2013-06-11
14:48 |
Measurement of color coherence effects in pp collisions at root s = 7 TeV
/CMS Collaboration
A study of color coherence effects in pp collisions at a center-of-mass energy of 7 TeV has been performed.
The data used in the analysis were collected in 2010 by the CMS detector at the LHC and correspond to an integrated luminosity of $36$ ${\rm{pb}}^{-1}$.
Events are selected in which there are at least three jets with the two leading jets in transverse momentum having a pronounced back-to-back topology.
The measurement of the azimuthal angular correlation between the second and third jets is compared to the predictions of Monte-Carlo models with different implementations of color coherence effects..
CMS-PAS-SMP-12-010.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004: PDF; Figure_005: PDF; Fulltext in PDF: PDF;
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2013-06-01
10:11 |
Phenomenological MSSM interpretation of the CMS 2011 5fb-1 results
/CMS Collaboration
We interpret within the phenomenological MSSM (pMSSM) results obtained
by CMS using a $pp$ data set collected in 2011 at 7~TeV, corresponding
to an integrated luminosity of 5~fb$^{-1}$.
The pMSSM is a 19-parameter realization of the MSSM defined at the SUSY
scale, that captures most of the features of the general R-parity
conserving weak-scale MSSM.
A global Bayesian analysis is performed that yields posterior
probability densities of model parameters, masses and observables. We
provide conclusions that are more generic, and therefore more robust,
than those derived in more constrained setups, including simplified
models and models that impose particular SUSY breaking schemes, such
as the CMSSM.
%Our results also comprise We also study implications for the MSSM Higgs sector,
as well as for dark matter searches. [...]
CMS-PAS-SUS-12-030.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_002-c: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_003-c: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_008: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_009-c: PDF; Figure_009-d: PDF; Figure_009-e: PDF; Figure_009-f: PDF; Figure_009-g: PDF; Figure_009-h: PDF; Figure_009-i: PDF; Figure_009-j: PDF; Figure_009-k: PDF; Figure_009-l: PDF; Figure_009-m: PDF; Figure_009-n: PDF; Figure_009-o: PDF; Figure_009-p: PDF; Figure_009-q: PDF; Figure_009-r: PDF; Figure_009-s: PDF; Figure_009-t: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_010-c: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_012-a: PDF; Figure_012-b: PDF; Figure_012-c: PDF; Figure_012-d: PDF; Figure_012-e: PDF; Figure_012-f: PDF; Figure_012-g: PDF; Figure_012-h: PDF; Figure_012-i: PDF; Figure_013-a: PDF; Figure_013-b: PDF; Figure_013-c: PDF; Figure_013-d: PDF; Figure_013-e: PDF; Figure_013-f: PDF; Figure_013-g: PDF; Figure_013-h: PDF; Figure_013-i: PDF; Figure_014: PDF; Figure_015: PDF; Figure_016-a: PDF; Figure_016-b: PDF; Figure_016-c: PDF; Figure_016-d: PDF; Figure_016-e: PDF; Figure_016-f: PDF; Figure_017-a: PDF; Figure_017-b: PDF; Figure_017-c: PDF; Figure_017-d: PDF; Figure_018: PDF; Figure_019: PDF; Figure_020-a: PDF; Figure_020-b: PDF; Figure_020-c: PDF; Figure_021: PDF; Figure_022-a: PDF; Figure_022-b: PDF; Figure_022-c: PDF; Figure_023: PDF; Figure_024: PDF; Figure_025-a: PDF; Figure_025-b: PDF; Figure_025-c: PDF; Figure_025-d: PDF; Figure_025-e: PDF; Figure_025-f: PDF; Figure_026-a: PDF; Figure_026-b: PDF; Figure_026-c: PDF; Figure_026-d: PDF; Figure_026-e: PDF; Figure_027-a: PDF; Figure_027-b: PDF; Figure_028: PDF; Figure_029-a: PDF; Figure_029-b: PDF; Figure_030: PDF; Figure_031: PDF; Fulltext in PDF: PDF;
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2013-05-22
22:44 |
Search for RPV SUSY in the four-lepton final state
/CMS Collaboration
We present a search for anomalous production of events with four isolated leptons in $19.5\,\text{fb}^{\text{$-$1}}$ of data collected by the CMS experiment in $pp$ collisions at $\sqrt{s}$ = 8 TeV. No excess of events is observed over the standard model background. [...]
CMS-PAS-SUS-13-010.-
Geneva : CERN, 2013
Figure_001-a: PDF; Figure_001-b: PDF; Figure_001-c: PDF; Figure_001-d: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003: PDF; Figure_004-a: PNG; Figure_004-b: PNG; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_007-c: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_009: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_012-a: PDF; Figure_012-b: PDF; Figure_013-a: PDF; Figure_013-b: PDF; Figure_014-a: PDF; Figure_014-b: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Fulltext in PDF: PDF;
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2013-05-22
16:12 |
Search for baryon number violating top quark decays in pp collisions at 8 TeV
/CMS Collaboration
A search for the decay of top quarks that violate baryon number conservation
is performed using pp collisions produced by the LHC at $\sqrt{s}=8$
TeV. The top quark decay signature considered in this analysis
consists of one light lepton (electron or muon), two jets, but no
neutrino in the final state. [...]
CMS-PAS-B2G-12-023.-
Geneva : CERN, 2013
Figure_001-a: PDF; Figure_001-b: PDF; Figure_002: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_003-c: PDF; Figure_003-d: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: PDF; Fulltext in PDF: PDF;
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2013-05-22
16:10 |
Prompt psi(2S) polarization in pp collisions at 7 TeV
/CMS Collaboration
The polarization of prompt $\psi$(2S) mesons is
measured in proton-proton collisions at $\sqrt{s} = 7\,$TeV, using a data sample
of $\psi\mathrm{(2S)} \rightarrow \mu^+\mu^-$ decays collected by the CMS experiment,
corresponding to an integrated luminosity of 4.9$\,$fb$^{-1}$.
The dimuon decay angular distributions are analysed in three different
polarization frames. The prompt $\psi$(2S) polarization parameters $\lambda_\vartheta$,
$\lambda_\varphi$, and $\lambda_{\vartheta\varphi}$, as well as the frame-invariant
$\tilde{\lambda}$, are measured as a function of the $\psi$(2S) transverse
momentum, $p_{\rm T}$, between 14 and 50$\,$GeV, in the rapidity ranges $|y|<0.6$ and $0.6<|y|<1.2$.
No evidence of large transverse or longitudinal polarizations is seen in the
explored kinematic region..
CMS-PAS-BPH-13-003.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004: PDF; Figure_005: PDF; Fulltext in PDF: PDF;
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2013-05-19
22:15 |
Upsilon(1S), Upsilon(2S) and Upsilon(3S) cross section measurements in pp collisions at sqrt(s) = 7 TeV
/CMS Collaboration
The differential cross section as a function of transverse momentum for the production of the $\Upsilon(nS)$ ($n$=1,2,3) states decaying into a pair of muons has been measured in pp collisions at $\sqrt{s}$ = 7 TeV using 4.9 fb$^{-1}$ of data collected by the CMS detector. The analysis selected events with dimuon rapidity $|y(\mu\mu)|< 0.6$, and the measurements cover dimuon transverse momentum in the range $p_T(\mu\mu)=$10-100 GeV. [...]
CMS-PAS-BPH-12-006.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Fulltext in PDF: PDF;
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2013-05-18
10:48 |
Measurement of diffraction dissociation cross sections at sqrt(s)=7 TeV at the LHC
/CMS Collaboration
Results are presented for the single- and double-diffractive cross sections in pp collisions at $\sqrt{s}=7$ TeV at the LHC using the CMS detector. The differential SD cross section is measured as a function of $\xi$, the forward momentum loss of the incoming proton, for $-5.5<\log_{10}\xi<-2.5$. [...]
CMS-PAS-FSQ-12-005.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005: PDF; Figure_006: PDF; Figure_007: PDF; Figure_008: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_010: PDF; Figure_011: PDF; Figure_012: PDF; Figure_013: PDF; Figure_014: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_015-c: PDF; Figure_015-d: PDF; Figure_016: PDF; Fulltext in PDF: PDF;
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2013-05-17
12:28 |
Search for RPV SUSY resonant second generation slepton production in same-sign dimuon events at sqrt(s) = 7 TeV
/CMS Collaboration
A search for resonant production of second generation sleptons ($\tilde{\mu}$,
$\tilde{\nu}_{\mu}$) via the R-parity violating coupling $\lambda'_{211}$,
with two same-sign muons and at least two jets in the final state is
performed. While one muon is expected to be produced directly in the slepton
decay, the second muon and at least two jets are produced in the subsequent
decay of a neutralino or chargino originating from the resonant slepton. [...]
CMS-PAS-SUS-13-005.-
Geneva : CERN, 2013
Figure_001-a: PDF; Figure_001-b: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Fulltext in PDF: PDF;
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2013-05-16
23:14 |
Measurement of the double-differential inclusive jet cross
section at sqrt(s) = 8 TeV with the CMS detector
/CMS Collaboration
% A measurement of the inclusive jet cross section, double-differential in jet transverse momentum $p_\mathrm{T}$ and absolute jet rapidity $|y|$, is presented. Data from LHC proton-proton collisions at $\sqrt{s}=8\TeV$, corresponding to an integrated luminosity of $10.71\,\mathrm{fb}^{-1}$, have been collected with the CMS detector [...]
CMS-PAS-SMP-12-012.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_002-c: PDF; Figure_002-d: PDF; Figure_002-e: PDF; Figure_002-f: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_003-c: PDF; Figure_003-d: PDF; Figure_003-e: PDF; Figure_003-f: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: PDF; Figure_004-e: PDF; Figure_004-f: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_005-c: PDF; Figure_005-d: PDF; Figure_005-e: PDF; Figure_005-f: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Figure_006-d: PDF; Figure_006-e: PDF; Figure_006-f: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_007-c: PDF; Figure_007-d: PDF; Figure_007-e: PDF; Figure_007-f: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_008-c: PDF; Figure_008-d: PDF; Figure_008-e: PDF; Figure_008-f: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_009-c: PDF; Figure_009-d: PDF; Figure_009-e: PDF; Figure_009-f: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_010-c: PDF; Figure_010-d: PDF; Figure_010-e: PDF; Figure_010-f: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_011-c: PDF; Figure_011-d: PDF; Figure_011-e: PDF; Figure_011-f: PDF; Fulltext in PDF: PDF;
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2013-05-16
18:03 |
Higgs to bb in the VBF channel
/CMS Collaboration
A search for the standard model Higgs boson in the vector boson fusion production channel with decay to bottom quarks is reported. A data sample comprising 19.0~fb$^{-1}$ of proton-proton collisions at $\sqrt{s}=8$~TeV collected during the 2012 running period has been analyzed and 95\% Confidence Level upper limits are derived for five mass points from 115 to 135 GeV. [...]
CMS-PAS-HIG-13-011.-
Geneva : CERN, 2013
Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005: PDF; Figure_006: PDF; Figure_007: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_008-c: PDF; Figure_008-d: PDF; Figure_009: PDF; Fulltext in PDF: PDF;
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