2015-03-04
17:21 |
Search for Associated Production of a Single Top Quark and a Higgs Boson in Leptonic Channels
/CMS Collaboration
A search for the production of a Higgs boson in association with a single top quark is presented, focusing on leptonic signatures provided by the $\mathrm{H}\rightarrow\mathrm{W}\mathrm{W}$ and $\mathrm{H}\rightarrow\tau\tau$ decay modes.
Due to a strong interference of the two main contributing diagrams, the production cross section of this process benefits from a substantial enhancement in the case of negative values of the top-Higgs coupling, $C_{\mathrm{t}}$.
The analysis exploits signatures with two same-sign and three leptons in the final state, and uses the full data sample collected with the CMS detector at the LHC at a center of mass energy of 8~TeV, which corresponds to an integrated luminosity of $19.7 \pm 0.5\,\mathrm{fb}^{-1}$.
Multivariate techniques are used to discriminate the signal from the dominant backgrounds.
The analysis yields a 95\% confidence level upper limit on the single top quark plus Higgs boson production cross section of 6.7 times the expectation for $C_{\mathrm{t}}$~=~-1, with an expected limit of 5.0..
CMS-PAS-HIG-14-026.-
Geneva : CERN, 2015
Figure_001-a: PDF; Figure_001-b: 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_002-g: PDF; Figure_002-h: 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_003-g: PDF; Figure_003-h: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: PDF; Figure_004-e: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_005-c: PDF; Figure_006: PDF; Fulltext in PDF: PDF;
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2015-02-27
17:00 |
Search for long-lived particles decaying to final states that include dileptons
/CMS Collaboration
A search has been performed for long-lived particles, which decay to a final state that includes a pair of leptons ($e^+e^-$ or $\mu^+\mu^-$).
The experimental signature is a distinctive topology consisting of a pair of charged leptons originating from a displaced secondary vertex. Events were collected by the CMS detector at the LHC during pp collisions at $\sqrt{s} = 8$~TeV, and selected from data samples corresponding to 19.6 (20.5)~fb$^{-1}$ of integrated luminosity in the electron (muon) channel. [...]
CMS-PAS-EXO-12-037.-
Geneva : CERN, 2014
Figure_001-a: PDF; Figure_001-b: 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-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_009-a: PDF; Figure_009-b: 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; Fulltext in PDF: PDF;
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2015-01-27
14:42 |
Search for new physics in final states with low transverse energy photon and missing transverse energy
/CMS Collaboration
We present a search for new physics in the final state of a low transverse energy photon and missing transverse energy using 7.3 $fb^{-1}$ of $\sqrt{s} = 8$ TeV LHC proton-proton collisions collected with the Compact Muon Solenoid (CMS) detector. This analysis extends the high-energy single-photon searches to a lower-energy regime. [...]
CMS-PAS-HIG-14-024.-
Geneva : CERN, 2015
Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003: PDF; Figure_004-a: PDF; Figure_004-b: PDF; 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; Fulltext in PDF: PDF;
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2015-01-27
12:41 |
Jet-track correlations in PbPb collisions at 2.76 TeV
/CMS Collaboration
Medium-induced changes to charged particle correlations associated with high momentum jets in PbPb collisions are explored by comparing such measurements to pp reference data. This jet-track correlation analysis uses data sets from PbPb and pp collisions with integrated luminosities of 166 $\mu \rm{b}^{-1}$ and 5.3 pb$^{-1}$, respectively, collected in 2011 and 2013 at collision energies of $\sqrt{s_{NN}} = 2.76$~TeV. [...]
CMS-PAS-HIN-14-016.-
Geneva : CERN, 2015
Figure_001: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004: PDF; Figure_005: PDF; Figure_006: PDF; Figure_007: PDF; Figure_008: PDF; Figure_009: PDF; Figure_010: PDF; Figure_011: PDF; Figure_012: PDF; Fulltext in PDF: PDF;
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2015-01-15
07:34 |
Supersymmetry discovery potential in future LHC and HL-LHC running with the CMS detector
/CMS Collaboration
The search for supersymmetry (SUSY) is a major goal of the LHC
physics program. The number of SUSY scenarios is large, and both high
luminosity data samples and the full set of CMS detector capabilities
are required to provide sensitivity to the broad range of signatures, cross sections, and decay branching fractions that can arise. [...]
CMS-PAS-SUS-14-012.-
Geneva : CERN, 2015
Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_002-c: PDF; Figure_002-d: PDF; Figure_002-e: 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_010: 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_013-c: PDF; Figure_014-a: PDF; Figure_014-b: PDF; Figure_014-c: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_016: PDF; Figure_017-a: PDF; Figure_017-b: PDF; Figure_018-a: PDF; Figure_018-b: PDF; Figure_019-a: PDF; Figure_019-b: PDF; Figure_020-a: PDF; Figure_020-b: PDF; Figure_021-a: PDF; Figure_021-b: PDF; Figure_022-a: PDF; Figure_022-b: PDF; Figure_023: PDF; Figure_024-a: PDF; Figure_024-b: PDF; Fulltext in PDF: PDF;
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2015-01-14
12:31 |
Z' to tau tau - emu final state
/CMS Collaboration
A search for new physics beyond the standard model in the high-mass ditau final state with one tau decaying in the electron channel and one tau decaying in the muon channel is performed using proton-proton collisions at $\sqrt{s}$ = 8 TeV recorded by the CMS experiment at the LHC. The data correspond to an integrated luminosity of 19.7 fb$^{-1}$. [...]
CMS-PAS-EXO-12-046.-
Geneva : CERN, 2015
Figure_001: PDF; Figure_002: PDF; Figure_003: PDF; Fulltext in PDF: PDF;
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2015-01-13
22:17 |
Search for Neutral Octo-triplet Particles in the Z+jets Channel in pp Collisions at sqrt{s} = 8 TeV
/CMS Collaboration
A search for pair production of neutral color-octet weak-triplet scalar particles ($\Theta^{0}$) is performed in processes where one $\Theta^{0}$ decays to a pair of b-quark jets and the other to a Z boson plus a jet, with the Z boson decaying to a pair of electrons or muons.
The search is performed with data collected by the CMS detector at the LHC corresponding to an integrated luminosity of 19.7${fb}^{-1}$ of proton-proton collisions at $\sqrt{s}$ = 8TeV.
The number of observed events is found to be in agreement with the standard model prediction.
The 95\% confidence level upper limit on the cross section times branching fraction, relative to the theoretical expectation, is obtained as a function of $\Theta^{0}$ mass. The 95\% confidence level lower bounds on the $\Theta^{0}$ mass are found to be 623 and 426GeV, for two different octo-triplet benchmark scenarios.
This is the first direct experimental bound on the $\Theta^{0}$ production model..
CMS-PAS-EXO-12-007.-
Geneva : CERN, 2014
Figure_001-a: PDF; Figure_001-b: PDF; Figure_002: PDF; Figure_003-a: PNG; Figure_003-b: PNG; Figure_004-a: PNG; Figure_004-b: PNG; Figure_005-a: PNG; Figure_005-b: PNG; Figure_006-a: PNG; Figure_006-b: PNG; Figure_006-c: PNG; Figure_006-d: PNG; Figure_007-a: PNG; Figure_007-b: PNG; Figure_008-a: PNG; Figure_008-b: PNG; Figure_009: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Fulltext in PDF: PDF;
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2014-12-11
23:12 |
Search for vector-like quarks in final states with a single lepton and jets in pp collisions at sqrt s = 8 TeV
/CMS Collaboration
A search is presented for the pair production of vector-like quarks, $\mathrm{T\bar{T}}$, coupled to $\mathrm{b}$-quarks, and $\mathrm{Q\bar{Q}}$ coupled to light quarks, in proton-proton collisions at $\sqrt{s} = 8$ TeV at the Large Hadron Collider, LHC. The data were collected by the CMS experiment during the 2012 LHC run, and correspond to an integrated luminosity of 19.7 fb$^{-1}$. [...]
CMS-PAS-B2G-12-017.-
Geneva : CERN, 2014
Figure_001-a: PNG; Figure_001-b: PNG; 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-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Fulltext in PDF: PDF;
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2014-11-22
18:35 |
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2014-11-15
19:37 |
Search for a pseudoscalar boson A decaying into a Z and an h boson in the llbb final state
/CMS Collaboration
A search for an extended Higgs sector is carried out in the decay chain of a pseudoscalar heavy Higgs boson A into a Z boson and a light Higgs boson h, with the Z decaying into a pair of leptons (electrons or muons) and the h into a pair of b-quarks. The light boson h is assumed to be the recently discovered standard model-like Higgs boson with a $125\,\text{GeV}$ mass. [...]
CMS-PAS-HIG-14-011.-
Geneva : CERN, 2014
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_003-e: PDF; Figure_003-f: PDF; Figure_004: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Fulltext in PDF: PDF;
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