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CMS Physics Analysis Summaries

Letzte Einträge:
2018-07-07
19:12
Measurement of electroweak WZ production and search for new physics in pp collisions at sqrt(s) = 13 TeV /CMS Collaboration
A measurement of WZ electroweak vector boson scattering is presented. The analysis is based on a data sample of proton--proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$ collected with the CMS detector and corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$. [...]
CMS-PAS-SMP-18-001.- 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: PDF; Figure_004: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007: PDF; Figure_008: PDF; Fulltext in PDF: PDF;

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2018-07-06
13:30
Search for excited leptons in the $\ell\ell\gamma$ final state in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$ /CMS Collaboration
A search is presented for excited electrons and muons using a data sample of proton-proton collisions at a center-of-mass energy of $\sqrt{s}=13~\mathrm{TeV}$, collected with the CMS detector in 2016 and corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$. This is the first search in the $\ell\ell\gamma$ final state in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$. [...]
CMS-PAS-EXO-18-004.- 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_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: PDF; Fulltext in PDF: PDF;

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2018-07-05
21:12
Measurements of the $\mathrm{pp}\to\mathrm{WZ}$ inclusive and differential production cross section and constraints on charged anomalous triple gauge couplings at $\sqrt{s} = 13~\mathrm{TeV}$. /CMS Collaboration
The $\mathrm{WZ}$ production cross section is measured in proton-proton collisions using $35.9~\mathrm{fb}^{-1}$ of data collected with the CMS detector. An estimate of the inclusive cross section yields a result of $\sigma_{\textrm{tot}}(\mathrm{pp} \rightarrow \mathrm{WZ}) = 48.09 \textrm{ }^{+1.00}_{-0.96}~(\mathrm{stat}) \textrm{ }^{+0.44}_{-0.37}~(\textrm{theo}) \textrm{ }^{+2.39}_{-2.17}~(\mathrm{syst}) \pm 1.39~(\textrm{lumi})~\mathrm{pb}$, for a total uncertainty of $-2.78$ and $+2.98~\mathrm{pb}$. [...]
CMS-PAS-SMP-18-002.- 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_004-c: PDF; Figure_004-d: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_005-c: PDF; Figure_005-d: PDF; Figure_006: PDF; Figure_007: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_008-c: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_009-c: 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_013-a: PDF; Figure_013-b: PDF; Figure_014-a: PDF; Figure_014-b: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_016-a: PDF; Figure_016-b: PDF; Figure_016-c: PDF; Figure_017-a: PDF; Figure_017-b: PDF; Figure_017-c: PDF; Fulltext in PDF: PDF;

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2018-07-05
20:49
Combined measurement and interpretation of differential Higgs boson production cross sections at $\sqrt{s}$=13 TeV /CMS Collaboration
The differential Higgs boson production cross sections are sensitive probes for new physics beyond the standard model. In particular, new physics may contribute in the gluon-gluon fusion loop, the dominant Higgs boson production mechanism at the LHC, and manifest itself as deviations from the expected standard model distributions. [...]
CMS-PAS-HIG-17-028.- Geneva : CERN, 2018 Figure_001-a: PDF; Figure_001-b: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003: PDF; Figure_004: PDF; Figure_005: 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: PDF; Figure_013: PDF; Figure_014: PDF; Fulltext in PDF: PDF;

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2018-07-05
20:49
Search for low mass resonances decaying into bottom quark-antiquark pairs in pp collisions at $\sqrt{s} = 13~\mathrm{TeV}$ /CMS Collaboration
A search for narrow scalar resonances decaying to bottom quark-antiquark pairs is presented. The search is based on events collected in $\sqrt{s}=13~\mathrm{TeV}$ proton-proton collisions with the CMS detector at the CERN LHC. [...]
CMS-PAS-EXO-17-024.- 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_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_006-a: PDF; Figure_006-b: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Fulltext in PDF: PDF;

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2018-07-05
17:32
Search for the associated production of a Higgs boson and a single top quark in pp collisions at $\sqrt{s} = 13\,\mathrm{TeV}$ /CMS Collaboration
A search for the production of Higgs boson in association with a single top quark is presented, based on data collected in 2016 with the CMS detector at the LHC at a center of mass energy of $13~\mathrm{TeV}$, which corresponds to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$. The production cross section of this process is highly sensitive to the absolute values of the modifiers of the top quark-Higgs boson coupling, $\kappa_{\mathrm{t}}$, and the coupling of vector bosons to the Higgs boson, $\kappa_{\mathrm{V}}$, as well as their relative signs with respect to the standard model. [...]
CMS-PAS-HIG-18-009.- Geneva : CERN, 2018 Figure_001-a: PDF; Figure_001-b: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004: PDF; Fulltext in PDF: PDF;

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2018-07-05
16:43
Search for a vector-like quark decaying to a top quark and a W boson /CMS Collaboration
A search is presented for single production of vector-like quarks (VLQs) in proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$ recorded with the CMS experiment at the LHC. The analyzed data sample corresponds to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$. [...]
CMS-PAS-B2G-17-018.- 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_003-c: PDF; Figure_003-d: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: 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_006-c: PDF; Figure_006-d: 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; Fulltext in PDF: PDF;

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2018-07-05
16:41
Search for a heavy resonance decaying to a top quark and a vector-like top quark in the lepton+jets final state /CMS Collaboration
A search is presented for a heavy spin-1 resonance $\mathrm{Z}^\prime$ decaying to a top quark and a vector-like top quark T in the lepton+jets final state. The search is performed using a data set of proton-proton collisions at a centre-of-mass energy of $13~\mathrm{TeV}$ corresponding to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$ as recorded by the CMS experiment at the CERN LHC in the year 2016. [...]
CMS-PAS-B2G-17-015.- Geneva : CERN, 2018 Figure_001: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: 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_008-a: PDF; Figure_008-b: PDF; Figure_009: PDF; Fulltext in PDF: PDF;

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2018-07-05
16:40
CMS luminosity measurement using 2016 proton-nucleus collisions at nucleon-nucleon center-of-mass energy of 8.16 TeV /CMS Collaboration
The calibration of the integrated luminosity delivered to the CMS experiment during the 2016 lead-proton (Pbp) and proton-lead (pPb) periods at $\sqrt{s_{\rm{NN}}}=8.16\ {\rm TeV}$ is presented. Three different subdetectors are used: the forward hadronic calorimeter, the pixel luminosity telescope, and the silicon tracker. [...]
CMS-PAS-LUM-17-002.- 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_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Figure_006-d: 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_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_014-a: PDF; Figure_014-b: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_016-a: PDF; Figure_016-b: PDF; Figure_017-a: PNG; Figure_017-b: PNG; Fulltext in PDF: PDF;

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2018-07-05
12:55
Performance of missing transverse momentum in pp collisions at sqrt(s)=13 TeV using the CMS detector /CMS Collaboration
The performance of algorithms for the reconstruction of missing transverse momentum for data from proton-proton collisions with a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC is presented. The data sample corresponds to an integrated luminosity of 35.9 fb$^{-1}$. [...]
CMS-PAS-JME-17-001.- Geneva : CERN, 2018 Figure_001-a: PDF; Figure_001-b: PDF; Figure_002: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004: PNG; Figure_005-a: PNG; Figure_005-b: PNG; Figure_006: PDF; Figure_007-a: PNG; Figure_007-b: PNG; Figure_008-a: PDF; Figure_008-b: PDF; Figure_008-c: 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: 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-a: PDF; Figure_012-b: PDF; Figure_013-a: PDF; Figure_013-b: PDF; Figure_013-c: PDF; Figure_013-d: PDF; Figure_014: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_016-a: PDF; Figure_016-b: 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_018-c: PDF; Figure_018-d: PDF; Figure_019-a: PDF; Figure_019-b: 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_021-c: PDF; Figure_021-d: PDF; Figure_022-a: PDF; Figure_022-b: PDF; Fulltext in PDF: PDF;

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