eng Barisonzi, M Becker, K Bergeaas Kuutmann, E Boek, T Brooijmans, G Calvet, S Camacho Toro, R Choudalakis, G Febbraro, R Ferrando, J Ferrara, V Fiedler, F Heck, T Issever, C Ji, W Johns, K Karagoz, M Kaushik, V Khoriauli, G Kuhl, T Lange, C Lenz, T Livermore, S Masetti, L Maettig, P Mechtel, M Oliver, E Pallin, D Sinervo, P Sturm, P Villaplana, M Vos, M Wasicki, C Wicke, D Zhu, H A Search for $t\bar{t}$ Resonances in the Lepton Plus Jets Channel using 1.04 fb$^{-1}$ of $pp$ Collisions at $\sqrt{s} = 7$ TeV Detectors and Experimental Techniques ATLAS-COM-CONF-2011-141 A search for top quark pair ($t\bar{t}$) resonances in the lepton plus jets final states has been performed with the ATLAS experiment at the LHC. The search uses a data sample corresponding to an integrated luminosity of 1.04 fb$^{-1}$, and was recorded in 2011 at a proton-proton centre-of-mass energy of 7 TeV. No evidence for a resonance is found. Using the reconstructed $t\bar{t}$ mass spectrum, limits are set on the production cross-section times branching ratio to $t\bar{t}$ for narrow and wide resonances. For narrow $Z'$ models, the observed 95% C.L. limits range from approximately 12.9 pb to 1.1 pb for masses going from $m_{Z'}=$ 500 GeV to $m_{Z'}=$ 1300 GeV, excluding a leptophobic topcolor $Z'$ boson with $m_{Z'} <$ 1000 GeV at 95% C.L. In Randall-Sundrum models, Kaluza-Klein gluons with masses below 1350 GeV are excluded at 95% C.L. 2011-07-27 http://cds.cern.ch/record/1371027 Conference talks on ATLAS http://cds.cern.ch/record/1371027 eng Barisonzi, M Becker, K Bergeaas Kuutmann, E Boek, T Brooijmans, G Calvet, S Camacho Toro, R Choudalakis, G Febbraro, R Ferrando, J Ferrara, V Fiedler, F Heck, T Issever, C Ji, W Johns, K Karagoz, M Kaushik, V Khoriauli, G Kuhl, T Lange, C Lenz, T Livermore, S Masetti, L Maettig, P Mechtel, M Oliver, E Pallin, D Sinervo, P Sturm, P Villaplana, M Vos, M Wasicki, C Wicke, D Zhu, H A Search for $t\bar{t}$ Resonances in the Lepton Plus Jets Channel in 1.04 fb$^{-1}$ of $pp$ Collisions at $\sqrt{s} = 7$ TeV Detectors and Experimental Techniques ATL-COM-PHYS-2011-989 Many models of physics beyond the standard model predict the existence of new resonances that decay to top quark pairs. This paper describes a search for such resonances in the $\ell + jets$ final state in 1.04 fb$^{-1}$ of data collected by the ATLAS experiment in $pp$ collisions at $\sqrt{s} = 7$ TeV in 2011. 95\% C.L. limits are set on the production cross-section times branching ratio to top quark pairs of such resonances, ranging from approximately 21 pb at $m=$ 500 GeV to 0.4 pb at $m=$ 1300 GeV, excluding a leptophobic topcolor $Z'$ boson with 650 GeV $< m_{Z'} <$ 1150 GeV at 95\% C.L. In Randall-Sundrum models, Kaluza-Klein gluons with masses below 1480 GeV are excluded at 95\% C.L. 2011-07-23 http://cds.cern.ch/record/1370071 Physics http://cds.cern.ch/record/1370071 eng Allwood-Spires, S Barisonzi, M Beauchemin, H Bruneliere, R Buchanan, J Castro, N F Devetak, E Feng, C Ferrando, J Hawkings, R Hirschbuehl, D Husemann, U Kersevan, B P Khoriauli, G Kuhl, T Lenz, T Mijovc, L Papadelis, A Sanders, M P Shan, L-Y Sturm, P Veloso, F Verkerke, W Vlasov, N Wasicki, C Monte Carlo samples used for top physics: Top Working Group Note IX Detectors and Experimental Techniques ATL-COM-PHYS-2010-836 This note documents the standard Monte Carlo samples to be used for top rediscovery analyses with 7 TeV data. The dataset numbers, cross sections and statistics are detailed. In addition the justification of k-factors for the different signal and background processes is discussed. A new tool for matching heavy flavour production events in Alpgen samples is described. 2010-10-09 http://cds.cern.ch/record/1298803 Physics http://cds.cern.ch/record/1298803 Supporting document for top paper eng Bellagamba, L Bruni, G Di Sipio, R Husemann, U Wasicki, C Zoccoli1, A Validation of the POWHEG MC Generator for the ATLAS Experiment Detectors and Experimental Techniques ATL-COM-PHYS-2010-699 The POWHEG (POsitive-Weighted Hard-Emission-first Generator) method is a prescription for interfacing NLO calculations with parton shower generators. This method differs for some important details that will be described in the following from the approach implemented in the MC@NLO generator. MC@NLO has been widely deployed in the context of the ATLAS experiment for several years. The aim of this work is to show that POWHEG is now mature enough to be fully used for the simulation of high-energy events. This will make possible the evaluation of the systematic uncertainty due to different choices of the event generation model. Unlike MC@NLO, POWHEG produces unweighted events, and can be easily used with different programs implementing the Monte Carlo parton showering algorithm. Until now POWHEG has been applied to the following processes: ZZ pair hadro-production, heavy-flavor production, e+e− annihilation into hadrons and into top pairs, Drell-Yan vector boson production, W′ production, Higgs boson production via gluon fusion, Higgs-strahlung and vector boson fusion, single-top production and Z+1 jet production. As for the ATLAS experiment, it has been successfully interfacedto HERWIG and Pythia within the ATHENA framework for the production of tt ̄ and W/Z+jets samples. In this work the comparison between POWHEG and MC@NLO has been carried out using pp→tt ̄+X non full-hadronic samples. This note is organized as follows: i n section 2, the POWHEG formalism is presented. In section 3 a comparison between POWHEG and MC@NLO is carried out at generator level, showing the remarkable degree of agreement between the two. In section 4, the main difference between the two approaches (namely the so-called “dip” problem) is explained. Section 5 concerns the tuning of ISR- and FSR- parameters and how they affect the efficiency of the baseline selection of tt ̄ events in the lepton+jets channel at generator level. Finally, section 6 shows the result of the full simulation of the ATLAS detector and the distribution of some relevant quantities after the baseline selection. Section 7 contains some concluding remarks. 2010-08-23 http://cds.cern.ch/record/1288261 Physics http://cds.cern.ch/record/1288261 eng Abi, B Acharya, B Adelman, J Allwood-Spires, S Arguin, J-F Bachacou, H Barisonzi, M Beauchemin, H Bellagamba, L Benekos, N Benslama, K Bentvelsen, S Berge, D Besana, M I Bondioli, M Bosman, M Boudreau, J Bousson, N Brock, I C Brooijmans, G Bruneliere, R Bruni, G Buchanan, J Calkins, R Canepa, A Castro, N F Cerrito, L Charkaborty, D Chevalier, L Cinca, D Clement, B Cobal, M Cooper, B Cortes-Gonzalez, A Cortiana, G Costa, M J Cowden, C Cranmer, K Cristinziani, M Delemnotex, T Derue, F De Sanctis, U Devetak, E DeViveiros, P O Doglioni, C Donini, J Doxiadis, A Elsing, M Erdmann, J Etienvre, A I Farrel, S Federic, P Feligioni, L Feng, C Ferrando, J Ferrara, V Ferrari, A Ferrari, P Filthaut, F Finelli, K Fiorini, L Gaponenko, A Garberson, F Garitaonandia, H Gellerstedt, K Ghodbane, N Grundler, U Guo, B Golling, T Guindon, S Haefner, P Hawkings, R Heelan, L Heim, S Helsens, C Heinemann, B Henrichs, A Hirsch, F Hirschbuhl, D Holzbauer, J Husemann, U Issever, C Johns, K Ju, X Juste, A Kaplan, B Kaushik, V Kendziorra, C Khandanyan, H Khanov, A Kersevan, B P Khoriauli, G Konstantinidis, N Kovesarki, P Krasznahorkay, A Kroninger, K Kruse, M Kuhl, T Kumar Jana, D Lange, C Lapoire, C Lari, T Lei, X Lemmer, B Lenz, T Lessard, J R Lewis, G Leyko, A Liao, H Liss, T Lleres, A Liu, C Loginov, A Losada, M A Loureiro Mattioli, K Lucotte, A Marti I Garcia, S Marzin, A Ming, Y Mir Martinez, L M McLaughlan, T Meloni, F Moreno Llacer, M Mijovic, L Moyse, E Mussche, I Nadal, J zur Nedden, M Nisius, R Nugent, I M Nuncio-Quiroz, E Oakham, G Okawa, H Okumura, Y Pallin, D Palmer, J Papadelis, A Petteni, M Piegaia, R Pinamonti, M Pleier, M A Poghosyan, T Poll, A J Pope, B Psoroulas, S Radics, B Rizatdinova, F Romeo, G Ruehr, F Ryan, P Roe, A Salamanna, G Saleem, M Sanders, M P Schwienhorst, R Schwindling, J Searcy, J Shabalina, E Shan, L Y Sherman, D Sidoti, A Sinervo, P Di Sipio, R Skubic, P Sjoelin, J Sturm, P Suruliz, K Spano, F Ta, D B Taffard, A Takahashi, Y Talby, M Tardif, D Tannoury, N Theveneaux-Pelzer, T Thomas, J Tipton, P L Toggerson, B Tomoto, M Troncon, C Tsiakiris, M Tsulaia, V Uchida, K Urbaniec, D Vacavant, L Veloso, F Verkerke, W Vlasov, N Vorwerk, V Vreeswijk, M van Vulpen, I Wall, R Walsh, B Wang, J Wasicki, C Watson, M F Werth, M Whiteson, D Zhou, N Zhu, H Yu, J Background studies for top-pair production in lepton plus jets final states in sqrt(s)=7 TeV ATLAS data Detectors and Experimental Techniques ATLAS-COM-CONF-2010-085 The search for top quark pairs at the LHC requires the selection of events with leptons, high jet multiplicity, b-tagged jets and missing transverse energy, and the study of control samples with lower jet multiplicity to evaluate the backgrounds. A first study of the backgrounds in the lepton plus jets channel is presented using 295 nb^-1 of ATLAS pp collision data taken at 7 TeV, including a data-driven determination of the contribution QCD multi-jet events. 2010-08-10 http://cds.cern.ch/record/1284257 Conference talks on ATLAS http://cds.cern.ch/record/1284257 eng Abi, B Acharya, B Adelman, J Allwood-Spires, S Arguin, J-F Bachacou, H Barisonzi, M Beauchemin, H Bellagamba, L Benekos, N Benslama, K Bentvelsen, S Berge, D Besana, M I Bondioli, M Bosman, M Boudreau, J Bousson, N Brock, I C Brooijmans, G Bruneliere, R Bruni, G Buchanan, J Calkins, R Canepa, A Castro, N F Cerrito, L Charkaborty, D Chevalier, L Cinca, D Clement, B Cobal, M Cooper, B Cortes-Gonzalez, A Cortiana, G Costa, M J Cowden, C Cranmer, K Cristinziani, M Delemnotex, T Derue, F De Sanctis, U Devetak, E DeViveiros, P O Doglioni, C Donini, J Doxiadis, A Elsing, M Erdmann, J Etienvre, A I Farrel, S Federic, P Feligioni, L Feng, C Ferrando, J Ferrara, V Ferrari, A Ferrari, P Filthaut, F Finelli, K Fiorini, L Gaponenko, A Garberson, F Garitaonandia, H Gellerstedt, K Ghodbane, N Grundler, U Guo, B Golling, T Haefner, P Hawkings, R Heelan, L Heim, S Helsens, C Heinemann, B Henrichs, A Hirsch, F Hirschbuhl, D Holzbauer, J Husemann, U Issever, C Johns, K Ju, X Juste, A Kaplan, B Kaushik, V Kendziorra, C Khandanyan, H Khanov, A Kersevan, B P Khoriauli, G Konstantinidis, N Kovesarki, P Krasznahorkay, A Kroninger, K Kruse, M Kuhl, T Kumar Jana, D Lange, C Lapoire, C Lari, T Lei, X Lemmer, B Lenz, T Lessard, J R Lewis, G Leyko, A Liao, H Liss, T Lleres, A Liu, C Loginov, A Losada, M A Loureiro Mattioli, K Lucotte, A Marti i García, S Marzin, A Ming, Y Mir Martinez, L M McLaughlan, T Meloni, F Moreno Llacer, M Mijovic, L Moyse, E Mussche, I Nadal, J zur Nedden, M Nisius, R Nugent, I M Nuncio-Quiroz, E Oakham, G Okawa, H Okumura, Y Pallin, D Palmer, J Papadelis, A Petteni, M Piegaia, R Pinamonti, M Pleier, M A Poghosyan, T Poll, A J Pope, B Psoroulas, S Radics, B Rizatdinova, F Romeo, G Ruehr, F Ryan, P Roe, A Salamanna, G Saleem, M Sanders, M P Schwienhorst, R Schwindling, J Searcy, J Shabalina, E Shan, L Y Sherman, D Sidoti, A Sinervo, P Di Sipio, R Skubic, P Sjoelin, J Sturm, P Suruliz, K Spano, F Ta, D B Taffard, A Takahashi, Y Talby, M Tardif, D Tannoury, N Theveneaux-Pelzer, T Thomas, J Tipton, P L Toggerson, B Tomoto, M Troncon, C Tsiakiris, M Tsulaia, V Uchida, K Urbaniec, D Vacavant, L Veloso, F Verkerke, W Vlasov, N Vorwerk, V Vreeswijk, M van Vulpen, I Wall, R Walsh, B Wang, J Wasicki, C Watson, M F Werth, M Whiteson, D Zhou, N Zhu, H Yu, J Search for top pair candidate events in ATLAS at sqrt(s)=7 TeV Detectors and Experimental Techniques ATLAS-COM-CONF-2010-046 A search is performed for events consistent with top quark pair production in 280 nb^-1 of ATLAS pp collision data taken at sqrt(s)=7 TeV. Several candidate events are observed, in both the lepton plus jets and dilepton topologies. The properties of these events are described, and compared to the expectations from Monte Carlo simulation. 2010-07-16 http://cds.cern.ch/record/1278460 Conference talks on ATLAS http://cds.cern.ch/record/1278460 gerWasicki, ChristophMonte-Carlo-Simulation von Top-Paaren in nächstführender Ordnung am ATLAS-ExperimentParticle Physics - ExperimentCERN-THESIS-2010-169Due to the probabilistic nature of quantum mechanics, the structure of individual events in particle physics is not calculable ab initio. Therefore, Monte Carlo simulations mark an important tool for understanding experiments in elementary particle physics. Most current Monte Carlo generators employ leading-order matrix elements; these cannot meet the level of accuracy that can be reached by the ATLAS experiment. Although calculations in next-to-leading order have been known for some years, their implementation for generating physically meaningful events is not trivial. The first successful implementation, which defines the standard in this area, is MC@NLO. An alternative approach is the Powheg method, which is examined in more detail in this thesis on the basis of top pair production. The results of both methods are compared and differences are evaluated. It is shown that Powheg represents a viable alternative to MC@NLO that avoids some of its shortcomings. In particular, the method is independent of the parton shower formalism, which allows combining it with the Pythia generator. In this combination, variations of space- and time-like emissions in parton showers are investigated and compared with the results in leading order. The analysis suggests that variations remain substantially valid with matrix elements in next-to-leading order. Nevertheless, significant differences between the two matrix elements are discovered tha t require further study.Freie Universitaet Berlin2010http://cds.cern.ch/record/1312615http://cds.cern.ch/record/1312615oai:cds.cern.ch:1312615Presented on 01 Jul 2010 eng Allwood-Spires, S Barisonzi, M Beauchemin, H Bruneliere, R Buchanan, J Castro, N F Devetak, E Feng, C Ferrando, J Hawkings, R Hirschbuehl, D Husemann, U Kersevan, B P Khoriauli, G Kuhl, T Lenz, T Mijovc, L Papadelis, A Sanders, M P Shan, L-Y Sturm, P Veloso, F Verkerke, W Vlasov, N Wasicki, C Monte Carlo samples used for top physics Detectors and Experimental Techniques ATL-PHYS-INT-2010-132 This note documents the standard Monte Carlo samples to be used for top rediscovery analyses with 7 TeV data. The dataset numbers, cross sections and statistics are detailed. In addition the justification of k-factors for the different signal and background processes is discussed. A new tool for matching heavy flavour production events in Alpgen samples is described. 2010-12-08 http://cds.cern.ch/record/1312945 Physics http://cds.cern.ch/record/1312945 eng Bellagamba, L Bruni, G Di Sipio, R Husemann, U Wasicki, C Zoccoli1, A Validation of the POWHEG MC Generator for the ATLAS Experiment Detectors and Experimental Techniques ATL-PHYS-INT-2011-038 The POWHEG (POsitive-Weighted Hard-Emission-first Generator) method is a prescription for interfacing NLO calculations with parton shower generators. This method differs for some important details that will be described in the following from the approach implemented in the MC@NLO generator. MC@NLO has been widely deployed in the context of the ATLAS experiment for several years. The aim of this work is to show that POWHEG is now mature enough to be fully used for the simulation of high-energy events. This will make possible the evaluation of the systematic uncertainty due to different choices of the event generation model. Unlike MC@NLO, POWHEG produces unweighted events, and can be easily used with different programs implementing the Monte Carlo parton showering algorithm. Until now POWHEG has been applied to the following processes: ZZ pair hadro-production, heavy-flavor production, e+e− annihilation into hadrons and into top pairs, Drell-Yan vector boson production, W′ production, Higgs boson production via gluon fusion, Higgs-strahlung and vector boson fusion, single-top production and Z+1 jet production. As for the ATLAS experiment, it has been successfully interfacedto HERWIG and Pythia within the ATHENA framework for the production of tt ̄ and W/Z+jets samples. In this work the comparison between POWHEG and MC@NLO has been carried out using pp→tt ̄+X non full-hadronic samples. This note is organized as follows: i n section 2, the POWHEG formalism is presented. In section 3 a comparison between POWHEG and MC@NLO is carried out at generator level, showing the remarkable degree of agreement between the two. In section 4, the main difference between the two approaches (namely the so-called “dip” problem) is explained. Section 5 concerns the tuning of ISR- and FSR- parameters and how they affect the efficiency of the baseline selection of tt ̄ events in the lepton+jets channel at generator level. Finally, section 6 shows the result of the full simulation of the ATLAS detector and the distribution of some relevant quantities after the baseline selection. Section 7 contains some concluding remarks. 2011-04-19 http://cds.cern.ch/record/1345724 Physics http://cds.cern.ch/record/1345724 eng Collaboration, A Performance of the ATLAS Inner Detector Track and Vertex Reconstruction in the High Pile-Up LHC Environment Detectors and Experimental Techniques ATLAS-COM-CONF-2012-014 The performance of the ATLAS inner detector in a high occupancy environment of approximately 30 inelastic proton-proton interactions per bunch crossing is presented. The track and vertex reconstruction algorithms are studied in data by comparing track and vertex properties such as multiplicities, track impact parameters, the number of hits on track and detector occupancies for a varying number of proton-proton interactions per bunch crossing. Several simulated samples are used to estimate the track and vertex reconstruction efficiency and to quantify the level of agreement between data and simulation. It is shown that although pile-up has a significant impact in many areas, the detector design and reconstruction algorithms are sufficiently robust to maintain a good performance in such a high pile-up environment. 2012-02-15 http://cds.cern.ch/record/1424371 Conference talks on ATLAS http://cds.cern.ch/record/1424371 eng Adelman, J Andreazza, A Elsing, M Gadatsch, S Gray, HM Pagan Griso, S Salzburger, A Selbach, K Wasicki, C Wildauer, A Performance of the ATLAS Inner Detector Track and Vertex Reconstruction in the High Pile-Up LHC Environment Detectors and Experimental Techniques ATL-COM-PHYS-2012-106 Excellent LHC performance has resulted in more than 5~fb$^{-1}$ of data being delivered to ATLAS in 2011. Partly, this was achieved by increasing the average number of interactions per bunch crossing. As a consequence, the average number of interactions per bunch crossing (or pile-up) reached $sim$15 in the latter part of the year. Current projections indicate that the peak may be as high as 30 in 2012, beyond the design specifications. A high pile-up environment poses many challenges for physics analyses and, in particular, in maintaining object reconstruction efficiency and quality. This document present a study of Inner Detector performance in a high pile-up environment ranging from detector performance to tracking and vertexing studies. To do this, the data delivered in two high intensity fills near the end of the 2011 data-taking period was analysed. In addition, the modelling of this pile-up in simulation is discussed. It will be shown that although pile-up has a significant impact in many areas, the detector design and reconstruction algorithms are sufficiently robust to maintain performance in such a high density environment. 2012-01-02 http://cds.cern.ch/record/1420939 Physics http://cds.cern.ch/record/1420939 eng Wasicki, C ATLAS Inner Detector Track Reconstruction in high pile-up Detectors and Experimental Techniques ATL-COM-PHYS-2012-275 With an average number of up to 23 pile-up interactions per bunch crossing (μ) in 2011 data taking the ATLAS Inner Detector (ID) already reached its design specifications. This poster presents studies in data and simulation demonstrating that the ID track reconstruction is well-prepared for the high pile-up expected in 2012. 2012-03-10 http://cds.cern.ch/record/1430739 Physics http://cds.cern.ch/record/1430739 21. March 2012 engWasicki, CTrack and vertex reconstruction of the ATLAS Inner Detector in the high multiplicity LHC environmentDetectors and Experimental TechniquesATL-PHYS-PROC-2012-111With an average number of up to 30 pile-up interactions per bunch crossing in 2012 data, the ATLAS Inner Detector at the LHC is performing in an environment beyond its design specifications. This has a significant impact on event reconstruction such as additional demands on CPU time and disk space as well as an increased probability to reconstruct fake tracks. Therefore the track and vertex reconstruction performance has been optimised in several high pile-up scenarios. Studies in data and simulation are presented which demonstrate that the performance of the Inner Detector track and vertex reconstruction is robust even in a high pile-up environment.2012-06-29http://cds.cern.ch/record/1458901Physicshttp://cds.cern.ch/record/1458901oai:cds.cern.ch:1458901 doi:10.1007/JHEP08(2015)148engAad, GeorgesAbbott, BradAbdallah, JalalAbdinov, OvsatAben, RosemarieAbolins, MarisAbouZeid, OssamaAbramowicz, HalinaAbreu, HensoAbreu, RicardoAbulaiti, YimingAcharya, Bobby SamirAdamczyk, LeszekAdams, DavidAdelman, JahredAdomeit, StefanieAdye, TimAffolder, TonyAgatonovic-Jovin, TatjanaAguilar-Saavedra, Juan AntonioAhlen, StevenAhmadov, FaigAielli, GiulioAkerstedt, HenrikÅkesson, Torsten Paul AkeAkimoto, GingaAkimov, AndreiAlberghi, Gian LuigiAlbert, JustinAlbrand, SolveigAlconada Verzini, Maria JosefinaAleksa, MartinAleksandrov, IgorAlexa, CalinAlexander, GideonAlexopoulos, TheodorosAlhroob, MuhammadAlimonti, GianlucaAlio, LionAlison, JohnAlkire, Steven PatrickAllbrooke, BenedictAllport, PhillipAloisio, AlbertoAlonso, AlejandroAlonso, FranciscoAlpigiani, CristianoAltheimer, Andrew DavidAlvarez Gonzalez, BarbaraΆlvarez Piqueras, DamiánAlviggi, MariagraziaAmadio, Brian ThomasAmako, KatsuyaAmaral Coutinho, YaraAmelung, ChristophAmidei, DanteAmor Dos Santos, Susana PatriciaAmorim, AntonioAmoroso, SimoneAmram, NirAmundsen, GlennAnastopoulos, ChristosAncu, Lucian StefanAndari, NansiAndeen, TimothyAnders, Christoph FalkAnders, GabrielAnders, John KennethAnderson, KelbyAndreazza, AttilioAndrei, George VictorAngelidakis, StylianosAngelozzi, IvanAnger, PhilippAngerami, AaronAnghinolfi, FrancisAnisenkov, AlexeyAnjos, NunoAnnovi, AlbertoAntonelli, MarioAntonov, AlexeyAntos, JaroslavAnulli, FabioAoki, MasatoAperio Bella, LudovicaArabidze, GiorgiArai, YasuoAraque, Juan PedroArce, AyanaArduh, Francisco AnuarArguin, Jean-FrancoisArgyropoulos, SpyridonArik, MetinArmbruster, Aaron JamesArnaez, OlivierArnal, VanessaArnold, HannahArratia, MiguelArslan, OzanArtamonov, AndreiArtoni, GiacomoAsai, ShojiAsbah, NedaaAshkenazi, AdiÅsman, BarbroAsquith, LilyAssamagan, KeteviAstalos, RobertAtkinson, MarkusAtlay, Naim BoraAuerbach, BenjaminAugsten, KamilAurousseau, MathieuAvolio, GiuseppeAxen, BradleyAyoub, Mohamad KassemAzuelos, GeorgesBaak, MaxBaas, AlessandraBacci, CesareBachacou, HenriBachas, KonstantinosBackes, MoritzBackhaus, MalteBagiacchi, PaoloBagnaia, PaoloBai, YuBain, TravisBaines, JohnBaker, Oliver KeithBalek, PetrBalestri, ThomasBalli, FabriceBanas, ElzbietaBanerjee, SwagatoBannoura, Arwa A EBansil, Hardeep SinghBarak, LironBarberio, Elisabetta LuigiaBarberis, DarioBarbero, MarlonBarillari, TeresaBarisonzi, MarcelloBarklow, TimothyBarlow, NickBarnes, Sarah LouiseBarnett, BruceBarnett, MichaelBarnovska, ZuzanaBaroncelli, AntonioBarone, GaetanoBarr, AlanBarreiro, FernandoBarreiro Guimarães da Costa, JoãoBartoldus, RainerBarton, Adam EdwardBartos, PavolBasalaev, ArtemBassalat, AhmedBasye, AustinBates, RichardBatista, Santiago JuanBatley, RichardBattaglia, MarcoBauce, MatteoBauer, FlorianBawa, Harinder SinghBeacham, James BakerBeattie, Michael DavidBeau, TristanBeauchemin, Pierre-HuguesBeccherle, RobertoBechtle, PhilipBeck, Hans PeterBecker, Anne KathrinBecker, MauriceBecker, SebastianBeckingham, MatthewBecot, CyrilBeddall, AndrewBeddall, AydaBednyakov, VadimBee, ChristopherBeemster, LarsBeermann, ThomasBegel, MichaelBehr, Janna KatharinaBelanger-Champagne, CamilleBell, WilliamBella, GideonBellagamba, LorenzoBellerive, AlainBellomo, MassimilianoBelotskiy, KonstantinBeltramello, OlgaBenary, OdetteBenchekroun, DrissBender, MichaelBendtz, KatarinaBenekos, NektariosBenhammou, YanBenhar Noccioli, EleonoraBenitez Garcia, Jorge-ArmandoBenjamin, DouglasBensinger, JamesBentvelsen, StanBeresford, LydiaBeretta, MatteoBerge, DavidBergeaas Kuutmann, ElinBerger, NicolasBerghaus, FrankBeringer, JürgBernard, ClareBernard, Nathan RogersBernius, CatrinBernlochner, Florian UrsBerry, TraceyBerta, PeterBertella, ClaudiaBertoli, 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BenjaminXella, StefaniaXu, DaXu, LailinYabsley, BruceYacoob, SahalYakabe, RyotaYamada, MihoYamaguchi, YoheiYamamoto, AkiraYamamoto, ShimpeiYamanaka, TakashiYamauchi, KatsuyaYamazaki, YujiYan, ZhenYang, HaijunYang, HongtaoYang, YiYao, LiwenYao, WeimingYasu, YoshijiYatsenko, ElenaYau Wong, Kaven HenryYe, JingboYe, ShuweiYeletskikh, IvanYen, Andy LYildirim, EdaYorita, KoheiYoshida, RikutaroYoshihara, KeisukeYoung, CharlesYoung, Christopher JohnYoussef, SaulYu, David Ren-HwaYu, JaehoonYu, JiamingYu, JieYuan, LiYurkewicz, AdamYusuff, ImranZabinski, BartlomiejZaidan, RemiZaitsev, AlexanderZalieckas, JustasZaman, AungshumanZambito, StefanoZanello, LuciaZanzi, DanieleZeitnitz, ChristianZeman, MartinZemla, AndrzejZengel, KeithZenin, OlegŽeniš, TiborZerwas, DirkZhang, DongliangZhang, FangzhouZhang, JinlongZhang, LeiZhang, RuiqiZhang, XueyaoZhang, ZhiqingZhao, XiandongZhao, YongkeZhao, ZhengguoZhemchugov, AlexeyZhong, JiahangZhou, BingZhou, ChenZhou, LeiZhou, LiZhou, NingZhu, Cheng GuangZhu, HongboZhu, JunjieZhu, YingchunZhuang, XuaiZhukov, KonstantinZibell, AndreZieminska, DariaZimine, NikolaiZimmermann, ChristophZimmermann, StephanieZinonos, ZinonasZinser, MarkusZiolkowski, MichaelŽivković, LidijaZobernig, GeorgZoccoli, Antoniozur Nedden, MartinZurzolo, GiovanniZwalinski, LukaszA search for $t\bar{t}$ resonances using lepton-plus-jets events in proton--proton collisions at $\sqrt{s} = 8$ TeV with the ATLAS detectorParticle Physics - ExperimentarXiv:1505.07018CERN-PH-EP-2015-090CERN-PH-EP-2015-090A search for new particles that decay into top quark pairs is reported. The search is performed with the ATLAS experiment at the LHC using an integrated luminosity of 20.3 fb$^{-1}$ of proton--proton collision data collected at a centre-of-mass energy of $\sqrt{s}=8$ TeV. The lepton-plus-jets final state is used, where the top pair decays to $W^+bW^-\bar{b}$, with one $W$ boson decaying leptonically and the other hadronically. The invariant mass spectrum of top quark pairs is examined for local excesses or deficits that are inconsistent with the Standard Model predictions. No evidence for a top quark pair resonance is found, and 95% confidence-level limits on the production rate are determined for massive states in benchmark models. The upper limits on the cross-section times branching ratio of a narrow $Z'$ boson decaying to top pairs range from 4.2 pb to 0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A narrow leptophobic topcolour $Z'$ boson with mass below 1.8 TeV is excluded. Upper limits are set on the cross-section times branching ratio for a broad colour-octet resonance with $\Gamma/m =$ 15% decaying to $t\bar{t}$. These range from 2.5 pb to 0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza--Klein excitation of the gluon in a Randall--Sundrum model is excluded for masses below 2.2 TeV.A search for new particles that decay into top quark pairs is reported. The search is performed with the ATLAS experiment at the LHC using an integrated luminosity of 20.3 fb$^{−1}$ of proton-proton collision data collected at a centre-of-mass energy of $ \sqrt{s}=8 $ TeV. The lepton-plus-jets final state is used, where the top pair decays to $ {W}^{+}b{W}^{-}\overline{b} $ , with one W boson decaying leptonically and the other hadronically. The invariant mass spectrum of top quark pairs is examined for local excesses or deficits that are inconsistent with the Standard Model predictions. No evidence for a top quark pair resonance is found, and 95% confidence-level limits on the production rate are determined for massive states in benchmark models. The upper limits on the cross-section times branching ratio of a narrow Z′ boson decaying to top pairs range from 4.2 pb to 0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A narrow leptophobic topcolour Z′ boson with mass below 1.8 TeV is excluded. Upper limits are set on the cross-section times branching ratio for a broad colour-octet resonance with Γ/m = 15% decaying to $ t\overline{t} $ . These range from 4.8 pb to 0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza-Klein excitation of the gluon in a Randall-Sundrum model is excluded for masses below 2.2 TeV.A search for new particles that decay into top quark pairs is reported. The search is performed with the ATLAS experiment at the LHC using an integrated luminosity of 20.3 fb$^{-1}$ of proton-proton collision data collected at a centre-of-mass energy of $\sqrt{s}=8$ TeV. The lepton-plus-jets final state is used, where the top pair decays to $W^+bW^-\bar{b}$, with one $W$ boson decaying leptonically and the other hadronically. The invariant mass spectrum of top quark pairs is examined for local excesses or deficits that are inconsistent with the Standard Model predictions. No evidence for a top quark pair resonance is found, and 95% confidence-level limits on the production rate are determined for massive states in benchmark models. The upper limits on the cross-section times branching ratio of a narrow $Z'$ boson decaying to top pairs range from 4.2 pb to 0.03 pb for resonance masses from 0.4 TeV to 3.0 TeV. A narrow leptophobic topcolour $Z'$ boson with mass below 1.8 TeV is excluded. Upper limits are set on the cross-section times branching ratio for a broad colour-octet resonance with $\Gamma/m =$ 15% decaying to $t\bar{t}$. These range from 2.5 pb to 0.03 pb for masses from 0.4 TeV to 3.0 TeV. A Kaluza-Klein excitation of the gluon in a Randall-Sundrum model is excluded for masses below 2.2 TeV.2015-05-22http://cds.cern.ch/record/201786210.1007/JHEP08(2015)148http://cds.cern.ch/record/2017862oai:cds.cern.ch:201786237 pages plus author list (53 pages total), 12 figures, 2 tables, published version, all figures including auxiliary figures are available at https://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/TOPQ-2012-18/ doi:10.1007/JHEP09(2012)041engAad, GeorgesAbajyan, TatevikAbbott, BradAbdallah, JalalAbdel Khalek, SamahAbdelalim, Ahmed AliAbdinov, OvsatAben, RosemarieAbi, BabakAbolins, MarisAbouZeid, OssamaAbramowicz, HalinaAbreu, HensoAcerbi, EmilioAcharya, Bobby SamirAdamczyk, LeszekAdams, DavidAddy, TettehAdelman, JahredAdomeit, StefanieAdragna, PaoloAdye, TimAefsky, ScottAguilar-Saavedra, Juan AntonioAgustoni, MarcoAharrouche, MohamedAhlen, StevenAhles, FlorianAhmad, AshfaqAhsan, MahsanaAielli, GiulioAkdogan, TaylanÅkesson, Torsten Paul AkeAkimoto, GingaAkimov, AndreiAlam, MohammadAlam, Muhammad AftabAlbert, JustinAlbrand, SolveigAleksa, MartinAleksandrov, IgorAlessandria, FrancoAlexa, CalinAlexander, GideonAlexandre, GauthierAlexopoulos, TheodorosAlhroob, MuhammadAliev, MalikAlimonti, GianlucaAlison, JohnAllbrooke, BenedictAllport, PhillipAllwood-Spiers, SarahAlmond, JohnAloisio, AlbertoAlon, RazAlonso, AlejandroAlonso, FranciscoAlvarez Gonzalez, BarbaraAlviggi, MariagraziaAmako, KatsuyaAmelung, ChristophAmmosov, VladimirAmorim, AntonioAmram, NirAnastopoulos, ChristosAncu, Lucian StefanAndari, NansiAndeen, TimothyAnders, Christoph FalkAnders, GabrielAnderson, KelbyAndreazza, AttilioAndrei, George VictorAnduaga, XabierAnger, PhilippAngerami, AaronAnghinolfi, FrancisAnisenkov, AlexeyAnjos, NunoAnnovi, AlbertoAntonaki, AriadniAntonelli, MarioAntonov, AlexeyAntos, JaroslavAnulli, FabioAoki, MasatoAoun, SaharAperio Bella, LudovicaApolle, RudiArabidze, GiorgiAracena, IgnacioArai, YasuoArce, AyanaArfaoui, SamirArguin, Jean-FrancoisArik, EnginArik, MetinArmbruster, Aaron JamesArnaez, OlivierArnal, VanessaArnault, ChristianArtamonov, AndreiArtoni, GiacomoArutinov, DavidAsai, ShojiAsfandiyarov, RuslanAsk, StefanÅsman, BarbroAsquith, LilyAssamagan, KeteviAstbury, AlanAubert, BernardAuge, EtienneAugsten, KamilAurousseau, MathieuAvolio, GiuseppeAvramidou, Rachel MariaAxen, DavidAzuelos, GeorgesAzuma, YuyaBaak, MaxBaccaglioni, GiuseppeBacci, CesareBach, AndreBachacou, HenriBachas, KonstantinosBackes, MoritzBackhaus, MalteBadescu, ElisabetaBagnaia, PaoloBahinipati, SeemaBai, YuBailey, DavidBain, TravisBaines, JohnBaker, Oliver KeithBaker, MarkBaker, SarahBanas, ElzbietaBanerjee, PiyaliBanerjee, SwagatoBanfi, DaniloBangert, Andrea MichelleBansal, VikasBansil, Hardeep SinghBarak, LironBaranov, SergeiBarbaro Galtieri, AngelaBarber, TomBarberio, Elisabetta LuigiaBarberis, DarioBarbero, MarlonBardin, DmitriBarillari, TeresaBarisonzi, MarcelloBarklow, TimothyBarlow, NickBarnett, BruceBarnett, MichaelBaroncelli, AntonioBarone, GaetanoBarr, 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StefanValladolid Gallego, EvaVallecorsa, SofiaValls Ferrer, Juan AntonioVan Der Deijl, Pietervan der Geer, Rogiervan der Graaf, HarryVan Der Leeuw, Robinvan der Poel, Eggevan der Ster, Danielvan Eldik, Nielsvan Gemmeren, Petervan Vulpen, IvoVanadia, MarcoVandelli, WainerVaniachine, AlexandreVankov, PeterVannucci, FrancoisVari, RiccardoVarol, TulinVarouchas, DimitrisVartapetian, ArmenVarvell, KevinVassilakopoulos, VassiliosVazeille, FrancoisVazquez Schroeder, TamaraVegni, GuidoVeillet, Jean-JacquesVeloso, FilipeVeness, RaymondVeneziano, StefanoVentura, AndreaVentura, DanielVenturi, ManuelaVenturi, NicolaVercesi, ValerioVerducci, MonicaVerkerke, WouterVermeulen, JosVest, AnjaVetterli, MichelVichou, IreneVickey, TrevorVickey Boeriu, Oana ElenaViehhauser, GeorgViel, SimonVilla, MauroVillaplana Perez, MiguelVilucchi, ElisabettaVincter, ManuellaVinek, ElisabethVinogradov, VladimirVirchaux, MarcVirzi, JosephVitells, OferViti, MicheleVivarelli, IacopoVives Vaque, FrancescVlachos, 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BenjaminXella, StefaniaXiao, MengXie, SongXu, ChaoXu, DaYabsley, BruceYacoob, SahalYamada, MihoYamaguchi, HiroshiYamamoto, AkiraYamamoto, KyokoYamamoto, ShimpeiYamamura, TaikiYamanaka, TakashiYamaoka, JaredYamazaki, TakayukiYamazaki, YujiYan, ZhenYang, HaijunYang, Un-KiYang, YiYang, ZhaoyuYanush, SergueiYao, LiwenYao, YushuYasu, YoshijiYbeles Smit, Gabriel ValentijnYe, JingboYe, ShuweiYilmaz, MetinYoosoofmiya, RezaYorita, KoheiYoshida, RikturaYoung, CharlesYoung, Christopher JohnYoussef, SaulYu, DantongYu, JaehoonYu, JieYuan, LiYurkewicz, AdamByszewski, MarcinZabinski, BartlomiejZaidan, RemiZaitsev, AlexanderZajacova, ZuzanaZanello, LuciaZaytsev, AlexanderZeitnitz, ChristianZeman, MartinZemla, AndrzejZendler, CarolinZenin, OlegŽeniš, TiborZinonos, ZinonasZenz, SethZerwas, DirkZevi della Porta, GiovanniZhan, ZhichaoZhang, DongliangZhang, HuaqiaoZhang, JinlongZhang, XueyaoZhang, ZhiqingZhao, LongZhao, TianchiZhao, ZhengguoZhemchugov, AlexeyZhong, JiahangZhou, BingZhou, NingZhou, YueZhu, Cheng GuangZhu, HongboZhu, JunjieZhu, YingchunZhuang, XuaiZhuravlov, VadymZieminska, DariaZimin, NikolaiZimmermann, RobertZimmermann, SimoneZimmermann, StephanieZiolkowski, MichaelZitoun, RobertŽivković, LidijaZmouchko, ViatcheslavZobernig, GeorgZoccoli, Antoniozur Nedden, MartinZutshi, VishnuZwalinski, LukaszA search for $t\bar{t}$ resonances in lepton+jets events with highly boosted top quarks collected in $pp$ collisions at $\sqrt{s}$ = 7 TeV with the ATLAS detectorParticle Physics - ExperimentarXiv:1207.2409CERN-PH-EP-2012-158CERN-PH-EP-2012-158A search for resonant production of high-mass top-quark pairs is performed on 2.05 fb$^{-1}$ of proton-proton collisions at $\sqrt{s}$ = 7 TeV collected in 2011 with the ATLAS experiment at the Large Hadron Collider. This analysis of the lepton+jets final state is specifically designed for the particular topology that arises from the decay of highly boosted top quarks. The observed $t\bar{t}$ invariant mass spectrum is found to be compatible with the Standard Model prediction and 95% credibility level upper limits are derived on the $t\bar{t}$ production rate through new massive states. An upper limit of 0.7 pb is set on the production cross section times branching fraction of a narrow 1 TeV resonance. A Kaluza-Klein gluon with a mass smaller than 1.5 TeV is excluded.A search for resonant production of high-mass top-quark pairs is performed on 2.05 fb^-1 of proton-proton collisions at sqrt(s) = 7 TeV collected in 2011 with the ATLAS experiment at the Large Hadron Collider. This analysis of the lepton+jets final state is specifically designed for the particular topology that arises from the decay of highly boosted top quarks. The observed ttbar invariant mass spectrum is found to be compatible with the Standard Model prediction and 95% credibility level upper limits are derived on the ttbar production rate through new massive states. An upper limit of 0.7 pb is set on the production cross section times branching fraction of a narrow 1 TeV resonance. A Kaluza-Klein gluon with a mass smaller than 1.5 TeV is excluded.2012-07-11http://cds.cern.ch/record/146122510.1007/JHEP09(2012)041http://cds.cern.ch/record/1461225oai:cds.cern.ch:1461455Comments: 25 pages plus author list (47 pages total), 7 figures, 4 tables, matches published JHEP version25 pages plus author list (47 pages total), 7 figures, 4 tables, matches published JHEP version