signal selection, 4630 events are observed in this data sample. The observed number of events is consistent with the total expected background of 4900 ± 600 events. Exclusion limits at the 95% confidence level are derived for the production cross section of a generic Higgs boson phi as a function of the Higgs boson mass and for A/H/h production in the Minimal Supersymmetric Standard Model (MSSM) as a function of the parameters mA and tan beta. INTNOTEATLASPRIV

Search for charged Higgs bosons in the $\tau\mbox{(hadronic)}$+jets final state with 1.03 fb$^{−1}$ of $pp$ collision data recorded at $\sqrt{s} = 7$ TeV with the ATLAS Experiment Czodrowski P Flechl M Isaksson C Kopp A Martyniuk A McCarn A Owen M zur Nedden M Neubauer M Patel N Randle-Conde A Riu I Saavedra A Sekula S Vickey T 2011 The experimental observation of charged Higgs bosons, $H^{\pm}$, which are predicted by many theories with an extended Higgs sector, would indicate new physics beyond the Standard Model. In the minimal supersymmetric extension to the Standard Model (MSSM), for example, the dominant production mode at the LHC for these Higgs bosons, when $m_{H^+} < m_t$, takes place in $t\overline{t}$ events via the top quark decay $t\rightarrow H^{+}b$ with $H^{+}\rightarrow\tau\nu$ dominating for most values of $\tan\beta$, the ratio of the vacuum expectation values of the two Higgs doublets. This note presents the results of a search for charged Higgs bosons in 1.03 fb$^{-1}$ of $\sqrt{s}=7$ TeV proton-proton collision data using the $\tau$+jets channel with a hadronically-decaying $\tau$ in the final state. The data agree with Standard-Model expectation. Thus, limits on $H^{+}$ production in $t\bar{t}$ events have been set: $\mathrm{BR}(t \to bH^{+}) \cdot \mathrm{BR}(H^+ \to \tau\nu)<0.03-0.17$ in the mass range 90-160 GeV. Interpreted in the context of the MSSM, this allows to exclude a region above about $\tan \beta=30$ in the mass range $100 < m_{H^+}$ [GeV] $< 150$. INTNOTEATLASPRIV

Search for Charged Higgs Bosons in the $\tau$+jets Final State in $t\overline{t}$ Decays with 1.03 fb$^{-1}$ of $pp$ Collision Data Recorded at $\sqrt{s} = 7$ TeV with the ATLAS Experiment Cavaliere V Czodrowski P Flechl M Isaksson C Kopp A Martyniuk A McCarn A Owen M zur Nedden M Neubauer M Patel N Randle-Conde A Riu I Saavedra A Sekula S Vickey T 2011 This note presents the results of a search for charged Higgs bosons, $H^{\pm}$, in 1.03 fb$^{-1}$ of proton-proton collision data recorded at $\sqrt{s}=7$ TeV with the ATLAS experiment at the LHC using the $\tau$+jets channel in $t\overline{t}$ decays with a hadronically decaying $\tau$ lepton in the final state. The data agree with the SM expectation leading to a limit on the product of branching ratios BR($t \to bH^{\pm}) \times$ BR($H^\pm \to \tau\nu$) of $0.03-0.10$ for $H^\pm$ masses in the range $90 \GeV<m_{H^\pm}<160 \GeV$. In the context of the MSSM values of $\tan \beta$ larger than $22-30$ are excluded in the mass range $90 \GeV< m_{H^\pm}< 140 \GeV$. INTNOTEATLASPRIV

The search for NMMSM ``Ideal Higgs Scenario'' at ATLAS Jez P Niels Bohr Institute 2011 The Next-to-minimal supersymmetric extension of the Standard Model (NMSSM) has one additional gauge singlet field on top of the particle content of the widely known MSSM. This leads to 2 new neutral bosons in the Higgs sector and one new fermion (5th neutralino). The NMSSM phenomenology can therefore be quite different from MSSM expectations. The ``Ideal Higgs'' scenario expects the existence of a CP-even SM-like Higgs boson $h_1$ below the LEP mass limits (100-110 GeV) decaying predominantly to the pair of very light CP-odd Higgs bosons $a_1$ which then decay to the pairs of $\tau$ leptons. The $a_1$ mass has already been quite constrained from below by B-factories, but limits for the mass of $a_1$ close to the $\Upsilon$ resonances are still quite weak. This note presents search for the $a_1$ resonances being produced directly by gluon fusion with both $\tau$ leptons decaying leptonically to electron and muon. Finding no evidence of $a_1$, new limits are set on $\sigma(gg\to a_1)\times BR(a_1\to\tau\tau)$ and interpreted in terms of phenomenological NMSSM parameters. INTNOTEATLASPRIV

Discovery potential of neutral MSSM higgs bosons decaying to tau-lepton pairs in the ATLAS experiment Davey William Edwin Melbourne U. Milan U. The Large Hadron Collider (LHC) is the highest energy particle collider ever built. It recently began operation at CERN and will probe physics at unprecedented scales. ATLAS is a particle detector located at one of the collision points on the LHC ring and is designed to be sensitive to the wide range of physics that could be produced. The primary objective of the LHC experiments is to determine the mechanism of electroweak symmetry breaking, of which many theoretical models exist. In the Minimal Supersymmetric Standard Model (MSSM), electroweak symmetry breaking is achieved through the Higgs mechanism, however, the Higgs sector must be extended with respect to the Standard Model and contains five physical Higgs bosons. The discovery potential of the MSSM Higgs bosons in ATLAS has been evaluated in previous studies, demonstrating adequate sensitivity for discovery or exclusion over a large region of the parameter space. However, these studies were performed using now outdated software, without an estimation of the expected systematic uncertainties or the inclusion of data-driven background estimation procedures. In this thesis, the discovery potential of the neutral MSSM Higgs bosons when decaying to tau-lepton pairs in the ATLAS experiment is evaluated. One tau is required to decay leptonically while the other is required to decay hadronically. Higgs boson mass hypotheses in the range 150 GeV - 800 GeV are considered. The study assumes a proton-proton collision energy of 14 TeV and an integrated luminosity of 30 fb−1 . The expected systematic uncertainty on the background measurement is evaluated and included in the calculation of the discovery potential. Data-driven estimation techniques are developed for the W+jets and QCD di-jet backgrounds. The contributions of all signal and background processes are estimated using Monte Carlo simulated event samples. The discovery potential is interpreted in the mmax h benchmark scenario, and is presented in the mA-tan β plane. A small degradation in performance with respect to the previous studies is found for Higgs boson masses below 450 GeV due to the inclusion of systematic uncertainties. It is confirmed that a large fraction of the parameter space will be accessible to the ATLAS experiment, which will be able to probe far beyond the regions already excluded by the LEP and Tevatron experiments. Two separate studies are also included, describing contributions to the modelling of hadronic tau reconstruction in the ATLAS fast simulation packages ATLFAST-I and ATLFAST-II. Firstly, a complete parameterisation of the calorimeter-based hadronic tau reconstruction for use in ATLFAST-I is presented. Secondly, the validation of the track-based hadronic tau reconstruction in ATLFAST-II is presented, including the extraction of correction terms to match the performance in ATLFAST-II to the standard ATLAS simulation. technical-report

Higgs Search at the LHC Rosati S 2011 This is the talk to be presented at the workshop: LC11 Workshop: Understanding QCD at Linear Colliders in searching for old and new physics. Most recent ATLAS and CMS results on Standard Model and MSSM Higgs Boson Searches are presented. INTNOTEATLASPRIV

Search for Charged Higgs Bosons in the $\tau$+jets Final State in $t\overline{t}$ Decays with 1.03 fb$^{-1}$ of $pp$ Collision Data Recorded at $\sqrt{s} = 7$ TeV with the ATLAS Experiment---Supporting Note Cavaliere V Czodrowski P Flechl M Isaksson C Kopp A Martyniuk A McCarn A Owen M zur Nedden M Neubauer M Patel N Randle-Conde A Riu I Saavedra A Sekula S Vickey T 2011 This note presents the results of a search for charged Higgs bosons, $H^{\pm}$, in 1.03 fb$^{-1}$ of proton-proton collision data recorded at $\sqrt{s}=7$ TeV with the ATLAS experiment at the LHC using the $\tau$+jets channel in $t\overline{t}$ decays with a hadronically decaying $\tau$ lepton in the final state. The data agree with the SM expectation leading to a limit on the product of branching ratios BR($t \to bH^{\pm}) \times$ BR($H^\pm \to \tau\nu$) of $0.03-0.10$ for $H^\pm$ masses in the range $90 \GeV<m_{H^\pm}<160 \GeV$. In the context of the MSSM values of $\tan \beta$ larger than $22-30$ are excluded in the mass range $90 \GeV< m_{H^\pm}< 140 \GeV$. INTNOTEATLASINT

First results on Higgs boson searches (SM + MSSM) and prospects from ATLAS Elmsheuser J LMU Munich 2011 The search for the Standard Model-like Higgs boson over a wide mass region and in multiple channels is presented, based on the ATLAS data collected in 2010. The first combination of these channels is also shown. In the area of MSSM Higgs bosons, new exclusion limits and exploratory studies are presented. These searches give sensitivity to various theoretical predictions which surpasses anything previously available. All observations are in agreement with the expectations from the background-only hypothesis. Hence exclusion limits at 95\% confidence level are derived. INTNOTEATLASPRIV

Search for charged Higgs bosons in the $\tau$+lepton final state in \ttbar\ decays with 1.03 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 7$ TeV with the ATLAS Experiment Cavaliere V Czodrowski P Flechl M Isaksson C Kopp A Martyniuk A McCarn A Owen M zur Nedden M Neubauer M Patel N Randle-Conde A Riu I Saavedra A Sekula S Vickey T 2011 This note presents the results of a search for charged Higgs bosons in 1.03 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=7$ TeV using the $\tau$+lepton channel in \ttbar\ decays with a hadronically decaying $\tau$ lepton in the final state. The data agree with the SM expectation leading to a limit on the product of branching ratios BR($t \to bH^{+}) \times$ BR($H^+ \to \tau\nu$) of $XXX$ for $H^+$ masses in the range $90 \GeV<M_{H^\pm}<160 \GeV$. In the context of the MSSM this excludes a region above $\tan \beta = YYY$ in the mass range $AAA \GeV< M_{H^\pm}< BBB \GeV$. INTNOTEATLASPRIV

Tau physics in ATLAS Kuehn S Albert-Luwdigs Universitaet Freiburg 2011 The ATLAS experiment has an extensive physics program, involving tau lepton final states. In these proceedings, the identification of hadronically decaying tau leptons is described. Investigations with Standard Model processes, namely the observation of W to tau nu and a Z to tau tau production cross section measurement, are given. Finally, results on the MSSM Higgs boson search are presented, with exclusion limits at the 95% confidence level. INTNOTEATLASPRIV

Search for neutral MSSM Higgs bosons decaying to tau+tau- pairs in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector 2011 A search for neutral Higgs bosons decaying to pairs of tau leptons with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of 7 TeV, recorded in 2011 and corresponding to an integrated luminosity of 1.06 fb^−1 . After signal selection, 4630 events are observed in this data sample. The observed number of events is consistent with the total expected background of 4900 ± 600 events. Exclusion limits at the 95% confidence level are derived for the production cross section of a generic Higgs boson phi as a function of the Higgs boson mass and for A/H/h production in the Minimal Supersymmetric Standard Model (MSSM) as a function of the parameters mA and tan beta. INTNOTEATLASPUBL

Search for Charged Higgs Bosons in the $\tau$+jets Final State in $t\overline{t}$ Decays with 1.03 fb$^{-1}$ of $pp$ Collision Data Recorded at $\sqrt{s} = 7$ TeV with the ATLAS Experiment 2011 This note presents the results of a search for charged Higgs bosons, $H^{\pm}$, in 1.03 fb$^{-1}$ of proton-proton collision data recorded at $\sqrt{s}=7$ TeV with the ATLAS experiment at the LHC using the $\tau$+jets channel in $t\overline{t}$ decays with a hadronically decaying $\tau$ lepton in the final state. The data agree with the SM expectation leading to a limit on the product of branching ratios BR($t \to bH^{\pm}) \times$ BR($H^\pm \to \tau\nu$) of $0.03-0.10$ for $H^\pm$ masses in the range $90 \GeV<m_{H^\pm}<160 \GeV$. In the context of the MSSM values of $\tan \beta$ larger than $22-30$ are excluded in the mass range $90 \GeV< m_{H^\pm}< 140 \GeV$. INTNOTEATLASPUBL

Tau physics in ATLAS Kuehn S Freiburg U. 2011 The ATLAS experiment has an extensive physics program, involving tau lepton final states. In these proceedings, the identification of hadronically decaying tau leptons is described. Investigations with Standard Model processes, namely the observation of W to tau nu and a Z to tau tau production cross section measurement, are given. Finally, results on the MSSM Higgs boson search are presented, with exclusion limits at the 95% confidence level. INTNOTEATLASPUBL

Search for Charged Higgs Bosons in the $\tau$+jets Final State in $t\overline{t}$ Decays with 1.03 fb$^{-1}$ of $pp$ Collision Data Recorded at $\sqrt{s} = 7$ TeV with the ATLAS Experiment Flechl M Sekula S Vickey T 2011 This paper presents the results of a search for charged Higgs bosons, $H^{\pm}$, in 1.03 fb$^{-1}$ of proton-proton collision data recorded at $\sqrt{s}=7$ TeV with the ATLAS experiment at the LHC using the $\tau$+jets and $\tau$+lepton channels in $t\overline{t}$ decays with a hadronically decaying $\tau$ lepton in the final state. The data agree with the SM expectation leading to a limit on the product of branching ratios BR($t \to bH^{\pm}) \times$ BR($H^\pm \to \tau\nu$) of XXX for $H^\pm$ masses in the range $90 \GeV<m_{H^\pm}<160 \GeV$. In the context of the MSSM values of $\tan \beta$ larger than YYY are excluded in the mass range ZZZ $\GeV$. INTNOTEATLASPRIV

Search for charged Higgs bosons in the $\tau$+lepton final state in $t\bar{t}$ decays with 1.03 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 7$ TeV with the ATLAS Experiment Cavaliere V Czodrowski P Flechl M Isaksson C Kopp A Martyniuk A McCarn A zur Nedden M Neubauer M Owen M Patel N Randle-Conde A Riu I Saavedra A Sekula S Vickey T 2011 This note presents the results of a search for charged Higgs bosons in 1.03 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=7$ TeV using the $ \tau$+lepton channel in $t\bar{t}$ decays with a hadronically decaying $\tau$ lepton in the final state. The data agree with the SM expectation leading to a limit on the product of branching ratios BR($t \to bH^{+}) \times$ BR($H^+ \to \tau \nu$) of 0.05-0.15 for $H^+$ masses in the range 90 GeV <$M_{H^\pm}$<160 GeV. INTNOTEATLASPRIV

Search for neutral and charged MSSM Higgs bosons in ATLAS Flechl M Freiburg 2011 The results of Higgs boson searches in the context of the Minimal Supersymmetric extension of the Standard Model (MSSM) in proton-proton collisions with the ATLAS detector based on collected data corresponding to up to 36 pb$^{-1}$ are presented. Searches in the channels $H^+ -> cs$, $H^+ -> tau nu$, and $H -> tautau$ are discussed. All observations agree with the expectation of the Standard Model (SM)-only hypothesis and thus exclusion limits are derived. INTNOTEATLASPRIV

Search for charged Higgs bosons in ATLAS Pelikan D Uppsala University 2011 Charged Higgs bosons are predicted in several extensions of the Standard Model, where there is more than one doublet of complex scalars in the Higgs sector, for instance Two-Higgs-Doublet Models (2HDM), which is also the case in the Minimal Supersymmetric Standard Model (MSSM). For m(H+) &lt; m(top), the dominant production mode for charged Higgs bosons at the LHC is via the decay t -&gt; bH+ of one of the top quarks in ttbar events. We present results on the search for such light charged Higgs bosons in the ATLAS experiment, with emphasis on the decays H+ -&gt; tau+nu. INTNOTEATLASPRIV

Talk "Higgs Hunting in ATLAS" Andari N 2011 A talk to give in the International Workshop LHC on the March - IHEP- Protvino-Russia about the SM and MSSM Higgs searches in ATLAS. INTNOTEATLASPRIV

PoS PoS Search for neutral and charged MSSM Higgs bosons in ATLAS Flechl Martin Freiburg U. 2011 EPS-HEP2011 The results of Higgs boson searches in the context of the Minimal Supersymmetric extension of the Standard Model (MSSM) in proton-proton collisions with the ATLAS detector based on collected data corresponding to up to 36 pb$^{-1}$ are presented. Searches in the channels $H^+ -> cs$, $H^+ -> tau nu$, and $H -> tautau$ are discussed. All observations agree with the expectation of the Standard Model (SM)-only hypothesis and thus exclusion limits are derived. research-article

Search for a charged Higgs boson decaying via H+ to tau(lep)+nu in ttbar events with one or two light leptons in the final state using 1.03/fb of pp collision data recorded at sqrt(s) = 7 TeV with the ATLAS detector 2011 This paper presents the results of a search for charged Higgs bosons by the ATLAS experiment, based on 1.03/fb of proton-proton collision data at sqrt(s) = 7 TeV using the single-lepton and dilepton channels in ttbar decays with a leptonically decaying tau in the final state. The data agree with the Standard Model expectation. Assuming B(H+ to tau+nu)=1, this leads to upper limits on the branching fraction B(t to bH+) between 5.2% and 14.1% for H+ masses in the range 90 GeV < m(H+) <160 GeV. In the context of the mh_max scenario of the MSSM, values of tan(beta) larger than 30-56 are excluded for H+ masses in the range 90 GeV < m(H+) < 140 GeV. INTNOTEATLASPUBL

Search for a charged Higgs boson H+ decaying via to tau(lep)+nu in ttbar events with one or two light leptons in the final state using 1.03/fb of pp collision data recorded at sqrt(s) = 7 TeV with the ATLAS detector Barak L Breaden-Madden W Cheu E Collins-Tooth C Ferrari A Flechl M Gross E Groth-Jensen J Hattrem Raddum S Madsen A Mal P Nakamura K Pelikan D Quilty D Read A Wright M 2011 This paper presents the results of a search for charged Higgs bosons by the ATLAS experiment, based on 1.03/fb of proton-proton collision data at sqrt(s) = 7 TeV using the single-lepton and dilepton channels in ttbar decays with a leptonically decaying tau in the final state. The data agree with the Standard Model expectation. Assuming B(H+ to tau+nu)=1, this leads to upper limits on the branching fraction B(t to bH+) between 5.2% and 14.1% for H+ masses in the range 90 GeV < m(H+) <160 GeV. In the context of the mh_max scenario of the MSSM, values of tan(beta) larger then 30-56 are excluded for H+ masses in the range 90 GeV < m(H+) < 140 GeV. INTNOTEATLASINT

ATLAS Higgs Searches Abreu Henso LAL-Orsay 2011 A search for the Standard Model Higgs boson at the Large Hadron Collider (LHC) running at a centre-of-mass energy of 7 TeV is reported, based on a total integrated luminosity of 1.0 to 2.3 fb−1 collected by the ATLAS detector in 2011. Several Higgs boson decay channels are combined in a mass range from 110 GeV to 600 GeV. No significant evidence for a signal is observed. The Standard Model Higgs boson mass ranges from 146 GeV to 232 GeV, 256 GeV to 282 GeV and 296 GeV to 466 GeV are excluded at the 95% CL, while the expected Standard Model Higgs boson exclusion in the absence of signal ranges to 131 GeV to 447 GeV. In addition, the search for the neutral Higgs bosons in the Minimal Supersymmetric extension to the Standard Model (MSSM) is presented, where exclusion limits at the 95% CL are derived for the production cross section of a generic Higgs boson phi as a function of the Higgs boson mass and for A/H/h-> tau tau in the MSSM as a function of the parameters mA and tanB in the m^max_h scenario. INTNOTEATLASPRIV

Higgs Searches With ATLAS Wiglesworth C 2011 The search for the Standard Model Higgs boson with the ATLAS detector at the LHC is reported. The search combines several decay channels in the mass range 110 to to 600 GeV and derives upper limits on the production cross section as a function of mass. A search for neutral Higgs bosons (A/H/h) in the MSSM decaying to τ lepton pairs is also reported, where upper limits on the production cross sections are derived as a function of the parameters mA and tanβ. The searches are based on a dataset corresponding to an integrated luminosity ranging from 1.0 fb−1 to 2.3 fb−1 of pp collisions at a centre-of-mass energy of 7 TeV. INTNOTEATLASPRIV

Higgs Searches With ATLAS Wiglesworth C Queen Mary, U. of London 2011 The search for the Standard Model Higgs boson with the ATLAS detector at the LHC is reported. The search combines several decay channels in the mass range 110 to to 600 GeV and derives upper limits on the production cross section as a function of mass. A search for neutral Higgs bosons (A/H/h) in the MSSM decaying to τ lepton pairs is also reported, where upper limits on the production cross sections are derived as a function of the parameters mA and tanβ. The searches are based on a dataset corresponding to an integrated luminosity ranging from 1.0 fb−1 to 2.3 fb−1 of pp collisions at a centre-of-mass energy of 7 TeV. INTNOTEATLASPUBL

Bohr Inst. Copenhagen A search for supersymmetric low mass Higgs boson at the LHC with the ATLAS detector Jez Pavel Bohr Inst. 2011 The Next-to-minimal supersymmetric extension of the Standard Model (NMSSM) has one additional gauge singlet field on top of the particle content of the widely known MSSM. This leads to two new neutral bosons in the Higgs sector and one new fermion (5th neutralino). The NMSSM phenomenology can therefore be quite different from MSSM expectations. The ``Ideal Higgs'' scenario expects existence of a CP-even SM-like Higgs boson $h_1$ below the LEP mass limits (100-110 GeV) decaying predominantly to the pair of light (less than 11 GeV) CP-odd Higgs bosons $a_1$ which then decay to the pairs of $ au$ leptons. The mass of $a_1$ has already been quite constrained from below by B-factories, but limits for the mass of $a_1$ close to the $Upsilon$ resonances are still quite weak. This thesis presents a search for the $a_1$ resonances being produced directly by gluon fusion with both $ au$ leptons decaying leptonically to an electron and a muon and sets new experimental limits in a mass region close to the $Upsilon$ resonances. The tau trigger is a key element of the study of low mass Higgs bosons, including the indirect production of the $a_1$ via $h_1 o a_1 a_1 o 4 au$. The LHC data delivers more than one interaction per event - so-called pile-up and the amount of pile-up will increase significantly in 2012. Data and Monte Carlo simulations have been studied to find the effect of pile-up on the tau trigger performance. Eventually, the trigger selection was optimized for the pile-up environment. technical-report

Searches for Charged Higgs Bosons in ATLAS Czodrowski P Technische Universitaet Dresden 2011 The charged Higgs boson is predicted by many extended Higgs scenarios, such as models containing Higgs triplets and Two-Higgs-Doublet Models (2HDM). The observation of charged Higgs bosons, $H^+$, would indicate physics beyond the Standard Model (SM). Both analyses presented here consider the type-II 2HDM, which is also the Higgs sector of the Minimal Supersymmetric Standard Model (MSSM). For charged Higgs boson masses, $m_{H^+}$, smaller than the top quark mass, $m_t$, the dominant production mode at the LHC for $H^+$ is through top quark decay via $t\to bH^+$. The dominant source of top quarks at the LHC is $t\bar{t}$ production. INTNOTEATLASPRIV

Nuovo Cimento C Nuovo Cimento C Searches for Charged Higgs Bosons in ATLAS Czodrowski P TU, Dresden (main) 2012 035 213 216 The charged Higgs boson is predicted by many extended Higgs scenarios, such as models containing Higgs triplets and Two-Higgs-Doublet Models (2HDM). The observation of charged Higgs bosons, $H^+$, would indicate physics beyond the Standard Model (SM). Both analyses presented here consider the type-II 2HDM, which is also the Higgs sector of the Minimal Supersymmetric Standard Model (MSSM). For charged Higgs boson masses, $m_{H^+}$, smaller than the top quark mass, $m_t$, the dominant production mode at the LHC for $H^+$ is through top quark decay via $t\to bH^+$. The dominant source of top quarks at the LHC is $t\bar{t}$ production. research-article

ATLAS Higgs Searches Abreu Henso Orsay, LAL 2012 A search for the Standard Model Higgs boson at the Large Hadron Collider (LHC) running at a centre-of-mass energy of 7 TeV is reported, based on a total integrated luminosity of 1.0 to 2.3 fb−1 collected by the ATLAS detector in 2011. Several Higgs boson decay channels are combined in a mass range from 110 GeV to 600 GeV. No significant evidence for a signal is observed. The Standard Model Higgs boson mass ranges from 146 GeV to 232 GeV, 256 GeV to 282 GeV and 296 GeV to 466 GeV are excluded at the 95% CL, while the expected Standard Model Higgs boson exclusion in the absence of signal ranges to 131 GeV to 447 GeV. In addition, the search for the neutral Higgs bosons in the Minimal Supersymmetric extension to the Standard Model (MSSM) is presented, where exclusion limits at the 95% CL are derived for the production cross section of a generic Higgs boson phi as a function of the Higgs boson mass and for A/H/h-> tau tau in the MSSM as a function of the parameters mA and tanB in the m^max_h scenario. INTNOTEATLASPUBL

Search for charged Higgs bosons in ATLAS Pelikan D Uppsala 2012 Charged Higgs bosons are predicted in several extensions of the Standard Model, where the Higgs sector contains more than one doublet of complex scalars, for instance in the Minimal Supersymmetric Standard Model (MSSM). For $m_{H^+} < m_{top}$, the dominant production mode for charged Higgs bosons at the LHC is via the decay $t\rightarrow bH^+$ of one of the top quarks in $t\bar{t}$ events. We present results on the search for such light charged Higgs bosons in the ATLAS experiment, with emphasis on the decay $H^+ \rightarrow \tau \nu$. INTNOTEATLASPRIV

EPJ Web Conf. EPJ Web Conf. Search for charged Higgs bosons in ATLAS Pelikan Daniel Uppsala U. 2012 28 Charged Higgs bosons are predicted in several extensions of the Standard Model, where the Higgs sector contains more than one doublet of complex scalars, for instance in the Minimal Supersymmetric Standard Model (MSSM). For $m_{H^+} < m_{\mathrm{top}}$, the dominant production mode for charged Higgs bosons at the LHC is via the decay $t\rightarrow bH^+$ of one of the top quarks in $t\bar{t}$ events. We present results on the search for such light charged Higgs bosons in the ATLAS experiment, with emphasis on the decay $H^+ \rightarrow \tau \nu$. research-article

Search for Neutral MSSM Higgs Bosons in the Channel $h/A/H \rightarrow \mu^{+}\mu^{-}$ with the ATLAS Detector Stern S MPI Munich Kortner S MPI Munich 2012 This note presents the search for neutral MSSM Higgs bosons decaying into two muons with the ATLAS detector at the LHC. The analysis is performed on 4.8 fb$^{-1}$ of proton-proton collisions at a centre-of-mass energy of $\sqrt{s} =$ 7 TeV recorded in 2011. Events are categorized according to the number of $b$-jets in the final state. The total dimuon background background is estimated purely from data. No significant excess compared to the Standard Model expectation is found in the data. Exclusion limits on the MSSM parameter $\tan \beta$ and on the cross section times branching fraction for both relevant production mechanisms are set as a function of the mass of the pseudo-scalar or generic Higgs boson, respectively, in the range from 120 to 300 GeV. INTNOTEATLASPRIV

Search for charged Higgs bosons in the tau+jets final state in ttbar decays with 4.6 fb−1 of pp collision data recorded at √s = 7 TeV with the ATLAS Experiment — Supporting Note Assamagan P Bernius C Casado P Cavaliere V Czodrowski P Chakraborty D Greenwood D Ferrari A Flechl M Hattrem Raddum S Kopp A Mal P McCarn A Neubauer M Patel N Randle-Conde A Read A L Rocha de Lima G Saavedra A Schumacher M Sekula S 2012 The experimental observation of charged Higgs bosons, H±, which are predicted by many models with an extended Higgs sector, would indicate physics beyond the Standard Model (SM). This note presents the results of a search for charged Higgs bosons in \LUMI of proton-proton collision data at √s = 7 TeV using the tau+jets channel in ttbar decays with a hadronically decaying tau lepton in the final state. The data agree with the SM expectation leading to a limit on the branching ratio BR(t -> b H+) of 0.01-0.06 for charged Higgs boson masses (m_{H+}) in the range 90 GeV < m_{H+} < 160 GeV, assuming BR(H+ -> tau nu)=1. In the context of the m_h-max scenario of the MSSM, this excludes a region above tan(beta) = 10-22 in the mass range 90 GeV < m_{H+} < 150 GeV. INTNOTEATLASPRIV

Search for a charged Higgs boson decaying via H+ -> tau(had)nu+lepton in ttbar events using 4.6 fb−1 of pp collision data recorded at sqrt(s) = 7 TeV with the ATLAS detector — Supporting note Behar S Buszello C Czodrowski P Ferrari A Flechl M Hattrem Raddum S Isaksson C Madsen A McCarn A zur Nedden M Neubauer M Patel N Pelikan D Read A Rozen Y Saavedra A 2012 This note reports on the results of a search for charged Higgs bosons in the ATLAS experiment, based on 4.6 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=7$ TeV, using $t\bar{t}$ decays with a hadronically decaying $\tau$ and one light lepton (electron or muon) in the final state. The data agree with the Standard Model expectation. Assuming ${\cal B}(H^+ \rightarrow \tau\nu) = 1$, this leads to upper limits on the branching fraction ${\cal B}(t \rightarrow bH^{+})$ between 3% and 7% for charged Higgs boson masses ($m_{H^+}$) in the range $90\,\mbox{GeV} < m_{H^+} <160\,\mbox{GeV}$. In the context of the $m_h^{\text{max}}$ scenario of the MSSM, values of $\tan\beta$ larger than 22-50 are excluded for charged Higgs boson masses in the range $90\,\mbox{GeV} < m_{H^+} < 150\,\mbox{GeV}$. INTNOTEATLASPRIV

Search for a charged Higgs boson decaying via H+ -> tau(lep) + jets in ttbar events using 4.6 fb−1 of pp collision data recorded at sqrt(s) = 7 TeV with the ATLAS detector — Supporting note Barak L Ferrari A Flechl M Gross E Groth-Jensen J Hattrem Raddum S Read A 2012 This note reports on the results of a search for charged Higgs bosons in the ATLAS experiment, based on 4.6 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=7$ TeV using the lepton+jets channel in $t\bar{t}$ decays with a leptonically decaying $\tau$ in the final state. The data agree with the Standard Model expectation. Assuming ${\cal B}(H^+ \rightarrow \tau\nu) = 1$, this leads to upper limits on the branching fraction ${\cal B}(t \rightarrow bH^{+})$ between 4% and 15% for charged Higgs boson masses ($m_{H^+}$) in the range $90\,\mbox{GeV} < m_{H^+} <160\,\mbox{GeV}$. In the context of the $m_h^{\text{max}}$ scenario of the MSSM, values of $\tan\beta$ larger than 27-44 are excluded for charged Higgs boson masses in the range $90\,\mbox{GeV} < m_{H^+} < 140\,\mbox{GeV}$. INTNOTEATLASPRIV

Search for charged Higgs bosons decaying via H+ -> tau nu in ttbar events using 4.6 fb−1 of pp collision data at sqrt(s) = 7 TeV with the ATLAS detector Collaboration ATLAS 2012 This paper presents the results of a search for charged Higgs bosons by the ATLAS experiment, based on 4.6 fb−1 of LHC proton-proton collision data at √s = 7 TeV, using ttbar decays with a tau lepton in the final state. The data agree with the Standard Model expectation. Assuming B(H+ → τν) = 1, this leads to upper limits on the branching ratio B(t → bH+) between ?.?% and ?.?% for H+ masses in the range 90 GeV < mH+ < 160 GeV. In the context of the mh-max scenario of the MSSM, values of tan β larger than ??–?? are excluded for H+ masses in the range 90 GeV < mH+ < 140 GeV. INTNOTEATLASPRIV

Search for Neutral MSSM Higgs Bosons H → τ+τ− → lτh with the ATLAS Detector in 7 TeV Collisions Bristow T University of the Withwaterstrand Goussiou A University of Washington Glatzer J University of Freiburg, University of Bonn Keller J University of Washington Krosenberg J University of Bonn Rompotis N University of Washington Thoma S University of Freiburg Vickey T University of the Withwaterstrand Wang T University of Bonn 2012 We report a search for neutral Higgs bosons produced in proton-proton collisions delivered by the Large Hadron Collider (LHC) at center-of-mass energy 7 TeV and recorded by the ATLAS detector. The data correspond to an integrated luminosity of 4660 pb−1. The search focuses on final states where the Higgs bosons decay in a τ+τ− pair with one τ lepton decaying leptonically and the other hadronically. Two searches, which use the presence or not of a b-quark in the final state to distinguish among different Higgs production mechanisms, are combined in order to increase sensitivity. The data are found to be consistent with Standard Model (SM) expectations and upper limits on the cross section times the branching ratio of a hypothesized Higgs boson are interpreted in the minimal supersymmetric standard model (MSSM) parameter space excluding tan β &amp;gt; XX for CP-odd Higgs mass XXX Gev. INTNOTEATLASPRIV

Search for Neutral MSSM Higgs Bosons $H\to\tau^+\tau^-\to\tau_h\tau_h$ + 2 neutrinos with the ATLAS Detector in proton-proton collision at $sqrt(s)=7 TeV$ with the ATLAS Experiment Davey W University of Bonn Dawe N Simon Fraser University Dingfelder J University of Bonn Glatzer J University of Freiburg, University of Bonn Grimm K Lancaster University Mader W Technische Universitaet Dresden Morgenstern M Technische Universitaet Dresden Rosendahl P University of Bergen Scutti F University of Bonn Strassner A Technische Universitaet Dresden Trottier-McDonald M Simon Fraser University Tsuno S KEK Xella S University of Copenhagen Zanzi D MPI Munich Zinonos Z INFN Sezione di Pisa 2012 A search for neutral MSSM Higgs bosons $A$, $H$, $h$ with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of $7 TeV$, corresponding to an integrated luminosity of $4.66 fb^-1$ and focuses on Higgs decays into two $\tau$ leptons, $A/H/h\to\tau^+\tau^-$, where both $\tau$ leptons decay hadronically. The search is pursued in two exclusive bins with at least one identified b-jet or without identified b-jet. After signal selection, XX events are observed in this data sample in the channel with b-jets and YY events are observed in the channel without b-jets. The observed number of events is (not) consistent with the background estimate of 65.2 events and 1104.6 events. An exclusion limit for the neutral MSSM CP-odd Higgs boson, $A$, production is derived as a function of cross section times branching ratio. This limit is also presented as a function of two parameters $m_A$ and $\tan\beta$. INTNOTEATLASPRIV

Dresden, Tech. U. Dresden Measurement of the Cross Section for the Process $pp \to \gamma^{∗}/Z \to \tau^{+}\tau^{-}$ and a Search for Neutral MSSM Higgs Bosons with the ATLAS Detector Gumpert Christian Dresden, Tech. U. 2011 The search for Higgs bosons is among the primary goals of the ATLAS experiment. The minimal supersymmetric extension to the Standard Model contains three neutral Higgs bosons which are detectable through their decays into pairs of tau leptons. A major background for this discovery channel in the low mass region $M_{A} = 100-150 GeV$ arises from $\gamma^{*}/Z \to \tau^{+}\tau^{-}$ events. In this thesis, the cross section of the process $pp \to \gamma^{*}/Z \to \tau^{+}\tau^{-}$ is measured by investigating the fully leptonic final state. Therefore, $L = 35.5 pb^{-1}$ of data from proton-proton collisions recorded by the ATLAS detector at a centre-of-mass energy of 7TeV are analysed. The result obtained is $\sigma(pp \to \gamma^{*}/Z \to \tau^{+}\tau^{-})= 1.05 \pm 0.13(stat.)\pm 0.10(syst.)\pm 0.04(lumi.)nb$ and is in agreement with the theoretical prediction. Furthermore, the discovery channel $pp \to h/H/A \to \tau^{+}\tau^{-}$ is analysed in the purely leptonic final state for the low mass region $M_{A}=100-150 GeV$. An optimisation of the event selection by the usage of multivariate techniques is investigated. The optimal selection strategy is applied on $L = 1.06 fb({-1}$ of data recorded by the ATLAS detector. As the statistical analysis does not yield a significant deviation from the Standard Model expectation, exclusion limits in the $M_{A}\times tan \beta$ parameter space of the MSSM are derived. In the context of the $m_{h}^{max}$ scenario, this thesis concludes that values of $tan \beta > 32-51$ depending on the parameter $M_A$ are excluded at a 95% confidence level. technical-report

ATLAS Search for NMSSM H+ to a1 W with 4.7 fb-1 Potter CT University of Oregon 2012 The Next-to Minimal Supersymmetric Model (NMSSM) is motivated by mu-term problem of the Minimal Supersymmetric Model (MSSM) and may explain anomalous experimental measurements. The NMSSM can significantly alter the phenomenology of the MSSM Higgs sector by allowing Higgs-to-Higgs decays thereby suppressing standard search channels. If the lightest CP-odd NMSSM Higgs Boson a1 satisfies 2Mtau &lt; Ma1 &lt; 2Mb, the dominant decay is a1 to tau+tau- with a1 to mu+mu- at a suppressed but measurable level. We present a search in 2011 data collected at the Large Hadron Collider for a light charged Higgs produced from top quark decay t to bH+ with subsequent decay H+ to a1W with an integrated luminosity of 4.7fb-1 at 7 TeV center-of-mass energy. INTNOTEATLASPRIV

ATLAS Higgs Searches Andari N 2012 A combined search for the Standard Model Higgs boson with the ATLAS experiment at LHC using datasets corresponding to integrated luminosities from 1.0 to 2.3 fb-1 of pp collision at sqrt{s}=7 TeV is presented. The Higgs boson mass ranges 146 - 230 GeV, 256 - 282 GeV and 296 - 459 GeV are excluded at 95% Confidence Level, while the range 131 - 450 GeV is expected to be excluded in the absence of a signal. Searches in several decay channels are discussed. No significant excess was observed in any of these channels for the entire mass range from 110 to 600 GeV. In addition, a search for neutral Higgs bosons in the Minimal Supersymmetric extension to the Standard Model (MSSM) is presented. INTNOTEATLASPRIV

Search for Neutral MSSM Higgs Bosons in $A^0/h^0/H^0 \rightarrow \tau^+\tau^- \rightarrow e^\pm\mu^\mp + 4\nu$ Final States with $b$-Tagged Jets in Proton-Proton Collisions at $\sqrt{s}=7\,\textrm{TeV}$ with the ATLAS Detector von Radziewski Holger Albert-Ludwigs-Universitaet Freiburg, Fakultaet fuer Mathematik und Physik Lai Stanley Albert-Ludwigs-Universitaet Freiburg, Fakultaet fuer Mathematik und Physik Warsinsky Markus Albert-Ludwigs-Universitaet Freiburg, Fakultaet fuer Mathematik und Physik Schumacher Markus Albert-Ludwigs-Universitaet Freiburg, Fakultaet fuer Mathematik und Physik 2012 A search for neutral MSSM Higgs bosons $A$, $H$, $h$ with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of $7\TeV$, corresponding to an integrated luminosity of 4.66 fb$^{-1}$ and focuses on Higgs decays into two tau leptons, $A/H/h\to\tau^+\tau^-$, one tau lepton decays via $\tau \rightarrow \mu \nu_{\tau} \nu_{\mu}$ and the other decays via $\tau \rightarrow e \nu_{\tau} \nu_e$. In addition, one identified $b$-jet is required, to increase sensitivity to Higgs boson production in association with $b$-jets ($b\bar{b}H$). No excess of events beyond Standard Model expectation is observed and exclusion limits are presented in the $m_A$ vs. $\tan\beta$ plane of the $m_H^\text{max}$ scenario. INTNOTEATLASPRIV

ATLAS Higgs Searches Andari N Orsay, LAL 2012 A combined search for the Standard Model Higgs boson with the ATLAS experiment at LHC using datasets corresponding to integrated luminosities from 1.0 to 2.3 fb-1 of pp collision at sqrt{s}=7 TeV is presented. The Higgs boson mass ranges 146 - 230 GeV, 256 - 282 GeV and 296 - 459 GeV are excluded at 95% Confidence Level, while the range 131 - 450 GeV is expected to be excluded in the absence of a signal. Searches in several decay channels are discussed. No significant excess was observed in any of these channels for the entire mass range from 110 to 600 GeV. In addition, a search for neutral Higgs bosons in the Minimal Supersymmetric extension to the Standard Model (MSSM) is presented. INTNOTEATLASPUBL

Combined limits for H+ -> taunu in ttbar decays with 4.6 fb^{-1} of pp collision data recorded at $sqrt{s} = 7$ TeV with the ATLAS experiment --- Supporting Note Flechl M Freiburg Hattrem Raddum S Oslo Read AL Oslo 2012 The experimental observation of charged Higgs bosons which are predicted by many models with an extended Higgs sector, would indicate physics beyond the Standard Model (SM). This note presents the details of the combination of the results from a search for charged Higgs bosons in 4.6 fb-1 of proton-proton collision data at sqrt{s}=7 TeV in three H+ -> taunu final states in tbar decays. The data agree with the SM expectation leading to a limit on the branching ratio BR(t -> bH+) of 0.01-0.05 for charged Higgs boson masses (m_H+) in the range 90 GeV<m_H+<160 GeV, assuming BR(H+ -> taunu)=1. In the context of the mh-max scenario of the MSSM, this excludes a region above eta = 13-26 in the mass range 90 GeV< m_H+< 150 GeV. INTNOTEATLASPRIV

Search for Neutral MSSM Higgs Bosons in $A/h/H \rightarrow \tau^+ \tau^- \rightarrow e\mu + 4\nu$ Final State with 0 Jets in Proton-Proton Collisions at $\sqrt{s}=7$ TeV with the ATLAS Detector Friedrich F IKTP Dresden Gumpert C IKTP Dresden Kobel M IKTP Dresden Mader W IKTP Dresden Morgenstern M IKTP Dresden Straessner A IKTP Dresden 2012 A search for neutral MSSM Higgs bosons $A$, $H$, $h$ with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collision data taken at a center-of-mass energy of 7 TeV, corresponding to an integrated luminosity of $4.66\text{fb}^{-1}$. It focuses on Higgs decays into two tau leptons, $A/H/h \to \tau^+ \tau^-$, where one tau lepton decays via $\tau \rightarrow \mu \nu_{\tau} \nu_{\mu}$ and the other via $\tau \rightarrow e \nu_{\tau} \nu_e$. Additionally, only events with no reconstructed jets are considered to increase the sensitivity to Higgs production via gluon-fusion. No significant excess of events beyond the Standard Model expectation is observed and exclusion limits are calculated in the $m_A-\tan \beta$ plane in the $m_h^\mathrm{max}$ scenario. INTNOTEATLASPRIV

Search for charged Higgs bosons decaying via H+ -> tau nu in ttbar events using 4.6 fb−1 of pp collision data at sqrt(s) = 7 TeV with the ATLAS detector Collaboration ATLAS 2012 The results of a search for charged Higgs bosons are presented. The analysis is based on 4.6/fb of proton-proton ($pp$) collision data at $\sqrt{s}=7$ TeV collected by the ATLAS experiment at the Large Hadron Collider, using $t\bar{t}$ events with a $\tau$ lepton in the final state. The data are consistent with the expected background from Standard Model processes. Assuming that the branching fraction ${\cal B}(H^{\pm} \rightarrow \tau\nu)$ is 100%, this leads to upper limits on ${\cal B}(t \rightarrow bH^{+})$ between 5% and 1% for charged Higgs boson masses $(m_{H^+})$ ranging from 90 to 160 GeV, respectively. In the context of the $m_h^{\text{max}}$ scenario of the MSSM, values of $\tan\beta$ larger than 13-26 are excluded for charged Higgs boson masses in the range $90~\mbox{GeV} < m_{H^+} < 150~\mbox{GeV}$. INTNOTEATLASPRIV

Search for charged Higgs bosons decaying via H+ -> tau nu in ttbar events using 4.6 fb−1 of pp collision data at sqrt(s) = 7 TeV with the ATLAS detector 2012 The results of a search for charged Higgs bosons are presented. The analysis is based on 4.6/fb of proton-proton ($pp$) collision data at $\sqrt{s}=7$ TeV collected by the ATLAS experiment at the Large Hadron Collider, using $t\bar{t}$ events with a $\tau$ lepton in the final state. The data are consistent with the expected background from Standard Model processes. Assuming that the branching fraction ${\cal B}(H^{\pm} \rightarrow \tau\nu)$ is 100%, this leads to upper limits on ${\cal B}(t \rightarrow bH^{+})$ between 5% and 1% for charged Higgs boson masses $(m_{H^+})$ ranging from 90 to 160 GeV, respectively. In the context of the $m_h^{\text{max}}$ scenario of the MSSM, values of $\tan\beta$ larger than 13-26 are excluded for charged Higgs boson masses in the range $90~\mbox{GeV} < m_{H^+} < 150~\mbox{GeV}$. INTNOTEATLASPUBL

LHCC Poster: Search for the MSSM Higgs bosons with the ATLAS detector v Radziewski H University of Freiburg, Germany 2012 Poster to be presented at LHCC Poster Session, from ATLAS-CONF-2011-132 and ATLAS-CONF-2012-011 INTNOTEATLASPRIV

Beyond Standard Model Higgs searches at ATLAS Lenzi B 2012 Talk to be given at DIS INTNOTEATLASPRIV

Physics with Tau Lepton Final States in ATLAS Trottier-McDonald M Simon Fraser University 2012 Physics involving tau lepton signatures form an integral part of the ATLAS physics programme. Tau lepton identification is used in many analyses at ATLAS such as searches for exotic phenomena and Higgs bosons, as well as Standard Model measurements of cross-sections. The performance of the reconstruction and identification algorithms for hadronically decaying tau leptons is reviewed. The cross-section measurement of the Z boson decaying to a pair of tau leptons is discussed, as well as the search for heavier ditau resonances such as supersymmetric Higgs bosons. INTNOTEATLASPRIV

Search for non Standard Model Higgs Bosons with ATLAS Anders C 2012 Slides for MCTP 12 on searches for non Standard Model Higgs Bosons with ATLAS. Include are: fermiophobic Higgs, neutral MSSM Higgs, charged Higgs, doubly charged Higgs and nMSSM a_1 to mumu. INTNOTEATLASPRIV

Physics with Tau Lepton Final States in ATLAS Trottier-McDonald M Simon Fraser U. 2012 Physics involving tau lepton signatures form an integral part of the ATLAS physics programme. Tau lepton identification is used in many analyses at ATLAS such as searches for exotic phenomena and Higgs bosons, as well as Standard Model measurements of cross-sections. The performance of the reconstruction and identification algorithms for hadronically decaying tau leptons is reviewed. The cross-section measurement of the Z boson decaying to a pair of tau leptons is discussed, as well as the search for heavier ditau resonances such as supersymmetric Higgs bosons. INTNOTEATLASPUBL

JHEP JHEP Search for charged Higgs bosons decaying via $H^{\pm} \to \tau \nu$ in $t\bar{t}$ events using pp collision data at $\sqrt{s}$ = 7 TeV with the ATLAS detector Abbott Brad Oklahoma U. Abdallah Jalal Barcelona, IFAE Abdel Khalek Samah Orsay, LAL Abdelalim Ahmed Ali Geneva U. Abdinov Ovsat Baku, Inst. Phys. Abi Babak Oklahoma State U. Abolins Maris Michigan State U. AbouZeid Ossama Toronto U. Abramowicz Halina Tel Aviv U. Abreu Henso IRFU, Saclay Acerbi Emilio INFN, Milan Milan U. Acharya Bobby Samir INFN, Udine ICTP, Trieste Adamczyk Leszek AGH-UST, Cracow Adams David Brookhaven Addy Tetteh Hampton U. Adelman Jahred Yale U. Adomeit Stefanie Munich U. Adragna Paolo Queen Mary, U. of London Adye Tim Rutherford Aefsky Scott Brandeis U. Aguilar-Saavedra Juan Antonio CAFPE, Granada LIP, Lisbon Aharrouche Mohamed Mainz U. Ahlen Steven Boston U. Ahles Florian Freiburg U. Ahmad Ashfaq SUNY, Stony Brook Ahsan Mahsana Southern Methodist U. Aielli Giulio INFN, Rome Rome U., Tor Vergata Akdogan Taylan Bogazici U. Åkesson Torsten Paul Ake Lund U. Akimoto Ginga ICTP, Trieste Akimov Andrei Lebedev Inst. Akiyama Kunihiro Kobe U. Alam Mohammad SUNY, Albany Alam Muhammad Aftab Royal Holloway, U. of London Albert Justin Victoria U. Albrand Solveig LPSC, Grenoble Aleksa Martin CERN Aleksandrov Igor Dubna, JINR Alessandria Franco INFN, Milan Alexa Calin Bucharest, IFIN-HH Alexander Gideon Tel Aviv U. Alexandre Gauthier Geneva U. Alexopoulos Theodoros Natl. Tech. U., Athens Alhroob Muhammad INFN, Udine Udine U. Aliev Malik Humboldt U., Berlin Alimonti Gianluca INFN, Milan Alison John Pennsylvania U. Allbrooke Benedict Birmingham U. Allport Phillip Liverpool U. Allwood-Spiers Sarah Glasgow U. Almond John Manchester U. Aloisio Alberto INFN, Naples Naples U. Alon Raz Weizmann Inst. Alonso Alejandro Lund U. Alvarez Gonzalez Barbara Michigan State U. Alviggi Mariagrazia INFN, Naples Naples U. Amako Katsuya KEK, Tsukuba Amelung Christoph Brandeis U. Ammosov Vladimir Serpukhov, IHEP Amorim Antonio LIP, Lisbon Lisbon U., CFNUL Amorós Gabriel Valencia U., IFIC Amram Nir Tel Aviv U. Anastopoulos Christos CERN Ancu Lucian Stefan Bern U., LHEP Andari Nansi Orsay, LAL Andeen Timothy Nevis Labs, Columbia U. Anders Christoph Falk Bonn U. Anders Gabriel Kirchhoff Inst. Phys. Anderson Kelby Chicago U., EFI Andreazza Attilio INFN, Milan Milan U. Andrei George Victor Kirchhoff Inst. Phys. Anduaga Xabier La Plata U. Angerami Aaron Nevis Labs, Columbia U. Anghinolfi Francis CERN Anisenkov Alexey Novosibirsk, IYF Anjos Nuno LIP, Lisbon Annovi Alberto Frascati Antonaki Ariadni Athens U. Antonelli Mario Frascati Antonov Alexey Moscow Phys. Eng. Inst. Antos Jaroslav Kosice, IEF Anulli Fabio INFN, Rome Aoun Sahar Marseille, CPPM Aperio Bella Ludovica Annecy, LAPP Apolle Rudi Oxford U. Rutherford Arabidze Giorgi Michigan State U. Aracena Ignacio SLAC Arai Yasuo KEK, Tsukuba Arce Ayana Duke U. Arfaoui Samir SUNY, Stony Brook Arguin Jean-Francois LBL, Berkeley Arik Engin Bogazici U. Arik Metin Bogazici U. Armbruster Aaron James Michigan U. Arnaez Olivier Mainz U. Arnal Vanessa Madrid, Autonoma U. Arnault Christian Orsay, LAL Artamonov Andrei Moscow, ITEP Artoni Giacomo INFN, Rome Rome U. Arutinov David Bonn U. Asai Shoji ICTP, Trieste Asfandiyarov Ruslan Wisconsin U., Madison Ask Stefan Cambridge U. Åsman Barbro Stockholm U. Stockholm U., OKC Asquith Lily Argonne Assamagan Ketevi Brookhaven Astbury Alan Victoria U. Aubert Bernard Annecy, LAPP Auge Etienne Orsay, LAL Augsten Kamil Prague, Tech. U. Aurousseau Mathieu Johannesburg U. Avolio Giuseppe UC, Irvine Avramidou Rachel Maria Natl. Tech. U., Athens Axen David British Columbia U. Azuelos Georges Montreal U. TRIUMF Azuma Yuya ICTP, Trieste Baak Max CERN Baccaglioni Giuseppe INFN, Milan Bacci Cesare INFN, Rome Rome III U. Bach Andre LBL, Berkeley Bachacou Henri IRFU, Saclay Bachas Konstantinos CERN Backes Moritz Geneva U. Backhaus Malte Bonn U. Badescu Elisabeta Bucharest, IFIN-HH Bagnaia Paolo INFN, Rome Rome U. Bahinipati Seema Alberta U. Bai Yu Beijing, Inst. High Energy Phys. Bailey David Toronto U. Bain Travis Toronto U. Baines John Rutherford Baker Oliver Keith Yale U. Baker Mark Brookhaven Baker Sarah University Coll. London Banas Elzbieta Cracow, INP Banerjee Piyali Montreal U. Banerjee Swagato Wisconsin U., Madison Banfi Danilo CERN Bangert Andrea Michelle Sydney U. Bansal Vikas Victoria U. Bansil Hardeep Singh Birmingham U. Barak Liron Weizmann Inst. Baranov Sergei Lebedev Inst. Barbaro Galtieri Angela LBL, Berkeley Barber Tom Freiburg U. Barberio Elisabetta Luigia Melbourne U. Barberis Dario INFN, Genoa Genoa U. Barbero Marlon Bonn U. Bardin Dmitri Dubna, JINR Barillari Teresa Munich, Max Planck Inst. Barisonzi Marcello Wuppertal U. Barklow Timothy SLAC Barlow Nick Cambridge U. Barnett Bruce Rutherford Barnett Michael LBL, Berkeley Baroncelli Antonio INFN, Rome Barone Gaetano Geneva U. Barr Alan Oxford U. Barreiro Fernando Madrid, Autonoma U. Barreiro Guimarães da Costa João Harvard U., Phys. Dept. Barrillon Pierre Orsay, LAL Bartoldus Rainer SLAC Barton Adam Edward Lancaster U. Bartsch Valeria Sussex U. Bates Richard Glasgow U. Batkova Lucia Comenius U. Batley Richard Cambridge U. Battaglia Andreas Bern U., LHEP Battistin Michele CERN Bauer Florian IRFU, Saclay Bawa Harinder Singh SLAC Fresno State Beale Steven Munich U. Beau Tristan Paris U., VI-VII Beauchemin Pierre-Hugues Tufts U. Beccherle Roberto INFN, Genoa Bechtle Philip Bonn U. Beck Hans Peter Bern U., LHEP Becker Sebastian Munich U. Beckingham Matthew Washington U., Seattle Becks Karl-Heinz Wuppertal U. Beddall Andrew Gaziantep U. Beddall Ayda Gaziantep U. Bedikian Sourpouhi Yale U. Bednyakov Vadim Dubna, JINR Bee Christopher Marseille, CPPM Begel Michael Brookhaven Behar Harpaz Silvia Technion Behera Prafulla Iowa U. Beimforde Michael Munich, Max Planck Inst. Belanger-Champagne Camille McGill U. Bell Paul Geneva U. Bell William Geneva U. Bella Gideon Tel Aviv U. Bellagamba Lorenzo INFN, Bologna Bellina Francesco CERN Bellomo Massimiliano CERN Belloni Alberto Harvard U., Phys. Dept. Beloborodova Olga Novosibirsk, IYF Novosibirsk State U. Belotskiy Konstantin Moscow Phys. Eng. Inst. Beltramello Olga CERN Benary Odette Tel Aviv U. Benchekroun Driss Casablanca U. Bendtz Katarina Stockholm U. Stockholm U., OKC Benekos Nektarios Illinois U., Urbana Benhammou Yan Tel Aviv U. Benhar Noccioli Eleonora Geneva U. Benitez Garcia Jorge-Armando York U., Canada Benjamin Douglas Duke U. Benoit Mathieu Orsay, LAL Bensinger James Brandeis U. Benslama Kamal Regina U. Bentvelsen Stan FOM, Amsterdam Berge David CERN Bergeaas Kuutmann Elin DESY Berger Nicolas Annecy, LAPP Berghaus Frank Victoria U. Berglund Elina FOM, Amsterdam Beringer Jürg LBL, Berkeley Bernat Pauline University Coll. London Bernhard Ralf Freiburg U. Bernius Catrin Brookhaven Berry Tracey Royal Holloway, U. of London Bertella Claudia Marseille, CPPM Bertin Antonio INFN, Bologna Bologna U. Bertolucci Federico INFN, Pisa Pisa U. Besana Maria Ilaria INFN, Milan Milan U. Besson Nathalie IRFU, Saclay Bethke Siegfried Munich, Max Planck Inst. Bhimji Wahid Edinburgh U. Bianchi Riccardo-Maria CERN Bianco Michele INFN, Lecce Salento U. Biebel Otmar Munich U. Bieniek Stephen Paul University Coll. London Bierwagen Katharina Gottingen U., II. Phys. Inst. Biesiada Jed LBL, Berkeley Biglietti Michela INFN, Rome Bilokon Halina Frascati Bindi Marcello INFN, Bologna Bologna U. Binet Sebastien Orsay, LAL Bingul Ahmet Gaziantep U. Bini Cesare INFN, Rome Rome U. Biscarat Catherine CC, Villeurbanne Bitenc Urban Freiburg U. Black Kevin Boston U. Blair Robert Argonne Blanchard Jean-Baptiste IRFU, Saclay Blanchot Georges CERN Blazek Tomas Comenius U. Blocker Craig Brandeis U. Blocki Jacek Cracow, INP Blondel Alain Geneva U. Blum Walter Mainz U. Blumenschein Ulrike Gottingen U., II. Phys. Inst. Bobbink Gerjan FOM, Amsterdam Bobrovnikov Victor Novosibirsk, IYF Bocchetta Simona Serena Lund U. Bocci Andrea Duke U. Boddy Christopher Richard Oxford U. Boehler Michael DESY Boek Jennifer Wuppertal U. Boelaert Nele Bohr Inst. Bogaerts Joannes Andreas CERN Bogdanchikov Alexander Novosibirsk, IYF Bogouch Andrei Minsk, Inst. Phys. Bohm Christian Stockholm U. Bohm Jan Prague, Inst. Phys. Boisvert Veronique Royal Holloway, U. of London Bold Tomasz AGH-UST, Cracow Boldea Venera Bucharest, IFIN-HH Bolnet Nayanka Myriam IRFU, Saclay Bomben Marco Paris U., VI-VII Bona Marcella Queen Mary, U. of London Bondioli Mario UC, Irvine Boonekamp Maarten IRFU, Saclay Booth Chris Sheffield U. Bordoni Stefania Paris U., VI-VII Borer Claudia Bern U., LHEP Borisov Anatoly Serpukhov, IHEP Borissov Guennadi Lancaster U. Borjanovic Iris Belgrade U. Borri Marcello Manchester U. Borroni Sara Michigan U. Bortolotto Valerio INFN, Rome Rome III U. Bos Kors FOM, Amsterdam Boscherini Davide INFN, Bologna Bosman Martine Barcelona, IFAE Boterenbrood Hendrik FOM, Amsterdam Botterill David Rutherford Bouchami Jihene Montreal U. Boudreau Joseph Pittsburgh U. Bouhova-Thacker Evelina Vassileva Lancaster U. Boumediene Djamel Eddine Clermont-Ferrand U. Bourdarios Claire Orsay, LAL Bousson Nicolas Marseille, CPPM Boveia Antonio Chicago U., EFI Boyd James CERN Boyko Igor Dubna, JINR Bozhko Nikolay Serpukhov, IHEP Bozovic-Jelisavcic Ivanka VINCA Inst. Nucl. Sci., Belgrade Bracinik Juraj Birmingham U. Branchini Paolo INFN, Rome Brandt Andrew Texas U., Arlington Brandt Gerhard Oxford U. Brandt Oleg Gottingen U., II. Phys. Inst. Bratzler Uwe Tokyo Metropolitan U. Brau Benjamin Massachusetts U., Amherst Brau James Oregon U. Braun Helmut Wuppertal U. Brelier Bertrand Toronto U. Bremer Johan CERN Brendlinger Kurt Pennsylvania U. Brenner Richard Uppsala U., Inst. Theor. Phys. Bressler Shikma Weizmann Inst. Britton Dave Glasgow U. Brochu Frederic Cambridge U. Brock Ian Bonn U. Brock Raymond Michigan State U. Brodet Eyal Tel Aviv U. Broggi Francesco INFN, Milan Bromberg Carl Michigan State U. Bronner Johanna Munich, Max Planck Inst. Brooijmans Gustaaf Nevis Labs, Columbia U. Brooks William Santa Maria U., Valparaiso Brown Gareth Manchester U. Brown Heather Texas U., Arlington Bruckman de Renstrom Pawel Cracow, INP Bruncko Dusan Kosice, IEF Bruneliere Renaud Freiburg U. Brunet Sylvie Indiana U. Bruni Alessia INFN, Bologna Bruni Graziano INFN, Bologna Bruschi Marco INFN, Bologna Buanes Trygve Bergen U. Buat Quentin LPSC, Grenoble Bucci Francesca Geneva U. Buchanan James Oxford U. Buchholz Peter Siegen U. Buckingham Ryan Oxford U. Buckley Andrew Edinburgh U. Buda Stelian Ioan Bucharest, IFIN-HH Budagov Ioulian Dubna, JINR Budick Burton New York U. Büscher Volker Mainz U. Bugge Lars Oslo U. Bulekov Oleg Moscow Phys. Eng. Inst. Bundock Aaron Colin Liverpool U. Bunse Moritz Dortmund U. Buran Torleiv Oslo U. Burckhart Helfried CERN Burdin Sergey Liverpool U. Burgess Thomas Bergen U. Burke Stephen Rutherford Busato Emmanuel Clermont-Ferrand U. Bussey Peter Glasgow U. Buszello Claus-Peter Uppsala U., Inst. Theor. Phys. Butler Bart SLAC Butler John Boston U. Buttar Craig Glasgow U. Butterworth Jonathan University Coll. London Buttinger William Cambridge U. Cabrera Urbán Susana Valencia U., IFIC Caforio Davide INFN, Bologna Bologna U. Cakir Orhan Ankara U. Calafiura Paolo LBL, Berkeley Calderini Giovanni Paris U., VI-VII Calfayan Philippe Munich U. Calkins Robert Northern Illinois U. Caloba Luiz Rio de Janeiro Federal U. Caloi Rita INFN, Rome Rome U. Calvet David Clermont-Ferrand U. Calvet Samuel Clermont-Ferrand U. Camacho Toro Reina Clermont-Ferrand U. Camarri Paolo INFN, Rome Rome U., Tor Vergata Cameron David Oslo U. Caminada Lea Michaela LBL, Berkeley Campana Simone CERN Campanelli Mario University Coll. London Canale Vincenzo INFN, Naples Naples U. Canelli Florencia Chicago U., EFI Fermilab Canepa Anadi TRIUMF Cantero Josu Madrid, Autonoma U. Capasso Luciano INFN, Naples Naples U. Capeans Garrido Maria Del Mar CERN Caprini Irinel Bucharest, IFIN-HH Caprini Mihai Bucharest, IFIN-HH Capriotti Daniele Munich, Max Planck Inst. Capua Marcella INFN, Cosenza Calabria U. Caputo Regina Mainz U. Cardarelli Roberto INFN, Rome Carli Tancredi CERN Carlino Gianpaolo INFN, Naples Carminati Leonardo INFN, Milan Milan U. Caron Bryan McGill U. Caron Sascha NIKHEF, Amsterdam Carquin Edson Santa Maria U., Valparaiso Carrillo Montoya German D Wisconsin U., Madison Carter Antony Queen Mary, U. of London Carter Janet Cambridge U. Carvalho João LIP, Lisbon Coimbra U. Casadei Diego New York U. Casado Maria Pilar Barcelona, IFAE Cascella Michele INFN, Pisa Pisa U. Caso Carlo INFN, Genoa Genoa U. Castaneda Hernandez Alfredo Martin Wisconsin U., Madison Castaneda-Miranda Elizabeth Wisconsin U., Madison Castillo Gimenez Victoria Valencia U., IFIC Castro Nuno Filipe LIP, Lisbon Cataldi Gabriella INFN, Lecce Catastini Pierluigi Harvard U., Phys. Dept. Catinaccio Andrea CERN Catmore James CERN Cattai Ariella CERN Cattani Giordano INFN, Rome Rome U., Tor Vergata Caughron Seth Michigan State U. Cauz Diego INFN, Udine Udine U. Cavalleri Pietro Paris U., VI-VII Cavalli Donatella INFN, Milan Cavalli-Sforza Matteo Barcelona, IFAE Cavasinni Vincenzo INFN, Pisa Pisa U. Ceradini Filippo INFN, Rome Rome III U. Santiago Cerqueira Augusto Juiz de Fora U. Cerri Alessandro CERN Cerrito Lucio Queen Mary, U. of London Cerutti Fabio Frascati Cetin Serkant Ali Dogus U., Kadikoy Chafaq Aziz Casablanca U. Chakraborty Dhiman Northern Illinois U. Chalupkova Ina Charles U. Chan Kevin Alberta U. Chapleau Bertrand McGill U. Chapman John Derek Cambridge U. Chapman John Wehrley Michigan U. Chareyre Eve Paris U., VI-VII Charlton Dave Birmingham U. Chavda Vikash Manchester U. Chavez Barajas Carlos Alberto CERN Cheatham Susan McGill U. Chekanov Sergei Argonne Chekulaev Sergey TRIUMF Chelkov Gueorgui Dubna, JINR Chelstowska Magda Anna NIKHEF, Amsterdam Chen Chunhui Iowa State U. Chen Hucheng Brookhaven Chen Shenjian Nanjing U. Chen Xin Wisconsin U., Madison Cheplakov Alexander Dubna, JINR Cherkaoui El Moursli Rajaa Mohammed V U., Agdal Chernyatin Valeriy Brookhaven Cheu Elliott Arizona U. Cheung Sing-Leung Toronto U. Chevalier Laurent IRFU, Saclay Chiefari Giovanni INFN, Naples Naples U. Chikovani Leila Tbilisi, Inst. Phys. Childers John Taylor CERN Chilingarov Alexandre Lancaster U. Chiodini Gabriele INFN, Lecce Chisholm Andrew Birmingham U. Chislett Rebecca Thalatta University Coll. London Chizhov Mihail Dubna, JINR Choudalakis Georgios Chicago U., EFI Chouridou Sofia UC, Santa Cruz Christidi Illectra-Athanasia University Coll. London Christov Asen Freiburg U. Chromek-Burckhart Doris CERN Chu Ming-Lee Taiwan, Inst. Phys. Chudoba Jiri Prague, Inst. Phys. Ciapetti Guido INFN, Rome Rome U. Ciftci Abbas Kenan Ankara U. Ciftci Rena Ankara U. Cinca Diane Clermont-Ferrand U. Cindro Vladimir Stefan Inst., Ljubljana Ciocca Claudia INFN, Bologna Ciocio Alessandra LBL, Berkeley Cirilli Manuela Michigan U. Citterio Mauro INFN, Milan Ciubancan Mihai Bucharest, IFIN-HH Clark Allan G Geneva U. Clark Philip James Edinburgh U. Cleland Bill Pittsburgh U. Clemens Jean-Claude Marseille, CPPM Clement Benoit LPSC, Grenoble Clement Christophe Stockholm U. Stockholm U., OKC Coadou Yann Marseille, CPPM Cobal Marina INFN, Udine Udine U. Coccaro Andrea Washington U., Seattle Cochran James H Iowa State U. Coe Paul Oxford U. Cogan Joshua Godfrey SLAC Coggeshall James Illinois U., Urbana Cogneras Eric CC, Villeurbanne Colas Jacques Annecy, LAPP Colijn Auke-Pieter FOM, Amsterdam Collins Neil Birmingham U. Collins-Tooth Christopher Glasgow U. Collot Johann LPSC, Grenoble Colon German Massachusetts U., Amherst Conde Muiño Patricia LIP, Lisbon Coniavitis Elias Oxford U. Conidi Maria Chiara Barcelona, IFAE Consonni Sofia Maria INFN, Milan Milan U. Consorti Valerio Freiburg U. Constantinescu Serban Bucharest, IFIN-HH Conta Claudio INFN, Pavia Pavia U. Conti Geraldine Harvard U., Phys. Dept. Conventi Francesco INFN, Naples Naples, Inst. U. Navale Cooke Mark LBL, Berkeley Cooper Ben University Coll. London Cooper-Sarkar Amanda Oxford U. Copic Katherine LBL, Berkeley Cornelissen Thijs Wuppertal U. Corradi Massimo INFN, Bologna Corriveau Francois McGill U. IPP, Canada Cortes-Gonzalez Arely Illinois U., Urbana Cortiana Giorgio Munich, Max Planck Inst. Costa Giuseppe INFN, Milan Costa María José Valencia U., IFIC Costanzo Davide Sheffield U. Costin Tudor Chicago U., EFI Côté David CERN Courneyea Lorraine Victoria U. Cowan Glen Royal Holloway, U. of London Cowden Christopher Cambridge U. Cox Brian Manchester U. Cranmer Kyle New York U. Crescioli Francesco INFN, Pisa Pisa U. Cristinziani Markus Bonn U. Crosetti Giovanni INFN, Cosenza Calabria U. Crupi Roberto INFN, Lecce Salento U. Crépé-Renaudin Sabine LPSC, Grenoble Cuciuc Constantin-Mihai Bucharest, IFIN-HH Cuenca Almenar Cristóbal Yale U. Cuhadar Donszelmann Tulay Sheffield U. Curatolo Maria Frascati Curtis Chris Birmingham U. Cuthbert Cameron Sydney U. Cwetanski Peter Indiana U. Czirr Hendrik Siegen U. Czodrowski Patrick Dresden, Tech. U. Czyczula Zofia Yale U. D'Auria Saverio Glasgow U. D'Onofrio Monica Liverpool U. D'Orazio Alessia INFN, Rome Rome U. Da Via Cinzia Manchester U. Dabrowski Wladyslaw AGH-UST, Cracow Dafinca Alexandru Oxford U. Dai Tiesheng Michigan U. Dallapiccola Carlo Massachusetts U., Amherst Dam Mogens Bohr Inst. Dameri Mauro INFN, Genoa Genoa U. Damiani Daniel UC, Santa Cruz Danielsson Hans Olof CERN Dao Valerio Geneva U. Darbo Giovanni INFN, Genoa Darlea Georgiana Lavinia Bucharest, Polytechnic Inst. Davey Will Bonn U. Davidek Tomas Charles U. Davidson Nadia Melbourne U. Davidson Ruth Lancaster U. Davies Eleanor Oxford U. Rutherford Davies Merlin Montreal U. Davison Adam University Coll. London Davygora Yuriy Kirchhoff Inst. Phys. Dawe Edmund Simon Fraser U. Dawson Ian Sheffield U. Daya-Ishmukhametova Rozmin Brandeis U. De Kaushik Texas U., Arlington de Asmundis Riccardo INFN, Naples De Castro Stefano INFN, Bologna Bologna U. De Cecco Sandro Paris U., VI-VII de Graat Julien Munich U. De Groot Nicolo NIKHEF, Amsterdam de Jong Paul FOM, Amsterdam De La Taille Christophe Orsay, LAL De la Torre Hector Madrid, Autonoma U. De Lorenzi Francesco Iowa State U. De Lotto Barbara INFN, Udine Udine U. de Mora Lee Lancaster U. De Nooij Lucie FOM, Amsterdam De Pedis Daniele INFN, Rome De Salvo Alessandro INFN, Rome De Sanctis Umberto INFN, Udine Udine U. De Santo Antonella Sussex U. De Vivie De Regie Jean-Baptiste Orsay, LAL De Zorzi Guido INFN, Rome Rome U. Dearnaley William James Lancaster U. Debbe Ramiro Brookhaven Debenedetti Chiara Edinburgh U. Dechenaux Benjamin LPSC, Grenoble Dedovich Dmitri Dubna, JINR Degenhardt James Pennsylvania U. Del Papa Carlo INFN, Udine Udine U. Del Peso Jose Madrid, Autonoma U. Del Prete Tarcisio INFN, Pisa Pisa U. Delemontex Thomas LPSC, Grenoble Deliyergiyev Maksym Stefan Inst., Ljubljana Dell'Acqua Andrea CERN Dell'Asta Lidia Boston U. Della Pietra Massimo INFN, Naples Naples, Inst. U. Navale della Volpe Domenico INFN, Naples Naples U. Delmastro Marco Annecy, LAPP Delsart Pierre-Antoine LPSC, Grenoble Deluca Carolina SUNY, Stony Brook Demers Sarah Yale U. Demichev Mikhail Dubna, JINR Demirkoz Bilge Barcelona, IFAE Middle East Tech. U., Ankara Deng Jianrong UC, Irvine Denisov Sergey Serpukhov, IHEP Derendarz Dominik Cracow, INP Derkaoui Jamal Eddine Oujda U. Derue Frederic Paris U., VI-VII Dervan Paul Liverpool U. Desch Klaus Kurt Bonn U. Devetak Erik SUNY, Stony Brook Deviveiros Pier-Olivier FOM, Amsterdam Dewhurst Alastair Rutherford DeWilde Burton SUNY, Stony Brook Dhaliwal Saminder Toronto U. Dhullipudi Ramasudhakar Brookhaven Louisiana Tech. U. Di Ciaccio Anna INFN, Rome Rome U., Tor Vergata Di Ciaccio Lucia Annecy, LAPP Di Girolamo Alessandro CERN Di Girolamo Beniamino CERN Di Luise Silvestro INFN, Rome Rome III U. Di Mattia Alessandro Wisconsin U., Madison Di Micco Biagio CERN Di Nardo Roberto Frascati Di Simone Andrea INFN, Rome Rome U., Tor Vergata Di Sipio Riccardo INFN, Bologna Bologna U. Diaz Marco Aurelio Valparaiso U., Catolica Diblen Faruk Gaziantep U. Diehl Edward Michigan U. Dietrich Janet DESY Dietzsch Thorsten Kirchhoff Inst. Phys. Diglio Sara Melbourne U. Dindar Yagci Kamile Southern Methodist U. Dingfelder Jochen Bonn U. Dionisi Carlo INFN, Rome Rome U. Dita Petre Bucharest, IFIN-HH Dita Sanda Bucharest, IFIN-HH Dittus Fridolin CERN Djama Fares Marseille, CPPM Djobava Tamar Tbilisi State U. Barros do Vale Maria Aline Sao Joao del-Rei Fed. U. Do Valle Wemans André LIP, Lisbon Doan Thi Kieu Oanh Annecy, LAPP Dobbs Matt McGill U. Dobinson Robert CERN Dobos Daniel CERN Dobson Ellie CERN University Coll. London Dodd Jeremy Nevis Labs, Columbia U. Doglioni Caterina Geneva U. Doherty Tom Glasgow U. Doi Yoshikuni KEK, Tsukuba Dolejsi Jiri Charles U. Dolenc Irena Stefan Inst., Ljubljana Dolezal Zdenek Charles U. Dolgoshein Boris Moscow Phys. Eng. Inst. Dohmae Takeshi ICTP, Trieste Donadelli Marisilvia Sao Paulo U. Donega Mauro Pennsylvania U. Donini Julien Clermont-Ferrand U. Dopke Jens CERN Doria Alessandra INFN, Naples Dos Anjos Andre Wisconsin U., Madison Dotti Andrea INFN, Pisa Pisa U. Dova Maria-Teresa La Plata U. Doxiadis Alexander FOM, Amsterdam Doyle Tony Glasgow U. Dris Manolis Natl. Tech. U., Athens Dubbert Jörg Munich, Max Planck Inst. Dube Sourabh LBL, Berkeley Duchovni Ehud Weizmann Inst. Duckeck Guenter Munich U. Dudarev Alexey CERN Dudziak Fanny Iowa State U. Dührssen Michael CERN Duerdoth Ian Manchester U. Duflot Laurent Orsay, LAL Dufour Marc-Andre McGill U. Dunford Monica CERN Duran Yildiz Hatice Ankara U. Duxfield Robert Sheffield U. Dwuznik Michal AGH-UST, Cracow Dydak Friedrich CERN Düren Michael Giessen U. Ebke Johannes Munich U. Eckweiler Sebastian Mainz U. Edmonds Keith Mainz U. Edwards Clive Royal Holloway, U. of London Edwards Nicholas Charles Glasgow U. Ehrenfeld Wolfgang DESY Eifert Till SLAC Eigen Gerald Bergen U. Einsweiler Kevin LBL, Berkeley Eisenhandler Eric Queen Mary, U. of London Ekelof Tord Uppsala U., Inst. Theor. Phys. El Kacimi Mohamed Cadi Ayyad U., Marrakech Ellert Mattias Uppsala U., Inst. Theor. Phys. Elles Sabine Annecy, LAPP Ellinghaus Frank Mainz U. Ellis Katherine Queen Mary, U. of London Ellis Nicolas CERN Elmsheuser Johannes Munich U. Elsing Markus CERN Emeliyanov Dmitry Rutherford Engelmann Roderich SUNY, Stony Brook Engl Albert Munich U. Epp Brigitte Innsbruck U. Eppig Andrew Michigan U. Erdmann Johannes Gottingen U., II. Phys. Inst. Ereditato Antonio Bern U., LHEP Eriksson Daniel Stockholm U. Ernst Jesse SUNY, Albany Ernst Michael Brookhaven Ernwein Jean IRFU, Saclay Errede Deborah Illinois U., Urbana Errede Steven Illinois U., Urbana Ertel Eugen Mainz U. Escalier Marc Orsay, LAL Escobar Carlos Pittsburgh U. Espinal Curull Xavier Barcelona, IFAE Esposito Bellisario Frascati Etienne Francois Marseille, CPPM Etienvre Anne-Isabelle IRFU, Saclay Etzion Erez Tel Aviv U. Evangelakou Despoina Gottingen U., II. Phys. Inst. Evans Hal Indiana U. Fabbri Laura INFN, Bologna Bologna U. Fabre Caroline CERN Fakhrutdinov Rinat Serpukhov, IHEP Falciano Speranza INFN, Rome Fang Yaquan Wisconsin U., Madison Fanti Marcello INFN, Milan Milan U. Farbin Amir Texas U., Arlington Farilla Addolorata INFN, Rome Farley Jason SUNY, Stony Brook Farooque Trisha Toronto U. Farrell Steven UC, Irvine Farrington Sinead Oxford U. Farthouat Philippe CERN Fassnacht Patrick CERN Fassouliotis Dimitrios Athens U. Fatholahzadeh Baharak Toronto U. Favareto Andrea INFN, Milan Milan U. Fayard Louis Orsay, LAL Fazio Salvatore INFN, Cosenza Calabria U. Febbraro Renato Clermont-Ferrand U. Federic Pavol Comenius U. Fedin Oleg St. Petersburg, INP Fedorko Woiciech Michigan State U. Fehling-Kaschek Mirjam Freiburg U. Feligioni Lorenzo Marseille, CPPM Fellmann Denis Argonne Feng Cunfeng Shandong U. Feng Eric Chicago U., EFI Fenyuk Alexander Serpukhov, IHEP Ferencei Jozef Kosice, IEF Fernando Waruna Argonne Ferrag Samir Glasgow U. Ferrando James Glasgow U. Ferrara Valentina DESY Ferrari Arnaud Uppsala U., Inst. Theor. Phys. Ferrari Pamela FOM, Amsterdam Ferrari Roberto INFN, Pavia Ferreira de Lima Danilo Enoque Glasgow U. Ferrer Antonio Valencia U., IFIC Ferrere Didier Geneva U. Ferretti Claudio Michigan U. Ferretto Parodi Andrea INFN, Genoa Genoa U. Fiascaris Maria Chicago U., EFI Fiedler Frank Mainz U. Filipčič Andrej Stefan Inst., Ljubljana Filthaut Frank NIKHEF, Amsterdam Fincke-Keeler Margret Victoria U. Fiolhais Miguel LIP, Lisbon Coimbra U. Fiorini Luca Valencia U., IFIC Firan Ana Southern Methodist U. Fischer Gordon DESY Fisher Matthew Ohio State U. Flechl Martin Freiburg U. Fleck Ivor Siegen U. Fleckner Johanna Mainz U. Fleischmann Philipp Wurzburg U. Fleischmann Sebastian Wuppertal U. Flick Tobias Wuppertal U. Floderus Anders Lund U. Flores Castillo Luis Wisconsin U., Madison Flowerdew Michael Munich, Max Planck Inst. Fonseca Martin Teresa Bern U., LHEP Forbush David Alan Washington U., Seattle Formica Andrea IRFU, Saclay Forti Alessandra Manchester U. Fortin Dominique TRIUMF Fournier Daniel Orsay, LAL Fox Harald Lancaster U. Francavilla Paolo Barcelona, IFAE Franchino Silvia INFN, Pavia Pavia U. Francis David CERN Frank Tal Weizmann Inst. Franklin Melissa Harvard U., Phys. Dept. Franz Sebastien CERN Fraternali Marco INFN, Pavia Pavia U. Fratina Sasa Pennsylvania U. French Sky Cambridge U. Friedrich Conrad DESY Friedrich Felix Dresden, Tech. U. Froeschl Robert CERN Froidevaux Daniel CERN Frost James Cambridge U. Fukunaga Chikara Tokyo Metropolitan U. Fullana Torregrosa Esteban CERN Fulsom Bryan Gregory SLAC Fuster Juan Valencia U., IFIC Gabaldon Carolina CERN Gabizon Ofir Weizmann Inst. Gadfort Thomas Brookhaven Gadomski Szymon Geneva U. Gagliardi Guido INFN, Genoa Genoa U. Gagnon Pauline Indiana U. Galea Cristina Munich U. Gallas Elizabeth Oxford U. Gallo Valentina Santina Bern U., LHEP Gallop Bruce Rutherford Gallus Petr Prague, Inst. Phys. Gan KK Ohio State U. Gao Yongsheng SLAC Fresno State Gaponenko Andrei LBL, Berkeley Garberson Ford Yale U. Garcia-Sciveres Maurice LBL, Berkeley García Carmen Valencia U., IFIC García Navarro José Enrique Valencia U., IFIC Gardner Robert Chicago U., EFI Garelli Nicoletta CERN Garitaonandia Hegoi FOM, Amsterdam Garonne Vincent CERN Garvey John Birmingham U. Gatti Claudio Frascati Gaudio Gabriella INFN, Pavia Gaur Bakul Siegen U. Gauthier Lea IRFU, Saclay Gauzzi Paolo INFN, Rome Rome U. Gavrilenko Igor Lebedev Inst. Gay Colin British Columbia U. Gaycken Goetz Bonn U. Gazis Evangelos Natl. Tech. U., Athens Ge Peng Shandong U. Gecse Zoltan British Columbia U. Gee Norman Rutherford Geerts Daniël Alphonsus Adrianus FOM, Amsterdam Geich-Gimbel Christoph Bonn U. Gellerstedt Karl Stockholm U. Stockholm U., OKC Gemme Claudia INFN, Genoa Gemmell Alistair Glasgow U. Genest Marie-Hélène LPSC, Grenoble Gentile Simonetta INFN, Rome Rome U. George Matthias Gottingen U., II. Phys. Inst. George Simon Royal Holloway, U. of London Gerlach Peter Wuppertal U. Gershon Avi Tel Aviv U. Geweniger Christoph Kirchhoff Inst. Phys. Ghazlane Hamid CNESTEN, Rabat Ghodbane Nabil Clermont-Ferrand U. Giacobbe Benedetto INFN, Bologna Giagu Stefano INFN, Rome Rome U. Giakoumopoulou Victoria Athens U. Giangiobbe Vincent Barcelona, IFAE Gianotti Fabiola CERN Gibbard Bruce Brookhaven Gibson Adam Toronto U. Gibson Stephen CERN Gillberg Dag Carleton U. Gillman Tony Rutherford Gingrich Douglas Alberta U. TRIUMF Ginzburg Jonatan Tel Aviv U. Giokaris Nikos Athens U. Giordani MarioPaolo Udine U. Giordano Raffaele INFN, Naples Naples U. Giorgi Francesco Michelangelo Humboldt U., Berlin Giovannini Paola Munich, Max Planck Inst. Giraud Pierre-Francois IRFU, Saclay Giugni Danilo INFN, Milan Giunta Michele Montreal U. Giusti Paolo INFN, Bologna Gjelsten Børge Kile Oslo U. Gladilin Leonid Moscow State U. Glasman Claudia Madrid, Autonoma U. Glatzer Julian Freiburg U. Glazov Alexandre DESY Glitza Karl-Walter Wuppertal U. Glonti George Dubna, JINR Goddard Jack Robert Queen Mary, U. of London Godfrey Jennifer Simon Fraser U. Godlewski Jan CERN Goebel Martin DESY Göpfert Thomas Dresden, Tech. U. Goeringer Christian Mainz U. Gössling Claus Dortmund U. Göttfert Tobias Munich, Max Planck Inst. Goldfarb Steven Michigan U. Golling Tobias Yale U. Gomes Agostinho LIP, Lisbon Lisbon U., CFNUL Gomez Fajardo Luz Stella DESY Gonçalo Ricardo Royal Holloway, U. of London Goncalves Pinto Firmino Da Costa Joao DESY Gonella Laura Bonn U. Gonzalez Saul Wisconsin U., Madison González de la Hoz Santiago Valencia U., IFIC Gonzalez Parra Garoe Barcelona, IFAE Gonzalez Silva Laura Buenos Aires U. Gonzalez-Sevilla Sergio Geneva U. Goodson Jeremiah Jet SUNY, Stony Brook Goossens Luc CERN Gorbounov Petr Andreevich Moscow, ITEP Gordon Howard Brookhaven Gorelov Igor New Mexico U. Gorfine Grant Wuppertal U. Gorini Benedetto CERN Gorini Edoardo INFN, Lecce Salento U. Gorišek Andrej Stefan Inst., Ljubljana Gornicki Edward Cracow, INP Gosdzik Bjoern DESY Goshaw Alfred Argonne Gosselink Martijn FOM, Amsterdam Gostkin Mikhail Ivanovitch Dubna, JINR Gough Eschrich Ivo UC, Irvine Gouighri Mohamed Casablanca U. Goujdami Driss Cadi Ayyad U., Marrakech Goulette Marc Phillippe Geneva U. Goussiou Anna Washington U., Seattle Goy Corinne Annecy, LAPP Gozpinar Serdar Brandeis U. Grabowska-Bold Iwona AGH-UST, Cracow Grafström Per CERN Grahn Karl-Johan DESY Grancagnolo Francesco INFN, Lecce Grancagnolo Sergio Humboldt U., Berlin Grassi Valerio SUNY, Stony Brook Gratchev Vadim St. Petersburg, INP Grau Nathan Nevis Labs, Columbia U. Gray Heather CERN Gray Julia Ann SUNY, Stony Brook Graziani Enrico INFN, Rome Grebenyuk Oleg St. Petersburg, INP Greenshaw Timothy Liverpool U. Greenwood Zeno Dixon Brookhaven Louisiana Tech. U. Gregersen Kristian Bohr Inst. Gregor Ingrid-Maria DESY Grenier Philippe SLAC Griffiths Justin Washington U., Seattle Grigalashvili Nugzar Dubna, JINR Grillo Alexander UC, Santa Cruz Grinstein Sebastian Barcelona, IFAE Grishkevich Yaroslav Moscow State U. Grivaz Jean-Francois Orsay, LAL Gross Eilam Weizmann Inst. Grosse-Knetter Joern Gottingen U., II. Phys. Inst. Groth-Jensen Jacob Weizmann Inst. Grybel Kai Siegen U. Guest Daniel Yale U. Guicheney Christophe Clermont-Ferrand U. Guida Angelo INFN, Lecce Salento U. Guindon Stefan Gottingen U., II. Phys. Inst. Guler Hulya McGill U. Montreal U. Gunther Jaroslav Prague, Inst. Phys. Guo Bin Toronto U. Guo Jun Nevis Labs, Columbia U. Gushchin Vladimir Serpukhov, IHEP Gutierrez Phillip Oklahoma U. Guttman Nir Tel Aviv U. Gutzwiller Olivier Wisconsin U., Madison Guyot Claude IRFU, Saclay Gwenlan Claire Oxford U. Gwilliam Carl Liverpool U. Haas Andy SLAC Haas Stefan CERN Haber Carl LBL, Berkeley Hadavand Haleh Khani Southern Methodist U. Hadley David Birmingham U. Haefner Petra Munich, Max Planck Inst. Hahn Ferdinand CERN Haider Stefan CERN Hajduk Zbigniew Cracow, INP Hakobyan Hrachya Yerevan Phys. Inst. Hall David Oxford U. Haller Johannes Gottingen U., II. Phys. Inst. Hamacher Klaus Wuppertal U. Hamal Petr Palacky U. Hamer Matthias Gottingen U., II. Phys. Inst. Hamilton Andrew Witwatersrand U. Cape Town U. Hamilton Samuel Tufts U. Han Liang Hefei, CUST Hanagaki Kazunori Osaka U. Hanawa Keita Tsukuba U. Hance Michael LBL, Berkeley Handel Carsten Mainz U. Hanke Paul Kirchhoff Inst. Phys. Hansen John Renner Bohr Inst. Hansen Jørgen Beck Bohr Inst. Hansen Jorn Dines Bohr Inst. Hansen Peter Henrik Bohr Inst. Hansson Per SLAC Hara Kazuhiko Tsukuba U. Hare Gabriel UC, Santa Cruz Harenberg Torsten Wuppertal U. Harkusha Siarhei Minsk, Inst. Phys. Harper Devin Michigan U. Harrington Robert Edinburgh U. Harris Orin Washington U., Seattle Harrison Karl Birmingham U. Hartert Jochen Freiburg U. Hartjes Fred FOM, Amsterdam Haruyama Tomiyoshi KEK, Tsukuba Harvey Alex Hampton U. Hasegawa Satoshi Nagoya U. Hasegawa Yoji Shinshu U. Hassani Samira IRFU, Saclay Haug Sigve Bern U., LHEP Hauschild Michael CERN Hauser Reiner Michigan State U. Havranek Miroslav Bonn U. Hawkes Christopher Birmingham U. Hawkings Richard John CERN Hawkins Anthony David Lund U. Hawkins Donovan UC, Irvine Hayakawa Takashi Kobe U. Hayashi Takayasu Tsukuba U. Hayden Daniel Royal Holloway, U. of London Hayward Helen Liverpool U. Haywood Stephen Rutherford He Mao Shandong U. Head Simon Birmingham U. Hedberg Vincent Lund U. Heelan Louise Texas U., Arlington Heim Sarah Michigan State U. Heinemann Beate LBL, Berkeley Heisterkamp Simon Bohr Inst. Helary Louis Annecy, LAPP Heller Claudio Munich U. Heller Matthieu CERN Hellman Sten Stockholm U. Stockholm U., OKC Hellmich Dennis Bonn U. Helsens Clement Barcelona, IFAE Henderson Robert Lancaster U. Henke Michael Kirchhoff Inst. Phys. Henrichs Anna Gottingen U., II. Phys. Inst. Henriques Correia Ana Maria CERN Henrot-Versille Sophie Orsay, LAL Henry-Couannier Frédéric Marseille, CPPM Hensel Carsten Gottingen U., II. Phys. Inst. Henß Tobias Wuppertal U. Medina Hernandez Carlos Texas U., Arlington Hernández Jiménez Yesenia Valencia U., IFIC Herrberg Ruth Humboldt U., Berlin Herten Gregor Freiburg U. Hertenberger Ralf Munich U. Hervas Luis CERN Hesketh Gavin Grant University Coll. London Hessey Nigel FOM, Amsterdam Higón-Rodriguez Emilio Valencia U., IFIC Hill John Cambridge U. Hiller Karl Heinz DESY Hillert Sonja Bonn U. Hillier Stephen Birmingham U. Hinchliffe Ian LBL, Berkeley Hines Elizabeth Pennsylvania U. Hirose Minoru Osaka U. Hirsch Florian Dortmund U. Hirschbuehl Dominic Wuppertal U. Hobbs John SUNY, Stony Brook Hod Noam Tel Aviv U. Hodgkinson Mark Sheffield U. Hodgson Paul Sheffield U. Hoecker Andreas CERN Hoeferkamp Martin New Mexico U. Hoffman Julia Southern Methodist U. Hoffmann Dirk Marseille, CPPM Hohlfeld Marc Mainz U. Holder Martin Siegen U. Holmgren Sven-Olof Stockholm U. Holy Tomas Prague, Tech. U. Holzbauer Jenny Michigan State U. Hong Tae Min Pennsylvania U. Hooft van Huysduynen Loek New York U. Horn Claus SLAC Horner Stephan Freiburg U. Hostachy Jean-Yves LPSC, Grenoble Hou Suen Taiwan, Inst. Phys. Hoummada Abdeslam Casablanca U. Howarth James Manchester U. Hristova Ivana Humboldt U., Berlin Hrivnac Julius Orsay, LAL Hruska Ivan Prague, Inst. Phys. Hryn'ova Tetiana Annecy, LAPP Hsu Pai-hsien Jennifer Mainz U. Hsu Shih-Chieh LBL, Berkeley Hubacek Zdenek Prague, Tech. U. Hubaut Fabrice Marseille, CPPM Huegging Fabian Bonn U. Huettmann Antje DESY Huffman Todd Brian Oxford U. Hughes Emlyn Nevis Labs, Columbia U. Hughes Gareth Lancaster U. Huhtinen Mika CERN Hurwitz Martina LBL, Berkeley Husemann Ulrich DESY Huseynov Nazim Dubna, JINR Baku, Inst. Phys. Huston Joey Michigan State U. Huth John Harvard U., Phys. Dept. Iacobucci Giuseppe Geneva U. Iakovidis Georgios Natl. Tech. U., Athens Ibbotson Michael Manchester U. Ibragimov Iskander Siegen U. Iconomidou-Fayard Lydia Orsay, LAL Idarraga John Orsay, LAL Iengo Paolo INFN, Naples Igonkina Olga FOM, Amsterdam Ikegami Yoichi KEK, Tsukuba Ikeno Masahiro KEK, Tsukuba Iliadis Dimitrios Aristotle U., Thessaloniki Ilic Nikolina Toronto U. Imori Masatoshi ICTP, Trieste Ince Tayfun Bonn U. Inigo-Golfin Joaquin CERN Ioannou Pavlos Athens U. Iodice Mauro INFN, Rome Iordanidou Kalliopi Athens U. Ippolito Valerio INFN, Rome Rome U. Irles Quiles Adrian Valencia U., IFIC Isaksson Charlie Uppsala U., Inst. Theor. Phys. Ishikawa Akimasa Kobe U. Ishino Masaya Kyoto U. Ishmukhametov Renat Southern Methodist U. Issever Cigdem Oxford U. Istin Serhat Bogazici U. Ivashin Anton Serpukhov, IHEP Iwanski Wieslaw Cracow, INP Iwasaki Hiroyuki KEK, Tsukuba Izen Joseph Southern Methodist U. Izzo Vincenzo INFN, Naples Jackson Brett Pennsylvania U. Jackson John Liverpool U. Jackson Paul SLAC Jaekel Martin CERN Jain Vivek Indiana U. Jakobs Karl Freiburg U. Jakobsen Sune Bohr Inst. Jakubek Jan Prague, Tech. U. Jana Dilip Oklahoma U. Jansen Eric University Coll. London Jansen Hendrik CERN Jantsch Andreas Munich, Max Planck Inst. Janus Michel Freiburg U. Jarlskog Göran Lund U. Jeanty Laura Harvard U., Phys. Dept. Jen-La Plante Imai Chicago U., EFI Jenni Peter CERN Jeremie Andrea Annecy, LAPP Jež Pavel Bohr Inst. Jézéquel Stéphane Annecy, LAPP Jha Manoj Kumar INFN, Bologna Ji Haoshuang Wisconsin U., Madison Ji Weina Mainz U. Jia Jiangyong SUNY, Stony Brook Jiang Yi Hefei, CUST Jimenez Belenguer Marcos DESY Jin Shan Beijing, Inst. High Energy Phys. Jinnouchi Osamu Tokyo Inst. Tech. Joergensen Morten Dam Bohr Inst. Joffe David Southern Methodist U. Johansen Lars Bergen U. Johansen Marianne Stockholm U. Stockholm U., OKC Johansson Erik Stockholm U. Johansson Per Sheffield U. Johnert Sebastian DESY Johns Kenneth Arizona U. Jon-And Kerstin Stockholm U. Stockholm U., OKC Jones Graham Oxford U. Jones Roger Lancaster U. Jones Tim Liverpool U. Joram Christian CERN Jorge Pedro LIP, Lisbon Joshi Kiran Daniel Manchester U. Jovicevic Jelena Royal Inst. Tech., Stockholm Jovin Tatjana VINCA Inst. Nucl. Sci., Belgrade Ju Xiangyang Wisconsin U., Madison Jung Christian Dortmund U. Jungst Ralph Markus CERN Juranek Vojtech Prague, Inst. Phys. Jussel Patrick Innsbruck U. Juste Rozas Aurelio Barcelona, IFAE Kabana Sonja Bern U., LHEP Kaci Mohammed Valencia U., IFIC Kaczmarska Anna Cracow, INP Kadlecik Peter Bohr Inst. Kado Marumi Orsay, LAL Kagan Harris Ohio State U. Kagan Michael Harvard U., Phys. Dept. Kajomovitz Enrique Technion Kalinin Sergey Wuppertal U. Kalinovskaya Lidia Dubna, JINR Kama Sami Southern Methodist U. Kanaya Naoko ICTP, Trieste Kaneda Michiru CERN Kaneti Steven Cambridge U. Kanno Takayuki Tokyo Inst. Tech. Kantserov Vadim Moscow Phys. Eng. Inst. Kanzaki Junichi KEK, Tsukuba Kaplan Benjamin Yale U. Kapliy Anton Chicago U., EFI Kaplon Jan CERN Kar Deepak Glasgow U. Karagounis Michael Bonn U. Karnevskiy Mikhail DESY Kartvelishvili Vakhtang Lancaster U. Karyukhin Andrey Serpukhov, IHEP Kashif Lashkar Wisconsin U., Madison Kasieczka Gregor Heidelberg U. Kass Richard Ohio State U. Kastanas Alex Bergen U. Kataoka Mayuko Annecy, LAPP Kataoka Yousuke ICTP, Trieste Katsoufis Elias Natl. Tech. U., Athens Katzy Judith DESY Kaushik Venkatesh Arizona U. Kawagoe Kiyotomo Kyushu U. Kawamoto Tatsuo ICTP, Trieste Kawamura Gen Mainz U. Kayl Manuel FOM, Amsterdam Kazanin Vassili Novosibirsk, IYF Kazarinov Makhail Dubna, JINR Keeler Richard Victoria U. Kehoe Robert Southern Methodist U. Keil Markus Gottingen U., II. Phys. Inst. Kekelidze George Dubna, JINR Keller John Washington U., Seattle Kennedy John Munich U. Kenyon Mike Glasgow U. Kepka Oldrich Prague, Inst. Phys. Kerschen Nicolas CERN Kerševan Borut Paul Stefan Inst., Ljubljana Kersten Susanne Wuppertal U. Kessoku Kohei ICTP, Trieste Keung Justin Toronto U. Khalil-zada Farkhad Baku, Inst. Phys. Khandanyan Hovhannes Illinois U., Urbana Khanov Alexander Oklahoma State U. Kharchenko Dmitri Dubna, JINR Khodinov Alexander Moscow Phys. Eng. Inst. Khomich Andrei Kirchhoff Inst. Phys. Khoo Teng Jian Cambridge U. Khoriauli Gia Bonn U. Khoroshilov Andrey Wuppertal U. Khovanskiy Valery Moscow, ITEP Khramov Evgeniy Dubna, JINR Khubua Jemal Tbilisi State U. Kim Hyeon Jin Stockholm U. Stockholm U., OKC Kim Min Suk Alberta U. Kim Shinhong Tsukuba U. Kimura Naoki Waseda U. Kind Oliver Humboldt U., Berlin King Barry Liverpool U. King Matthew Kobe U. King Robert Steven Beaufoy Oxford U. Kirk Julie Rutherford Kiryunin Andrey Munich, Max Planck Inst. Kishimoto Tomoe Kobe U. Kisielewska Danuta AGH-UST, Cracow Kittelmann Thomas Pittsburgh U. Kiver Andrey Serpukhov, IHEP Kladiva Eduard Kosice, IEF Klein Max Liverpool U. Klein Uta Liverpool U. Kleinknecht Konrad Mainz U. Klemetti Miika McGill U. Klier Amit Weizmann Inst. Klimek Pawel Stockholm U. Stockholm U., OKC Klimentov Alexei Brookhaven Klingenberg Reiner Dortmund U. Klinger Joel Alexander Manchester U. Klinkby Esben Bohr Inst. Klioutchnikova Tatiana CERN Klok Peter NIKHEF, Amsterdam Klous Sander FOM, Amsterdam Kluge Eike-Erik Kirchhoff Inst. Phys. Kluge Thomas Liverpool U. Kluit Peter FOM, Amsterdam Kluth Stefan Munich, Max Planck Inst. Knecht Neil Toronto U. Kneringer Emmerich Innsbruck U. Knoops Edith Marseille, CPPM Knue Andrea Gottingen U., II. Phys. Inst. Ko Byeong Rok Duke U. Kobayashi Tomio ICTP, Trieste Kobel Michael Dresden, Tech. U. Kocian Martin SLAC Kodys Peter Charles U. Köneke Karsten CERN König Adriaan NIKHEF, Amsterdam Koenig Sebastian Mainz U. Köpke Lutz Mainz U. Koetsveld Folkert NIKHEF, Amsterdam Koevesarki Peter Bonn U. Koffas Thomas Carleton U. Koffeman Els FOM, Amsterdam Kogan Lucy Anne Oxford U. Kohlmann Simon Wuppertal U. Kohn Fabian Gottingen U., II. Phys. Inst. Kohout Zdenek Prague, Tech. U. Kohriki Takashi KEK, Tsukuba Koi Tatsumi SLAC Kolachev Guennady Novosibirsk, IYF Kolanoski Hermann Humboldt U., Berlin Kolesnikov Vladimir Dubna, JINR Koletsou Iro INFN, Milan Koll James Michigan State U. Kollefrath Michael Freiburg U. Komar Aston Lebedev Inst. Komori Yuto ICTP, Trieste Kondo Takahiko KEK, Tsukuba Kono Takanori DESY Hamburg U. Kononov Anatoly Freiburg U. Konoplich Rostislav New York U. Manhattan Coll., Riverdale Konstantinidis Nikolaos University Coll. London Kootz Andreas Wuppertal U. Koperny Stefan AGH-UST, Cracow Kopp Anna Katharina Freiburg U. Korcyl Krzysztof Cracow, INP Kordas Kostantinos Aristotle U., Thessaloniki Korn Andreas Oxford U. Korol Aleksandr Novosibirsk, IYF Korolkov Ilya Barcelona, IFAE Korolkova Elena Sheffield U. Korotkov Vladislav Serpukhov, IHEP Kortner Oliver Munich, Max Planck Inst. Kortner Sandra Munich, Max Planck Inst. Kostyukhin Vadim Bonn U. Kotov Sergey Munich, Max Planck Inst. Kotov Vladislav Dubna, JINR Kotwal Ashutosh Duke U. Kourkoumelis Christine Athens U. Kouskoura Vasiliki Aristotle U., Thessaloniki Koutsman Alex TRIUMF Kowalewski Robert Victor Victoria U. Kowalski Tadeusz AGH-UST, Cracow Kozanecki Witold IRFU, Saclay Kozhin Anatoly Serpukhov, IHEP Kral Vlastimil Prague, Tech. U. Kramarenko Viktor Moscow State U. Kramberger Gregor Stefan Inst., Ljubljana Krasny Mieczyslaw Witold Paris U., VI-VII Krasznahorkay Attila New York U. Kraus James Michigan State U. Kraus Jana Bonn U. Krejci Frantisek Prague, Tech. U. Kretzschmar Jan Liverpool U. Krieger Nina Gottingen U., II. Phys. Inst. Krieger Peter Toronto U. Kroeninger Kevin Gottingen U., II. Phys. Inst. Kroha Hubert Munich, Max Planck Inst. Kroll Joe Pennsylvania U. Kroseberg Juergen Bonn U. Krstic Jelena Belgrade U. Kruchonak Uladzimir Dubna, JINR Krüger Hans Bonn U. Kruker Tobias Bern U., LHEP Krumnack Nils Iowa State U. Krumshteyn Zinovii Dubna, JINR Kruth Andre Bonn U. Kubota Takashi Melbourne U. Kuday Sinan Ankara U. Kuehn Susanne Freiburg U. Kugel Andreas Heidelberg U. Kuhl Thorsten DESY Kuhn Dietmar Innsbruck U. Kukhtin Victor Dubna, JINR Kulchitsky Yuri Minsk, Inst. Phys. Kuleshov Sergey Santa Maria U., Valparaiso Kummer Christian Munich U. Kuna Marine Paris U., VI-VII Kunkle Joshua Pennsylvania U. Kupco Alexander Prague, Inst. Phys. Kurashige Hisaya Kobe U. Kurata Masakazu Tsukuba U. Kurochkin Yurii Minsk, Inst. Phys. Kus Vlastimil Prague, Inst. Phys. Kuwertz Emma Sian Royal Inst. Tech., Stockholm Kuze Masahiro Tokyo Inst. Tech. Kvita Jiri Simon Fraser U. Kwee Regina Humboldt U., Berlin La Rosa Alessandro Geneva U. La Rotonda Laura INFN, Cosenza Calabria U. Labarga Luis Madrid, Autonoma U. Labbe Julien Annecy, LAPP Lablak Said Casablanca U. Lacasta Carlos Valencia U., IFIC Lacava Francesco INFN, Rome Rome U. Lacker Heiko Humboldt U., Berlin Lacour Didier Paris U., VI-VII Lacuesta Vicente Ramón Valencia U., IFIC Ladygin Evgueni Dubna, JINR Lafaye Remi Annecy, LAPP Laforge Bertrand Paris U., VI-VII Lagouri Theodota Madrid, Autonoma U. Lai Stanley Freiburg U. Laisne Emmanuel LPSC, Grenoble Lamanna Massimo CERN Lambourne Luke University Coll. London Lampen Caleb Arizona U. Lampl Walter Arizona U. Lancon Eric IRFU, Saclay Landgraf Ulrich Freiburg U. Landon Murrough Queen Mary, U. of London Lane Jenna Manchester U. Lange Clemens DESY Lankford Andrew UC, Irvine Lanni Francesco Brookhaven Lantzsch Kerstin Wuppertal U. Laplace Sandrine Paris U., VI-VII Lapoire Cecile Bonn U. Laporte Jean-Francois IRFU, Saclay Lari Tommaso INFN, Milan Larner Aimee Oxford U. Lassnig Mario CERN Laurelli Paolo Frascati Lavorini Vincenzo INFN, Cosenza Calabria U. Lavrijsen Wim LBL, Berkeley Laycock Paul Liverpool U. Le Dortz Olivier Paris U., VI-VII Le Guirriec Emmanuel Marseille, CPPM Le Maner Christophe Toronto U. Le Menedeu Eve Barcelona, IFAE LeCompte Thomas Argonne Ledroit-Guillon Fabienne Agnes Marie LPSC, Grenoble Lee Hurng-Chun FOM, Amsterdam Lee Jason Osaka U. Lee Shih-Chang Taiwan, Inst. Phys. Lee Lawrence Yale U. Lefebvre Michel Victoria U. Legendre Marie IRFU, Saclay LeGeyt Benjamin Pennsylvania U. Legger Federica Munich U. Leggett Charles LBL, Berkeley Lehmacher Marc Bonn U. Lehmann Miotto Giovanna CERN Lei Xiaowen Arizona U. Leite Marco Aurelio Lisboa Sao Paulo U. Leitner Rupert Charles U. Lellouch Daniel Weizmann Inst. Lemmer Boris Gottingen U., II. Phys. Inst. Lendermann Victor Kirchhoff Inst. Phys. Leney Katharine Witwatersrand U. Lenz Tatiana FOM, Amsterdam Lenzen Georg Wuppertal U. Lenzi Bruno CERN Leonhardt Kathrin Dresden, Tech. U. Leontsinis Stefanos Natl. Tech. U., Athens Lepold Florian Kirchhoff Inst. Phys. Leroy Claude Montreal U. Lessard Jean-Raphael Victoria U. Lester Christopher Cambridge U. Lester Christopher Michael Pennsylvania U. Levêque Jessica Annecy, LAPP Levin Daniel Michigan U. Levinson Lorne Weizmann Inst. Lewis Adrian Oxford U. Lewis George New York U. Leyko Agnieszka Bonn U. Leyton Michael Humboldt U., Berlin Li Bo Marseille, CPPM Li Haifeng Wisconsin U., Madison Shandong U. Li Shu Hefei, CUST Marseille, CPPM Li Xuefei Michigan U. Liang Zhijun Oxford U. Zhongshan U. Liao Hongbo Clermont-Ferrand U. Liberti Barbara INFN, Rome Lichard Peter CERN Lichtnecker Markus Munich U. Lie Ki Illinois U., Urbana Liebig Wolfgang Bergen U. Limbach Christian Bonn U. Limosani Antonio Melbourne U. Limper Maaike Iowa U. Lin Simon Taiwan, Inst. Phys. Linde Frank FOM, Amsterdam Linnemann James Michigan State U. Lipeles Elliot Pennsylvania U. Lipniacka Anna Bergen U. Liss Tony Illinois U., Urbana Lissauer David Brookhaven Lister Alison Geneva U. Litke Alan UC, Santa Cruz Liu Chuanlei Carleton U. Liu Dong Taiwan, Inst. Phys. Liu Hao Michigan U. Liu Jianbei Michigan U. Liu Minghui Hefei, CUST Liu Yanwen Hefei, CUST Livan Michele INFN, Pavia Pavia U. Livermore Sarah Oxford U. Lleres Annick LPSC, Grenoble Llorente Merino Javier Madrid, Autonoma U. Lloyd Stephen Queen Mary, U. of London Lobodzinska Ewelina DESY Loch Peter Arizona U. Lockman William UC, Santa Cruz Loddenkoetter Thomas Bonn U. Loebinger Fred Manchester U. Loginov Andrey Yale U. Loh Chang Wei British Columbia U. Lohse Thomas Humboldt U., Berlin Lohwasser Kristin Freiburg U. Lokajicek Milos Prague, Inst. Phys. Lombardo Vincenzo Paolo Annecy, LAPP Long Robin Eamonn Lancaster U. Lopes Lourenco LIP, Lisbon Lopez Mateos David Harvard U., Phys. Dept. Lorenz Jeanette Munich U. Lorenzo Martinez Narei Orsay, LAL Losada Marta Antonio Narino U. Loscutoff Peter LBL, Berkeley Lo Sterzo Francesco INFN, Rome Rome U. Losty Michael TRIUMF Lou Xinchou Southern Methodist U. Lounis Abdenour Orsay, LAL Loureiro Karina Antonio Narino U. Love Jeremy Boston U. Love Peter Lancaster U. Lowe Andrew SLAC Fresno State Lu Feng Beijing, Inst. High Energy Phys. Lubatti Henry Washington U., Seattle Luci Claudio INFN, Rome Rome U. Lucotte Arnaud LPSC, Grenoble Ludwig Andreas Dresden, Tech. U. Ludwig Dörthe DESY Ludwig Inga Freiburg U. Ludwig Jens Freiburg U. Luehring Frederick Indiana U. Luijckx Guy FOM, Amsterdam Lukas Wolfgang Innsbruck U. Lumb Debra Freiburg U. Luminari Lamberto INFN, Rome Lund Esben Oslo U. Lund-Jensen Bengt Royal Inst. Tech., Stockholm Lundberg Björn Lund U. Lundberg Johan Stockholm U. Stockholm U., OKC Lundquist Johan Bohr Inst. Lungwitz Matthias Mainz U. Lynn David Brookhaven Lys Jeremy LBL, Berkeley Lytken Else Lund U. Ma Hong Brookhaven Ma Lian Liang Wisconsin U., Madison Macana Goia Jorge Andres Montreal U. Maccarrone Giovanni Frascati Macchiolo Anna Munich, Max Planck Inst. Maček Boštjan Stefan Inst., Ljubljana Machado Miguens Joana LIP, Lisbon Mackeprang Rasmus Bohr Inst. Madaras Ronald LBL, Berkeley Mader Wolfgang Dresden, Tech. U. Madsen Alexander Kondrup Uppsala U., Inst. Theor. Phys. Maenner Reinhard Heidelberg U. Maeno Tadashi Brookhaven Mättig Peter Wuppertal U. Mättig Stefan DESY Magnoni Luca CERN Magradze Erekle Gottingen U., II. Phys. Inst. Mahboubi Kambiz Freiburg U. Mahmoud Sara Liverpool U. Mahout Gilles Birmingham U. Maiani Camilla INFN, Rome Rome U. Maidantchik Carmen Rio de Janeiro Federal U. Maio Amélia LIP, Lisbon Lisbon U., CFNUL Majewski Stephanie Brookhaven Makida Yasuhiro KEK, Tsukuba Makovec Nikola Orsay, LAL Mal Prolay IRFU, Saclay Malaescu Bogdan CERN Malecki Pawel Cracow, INP Malecki Piotr Cracow, INP Maleev Victor St. Petersburg, INP Malek Fairouz LPSC, Grenoble Mallik Usha Iowa U. Malon David Argonne Malone Caitlin SLAC Maltezos Stavros Natl. Tech. U., Athens Malyshev Vladimir Novosibirsk, IYF Malyukov Sergei CERN Mameghani Raphael Munich U. Mamuzic Judita VINCA Inst. Nucl. Sci., Belgrade Manabe Atsushi KEK, Tsukuba Mandelli Luciano INFN, Milan Mandić Igor Stefan Inst., Ljubljana Mandrysch Rocco Humboldt U., Berlin Maneira José LIP, Lisbon Mangeard Pierre-Simon Michigan State U. Manhaes de Andrade Filho Luciano Rio de Janeiro Federal U. Mann Alexander Gottingen U., II. Phys. Inst. Manning Peter UC, Santa Cruz Manousakis-Katsikakis Arkadios Athens U. Mansoulie Bruno IRFU, Saclay Mapelli Alessandro CERN Mapelli Livio CERN March Luis Madrid, Autonoma U. Marchand Jean-Francois Carleton U. Marchese Fabrizio INFN, Rome Rome U., Tor Vergata Marchiori Giovanni Paris U., VI-VII Marcisovsky Michal Prague, Inst. Phys. Marino Christopher Victoria U. Marroquim Fernando Rio de Janeiro Federal U. Marshall Zach CERN Martens Kalen Toronto U. Marti-Garcia Salvador Valencia U., IFIC Martin Brian CERN Martin Brian Thomas Michigan State U. Martin Jean-Pierre Montreal U. Martin Tim Birmingham U. Martin Victoria Jane Edinburgh U. Martin dit Latour Bertrand Geneva U. Martin-Haugh Stewart Sussex U. Martinez Mario Barcelona, IFAE Martinez Outschoorn Verena Harvard U., Phys. Dept. Martyniuk Alex Victoria U. Marx Marilyn Manchester U. Marzano Francesco INFN, Rome Marzin Antoine Oklahoma U. Masetti Lucia Mainz U. Mashimo Tetsuro ICTP, Trieste Mashinistov Ruslan Lebedev Inst. Masik Jiri Manchester U. Maslennikov Alexey Novosibirsk, IYF Massa Ignazio INFN, Bologna Bologna U. Massaro Graziano FOM, Amsterdam Massol Nicolas Annecy, LAPP Mastrandrea Paolo INFN, Rome Rome U. Mastroberardino Anna INFN, Cosenza Calabria U. Masubuchi Tatsuya ICTP, Trieste Matricon Pierre Orsay, LAL Matsunaga Hiroyuki ICTP, Trieste Matsushita Takashi Kobe U. Mattravers Carly Oxford U. Rutherford Maurer Julien Marseille, CPPM Maxfield Stephen Liverpool U. Mayne Anna Sheffield U. Mazini Rachid Taiwan, Inst. Phys. Mazur Michael Bonn U. Mazzaferro Luca INFN, Rome Rome U., Tor Vergata Mazzanti Marcello INFN, Milan Mc Kee Shawn Patrick Michigan U. McCarn Allison Illinois U., Urbana McCarthy Robert SUNY, Stony Brook McCarthy Tom Carleton U. McCubbin Norman Rutherford McFarlane Kenneth Hampton U. Mcfayden Josh Sheffield U. McGlone Helen Glasgow U. Mchedlidze Gvantsa Tbilisi State U. Mclaughlan Tom Birmingham U. McMahon Steve Rutherford McPherson Robert Victoria U. IPP, Canada Meade Andrew Massachusetts U., Amherst Mechnich Joerg FOM, Amsterdam Mechtel Markus Wuppertal U. Medinnis Mike DESY Meera-Lebbai Razzak Oklahoma U. Meguro Tatsuma Osaka U. Mehlhase Sascha Bohr Inst. Mehta Andrew Liverpool U. Meier Karlheinz Kirchhoff Inst. Phys. Meirose Bernhard Lund U. Melachrinos Constantinos Chicago U., EFI Mellado Garcia Bruce Rafael Wisconsin U., Madison Meloni Federico INFN, Milan Milan U. Mendoza Navas Luis Antonio Narino U. Meng Zhaoxia Taiwan, Inst. Phys. Shandong U. Mengarelli Alberto INFN, Bologna Bologna U. Menke Sven Munich, Max Planck Inst. Meoni Evelin Barcelona, IFAE Mercurio Kevin Michael Harvard U., Phys. Dept. Mermod Philippe Geneva U. Merola Leonardo INFN, Naples Naples U. Meroni Chiara INFN, Milan Merritt Frank Chicago U., EFI Merritt Hayes Ohio State U. Messina Andrea CERN INFN, Rome Metcalfe Jessica New Mexico U. Mete Alaettin Serhan Iowa State U. Meyer Carsten Mainz U. Meyer Christopher Chicago U., EFI Meyer Jean-Pierre IRFU, Saclay Meyer Jochen Wurzburg U. Meyer Joerg Gottingen U., II. Phys. Inst. Meyer Thomas Christian CERN Meyer W Thomas Iowa State U. Miao Jiayuan Shandong U. Michal Sebastien CERN Micu Liliana Bucharest, IFIN-HH Middleton Robin Rutherford Migas Sylwia Liverpool U. Mijović Liza DESY Mikenberg Giora Weizmann Inst. Mikestikova Marcela Prague, Inst. Phys. Mikuž Marko Stefan Inst., Ljubljana Miller David Chicago U., EFI Miller Robert Michigan State U. Mills Bill British Columbia U. Mills Corrinne Harvard U., Phys. Dept. Milov Alexander Weizmann Inst. Milstead David Stockholm U. Stockholm U., OKC Milstein Dmitry Weizmann Inst. Minaenko Andrey Serpukhov, IHEP Miñano Moya Mercedes Valencia U., IFIC Minashvili Irakli Dubna, JINR Mincer Allen New York U. Mindur Bartosz AGH-UST, Cracow Mineev Mikhail Dubna, JINR Ming Yao Wisconsin U., Madison Mir Lluisa-Maria Barcelona, IFAE Mirabelli Giovanni INFN, Rome Misiejuk Andrzej Royal Holloway, U. of London Mitrevski Jovan UC, Santa Cruz Mitsou Vasiliki A Valencia U., IFIC Mitsui Shingo KEK, Tsukuba Miyagawa Paul Sheffield U. Miyazaki Kazuki Kobe U. Mjörnmark Jan-Ulf Lund U. Moa Torbjoern Stockholm U. Stockholm U., OKC Mockett Paul Washington U., Seattle Moed Shulamit Harvard U., Phys. Dept. Moeller Victoria Cambridge U. Mönig Klaus DESY Möser Nicolas Bonn U. Mohapatra Soumya SUNY, Stony Brook Mohr Wolfgang Freiburg U. Moles-Valls Regina Valencia U., IFIC Molina-Perez Jorge CERN Monk James University Coll. London Monnier Emmanuel Marseille, CPPM Montesano Simone INFN, Milan Milan U. Monticelli Fernando La Plata U. Monzani Simone INFN, Bologna Bologna U. Moore Roger Alberta U. Moorhead Gareth Melbourne U. Mora Herrera Clemencia Geneva U. Moraes Arthur Glasgow U. Morange Nicolas IRFU, Saclay Morel Julien Gottingen U., II. Phys. Inst. Morello Gianfranco INFN, Cosenza Calabria U. Moreno Deywis Mainz U. Moreno Llácer María Valencia U., IFIC Morettini Paolo INFN, Genoa Morgenstern Marcus Dresden, Tech. U. Morii Masahiro Harvard U., Phys. Dept. Morin Jerome Queen Mary, U. of London Morley Anthony Keith CERN Mornacchi Giuseppe CERN Morris John Queen Mary, U. of London Morvaj Ljiljana Nagoya U. Moser Hans-Guenther Munich, Max Planck Inst. Mosidze Maia Tbilisi State U. Moss Josh Ohio State U. Mount Richard SLAC Mountricha Eleni Natl. Tech. U., Athens IRFU, Saclay Mouraviev Sergei Lebedev Inst. Moyse Edward Massachusetts U., Amherst Mueller Felix Kirchhoff Inst. Phys. Mueller James Pittsburgh U. Mueller Klemens Bonn U. Müller Thomas Munich U. Mueller Timo Mainz U. Muenstermann Daniel CERN Munwes Yonathan Tel Aviv U. Murray Bill Rutherford Mussche Ido FOM, Amsterdam Musto Elisa INFN, Naples Naples U. Myagkov Alexey Serpukhov, IHEP Myska Miroslav Prague, Inst. Phys. Nadal Jordi Barcelona, IFAE Nagai Koichi Tsukuba U. Nagano Kunihiro KEK, Tsukuba Nagarkar Advait Ohio State U. Nagasaka Yasushi Hiroshima Inst. Tech. Nagel Martin Munich, Max Planck Inst. Nairz Armin Michael CERN Nakahama Yu CERN Nakamura Koji ICTP, Trieste Nakamura Tomoaki ICTP, Trieste Nakano Itsuo Okayama U. Nanava Gizo Bonn U. Napier Austin Tufts U. Narayan Rohin Heidelberg U. Nash Michael University Coll. London Rutherford Nattermann Till Bonn U. Naumann Thomas DESY Navarro Gabriela Antonio Narino U. Neal Homer Michigan U. Nechaeva Polina Lebedev Inst. Neep Thomas James Manchester U. Negri Andrea INFN, Pavia Pavia U. Negri Guido CERN Nektarijevic Snezana Geneva U. Nelson Andrew UC, Irvine Nelson Timothy Knight SLAC Nemecek Stanislav Prague, Inst. Phys. Nemethy Peter New York U. Nepomuceno Andre Asevedo Rio de Janeiro Federal U. Nessi Marzio CERN Geneva U. Neubauer Mark Illinois U., Urbana Neusiedl Andrea Mainz U. Neves Ricardo New York U. Nevski Pavel Brookhaven Newman Paul Birmingham U. Nguyen Thi Hong Van IRFU, Saclay Nickerson Richard Oxford U. Nicolaidou Rosy IRFU, Saclay Nicolas Ludovic Sheffield U. Nicquevert Bertrand CERN Niedercorn Francois Orsay, LAL Nielsen Jason UC, Santa Cruz Nikiforou Nikiforos Nevis Labs, Columbia U. Nikiforov Andriy Humboldt U., Berlin Nikolaenko Vladimir Serpukhov, IHEP Nikolic-Audit Irena Paris U., VI-VII Nikolics Katalin Geneva U. Nikolopoulos Konstantinos Brookhaven Nilsen Henrik Freiburg U. Nilsson Paul Texas U., Arlington Ninomiya Yoichi ICTP, Trieste Nisati Aleandro INFN, Rome Nishiyama Tomonori Kobe U. Nisius Richard Munich, Max Planck Inst. Nodulman Lawrence Argonne Nomachi Masaharu Osaka U. Nomidis Ioannis Aristotle U., Thessaloniki Nordberg Markus CERN Norton Peter Rutherford Novakova Jana Charles U. Nozaki Mitsuaki KEK, Tsukuba Nozka Libor Palacky U. Nugent Ian Michael TRIUMF Nuncio-Quiroz Adriana-Elizabeth Bonn U. Nunes Hanninger Guilherme Melbourne U. Nunnemann Thomas Munich U. Nurse Emily University Coll. London O'Brien Brendan Joseph Edinburgh U. O'Neale Steve Birmingham U. O'Neil Dugan Simon Fraser U. O'Shea Val Glasgow U. Oakes Louise Beth Munich U. Oakham Gerald Carleton U. TRIUMF Oberlack Horst Munich, Max Planck Inst. Ocariz Jose Paris U., VI-VII Ochi Atsuhiko Kobe U. Oda Susumu ICTP, Trieste Odaka Shigeru KEK, Tsukuba Odier Jerome Marseille, CPPM Ogren Harold Indiana U. Oh Alexander Manchester U. Oh Seog Duke U. Ohm Christian Stockholm U. Stockholm U., OKC Ohshima Takayoshi Nagoya U. Okada Shogo Kobe U. Okawa Hideki UC, Irvine Okumura Yasuyuki Nagoya U. Okuyama Toyonobu ICTP, Trieste Olariu Albert Bucharest, IFIN-HH Olchevski Alexander Dubna, JINR Olivares Pino Sebastian Andres Valparaiso U., Catolica Oliveira Miguel Alfonso LIP, Lisbon Coimbra U. Oliveira Damazio Denis Brookhaven Oliver Garcia Elena Valencia U., IFIC Olivito Dominick Pennsylvania U. Olszewski Andrzej Cracow, INP Olszowska Jolanta Cracow, INP Onofre António LIP, Lisbon Minho U. Onyisi Peter Chicago U., EFI Oram Christopher TRIUMF Oreglia Mark Chicago U., EFI Oren Yona Tel Aviv U. Orestano Domizia INFN, Rome Rome III U. Orlando Nicola INFN, Lecce Salento U. Orlov Iliya Novosibirsk, IYF Oropeza Barrera Cristina Glasgow U. Orr Robert Toronto U. Osculati Bianca INFN, Genoa Genoa U. Ospanov Rustem Pennsylvania U. Osuna Carlos Barcelona, IFAE Otero y Garzon Gustavo Buenos Aires U. Ottersbach John FOM, Amsterdam Ouchrif Mohamed Oujda U. Ouellette Eric Victoria U. Ould-Saada Farid Oslo U. Ouraou Ahmimed IRFU, Saclay Ouyang Qun Beijing, Inst. High Energy Phys. Ovcharova Ana LBL, Berkeley Owen Mark Manchester U. Owen Simon Sheffield U. Ozcan Veysi Erkcan Bogazici U. Ozturk Nurcan Texas U., Arlington Pacheco Pages Andres Barcelona, IFAE Padilla Aranda Cristobal Barcelona, IFAE Pagan Griso Simone LBL, Berkeley Paganis Efstathios Sheffield U. Paige Frank Brookhaven Pais Preema Massachusetts U., Amherst Pajchel Katarina Oslo U. Palacino Gabriel York U., Canada Paleari Chiara Arizona U. Palestini Sandro CERN Pallin Dominique Clermont-Ferrand U. Palma Alberto LIP, Lisbon Palmer Jody Birmingham U. Pan Yibin Wisconsin U., Madison Panagiotopoulou Evgenia Natl. Tech. U., Athens Panikashvili Natalia Michigan U. Panitkin Sergey Brookhaven Pantea Dan Bucharest, IFIN-HH Papadelis Aras Stockholm U. Papadopoulou Theodora Natl. Tech. U., Athens Paramonov Alexander Argonne Paredes Hernandez Daniela Clermont-Ferrand U. Park Woochun Brookhaven South Carolina U. Parker Andy Cambridge U. Parodi Fabrizio INFN, Genoa Genoa U. Parsons John Nevis Labs, Columbia U. Parzefall Ulrich Freiburg U. Pashapour Shabnaz Gottingen U., II. Phys. Inst. Pasqualucci Enrico INFN, Rome Passaggio Stefano INFN, Genoa Passeri Antonio INFN, Rome Pastore Fernanda INFN, Rome Rome III U. Pastore Francesca Royal Holloway, U. of London Pásztor Gabriella Geneva U. Budapest, RMKI Pataraia Sophio Wuppertal U. Patel Nikhul Sydney U. Pater Joleen Manchester U. Patricelli Sergio INFN, Naples Naples U. Pauly Thilo CERN Pecsy Martin Comenius U. Pedraza Morales Maria Isabel Wisconsin U., Madison Peleganchuk Sergey Novosibirsk, IYF Pelikan Daniel Uppsala U., Inst. Theor. Phys. Peng Haiping Hefei, CUST Penning Bjoern Chicago U., EFI Penson Alexander Nevis Labs, Columbia U. Penwell John Indiana U. Perantoni Marcelo Rio de Janeiro Federal U. Perez Kerstin Nevis Labs, Columbia U. Caltech Perez Cavalcanti Tiago DESY Perez Codina Estel TRIUMF Pérez García-Estañ María Teresa Valencia U., IFIC Perez Reale Valeria Nevis Labs, Columbia U. Perini Laura INFN, Milan Milan U. Pernegger Heinz CERN Perrino Roberto INFN, Lecce Perrodo Pascal Annecy, LAPP Persembe Seda Ankara U. Peshekhonov Vladimir Dubna, JINR Peters Krisztian CERN Petersen Brian CERN Petersen Jorgen CERN Petersen Troels Bohr Inst. Petit Elisabeth Annecy, LAPP Petridis Andreas Aristotle U., Thessaloniki Petridou Chariclia Aristotle U., Thessaloniki Petrolo Emilio INFN, Rome Petrucci Fabrizio INFN, Rome Rome III U. Petschull Dennis DESY Petteni Michele Simon Fraser U. Pezoa Raquel Santa Maria U., Valparaiso Phan Anna Melbourne U. Phillips Peter William Rutherford Piacquadio Giacinto CERN Picazio Attilio Geneva U. Piccaro Elisa Queen Mary, U. of London Piccinini Maurizio INFN, Bologna Bologna U. Piec Sebastian Marcin DESY Piegaia Ricardo Buenos Aires U. Pignotti David Ohio State U. Pilcher James Chicago U., EFI Pilkington Andrew Manchester U. Pina João Antonio LIP, Lisbon Lisbon U., CFNUL Pinamonti Michele INFN, Udine Udine U. Pinder Alex Oxford U. Pinfold James Alberta U. Pinto Belmiro LIP, Lisbon Pizio Caterina INFN, Milan Milan U. Plamondon Mathieu Victoria U. Pleier Marc-Andre Brookhaven Plotnikova Elena Dubna, JINR Poblaguev Andrei Brookhaven Poddar Sahill Kirchhoff Inst. Phys. Podlyski Fabrice Clermont-Ferrand U. Poggioli Luc Orsay, LAL Poghosyan Tatevik Bonn U. Pohl Martin Geneva U. Polci Francesco LPSC, Grenoble Polesello Giacomo INFN, Pavia Policicchio Antonio INFN, Cosenza Calabria U. Polini Alessandro INFN, Bologna Poll James Queen Mary, U. of London Polychronakos Venetios Brookhaven Pomarede Daniel Marc IRFU, Saclay Pomeroy Daniel Brandeis U. Pommès Kathy CERN Pontecorvo Ludovico INFN, Rome Pope Bernard Michigan State U. Popeneciu Gabriel Alexandru Bucharest, IFIN-HH Popovic Dragan Belgrade U. Poppleton Alan CERN Portell Bueso Xavier CERN Pospelov Guennady Munich, Max Planck Inst. Pospisil Stanislav Prague, Tech. U. Potrap Igor Munich, Max Planck Inst. Potter Christina Sussex U. Potter Christopher Oregon U. Poulard Gilbert CERN Poveda Joaquin Wisconsin U., Madison Pozdnyakov Valery Dubna, JINR Prabhu Robindra University Coll. London Pralavorio Pascal Marseille, CPPM Pranko Aliaksandr LBL, Berkeley Prasad Srivas CERN Pravahan Rishiraj Brookhaven Prell Soeren Iowa State U. Pretzl Klaus Peter Bern U., LHEP Price Darren Indiana U. Price Joe Liverpool U. Price Lawrence Argonne Prieur Damien Pittsburgh U. Primavera Margherita INFN, Lecce Prokofiev Kirill New York U. Prokoshin Fedor Santa Maria U., Valparaiso Protopopescu Serban Brookhaven Proudfoot James Argonne Prudent Xavier Dresden, Tech. U. Przybycien Mariusz AGH-UST, Cracow Przysiezniak Helenka Annecy, LAPP Psoroulas Serena Bonn U. Ptacek Elizabeth Oregon U. Pueschel Elisa Massachusetts U., Amherst Purdham John Michigan U. Purohit Milind Brookhaven South Carolina U. Puzo Patrick Orsay, LAL Pylypchenko Yuriy Iowa U. Qian Jianming Michigan U. Qin Zhonghua DESY Quadt Arnulf Gottingen U., II. Phys. Inst. Quarrie David LBL, Berkeley Quayle William Wisconsin U., Madison Quinonez Fernando Valparaiso U., Catolica Raas Marcel NIKHEF, Amsterdam Radescu Voica DESY Radloff Peter Oregon U. Rador Tonguc Bogazici U. Ragusa Francesco INFN, Milan Milan U. Rahal Ghita CC, Villeurbanne Rahimi Amir Ohio State U. Rahm David Brookhaven Rajagopalan Srinivasan Brookhaven Rammensee Michael Freiburg U. Rammes Marcus Siegen U. Randle-Conde Aidan Sean Southern Methodist U. Randrianarivony Koloina Carleton U. Rauscher Felix Munich U. Rave Tobias Christian Freiburg U. Raymond Michel CERN Read Alexander Lincoln Oslo U. Rebuzzi Daniela INFN, Pavia Pavia U. Redelbach Andreas Wurzburg U. Redlinger George Brookhaven Reece Ryan Pennsylvania U. Reeves Kendall Southern Methodist U. Reinherz-Aronis Erez Tel Aviv U. Reinsch Andreas Oregon U. Reisinger Ingo Dortmund U. Rembser Christoph CERN Ren Zhongliang Taiwan, Inst. Phys. Renaud Adrien Orsay, LAL Rescigno Marco INFN, Rome Resconi Silvia INFN, Milan Resende Bernardo IRFU, Saclay Reznicek Pavel Munich U. Rezvani Reyhaneh Toronto U. Richter Robert Munich, Max Planck Inst. Richter-Was Elzbieta Annecy, LAPP Ridel Melissa Paris U., VI-VII Rijpstra Manouk FOM, Amsterdam Rijssenbeek Michael SUNY, Stony Brook Rimoldi Adele INFN, Pavia Pavia U. Rinaldi Lorenzo INFN, Bologna Rios Ryan Randy Southern Methodist U. Riu Imma Barcelona, IFAE Rivoltella Giancesare INFN, Milan Milan U. Rizatdinova Flera Oklahoma State U. Rizvi Eram Queen Mary, U. of London Robertson Steven McGill U. IPP, Canada Robichaud-Veronneau Andree Oxford U. Robinson Dave Cambridge U. Robinson James University Coll. London Robson Aidan Glasgow U. Rocha de Lima Jose Guilherme Northern Illinois U. Roda Chiara INFN, Pisa Pisa U. Roda Dos Santos Denis CERN Rodriguez Diego Antonio Narino U. Roe Adam Gottingen U., II. Phys. Inst. Roe Shaun CERN Røhne Ole Oslo U. Rolli Simona Tufts U. Romaniouk Anatoli Moscow Phys. Eng. Inst. Romano Marino INFN, Bologna Bologna U. Romeo Gaston Buenos Aires U. Romero Adam Elena Valencia U., IFIC Roos Lydia Paris U., VI-VII Ros Eduardo Valencia U., IFIC Rosati Stefano INFN, Rome Rosbach Kilian Geneva U. Rose Anthony Sussex U. Rose Matthew Royal Holloway, U. of London Rosenbaum Gabriel Toronto U. Rosenberg Eli Iowa State U. Rosendahl Peter Lundgaard Bergen U. Rosenthal Oliver Siegen U. Rosselet Laurent Geneva U. Rossetti Valerio Barcelona, IFAE Rossi Elvira INFN, Rome Rome U. Rossi Leonardo Paolo INFN, Genoa Rotaru Marina Bucharest, IFIN-HH Roth Itamar Weizmann Inst. Rothberg Joseph Washington U., Seattle Rousseau David Orsay, LAL Royon Christophe IRFU, Saclay Rozanov Alexander Marseille, CPPM Rozen Yoram Technion Ruan Xifeng Beijing, Inst. High Energy Phys. Orsay, LAL Rubbo Francesco Barcelona, IFAE Rubinskiy Igor DESY Ruckert Benjamin Munich U. Ruckstuhl Nicole FOM, Amsterdam Rud Viacheslav Moscow State U. Rudolph Christian Dresden, Tech. U. Rudolph Gerald Innsbruck U. Rühr Frederik Arizona U. Ruggieri Federico INFN, Rome Rome III U. Ruiz-Martinez Aranzazu Iowa State U. Rumyantsev Leonid Dubna, JINR Runge Kay Freiburg U. Rurikova Zuzana Freiburg U. Rusakovich Nikolai Dubna, JINR Rutherfoord John Arizona U. Ruwiedel Christoph LBL, Berkeley Ruzicka Pavel Prague, Inst. Phys. Ryabov Yury St. Petersburg, INP Ryan Patrick Michigan State U. Rybar Martin Charles U. Rybkin Grigori Orsay, LAL Ryder Nick Oxford U. Saavedra Aldo Sydney U. Sadeh Iftach Tel Aviv U. Sadrozinski Hartmut UC, Santa Cruz Sadykov Renat Dubna, JINR Safai Tehrani Francesco INFN, Rome Sakamoto Hiroshi ICTP, Trieste Salamanna Giuseppe Queen Mary, U. of London Salamon Andrea INFN, Rome Saleem Muhammad Oklahoma U. Salek David CERN Salihagic Denis Munich, Max Planck Inst. Salnikov Andrei SLAC Salt José Valencia U., IFIC Salvachua Ferrando Belén Argonne Salvatore Daniela INFN, Cosenza Calabria U. Salvatore Pasquale Fabrizio Sussex U. Salvucci Antonio NIKHEF, Amsterdam Salzburger Andreas CERN Sampsonidis Dimitrios Aristotle U., Thessaloniki Samset Björn Hallvard Oslo U. Sanchez Arturo INFN, Naples Naples U. Sanchez Martinez Victoria Valencia U., IFIC Sandaker Heidi Bergen U. Sander Heinz Georg Mainz U. Sanders Michiel Munich U. Sandhoff Marisa Wuppertal U. Sandoval Tanya Cambridge U. Sandoval Carlos Antonio Narino U. Sandstroem Rikard Munich, Max Planck Inst. Sankey Dave Rutherford Sansoni Andrea Frascati Santamarina Rios Cibran McGill U. Santoni Claudio Clermont-Ferrand U. Santonico Rinaldo INFN, Rome Rome U., Tor Vergata Santos Helena LIP, Lisbon Saraiva João LIP, Lisbon Sarangi Tapas Wisconsin U., Madison Sarkisyan-Grinbaum Edward Texas U., Arlington Sarri Francesca INFN, Pisa Pisa U. Sartisohn Georg Wuppertal U. Sasaki Osamu KEK, Tsukuba Sasao Noboru Kyoto U. Satsounkevitch Igor Minsk, Inst. Phys. Sauvage Gilles Annecy, LAPP Sauvan Emmanuel Annecy, LAPP Sauvan Jean-Baptiste Orsay, LAL Savard Pierre Toronto U. TRIUMF Savinov Vladimir Pittsburgh U. Savu Dan Octavian CERN Sawyer Lee Brookhaven Louisiana Tech. U. Saxon David Glasgow U. Saxon James Pennsylvania U. Sbarra Carla INFN, Bologna Sbrizzi Antonio INFN, Bologna Bologna U. Scallon Olivia Montreal U. Scannicchio Diana UC, Irvine Scarcella Mark Sydney U. Schaarschmidt Jana Orsay, LAL Schacht Peter Munich, Max Planck Inst. Schaefer Douglas Pennsylvania U. Schäfer Uli Mainz U. Schaepe Steffen Bonn U. Schaetzel Sebastian Heidelberg U. Schaffer Arthur Orsay, LAL Schaile Dorothee Munich U. Schamberger R. Dean SUNY, Stony Brook Schamov Andrey Novosibirsk, IYF Scharf Veit Kirchhoff Inst. Phys. Schegelsky Valery St. Petersburg, INP Scheirich Daniel Michigan U. Schernau Michael UC, Irvine Scherzer Max Nevis Labs, Columbia U. Schiavi Carlo INFN, Genoa Genoa U. Schieck Jochen Munich U. Schioppa Marco INFN, Cosenza Calabria U. Schlenker Stefan CERN Schmidt Evelyn Freiburg U. Schmieden Kristof Bonn U. Schmitt Christian Mainz U. Schmitt Sebastian Heidelberg U. Schmitz Martin Bonn U. Schöning André Heidelberg U. Schott Matthias CERN Schouten Doug TRIUMF Schovancova Jaroslava Prague, Inst. Phys. Schram Malachi McGill U. Schroeder Christian Mainz U. Schroer Nicolai Heidelberg U. Schultens Martin Johannes Bonn U. Schultes Joachim Wuppertal U. Schultz-Coulon Hans-Christian Kirchhoff Inst. Phys. Schulz Holger Humboldt U., Berlin Schumacher Jan Bonn U. Schumacher Markus Freiburg U. Schumm Bruce UC, Santa Cruz Schune Philippe IRFU, Saclay Schwanenberger Christian Manchester U. Schwartzman Ariel SLAC Schwemling Philippe Paris U., VI-VII Schwienhorst Reinhard Michigan State U. Schwierz Rainer Dresden, Tech. U. Schwindling Jerome IRFU, Saclay Schwindt Thomas Bonn U. Schwoerer Maud Annecy, LAPP Sciolla Gabriella Brandeis U. Scott Bill Rutherford Searcy Jacob Oregon U. Sedov George DESY Sedykh Evgeny St. Petersburg, INP Seidel Sally New Mexico U. Seiden Abraham UC, Santa Cruz Seifert Frank Dresden, Tech. U. Seixas José Rio de Janeiro Federal U. Sekhniaidze Givi INFN, Naples Sekula Stephen Southern Methodist U. Selbach Karoline Elfriede Edinburgh U. Seliverstov Dmitry St. Petersburg, INP Sellden Bjoern Stockholm U. Sellers Graham Liverpool U. Seman Michal Kosice, IEF Semprini-Cesari Nicola INFN, Bologna Bologna U. Serfon Cedric Munich U. Serin Laurent Orsay, LAL Serkin Leonid Gottingen U., II. Phys. Inst. Seuster Rolf Munich, Max Planck Inst. Severini Horst Oklahoma U. Sfyrla Anna CERN Shabalina Elizaveta Gottingen U., II. Phys. Inst. Shamim Mansoora Oregon U. Shan Lianyou Beijing, Inst. High Energy Phys. Shank James Boston U. Shao Qi Tao Melbourne U. Shapiro Marjorie LBL, Berkeley Shatalov Pavel Moscow, ITEP Shaw Kate INFN, Udine Udine U. Sherman Daniel Yale U. Sherwood Peter University Coll. London Shibata Akira New York U. Shichi Hideharu Nagoya U. Shimizu Shima CERN Shimojima Makoto Nagasaki Inst. Appl. Sci. Shin Taeksu Hampton U. Shiyakova Maria Dubna, JINR Shmeleva Alevtina Lebedev Inst. Shochet Mel Chicago U., EFI Short Daniel Oxford U. Shrestha Suyog Iowa State U. Shulga Evgeny Moscow Phys. Eng. Inst. Shupe Michael Arizona U. Sicho Petr Prague, Inst. Phys. Sidoti Antonio INFN, Rome Siegert Frank Freiburg U. Sijacki Djordje Belgrade U. Silbert Ohad Weizmann Inst. Silva José LIP, Lisbon Silver Yiftah Tel Aviv U. Silverstein Daniel SLAC Silverstein Samuel Stockholm U. Simak Vladislav Prague, Tech. U. Simard Olivier IRFU, Saclay Simic Ljiljana Belgrade U. Simion Stefan Orsay, LAL Simmons Brinick University Coll. London Simoniello Rosa INFN, Milan Milan U. Simonyan Margar Bohr Inst. Sinervo Pekka Toronto U. Sinev Nikolai Oregon U. Sipica Valentin Siegen U. Siragusa Giovanni Wurzburg U. Sircar Anirvan Brookhaven Sisakyan Alexei Dubna, JINR Sivoklokov Serguei Moscow State U. Sjölin Jörgen Stockholm U. Stockholm U., OKC Sjursen Therese Bergen U. Skinnari Louise Anastasia LBL, Berkeley Skottowe Hugh Philip Harvard U., Phys. Dept. Skovpen Kirill Novosibirsk, IYF Skubic Patrick Oklahoma U. Slater Mark Birmingham U. Slavicek Tomas Prague, Tech. U. Sliwa Krzysztof Tufts U. Smakhtin Vladimir Weizmann Inst. Smart Ben Edinburgh U. Smirnov Sergei Moscow Phys. Eng. Inst. Smirnov Yury Moscow Phys. Eng. Inst. Smirnova Lidia Moscow State U. Smirnova Oxana Lund U. Smith Ben Campbell Harvard U., Phys. Dept. Smith Douglas SLAC Smith Kenway Glasgow U. Smizanska Maria Lancaster U. Smolek Karel Prague, Tech. U. Snesarev Andrei Lebedev Inst. Snow Steve Manchester U. Snow Joel Oklahoma U. Snyder Scott Brookhaven Sobie Randall Victoria U. IPP, Canada Sodomka Jaromir Prague, Tech. U. Soffer Abner Tel Aviv U. Solans Carlos Valencia U., IFIC Solar Michael Prague, Tech. U. Solc Jaroslav Prague, Tech. U. Soldatov Evgeny Moscow Phys. Eng. Inst. Soldevila Urmila Valencia U., IFIC Solfaroli Camillocci Elena INFN, Rome Rome U. Solodkov Alexander Serpukhov, IHEP Solovyanov Oleg Serpukhov, IHEP Soni Nitesh Alberta U. Sopko Vit Prague, Tech. U. Sopko Bruno Prague, Tech. U. Sosebee Mark Texas U., Arlington Soualah Rachik INFN, Udine Udine U. Soukharev Andrey Novosibirsk, IYF Spagnolo Stefania INFN, Lecce Salento U. Spanò Francesco Royal Holloway, U. of London Spighi Roberto INFN, Bologna Spigo Giancarlo CERN Spila Federico INFN, Rome Rome U. Spiwoks Ralf CERN Spousta Martin Charles U. Spreitzer Teresa Toronto U. Spurlock Barry Texas U., Arlington St Denis Richard Dante Glasgow U. Stahlman Jonathan Pennsylvania U. Stamen Rainer Kirchhoff Inst. Phys. Stanecka Ewa Cracow, INP Stanek Robert Argonne Stanescu Cristian INFN, Rome Stanescu-Bellu Madalina DESY Stapnes Steinar Oslo U. Starchenko Evgeny Serpukhov, IHEP Stark Jan LPSC, Grenoble Staroba Pavel Prague, Inst. Phys. Starovoitov Pavel DESY Staude Arnold Munich U. Stavina Pavel Comenius U. Steele Genevieve Glasgow U. Steinbach Peter Dresden, Tech. U. Steinberg Peter Brookhaven Stekl Ivan Prague, Tech. U. Stelzer Bernd Simon Fraser U. Stelzer Harald Joerg Michigan State U. Stelzer-Chilton Oliver TRIUMF Stenzel Hasko Giessen U. Stern Sebastian Munich, Max Planck Inst. Stewart Graeme CERN Stillings Jan Andre Bonn U. Stockton Mark McGill U. Stoerig Kathrin Freiburg U. Stoicea Gabriel Bucharest, IFIN-HH Stonjek Stefan Munich, Max Planck Inst. Strachota Pavel Charles U. Stradling Alden Texas U., Arlington Straessner Arno Dresden, Tech. U. Strandberg Jonas Royal Inst. Tech., Stockholm Strandberg Sara Stockholm U. Stockholm U., OKC Strandlie Are Oslo U. Strang Michael Ohio State U. Strauss Emanuel SLAC Strauss Michael Oklahoma U. Strizenec Pavol Kosice, IEF Ströhmer Raimund Wurzburg U. Strom David Oregon U. Strong John Royal Holloway, U. of London Stroynowski Ryszard Southern Methodist U. Strube Jan Rutherford Stugu Bjarne Bergen U. Stumer Iuliu Brookhaven Stupak John SUNY, Stony Brook Sturm Philipp Wuppertal U. Styles Nicholas Adam DESY Soh Dart-yin Taiwan, Inst. Phys. Zhongshan U. Su Dong SLAC Subramania Halasya Siva Alberta U. Succurro Antonella Barcelona, IFAE Sugaya Yorihito Osaka U. Suhr Chad Northern Illinois U. Suita Koichi Kobe U. Suk Michal Charles U. Sulin Vladimir Lebedev Inst. Sultansoy Saleh TOBB ETU, Ankara Sumida Toshi Kyoto U. Sun Xiaohu LPSC, Grenoble Sundermann Jan Erik Freiburg U. Suruliz Kerim Sheffield U. Susinno Giancarlo INFN, Cosenza Calabria U. Sutton Mark Sussex U. Suzuki Yu KEK, Tsukuba Suzuki Yuta Kobe U. Svatos Michal Prague, Inst. Phys. Swedish Stephen British Columbia U. Sykora Ivan Comenius U. Sykora Tomas Charles U. Sánchez Javier Valencia U., IFIC Ta Duc FOM, Amsterdam Tackmann Kerstin DESY Taffard Anyes UC, Irvine Tafirout Reda TRIUMF Taiblum Nimrod Tel Aviv U. Takahashi Yuta Nagoya U. Takai Helio Brookhaven Takashima Ryuichi Kyoto U. of Education Takeda Hiroshi Kobe U. Takeshita Tohru Shinshu U. Takubo Yosuke KEK, Tsukuba Talby Mossadek Marseille, CPPM Talyshev Alexey Novosibirsk, IYF Novosibirsk State U. Tamsett Matthew Brookhaven Tanaka Junichi ICTP, Trieste Tanaka Reisaburo Orsay, LAL Tanaka Satoshi Ritsumeikan U. Tanaka Shuji KEK, Tsukuba Tanasijczuk Andres Jorge Simon Fraser U. Tani Kazutoshi Kobe U. Tannoury Nancy Marseille, CPPM Tapprogge Stefan Mainz U. Tardif Dominique Toronto U. Tarem Shlomit Technion Tarrade Fabien Carleton U. Tartarelli Giuseppe Francesco INFN, Milan Tas Petr Charles U. Tasevsky Marek Prague, Inst. Phys. Tassi Enrico INFN, Cosenza Calabria U. Tatarkhanov Mous LBL, Berkeley Tayalati Yahya Oujda U. Taylor Christopher University Coll. London Taylor Frank MIT Taylor Geoffrey Melbourne U. Taylor Wendy York U., Canada Teinturier Marthe Orsay, LAL Teixeira Dias Castanheira Matilde Queen Mary, U. of London Teixeira-Dias Pedro Royal Holloway, U. of London Temming Kim Katrin Freiburg U. Ten Kate Herman CERN Teng Ping-Kun Taiwan, Inst. Phys. Terada Susumu KEK, Tsukuba Terashi Koji ICTP, Trieste Terron Juan Madrid, Autonoma U. Testa Marianna Frascati Teuscher Richard Toronto U. IPP, Canada Therhaag Jan Bonn U. Theveneaux-Pelzer Timothée Paris U., VI-VII Thioye Moustapha Yale U. Thoma Sascha Freiburg U. Thomas Juergen Birmingham U. Thompson Emily Nevis Labs, Columbia U. Thompson Paul Birmingham U. Thompson Peter Toronto U. Thompson Stan Glasgow U. Thomsen Lotte Ansgaard Bohr Inst. Thomson Evelyn Pennsylvania U. Thomson Mark Cambridge U. Thun Rudolf Michigan U. Tian Feng Nevis Labs, Columbia U. Tibbetts Mark James LBL, Berkeley Tic Tomáš Prague, Inst. Phys. Tikhomirov Vladimir Lebedev Inst. Tikhonov Yury Novosibirsk, IYF Novosibirsk State U. Timoshenko Sergey Moscow Phys. Eng. Inst. Tipton Paul Yale U. Tique Aires Viegas Florbela De Jes CERN Tisserant Sylvain Marseille, CPPM Todorov Theodore Annecy, LAPP Todorova-Nova Sharka Tufts U. Toggerson Brokk UC, Irvine Tojo Junji Kyushu U. Tokár Stanislav Comenius U. Tokunaga Kaoru Kobe U. Tokushuku Katsuo KEK, Tsukuba Tollefson Kirsten Michigan State U. Tomoto Makoto Nagoya U. Tompkins Lauren Chicago U., EFI Toms Konstantin New Mexico U. Tonoyan Arshak Bergen U. Topfel Cyril Bern U., LHEP Topilin Nikolai Dubna, JINR Torchiani Ingo CERN Torrence Eric Oregon U. Torres Heberth Paris U., VI-VII Torró Pastor Emma Valencia U., IFIC Toth Jozsef Marseille, CPPM Budapest, RMKI Touchard Francois Marseille, CPPM Tovey Daniel Sheffield U. Trefzger Thomas Wurzburg U. Tremblet Louis CERN Tricoli Alesandro CERN Trigger Isabel Marian TRIUMF Trincaz-Duvoid Sophie Paris U., VI-VII Tripiana Martin La Plata U. Trischuk William Toronto U. Trocmé Benjamin LPSC, Grenoble Troncon Clara INFN, Milan Trottier-McDonald Michel Simon Fraser U. Trzebinski Maciej Cracow, INP Trzupek Adam Cracow, INP Tsarouchas Charilaos CERN Tseng Jeffrey Oxford U. Tsiakiris Menelaos FOM, Amsterdam Tsiareshka Pavel Minsk, Inst. Phys. Tsionou Dimitra Annecy, LAPP Sheffield U. Tsipolitis Georgios Natl. Tech. U., Athens Tsiskaridze Vakhtang Freiburg U. Tskhadadze Edisher Tbilisi, Inst. Phys. Tsukerman Ilya Moscow, ITEP Tsulaia Vakhtang LBL, Berkeley Tsung Jieh-Wen Bonn U. Tsuno Soshi KEK, Tsukuba Tsybychev Dmitri SUNY, Stony Brook Tua Alan Sheffield U. Tudorache Alexandra Bucharest, IFIN-HH Tudorache Valentina Bucharest, IFIN-HH Tuggle Joseph Chicago U., EFI Turala Michal Cracow, INP Turecek Daniel Prague, Tech. U. Turk Cakir Ilkay TAEK, Ankara Turlay Emmanuel FOM, Amsterdam Turra Ruggero INFN, Milan Milan U. Tuts Michael Nevis Labs, Columbia U. Tykhonov Andrii Stefan Inst., Ljubljana Tylmad Maja Stockholm U. Stockholm U., OKC Tyndel Mike Rutherford Tzanakos George Athens U. Uchida Kirika Bonn U. Ueda Ikuo ICTP, Trieste Ueno Ryuichi Carleton U. Ugland Maren Bergen U. Uhlenbrock Mathias Bonn U. Uhrmacher Michael Gottingen U., II. Phys. Inst. Ukegawa Fumihiko Tsukuba U. Unal Guillaume CERN Undrus Alexander Brookhaven Unel Gokhan UC, Irvine Unno Yoshinobu KEK, Tsukuba Urbaniec Dustin Nevis Labs, Columbia U. Usai Giulio Texas U., Arlington Uslenghi Massimiliano INFN, Pavia Pavia U. Vacavant Laurent Marseille, CPPM Vacek Vaclav Prague, Tech. U. Vachon Brigitte McGill U. Vahsen Sven LBL, Berkeley Valenta Jan Prague, Inst. Phys. Valente Paolo INFN, Rome Valentinetti Sara INFN, Bologna Bologna U. Valkar Stefan Charles U. Valladolid Gallego Eva Valencia U., IFIC Vallecorsa Sofia Technion Valls Ferrer Juan Antonio Valencia U., IFIC van der Graaf Harry FOM, Amsterdam van der Kraaij Erik FOM, Amsterdam Van Der Leeuw Robin FOM, Amsterdam van der Poel Egge FOM, Amsterdam van der Ster Daniel CERN van Eldik Niels Massachusetts U., Amherst van Gemmeren Peter Argonne van Vulpen Ivo FOM, Amsterdam Vanadia Marco Munich, Max Planck Inst. Vandelli Wainer CERN Vaniachine Alexandre Argonne Vankov Peter DESY Vannucci Francois Paris U., VI-VII Vari Riccardo INFN, Rome Varol Tulin Massachusetts U., Amherst Varouchas Dimitris LBL, Berkeley Vartapetian Armen Texas U., Arlington Varvell Kevin Sydney U. Vassilakopoulos Vassilios Hampton U. Vazeille Francois Clermont-Ferrand U. Vazquez Schroeder Tamara Gottingen U., II. Phys. Inst. Vegni Guido INFN, Milan Milan U. Veillet Jean-Jacques Orsay, LAL Veloso Filipe LIP, Lisbon Veness Raymond CERN Veneziano Stefano INFN, Rome Ventura Andrea INFN, Lecce Salento U. Ventura Daniel Massachusetts U., Amherst Venturi Manuela Freiburg U. Venturi Nicola Toronto U. Vercesi Valerio INFN, Pavia Verducci Monica Washington U., Seattle Verkerke Wouter FOM, Amsterdam Vermeulen Jos FOM, Amsterdam Vest Anja Dresden, Tech. U. Vetterli Michel Simon Fraser U. TRIUMF Vichou Irene Illinois U., Urbana Vickey Trevor Witwatersrand U. Oxford U. Vickey Boeriu Oana Elena Witwatersrand U. Viehhauser Georg Oxford U. Viel Simon British Columbia U. Villa Mauro INFN, Bologna Bologna U. Villaplana Perez Miguel Valencia U., IFIC Vilucchi Elisabetta Frascati Vincter Manuella Carleton U. Vinek Elisabeth CERN Vinogradov Vladimir Dubna, JINR Virchaux Marc IRFU, Saclay Virzi Joseph LBL, Berkeley Vitells Ofer Weizmann Inst. Viti Michele DESY Vivarelli Iacopo Freiburg U. Vives Vaque Francesc Alberta U. Vlachos Sotirios Natl. Tech. U., Athens Vladoiu Dan Munich U. Vlasak Michal Prague, Tech. U. Vogel Adrian Bonn U. Vokac Petr Prague, Tech. U. Volpi Guido Frascati Volpi Matteo Melbourne U. Volpini Giovanni INFN, Milan von der Schmitt Hans Munich, Max Planck Inst. von Loeben Joerg Munich, Max Planck Inst. von Radziewski Holger Freiburg U. von Toerne Eckhard Bonn U. Vorobel Vit Charles U. Vorwerk Volker Barcelona, IFAE Vos Marcel Valencia U., IFIC Voss Rudiger CERN Voss Thorsten Tobias Wuppertal U. Vossebeld Joost Liverpool U. Vranjes Nenad IRFU, Saclay Vranjes Milosavljevic Marija FOM, Amsterdam Vrba Vaclav Prague, Inst. Phys. Vreeswijk Marcel FOM, Amsterdam Vu Anh Tuan Freiburg U. Vuillermet Raphael CERN Vukotic Ilija Orsay, LAL Wagner Wolfgang Wuppertal U. Wagner Peter Pennsylvania U. Wahlen Helmut Wuppertal U. Wahrmund Sebastian Dresden, Tech. U. Wakabayashi Jun Nagoya U. Walch Shannon Michigan U. Walder James Lancaster U. Walker Rodney Munich U. Walkowiak Wolfgang Siegen U. Wall Richard Yale U. Waller Peter Liverpool U. Wang Chiho Duke U. Wang Haichen Wisconsin U., Madison Wang Hulin Hefei, CUST Taiwan, Inst. Phys. Wang Jike Taiwan, Inst. Phys. Wang Jin LPSC, Grenoble Wang Joshua C Washington U., Seattle Wang Rui New Mexico U. Wang Song-Ming Taiwan, Inst. Phys. Wang Tan Bonn U. Warburton Andreas McGill U. Ward Patricia Cambridge U. Warsinsky Markus Freiburg U. Washbrook Andrew Edinburgh U. Wasicki Christoph DESY Watkins Peter Birmingham U. Watson Alan Birmingham U. Watson Ian Sydney U. Watson Miriam Birmingham U. Watts Gordon Washington U., Seattle Watts Stephen Manchester U. Waugh Anthony Sydney U. Waugh Ben University Coll. London Weber Marc Rutherford Weber Michele Bern U., LHEP Weber Pavel Gottingen U., II. Phys. Inst. Weidberg Anthony Oxford U. Weigell Philipp Munich, Max Planck Inst. Weingarten Jens Gottingen U., II. Phys. Inst. Weiser Christian Freiburg U. Wellenstein Hermann Brandeis U. Wells Phillippa CERN Wenaus Torre Brookhaven Wendland Dennis Humboldt U., Berlin Weng Zhili Taiwan, Inst. Phys. Zhongshan U. Wengler Thorsten CERN Wenig Siegfried CERN Wermes Norbert Bonn U. Werner Matthias Freiburg U. Werner Per CERN Werth Michael UC, Irvine Wessels Martin Kirchhoff Inst. Phys. Wetter Jeffrey Tufts U. Weydert Carole LPSC, Grenoble Whalen Kathleen Carleton U. Wheeler-Ellis Sarah Jane UC, Irvine White Andrew Texas U., Arlington White Martin Melbourne U. White Sebastian INFN, Pisa Pisa U. Whitehead Samuel Robert Oxford U. Whiteson Daniel UC, Irvine Whittington Denver Indiana U. Wicek Francois Orsay, LAL Wicke Daniel Wuppertal U. Wickens Fred Rutherford Wiedenmann Werner Wisconsin U., Madison Wielers Monika Rutherford Wienemann Peter Bonn U. Wiglesworth Craig Queen Mary, U. of London Wiik-Fuchs Liv Antje Mari Freiburg U. Wijeratne Peter Alexander University Coll. London Wildauer Andreas Valencia U., IFIC Wildt Martin Andre DESY Hamburg U. Wilhelm Ivan Charles U. Wilkens Henric George CERN Will Jonas Zacharias Munich U. Williams Eric Nevis Labs, Columbia U. Williams Hugh Pennsylvania U. Willis William Nevis Labs, Columbia U. Willocq Stephane Massachusetts U., Amherst Wilson John Birmingham U. Wilson Michael Galante SLAC Wilson Alan Michigan U. Wingerter-Seez Isabelle Annecy, LAPP Winkelmann Stefan Freiburg U. Winklmeier Frank CERN Wittgen Matthias SLAC Wolter Marcin Wladyslaw Cracow, INP Wolters Helmut LIP, Lisbon Coimbra U. Wong Wei-Cheng Southern Methodist U. Wooden Gemma Michigan U. Wosiek Barbara Cracow, INP Wotschack Jorg CERN Woudstra Martin Massachusetts U., Amherst Wozniak Krzysztof Cracow, INP Wraight Kenneth Glasgow U. Wright Catherine Glasgow U. Wright Michael Glasgow U. Wrona Bozydar Liverpool U. Wu Sau Lan Wisconsin U., Madison Wu Xin Geneva U. Wu Yusheng Hefei, CUST Michigan U. Wulf Evan Nevis Labs, Columbia U. Wynne Benjamin Edinburgh U. Xella Stefania Bohr Inst. Xiao Meng IRFU, Saclay Xie Song Freiburg U. Xu Chao Hefei, CUST IRFU, Saclay Xu Da Sheffield U. Yabsley Bruce Sydney U. Yacoob Sahal Witwatersrand U. Yamada Miho KEK, Tsukuba Yamaguchi Hiroshi ICTP, Trieste Yamamoto Akira KEK, Tsukuba Yamamoto Kyoko Iowa State U. Yamamoto Shimpei ICTP, Trieste Yamamura Taiki ICTP, Trieste Yamanaka Takashi ICTP, Trieste Yamaoka Jared Duke U. Yamazaki Takayuki ICTP, Trieste Yamazaki Yuji Kobe U. Yan Zhen Boston U. Yang Haijun Michigan U. Yang Un-Ki Manchester U. Yang Yi Indiana U. Yang Zhaoyu Stockholm U. Stockholm U., OKC Yanush Serguei Minsk, High Energy Phys. Ctr. Yao Liwen Beijing, Inst. High Energy Phys. Yao Yushu LBL, Berkeley Yasu Yoshiji KEK, Tsukuba Ybeles Smit Gabriel Valentijn Regina U. Ye Jingbo Southern Methodist U. Ye Shuwei Brookhaven Yilmaz Metin Gazi U. Yoosoofmiya Reza Pittsburgh U. Yorita Kohei Waseda U. Yoshida Riktura Argonne Young Charles SLAC Young Christopher John Oxford U. Youssef Saul Boston U. Yu Dantong Brookhaven Yu Jaehoon Texas U., Arlington Yu Jie Oklahoma State U. Yuan Li Kobe U. Yurkewicz Adam Northern Illinois U. Zabinski Bartlomiej Cracow, INP Zaidan Remi Iowa U. Zaitsev Alexander Serpukhov, IHEP Zajacova Zuzana CERN Zanello Lucia INFN, Rome Rome U. Zaytsev Alexander Novosibirsk, IYF Zeitnitz Christian Wuppertal U. Zeller Michael Yale U. Zeman Martin Prague, Inst. Phys. Zemla Andrzej Cracow, INP Zendler Carolin Bonn U. Zenin Oleg Serpukhov, IHEP Ženiš Tibor Comenius U. Zinonos Zinonas INFN, Pisa Pisa U. Zenz Seth LBL, Berkeley Zerwas Dirk Orsay, LAL Zevi della Porta Giovanni Harvard U., Phys. Dept. Zhan Zhichao Shandong U. Zhang Dongliang Hefei, CUST Taiwan, Inst. Phys. Zhang Huaqiao Michigan State U. Zhang Jinlong Argonne Zhang Xueyao Shandong U. Zhang Zhiqing Orsay, LAL Zhao Long New York U. Zhao Tianchi Washington U., Seattle Zhao Zhengguo Hefei, CUST Zhemchugov Alexey Dubna, JINR Zhong Jiahang Oxford U. Zhou Bing Michigan U. Zhou Ning UC, Irvine Zhou Yue Taiwan, Inst. Phys. Zhu Cheng Guang Shandong U. Zhu Hongbo DESY Zhu Junjie Michigan U. Zhu Yingchun Hefei, CUST Zhuang Xuai Munich U. Zhuravlov Vadym Munich, Max Planck Inst. Zieminska Daria Indiana U. Zimmermann Robert Bonn U. Zimmermann Simone Bonn U. Zimmermann Stephanie Freiburg U. Ziolkowski Michael Siegen U. Zitoun Robert Annecy, LAPP Živković Lidija Nevis Labs, Columbia U. Zmouchko Viatcheslav Serpukhov, IHEP Zobernig Georg Wisconsin U., Madison Zoccoli Antonio INFN, Bologna Bologna U. zur Nedden Martin Humboldt U., Berlin Zutshi Vishnu Northern Illinois U. Zwalinski Lukasz CERN Aad Georges Freiburg U. 2012 06 The results of a search for charged Higgs bosons are presented. The analysis is based on 4.6/fb of proton-proton collision data at $\sqrt{s}$ = 7 TeV collected by the ATLAS experiment at the Large Hadron Collider, using top quark pair events with a tau lepton in the final state. The data are consistent with the expected background from Standard Model processes. Assuming that the branching ratio of the charged Higgs boson to a tau lepton and a neutrino is 100%, this leads to upper limits on the branching ratio of top quark decays to a b quark and a charged Higgs boson between 5% and 1% for charged Higgs boson masses ranging from 90 GeV to 160 GeV, respectively. In the context of the mh-max scenario of the MSSM, tan(beta) above 12-26, as well as between 1 and 2-6, can be excluded for charged Higgs boson masses between 90 GeV and 150 GeV. research-article

Combined limits for H+ -> taunu in ttbar decays with 4.6 fb^{-1} of pp collision data recorded at $sqrt{s} = 7$ TeV with the ATLAS experiment --- Supporting Note Flechl M Freiburg Hattrem Raddum S Oslo Read AL Oslo 2012 The experimental observation of charged Higgs bosons which are predicted by many models with an extended Higgs sector, would indicate physics beyond the Standard Model (SM). This note presents the details of the combination of the results from a search for charged Higgs bosons in 4.6 fb-1 of proton-proton collision data at sqrt{s}=7 TeV in three H+ -> taunu final states in tbar decays. The data agree with the SM expectation leading to a limit on the branching ratio BR(t -> bH+) of 0.01-0.05 for charged Higgs boson masses (m_H+) in the range 90 GeV<m_H+<160 GeV, assuming BR(H+ -> taunu)=1. In the context of the mh-max scenario of the MSSM, this excludes a region above eta = 13-26 in the mass range 90 GeV< m_H+< 150 GeV. INTNOTEATLASINT

Search for a charged Higgs boson decaying via H+ -> tau(lep) + jets in ttbar events using 4.6 fb−1 of pp collision data recorded at sqrt(s) = 7 TeV with the ATLAS detector — Supporting note Barak L Ferrari A Flechl M Gross E Groth-Jensen J Hattrem Raddum S Read A 2012 This note reports on the results of a search for charged Higgs bosons in the ATLAS experiment, based on 4.6 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=7$ TeV using the lepton+jets channel in $t\bar{t}$ decays with a leptonically decaying $\tau$ in the final state. The data agree with the Standard Model expectation. Assuming ${\cal B}(H^+ \rightarrow \tau\nu) = 1$, this leads to upper limits on the branching fraction ${\cal B}(t \rightarrow bH^{+})$ between 4% and 15% for charged Higgs boson masses ($m_{H^+}$) in the range $90\,\mbox{GeV} < m_{H^+} <160\,\mbox{GeV}$. In the context of the $m_h^{\text{max}}$ scenario of the MSSM, values of $\tan\beta$ larger than 27-44 are excluded for charged Higgs boson masses in the range $90\,\mbox{GeV} < m_{H^+} < 140\,\mbox{GeV}$. INTNOTEATLASINT

Search for a charged Higgs boson decaying via H+ -> tau(had)nu+lepton in ttbar events using 4.6 fb−1 of pp collision data recorded at sqrt(s) = 7 TeV with the ATLAS detector — Supporting note Behar S Buszello C Czodrowski P Ferrari A Flechl M Hattrem Raddum S Isaksson C Madsen A McCarn A zur Nedden M Neubauer M Patel N Pelikan D Read A Rozen Y Saavedra A 2012 This note reports on the results of a search for charged Higgs bosons in the ATLAS experiment, based on 4.6 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=7$ TeV, using $t\bar{t}$ decays with a hadronically decaying $\tau$ and one light lepton (electron or muon) in the final state. The data agree with the Standard Model expectation. Assuming ${\cal B}(H^+ \rightarrow \tau\nu) = 1$, this leads to upper limits on the branching fraction ${\cal B}(t \rightarrow bH^{+})$ between 3% and 7% for charged Higgs boson masses ($m_{H^+}$) in the range $90\,\mbox{GeV} < m_{H^+} <160\,\mbox{GeV}$. In the context of the $m_h^{\text{max}}$ scenario of the MSSM, values of $\tan\beta$ larger than 22-50 are excluded for charged Higgs boson masses in the range $90\,\mbox{GeV} < m_{H^+} < 150\,\mbox{GeV}$. INTNOTEATLASINT

Search for charged Higgs bosons in the tau+jets final state in ttbar decays with 4.6 fb−1 of pp collision data recorded at √s = 7 TeV with the ATLAS Experiment — Supporting Note Assamagan P Bernius C Casado P Cavaliere V Czodrowski P Chakraborty D Greenwood D Ferrari A Flechl M Hattrem Raddum S Kopp A Mal P McCarn A Neubauer M Patel N Randle-Conde A Read A L Rocha de Lima G Saavedra A Schumacher M Sekula S 2012 The experimental observation of charged Higgs bosons, H±, which are predicted by many models with an extended Higgs sector, would indicate physics beyond the Standard Model (SM). This note presents the results of a search for charged Higgs bosons in \LUMI of proton-proton collision data at √s = 7 TeV using the tau+jets channel in ttbar decays with a hadronically decaying tau lepton in the final state. The data agree with the SM expectation leading to a limit on the branching ratio BR(t -> b H+) of 0.01-0.06 for charged Higgs boson masses (m_{H+}) in the range 90 GeV < m_{H+} < 160 GeV, assuming BR(H+ -> tau nu)=1. In the context of the m_h-max scenario of the MSSM, this excludes a region above tan(beta) = 10-22 in the mass range 90 GeV < m_{H+} < 150 GeV. INTNOTEATLASINT

Highlights from the LHC Straessner Arno TU Dresden 2012 The Large Hadron Collider (LHC) and the two multi-purpose LHC Detectors, ATLAS and CMS, have been operated successfully at record centre-of-mass energies of 7-8 TeV. This talk presents the main physics results from proton-proton collisions based on a total luminosity of 2 x 5 fb^-1. Most recent results from Standard Model measurements, Standard Model and MSSM Higgs searches, as well as searches for supersymmetric and exotic particles are reported. Prospects for the ongoing and future data taking are presented. INTNOTEATLASPRIV

BSM Higgs Searches at the LHC Rompotis N University of Washington 2012 This presentation summarizes recent Beyond Standard Model (BSM) Higgs searches with 2011 LHC data collected by ATLAS and CMS experiments. The searches described here include MSSM Higgs, Higgs in SM with a 4th generation of fermions, fermiophobic Higgs, doubly charged Higgs, light scalar Higgs and Higgs decaying to long lived particles. INTNOTEATLASPRIV

Search for Higgs bosons decaying into tau leptons with ATLAS Randle-Conde AS Dallas SMU 2012 Search for Higgs bosons decaying into tau leptons with ATLAS, including MSSM neutral Higgs boson, charged bosons, and SM Higgs boson. INTNOTEATLASPRIV

Searches for Beyond-Standard Model Higgs bosons at ATLAS Lenzi B CERN 2012 The results of the searches for Higgs bosons beyond the Standard Model with the ATLAS detector, based on 2011 proton-proton collision data recorded at the Large Hadron Collider (LHC) at a centre-of-mass energy of 7 TeV are reported. No significant excess is observed and exclusion limits are set on the production of neutral Higgs bosons from a fermiophobic benchmark model and the minimal supersymmetric model (MSSM), as well as charged and doubly-charged Higgs bosons. INTNOTEATLASPRIV

Searches for Beyond-Standard Model Higgs bosons at ATLAS Lenzi B CERN 2012 The results of the searches for Higgs bosons beyond the Standard Model with the ATLAS detector, based on 2011 proton-proton collision data recorded at the Large Hadron Collider (LHC) at a centre-of-mass energy of 7 TeV are reported. No significant excess is observed and exclusion limits are set on the production of neutral Higgs bosons from a fermiophobic benchmark model and the minimal supersymmetric model (MSSM), as well as charged and doubly-charged Higgs bosons. INTNOTEATLASPUBL

Higgs Boson Searches with ATLAS Prokofiev K NYU 2012 One of the primary goals of the ATLAS experiment at Large Hadron Collider is to investigate the mechanism of electroweak symmetry breaking by searching for the Higgs bosons. Presented in this contribution is the summary of the recent results concerning the Higgs searches in ATLAS. Both Standard Model and Supersymmetric hypotheses are investigated. Current combined exclusion limits produced by the ATLAS collaboration are discussed. INTNOTEATLASPRIV

Combined Search for a neutral MSSM Higgs boson decaying to τ+τ− or μμ pairs in pp Collisions at sqrt s = 7 TeV with the ATLAS detector Bristow T University of the Withwaterstrand Davey W University of Bonn Dawe N Simon Fraser University Dingfelder J University of Bonn Glatzer J University of Freiburg, University of Bonn Grimm K Lancaster University Goussiou A University of Washington Keller J University of Washington Kortner S MPI Munich Krosenberg J University of Bonn Lai S Albert-Ludwigs-Universitaet Freiburg Mader W Technische Universitaet Dresden Morgenstern M Technische Universitaet Dresden Rompotis N University of Washington Rosendahl P University of Bergen Schumacher M Albert-Ludwigs-Universitaet Freiburg Scutti F University of Bonn Stern S MPI Munich Strassner A Technische Universitaet Dresden Thoma S University of Freiburg Trottier-McDonald M Simon Fraser University Tsuno S KEK Vickey T University of the Withwaterstrand Wang T University of Bonn Warsinsky M Albert-Ludwigs-Universitaet Freiburg v Radziewski H Albert-Ludwigs-Universitaet Freiburg Xella S University of Copenhagen Zanzi D MPI Munich Zinonos Z INFN Sezione di Pisa 2012 The combination of the searches for a neutral Higgs boson in the decay channel H -&gt; tautau and H -&gt; mumu is presented based on proton-proton collisions at a centre-of-mass energy of 7 TeV. The data corresponds to an integrated luminosity of 4.7-4.8 fb−1 collected with the ATLAS experiment at the Large Hadron Collider. This paper discusses the technicalities of the combination of the four independent results obtained from each of the tau(lep)tau(lep), tau(lep)tau(had), tau(had)tau(had) and mumu final states. The result of the search is interpreted in the context of MSSM with limits in the tan beta vs mA. Also cross-section limits for the production of a neutral higgs boson via gluon-gluon fusion and in association with b-quarks are presented. No significant excess of events are observed over background expectations and exclusion limits are derived in the (CP-odd) Higgs mass range 90 GeV &lt; mH &lt; 500 GeV. INTNOTEATLASPRIV

Search for Neutral MSSM Higgs bosons in $\sqrt{s} = 7$ TeV pp collisions at ATLAS Collaboration A 2012 A search for the neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) with the ATLAS detector at the Large Hadron Collider is reported. The analysis is based on a data sample of proton-proton collisions at a centre-of-mass energy of 7 TeV recorded in 2011 and corresponding to an integrated luminosity of 4.7 − 4.8 fb$^{−1}$. Higgs decays into muons and $\tau$ leptons are considered, and events are categorized according to the presence or absence of a b-quark in the final state. No statistically significant excess over the expected background is observed. Upper limits on the MSSM parameter $ \tan\beta$ and on the cross-section times branching ratio for both relevant production mechanisms are set as a function of the mass of the CP-odd or generic Higgs boson, respectively. INTNOTEATLASPRIV

ATLAS Searches for Higgs Bosons Beyond the Standard Model Vickey T 2012 This presentation at "Origin of Mass 2012" summarizes recent Beyond Standard Model (BSM) Higgs searches with 2011 7 TeV LHC data collected by ATLAS. The searches described here include: MSSM Higgs, Higgs in SM with a 4th generation of fermions, fermiophobic Higgs, doubly charged Higgs, light scalar Higgs and Higgs decaying to long lived particles. INTNOTEATLASPRIV

ATLAS Searches for Higgs Bosons Beyond the Standard Model Vickey T 2012 The latest ATLAS search results for Beyond the Standard Model Higgs bosons are shown. Results shown are all with the 2011 7 TeV dataset and include: SM4, Fermiophobic, MSSM, charged Higgs, NMSSM and Hidden Valley. INTNOTEATLASPRIV

Search for Neutral MSSM Higgs bosons in $sqrt{s} = 7$ TeV pp collisions at ATLAS Collaboration A 2012 A search for the neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is performed. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of $7\,\TeV$ recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and corresponds to an integrated luminosity of \currentlumirange. Higgs boson decays into oppositely-charged muon or $\tau$ lepton pairs, for final states requiring either the presence or absence of $b$-jets are considered. As no statistically significant excess over the expected background is observed, exclusion limits at the \unit[95]{\%} confidence level are derived for the production cross section of a generic Higgs boson, $\phi$, as a function of the Higgs boson mass and for \Higgses{} production in the MSSM as a function of the parameters $m_A$ and $\tan\beta$ in the \mhmax{} scenario. INTNOTEATLASPRIV

Search for Neutral MSSM Higgs bosons in $sqrt{s} = 7$ TeV pp collisions at ATLAS Collaboration A 2012 A search for the neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7 TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 − 4.8 $fb^{−1}$. Higgs boson decays into oppositely-charged muon or $\tau$ lepton pairs are considered for final states requiring either the presence or absence of $b$ jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived for the production cross section of a generic Higgs boson, $\phi$, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters $m_{A}$ and $\tan \beta$ in the m$_{max}^{h}$ scenario with $\mu > 0$. INTNOTEATLASPRIV

Search for the neutral MSSM Higgs bosons in the H-&gt;tautau and H-&gt;mumu decay modes with the ATLAS detector at the LHC Thoma S University of Freiburg 2012 The Minimal Supersymmetric extension of the Standard Model (MSSM) predicts the existence of three neutral and two charged Higgs bosons. The search for the neutral MSSM Higgs bosons in the H-&gt; tau+ tau- and H-&gt; mu+ mu- decay modes has been performed using proton-proton collision data recently collected with the ATLAS detector at the Large Hadron Collider. The exclusion limits at the 95% confidence level are discussed as a function of the mA and tan beta parameters. INTNOTEATLASPRIV

Optimisation of the search for MSSM Higgs Bosons in the decay channel $A/H/h \rightarrow \tau^+\tau^- \rightarrow \mu + \tau_{had} + \nu_\mu + 2 \nu_\tau$ with the ATLAS detector Langrock Stefanie CERN The optimisation of the search for the neutral MSSM Higgs bosons in the decay channel $A/H/h \rightarrow \tau^+\tau^- \rightarrow \mu + \tau_{had} + \nu_\mu + 2 \nu_\tau$ with the ATLAS detector is presented. The ATLAS data of the data taking period in 2011 at $\sqrt{s} = 7$\,TeV with an overall integrated luminosity of $L_{\text{int}} = 4.7$\,$\text{fb}^{-1}$ is used. For the optimisation, multivariate methods such as Boosted Decision Trees and Likelihood Estimators were trained against two of the major backgrounds in this decay channel, the $W+$jets background and the QCD background. The training was carried out separately for both backgrounds using a potential signal at $m_A = 120$\,GeV and $\text{tan}\beta = 20$ within the $m_h^{\text{max}}$ benchmark scenario. The Boosted Decision Trees were found to give the best performance in both cases. An overall background rejection of $57.9$\,\% was achieved and the $\frac{s}{\sqrt{b}}$ significance for the given working point was improved by $8.1$\,\% to $4.36$. technical-report

Highlights from the LHC Straessner Arno TU Dresden 2012 The Large Hadron Collider (LHC) and the two multi-purpose LHC Detectors, ATLAS and CMS, have been operated successfully at record centre-of-mass energies of 7-8 TeV. This article presents the main physics results from proton-proton collisions based on a total luminosity of 2 x 5 fb^-1. Most recent results from Standard Model measurements, Standard Model and MSSM Higgs searches, as well as searches for supersymmetric and exotic particles are reported. Prospects for the ongoing and future data taking are presented. INTNOTEATLASPRIV

Search for BSM Higgs bosons in the mumu decay channel with the ATLAS experiment Stern S MPI Munich 2012 Two searches for BSM Higgs bosons decaying in two muons are presented. Neutral MSSM Higgs searches $h/A/h\rightarrow\mu\mu$ have been performed using 4.8 $fb^{-1}$ of 2011 data collected with the ATLAS detector at the LHC. Searches for the NMSSM decay $a_{1}\rightarrow\mu\mu$ have been performed on 39 $pb^{-1}$ of 2010 data. No excess of events compared to the Standard Model expectations is observed in both searches. Exclusion limits have been evaluated at the 95% confidence level. INTNOTEATLASPRIV

Search for Neutral MSSM Higgs bosons in $sqrt{s} = 7$ TeV pp collisions at ATLAS 2012 A search for the neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7 TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 − 4.8 $fb^{−1}$. Higgs boson decays into oppositely-charged muon or $\tau$ lepton pairs are considered for final states requiring either the presence or absence of $b$ jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived for the production cross section of a generic Higgs boson, $\phi$, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters $m_{A}$ and $\tan \beta$ in the m$_{max}^{h}$ scenario with $\mu > 0$. INTNOTEATLASPUBL

Beyond Standard Model Higgs searches at ATLAS Rompotis N University of Washington 2012 A review of Beyond Standard model Higgs searches at ATLAS using LHC pp collision at sqrt(s) = 7 TeV is presented. The searches discussed here include MSSM and NMSSM Higgs, fermiophobic Higgs, Higgs decaying to light pseudoscalar particles, doubly charged Higgs and Higgs decaying to long lived particles. INTNOTEATLASPRIV

Search for Neutral MSSM Higgs Bosons in $A^0/h^0/H^0 \rightarrow \tau^+\tau^- \rightarrow e^\pm\mu^\mp + 4\nu$ Final States Without $b$-Tagged Jets in Proton-Proton Collisions at $\sqrt{s}=7\,\TeV$ with the ATLAS Detector v Radziewski H Albert-Ludwigs-Universitaet Freiburg, Germany Lai S Albert-Ludwigs-Universitaet Freiburg, Germany Schumacher M Albert-Ludwigs-Universitaet Freiburg, Germany Warsinsky M Albert-Ludwigs-Universitaet Freiburg, Germany 2012 A search for neutral MSSM Higgs bosons $A^0$, $H^0$, $h^0$ with the ATLAS detector at the LHC is presented. The analysis is based on proton-proton collisions at a center-of-mass energy of $7\TeV$, corresponding to an integrated luminosity of 4.66 fb$^{-1}$ and focuses on Higgs decays into two tau leptons, $A^0/H^0/h^0\to\tau^+\tau^-$, one tau lepton decays via $\tau \rightarrow \mu \nu_{\tau} \nu_{\mu}$ and the other decays via $\tau \rightarrow e \nu_{\tau} \nu_e$. In addition, the absence of identified $b$-jets is required, complementing the search for Higgs bosons produced in association with with $b$-jets ($b\bar{b}H$). Expected exclusion limits at 95\% CL are placed on the cross-section times branching ratio $\sigma \times BR(\phi \rightarrow \tau\tau)$. Limits are also presented in the $m_A$ vs. $\tan\beta$ plane of the $m_h^{max}$ scenario. INTNOTEATLASPRIV

Highlights from the LHC Straessner Arno Dresden, Tech. U. 2012 The Large Hadron Collider (LHC) and the two multi-purpose LHC Detectors, ATLAS and CMS, have been operated successfully at record centre-of-mass energies of 7-8 TeV. This article presents the main physics results from proton-proton collisions based on a total luminosity of 2 x 5 fb^-1. Most recent results from Standard Model measurements, Standard Model and MSSM Higgs searches, as well as searches for supersymmetric and exotic particles are reported. Prospects for the ongoing and future data taking are presented. INTNOTEATLASPUBL

Schnittoptimierung der Suche nach neutralen MSSM Higgs-Bosonen im Zweimyonenkanal am ATLAS-Detektor bei einer Schwerpunktsenergie von √s=7TeV Grohs J Philipp Dresden, Tech. U. One of the main tasks of the ATLAS detector at the LHC accelerator ring in the vicinity of Geneva is the search for the cause of the gauge symmetry breaking of the electroweak force. The minimal super symmetric extension of the standard model of particles (MSSM) explains this symmetry breaking by the existence of Higgs fields, which manifests itself among other by three electrically neutral Higgs bosons. The present thesis deals with the search for these particles in the dimuon channel. This channel has compared to the decay into b-quarks or Tau-leptons a very small branching ratio, but it leaves a very clear signal in the detector and allows therefore, if the searched Higgs bosons exist, a precise measurement of their properties. The aim of this thesis is to optimize the cut selection by which the signal should be separated from the background. Therefore, the predictions of three Monte Carlo generators are compared with the ATLAS data for agreement. Based on the best available simulation of the background, the cut selection is optimized with regard to the determination of limits on the Higgs bosons cross section. technical-report

Search for the Standard Model and MSSM Higgs bosons in the H-&gt;tautau decay mode with ATLAS Schwindt T Bonn University 2012 A Higgs boson search in the H-&gt; tau^+ tau^- decay mode has been performed using recent data collected with the ATLAS detector at the Large Hadron Collider. The search for the Standard Model Higgs boson was performed in the mass range of 100-150 GeV. Upper limits on the cross-section times branching ratio are derived. The Minimal Supersymmetric extension of the Standard Model (MSSM) predicts the existence of three neutral and two charged Higgs bosons. The neutral Higgs bosons are searched through their decays into pairs of oppositely charged tau leptons. The exclusion limits at the 95% confidence level are discussed as a function of the mA and tan beta parameters. INTNOTEATLASPRIV

Search for charged Higgs bosons decaying to tau+nu in top-antitop events with the ATLAS detector at the LHC Chakraborty D 2012 The ATLAS collaboration has performed a model-independent search for charged Higgs bosons in decays of pair-produced to pquarks using 4.6/fb of proton-proton collisions at sqrt(s) = 7 TeV. The charged Higgs are assumed to decay exclusively to a tau lepton and its associated neutrino. Three different final states are considered. In the absence of any significant excess of events over Standard Model expectations, 95% C.L. upper limits of 0.5 to 0.1 are placed on the branching fraction of the top quark decaying into a charged Higgs and a b quark, for charged Higgs boson masses of 90 GeV to 160 GeV, respectively. INTNOTEATLASPRIV

Search for Higgs bosons decaying into tau leptons with ATLAS Randle-Conde AS Southern Methodist University 2012 In these proceedings the status of the searches for Higgs bosons decaying with τ leptons in the final state using the ATLAS detector are presented. The analyses search for Higgs bosons using up to int Ldt = 4.6fb−1 of pp collision data at √s = 7TeV provided by the LHC. INTNOTEATLASPRIV

Recherche du boson de Higgs chargé dans le canal H+ -> tb et étiquetage des jets b avec l'expérience ATLAS auprès du LHC. Zaidan R Marseille, CPPM The only particle of the Standard Model that has not yet been discovered is the Higgs boson, which explains the origin of the masses of elementary particles. In the Minimal Supersymmetric extention to the Standard Model (MSSM), the Higgs sector consists of five bosons, two of which are charged. The search for a charged Higgs boson in the gg ¯tbH+(H+ ! t¯b) channel, is the main topic of this analysis. We present an analysis that uses a likelihood function to resolve combinatorics while reconstructing the charged Higgs boson, and the b-tagging to suppress the t¯t+jets background. We also present the difficulties due to the combinatoric background reducing the discovery potential of this channel. The presence of 4 b quarks in the final state that we are looking at, makes the b-tagging an important tool for the analysis. Therefore, a part of this work is dedicated to the study of b-tagging. We present in the context of the preperation for the first data, several studies dedicated to the optimisation and the understanding of the b-taggingperformance. We also present the commissioning of a simple tagger (JetProb) to be used with first data analysis. technical-report

Beyond Standard Model Higgs Searches with the ATLAS detector at the LHC Rompotis N University of Washington 2012 A review of Beyond Standard model Higgs searches at ATLAS using LHC pp collision at sqrt(s) = 7 TeV is presented. The searches discussed here include MSSM Higgs, Higgs decaying to light pseudoscalar particles and Higgs decaying to long lived particles. INTNOTEATLASPRIV

Search for Higgs bosons decaying into tau leptons with ATLAS Randle-Conde AS Southern Methodist U. 2012 In these proceedings the status of the searches for Higgs bosons decaying with τ leptons in the final state using the ATLAS detector are presented. The analyses search for Higgs bosons using up to int Ldt = 4.6fb−1 of pp collision data at √s = 7TeV provided by the LHC. INTNOTEATLASPUBL

Search for neutral MSSM Higgs Bosons in the h/A/H to tau^+ tau^- Decay Mode with the ATLAS Detector Mitani T 2012 A search for neutral MSSM Higgs bosons (h/A/H) in the tau^+ tau^- decay mode has been performed using proton-proton collision data collected with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 7 TeV during 2011. The search was performed in the mass range of 90 - 500 GeV. Upper limits on the cross-section times branching ratio for both b-associated and gluon-fusion production modes are derived. Exclusion limits are also shown in the $m_A$-$ aneta$ plane for the mh-max benchmark scenario. INTNOTEATLASPRIV

Summary of non-SM Higgs boson searches at the LHC Davey W E 2012 A review of searches for non-Standard Model Higgs bosons conducted at the Large Hadron Collider is presented. The searches use datasets corresponding to integrated luminosities of up to 5\ifb{} collected by the ATLAS and CMS experiments during 7\,TeV proton-proton collisions. Searches for neutral and charged MSSM Higgs bosons, the light CP-odd neutral Higgs boson of the NMSSM, fermiophobic Higgs bosons and doubly charged Higgs bosons are conducted. No evidence for these signals are observed. INTNOTEATLASPRIV

Search for H+->tau(had)+nu in ATLAS Czodrowski P Technical University Dresden, Germany 2012 This talk shall summarize the search efforts of the ATLAS collaboration for the (light) charged Higgs bosons decaying into hadronically decaying tau leptons and with a special focus on the presentation the new results which were won by utilizing the an ratio method approach on the so called tau+lepton final state. These new results are then combined with the existing ones from the other final states yielding improved sensitivity. As no excess is observed, limits are set on the branching ratio of top quarks decaying to charged Higgs bosons. INTNOTEATLASPRIV

Summary of non-SM Higgs boson searches at the LHC Davey W E Bonn U. 2012 A review of searches for non-Standard Model Higgs bosons conducted at the Large Hadron Collider is presented. The searches use datasets corresponding to integrated luminosities of up to 5\ifb{} collected by the ATLAS and CMS experiments during 7\,TeV proton-proton collisions. Searches for neutral and charged MSSM Higgs bosons, the light CP-odd neutral Higgs boson of the NMSSM, fermiophobic Higgs bosons and doubly charged Higgs bosons are conducted. No evidence for these signals are observed. INTNOTEATLASPUBL

Search for the neutral MSSM Higgs bosons in the H->tau+tau− and H->mu+mu− decay modes with the ATLAS detector at the LHC Thoma S University of Freiburg 2012 The Minimal Supersymmetric extension of the Standard Model (MSSM) predicts the existence of three neutral and two charged Higgs bosons. The search for the neutral MSSM Higgs bosons in the tau+tau− and mu+mu− decay modes has been performed using proton-proton collision data recently collected with the ATLAS detector at the Large Hadron Collider. The exclusion limits at the 95% confidence level are discussed as a function of the mA and tanb parameters. INTNOTEATLASPRIV

Searches for MSSM Higgs Bosons at ATLAS and CMS Lai S University of Freiburg 2012 The Minimal Supersymmetric extension of the Standard Model (MSSM) predicts the existence of three neutral and two charged Higgs bosons. The search for the MSSM Higgs bosons is presented, based on the proton-proton collisions recorded in 2011 and 2012 by the ATLAS and CMS experiments at the LHC. The neutral Higgs bosons are searched through their decays into pairs of oppositely charged tau leptons or muons. The exclusion limits at the 95% confidence level are discussed in an model-independent way, as well as a function of the mA and tan beta parameters .The search for the charged Higgs bosons is based on their production through the decays of top quarks in the $t\bar{t}$ process, $t \to bH^+$. The Higgs bosons subsequently decay predominantly into a tau lepton and a neutrino. Upper limits are set on the branching fraction B(t to bH+), combining the final states with leptonic and hadronic tau decay modes. INTNOTEATLASPRIV

Search for BSM Higgs bosons in the $\mu^{+}\mu^{-}$ decay channel with the ATLAS experiment Stern S Munich, Max Planck Inst. 2012 Two searches for Higgs bosons in theories beyond the Standard Model (BMS) with the ATLAS experiment at the LHC are presented. The search for the neutral MSSM Higgs bosons decaying directly to two muon, $h/A/H\rightarrow\mu^{+}\mu^{-}$, was performed using $pp$ collisions recorded with the ATLAS detector in 2011 at a centre-of-mass energy of $\sqrt{s}=7\,TeV$ and corresponding to an integrated luminosity of $4.8\,fb^{-1}$. The search for the light CP-odd Higgs boson of the NMSSM, $a_1\rightarrow\mu^{+}\mu^{-}$, was performed on a data set with integrated luminosity of $35\,pb^{-1}$, recorded in 2010 at $\sqrt{s}=7\,TeV$. In both searches, no significant excess of events was found in the data with respect to the Standard Model expectation. Exclusion limits at the $95\,\%$ confidence level were evaluated. INTNOTEATLASPUBL

Search for the neutral MSSM Higgs bosons in the H->tau+tau− and H->mu+mu− decay modes with the ATLAS detector at the LHC Thoma S Fribourg U. 2012 The Minimal Supersymmetric extension of the Standard Model (MSSM) predicts the existence of three neutral and two charged Higgs bosons. The search for the neutral MSSM Higgs bosons in the tau+tau− and mu+mu− decay modes has been performed using proton-proton collision data recently collected with the ATLAS detector at the Large Hadron Collider. The exclusion limits at the 95% confidence level are discussed as a function of the mA and tanb parameters. INTNOTEATLASPUBL

Nucl. Phys. B, Proc. Suppl. Nucl. Phys. B, Proc. Suppl. Search for neutral MSSM Higgs Bosons in the h/A/H to tau^+ tau^- Decay Mode with the ATLAS Detector Mitani T Waseda U., RISE 2014 253-255 220 221 In this proceeding a search for neutral Minimal Supersymmetric Standard Model (MSSM) Higgs bosons in the h/A/H to $ \tau^{+} \tau^{-} $ decay mode is reported. The analysis search for MSSM Higgs bosons using up to$ \int L dt = 4.7 $ fb$^{-1}$ of $pp$ collision data at the Large Hadron Collider at $ \sqrt[]{s}=7$TeV during 2011. Upper limits on the cross-section times branching ratio for both $b$-associated and gluon-fusion production modes are derived in the mass range of 90 - 500 GeV. Exclusion limits are also shown in the $m_{A}$ and $ \tan{\beta}$ plane for the $m_{h}^{max}$ scenario with $ \mu > 0$. research-article

Search for H± → τ±(had)+ν in ATLAS Czodrowski P Dresden, Tech. U. 2012 Decays of top quarks in 4.6 fb$^{-1}$ of proton-proton collisions data at $\sqrt{s}=7$ TeV collected by the ATLAS experiment at the Large Hadron Collider at CERN were selected and analyzed to search for signatures of charged Higgs bosons with a hadronically decaying $\tau$ lepton in the final state. The data are consistent with the expected background from Standard Model processes. Assuming a branching ratio of the charged Higgs boson to a $\tau$ lepton and a neutrino of 100% and combining with the leptonically decaying $\tau$ analysis upper limits on the branching ratio of top quark decays to a $b$ quark and a charged Higgs boson between 5% and 1% for charged Higgs boson masses ranging from 90 GeV to 160 GeV, respectively are obtained. In the context of the $m_h^{\mathrm{max}}$ scenario of the MSSM, $\tan\beta$ above 12-26, as well as between 1 and 2-6, can be excluded for charged Higgs boson masses between 90 GeV and 150 GeV. INTNOTEATLASPUBL

Beyond the standard model Higgs searches with ATLAS KLUIT P M NIKHEF, Amsterdam 2012 A summary of the results - based on the 2011 and 2012 data - of the ATLAS experiment for Beyond the Standard Model Higgs searches will be presented. INTNOTEATLASPUBL

Search for long-lived neutral particle decays with first 1.94 fb$^-1$ of 2011 data collected with the ATLAS detector at the LHC Salvatore D U. Calabria, Arcavacata di Rende (main) 2013 Many extensions of the Standard Model (SM) include neutral weakly-coupled particles that can be long-lived. These long-lived partcles occur in many models, included gauge-mediated extensions of the Minimal Supersymmetric Model (MSSM), MSSM with R-parity violation, inelastic dark matter and the Hidden Valley (HV) scenario. Results are presented on the first ATLAS searches at the LHC for possible rare Higgs boson decays to pair of neutral, long-lived hidden-sector particles that lead to final states containing fermion anti-fermion pairs or pairs of collimated jets. No excess of events above the expected background have been observed for 1.94$fb^{-1}$ of data collected in 2011 at a center of mass energy of 7 TeV. Limits are presented as a function of the proper lifetime of the long-lived neutral particle. INTNOTEATLASPUBL

EPJ Web Conf. EPJ Web Conf. Searches for MSSM Higgs Bosons at ATLAS and CMS Lai Stan Freiburg U. 2013 49 The Minimal Supersymmetric extension of the Standard Model (MSSM) predicts the existence of three neutral and two charged Higgs bosons. Searches for these MSSM Higgs bosons are presented, based on proton-proton collisions recorded in 2011 and 2012 by the ATLAS and CMS experiments at the LHC. The neutral Higgs bosons are searched through their decays into pairs of oppositely charged tau leptons. The exclusion limits at 95% confidence level are shown as a function of the $m_A$ and $\tan\beta$ parameters. The search for the charged Higgs bosons is based on their production through the decays of top quarks in the $t\bar{t}$ process, $t \to bH^+$. The Higgs bosons subsequently decay predominantly into a tau lepton and a neutrino. Upper limits are set on the branching fraction $B(t \to bH^+)$, combining the final states with leptonic and hadronic tau decay modes. research-article

Searches for neutral and charged Higgs bosons in the ATLAS experiment as a test of physics beyond the Standard Model Ferrari A Uppsala U. 2013 In several theories beyond the Standard Model, the Higgs sector consists of more than one complex scalar doublet. For instance, supersymmetric models such as the MSSM have five physical Higgs states, two charged and three neutral. In this paper, a review of the searches for new neutral and charged Higgs bosons at the Large Hadron Collider, with the ATLAS experiment, is presented. INTNOTEATLASPUBL

Mass reconstruction techniques and cross section measurement for $Z\to \tau\tau \to e\mu+4\nu$ with the ATLAS experiment Kormoll Kathrin Dresden, Tech. U. A central aspect of modern particle physics is the search for the Higgs boson. First, the Higgs boson remains the only particle of the Standard Model not being proven experimentally. Secondly, its possible observation may improve our understanding of new physics. With the start of operation of the LHC at the European Organization for Nuclear Research (CERN), proton-proton collisions with a centre of mass energy being as high as ${\sqrt{s}=7}$ TeV and ${\sqrt{s}=8}$ TeV could be achieved.\\ This work measures the cross section of the process ${pp\to Z^{0}/\gamma^{*} \rightarrow \tau^{+}\tau^{-}}$ in the mixed leptonic final state with data of the ATLAS detector. The decay of the coherent sum of the photon, $\gamma^{*}$, and the $Z^{0}$ boson is an irreducible background for Higgs boson decays into two $\tau$-leptons. For the Higgs boson search a precise knowledge of its mass spectrum and its normalisation is essential. The data used are equal to an integrated luminosity of L = 35.51 pb$^{-1}$ with a centre of mass energy of ${\sqrt{s}=7}$ TeV. A cross section of ${\sigma^{\mathrm{tot.}}_{Z/\gamma^*} \times \mathrm{BR}(Z \rightarrow \tau\tau)=(1041 \pm 143 \pm 74 \pm 35)}$ pb is yielded, with its statistical and systematic uncertainties as well as uncertainties from luminosity determination. The result is compatible with the results from theoretical calculations and that from other experiments within their uncertainties.\\ The second part of this work examines mass reconstruction methods of decays into two $\tau$-leptons. The analysis concentrates on Higgs bosons, $\phi$, of the minimal supersymmetric extension of the Standard Model, the MSSM. In particular, the decay of Higgs bosons to two $\tau$-leptons and further into an electron, a muon and four neutrinos is examined, $\phi\to\tau^+\tau^-\to e\mu+4\nu$. The appropriate mass reconstruction techniques being investigated are the visible mass, the effective mass and the early and late projected transverse mass. Furthermore, a dependency of the mass distributions on the transverse momentum of the leptons and on the missing transverse energy is observed. However, a dependency on the transverse momentum of the highest $p_{T}$ jet was not found. The elimination of the variable dependencies leads to a worse separation power between the signal and background processes as well as a worse resolution between different Higgs boson masses. The work concludes with a calibration of the masses calculated with the analysed mass reconstruction techniques. technical-report

Searches for BSM Higgs Bosons at the LHC Boehler M Freiburg U. 2013 Searches for Higgs bosons in different extensions of the Standard Model which predict additional neutral and charged Higgs bosons are presented, such as: The Minimal Supersymmetric extension of the Standard Model (MSSM), the next-to Minimal Supersymmetric extension of the Standard Model (nMSSM), two Higgs doublet models, four-generation and fermiophobic models. Results are based on data collected by the ATLAS and CMS experiments in proton-proton collisions at centre-of-mass energies of 7 TeV and 8 TeV. No excess is found in either charged nor neutral Higgs Boson searches. Model-independent and model-dependent exclusion limits are presented for these searches. research-article

EPJ Web Conf. EPJ Web Conf. Search for Long-lived Particles and Lepton-Jets with the ATLAS detector Salvatore D Calabria U. 2013 60 Many extensions of the Standard Model (SM) include neutral weakly-coupled particles that can be long-lived. These long-lived particles occur in many models, included gauge-mediated extensions of the Minimal Supersymmetric Model (MSSM), MSSM with R-parity violation, inelastic dark matter and the Hidden Valley (HV) scenario. Results are presented on the ATLAS searches at the LHC for possible rare Higgs boson decays to pair of neutral, long-lived hidden-sector particles that lead to final states containing collimated lepton jets (LJ) or fermion anti-fermion pairs. No excess of events above the expected background has been observed on data collected in 2011 at a center of mass energy of 7 TeV and limits on the cross sections are set. research-article

Bonn U. Bonn Search for MSSM Higgs Bosons in Di-$τ$ Final States with the ATLAS Experiment Anders Christoph Falk Bonn U. 2013 A search for neutral MSSM Higgs bosons decaying into a $\tau$ lepton pair, $A/H/h \rightarrow\tau^+\tau^−$, is presented. The search is based on proton–proton collision events recorded with the ATLAS detector at the Large Hadron Collider at a center-of-mass energy $\sqrt{s} = 7$ TeV, corresponding to an integrated luminosity of 2.1 fb$^{−1}$. One of the tau leptons is reconstructed in a leptonic, the other in a hadronic final state. The contributions of the main background processes have been estimated using data driven methods. For the $Z/\gamma^* → \tau^+\tau^−$ background an embedding method has been used, that replaces the muons in reconstructed Z/gamma* → mu+mu− events with simulated tau leptons. The event yield of the W + jets background has been studied in a sideband control region and the simulation has been normalized to agree with the sideband data. The contribution from QCD multi-jet processes has been estimated from three data control regions. Systematic uncertainties due to these background estimates have been identified and studied as well as systematic uncertainties affecting the simulated signal and background event samples. The dominating systematic uncertainty has been found to be due to the uncertainty on the energy scales of jets and hadronically decaying tau leptons. In total 4065 data events have been selected and the number of expected events from Standard Model background processes has been estimated to be $4151\pm66\pm796$, where the first error is statistical and the second error is systematic. As no excess over the Standard Model expectation is found, exclusion limits at the 95% confidence level are set on the production cross section of a generic Higgs boson, in dependence of its mass and on the production of the neutral MSSM Higgs bosons $A/H/h$ as a function of the parameters $\tan\beta$ and $m_A$ in the $m_{h}^{\text{max}}$ scenario. These exclusion limits represent significant improvements over those obtained by similar searches of other experiments at LEP and the Tevatron. technical-report

EPJ Web Conf. EPJ Web Conf. BSM Higgs results from ATLAS and CMS Flechl Martin Freiburg U. 2013 60 Searches for Higgs bosons in different extensions of the Standard Model (SM) are presented. These include the Minimal Supersymmetric extension of the SM (MSSM), the next-to-MSSM (NMSSM), models with additional scalar singlets, doublets, or triplets, and generic searches for models with couplings modified with respect to the SM or for non-SM Higgs boson decay channels. Results are based on data collected by the ATLAS and CMS experiments in 2011 and 2012 at the LHC. No excess is found in any of the searches and thus the resulting exclusion limits are given. research-article

Qucosa (Open Access) Dresden Search for Charged Higgs Bosons with the ATLAS Detector at the LHC Czodrowski Patrick Dresden, Tech. U. 2013 The discovery of a charged Higgs boson, $H^+$, would be an unambiguous evidence for physics beyond the Standard Model. In this thesis a search for the $H^+$, with the ATLAS experiment at the Large Hadron Collider, LHC, at CERN based on data taken in 2011, are described. A re-analysis of the charged Higgs boson search, utilising the ratio-method, was performed, which greatly enhanced the sensitivity compared to the traditional direct search approach. Light charged Higgs bosons, with a mass lower than the top quark mass, can be produced in top quark decays. Due to the large production cross-section of top quark pairs the light charged Higgs bosons are accessible with early LHC data, in contrast to charged Higgs bosons heavier than the top quark mass. For light charged Higgs bosons the decay via $H^\pm \to \tau^\pm \nu$ is predominant in most theories and scenarios, in the most parts of their phase space. Therefore the $\tau$ identification and the $\tau$ mis-identification probabilities play an important role in the charged Higgs boson search. A tag-and-probe selection of $Z\to ee$ events was developed in order to asses the mis-identification probability of electrons as hadronically decaying $\tau$ leptons, utilising the very first data taken in 2010. The results of this analysis on the one hand provided scale factors crucial for all analyses utilising the electron veto algorithms of the $\tau$ identification. On the other hand a data-driven estimation technique for backgrounds stemming from electrons mis-identified as hadronically decaying $\tau$ leptons, dedicated for the charged Higgs boson search, was developed and successfully implemented, based upon the results of the tag-and-probe mis-identification results. Trigger studies for the charged Higgs boson search aiming at the highest feasible signal efficiencies with the utilised combination of $\tau$ trigger and missing transverse energy trigger, during the 2012 data taking at a centre of mass energy of 8 TeV, were performed. Novel trigger items were designed, thoroughly tested and finally implemented into the trigger menu of the ATLAS experiment for data taking in 2012. A direct charged Higgs boson search in three channels with $\tau$ leptons in the final state, was performed on the full dataset, with an integrated luminosity of 4.6 fb$^{-1}$, taken in 2011 at a centre of mass energy of 7 TeV. No significant excess over the Standard Model expectation was observed in data, thus limits on ${\cal B}( t \to bH^+)$ were set. Finally the channel with a hadronically decaying $\tau$ lepton and an additional electron or muon in the final state from the $t\bar{t}$ decay was re-analysed with the so-called ratio-method. This method measures ratios of event yields instead of evaluating distributions of discriminating variables, thus most of the dominating systematic uncertainties intrinsically cancel to first order. The observed data are found to be in agreement with the Standard Model predictions. Utilising the ratio-method the limits obtained on ${\cal B}( t \to bH^+)$ were significantly improved, compared to the direct search in this channel. When the results of the ratio-method analysis are combined with the results of the direct search for charged Higgs bosons in $t\bar{t}$ decays, with a hadronically decaying $\tau$ lepton and jets in the final state, upper limits on ${\cal B}(t\to bH^+)$ are set in the range of 0.8 % $-$ 3.4 %, for $m_{H^+}$ between 90 GeV and 160 GeV. The limits set on ${\cal B}(t\to bH^+)$ have direct implications on the identity of the Higgs-like particle, with a mass of approximately 126 GeV discovered in 2012 at the LHC, if the Minimal Supersymmetric extension of the Standard Model (MSSM) is realised in nature. technical-report

Searches for Higgs Boson Decays to Muon Pairs in the Standard Model and in its Minimal Supersymmetric Extension with the ATLAS Detector Stern Sebastian Munich, Max Planck Inst. Two studies of Higgs boson decays to two oppositely charged muons in the Standard Model and in its minimal supersymmetric extension with the ATLAS experiment at the Large Hadron Collider (LHC) at CERN are presented. The search for the decays of the neutral Higgs bosons, $h$, $A$ and $H$, of the Minimal Supersymmetric Extension of the Standard Model (MSSM) to $\mu^{+}\mu^{-}$ is performed in proton-proton collisions at a centre-of-mass energy of 7 TeV based on the data recorded in 2011 which correspond to an integrated luminosity of 4.8 fb$^{-1}$. The branching fraction for the $h/A/H\rightarrow\mu^{+}\mu^{-}$ decay is about 300 times smaller compared to the most sensitive $h/A/H\rightarrow\tau^{+}\tau^{-}$ decay channel. But due to the very high experimental $\mu^{+}\mu^{-}$ mass resolution, the signal appears as narrow resonances in the $\mu^{+}\mu^{-}$ invariant mass distribution on top of a continuous background. Motivated by the two Higgs boson production modes, via gluon fusion and in association with b quarks, the search is performed in two complementary event categories either without or with at least one reconstructed b jet in the selected $\mu^{+}\mu^{-}$ events. The two event categories have different signal-to-background ratios and their statistical combination improves the sensitivity of the search. Signal and background are parametrised by analytic functions. The total background contribution is estimated directly from the data. No significant excess of events above the Standard Model background is observed. Exclusion limits are derived for the MSSM $m_h^\text{max}$ benchmark scenario with positive Higgs mixing parameter as a function of the free parameters $m_A$ and $\tan\beta$. In addition, less model-dependent exclusion limits are set on the production cross section times branching fraction of a generic Higgs boson, $\phi$, produced in either gluon fusion or in association with b quarks as a function its mass, $m_\phi$. The second study evaluates the physics potential of the ATLAS experiment for the search for the rare decay of the Standard Model Higgs boson with a mass of 125 GeV to $\mu^{+}\mu^{-}$. The study uses Monte Carlo simulations of the proton-proton collisions at a centre-of-mass energy of 14 TeV with simplified description of the detector response. The sensitivity is evaluated for two benchmark scenarios with integrated luminosities of 300 fb$^{-1}$ and 3000 fb$^{-1}$ which are expected to be reached after two stages of luminosity upgrades of the LHC machine. The prospects are expressed in terms of expected exclusion limits and signal significances and contribute to the combined Higgs boson coupling measurement. With the proposed data set of 3000 fb$^{-1}$, decays of the Standard Model Higgs boson with mass of 125 GeV to $\mu^{+}\mu^{-}$ are expected to be discovered with a significance of more than 6 standard deviations. Higgs boson couplings to the second-generation leptons can be determined with an accuracy of about 25 % relative to the third-generation lepton couplings. technical-report

ATLAS Searches for Beyond the Standard Model Higgs Bosons Potter C.T. Oregon U. 2013 The present status of ATLAS searches for Higgs bosons in extensions of the Standard Model (SM) is presented. This includes searches for the Higgs bosons of the Two-Higgs-Doublet Model (2HDM), the Minimal Supersymmetric Model (MSSM), the Next-to-Minimal Supersymmetric Model (NMSSM) and models with an invisibly decaying Higgs boson. A review of the phenomenology of the Higgs sectors of these models is given together with the search strategy and the resulting experimental constraints. PREPRINT

Sensitivity to New Phenomena via Higgs Couplings with the ATLAS Detector at a High-Luminosity LHC 2013 The ATLAS experiment at the LHC determines the couplings of the Higgs boson to other particles using the combination of measurements from multiple production and decay channels. The expected precision with which these couplings can be measured at a High-Luminosity LHC has been estimated elsewhere using parametrized acceptances, efficiencies, and resolutions to approximate the expected detector performance. Expected limits on an additional electroweak singlet, an additional electroweak doublet (two-Higgs-doublet model), and dark matter are derived here using the estimated precision on the coupling measurements with 300 and 3000 $\textrm{fb}^{-1}$ of $pp$ collision data at $\sqrt{s}=14$~TeV. The reach for new phenomena is significantly enhanced at a High-Luminosity LHC compared to the corresponding sensitivities at lower integrated luminosities. INTNOTEATLASPUBL

Searches for Supersymmetry in Multilepton Final States with the ATLAS Detector Farrell Steven UC, Irvine Two searches for supersymmetry in multilepton final states are presented using $pp$ collisions at $\sqrt{s} = 8~$TeV in the ATLAS detector. First, a search for electroweak production of charginos and neutralinos in the three-lepton plus missing transverse momentum channel is detailed with an emphasis on the fake-lepton background estimation technique. No significant excess above the Standard Model prediction is observed in the signal regions. Exclusion limits are thus placed on simplified models of $\tilde\chi^\pm_1\tilde\chi^0_2$ production and decays via intermediate sleptons, SM gauge bosons, and Higgs bosons. The results are also interpreted in terms of the phenomenological MSSM. Next, a search for $R$-parity violating and $R$-parity conserving supersymmetric scenarios in the four-lepton channel is presented. No significant excess is observed, so exclusion limits are placed on $R$-parity violating simplified models in which the lightest supersymmetric particle is the lightest neutralino, which promptly decays to leptons. Exclusion limits are also placed on $R$-parity conserving simplified models of $\tilde\chi^0_2\tilde\chi^0_3$ production. technical-report

Search for heavy resonances decaying into the fully hadronic di-tau final state with the ATLAS detector Morgenstern Marcus Matthias Dresden, Tech. U. The discovery of a heavy neutral particle would be a direct hint for new physics beyond the Standard Model. In this thesis searches for new heavy neutral particles decaying into two tau leptons, which further decay into hadrons, are presented. They cover neutral Higgs bosons in the context of the minimal supersymmetric extension of the Standard Model (MSSM) as well as $Z'$ bosons, predicted by various theories with an extended gauge sector. Both analyses are based on the full 2012 proton-proton collision dataset taken by the ATLAS experiment at the Large Hadron Collider (LHC). The extended Higgs sector in the MSSM suggests additional heavy neutral Higgs bosons which decay into tau leptons in about 10\% of the time. Given that the dominant final state, $\phi\to b\bar{b}$, suffers from tremendous QCD initiated backgrounds, the decay into two tau leptons is the most promising final state to discover such new resonances. The fully hadronic final state is the dominant one with a branching fraction of about 42\%. It governs the sensitivity, in particular at high transverse momentum when the QCD multijet background becomes small. Other theoretical extensions of the Standard Model, which are mainly driven by the concept of gauge unification, predict additional heavy particles arising from an extended underlying gauge group. Some of them further predict an enhanced coupling to fermions of the third generation. This motivates the search for $Z'$ bosons in the fully hadronic di-tau final state. One major challenge in physics analyses involving tau leptons is to have an outstanding performance of trigger and identification algorithms suitable to select real tau leptons with high efficiency, while rejecting fake taus originating from quark or gluon initiated jets. In this work a new tau trigger concept based on multivariate classifiers has been developed and became the default tau trigger algorithm in 2012 data-taking. An updated tau identification technique based on the log-likelihood approach has been provided for 2011 data-taking. Furthermore, a new framework has been developed to perform the tuning of the tau identification algorithm and exploited for the optimisation for 2012 data-taking, accordingly. The search for new heavy neutral Higgs bosons in the context of the MSSM has been performed exploiting the full 2012 dataset corresponding to an integrated luminosity of 19.5~fb$^{-1}$ taken at a centre-of-mass energy of $\sqrt{s} = $8~TeV. Updated event selection criteria and novel data-driven background estimation techniques have been developed and are suitable to increase the sensitivity of the analysis significantly. No deviations from the Standard Model prediction are observed, and thus 95\% C.L. exclusion limits on the production cross section times branching ratio, $\sigma(pp\to\phi)\times\text{BR}(\phi\to\tau\tau)$, are derived exploiting the $\mathrm{CL_{s}}$ method. The exclusion ranges from 13.0~pb at 150~GeV to 7.0~fb at 1~TeV for Higgs boson production in association with b-quarks and from 23.6~pb at 150~GeV to 7.5~fb at 1~TeV for Higgs bosons produced via gluon-gluon fusion. The obtained exclusion limit on $\sigma(pp\to\phi)\times\text{BR}(\phi\to\tau\tau)$ can be related to an exclusion of the MSSM parameter space in the $M_A$-$\tan\beta$-plane. Various benchmark scenario are considered. The "standard candle" is the $m_{\mathrm{h}}^\mathrm{max}$ scenario, for which $\tan\beta$ values between 13.3 and 55 can be excluded at 95\% C.L. in the considered mass range. Updated benchmark scenarios designed to incorporate the recently discovered SM-like Higgs boson were suggested and analysed as well. In the $m_{\mathrm{h}}^\mathrm{mod+}$ ($m_{\mathrm{h}}^\mathrm{mod-}$) scenario $\tan\beta$ values between 13.5 (13.3) and 55 (52) can be excluded. Finally, a search for heavy neutral resonances in the context of $Z'$ bosons was performed. As in the search for new Higgs bosons, no deviation from the Standard Model prediction is observed, and hence exclusion limits on the production cross section times branching ratio, $\sigma(pp\toZ')\times\text{BR}(Z'\to\tau\tau)$, and on the $Z'$ boson mass are derived exploiting the Bayesian approach. $Z'$ bosons with $M_{Z'} < $1.9~TeV can be excluded at 95\% credibility, and thus mark the strongest exclusion limit obtained in the di-tau final state by any collider experiment so far. technical-report

Combinations of Results of Higgs production in all decay channels at LHC Di Micco B Rome III U. INFN, Rome3 2014 11 14 This paper describes the present status of the Higgs production measurements in all decay channels at LHC. The decay channels H to b bbar and H to tau tau have been recently analysed by the ATLAS experiments and combined for the first time with the di-boson channels: H to gamma gamma, H to WW and H to ZZ. Updated results on the measurement of the couplings of the Higgs bosons to fermions and bosons are shown and they are compared to the available CMS coupling results. Recent results from CMS, not included in the combination of all channels, on the H to tau tau, H to b bbar , H to WW and H to ZZ decays are also shown for comparison. The impact of the ATLAS coupling results on the simplified-MSSM model is shown. research-article

Search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model in pp collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector 2014 A search for the neutral Higgs bosons predicted by the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is performed on data from proton-proton collisions at a centre-of-mass energy of 8TeV collected with the ATLAS detector at the Large Hadron Collider (LHC). The sample was collected in 2012 and corresponds to an integrated luminosity of 19.5-20.3 fb$^{−1}$ Higgs bosons decays into oppositely-charged $\tau$ lepton pairs are considered for final states. No significant excess over the expected background is observed and exclusion limits at the 95\% confidence level are derived for the production cross section of a scalar field as a function of its mass, and for h/H/A production in the MSSM as a function of the parameters $m_A$ and $\tan\beta$. INTNOTEATLASPUBL

Search for Neutral MSSM Higgs Bosons in $A/h/H \rightarrow \tau\tau \rightarrow e\mu + 4\nu$ Decays with the ATLAS Detector Manfredini Alessandro Munich, Max Planck Inst. A search for the neutral Higgs bosons $A$, $h$, $H$ of the minimal supersymmetric extension of the Standard Model with the ATLAS detector at the LHC is presented based on proton-proton collisions data at a center-of-mass energy of 8 TeV corresponding to an integrated luminosity of 20 $fb^{-1}$. The search is performed for Higgs decays into $\tau$ lepton pairs and subsequet decay via $\tau^{+}\tau^{-}\rightarrow e \mu + 4 \nu$. The results are interpreted in the $m_h^{mod}$ benchmark scenario, no significant excess over the expected Standard Model background is observed. technical-report

Search for neutral Minimally Supersymmetric Standard Model Higgs decaying to two hadronic taus with the ATLAS detector in pp collisions at 7 TeV center of mass energy Dhaliwal Saminder Toronto U. This thesis presents the first search for a neutral Minimal Supersymmetric Standard Model Higgs boson decaying to a pair of hadronic taus in proton-proton collisions with a center-of-mass energy of √s = 7 TeV. Results are presented for an integrated luminosity of 1.056 fb−1 using data from the ATLAS detector at the Large Hadron Collider. After signal selection, 245 events are observed. The number of events is consistent with the background estimate of 256 ± 26. An exclusion limit for the Higgs boson production is derived as a function of (cross-section)×(branching ratio). This limit is presented as a function of two parameters: mA and tanβ in the m_h^max scenario. A point in the (mA, tanβ) phase space is excluded if the signal hypothesis is rejected at the 95% confidence level. technical-report

JHEP JHEP Search for neutral Higgs bosons of the minimal supersymmetric standard model in $pp$ collisions at $\sqrt{s}$ = 8 TeV with the ATLAS detector Aad Georges Marseille, CPPM Abbott Brad Oklahoma U. Abdallah Jalal Taiwan, Inst. Phys. Abdel Khalek Samah Orsay, LAL Abdinov Ovsat Baku, Inst. Phys. Aben Rosemarie FOM, Amsterdam Abi Babak Oklahoma State U. Abolins Maris Michigan State U. AbouZeid Ossama Toronto U. Abramowicz Halina Tel Aviv U. Abreu Henso Technion Abreu Ricardo CERN Abulaiti Yiming Stockholm U. Stockholm U., OKC Acharya Bobby Samir INFN, Udine ICTP, Trieste King's Coll. London Adamczyk Leszek AGH-UST, Cracow Adams David Brookhaven Adelman Jahred Yale U. Adomeit Stefanie Munich U. Adye Tim Rutherford Agatonovic-Jovin Tatjana Belgrade U. Aguilar-Saavedra Juan Antonio LIP, Lisbon CAFPE, Granada Agustoni Marco Bern U., LHEP Ahlen Steven Boston U. Ahmadov Faig Dubna, JINR Baku, Inst. Phys. Aielli Giulio INFN, Rome Rome U., Tor Vergata Akerstedt Henrik Stockholm U. Stockholm U., OKC Åkesson Torsten Paul Ake Lund U. Akimoto Ginga Tokyo U., ICEPP Akimov Andrei Lebedev Inst. Alberghi Gian Luigi INFN, Bologna Bologna U. Albert Justin Victoria U. Albrand Solveig LPSC, Grenoble Alconada Verzini Maria Josefina La Plata U. Aleksa Martin CERN Aleksandrov Igor Dubna, JINR Alexa Calin Bucharest, IFIN-HH Alexander Gideon Tel Aviv U. Alexandre Gauthier Geneva U. Alexopoulos Theodoros Natl. Tech. U., Athens Alhroob Muhammad Oklahoma U. Alimonti Gianluca INFN, Milan Alio Lion Marseille, CPPM Alison John Chicago U., EFI Allbrooke Benedict Birmingham U. Allison Lee John Lancaster U. Allport Phillip Liverpool U. Aloisio Alberto INFN, Naples Naples U. Alonso Alejandro Bohr Inst. Alonso Francisco La Plata U. Alpigiani Cristiano Queen Mary, U. of London Altheimer Andrew David Nevis Labs, Columbia U. Alvarez Gonzalez Barbara Michigan State U. Alviggi Mariagrazia INFN, Naples Naples U. Amako Katsuya KEK, Tsukuba Amaral Coutinho Yara Rio de Janeiro Federal U. Amelung Christoph Brandeis U. Amidei Dante Michigan U. Amor Dos Santos Susana Patricia LIP, Lisbon Coimbra U. Amorim Antonio LIP, Lisbon Lisbon U., CFNUL Amoroso Simone Freiburg U. Amram Nir Tel Aviv U. Amundsen Glenn Brandeis U. Anastopoulos Christos Sheffield U. Ancu Lucian Stefan Geneva U. Andari Nansi CERN Andeen Timothy Nevis Labs, Columbia U. Anders Christoph Falk Heidelberg U. Anders Gabriel CERN Anderson Kelby Chicago U., EFI Andreazza Attilio INFN, Milan Milan U. Andrei George Victor Kirchhoff Inst. Phys. Anduaga Xabier La Plata U. Angelidakis Stylianos Athens U. Angelozzi Ivan FOM, Amsterdam Anger Philipp Dresden, Tech. U. Angerami Aaron Nevis Labs, Columbia U. Anghinolfi Francis CERN Anisenkov Alexey Novosibirsk, IYF Novosibirsk State U. Anjos Nuno Barcelona, IFAE Annovi Alberto Frascati Antonaki Ariadni Athens U. Antonelli Mario Frascati Antonov Alexey Moscow Phys. Eng. Inst. Antos Jaroslav Kosice, IEF Anulli Fabio INFN, Rome Aoki Masato KEK, Tsukuba Aperio Bella Ludovica Birmingham U. Apolle Rudi Oxford U. Rutherford Arabidze Giorgi Michigan State U. Aracena Ignacio SLAC Arai Yasuo KEK, Tsukuba Araque Juan Pedro LIP, Lisbon Arce Ayana Duke U. Arduh Francisco Anuar La Plata U. Arguin Jean-Francois Montreal U. Argyropoulos Spyridon DESY Arik Metin Bogazici U. Armbruster Aaron James CERN Arnaez Olivier CERN Arnal Vanessa Madrid, Autonoma U. Arnold Hannah Freiburg U. Arratia Miguel Cambridge U. Arslan Ozan Bonn U. Artamonov Andrei Moscow, ITEP Artoni Giacomo Brandeis U. Asai Shoji Tokyo U., ICEPP Asbah Nedaa DESY Ashkenazi Adi Tel Aviv U. Åsman Barbro Stockholm U. Stockholm U., OKC Asquith Lily Argonne Assamagan Ketevi Brookhaven Astalos Robert Comenius U. Atkinson Markus Illinois U., Urbana Atlay Naim Bora Siegen U. Auerbach Benjamin Argonne Augsten Kamil Prague, Tech. U. Aurousseau Mathieu Johannesburg U. Avolio Giuseppe CERN Axen Bradley LBL, Berkeley Azuelos Georges Montreal U. TRIUMF Azuma Yuya Tokyo U., ICEPP Baak Max CERN Baas Alessandra Kirchhoff Inst. Phys. Bacci Cesare INFN, Rome Rome III U. Bachacou Henri IRFU, Saclay Bachas Konstantinos Aristotle U., Thessaloniki Backes Moritz CERN Backhaus Malte CERN Backus Mayes John SLAC Badescu Elisabeta Bucharest, IFIN-HH Bagiacchi Paolo INFN, Rome Rome U. Bagnaia Paolo INFN, Rome Rome U. Bai Yu Beijing, Inst. High Energy Phys. Bain Travis Nevis Labs, Columbia U. Baines John Rutherford Baker Oliver Keith Yale U. Balek Petr Charles U. Balli Fabrice IRFU, Saclay Banas Elzbieta Cracow, INP Banerjee Swagato Wisconsin U., Madison Bannoura Arwa A E Wuppertal U. Bansal Vikas Victoria U. Bansil Hardeep Singh Birmingham U. Barak Liron Weizmann Inst. Baranov Sergei Lebedev Inst. Barberio Elisabetta Luigia Melbourne U. Barberis Dario INFN, Genoa Genoa U. Barbero Marlon Marseille, CPPM Barillari Teresa Munich, Max Planck Inst. 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Beckingham Matthew Warwick U. Becot Cyril Orsay, LAL Beddall Andrew Gaziantep U. Beddall Ayda Gaziantep U. Bedikian Sourpouhi Yale U. Bednyakov Vadim Dubna, JINR Bee Christopher SUNY, Stony Brook Beemster Lars FOM, Amsterdam Beermann Thomas Wuppertal U. Begel Michael Brookhaven Behr Katharina Oxford U. Belanger-Champagne Camille McGill U. Bell Paul Geneva U. Bell William Geneva U. Bella Gideon Tel Aviv U. Bellagamba Lorenzo INFN, Bologna Bellerive Alain Carleton U. Bellomo Massimiliano Massachusetts U., Amherst Belotskiy Konstantin Moscow Phys. Eng. Inst. Beltramello Olga CERN Benary Odette Tel Aviv U. Benchekroun Driss Casablanca U. Bendtz Katarina Stockholm U. Stockholm U., OKC Benekos Nektarios Illinois U., Urbana Benhammou Yan Tel Aviv U. Benhar Noccioli Eleonora Geneva U. Benitez Garcia Jorge-Armando York U., Canada Benjamin Douglas Duke U. Bensinger James Brandeis U. Bentvelsen Stan FOM, Amsterdam Berge David FOM, Amsterdam Bergeaas Kuutmann Elin Uppsala U., Inst. Theor. Phys. Berger Nicolas Annecy, LAPP Berghaus Frank Victoria U. Beringer Jürg LBL, Berkeley Bernard Clare Boston U. Bernat Pauline University Coll. London Bernius Catrin Louisiana Tech. U. Bernlochner Florian Urs Victoria U. Berry Tracey Royal Holloway, U. of London Berta Peter Charles U. Bertella Claudia Marseille, CPPM Bertoli Gabriele Stockholm U. Stockholm U., OKC Bertolucci Federico INFN, Pisa Pisa U. Bertsche Carolyn Oklahoma U. Bertsche David Oklahoma U. Besana Maria Ilaria INFN, Milan Besjes Geert-Jan NIKHEF, Amsterdam Bessidskaia Olga Stockholm U. Stockholm U., OKC Bessner Martin Florian DESY Besson Nathalie IRFU, Saclay Betancourt Christopher Freiburg U. Bethke Siegfried Munich, Max Planck Inst. Bhimji Wahid Edinburgh U. Bianchi Riccardo-Maria Pittsburgh U. Bianchini Louis Brandeis U. Bianco Michele CERN Biebel Otmar Munich U. Bieniek Stephen Paul University Coll. London Bierwagen Katharina Gottingen U., II. Phys. Inst. 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Boisvert Veronique Royal Holloway, U. of London Bold Tomasz AGH-UST, Cracow Boldea Venera Bucharest, IFIN-HH Boldyrev Alexey Moscow State U. Bomben Marco Paris U., VI-VII Bona Marcella Queen Mary, U. of London Boonekamp Maarten IRFU, Saclay Borisov Anatoly Serpukhov, IHEP Borissov Guennadi Lancaster U. Borri Marcello Manchester U. Borroni Sara DESY Bortfeldt Jonathan Munich U. Bortolotto Valerio Hong Kong, Chinese U. Bos Kors FOM, Amsterdam Boscherini Davide INFN, Bologna Bosman Martine Barcelona, IFAE Boterenbrood Hendrik FOM, Amsterdam Boudreau Joseph Pittsburgh U. Bouffard Julian SUNY, Albany Bouhova-Thacker Evelina Vassileva Lancaster U. Boumediene Djamel Eddine Clermont-Ferrand U. Bourdarios Claire Orsay, LAL Bousson Nicolas Oklahoma State U. Boutouil Sara Oujda U. Boveia Antonio Chicago U., EFI Boyd James CERN Boyko Igor Dubna, JINR Bozic Ivan Belgrade U. Bracinik Juraj Birmingham U. Brandt Andrew Texas U., Arlington Brandt Gerhard LBL, Berkeley Brandt Oleg Kirchhoff Inst. Phys. Bratzler Uwe Tokyo Metropolitan U. Brau Benjamin Massachusetts U., Amherst Brau James Oregon U. Braun Helmut Wuppertal U. Brazzale Simone Federico INFN, Udine Udine U. Brelier Bertrand Toronto U. Brendlinger Kurt Pennsylvania U. Brennan Amelia Jean Melbourne U. Brenner Richard Uppsala U., Inst. Theor. Phys. Bressler Shikma Weizmann Inst. Bristow Kieran Witwatersrand U. Bristow Timothy Michael Edinburgh U. Britton Dave Glasgow U. Brochu Frederic Cambridge U. Brock Ian Bonn U. Brock Raymond Michigan State U. Bromberg Carl Michigan State U. Bronner Johanna Munich, Max Planck Inst. Brooijmans Gustaaf Nevis Labs, Columbia U. Brooks Timothy Royal Holloway, U. of London Brooks William Santa Maria U., Valparaiso Brosamer Jacquelyn LBL, Berkeley Brost Elizabeth Oregon U. Brown Jonathan LPSC, Grenoble Bruckman de Renstrom Pawel Cracow, INP Bruncko Dusan Kosice, IEF Bruneliere Renaud Freiburg U. Brunet Sylvie Indiana U. 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London Butti Pierfrancesco FOM, Amsterdam Buttinger William Cambridge U. Buzatu Adrian Glasgow U. Byszewski Marcin Natl. Tech. U., Athens Cabrera Urbán Susana Valencia U., IFIC Caforio Davide INFN, Bologna Bologna U. Cakir Orhan Ankara U. Calafiura Paolo LBL, Berkeley Calandri Alessandro IRFU, Saclay Calderini Giovanni Paris U., VI-VII Calfayan Philippe Munich U. Calkins Robert Northern Illinois U. Caloba Luiz Rio de Janeiro Federal U. Calvet David Clermont-Ferrand U. Calvet Samuel Clermont-Ferrand U. Camacho Toro Reina Geneva U. Camarda Stefano DESY Cameron David Oslo U. Caminada Lea Michaela LBL, Berkeley Caminal Armadans Roger Barcelona, IFAE Campana Simone CERN Campanelli Mario University Coll. London Campoverde Angel SUNY, Stony Brook Canale Vincenzo INFN, Naples Naples U. Canepa Anadi TRIUMF Cano Bret Marc Queen Mary, U. of London Cantero Josu Madrid, Autonoma U. Cantrill Robert LIP, Lisbon Cao Tingting Southern Methodist U. Capeans Garrido Maria Del Mar CERN Caprini Irinel Bucharest, IFIN-HH Caprini Mihai Bucharest, IFIN-HH Capua Marcella INFN, Cosenza Calabria U. Caputo Regina Mainz U. Cardarelli Roberto INFN, Rome Carli Tancredi CERN Carlino Gianpaolo INFN, Naples Carminati Leonardo INFN, Milan Milan U. Caron Sascha NIKHEF, Amsterdam Carquin Edson Chile U., Catolica Carrillo-Montoya German D Witwatersrand U. Carter Janet Cambridge U. Carvalho João LIP, Lisbon Coimbra U. Casadei Diego University Coll. London Casado Maria Pilar Barcelona, IFAE Casolino Mirkoantonio Barcelona, IFAE Castaneda-Miranda Elizabeth Johannesburg U. Castelli Angelantonio FOM, Amsterdam Castillo Gimenez Victoria Valencia U., IFIC Castro Nuno Filipe LIP, Lisbon Catastini Pierluigi Harvard U., Phys. Dept. Catinaccio Andrea CERN Catmore James Oslo U. Cattai Ariella CERN Cattani Giordano INFN, Rome Rome U., Tor Vergata Caudron Julien Mainz U. Cavaliere Viviana Illinois U., Urbana Cavalli Donatella INFN, Milan Cavalli-Sforza Matteo Barcelona, IFAE Cavasinni Vincenzo INFN, Pisa Pisa U. Ceradini Filippo INFN, Rome Rome III U. Cerio Benjamin Duke U. Cerny Karel Charles U. Santiago Cerqueira Augusto Juiz de Fora U. Cerri Alessandro Sussex U. Cerrito Lucio Queen Mary, U. of London Cerutti Fabio LBL, Berkeley Cerv Matevz CERN Cervelli Alberto Bern U., LHEP Cetin Serkant Ali Dogus U., Kadikoy Chafaq Aziz Casablanca U. Chakraborty Dhiman Northern Illinois U. Chalupkova Ina Charles U. Chang Philip Illinois U., Urbana Chapleau Bertrand McGill U. Chapman John Derek Cambridge U. Charfeddine Driss Orsay, LAL Charlton Dave Birmingham U. Chau Chav Chhiv Toronto U. Chavez Barajas Carlos Alberto Sussex U. Cheatham Susan McGill U. Chegwidden Andrew Michigan State U. Chekanov Sergei Argonne Chekulaev Sergey TRIUMF Chelkov Gueorgui Dubna, JINR Tomsk State U. Chelstowska Magda Anna Michigan U. Chen Chunhui Iowa State U. Chen Hucheng Brookhaven Chen Karen SUNY, Stony Brook Chen Liming Shandong U. Marseille, CPPM Chen Shenjian Nanjing U. Chen Xin Tsinghua U., Beijing Chen Ye Kobe U. Chen Yujiao Nevis Labs, Columbia U. Cheng Hok Chuen Michigan U. Cheng Yangyang Chicago U., EFI Cheplakov Alexander Dubna, JINR Cherkaoui El Moursli Rajaa Mohammed V U., Agdal Chernyatin Valeriy Brookhaven Cheu Elliott Arizona U. Chevalier Laurent IRFU, Saclay Chiarella Vitaliano Frascati Chiefari Giovanni INFN, Naples Naples U. Childers John Taylor Argonne Chilingarov Alexandre Lancaster U. Chiodini Gabriele INFN, Lecce Chisholm Andrew Birmingham U. Chislett Rebecca Thalatta University Coll. London Chitan Adrian Bucharest, IFIN-HH Chizhov Mihail Dubna, JINR Chouridou Sofia Athens U. Chow Bonnie Kar Bo Munich U. Chromek-Burckhart Doris CERN Chu Ming-Lee Taiwan, Inst. Phys. Chudoba Jiri Prague, Inst. Phys. Chwastowski Janusz Cracow, INP Chytka Ladislav Palacky U. Ciapetti Guido INFN, Rome Rome U. Ciftci Abbas Kenan Ankara U. Ciftci Rena Ankara U. Cinca Diane Glasgow U. Cindro Vladimir Stefan Inst., Ljubljana Ciocio Alessandra LBL, Berkeley Citron Zvi Hirsh Weizmann Inst. Citterio Mauro INFN, Milan Ciubancan Mihai Bucharest, IFIN-HH Clark Allan G Geneva U. Clark Philip James Edinburgh U. Clarke Robert LBL, Berkeley Cleland Bill Pittsburgh U. Clemens Jean-Claude Marseille, CPPM Clement Christophe Stockholm U. Stockholm U., OKC Coadou Yann Marseille, CPPM Cobal Marina INFN, Udine Udine U. Coccaro Andrea Washington U., Seattle Cochran James H Iowa State U. Coffey Laurel Brandeis U. Cogan Joshua Godfrey SLAC Cole Brian Nevis Labs, Columbia U. Cole Stephen Northern Illinois U. Colijn Auke-Pieter FOM, Amsterdam Collot Johann LPSC, Grenoble Colombo Tommaso Heidelberg U. Compostella Gabriele Munich, Max Planck Inst. Conde Muiño Patricia LIP, Lisbon Lisbon U., CFNUL Coniavitis Elias Freiburg U. Connell Simon Henry Johannesburg U. Connelly Ian Royal Holloway, U. of London Consonni Sofia Maria INFN, Milan Milan U. Consorti Valerio Freiburg U. Constantinescu Serban Bucharest, IFIN-HH Conta Claudio INFN, Pavia Pavia U. Conti Geraldine Harvard U., Phys. Dept. Conventi Francesco INFN, Naples Naples, Inst. U. Navale Cooke Mark LBL, Berkeley Cooper Ben University Coll. London Cooper-Sarkar Amanda Oxford U. Cooper-Smith Neil Royal Holloway, U. of London Copic Katherine LBL, Berkeley Cornelissen Thijs Wuppertal U. Corradi Massimo INFN, Bologna Corriveau Francois McGill U. IPP, Canada Corso-Radu Alina UC, Irvine Cortes-Gonzalez Arely Barcelona, IFAE Cortiana Giorgio Munich, Max Planck Inst. Costa Giuseppe INFN, Milan Costa María José Valencia U., IFIC Costanzo Davide Sheffield U. Côté David Texas U., Arlington Cottin Giovanna Cambridge U. Cowan Glen Royal Holloway, U. of London Cox Brian Manchester U. Cranmer Kyle New York U. Cree Graham Carleton U. Crépé-Renaudin Sabine LPSC, Grenoble Crescioli Francesco Paris U., VI-VII Cribbs Wayne Allen Stockholm U. Stockholm U., OKC Crispin Ortuzar Mireia Oxford U. Cristinziani Markus Bonn U. Croft Vince NIKHEF, Amsterdam Crosetti Giovanni INFN, Cosenza Calabria U. Cuciuc Constantin-Mihai Bucharest, IFIN-HH Cuhadar Donszelmann Tulay Sheffield U. Cummings Jane Yale U. Curatolo Maria Frascati Cuthbert Cameron Sydney U. Czirr Hendrik Siegen U. Czodrowski Patrick Alberta U. D'Auria Saverio Glasgow U. D'Onofrio Monica Liverpool U. Da Cunha Sargedas De Sousa Mario Jose LIP, Lisbon Lisbon U., CFNUL Da Via Cinzia Manchester U. Dabrowski Wladyslaw AGH-UST, Cracow Dafinca Alexandru Oxford U. Dai Tiesheng Michigan U. Dale Orjan Bergen U. Dallaire Frederick Montreal U. Dallapiccola Carlo Massachusetts U., Amherst Dam Mogens Bohr Inst. Daniells Andrew Christopher Birmingham U. Dano Hoffmann Maria IRFU, Saclay Dao Valerio Freiburg U. Darbo Giovanni INFN, Genoa Darmora Smita Texas U., Arlington Dassoulas James DESY Dattagupta Aparajita Indiana U. Davey Will Bonn U. David Claire Victoria U. Davidek Tomas Charles U. Davies Eleanor Oxford U. Rutherford Davies Merlin Tel Aviv U. Davignon Olivier Paris U., VI-VII Davison Adam University Coll. London Davison Peter University Coll. London Davygora Yuriy Kirchhoff Inst. Phys. Dawe Edmund Simon Fraser U. Dawson Ian Sheffield U. Daya-Ishmukhametova Rozmin Massachusetts U., Amherst De Kaushik Texas U., Arlington de Asmundis Riccardo INFN, Naples De Castro Stefano INFN, Bologna Bologna U. De Cecco Sandro Paris U., VI-VII De Groot Nicolo NIKHEF, Amsterdam de Jong Paul FOM, Amsterdam De la Torre Hector Madrid, Autonoma U. De Lorenzi Francesco Iowa State U. De Nooij Lucie FOM, Amsterdam De Pedis Daniele INFN, Rome De Salvo Alessandro INFN, Rome De Sanctis Umberto Sussex U. De Santo Antonella Sussex U. De Vivie De Regie Jean-Baptiste Orsay, LAL Dearnaley William James Lancaster U. Debbe Ramiro Brookhaven Debenedetti Chiara UC, Santa Cruz Dechenaux Benjamin LPSC, Grenoble Dedovich Dmitri Dubna, JINR Deigaard Ingrid FOM, Amsterdam Del Peso Jose Madrid, Autonoma U. Del Prete Tarcisio INFN, Pisa Pisa U. Deliot Frederic IRFU, Saclay Delitzsch Chris Malena Geneva U. Deliyergiyev Maksym Stefan Inst., Ljubljana Dell'Acqua Andrea CERN Dell'Asta Lidia Boston U. Dell'Orso Mauro INFN, Pisa Pisa U. Della Pietra Massimo INFN, Naples Naples, Inst. U. Navale della Volpe Domenico Geneva U. Delmastro Marco Annecy, LAPP Delsart Pierre-Antoine LPSC, Grenoble Deluca Carolina FOM, Amsterdam DeMarco David Toronto U. Demers Sarah Yale U. Demichev Mikhail Dubna, JINR Demilly Aurelien Paris U., VI-VII Denisov Sergey Serpukhov, IHEP Derendarz Dominik Cracow, INP Derkaoui Jamal Eddine Oujda U. Derue Frederic Paris U., VI-VII Dervan Paul Liverpool U. Desch Klaus Kurt Bonn U. Deterre Cecile DESY Deviveiros Pier-Olivier FOM, Amsterdam Dewhurst Alastair Rutherford Dhaliwal Saminder FOM, Amsterdam Di Ciaccio Anna INFN, Rome Rome U., Tor Vergata Di Ciaccio Lucia Annecy, LAPP Di Domenico Antonio INFN, Rome Rome U. Di Donato Camilla INFN, Naples Naples U. Di Girolamo Alessandro CERN Di Girolamo Beniamino CERN Di Mattia Alessandro Technion Di Micco Biagio INFN, Rome Rome III U. Di Nardo Roberto Frascati Di Simone Andrea Freiburg U. Di Sipio Riccardo INFN, Bologna Bologna U. Di Valentino David Carleton U. Dias Flavia Edinburgh U. Diaz Marco Aurelio Chile U., Catolica Diehl Edward Michigan U. Dietrich Janet DESY Dietzsch Thorsten Kirchhoff Inst. Phys. Diglio Sara Marseille, CPPM Dimitrievska Aleksandra Belgrade U. Dingfelder Jochen Bonn U. Dita Petre Bucharest, IFIN-HH Dita Sanda Bucharest, IFIN-HH Dittus Fridolin CERN Djama Fares Marseille, CPPM Djobava Tamar Tbilisi State U. Djuvsland Julia Isabell Kirchhoff Inst. Phys. Barros do Vale Maria Aline Sao Joao del-Rei Fed. U. Do Valle Wemans André LIP, Lisbon New Lisbon U. Dobos Daniel CERN Doglioni Caterina Geneva U. Doherty Tom Glasgow U. Dohmae Takeshi Tokyo U., ICEPP Dolejsi Jiri Charles U. Dolezal Zdenek Charles U. Dolgoshein Boris Moscow Phys. Eng. Inst. Donadelli Marisilvia Sao Paulo U. Donati Simone INFN, Pisa Pisa U. Dondero Paolo INFN, Pavia Pavia U. Donini Julien Clermont-Ferrand U. Dopke Jens Rutherford Doria Alessandra INFN, Naples Dova Maria-Teresa La Plata U. Doyle Tony Glasgow U. Dris Manolis Natl. Tech. U., Athens Dubbert Jörg Michigan U. Dube Sourabh LBL, Berkeley Dubreuil Emmanuelle Clermont-Ferrand U. Duchovni Ehud Weizmann Inst. Duckeck Guenter Munich U. Ducu Otilia Anamaria Bucharest, IFIN-HH Duda Dominik Wuppertal U. Dudarev Alexey CERN Dudziak Fanny Iowa State U. Duflot Laurent Orsay, LAL Duguid Liam Royal Holloway, U. of London Dührssen Michael CERN Dunford Monica Kirchhoff Inst. Phys. Duran Yildiz Hatice Ankara U. Düren Michael Giessen U. Durglishvili Archil Tbilisi State U. Dwuznik Michal AGH-UST, Cracow Dyndal Mateusz AGH-UST, Cracow Ebke Johannes Munich U. Edson William SUNY, Albany Edwards Nicholas Charles Edinburgh U. Ehrenfeld Wolfgang Bonn U. Eifert Till SLAC Eigen Gerald Bergen U. Einsweiler Kevin LBL, Berkeley Ekelof Tord Uppsala U., Inst. Theor. Phys. El Kacimi Mohamed Cadi Ayyad U., Marrakech Ellert Mattias Uppsala U., Inst. Theor. Phys. Elles Sabine Annecy, LAPP Ellinghaus Frank Mainz U. Ellis Nicolas CERN Elmsheuser Johannes Munich U. Elsing Markus CERN Emeliyanov Dmitry Rutherford Enari Yuji Tokyo U., ICEPP Endner Oliver Chris Mainz U. Endo Masaki Osaka U. Engelmann Roderich SUNY, Stony Brook Erdmann Johannes Yale U. Ereditato Antonio Bern U., LHEP Eriksson Daniel Stockholm U. Ernis Gunar Wuppertal U. Ernst Jesse SUNY, Albany Ernst Michael Brookhaven Ernwein Jean IRFU, Saclay Errede Deborah Illinois U., Urbana Errede Steven Illinois U., Urbana Ertel Eugen Mainz U. Escalier Marc Orsay, LAL Esch Hendrik Dortmund U. Escobar Carlos Pittsburgh U. Esposito Bellisario Frascati Etienvre Anne-Isabelle IRFU, Saclay Etzion Erez Tel Aviv U. Evans Hal Indiana U. Ezhilov Alexey St. Petersburg, INP Fabbri Laura INFN, Bologna Bologna U. Facini Gabriel Chicago U., EFI Fakhrutdinov Rinat Serpukhov, IHEP Falciano Speranza INFN, Rome Falla Rebecca Jane University Coll. London Faltova Jana Charles U. Fang Yaquan Beijing, Inst. High Energy Phys. Fanti Marcello INFN, Milan Milan U. Farbin Amir Texas U., Arlington Farilla Addolorata INFN, Rome Farooque Trisha Barcelona, IFAE Farrell Steven LBL, Berkeley Farrington Sinead Warwick U. Farthouat Philippe CERN Fassi Farida Mohammed V U., Agdal Fassnacht Patrick CERN Fassouliotis Dimitrios Athens U. Favareto Andrea INFN, Genoa Genoa U. Fayard Louis Orsay, LAL Federic Pavol Comenius U. Fedin Oleg St. Petersburg, INP St. Petersburg Polytechnic Inst. Fedorko Wojciech British Columbia U. Fehling-Kaschek Mirjam Freiburg U. Feigl Simon CERN Feligioni Lorenzo Marseille, CPPM Feng Cunfeng Shandong U. Feng Eric Argonne Feng Haolu Michigan U. Fenyuk Alexander Serpukhov, IHEP Fernandez Perez Sonia CERN Ferrag Samir Glasgow U. Ferrando James Glasgow U. Ferrari Arnaud Uppsala U., Inst. Theor. Phys. Ferrari Pamela FOM, Amsterdam Ferrari Roberto INFN, Pavia Ferreira de Lima Danilo Enoque Glasgow U. Ferrer Antonio Valencia U., IFIC Ferrere Didier Geneva U. Ferretti Claudio Michigan U. Ferretto Parodi Andrea INFN, Genoa Genoa U. Fiascaris Maria Chicago U., EFI Fiedler Frank Mainz U. Filipčič Andrej Stefan Inst., Ljubljana Filipuzzi Marco DESY Filthaut Frank NIKHEF, Amsterdam Fincke-Keeler Margret Victoria U. Finelli Kevin Daniel Sydney U. Fiolhais Miguel LIP, Lisbon Coimbra U. Fiorini Luca Valencia U., IFIC Firan Ana Southern Methodist U. Fischer Adam SUNY, Albany Fischer Julia Wuppertal U. Fisher Wade Cameron Michigan State U. Fitzgerald Eric Andrew Brandeis U. Flechl Martin Freiburg U. Fleck Ivor Siegen U. Fleischmann Philipp Michigan U. Fleischmann Sebastian Wuppertal U. Fletcher Gareth Thomas Sheffield U. Fletcher Gregory Queen Mary, U. of London Flick Tobias Wuppertal U. Floderus Anders Lund U. Flores Castillo Luis Hong Kong, Chinese U. Florez Bustos Andres Carlos York U., Canada Flowerdew Michael Munich, Max Planck Inst. Formica Andrea IRFU, Saclay Forti Alessandra Manchester U. Fortin Dominique TRIUMF Fournier Daniel Orsay, LAL Fox Harald Lancaster U. Fracchia Silvia Barcelona, IFAE Francavilla Paolo Paris U., VI-VII Franchini Matteo INFN, Bologna Bologna U. Franchino Silvia CERN Francis David CERN Franconi Laura Oslo U. Franklin Melissa Harvard U., Phys. Dept. Franz Sebastien Innsbruck U. Fraternali Marco INFN, Pavia Pavia U. French Sky Cambridge U. Friedrich Conrad DESY Friedrich Felix Dresden, Tech. U. Froidevaux Daniel CERN Frost James Cambridge U. Fukunaga Chikara Tokyo Metropolitan U. Fullana Torregrosa Esteban Mainz U. Fulsom Bryan Gregory SLAC Fuster Juan Valencia U., IFIC Gabaldon Carolina LPSC, Grenoble Gabizon Ofir Wuppertal U. Gabrielli Alessandro INFN, Bologna Bologna U. Gabrielli Andrea INFN, Rome Rome U. Gadatsch Stefan FOM, Amsterdam Gadomski Szymon Geneva U. Gagliardi Guido INFN, Genoa Genoa U. Gagnon Pauline Indiana U. Galea Cristina NIKHEF, Amsterdam Galhardo Bruno LIP, Lisbon Coimbra U. Gallas Elizabeth Oxford U. Gallo Valentina Santina Bern U., LHEP Gallop Bruce Rutherford Gallus Petr Prague, Tech. U. Galster Gorm Aske Gram Krohn Bohr Inst. Gan KK Ohio State U. Gao Jun Hefei, CUST Marseille, CPPM Gao Yongsheng SLAC Fresno State Garay Walls Francisca Edinburgh U. Garberson Ford Yale U. García Carmen Valencia U., IFIC García Navarro José Enrique Valencia U., IFIC Garcia-Sciveres Maurice LBL, Berkeley Gardner Robert Chicago U., EFI Garelli Nicoletta SLAC Garonne Vincent CERN Gatti Claudio Frascati Gaudio Gabriella INFN, Pavia Gaur Bakul Siegen U. Gauthier Lea Montreal U. Gauzzi Paolo INFN, Rome Rome U. Gavrilenko Igor Lebedev Inst. Gay Colin British Columbia U. Gaycken Goetz Bonn U. Gazis Evangelos Natl. Tech. U., Athens Ge Peng Shandong U. Gecse Zoltan British Columbia U. Gee Norman Rutherford Geerts Daniël Alphonsus Adrianus FOM, Amsterdam Geich-Gimbel Christoph Bonn U. Gellerstedt Karl Stockholm U. Stockholm U., OKC Gemme Claudia INFN, Genoa Gemmell Alistair Glasgow U. Genest Marie-Hélène LPSC, Grenoble Gentile Simonetta INFN, Rome Rome U. George Matthias Gottingen U., II. Phys. Inst. George Simon Royal Holloway, U. of London Gerbaudo Davide UC, Irvine Gershon Avi Tel Aviv U. Ghazlane Hamid CNESTEN, Rabat Ghodbane Nabil Clermont-Ferrand U. Giacobbe Benedetto INFN, Bologna Giagu Stefano INFN, Rome Rome U. Giangiobbe Vincent Barcelona, IFAE Giannetti Paola INFN, Pisa Pisa U. Gianotti Fabiola CERN Gibbard Bruce Brookhaven Gibson Stephen Royal Holloway, U. of London Gilchriese Murdock LBL, Berkeley Gillam Thomas Cambridge U. Gillberg Dag CERN Gilles Geoffrey Clermont-Ferrand U. Gingrich Douglas Alberta U. TRIUMF Giokaris Nikos Athens U. Giordani MarioPaolo INFN, Udine Udine U. Giordano Raffaele INFN, Naples Naples U. Giorgi Filippo Maria INFN, Bologna Giorgi Francesco Michelangelo Humboldt U., Berlin Giraud Pierre-Francois IRFU, Saclay Giugni Danilo INFN, Milan Giuliani Claudia Freiburg U. Giulini Maddalena Heidelberg U. Gjelsten Børge Kile Oslo U. Gkaitatzis Stamatios Aristotle U., Thessaloniki Gkialas Ioannis Aristotle U., Thessaloniki Aegean U., Chios Gkougkousis Evangelos Leonidas Orsay, LAL Gladilin Leonid Moscow State U. Glasman Claudia Madrid, Autonoma U. Glatzer Julian CERN Glaysher Paul Edinburgh U. Glazov Alexandre DESY Glonti George Dubna, JINR Goblirsch-Kolb Maximilian Munich, Max Planck Inst. Goddard Jack Robert Queen Mary, U. of London Godlewski Jan CERN Goeringer Christian Mainz U. Goldfarb Steven Michigan U. Golling Tobias Yale U. Golubkov Dmitry Serpukhov, IHEP Gomes Agostinho LIP, Lisbon Lisbon U., CFNUL Gomez Fajardo Luz Stella DESY Gonçalo Ricardo LIP, Lisbon Goncalves Pinto Firmino Da Costa Joao IRFU, Saclay Gonella Laura Bonn U. González de la Hoz Santiago Valencia U., IFIC Gonzalez Parra Garoe Barcelona, IFAE Gonzalez-Sevilla Sergio Geneva U. Goossens Luc CERN Gorbounov Petr Andreevich Moscow, ITEP Gordon Howard Brookhaven Gorelov Igor New Mexico U. Gorini Benedetto CERN Gorini Edoardo INFN, Lecce Salento U. Gorišek Andrej Stefan Inst., Ljubljana Gornicki Edward Cracow, INP Goshaw Alfred Argonne Gössling Claus Dortmund U. Gostkin Mikhail Ivanovitch Dubna, JINR Gouighri Mohamed Casablanca U. Goujdami Driss Cadi Ayyad U., Marrakech Goulette Marc Phillippe Geneva U. Goussiou Anna Washington U., Seattle Goy Corinne Annecy, LAPP Grabas Herve Marie Xavier UC, Santa Cruz Graber Lars Gottingen U., II. Phys. Inst. Grabowska-Bold Iwona AGH-UST, Cracow Grafström Per INFN, Bologna Bologna U. Grahn Karl-Johan DESY Gramling Johanna Geneva U. Gramstad Eirik Oslo U. Grancagnolo Sergio Humboldt U., Berlin Grassi Valerio SUNY, Stony Brook Gratchev Vadim St. Petersburg, INP Gray Heather CERN Graziani Enrico INFN, Rome Grebenyuk Oleg St. Petersburg, INP Greenwood Zeno Dixon Louisiana Tech. U. Gregersen Kristian University Coll. London Gregor Ingrid-Maria DESY Grenier Philippe SLAC Griffiths Justin Texas U., Arlington Grillo Alexander UC, Santa Cruz Grimm Kathryn Lancaster U. Grinstein Sebastian Barcelona, IFAE ICREA, Barcelona Gris Philippe Luc Yves Clermont-Ferrand U. Grishkevich Yaroslav Moscow State U. Grivaz Jean-Francois Orsay, LAL Grohs Johannes Philipp Dresden, Tech. U. Grohsjean Alexander DESY Gross Eilam Weizmann Inst. Grosse-Knetter Joern Gottingen U., II. Phys. Inst. Grossi Giulio Cornelio INFN, Rome Rome U., Tor Vergata Groth-Jensen Jacob Weizmann Inst. Grout Zara Jane Sussex U. Guan Liang Hefei, CUST Guenther Jaroslav Prague, Tech. U. Guescini Francesco Geneva U. Guest Daniel Yale U. Gueta Orel Tel Aviv U. Guicheney Christophe Clermont-Ferrand U. Guido Elisa INFN, Genoa Genoa U. Guillemin Thibault Orsay, LAL Guindon Stefan SUNY, Albany Gul Umar Glasgow U. Gumpert Christian Dresden, Tech. U. Guo Jun Nevis Labs, Columbia U. Gupta Shaun Oxford U. Gutierrez Phillip Oklahoma U. Gutierrez Ortiz Nicolas Gilberto Glasgow U. Gutschow Christian University Coll. London Guttman Nir Tel Aviv U. Guyot Claude IRFU, Saclay Gwenlan Claire Oxford U. Gwilliam Carl Liverpool U. Haas Andy New York U. Haber Carl LBL, Berkeley Hadavand Haleh Khani Texas U., Arlington Haddad Nacim Mohammed V U., Agdal Haefner Petra Bonn U. Hageböck Stephan Bonn U. Hajduk Zbigniew Cracow, INP Hakobyan Hrachya Yerevan Phys. Inst. Haleem Mahsana DESY Hall David Oxford U. Halladjian Garabed Michigan State U. Hamacher Klaus Wuppertal U. Hamal Petr Palacky U. Hamano Kenji Victoria U. Hamer Matthias Gottingen U., II. Phys. Inst. Hamilton Andrew Cape Town U. Hamilton Samuel Tufts U. Hamity Guillermo Nicolas Witwatersrand U. Hamnett Phillip George DESY Han Liang Hefei, CUST Hanagaki Kazunori Osaka U. Hanawa Keita Tokyo U., ICEPP Hance Michael LBL, Berkeley Hanke Paul Kirchhoff Inst. Phys. Hanna Remie IRFU, Saclay Hansen Jørgen Beck Bohr Inst. Hansen Jorn Dines Bohr Inst. Hansen Peter Henrik Bohr Inst. Hara Kazuhiko Tsukuba U. Hard Andrew Wisconsin U., Madison Harenberg Torsten Wuppertal U. Hariri Faten Orsay, LAL Harkusha Siarhei Minsk, Inst. Phys. Harper Devin Michigan U. Harrington Robert Edinburgh U. Harris Orin Washington U., Seattle Harrison Paul Fraser Warwick U. Hartjes Fred FOM, Amsterdam Hasegawa Makoto Kobe U. Hasegawa Satoshi Nagoya U. Hasegawa Yoji Shinshu U. Hasib A Oklahoma U. Hassani Samira IRFU, Saclay Haug Sigve Bern U., LHEP Hauschild Michael CERN Hauser Reiner Michigan State U. Hauswald Lorenz Dresden, Tech. U. Havranek Miroslav Prague, Inst. Phys. Hawkes Christopher Birmingham U. Hawkings Richard John CERN Hawkins Anthony David Lund U. Hayashi Takayasu Tsukuba U. Hayden Daniel Michigan State U. Hays Chris Oxford U. Hayward Helen Liverpool U. Haywood Stephen Rutherford Head Simon Birmingham U. Heck Tobias Mainz U. Hedberg Vincent Lund U. Heelan Louise Texas U., Arlington Heim Sarah Pennsylvania U. Heim Timon Wuppertal U. Heinemann Beate LBL, Berkeley Heinrich Lukas New York U. Hejbal Jiri Prague, Inst. Phys. Helary Louis Boston U. Heller Claudio Munich U. Heller Matthieu CERN Hellman Sten Stockholm U. Stockholm U., OKC Hellmich Dennis Bonn U. Helsens Clement CERN Henderson James Oxford U. Henderson Robert Lancaster U. Heng Yang Wisconsin U., Madison Hengler Christopher DESY Henrichs Anna Yale U. Henriques Correia Ana Maria CERN Henrot-Versille Sophie Orsay, LAL Herbert Geoffrey Henry Humboldt U., Berlin Hernández Jiménez Yesenia Valencia U., IFIC Herrberg-Schubert Ruth Humboldt U., Berlin Herten Gregor Freiburg U. Hertenberger Ralf Munich U. Hervas Luis CERN Hesketh Gavin Grant University Coll. London Hessey Nigel FOM, Amsterdam Hickling Robert Queen Mary, U. of London Higón-Rodriguez Emilio Valencia U., IFIC Hill Ewan Victoria U. Hill John Cambridge U. Hiller Karl Heinz DESY Hillert Sonja Bonn U. Hillier Stephen Birmingham U. Hinchliffe Ian LBL, Berkeley Hines Elizabeth Pennsylvania U. Hirose Minoru Tokyo Inst. Tech. Hirschbuehl Dominic Wuppertal U. Hobbs John SUNY, Stony Brook Hod Noam FOM, Amsterdam Hodgkinson Mark Sheffield U. Hodgson Paul Sheffield U. Hoecker Andreas CERN Hoeferkamp Martin New Mexico U. Hoenig Friedrich Munich U. Hoffman Julia Southern Methodist U. Hoffmann Dirk Marseille, CPPM Hohlfeld Marc Mainz U. Holmes Tova Ray LBL, Berkeley Hong Tae Min Pennsylvania U. Hooft van Huysduynen Loek New York U. Hopkins Walter Oregon U. Horii Yasuyuki Nagoya U. Hostachy Jean-Yves LPSC, Grenoble Hou Suen Taiwan, Inst. Phys. Hoummada Abdeslam Casablanca U. Howard Jacob Oxford U. Howarth James DESY Hrabovsky Miroslav Palacky U. Hristova Ivana Humboldt U., Berlin Hrivnac Julius Orsay, LAL Hryn'ova Tetiana Annecy, LAPP Hsu Catherine Witwatersrand U. Hsu Pai-hsien Jennifer Mainz U. Hsu Shih-Chieh Washington U., Seattle Hu Diedi Nevis Labs, Columbia U. Hu Xueye Michigan U. Huang Yanping DESY Hubacek Zdenek CERN Hubaut Fabrice Marseille, CPPM Huegging Fabian Bonn U. Huffman Todd Brian Oxford U. Hughes Emlyn Nevis Labs, Columbia U. Hughes Gareth Lancaster U. Huhtinen Mika CERN Hülsing Tobias Alexander Mainz U. Hurwitz Martina LBL, Berkeley Huseynov Nazim Dubna, JINR Baku, Inst. Phys. Huston Joey Michigan State U. Huth John Harvard U., Phys. Dept. Iacobucci Giuseppe Geneva U. Iakovidis Georgios Natl. Tech. U., Athens Ibragimov Iskander Siegen U. Iconomidou-Fayard Lydia Orsay, LAL Ideal Emma Yale U. Idrissi Zineb Mohammed V U., Agdal Iengo Paolo INFN, Naples Igonkina Olga FOM, Amsterdam Iizawa Tomoya Waseda U. Ikegami Yoichi KEK, Tsukuba Ikematsu Katsumasa Siegen U. Ikeno Masahiro KEK, Tsukuba Ilchenko Iurii Chicago U., EFI Texas U. Iliadis Dimitrios Aristotle U., Thessaloniki Ilic Nikolina Toronto U. Inamaru Yuki Kobe U. Ince Tayfun Munich, Max Planck Inst. Ioannou Pavlos Athens U. Iodice Mauro INFN, Rome Iordanidou Kalliopi Athens U. Ippolito Valerio Harvard U., Phys. Dept. Irles Quiles Adrian Valencia U., IFIC Isaksson Charlie Uppsala U., Inst. Theor. Phys. Ishino Masaya Kyoto U. Ishitsuka Masaki Tokyo Inst. Tech. Ishmukhametov Renat Ohio State U. Issever Cigdem Oxford U. Istin Serhat Bogazici U. Iturbe Ponce Julia Mariana Manchester U. Iuppa Roberto INFN, Rome Rome U., Tor Vergata Ivarsson Jenny Lund U. Iwanski Wieslaw Cracow, INP Iwasaki Hiroyuki KEK, Tsukuba Izen Joseph Texas U., Dallas Izzo Vincenzo INFN, Naples Jackson Brett Pennsylvania U. Jackson Matthew Liverpool U. Jackson Paul Adelaide U., Sch. Chem. Phys. Jaekel Martin CERN Jain Vivek SUNY, Albany Jakobs Karl Freiburg U. Jakobsen Sune CERN Jakoubek Tomas Prague, Inst. Phys. Jakubek Jan Prague, Tech. U. Jamin David Olivier Taiwan, Inst. Phys. Jana Dilip Louisiana Tech. U. Jansen Eric University Coll. London Jansen Hendrik CERN Janssen Jens Bonn U. Janus Michel Warwick U. Jarlskog Göran Lund U. Javadov Namig Dubna, JINR Baku, Inst. Phys. Javůrek Tomáš Freiburg U. Jeanty Laura LBL, Berkeley Jejelava Juansher Tbilisi, Inst. Phys. Ilia State U. Jeng Geng-yuan Sydney U. Jennens David Melbourne U. Jenni Peter Freiburg U. CERN Jentzsch Jennifer Dortmund U. Jeske Carl Warwick U. Jézéquel Stéphane Annecy, LAPP Ji Haoshuang Wisconsin U., Madison Jia Jiangyong SUNY, Stony Brook Jiang Yi Hefei, CUST Jimenez Belenguer Marcos DESY Jin Shan Beijing, Inst. High Energy Phys. Jinaru Adam Bucharest, IFIN-HH Jinnouchi Osamu Tokyo Inst. Tech. Joergensen Morten Dam Bohr Inst. Johansson Erik Stockholm U. Stockholm U., OKC Johansson Per Sheffield U. Johns Kenneth Arizona U. Jon-And Kerstin Stockholm U. Stockholm U., OKC Jones Graham Warwick U. Jones Roger Lancaster U. Jones Tim Liverpool U. Jongmanns Jan Kirchhoff Inst. Phys. Jorge Pedro LIP, Lisbon Lisbon U., CFNUL Joshi Kiran Daniel Manchester U. Jovicevic Jelena Royal Inst. Tech., Stockholm Ju Xiangyang Wisconsin U., Madison Jung Christian Dortmund U. Jungst Ralph Markus CERN Jussel Patrick Innsbruck U. Juste Rozas Aurelio Barcelona, IFAE ICREA, Barcelona Kaci Mohammed Valencia U., IFIC Kaczmarska Anna Cracow, INP Kado Marumi Orsay, LAL Kagan Harris Ohio State U. Kagan Michael SLAC Kajomovitz Enrique Duke U. Kalderon Charles William Oxford U. Kama Sami Southern Methodist U. Kamenshchikov Andrey Serpukhov, IHEP Kanaya Naoko Tokyo U., ICEPP Kaneda Michiru CERN Kaneti Steven Cambridge U. Kantserov Vadim Moscow Phys. Eng. Inst. Kanzaki Junichi KEK, Tsukuba Kaplan Benjamin New York U. Kapliy Anton Chicago U., EFI Kar Deepak Glasgow U. Karakostas Konstantinos Natl. Tech. U., Athens Karastathis Nikolaos Natl. Tech. U., Athens Kareem Mohammad Jawad Gottingen U., II. Phys. Inst. Karnevskiy Mikhail Mainz U. Karpov Sergey Dubna, JINR Karpova Zoya Dubna, JINR Karthik Krishnaiyengar New York U. Kartvelishvili Vakhtang Lancaster U. Karyukhin Andrey Serpukhov, IHEP Kashif Lashkar Wisconsin U., Madison Kasieczka Gregor Heidelberg U. Kass Richard Ohio State U. Kastanas Alex Bergen U. Kataoka Yousuke Tokyo U., ICEPP Katre Akshay Geneva U. Katzy Judith DESY Kaushik Venkatesh Arizona U. Kawagoe Kiyotomo Kyushu U. Kawamoto Tatsuo Tokyo U., ICEPP Kawamura Gen Gottingen U., II. Phys. Inst. Kazama Shingo Tokyo U., ICEPP Kazanin Vassili Novosibirsk, IYF Kazarinov Makhail Dubna, JINR Keeler Richard Victoria U. Kehoe Robert Southern Methodist U. Keil Markus Gottingen U., II. Phys. Inst. Keller John DESY Kempster Jacob Julian Royal Holloway, U. of London Keoshkerian Houry Annecy, LAPP Kepka Oldrich Prague, Inst. Phys. Kerševan Borut Paul Stefan Inst., Ljubljana Kersten Susanne Wuppertal U. Kessoku Kohei Tokyo U., ICEPP Keung Justin Toronto U. Khalil-zada Farkhad Baku, Inst. Phys. Khandanyan Hovhannes Stockholm U. Stockholm U., OKC Khanov Alexander Oklahoma State U. Khodinov Alexander Moscow Phys. Eng. Inst. Khomich Andrei Kirchhoff Inst. Phys. Khoo Teng Jian Cambridge U. Khoriauli Gia Bonn U. Khoroshilov Andrey Wuppertal U. Khovanskiy Valery Moscow, ITEP Khramov Evgeniy Dubna, JINR Khubua Jemal Tbilisi State U. Kim Hee Yeun Texas U., Arlington Kim Hyeon Jin Stockholm U. Stockholm U., OKC Kim Shinhong Tsukuba U. Kimura Naoki Waseda U. Kind Oliver Humboldt U., Berlin King Barry Liverpool U. King Matthew Valencia U., IFIC King Robert Steven Beaufoy Oxford U. King Samuel Burton British Columbia U. Kirk Julie Rutherford Kiryunin Andrey Munich, Max Planck Inst. Kishimoto Tomoe Kobe U. Kisielewska Danuta AGH-UST, Cracow Kiss Florian Freiburg U. Kiuchi Kenji Tsukuba U. Kladiva Eduard Kosice, IEF Klein Max Liverpool U. Klein Uta Liverpool U. Kleinknecht Konrad Mainz U. Klimek Pawel Stockholm U. Stockholm U., OKC Klimentov Alexei Brookhaven Klingenberg Reiner Dortmund U. Klinger Joel Alexander Manchester U. Klioutchnikova Tatiana CERN Klok Peter NIKHEF, Amsterdam Kluge Eike-Erik Kirchhoff Inst. Phys. Kluit Peter FOM, Amsterdam Kluth Stefan Munich, Max Planck Inst. Kneringer Emmerich Innsbruck U. Knoops Edith Marseille, CPPM Knue Andrea Glasgow U. Kobayashi Dai Tokyo Inst. Tech. Kobayashi Tomio Tokyo U., ICEPP Kobel Michael Dresden, Tech. U. Kocian Martin SLAC Kodys Peter Charles U. Koffas Thomas Carleton U. Koffeman Els FOM, Amsterdam Kogan Lucy Anne Oxford U. Kohlmann Simon Wuppertal U. Kohout Zdenek Prague, Tech. U. Kohriki Takashi KEK, Tsukuba Koi Tatsumi SLAC Kolanoski Hermann Humboldt U., Berlin Koletsou Iro Annecy, LAPP Koll James Michigan State U. Komar Aston Lebedev Inst. Komori Yuto Tokyo U., ICEPP Kondo Takahiko KEK, Tsukuba Kondrashova Nataliia DESY Köneke Karsten Freiburg U. König Adriaan NIKHEF, Amsterdam König Sebastian Mainz U. 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Lloyd Stephen Queen Mary, U. of London Lo Sterzo Francesco Taiwan, Inst. Phys. Lobodzinska Ewelina DESY Loch Peter Arizona U. Lockman William UC, Santa Cruz Loebinger Fred Manchester U. Loevschall-Jensen Ask Emil Bohr Inst. Loginov Andrey Yale U. Lohse Thomas Humboldt U., Berlin Lohwasser Kristin DESY Lokajicek Milos Prague, Inst. Phys. Lombardo Vincenzo Paolo Annecy, LAPP Long Brian Alexander Boston U. Long Jonathan Michigan U. Long Robin Eamonn Lancaster U. Lopes Lourenco LIP, Lisbon Lopez Mateos David Harvard U., Phys. Dept. Lopez Paredes Brais Sheffield U. Lopez Paz Ivan Barcelona, IFAE Lorenz Jeanette Munich U. Lorenzo Martinez Narei Indiana U. Losada Marta Antonio Narino U. Loscutoff Peter LBL, Berkeley Lou XinChou Texas U., Dallas Lounis Abdenour Orsay, LAL Love Jeremy Argonne Love Peter Lancaster U. Lowe Andrew SLAC Fresno State Lu Feng Beijing, Inst. High Energy Phys. Lu Nan Michigan U. Lubatti Henry Washington U., Seattle Luci Claudio INFN, Rome Rome U. 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Mapelli Livio CERN March Luis Witwatersrand U. Marchand Jean-Francois Carleton U. Marchiori Giovanni Paris U., VI-VII Marcisovsky Michal Prague, Inst. Phys. Marino Christopher Victoria U. Marjanovic Marija Belgrade U. Marques Carlos LIP, Lisbon Marroquim Fernando Rio de Janeiro Federal U. Marsden Stephen Philip Manchester U. Marshall Zach LBL, Berkeley Marti Lukas Fritz Bern U., LHEP Marti-Garcia Salvador Valencia U., IFIC Martin Brian CERN Martin Brian Thomas Michigan State U. Martin Tim Warwick U. Martin Victoria Jane Edinburgh U. Martin dit Latour Bertrand Bergen U. Martinez Homero IRFU, Saclay Martinez Mario Barcelona, IFAE ICREA, Barcelona Martin-Haugh Stewart Rutherford Martyniuk Alex University Coll. London Marx Marilyn Washington U., Seattle Marzano Francesco INFN, Rome Marzin Antoine CERN Masetti Lucia Mainz U. Mashimo Tetsuro Tokyo U., ICEPP Mashinistov Ruslan Lebedev Inst. Masik Jiri Manchester U. Maslennikov Alexey Novosibirsk, IYF Novosibirsk State U. 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Milov Alexander Weizmann Inst. Milstead David Stockholm U. Stockholm U., OKC Milstein Dmitry Weizmann Inst. Minaenko Andrey Serpukhov, IHEP Minami Yuto Tokyo U., ICEPP Minashvili Irakli Dubna, JINR Mincer Allen New York U. Mindur Bartosz AGH-UST, Cracow Mineev Mikhail Dubna, JINR Ming Yao Wisconsin U., Madison Mir Lluisa-Maria Barcelona, IFAE Mirabelli Giovanni INFN, Rome Mitani Takashi Waseda U. Mitrevski Jovan Munich U. Mitsou Vasiliki A Valencia U., IFIC Miucci Antonio Geneva U. Miyagawa Paul Sheffield U. Mjörnmark Jan-Ulf Lund U. Moa Torbjoern Stockholm U. Stockholm U., OKC Mochizuki Kazuya Marseille, CPPM Mohapatra Soumya Nevis Labs, Columbia U. Mohr Wolfgang Freiburg U. Molander Simon Stockholm U. Stockholm U., OKC Moles-Valls Regina Valencia U., IFIC Mönig Klaus DESY Monini Caterina LPSC, Grenoble Monk James Bohr Inst. Monnier Emmanuel Marseille, CPPM Montejo Berlingen Javier Barcelona, IFAE Monticelli Fernando La Plata U. Monzani Simone INFN, Rome Rome U. 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Nodulman Lawrence Argonne Nomachi Masaharu Osaka U. Nomidis Ioannis Carleton U. Norberg Scarlet Oklahoma U. Nordberg Markus CERN Novgorodova Olga Dresden, Tech. U. Nowak Sebastian Munich, Max Planck Inst. Nozaki Mitsuaki KEK, Tsukuba Nozka Libor Palacky U. Ntekas Konstantinos Natl. Tech. U., Athens Nunes Hanninger Guilherme Melbourne U. Nunnemann Thomas Munich U. Nurse Emily University Coll. London Nuti Francesco Melbourne U. O'Brien Brendan Joseph Edinburgh U. O'grady Fionnbarr Arizona U. O'Neil Dugan Simon Fraser U. O'Shea Val Glasgow U. Oakham Gerald Carleton U. TRIUMF Oberlack Horst Munich, Max Planck Inst. Obermann Theresa Bonn U. Ocariz Jose Paris U., VI-VII Ochi Atsuhiko Kobe U. Ochoa Ines University Coll. London Oda Susumu Kyushu U. Odaka Shigeru KEK, Tsukuba Ogren Harold Indiana U. Oh Alexander Manchester U. Oh Seog Duke U. Ohm Christian LBL, Berkeley Ohman Henrik Uppsala U., Inst. Theor. Phys. Oide Hideyuki CERN Okamura Wataru Osaka U. 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U., Athens Papageorgiou Konstantinos Aristotle U., Thessaloniki Aegean U., Chios Paramonov Alexander Argonne Paredes Hernandez Daniela Aristotle U., Thessaloniki Parker Michael Andrew Cambridge U. Parodi Fabrizio INFN, Genoa Genoa U. Parsons John Nevis Labs, Columbia U. Parzefall Ulrich Freiburg U. Pasqualucci Enrico INFN, Rome Passaggio Stefano INFN, Genoa Passeri Antonio INFN, Rome Pastore Fernanda INFN, Rome Rome III U. Pastore Francesca Royal Holloway, U. of London Pásztor Gabriella Carleton U. Pataraia Sophio Wuppertal U. Patel Nikhul Sydney U. Pater Joleen Manchester U. Patricelli Sergio INFN, Naples Naples U. Pauly Thilo CERN Pearce James Victoria U. Pedersen Lars Egholm Bohr Inst. Pedersen Maiken Oslo U. Pedraza Lopez Sebastian Valencia U., IFIC Pedro Rute LIP, Lisbon Lisbon U., CFNUL Peleganchuk Sergey Novosibirsk, IYF Pelikan Daniel Uppsala U., Inst. Theor. Phys. Peng Haiping Hefei, CUST Penning Bjoern Chicago U., EFI Penwell John Indiana U. Perepelitsa Dennis Brookhaven Perez Codina Estel TRIUMF Pérez García-Estañ María Teresa Valencia U., IFIC Perini Laura INFN, Milan Milan U. Pernegger Heinz CERN Perrella Sabrina INFN, Naples Naples U. Perrino Roberto INFN, Lecce Peschke Richard DESY Peshekhonov Vladimir Dubna, JINR Peters Krisztian CERN Peters Yvonne Manchester U. Petersen Brian CERN Petersen Troels Bohr Inst. Petit Elisabeth DESY Petridis Andreas Stockholm U. Stockholm U., OKC Petridou Chariclia Aristotle U., Thessaloniki Petrolo Emilio INFN, Rome Petrucci Fabrizio INFN, Rome Rome III U. Pettersson Nora Emilia Tokyo Inst. Tech. Pezoa Raquel Santa Maria U., Valparaiso Phillips Peter William Rutherford Piacquadio Giacinto SLAC Pianori Elisabetta Warwick U. Picazio Attilio Geneva U. Piccaro Elisa Queen Mary, U. of London Piccinini Maurizio INFN, Bologna Bologna U. Piegaia Ricardo Buenos Aires U. Pignotti David Ohio State U. Pilcher James Chicago U., EFI Pilkington Andrew University Coll. London Pina João Antonio LIP, Lisbon Lisbon U., CFNUL Pinamonti Michele INFN, Udine Udine U. SISSA, Trieste Pinder Alex Oxford U. Pinfold James Alberta U. Pingel Almut Bohr Inst. Pinto Belmiro LIP, Lisbon Pires Sylvestre Paris U., VI-VII Pitt Michael Weizmann Inst. Pizio Caterina INFN, Milan Milan U. Plazak Lukas Comenius U. Pleier Marc-Andre Brookhaven Pleskot Vojtech Charles U. Plotnikova Elena Dubna, JINR Plucinski Pawel Stockholm U. Stockholm U., OKC Pluth Daniel Iowa State U. Poddar Sahill Kirchhoff Inst. Phys. Podlyski Fabrice Clermont-Ferrand U. Poettgen Ruth Mainz U. Poggioli Luc Orsay, LAL Pohl David-leon Bonn U. Pohl Martin Geneva U. Polesello Giacomo INFN, Pavia Policicchio Antonio INFN, Cosenza Calabria U. Polifka Richard Toronto U. Polini Alessandro INFN, Bologna Pollard Christopher Samuel Duke U. Polychronakos Venetios Brookhaven Pommès Kathy CERN Pontecorvo Ludovico INFN, Rome Pope Bernard Michigan State U. Popeneciu Gabriel Alexandru INCDTIM, Cluj Napoca Popovic Dragan Belgrade U. Poppleton Alan CERN Portell Bueso Xavier Barcelona, IFAE Pospisil Stanislav Prague, Tech. U. Potamianos Karolos LBL, Berkeley Potrap Igor Dubna, JINR Potter Christina Sussex U. Potter Christopher Oregon U. Poulard Gilbert CERN Poveda Joaquin Indiana U. Pozdnyakov Valery Dubna, JINR Pralavorio Pascal Marseille, CPPM Pranko Aliaksandr LBL, Berkeley Prasad Srivas CERN Pravahan Rishiraj Texas U., Arlington Prell Soeren Iowa State U. Price Darren Manchester U. Price Joe Liverpool U. Price Lawrence Argonne Prieur Damien Pittsburgh U. Primavera Margherita INFN, Lecce Proissl Manuel Edinburgh U. Prokofiev Kirill Frascati Prokoshin Fedor Santa Maria U., Valparaiso Protopapadaki Eftychia-sofia IRFU, Saclay Protopopescu Serban Brookhaven Proudfoot James Argonne Przybycien Mariusz AGH-UST, Cracow Przysiezniak Helenka Annecy, LAPP Ptacek Elizabeth Oregon U. Puddu Daniele INFN, Rome Rome III U. 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Rebuzzi Daniela INFN, Pavia Pavia U. Redelbach Andreas Wurzburg U. Redlinger George Brookhaven Reece Ryan UC, Santa Cruz Reeves Kendall Texas U., Dallas Rehnisch Laura Humboldt U., Berlin Reisin Hernan Buenos Aires U. Relich Matthew UC, Irvine Rembser Christoph CERN Ren Huan Beijing, Inst. High Energy Phys. Ren Zhongliang Taiwan, Inst. Phys. Renaud Adrien Orsay, LAL Rescigno Marco INFN, Rome Resconi Silvia INFN, Milan Rezanova Olga Novosibirsk, IYF Novosibirsk State U. Reznicek Pavel Charles U. Rezvani Reyhaneh Montreal U. Richter Robert Munich, Max Planck Inst. Ridel Melissa Paris U., VI-VII Rieck Patrick Humboldt U., Berlin Rieger Julia Gottingen U., II. Phys. Inst. Rijssenbeek Michael SUNY, Stony Brook Rimoldi Adele INFN, Pavia Pavia U. Rinaldi Lorenzo INFN, Bologna Ritsch Elmar Innsbruck U. Riu Imma Barcelona, IFAE Rizatdinova Flera Oklahoma State U. Rizvi Eram Queen Mary, U. of London Robertson Steven McGill U. IPP, Canada Robichaud-Veronneau Andree McGill U. 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Rothberg Joseph Washington U., Seattle Rousseau David Orsay, LAL Royon Christophe IRFU, Saclay Rozanov Alexandre Marseille, CPPM Rozen Yoram Technion Ruan Xifeng Witwatersrand U. Rubbo Francesco Barcelona, IFAE Rubinskiy Igor DESY Rud Viacheslav Moscow State U. Rudolph Christian Dresden, Tech. U. Rudolph Matthew Scott Toronto U. Rühr Frederik Freiburg U. Ruiz-Martinez Aranzazu CERN Rurikova Zuzana Freiburg U. Rusakovich Nikolai Dubna, JINR Ruschke Alexander Munich U. Rutherfoord John Arizona U. Ruthmann Nils Freiburg U. Ryabov Yury St. Petersburg, INP Rybar Martin Charles U. Rybkin Grigori Orsay, LAL Ryder Nick Oxford U. Saavedra Aldo Sydney U. Sabato Gabriele FOM, Amsterdam Sacerdoti Sabrina Buenos Aires U. Saddique Asif Alberta U. Sadeh Iftach Tel Aviv U. Sadrozinski Hartmut UC, Santa Cruz Sadykov Renat Dubna, JINR Safai Tehrani Francesco INFN, Rome Sakamoto Hiroshi Tokyo U., ICEPP Sakurai Yuki Waseda U. Salamanna Giuseppe INFN, Rome Rome III U. 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Sapp Kevin Pittsburgh U. Sapronov Andrey Dubna, JINR Saraiva João LIP, Lisbon Lisbon U., CFNUL Sarrazin Bjorn Bonn U. Sartisohn Georg Wuppertal U. Sasaki Osamu KEK, Tsukuba Sasaki Yuichi Tokyo U., ICEPP Sauvage Gilles Annecy, LAPP Sauvan Emmanuel Annecy, LAPP Savard Pierre Toronto U. TRIUMF Savu Dan Octavian CERN Sawyer Craig Oxford U. Sawyer Lee Louisiana Tech. U. Saxon David Glasgow U. Saxon James Pennsylvania U. Sbarra Carla INFN, Bologna Sbrizzi Antonio INFN, Bologna Bologna U. Scanlon Tim University Coll. London Scannicchio Diana UC, Irvine Scarcella Mark Sydney U. Scarfone Valerio INFN, Cosenza Calabria U. Schaarschmidt Jana Weizmann Inst. Schacht Peter Munich, Max Planck Inst. Schaefer Douglas CERN Schaefer Ralph DESY Schaepe Steffen Bonn U. Schaetzel Sebastian Heidelberg U. Schäfer Uli Mainz U. Schaffer Arthur Orsay, LAL Schaile Dorothee Munich U. Schamberger R~Dean SUNY, Stony Brook Scharf Veit Kirchhoff Inst. Phys. 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Schumm Bruce UC, Santa Cruz Schune Philippe IRFU, Saclay Schwanenberger Christian Manchester U. Schwartzman Ariel SLAC Schwarz Thomas Andrew Michigan U. Schwegler Philipp Munich, Max Planck Inst. Schwemling Philippe IRFU, Saclay Schwienhorst Reinhard Michigan State U. Schwindling Jerome IRFU, Saclay Schwindt Thomas Bonn U. Schwoerer Maud Annecy, LAPP Sciacca Gianfranco Bern U., LHEP Scifo Estelle Orsay, LAL Sciolla Gabriella Brandeis U. Scott Bill Rutherford Scuri Fabrizio INFN, Pisa Pisa U. Scutti Federico Bonn U. Searcy Jacob Michigan U. Sedov George DESY Sedykh Evgeny St. Petersburg, INP Seema Pienpen Bonn U. Seidel Sally New Mexico U. Seiden Abraham UC, Santa Cruz Seifert Frank Prague, Tech. U. Seixas José Rio de Janeiro Federal U. Sekhniaidze Givi INFN, Naples Sekula Stephen Southern Methodist U. Selbach Karoline Elfriede Edinburgh U. Seliverstov Dmitry St. Petersburg, INP Sellers Graham Liverpool U. Semprini-Cesari Nicola INFN, Bologna Bologna U. Serfon Cedric CERN Serin Laurent Orsay, LAL Serkin Leonid Gottingen U., II. Phys. Inst. Serre Thomas Marseille, CPPM Seuster Rolf TRIUMF Severini Horst Oklahoma U. Sfiligoj Tina Stefan Inst., Ljubljana Sforza Federico Munich, Max Planck Inst. Sfyrla Anna CERN Shabalina Elizaveta Gottingen U., II. Phys. Inst. Shamim Mansoora Oregon U. Shan Lianyou Beijing, Inst. High Energy Phys. Shang Ruo-yu Illinois U., Urbana Shank James Boston U. Shapiro Marjorie LBL, Berkeley Shatalov Pavel Moscow, ITEP Shaw Kate INFN, Udine ICTP, Trieste Shehu Ciwake Yusufu Sussex U. Sherwood Peter University Coll. London Shi Liaoshan Taiwan, Inst. Phys. Zhongshan U. Shimizu Shima Kobe U. Shimmin Chase Owen UC, Irvine Shimojima Makoto Nagasaki Inst. Appl. Sci. Shiyakova Mariya Dubna, JINR Shmeleva Alevtina Lebedev Inst. Shochet Mel Chicago U., EFI Short Daniel Oxford U. Shrestha Suyog Iowa State U. Shulga Evgeny Moscow Phys. Eng. Inst. Shupe Michael Arizona U. Shushkevich Stanislav DESY Sicho Petr Prague, Inst. 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Yamamoto Akira KEK, Tsukuba Yamamoto Kyoko Iowa State U. Yamamoto Shimpei Tokyo U., ICEPP Yamamura Taiki Tokyo U., ICEPP Yamanaka Takashi Tokyo U., ICEPP Yamauchi Katsuya Nagoya U. Yamazaki Yuji Kobe U. Yan Zhen Boston U. Yang Haijun Shanghai Jiao Tong U. Yang Hongtao Wisconsin U., Madison Yang Un-Ki Manchester U. Yang Yi Ohio State U. Yanush Serguei Minsk, High Energy Phys. Ctr. Yao Liwen Beijing, Inst. High Energy Phys. Yao Weiming LBL, Berkeley Yasu Yoshiji KEK, Tsukuba Yatsenko Elena DESY Yau Wong Kaven Henry Bonn U. Ye Jingbo Southern Methodist U. Ye Shuwei Brookhaven Yeletskikh Ivan Dubna, JINR Yen Andy L Harvard U., Phys. Dept. Yildirim Eda DESY Yilmaz Metin Gazi U. Yoosoofmiya Reza Pittsburgh U. Yorita Kohei Waseda U. Yoshida Rikutaro Argonne Yoshihara Keisuke Tokyo U., ICEPP Young Charles SLAC Young Christopher John CERN Youssef Saul Boston U. Yu David Ren-Hwa LBL, Berkeley Yu Jaehoon Texas U., Arlington Yu Jiaming Michigan U. Yu Jie Oklahoma State U. Yuan Li Kobe U. Yurkewicz Adam Northern Illinois U. Yusuff Imran Cambridge U. Malaya U. Zabinski Bartlomiej Cracow, INP Zaidan Remi Iowa U. Zaitsev Alexander Serpukhov, IHEP Moscow, MIPT Zaman Aungshuman SUNY, Stony Brook Zambito Stefano Brandeis U. Zanello Lucia INFN, Rome Rome U. Zanzi Daniele Melbourne U. Zeitnitz Christian Wuppertal U. Zeman Martin Prague, Tech. U. Zemla Andrzej AGH-UST, Cracow Zengel Keith Brandeis U. Zenin Oleg Serpukhov, IHEP Ženiš Tibor Comenius U. Zerwas Dirk Orsay, LAL Zevi della Porta Giovanni Harvard U., Phys. Dept. Zhang Dongliang Michigan U. Zhang Fangzhou Wisconsin U., Madison Zhang Huaqiao Michigan State U. Zhang Jinlong Argonne Zhang Lei Taiwan, Inst. Phys. Zhang Xueyao Shandong U. Zhang Zhiqing Orsay, LAL Zhao Yongke Shandong U. Zhao Zhengguo Hefei, CUST Zhemchugov Alexey Dubna, JINR Zhong Jiahang Oxford U. Zhou Bing Michigan U. Zhou Lei Nevis Labs, Columbia U. Zhou Ning UC, Irvine Zhu Cheng Guang Shandong U. Zhu Hongbo Beijing, Inst. High Energy Phys. Zhu Junjie Michigan U. Zhu Yingchun Hefei, CUST Zhuang Xuai Beijing, Inst. High Energy Phys. Zhukov Konstantin Lebedev Inst. Zibell Andre Wurzburg U. Zieminska Daria Indiana U. Zimine Nikolai Dubna, JINR Zimmermann Christoph Mainz U. Zimmermann Robert Bonn U. Zimmermann Simone Bonn U. Zimmermann Stephanie Freiburg U. Zinonos Zinonas Gottingen U., II. Phys. Inst. Ziolkowski Michael Siegen U. Zobernig Georg Wisconsin U., Madison Zoccoli Antonio INFN, Bologna Bologna U. zur Nedden Martin Humboldt U., Berlin Zurzolo Giovanni INFN, Naples Naples U. Zutshi Vishnu Northern Illinois U. Zwalinski Lukasz CERN 2014 11 A search for the neutral Higgs bosons predicted by the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is performed on data from proton--proton collisions at a centre-of-mass energy of $8 TeV$ collected with the ATLAS detector at the Large Hadron Collider. The samples used for this search were collected in 2012 and correspond to integrated luminosities in the range 19.5 - 20.3 fb$^{-1}$. The MSSM Higgs bosons are searched for in the $\tau\tau$ final state. No significant excess over the expected background is observed, and exclusion limits are derived for the production cross section times branching fraction of a scalar particle as a function of its mass. The results are also interpreted in the MSSM parameter space for various benchmark scenarios. research-article

Measurement of the top quark pair production cross section in proton-proton collisions at center-of-mass energies of 7 TeV in final states with a $\tau$ lepton with the ATLAS detector Pérez García-Estañ Teresa Valencia U., Valencia U., IFIC The top quark is the heaviest elementary particle and has the largest coupling to the Standard Model Higgs boson. Top quark decays with a tau lepton in the final state play an important role in the search for SM and BSM Higgs bosons. In particular, if a charged Higgs boson exists as predicted by the MSSM, and its mass is lower than the top quark mass minus the bottom quark mass, the top quark predominantly decays into a charged Higgs boson and a $b$-quark: $t \rightarrow H^{+}b$. A heavy charged Higgs can also be produced associated with a top quark: tH$^{+}$. In some scenarios, the charged Higgs would decay predominantly to a tau lepton and a neutrino, producing then an excess in the $\ell + \tau$ channel over the other dilepton channels which, if observed, would constitute experimental evidence of the the existence of a charged Higgs boson. The $t\bar{t}$ production cross section in the lepton plus tau channel ($pp \rightarrow t\bar{t} \rightarrow\ell + \tau$) measurement presented in this thesis has been obtained analysing 2.05 $fb^{-1}$ of ATLAS data at $\sqrt{s} =$ 7 TeV collected during 2011. The $t\bar{t}(\ell+\tau)$ candidate events are selected based on the event topology of the final state: one high $p_T$ electron or muon, 2 high $E_T$ jets, at least one of them b-tagged, large missing transverse energy and one hadronically decaying $\tau$ lepton. The main background after the selection comes from semileptonic $t\bar{t}$ where a jet has been misidentified as a hadronically decaying tau. The only discriminator between this background and the signal is the tau identification. In this analysis we exploit a discriminant variable, $BDT_j$, obtained from a Boosted Decision Tree multi-variate technique specially trained to separate real taus from other jet types. The signal and background contributions to the signal region are then estimated using a $\chi^{2}$ fit of the $BDT_j$ distribution of the reconstructed taus in the data sample with a signal template derived from MC and background templates derived from data to minimize the systematic uncertainty. Two background templates are used, one for jets produced by the hadronization of light-quarks and another for jets produced by the hadronization of gluon, which constitute the main source of fake taus for the $t\bar{t}(\ell+\tau)$ signal after the selections. The parameters of the fit are the amount of both backgrounds and the amount of signal and the shapes of the templates are fixed. The measured $t\bar{t}(\ell+\tau)$ cross section \begin{equation*} \sigma_{t\bar{t}} = 151 \pm 11 ~{\rm (stat.)} \pm 15 ~{\rm (syst.)} \pm 5 ~{\rm (lumi.)} ~\rm{pb.} \end{equation*} exceeds the precision of the existing measurements in the same $\ell + \tau$ channel performed by CDF, DZero and CMS. Furthermore, it improves the results of previous measurements of the $t\bar{t}(\ell+\tau)$ cross section published at ATLAS, reducing the statistical uncertainty of the cross section measurement and improving the background description, building a background model which properly reflects the jet composition to correctly estimate the fake $\tau$ contamination in the signal region. The systematic uncertainties dominate the measurement and are kept at the same level as previous measurements. The observed cross section value agree well with the Standard Model theoretical expectation predicted with full NNLO precision, within uncertainties, and is consistent with the measured cross-sections using different decay channels by ATLAS. Therefore, we cannot make any claims of new physics. We have, however, developed a novel technique which has a great potential to achieve even higher precision when applied to high statistic samples and it can be used to test the SM and search for new physics in pp collisions in the $t\bar{t}(\ell+\tau)$ channel with the new data expected in 2015 when the LHC resumes the proton-proton collisions at 13-14 TeV. technical-report

SM and MSSM $H\rightarrow\tau\tau$ Schwindt Thomas Bonn U. 2014 After the discovery of a Higgs boson at the LHC in $\gamma\gamma$, $ZZ$ and $WW$ final states in 2012, the ATLAS collaboration also observes an excess of data over the predicted background in $\tau\tau$ final states, which is consistent with the decay of the discovered Higgs boson with $m_H\approx125$ GeV. With an observed (expected) significance of 4.1$\sigma$ (3.2$\sigma$), this is evidence for the coupling of this Higgs boson to fermions. The multi-variate analysis of a dataset corresponding to 20.3 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=8$ TeV is presented together with a separate cut-based analysis of the same dataset searching for $h/H/A{\rightarrow}\tau^+\tau^-$ decays in the context of the Minimal Supersymmetric Standard Model (MSSM). No excess of data over the expected backgrounds is observed in this search for additional Higgs bosons, and exclusion limits on the production cross section times branching fraction are derived and interpreted in the MSSM parameter space for different scenarios. INTNOTEATLASPUBL

Prospects for New Physics in Higgs Couplings Studies with the ATLAS Detector at the HL-LHC 2014 The ATLAS experiment at the LHC determines the couplings of the Higgs boson to other particles using the combination of measurements from multiple production and decay channels. The expected precision with which these couplings can be measured at the High-Luminosity LHC has been estimated elsewhere using parametrized acceptances, efficiencies, and resolutions to approximate the expected detector performance with the upgraded detector. Expected constraints on a non-standard mass scaling of the couplings, as well as models with an additional electroweak singlet, an additional electroweak doublet (two-Higgs-doublet model), a composite Higgs boson, a simplified Supersymmetric Standard Model (MSSM), and a Higgs portal to dark matter, are derived here using the estimated precision on the coupling measurements with 300 and 3000 $\textrm{fb}^{-1}$ of $pp$ collision data at $\sqrt{s}=14$ TeV. The sensitivity to new phenomena is significantly enhanced at the High-Luminosity LHC compared to the corresponding sensitivities at lower integrated luminosities. INTNOTEATLASPUBL

News from LHC: Recent Results on Higgs Physics Straessner A Dresden, Tech. U. 2014 The ATLAS and CMS experiments at the LHC have measured detailed properties of the SM-like Higgs boson discovered in 2012. Results on Higgs boson mass, width, spin and coupling determinations are presented. The parameters observed are furthermore interpreted in extensions to the Standard Model. Searches for additional Higgs bosons predicted in the general 2 Higgs Doublet Model (2HDM) and the Minimal Supersymmetric Standard Model (MSSM) are reported. INTNOTEATLASPUBL

Search for charged Higgs Bosons decaying via $H^+ \to \tau_{lep.} + \nu$ in $t\bar{t}$ events at $\sqrt{s}=7 TeV$ in ATLAS Breaden Madden William Dmitri Morgan Glagow U. This thesis for the degree of Master of Science by Research presents the theory, methodology and results of a search for charged Higgs bosons decaying via ${H^+ \to \tau_{lep.} + \nu}$ using single lepton and two lepton channels in ${t}$ quark pair (${t\bar{t}}$) events with a leptonically decaying ${\tau}$ in the final state based on ${1.03\textrm{ fb}^{-1}}$ of proton-proton collision data at centre of mass energy ${\sqrt{s}=7\textrm{ TeV}}$ from ATLAS, an experiment of the LHC, with special attention given to the statistical analysis and calculation involved in the limit setting process. For the single lepton channel, the expected number of Standard Model-like\linebreak${t\bar{t} \to b\bar{b}W^{+}W^{-}}$ background events lies between $0.99$ and $1.03$ times the Standard Model prediction, with uncertainties in the range ${2\%}$ -- ${3\%}$. For the two lepton channel, the expected number of Standard Model-like background events lies between $0.99$ and $1.03$ times the Standard Model prediction, with uncertainties in the range ${5\%}$ -- ${25\%}$. Assuming the branching fraction ${\mathcal{B}\left(H^{+} \to \tau\mu\right)=1}$, the upper limits on the branching fraction ${\mathcal{B}\left(t \to bH^{+}\right)}$ at the $95\%$ confidence level are between ${5.2\%}$ and ${14.1\%}$ for charged Higgs boson masses in the range ${90\textrm{ GeV}\leq m_{H^{+}}\leq 160\textrm{ GeV}}$. In the context of the ${m^{\textrm{max.}}_{h}}$ scenario of the MSSM, values of ${\tan\beta}$ greater than ${30}$--${56}$ are excluded in the mass range ${90\textrm{ GeV}\leq m_{H^{+}}\leq 140\textrm{ GeV}}$. The compatibility with background of the combination of the single lepton and two lepton channels ranges between ${26\%}$ and ${50\%}$, as measured by ${p_{0}}$ values. Hence, no indication of a ${H^{+}}$-like excess is found. technical-report

Charged Higgs boson searches and SemiConductor Tracker commissioning for the ATLAS experiment Mohn Bjarte Alsaker Bergen U. The ATLAS (A Toroidal Lhc ApparatuS) experiment is one of four major experiments presently being installed at the upcoming Large Hadron Collider (LHC) at the European Centre for Nuclear Research (CERN) outside Geneva. In this thesis we present work done on both the simulation of the ATLAS physics potential for a charged Higgs boson and the construction of the Semiconductor Tracker (SCT) - a subdetector within the ATLAS Inner Detector. The discovery of a charged Higgs boson would be an unambiguous sign of physics beyond the Standard Model (SM) and it is thus of great interest to study the ATLAS potential for a charged Higgs discovery. Two such studies have been conducted for this thesis. In the first study a large-mass-splitting Minimal Supersymmetric Standard Model (MSSM) is assumed in which the charged Higgs boson decays into a W boson and a neutral Higgs may receive a large branching ratio.We conclude, however, that charged Higgs searches in this decay channel are made difficult by a large irreducible SM background. Despite its small brancing ratio at high masses for the charged Higgs boson, the decay mode H± →τν remains the most powerful decay mode for a charged Higgs discovery. Discovery through this channel depends heavily on excellent detector performance and understanding of the background.We show that with detector full simulation and with more complete background samples this channel still remains the most powerful decay mode. We also show that it is possible to connect the discovery countour for charged Higgs boson masses below and above the top-quark mass. The SCT detector is a tracking detector based on silicon microstrip detector technology. It is a highly modular detector consisting of 4088 detector modules that are mounted on 4 barrels and 9x2 end cap disks. Some 320 of the SCT barrel detector modules were built by a Scandinavian collaboration and presented here are the results of this work and procedures for building and quality assurance. Each SCT detector module is powered by an individual high and low voltage supply and thus a large scale and robust power supply control system is needed for controlling the SCT detector. Presented in this thesis is work done to prepare the SCT power supply software for this task, as well as the results obtained during testing and development. As a part of the commissioning of the completed SCT barrel, a series of cosmic runs were performed. Data from these runs allowed for first studies of the detector alignment and alignment results and conlusions thereof are presented in this thesis. technical-report

JHEP JHEP Summary of the searches for squarks and gluinos using $\sqrt{s}$ = 8 TeV $pp$ collisions with the ATLAS experiment at the LHC Aad Georges Marseille, CPPM Abbott Brad Oklahoma U. Abdallah Jalal Taiwan, Inst. Phys. Abdinov Ovsat Baku, Inst. Phys. Aben Rosemarie FOM, Amsterdam Abolins Maris Michigan State U. AbouZeid Ossama Toronto U. Abramowicz Halina Tel Aviv U. Abreu Henso Technion Abreu Ricardo Oregon U. Abulaiti Yiming Stockholm U. Stockholm U., OKC Acharya Bobby Samir INFN, Udine ICTP, Trieste King's Coll. London Adamczyk Leszek AGH-UST, Cracow Adams David Brookhaven Adelman Jahred Northern Illinois U. Adomeit Stefanie Munich U. Adye Tim Rutherford Affolder Tony Liverpool U. Agatonovic-Jovin Tatjana Belgrade U. Agricola Johannes Gottingen U., II. Phys. Inst. Aguilar-Saavedra Juan Antonio LIP, Lisbon CAFPE, Granada Ahlen Steven Boston U. Ahmadov Faig Dubna, JINR Baku, Inst. Phys. Aielli Giulio INFN, Rome Rome U., Tor Vergata Akerstedt Henrik Stockholm U. Stockholm U., OKC Åkesson Torsten Paul Ake Lund U. Akimov Andrei Lebedev Inst. Alberghi Gian Luigi INFN, Bologna Bologna U. Albert Justin Victoria U. Albrand Solveig LPSC, Grenoble Alconada Verzini Maria Josefina La Plata U. Aleksa Martin CERN Aleksandrov Igor Dubna, JINR Alexa Calin Bucharest, IFIN-HH Alexander Gideon Tel Aviv U. Alexopoulos Theodoros Natl. Tech. U., Athens Alhroob Muhammad Oklahoma U. Alimonti Gianluca INFN, Milan Alio Lion Marseille, CPPM Alison John Chicago U., EFI Alkire Steven Patrick Nevis Labs, Columbia U. Allbrooke Benedict Sussex U. Allport Phillip Liverpool U. Aloisio Alberto INFN, Naples Naples U. Alonso Alejandro Bohr Inst. Alonso Francisco La Plata U. Alpigiani Cristiano Queen Mary, U. of London Altheimer Andrew David Nevis Labs, Columbia U. Alvarez Gonzalez Barbara CERN Άlvarez Piqueras Damián Valencia U., IFIC Alviggi Mariagrazia INFN, Naples Naples U. 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Santiago Cerqueira Augusto Juiz de Fora U. Cerri Alessandro Sussex U. Cerrito Lucio Queen Mary, U. of London Cerutti Fabio LBL, Berkeley Cerv Matevz CERN Cervelli Alberto Bern U., LHEP Cetin Serkant Ali Dogus U., Kadikoy Chafaq Aziz Casablanca U. Chakraborty Dhiman Northern Illinois U. Chalupkova Ina Charles U. Chang Philip Illinois U., Urbana Chapman John Derek Cambridge U. Charlton Dave Birmingham U. Chau Chav Chhiv Toronto U. Chavez Barajas Carlos Alberto Sussex U. Cheatham Susan Technion Chegwidden Andrew Michigan State U. Chekanov Sergei Argonne Chekulaev Sergey TRIUMF Chelkov Gueorgui Dubna, JINR Tomsk State U. Chelstowska Magda Anna Michigan U. Chen Chunhui Iowa State U. Chen Hucheng Brookhaven Chen Karen SUNY, Stony Brook Chen Liming Shandong U. Marseille, CPPM Chen Shenjian Nanjing U. Chen Xin Tsinghua U., Beijing Chen Ye Kobe U. Cheng Hok Chuen Michigan U. Cheng Yangyang Chicago U., EFI Cheplakov Alexander Dubna, JINR Cheremushkina Evgenia Serpukhov, IHEP Cherkaoui El Moursli Rajaa Mohammed V U., Agdal Chernyatin Valeriy Brookhaven Cheu Elliott Arizona U. Chevalier Laurent IRFU, Saclay Chiarella Vitaliano Frascati Chiarelli Giorgio INFN, Pisa Pisa U. Chiodini Gabriele INFN, Lecce Chisholm Andrew Birmingham U. Chislett Rebecca Thalatta University Coll. London Chitan Adrian Bucharest, IFIN-HH Chizhov Mihail Dubna, JINR Choi Kyungeon Indiana U. Chouridou Sofia Athens U. Chow Bonnie Kar Bo Munich U. Christodoulou Valentinos University Coll. London Chromek-Burckhart Doris CERN Chudoba Jiri Prague, Inst. Phys. Chuinard Annabelle Julia McGill U. Chwastowski Janusz Cracow, INP Chytka Ladislav Palacky U. Ciapetti Guido INFN, Rome Rome U. Ciftci Abbas Kenan Ankara U. Cinca Diane Glasgow U. Cindro Vladimir Stefan Inst., Ljubljana Cioara Irina Antonela Bonn U. Ciocio Alessandra LBL, Berkeley Citron Zvi Hirsh Weizmann Inst. Ciubancan Mihai Bucharest, IFIN-HH Clark Allan G Geneva U. Clark Brian Lee Harvard U., Phys. Dept. Clark Philip James Edinburgh U. Clarke Robert LBL, Berkeley Cleland Bill Pittsburgh U. Clement Christophe Stockholm U. Stockholm U., OKC Coadou Yann Marseille, CPPM Cobal Marina INFN, Udine Udine U. Coccaro Andrea Washington U., Seattle Cochran James H Iowa State U. Coffey Laurel Brandeis U. Cogan Joshua Godfrey SLAC Colasurdo Luca NIKHEF, Amsterdam Cole Brian Nevis Labs, Columbia U. Cole Stephen Northern Illinois U. Colijn Auke-Pieter FOM, Amsterdam Collot Johann LPSC, Grenoble Colombo Tommaso Heidelberg U. Compostella Gabriele Munich, Max Planck Inst. Conde Muiño Patricia LIP, Lisbon Lisbon U., CFNUL Coniavitis Elias Freiburg U. Connell Simon Henry Johannesburg U. Connelly Ian Royal Holloway, U. of London Consonni Sofia Maria INFN, Milan Milan U. Consorti Valerio Freiburg U. Constantinescu Serban Bucharest, IFIN-HH Conta Claudio INFN, Pavia Pavia U. Conti Geraldine CERN Conventi Francesco INFN, Naples Naples, Inst. U. Navale Cooke Mark LBL, Berkeley Cooper Ben University Coll. London Cooper-Sarkar Amanda Oxford U. Cornelissen Thijs Wuppertal U. Corradi Massimo INFN, Bologna Corriveau Francois McGill U. IPP, Canada Corso-Radu Alina UC, Irvine Cortes-Gonzalez Arely Barcelona, IFAE Cortiana Giorgio Munich, Max Planck Inst. Costa Giuseppe INFN, Milan Costa María José Valencia U., IFIC Costanzo Davide Sheffield U. Côté David Texas U., Arlington Cottin Giovanna Cambridge U. Cowan Glen Royal Holloway, U. of London Cox Brian Manchester U. Cranmer Kyle New York U. Cree Graham Carleton U. Crépé-Renaudin Sabine LPSC, Grenoble Crescioli Francesco Paris U., VI-VII Cribbs Wayne Allen Stockholm U. Stockholm U., OKC Crispin Ortuzar Mireia Oxford U. Cristinziani Markus Bonn U. Croft Vince NIKHEF, Amsterdam Crosetti Giovanni INFN, Cosenza Calabria U. Cuhadar Donszelmann Tulay Sheffield U. Cummings Jane Yale U. Curatolo Maria Frascati Cuthbert Cameron Sydney U. Czirr Hendrik Siegen U. Czodrowski Patrick Alberta U. D'Auria Saverio Glasgow U. D'Onofrio Monica Liverpool U. Da Cunha Sargedas De Sousa Mario Jose LIP, Lisbon Lisbon U., CFNUL Da Via Cinzia Manchester U. Dabrowski Wladyslaw AGH-UST, Cracow Dafinca Alexandru Oxford U. Dai Tiesheng Michigan U. Dale Orjan Bergen U. Dallaire Frederick Montreal U. Dallapiccola Carlo Massachusetts U., Amherst Dam Mogens Bohr Inst. Dandoy Jeffrey Rogers Chicago U., EFI Dang Nguyen Phuong Freiburg U. Daniells Andrew Christopher Birmingham U. Danninger Matthias British Columbia U. Dano Hoffmann Maria IRFU, Saclay Dao Valerio Freiburg U. Darbo Giovanni INFN, Genoa Darmora Smita Texas U., Arlington Dassoulas James Alberta U. Dattagupta Aparajita Indiana U. Davey Will Bonn U. David Claire Victoria U. Davidek Tomas Charles U. Davies Eleanor Oxford U. Rutherford Davies Merlin Tel Aviv U. Davison Peter University Coll. London Davygora Yuriy Kirchhoff Inst. Phys. Dawe Edmund Melbourne U. Dawson Ian Sheffield U. Daya-Ishmukhametova Rozmin Massachusetts U., Amherst De Kaushik Texas U., Arlington de Asmundis Riccardo INFN, Naples De Benedetti Abraham Oklahoma U. De Castro Stefano INFN, Bologna Bologna U. De Cecco Sandro Paris U., VI-VII De Groot Nicolo NIKHEF, Amsterdam de Jong Paul FOM, Amsterdam De la Torre Hector Madrid, Autonoma U. De Lorenzi Francesco Iowa State U. De Nooij Lucie FOM, Amsterdam De Pedis Daniele INFN, Rome De Salvo Alessandro INFN, Rome De Sanctis Umberto Sussex U. De Santo Antonella Sussex U. De Vivie De Regie Jean-Baptiste Orsay, LAL Dearnaley William James Lancaster U. Debbe Ramiro Brookhaven Debenedetti Chiara UC, Santa Cruz Dedovich Dmitri Dubna, JINR Deigaard Ingrid FOM, Amsterdam Del Peso Jose Madrid, Autonoma U. Del Prete Tarcisio INFN, Pisa Pisa U. Delgove David Orsay, LAL Deliot Frederic IRFU, Saclay Delitzsch Chris Malena Geneva U. Deliyergiyev Maksym Stefan Inst., Ljubljana Dell'Acqua Andrea CERN Dell'Asta Lidia Boston U. Dell'Orso Mauro INFN, Pisa Pisa U. Della Pietra Massimo INFN, Naples Naples, Inst. U. Navale della Volpe Domenico Geneva U. Delmastro Marco Annecy, LAPP Delsart Pierre-Antoine LPSC, Grenoble Deluca Carolina FOM, Amsterdam DeMarco David Toronto U. Demers Sarah Yale U. Demichev Mikhail Dubna, JINR Demilly Aurelien Paris U., VI-VII Denisov Sergey Serpukhov, IHEP Derendarz Dominik Cracow, INP Derkaoui Jamal Eddine Oujda U. Derue Frederic Paris U., VI-VII Dervan Paul Liverpool U. Desch Klaus Kurt Bonn U. Deterre Cecile DESY Deviveiros Pier-Olivier CERN Dewhurst Alastair Rutherford Dhaliwal Saminder Brandeis U. Di Ciaccio Anna INFN, Rome Rome U., Tor Vergata Di Ciaccio Lucia Annecy, LAPP Di Domenico Antonio INFN, Rome Rome U. Di Donato Camilla INFN, Naples Naples U. Di Girolamo Alessandro CERN Di Girolamo Beniamino CERN Di Mattia Alessandro Technion Di Micco Biagio INFN, Rome Rome III U. Di Nardo Roberto Frascati Di Simone Andrea Freiburg U. Di Sipio Riccardo Toronto U. Di Valentino David Carleton U. Diaconu Cristinel Marseille, CPPM Diamond Miriam Toronto U. Dias Flavia Edinburgh U. Diaz Marco Aurelio Chile U., Catolica Diehl Edward Michigan U. Dietrich Janet Humboldt U., Berlin Diglio Sara Marseille, CPPM Dimitrievska Aleksandra Belgrade U. Dingfelder Jochen Bonn U. Dita Petre Bucharest, IFIN-HH Dita Sanda Bucharest, IFIN-HH Dittus Fridolin CERN Djama Fares Marseille, CPPM Djobava Tamar Tbilisi State U. Djuvsland Julia Isabell Kirchhoff Inst. Phys. Barros do Vale Maria Aline Sao Joao del-Rei Fed. U. Dobos Daniel CERN Dobre Monica Bucharest, IFIN-HH Doglioni Caterina Lund U. Dohmae Takeshi Tokyo U., ICEPP Dolejsi Jiri Charles U. Dolezal Zdenek Charles U. Dolgoshein Boris Moscow Phys. Eng. Inst. Donadelli Marisilvia Sao Paulo U. Donati Simone INFN, Pisa Pisa U. Dondero Paolo INFN, Pavia Pavia U. Donini Julien Clermont-Ferrand U. Dopke Jens Rutherford Doria Alessandra INFN, Naples Dova Maria-Teresa La Plata U. Doyle Tony Glasgow U. Drechsler Eric Gottingen U., II. Phys. Inst. Dris Manolis Natl. Tech. U., Athens Dubreuil Emmanuelle Clermont-Ferrand U. Duchovni Ehud Weizmann Inst. Duckeck Guenter Munich U. Ducu Otilia Anamaria Bucharest, IFIN-HH Marseille, CPPM Duda Dominik FOM, Amsterdam Dudarev Alexey CERN Duflot Laurent Orsay, LAL Duguid Liam Royal Holloway, U. of London Dührssen Michael CERN Dunford Monica Kirchhoff Inst. Phys. Duran Yildiz Hatice Ankara U. Düren Michael Giessen U. Durglishvili Archil Tbilisi State U. Duschinger Dirk Dresden, Tech. U. Dyndal Mateusz AGH-UST, Cracow Eckardt Christoph DESY Ecker Katharina Maria Munich, Max Planck Inst. Edgar Ryan Christopher Michigan U. Edson William SUNY, Albany Edwards Nicholas Charles Edinburgh U. Ehrenfeld Wolfgang Bonn U. Eifert Till CERN Eigen Gerald Bergen U. Einsweiler Kevin LBL, Berkeley Ekelof Tord Uppsala U., Inst. Theor. Phys. El Kacimi Mohamed Cadi Ayyad U., Marrakech Ellert Mattias Uppsala U., Inst. Theor. Phys. Elles Sabine Annecy, LAPP Ellinghaus Frank Wuppertal U. Elliot Alison Victoria U. Ellis Nicolas CERN Elmsheuser Johannes Munich U. Elsing Markus CERN Emeliyanov Dmitry Rutherford Enari Yuji Tokyo U., ICEPP Endner Oliver Chris Mainz U. Endo Masaki Osaka U. Erdmann Johannes Dortmund U. Ereditato Antonio Bern U., LHEP Ernis Gunar Wuppertal U. Ernst Jesse SUNY, Albany Ernst Michael Brookhaven Errede Steven Illinois U., Urbana Ertel Eugen Mainz U. Escalier Marc Orsay, LAL Esch Hendrik Dortmund U. Escobar Carlos Pittsburgh U. Esposito Bellisario Frascati Etienvre Anne-Isabelle IRFU, Saclay Etzion Erez Tel Aviv U. Evans Hal Indiana U. Ezhilov Alexey St. Petersburg, INP Fabbri Laura INFN, Bologna Bologna U. Facini Gabriel Chicago U., EFI Fakhrutdinov Rinat Serpukhov, IHEP Falciano Speranza INFN, Rome Falla Rebecca Jane University Coll. London Faltova Jana Charles U. Fang Yaquan Beijing, Inst. High Energy Phys. Fanti Marcello INFN, Milan Milan U. Farbin Amir Texas U., Arlington Farilla Addolorata INFN, Rome Farooque Trisha Barcelona, IFAE Farrell Steven LBL, Berkeley Farrington Sinead Warwick U. Farthouat Philippe CERN Fassi Farida Mohammed V U., Agdal Fassnacht Patrick CERN Fassouliotis Dimitrios Athens U. Faucci Giannelli Michele Royal Holloway, U. of London Favareto Andrea INFN, Genoa Genoa U. Fayard Louis Orsay, LAL Federic Pavol Comenius U. Fedin Oleg St. Petersburg, INP St. Petersburg Polytechnic Inst. Fedorko Wojciech British Columbia U. Feigl Simon CERN Feligioni Lorenzo Marseille, CPPM Feng Cunfeng Shandong U. Feng Eric Argonne Feng Haolu Michigan U. Fenyuk Alexander Serpukhov, IHEP Feremenga Last Texas U., Arlington Fernandez Martinez Patricia Valencia U., IFIC Fernandez Perez Sonia CERN Ferrando James Glasgow U. Ferrari Arnaud Uppsala U., Inst. Theor. Phys. Ferrari Pamela FOM, Amsterdam Ferrari Roberto INFN, Pavia Ferreira de Lima Danilo Enoque Glasgow U. Ferrer Antonio Valencia U., IFIC Ferrere Didier Geneva U. Ferretti Claudio Michigan U. Ferretto Parodi Andrea INFN, Genoa Genoa U. Fiascaris Maria Chicago U., EFI Fiedler Frank Mainz U. Filipčič Andrej Stefan Inst., Ljubljana Filipuzzi Marco DESY Filthaut Frank NIKHEF, Amsterdam Fincke-Keeler Margret Victoria U. Finelli Kevin Daniel Sydney U. Fiolhais Miguel LIP, Lisbon Coimbra U. Fiorini Luca Valencia U., IFIC Firan Ana Southern Methodist U. Fischer Adam SUNY, Albany Fischer Cora Barcelona, IFAE Fischer Julia Wuppertal U. Fisher Wade Cameron Michigan State U. Fitzgerald Eric Andrew Brandeis U. Flaschel Nils DESY Fleck Ivor Siegen U. Fleischmann Philipp Michigan U. Fleischmann Sebastian Wuppertal U. Fletcher Gareth Thomas Sheffield U. Fletcher Gregory Queen Mary, U. of London Fletcher Rob Roy MacGregor Pennsylvania U. Flick Tobias Wuppertal U. Floderus Anders Lund U. Flores Castillo Luis Hong Kong, Chinese U. Flowerdew Michael Munich, Max Planck Inst. Formica Andrea IRFU, Saclay Forti Alessandra Manchester U. Fournier Daniel Orsay, LAL Fox Harald Lancaster U. Fracchia Silvia Barcelona, IFAE Francavilla Paolo Paris U., VI-VII Franchini Matteo INFN, Bologna Bologna U. Francis David CERN Franconi Laura Oslo U. Franklin Melissa Harvard U., Phys. Dept. Frate Meghan UC, Irvine Fraternali Marco INFN, Pavia Pavia U. Freeborn David University Coll. London French Sky Cambridge U. Friedrich Felix Dresden, Tech. U. Froidevaux Daniel CERN Frost James Oxford U. Fukunaga Chikara Tokyo Metropolitan U. Fullana Torregrosa Esteban Mainz U. Fulsom Bryan Gregory SLAC Fusayasu Takahiro Nagasaki Inst. Appl. Sci. Fuster Juan Valencia U., IFIC Gabaldon Carolina LPSC, Grenoble Gabizon Ofir Wuppertal U. Gabrielli Alessandro INFN, Bologna Bologna U. Gabrielli Andrea INFN, Rome Rome U. Gach Grzegorz AGH-UST, Cracow Gadatsch Stefan CERN Gadomski Szymon Geneva U. Gagliardi Guido INFN, Genoa Genoa U. Gagnon Pauline Indiana U. Galea Cristina NIKHEF, Amsterdam Galhardo Bruno LIP, Lisbon Coimbra U. Gallas Elizabeth Oxford U. Gallop Bruce Rutherford Gallus Petr Prague, Tech. U. Galster Gorm Aske Gram Krohn Bohr Inst. Gan KK Ohio State U. Gao Jun Hefei, CUST Marseille, CPPM Gao Yanyan Edinburgh U. Gao Yongsheng SLAC Fresno State Garay Walls Francisca Edinburgh U. Garberson Ford Yale U. García Carmen Valencia U., IFIC García Navarro José Enrique Valencia U., IFIC Garcia-Sciveres Maurice LBL, Berkeley Gardner Robert Chicago U., EFI Garelli Nicoletta SLAC Garonne Vincent Oslo U. Gatti Claudio Frascati Gaudiello Andrea INFN, Genoa Genoa U. Gaudio Gabriella INFN, Pavia Gaur Bakul Siegen U. Gauthier Lea Montreal U. Gauzzi Paolo INFN, Rome Rome U. Gavrilenko Igor Lebedev Inst. Gay Colin British Columbia U. Gaycken Goetz Bonn U. Gazis Evangelos Natl. Tech. U., Athens Ge Peng Shandong U. Gecse Zoltan British Columbia U. Gee Norman Rutherford Geich-Gimbel Christoph Bonn U. Geisler Manuel Patrice Kirchhoff Inst. Phys. Gemme Claudia INFN, Genoa Genest Marie-Hélène LPSC, Grenoble Gentile Simonetta INFN, Rome Rome U. George Matthias Gottingen U., II. Phys. Inst. George Simon Royal Holloway, U. of London Gerbaudo Davide UC, Irvine Gershon Avi Tel Aviv U. Ghasemi Sara Siegen U. Ghazlane Hamid CNESTEN, Rabat Giacobbe Benedetto INFN, Bologna Giagu Stefano INFN, Rome Rome U. Giangiobbe Vincent Barcelona, IFAE Giannetti Paola INFN, Pisa Pisa U. Gibbard Bruce Brookhaven Gibson Stephen Royal Holloway, U. of London Gilchriese Murdock LBL, Berkeley Gillam Thomas Cambridge U. Gillberg Dag CERN Gilles Geoffrey Clermont-Ferrand U. Gingrich Douglas Alberta U. TRIUMF Giokaris Nikos Athens U. Giordani MarioPaolo INFN, Udine Udine U. Giorgi Filippo Maria INFN, Bologna Giorgi Francesco Michelangelo Humboldt U., Berlin Giraud Pierre-Francois IRFU, Saclay Giromini Paolo Frascati Giugni Danilo INFN, Milan Giuliani Claudia Freiburg U. Giulini Maddalena Heidelberg U. Gjelsten Børge Kile Oslo U. Gkaitatzis Stamatios Aristotle U., Thessaloniki Gkialas Ioannis Aristotle U., Thessaloniki Gkougkousis Evangelos Leonidas Orsay, LAL Gladilin Leonid Moscow State U. Glasman Claudia Madrid, Autonoma U. Glatzer Julian CERN Glaysher Paul Edinburgh U. Glazov Alexandre DESY Goblirsch-Kolb Maximilian Munich, Max Planck Inst. Goddard Jack Robert Queen Mary, U. of London Godlewski Jan Cracow, INP Goldfarb Steven Michigan U. Golling Tobias Geneva U. Golubkov Dmitry Serpukhov, IHEP Gomes Agostinho LIP, Lisbon Lisbon U., CFNUL Gonçalo Ricardo LIP, Lisbon Goncalves Pinto Firmino Da Costa Joao IRFU, Saclay Gonella Laura Bonn U. González de la Hoz Santiago Valencia U., IFIC Gonzalez Parra Garoe Barcelona, IFAE Gonzalez-Sevilla Sergio Geneva U. Goossens Luc CERN Gorbounov Petr Andreevich Moscow, ITEP Gordon Howard Brookhaven Gorelov Igor New Mexico U. Gorini Benedetto CERN Gorini Edoardo INFN, Lecce Salento U. Gorišek Andrej Stefan Inst., Ljubljana Gornicki Edward Cracow, INP Goshaw Alfred Duke U. Gössling Claus Dortmund U. Gostkin Mikhail Ivanovitch Dubna, JINR Goujdami Driss Cadi Ayyad U., Marrakech Goussiou Anna Washington U., Seattle Govender Nicolin Johannesburg U. Gozani Eitan Technion Grabas Herve Marie Xavier UC, Santa Cruz Graber Lars Gottingen U., II. Phys. Inst. Grabowska-Bold Iwona AGH-UST, Cracow Gradin Per Olov Joakim Uppsala U., Inst. Theor. Phys. Grafström Per INFN, Bologna Bologna U. Grahn Karl-Johan DESY Gramling Johanna Geneva U. Gramstad Eirik Oslo U. Grancagnolo Sergio Humboldt U., Berlin Gratchev Vadim St. Petersburg, INP Gray Heather CERN Graziani Enrico INFN, Rome Greenwood Zeno Dixon Louisiana Tech. U. Gregersen Kristian University Coll. London Gregor Ingrid-Maria DESY Grenier Philippe SLAC Griffiths Justin Texas U., Arlington Grillo Alexander UC, Santa Cruz Grimm Kathryn Lancaster U. Grinstein Sebastian Barcelona, IFAE ICREA, Barcelona Gris Philippe Luc Yves Clermont-Ferrand U. Grivaz Jean-Francois Orsay, LAL Grohs Johannes Philipp Dresden, Tech. U. Grohsjean Alexander DESY Gross Eilam Weizmann Inst. Grosse-Knetter Joern Gottingen U., II. Phys. Inst. Grossi Giulio Cornelio Louisiana Tech. U. Grout Zara Jane Sussex U. Guan Liang Michigan U. Guenther Jaroslav Prague, Tech. U. Guescini Francesco Geneva U. Guest Daniel Yale U. Gueta Orel Tel Aviv U. Guido Elisa INFN, Genoa Genoa U. Guillemin Thibault Orsay, LAL Guindon Stefan SUNY, Albany Gul Umar Glasgow U. Gumpert Christian Dresden, Tech. U. Guo Jun Shanghai Jiao Tong U. Guo Yicheng Hefei, CUST Gupta Shaun Oxford U. Gustavino Giuliano INFN, Rome Rome U. Gutierrez Phillip Oklahoma U. Gutierrez Ortiz Nicolas Gilberto University Coll. London Gutschow Christian Dresden, Tech. U. Guyot Claude IRFU, Saclay Gwenlan Claire Oxford U. Gwilliam Carl Liverpool U. Haas Andy New York U. Haber Carl LBL, Berkeley Hadavand Haleh Khani Texas U., Arlington Haddad Nacim Mohammed V U., Agdal Haefner Petra Bonn U. Hageböck Stephan Bonn U. Hajduk Zbigniew Cracow, INP Hakobyan Hrachya Yerevan Phys. Inst. Haleem Mahsana DESY Haley Joseph Oklahoma State U. Hall David Oxford U. Halladjian Garabed Michigan State U. Hallewell Gregory David Marseille, CPPM Hamacher Klaus Wuppertal U. Hamal Petr Palacky U. Hamano Kenji Victoria U. Hamilton Andrew Cape Town U. Hamity Guillermo Nicolas Sheffield U. Hamnett Phillip George DESY Han Liang Hefei, CUST Hanagaki Kazunori KEK, Tsukuba Osaka U. Hanawa Keita Tokyo U., ICEPP Hance Michael LBL, Berkeley Hanke Paul Kirchhoff Inst. Phys. Hanna Remie IRFU, Saclay Hansen Jørgen Beck Bohr Inst. Hansen Jorn Dines Bohr Inst. Hansen Maike Christina Bonn U. Hansen Peter Henrik Bohr Inst. Hara Kazuhiko Tsukuba U. Hard Andrew Wisconsin U., Madison Harenberg Torsten Wuppertal U. Hariri Faten Orsay, LAL Harkusha Siarhei Minsk, Inst. Phys. Harrington Robert Edinburgh U. Harrison Paul Fraser Warwick U. Hartjes Fred FOM, Amsterdam Hasegawa Makoto Kobe U. Hasegawa Satoshi Nagoya U. Hasegawa Yoji Shinshu U. Hasib A Oklahoma U. Hassani Samira IRFU, Saclay Haug Sigve Bern U., LHEP Hauser Reiner Michigan State U. Hauswald Lorenz Dresden, Tech. U. Havranek Miroslav Prague, Inst. Phys. Hawkes Christopher Birmingham U. Hawkings Richard John CERN Hawkins Anthony David Lund U. Hayashi Takayasu Tsukuba U. Hayden Daniel Michigan State U. Hays Chris Oxford U. Hays Jonathan Michael Queen Mary, U. of London Hayward Helen Liverpool U. Haywood Stephen Rutherford Head Simon Birmingham U. Heck Tobias Mainz U. Hedberg Vincent Lund U. Heelan Louise Texas U., Arlington Heim Sarah Pennsylvania U. Heim Timon Wuppertal U. Heinemann Beate LBL, Berkeley Heinrich Lukas New York U. Hejbal Jiri Prague, Inst. Phys. Helary Louis Boston U. Hellman Sten Stockholm U. Stockholm U., OKC Hellmich Dennis Bonn U. Helsens Clement Barcelona, IFAE Henderson James Oxford U. Henderson Robert Lancaster U. Heng Yang Wisconsin U., Madison Hengler Christopher DESY Henrichs Anna Yale U. Henriques Correia Ana Maria CERN Henrot-Versille Sophie Orsay, LAL Herbert Geoffrey Henry Humboldt U., Berlin Hernández Jiménez Yesenia Valencia U., IFIC Herrberg-Schubert Ruth Humboldt U., Berlin Herten Gregor Freiburg U. Hertenberger Ralf Munich U. Hervas Luis CERN Hesketh Gavin Grant University Coll. London Hessey Nigel FOM, Amsterdam Hetherly Jeffrey Wayne Southern Methodist U. Hickling Robert Queen Mary, U. of London Higón-Rodriguez Emilio Valencia U., IFIC Hill Ewan Victoria U. Hill John Cambridge U. Hiller Karl Heinz DESY Hillier Stephen Birmingham U. Hinchliffe Ian LBL, Berkeley Hines Elizabeth Pennsylvania U. Hinman Rachel Reisner LBL, Berkeley Hirose Minoru Tokyo Inst. Tech. Hirschbuehl Dominic Wuppertal U. Hobbs John SUNY, Stony Brook Hod Noam FOM, Amsterdam Hodgkinson Mark Sheffield U. Hodgson Paul Sheffield U. Hoecker Andreas CERN Hoeferkamp Martin New Mexico U. Hoenig Friedrich Munich U. Hohlfeld Marc Mainz U. Hohn David Bonn U. Holmes Tova Ray LBL, Berkeley Homann Michael Dortmund U. Hong Tae Min Pittsburgh U. Hooft van Huysduynen Loek New York U. Hopkins Walter Oregon U. Horii Yasuyuki Nagoya U. Horton Arthur James Simon Fraser U. Hostachy Jean-Yves LPSC, Grenoble Hou Suen Taiwan, Inst. Phys. Hoummada Abdeslam Casablanca U. Howard Jacob Oxford U. Howarth James DESY Hrabovsky Miroslav Palacky U. Hristova Ivana Humboldt U., Berlin Hrivnac Julius Orsay, LAL Hryn'ova Tetiana Annecy, LAPP Hrynevich Aliaksei Minsk, High Energy Phys. Ctr. Hsu Catherine Witwatersrand U. Hsu Pai-hsien Jennifer Taiwan, Inst. Phys. Taiwan, Natl. Tsing Hua U. Hsu Shih-Chieh Washington U., Seattle Hu Diedi Nevis Labs, Columbia U. Hu Qipeng Hefei, CUST Hu Xueye Michigan U. Huang Yanping DESY Hubacek Zdenek Prague, Tech. U. Hubaut Fabrice Marseille, CPPM Huegging Fabian Bonn U. Huffman Todd Brian Oxford U. Hughes Emlyn Nevis Labs, Columbia U. Hughes Gareth Lancaster U. Huhtinen Mika CERN Hülsing Tobias Alexander Mainz U. Huseynov Nazim Dubna, JINR Baku, Inst. Phys. Huston Joey Michigan State U. Huth John Harvard U., Phys. Dept. Iacobucci Giuseppe Geneva U. Iakovidis Georgios Brookhaven Ibragimov Iskander Siegen U. Iconomidou-Fayard Lydia Orsay, LAL Ideal Emma Yale U. Idrissi Zineb Mohammed V U., Agdal Iengo Paolo CERN Igonkina Olga FOM, Amsterdam Iizawa Tomoya Waseda U. Ikegami Yoichi KEK, Tsukuba Ikematsu Katsumasa Siegen U. Ikeno Masahiro KEK, Tsukuba Ilchenko Iurii Chicago U., EFI Texas U. Iliadis Dimitrios Aristotle U., Thessaloniki Ilic Nikolina SLAC Ince Tayfun Munich, Max Planck Inst. Introzzi Gianluca INFN, Pavia Pavia U. Ioannou Pavlos Athens U. Iodice Mauro INFN, Rome Iordanidou Kalliopi Nevis Labs, Columbia U. Ippolito Valerio Harvard U., Phys. Dept. Irles Quiles Adrian Valencia U., IFIC Isaksson Charlie Uppsala U., Inst. Theor. Phys. Ishino Masaya Kyoto U. Ishitsuka Masaki Tokyo Inst. Tech. Ishmukhametov Renat Ohio State U. Issever Cigdem Oxford U. Istin Serhat Bogazici U. Iturbe Ponce Julia Mariana Manchester U. Iuppa Roberto INFN, Rome Rome U., Tor Vergata Ivarsson Jenny Lund U. Iwanski Wieslaw Cracow, INP Iwasaki Hiroyuki KEK, Tsukuba Izen Joseph Texas U., Dallas Izzo Vincenzo INFN, Naples Jabbar Samina Alberta U. Jackson Brett Pennsylvania U. Jackson Matthew Liverpool U. Jackson Paul Adelaide U., Sch. Chem. Phys. Jaekel Martin CERN Jain Vivek SUNY, Albany Jakobs Karl Freiburg U. Jakobsen Sune CERN Jakoubek Tomas Prague, Inst. Phys. Jakubek Jan Prague, Tech. U. Jamin David Olivier Oklahoma State U. Jana Dilip Louisiana Tech. U. Jansen Eric University Coll. London Jansky Roland Innsbruck U. Janssen Jens Bonn U. Janus Michel Gottingen U., II. Phys. Inst. Jarlskog Göran Lund U. Javadov Namig Dubna, JINR Baku, Inst. Phys. Javůrek Tomáš Freiburg U. Jeanty Laura LBL, Berkeley Jejelava Juansher Tbilisi, Inst. Phys. Ilia State U. Jeng Geng-yuan Sydney U. Jennens David Melbourne U. Jenni Peter Freiburg U. CERN Jentzsch Jennifer Dortmund U. Jeske Carl Warwick U. Jézéquel Stéphane Annecy, LAPP Ji Haoshuang Wisconsin U., Madison Jia Jiangyong SUNY, Stony Brook Jiang Yi Hefei, CUST Jiggins Stephen University Coll. London Jimenez Pena Javier Valencia U., IFIC Jin Shan Beijing, Inst. High Energy Phys. Jinaru Adam Bucharest, IFIN-HH Jinnouchi Osamu Tokyo Inst. Tech. Joergensen Morten Dam Bohr Inst. Johansson Per Sheffield U. Johns Kenneth Arizona U. Jon-And Kerstin Stockholm U. Stockholm U., OKC Jones Graham Warwick U. Jones Roger Lancaster U. Jones Tim Liverpool U. Jongmanns Jan Kirchhoff Inst. Phys. Jorge Pedro LIP, Lisbon Lisbon U., CFNUL Joshi Kiran Daniel Manchester U. Jovicevic Jelena TRIUMF Ju Xiangyang Wisconsin U., Madison Jung Christian Dortmund U. Jussel Patrick Innsbruck U. Juste Rozas Aurelio Barcelona, IFAE ICREA, Barcelona Kaci Mohammed Valencia U., IFIC Kaczmarska Anna Cracow, INP Kado Marumi Orsay, LAL Kagan Harris Ohio State U. Kagan Michael SLAC Kahn Sebastien Jonathan Marseille, CPPM Kajomovitz Enrique Duke U. Kalderon Charles William Oxford U. Kama Sami Southern Methodist U. Kamenshchikov Andrey Serpukhov, IHEP Kanaya Naoko Tokyo U., ICEPP Kaneti Steven Cambridge U. Kantserov Vadim Moscow Phys. Eng. Inst. Kanzaki Junichi KEK, Tsukuba Kaplan Benjamin New York U. Kaplan Laser Seymour Wisconsin U., Madison Kapliy Anton Chicago U., EFI Kar Deepak Witwatersrand U. Karakostas Konstantinos Natl. Tech. U., Athens Karamaoun Andrew Alberta U. Karastathis Nikolaos Natl. Tech. U., Athens FOM, Amsterdam Kareem Mohammad Jawad Gottingen U., II. Phys. Inst. Karentzos Efstathios Natl. Tech. U., Athens Karnevskiy Mikhail Mainz U. Karpov Sergey Dubna, JINR Karpova Zoya Dubna, JINR Karthik Krishnaiyengar New York U. Kartvelishvili Vakhtang Lancaster U. Karyukhin Andrey Serpukhov, IHEP Kashif Lashkar Wisconsin U., Madison Kass Richard Ohio State U. Kastanas Alex Bergen U. Kataoka Yousuke Tokyo U., ICEPP Kato Chikuma Tokyo U., ICEPP Katre Akshay Geneva U. Katzy Judith DESY Kawagoe Kiyotomo Kyushu U. Kawamoto Tatsuo Tokyo U., ICEPP Kawamura Gen Gottingen U., II. Phys. Inst. Kazama Shingo Tokyo U., ICEPP Kazanin Vassili Novosibirsk, IYF Novosibirsk State U. Keeler Richard Victoria U. Kehoe Robert Southern Methodist U. Keller John DESY Kempster Jacob Julian Royal Holloway, U. of London Keoshkerian Houry Manchester U. Kepka Oldrich Prague, Inst. Phys. Kerševan Borut Paul Stefan Inst., Ljubljana Kersten Susanne Wuppertal U. Keyes Robert McGill U. Khalil-zada Farkhad Baku, Inst. Phys. Khandanyan Hovhannes Stockholm U. Stockholm U., OKC Khanov Alexander Oklahoma State U. Kharlamov Alexey Novosibirsk, IYF Novosibirsk State U. Khoo Teng Jian Cambridge U. Khovanskiy Valery Moscow, ITEP Khramov Evgeniy Dubna, JINR Khubua Jemal Tbilisi State U. GTU, Tbilisi Kido Shogo Kobe U. Kim Hee Yeun Texas U., Arlington Kim Shinhong Tsukuba U. Kim Young-Kee Chicago U., EFI Kimura Naoki Aristotle U., Thessaloniki Kind Oliver Maria Humboldt U., Berlin King Barry Liverpool U. King Matthew Valencia U., IFIC King Samuel Burton British Columbia U. Kirk Julie Rutherford Kiryunin Andrey Munich, Max Planck Inst. Kishimoto Tomoe Kobe U. Kisielewska Danuta AGH-UST, Cracow Kiss Florian Freiburg U. Kiuchi Kenji Tsukuba U. Kivernyk Oleh IRFU, Saclay Kladiva Eduard Kosice, IEF Klein Matthew Henry Nevis Labs, Columbia U. Klein Max Liverpool U. Klein Uta Liverpool U. Kleinknecht Konrad Mainz U. Klimek Pawel Stockholm U. Stockholm U., OKC Klimentov Alexei Brookhaven Klingenberg Reiner Dortmund U. Klinger Joel Alexander Sheffield U. Klioutchnikova Tatiana CERN Kluge Eike-Erik Kirchhoff Inst. Phys. Kluit Peter FOM, Amsterdam Kluth Stefan Munich, Max Planck Inst. Knapik Joanna Cracow, INP Kneringer Emmerich Innsbruck U. Knoops Edith Marseille, CPPM Knue Andrea Glasgow U. Kobayashi Aine Tokyo U., ICEPP Kobayashi Dai Tokyo Inst. Tech. Kobayashi Tomio Tokyo U., ICEPP Kobel Michael Dresden, Tech. U. Kocian Martin SLAC Kodys Peter Charles U. Koffas Thomas Carleton U. Koffeman Els FOM, Amsterdam Kogan Lucy Anne Oxford U. Kohlmann Simon Wuppertal U. Kohout Zdenek Prague, Tech. U. Kohriki Takashi KEK, Tsukuba Koi Tatsumi SLAC Kolanoski Hermann Humboldt U., Berlin Koletsou Iro Annecy, LAPP Komar Aston Lebedev Inst. Komori Yuto Tokyo U., ICEPP Kondo Takahiko KEK, Tsukuba Kondrashova Nataliia DESY Köneke Karsten Freiburg U. König Adriaan NIKHEF, Amsterdam Kono Takanori KEK, Tsukuba Konoplich Rostislav New York U. Manhattan Coll., Riverdale Konstantinidis Nikolaos University Coll. London Kopeliansky Revital Technion Koperny Stefan AGH-UST, Cracow Köpke Lutz Mainz U. Kopp Anna Katharina Freiburg U. Korcyl Krzysztof Cracow, INP Kordas Kostantinos Aristotle U., Thessaloniki Korn Andreas University Coll. London Korol Aleksandr Novosibirsk, IYF Novosibirsk State U. Korolkov Ilya Barcelona, IFAE Korolkova Elena Sheffield U. Kortner Oliver Munich, Max Planck Inst. Kortner Sandra Munich, Max Planck Inst. Kosek Tomas Charles U. Kostyukhin Vadim Bonn U. Kotov Vladislav Dubna, JINR Kotwal Ashutosh Duke U. Kourkoumeli-Charalampidi Athina Aristotle U., Thessaloniki Kourkoumelis Christine Athens U. Kouskoura Vasiliki Brookhaven Koutsman Alex TRIUMF Kowalewski Robert Victor Victoria U. Kowalski Tadeusz AGH-UST, Cracow Kozanecki Witold IRFU, Saclay Kozhin Anatoly Serpukhov, IHEP Kramarenko Viktor Moscow State U. Kramberger Gregor Stefan Inst., Ljubljana Krasnopevtsev Dimitriy Moscow Phys. Eng. Inst. Krasny Mieczyslaw Witold Paris U., VI-VII Krasznahorkay Attila CERN Kraus Jana Bonn U. Kravchenko Anton Brookhaven Kreiss Sven New York U. Kretz Moritz Heidelberg U. Kretzschmar Jan Liverpool U. Kreutzfeldt Kristof Giessen U. Krieger Peter Toronto U. Krizka Karol Chicago U., EFI Kroeninger Kevin Dortmund U. Kroha Hubert Munich, Max Planck Inst. Kroll Joe Pennsylvania U. Kroseberg Juergen Bonn U. Krstic Jelena Belgrade U. Kruchonak Uladzimir Dubna, JINR Krüger Hans Bonn U. Krumnack Nils Iowa State U. Kruse Amanda Wisconsin U., Madison Kruse Mark Duke U. Kruskal Michael Boston U. Kubota Takashi Melbourne U. Kucuk Hilal University Coll. London Kuday Sinan Istanbul Aydin U. Kuehn Susanne Freiburg U. Kugel Andreas Heidelberg U. Kuger Fabian Wurzburg U. Kuhl Andrew UC, Santa Cruz Kuhl Thorsten DESY Kukhtin Victor Dubna, JINR Kulchitsky Yuri Minsk, Inst. Phys. Kuleshov Sergey Santa Maria U., Valparaiso Kuna Marine INFN, Rome Rome U. Kunigo Takuto Kyoto U. Kupco Alexander Prague, Inst. Phys. Kurashige Hisaya Kobe U. Kurochkin Yurii Minsk, Inst. Phys. Kus Vlastimil Prague, Inst. Phys. Kuwertz Emma Sian Victoria U. Kuze Masahiro Tokyo Inst. Tech. Kvita Jiri Palacky U. Kwan Tony Victoria U. Kyriazopoulos Dimitrios Sheffield U. La Rosa Alessandro UC, Santa Cruz La Rosa Navarro Jose Luis Sao Paulo U. La Rotonda Laura INFN, Cosenza Calabria U. Lacasta Carlos Valencia U., IFIC Lacava Francesco INFN, Rome Rome U. Lacey James Carleton U. Lacker Heiko Humboldt U., Berlin Lacour Didier Paris U., VI-VII Lacuesta Vicente Ramón Valencia U., IFIC Ladygin Evgueni Dubna, JINR Lafaye Remi Annecy, LAPP Laforge Bertrand Paris U., VI-VII Lagouri Theodota Yale U. Lai Stanley Gottingen U., II. Phys. Inst. Lambourne Luke University Coll. London Lammers Sabine Indiana U. Lampen Caleb Arizona U. Lampl Walter Arizona U. Lançon Eric IRFU, Saclay Landgraf Ulrich Freiburg U. Landon Murrough Queen Mary, U. of London Lang Valerie Susanne Kirchhoff Inst. Phys. Lange J örn Christian Barcelona, IFAE Lankford Andrew UC, Irvine Lanni Francesco Brookhaven Lantzsch Kerstin CERN Lanza Agostino INFN, Pavia Laplace Sandrine Paris U., VI-VII Lapoire Cecile CERN Laporte Jean-Francois IRFU, Saclay Lari Tommaso INFN, Milan Lasagni Manghi Federico INFN, Bologna Bologna U. 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London Lenz Tatjana Bonn U. Lenzi Bruno CERN Leone Robert Arizona U. Leone Sandra INFN, Pisa Pisa U. Leonidopoulos Christos Edinburgh U. Leontsinis Stefanos Natl. Tech. U., Athens Leroy Claude Montreal U. Lester Christopher Cambridge U. Levchenko Mikhail St. Petersburg, INP Levêque Jessica Annecy, LAPP Levin Daniel Michigan U. Levinson Lorne Weizmann Inst. Levy Mark Birmingham U. Lewis Adrian Oxford U. Leyko Agnieszka Bonn U. Leyton Michael Texas U., Dallas Li Bing Hefei, CUST Taiwan, Inst. Phys. Li Haifeng SUNY, Stony Brook Li Ho Ling Chicago U., EFI Li Lei Duke U. Li Liang Shanghai Jiao Tong U. Li Shu Duke U. Li Xingguo Manchester U. Li Yichen Nanjing U. Orsay, LAL Liang Zhijun UC, Santa Cruz Liao Hongbo Clermont-Ferrand U. Liberti Barbara INFN, Rome Liblong Aaron Toronto U. Lichard Peter CERN Lie Ki Illinois U., Urbana Liebal Jessica Bonn U. Liebig Wolfgang Bergen U. Limbach Christian Bonn U. Limosani Antonio Sydney U. Lin Simon Taiwan, Inst. Phys. Lin Tai-Hua Mainz U. Linde Frank FOM, Amsterdam Lindquist Brian Edward SUNY, Stony Brook Linnemann James Michigan State U. Lipeles Elliot Pennsylvania U. Lipniacka Anna Bergen U. Lisovyi Mykhailo Heidelberg U. Liss Tony Illinois U., Urbana Lissauer David Brookhaven Lister Alison British Columbia U. Litke Alan UC, Santa Cruz Liu Bo Taiwan, Inst. Phys. Shandong U. Liu Dong Taiwan, Inst. Phys. Liu Hao Michigan U. Liu Jian Marseille, CPPM Liu Jianbei Hefei, CUST Liu Kun Marseille, CPPM Liu Lulu Illinois U., Urbana Liu Miaoyuan Duke U. Liu Minghui Hefei, CUST Liu Yanwen Hefei, CUST Livan Michele INFN, Pavia Pavia U. Lleres Annick LPSC, Grenoble Llorente Merino Javier Madrid, Autonoma U. Lloyd Stephen Queen Mary, U. of London Lo Sterzo Francesco Taiwan, Inst. Phys. Lobodzinska Ewelina DESY Loch Peter Arizona U. Lockman William UC, Santa Cruz Loebinger Fred Manchester U. Loevschall-Jensen Ask Emil Bohr Inst. Loginov Andrey Yale U. Lohse Thomas Humboldt U., Berlin Lohwasser Kristin DESY Lokajicek Milos Prague, Inst. Phys. Long Brian Alexander Boston U. Long Jonathan David Michigan U. Long Robin Eamonn Lancaster U. Looper Kristina Anne Ohio State U. Lopes Lourenco LIP, Lisbon Lopez Mateos David Harvard U., Phys. Dept. Lopez Paredes Brais Sheffield U. Lopez Paz Ivan Barcelona, IFAE Lorenz Jeanette Munich U. Lorenzo Martinez Narei Indiana U. Losada Marta Antonio Narino U. Loscutoff Peter LBL, Berkeley Lösel Philipp Jonathan Munich U. Lou XinChou Beijing, Inst. High Energy Phys. Lounis Abdenour Orsay, LAL Love Jeremy Argonne Love Peter Lancaster U. Lu Nan Michigan U. Lubatti Henry Washington U., Seattle Luci Claudio INFN, Rome Rome U. Lucotte Arnaud LPSC, Grenoble Luehring Frederick Indiana U. Lukas Wolfgang Innsbruck U. Luminari Lamberto INFN, Rome Lundberg Olof Stockholm U. Stockholm U., OKC Lund-Jensen Bengt Royal Inst. Tech., Stockholm Lynn David Brookhaven Lysak Roman Prague, Inst. Phys. Lytken Else Lund U. Ma Hong Brookhaven Ma Lian Liang Shandong U. Maccarrone Giovanni Frascati Macchiolo Anna Munich, Max Planck Inst. Macdonald Calum Michael Sheffield U. Maček Boštjan Stefan Inst., Ljubljana Machado Miguens Joana Pennsylvania U. Lisbon U., CFNUL Macina Daniela CERN Madaffari Daniele Marseille, CPPM Madar Romain Clermont-Ferrand U. Maddocks Harvey Jonathan Lancaster U. Mader Wolfgang Dresden, Tech. U. Madsen Alexander Uppsala U., Inst. Theor. Phys. Maeda Junpei Kobe U. Maeland Steffen Bergen U. Maeno Tadashi Brookhaven Maevskiy Artem Moscow State U. Magradze Erekle Gottingen U., II. Phys. Inst. Mahboubi Kambiz Freiburg U. Mahlstedt Joern FOM, Amsterdam Maiani Camilla IRFU, Saclay Maidantchik Carmen Rio de Janeiro Federal U. Maier Andreas Alexander Munich, Max Planck Inst. Maier Thomas Munich U. Maio Amélia LIP, Lisbon Lisbon U., CFNUL Majewski Stephanie Oregon U. Makida Yasuhiro KEK, Tsukuba Makovec Nikola Orsay, LAL Malaescu Bogdan Paris U., VI-VII Malecki Pawel Cracow, INP Maleev Victor St. Petersburg, INP Malek Fairouz LPSC, Grenoble Mallik Usha Iowa U. Malon David Argonne Malone Caitlin SLAC Maltezos Stavros Natl. Tech. U., Athens Malyshev Vladimir Novosibirsk, IYF Malyukov Sergei CERN Mamuzic Judita DESY Mancini Giada Frascati Mandelli Beatrice CERN Mandelli Luciano INFN, Milan Mandić Igor Stefan Inst., Ljubljana Mandrysch Rocco Iowa U. Maneira José LIP, Lisbon Lisbon U., CFNUL Manfredini Alessandro Munich, Max Planck Inst. Manhaes de Andrade Filho Luciano Juiz de Fora U. Manjarres Ramos Joany York U., Canada Mann Alexander Munich U. Manousakis-Katsikakis Arkadios Athens U. Mansoulie Bruno IRFU, Saclay Mantifel Rodger McGill U. Mantoani Matteo Gottingen U., II. Phys. Inst. Mapelli Livio CERN March Luis Witwatersrand U. Marchiori Giovanni Paris U., VI-VII Marcisovsky Michal Prague, Inst. Phys. Marino Christopher Victoria U. Marjanovic Marija Belgrade U. Marley Daniel Michigan U. Marroquim Fernando Rio de Janeiro Federal U. Marsden Stephen Philip Manchester U. Marshall Zach LBL, Berkeley Marti Lukas Fritz Bern U., LHEP Marti-Garcia Salvador Valencia U., IFIC Martin Brian Thomas Michigan State U. Martin Tim Warwick U. Martin Victoria Jane Edinburgh U. Martin dit Latour Bertrand Bergen U. Martinez Mario Barcelona, IFAE ICREA, Barcelona Martin-Haugh Stewart Rutherford Martoiu Victor Sorin Bucharest, IFIN-HH Martyniuk Alex University Coll. London Marx Marilyn Washington U., Seattle Marzano Francesco INFN, Rome Marzin Antoine CERN Masetti Lucia Mainz U. Mashimo Tetsuro Tokyo U., ICEPP Mashinistov Ruslan Lebedev Inst. Masik Jiri Manchester U. Maslennikov Alexey Novosibirsk, IYF Novosibirsk State U. Massa Ignazio INFN, Bologna Bologna U. Massa Lorenzo INFN, Bologna Bologna U. Massol Nicolas Annecy, LAPP Mastrandrea Paolo SUNY, Stony Brook Mastroberardino Anna INFN, Cosenza Calabria U. Masubuchi Tatsuya Tokyo U., ICEPP Mättig Peter Wuppertal U. Mattmann Johannes Mainz U. Maurer Julien Bucharest, IFIN-HH Maxfield Stephen Liverpool U. Maximov Dmitriy Novosibirsk, IYF Novosibirsk State U. Mazini Rachid Taiwan, Inst. Phys. Mazza Simone Michele INFN, Milan Milan U. Mazzaferro Luca INFN, Rome Rome U., Tor Vergata Mc Goldrick Garrin Toronto U. Mc Kee Shawn Patrick Michigan U. McCarn Allison Michigan U. McCarthy Robert SUNY, Stony Brook McCarthy Tom Carleton U. McCubbin Norman Rutherford McFarlane Kenneth Hampton U. Mcfayden Josh University Coll. London Mchedlidze Gvantsa Gottingen U., II. Phys. Inst. McMahon Steve Rutherford McPherson Robert Victoria U. IPP, Canada Medinnis Michael DESY Meehan Samuel Cape Town U. Mehlhase Sascha Munich U. Mehta Andrew Liverpool U. Meier Karlheinz Kirchhoff Inst. Phys. Meineck Christian Munich U. Meirose Bernhard Texas U., Dallas Mellado Garcia Bruce Rafael Witwatersrand U. Meloni Federico Bern U., LHEP Mengarelli Alberto INFN, Bologna Bologna U. Menke Sven Munich, Max Planck Inst. Meoni Evelin Tufts U. Mercurio Kevin Michael Harvard U., Phys. Dept. Mergelmeyer Sebastian Bonn U. Mermod Philippe Geneva U. Merola Leonardo INFN, Naples Naples U. Meroni Chiara INFN, Milan Merritt Frank Chicago U., EFI Messina Andrea INFN, Rome Rome U. Metcalfe Jessica Brookhaven Mete Alaettin Serhan UC, Irvine Meyer Carsten Mainz U. Meyer Christopher Pennsylvania U. Meyer Jean-Pierre IRFU, Saclay Meyer Jochen FOM, Amsterdam Meyer Zu Theenhausen Hanno Kirchhoff Inst. Phys. Middleton Robin Rutherford Miglioranzi Silvia INFN, Udine Udine U. Mijović Liza Bonn U. Mikenberg Giora Weizmann Inst. Mikestikova Marcela Prague, Inst. Phys. Mikuž Marko Stefan Inst., Ljubljana Milesi Marco Melbourne U. Milic Adriana CERN Miller David Chicago U., EFI Mills Corrinne Edinburgh U. Milov Alexander Weizmann Inst. Milstead David Stockholm U. Stockholm U., OKC Minaenko Andrey Serpukhov, IHEP Minami Yuto Tokyo U., ICEPP Minashvili Irakli Dubna, JINR Mincer Allen New York U. Mindur Bartosz AGH-UST, Cracow Mineev Mikhail Dubna, JINR Ming Yao Wisconsin U., Madison Mir Lluisa-Maria Barcelona, IFAE Mitani Takashi Waseda U. Mitrevski Jovan Munich U. Mitsou Vasiliki A Valencia U., IFIC Miucci Antonio Geneva U. Miyagawa Paul Sheffield U. Mjörnmark Jan-Ulf Lund U. Moa Torbjoern Stockholm U. Stockholm U., OKC Mochizuki Kazuya Marseille, CPPM Mohapatra Soumya Nevis Labs, Columbia U. Mohr Wolfgang Freiburg U. Molander Simon Stockholm U. Stockholm U., OKC Moles-Valls Regina Bonn U. Mönig Klaus DESY Monini Caterina LPSC, Grenoble Monk James Bohr Inst. Monnier Emmanuel Marseille, CPPM Montejo Berlingen Javier Barcelona, IFAE Monticelli Fernando La Plata U. Monzani Simone INFN, Rome Rome U. Moore Roger Alberta U. Morange Nicolas Orsay, LAL Moreno Deywis Antonio Narino U. Moreno Llácer María Gottingen U., II. Phys. Inst. Morettini Paolo INFN, Genoa Mori Daniel Simon Fraser U. Morii Masahiro Harvard U., Phys. Dept. Morinaga Masahiro Tokyo U., ICEPP Morisbak Vanja Oslo U. Moritz Sebastian Mainz U. Morley Anthony Keith Sydney U. Mornacchi Giuseppe CERN Morris John Queen Mary, U. of London Mortensen Simon Stark Bohr Inst. Morton Alexander Glasgow U. Morvaj Ljiljana Nagoya U. Mosidze Maia Tbilisi State U. Moss Josh Ohio State U. Motohashi Kazuki Tokyo Inst. Tech. Mount Richard SLAC Mountricha Eleni Brookhaven Mouraviev Sergei Lebedev Inst. Moyse Edward Massachusetts U., Amherst Muanza Steve Marseille, CPPM Mudd Richard Birmingham U. Mueller Felix Munich, Max Planck Inst. Mueller James Pittsburgh U. Mueller Ralph Soeren Peter Munich U. Mueller Thibaut Cambridge U. Muenstermann Daniel Geneva U. Mullen Paul Glasgow U. Mullier Geoffrey Bern U., LHEP Murillo Quijada Javier Alberto Birmingham U. Murray Bill Warwick U. Rutherford Musheghyan Haykuhi Gottingen U., II. Phys. Inst. Musto Elisa Technion Myagkov Alexey Serpukhov, IHEP Moscow, MIPT Myska Miroslav Prague, Tech. U. Nachman Benjamin Philip SLAC Nackenhorst Olaf Gottingen U., II. Phys. Inst. Nadal Jordi Gottingen U., II. Phys. Inst. Nagai Koichi Oxford U. Nagai Ryo Tokyo Inst. Tech. Nagai Yoshikazu Marseille, CPPM Nagano Kunihiro KEK, Tsukuba Nagarkar Advait Ohio State U. Nagasaka Yasushi Hiroshima Inst. Tech. Nagata Kazuki Tsukuba U. Nagel Martin Munich, Max Planck Inst. Nagy Elemer Marseille, CPPM Nairz Armin Michael CERN Nakahama Yu CERN Nakamura Koji KEK, Tsukuba Nakamura Tomoaki Tokyo U., ICEPP Nakano Itsuo Okayama U. Namasivayam Harisankar Texas U., Dallas Naranjo Garcia Roger Felipe DESY Narayan Rohin Chicago U., EFI Narrias Villar Daniel Isaac Kirchhoff Inst. Phys. Naumann Thomas DESY Navarro Gabriela Antonio Narino U. Nayyar Ruchika Arizona U. Neal Homer Michigan U. Nechaeva Polina Lebedev Inst. Neep Thomas James Manchester U. Nef Pascal Daniel SLAC Negri Andrea INFN, Pavia Pavia U. Negrini Matteo INFN, Bologna Nektarijevic Snezana NIKHEF, Amsterdam Nellist Clara Orsay, LAL Nelson Andrew UC, Irvine Nemecek Stanislav Prague, Inst. Phys. Nemethy Peter New York U. Nepomuceno Andre Asevedo Rio de Janeiro Federal U. Nessi Marzio CERN Geneva U. Neubauer Mark Illinois U., Urbana Neumann Manuel Wuppertal U. Neves Ricardo New York U. Nevski Pavel Brookhaven Newman Paul Birmingham U. Nguyen Duong Hai Argonne Nickerson Richard Oxford U. Nicolaidou Rosy IRFU, Saclay Nicquevert Bertrand CERN Nielsen Jason UC, Santa Cruz Nikiforou Nikiforos Nevis Labs, Columbia U. Nikiforov Andriy Humboldt U., Berlin Nikolaenko Vladimir Serpukhov, IHEP Moscow, MIPT Nikolic-Audit Irena Paris U., VI-VII Nikolopoulos Konstantinos Birmingham U. Nilsen Jon Kerr Oslo U. Nilsson Paul Brookhaven Ninomiya Yoichi Tokyo U., ICEPP Nisati Aleandro INFN, Rome Nisius Richard Munich, Max Planck Inst. Nobe Takuya Tokyo U., ICEPP Nomachi Masaharu Osaka U. Nomidis Ioannis Carleton U. Nooney Tamsin Queen Mary, U. of London Norberg Scarlet Oklahoma U. Nordberg Markus CERN Novgorodova Olga Dresden, Tech. U. Nowak Sebastian Munich, Max Planck Inst. Nozaki Mitsuaki KEK, Tsukuba Nozka Libor Palacky U. Ntekas Konstantinos Natl. Tech. U., Athens Nunes Hanninger Guilherme Melbourne U. Nunnemann Thomas Munich U. Nurse Emily University Coll. London Nuti Francesco Melbourne U. O'Brien Brendan Joseph Edinburgh U. O'grady Fionnbarr Arizona U. O'Neil Dugan Simon Fraser U. O'Shea Val Glasgow U. Oakham Gerald Carleton U. TRIUMF Oberlack Horst Munich, Max Planck Inst. Obermann Theresa Bonn U. Ocariz Jose Paris U., VI-VII Ochi Atsuhiko Kobe U. Ochoa Ines University Coll. London Ochoa-Ricoux Juan Pedro Chile U., Catolica Oda Susumu Kyushu U. Odaka Shigeru KEK, Tsukuba Ogren Harold Indiana U. Oh Alexander Manchester U. Oh Seog Duke U. Ohm Christian LBL, Berkeley Ohman Henrik Uppsala U., Inst. Theor. Phys. Oide Hideyuki CERN Okamura Wataru Osaka U. Okawa Hideki Tsukuba U. Okumura Yasuyuki Chicago U., EFI Okuyama Toyonobu KEK, Tsukuba Olariu Albert Bucharest, IFIN-HH Olivares Pino Sebastian Andres Edinburgh U. Oliveira Damazio Denis Brookhaven Oliver Garcia Elena Valencia U., IFIC Olszewski Andrzej Cracow, INP Olszowska Jolanta Cracow, INP Onofre António LIP, Lisbon Minho U. Onyisi Peter Chicago U., EFI Texas U. Oram Christopher TRIUMF Oreglia Mark Chicago U., EFI Oren Yona Tel Aviv U. Orestano Domizia INFN, Rome Rome III U. Orlando Nicola Aristotle U., Thessaloniki Oropeza Barrera Cristina Glasgow U. Orr Robert Toronto U. Osculati Bianca INFN, Genoa Genoa U. Ospanov Rustem Manchester U. Otero y Garzon Gustavo Buenos Aires U. Otono Hidetoshi Kyushu U. Ouchrif Mohamed Oujda U. Ould-Saada Farid Oslo U. Ouraou Ahmimed IRFU, Saclay Oussoren Koen Pieter FOM, Amsterdam Ouyang Qun Beijing, Inst. High Energy Phys. Ovcharova Ana LBL, Berkeley Owen Mark Glasgow U. Owen Rhys Edward Birmingham U. Ozcan Veysi Erkcan Bogazici U. Ozturk Nurcan Texas U., Arlington Pachal Katherine Simon Fraser U. Pacheco Pages Andres Barcelona, IFAE Padilla Aranda Cristobal Barcelona, IFAE Pagáčová Martina Freiburg U. Pagan Griso Simone LBL, Berkeley Paganis Efstathios Sheffield U. Paige Frank Brookhaven Pais Preema Massachusetts U., Amherst Pajchel Katarina Oslo U. Palacino Gabriel York U., Canada Palestini Sandro CERN Palka Marek Jagiellonian U. Pallin Dominique Clermont-Ferrand U. Palma Alberto LIP, Lisbon Lisbon U., CFNUL Pan Yibin Wisconsin U., Madison Panagiotopoulou Evgenia Natl. Tech. U., Athens Pandini Carlo Enrico Paris U., VI-VII Panduro Vazquez William Royal Holloway, U. of London Pani Priscilla Stockholm U. Stockholm U., OKC Panitkin Sergey Brookhaven Pantea Dan Bucharest, IFIN-HH Paolozzi Lorenzo Geneva U. Papadopoulou Theodora Natl. Tech. U., Athens Papageorgiou Konstantinos Aristotle U., Thessaloniki Paramonov Alexander Argonne Paredes Hernandez Daniela Aristotle U., Thessaloniki Parker Michael Andrew Cambridge U. Parker Kerry Ann Sheffield U. Parodi Fabrizio INFN, Genoa Genoa U. Parsons John Nevis Labs, Columbia U. Parzefall Ulrich Freiburg U. Pasqualucci Enrico INFN, Rome Passaggio Stefano INFN, Genoa Pastore Fernanda INFN, Rome Rome III U. Pastore Francesca Royal Holloway, U. of London Pásztor Gabriella Carleton U. Pataraia Sophio Wuppertal U. Patel Nikhul Sydney U. Pater Joleen Manchester U. Pauly Thilo CERN Pearce James Victoria U. Pearson Benjamin Oklahoma U. Pedersen Lars Egholm Bohr Inst. Pedersen Maiken Oslo U. Pedraza Lopez Sebastian Valencia U., IFIC Pedro Rute LIP, Lisbon Lisbon U., CFNUL Peleganchuk Sergey Novosibirsk, IYF Novosibirsk State U. Pelikan Daniel Uppsala U., Inst. Theor. Phys. Penc Ondrej Prague, Inst. Phys. Peng Cong Beijing, Inst. High Energy Phys. 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Serfon Cedric CERN Serin Laurent Orsay, LAL Serkin Leonid INFN, Udine ICTP, Trieste Serre Thomas Marseille, CPPM Sessa Marco INFN, Rome Rome III U. Seuster Rolf TRIUMF Severini Horst Oklahoma U. Sfiligoj Tina Stefan Inst., Ljubljana Sforza Federico CERN Sfyrla Anna CERN Shabalina Elizaveta Gottingen U., II. Phys. Inst. Shamim Mansoora Oregon U. Shan Lianyou Beijing, Inst. High Energy Phys. Shang Ruo-yu Illinois U., Urbana Shank James Boston U. Shapiro Marjorie LBL, Berkeley Shatalov Pavel Moscow, ITEP Shaw Kate INFN, Udine ICTP, Trieste Shaw Savanna Marie Manchester U. Shcherbakova Anna Stockholm U. Stockholm U., OKC Shehu Ciwake Yusufu Sussex U. Sherwood Peter University Coll. London Shi Liaoshan Taiwan, Inst. Phys. Zhongshan U. Shimizu Shima Kobe U. Shimmin Chase Owen UC, Irvine Shimojima Makoto Nagasaki Inst. Appl. Sci. Shiyakova Mariya Dubna, JINR Shmeleva Alevtina Lebedev Inst. Shoaleh Saadi Diane Montreal U. Shochet Mel Chicago U., EFI Shojaii Seyedruhollah INFN, Milan Milan U. 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Skottowe Hugh Philip Harvard U., Phys. Dept. Skubic Patrick Oklahoma U. Slater Mark Birmingham U. Slavicek Tomas Prague, Tech. U. Slawinska Magdalena FOM, Amsterdam Sliwa Krzysztof Tufts U. Smakhtin Vladimir Weizmann Inst. Smart Ben Edinburgh U. Smestad Lillian Bergen U. Smirnov Sergei Moscow Phys. Eng. Inst. Smirnov Yury Moscow Phys. Eng. Inst. Smirnova Lidia Moscow State U. Lomonosov Moscow State U. Smirnova Oxana Lund U. Smith Matthew Nevis Labs, Columbia U. Smith Russell Nevis Labs, Columbia U. Smizanska Maria Lancaster U. Smolek Karel Prague, Tech. U. Snesarev Andrei Lebedev Inst. Snidero Giacomo Queen Mary, U. of London Snyder Scott Brookhaven Sobie Randall Victoria U. IPP, Canada Socher Felix Dresden, Tech. U. Soffer Abner Tel Aviv U. Soh Dart-yin Taiwan, Inst. Phys. Zhongshan U. Solans Carlos CERN Solar Michael Prague, Tech. U. Solc Jaroslav Prague, Tech. U. Soldatov Evgeny Moscow Phys. Eng. Inst. Soldevila Urmila Valencia U., IFIC Solodkov Alexander Serpukhov, IHEP Soloshenko Alexei Dubna, JINR Solovyanov Oleg Serpukhov, IHEP Solovyev Victor St. Petersburg, INP Sommer Philip Freiburg U. Song Hong Ye Hefei, CUST Soni Nitesh Adelaide U., Sch. Chem. Phys. Sood Alexander LBL, Berkeley Sopczak Andre Prague, Tech. U. Sopko Bruno Prague, Tech. U. Sopko Vit Prague, Tech. U. Sorin Veronica Barcelona, IFAE Sosa David Heidelberg U. Sosebee Mark Texas U., Arlington Sotiropoulou Calliope Louisa INFN, Pisa Pisa U. Soualah Rachik INFN, Udine Udine U. Soukharev Andrey Novosibirsk, IYF Novosibirsk State U. South David DESY Sowden Benjamin Royal Holloway, U. of London Spagnolo Stefania INFN, Lecce Salento U. Spalla Margherita INFN, Pisa Pisa U. Spanò Francesco Royal Holloway, U. of London Spearman William Robert Harvard U., Phys. Dept. Sperlich Dennis Humboldt U., Berlin Spettel Fabian Munich, Max Planck Inst. Spighi Roberto INFN, Bologna Spigo Giancarlo CERN Spiller Laurence Anthony Melbourne U. Spousta Martin Charles U. Spreitzer Teresa Toronto U. St Denis Richard Dante Glasgow U. Staerz Steffen Dresden, Tech. U. Stahlman Jonathan Pennsylvania U. Stamen Rainer Kirchhoff Inst. Phys. Stamm Soren Humboldt U., Berlin Stanecka Ewa Cracow, INP Stanescu Cristian INFN, Rome Stanescu-Bellu Madalina DESY Stanitzki Marcel Michael DESY Stapnes Steinar Oslo U. Starchenko Evgeny Serpukhov, IHEP Stark Jan LPSC, Grenoble Staroba Pavel Prague, Inst. Phys. Starovoitov Pavel Kirchhoff Inst. Phys. Staszewski Rafal Cracow, INP Stavina Pavel Comenius U. Steinberg Peter Brookhaven Stelzer Bernd Simon Fraser U. Stelzer Harald Joerg CERN Stelzer-Chilton Oliver TRIUMF Stenzel Hasko Giessen U. Stewart Graeme Glasgow U. Stillings Jan Andre Bonn U. Stockton Mark McGill U. Stoebe Michael McGill U. Stoicea Gabriel Bucharest, IFIN-HH Stolte Philipp Gottingen U., II. Phys. Inst. Stonjek Stefan Munich, Max Planck Inst. 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Tavares Delgado Ademar LIP, Lisbon Lisbon U., CFNUL Tayalati Yahya Oujda U. Taylor Frank MIT Taylor Geoffrey Melbourne U. Taylor Wendy York U., Canada Teischinger Florian Alfred CERN Teixeira Dias Castanheira Matilde Queen Mary, U. of London Teixeira-Dias Pedro Royal Holloway, U. of London Temming Kim Katrin Freiburg U. Temple Darren Simon Fraser U. Ten Kate Herman CERN Teng Ping-Kun Taiwan, Inst. Phys. Teoh Jia Jian Osaka U. Tepel Fabian-Phillipp Wuppertal U. Terada Susumu KEK, Tsukuba Terashi Koji Tokyo U., ICEPP Terron Juan Madrid, Autonoma U. Terzo Stefano Munich, Max Planck Inst. Testa Marianna Frascati Teuscher Richard Toronto U. IPP, Canada Theveneaux-Pelzer Timothée Clermont-Ferrand U. Thomas Juergen Birmingham U. Thomas-Wilsker Joshuha Royal Holloway, U. of London Thompson Emily Nevis Labs, Columbia U. Thompson Paul Birmingham U. Thompson Ray Manchester U. Thompson Stan Glasgow U. Thomsen Lotte Ansgaard Yale U. Thomson Evelyn Pennsylvania U. Thomson Mark Cambridge U. 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Zhang Fangzhou Wisconsin U., Madison Zhang Huijun Nanjing U. Zhang Jinlong Argonne Zhang Lei Freiburg U. Zhang Ruiqi Hefei, CUST Zhang Xueyao Shandong U. Zhang Zhiqing Orsay, LAL Zhao Xiandong Southern Methodist U. Zhao Yongke Shandong U. Orsay, LAL Zhao Zhengguo Hefei, CUST Zhemchugov Alexey Dubna, JINR Zhong Jiahang Oxford U. Zhou Bing Michigan U. Zhou Chen Duke U. Zhou Lei Nevis Labs, Columbia U. Zhou Li Southern Methodist U. Zhou Ning Tsinghua U., Beijing Zhu Cheng Guang Shandong U. Zhu Hongbo Beijing, Inst. High Energy Phys. Zhu Junjie Michigan U. Zhu Yingchun Hefei, CUST Zhuang Xuai Beijing, Inst. High Energy Phys. Zhukov Konstantin Lebedev Inst. Zibell Andre Wurzburg U. Zieminska Daria Indiana U. Zimine Nikolai Dubna, JINR Zimmermann Christoph Mainz U. Zimmermann Stephanie Freiburg U. Zinonos Zinonas Gottingen U., II. Phys. Inst. Zinser Markus Mainz U. Ziolkowski Michael Siegen U. Živković Lidija Belgrade U. Zobernig Georg Wisconsin U., Madison Zoccoli Antonio INFN, Bologna Bologna U. zur Nedden Martin Humboldt U., Berlin Zurzolo Giovanni INFN, Naples Naples U. Zwalinski Lukasz CERN 2015 10 A summary is presented of ATLAS searches for gluinos and first- and second-generation squarks in final states containing jets and missing transverse momentum, with or without leptons or $b$-jets, in the $\sqrt{s}$ = 8 TeV data set collected at the Large Hadron Collider in 2012. This paper reports the results of new interpretations and statistical combinations of previously published analyses, as well as a new analysis.  Since no significant excess of events over the Standard Model expectation is observed, the data are used to set limits in a variety of models.   In all the considered simplified models that assume R-parity conservation, the limit on the gluino mass exceeds 1150 GeV at 95% confidence level, for an LSP mass smaller than 100 GeV. Furthermore, exclusion limits are set for left-handed squarks in a phenomenological MSSM model, a minimal Supergravity/Constrained MSSM model, R-parity-violation scenarios, a minimal gauge-mediated supersymmetry breaking model, a natural gauge mediation model, a non-universal Higgs mass model with gaugino mediation and a minimal model of universal extra dimensions. research-article

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JHEP JHEP Summary of the ATLAS experiment's sensitivity to supersymmetry after LHC Run 1 - interpreted in the phenomenological MSSM Aad Georges Marseille, CPPM Abbott Brad Oklahoma U. Abdallah Jalal Taiwan, Inst. Phys. Abdinov Ovsat Baku, Inst. Phys. Aben Rosemarie FOM, Amsterdam Abolins Maris Michigan State U. AbouZeid Ossama Toronto U. Abramowicz Halina Tel Aviv U. Abreu Henso Technion Abreu Ricardo Oregon U. Abulaiti Yiming Stockholm U. Stockholm U., OKC Acharya Bobby Samir INFN, Udine ICTP, Trieste King's Coll. London Adamczyk Leszek AGH-UST, Cracow Adams David Brookhaven Adelman Jahred Northern Illinois U. Adomeit Stefanie Munich U. Adye Tim Rutherford Affolder Tony Liverpool U. Agatonovic-Jovin Tatjana Belgrade U. Agricola Johannes Gottingen U., II. Phys. Inst. Aguilar-Saavedra Juan Antonio LIP, Lisbon CAFPE, Granada Ahlen Steven Boston U. Ahmadov Faig Dubna, JINR Baku, Inst. Phys. Aielli Giulio INFN, Rome Rome U., Tor Vergata Akerstedt Henrik Stockholm U. Stockholm U., OKC Åkesson Torsten Paul Ake Lund U. Akimov Andrei Lebedev Inst. Alberghi Gian Luigi INFN, Bologna Bologna U. Albert Justin Victoria U. Albrand Solveig LPSC, Grenoble Alconada Verzini Maria Josefina La Plata U. Aleksa Martin CERN Aleksandrov Igor Dubna, JINR Alexa Calin Bucharest, IFIN-HH Alexander Gideon Tel Aviv U. Alexopoulos Theodoros Natl. Tech. U., Athens Alhroob Muhammad Oklahoma U. Alimonti Gianluca INFN, Milan Alio Lion Marseille, CPPM Alison John Chicago U., EFI Alkire Steven Patrick Nevis Labs, Columbia U. Allbrooke Benedict Sussex U. Allport Phillip Birmingham U. Aloisio Alberto INFN, Naples Naples U. Alonso Alejandro Bohr Inst. Alonso Francisco La Plata U. Alpigiani Cristiano Washington U., Seattle Altheimer Andrew David Nevis Labs, Columbia U. Alvarez Gonzalez Barbara CERN Άlvarez Piqueras Damián Valencia U., IFIC Alviggi Mariagrazia INFN, Naples Naples U. 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Bianco Michele CERN Biebel Otmar Munich U. Biedermann Dustin Humboldt U., Berlin Bieniek Stephen Paul University Coll. London Biesuz Nicolo Vladi INFN, Pisa Pisa U. Biglietti Michela INFN, Rome Bilbao De Mendizabal Javier Geneva U. Bilokon Halina Frascati Bindi Marcello Gottingen U., II. Phys. Inst. Binet Sebastien Orsay, LAL Bingul Ahmet Gaziantep U. Bini Cesare INFN, Rome Rome U. Biondi Silvia INFN, Bologna Bologna U. Bjergaard David Martin Duke U. Black Curtis Sydney U. Black James SLAC Black Kevin Boston U. Blackburn Daniel Washington U., Seattle Blair Robert Argonne Blanchard Jean-Baptiste IRFU, Saclay Blanco Jacobo Ezequiel Royal Holloway, U. of London Blazek Tomas Comenius U. Bloch Ingo DESY Blocker Craig Brandeis U. Blum Walter Mainz U. Blumenschein Ulrike Gottingen U., II. Phys. Inst. Blunier Sylvain Chile U., Catolica Bobbink Gerjan FOM, Amsterdam Bobrovnikov Victor Novosibirsk, IYF Novosibirsk State U. Bocchetta Simona Serena Lund U. Bocci Andrea Duke U. 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Bruckman de Renstrom Pawel Cracow, INP Bruncko Dusan Kosice, IEF Bruneliere Renaud Freiburg U. Bruni Alessia INFN, Bologna Bruni Graziano INFN, Bologna Bruschi Marco INFN, Bologna Bruscino Nello Bonn U. Bryngemark Lene Lund U. Buanes Trygve Bergen U. Buat Quentin Simon Fraser U. Buchholz Peter Siegen U. Buckley Andrew Glasgow U. Buda Stelian Ioan Bucharest, IFIN-HH Budagov Ioulian Dubna, JINR Buehrer Felix Freiburg U. Bugge Lars Oslo U. Bugge Magnar Kopangen Oslo U. Bulekov Oleg Moscow Phys. Eng. Inst. Bullock Daniel Texas U., Arlington Burckhart Helfried CERN Burdin Sergey Liverpool U. Burgard Carsten Daniel Freiburg U. Burghgrave Blake Northern Illinois U. Burke Stephen Rutherford Burmeister Ingo Dortmund U. Busato Emmanuel Clermont-Ferrand U. Büscher Daniel Freiburg U. Büscher Volker Mainz U. Bussey Peter Glasgow U. Butler John Boston U. Butt Aatif Imtiaz Alberta U. Buttar Craig Glasgow U. Butterworth Jonathan University Coll. London Butti Pierfrancesco FOM, Amsterdam Buttinger William Brookhaven Buzatu Adrian Glasgow U. Buzykaev Aleksey Novosibirsk, IYF Novosibirsk State U. Cabrera Urbán Susana Valencia U., IFIC Caforio Davide Prague, Tech. U. Cairo Valentina INFN, Cosenza Calabria U. Cakir Orhan Ankara U. Calace Noemi Geneva U. Calafiura Paolo LBL, Berkeley Calandri Alessandro IRFU, Saclay Calderini Giovanni Paris U., VI-VII Calfayan Philippe Munich U. Caloba Luiz Rio de Janeiro Federal U. Calvet David Clermont-Ferrand U. Calvet Samuel Clermont-Ferrand U. Camacho Toro Reina Chicago U., EFI Camarda Stefano DESY Camarri Paolo INFN, Rome Rome U., Tor Vergata Cameron David Oslo U. Caminal Armadans Roger Illinois U., Urbana Campana Simone CERN Campanelli Mario University Coll. London Campoverde Angel SUNY, Stony Brook Canale Vincenzo INFN, Naples Naples U. Canepa Anadi TRIUMF Cano Bret Marc Shanghai Jiao Tong U. Cantero Josu Madrid, Autonoma U. Cantrill Robert LIP, Lisbon Cao Tingting Southern Methodist U. Capeans Garrido Maria Del Mar CERN Caprini Irinel Bucharest, IFIN-HH Caprini Mihai Bucharest, IFIN-HH Capua Marcella INFN, Cosenza Calabria U. Caputo Regina Mainz U. Carbone Ryne Michael Nevis Labs, Columbia U. Cardarelli Roberto INFN, Rome Cardillo Fabio Freiburg U. Carli Tancredi CERN Carlino Gianpaolo INFN, Naples Carminati Leonardo INFN, Milan Milan U. Caron Sascha NIKHEF, Amsterdam Carquin Edson Chile U., Catolica Carrillo-Montoya German D CERN Carter Janet Cambridge U. Carvalho João LIP, Lisbon Coimbra U. Casadei Diego University Coll. London Casado Maria Pilar Barcelona, IFAE Casolino Mirkoantonio Barcelona, IFAE Castaneda-Miranda Elizabeth Cape Town U. Castelli Angelantonio FOM, Amsterdam Castillo Gimenez Victoria Valencia U., IFIC Castro Nuno Filipe LIP, Lisbon Porto U. Catastini Pierluigi Harvard U., Phys. Dept. Catinaccio Andrea CERN Catmore James Oslo U. Cattai Ariella CERN Caudron Julien Mainz U. Cavaliere Viviana Illinois U., Urbana Cavalli Donatella INFN, Milan Cavalli-Sforza Matteo Barcelona, IFAE Cavasinni Vincenzo INFN, Pisa Pisa U. Ceradini Filippo INFN, Rome Rome III U. Cerio Benjamin Duke U. Cerny Karel Charles U. Santiago Cerqueira Augusto Juiz de Fora U. Cerri Alessandro Sussex U. Cerrito Lucio Queen Mary, U. of London Cerutti Fabio LBL, Berkeley Cerv Matevz CERN Cervelli Alberto Bern U., LHEP Cetin Serkant Ali Dogus U., Kadikoy Chafaq Aziz Casablanca U. Chakraborty Dhiman Northern Illinois U. Chalupkova Ina Charles U. Chang Philip Illinois U., Urbana Chapman John Derek Cambridge U. Charlton Dave Birmingham U. Chau Chav Chhiv Toronto U. Chavez Barajas Carlos Alberto Sussex U. Cheatham Susan Technion Chegwidden Andrew Michigan State U. Chekanov Sergei Argonne Chekulaev Sergey TRIUMF Chelkov Gueorgui Dubna, JINR Tomsk State U. Chelstowska Magda Anna Michigan U. Chen Chunhui Iowa State U. Chen Hucheng Brookhaven Chen Karen SUNY, Stony Brook Chen Liming Shandong U. Marseille, CPPM Chen Shenjian Nanjing U. Chen Shion Tokyo U., ICEPP Chen Xin Tsinghua U., Beijing Chen Ye Kobe U. Cheng Hok Chuen Michigan U. Cheng Yangyang Chicago U., EFI Cheplakov Alexander Dubna, JINR Cheremushkina Evgenia Serpukhov, IHEP Cherkaoui El Moursli Rajaa Rabat U. Chernyatin Valeriy Brookhaven Cheu Elliott Arizona U. Chevalier Laurent IRFU, Saclay Chiarella Vitaliano Frascati Chiarelli Giorgio INFN, Pisa Pisa U. Chiodini Gabriele INFN, Lecce Chisholm Andrew Birmingham U. Chislett Rebecca Thalatta University Coll. London Chitan Adrian Bucharest, IFIN-HH Chizhov Mihail Dubna, JINR Choi Kyungeon Indiana U. Chouridou Sofia Athens U. Chow Bonnie Kar Bo Munich U. Christodoulou Valentinos University Coll. London Chromek-Burckhart Doris CERN Chudoba Jiri Prague, Inst. Phys. Chuinard Annabelle Julia McGill U. Chwastowski Janusz Cracow, INP Chytka Ladislav Palacky U. Ciapetti Guido INFN, Rome Rome U. Ciftci Abbas Kenan Ankara U. Cinca Diane Glasgow U. Cindro Vladimir Stefan Inst., Ljubljana Cioara Irina Antonela Bonn U. Ciocio Alessandra LBL, Berkeley Cirotto Francesco INFN, Naples Naples U. Citron Zvi Hirsh Weizmann Inst. Ciubancan Mihai Bucharest, IFIN-HH Clark Allan G Geneva U. Clark Brian Lee Harvard U., Phys. Dept. Clark Philip James Edinburgh U. Clarke Robert LBL, Berkeley Clement Christophe Stockholm U. Stockholm U., OKC Coadou Yann Marseille, CPPM Cobal Marina INFN, Udine Udine U. Coccaro Andrea Geneva U. Cochran James H Iowa State U. Coffey Laurel Brandeis U. Cogan Joshua Godfrey SLAC Colasurdo Luca NIKHEF, Amsterdam Cole Brian Nevis Labs, Columbia U. Cole Stephen Northern Illinois U. Colijn Auke-Pieter FOM, Amsterdam Collot Johann LPSC, Grenoble Colombo Tommaso Heidelberg U. Compostella Gabriele Munich, Max Planck Inst. Conde Muiño Patricia LIP, Lisbon Lisbon U., CFNUL Coniavitis Elias Freiburg U. Connell Simon Henry Johannesburg U. Connelly Ian Royal Holloway, U. of London Consorti Valerio Freiburg U. Constantinescu Serban Bucharest, IFIN-HH Conta Claudio INFN, Pavia Pavia U. Conti Geraldine CERN Conventi Francesco INFN, Naples Naples, Inst. U. Navale Cooke Mark LBL, Berkeley Cooper Ben University Coll. London Cooper-Sarkar Amanda Oxford U. Cornelissen Thijs Wuppertal U. Corradi Massimo INFN, Bologna Corriveau Francois McGill U. IPP, Canada Corso-Radu Alina UC, Irvine Cortes-Gonzalez Arely Barcelona, IFAE Cortiana Giorgio Munich, Max Planck Inst. Costa Giuseppe INFN, Milan Costa María José Valencia U., IFIC Costanzo Davide Sheffield U. Côté David Texas U., Arlington Cottin Giovanna Cambridge U. Cowan Glen Royal Holloway, U. of London Cox Brian Manchester U. Cranmer Kyle New York U. Cree Graham Carleton U. Crépé-Renaudin Sabine LPSC, Grenoble Crescioli Francesco Paris U., VI-VII Cribbs Wayne Allen Stockholm U. Stockholm U., OKC Crispin Ortuzar Mireia Oxford U. Cristinziani Markus Bonn U. Croft Vince NIKHEF, Amsterdam Crosetti Giovanni INFN, Cosenza Calabria U. 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Rutherford Davies Merlin Tel Aviv U. Davison Peter University Coll. London Davygora Yuriy Kirchhoff Inst. Phys. Dawe Edmund Melbourne U. Dawson Ian Sheffield U. Daya-Ishmukhametova Rozmin Massachusetts U., Amherst De Kaushik Texas U., Arlington de Asmundis Riccardo INFN, Naples De Benedetti Abraham Oklahoma U. De Castro Stefano INFN, Bologna Bologna U. De Cecco Sandro Paris U., VI-VII De Groot Nicolo NIKHEF, Amsterdam de Jong Paul FOM, Amsterdam De la Torre Hector Madrid, Autonoma U. De Lorenzi Francesco Iowa State U. De Pedis Daniele INFN, Rome De Salvo Alessandro INFN, Rome De Sanctis Umberto Sussex U. De Santo Antonella Sussex U. De Vivie De Regie Jean-Baptiste Orsay, LAL Dearnaley William James Lancaster U. Debbe Ramiro Brookhaven Debenedetti Chiara UC, Santa Cruz Dedovich Dmitri Dubna, JINR Deigaard Ingrid FOM, Amsterdam Del Peso Jose Madrid, Autonoma U. Del Prete Tarcisio INFN, Pisa Pisa U. Delgove David Orsay, LAL Deliot Frederic IRFU, Saclay Delitzsch Chris Malena Geneva U. Deliyergiyev Maksym Stefan Inst., Ljubljana Dell'Acqua Andrea CERN Dell'Asta Lidia Boston U. Dell'Orso Mauro INFN, Pisa Pisa U. Della Pietra Massimo INFN, Naples Naples, Inst. U. Navale della Volpe Domenico Geneva U. Delmastro Marco Annecy, LAPP Delsart Pierre-Antoine LPSC, Grenoble Deluca Carolina FOM, Amsterdam DeMarco David Toronto U. Demers Sarah Yale U. Demichev Mikhail Dubna, JINR Demilly Aurelien Paris U., VI-VII Denisov Sergey Serpukhov, IHEP Derendarz Dominik Cracow, INP Derkaoui Jamal Eddine Oujda U. Derue Frederic Paris U., VI-VII Dervan Paul Liverpool U. Desch Klaus Kurt Bonn U. Deterre Cecile DESY Deviveiros Pier-Olivier CERN Dewhurst Alastair Rutherford Dhaliwal Saminder Brandeis U. Di Ciaccio Anna INFN, Rome Rome U., Tor Vergata Di Ciaccio Lucia Annecy, LAPP Di Domenico Antonio INFN, Rome Rome U. Di Donato Camilla INFN, Naples Naples U. Di Girolamo Alessandro CERN Di Girolamo Beniamino CERN Di Mattia Alessandro Technion Di Micco Biagio INFN, Rome Rome III U. Di Nardo Roberto Frascati Di Simone Andrea Freiburg U. Di Sipio Riccardo Toronto U. Di Valentino David Carleton U. Diaconu Cristinel Marseille, CPPM Diamond Miriam Toronto U. Dias Flavia Edinburgh U. Diaz Marco Aurelio Chile U., Catolica Diehl Edward Michigan U. Dietrich Janet Humboldt U., Berlin Diglio Sara Marseille, CPPM Dimitrievska Aleksandra Belgrade U. Dingfelder Jochen Bonn U. Dita Petre Bucharest, IFIN-HH Dita Sanda Bucharest, IFIN-HH Dittus Fridolin CERN Djama Fares Marseille, CPPM Djobava Tamar Tbilisi State U. Djuvsland Julia Isabell Kirchhoff Inst. Phys. Barros do Vale Maria Aline Sao Joao del-Rei Fed. U. Dobos Daniel CERN Dobre Monica Bucharest, IFIN-HH Doglioni Caterina Lund U. Dohmae Takeshi Tokyo U., ICEPP Dolejsi Jiri Charles U. Dolezal Zdenek Charles U. Dolgoshein Boris Moscow Phys. Eng. Inst. Donadelli Marisilvia Sao Paulo U. Donati Simone INFN, Pisa Pisa U. Dondero Paolo INFN, Pavia Pavia U. Donini Julien Clermont-Ferrand U. Dopke Jens Rutherford Doria Alessandra INFN, Naples Dova Maria-Teresa La Plata U. Doyle Tony Glasgow U. Drechsler Eric Gottingen U., II. Phys. Inst. Dris Manolis Natl. Tech. U., Athens Dubreuil Emmanuelle Clermont-Ferrand U. Duchovni Ehud Weizmann Inst. Duckeck Guenter Munich U. Ducu Otilia Anamaria Bucharest, IFIN-HH Marseille, CPPM Duda Dominik FOM, Amsterdam Dudarev Alexey CERN Duflot Laurent Orsay, LAL Duguid Liam Royal Holloway, U. of London Dührssen Michael CERN Dunford Monica Kirchhoff Inst. Phys. Duran Yildiz Hatice Ankara U. Düren Michael Giessen U. Durglishvili Archil Tbilisi State U. Duschinger Dirk Dresden, Tech. U. Dutta Baishali DESY Dyndal Mateusz AGH-UST, Cracow Eckardt Christoph DESY Ecker Katharina Maria Munich, Max Planck Inst. Edgar Ryan Christopher Michigan U. Edson William SUNY, Albany Edwards Nicholas Charles Edinburgh U. Ehrenfeld Wolfgang Bonn U. Eifert Till CERN Eigen Gerald Bergen U. Einsweiler Kevin LBL, Berkeley Ekelof Tord Uppsala U., Inst. Theor. Phys. El Kacimi Mohamed Cadi Ayyad U., Marrakech Ellert Mattias Uppsala U., Inst. Theor. Phys. Elles Sabine Annecy, LAPP Ellinghaus Frank Wuppertal U. Elliot Alison Victoria U. Ellis Nicolas CERN Elmsheuser Johannes Munich U. Elsing Markus CERN Emeliyanov Dmitry Rutherford Enari Yuji Tokyo U., ICEPP Endner Oliver Chris Mainz U. Endo Masaki Osaka U. Erdmann Johannes Dortmund U. Ereditato Antonio Bern U., LHEP Ernis Gunar Wuppertal U. Ernst Jesse SUNY, Albany Ernst Michael Brookhaven Errede Steven Illinois U., Urbana Ertel Eugen Mainz U. Escalier Marc Orsay, LAL Esch Hendrik Dortmund U. Escobar Carlos Pittsburgh U. Esposito Bellisario Frascati Etienvre Anne-Isabelle IRFU, Saclay Etzion Erez Tel Aviv U. Evans Hal Indiana U. Ezhilov Alexey St. Petersburg, INP Fabbri Laura INFN, Bologna Bologna U. Facini Gabriel Chicago U., EFI Fakhrutdinov Rinat Serpukhov, IHEP Falciano Speranza INFN, Rome Falla Rebecca Jane University Coll. London Faltova Jana Charles U. Fang Yaquan Beijing, Inst. High Energy Phys. Fanti Marcello INFN, Milan Milan U. Farbin Amir Texas U., Arlington Farilla Addolorata INFN, Rome Farooque Trisha Barcelona, IFAE Farrell Steven LBL, Berkeley Farrington Sinead Warwick U. Farthouat Philippe CERN Fassi Farida Rabat U. Fassnacht Patrick CERN Fassouliotis Dimitrios Athens U. Faucci Giannelli Michele Royal Holloway, U. of London Favareto Andrea INFN, Genoa Genoa U. Fawcett William James Oxford U. Fayard Louis Orsay, LAL Fedin Oleg St. Petersburg, INP St. Petersburg Polytechnic Inst. Fedorko Wojciech British Columbia U. Feigl Simon CERN Feligioni Lorenzo Marseille, CPPM Feng Cunfeng Shandong U. Feng Eric CERN Feng Haolu Michigan U. Fenyuk Alexander Serpukhov, IHEP Feremenga Last Texas U., Arlington Fernandez Martinez Patricia Valencia U., IFIC Fernandez Perez Sonia CERN Ferrando James Glasgow U. Ferrari Arnaud Uppsala U., Inst. Theor. Phys. Ferrari Pamela FOM, Amsterdam Ferrari Roberto INFN, Pavia Ferreira de Lima Danilo Enoque Glasgow U. Ferrer Antonio Valencia U., IFIC Ferrere Didier Geneva U. Ferretti Claudio Michigan U. Ferretto Parodi Andrea INFN, Genoa Genoa U. Fiascaris Maria Chicago U., EFI Fiedler Frank Mainz U. Filipčič Andrej Stefan Inst., Ljubljana Filipuzzi Marco DESY Filthaut Frank NIKHEF, Amsterdam Fincke-Keeler Margret Victoria U. Finelli Kevin Daniel Sydney U. Fiolhais Miguel LIP, Lisbon Coimbra U. Fiorini Luca Valencia U., IFIC Firan Ana Southern Methodist U. Fischer Adam SUNY, Albany Fischer Cora Barcelona, IFAE Fischer Julia Wuppertal U. Fisher Wade Cameron Michigan State U. Flaschel Nils DESY Fleck Ivor Siegen U. Fleischmann Philipp Michigan U. Fletcher Gareth Thomas Sheffield U. Fletcher Gregory Queen Mary, U. of London Fletcher Rob Roy MacGregor Pennsylvania U. Flick Tobias Wuppertal U. Floderus Anders Lund U. Flores Castillo Luis Hong Kong, Chinese U. Flowerdew Michael Munich, Max Planck Inst. Formica Andrea IRFU, Saclay Forti Alessandra Manchester U. Fournier Daniel Orsay, LAL Fox Harald Lancaster U. Fracchia Silvia Barcelona, IFAE Francavilla Paolo Paris U., VI-VII Franchini Matteo INFN, Bologna Bologna U. Francis David CERN Franconi Laura Oslo U. Franklin Melissa Harvard U., Phys. Dept. Frate Meghan UC, Irvine Fraternali Marco INFN, Pavia Pavia U. Freeborn David University Coll. London French Sky Cambridge U. Friedrich Felix Dresden, Tech. U. Froidevaux Daniel CERN Frost James Oxford U. Fukunaga Chikara Tokyo Metropolitan U. Fullana Torregrosa Esteban Mainz U. Fulsom Bryan Gregory SLAC Fusayasu Takahiro Nagasaki Inst. Appl. Sci. Fuster Juan Valencia U., IFIC Gabaldon Carolina LPSC, Grenoble Gabizon Ofir Wuppertal U. Gabrielli Alessandro INFN, Bologna Bologna U. Gabrielli Andrea LBL, Berkeley Gach Grzegorz Birmingham U. Gadatsch Stefan CERN Gadomski Szymon Geneva U. Gagliardi Guido INFN, Genoa Genoa U. Gagnon Pauline Indiana U. Galea Cristina NIKHEF, Amsterdam Galhardo Bruno LIP, Lisbon Coimbra U. Gallas Elizabeth Oxford U. Gallop Bruce Rutherford Gallus Petr Prague, Tech. U. Galster Gorm Aske Gram Krohn Bohr Inst. Gan KK Ohio State U. Gao Jun Hefei, CUST Marseille, CPPM Gao Yanyan Edinburgh U. Gao Yongsheng SLAC Fresno State Garay Walls Francisca Edinburgh U. Garberson Ford Yale U. García Carmen Valencia U., IFIC García Navarro José Enrique Valencia U., IFIC Garcia-Sciveres Maurice LBL, Berkeley Gardner Robert Chicago U., EFI Garelli Nicoletta SLAC Garonne Vincent Oslo U. Gatti Claudio Frascati Gaudiello Andrea INFN, Genoa Genoa U. Gaudio Gabriella INFN, Pavia Gaur Bakul Siegen U. Gauthier Lea Montreal U. Gauzzi Paolo INFN, Rome Rome U. Gavrilenko Igor Lebedev Inst. Gay Colin British Columbia U. Gaycken Goetz Bonn U. Gazis Evangelos Natl. Tech. U., Athens Ge Peng Shandong U. Gecse Zoltan British Columbia U. Gee Norman Rutherford Geich-Gimbel Christoph Bonn U. Geisler Manuel Patrice Kirchhoff Inst. Phys. Gemme Claudia INFN, Genoa Genest Marie-Hélène LPSC, Grenoble Gentile Simonetta INFN, Rome Rome U. George Matthias Gottingen U., II. Phys. Inst. George Simon Royal Holloway, U. of London Gerbaudo Davide UC, Irvine Gershon Avi Tel Aviv U. Ghasemi Sara Siegen U. Ghazlane Hamid CNESTEN, Rabat Giacobbe Benedetto INFN, Bologna Giagu Stefano INFN, Rome Rome U. Giangiobbe Vincent Barcelona, IFAE Giannetti Paola INFN, Pisa Pisa U. Gibbard Bruce Brookhaven Gibson Stephen Royal Holloway, U. of London Gignac Matthew British Columbia U. Gilchriese Murdock LBL, Berkeley Gillam Thomas Cambridge U. Gillberg Dag CERN Gilles Geoffrey Clermont-Ferrand U. Gingrich Douglas Alberta U. TRIUMF Giokaris Nikos Athens U. Giordani MarioPaolo INFN, Udine Udine U. Giorgi Filippo Maria INFN, Bologna Giorgi Francesco Michelangelo Humboldt U., Berlin Giraud Pierre-Francois IRFU, Saclay Giromini Paolo Frascati Giugni Danilo INFN, Milan Giuliani Claudia Freiburg U. Giulini Maddalena Heidelberg U. Gjelsten Børge Kile Oslo U. Gkaitatzis Stamatios Aristotle U., Thessaloniki Gkialas Ioannis Aristotle U., Thessaloniki Gkougkousis Evangelos Leonidas Orsay, LAL Gladilin Leonid Moscow State U. Glasman Claudia Madrid, Autonoma U. Glatzer Julian CERN Glaysher Paul Edinburgh U. Glazov Alexandre DESY Goblirsch-Kolb Maximilian Munich, Max Planck Inst. Goddard Jack Robert Queen Mary, U. of London Godlewski Jan Cracow, INP Goldfarb Steven Michigan U. Golling Tobias Geneva U. Golubkov Dmitry Serpukhov, IHEP Gomes Agostinho LIP, Lisbon Lisbon U., CFNUL Gonçalo Ricardo LIP, Lisbon Goncalves Pinto Firmino Da Costa Joao IRFU, Saclay Gonella Laura Bonn U. González de la Hoz Santiago Valencia U., IFIC Gonzalez Parra Garoe Barcelona, IFAE Gonzalez-Sevilla Sergio Geneva U. Goossens Luc CERN Gorbounov Petr Andreevich Moscow, ITEP Gordon Howard Brookhaven Gorelov Igor New Mexico U. Gorini Benedetto CERN Gorini Edoardo INFN, Lecce Salento U. Gorišek Andrej Stefan Inst., Ljubljana Gornicki Edward Cracow, INP Goshaw Alfred Duke U. Gössling Claus Dortmund U. Gostkin Mikhail Ivanovitch Dubna, JINR Goujdami Driss Cadi Ayyad U., Marrakech Goussiou Anna Washington U., Seattle Govender Nicolin Johannesburg U. Gozani Eitan Technion Grabas Herve Marie Xavier UC, Santa Cruz Graber Lars Gottingen U., II. Phys. Inst. Grabowska-Bold Iwona AGH-UST, Cracow Gradin Per Olov Joakim Uppsala U., Inst. Theor. Phys. Grafström Per INFN, Bologna Bologna U. Grahn Karl-Johan DESY Gramling Johanna Geneva U. Gramstad Eirik Oslo U. Grancagnolo Sergio Humboldt U., Berlin Gratchev Vadim St. Petersburg, INP Gray Heather CERN Graziani Enrico INFN, Rome Greenwood Zeno Dixon Louisiana Tech. U. Grefe Christian Bonn U. Gregersen Kristian University Coll. London Gregor Ingrid-Maria DESY Grenier Philippe SLAC Griffiths Justin Texas U., Arlington Grillo Alexander UC, Santa Cruz Grimm Kathryn Lancaster U. Grinstein Sebastian Barcelona, IFAE ICREA, Barcelona Gris Philippe Luc Yves Clermont-Ferrand U. Grivaz Jean-Francois Orsay, LAL Grohs Johannes Philipp Dresden, Tech. U. Grohsjean Alexander DESY Gross Eilam Weizmann Inst. Grosse-Knetter Joern Gottingen U., II. Phys. Inst. Grossi Giulio Cornelio Louisiana Tech. U. Grout Zara Jane Sussex U. Guan Liang Michigan U. Guenther Jaroslav Prague, Tech. U. Guescini Francesco Geneva U. Guest Daniel Yale U. Gueta Orel Tel Aviv U. Guido Elisa INFN, Genoa Genoa U. Guillemin Thibault Orsay, LAL Guindon Stefan SUNY, Albany Gul Umar Glasgow U. Gumpert Christian Dresden, Tech. U. Guo Jun Shanghai Jiao Tong U. Guo Yicheng Hefei, CUST Michigan U. Gupta Shaun Oxford U. Gustavino Giuliano INFN, Rome Rome U. Gutierrez Phillip Oklahoma U. Gutierrez Ortiz Nicolas Gilberto University Coll. London Gutschow Christian Dresden, Tech. U. Guyot Claude IRFU, Saclay Gwenlan Claire Oxford U. Gwilliam Carl Liverpool U. Haas Andy New York U. Haber Carl LBL, Berkeley Hadavand Haleh Khani Texas U., Arlington Haddad Nacim Rabat U. Haefner Petra Bonn U. Hageböck Stephan Bonn U. Hajduk Zbigniew Cracow, INP Hakobyan Hrachya Yerevan Phys. Inst. Haleem Mahsana DESY Haley Joseph Oklahoma State U. Hall David Oxford U. Halladjian Garabed Michigan State U. Hallewell Gregory David Marseille, CPPM Hamacher Klaus Wuppertal U. Hamal Petr Palacky U. Hamano Kenji Victoria U. Hamilton Andrew Cape Town U. Hamity Guillermo Nicolas Sheffield U. Hamnett Phillip George DESY Han Liang Hefei, CUST Hanagaki Kazunori KEK, Tsukuba Osaka U. Hanawa Keita Tokyo U., ICEPP Hance Michael UC, Santa Cruz Haney Bijan Pennsylvania U. Hanke Paul Kirchhoff Inst. Phys. Hanna Remie IRFU, Saclay Hansen Jørgen Beck Bohr Inst. Hansen Jorn Dines Bohr Inst. Hansen Maike Christina Bonn U. Hansen Peter Henrik Bohr Inst. Hara Kazuhiko Tsukuba U. Hard Andrew Wisconsin U., Madison Harenberg Torsten Wuppertal U. Hariri Faten Orsay, LAL Harkusha Siarhei Minsk, Inst. Phys. Harrington Robert Edinburgh U. Harrison Paul Fraser Warwick U. Hartjes Fred FOM, Amsterdam Hasegawa Makoto Kobe U. Hasegawa Yoji Shinshu U. Hasib A Oklahoma U. Hassani Samira IRFU, Saclay Haug Sigve Bern U., LHEP Hauser Reiner Michigan State U. Hauswald Lorenz Dresden, Tech. U. Havranek Miroslav Prague, Inst. Phys. Hawkes Christopher Birmingham U. Hawkings Richard John CERN Hawkins Anthony David Lund U. Hayashi Takayasu Tsukuba U. Hayden Daniel Michigan State U. Hays Chris Oxford U. Hays Jonathan Michael Queen Mary, U. of London Hayward Helen Liverpool U. Haywood Stephen Rutherford Head Simon Birmingham U. Heck Tobias Mainz U. Hedberg Vincent Lund U. Heelan Louise Texas U., Arlington Heim Sarah Pennsylvania U. Heim Timon Wuppertal U. Heinemann Beate LBL, Berkeley Heinrich Lukas New York U. Hejbal Jiri Prague, Inst. Phys. Helary Louis Boston U. Hellman Sten Stockholm U. Stockholm U., OKC Hellmich Dennis Bonn U. Helsens Clement Barcelona, IFAE Henderson James Oxford U. Henderson Robert Lancaster U. Heng Yang Wisconsin U., Madison Hengler Christopher DESY Henkelmann Steffen British Columbia U. Henrichs Anna Yale U. Henriques Correia Ana Maria CERN Henrot-Versille Sophie Orsay, LAL Herbert Geoffrey Henry Humboldt U., Berlin Hernández Jiménez Yesenia Valencia U., IFIC Herten Gregor Freiburg U. Hertenberger Ralf Munich U. Hervas Luis CERN Hesketh Gavin Grant University Coll. London Hessey Nigel FOM, Amsterdam Hetherly Jeffrey Wayne Southern Methodist U. Hickling Robert Queen Mary, U. of London Higón-Rodriguez Emilio Valencia U., IFIC Hill Ewan Victoria U. Hill John Cambridge U. Hiller Karl Heinz DESY Hillier Stephen Birmingham U. Hinchliffe Ian LBL, Berkeley Hines Elizabeth Pennsylvania U. Hinman Rachel Reisner LBL, Berkeley Hirose Minoru Tokyo Inst. Tech. Hirschbuehl Dominic Wuppertal U. Hobbs John SUNY, Stony Brook Hod Noam FOM, Amsterdam Hodgkinson Mark Sheffield U. Hodgson Paul Sheffield U. Hoecker Andreas CERN Hoeferkamp Martin New Mexico U. Hoenig Friedrich Munich U. Hohlfeld Marc Mainz U. Hohn David Bonn U. Holmes Tova Ray LBL, Berkeley Homann Michael Dortmund U. Hong Tae Min Pittsburgh U. Hopkins Walter Oregon U. Horii Yasuyuki Nagoya U. Horton Arthur James Simon Fraser U. Hostachy Jean-Yves LPSC, Grenoble Hou Suen Taiwan, Inst. Phys. Hoummada Abdeslam Casablanca U. Howard Jacob Oxford U. Howarth James DESY Hrabovsky Miroslav Palacky U. Hristova Ivana Humboldt U., Berlin Hrivnac Julius Orsay, LAL Hryn'ova Tetiana Annecy, LAPP Hrynevich Aliaksei Minsk, High Energy Phys. Ctr. Hsu Catherine Witwatersrand U. Hsu Pai-hsien Jennifer Taiwan, Inst. Phys. Taiwan, Natl. Tsing Hua U. Hsu Shih-Chieh Washington U., Seattle Hu Diedi Nevis Labs, Columbia U. Hu Qipeng Hefei, CUST Hu Xueye Michigan U. Huang Yanping DESY Hubacek Zdenek Prague, Tech. U. Hubaut Fabrice Marseille, CPPM Huegging Fabian Bonn U. Huffman Todd Brian Oxford U. Hughes Emlyn Nevis Labs, Columbia U. Hughes Gareth Lancaster U. Huhtinen Mika CERN Hülsing Tobias Alexander Mainz U. Huseynov Nazim Dubna, JINR Baku, Inst. Phys. Huston Joey Michigan State U. Huth John Harvard U., Phys. Dept. Iacobucci Giuseppe Geneva U. Iakovidis Georgios Brookhaven Ibragimov Iskander Siegen U. Iconomidou-Fayard Lydia Orsay, LAL Ideal Emma Yale U. Idrissi Zineb Rabat U. Iengo Paolo CERN Igonkina Olga FOM, Amsterdam Iizawa Tomoya Waseda U. Ikegami Yoichi KEK, Tsukuba Ikematsu Katsumasa Siegen U. Ikeno Masahiro KEK, Tsukuba Ilchenko Iurii Chicago U., EFI Texas U. Iliadis Dimitrios Aristotle U., Thessaloniki Ilic Nikolina SLAC Ince Tayfun Munich, Max Planck Inst. Introzzi Gianluca INFN, Pavia Pavia U. Ioannou Pavlos Athens U. Iodice Mauro INFN, Rome Iordanidou Kalliopi Nevis Labs, Columbia U. Ippolito Valerio Harvard U., Phys. Dept. Irles Quiles Adrian Valencia U., IFIC Isaksson Charlie Uppsala U., Inst. Theor. Phys. Ishino Masaya Kyoto U. Ishitsuka Masaki Tokyo Inst. Tech. Ishmukhametov Renat Ohio State U. Issever Cigdem Oxford U. Istin Serhat Bogazici U. Iturbe Ponce Julia Mariana Manchester U. Iuppa Roberto INFN, Rome Rome U., Tor Vergata Ivarsson Jenny Lund U. Iwanski Wieslaw Cracow, INP Iwasaki Hiroyuki KEK, Tsukuba Izen Joseph Texas U., Dallas Izzo Vincenzo INFN, Naples Jabbar Samina Alberta U. Jackson Brett Pennsylvania U. Jackson Matthew Liverpool U. Jackson Paul Adelaide U., Sch. Chem. Phys. Jaekel Martin CERN Jain Vivek SUNY, Albany Jakobs Karl Freiburg U. Jakobsen Sune CERN Jakoubek Tomas Prague, Inst. Phys. Jakubek Jan Prague, Tech. U. Jamin David Olivier Oklahoma State U. Jana Dilip Louisiana Tech. U. Jansen Eric University Coll. London Jansky Roland Innsbruck U. Janssen Jens Bonn U. Janus Michel Gottingen U., II. Phys. Inst. Jarlskog Göran Lund U. Javadov Namig Dubna, JINR Baku, Inst. Phys. Javůrek Tomáš Freiburg U. Jeanty Laura LBL, Berkeley Jejelava Juansher Tbilisi, Inst. Phys. Ilia State U. Jeng Geng-yuan Sydney U. Jennens David Melbourne U. Jenni Peter Freiburg U. CERN Jentzsch Jennifer Dortmund U. Jeske Carl Warwick U. Jézéquel Stéphane Annecy, LAPP Ji Haoshuang Wisconsin U., Madison Jia Jiangyong SUNY, Stony Brook Jiang Yi Hefei, CUST Jiggins Stephen University Coll. London Jimenez Pena Javier Valencia U., IFIC Jin Shan Beijing, Inst. High Energy Phys. Jinaru Adam Bucharest, IFIN-HH Jinnouchi Osamu Tokyo Inst. Tech. Joergensen Morten Dam Bohr Inst. Johansson Per Sheffield U. Johns Kenneth Arizona U. Johnson William Joseph Washington U., Seattle Jon-And Kerstin Stockholm U. Stockholm U., OKC Jones Graham Warwick U. Jones Roger Lancaster U. Jones Tim Liverpool U. Jongmanns Jan Kirchhoff Inst. Phys. Jorge Pedro LIP, Lisbon Lisbon U., CFNUL Joshi Kiran Daniel Manchester U. Jovicevic Jelena TRIUMF Ju Xiangyang Wisconsin U., Madison Jussel Patrick Innsbruck U. Juste Rozas Aurelio Barcelona, IFAE ICREA, Barcelona Kaci Mohammed Valencia U., IFIC Kaczmarska Anna Cracow, INP Kado Marumi Orsay, LAL Kagan Harris Ohio State U. Kagan Michael SLAC Kahn Sebastien Jonathan Marseille, CPPM Kajomovitz Enrique Duke U. Kalderon Charles William Oxford U. Kama Sami Southern Methodist U. Kamenshchikov Andrey Serpukhov, IHEP Kanaya Naoko Tokyo U., ICEPP Kaneti Steven Cambridge U. Kantserov Vadim Moscow Phys. Eng. Inst. Kanzaki Junichi KEK, Tsukuba Kaplan Benjamin New York U. Kaplan Laser Seymour Wisconsin U., Madison Kapliy Anton Chicago U., EFI Kar Deepak Witwatersrand U. Karakostas Konstantinos Natl. Tech. U., Athens Karamaoun Andrew Alberta U. Karastathis Nikolaos Natl. Tech. U., Athens FOM, Amsterdam Kareem Mohammad Jawad Gottingen U., II. Phys. Inst. Karentzos Efstathios Natl. Tech. U., Athens Karnevskiy Mikhail Mainz U. Karpov Sergey Dubna, JINR Karpova Zoya Dubna, JINR Karthik Krishnaiyengar New York U. Kartvelishvili Vakhtang Lancaster U. Karyukhin Andrey Serpukhov, IHEP Kasahara Kota Tsukuba U. Kashif Lashkar Wisconsin U., Madison Kass Richard Ohio State U. Kastanas Alex Bergen U. Kataoka Yousuke Tokyo U., ICEPP Kato Chikuma Tokyo U., ICEPP Katre Akshay Geneva U. Katzy Judith DESY Kawade Kentaro Nagoya U. Kawagoe Kiyotomo Kyushu U. Kawamoto Tatsuo Tokyo U., ICEPP Kawamura Gen Gottingen U., II. Phys. Inst. Kazama Shingo Tokyo U., ICEPP Kazanin Vassili Novosibirsk, IYF Novosibirsk State U. Keeler Richard Victoria U. Kehoe Robert Southern Methodist U. Keller John DESY Kempster Jacob Julian Royal Holloway, U. of London Keoshkerian Houry Manchester U. Kepka Oldrich Prague, Inst. Phys. Kerševan Borut Paul Stefan Inst., Ljubljana Kersten Susanne Wuppertal U. Keyes Robert McGill U. Khalil-zada Farkhad Baku, Inst. Phys. Khandanyan Hovhannes Stockholm U. Stockholm U., OKC Khanov Alexander Oklahoma State U. Kharlamov Alexey Novosibirsk, IYF Novosibirsk State U. Khoo Teng Jian Cambridge U. Khovanskiy Valery Moscow, ITEP Khramov Evgeniy Dubna, JINR Khubua Jemal Tbilisi State U. GTU, Tbilisi Kido Shogo Kobe U. Kim Hee Yeun Texas U., Arlington Kim Shinhong Tsukuba U. Kim Young-Kee Chicago U., EFI Kimura Naoki Aristotle U., Thessaloniki Kind Oliver Maria Humboldt U., Berlin King Barry Liverpool U. King Matthew Valencia U., IFIC King Samuel Burton British Columbia U. Kirk Julie Rutherford Kiryunin Andrey Munich, Max Planck Inst. Kishimoto Tomoe Kobe U. Kisielewska Danuta AGH-UST, Cracow Kiss Florian Freiburg U. Kiuchi Kenji Tsukuba U. Kivernyk Oleh IRFU, Saclay Kladiva Eduard Kosice, IEF Klein Matthew Henry Nevis Labs, Columbia U. Klein Max Liverpool U. Klein Uta Liverpool U. Kleinknecht Konrad Mainz U. Klimek Pawel Stockholm U. Stockholm U., OKC Klimentov Alexei Brookhaven Klingenberg Reiner Dortmund U. Klinger Joel Alexander Sheffield U. Klioutchnikova Tatiana CERN Kluge Eike-Erik Kirchhoff Inst. Phys. Kluit Peter FOM, Amsterdam Kluth Stefan Munich, Max Planck Inst. Knapik Joanna Cracow, INP Kneringer Emmerich Innsbruck U. Knoops Edith Marseille, CPPM Knue Andrea Glasgow U. Kobayashi Aine Tokyo U., ICEPP Kobayashi Dai Tokyo Inst. Tech. Kobayashi Tomio Tokyo U., ICEPP Kobel Michael Dresden, Tech. U. Kocian Martin SLAC Kodys Peter Charles U. Koffas Thomas Carleton U. Koffeman Els FOM, Amsterdam Kogan Lucy Anne Oxford U. Kohlmann Simon Wuppertal U. Kohout Zdenek Prague, Tech. U. Kohriki Takashi KEK, Tsukuba Koi Tatsumi SLAC Kolanoski Hermann Humboldt U., Berlin Kolb Mathis Heidelberg U. Koletsou Iro Annecy, LAPP Komar Aston Lebedev Inst. Komori Yuto Tokyo U., ICEPP Kondo Takahiko KEK, Tsukuba Kondrashova Nataliia DESY Köneke Karsten Freiburg U. König Adriaan NIKHEF, Amsterdam Kono Takanori KEK, Tsukuba Konoplich Rostislav New York U. Manhattan Coll., Riverdale Konstantinidis Nikolaos University Coll. London Kopeliansky Revital Technion Koperny Stefan AGH-UST, Cracow Köpke Lutz Mainz U. Kopp Anna Katharina Freiburg U. Korcyl Krzysztof Cracow, INP Kordas Kostantinos Aristotle U., Thessaloniki Korn Andreas University Coll. London Korol Aleksandr Novosibirsk, IYF Novosibirsk State U. 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Kroll Joe Pennsylvania U. Kroseberg Juergen Bonn U. Krstic Jelena Belgrade U. Kruchonak Uladzimir Dubna, JINR Krüger Hans Bonn U. Krumnack Nils Iowa State U. Kruse Amanda Wisconsin U., Madison Kruse Mark Duke U. Kruskal Michael Boston U. Kubota Takashi Melbourne U. Kucuk Hilal University Coll. London Kuday Sinan Istanbul Aydin U. Kuehn Susanne Freiburg U. Kugel Andreas Heidelberg U. Kuger Fabian Wurzburg U. Kuhl Andrew UC, Santa Cruz Kuhl Thorsten DESY Kukhtin Victor Dubna, JINR Kukla Romain IRFU, Saclay Kulchitsky Yuri Minsk, Inst. Phys. Kuleshov Sergey Santa Maria U., Valparaiso Kuna Marine INFN, Rome Rome U. Kunigo Takuto Kyoto U. Kupco Alexander Prague, Inst. Phys. Kurashige Hisaya Kobe U. Kurochkin Yurii Minsk, Inst. Phys. Kus Vlastimil Prague, Inst. Phys. Kuwertz Emma Sian Victoria U. Kuze Masahiro Tokyo Inst. Tech. Kvita Jiri Palacky U. Kwan Tony Victoria U. Kyriazopoulos Dimitrios Sheffield U. La Rosa Alessandro UC, Santa Cruz La Rosa Navarro Jose Luis Sao Paulo U. 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Lytken Else Lund U. Ma Hong Brookhaven Ma Lian Liang Shandong U. Maccarrone Giovanni Frascati Macchiolo Anna Munich, Max Planck Inst. Macdonald Calum Michael Sheffield U. Maček Boštjan Stefan Inst., Ljubljana Machado Miguens Joana Pennsylvania U. Lisbon U., CFNUL Macina Daniela CERN Madaffari Daniele Marseille, CPPM Madar Romain Clermont-Ferrand U. Maddocks Harvey Jonathan Lancaster U. Mader Wolfgang Dresden, Tech. U. Madsen Alexander Uppsala U., Inst. Theor. Phys. Maeda Junpei Kobe U. Maeland Steffen Bergen U. Maeno Tadashi Brookhaven Maevskiy Artem Moscow State U. Magradze Erekle Gottingen U., II. Phys. Inst. Mahboubi Kambiz Freiburg U. Mahlstedt Joern FOM, Amsterdam Maiani Camilla IRFU, Saclay Maidantchik Carmen Rio de Janeiro Federal U. Maier Andreas Alexander Munich, Max Planck Inst. Maier Thomas Munich U. Maio Amélia LIP, Lisbon Lisbon U., CFNUL Majewski Stephanie Oregon U. Makida Yasuhiro KEK, Tsukuba Makovec Nikola Orsay, LAL Malaescu Bogdan Paris U., VI-VII Malecki Pawel Cracow, INP Maleev Victor St. Petersburg, INP Malek Fairouz LPSC, Grenoble Mallik Usha Iowa U. Malon David Argonne Malone Caitlin SLAC Maltezos Stavros Natl. Tech. U., Athens Malyshev Vladimir Novosibirsk, IYF Malyukov Sergei CERN Mamuzic Judita DESY Mancini Giada Frascati Mandelli Beatrice CERN Mandelli Luciano INFN, Milan Mandić Igor Stefan Inst., Ljubljana Mandrysch Rocco Iowa U. Maneira José LIP, Lisbon Lisbon U., CFNUL Manfredini Alessandro Munich, Max Planck Inst. Manhaes de Andrade Filho Luciano Juiz de Fora U. Manjarres Ramos Joany York U., Canada Mann Alexander Munich U. Manousakis-Katsikakis Arkadios Athens U. Mansoulie Bruno IRFU, Saclay Mantifel Rodger McGill U. Mantoani Matteo Gottingen U., II. Phys. Inst. Mapelli Livio CERN March Luis Witwatersrand U. Marchiori Giovanni Paris U., VI-VII Marcisovsky Michal Prague, Inst. Phys. Marino Christopher Victoria U. 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Robinson James DESY Robson Aidan Glasgow U. Roda Chiara INFN, Pisa Pisa U. Roe Shaun CERN Røhne Ole Oslo U. Rolli Simona Tufts U. Romaniouk Anatoli Moscow Phys. Eng. Inst. Romano Marino INFN, Bologna Bologna U. Romano Saez Silvestre Marino Clermont-Ferrand U. Romero Adam Elena Valencia U., IFIC Rompotis Nikolaos Washington U., Seattle Ronzani Manfredi Freiburg U. Roos Lydia Paris U., VI-VII Ros Eduardo Valencia U., IFIC Rosati Stefano INFN, Rome Rosbach Kilian Freiburg U. Rose Peyton UC, Santa Cruz Rosendahl Peter Lundgaard Bergen U. Rosenthal Oliver Siegen U. Rossetti Valerio Stockholm U. Stockholm U., OKC Rossi Elvira INFN, Naples Naples U. Rossi Leonardo Paolo INFN, Genoa Rosten Jonatan Cambridge U. Rosten Rachel Washington U., Seattle Rotaru Marina Bucharest, IFIN-HH Roth Itamar Weizmann Inst. Rothberg Joseph Washington U., Seattle Rousseau David Orsay, LAL Royon Christophe IRFU, Saclay Rozanov Alexandre Marseille, CPPM Rozen Yoram Technion Ruan Xifeng Witwatersrand U. Rubbo Francesco SLAC Rubinskiy Igor DESY Rud Viacheslav Moscow State U. Rudolph Christian Dresden, Tech. U. Rudolph Matthew Scott Toronto U. Rühr Frederik Freiburg U. Ruiz-Martinez Aranzazu CERN Rurikova Zuzana Freiburg U. Rusakovich Nikolai Dubna, JINR Ruschke Alexander Munich U. Russell Heather Washington U., Seattle Rutherfoord John Arizona U. Ruthmann Nils CERN Ryabov Yury St. Petersburg, INP Rybar Martin Illinois U., Urbana Rybkin Grigori Orsay, LAL Ryder Nick Oxford U. Saavedra Aldo Sydney U. Sabato Gabriele FOM, Amsterdam Sacerdoti Sabrina Buenos Aires U. Saddique Asif Alberta U. Sadrozinski Hartmut UC, Santa Cruz Sadykov Renat Dubna, JINR Safai Tehrani Francesco INFN, Rome Saha Puja Northern Illinois U. Sahinsoy Merve Kirchhoff Inst. Phys. Saimpert Matthias IRFU, Saclay Saito Tomoyuki Tokyo U., ICEPP Sakamoto Hiroshi Tokyo U., ICEPP Sakurai Yuki Waseda U. Salamanna Giuseppe INFN, Rome Rome III U. Salamon Andrea INFN, Rome Salazar Loyola Javier Esteban Santa Maria U., Valparaiso Saleem Muhammad Oklahoma U. Salek David FOM, Amsterdam Sales De Bruin Pedro Henrique Washington U., Seattle Salihagic Denis Munich, Max Planck Inst. Salnikov Andrei SLAC Salt José Valencia U., IFIC Salvatore Daniela INFN, Cosenza Calabria U. Salvatore Pasquale Fabrizio Sussex U. Salvucci Antonio Hong Kong, Chinese U. Salzburger Andreas CERN Sammel Dirk Freiburg U. Sampsonidis Dimitrios Aristotle U., Thessaloniki Sanchez Arturo INFN, Naples Naples U. Sánchez Javier Valencia U., IFIC Sanchez Martinez Victoria Valencia U., IFIC Sandaker Heidi Oslo U. Sandbach Ruth Laura Queen Mary, U. of London Sander Heinz Georg Mainz U. Sanders Michiel Munich U. Sandhoff Marisa Wuppertal U. Sandoval Carlos Antonio Narino U. Sandstroem Rikard Munich, Max Planck Inst. Sankey Dave Rutherford Sannino Mario INFN, Genoa Genoa U. Sansoni Andrea Frascati Santoni Claudio Clermont-Ferrand U. Santonico Rinaldo INFN, Rome Rome U., Tor Vergata Santos Helena LIP, Lisbon Santoyo Castillo Itzebelt Sussex U. Sapp Kevin Pittsburgh U. Sapronov Andrey Dubna, JINR Saraiva João LIP, Lisbon Lisbon U., CFNUL Sarrazin Bjorn Bonn U. Sasaki Osamu KEK, Tsukuba Sasaki Yuichi Tokyo U., ICEPP Sato Koji Tsukuba U. Sauvage Gilles Annecy, LAPP Sauvan Emmanuel Annecy, LAPP Savage Graham Royal Holloway, U. of London Savard Pierre Toronto U. TRIUMF Sawyer Craig Rutherford Sawyer Lee Louisiana Tech. U. Saxon James Chicago U., EFI Sbarra Carla INFN, Bologna Sbrizzi Antonio INFN, Bologna Bologna U. Scanlon Tim University Coll. London Scannicchio Diana UC, Irvine Scarcella Mark Sydney U. Scarfone Valerio INFN, Cosenza Calabria U. Schaarschmidt Jana Weizmann Inst. Schacht Peter Munich, Max Planck Inst. Schaefer Douglas CERN Schaefer Ralph DESY Schaeffer Jan Mainz U. Schaepe Steffen Bonn U. Schaetzel Sebastian Heidelberg U. Schäfer Uli Mainz U. Schaffer Arthur Orsay, LAL Schaile Dorothee Munich U. Schamberger R Dean SUNY, Stony Brook Scharf Veit Kirchhoff Inst. Phys. Schegelsky Valery St. Petersburg, INP Scheirich Daniel Charles U. Schernau Michael UC, Irvine Schiavi Carlo INFN, Genoa Genoa U. Schillo Christian Freiburg U. Schioppa Marco INFN, Cosenza Calabria U. Schlenker Stefan CERN Schmieden Kristof CERN Schmitt Christian Mainz U. Schmitt Sebastian Heidelberg U. Schmitt Stefan DESY Schneider Basil TRIUMF Schnellbach Yan Jie Liverpool U. Schnoor Ulrike Dresden, Tech. U. Schoeffel Laurent IRFU, Saclay Schoening Andre Heidelberg U. Schoenrock Bradley Daniel Michigan State U. Schopf Elisabeth Bonn U. Schorlemmer Andre Lukas Gottingen U., II. Phys. Inst. Schott Matthias Mainz U. Schouten Doug TRIUMF Schovancova Jaroslava Texas U., Arlington Schramm Steven Geneva U. Schreyer Manuel Wurzburg U. Schuh Natascha Mainz U. Schultens Martin Johannes Bonn U. Schultz-Coulon Hans-Christian Kirchhoff Inst. Phys. Schulz Holger Humboldt U., Berlin Schumacher Markus Freiburg U. Schumm Bruce UC, Santa Cruz Schune Philippe IRFU, Saclay Schwanenberger Christian Manchester U. Schwartzman Ariel SLAC Schwarz Thomas Andrew Michigan U. Schwegler Philipp Munich, Max Planck Inst. Schweiger Hansdieter Manchester U. Schwemling Philippe IRFU, Saclay Schwienhorst Reinhard Michigan State U. Schwindling Jerome IRFU, Saclay Schwindt Thomas Bonn U. Sciacca Gianfranco Bern U., LHEP Scifo Estelle Orsay, LAL Sciolla Gabriella Brandeis U. Scuri Fabrizio INFN, Pisa Pisa U. Scutti Federico Bonn U. Searcy Jacob Michigan U. Sedov George DESY Sedykh Evgeny St. Petersburg, INP Seema Pienpen Bonn U. Seidel Sally New Mexico U. Seiden Abraham UC, Santa Cruz Seifert Frank Prague, Tech. U. Seixas José Rio de Janeiro Federal U. Sekhniaidze Givi INFN, Naples Sekhon Karishma Michigan U. Sekula Stephen Southern Methodist U. Seliverstov Dmitry St. Petersburg, INP Semprini-Cesari Nicola INFN, Bologna Bologna U. 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Soldevila Urmila Valencia U., IFIC Solodkov Alexander Serpukhov, IHEP Soloshenko Alexei Dubna, JINR Solovyanov Oleg Serpukhov, IHEP Solovyev Victor St. Petersburg, INP Sommer Philip Freiburg U. Song Hong Ye Hefei, CUST Taiwan, Inst. Phys. Soni Nitesh Adelaide U., Sch. Chem. Phys. Sood Alexander LBL, Berkeley Sopczak Andre Prague, Tech. U. Sopko Bruno Prague, Tech. U. Sopko Vit Prague, Tech. U. Sorin Veronica Barcelona, IFAE Sosa David Heidelberg U. Sosebee Mark Texas U., Arlington Sotiropoulou Calliope Louisa INFN, Pisa Pisa U. Soualah Rachik INFN, Udine Udine U. Soukharev Andrey Novosibirsk, IYF Novosibirsk State U. South David DESY Sowden Benjamin Royal Holloway, U. of London Spagnolo Stefania INFN, Lecce Salento U. Spalla Margherita INFN, Pisa Pisa U. Spangenberg Martin Warwick U. Spanò Francesco Royal Holloway, U. of London Spearman William Robert Harvard U., Phys. Dept. Sperlich Dennis Humboldt U., Berlin Spettel Fabian Munich, Max Planck Inst. 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Torró Pastor Emma Washington U., Seattle Toth Jozsef Marseille, CPPM Budapest, RMKI Touchard Francois Marseille, CPPM Tovey Daniel Sheffield U. Trefzger Thomas Wurzburg U. Tremblet Louis CERN Tricoli Alessandro CERN Trigger Isabel Marian TRIUMF Trincaz-Duvoid Sophie Paris U., VI-VII Tripiana Martin Barcelona, IFAE Trischuk William Toronto U. Trocmé Benjamin LPSC, Grenoble Troncon Clara INFN, Milan Trottier-McDonald Michel LBL, Berkeley Trovatelli Monica Victoria U. Truong Loan INFN, Udine Udine U. Trzebinski Maciej Cracow, INP Trzupek Adam Cracow, INP Tsarouchas Charilaos CERN Tseng Jeffrey Oxford U. Tsiareshka Pavel Minsk, Inst. Phys. Tsionou Dimitra Aristotle U., Thessaloniki Tsipolitis Georgios Natl. Tech. U., Athens Tsirintanis Nikolaos Athens U. Tsiskaridze Shota Barcelona, IFAE Tsiskaridze Vakhtang Freiburg U. Tskhadadze Edisher Tbilisi, Inst. Phys. Tsukerman Ilya Moscow, ITEP Tsulaia Vakhtang LBL, Berkeley Tsuno Soshi KEK, Tsukuba Tsybychev Dmitri SUNY, Stony Brook Tudorache Alexandra Bucharest, IFIN-HH Tudorache Valentina Bucharest, IFIN-HH Tuna Alexander Naip Harvard U., Phys. Dept. Tupputi Salvatore INFN, Bologna Bologna U. Turchikhin Semen Moscow State U. Lomonosov Moscow State U. Turecek Daniel Prague, Tech. U. Turra Ruggero INFN, Milan Milan U. Turvey Andrew John Southern Methodist U. Tuts Michael Nevis Labs, Columbia U. Tykhonov Andrii Geneva U. Tylmad Maja Stockholm U. Stockholm U., OKC Tyndel Mike Rutherford Ueda Ikuo Tokyo U., ICEPP Ueno Ryuichi Carleton U. Ughetto Michael Stockholm U. Stockholm U., OKC Ugland Maren Bergen U. Ukegawa Fumihiko Tsukuba U. Unal Guillaume CERN Undrus Alexander Brookhaven Unel Gokhan UC, Irvine Ungaro Francesca Freiburg U. Unno Yoshinobu KEK, Tsukuba Unverdorben Christopher Munich U. Urban Jozef Kosice, IEF Urquijo Phillip Melbourne U. Urrejola Pedro Mainz U. 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Yao Weiming LBL, Berkeley Yap Yee Chinn Paris U., VI-VII Yasu Yoshiji KEK, Tsukuba Yatsenko Elena Annecy, LAPP Yau Wong Kaven Henry Bonn U. Ye Jingbo Southern Methodist U. Ye Shuwei Brookhaven Yeletskikh Ivan Dubna, JINR Yen Andy L Harvard U., Phys. Dept. Yildirim Eda DESY Yorita Kohei Waseda U. Yoshida Rikutaro Argonne Yoshihara Keisuke Pennsylvania U. Young Charles SLAC Young Christopher John CERN Youssef Saul Boston U. Yu David Ren-Hwa LBL, Berkeley Yu Jaehoon Texas U., Arlington Yu Jiaming Michigan U. Yu Jie Oklahoma State U. Yuan Li Kobe U. Yuen Stephanie P Bonn U. Yurkewicz Adam Northern Illinois U. Yusuff Imran Cambridge U. Malaya U. Zabinski Bartlomiej Cracow, INP Zaidan Remi Iowa U. Zaitsev Alexander Serpukhov, IHEP Moscow, MIPT Zalieckas Justas Bergen U. Zaman Aungshuman SUNY, Stony Brook Zambito Stefano Harvard U., Phys. Dept. Zanello Lucia INFN, Rome Rome U. Zanzi Daniele Melbourne U. Zeitnitz Christian Wuppertal U. Zeman Martin Prague, Tech. U. Zemla Andrzej AGH-UST, Cracow Zeng Qi SLAC Zengel Keith Brandeis U. Zenin Oleg Serpukhov, IHEP Ženiš Tibor Comenius U. Zerwas Dirk Orsay, LAL Zhang Dongliang Michigan U. Zhang Fangzhou Wisconsin U., Madison Zhang Guangyi Hefei, CUST Zhang Huijun Nanjing U. Zhang Jinlong Argonne Zhang Lei Freiburg U. Zhang Ruiqi Hefei, CUST Marseille, CPPM Zhang Xueyao Shandong U. Zhang Zhiqing Orsay, LAL Zhao Xiandong Southern Methodist U. Zhao Yongke Shandong U. Orsay, LAL Zhao Zhengguo Hefei, CUST Zhemchugov Alexey Dubna, JINR Zhong Jiahang Oxford U. Zhou Bing Michigan U. Zhou Chen Duke U. Zhou Lei Nevis Labs, Columbia U. Zhou Li Southern Methodist U. Zhou Mingliang SUNY, Stony Brook Zhou Ning Tsinghua U., Beijing Zhu Cheng Guang Shandong U. Zhu Hongbo Beijing, Inst. High Energy Phys. Zhu Junjie Michigan U. Zhu Yingchun Hefei, CUST Zhuang Xuai Beijing, Inst. High Energy Phys. Zhukov Konstantin Lebedev Inst. Zibell Andre Wurzburg U. Zieminska Daria Indiana U. Zimine Nikolai Dubna, JINR Zimmermann Christoph Mainz U. Zimmermann Stephanie Freiburg U. Zinonos Zinonas Gottingen U., II. Phys. Inst. Zinser Markus Mainz U. Ziolkowski Michael Siegen U. Živković Lidija Belgrade U. Zobernig Georg Wisconsin U., Madison Zoccoli Antonio INFN, Bologna Bologna U. zur Nedden Martin Humboldt U., Berlin Zurzolo Giovanni INFN, Naples Naples U. Zwalinski Lukasz CERN 2015 10 A summary of the constraints from the ATLAS experiment on $R$-parity conserving supersymmetry is presented. Results from 22 separate ATLAS searches are considered, each based on analysis of up to 20.3 fb$^{-1}$ of proton-proton collision data at the centre-of-mass energy of $\sqrt{s}$ = 7 and 8 TeV at the Large Hadron Collider.  The results are interpreted in the context of the 19-parameter phenomenological minimal supersymmetric standard model, in which the lightest supersymmetric particle is a neutralino, taking into account constraints from previous precision electroweak and flavour measurements as well as from dark matter related measurements.  The results are presented in terms of constraints on supersymmetric particle masses and are compared to limits from simplified models. The impact of ATLAS searches on parameters such as the dark matter relic density, the couplings of the observed Higgs boson, and the degree of electroweak fine-tuning is also shown.  Spectra for surviving supersymmetry model points with low fine-tunings are presented. research-article

PoS PoS Summary of SUSY constraints from ATLAS using the phenomenological MSSM Fawcett William James Department of Physics, Oxford University 2016 LeptonPhoton2015 A summary of the ATLAS collaboration's sensitivity to $R$-parity conserving supersymmetry is presented. A total of 22 beyond-the-Standard-Model searches for exotic particles, heavy Higgs bosons and supersymmetric partner particles have been combined to test the validity of a large class of supersymmetric scenarios. In this selection of models, all relevant dark matter, heavy flavour and precision electroweak measurements have been taken into account. The results of these searches are interpreted in the 19-parameter phenomenological-MSSM, and allow one to see where there is room for new physics still to be hiding, in some cases at surprisingly low masses. This is the first time such a large-scale study of this kind has been attempted by an LHC collaboration. research-article

A Search for the Neutral Higgs Bosons of the Minimal Supersymmetric Standard Model with the ATLAS Detector at the Large Hadron Collider Keller John Stakely DESY, Zeuthen A search for the neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM), produced in proton-proton collisions recorded by the ATLAS detector, is pre-sented. The data correspond to an integrated luminosity of 20.3 fb −1 , with a center of mass energy of 8 TeV. The search focuses on final states where the Higgs bosons decay into a τ+ τ− pair, with one τ lepton decaying leptonically and the other hadronically. Two analyses are performed which separately target low-mass and high-mass Higgs bosons, with the former divided into two sub-channels based on the presence or absence of a b-jet in final state. No evidence of new Higgs bosons is found, and upper limits are set on the cross-section times branching ratio of such Higgs bosons, and on the MSSM parameters m A and tanβ. technical-report

Search for Neutral Minimal Supersymmetric Standard Model Higgs Bosons $H/A \to \tau \tau$ produced in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS Detector 2015 A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) decaying to a pair of $\tau$ leptons is performed using a data sample corresponding to an integrated luminosity of 3.2 fb$^{-1}$ from $\sqrt{s} = 13$ TeV proton-proton collisions recorded by the ATLAS detector at the LHC. The heavy resonance produced via gluon-fusion or $b$-associated production is assumed to decay to a $\tau^+ \tau^-$ pair with at least one $\tau$ lepton decaying hadronically. The search is performed in the mass range of 200 GeV - 1.2 TeV. The data are in good agreement with the background predicted by the Standard Model and hence results are given in terms of upper limits on the production cross section times branching fraction of a scalar boson as a function of its mass. The results are interpreted in a range of MSSM scenarios. The most stringent constraints on $\tan\beta$ for the search excludes $\tan\beta > 10$ for $m_A = 200$ GeV. This analysis improves on the limits of the previous ATLAS analysis, based on data collected at $\sqrt{s}=8$ TeV, for the mass range $m_A > 700$ GeV. INTNOTEATLASPUBL

Status and prospects for BSM ( (N)MSSM) Higgs searches at the LHC Casado Maria Pilar Barcelona, IFAE 2016 Searches for Beyond the Standard Model (BSM) Higgs processes in the context of Minimal Supersymmetric Standard Model (MSSM) and Next to MSSM (NMSSM) are presented. The results are based on the first LHC run of pp collision data recorded by the ATLAS and CMS experiments at the CERN Large Hadron Collider at centre-of-mass energies of 7 and 8 TeV, corresponding to an integrated luminosity of about 5 and 20 fb-1 respectively. Current searches constrain large parts of the parameter space. No evidence for BSM Higgs is found. INTNOTEATLASPUBL

Status and prospects for BSM ( (N)MSSM) Higgs searches at the LHC Casado M.P. Barcelona, IFAE 2016 Searches for Beyond the Standard Model Higgs processes in the context of Minimal Supersymmetric Standard Model and Next to MSSM are presented. The results are based on the first LHC run of pp collision data recorded by the ATLAS and CMS experiments at the CERN Large Hadron Collider at centre-of-mass energies of 7 and 8 TeV, corresponding to integrated luminosities of about 5 and 20 fb$^{-1}$ respectively. Current searches constrain large parts of the parameter space. No evidence for BSM Higgs is found. PREPRINT

Eur. Phys. J. C Eur. Phys. J. C Search for Minimal Supersymmetric Standard Model Higgs bosons $H/A$ and for a $Z^{\prime}$ boson in the $\tau \tau$ final state produced in $pp$ collisions at $\sqrt{s}=13$~TeV with the ATLAS Detector Aaboud Morad Oujda U. Aad Georges Marseille, CPPM Abbott Brad Oklahoma U. Abdallah Jalal Texas U., Arlington Abdinov Ovsat Baku, Inst. Phys. Abeloos Baptiste Orsay, LAL Aben Rosemarie FOM, Amsterdam AbouZeid Ossama UC, Santa Cruz Abraham Nicola Sussex U. Abramowicz Halina Tel Aviv U. Abreu Henso Technion Abreu Ricardo Oregon U. Abulaiti Yiming Stockholm U. Stockholm U., OKC Acharya Bobby Samir INFN, Udine ICTP, Trieste King's Coll. London Adachi Shunsuke Tokyo U., ICEPP Adamczyk Leszek AGH-UST, Cracow Adams David Brookhaven Adelman Jahred Northern Illinois U. Adomeit Stefanie Munich U. Adye Tim Rutherford Affolder Tony Liverpool U. Agatonovic-Jovin Tatjana Belgrade U. Agricola Johannes Gottingen U., II. Phys. Inst. Aguilar-Saavedra Juan Antonio LIP, Lisbon CAFPE, Granada Ahlen Steven Boston U. Ahmadov Faig Dubna, JINR Baku, Inst. Phys. Aielli Giulio INFN, Rome Rome U., Tor Vergata Akerstedt Henrik Stockholm U. Stockholm U., OKC Åkesson Torsten Paul Ake Lund U. Akimov Andrei Lebedev Inst. Alberghi Gian Luigi INFN, Bologna Bologna U. Albert Justin Victoria U. Albrand Solveig LPSC, Grenoble Alconada Verzini Maria Josefina La Plata U. Aleksa Martin CERN Aleksandrov Igor Dubna, JINR Alexa Calin Bucharest, IFIN-HH Alexander Gideon Tel Aviv U. Alexopoulos Theodoros Natl. Tech. U., Athens Alhroob Muhammad Oklahoma U. Ali Babar Prague, Tech. U. Aliev Malik INFN, Lecce Salento U. Alimonti Gianluca INFN, Milan Alison John Chicago U., EFI Alkire Steven Patrick Nevis Labs, Columbia U. Allbrooke Benedict Sussex U. Allen Benjamin William Oregon U. Allport Phillip Birmingham U. Aloisio Alberto INFN, Naples Naples U. Alonso Alejandro Bohr Inst. Alonso Francisco La Plata U. 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Bucharest, IFIN-HH Duda Dominik FOM, Amsterdam Dudarev Alexey CERN Dudder Andreas Christian Mainz U. Duffield Emily Marie LBL, Berkeley Duflot Laurent Orsay, LAL Dührssen Michael CERN Dumancic Mirta Weizmann Inst. Dunford Monica Kirchhoff Inst. Phys. Duran Yildiz Hatice Ankara U. Düren Michael Giessen U. Durglishvili Archil Tbilisi State U. Duschinger Dirk Dresden, Tech. U. Dutta Baishali DESY Dyndal Mateusz DESY Eckardt Christoph DESY Ecker Katharina Maria Munich, Max Planck Inst. Edgar Ryan Christopher Michigan U. Edwards Nicholas Charles Edinburgh U. Eifert Till CERN Eigen Gerald Bergen U. Einsweiler Kevin LBL, Berkeley Ekelof Tord Uppsala U., Inst. Theor. Phys. El Kacimi Mohamed Cadi Ayyad U., Marrakech Ellajosyula Venugopal Marseille, CPPM Ellert Mattias Uppsala U., Inst. Theor. Phys. Elles Sabine Annecy, LAPP Ellinghaus Frank Wuppertal U. Elliot Alison Victoria U. Ellis Nicolas CERN Elmsheuser Johannes Brookhaven Elsing Markus CERN Emeliyanov Dmitry Rutherford Enari Yuji Tokyo U., ICEPP Endner Oliver Chris Mainz U. Ennis Joseph Stanford Warwick U. Erdmann Johannes Dortmund U. Ereditato Antonio Bern U., LHEP Ernis Gunar Wuppertal U. Ernst Jesse SUNY, Albany Ernst Michael Brookhaven Errede Steven Illinois U., Urbana Ertel Eugen Mainz U. Escalier Marc Orsay, LAL Esch Hendrik Dortmund U. Escobar Carlos Pittsburgh U. Esposito Bellisario Frascati Etienvre Anne-Isabelle IRFU, Saclay Etzion Erez Tel Aviv U. Evans Hal Indiana U. Ezhilov Alexey St. Petersburg, INP Ezzi Mohammed Mohammed V U., Agdal Fabbri Federica INFN, Bologna Bologna U. Fabbri Laura INFN, Bologna Bologna U. Facini Gabriel Chicago U., EFI Fakhrutdinov Rinat Serpukhov, IHEP Falciano Speranza INFN, Rome Falla Rebecca Jane University Coll. London Faltova Jana CERN Fang Yaquan Beijing, Inst. High Energy Phys. Fanti Marcello INFN, Milan Milan U. Farbin Amir Texas U., Arlington Farilla Addolorata INFN, Rome Farina Christian Pittsburgh U. Farina Edoardo Maria INFN, Pavia Pavia U. Farooque Trisha Barcelona, IFAE Farrell Steven LBL, Berkeley Farrington Sinead Warwick U. Farthouat Philippe CERN Fassi Farida Mohammed V U., Agdal Fassnacht Patrick CERN Fassouliotis Dimitrios Athens U. Faucci Giannelli Michele Royal Holloway, U. of London Favareto Andrea INFN, Genoa Genoa U. Fawcett William James Oxford U. Fayard Louis Orsay, LAL Fedin Oleg St. Petersburg, INP St. Petersburg Polytechnic Inst. Fedorko Wojciech British Columbia U. Feigl Simon Oslo U. Feligioni Lorenzo Marseille, CPPM Feng Cunfeng Shandong U. Feng Eric CERN Feng Haolu Michigan U. Fenyuk Alexander Serpukhov, IHEP Feremenga Last Texas U., Arlington Fernandez Martinez Patricia Valencia U., IFIC Fernandez Perez Sonia Barcelona, IFAE Ferrando James DESY Ferrari Arnaud Uppsala U., Inst. Theor. Phys. Ferrari Pamela FOM, Amsterdam Ferrari Roberto INFN, Pavia Ferreira de Lima Danilo Enoque Heidelberg U. Ferrer Antonio Valencia U., IFIC Ferrere Didier Geneva U. Ferretti Claudio Michigan U. Ferretto Parodi Andrea INFN, Genoa Genoa U. Fiedler Frank Mainz U. Filipčič Andrej Stefan Inst., Ljubljana Filipuzzi Marco DESY Filthaut Frank NIKHEF, Amsterdam Fincke-Keeler Margret Victoria U. Finelli Kevin Daniel Sydney U. Fiolhais Miguel LIP, Lisbon Coimbra U. Fiorini Luca Valencia U., IFIC Firan Ana Southern Methodist U. Fischer Adam SUNY, Albany Fischer Cora Barcelona, IFAE Fischer Julia Wuppertal U. Fisher Wade Cameron Michigan State U. Flaschel Nils DESY Fleck Ivor Siegen U. Fleischmann Philipp Michigan U. Fletcher Gareth Thomas Sheffield U. Fletcher Rob Roy MacGregor Pennsylvania U. Flick Tobias Wuppertal U. Flores Castillo Luis Hong Kong, Chinese U. Flowerdew Michael Munich, Max Planck Inst. Forcolin Giulio Tiziano Manchester U. Formica Andrea IRFU, Saclay Forti Alessandra Manchester U. Foster Andrew Geoffrey Birmingham U. Fournier Daniel Orsay, LAL Fox Harald Lancaster U. Fracchia Silvia Barcelona, IFAE Francavilla Paolo Paris U., VI-VII Franchini Matteo INFN, Bologna Bologna U. Francis David CERN Franconi Laura Oslo U. Franklin Melissa Harvard U., Phys. Dept. Frate Meghan UC, Irvine Fraternali Marco INFN, Pavia Pavia U. Freeborn David University Coll. London Fressard-Batraneanu Silvia CERN Friedrich Felix Dresden, Tech. U. Froidevaux Daniel CERN Frost James Oxford U. Fukunaga Chikara Tokyo Metropolitan U. Fullana Torregrosa Esteban Mainz U. Fusayasu Takahiro Nagasaki Inst. Appl. Sci. Fuster Juan Valencia U., IFIC Gabaldon Carolina LPSC, Grenoble Gabizon Ofir Wuppertal U. Gabrielli Alessandro INFN, Bologna Bologna U. Gabrielli Andrea LBL, Berkeley Gach Grzegorz AGH-UST, Cracow Gadatsch Stefan CERN Gadomski Szymon Royal Holloway, U. of London Gagliardi Guido INFN, Genoa Genoa U. Gagnon Louis Guillaume Montreal U. Gagnon Pauline Indiana U. Galea Cristina NIKHEF, Amsterdam Galhardo Bruno LIP, Lisbon Coimbra U. Gallas Elizabeth Oxford U. Gallop Bruce Rutherford Gallus Petr Prague, Tech. U. Galster Gorm Aske Gram Krohn Bohr Inst. Gan KK Ohio State U. Gao Jun Hefei, CUST Gao Yanyan Edinburgh U. Gao Yongsheng SLAC Fresno State Garay Walls Francisca Edinburgh U. García Carmen Valencia U., IFIC García Navarro José Enrique Valencia U., IFIC Garcia-Sciveres Maurice LBL, Berkeley Gardner Robert Chicago U., EFI Garelli Nicoletta SLAC Garonne Vincent Oslo U. Gascon Bravo Alberto DESY Gasnikova Ksenia DESY Gatti Claudio Frascati Gaudiello Andrea INFN, Genoa Genoa U. Gaudio Gabriella INFN, Pavia Gauthier Lea Montreal U. Gavrilenko Igor Lebedev Inst. Gay Colin British Columbia U. Gaycken Goetz Bonn U. Gazis Evangelos Natl. Tech. U., Athens Gecse Zoltan British Columbia U. Gee Norman Rutherford Geich-Gimbel Christoph Bonn U. Geisen Marc Mainz U. Geisler Manuel Patrice Kirchhoff Inst. Phys. Gellerstedt Karl Stockholm U. Stockholm U., OKC Gemme Claudia INFN, Genoa Genest Marie-Hélène LPSC, Grenoble Geng Cong Hefei, CUST Michigan U. Gentile Simonetta INFN, Rome Rome U. Gentsos Christos Aristotle U., Thessaloniki George Simon Royal Holloway, U. of London Gerbaudo Davide Barcelona, IFAE Gershon Avi Tel Aviv U. Ghasemi Sara Siegen U. Ghneimat Mazuza Bonn U. Giacobbe Benedetto INFN, Bologna Giagu Stefano INFN, Rome Rome U. Giannetti Paola INFN, Pisa Pisa U. Gibbard Bruce Brookhaven Gibson Stephen Royal Holloway, U. of London Gignac Matthew British Columbia U. Gilchriese Murdock LBL, Berkeley Gillam Thomas Cambridge U. Gillberg Dag Carleton U. Gilles Geoffrey Wuppertal U. Gingrich Douglas Alberta U. TRIUMF Giokaris Nikos Athens U. Giordani MarioPaolo INFN, Udine Udine U. Giorgi Filippo Maria INFN, Bologna Giorgi Francesco Michelangelo Humboldt U., Berlin Giraud Pierre-Francois IRFU, Saclay Giromini Paolo Harvard U., Phys. Dept. Giugni Danilo INFN, Milan Giuli Francesco Oxford U. Giuliani Claudia Munich, Max Planck Inst. Giulini Maddalena Heidelberg U. Gjelsten Børge Kile Oslo U. Gkaitatzis Stamatios Aristotle U., Thessaloniki Gkialas Ioannis Aristotle U., Thessaloniki Gkougkousis Evangelos Leonidas Orsay, LAL Gladilin Leonid Moscow State U. Glasman Claudia Madrid, Autonoma U. Glatzer Julian Freiburg U. Glaysher Paul Edinburgh U. Glazov Alexandre DESY Goblirsch-Kolb Maximilian Brandeis U. Godlewski Jan Cracow, INP Goldfarb Steven Melbourne U. Golling Tobias Geneva U. Golubkov Dmitry Serpukhov, IHEP Gomes Agostinho LIP, Lisbon Lisbon U., CFNUL Gonçalo Ricardo LIP, Lisbon Goncalves Pinto Firmino Da Costa Joao IRFU, Saclay Gonella Giulia Freiburg U. Gonella Laura Birmingham U. Gongadze Alexi Dubna, JINR González de la Hoz Santiago Valencia U., IFIC Gonzalez Parra Garoe Barcelona, IFAE Gonzalez-Sevilla Sergio Geneva U. Goossens Luc CERN Gorbounov Petr Andreevich Moscow, ITEP Gordon Howard Brookhaven Gorelov Igor New Mexico U. Gorini Benedetto CERN Gorini Edoardo INFN, Lecce Salento U. Gorišek Andrej Stefan Inst., Ljubljana Gornicki Edward Cracow, INP Goshaw Alfred Duke U. Gössling Claus Dortmund U. Gostkin Mikhail Ivanovitch Dubna, JINR Goudet Christophe Raymond Orsay, LAL Goujdami Driss Cadi Ayyad U., Marrakech Goussiou Anna Washington U., Seattle Govender Nicolin Johannesburg U. CHPC, Cape Town Gozani Eitan Technion Graber Lars Gottingen U., II. Phys. Inst. Grabowska-Bold Iwona AGH-UST, Cracow Gradin Per Olov Joakim LPSC, Grenoble Grafström Per INFN, Bologna Bologna U. Gramling Johanna Geneva U. Gramstad Eirik Oslo U. Grancagnolo Sergio Humboldt U., Berlin Gratchev Vadim St. Petersburg, INP Gravila Paul Mircea West Timisoara U. Gray Heather CERN Graziani Enrico INFN, Rome Greenwood Zeno Dixon Louisiana Tech. U. Grefe Christian Bonn U. Gregersen Kristian University Coll. London Gregor Ingrid-Maria DESY Grenier Philippe SLAC Grevtsov Kirill Annecy, LAPP Griffiths Justin Texas U., Arlington Grillo Alexander UC, Santa Cruz Grimm Kathryn Lancaster U. Grinstein Sebastian Barcelona, IFAE ICREA, Barcelona Gris Philippe Luc Yves Clermont-Ferrand U. Grivaz Jean-Francois Orsay, LAL Groh Sabrina Mainz U. Grohs Johannes Philipp Dresden, Tech. U. Gross Eilam Weizmann Inst. Grosse-Knetter Joern Gottingen U., II. Phys. Inst. Grossi Giulio Cornelio Louisiana Tech. U. Grout Zara Jane University Coll. London Guan Liang Michigan U. Guan Wen Wisconsin U., Madison Guenther Jaroslav Innsbruck U. Guescini Francesco Geneva U. Guest Daniel UC, Irvine Gueta Orel Tel Aviv U. Guido Elisa INFN, Genoa Genoa U. Guillemin Thibault Annecy, LAPP Guindon Stefan SUNY, Albany Gul Umar Glasgow U. Gumpert Christian CERN Guo Jun Shanghai Jiao Tong U. Guo Yicheng Hefei, CUST Michigan U. Gupta Ruchi Southern Methodist U. Gupta Shaun Oxford U. Gustavino Giuliano INFN, Rome Rome U. Gutierrez Phillip Oklahoma U. Gutierrez Ortiz Nicolas Gilberto University Coll. London Gutschow Christian Dresden, Tech. U. Guyot Claude IRFU, Saclay Gwenlan Claire Oxford U. Gwilliam Carl Liverpool U. Haas Andy New York U. Haber Carl LBL, Berkeley Hadavand Haleh Khani Texas U., Arlington Haddad Nacim Mohammed V U., Agdal Hadef Asma Marseille, CPPM Hageböck Stephan Bonn U. Hagihara Mutsuto Tsukuba U. Hajduk Zbigniew Cracow, INP Hakobyan Hrachya Yerevan Phys. Inst. Haleem Mahsana DESY Haley Joseph Oklahoma State U. Halladjian Garabed Michigan State U. Hallewell Gregory David Marseille, CPPM Hamacher Klaus Wuppertal U. Hamal Petr Palacky U. Hamano Kenji Victoria U. Hamilton Andrew Cape Town U. Hamity Guillermo Nicolas Sheffield U. Hamnett Phillip George DESY Han Liang Hefei, CUST Hanagaki Kazunori KEK, Tsukuba Osaka U. Hanawa Keita Tokyo U., ICEPP Hance Michael UC, Santa Cruz Haney Bijan Pennsylvania U. Hanke Paul Kirchhoff Inst. Phys. Hanna Remie IRFU, Saclay Hansen Jørgen Beck Bohr Inst. Hansen Jorn Dines Bohr Inst. Hansen Maike Christina Bonn U. Hansen Peter Henrik Bohr Inst. Hara Kazuhiko Tsukuba U. Hard Andrew Wisconsin U., Madison Harenberg Torsten Wuppertal U. Hariri Faten Orsay, LAL Harkusha Siarhei Minsk, Inst. Phys. Harrington Robert Edinburgh U. Harrison Paul Fraser Warwick U. Hartjes Fred FOM, Amsterdam Hartmann Nikolai Marcel Munich U. Hasegawa Makoto Kobe U. Hasegawa Yoji Shinshu U. Hasib A Oklahoma U. Hassani Samira IRFU, Saclay Haug Sigve Bern U., LHEP Hauser Reiner Michigan State U. Hauswald Lorenz Dresden, Tech. U. Havranek Miroslav Prague, Inst. Phys. Hawkes Christopher Birmingham U. Hawkings Richard John CERN Hayakawa Daiki Tokyo Inst. Tech. Hayden Daniel Michigan State U. Hays Chris Oxford U. Hays Jonathan Michael Queen Mary, U. of London Hayward Helen Liverpool U. Haywood Stephen Rutherford Head Simon Birmingham U. Heck Tobias Mainz U. Hedberg Vincent Lund U. Heelan Louise Texas U., Arlington Heim Sarah Pennsylvania U. Heim Timon LBL, Berkeley Heinemann Beate LBL, Berkeley Heinrich Jochen Jens Munich U. Heinrich Lukas New York U. Heinz Christian Giessen U. Hejbal Jiri Prague, Inst. Phys. Helary Louis CERN Hellman Sten Stockholm U. Stockholm U., OKC Helsens Clement CERN Henderson James Oxford U. Henderson Robert Lancaster U. Heng Yang Wisconsin U., Madison Henkelmann Steffen British Columbia U. Henriques Correia Ana Maria CERN Henrot-Versille Sophie Orsay, LAL Herbert Geoffrey Henry Humboldt U., Berlin Herde Hannah Brandeis U. Herget Verena Wurzburg U. Hernández Jiménez Yesenia Valencia U., IFIC Herten Gregor Freiburg U. Hertenberger Ralf Munich U. Hervas Luis CERN Hesketh Gavin Grant University Coll. London Hessey Nigel FOM, Amsterdam Hetherly Jeffrey Wayne Southern Methodist U. Hickling Robert Queen Mary, U. of London Higón-Rodriguez Emilio Valencia U., IFIC Hill Ewan Victoria U. Hill John Cambridge U. Hiller Karl Heinz DESY Hillier Stephen Birmingham U. Hinchliffe Ian LBL, Berkeley Hines Elizabeth Pennsylvania U. Hinman Rachel Reisner LBL, Berkeley Hirose Minoru Freiburg U. Hirschbuehl Dominic Wuppertal U. Hobbs John SUNY, Stony Brook Hod Noam TRIUMF Hodgkinson Mark Sheffield U. Hodgson Paul Sheffield U. Hoecker Andreas CERN Hoeferkamp Martin New Mexico U. Hoenig Friedrich Munich U. Hohn David Bonn U. Holmes Tova Ray LBL, Berkeley Homann Michael Dortmund U. Honda Takuya KEK, Tsukuba Hong Tae Min Pittsburgh U. Hooberman Benjamin Henry Illinois U., Urbana Hopkins Walter Oregon U. Horii Yasuyuki Nagoya U. Horton Arthur James Simon Fraser U. Hostachy Jean-Yves LPSC, Grenoble Hou Suen Taiwan, Inst. Phys. Hoummada Abdeslam Casablanca U. Howarth James DESY Hoya Joaquin La Plata U. Hrabovsky Miroslav Palacky U. Hristova Ivana Humboldt U., Berlin Hrivnac Julius Orsay, LAL Hryn'ova Tetiana Annecy, LAPP Hrynevich Aliaksei Minsk, High Energy Phys. Ctr. Hsu Catherine Witwatersrand U. Hsu Pai-hsien Jennifer Taiwan, Inst. Phys. Taiwan, Natl. Tsing Hua U. Hsu Shih-Chieh Washington U., Seattle Hu Qipeng Hefei, CUST Hu Shuyang Shanghai Jiao Tong U. Huang Yanping DESY Hubacek Zdenek Prague, Tech. U. Hubaut Fabrice Marseille, CPPM Huegging Fabian Bonn U. Huffman Todd Brian Oxford U. Hughes Emlyn Nevis Labs, Columbia U. Hughes Gareth Lancaster U. Huhtinen Mika CERN Huo Peng SUNY, Stony Brook Huseynov Nazim Dubna, JINR Baku, Inst. Phys. Huston Joey Michigan State U. Huth John Harvard U., Phys. Dept. Iacobucci Giuseppe Geneva U. Iakovidis Georgios Brookhaven Ibragimov Iskander Siegen U. Iconomidou-Fayard Lydia Orsay, LAL Ideal Emma Yale U. Idrissi Zineb Mohammed V U., Agdal Iengo Paolo CERN Igonkina Olga FOM, Amsterdam NIKHEF, Amsterdam Iizawa Tomoya Waseda U. Ikegami Yoichi KEK, Tsukuba Ikeno Masahiro KEK, Tsukuba Ilchenko Yuriy Texas U. Iliadis Dimitrios Aristotle U., Thessaloniki Ilic Nikolina SLAC Ince Tayfun Munich, Max Planck Inst. Introzzi Gianluca INFN, Pavia Pavia U. Ioannou Pavlos Athens U. Iodice Mauro INFN, Rome Iordanidou Kalliopi Nevis Labs, Columbia U. Ippolito Valerio Harvard U., Phys. Dept. Ishijima Naoki Osaka U. Ishino Masaya Tokyo U., ICEPP Ishitsuka Masaki Tokyo Inst. Tech. Ishmukhametov Renat Ohio State U. Issever Cigdem Oxford U. Istin Serhat Bogazici U. Ito Fumiaki Tsukuba U. Iturbe Ponce Julia Mariana Manchester U. Iuppa Roberto INFN, Rome Rome U., Tor Vergata Iwanski Wieslaw Innsbruck U. Iwasaki Hiroyuki KEK, Tsukuba Izen Joseph Texas U., Dallas Izzo Vincenzo INFN, Naples Jabbar Samina Alberta U. Jackson Brett Pennsylvania U. Jackson Paul Adelaide U., Sch. Chem. Phys. Jain Vivek SUNY, Albany Jakobi Katharina Bianca Mainz U. Jakobs Karl Freiburg U. Jakobsen Sune CERN Jakoubek Tomas Prague, Inst. Phys. Jamin David Olivier Oklahoma State U. Jana Dilip Louisiana Tech. U. Jansky Roland Innsbruck U. Janssen Jens Bonn U. Janus Michel Gottingen U., II. Phys. Inst. Jarlskog Göran Lund U. Javadov Namig Dubna, JINR Baku, Inst. Phys. Javůrek Tomáš Freiburg U. Jeanneau Fabien IRFU, Saclay Jeanty Laura LBL, Berkeley Jeng Geng-yuan Sydney U. Jennens David Melbourne U. Jenni Peter Freiburg U. CERN Jeske Carl Warwick U. Jézéquel Stéphane Annecy, LAPP Ji Haoshuang Wisconsin U., Madison Jia Jiangyong SUNY, Stony Brook Jiang Hai Iowa State U. Jiang Yi Hefei, CUST Jiggins Stephen University Coll. London Jimenez Pena Javier Valencia U., IFIC Jin Shan Beijing, Inst. High Energy Phys. Jinaru Adam Bucharest, IFIN-HH Jinnouchi Osamu Tokyo Inst. Tech. Jivan Harshna Witwatersrand U. Johansson Per Sheffield U. Johns Kenneth Arizona U. Johnson William Joseph Washington U., Seattle Jon-And Kerstin Stockholm U. Stockholm U., OKC Jones Graham Warwick U. Jones Roger Lancaster U. Jones Sarah Arizona U. Jones Tim Liverpool U. Jongmanns Jan Kirchhoff Inst. Phys. Jorge Pedro LIP, Lisbon Lisbon U., CFNUL Jovicevic Jelena TRIUMF Ju Xiangyang Wisconsin U., Madison Juste Rozas Aurelio Barcelona, IFAE ICREA, Barcelona Köhler Markus Konrad Weizmann Inst. Kaczmarska Anna Cracow, INP Kado Marumi Orsay, LAL Kagan Harris Ohio State U. Kagan Michael SLAC Kahn Sebastien Jonathan Marseille, CPPM Kaji Toshiaki Waseda U. Kajomovitz Enrique Duke U. Kalderon Charles William Oxford U. Kaluza Adam Mainz U. Kama Sami Southern Methodist U. Kamenshchikov Andrey Serpukhov, IHEP Kanaya Naoko Tokyo U., ICEPP Kaneti Steven Cambridge U. Kanjir Luka Stefan Inst., Ljubljana Kantserov Vadim Moscow Phys. Eng. Inst. Kanzaki Junichi KEK, Tsukuba Kaplan Benjamin New York U. Kaplan Laser Seymour Wisconsin U., Madison Kapliy Anton Chicago U., EFI Kar Deepak Witwatersrand U. Karakostas Konstantinos Natl. Tech. U., Athens Karamaoun Andrew Alberta U. Karastathis Nikolaos Natl. Tech. U., Athens Kareem Mohammad Jawad Gottingen U., II. Phys. Inst. Karentzos Efstathios Natl. Tech. U., Athens Karnevskiy Mikhail Mainz U. Karpov Sergey Dubna, JINR Karpova Zoya Dubna, JINR Karthik Krishnaiyengar New York U. Kartvelishvili Vakhtang Lancaster U. Karyukhin Andrey Serpukhov, IHEP Kasahara Kota Tsukuba U. Kashif Lashkar Wisconsin U., Madison Kass Richard Ohio State U. Kastanas Alex Bergen U. Kataoka Yousuke Tokyo U., ICEPP Kato Chikuma Tokyo U., ICEPP Katre Akshay Geneva U. Katzy Judith DESY Kawagoe Kiyotomo Kyushu U. Kawamoto Tatsuo Tokyo U., ICEPP Kawamura Gen Gottingen U., II. Phys. Inst. Kazanin Vassili Novosibirsk, IYF Novosibirsk State U. Keeler Richard Victoria U. Kehoe Robert Southern Methodist U. Keller John DESY Kempster Jacob Julian Royal Holloway, U. of London Nagoya U. Keoshkerian Houry Toronto U. Kepka Oldrich Prague, Inst. Phys. Kerševan Borut Paul Stefan Inst., Ljubljana Kersten Susanne Wuppertal U. Keyes Robert McGill U. Khader Mazin Illinois U., Urbana Khalil-zada Farkhad Baku, Inst. Phys. Khanov Alexander Oklahoma State U. Kharlamov Alexey Novosibirsk, IYF Novosibirsk State U. Kharlamova Tatyana Novosibirsk, IYF Khoo Teng Jian Geneva U. Khovanskiy Valery Moscow, ITEP Khramov Evgeniy Dubna, JINR Khubua Jemal Tbilisi State U. GTU, Tbilisi Kido Shogo Kobe U. Kilby Callum Royal Holloway, U. of London Kim Hee Yeun Texas U., Arlington Kim Shinhong Tsukuba U. Kim Young-Kee Chicago U., EFI Kimura Naoki Aristotle U., Thessaloniki Kind Oliver Maria Humboldt U., Berlin King Barry Liverpool U. King Matthew Valencia U., IFIC Kirk Julie Rutherford Kiryunin Andrey Munich, Max Planck Inst. Kishimoto Tomoe Tokyo U., ICEPP Kisielewska Danuta AGH-UST, Cracow Kiss Florian Freiburg U. Kiuchi Kenji Tsukuba U. Kivernyk Oleh IRFU, Saclay Kladiva Eduard Kosice, IEF Klein Matthew Henry Nevis Labs, Columbia U. Klein Max Liverpool U. Klein Uta Liverpool U. Kleinknecht Konrad Mainz U. Klimek Pawel Northern Illinois U. Klimentov Alexei Brookhaven Klingenberg Reiner Dortmund U. Klinger Joel Alexander Sheffield U. Klioutchnikova Tatiana CERN Kluge Eike-Erik Kirchhoff Inst. Phys. Kluit Peter FOM, Amsterdam Kluth Stefan Munich, Max Planck Inst. Knapik Joanna Cracow, INP Kneringer Emmerich Innsbruck U. Knoops Edith Marseille, CPPM Knue Andrea Glasgow U. Kobayashi Aine Tokyo U., ICEPP Kobayashi Dai Tokyo Inst. Tech. Kobayashi Tomio Tokyo U., ICEPP Kobel Michael Dresden, Tech. U. Kocian Martin SLAC Kodys Peter Charles U. Koehler Nicolas Maximilian Munich, Max Planck Inst. Koffas Thomas Carleton U. Koffeman Els FOM, Amsterdam Koi Tatsumi SLAC Kolanoski Hermann Humboldt U., Berlin Kolb Mathis Heidelberg U. Koletsou Iro Annecy, LAPP Komar Aston Lebedev Inst. Komori Yuto Tokyo U., ICEPP Kondo Takahiko KEK, Tsukuba Kondrashova Nataliia DESY Köneke Karsten Freiburg U. König Adriaan NIKHEF, Amsterdam Kono Takanori KEK, Tsukuba Ochanomizu U. Konoplich Rostislav New York U. Manhattan Coll., Riverdale Konstantinidis Nikolaos University Coll. London Kopeliansky Revital Indiana U. Koperny Stefan AGH-UST, Cracow Köpke Lutz Mainz U. Kopp Anna Katharina Freiburg U. Korcyl Krzysztof Cracow, INP Kordas Kostantinos Aristotle U., Thessaloniki Korn Andreas University Coll. London Korol Aleksandr Novosibirsk, IYF Novosibirsk State U. Korolkov Ilya Barcelona, IFAE Korolkova Elena Sheffield U. Kortner Oliver Munich, Max Planck Inst. Kortner Sandra Munich, Max Planck Inst. Kosek Tomas Charles U. Kostyukhin Vadim Bonn U. Kotwal Ashutosh Duke U. Kourkoumeli-Charalampidi Athina INFN, Pavia Pavia U. Kourkoumelis Christine Athens U. Kouskoura Vasiliki Brookhaven Kowalewska Anna Bozena Cracow, INP Kowalewski Robert Victor Victoria U. Kowalski Tadeusz AGH-UST, Cracow Kozakai Chihiro Tokyo U., ICEPP Kozanecki Witold IRFU, Saclay Kozhin Anatoly Serpukhov, IHEP Kramarenko Viktor Moscow State U. Kramberger Gregor Stefan Inst., Ljubljana Krasnopevtsev Dimitriy Moscow Phys. Eng. Inst. Krasny Mieczyslaw Witold Paris U., VI-VII Krasznahorkay Attila CERN Kravchenko Anton Brookhaven Kretz Moritz Heidelberg U. Kretzschmar Jan Liverpool U. Kreutzfeldt Kristof Giessen U. Krieger Peter Toronto U. Krizka Karol Chicago U., EFI Kroeninger Kevin Dortmund U. Kroha Hubert Munich, Max Planck Inst. Kroll Joe Pennsylvania U. Kroseberg Juergen Bonn U. Krstic Jelena Belgrade U. Kruchonak Uladzimir Dubna, JINR Krüger Hans Bonn U. Krumnack Nils Iowa State U. Kruse Mark Duke U. Kruskal Michael Boston U. Kubota Takashi Melbourne U. Kucuk Hilal University Coll. London Kuday Sinan Istanbul Aydin U. Kuechler Jan Thomas Wuppertal U. Kuehn Susanne Freiburg U. Kugel Andreas Heidelberg U. Kuger Fabian Wurzburg U. Kuhl Andrew UC, Santa Cruz Kuhl Thorsten DESY Kukhtin Victor Dubna, JINR Kukla Romain IRFU, Saclay Kulchitsky Yuri Minsk, Inst. Phys. Kuleshov Sergey Santa Maria U., Valparaiso Kuna Marine INFN, Rome Rome U. Kunigo Takuto Kyoto U. Kupco Alexander Prague, Inst. Phys. Kurashige Hisaya Kobe U. Kurochkin Yurii Minsk, Inst. Phys. Kus Vlastimil Prague, Inst. Phys. Kuwertz Emma Sian Victoria U. Kuze Masahiro Tokyo Inst. Tech. Kvita Jiri Palacky U. Kwan Tony Victoria U. Kyriazopoulos Dimitrios Sheffield U. La Rosa Alessandro Munich, Max Planck Inst. La Rosa Navarro Jose Luis Sao Paulo U. La Rotonda Laura INFN, Cosenza Calabria U. Lacasta Carlos Valencia U., IFIC Lacava Francesco INFN, Rome Rome U. Lacey James Carleton U. Lacker Heiko Humboldt U., Berlin Lacour Didier Paris U., VI-VII Lacuesta Vicente Ramón Valencia U., IFIC Ladygin Evgueni Dubna, JINR Lafaye Remi Annecy, LAPP Laforge Bertrand Paris U., VI-VII Lagouri Theodota Yale U. Lai Stanley Gottingen U., II. Phys. Inst. Lammers Sabine Indiana U. Lampl Walter Arizona U. Lançon Eric IRFU, Saclay Landgraf Ulrich Freiburg U. Landon Murrough Queen Mary, U. of London Lanfermann Marie Christine Geneva U. Lang Valerie Susanne Kirchhoff Inst. Phys. Lange J örn Christian Barcelona, IFAE Lankford Andrew UC, Irvine Lanni Francesco Brookhaven Lantzsch Kerstin Bonn U. Lanza Agostino INFN, Pavia Laplace Sandrine Paris U., VI-VII Lapoire Cecile CERN Laporte Jean-Francois IRFU, Saclay Lari Tommaso INFN, Milan Lasagni Manghi Federico INFN, Bologna Bologna U. Lassnig Mario CERN Laurelli Paolo Frascati Lavrijsen Wim LBL, Berkeley Law Alexander UC, Santa Cruz Laycock Paul Liverpool U. Lazovich Tomo Harvard U., Phys. Dept. Lazzaroni Massimo INFN, Milan Milan U. Le Brian Melbourne U. Le Dortz Olivier Paris U., VI-VII Le Guirriec Emmanuel Marseille, CPPM Le Quilleuc Eloi IRFU, Saclay LeBlanc Matthew Edgar Victoria U. LeCompte Thomas Argonne Ledroit-Guillon Fabienne Agnes Marie LPSC, Grenoble Lee Claire Alexandra Brookhaven Lee Shih-Chang Taiwan, Inst. Phys. Lee Lawrence Adelaide U., Sch. Chem. Phys. Lefebvre Benoit McGill U. Lefebvre Guillaume Paris U., VI-VII Lefebvre Michel Victoria U. Legger Federica Munich U. 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Morley Anthony Keith Sydney U. Mornacchi Giuseppe CERN Morris John Queen Mary, U. of London Mortensen Simon Stark Bohr Inst. Morvaj Ljiljana SUNY, Stony Brook Mosidze Maia Tbilisi State U. Moss Josh SLAC Motohashi Kazuki Tokyo Inst. Tech. Mount Richard SLAC Mountricha Eleni Brookhaven Moyse Edward Massachusetts U., Amherst Muanza Steve Marseille, CPPM Mudd Richard Birmingham U. Mueller Felix Munich, Max Planck Inst. Mueller James Pittsburgh U. Mueller Ralph Soeren Peter Munich U. Mueller Thibaut Cambridge U. Muenstermann Daniel Lancaster U. Mullen Paul Glasgow U. Mullier Geoffrey Bern U., LHEP Munoz Sanchez Francisca Javiela Manchester U. Murillo Quijada Javier Alberto Birmingham U. Murray Bill Warwick U. Rutherford Musheghyan Haykuhi Gottingen U., II. Phys. Inst. Muškinja Miha Stefan Inst., Ljubljana Myagkov Alexey Serpukhov, IHEP Moscow, MIPT Myska Miroslav Prague, Tech. U. Nachman Benjamin Philip SLAC Nackenhorst Olaf Geneva U. Nagai Koichi Oxford U. 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Pedersen Maiken Oslo U. Pedraza Lopez Sebastian Valencia U., IFIC Pedro Rute LIP, Lisbon Lisbon U., CFNUL Peleganchuk Sergey Novosibirsk, IYF Novosibirsk State U. Penc Ondrej Prague, Inst. Phys. Peng Cong Beijing, Inst. High Energy Phys. Peng Haiping Hefei, CUST Penwell John Indiana U. Peralva Bernardo Juiz de Fora U. Perego Marta Maria IRFU, Saclay Perepelitsa Dennis Brookhaven Perez Codina Estel TRIUMF Perini Laura INFN, Milan Milan U. Pernegger Heinz CERN Perrella Sabrina INFN, Naples Naples U. Peschke Richard DESY Peshekhonov Vladimir Dubna, JINR Peters Krisztian DESY Peters Yvonne Manchester U. Petersen Brian CERN Petersen Troels Bohr Inst. Petit Elisabeth LPSC, Grenoble Petridis Andreas Adelaide U., Sch. Chem. Phys. Petridou Chariclia Aristotle U., Thessaloniki Petroff Pierre Orsay, LAL Petrolo Emilio INFN, Rome Petrov Mariyan Oxford U. Petrucci Fabrizio INFN, Rome Rome III U. 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Polesello Giacomo INFN, Pavia Poley Anne-luise DESY Policicchio Antonio INFN, Cosenza Calabria U. Polifka Richard Toronto U. Polini Alessandro INFN, Bologna Pollard Christopher Samuel Glasgow U. Polychronakos Venetios Brookhaven Pommès Kathy CERN Pontecorvo Ludovico INFN, Rome Pope Bernard Michigan State U. Popeneciu Gabriel Alexandru INCDTIM, Cluj Napoca Poppleton Alan CERN Pospisil Stanislav Prague, Tech. U. Potamianos Karolos LBL, Berkeley Potrap Igor Dubna, JINR Potter Christina Cambridge U. Potter Christopher Oregon U. Poulard Gilbert CERN Poveda Joaquin CERN Pozdnyakov Valery Dubna, JINR Pozo Astigarraga Mikel Eukeni CERN Pralavorio Pascal Marseille, CPPM Pranko Aliaksandr LBL, Berkeley Prell Soeren Iowa State U. Price Darren Manchester U. Price Lawrence Argonne Primavera Margherita INFN, Lecce Prince Sebastien McGill U. Prokofiev Kirill Hong Kong U. Sci. Tech. Prokoshin Fedor Santa Maria U., Valparaiso Protopopescu Serban Brookhaven Proudfoot James Argonne Przybycien Mariusz AGH-UST, Cracow Puddu Daniele INFN, Rome Rome III U. Purohit Milind Brookhaven South Carolina U. Puzo Patrick Orsay, LAL Qian Jianming Michigan U. Qin Gang Glasgow U. Qin Yang Manchester U. Quadt Arnulf Gottingen U., II. Phys. Inst. Quayle William INFN, Udine ICTP, Trieste Queitsch-Maitland Michaela Manchester U. Quilty Donnchadha Glasgow U. Raddum Silje Oslo U. Radeka Veljko Brookhaven Radescu Voica Oxford U. Radhakrishnan Sooraj Krishnan SUNY, Stony Brook Radloff Peter Oregon U. Rados Pere Melbourne U. Ragusa Francesco INFN, Milan Milan U. Rahal Ghita CC, Villeurbanne Raine John Andrew Manchester U. Rajagopalan Srinivasan Brookhaven Rammensee Michael CERN Rangel-Smith Camila Uppsala U., Inst. Theor. Phys. Ratti Maria Giulia INFN, Milan Milan U. Rauscher Felix Munich U. Rave Stefan Mainz U. Ravenscroft Thomas Glasgow U. Ravinovich Ilia Weizmann Inst. Raymond Michel CERN Read Alexander Lincoln Oslo U. Readioff Nathan Peter Liverpool U. Reale Marilea INFN, Lecce Salento U. Rebuzzi Daniela INFN, Pavia Pavia U. Redelbach Andreas Wurzburg U. Redlinger George Brookhaven Reece Ryan UC, Santa Cruz Reed Robert Witwatersrand U. Reeves Kendall Texas U., Dallas Rehnisch Laura Humboldt U., Berlin Reichert Joseph Pennsylvania U. Reiss Andreas Mainz U. Rembser Christoph CERN Ren Huan Beijing, Inst. High Energy Phys. Rescigno Marco INFN, Rome Resconi Silvia INFN, Milan Rezanova Olga Novosibirsk, IYF Novosibirsk State U. Reznicek Pavel Charles U. Rezvani Reyhaneh Montreal U. Richter Robert Munich, Max Planck Inst. Richter Stefan University Coll. London Richter-Was Elzbieta Jagiellonian U. Ricken Oliver Bonn U. Ridel Melissa Paris U., VI-VII Rieck Patrick Humboldt U., Berlin Riegel Christian Johann Wuppertal U. Rieger Julia Gottingen U., II. Phys. Inst. Rifki Othmane Oklahoma U. 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Zhang Fangzhou Wisconsin U., Madison Zhang Guangyi Hefei, CUST Taiwan, Inst. Phys. Zhang Huijun Nanjing U. Zhang Jinlong Argonne Zhang Lei Freiburg U. Zhang Rui Bonn U. Zhang Ruiqi Hefei, CUST Marseille, CPPM Zhang Xueyao Shandong U. Zhang Zhiqing Orsay, LAL Zhao Xiandong Southern Methodist U. Zhao Yongke Shandong U. Zhao Zhengguo Hefei, CUST Zhemchugov Alexey Dubna, JINR Zhong Jiahang Oxford U. Zhou Bing Michigan U. Zhou Chen Wisconsin U., Madison Zhou Lei Nevis Labs, Columbia U. Zhou Li Southern Methodist U. Zhou Mingliang SUNY, Stony Brook Zhou Ning Tsinghua U., Beijing Zhu Cheng Guang Shandong U. Zhu Hongbo Beijing, Inst. High Energy Phys. Zhu Junjie Michigan U. Zhu Yingchun Hefei, CUST Zhuang Xuai Beijing, Inst. High Energy Phys. Zhukov Konstantin Lebedev Inst. Zibell Andre Wurzburg U. Zieminska Daria Indiana U. Zimine Nikolai Dubna, JINR Zimmermann Christoph Mainz U. Zimmermann Stephanie Freiburg U. Zinonos Zinonas Gottingen U., II. Phys. Inst. Zinser Markus Mainz U. Ziolkowski Michael Siegen U. Živković Lidija Belgrade U. Zobernig Georg Wisconsin U., Madison Zoccoli Antonio INFN, Bologna Bologna U. zur Nedden Martin Humboldt U., Berlin Zwalinski Lukasz CERN 2016 76 A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) and for a heavy neutral $Z^{\prime}$ boson is performed using a data sample corresponding to an integrated luminosity of 3.2~fb$^{-1}$ from proton--proton collisions at $\sqrt{s} = 13$~TeV recorded by the ATLAS detector at the LHC. The heavy resonance is assumed to decay to a $\tau^+ \tau^-$ pair with at least one $\tau$ lepton decaying to final states with hadrons and a neutrino. The search is performed in the mass range of 0.2--1.2~TeV for the MSSM neutral Higgs bosons and 0.5--2.5~TeV for the heavy neutral $Z^{\prime}$ boson. The data are in good agreement with the background predicted by the Standard Model and hence results are given as upper limits on the production cross section times branching fraction of the boson decay to $\tau^+\tau^-$ as a function of the boson mass. The results are interpreted in MSSM and $Z^{\prime}$ benchmark scenarios. The most stringent MSSM parameter space constraints for the Higgs boson search exclude at 95\% confidence level (CL) $\tan\beta > 7.6$ for $m_A = 200$~GeV in the $m_{h}^{\textrm{mod+}}$ MSSM scenario. This analysis extends the MSSM limits from previous searches for the mass range $m_A > 500$~GeV. For the Sequential Standard Model, a $Z^{\prime}_\mathrm{SSM}$ mass up to 1.90~TeV is excluded at 95\% CL and masses up to 1.82--2.17~TeV are excluded for a $Z^{\prime}_{\mathrm{SFM}}$ of the Strong Flavour Model. research-article

Search for charged Higgs bosons in the τ+jets final state using 14.7 fb−1 of pp collision data recorded at s√=13 TeV with the ATLAS experiment 2016 The experimental observation of charged Higgs bosons, H±, which are predicted by several models with an extended Higgs sector, would indicate physics beyond the Standard Model. This note presents the results of a search for charged Higgs bosons in 14.7 fb−1 of pp collision data at √ s = 13 TeV recorded by the ATLAS detector at the LHC. The search targets the τ+jets channel in top-quark-associated H ± production with a hadronically decaying W boson and τ lepton in the final state. No evidence of a charged Higgs boson is found. For the mass range of mH± = 200 − 2000 GeV, upper limits are set on the production cross section of the charged Higgs boson with the subsequent decay H± → τν in a range of 2.0 − 0.008 pb. INTNOTEATLASPUBL

Search for Minimal Supersymmetric Standard Model Higgs Bosons $H/A$ in the $\tau\tau$ final state in up to 13.3 fb$^{−1}$ of pp collisions at $\sqrt{s}$= 13 TeV with the ATLAS Detector 2016 A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is performed using a data sample corresponding to an integrated luminosity of up to 13.3 fb$^{-1}$ from proton--proton collisions at $\sqrt{s} = 13$ TeV recorded by the ATLAS detector at the LHC. The heavy resonance is assumed to decay to a $\tau\tau$ pair with at least one $\tau$ lepton decaying hadronically. The search is performed in the mass range of 0.2-1.2 TeV. The data are in good agreement with the background predicted by the Standard Model, hence results are given as upper limits on the production cross section times branching fraction as a function of the Higgs boson mass. The results are interpreted in MSSM benchmark scenarios. The most stringent MSSM parameter space constraints from the search exclude at 95% confidence level $\tan\beta > 9$ for $m_A = 200$~\GeV\ and $\tan\beta > 50$ for $m_A = 1200$~\GeV\ in the $m_{h}^{\text{mod+}}$ MSSM scenario. INTNOTEATLASPUBL

PoS PoS Search for Neutral Minimal Supersymmetric Standard Model Higgs bosons H/A $\to\tau\tau$ produced in \emph{pp} collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector Alvarez Piqueras Damian Valencia U., IFIC 2016 LHCP2016 This analysis corresponds to the search of a heavy neutral Higgs boson of the Minimal Supersymmetric extension of the Standard Model (MSSM) decaying to a pair of tau leptons using proton-proton collisions at $\sqrt{s} = 13$ TeV corresponding to an integrated luminosity of 3.2 fb$^{-1}$ recorded by the ATLAS detector for the Run II of the LHC. The analysis focuses on Higgs bosons produced in the mass range between 200 GeV and 1200 GeV by gluon-gluon fusion and associated production with a $b$-quark for which it defines two separated and optimized categories. The analysis is also split according to the tau decay modes, where at least one of the tau leptons decay to hadrons and a tau neutrino. The estimation of the backgrounds is done using data-driven techniques for leading backgrounds (multijet, W+jets) and MC models for other contributions. The analysis was preliminarily released in December 2015 with the reference ATLAS-CONF-2015-061. research-article

Search for Pair-Produced Supersymmetric Top Quark Partners with the ATLAS Experiment Abulaiti Yiming Stockholm U. Searches for the supersymmetric partner of the top quark (stop) are motivated by natural supersymmetry, where the stop has to be light to cancel the large radiative corrections to the Higgs boson mass. This thesis presents three different searches for the stop at √s = 8 TeV and √s = 13 TeV using data from the ATLAS experiment at CERN’s Large Hadron Collider. The thesis also includes a study of the primary vertex reconstruction performance in data and simulation at √s = 7 TeV using tt and Z events. All stop searches presented are carried out in final states with a single lepton, four or more jets and large missing transverse energy. A search for direct stop pair production is conducted with 20.3 fb−1 of data at a center-of-mass energy of √s = 8 TeV. Several stop decay scenarios are considered, including those to a top quark and the lightest neutralino and to a bottom quark and the lightest chargino. The sensitivity of the analysis is also studied in the context of various phenomenological MSSM models in which more complex decay scenarios can be present. Two different analyses are carried out at √s = 13 TeV. The first one is a search for both gluino-mediated and direct stop pair production with 3.2 fb−1 of data while the second one is a search for direct stop pair production with 13.2 fb−1 of data in the decay scenario to a bottom quark and the lightest chargino. The results of the analyses show no significant excess over the Standard Model predictions in the observed data. Consequently, exclusion limits are set at 95% CL on the masses of the stop and the lightest neutralino. technical-report

Higgs boson parameters and decays into fermions Bluj Michal Jacek NCBJ, Swierk 2016 In 2012 the discovery of a new boson with a mass of about 125 GeV and properties in agreement with those expected for the Higgs boson in the standard model was announced. In this note we review the results of searches for the fermionic decays the Higgs boson and the study of its properties performed with the proton-proton collision data recorded by the ATLAS and CMS detectors at the LHC in 2011 and 2012, corresponding to an integrated luminosity of approximately 5~fb$^{-1}$ and approximately 20~fb$^{-1}$ per experiment at $\sqrt{s}=7$~TeV and $\sqrt{s}=8$~TeV, respectively. Decay rates to fermions and extracted couplings are consistent with the expectation of the standard model. In addition, we present a search for lepton flavour violating decays of the Higgs boson which can occur in several extensions of the standard model, and a search for neutral Higgs bosons decaying to tau pairs performed in the context of the minimal supersymmetric extension of the standard model (MSSM). INTNOTECMSPUBL

PoS PoS Search for the decay of the Higgs boson into two nMSSM pseudo-scalar particles Živković Lidija Institute of Physics, University of Belgrade 2016 ICHEP2016 The next to MSSM theory predicts the existence of a light pseudoscalar boson "a", and the decay of the Higgs boson into a pair of such particles. The search for this model in several final states relative to different decay modes of the "a" particle, is presented using 20.3~fb$^{-1}$ at the $\sqrt{s}=8$~TeV and 3.2~fb$^{-1}$ at the $\sqrt{s}=13$~TeV. research-article

A search for charged Higgs boson with the ATLAS detector at the LHC Cohen Hadar Tel Aviv U. (main) This dissertation considers the search for a charged Higgs boson (H±) in proton-proton collisions with centre-of-mass energies of 7 TeV and 8 TeV, using data collected by the ATLAS experiment at the Large Hadron Collider at CERN. The discovery of such a charged Higgs boson would be a clear indication for physics beyond the Standard Model. The first data collected during the LHC Run-I is analysed, searching for a heavy charged Higgs bosons (above the top quark mass). This study covers the gb -> tH± ->ttb where one top-quark decays leptonically and the other decays hadronically. A significant background originating from tt ̄ processes, in addition to others, may conceal the charged Higgs decay in the data. Methods using boosted decision trees to con- strain such backgrounds and provide signal to background discrimination are presented. Upper limits on the production cross section times branching ratio of H± are derived for the mass range of 200 GeV <=mH± <= 600 GeV for six MSSM benchmark scenarios. technical-report

Searches for Beyond Standard Model Higgs Bosons in $pp$ collisions at $\sqrt{s} = 8$ and 13 TeV with the ATLAS detector Sales De Bruin Pedro Henrique Washington U., Seattle The searches for a Beyond Standard Model (BSM) heavy CP-odd Higgs boson $A$ decaying to $Zh$ in the context of two-Higgs-doublet models (2HDM), and Minimal Supersymmetric Standard Model (MSSM) neutral Higgs bosons $H/A$ decaying to a tau pair are presented. The search for the heavy CP-odd Higgs boson, $A$, is conducted through the $A \rightarrow Zh\rightarrow ll\tau_{lep}\tau_{had}$ decay channel using 20.3 fb$^{-1}$ of proton-proton collision data collected by the ATLAS detector at a center-of-mass of 8 TeV. The search for the neutral MSSM $H/A$ decaying to a tau pair in the lephad $b$-veto final state is done using 3.2 fb$^{-1}$ of protonproton collision data recorded by the ATLAS detector at a center-of-mass of 13 TeV. The observed data agrees with the Standard Model background prediction, and upper limits are set on cross-section times branching ratio of neutral BSM Higgs bosons. technical-report

Search for Neutral MSSM Higgs Bosons Decaying to ${\tau}_{had} {\tau}_{had}$ in $\sqrt{s}$ = 7 TeV Proton–Proton Collisions with the ATLAS Detector Glatzer Julian Barcelona, IFAE In this thesis a search for the neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) in the h/A/H -> tau_had tau_had decay channel is described. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7 TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb^-1. Final states with two hadronic tau-lepton decays requiring either the presence or absence of b-jets are considered and the selection is optimised for Higgs bosons in b-quark associated and gluon-fusion production. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived in combination with the h/A/H -> mu mu, h/A/H -> tau_e tau_mu and h/A/H -> tau_lep tau_had decay channels. The exclusion limits are shown for the production cross section of a generic neutral Higgs boson, phi, as a function of the Higgs boson mass and for h/H/A production in the MSSM as a function of the parameters m_A and tan(beta) in the m_h-max scenario. technical-report

University of Oxford Oxford, United Kingdom A search for neutral high-mass Higgs bosons decaying into pairs of hadronically decaying tau leptons in 13 TeV collisions recorded by the ATLAS detector Pickering Mark Andrew Oxford U. 2017 This thesis outlines the search for neutral Higgs bosons in a mass range of $m_{H/A} = 200\,\mathrm{GeV} - 1.2\,\mathrm{TeV}$, decaying to a pair of hadronically decaying tau leptons. The search is performed using $\sqrt{s} = 13\,\mathrm{TeV}$ proton-proton collision data, corresponding to an integrated luminosity of $3.21\,\mathrm{fb^{-1}}$, recorded by the ATLAS detector. No excess over the predicted Standard Model background is observed and upper limits are placed on the production cross section times branching fraction as a function of the mass of the scalar resonance. When combined with the results of the analysis where one of the tau leptons decays to either a muon or electron, the 95 % confidence level upper limit on the cross section times branching fraction ranges from 1.4 pb at $m_{H/A} = 200\,\mathrm{GeV}$ to 0.025 pb at $m_{H/A} = 1.2\,\mathrm{TeV}$ for a scalar boson produced via gluon-gluon fusion, and 1.6 pb at $m_{H/A} = 200\,\mathrm{GeV}$ to 0.028 pb at $m_{H/A} = 1.2\,\mathrm{TeV}$ for a scalar boson produced via $b$-associated production. The results are interpreted in the Minimal Supersymmetric extension to the Standard Model (MSSM) as a limit on the value of $\,\mathrm{\tan}\beta$, as a function of the mass of the neutral CP-odd MSSM Higgs boson. In the $m_h^{\,\mathrm{mod+}}$ scenario, the 95 % confidence level upper limit is $\,\mathrm{\tan}\beta < 7.6$ for $m_{A} = 200\,\mathrm{GeV}$, and $\,\mathrm{\tan}\beta < 47$ for $m_{A} = 1\,\mathrm{TeV}$. For the mass range $m_{A} > 500\,\mathrm{GeV}$, the upper limit on $\,\mathrm{\tan}\beta$ is improved in comparison to previous ATLAS searches. technical-report

Search for additional heavy neutral Higgs and gauge bosons in the ditau final state produced in 36.1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector 2017 A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) and for heavy neutral $Z^{\prime}$ bosons is performed using a data sample corresponding to an integrated luminosity of 36.1 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC during 2015 and 2016. The heavy resonance is assumed to decay to $\tau^+\tau^-$ with at least one tau lepton decaying to final states with hadrons and a neutrino. The search is performed in the mass range of 0.2-2.25 TeV for the MSSM neutral Higgs bosons and 0.2-4.0 TeV for the heavy neutral $Z^{\prime}$ boson. The data are in good agreement with the background predicted by the Standard Model. The results are interpreted in MSSM and $Z^{\prime}$ benchmark scenarios. In the context of the hMSSM scenario, the most stringent limits for the combined search exclude $\tan\beta$ > 1.0 for $m_{A}$ = 0.25 TeV and $\tan\beta$ > 45 for $m_{A}$ = 1.5 TeV at the 95% confidence level (CL). For the Sequential Standard Model, a $Z^{\prime}_\mathrm{SSM}$ mass up to 2.42 TeV is excluded at 95% CL and masses up to 2.25-2.60 TeV are excluded for a $Z^{\prime}_\mathrm{SFM}$ of the Strong Flavour Model. INTNOTEATLASPUBL

Systematic and Experimental Uncertainties in the Search for Neutral MSSM Higgs Bosons Decaying to Two Tau Leptons Hauswald Lorenz Dresden, Tech. U. For every physics measurement it is essential to precisely know its uncertainty. At the search for neutral MSSM Higgs bosons the decay channel to two tau leptons plays a major role. For this channel the influence of the uncertainty of Monte Carlo generator parameters on the acceptance of the analyses is studied in this thesis. The corresponding uncertainties are found to be in the range of $0$ to $30\,\%$. Physics with tau leptons is exceptionally challenging, because they can decay into hadrons, which, at the Large Hadron Collider, are hardly distinguishable from the overwhelming QCD background. Sophisticated multivariate algorithms aim to identify them correctly. The impact of experimental uncertainties on the outcome of the identification algortihms is subject of the second part of the thesis. The uncertainties obtained are below $7\,\%$. technical-report

Search for Heavy Neutral Higgs Bosons in the $\tau^+\tau^-$ Final State in LHC Proton-Proton Collisions at $\sqrt{s} = 13\,\mathrm{TeV}$ with the ATLAS Detector Hauswald Lorenz Dresden, Tech. U. There are experimental and theoretical indications that the Standard Model of particle physics, although tremendously successful, is not sufficient to describe the universe, even at energies well below the Planck scale. One of the most promising new theories to resolve major open questions, the Minimal Supersymmetric Standard Model, predicts additional neutral and charged Higgs bosons, among other new particles. For the search of the new heavy neutral bosons, the decay into two hadronically decaying tau leptons is especially interesting, as in large parts of the search parameter space it has the second largest branching ratio while allowing for a considerably better background rejection than the leading decay into $b$-quark pairs. This search, based on proton-proton collisions recorded at $\sqrt{s} = 13\,\mathrm{TeV}$ in 2015 and early 2016 by the ATLAS experiment at the Large Hadron Collider at CERN, is presented in this thesis. No significant deviation from the Standard Model expectation is observed and CL$_\mathrm{s}$ exclusion limits are determined, both model-independent and in various MSSM benchmark scenarios. The MSSM exclusion limits are significantly stronger compared to previous searches, due to the increased collision energy and improvements of the event selection and background estimation techniques. The upper limit on $\tan\beta$ at $95\,\%$ confidence level in the $m_h^{\mathrm{mod}+}$ MSSM benchmark scenario ranges from $10$ at $m_A = 300\,\mathrm{GeV}$ to $48$ at $m_A = 1.2\,\mathrm{TeV}$. technical-report

Search for neutral MSSM Higgs bosons in the fully hadronic di-tau decay channel with the ATLAS detector Wahrmund Sebastian Dresden, Tech. U. The search for additional heavy neutral Higgs bosons predicted in Minimal Supersymmetric Extensions of the Standard Model is presented, using the direct decay channel into two tau leptons which themselves decay hadronically. The study is based on proton-proton collisions recorded in 2011 at a center-of-mass energy of 7 TeV with the ATLAS detector at the Large Hadron Collider at CERN. With a sample size corresponding to an integrated luminosity of $4.5\,\text{fb}^{−1}$, no significant excess above the expected Standard Model background prediction is observed and $\text{CL}_\text{S}$ exclusion limits at a 95% confidence level are evaluated for values of the CP-odd Higgs boson mass mA between 140 GeV to 800 GeV within the context of the $m_\text{h}^{\text{max}}$ and $m^{\text{mod}\pm}_\text{h}$ benchmark scenarios. The results are combined with searches for neutral Higgs h bosons performed using proton-proton collisions at a center-of-mass energy of 8 TeV recorded with the ATLAS detector in 2012, with a corresponding integrated luminosity of $19.5\,\text{fb}^{−1}$. The combination allowed an improvement of the exclusion limit at the order of 1 to 3 units in tan β. Within the context of this study, the structure of additional interactions during a single proton-proton collision (the “underlying event”) in di-jet final states is analyzed using collision data at a center-of-mass energy of 7 TeV recorded with the ATLAS detector in 2010, with a corresponding integrated luminosity of $37\,\text{pb}^{−1}$. The contribution of the underlying event is measured up to an energy scale of 800 GeV and compared to the predictions of various models. For several models, significant deviations compared to the measurements are found and the results are provided for the optimization of simulation algorithms. technical-report

Search for Higgs bosons and for Supersymmetric particles at particle collider experiments Muanza Steve Marseille, CPPM The corner stone of the Standard Model (SM) of Particle Physics is the Higgs mechanism. It explains how the bosons W, Z and H acquire a mass via weak interactions. In addition it explains how the charged fermions also acquire a mass through Yukawa interactions. And on top of this, it regularizes the scattering of longitudinal W and Z bosons at high energy. The discovery of a Higgs boson by the ATLAS and the CMS collaborations in 2012 marked the culminating success of the SM at explaining most of the known phenomena. However a few other phenomena such as the Dark Matter and the Dark energy cannot be explained by the SM particles. What's more, the SM leaves several open questions such as a quest for a quantum theory for gravity, the naturalness in the Higgs sector, a possible Grand Unification,... The common thread in topics presented in this habilitation thesis is the search for manifestations of a TeV scale supersymmetric (SUSY) extension of the Standard Model at particle collider experiments. Among the predictions of such models is the presence of a light Higgs boson as well as the presence of SUSY partners of the SM particles. In the first part of this document I remind the structure of the SM and the MSSM, its minimal supersymmetric extension. In the second part I relate searches for Higgs bosons to which I participated in the L3 experiment for the LEP Run2. In the third part I report a search for SUSY partciles at the TEVATRON Run2 using the D0 detector. In the fourth part I report on recent works concentrating on the ATLAS experiment at the LHC Run1. Firstly, I report on an analysis that uses the Higgs boson as a probe to search for SUSY, secondly I present a new method that I designed for some indirect mass measurements using their production integral charge asymmetry at the LHC. technical-report

Study of the Higgs boson discovery potential in the process $pp \to H/A \to \mu^+\mu^-/\tau^+\tau^-$ with the ATLAS detector Dedes Georgios Munich, Tech. U. 2008 In this thesis, the discovery potential of the ATLAS experiment at the Large Hadron Collider (LHC) at CERN for the heavy neutral Higgs bosons H/A of the Min- imal Supersymmetric extension of the Standard Model of particle physics (MSSM) in the decay channels H/A → τ + τ − → e/μ + X and H/A → μ+ μ− has been studied. The ATLAS detector is designed to study the full spectrum of the physics phenomena occuring in the proton-proton collisions at 14 TeV center-of-mass energy and to provide answers to the question of the origin of particle masses and of elec- troweak symmetry breaking. For the studies, the ATLAS muon spectrometer plays an important role. The spectrometer allows for a precise muon momentum measure- ment independently of other ATLAS subdetectors. The performance of the muon spectrometer depends strongly on the performance of the muon tracking detectors, the Monitored Drift Tube Chambers (MDT). Computer programs have been developed in order to test and verify the ATLAS muon spectrometer simulation, an essential ingredient for data analysis. In addi- tion, dedicated programs for the monitoring of the quality of the data collected by the muon spectrometer have been developed and tested with data from cosmic ray muons. High-quality cosmic ray muon data have been used for the calibration of the MDT-chambers. A new calibration method, called analytical autocalibration, has been tested. The proposed method achieved the required accuracy of 20 μm in the determination of the space-to-drift-time relationship of the drift tubes of the MDT chambers with only 2000 muon tracks per chamber. Reliable muon detector simulation and calibration are essential for the study of the MSSM Higgs boson decays H/A → τ + τ − → e/μ + X and H/A → μ+ μ− and of the corresponding background processes. The signal selection and background rejection requirements have been optimized for maximum signal significance. The following results have been obtained for different assumptions on the MSSM Higgs boson mass mA and on the ratio tanβ of the vacuum expectation values of the two MSSM Higgs boson doublets: For the decay into τ -pairs, 5σ signal significance is obtained for tanβ 5 and mA = 150 GeV/c2 or for tanβ 25 and mA = 600 GeV/c2 for an integrated luminosity of 30 fb−1 . For the decay into muon pairs, 5σ signal significance is achieved for tanβ 20 and mA = 200 GeV/c2 or for tanβ 60 and mA = 450 GeV/c2 for an integrated luminosity of 30 fb−1 . In addition, the mass of the Higgs boson H/A can be measured in the decay H/A → μ+ μ− exploiting the high muon momentum resolution of the ATLAS detector. The measurement accuracy degrades with increasing mass. A Higgs boson mass of 200 GeV/c2 can be etermined with an accuracy of 2%. technical-report

ATLAS level-1 jet trigger rates and study of the ATLAS discovery potential of the neutral MSSM Higgs bosons in b-jet decay channels Mahboubi Kambiz Kirchhoff Inst. Phys. Heidelberg U. 2001 The response of the ATLAS calorimeters to electrons, photons and hadrons, in terms of the longitudinal and lateral shower development, is parameterized using the GEANT package and a detailed detector description (DICE). The parameterizations are implemented in the ATLAS Level-1 (LVL1) Calorimeter Trigger fast simulation package which, based on an average detector geometry, simulates the complete chain of the LVL1 calorimeter trigger system. In addition, pile-up effects due to multiple primary interactions are implemented taking into account the shape and time history of the trigger signals. An interface to the fast physics simulation package (ATLFAST) is also developed in order to perform ATLAS physics analysis, including the LVL1 trigger effects, in a consistent way. The simulation tools, the details of the parameterization and the interface are described. The LVL1 jet trigger thresholds corresponding to the current trigger menus are determined within the framework of the fast simulation, and the LVL1 jet trigger rates are estimated. Further, the combination of Et-miss signature with jet and tau triggers is also discussed. A study of the discovery potential of the ATLAS experiment of the neutral MSSM Higgs bosons in the decay channels with multi b-jet final state topologies, namely H -> h,h -> bb,bb and bb,A/H -> bb,bb, is performed. The signal acceptance of the ATLAS LVL1 jet trigger, based on the determined trigger thresholds, is evaluated. Given the dominating jet trigger rates from the QCD multi-jet processes, the b-tagging capability of the LVL2 trigger is essential for the Higgs discovery in these channels. Canonical ATLAS b-tag/mistag efficiencies are applied on reconstructed jets. Finally, 5-sigma discovery contours in the (tan(beta), mA) plane are derived. technical-report

Search for neutral and charged BSM Higgs bosons with the ATLAS detector Álvarez Piqueras Damián Instituto de Fisica Corpuscular (IFIC), Centro Mixto Universidad de Valencia - CSIC 2017 Several theories beyond the Standard Model, like the EWS or 2HDM models, predict the existence of high mass neutral or charged Higgs particles. In this presentation the latest ATLAS results on searches for these particles will be discussed. INTNOTEATLASPUBL

Search for Neutral Higgs Bosons of the MSSM decaying to τhad τhad in proton-proton collisions at √s = 8 TeV with the ATLAS detector Scutti Federico Bonn U. A search for the neutral Higgs bosons predicted by the Minimal Supersymmetric Standard Model, h, H and A, is presented in this thesis. It is based on a data sample with an integrated luminosity of Lint = 19.5 fb−1 from proton-proton collisions with a center-of-mass energy of √ s = 8 TeV produced at the LHC and recorded by the ATLAS experiment in 2012. The search is performed in the decay channel with two tau leptons decaying hadronically, h/H/A → τhadτhad. The selection of events is based on the kinematic and topological properties of a heavy neutral Higgs boson produced by bb¯ annihilation and the gluon-gluon fusion production mechanisms. The search significantly improves upon the sensitivity of previous searches, and leads the sensitivity of the h/H/A → ττ combined search, where other tau decay modes are selected in the final state, for signal masses mA & 350 GeV. As no significant excess is found, exclusion limits are set in the space of the two leading-order free parameters of the MSSM, mA and tanβ. After the discovery of a Higgs boson in 2012, with a mass of mH = 125.09 ± 0.24 GeV, new phenomenological scenarios of the MSSM were proposed. In this search, exclusion limits are obtained for these various scenarios in the mass range mA = 170 − 1000 GeV. Model-independent exclusion limits were also obtained for the cross-section of the production of a generic resonance, φ, by bb¯ annihilation and gluon-gluon fusion. Excluded cross-sections at 95% confidence level are as high as σexcl.(bb¯ → φ → ττ) ≈ 4.2 pb and σexcl.(gg → φ → ττ) ≈ 6.8 pb at mφ = 170 GeV and σexcl.(bb¯ → φ → ττ) ≈ 9.2 fb and σexcl.(gg → φ → ττ) ≈ 10 fb at mφ = 1000 GeV. technical-report

Nuovo Cimento C Nuovo Cimento C Search for additional Higgs bosons Meyer Jochen Department of Physics, Technion 2018 40 The discovery of a Higgs boson with the mass of about 125 GeV completed the particle content predicted by the Standard Model. Even though this model is well-established and consistent with many measurements, it is not capable to solely explain some observations. Many extension addressing this fact introduce additional Higgs-like bosons which can be either neutral, singly-charged or even doubly-charged. The current status of searches based on data of the ATLAS and CMS experiments at the LHC are presented. No indications for such particles were however found. research-article

Search for Neutral MSSM Higgs Bosons H/A -> tau tau at ATLAS Muckhoff Verena Bonn U. technical-report

Measurement of the Higgs boson coupling with tau leptons and search for an additional neutral MSSM Higgs boson with the ATLAS detector Alvarez Piqueras Damian Valencia U., IFIC The aim of this thesis is the search for the Standard Model Higgs boson and for additional heavy MSSM Higgs bosons in the $\tau\tau$ channel with the ATLAS detector of the LHC. The search for the Higgs boson predicted by the Standard Model is performed using the full integrated luminosity of the Run 1 of the LHC: 4.5 fb$^{-1}$ of data collected at an energy in the center of mass of 7 TeV and 20.3 fb$^{-1}$ of data collected at an energy in the center of mass of 8 TeV. The analysis enhances the sensitivity to signal events by implementing a Boosted Decision Tree trained on the signal and background models. The BDT score distribution shows an excess of data over the background expectation, with an observed (expected) statistical significance of 4.5 $\sigma$ (3.4 $\sigma$), which provides evidence for the direct coupling of the Higgs boson to fermions. The measured signal strength normalized to the Standard Model expectation of $\mu = 1.43^{+0.43}_{-0.37}$ is consistent with the predicted Yukawa coupling strength in the Standard Model. The search for additional neutral Higgs bosons predicted by the Minimal Super-symmetric extension of the Standard Model is performed using 3.21 fb$^{-1}$ of data collected during the first year of the Run 2 of the LHC, at an energy in the center of mass of 13 TeV. The data is in good agreement with the background predicted by the Standard Model. Therefore, exclusion limits on the cross-section times branching ratio of the different MSSM production modes and on the $\tan \beta -m_A$ space for different MSSM benchmark scenarios are extracted. The most stringent constraints exclude at 95% confidence level $\tan \beta > 7.6 $ for $m_A = 200 $ GeV in the MSSM $m_h^{\textrm{mod+}}$ scenario. technical-report

PoS PoS Search for additional neutral Higgs bosons in the MSSM Tanaka Junichi Tokyo U., ICEPP 2019 ICHEP2018 Two searches for neutral heavy Higgs: $H/A \rightarrow \tau\tau$ and $A \rightarrow Zh, h \rightarrow b\bar{b}$ are presented with 36.1 fb$^{-1}$ of data at $\sqrt{s} = 13$ TeV recorded by the ATLAS detector at the LHC. There is no statistically significant excess. Upper limits on cross-section times branching fraction and the interpretation of results in the $m_A$-$\tan\beta$ plane are shown within the MSSM. Large areas of high $\tan\beta$ are excluded by $H/A \rightarrow \tau\tau$: $\tan\beta>15$ for $m_A = 1$ TeV in the hMSSM scenario at the 95% confidence level. research-article

Searches for additional charged Higgs bosons in the MSSM Mir Lluisa-Maria Institut de Fisica d'Altes Energies (IFAE), Barcelona Institute of Science and Technology, Barcelona, Spain 2018 Searches for a charged Higgs boson in various decay channels using 36.1 ifb of pp collision data at a centre-of-mass energy of 13 TeV collected with the ATLAS detector at the Large Hadron Collider are presented. No significant excess above the background-only hypothesis is observed and upper limits on the production cross-section times the branching ratio of the charged Higgs boson as a function of its mass are derived. The results are interpreted in benchmark scenarios of the Minimal Supersymmetric Standard Model. INTNOTEATLASPUBL

Prospects for the search for additional Higgs bosons in the ditau final state with the ATLAS detector at HL-LHC 2018 Estimates of the sensitivity of the search for a heavy neutral Higgs boson in the $\tau\tau$ final state with the full High-Luminosity LHC dataset of 3000 $fb^{-1}$ proton-proton collisions at $\sqrt{s} =$ 14 TeV are presented. These estimates are based on the extrapolation of current results obtained with the 36.1 $fb^{-1}$ ATLAS dataset collected in 2015-2016 at $\sqrt{s} =$ 13 TeV. The expected 95 % CL upper exclusion limits or, in alternative, the expected 5 $\sigma$ discovery reach are presented in terms of cross section times branching fraction of the gluon fusion production and $b$-associated production. In the hypothesis that no signal emerges, results are interpreted in the context of MSSM benchmark scenarios, e.g. in the hMSSM scenario $\tan\beta>1$ is expected to be excluded for the mass range $250< m_A < 350$ GeV. The parameter space with the expected 5 $\sigma$ discovery reach is also shown. The impact of the systematic uncertainties is also discussed. INTNOTEATLASPUBL

PoS PoS Searches for BSM Higgs bosons in fermionic decays in ATLAS Bailey Adam Instituto de Fisica Corpuscular (IFIC), Centro Mixto Universidad de Valencia - CSIC 2019 339 Beyond the standard model theories such as the MSSM and other two-Higgs-doublet-models predict an extended Higgs sector. In some scenarios the additional Higgs bosons can have significant branching ratios to fermions. The ATLAS detector at the LHC has set stringent limits on beyond the standard model Higgs bosons from 36.1 fb$^{ -1}$ of proton-proton collision data collected in Run 2. This report summarises some of the searches for heavy neutral beyond the standard model Higgs bosons in τ and top final states. research-article

Search for charged Higgs bosons decaying into top and bottom quarks with single-lepton final states using $pp$ collisions collected at a centre-of-mass energy of 13 TeV by the ATLAS detector Peri Francesco Humboldt U., Berlin 2019 This thesis presents a search for charged Higgs bosons produced in proton–proton collisions at a centre-of-mass energy of 13 TeV, using 36.1 fb$^{−1}$ of data collected by the ATLAS detector at the LHC in 2015 and 2016. The existence of charged Higgs bosons is predicted by various theories Beyond the Standard Model and it is motivated by the inadequacy of the Standard Model to explain some observed experimental phenomena. The work focuses on charged Higgs bosons heavier than the top quark and decaying via $H$± → $tb$. The production in association with a top and a bottom quark ($pp$ → $tbH$$^{±}$) is investigated in the mass range between 200 and 2000 GeV. A final state containing one charged lepton and jets is considered. Multiple kinematic variables are combined using a boosted decision tree (BDT) in order to separate signal and background. The output of the BDT is used to perform a profile likelihood fit of the Monte Carlo predictions to the observed data. No significant excess of events above the expected Standard Model background is observed, therefore upper limits are set for the cross-section of the charged Higgs boson production times the branching fraction of its decay.Limits are also provided for the tanβ parameter of the MSSM, in the m$^{mod-}_{h}$ and hMSSM benchmark scenarios. The work improves the reach of all previous searches, including for the first time masses ranging up to 2000 GeV. technical-report

Interpretations of the combined measurement of Higgs boson production and decay 2020 First combined measurements of the Higgs boson production and decay using up to 139 fb$^{−1}$ of proton–proton collision data at √s = 13 TeV recorded by the ATLAS experiment have recently been performed. This note presents two interpretations of these combined Higgs boson measurements. Measurements targeting Simplified Template Cross Sections in different decay channels are reparameterized in terms of the impact of Standard Model Effective Field Theory (SMEFT) operators and constraints are reported on the corresponding Wilson coefficients. Measurements are furthermore interpreted in several MSSM benchmark scenarios, resulting in constraints on the MSSM parameters ($m_A, \tan β$) that are complementary to those obtained from direct searches for additional Higgs bosons. For all interpretations, no significant deviations from the Standard Model are observed. INTNOTEATLASPUBL

Search for chargino and neutralino production using final states with two soft leptons in pp collisions at √s = 13 TeV Akatsuka Shunichi The Standard Model (SM) of particle physics successfully explains most of the experimental results. Yet, there are some phenomena that cannot be described by the SM, and that implies a new physics beyond the SM. Supersymmetry (SUSY) is one of the natural extensions of the SM, based on boson–fermion symmetry, which predicts existence of a supersymmetric partner for each SM particle. The Minimal Supersymmetric Standard Model (MSSM) with the R-parity conservation is expected to solve several problems in the SM. The masses of the SUSY particles depend on the parameters in the MSSM Lagrangian, which provides various scenarios with different mass spectra. Many scenarios in the MSSM favor the SUSY particles lighter than O(TeV), thus they can be probed by the experiments at the Large Hadron Collider (LHC). The naturalness argument on the Higgs boson mass supports the “Higgsino scenario”, whereas the compatibility of the SUSY particle with the dark matter motivates the “Wino/Bino scenario”. Both of the scenarios predict compressed mass spectra, where the mass of the lightest neutralino \tilde{Chi}^0_1 is close to the masses of the chargino \tilde{Chi}^{\pm}_1 and the second-to-lightest neutralino \tilde{Chi}^0_2. In those scenarios, only low-momentum particles are kinematically allowed to appear in the decay of \tilde{Chi}^0_2 / \tilde{Chi}^{\pm}_1 into \tilde{Chi}^0_1. This thesis presents results of search for electroweak production of \tilde{Chi}^{\pm}_1 , \tilde{Chi}^0_2 and \tilde{Chi}^0_1 with compressed mass spectra. The search uses 139 fb^{−1} of \sqrt{s} = 13 TeV proton--proton collision data at the LHC collected by the ATLAS detector. The search assumes pair production of SUSY particles via electroweak interactions, which decay into the lightest neutralinos \tilde{Chi}^0_1 and SM particles. The lightest neutralinos are invisible in the detector, thus are observed as missing momentum in the transverse direction. The decay process \tilde{Chi}^0_2 \to Z^* \tilde{Chi}^0_1 followed by Z \to ll leads to a characteristic kinematic edge in the spectrum of the invariant mass of the two leptons, at ∆m = m(\tilde{Chi}^0_2) − m(\tilde{Chi}^0_1). The search exploits this feature, using events with two leptons that form a small invariant mass. Events with missing transverse momentum and two same-flavor, oppositely charged leptons are selected, with presence of hadronic activity from initial-state radiation. The compressed mass spectrum expected in the Higgsino and the Wino/Bino scenarios leads to small transverse momentum (pT) of the two leptons. Various new techniques to efficiently reconstruct low-pT leptons, as well as data-driven methods to estimate the backgrounds are applied in the search to enhance the sensitivity for the compressed scenarios. Finally no signals from the MSSM are observed in this search. The data are consistent with predictions from the SM, and the 95% C.L. exclusion limits on the mass of the second-to-lightest neutralino m(\tilde{Chi}^0_2) are set as functions of the mass difference ∆m = m(\tilde{Chi}^0_2) − m(\tilde{Chi}^0_1), for the Higgsino and the Wino/Bino scenarios. For the Higgsino scenario, the lower limits on m(\tilde{Chi}^0_2) is set at 193 GeV for \Delta m = 9.3 GeV, and 92.4 GeV for \Delta m = 2.3 GeV. For the Wino/Bino scenario, two different parameters that produce the same mass spectra are considered. In the first parameter set, the lower limits on m(\tilde{Chi}^0_2) is set at 240 GeV for \Delta m = 7.0 GeV and 92.4 GeV for \Delta m = 1.5 GeV. In the second parameter set, the lower limits on m(\tilde{Chi}^0_2) is set at 241 GeV for \Delta m = 9.0 GeV and 92.4 GeV for \Delta m = 1.7 GeV. Studies using multi-variate analysis techniques for lepton reconstruction are also presented. With including this method, the expected lower limits on m(\tilde{Chi}^0_2) are found to improve by about 15 GeV in the regions with \Delta m larger than 10 GeV, for both parameters sets in the Wino/Bino scenarios. technical-report

Search for trilepton resonances from $R$-parity violating chargino decays in the $B-L$ MSSM Dyckes Ian University of Pennsylvania (US) This dissertation presents a search for the electroweak pair-production of charginos and the associated production of charginos and neutralinos in the $B-L$ Minimal Supersymmetric Standard Model with spontaneous $R$-parity violation. The chargino and neutralino each decay via $R$-parity violating couplings to a charged lepton or neutrino and a $W$, $Z$, or Higgs boson. This analysis searches for resonances in the trilepton invariant mass spectrum, targeting events with charginos decaying to three electrons or muons via a leptonically decaying $Z$ boson. The dataset includes $139\;\text{fb}^{-1}$ of $\sqrt{s}=13\;\text{TeV}$ proton-proton collisions produced at the Large Hadron Collider and collected by the ATLAS detector. With no significant excess observed, limits are set on chargino and neutralino masses between $100\;\text{GeV}$ and $1100\;\text{GeV}$, depending on the assumed branching fractions to leptons (electron, muon, or $\tau$-lepton) and bosons ($W$, $Z$, or Higgs). technical-report

Search for Heavy Higgs Bosons Decaying into Two Tau Leptons with the ATLAS Detector using ${\rm pp}$ Collisions at $\sqrt{{\rm s}}=13$ TeV Ye Hanfei Nanjing University (CN) 2021 A search for heavy neutral Higgs bosons is performed using the LHC Run 2 data, corresponding to an integrated luminosity of 139 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=13$ TeV recorded by the ATLAS detector. The heavy resonance search is performed over the mass range 0.2-2.5 TeV in the $\tau^{+}\tau^{-}$ decay with at least one $\tau$-lepton decaying into handronical final states. The data are in good agreement with the Standard Model predictions. Results are interpreted in terms of several MSSM scenarios. INTNOTEATLASPUBL

Search for heavy neutral Higgs bosons decaying into the fully hadronic di-tau final state with ATLAS Maerker Max Dresden, Tech. U. Although the Standard Model of particle physics is one of the most successful and well-tested theories in physics, many extensions to the Standard Model were proposed that aim to resolve its shortcomings. Many of these models extend the Standard Model by adding additional symmetries such as Supersymmetry with one of the simplest being the Minimal Supersymmetric Standard Model (MSSM). Supersymmetric models also require the presence of a second Higgs-doublet field which predicts the existence of additional Higgs bosons. Hence, the search for these additional Higgs bosons provides an important window into investigating physics beyond the Standard Model. In this thesis, the search for additional heavy neutral Higgs bosons $A$ and $H$ decaying into a fully hadronic tau lepton pair is presented based on $139\,\text{fb}^{-1}$ of data taken by the ATLAS detector during the full LHC Run-2 data taking period from 2015 to 2018. Since no significant excess of data with respect to the background estimation was found, the results are presented in terms of $95\,\%$ CL upper exclusion limits on the cross-section times branching ratio for Higgs bosons produced via gluon-gluon fusion and $b$-associated production. Different Higgs boson mass hypotheses are taken into account ranging from $200\,\text{GeV}$ to $2500\,\text{GeV}$. A combination with the semi-leptonic search channel is performed whose exclusion limits are transformed into the $m_{A}$-$\tan\beta$ parameter space of the hMSSM and various $m_{h}^{125}$ benchmark model scenarios. The combined exclusion limit set in the hMSSM model is compared to the previous publications by the ATLAS and CMS collaboration based on early Run-2 data of $36.1\,\text{fb}^{-1}$ and $35.9\,\text{fb}^{-1}$ respectively. Compared to previous exclusion limits set by ATLAS (CMS) for the hMSSM scenario, significant improvements are observed ranging between $11\,\%$ ($10\,\%$) at $m_A=500\,\text{GeV}$ up to $63\,\%$ ($67\,\%$) at $m_A=1200\,\text{GeV}$. In addition to the Higgs boson search, a novel algorithm is presented to identify and select charged particle tracks reconstructed in the ATLAS inner detector originating from hadronic tau lepton decays. The identification of these tracks is an important part of the tau lepton reconstruction and identification at ATLAS and provides information about the decay multiplicity and charge of the tau lepton. By deploying state-of-the-art recurrent neural networks the reconstruction efficiency for tau leptons with a true decay multiplicity of 1 and 3 charged hadrons improves by about $10\,\%$ and $20\,\%$ respectively. With this improvement, the neural networks achieve a reconstruction efficiency close to the maximum efficiency possible. By exploiting the flexibility of the neural networks, they can be optimized for both offline data analysis and fast software trigger applications. technical-report

Searching for Beyond-the-Standard-Model Physics Using Signatures with Tau Leptons in the Final State at the ATLAS Experiment Krzysiak Janina Anna Polish Academy of Sciences (PL) The main focus of this thesis is the search for heavy, neutral Higgs bosons decaying to two tau leptons. The existence of such bosons is predicted by certain Beyond-the-Standard-Model (BSM) models such as Two-Higgs-Doublet Models and the Minimal Supersymmetric Standard Model (MSSM). The search was conducted in the mass range between 200 GeV and 2.5 TeV using proton-proton collision data collected by the ATLAS detector at the LHC in the years 2015-2018 at a center-of-mass energy of 13 TeV. The analysis was split into two rounds. In the first round, the analysis group followed the same strategy as the one used in a previous paper analyzing only 2015 and 2016 data. The author’s main task within the analysis group was to validate the estimation of background contributions with QCD jets misidentified as tau leptons in events where one of the tau leptons decays to leptons and the other one to hadrons and a neutrino (‘$\tau_\text{lep}\tau_\text{had}$ decay channel’). In this analysis round, no evidence of new bosons was found, and new exclusion limits were set on the BSM Higgs boson production cross-section times the branching ratio to two tau leptons (model-independent limit) and on the phase space of two MSSM benchmark scenarios (model-dependent limits). In the second analysis round, improvements were introduced to the analysis strategy. The author’s task was to develop machine learning models for discriminating between signal and background events in the $\tau_\text{lep}\tau_\text{had}$ decay channel. The goal was to obtain a better performance compared to the standard final discriminating variable, the mass variable $m_T^\text{tot}$. Boosted decision trees and mass-parameterized neural networks were trained using mass variables and kinematic variables. Ultimately, the best performance was obtained with boosted decision trees, improving the expected model-independent exclusion limits by up to 67.5% and 28.6% for low-signal-mass events with and without $b$-jets in the final state, respectively. At the time of submitting this thesis, the second analysis round was ongoing. Two additional areas of focus are presented in this thesis. The first is a theoretical examination of the possible link between the Higgs mass fine-tuning problem and the cosmological constant problem, taking into consideration Veltman and Pauli divergence-cancelling conditions, as well as the Standard Model effective field theory. The possible role of BSM Higgs bosons is discussed here. This part of the thesis is the result of a collaboration between the author and Steven Bass. The second area of focus is the validation of ATLAS Monte Carlo samples containing tau leptons. Validation studies included polarization measurements, branching ratio and kinematic variable checks, and comparisons of input variables for the ATLAS tau-lepton-identifying boosted decision tree model. technical-report

Application of the Profile Likelihood Method to constrain the parameter space of MSSM Higgs bosons’ cross section Lorenz Christian Technische Universitaet Dresden (DE) The subject of this thesis is a basic introduction to statistical methods which are frequently used in various scientific fields. Concepts of parameter estimation and hypothesis tests are discussed and finally applied to particle physics. technical-report

Interpretations of the ATLAS measurements of Higgs boson production and decay rates and differential cross-sections in $pp$ collisions at $\sqrt{s}=13$ TeV 2023 Measurements of the Higgs boson production and decay rates and differential cross-sections have recently been performed by the ATLAS experiment in several decay channels using up to 139 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=13$ TeV recorded at the Large Hadron Collider. This note presents multiple interpretations of these Higgs boson measurements. Measurements of production-mode cross-sections, simplified template cross-sections or fiducial differential cross-sections in different decay channels are reparameterised in terms of the impact of Standard Model Effective Field Theory operators, and constraints are reported on the corresponding Wilson coefficients. Production and decay rate measurements are interpreted in UV-complete extensions of the Standard Model, namely the two-Higgs-doublet model (2HDM) near the alignment limit and the Minimal Supersymmetric Standard Model (MSSM) for various MSSM benchmark scenarios. The constraints on the 2HDM parameters $(\cos(\beta-\alpha), \textrm{tan}\beta)$ and the MSSM parameters $(m_A, \textrm{tan}\beta)$ are complementary to those obtained from direct searches for additional Higgs bosons. INTNOTEATLASPUBL

Whiterose https://etheses.whiterose.ac.uk/33663/ The Search for Beyond the Standard Model Physics using Tau Leptons at the ATLAS Detector Norfolk Mitch University of Sheffield (GB) 2023 The limitations of the Standard Model (SM) of particle physics have perplexed physicists for many years, prompting the exploration of various theoretical SM extensions. This thesis utilises data from the ATLAS experiment, obtained through proton-proton collisions with an integrated luminosity of 139 fb$^{−1}$ at a centre-of-mass energy of 13 TeV, to search for particles predicted by these theories. Searches for Z′ bosons and leptoquarks (LQ) are conducted by employing analysis techniques developed during the 2020 ATLAS search for heavy neutral Higgs boson ($H/A/h$) decays to two tau leptons, as predicted by the Minimal Supersymmetric Standard Model (MSSM). In addition, this thesis presents preliminary work on enhancing the 2020 MSSM $H/A/h \rightarrow \tau^{+}\tau^{-}$ analysis using machine learning techniques and other optimisations. Finally, the progress made by the University of Sheffield towards the mass production of strip barrel modules for the forthcoming ATLAS Inner Tracker upgrade is discussed. No significant deviations from the predictions of the SM are observed in any of the searches. Consequently, upper limits at 95% confidence level are established for various parameters, and the observed limits are utilised to exclude mass ranges for specific models. The Sequential Standard Model (SSM) is used to define the $Z′$ particle in this thesis, and the search results contribute to the ATLAS combination effort investigating the Heavy Vector Triplet (HVT) model. For the SSM, Z′ masses below 3.06 TeV are excluded. Additional constraints are provided on the HVT model, for the fermion-Higgs {g$_f$ , g$_H$ } and generation-inclusive (third-generation) quark-lepton {$g_q, g_{\ell}$} ({$g_{q3} , g_{\ell 3} $}) coupling parameter planes, assuming fermion universality and the Model A benchmark scenario ($g_H$ = −0.56), respectively. In the LQ analysis, masses below 1.28 TeV (1.35 TeV) are excluded for the ̃$S_1 (U_1)$ models. By employing the machine learning and optimisation techniques to enhance the 2020 results, up to 4.2 (2.6) times improvement in the cross-section $\times$ branching ratio upper limit as a function of signal mass is demonstrated for the b-associated (gluon-gluon fusion) production modes. Improvements of up to 3.1 (2.9) in the $\tan \beta$ upper limit as a function of $m_A$ are shown for the hMSSM ($M_h^{125}) benchmark scenarios. The improvements for the MSSM occur exclusively at lower mass points. technical-report

JHEP JHEP Interpretations of the ATLAS measurements of Higgs boson production and decay rates and differential cross-sections in $pp$ collisions at $\sqrt{s}=13$ TeV Aad Georges Marseille, CPPM Abbott Braden Keim Oklahoma U. Abeling Kira Gottingen U., II. Phys. Inst. Abicht Nils Julius Dortmund U. Abidi Haider Brookhaven Aboulhorma Asmaa Mohammed V U., Agdal Abramowicz Halina Tel Aviv U. Abreu Henso Technion Abulaiti Yiming New York U. Acharya Bobby Samir INFN, Udine ICTP, Trieste King's Coll. London Adam Bourdarios Claire Annecy, LAPP Adamczyk Leszek AGH-UST, Cracow Addepalli Sagar Brandeis U. Addison Matt Manchester U. Adelman Jahred Northern Illinois U. Adiguzel Aytul Istanbul U. Adye Tim Rutherford Affolder A.A. UC, Santa Cruz Affolder Tony UC, Santa Cruz Afik Yoav CERN Agaras Merve Nazlim Barcelona, IFAE Agarwala Jinky INFN, Pavia Pavia U. Aggarwal Anamika Mainz U. Agheorghiesei Catalin Cuza U., Iasi Ahmad Ammara CERN Ahmadov Faig CERN Baku, Inst. Phys. Ahmed Waleed Syed McGill U. Ahuja Sudha Royal Holloway, U. of London Ai Xiaocong Hefei, CUST Aielli Giulio Rome U., Tor Vergata Aikot Arya Valencia U., IFIC Ait Tamlihat Malak Mohammed V U., Agdal Aitbenchikh Brahim Casablanca U. Aizenberg Iakov Weizmann Inst. Akbiyik Melike Mainz U. Akesson Torsten Lund U. Akimov Andrei CERN Akiyama Daiya Waseda U. Akolkar Nilima Nilesh Bonn U. Aktas Sina Bogazici U. Al Khoury Konie Nevis Labs, Columbia U. Alberghi Gian Luigi INFN, Bologna Albert Justin Victoria U. Albicocco Pietro Frascati Albouy Guillaume Lucas LPSC, Grenoble Alderweireldt Sara Edinburgh U. Alegria Zackary Lee Oklahoma State U. Aleksa Martin CERN Aleksandrov I.N. CERN Alexa Calin Bucharest, IFIN-HH Alexopoulos Theodoros Natl. Tech. U., Athens Alfonsi Fabrizio INFN, Bologna Algren Malte Geneva U. Alhroob Muhammad Oklahoma U. Ali Babar Prague, Tech. U. Ali H.M. J. Lancaster U. Ali Shahzad Taiwan, Inst. Phys. Alibocus Samuel William Liverpool U. Aliev Malik SUNY, Stony Brook Alimonti Gianluca INFN, Milan Alkakhi Wael Gottingen U., II. Phys. Inst. Allaire Corentin IJCLab, Orsay Allbrooke Benedict Sussex U. Allen Julia Frances Edinburgh U. Allendes Flores Cristian Andres Santa Maria U., Valparaiso Allport Philip Patrick Birmingham U. Aloisio Alberto Naples U. Alonso Francisco La Plata U. Alpigiani Cristiano Washington U., Seattle Alvarez Estevez Manuel Madrid, Autonoma U. Alvarez Fernandez Adrian Mainz U. Alves Cardoso Mario Geneva U. Alviggi Mariagrazia Naples U. Aly Mohamed Manchester U. Do Amaral Coutinho Yara Rio de Janeiro Federal U. Ambler Alessandro McGill U. Amelung Christoph CERN Amerl Maximilian Manchester U. Ames Christoph Munich U. Amidei Dante Michigan U. Amor Dos Santos Susana Patricia LIP, Lisbon Amos Kieran Robert Valencia U., IFIC Ananiev Viktor Oslo U. Anastopoulos Christos Sheffield U. Andeen Timothy Robert Texas U. Anders John Kenneth CERN Andrean Stefio Yosse Stockholm U. Stockholm U., OKC Andreazza Attilio INFN, Milan Milan U. Angelidakis Stylianos Athens U. Angerami Aaron Nevis Labs, Columbia U. LLNL, Livermore Anisenkov Alexey CERN Annovi Alberto INFN, Pisa Antel Claire Geneva U. Anthony Matthew Thomas Sheffield U. Antipov Egor SUNY, Stony Brook Antonelli Mario Frascati Anulli Fabio INFN, Rome Aoki Masato KEK, Tsukuba Aoki Takumi Tokyo U., ICEPP Aparisi Pozo Javier Alberto Valencia U., IFIC Aparo Marco Sussex U. Aperio Bella Ludovica DESY Appelt Christian Humboldt U., Berlin Apyan Aram Brandeis U. Aranzabal Barrio Nordin CERN Arbiol Val Sergio Javier Cracow, INP Arcangeletti Chiara Frascati Arce Ayana Tamu Duke U. Arena Eloisa Liverpool U. Arguin Jean-Francois Montreal U. Argyropoulos Spyros Freiburg U. Arling Jan-Hendrik DESY Arnaez Olivier Annecy, LAPP Arnold Hannah Nikhef, Amsterdam Artoni Giacomo INFN, Rome Rome U. Asada Haruka Nagoya U. Asai Kanae Ochanomizu U. Asai Shoji Tokyo U., ICEPP Asbah Nedaa Alexandra Harvard U., Phys. Dept. Assahsah Jihad Oujda U. Assamagan Ketevi Adikle Brookhaven Astalos Robert Comenius U. Atashi S. UC, Irvine Atashi Rose UC, Irvine Atkin Ryan Justin Cape Town U. Atkinson Markus Julian Illinois U., Urbana Atmani Hicham Mohammed VI Polytech. U. Atmasiddha Prachi Pennsylvania U. Augsten Kamil Prague, Tech. U. Auricchio Silvia Naples U. Auriol Adrien Birmingham U. Austrup Volker Andreas Manchester U. Avolio Giuseppe CERN Axiotis Konstantinos Geneva U. Azuelos Georges Montreal U. TRIUMF Babal Dominik Kosice, IEF Bachacou Henri IRFU, Saclay Bachas Konstantinos Aristotle U., Thessaloniki Thessaly U. Bachiu Alexander Carleton U. Backman Karl Filip Stockholm U. Stockholm U., OKC Badea Anthony Harvard U., Phys. Dept. Baer Tamas Marton Michigan U. Bagnaia Paolo INFN, Rome Rome U. Bahmani Marzieh Humboldt U., Berlin Bahner Daniel Freiburg U. Bailey Adam Valencia U., IFIC Bailey Virginia Illinois U., Urbana Baines John Rutherford Baines Luke Queen Mary, U. of London Baker Keith Yale U. Bakos Evelin Belgrade U. Bakshi Gupta Debottam Texas U., Arlington Balakrishnan Veena Oklahoma U. Balasubramanian Rahul Nikhef, Amsterdam Baldin Evgenii CERN Balek Petr AGH-UST, Cracow Ballabene Eric INFN, Bologna Bologna U. Balli Fabrice IRFU, Saclay Baltes Lisa Marie Kirchhoff Inst. Phys. Balunas William Keaton Cambridge U. Balz Johannes Mainz U. Banas Elzbieta Cracow, INP Bandieramonte Marilena Pittsburgh U. Bandyopadhyay Anjishnu Bonn U. Bansal Shubham Bonn U. Barak Liron Tel Aviv U. Barakat Marawan DESY Barberio Elisabetta Melbourne U. Barberis Dario INFN, Genoa Genoa U. Barbero Marlon Benoit Marseille, CPPM Barel Marten Zefanja Nikhef, Amsterdam Barends Kevin Nicholas Cape Town U. Barillari Teresa Munich, Max Planck Inst. Barisits Martin CERN Barklow Tim SLAC Baron Petr Palacky U. Baron Moreno D.A. Manchester U. Baroncelli Toni Hefei, CUST Baroncelli A. Hefei, CUST Barone Gaetano Brookhaven Barr Alan Oxford U. Barr Jackson University Coll. London Barranco Navarro Laura Stockholm U. Stockholm U., OKC Barreiro Alonso Fernando Madrid, Autonoma U. Barreiro Alonso Barreiro Madrid, Autonoma U. Barreiro Guimaraes Da Costa Joao Beijing, Inst. High Energy Phys. Barron Uriel Tel Aviv U. Barros Teixeira M.G. LIP, Lisbon Barsov Sergey CERN Bartels Falk Kirchhoff Inst. Phys. Bartoldus Rainer SLAC Barton Adam Edward Lancaster U. Bartos Pavol Comenius U. Basan Alexander Mainz U. Baselga Bacardit Marta Dortmund U. Bassalat Ahmed IJCLab, Orsay An Najah Natl. U. Basso Matthew Joseph TRIUMF Basson Candice Ruth Manchester U. Bates Richard Glasgow U. Batlamous Souad Mohammed V U., Agdal Batley Richard Cambridge U. Batool Binish Siegen U. Battaglia Marco UC, Santa Cruz Battulga Daariimaa Humboldt U., Berlin Bauce Matteo INFN, Rome Rome U. Bauer Michael CERN Bauer Patrick Bonn U. Bazzano Hurrell L.T. Buenos Aires U. Beacham James Duke U. Beau Tristan Paris U., VI-VII Beaucamp Jean Yves La Plata U. Beauchemin Pierre-Hugues Tufts U. Becherer Fabian Freiburg U. Bechtle Philip Bonn U. Beck Hans Peter Bern U., LHEP Fribourg U. Becker Kathrin Warwick U. Beddall Andrew Istinye U., Istanbul Bednyakov Vadim CERN Bee Chris SUNY, Stony Brook Beemster Lars Belgrade U. Beermann Thomas CERN Begalli Marcia Rio de Janeiro State U. Begel Michael Brookhaven Behera Arabinda SUNY, Stony Brook Behr Janna Katharina DESY Beirer Joshua Falco CERN Beisiegel Florian Bonn U. Belfkir Mohamed United Arab Emirates U. Bella Gideon Tel Aviv U. Bellagamba Lorenzo INFN, Bologna Bellerive Alain Carleton U. Bellos Panagiotis Birmingham U. Beloborodov Konstantin CERN Benchekroun Driss Casablanca U. Bendebba Fatima Casablanca U. Benhammou Yan Tel Aviv U. Benoit Mathieu Brookhaven Bensinger J.R. Brandeis U. Bentvelsen Stan Nikhef, Amsterdam Beresford Lydia Audrey DESY Beretta Matteo Mario Frascati Bergeaas Kuutmann Elin Uppsala U., Inst. Theor. Phys. Berger Nicolas Annecy, LAPP Bergmann Benedikt Ludwig Prague, Tech. U. Beringer Juerg LBL, Berkeley Bernardi Gregorio APC, Paris Bernius Catrin SLAC Bernlochner Florian Urs Bonn U. Bernon Florent CERN Marseille, CPPM Berrocal Guardia Adrian Barcelona, IFAE Berry Tracey Royal Holloway, U. of London Berta Peter Charles U. Berthold Anne-Sophie Dresden, Tech. U. Bertram Iain Lancaster U. Bethke Siegfried Munich, Max Planck Inst. Betti Alessandra INFN, Rome Rome U. Bevan Adrian Queen Mary, U. of London Bhalla Naman Kumar Freiburg U. Bhamjee Muaaz Johannesburg U. Bhatta Somadutta SUNY, Stony Brook Bhattacharya Deb Sankar Wurzburg U. Bhattarai Prajita SLAC Bhopatkar Vallary Shashikant Oklahoma State U. Bi Ran Brookhaven Colorado U. Bianchi Riccardo Maria Pittsburgh U. Bianco Gianluca INFN, Bologna Bologna U. Biebel Otmar Munich U. Bielski Rafal Oregon U. Biglietti Michela Rome III U. Bindi Marcello Gottingen U., II. Phys. Inst. Bingul Ahmet Gaziantep U. Bini Cesare INFN, Rome Rome U. Biondini Alessandro Liverpool U. Birch-Sykes Callum Jacob Manchester U. Bird Gareth Adam Birmingham U. Rutherford Birman Mattias Weizmann Inst. Biros Marek Charles U. Biryukov Stanislav Sussex U. Bisanz Tobias Dortmund U. Bisceglie Emanuele INFN, Cosenza Calabria U. Biswal Jyoti Prakash Rutherford Biswas Diptaparna Siegen U. Bitadze Alexander Manchester U. Bjoerke Kristian Oslo U. Bloch Ingo DESY Blue Andrew James Glasgow U. Blumenschein Ulla Queen Mary, U. of London Blumenthal Julian Mainz U. Bobbink Gerjan Nikhef, Amsterdam Bobrovnikov Viktor CERN Boehler Michael Freiburg U. Boehm B. Wurzburg U. Bohm Burkhard Wurzburg U. Bogavac Danijela CERN Bogdanchikov Alexander CERN Bohm Christian Stockholm U. Boisvert Veronique Royal Holloway, U. of London Bokan Petar DESY Bold Tomasz AGH-UST, Cracow Bomben Marco APC, Paris Bona Marcella Queen Mary, U. of London Boonekamp Maarten IRFU, Saclay Booth Callum Dale Royal Holloway, U. of London Borbely Albert Gyorgy Glasgow U. Bordulev Iurii CERN Borecka-Bielska Hanna Maria Montreal U. Borissov Guennadi Lancaster U. Bortoletto Daniela Oxford U. Boscherini Davide INFN, Bologna Fernandez-Bosman Martine Barcelona, IFAE Bossio Sola J.D. CERN Bouaouda Khalil Casablanca U. Bouchhar Naseem Valencia U., IFIC Boudreau Joseph Pittsburgh U. Bouhova-Thacker E.V. Lancaster U. Boumediene Djamel Eddine Clermont-Ferrand U. Bouquet Romain Victoria U. Boveia Antonio Ohio State U. Boyd Jamie CERN Boye Diallo Brookhaven Boyko Igor CERN Bracinik Juraj Birmingham U. Brahimi Nihal Tsung-Dao Lee Inst., Shanghai Brandt Gerhard Immanuel Wuppertal U. Brandt Oleg Cambridge U. Braren Frued Erik DESY Brau Benjamin Paul Massachusetts U., Amherst Brau J.E. Oregon U. Schimmel Brener Roy Weizmann Inst. Brenner Lydia Nikhef, Amsterdam Brenner Richard Uppsala U., Inst. Theor. Phys. Bressler Shikma Weizmann Inst. Britton David Glasgow U. Britzger Daniel Munich, Max Planck Inst. Brock Ian Bonn U. Brock Raymond Michigan State U. Brooijmans Gustaaf Nevis Labs, Columbia U. Brooks William King Santa Maria U., Valparaiso Brost Elizabeth Brookhaven Brost Liza Brookhaven Brown Leesa Victoria U. Bruce Laura Elaine Harvard U., Phys. Dept. Bruckler Tim Lukas Oxford U. Bruckman De Renstrom Pawel Cracow, INP Bruers Ben DESY Bruni Alessia INFN, Bologna Bruni Graziano INFN, Bologna Bruschi Marco INFN, Bologna Bruscino Nello INFN, Rome Rome U. Buanes Trygve Bergen U. Buat Quentin Washington U., Seattle Buchin Daniel Alexander Munich, Max Planck Inst. Buckley Andy Glasgow U. Bulekov Oleg CERN Bullard Brendon SLAC Burdin Sergey Liverpool U. Burgard Carsten Dortmund U. Burger Angela Maria Clermont-Ferrand U. Burghgrave Blake Oliver Texas U., Arlington Burlayenko Oleksandr Freiburg U. Burr J.T. P. Cambridge U. Burton Charles Texas U. Burzynski Jackson Carl Simon Fraser U. Busch Elena Laura Nevis Labs, Columbia U. Buescher Volker Mainz U. Bussey Peter John Glasgow U. Butler John Mark Boston U. Buttar Craig Macleod Glasgow U. Butterworth Jonathan University Coll. London Buttinger Will Rutherford Buttinger William Rutherford Buxo Vazquez Carlos Josue Michigan State U. Buzykaev Alexey CERN Cabrera Urban Susana Valencia U., IFIC Cadamuro Luca IJCLab, Orsay Caforio Davide Giessen U. Cai Huacheng Pittsburgh U. Cai Yuchen Beijing, Inst. High Energy Phys. UCAS, Beijing Cai Yizhou Nanjing U. Cairo Valentina CERN Cakir Orhan Ankara U. Calace Noemi CERN Calafiura Paolo LBL, Berkeley Calderini Giovanni Paris U., VI-VII Calfayan Philippe Indiana U. Callea Giuseppe Glasgow U. Caloba Luiz Pereira Rio de Janeiro Federal U. Calvet David Clermont-Ferrand U. Calvet Samuel Clermont-Ferrand U. Calvet Thomas Philippe Marseille, CPPM Calvetti Milene INFN, Pisa Pisa U. Camacho Toro Reina Coromoto Paris U., VI-VII Camarda Stefano CERN Camarero Munoz Daniel Brandeis U. Camarri Paolo Rome U., Tor Vergata Camerlingo Maria Teresa Naples U. Cameron David CERN Camincher Clement Victoria U. Campanelli Mario University Coll. London Camplani Alessandra Bohr Inst. Canale Vincenzo Naples U. Canesse Auriane McGill U. Cantero Garcia Josu Valencia U., IFIC Cao Yumeng Illinois U., Urbana Capocasa Francesca Brandeis U. Capua Marcella INFN, Cosenza Calabria U. Carbone Antonio INFN, Milan Milan U. Cardarelli Roberto Rome U., Tor Vergata Cardenas Juan Carlos, Jr. Texas U., Arlington Cardillo Fabio Valencia U., IFIC Carducci Giovandomenico INFN, Cosenza Calabria U. Carli Tancredi CERN Carlino Giampaolo Naples U. Carlotto Juan Ignacio Barcelona, IFAE Carlson B.T. Pittsburgh U. Westmont Coll. Carlson Evan Michael Victoria U. TRIUMF Carminati Leonardo INFN, Milan Milan U. Carnelli Alberto IRFU, Saclay Carnesale Maria INFN, Rome Rome U. Caron Sascha Nijmegen U. Carquin Lopez Edson Santa Maria U., Valparaiso Carra Sonia INFN, Milan Carratta Giuseppe INFN, Bologna Bologna U. Carrio Argos Fernando Witwatersrand U. Carter J.W. S. Toronto U. Carter Thomas Michael Edinburgh U. Casado Lechuga Maria Del Pilar Barcelona, IFAE Barcelona, Autonoma U. Caspar Maximilian DESY Castillo Florencia Luciana Annecy, LAPP Castillo Garcia Lucia Barcelona, IFAE Castillo Gimenez Victoria Valencia U., IFIC Castro Nuno LIP, Lisbon Minho U. Catinaccio Andrea CERN Catmore James Oslo U. Cavaliere Viviana Brookhaven Cavalli Noemi INFN, Bologna Bologna U. Cavasinni Vincenzo INFN, Pisa Pisa U. Cekmecelioglu Yusuf Can DESY Celebi Emre Bogazici U. Celli Federico Oxford U. Centonze Martino Salomone INFN, Lecce Salento U. Cepaitis Vilius Geneva U. Cerny Karel Palacky U. Santiago Cerqueira Augusto Juiz de Fora U. Cerri Alex Sussex U. Cerrito Lucio Rome U., Tor Vergata Cerutti Fabio LBL, Berkeley Cervato Beatrice Siegen U. Cervelli Alberto INFN, Bologna Cesarini Gianmario Frascati Cetin Serkant Istinye U., Istanbul Chakraborty Dhiman Northern Illinois U. Chan Jay Wisconsin U., Madison Chan Wai Yuen Tokyo U., ICEPP Chapman John Derek Cambridge U. Chapon Emilien IRFU, Saclay Chargeishvili Bakar Tbilisi State U. Charlton Dave Birmingham U. Chatterjee Meghranjana Bern U., LHEP Chauhan Chainika Charles U. Chekanov Sergei Argonne Chekulaev Sergey TRIUMF Chelkov G.A. CERN Chen Andy Michigan U. Chen Boping Tel Aviv U. Chen Charlie Victoria U. Chen Huirun Nanjing U. Chen Hucheng Brookhaven Chen Jing Shanghai Jiao Tong U. Chen Jiayi Simon Fraser U. Chen Maggie Oxford U. Chen Shion Tokyo U., ICEPP Chen Shenjian Nanjing U. Chen Xiang Shanghai Jiao Tong U. IRFU, Saclay Chen Xin Tsinghua U., Beijing CICQM, Beijing Chen Ye Hefei, CUST Cheng Alkaid Wisconsin U., Madison Cheng Hok Chuen Tom Hong Kong, Chinese U. Cheong Sanha SLAC Cheplakov Alexander CERN Cheremushkina Evgeniya DESY Cherepanova Elizaveta Nikhef, Amsterdam Cherkaoui El Moursli R. Mohammed V U., Agdal Cheu Elliott Arizona U. Cheung Kingman Taiwan, Natl. Tsing Hua U. Chevalier Laurent IRFU, Saclay Chiarella Vitaliano Frascati Chiarelli Giorgio INFN, Pisa Chiedde Nemer Marseille, CPPM Chiodini Gabriele INFN, Lecce Chisholm Andrew Stephen Birmingham U. Chitan Adrian Bucharest, IFIN-HH Chitishvili Mariam Valencia U., IFIC Chizhov Mihail CERN Sofia U. Choi Kyungeon Texas U. Chomont Arthur INFN, Rome Rome U. Chou Yuan-Tang Massachusetts U., Amherst Chow E.Y. S. Nijmegen U. Chowdhury Tasnuva Witwatersrand U. Chu Michael Kwok Lam Weizmann Inst. Chu Ming Chung Hong Kong, Chinese U. Chu Xiaotong Beijing, Inst. High Energy Phys. UCAS, Beijing Chudoba Jiri Prague, Inst. Phys. Chwastowski Janusz Cracow, INP Cieri Davide Munich, Max Planck Inst. Ciesla Krzysztof AGH-UST, Cracow Cindro Vladimir Stefan Inst., Ljubljana Ciocio Alessandra LBL, Berkeley Cirotto Francesco Naples U. Citron Z.H. Weizmann Inst. Ben Gurion U. of Negev Citterio Mauro INFN, Milan Ciubotaru Dan Andrei Bucharest, IFIN-HH Clark Allan Geneva U. Clark Philip Edinburgh U. Clarry Cameron Toronto U. Clavijo Columbie Jose Manuel DESY Clawson Savannah DESY Clement Christophe Stockholm U. Stockholm U., OKC Clercx Joshua DESY Coadou Yann Marseille, CPPM Cobal Marina INFN, Udine Udine U. Coccaro Andrea INFN, Genoa Coelho Barrue R.F. LIP, Lisbon Coelho Lopes De Sa Rafael Massachusetts U., Amherst Coelli Simone INFN, Milan Coimbra A.E. C. INFN, Milan Milan U. Cole Brian Andrew Nevis Labs, Columbia U. Collot Johann LPSC, Grenoble Conde Muino Patricia LIP, Lisbon Lisbon, IST Connell Matt Johannesburg U. Connell Simon Johannesburg U. Connelly Ian Allan Glasgow U. Conroy Eimear Isobel Oxford U. Conventi Francesco Naples U. Parthenope U., Naples Cooke Harry Birmingham U. Cooper-Sarkar A.M. Oxford U. Cordeiro Oudot Choi Artur Paris U., VI-VII Corpe Louie Dartmoor Clermont-Ferrand U. Corradi Massimo INFN, Rome Rome U. Corriveau Francois McGill U. IPP, Canada Cortes-Gonzalez Arely Humboldt U., Berlin Costa Mezquita Maria Jose Valencia U., IFIC Costanza Francesco Annecy, LAPP Costanzo Davide Sheffield U. Cote Benjamin Ohio State U. Cowan Glen Royal Holloway, U. of London Cranmer Kyle Stuart Wisconsin U., Madison Cremonini Davide INFN, Bologna Bologna U. Crepe-Renaudin Sabine LPSC, Grenoble Crescioli Francesco Paris U., VI-VII Cristinziani Markus Siegen U. Cristoforetti Marco TIFPA-INFN, Trento Trento U. Croft Vincent Alexander Nikhef, Amsterdam Crosby Jacob Edwin Oklahoma State U. Crosetti Nanni INFN, Cosenza Calabria U. Crosetti G. Frascati Calabria U. Cueto Gomez Ana Rosario Madrid, Autonoma U. Cuhadar Donszelmann Tulay UC, Irvine Cui Han Beijing, Inst. High Energy Phys. UCAS, Beijing Cui Zhaoyuan Arizona U. Cunningham W.R. Glasgow U. Cunningham Liam Glasgow U. Curcio Francesco INFN, Cosenza Calabria U. Czodrowski Patrick Karl CERN Czurylo Marta Heidelberg U. Da Cunha Sargedas De Sousa M.J. INFN, Genoa Genoa U. Da Fonseca Pinto Joao Victor Rio de Janeiro Federal U. Da Via Cinzia Manchester U. Dabrowski Wladyslaw AGH-UST, Cracow Dado Tomas Dortmund U. Dahbi Salah-Eddine Witwatersrand U. Dai Tiesheng Michigan U. Dal Santo Daniele Bern U., LHEP Dallapiccola Carlo Massachusetts U., Amherst Dam Mogens Bohr Inst. D'Amen Gabriele Brookhaven D'Amico Valerio Munich U. Damp Johannes Frederic Mainz U. Dandoy Jeff Carleton U. Daneri Maria Florencia Buenos Aires U. Danninger Matthias Simon Fraser U. Dao Valerio CERN Darbo Nanni INFN, Genoa Darbo G. INFN, Genoa Darmora Smita Argonne Das Sruthy Jyothi Brookhaven Colorado U. D'Auria Saverio INFN, Milan Milan U. David Claire York U., Canada Davidek Tomas Charles U. Davis-Purcell Benjamin Richard Carleton U. Dawson Ian Queen Mary, U. of London Day-Hall Henry Prague, Tech. U. De Kaushik Texas U., Arlington De Asmundis Riccardo Naples U. De Biase Nicola DESY De Castro Stefano INFN, Bologna Bologna U. De Groot Nicolo Nijmegen U. De Jong Paul Nikhef, Amsterdam De La Torre Perez Hector Northern Illinois U. De Maria Antonio Nanjing U. De Salvo Alessandro INFN, Rome De Sanctis Umberto Rome U., Tor Vergata De Santis Francesco INFN, Lecce Salento U. De Santo Antonella Sussex U. De Vivie De Regie Jean-Baptiste LPSC, Grenoble Dedovich Dmitri CERN Degens Jordy Nikhef, Amsterdam Deiana Allison Mccarn Southern Methodist U. Del Corso Francesca INFN, Bologna Bologna U. Del Peso Jose Madrid, Autonoma U. Del Rio Fer Kirchhoff Inst. Phys. Delagrange Line Paris U., VI-VII Deliot Frederic IRFU, Saclay Delitzsch Chris Malena Dortmund U. Della Pietra Massimo Naples U. Della Volpe Domenico Geneva U. Dell'Acqua Andrea CERN Dell'Asta Lidia INFN, Milan Milan U. Delmastro Marco Annecy, LAPP Delsart Pierre Antoine LPSC, Grenoble Demers Sarah Marie Yale U. Demichev Mikhail CERN Denisov Serguei CERN D'Eramo Louis Clermont-Ferrand U. Derendarz Dominik Karol Cracow, INP Derue Frederic Paris U., VI-VII Dervan Paul Liverpool U. Desch Klaus Bonn U. Deutsch Christopher Bonn U. Di Bello Francesco Armando INFN, Genoa Genoa U. Di Ciaccio Anna Rome U., Tor Vergata Di Ciaccio Lucia Annecy, LAPP Di Domenico Antonio INFN, Rome Rome U. Di Donato Camilla Naples U. Di Girolamo Alessandro CERN Di Gregorio Giulia CERN Di Luca Andrea TIFPA-INFN, Trento Trento U. Di Micco Biagio Rome III U. Di Nardo Roberto Rome III U. Diaconu Cristinel Marseille, CPPM Diamantopoulou Magda Carleton U. De Almeida Dias Flavia Nikhef, Amsterdam Dias Do Vale T. Simon Fraser U. Diaz Gutierrez Marco Aurelio Chile U., Catolica SAPHIR Millennium Inst. Diaz Capriles Federico Guillermo Bonn U. Didenko Mariia Valencia U., IFIC Diehl Edward Michigan U. Diehl Leena Freiburg U. Diez Cornell Sergio DESY Diez Pardos Carmen Siegen U. Dimitriadi Christina Uppsala U., Inst. Theor. Phys. Bonn U. Dimitrievska Aleksandra LBL, Berkeley Dingfelder Jochen Christian Bonn U. Dinu Ioan-Mihail Bucharest, IFIN-HH Dittmeier Sebastian Heidelberg U. Dittus Fido CERN Djama Fares Marseille, CPPM Djobava Tamar Tbilisi State U. Djuvsland Julia Isabell Bergen U. Doglioni Caterina Manchester U. Lund U. Dohnalova Adriana Comenius U. Dolejsi Jiri Charles U. Dolezal Zdenek Charles U. Dona Kristin Chicago U., EFI Donadelli Marisilvia Sao Paulo U. Dong Binbin Michigan State U. Donini Julien Noce Clermont-Ferrand U. D'Onofrio Adelina Naples U. D'Onofrio Monica Liverpool U. Dopke Jens Rutherford Doria Alessandra Naples U. Dos Santos Fernandes Nuno LIP, Lisbon Dougan Patrick Manchester U. Dova Maria Teresa La Plata U. Doyle Tony Glasgow U. Draguet Maxence Oxford U. Dreyer Etienne Weizmann Inst. Drivas-Koulouris Ioannis Natl. Tech. U., Athens Drnevich Matthew New York U. Drobac Alec Swenson Tufts U. Drozdova Mariia Geneva U. Du Dongshuo Hefei, CUST Du Pree Tristan Arnoldus Nikhef, Amsterdam Dubinin Filipp CERN Dubovsky Michal Comenius U. Duchovni Ehud Weizmann Inst. Duckeck Guenter Munich U. Ducu Otilia Anamaria Bucharest, IFIN-HH Duda Dominik Edinburgh U. Dudarev Alexey CERN Duden Emily Rose Brandeis U. D'Uffizi Matteo Manchester U. Duflot Laurent IJCLab, Orsay Duehrssen-Debling Michael CERN Dulsen Carsten Wuppertal U. Dumitriu Ana Elena Bucharest, IFIN-HH Dunford Monica Kirchhoff Inst. Phys. Dungs Sascha Dortmund U. Dunne Katherine Elaine Stockholm U. Stockholm U., OKC Duperrin Arnaud Marseille, CPPM Duran Yildiz H. Ankara U. Dueren Michael Johannes Giessen U. Durglishvili Archil Tbilisi State U. Dwyer Brianna Northern Illinois U. Dyckes G.I. LBL, Berkeley Dyndal Mateusz AGH-UST, Cracow Dziedzic Bartosz Sebastian Cracow, INP Earnshaw Zoe Olivia Sussex U. Eberwein Gregor Hieronymus Oxford U. Eckerova Barbora Comenius U. Eggebrecht Stephen Gottingen U., II. Phys. Inst. Purcino De Souza Edmar Egidio Paris U., VI-VII Ehrke Lukas Geneva U. Eigen Gerald Bergen U. Einsweiler Kevin Frank LBL, Berkeley Ekelof Tord Johan Carl Uppsala U., Inst. Theor. Phys. Ekman Per Alexander Lund U. El Farkh Saad Ibn Tofail U. El Ghazali Yassine Ibn Tofail U. El Jarrari Hassnae CERN El Moussaouy Ali Montreal U. Ellajosyula Venugopal Uppsala U., Inst. Theor. Phys. Ellert Mattias Uppsala U., Inst. Theor. Phys. Ellinghaus Frank Wuppertal U. Ellis Nick CERN Elmsheuser Johannes Brookhaven Elsing Markus CERN Emeliyanov Dmitry Rutherford Enari Yuji Tokyo U., ICEPP Ene Irina LBL, Berkeley Epari Shalini Barcelona, IFAE Erdmann Johannes Dortmund U. Erland Paula Agnieszka Cracow, INP Errenst Martin Wuppertal U. Escalier Marc IJCLab, Orsay Escobar Ibanez Carlos Valencia U., IFIC Etzion Erez Tel Aviv U. Gaspar De Andrade Evans Guiomar LIP, Lisbon Evans Hal Indiana U. Evans Levi Royal Holloway, U. of London Evans Meirin Oan Sussex U. Ezhilov Aleksei CERN Ezzarqtouni Sanae Casablanca U. Fabbri Federica Glasgow U. Fabbri Laura INFN, Bologna Bologna U. Facini Gabriel University Coll. London Fadeyev Vitaliy UC, Santa Cruz Fakhrutdinov Rinat CERN Fakoudis Dionysios Mainz U. Falciano Speranza INFN, Rome Falda Ulhoa Coelho L.F. CERN Falke Peter Johannes Bonn U. Faltova Jana Charles U. Fan Cunwei Illinois U., Urbana Fan Yunyun Beijing, Inst. High Energy Phys. Fang Yaquan Beijing, Inst. High Energy Phys. UCAS, Beijing Fanti Marcello INFN, Milan Milan U. Faraj Mohammed INFN, Udine ICTP, Trieste Farazpay Zahra Louisiana Tech. U. Farbin Amir Texas U., Arlington Farilla Ada Rome III U. Farooque Trisha Michigan State U. Farrington Sinead Edinburgh U. Fassi Farida Mohammed V U., Agdal Fassouliotis Dimitris Athens U. Faucci Giannelli Michele Rome U., Tor Vergata Fawcett William James Cambridge U. Fayard Louis IJCLab, Orsay Federic Pavol Charles U. Federicova Pavla Prague, Inst. Phys. Fedin Oleg CERN Fedotov Gleb CERN Feickert Matthew Wisconsin U., Madison Feligioni Lorenzo Marseille, CPPM Fellers Deion Elgin Oregon U. Feng Cunfeng Shandong U. Feng Minyu Tsinghua U., Beijing Feng Zhuoran Nikhef, Amsterdam Fenton Michael James UC, Irvine Fenyuk Alexandre CERN Ferencz Lars DESY Ferguson Ruby Alice Molly Lancaster U. Fernandez Luengo Sergio Ivan Santa Maria U., Valparaiso Fernandez Martinez Pablo Barcelona, IFAE Fernoux M.J. V. Marseille, CPPM Ferrando James DESY Ferrari Arnaud Uppsala U., Inst. Theor. Phys. Ferrari Pamela Nikhef, Amsterdam Nijmegen U. Ferrari Roberto INFN, Pavia Ferrere Didier Geneva U. Ferretti Claudio Michigan U. Fiedler Frank Mainz U. Fiedler Petr Prague, Tech. U. Filipcic Andrej Stefan Inst., Ljubljana Filmer Emily Adelaide U. Filthaut Frank Nijmegen U. Castro Nunes Fiolhais Miguel LIP, Lisbon Coimbra U. BMCC, New York Fiorini Luca Valencia U., IFIC Fisher Wade Cameron Michigan State U. Fitschen Tobias Manchester U. Fitzhugh Peter Michael IRFU, Saclay Fleck Ivor Siegen U. Fleischmann Philipp Michigan U. Flick Tobias Wuppertal U. Flores Marvin Philippines U., Quezon City Flores Castillo Luis Roberto Hong Kong, Chinese U. Flores Sanz De Acedo Leyre CERN Follega Francesco Maria TIFPA-INFN, Trento Trento U. Fomin Nikolai Bergen U. Foo Joel Hengwei Toronto U. Forland Blake Christopher Indiana U. Formica Andrea IRFU, Saclay Forti Alessandra Manchester U. Fortin Etienne Marie CERN Fortman Anne Winifred Harvard U., Phys. Dept. Foti Maria Giovanna LBL, Berkeley Fountas Leonidas Athens U. Aegean U., Chios Fournier Daniel IJCLab, Orsay Fox Harald Lancaster U. Francavilla Paolo INFN, Pisa Pisa U. Francescato Simone Harvard U., Phys. Dept. Franchellucci Stefano Geneva U. Franchini Matteo INFN, Bologna Bologna U. Franchino Silvia Kirchhoff Inst. Phys. Francis David CERN Franco Luca Nijmegen U. Franco Lima Vinicius CERN Franconi Laura DESY Franklin Melissa Harvard U., Phys. Dept. Frattari Guglielmo Brandeis U. Freegard Arran Charles Queen Mary, U. of London Spolidoro Freund Werner Rio de Janeiro Federal U. Frid Yuval Yitzhak Tel Aviv U. Friend Johnny Glasgow U. Fritzsche Nick Dresden, Tech. U. Froch Alexander Freiburg U. Froidevaux Daniel CERN Frost James Oxford U. Fu Yao Hefei, CUST Fuenzalida Garrido Sebastian Julio Santa Maria U., Valparaiso Fujimoto Minori Marseille, CPPM Fung Kin Yip Hong Kong, Chinese U. Simas Filho Eduardo Furtado De Rio de Janeiro Federal U. Furukawa Marin Tokyo U., ICEPP Fuster Verdu Juan Valencia U., IFIC Gabrielli Alessandro INFN, Bologna Bologna U. Gabrielli Andrea Toronto U. Gadow Philipp CERN Gagliardi Guido INFN, Genoa Genoa U. Gagnon Louis-Guillaume LBL, Berkeley Gallas Elizabeth Oxford U. Gallop Bruce Joseph Rutherford Gan Kock Kiam Ohio State U. Ganguly Sanmay Tokyo U., ICEPP Gao Yanyan Edinburgh U. Garay Walls Francisca Chile U., Catolica SAPHIR Millennium Inst. Garcia Berenice Brookhaven Garcia Carmen Valencia U., IFIC Garcia Alonso Andrea Nikhef, Amsterdam Garcia Caffaro Arianna Gemma Yale U. Garcia Navarro Jose Enrique Valencia U., IFIC Garcia-Sciveres Maurice LBL, Berkeley Gardner Gwen Llewellyn Pennsylvania U. Gardner Robert William, Jr. Chicago U., EFI Garelli Nicoletta Tufts U. Garg Diksha Iowa U. Garg Rocky Bala SLAC Stanford U., Phys. Dept. Gargan Jack Edinburgh U. Garner Christopher Andrew Toronto U. Garvey Cameron Michael Cape Town U. Do Nascimento Gaspar Philipp Rio de Janeiro Federal U. Gassmann Veritas Katharina Tufts U. Gaudio Gabriella INFN, Pavia Gautam Viveka Barcelona, IFAE Gauzzi Paolo INFN, Rome Rome U. Gavrilenko Igor CERN Gavriliuk Alexander CERN Gay Colin Warren British Columbia U. Gaycken Goetz DESY Gazis Evangelos Natl. Tech. U., Athens Geanta Andrei Alexandru Bucharest, IFIN-HH Gee Carolyn UC, Santa Cruz Gekow Alex Ohio State U. Gemme Claudia INFN, Genoa Genest Marie-Helene LPSC, Grenoble Gentile Simonetta INFN, Rome Rome U. Gentry Andrew Donald New Mexico U. George Simon Royal Holloway, U. of London George William Frederick Birmingham U. Geralis Theodoros Democritos Nucl. Res. Ctr. Gessinger-Befurt P. CERN Geyik Marvin Emin Wuppertal U. Ghani Mohammed Warwick U. Ghneimat Mazuza Mohammad A. Siegen U. Ghorbanian Keanu Queen Mary, U. of London Ghosal Arpan Siegen U. Ghosh Aishik UC, Irvine Ghosh Anindya Arizona U. Giacobbe Benedetto INFN, Bologna Giagu Stefano INFN, Rome Rome U. Giani Tommaso Nikhef, Amsterdam Giannetti Paola INFN, Pisa Giannini Antonio Hefei, CUST Gibson Stephen Royal Holloway, U. of London Gignac Matthew UC, Santa Cruz Gil Damian Jagiellonian U. Gilbert Alexander Kevin AGH-UST, Cracow Gilbert Benjamin Jacob Nevis Labs, Columbia U. Gillberg Dag Carleton U. Gilles Geoffrey Nikhef, Amsterdam Gillwald N.E. K. DESY Ginabat Louis Paris U., VI-VII Gingrich Doug Alberta U. TRIUMF Giordani Mapo INFN, Udine Udine U. Giraud Pierre-Francois IRFU, Saclay Giugliarelli Gilberto INFN, Udine Udine U. Giugni Danilo INFN, Milan Giuli Francesco CERN Gkialas Ioannis Athens U. Aegean U., Chios Gladilin Leonid CERN Glasman Claudia Madrid, Autonoma U. Gledhill Galen Rhodes Oregon U. Glemza Gediminas DESY Glisic Marija Oregon U. Gnesi Ivan INFN, Cosenza Enrico Fermi Ctr., Rome Go Yeonju Brookhaven Colorado U. Goblirsch-Kolb Maximilian Emanuel CERN Gocke Benedikt Dortmund U. Godin Dominique Montreal U. Gokturk Berare Bogazici U. Goldfarb Steven Melbourne U. Golling Tobias Geneva U. Gololo Mpho Gift Doctor Witwatersrand U. Golubkov Dmitry CERN Gombas Jason Peter Michigan State U. Da Silva Gomes Agostinho LIP, Lisbon Lisboa U., CFNUL Gomes Da Silva G. Siegen U. Gomez Delegido Antonio Jesus Valencia U., IFIC Morais Silva Goncalo Ricardo Jose LIP, Lisbon Coimbra U. Gonella Giulia Oregon U. Gonella Laura Birmingham U. Gongadze Alexi Georgia U. Gonnella Francesco Birmingham U. Gonski Julia Lynne Nevis Labs, Columbia U. González Andana R.Y. Edinburgh U. Gonzalez De La Hoz Santiago Valencia U., IFIC Gonzalez Fernandez Sergio Barcelona, IFAE Gonzalez Lopez Ricardo Liverpool U. Gonzalez Renteria Cesar LBL, Berkeley Gonzalez Rodrigues Marcus Vinicius DESY Gonzalez Suarez Rebeca Uppsala U., Inst. Theor. Phys. Gonzalez Sevilla Sergio Geneva U. Gonzalvo Rodriguez Galo Rafael Valencia U., IFIC Goossens Luc CERN Gorini Benedetto CERN Gorini Edoardo INFN, Lecce Salento U. Gorisek Andrej Stefan Inst., Ljubljana Gosart Thomas Christopher Pennsylvania U. Goshaw A.T. Duke U. Gostkin Mikhail CERN Goswami Soumyananda Oklahoma State U. Gottardo Carlo Alberto CERN Gotz Stefanie Andrea Munich U. Gouighri Mohamed Ibn Tofail U. Goumarre Vincent DESY Goussiou Anna Washington U., Seattle Govender Nicolin Johannesburg U. Grabowska-Bold Iwona AGH-UST, Cracow Graham Kevin Robert Carleton U. Gramstad Eirik Oslo U. Grancagnolo Sergio INFN, Lecce Salento U. Grandi Mario Sussex U. Grant Charles Michael Adelaide U. IRFU, Saclay Gravila Paul West Timisoara U. Gravili Francesco Giuseppe INFN, Lecce Salento U. Gray Heather LBL, Berkeley Greco Matteo INFN, Lecce Salento U. Grefe Christian Bonn U. Gregor Ingrid DESY Grenier Philippe SLAC Grewe Simon Gabriel Munich, Max Planck Inst. Grieco Chiara Barcelona, IFAE Grillo Alex UC, Santa Cruz Grimm Kathryn Fresno State Grimm Katy Fresno State Grinstein Sebastian Barcelona, IFAE ICREA, Barcelona Grivaz Jean-Francois IJCLab, Orsay Gross Eilam Weizmann Inst. Grosse-Knetter Joern Gottingen U., II. Phys. Inst. Grud Christopher Ryan Michigan U. Grundy James Cameron Oxford U. Guan Liang Michigan U. Guan Wen Brookhaven Gubbels Chris British Columbia U. Guerrero Rojas J.G. R. Valencia U., IFIC Guerrieri Giovanni INFN, Udine Udine U. Guescini Francesco Munich, Max Planck Inst. Gugel Ralf Mainz U. Guhit Jem Aizen Mendiola Michigan U. Guida Alessandro Humboldt U., Berlin Guilloton Eva Warwick U. Rutherford Guindon Stefan CERN Guo Fangyi Beijing, Inst. High Energy Phys. UCAS, Beijing Guo Jun Shanghai Jiao Tong U. Guo Linghua DESY Guo Yuxiang Michigan U. Gupta Ruchi DESY Gupta Rajat Pittsburgh U. Gurbuz Saime Bonn U. Gurdasani Simran Sunil Freiburg U. Gustavino Giuliano CERN Guth Manuel Geneva U. Gutierrez Phillip Oklahoma U. Gutierrez Zagazeta Luis Felipe Pennsylvania U. Gutsche Manuel Dresden, Tech. U. Gutschow Christian University Coll. London Gwenlan Claire Oxford U. Gwilliam Carl Liverpool U. Haaland Even Simonsen Oslo U. Haas Andrew New York U. Habedank Martin DESY Haber Carl LBL, Berkeley Hadavand Haleh Texas U., Arlington Hadef Asma Dresden, Tech. U. Hadzic Sejla Munich, Max Planck Inst. Hagan Alina Lancaster U. Hahn Jan Joachim Siegen U. Haines Emil University Coll. London Haleem Mahsana Wurzburg U. Haley Joseph Oklahoma State U. Hall Jack Joseph Sheffield U. Hallewell Gregory Marseille, CPPM Halser Lea Bern U., LHEP Hamano Kenji Victoria U. Hamer Matthias Bonn U. Hamity Guillermo Nicolas Edinburgh U. Hampshire Emily Royal Holloway, U. of London Han Jingyi Shandong U. Han Kunlin Hefei, CUST Han Liangliang Nanjing U. Han Liang Hefei, CUST Han Shuo LBL, Berkeley Han Yi Fei Toronto U. Hanagaki Kazunori KEK, Tsukuba Hance Mike UC, Santa Cruz Hangal Dhanush Anil Nevis Labs, Columbia U. LLNL, Livermore Hanif Hamza Simon Fraser U. Hank Michael Donald Pennsylvania U. Hankache Robert Manchester U. Hansen Jorgen Beck Bohr Inst. Hansen Dines Bohr Inst. Hansen Peter Bohr Inst. Hara Kazuhiko Tsukuba U. Harada Daigo Geneva U. Harenberg Torsten Wuppertal U. Harkusha Siarhei CERN Harris Matthew Leary Massachusetts U., Amherst Harris Ynyr Oxford U. Harrison Jack Barcelona, IFAE Harrison Natalie Ohio State U. Harrison Paul Fraser Warwick U. Hartman Nicole Michelle Munich, Max Planck Inst. Hartmann Nikolai Munich U. Hasegawa Yoji Shinshu U. Hauser Reiner Michigan State U. Hawkes Chris Birmingham U. Hawkings Richard CERN Hayashi Yuichiro Tokyo U., ICEPP Hayashida Shota Nagoya U. Hayden Daniel Michigan State U. Hayes Christopher Robyn Michigan U. Hayes Robin Nikhef, Amsterdam Hays Chris Oxford U. Hays Jonathan Queen Mary, U. of London Hayward Helen Liverpool U. He Fudong Hefei, CUST He Mingxu Beijing, Inst. High Energy Phys. UCAS, Beijing He Yunjian Tokyo Inst. Tech. He Yajun DESY Heatley Nathan Barry Queen Mary, U. of London Hedberg Vincent Lund U. Heggelund Andreas Lokken Oslo U. Hehir Natasha Queen Mary, U. of London Heidegger Constantin Freiburg U. Heidegger Kim Katrin Freiburg U. Heidorn William Dale Iowa State U. Heilman Jesse Carleton U. Heim Sarah DESY Heim Timon LBL, Berkeley Heinlein James Geddy Pennsylvania U. Heinrich Jochen Jens Oregon U. Heinrich Lukas Alexander Munich, Max Planck Inst. Tech. U., Munich (main) Hejbal Jiri Prague, Inst. Phys. Helary Louis DESY Held Alexander Wisconsin U., Madison Hellesund Simen Bergen U. Helling Cole Michael British Columbia U. Hellman Sten Stockholm U. Stockholm U., OKC Henderson R.C. W. Lancaster U. Henkelmann Lars Cambridge U. Henriques Correia Ana Maria CERN Herde Hannah Elizabeth Lund U. Hernandez Jimenez Yesenia SUNY, Stony Brook Herrmann Lena Maria Bonn U. Herrmann Tim Dresden, Tech. U. Herten Gregor Freiburg U. Hertenberger Ralf Munich U. Hervas Luis CERN Hesping Moritz Mainz U. Hessey Nigel TRIUMF Hibi Hiroaki Kobe U. Hill Ewan Chin Toronto U. Hillier Stephen Birmingham U. Hinds Julia Rose Michigan State U. Hinterkeuser Florian Bonn U. Hirose Minoru Osaka U. Hirose Shigeki Tsukuba U. Hirschbuehl Dominic Wuppertal U. Hitchings Thomas Glyn Manchester U. Hitchings T.G. Manchester U. Hiti Bojan Stefan Inst., Ljubljana Hobbs John David SUNY, Stony Brook Hobincu Radu Bucharest, Polytechnic Inst. Tal Hod Noam Weizmann Inst. Hodgkinson Mark Sheffield U. Hodkinson B.H. Cambridge U. Hoecker Andreas CERN Hofer Dustyn Dean Michigan U. Hofer Judith DESY Holm Tanja Bonn U. Holzbock Michael Munich, Max Planck Inst. Hommels L.B. A.H. Cambridge U. Honan Benjamin Paul Manchester U. Hong Jiangliu Shanghai Jiao Tong U. Hong Tae Min Pittsburgh U. Hooberman Benjamin Henry Illinois U., Urbana Hopkins Walter Argonne Horii Yasuyuki Nagoya U. Hou Suen Taiwan, Inst. Phys. Howard Alissa Shirley-Ann Stefan Inst., Ljubljana Howarth James William Glasgow U. Hoya Joaquin Argonne Hrabovsky Miroslav Palacky U. Hrynevich Aliaksei DESY Hrynova Tetiana Annecy, LAPP Hsu Pai-Hsien Taiwan, Natl. Tsing Hua U. Hsu Shih-Chieh Washington U., Seattle Hu Qipeng Hefei, CUST Hu Yifan Beijing, Inst. High Energy Phys. UCAS, Beijing Huang Shuhui Hong Kong U. Huang Xiaozhong Nanjing U. Huang Xinhui Beijing, Inst. High Energy Phys. UCAS, Beijing Huang Yicong Sheffield U. Huang Yanping Beijing, Inst. High Energy Phys. Huang Zuchen Manchester U. Hubacek Zdenek Prague, Tech. U. Hubner Michael Bonn U. Huegging Fabian Bonn U. Huffman Todd Brian Oxford U. Hugli Cedrine Alexandra DESY Huhtinen Mika CERN Huiberts Simon Kristian Bergen U. Hulsken Raphael Alain McGill U. Huseynov Nazim Baku, Inst. Phys. Huston Joey Michigan State U. Huth John Harvard U., Phys. Dept. Hyneman Rachel Jordan SLAC Iacobucci Giuseppe Geneva U. Iakovidis George Brookhaven Ibragimov Iskander Siegen U. Iconomidou-Fayard Lydia IJCLab, Orsay Iengo Paolo Naples U. Iguchi Ryunosuke Tokyo U., ICEPP Iizawa Tomoya Oxford U. Ikegami Yoichi KEK, Tsukuba Ilic Nikolina Toronto U. Imam Hajar Casablanca U. Ince Lezki Merve Geneva U. Ingebretsen Carlson Tom Stockholm U. Stockholm U., OKC Introzzi Gianluca INFN, Pavia Pavia U. Iodice Mauro Rome III U. Ippolito Valerio INFN, Rome Rome U. Irwin Rebecca Katie Liverpool U. Ishino Masaya Tokyo U., ICEPP Islam Wasikul Wisconsin U., Madison Issever Cigdem Humboldt U., Berlin DESY Istin Serhat Bogazici U. Yeditepe U. Ito Hiroki Waseda U. Iturbe Ponce J.M. Hong Kong, Chinese U. Iuppa Roberto TIFPA-INFN, Trento Trento U. Ivina Anna Weizmann Inst. Izen Joseph Michael Texas U., Dallas Izzo Vincenzo Naples U. Jacka Petr Prague, Inst. Phys. Prague, Tech. U. Jackson Paul Adelaide U. Jacobs Ruth Magdalena DESY Jaeger Benjamin Paul Simon Fraser U. Jagfeld Christoph Munich U. Jain Geetika TRIUMF Jain Prasham Freiburg U. Jakobs Karl Freiburg U. Jakoubek Tomas Weizmann Inst. Jamieson Jonathan Glasgow U. Janas Krzysztof AGH-UST, Cracow Javurkova Martina Massachusetts U., Amherst Jeanneau Fabien IRFU, Saclay Jeanty Laura Oregon U. Jejelava Juansher Tbilisi, Inst. Phys. Ilia State U. Jenni Peter Freiburg U. CERN Jessiman Callan Carleton U. Jezequel Stephane Annecy, LAPP Jia Chen Shandong U. Jia Jiangyong SUNY, Stony Brook Jia Xiaohe Harvard U., Phys. Dept. Jia Xuewei Beijing, Inst. High Energy Phys. UCAS, Beijing Jia Zihang Nanjing U. Jiggins Stephen DESY Jimenez Pena Javier Barcelona, IFAE Jin Shan Nanjing U. Jinaru Adam Bucharest, IFIN-HH Jinnouchi Osamu Tokyo Inst. Tech. Johansson Per Daniel Conny Sheffield U. Johns Kenneth Arizona U. Johnson Jacob Wayne UC, Santa Cruz Jones Dominic Cambridge U. Jones Eleanor DESY Jones Paul Cambridge U. Jones R.W. L. Lancaster U. Jones T.J. Liverpool U. Joos Hans Ludwig Gottingen U., II. Phys. Inst. CERN Joshi Roshan Ohio State U. Jovicevic Jelena Belgrade U. Ju Xiangyang LBL, Berkeley Junggeburth Johannes Massachusetts U., Amherst Junkermann Thomas Kirchhoff Inst. Phys. Juste Rozas Aurelio Barcelona, IFAE ICREA, Barcelona Juzek Monika Katarzyna Cracow, INP Kabana Sonia Tarapaca U. Kaczmarska Anna Cracow, INP Kado Marumi Munich, Max Planck Inst. Kagan Harris Ohio State U. Kagan Michael SLAC Kahn Alan Mathew Nevis Labs, Columbia U. Kahn Abraham Pennsylvania U. Kahra Christian Mainz U. Kaji Toshiaki Tokyo U., ICEPP Kajomovitz Must Enrique Technion Kakati Nilotpal Weizmann Inst. Kalaitzidou Ilia Freiburg U. Kalderon Will Brookhaven Kamenshchikov Andrey Toronto U. Kang Nathan Jihoon UC, Santa Cruz Kar Deepak Witwatersrand U. Karava Kla Oxford U. Kareem Mohammad York U., Canada Karentzos Efstathios Freiburg U. Karkanias Ioannis Aristotle U., Thessaloniki Karkout Osama Nikhef, Amsterdam Karpov Sergey CERN Karpova Zoya CERN Kartvelishvili Vato Lancaster U. Karyukhin Andrey CERN Kasimi Eirini Aristotle U., Thessaloniki Katzy Judith DESY Kaur Sandeep Carleton U. Kawade Kentaro Shinshu U. Kawale Mayuri Prabhakar Oklahoma U. Kawamoto Chihiro Kyoto U. Kawamoto Tatsuo Hefei, CUST Kay Ellis CERN Kaya F.I. Tufts U. Kaya Colette Tufts U. Kazakos Stergios Michigan State U. Kazanin Vassili CERN Ke Yan SUNY, Stony Brook Keaveney James Michael Cape Town U. Keeler Richard Victoria U. Kehris Gustavs Harvard U., Phys. Dept. Keller John Stakely Carleton U. Kelly Aidan Sean University Coll. London Kempster Jacob Julian Sussex U. Kennedy Kiley Elizabeth Nevis Labs, Columbia U. Kennedy Philip Mainz U. Kepka Oldrich Prague, Inst. Phys. Kerridge Benjamin Philip Warwick U. Kersten Susanne Wuppertal U. Kersevan Borut Paul Stefan Inst., Ljubljana Keshri Sumit IJCLab, Orsay Keszeghova Lucia Comenius U. Ketabchi Haghighat S. Toronto U. Khan Raees Ahmad Pittsburgh U. Khandoga Mykola Paris U., VI-VII Khanov Alexander Oklahoma State U. Kharlamov Alexey CERN Kharlamova Tatyana CERN Khoda Elham Washington U., Seattle Kholodenko Marina CERN Khoo Teng Jian Humboldt U., Berlin Khoriauli Gia Wurzburg U. Khubua J. Tbilisi State U. Khubua Djemal Tbilisi State U. Khwaira Yahya A.R. IJCLab, Orsay Kilgallon Aaron Joseph Oregon U. Kim Dongwon Stockholm U. Stockholm U., OKC Kim Young-Kee Chicago U., EFI Kimura Naoki University Coll. London Kingston Matthew Kevin Gottingen U., II. Phys. Inst. Kirchhoff Andreas Gottingen U., II. Phys. Inst. Kirfel Christian Bonn U. Kirfel Florian Bonn U. Kirk Julie Rutherford Kiryunin Andrei Munich, Max Planck Inst. Kitsaki Chara Natl. Tech. U., Athens Kivernyk Oleh Bonn U. Klassen Martin Kirchhoff Inst. Phys. Klein Christoph Thomas Carleton U. Klein Lucas Wurzburg U. Klein Matthew Henry Michigan U. Klein Max Liverpool U. Klein Samuel Byrne Geneva U. Klein Uta Liverpool U. Klimek Pawel Jan CERN Klimentov Alexei Brookhaven Klioutchnikova Tatiana CERN Kluit Peter Nikhef, Amsterdam Kluth Stefan Munich, Max Planck Inst. Kneringer Emmerich Innsbruck U. Knight Timothy Michael Toronto U. Knue Andrea Helen Dortmund U. Kobayashi Ren Kyoto U. Kobylianskii Dmitrii Weizmann Inst. Koch Simon Florian Oxford U. Kocian Martin SLAC Kodys Peter Charles U. Koeck D.M. U. Oregon, Eugene (main) Kock Daniela Oregon U. Konig Philipp Thomas Bonn U. Kourlitis Vangelis Munich, Max Planck Inst. Tech. U., Munich (main) Kowalewski Bob Victoria U. Kroll Jiri Prague, Inst. Phys. Kroll Ira Joseph Pennsylvania U. Koultchitski Yuri CERN Lee Shih-Chang Taiwan, Inst. Phys. Lee Suhyun Stockholm U. Stockholm U., OKC Li Chihao Hefei, CUST Li Changqiao Munich, Max Planck Inst. Li Heng Hefei, CUST Li Han Shandong U. Li Huanguo Nanjing U. Li Hui Tsinghua U., Beijing Li Haifeng Shandong U. Li Shuqi Beijing, Inst. High Energy Phys. UCAS, Beijing Li Shu Tsung-Dao Lee Inst., Shanghai Shanghai Jiao Tong U. Peking U., CHEP Li Zhiying Oxford U. Li Zhelun McGill U. Li Zhiyuan Liverpool U. Li Zhan Beijing, Inst. High Energy Phys. UCAS, Beijing Liu Bo Beijing, Inst. High Energy Phys. Liu Bingxuan Simon Fraser U. Liu Jianbei Hefei, CUST Liu Jesse Cambridge U. Liu Minghui Hefei, CUST Liu Mingyi Hefei, CUST Liu Yang SYSU, Guangzhou UCAS, Beijing Liu Yanlin Shandong U. Liu Yanwen Hefei, CUST Lou Xuanhong Stockholm U. Stockholm U., OKC Lou Xinchou Beijing, Inst. High Energy Phys. UCAS, Beijing Macdonell Danika Marina Victoria U. Malecki Pawel Cracow, INP Martinez-Perez Mario Barcelona, IFAE ICREA, Barcelona Martynwood Alex Christopher University Coll. London Mcdonald Millie Melbourne U. Mc Govern Bobby Pennsylvania U. Mir Martinez Lluisa Maria Barcelona, IFAE Carvalho Luisa LIP, Lisbon Murray Bill Warwick U. Rutherford Panduro Vazquez William Royal Holloway, U. of London Mihule Kristina Charles U. Pham Joni Melbourne U. Pottgen Ruth Lund U. Potter Tina Cambridge U. Koffas Thomas Carleton U. Kolay Orcun Dresden, Tech. U. Koletsou Iro Annecy, LAPP Komarek Tomas Palacky U. Koeneke Karsten Freiburg U. Kong A.X. Y. Adelaide U. Kono Takanori Ochanomizu U. Konstantinidis Nikolaos University Coll. London Kontaxakis Pantelis Geneva U. Konya Balazs Lund U. Kopeliansky Revital Indiana U. Koperny Stefan Zenon AGH-UST, Cracow Korcyl Krzysztof Marian Cracow, INP Kordas Kostas Aristotle U., Thessaloniki N/A Koren Guy Tel Aviv U. Korn Andreas University Coll. London Korn Steffen Gottingen U., II. Phys. Inst. Korolkov Ilya Barcelona, IFAE Korotkova Natalia CERN Kortman Bryan Nikhef, Amsterdam Kortner Oliver Munich, Max Planck Inst. Kortner Sandra Munich, Max Planck Inst. Kostecka Will Northern Illinois U. Kostyukhin Vadim Siegen U. Kotsokechagia Anastasia IRFU, Saclay Kotwal Ashutosh Duke U. Koulouris Aimilianos CERN Kourkoumeli-Charalampidi Athina INFN, Pavia Pavia U. Kourkoumelis Christine Athens U. Kourlitis E. Munich, Max Planck Inst. Tech. U., Munich (main) Kovanda Ondrej Sussex U. Kowalewski R. Victoria U. Kozanecki Witold IRFU, Saclay Kozhin Anatoli CERN Kramarenko Viktor CERN Kramberger Gregor Stefan Inst., Ljubljana Kramer Peter Mainz U. Krasny Mieczyslaw Witold Paris U., VI-VII Krasznahorkay Attila CERN Kraus Johanna Wanda Wuppertal U. Kremer Jakub DESY Kresse Tom Dresden, Tech. U. Kretzschmar Jan Liverpool U. Kreul Ken Matthias Humboldt U., Berlin Krieger Peter Toronto U. Krishnamurthy Samyukta Massachusetts U., Amherst Krivos Martin Charles U. Krizka Karol Birmingham U. Kroeninger Kevin Alexander Dortmund U. Kroha Hubert Munich, Max Planck Inst. Krowpman Kyle Stuart Michigan State U. Kruchonak Uladzimir CERN Krueger Hans Bonn U. Krumnack Nils Erik Iowa State U. Kruse Mark Duke U. Kuchinskaia Olesia CERN Kuday Sinan Ankara U. Kuehn Susanne CERN Kusters Roman Freiburg U. Kuhl Thorsten DESY Kukhtin Victor CERN Kulchitsky Y. Kuleshov Serguei Andres Bello Natl. U. SAPHIR Millennium Inst. Kumar Mukesh Witwatersrand U. Kumari Neelam DESY Kumari Priyanka York U., Canada Kupco Alexander Prague, Inst. Phys. Kupfer Tobias Dortmund U. Kupich Andrey CERN Kuprash Oleg Freiburg U. Kurashige Hisaya Kobe U. Kurchaninov Leonid TRIUMF Kurdysh Oleksii IJCLab, Orsay Kurochkin Yurii CERN Kurova Anastasia CERN Kuze Masahiro Tokyo Inst. Tech. Kvam Audrey Katherine Massachusetts U., Amherst Kvita Jiri Palacky U. Kwan Tony McGill U. Kyriacou Nicholas Michigan U. Laatu Lauri Antti Olavi Marseille, CPPM Lacasta Llacer Carlos Valencia U., IFIC Lacava Francesco INFN, Rome Rome U. Lacker Heiko Markus Humboldt U., Berlin Lacour Didier Paris U., VI-VII Lad Nisha University Coll. London Ladygin Evgueni CERN Laforge Bertrand Paris U., VI-VII Lagouri Theodota Tarapaca U. Lahbabi Fatima Zahra Casablanca U. Lai Stan Gottingen U., II. Phys. Inst. Lakomiec Inga Katarzyna AGH-UST, Cracow Lalloue Nathan LPSC, Grenoble Lambert Joseph Earl Victoria U. Lammers Sabine Wedam Indiana U. Lampl Walter Arizona U. Lampoudis Christos Aristotle U., Thessaloniki N/A Lancaster Alec Northern Illinois U. Lancon Eric Brookhaven Landgraf Ulrich Freiburg U. Landon Murrough Queen Mary, U. of London Lang Valerie Freiburg U. Langenberg Robert Johannes Massachusetts U., Amherst Langrekken Oda Kristin Berg Oslo U. Lankford Andrew James UC, Irvine Lanni Francesco CERN Lantzsch Kerstin Bonn U. Lanza Agostino INFN, Pavia Lapertosa Alessandro INFN, Genoa Genoa U. Laporte Jean-Francois IRFU, Saclay Lari Tommaso INFN, Milan Lasagni Manghi Federico INFN, Bologna Lassnig Mario CERN Latonova Vera Prague, Inst. Phys. Laudrain Antoine Mainz U. Laurier Alexandre Technion Lawlor Sean Dean Sheffield U. Lawrence Zak Manchester U. Lazaridou Roxani Warwick U. Lazzaroni Massimo INFN, Milan Milan U. Le Brian Manchester U. Le Boulicaut Ennis Elise Maria Duke U. Leban Blaz Stefan Inst., Ljubljana Lebedev Alexandre Iowa State U. Leblanc Matt Manchester U. Ledroit-Guillon F. LPSC, Grenoble Lee Ava Chloe Audrey University Coll. London Lee Ting Fung Liverpool U. Leeuw Lerothodi Leonard Johannesburg U. Lefebvre Helena Royal Holloway, U. of London Lefebvre Michel Victoria U. Leggett Charles LBL, Berkeley Lehmann Miotto Giovanna CERN Leigh Matthew Geneva U. Leight William Axel Massachusetts U., Amherst Leinonen Waltteri Nijmegen U. Leisos Antonios Aristotle U., Thessaloniki Hellenic Open U., Patras Lisboa Leite Marco Sao Paulo U. Leitgeb Clara Elisabeth DESY Leitner Rupert Charles U. Leney Katharine Southern Methodist U. Lenz Tatjana Bonn U. Leone Sandra INFN, Pisa Leonidopoulos Christos Edinburgh U. Leopold Alexander Royal Inst. Tech., Stockholm Leroy Claude Montreal U. Les Robert Michigan State U. Lester Christopher Cambridge U. Levchenko Mikhail CERN Leveque Jessica Annecy, LAPP Levin Dan Michigan U. Levinson Lorne Weizmann Inst. Lewicki Maciej Piotr Cracow, INP Lewis Daniel Annecy, LAPP Li Ang APC, Paris Li Bing Shandong U. Li Jialin Shanghai Jiao Tong U. Li Ke Washington U., Seattle Li Liang Shanghai Jiao Tong U. Li Mengran Beijing, Inst. High Energy Phys. UCAS, Beijing Li Quanyin Hefei, CUST Li Tong APC, Paris Li Xingguo McGill U. Liang Shiyi Beijing, Inst. High Energy Phys. UCAS, Beijing Liang Zhijun Beijing, Inst. High Energy Phys. Liberatore Marianna IRFU, Saclay Liberti Barbara Rome U., Tor Vergata Lie Ki Hong Kong U. Sci. Tech. Lieber Marin Juan Rio de Janeiro Federal U. Lien Hsuan-Chu Indiana U. Lin Kuan-Yu Michigan State U. Lindley Rachel Elizabeth Arizona U. Lindon Jack Alberta U. Lipeles Elliot Pennsylvania U. Lipniacka Anna Bergen U. Lister Alison British Columbia U. Little Jared Annecy, LAPP Liu Danning Tsung-Dao Lee Inst., Shanghai Shanghai Jiao Tong U. Liu Kun Tsung-Dao Lee Inst., Shanghai Shanghai Jiao Tong U. Liu Peilian Beijing, Inst. High Energy Phys. Liu Qibin Tsung-Dao Lee Inst., Shanghai Washington U., Seattle Shanghai Jiao Tong U. Liu Xiaotian Hefei, CUST Llorente Merino Javier Simon Fraser U. Lloyd Steve Queen Mary, U. of London Lobodzinska Ewelina Maria DESY Loch Peter Arizona U. Lohse Thomas Humboldt U., Berlin Lohwasser Kristin Sheffield U. Loiacono Eleonora DESY Lokajicek Milos Prague, Inst. Phys. Lomas Joshua David Birmingham U. Long Jonathan Illinois U., Urbana Longarini Iacopo UC, Irvine Longo Luigi INFN, Lecce Salento U. Longo Riccardo Illinois U., Urbana Lopez Paz Ivan Barcelona, Inst. Microelectron. Lopez Solis Alvaro DESY Lorenzo Martinez Narei Annecy, LAPP Lory Alexander Munich U. Loeschcke Centeno Gianna Sussex U. Loseva Olesia CERN Lounis Abdenour IJCLab, Orsay Love Jeremy Argonne Love Peter Lancaster U. Lu Gangcheng Beijing, Inst. High Energy Phys. UCAS, Beijing Lu Miaoran Iowa U. Lu Sicong Pennsylvania U. Lu Yun-Ju Taiwan, Natl. Tsing Hua U. Lubatti Henry Washington U., Seattle Luci Claudio INFN, Rome Rome U. Lucio Alves Fabio Lucio Nanjing U. Lucotte Arnaud LPSC, Grenoble Luehring Fred Indiana U. Luise Ilaria SUNY, Stony Brook Lukianchuk Oleksii IJCLab, Orsay Lundberg Olof Royal Inst. Tech., Stockholm Lund-Jensen Bengt Royal Inst. Tech., Stockholm Luongo Nicholas Argonne Lutz Margaret Tel Aviv U. Lux Adam Brayton Boston U. Lynn David Brookhaven Lyons Harry John Liverpool U. Lysak Roman Prague, Inst. Phys. Lytken Else Lund U. Lyubushkin Vladimir CERN Lyubushkina Tatiana CERN Lyukova Mars SUNY, Stony Brook Ma Hong Brookhaven Ma Kuo Hefei, CUST Ma Lianliang Shandong U. Ma Wenhao Hefei, CUST Ma Yanhui Oklahoma State U. Mac Donell D.M. Victoria U. Maccarrone Giovanni Frascati Macdonald Jack Mainz U. Machado De Abreu Farias Paulo Cesar Rio de Janeiro Federal U. Madar Romain Clermont-Ferrand U. Mader Wolfgang Franz Dresden, Tech. U. Madula Thandikire University Coll. London Maeda Junpei Kobe U. Maeno Tadashi Brookhaven Maguire Helen Ruth Sheffield U. Maiboroda Vera IRFU, Saclay Maio Amelia LIP, Lisbon Lisboa U., CFNUL Lisbon U., CFNUL Maj Klaudia AGH-UST, Cracow Majersky Oliver DESY Majewski Stephanie Oregon U. Makovec Nikola IJCLab, Orsay Maksimovic Veljko Belgrade U. Malaescu Bogdan Paris U., VI-VII Malecki Pa. Cracow, INP Maleev Victor CERN Malek Fairouz LPSC, Grenoble Mali Miha Stefan Inst., Ljubljana Malito Davide Royal Holloway, U. of London Mallik Usha Iowa U. Maltezos Stavros Natl. Tech. U., Athens Malyukov Sergey CERN Mamuzic Judita Barcelona, IFAE Mancini Giada Frascati Manco Giulia INFN, Pavia Pavia U. Mandalia Jesal Queen Mary, U. of London Mandic Igor Stefan Inst., Ljubljana Manhaes De Andrade Filho Luciano Juiz de Fora U. Maniatis Ioannis Michail Weizmann Inst. Manjarres Ramos J. Marseille, CPPM L2IT, Toulouse Mankad Dvij Weizmann Inst. Mann Alexander Munich U. Mansoulie Bruno IRFU, Saclay Manzoni Stefano CERN Mao Lining Shanghai Jiao Tong U. Mapekula Xola Gugulethu Johannesburg U. Marantis Alexandros Aristotle U., Thessaloniki Hellenic Open U., Patras Marchiori Giovanni APC, Paris Marcisovsky Michal Prague, Inst. Phys. Marcon Caterina INFN, Milan Marinescu Mihaela Birmingham U. Marium Sadia DESY Marjanovic Marija Oklahoma U. Marshall Emma Lancaster U. Marshall Zach LBL, Berkeley Marti I Garcia Salvador Valencia U., IFIC Martin T.A. Warwick U. Martin Victoria Edinburgh U. Martin Dit Latour Bertrand Bergen U. Martinelli Luca INFN, Rome Rome U. Martinez Agullo Pablo Valencia U., IFIC Martinez Outschoorn Verena Ingrid Massachusetts U., Amherst Martinez Suarez Paula Barcelona, IFAE Martin-Haugh Stewart Rutherford Martoiu Sorin Bucharest, IFIN-HH Martyniuk Alex Christopher University Coll. London Marzin Antoine CERN Mascione Daniela TIFPA-INFN, Trento Trento U. Masetti Lucia Mainz U. Mashimo Tetsuro Tokyo U., ICEPP Masik Jiri Manchester U. Maslennikov Alexei CERN Massa Lorenzo INFN, Bologna Massarotti Paolo Naples U. Mastrandrea Paolo INFN, Pisa Pisa U. Mastroberardino Anna INFN, Cosenza Calabria U. Masubuchi Tatsuya Tokyo U., ICEPP Mathisen Thomas Uppsala U., Inst. Theor. Phys. Matousek Jan Charles U. Matsuzawa Nobuo Tokyo U., ICEPP Maurer Julien Bucharest, IFIN-HH Macek Bostjan Stefan Inst., Ljubljana Maximov Dmitriy CERN Mazini Rachid Taiwan, Inst. Phys. Maznas Ioannis Aristotle U., Thessaloniki Mazza Maria Michigan State U. Mazza Simone Michele UC, Santa Cruz Mazzeo Elena INFN, Milan Milan U. Mc Ginn Christopher Brookhaven Mc Gowan John Patrick McGill U. Mc Kee Shawn Michigan U. McDonald E.F. Melbourne U. Mcdougall Ashley Ellen Nikhef, Amsterdam Mcfayden Josh Sussex U. Mchedlidze Gvantsa Tbilisi State U. Mckenzie Ryan Peter Witwatersrand U. Mclachlan Thomas Christopher DESY Mclaughlin Donal Joseph University Coll. London Mcmahon Steve Rutherford Mcpartland Conor Liverpool U. McPherson R.A. Victoria U. IPP, Canada Mehlhase Sascha Munich U. Mehta Andrew Liverpool U. Melini Davide Technion Mellado Garcia Bruce Witwatersrand U. Melo Andres Hugo Gottingen U., II. Phys. Inst. Meloni Federico DESY Mendes Jacques Da Costa Antonio Manuel Manchester U. Meng Huan Yu Toronto U. Meng Lingxin Lancaster U. Menke Sven Munich, Max Planck Inst. Mentink Matthias CERN Meoni Evelin INFN, Cosenza Calabria U. Mercado Gretel Northern Illinois U. Merlassino Claudia INFN, Udine Udine U. Merola Leonardo Naples U. Meroni Chiara INFN, Milan Milan U. Merz Garrett William Michigan U. Metcalfe Jessica Argonne Mete Alaettin Serhan Argonne Meyer Chris Indiana U. Meyer Jean-Pierre IRFU, Saclay Middleton Robin Rutherford Mijovic Liza Edinburgh U. Mikenberg George Weizmann Inst. Mikestikova Marcela Prague, Inst. Phys. Mikuz Marko Stefan Inst., Ljubljana Mildner Hannes Mainz U. Milic Adriana CERN Milke Chris Southern Methodist U. Miller David Chicago U., EFI Miller Laura Stephanie Carleton U. Milov Alexander Weizmann Inst. Milstead David Anthony Stockholm U. Stockholm U., OKC Min Tianjue Nanjing U. Minaenko Andrei CERN Minashvili Irakli Tbilisi State U. Mince Laurynas Glasgow U. Mincer Allen Irving New York U. Mindur Bartosz AGH-UST, Cracow Mineev Mikhail CERN Mino Yuya Kyoto U. Miralles Lopez Marcos Valencia U., IFIC Mironova Maria LBL, Berkeley Mishima Akihiro Tokyo U., ICEPP Missio Marion Nijmegen U. Mitra Ankush Warwick U. Mitsou Vasiliki Valencia U., IFIC Mitsumori Yuki Nagoya U. Miu Ovidiu Toronto U. Miyagawa Paul Queen Mary, U. of London Mkrtchyan Tigran Kirchhoff Inst. Phys. Mlinarevic Marin University Coll. London Mlinarevic Toni University Coll. London Mlynarikova Michaela CERN Mobius Silke Bern U., LHEP Moder Paul DESY Mogg Philipp Munich U. Mohamed Farook Mohamed Hijas New Mexico U. Fadol Mohammed Abdualazem Beijing, Inst. High Energy Phys. UCAS, Beijing Mohapatra Soumya Nevis Labs, Columbia U. Mokgatitswane Gaogalalwe Witwatersrand U. Moleri Luca Weizmann Inst. Mondal Buddhadeb Siegen U. Mondal Santu Prague, Tech. U. Monig Klaus DESY Monnier Emmanuel Marseille, CPPM Monsonis Romero Luis Valencia U., IFIC Montejo Berlingen Javier Barcelona, IFAE Montella Marco Ohio State U. Montereali Federico Rome III U. Monticelli Fernando La Plata U. Monzani Simone INFN, Udine Udine U. Morange Nicolas IJCLab, Orsay Moreno Llacer Maria Valencia U., IFIC Moreno Martinez Carlos Geneva U. Morettini Paolo INFN, Genoa Morgenstern Stefanie CERN Morii Masahiro Harvard U., Phys. Dept. Morinaga Masahiro Tokyo U., ICEPP Morley Anthony CERN Morodei Federico INFN, Rome Rome U. Morvaj Ljiljana CERN Moschovakos Paris CERN Moser Brian CERN Mosidze Maia Tbilisi State U. Moskalets Tetiana Freiburg U. Moskvitina Polina Nijmegen U. Moss Joshua Fresno State Cal State, Sacramento Moyse E.J. W. Massachusetts U., Amherst Mtintsilana Onesimo Witwatersrand U. Muanza Steve Marseille, CPPM Mueller James Alfred Pittsburgh U. Muenstermann Daniel Lancaster U. Müller R. Bern U., LHEP Mullier Geoffrey Uppsala U., Inst. Theor. Phys. Mullin Anna Jane Cambridge U. Mullin Joseph Pennsylvania U. Mungo Davide Toronto U. Munoz Perez David Valencia U., IFIC Munoz Sanchez Francisca Manchester U. Murin Martin Manchester U. Poveda Torres Ximo Valencia U., IFIC Proudfoot James Argonne Proudfoot Jimmy Argonne Qin Quake Manchester U. Rapheeha Phuti Witwatersrand U. Robles Manzano Marisol Mainz U. Robles Manzano Maria Mainz U. Romero Anabel Illinois U., Urbana Rossi Eleonora Oxford U. Rossi Elvira Naples U. Ruan Ruanxf Witwatersrand U. Schaffer R.D. IJCLab, Orsay Southern Methodist U. Chtcheguelski Valery CERN Schune Philippe IRFU, Saclay Schwemling Philippe IRFU, Saclay Sharma Abhishek CERN Sharma Abhishek British Columbia U. Shatalov Sppavel CERN Kirianova Anna CERN Shojaii Seyed Ruhollah Melbourne U. Sijacki Dorde Belgrade U. Cardoso Silva Julia Manuela Birmingham U. Sinha Supriya DESY Sinha Sukanya Manchester U. Solodkov Sanya CERN Starchenko Jenya CERN Sultanov Salekh TOBB ETU, Ankara Sun Siyuan Michigan U. Sun Shaojun Wisconsin U., Madison Tikhonov Iouri CERN Toldaiev Alex Indiana U. None None U. Copenhagen Tuts Mike Nevis Labs, Columbia U. Van De Wall Evan Richard Oklahoma State U. Mete Tulin Taiwan, Inst. Phys. Vetterli Michel Joseph Simon Fraser U. TRIUMF Volkotrub Yuriy AGH-UST, Cracow Wang Chen Mainz U. Wang Chenliang Shanghai Jiao Tong U. Wang Renjie Mainz U. Wang Rongkun Harvard U., Phys. Dept. Wang Rui Argonne Wang Song-Ming Taiwan, Inst. Phys. Wang Shuanggeng Shandong U. Wang Weitao Iowa U. Wang Wei Beijing, Inst. High Energy Phys. Wang Xin Nanjing U. Wang Xiaoning Illinois U., Urbana Wang Xi Shanghai Jiao Tong U. Wang Yufeng Tsung-Dao Lee Inst., Shanghai Wang Yuhao Nanjing U. Wang Zirui Michigan U. Wang Zhen Tsung-Dao Lee Inst., Shanghai Duke U. Shanghai Jiao Tong U. Wang Zhichen Michigan U. White Aaron Stephen Harvard U., Phys. Dept. White Andrew Texas U., Arlington Wu Minlin Hong Kong, Chinese U. Wu Mengqing Nijmegen U. Wurzinger Jonas Munich, Max Planck Inst. Tech. U., Munich (main) Murrone Alessia INFN, Milan Milan U. Muskinja Miha LBL, Berkeley Mwewa Chilufya Brookhaven Myagkov Alexei CERN Myers Andrew Joel Texas U., Arlington Myers Greg Indiana U. Myska Miroslav Prague, Tech. U. Nachman B.P. LBL, Berkeley Nackenhorst Olaf Dortmund U. Nag Abhishek Dresden, Tech. U. Nagai Koichi Oxford U. Nagano Kunihiro KEK, Tsukuba Nagle James Lawrence Brookhaven Colorado U. 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Ng Ying Wun Yvonne DESY Ngair Badr-Eddine Mohammed V U., Agdal Nguyen Hoang Dai Nghia Montreal U. Nickerson Richard Oxford U. Nikolaidou Rosy IRFU, Saclay Nielsen Jason UC, Santa Cruz Niemeyer Marcel Gottingen U., II. Phys. Inst. Niermann Joana Gottingen U., II. Phys. Inst. CERN Nikiforou Nikiforos CERN Nikolaenko Vladimir CERN Nikolic-Audit I. Paris U., VI-VII Nikolopoulos Konstantinos Birmingham U. Nilsson Paul Brookhaven Ninca Ilona-Stefana DESY Nindhito Herjuno Rah Geneva U. Ninio Gadi Tel Aviv U. Nisati Aleandro INFN, Rome Nishu Nishu Alberta U. Nisius Richard Munich, Max Planck Inst. Nitschke Jan-Eric Dresden, Tech. U. Nkadimeng Edward Khomotso Witwatersrand U. Nobe Takuya Tokyo U., ICEPP Noel Daniel Louis Cambridge U. Nommensen Thomas Sydney U. Norfolk Mitch Sheffield U. Bin Norisam Raif Rafideen University Coll. London Norman Bryce John Carleton U. Noury Meryem Casablanca U. Novak Jakob Stefan Inst., Ljubljana Novak Tadej DESY Novotny Lukas Prague, Tech. U. 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Orlando Nicola Barcelona, IFAE Orr Robert Toronto U. O'Shea Val Glasgow U. Osojnak Lauren Melissa Pennsylvania U. Ospanov Rustem Hefei, CUST Otero Y Garzon Gustavo Buenos Aires U. Otono Hidetoshi Kyushu U. Ott Philipp Sebastian Kirchhoff Inst. Phys. Ottino Gregory James LBL, Berkeley Ouchrif Mohamed Oujda U. Ouellette Jeff Brookhaven Ould-Saada Farid Oslo U. Owen Mark Andrew Glasgow U. Owen Rhys Edward Rutherford Oyulmaz Kaan Yuksel Bogazici U. Ozcan Erkcan Bogazici U. Ozturk Ferhat Cracow, INP Ozturk Nurcan Texas U., Arlington Ozturk Sertac Istinye U., Istanbul Pacey Holly Oxford U. Pacheco Pages Andreu Barcelona, IFAE Padilla Aranda Cristobal Barcelona, IFAE Padovano Giovanni INFN, Rome Rome U. Pagan Griso Simone LBL, Berkeley Palacino Caviedes Gabriel David Indiana U. Palazzo Alessandra INFN, Lecce Salento U. Palestini Sandro CERN Pan Jingjing Yale U. Pan Tong Hong Kong, Chinese U. Panchal D.K. Texas U. Pandini Carlo Nikhef, Amsterdam Panduro Vazquez J.G. Royal Holloway, U. of London Pandya Hitarthi Deepak Adelaide U. Pang Hao Tsinghua U., Beijing Pani Priscilla DESY Panizzo Giancarlo INFN, Udine Udine U. Paolozzi Lorenzo Geneva U. Papadatos Constantine Montreal U. Parajuli Santosh Southern Methodist U. Paramonov Alexander Argonne Paraskevopoulos Christos Natl. Tech. U., Athens Paredes Hernandez Daniela Katherinne Hong Kong U. Park Ki Ryeong Nevis Labs, Columbia U. Park Tae Hyoun Toronto U. Parker Andy Cambridge U. Parodi Fabrizio INFN, Genoa Genoa U. Parrish Elliot Northern Illinois U. Parrish Victoria Alexis Edinburgh U. Parsons John Nevis Labs, Columbia U. Parzefall Ulrich Freiburg U. Pascual Dias B. Montreal U. Pascual Dominguez Luis Tel Aviv U. Pasqualucci Enrico INFN, Rome Passaggio Stefano INFN, Genoa Pastore Francesca Royal Holloway, U. of London Pasuwan Patrawan Stockholm U. Stockholm U., OKC Patel Pragati Cracow, INP Patel Utsav Mukesh Duke U. Pater J.R. Manchester U. Pauly Thilo CERN Pearkes Jannicke Andree SLAC Pedersen Maiken Oslo U. Pedro Rute LIP, Lisbon Peleganchuk Sergey CERN Penc Ondrej CERN Pender Emily Alexandra Edinburgh U. Penski Katrin Elisabeth Munich U. Penzin Maksim CERN Sotto-Maior Peralva Bernardo Rio de Janeiro State U. Pereira Peixoto A.P. LPSC, Grenoble Pereira Sanchez Laura Stockholm U. Stockholm U., OKC Perepelitsa Dennis Brookhaven Colorado U. Perez Codina Estel TRIUMF Perganti Maria Natl. Tech. U., Athens Perini Laura INFN, Milan Milan U. Pernegger Heinz CERN Perrin Oceane Clermont-Ferrand U. Peters Krisztian DESY Peters Reinhild Manchester U. Petersen Brian CERN Petersen Troels Bohr Inst. Petit Elisabeth Marseille, CPPM Petousis Vlasios Prague, Tech. U. Petridou Chariclia Aristotle U., Thessaloniki N/A Petrukhin Alexey Siegen U. Pettee Mariel LBL, Berkeley Pettersson Nora Emilia CERN Petukhov Aleksandr CERN Petukhova K. Charles U. Pezoa Rivera Raquel Santa Maria U., Valparaiso Pezzotti Lorenzo CERN Pezzullo Gianantonio Yale U. Pham Minh Tuan Wisconsin U., Madison Phillips Peter Rutherford Piacquadio Giacinto SUNY, Stony Brook Pianori Elisabetta LBL, Berkeley Piazza Federica Oregon U. Piegaia Ricardo Buenos Aires U. Pietreanu Dorel Bucharest, IFIN-HH Pilkington Andrew Manchester U. Pinamonti Michele INFN, Udine Udine U. Pinfold James Alberta U. Pinheiro Pereira B.C. LIP, Lisbon Pinto Pinoargote Andres Eloy Mainz U. IRFU, Saclay Pintucci Laura INFN, Udine Udine U. Piper Katie Sussex U. Pirttikoski Antti Geneva U. Pizzi Dylan Carleton U. Pizzimento Luca Hong Kong U. Pizzini Alessio Nikhef, Amsterdam Pleier Marc-Andre Brookhaven Plesanovs Vladislavs Freiburg U. Pleskot Vojtech Charles U. Plotnikova Elena CERN Poddar Gitanjali Annecy, LAPP Poettgen R. Lund U. Poggioli Luc Paris U., VI-VII Pokharel Ishan Gottingen U., II. Phys. Inst. Polacek Stanislav Charles U. Polesello Giacomo INFN, Pavia Poley Anne-Luise Simon Fraser U. TRIUMF Polifka Richard Prague, Tech. U. Polini Alessandro INFN, Bologna Pollard Chris Warwick U. Pollock Zachary Ohio State U. Polychronakos Venetios Brookhaven Pompa Pacchi Elena INFN, Rome Rome U. Ponomarenko Daniil Nijmegen U. Pontecorvo Ludovico CERN Popa Stefan Transilvania U., Brasov Popeneciu Gabriel INCDTIM, Cluj Napoca Poreba Aleksandra CERN Portillo Quintero Dilia Maria TRIUMF Pospisil Stanislav Prague, Tech. U. Postill Michael Antony Sheffield U. Postolache Petronel Cuza U., Iasi Potamianos Karolos Warwick U. Potepa Patrycja Anna AGH-UST, Cracow Potrap Igor CERN Potti Harish Adelaide U. Poulsen Trine DESY Poveda J. Valencia U., IFIC Pozo Astigarraga Eukeni CERN Prades Ibanez Alberto Valencia U., IFIC Pretel Jose Freiburg U. Price Darren Manchester U. Primavera Margherita INFN, Lecce Principe Martin Miguel Angel Madrid, Autonoma U. Privara Radek Palacky U. Procter Tomasz Glasgow U. Proffitt Mason Washington U., Seattle Proklova Nadezhda Pennsylvania U. Prokofiev Kirill Hong Kong U. Sci. Tech. Proto Giorgia Munich, Max Planck Inst. Protopopescu Serban Brookhaven Przybycien Mariusz AGH-UST, Cracow Przygoda Witold Wojciech Jagiellonian U. Puddefoot Joshua Eldon Sheffield U. Pudzha Dennis CERN Pyatiizbyantseva Diana CERN Qian Jianming Michigan U. Dong Qichen Manchester U. Qin Y. Manchester U. Qiu Tong Edinburgh U. Quadt Arnulf Gottingen U., II. Phys. Inst. Queitsch-Maitland Michaela Manchester U. Quetant Guillaume Geneva U. Quinn Ryan British Columbia U. Rabanal Bolanos Gabriel Harvard U., Phys. Dept. Rafanoharana Dimbiniaina Freiburg U. Ragusa Francesco INFN, Milan Milan U. Rainbolt Lacey Chicago U., EFI Raine Johnny Geneva U. Rajagopalan Srini Brookhaven Ramakoti Ekaterina CERN Ramirez-Berend Ian Alejandro Carleton U. Ran Kunlin DESY UCAS, Beijing Rasheed Hammad Bucharest, IFIN-HH Raskina Valentina Paris U., VI-VII Rassloff Damir Fabrice Kirchhoff Inst. Phys. Rave Stefan Mainz U. Ravina Baptiste Gottingen U., II. Phys. Inst. Ravinovich Ilia Weizmann Inst. Raymond Michel CERN Read Alexander Lincoln Oslo U. Readioff Nathan Peter Sheffield U. Rebuzzi Daniela INFN, Pavia Pavia U. Redlinger George Brookhaven Reed Alice Munich, Max Planck Inst. Reeves Kendall Brandeis U. Reidelsturz Joshua Aaron Wuppertal U. Reikher David Tel Aviv U. Rej Amartya Dortmund U. Rembser Christoph CERN Renardi Alessia DESY Renda Michele Bucharest, IFIN-HH Rendel Marian Benedikt Munich, Max Planck Inst. Renner Frederic DESY Rennie Adam UC, Irvine Rescia Alberto DESY Resconi Silvia INFN, Milan Ressegotti Martina INFN, Genoa Genoa U. Rettie Sebastien CERN Reyes Rivera Jose Gabriel Michigan State U. Reynolds Elliot LBL, Berkeley Rezanova Olga CERN Reznicek Pavel Charles U. Ribaric Neza Lancaster U. Ricci Ester TIFPA-INFN, Trento Trento U. Richter Robert Munich, Max Planck Inst. Richter Stefan Stockholm U. Stockholm U., OKC Richter-Was Elzbieta Jagiellonian U. Ridel Melissa Paris U., VI-VII Ridouani Selaiman Oujda U. Rieck Patrick New York U. Riedler Petra CERN Riefel Ellen Maria Stockholm U. Stockholm U., OKC Rieger Oliver Nikhef, Amsterdam Rijssenbeek Michael SUNY, Stony Brook Rimoldi Adele INFN, Pavia Pavia U. Rimoldi Marco CERN Rinaldi Lorenzo INFN, Bologna Bologna U. Rinn Timothy Thomas Brookhaven Rinnagel Maximilian Paul Munich U. Ripellino Giulia Uppsala U., Inst. Theor. Phys. Riu Imma Barcelona, IFAE Rivadeneira Bracho Pablo Andres DESY Rivera Vergara Juan Cristobal Victoria U. Rizatdinova Flera Oklahoma State U. Rizvi Eram Syed Queen Mary, U. of London Roberts Bryn Arthur Warwick U. Roberts Ryan LBL, Berkeley Robertson Steven McGill U. IPP, Canada Robinson Dave Cambridge U. Robles Gajardo Carolina Michel Santa Maria U., Valparaiso Robson Aidan Glasgow U. Rocchi Alessandro Rome U., Tor Vergata Roda Chiara INFN, Pisa Pisa U. Rodriguez Bosca Sergi Kirchhoff Inst. Phys. Rodriguez Garcia Yohany Antonio Narino U. Rodriguez Rodriguez Arturo Freiburg U. Rodriguez Vera Ana Maria York U., Canada Roe Shaun CERN Roemer Jonas Till UC, Irvine Roepe-Gier Amber UC, Santa Cruz Roggel Jens Wuppertal U. Rohne Ole Oslo U. Rojas Caballero Rimsky Alejandro Massachusetts U., Amherst Roland Christophe Paris U., VI-VII Roloff Jennifer Brookhaven Romaniouk Anatoli CERN Romano Emanuele INFN, Pavia Pavia U. Romano Marino INFN, Bologna Rompotis Nikolaos Liverpool U. Roos Lydia Paris U., VI-VII Rosati Stefano INFN, Rome Rosser Benjamin John Chicago U., EFI Rossi Leonardo INFN, Genoa Rossini Lorenzo Freiburg U. Rosten Rachel Christine Ohio State U. Rotaru Marina Bucharest, IFIN-HH Rottler Benjamin Freiburg U. Rougier Charline Marseille, CPPM L2IT, Toulouse Rousseau David IJCLab, Orsay Rousso David Cambridge U. Roy Avik Illinois U., Urbana Roy-Garand Sebastien Toronto U. Rozanov Alexandre Marseille, CPPM Rozario Z.M. A. Glasgow U. Rozen Yoram Technion Ruan X. U. Witwatersrand, Johannesburg, Sch. Phys. Rubio Jimenez Adrian Valencia U., IFIC Ruby Adam James Liverpool U. Ruelas Rivera Victor Hugo Humboldt U., Berlin Ruggeri Tristan Andrew Adelaide U. Ruggiero Alessandro Oxford U. Ruiz Martinez Arantxa Valencia U., IFIC Rummler Andre CERN Rurikova Zuzana Freiburg U. Rusakovich Nikolai CERN Russell Heather Victoria U. Russo Graziella INFN, Rome Rome U. Rutherfoord John P. Arizona U. Rutherford Colmenares Sebastian Cambridge U. Rybacki Katherine Amy Lancaster U. Rybar Martin Charles U. Rye Eli Baverfjord Oslo U. Ryzhov Andrey Southern Methodist U. Sabater Iglesias Jorge Andres Geneva U. Sabatini Paolo Valencia U., IFIC Sadrozinski Hartmut UC, Santa Cruz Safai Tehrani Francesco INFN, Rome Safarzadeh Samani Batool Rutherford Safdari Murtaza SLAC Saha Shreya Victoria U. Sahinsoy Merve Munich, Max Planck Inst. Saibel Andrej Valencia U., IFIC Saimpert Matthias IRFU, Saclay Saito Masahiko Tokyo U., ICEPP Saito Tomoyuki Tokyo U., ICEPP Salamani Dalila CERN Salnikov Andy SLAC Salt Jose Valencia U., IFIC Salvador Salas Adrian Tel Aviv U. Salvatore Daniela INFN, Cosenza Calabria U. Salvatore Fabrizio Sussex U. Salzburger Andreas CERN Sammel Dirk Freiburg U. Sampsonidis Dimos Aristotle U., Thessaloniki N/A Sampsonidou Despoina Oregon U. Sanchez Martinez Francisco Javier Valencia U., IFIC Sanchez Pineda Arturos Annecy, LAPP Sanchez Sebastian Victoria Valencia U., IFIC Sandaker Heidi Oslo U. Sander Christian DESY Sandesara Jay Ajitbhai Massachusetts U., Amherst Sandhoff Marisa Wuppertal U. Sandoval Usme Carlos Colombia, U. Natl. Sankey D.P. C. Rutherford Sano Takane Kyoto U. Sansoni Andrea Frascati Santi Lorenzo INFN, Rome Rome U. Santoni Claudio Clermont-Ferrand U. Santos Helena LIP, Lisbon Lisboa U., CFNUL Santpur Sai Neha LBL, Berkeley Santra Arka Weizmann Inst. Saoucha Kamal U. Sharjah Mendes Saraiva Joao Gentil LIP, Lisbon Lisbon U., CFNUL Sardain Jad Mathieu Arizona U. Sasaki Osamu KEK, Tsukuba Sato Koji Tsukuba U. Sauer Christof Heidelberg U. Sauerburger Frank Freiburg U. Sauvan Emmanuel Annecy, LAPP Savard Pierre Toronto U. TRIUMF Sawada Ryu Tokyo U., ICEPP Sawyer Craig Rutherford Sawyer Lee Louisiana Tech. U. Sayago Galvan Ivan Valencia U., IFIC Sbarra Carla INFN, Bologna Sbrizzi Antonio INFN, Bologna Bologna U. Scanlon Timothy Paul University Coll. London Schaarschmidt Jana Washington U., Seattle Schacht Peter Munich, Max Planck Inst. Schaefer Uli Mainz U. Schaile Dorothee Munich U. Schamberger Robert Dean, Jr. SUNY, Stony Brook Scharf Christian Humboldt U., Berlin Schefer Meinrad Moritz Bern U., LHEP Schegelsky V.A. Scheirich Daniel Charles U. Schenck Ferdinand Humboldt U., Berlin Schernau Michael UC, Irvine Scheulen Chris Gottingen U., II. Phys. Inst. Schiavi Carlo INFN, Genoa Genoa U. Schioppa Enrico, Junior. INFN, Lecce Salento U. Schioppa Marco INFN, Cosenza Calabria U. Schlag Bastian SLAC Stanford U., Phys. Dept. Schleicher Katharina Freiburg U. Schlenker Stefan CERN Schmeing Jonas Wuppertal U. Schmidt Mustafa Andre Wuppertal U. Schmieden Kristof Mainz U. Schmitt Christian Mainz U. Schmitt Niklas Mainz U. Schmitt Stefan DESY Schoeffel Laurent Olivier IRFU, Saclay Schoening Andre Heidelberg U. Scholer Patrick Freiburg U. Schopf Elisabeth Oxford U. Schott Matthias Mainz U. Schovancova Jaroslava CERN Schramm Steven Geneva U. Schroeder Frederic Wuppertal U. Schroer Tomke Geneva U. Schultz-Coulon Hans-Christian Kirchhoff Inst. Phys. Schumacher Markus Freiburg U. Schumm Bruce Andrew UC, Santa Cruz Schune Ph. IRFU, Saclay Schuy Alexander Joseph Washington U., Seattle Schwartz Hava Rhian UC, Santa Cruz Schwartzman Ariel Gustavo SLAC Schwarz Thomas Andrew Michigan U. Schwemling Ph. IRFU, Saclay Schwienhorst Reinhard Michigan State U. Sciandra Andrea UC, Santa Cruz Sciolla Gabriella Brandeis U. 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Shaw Savanna Manchester U. Shcherbakova A. Shen Qiuping Shanghai Jiao Tong U. APC, Paris Sheppard Damian Joseph Simon Fraser U. Sherwood Peter University Coll. London Shi Liaoshan University Coll. London Shi Xin Beijing, Inst. High Energy Phys. Shimmin Chase Owen Yale U. Shinner James David Royal Holloway, U. of London Shipsey I.P. J. Oxford U. Shirabe Shohei Geneva U. Shiyakova Mariya CERN Sofiya, Inst. Nucl. Res. Shlomi Jonathan Weizmann Inst. Shochet M.J. Chicago U., EFI Shojaii Jafar Melbourne U. Shope David Richard Oslo U. Shrestha Bijay Oklahoma U. Shrestha Suyog Ohio State U. Washington Coll. Shrif Esra Mohammed Witwatersrand U. Shroff Maheyer Jamshed Victoria U. Sicho Petr Prague, Inst. Phys. Sickles Anne Marie Illinois U., Urbana Sideras Haddad Elias Witwatersrand U. Sidoti Antonio INFN, Bologna Siegert Frank Dresden, Tech. U. Sijacki Dj. Belgrade, Inst. Phys. Sili Francisco La Plata U. Silva Oliveira Marcos Vinicius Brookhaven Silverstein Samuel Stockholm U. Simion Stefan IJCLab, Orsay Simoniello Rosa CERN Simpson Ethan Lewis Glasgow U. Simpson Harry Sussex U. Simpson Liana Michigan U. Simpson Nathan Daniel Lund U. Simsek Sinem Istinye U., Istanbul Sindhu Sreelakshmi Gottingen U., II. Phys. Inst. Sinervo Pekka Toronto U. Singh Sahibjeet Toronto U. Sioli Maximiliano INFN, Bologna Bologna U. Siral Ismet CERN Sitnikova Elizaveta DESY Sivoklokov Serguei CERN Sjoelin Joergen Stockholm U. Stockholm U., OKC Skaf Ali Gottingen U., II. Phys. Inst. Skorda Eleni Birmingham U. Skubic Patrick Oklahoma U. Slawinska Magdalena Cracow, INP Smakhtin Vladimir Weizmann Inst. Smart Ben Harry Rutherford Smiesko Juraj CERN Smirnov Serge CERN Smirnov Yury CERN Smirnova Lidia CERN Smirnova Oxana Lund U. Smith Andrew Caldon Nevis Labs, Columbia U. Smith Emily Ann Chicago U., EFI Smith Hayden Alexander Oxford U. Smith James Liverpool U. Smith Rachel Emma Clarke SLAC Smizanska Maria Lancaster U. Smolek Karel Prague, Tech. U. 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Sperlich Dennis Freiburg U. Spigo Giancarlo CERN Spinali Sebastiano Lancaster U. Spiteri Dwayne Patrick Glasgow U. Spousta Martin Charles U. Staats Ezekiel Carleton U. Stabile Alberto INFN, Milan Milan U. Stamen Rainer Kirchhoff Inst. Phys. Stampekis Alexios Birmingham U. Standke Mark Bonn U. Stanecka Ewa Cracow, INP Stange Max Vincent Dresden, Tech. U. Stanislaus Beojan LBL, Berkeley Stanitzki Marcel DESY Stapf Birgit Sylvia DESY Starchenko E.A. Stark Giordon Holtsberg UC, Santa Cruz Stark Jan Marseille, CPPM L2IT, Toulouse Starko Darij Markian York U., Canada Staroba Pavel Prague, Inst. Phys. Starovoitov Pavel Kirchhoff Inst. Phys. Staerz Steffen McGill U. Staszewski Rafal Cracow, INP Stavropoulos George Democritos Nucl. Res. Ctr. Steentoft Jonas Uppsala U., Inst. Theor. Phys. Steinberg Peter Alan Brookhaven Stelzer Bernd Simon Fraser U. TRIUMF Stelzer Joerg Pittsburgh U. Stelzer-Chilton Oliver TRIUMF Stenzel Hasko Giessen U. Stevenson Thomas James Sussex U. Stewart Graeme A. CERN Stewart Joshua Ryan Oklahoma State U. Stockton Mark CERN Stoicea Gabriel Bucharest, IFIN-HH Stolarski Marcin LIP, Lisbon Stonjek Stefan Munich, Max Planck Inst. Straessner Arno Dresden, Tech. U. Strandberg Jonas Royal Inst. Tech., Stockholm Strandberg Sara Stockholm U. Stockholm U., OKC Stratmann Maren Wuppertal U. Strauss Mike Oklahoma U. Strebler Thomas Marseille, CPPM Strizenec Pavol Kosice, IEF Strohmer Raimund Wurzburg U. Strom David Oregon U. Stroynowski Ryszard Southern Methodist U. Strubig Antonia Stockholm U. Stockholm U., OKC Stucci Stefania Antonia Brookhaven Stugu Bjarne Bergen U. Stupak John Oklahoma U. Styles Nicholas DESY Su Dong SLAC Su Shixiang Hefei, CUST Su Wanyun Tsung-Dao Lee Inst., Shanghai Su Xiaowen Hefei, CUST IJCLab, Orsay Sugizaki Kaito Tokyo U., ICEPP Sulin Vladimir CERN Sullivan Matthew James Liverpool U. Sultan D.M. S. TIFPA-INFN, Trento Trento U. Sultanaliyeva Laily CERN Sultansoy S. TOBB ETU, Ankara Sumida Toshi Kyoto U. Sunneborn Gudnadottir O. Uppsala U., Inst. Theor. Phys. Sur Nairit Marseille, CPPM Sutton Mark Sussex U. Suzuki Hisanori Tsukuba U. Svatos Michal Prague, Inst. Phys. Swiatlowski Maximilian J. TRIUMF Swirski Thorben Wurzburg U. Sykora Ivan Comenius U. Sykora Martin Charles U. Sykora Tomas Charles U. Ta Duc Mainz U. Tackmann Kerstin DESY Hamburg U. Taffard Anyes UC, Irvine Tafirout Reda TRIUMF Tafoya Vargas Juan Salvador IJCLab, Orsay Takeva Emily Petrova Edinburgh U. Takubo Yosuke KEK, Tsukuba Talby Mossadek Marseille, CPPM Talyshev Alexei CERN Tam Kai Chung Hong Kong U. Tamir Nadav Michael Tel Aviv U. Tanaka Aoto Tokyo U., ICEPP Tanaka Junichi Tokyo U., ICEPP Tanaka Rei IJCLab, Orsay Tanasini Martino INFN, Genoa Genoa U. Tao Zhengcheng British Columbia U. Tapia Araya Sebastian Santa Maria U., Valparaiso Tapprogge Stefan Mainz U. Tarek Abouelfadl Mohamed A. Michigan State U. Tarem Shlomit Technion Tariq Khuram Beijing, Inst. High Energy Phys. 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London Yeletskikh Ivan CERN Yeo Beom Ki UC, Berkeley (main) Yeo Beomki UC, Berkeley (main) Yexley Melissa University Coll. London Yin Pengqi Nevis Labs, Columbia U. Yorita Kohei Waseda U. Younas Sulman Bucharest, IFIN-HH Young Christopher CERN Young Charlie SLAC Yu Chengjun Beijing, Inst. High Energy Phys. UCAS, Beijing Beijing, GUCAS Yu Yi Hefei, CUST Yuan Man Michigan U. Yuan Rui Shandong U. Yue Luzhan University Coll. London Zaazoua Mohamed Hefei, CUST Zabinski Bartlomiej Henryk Cracow, INP Zaid Estifa'A Edinburgh U. Zak Zuzanna Katarzyna Cracow, INP Zakareishvili Tamar Tbilisi State U. Zakharchuk Nataliia Carleton U. Zambito Stefano Geneva U. Zamora Saa Jilberto Antonio Andres Bello Natl. U. SAPHIR Millennium Inst. Zang Jiaqi Tokyo U., ICEPP Zanzi Daniele Freiburg U. Zaplatilek Ota Prague, Tech. U. Zeitnitz Christian Wuppertal U. Zeng Hao Beijing, Inst. High Energy Phys. Zeng Jiancong Illinois U., Urbana Zenger Todd Brandeis U. Zenin Oleg CERN Zenis Tibor Comenius U. Zenz Seth Queen Mary, U. of London Zerradi Soufiane Casablanca U. Zerwas Dirk IJCLab, Orsay Zhai Mingjie Beijing, Inst. High Energy Phys. UCAS, Beijing Zhang Bowen Nanjing U. Zhang Dengfeng Sheffield U. Zhang Jie Shandong U. Zhang Jinlong Argonne Zhang Kaili Beijing, Inst. High Energy Phys. UCAS, Beijing Zhang Lei Nanjing U. Zhang Peng Beijing, Inst. High Energy Phys. UCAS, Beijing Zhang Rui Wisconsin U., Madison Zhang Shuzhou Michigan U. Zhang Sijing Southern Methodist U. Zhang Tingyu Tokyo U., ICEPP Zhang Xiangke Shanghai Jiao Tong U. Zhang Xueyao Shandong U. Zhang Yulei Shanghai Jiao Tong U. APC, Paris Zhang Yuwen Ebony University Coll. London Zhang Yixiang Nanjing U. Zhang Zhicai LBL, Berkeley Zhang Zhiqing Philippe IJCLab, Orsay Zhao Haoran Washington U., Seattle Zhao Tongbin Shandong U. Zhao Yuzhan UC, Santa Cruz Zhao Zhengguo Hefei, CUST Zhemchugov Alexey CERN Zheng Jinchao Nanjing U. Zheng Kai Illinois U., Urbana Zheng Xiangxuan Hefei, CUST Zheng Zhi SLAC Zhong Dewen Illinois U., Urbana Zhou Bing Michigan U. Zhou Hao Arizona U. Zhou Ning Shanghai Jiao Tong U. Zhou You Arizona U. Zhu Chengguang Shandong U. Zhu Junjie Michigan U. Zhu Yifan Shanghai Jiao Tong U. Zhu Yingchun Hefei, CUST Zhuang Xuai Beijing, Inst. High Energy Phys. Zhukov Konstantin CERN Zhulanov Vladimir CERN Zimine Nikolai CERN Zinsser Joachim Heidelberg U. Ziolkowski Michal Siegen U. Zivkovic Lidija Belgrade U. Zoccoli Antonio INFN, Bologna Bologna U. Zoch Knut Harvard U., Phys. Dept. Zorbas Theodore Sheffield U. Zormpa Olga Democritos Nucl. Res. Ctr. Zou Wenkai Nevis Labs, Columbia U. Zwalinski Lukasz CERN 2024 2411 Measurements of the Higgs boson production times decay rates and differential cross-sections have recently been performed by the ATLAS experiment in several decay channels using up to 139 fb$^{-1}$ of proton-proton collision data at $\sqrt{s}=13$ TeV recorded at the Large Hadron Collider. This paper presents multiple interpretations of these Higgs boson measurements. Measurements of production-mode cross-sections, simplified template cross-sections and fiducial differential cross-sections in different decay channels are reparameterised in terms of the impact of Standard Model effective field theory operators, and constraints are reported on the corresponding Wilson coefficients. Production and decay rate measurements are interpreted in UV-complete extensions of the Standard Model, namely the two-Higgs-doublet model (2HDM) near the alignment limit and the Minimal Supersymmetric Standard Model (MSSM) for various MSSM benchmark scenarios. The constraints on the 2HDM parameters $(\cos(\beta-\alpha), \tan\beta)$ and the MSSM parameters $(m_A, \tan\beta)$ are complementary to those obtained from direct searches for additional Higgs bosons. research-article

ATLAS/CMS BSM Higgs Physics (including exotic Higgs and exotic Higgs decays) Sato Koji University of Tsukuba (JP) 2024 We review recent results on Higgs bosons in models beyond the Standard Model from the ATLAS and CMS experiments at the LHC. Topics include the current status of the searches for MSSM Higgs bosons, searches for exotic decay of the 125 GeV Higgs boson, and a selection of most recent analysis results based on full Run 2 dataset. INTNOTEATLASPUBL

Searches for Heavy Resonances: New Scalars and BSM Higgs Decays with ATLAS Run-2 Data Bahmani Marzieh Humboldt University of Berlin (DE) 2025 The Standard Model (SM) has been remarkably successful, yet several key questions remain open, including the nature of dark matter, the matter–antimatter asymmetry, and the origin of neutrino masses. Many extensions of the SM predict additional heavy particles, such as neutral scalars ($H$, $S$), pseudoscalars ($A$), and charged Higgs bosons ($H^\pm$, $H^{\pm\pm}$), as realised for example in Two-Higgs-Doublet Models, Supersymmetry, or hidden-sector Higgs models. We summarise ATLAS Run-2 searches for heavy resonances in these scenarios. Using \SI{140}{fb^{-1}} of $pp$ collisions at $\sqrt{s} $ =13 TeV, we present representative results in four channels: (i) $H^\pm\!\to W^\pm h\!\to\ell\nu b\bar b$, (ii) $H^\pm\!\to\tau\nu$, (iii) exotic decays $S\!\to Z_dZ_d\!\to 4\ell$, and (iv) model-independent dijet resonance searches using weakly supervised anomaly detection. No significant excess is observed. Limits are set in benchmark frameworks (2HDM, hMSSM/MSSM, HAHM) and on generic resonance cross sections, with notable sensitivity gains driven by advanced machine-learning techniques. research-article