2018-07-17
17:32 |
Search for a W' boson decaying to a vector-like quark and a top or bottom quark in the all-jets final state
/CMS Collaboration
A search for a heavy ${\mathrm{W}^\prime}$ resonance decaying to one ${\mathrm{B}}$ or ${\mathrm{T}}$ vector-like quark and either a top or bottom quark, respectively, is presented using proton-proton collision data collected in 2016 by the CMS detector at the LHC. Both decay channels result in a top quark, Higgs boson, and a b quark, each produced with significant energy. [...]
CMS-PAS-B2G-18-001.-
Geneva : CERN, 2018
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_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; Fulltext in PDF: PDF;
|
詳細記錄 - 相似記錄
|
2018-07-07
19:12 |
詳細記錄 - 相似記錄
|
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;
|
詳細記錄 - 相似記錄
|
2018-07-05
21:12 |
詳細記錄 - 相似記錄
|
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;
|
詳細記錄 - 相似記錄
|
2018-07-05
20:49 |
詳細記錄 - 相似記錄
|
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;
|
詳細記錄 - 相似記錄
|
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;
|
詳細記錄 - 相似記錄
|
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;
|
詳細記錄 - 相似記錄
|
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;
|
詳細記錄 - 相似記錄
|