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CMS Physics Analysis Summaries

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2016-08-24
23:41
Search for W' to tb in pp collisions at sqrt{s} = 13 TeV /CMS Collaboration
A search is performed for the production of a massive W' boson decaying to a top and a bottom quark. The data analyzed correspond to an integrated luminosity of 2.55~fb$^{-1}$ collected with the CMS detector at the LHC in proton-proton collisions at $\sqrt{s}=13$~TeV. [...]
CMS-PAS-B2G-16-009.- Geneva : CERN, 2016 Figure_001-a: PDF; Figure_001-b: PDF; Figure_001-c: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006: PDF; Fulltext in PDF: PDF;

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2016-08-23
09:42
Search for non-resonant pair production of Higgs bosons in the $\rm{b} \bar{\rm{b}} \rm{b} \bar{\rm{b}}$ final state with 13 TeV CMS data /CMS Collaboration
A search for non-resonant Higgs boson pair production in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$ is presented. The Higgs bosons are searched in the $\rm{b} \bar{\rm{b}}$ final state. [...]
CMS-PAS-HIG-16-026.- Geneva : CERN, 2016 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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2016-08-22
06:49
Search for Charged Higgs boson to ${\rm c\bar{b}}$ in lepton+jets channel using top quark pair events /CMS Collaboration
Results on the search for a light charged Higgs boson ${\rm H^{+}}$ decaying to ${\rm c\bar{b}}$ in top quark pair events using the CMS detector at the LHC are presented. %It is the first search for a charged Higgs boson in this decay mode. [...]
CMS-PAS-HIG-16-030.- Geneva : CERN, 2016 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_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_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: 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_011-c: 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_014-c: PDF; Fulltext in PDF: PDF;

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2016-08-21
17:26
Measurement of the differential cross sections for pairs of Z bosons produced in association with jets in pp collisions at $\sqrt{s} = 8~\mathrm{TeV}$ /CMS Collaboration
This note reports the measurement of the differential cross sections of two Z bosons produced in association with jets in pp collisions at a center-of-mass energy of $\sqrt{s}=8~\mathrm{TeV}$. This analysis is based on a data sample collected with the CMS experiment at the LHC, corresponding to an integrated luminosity of $19.7~\mathrm{fb}^{-1}$. [...]
CMS-PAS-SMP-15-012.- Geneva : CERN, 2016 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; Fulltext in PDF: PDF;

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2016-08-19
22:27
Search for anomalous couplings in semileptonic WW and WZ decays at sqrt(s) = 13 TeV /CMS Collaboration
The increased center of mass energy of the LHC Run II allows for a much larger reach to study possible deviations from the standard model in a generic manner, using an effective field theory approach. In this analysis we constrain additional operators that would lead to anomalous WW$\gamma$ or WWZ couplings by studying events with one W boson decaying to an electron or muon and neutrino and one W or Z boson decaying hadronically. [...]
CMS-PAS-SMP-16-012.- Geneva : CERN, 2016 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_003-d: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Fulltext in PDF: PDF;

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2016-08-15
12:26
Search for H(bb)H(gammagamma) decays at 13TeV /CMS Collaboration
The search for the production of a pair of Higgs bosons, in the final states containing two photons and two bottom quarks, is presented. Both resonant and nonresonant production mechanisms of the Higgs bosons are investigated. [...]
CMS-PAS-HIG-16-032.- Geneva : CERN, 2016 Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: 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; 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_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: PDF; Fulltext in PDF: PDF;

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2016-08-10
12:12
The potential to study exotic physics signatures at HL-LHC using the phase 2 upgraded CMS detector /CMS Collaboration
The high luminosity LHC (HL-LHC) run, which is due to start in 2025, is expected to collect an integrated luminosity of approximately 3000~fb$^{-1}$ at $\sqrt{s}=14$\TeV. The discovery and study of physics beyond the standard model will remain one of the major goals of the CMS collaboration during this period. [...]
CMS-PAS-EXO-14-007.- Geneva : CERN, 2016 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_004-c: PDF; Figure_004-d: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_005-c: PDF; Figure_006: 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_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: PDF; Figure_014: PDF; Figure_015: PDF; Figure_016: PDF; Figure_017-a: PDF; Figure_017-b: PDF; Figure_018: PDF; Figure_019-a: PDF; Figure_019-b: PDF; Figure_019-c: PDF; Figure_020-a: PDF; Figure_020-b: 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; Figure_023-a: PDF; Figure_023-b: PDF; Figure_024: PDF; Figure_025-a: PDF; Figure_025-b: PDF; Figure_026-a: PDF; Figure_026-b: PDF; Figure_026-c: PDF; Figure_026-d: PDF; Figure_027: PDF; Figure_028-a: PDF; Figure_028-b: PDF; Figure_029-a: PDF; Figure_029-b: PDF; Fulltext in PDF: PDF;

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2016-08-08
04:47
Search for new resonances decaying to $\mathrm{WW}/\mathrm{WZ} \to \ell\nu \mathrm{qq}$ /CMS Collaboration
A search for massive narrow resonances decaying to pairs of W and Z bosons in the $\ell\nu\mathrm{qq}$ final state is presented, based on $12.9~\mathrm{fb}^{-1}$ of pp collision data collected in 2016 by the CMS experiment at the CERN LHC with a center-of-mass energy of $13~\mathrm{TeV}$. Spin-1 and spin-2 resonances corresponding to masses in the range $600-4500~\mathrm{GeV}$ and decaying to WW/WZ are probed using the $\ell\nu\mathrm{qq}$ final state. [...]
CMS-PAS-B2G-16-020.- Geneva : CERN, 2016 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_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: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_009: PDF; Fulltext in PDF: PDF;

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2016-08-06
18:59
Search for new physics in the compressed mass spectra scenario using events with two soft opposite-sign leptons and missing momentum energy at 13 TeV /CMS Collaboration
A search for new physics in events with two low-momentum opposite-sign leptons and missing transverse momentum is presented using $12.9~\mathrm{fb}^{-1}$ of data collected at $13~\mathrm{TeV}$ in 2016. The observed data yields are compatible with the predictions for standard model processes. [...]
CMS-PAS-SUS-16-025.- Geneva : CERN, 2016 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_003-a: PDF; Figure_003-b: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Fulltext in PDF: PDF;

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2016-08-05
15:48
Search for Higgs boson pair production in the $\mathrm{b}\overline{\mathrm{b}} \mathrm{l}\nu \mathrm{l}\nu$ final state at $\sqrt{s} = 13~\mathrm{TeV}$ /CMS Collaboration
A search for pair-produced Higgs bosons decaying respectively into $\mathrm{b}\overline{\mathrm{b}}$ and $\mathrm{V}\mathrm{V}$ (with $\mathrm{V}$ either a $\mathrm{W}$ or a $\mathrm{Z}$ boson), with subsequent $\mathrm{V}\mathrm{V}$ decays into two leptons and two neutrinos, is presented. The analysis is based on a sample of proton-proton collisions at $\sqrt{s} = 13~\mathrm{TeV}$ at the LHC corresponding to an integrated luminosity of $2.30~\mathrm{fb}^{-1}$. [...]
CMS-PAS-HIG-16-024.- Geneva : CERN, 2016 Figure_001-a: PDF; Figure_001-b: PDF; Figure_001-c: PDF; Figure_001-d: PDF; Figure_001-e: 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; Figure_006-a: PDF; Figure_006-b: PDF; Fulltext in PDF: PDF;

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