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CMS Physics Analysis Summaries

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2018-11-17
06:40
Search for invisible decays of a Higgs boson produced through vector boson fusion at the High-Luminosity LHC /CMS Collaboration
The search for a Higgs boson decaying to invisible particles, produced through the vector boson fusion mode in the High-Luminosity LHC proton-proton collisions at $\sqrt{s}=14~\mathrm{TeV}$, is investigated based on simulation studies using Delphes, a fast-simulation package used to provide a parameterised response of the upgraded CMS detector. The event selection follows the existing CMS Run II data analysis, optimised for the High-Luminosity LHC conditions. [...]
CMS-PAS-FTR-18-016.- 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; Fulltext in PDF: PDF;

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2018-11-17
06:40
Sensitivity projections for Higgs boson properties measurements at the HL-LHC /CMS Collaboration
The expected sensitivities of Higgs boson measurements at the High-Luminosity LHC with integrated luminosities of up to $3000\,\text{fb}^{-1}$ are presented. These are determined by the extrapolation of analyses of $13\,\text{TeV}$ collision data, amounting to $35.9\,\text{fb}^{-1}$, collected during Run 2 of the LHC. [...]
CMS-PAS-FTR-18-011.- 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_006-a: PDF; Figure_006-b: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_008: PDF; Figure_009-a: PDF; Figure_009-b: 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_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_018-a: PDF; Figure_018-b: PDF; Figure_018-c: PDF; Figure_018-d: PDF; Figure_018-e: PDF; Figure_018-f: PDF; Figure_019-a: PDF; Figure_019-b: PDF; Figure_019-c: PDF; Figure_019-d: PDF; Figure_019-e: PDF; Figure_019-f: PDF; Figure_020-a: PDF; Figure_020-b: PDF; Figure_020-c: PDF; Figure_020-d: PDF; Figure_020-e: PDF; Figure_021-a: PDF; Figure_021-b: PDF; Figure_021-c: PDF; Figure_021-d: PDF; Figure_021-e: PDF; Figure_022-a: PDF; Figure_022-b: PDF; Figure_022-c: PDF; Figure_022-d: PDF; Figure_022-e: PDF; Figure_022-f: PDF; Figure_022-g: PDF; Figure_022-h: PDF; Figure_023-a: PDF; Figure_023-b: PDF; Figure_023-c: PDF; Figure_023-d: PDF; Figure_023-e: PDF; Figure_023-f: PDF; Figure_023-g: PDF; Figure_023-h: PDF; Figure_024-a: PDF; Figure_024-b: PDF; Figure_025-a: PDF; Figure_025-b: PDF; Figure_025-c: PDF; Figure_025-d: PDF; Figure_025-e: PDF; Figure_025-f: PDF; Figure_025-g: PDF; Figure_025-h: PDF; Figure_026-a: PDF; Figure_026-b: PDF; Figure_026-c: PDF; Figure_026-d: PDF; Figure_026-e: PDF; Figure_026-f: PDF; Figure_026-g: PDF; Figure_026-h: PDF; Figure_027-a: PDF; Figure_027-b: PDF; Figure_028-a: PDF; Figure_028-b: PDF; Fulltext in PDF: PDF;

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2018-11-13
23:52
Study of W$^\pm$W$^\pm$ production via vector boson scattering at the HL-LHC with the upgraded CMS detector /CMS Collaboration
The prospects for the study of W$^\pm$W$^\pm {\text{jj}}$ final states, produced in proton-proton collisions at centre-of-mass energy of 14 TeV via vector boson scattering (VBS), with the upgraded CMS detector at the High-Luminosity LHC (HL-LHC) are presented. The W bosons are detected via their leptonic decays: W$\rightarrow e\nu$ or $\mu\nu$. [...]
CMS-PAS-FTR-18-005.- Geneva : CERN, 2018 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_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007: PDF; Fulltext in PDF: PDF;

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2018-11-07
11:26
An embedding technique to determine genuine $\tau\tau$ backgrounds from CMS data /CMS Collaboration
The embedding technique allows an estimation of the genuine $\tau\tau$ standard model backgrounds from data, with minimal simulation input. In the data, the muons are removed from reconstructed $\mu\mu$ events and replaced with simulated tau leptons with the same kinematic properties. [...]
CMS-PAS-TAU-18-001.- Geneva : CERN, 2018 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_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_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-a: PDF; Figure_009-b: PDF; Figure_009-c: PDF; Figure_009-d: PDF; Figure_009-e: PDF; Figure_009-f: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_010-c: PDF; Figure_010-d: PDF; Figure_010-e: PDF; Figure_010-f: 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_012-c: PDF; Figure_012-d: 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_016-a: PDF; Figure_016-b: PDF; Fulltext in PDF: PDF;

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2018-11-01
14:10
Projection of searches for pair production of scalar leptoquarks decaying to a top quark and a charged lepton at the HL-LHC /CMS Collaboration
Projections for searches for pair-produced scalar leptoquarks decaying into top quarks and muons or tau leptons for high integrated luminosities of up to $3000\,\mathrm{fb}^{-1}$ at the high luminosity LHC are presented. This study is based on published analysis results of data recorded in the year 2016. [...]
CMS-PAS-FTR-18-008.- 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; Fulltext in PDF: PDF;

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2018-10-22
16:20
Search sensitivity for dark photons decaying to displaced muons with CMS at the high-luminosity LHC /CMS Collaboration
This note presents sensitivity studies for a search for pairs of displaced muons originating from long-lived dark photons using the Phase-2 CMS detector at the high-luminosity LHC with an integrated luminosity of $3000~\mathrm{fb}^{-1}$. Projected sensitivities are obtained for broad ranges of dark photon masses ($1-30~\mathrm{GeV}$) and lifetimes ($c\tau = 0.01 -10~\mathrm{m}$) in the context of Dark Supersymmetry models..
CMS-PAS-FTR-18-002.- Geneva : CERN, 2018 Figure_001-a: PNG; Figure_001-b: PNG; Figure_002: PDF; Figure_003: PNG; Figure_004: PDF; Figure_005: PDF; Figure_006: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_009: JPG; Figure_010-a: PDF; Figure_010-b: PDF; Fulltext in PDF: PDF;

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2018-10-22
16:14
Projection of the Mono-Z search for dark matter to the HL-LHC /CMS Collaboration
A study of the expected discovery sensitivity and exclusion power of a search for new invisible particles in events with a Z boson and missing transverse momentum at the high-luminosity LHC is presented. Sensitivity estimates are derived from a CMS Run 2 result with the use of rescaling techniques [...]
CMS-PAS-FTR-18-007.- 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: PDF; Fulltext in PDF: PDF;

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2018-09-26
10:52
Search for charged Higgs bosons with the H$^{\pm} \to \tau^{\pm}\nu_\tau$ decay channel in proton-proton collisions at $\sqrt{s}=13~\mathrm{TeV}$ /CMS Collaboration
A search for charged Higgs bosons is presented in the H$^{\pm} \to \tau^{\pm}\nu_\tau$ decay mode in hadronic and leptonic final states. The search is based on $35.9~\mathrm{fb}^{-1}$ of pp collision data recorded by the CMS experiment in 2016 at a center-of-mass energy of 13 TeV. [...]
CMS-PAS-HIG-18-014.- Geneva : CERN, 2018 Figure_001-a: PDF; Figure_001-b: PDF; Figure_001-c: 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; Fulltext in PDF: PDF;

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2018-09-20
17:30
Search for new physics via top quark production in dilepton final state at 13 TeV /CMS Collaboration
A search for new physics in top quark production is performed in proton-proton collisions at 13 TeV. The data-set corresponds to an integrated luminosity of $35.9~\mathrm{fb}^{-1}$, and was collected in 2016 by the CMS detector. [...]
CMS-PAS-TOP-17-020.- Geneva : CERN, 2018 Figure_001: PDF; Figure_002-a: PNG; Figure_002-b: PNG; Figure_002-c: PNG; Figure_003-a: PNG; Figure_003-b: PNG; Figure_003-c: PNG; Figure_003-d: PNG; Figure_003-e: PNG; Figure_003-f: PNG; Figure_004-a: PNG; Figure_004-b: PNG; Figure_004-c: PNG; Figure_004-d: PNG; Figure_005-a: PNG; Figure_005-b: PNG; Figure_005-c: PNG; Figure_006-a: PNG; Figure_006-b: PNG; Figure_006-c: PNG; Figure_007: PNG; Fulltext in PDF: PDF;

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2018-09-19
10:10
Measurement of the $\mathrm{t}\bar{\mathrm{t}}$ production cross section, the top quark mass, and the strong coupling constant using events in the dilepton final state in pp collisions at $\sqrt{s}=13\;\mathrm{TeV}$ /CMS Collaboration
A measurement of the top quark-antiquark ($\mathrm{t}\bar{\mathrm{t}}$) pair production cross section in proton-proton collisions at a centre-of-mass energy of $13\;\mathrm{TeV}$ is presented. The data correspond to an integrated luminosity of 35.9 $\mathrm{fb}^{-1}$, recorded by the CMS experiment at the CERN LHC in 2016. [...]
CMS-PAS-TOP-17-001.- Geneva : CERN, 2018 Figure_001-a: PDF; Figure_001-b: PDF; Figure_001-c: PDF; Figure_001-d: PDF; Figure_001-e: PDF; Figure_001-f: 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_004-d: PDF; Figure_004-e: PDF; Figure_004-f: PDF; Figure_004-g: PDF; Figure_004-h: PDF; Figure_004-i: PDF; Figure_004-j: PDF; Figure_004-k: PDF; Figure_004-l: 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_005-g: PDF; Figure_005-h: 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_006-g: PDF; Figure_006-h: 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_008-g: PDF; Figure_008-h: PDF; Figure_008-i: PDF; Figure_008-j: PDF; Figure_008-k: PDF; Figure_008-l: 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_009-g: PDF; Figure_009-h: PDF; Figure_009-i: PDF; Figure_009-j: PDF; Figure_009-k: PDF; Figure_009-l: PDF; Figure_010: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_012-a: PDF; Figure_012-b: PDF; Figure_013: PDF; Fulltext in PDF: PDF;

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