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CMS Physics Analysis Summaries

Ostatnio dodane:
2018-06-19
19:06
Search for the rare decays of Z bosons and Higgs bosons to $\mathrm{J/}\psi$ plus photon at $\sqrt{s}=13~\mathrm{TeV}$ /CMS Collaboration
A search for decays of $\mathrm{Z}$ and Higgs bosons to $\mathrm{J/}\psi$ and a photon, with the subsequent decay of the $\mathrm{J/}\psi$ to $\mu^{+}\mu^{-}$, in proton-proton ($\mathrm{pp}$) collisions at a center-of-mass energy ($\sqrt{s}$) of $13~\mathrm{TeV}$, is presented. The analysis uses a data sample corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$ collected with the CMS detector at the LHC in 2016. [...]
CMS-PAS-SMP-17-012.- Geneva : CERN, 2018 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-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-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Figure_006-d: PDF; Fulltext in PDF: PDF;

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2018-06-06
12:00
Measurements of differential cross sections for $\mathrm{t \bar t}$ production in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$ using events containing two leptons /CMS Collaboration
Measurements are presented of differential top quark pair ($\mathrm{t \bar t}$) production cross sections using events containing two leptons produced in proton-proton collisions at a centre-of-mass energy of 13 TeV. The data were recorded by the CMS experiment at the CERN LHC in 2016 and correspond to an integrated luminosity of $35.9~\mathrm{fb^{-1}}$. [...]
CMS-PAS-TOP-17-014.- Geneva : CERN, 2018 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_002-c: PDF; Figure_002-d: PDF; Figure_002-e: 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_005-a: PDF; Figure_005-b: PDF; Figure_005-c: PDF; Figure_005-d: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_007-c: PDF; Figure_007-d: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_008-c: PDF; Figure_008-d: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_009-c: PDF; Figure_009-d: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_010-c: PDF; Figure_010-d: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_011-c: PDF; Figure_011-d: PDF; Figure_012-a: PDF; Figure_012-b: PDF; Figure_013-a: PDF; Figure_013-b: PDF; Figure_013-c: PDF; Figure_013-d: PDF; Figure_014-a: PDF; Figure_014-b: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_015-c: PDF; Figure_015-d: PDF; Figure_016-a: PDF; Figure_016-b: PDF; Figure_016-c: PDF; Figure_016-d: PDF; Figure_017-a: PDF; Figure_017-b: PDF; Figure_017-c: PDF; Figure_017-d: PDF; Figure_018-a: PDF; Figure_018-b: PDF; Figure_019-a: PDF; Figure_019-b: PDF; Figure_019-c: PDF; Figure_019-d: PDF; Figure_020-a: PDF; Figure_020-b: PDF; Figure_020-c: PDF; Figure_020-d: PDF; Figure_021-a: PDF; Figure_021-b: PDF; Figure_022-a: PDF; Figure_022-b: PDF; Figure_022-c: PDF; Figure_022-d: PDF; Figure_023-a: PDF; Figure_023-b: PDF; Figure_024-a: PDF; Figure_024-b: PDF; Figure_024-c: PDF; Figure_024-d: PDF; Figure_025-a: PDF; Figure_025-b: PDF; Figure_026-a: PDF; Figure_026-b: PDF; Figure_027-a: PDF; Figure_027-b: PDF; Figure_028-a: PDF; Figure_028-b: PDF; Figure_029-a: PDF; Figure_029-b: PDF; Figure_030-a: PDF; Figure_030-b: PDF; Figure_031-a: PDF; Figure_031-b: PDF; Figure_032-a: PDF; Figure_032-b: PDF; Figure_033-a: PDF; Figure_033-b: PDF; Figure_034-a: PDF; Figure_034-b: PDF; Figure_035-a: PDF; Figure_035-b: PDF; Figure_036-a: PDF; Figure_036-b: PDF; Figure_037-a: PDF; Figure_037-b: PDF; Figure_038-a: PDF; Figure_038-b: PDF; Figure_039-a: PDF; Figure_039-b: PDF; Figure_040-a: PDF; Figure_040-b: PDF; Figure_041-a: PDF; Figure_041-b: PDF; Figure_042-a: PDF; Figure_042-b: PDF; Figure_043-a: PDF; Figure_043-b: PDF; Figure_044-a: PDF; Figure_044-b: PDF; Figure_045: PDF; Figure_046: PDF; Figure_047-a: PDF; Figure_047-b: PDF; Figure_048: PDF; Fulltext in PDF: PDF;

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2018-06-06
10:09
CMS luminosity measurement for the 2017 data-taking period at $\sqrt{s} = 13~\mathrm{TeV}$ /CMS Collaboration
The calibration for the luminosity measurement by the CMS experiment for the 2017 proton-proton LHC run at $\sqrt{s} = 13~\mathrm{TeV}$ is described. The principal calibration is derived from the analysis of the van der Meer scan program in CMS taken during LHC fill 6016. [...]
CMS-PAS-LUM-17-004.- Geneva : CERN, 2018 Figure_001-a: PDF; Figure_001-b: PDF; Figure_002: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_008: PDF; Figure_009: PNG; Figure_010-a: PNG; Figure_010-b: PNG; Figure_011-a: PNG; Figure_011-b: PNG; Figure_012-a: PNG; Figure_012-b: PNG; Figure_013-a: PNG; Figure_013-b: PNG; Figure_014-a: PNG; Figure_014-b: PNG; Fulltext in PDF: PDF;

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2018-06-05
00:15
Search for resonant $\mathrm{t\bar{t}}$ production in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$ /CMS Collaboration
A search for a heavy resonance decaying into top quark and antiquark $(\mathrm{t\bar{t}})$ pairs is performed using proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$. The search uses the full data set collected with the CMS detector in 2016, which corresponds to an integrated luminosity of $36~\mathrm{fb}^{-1}$. [...]
CMS-PAS-B2G-17-017.- Geneva : CERN, 2018 Figure_001-a: PDF; Figure_001-b: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_002-c: 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_005-c: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Figure_006-d: PDF; Figure_007: 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_010-a: PDF; Figure_010-b: PDF; Figure_010-c: PDF; Figure_010-d: 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; Figure_012: PDF; Figure_013-a: PDF; Figure_013-b: PDF; Figure_013-c: PDF; Figure_013-d: PDF; Fulltext in PDF: PDF;

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2018-06-04
18:39
Observation of the $\mathrm{B}^{*}_{\mathrm{s}2}(5840)^0\rightarrow\mathrm{B}^0\mathrm{K}^0_{\mathrm\scriptscriptstyle S}$ decay and studies of excited $\mathrm{B}^0_\mathrm{s}$ mesons in proton-proton collisions at $\sqrt{s}=8\,\mathrm{TeV}$ /CMS Collaboration
The observation of the $\mathrm{B}^{*}_{\mathrm{s}2}(5840)^0\rightarrow\mathrm{B}^0\mathrm{K}^0_{\mathrm\scriptscriptstyle S}$ decay is presented and a measurement of its relative branching fraction to the $\mathrm{B}^{*}_{\mathrm{s}2}(5840)^0\rightarrow\mathrm{B}^+\mathrm{K}^{-}$ decay using a data sample of $19.6\,\mathrm{fb}^{-1}$ collected with the CMS detector in proton-proton collision at the centre-of-mass energy $8\,\mathrm{TeV}$. The analysis is performed by studying P-wave $\mathrm{B}^{0}_\mathrm{s}$ meson decays into $\mathrm{B}^+\mathrm{K}^-$ and $\mathrm{B}^0 \mathrm{K}^0_{\mathrm\scriptscriptstyle S}$ states, where the ground-state $\mathrm{B}$ mesons are identified using the decays $\mathrm{B}^+ \rightarrow \mathrm{J}/\psi\mathrm{K}^+$ and $\mathrm{B}^0 \rightarrow \mathrm{J}/\psi\mathrm{K}^+ \pi^-$. [...]
CMS-PAS-BPH-16-003.- Geneva : CERN, 2018 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_005-c: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Fulltext in PDF: PDF;

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2018-06-04
18:39
Search for resonant production of second generation sleptons with same-sign dimuon events in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$ /CMS Collaboration
A search for resonant production of second generation sleptons ($\tilde{\mu}$, $\tilde{\nu}_{\mu}$) via the R-parity-violating coupling $\lambda'_{211}$, in events with two same-sign muons and at least two jets in the final state is presented. 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-17-008.- Geneva : CERN, 2018 Figure_001: PDF; Figure_002: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: PDF; Figure_005: PDF; Fulltext in PDF: PDF;

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2018-06-04
16:22
Search for the standard model Higgs boson decaying to a pair of $\tau$ leptons and produced in association with a W or a Z boson in proton-proton collisions at $\sqrt{s}=13$ TeV /CMS Collaboration
A search for the standard model Higgs boson produced in association with a W or a Z boson decaying leptonically is performed using a data sample of proton-proton collisions collected at $\sqrt{s} = 13$ TeV by the CMS experiment at the LHC corresponding to an integrated luminosity of 35.9 fb$^{-1}$. The Higgs boson is sought in its decay to a pair of $\tau$ leptons. [...]
CMS-PAS-HIG-18-007.- Geneva : CERN, 1900 Figure_001-a: PDF; Figure_001-b: PDF; Figure_001-c: PDF; Figure_001-d: PDF; Figure_002: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_003-c: PDF; Figure_003-d: PDF; Figure_004: PDF; Figure_005: PDF; Figure_006: PDF; Figure_007: PDF; Fulltext in PDF: PDF;

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2018-06-04
16:08
Search for narrow H-gamma resonances in proton-proton collisions at sqrt(s) = 13 TeV /CMS Collaboration
A search for heavy, narrow-width resonances decaying to a Higgs boson and a photon has been performed in proton-proton collision data corresponding to an integrated luminosity of 35.9 inverse femtobarns, collected with the CMS detector at the LHC at a center-of-mass energy of 13 TeV in 2016. Events in which a photon and a Lorentz-boosted Higgs boson that decays hadronically and reconstructed as a single, large-radius jet are considered, and the photon+jet invariant mass spectrum is analyzed to look for the presence of narrow-width resonances. [...]
CMS-PAS-EXO-17-019.- Geneva : CERN, 2018 Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_003-c: PDF; Fulltext in PDF: PDF;

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2018-06-04
15:13
Search for resonant and non-resonant production of Higgs boson pairs in the four b quark final state using boosted jets in proton-proton collisions at sqrt(s)=13 TeV /CMS Collaboration
A search is presented for the pair production of the standard model Higgs boson using data from proton-proton collisions at a centre-of-mass energy of $13~\text{TeV}$, collected by the CMS experiment at the CERN LHC in 2016, and corresponding to an integrated luminosity of $35.9~\text{fb}^{-1}$. The final state consists of two b quark-antiquark pairs, with at least one Higgs boson highly Lorentz-boosted and reconstructed as a single large-area jet. [...]
CMS-PAS-B2G-17-019.- Geneva : CERN, 2018 Figure_001-a: PDF; Figure_001-b: PDF; Figure_001-c: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_002-c: PDF; Figure_002-d: 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_005: PDF; Fulltext in PDF: PDF;

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2018-06-04
15:12
Search for a W' boson decaying to a $\tau$ lepton and a neutrino in proton-proton collisions at $\sqrt{s}$ = 13 TeV /CMS Collaboration
A search for new high-mass resonances decaying to a tau lepton and a neutrino is reported. The analysis uses proton-proton collision data collected by the CMS experiment at the LHC at $\sqrt{s}=13~\mathrm{TeV}$, corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$. [...]
CMS-PAS-EXO-17-008.- Geneva : CERN, 2018 Figure_001: PDF; Figure_002: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004: PDF; Figure_005: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007: PDF; Fulltext in PDF: PDF;

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