CERN Accelerating science

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1.
Operational Experience With the GEM Detector Assembly Lines for the CMS Forward Muon Upgrade / Abbaneo, D (CERN) ; Abbrescia, M (Bari Polytechnic ; INFN, Bari) ; Ahmad, A (NCP, Islamabad) ; Ahmed, W (NCP, Islamabad) ; Ali, C (Texas A-M) ; Altieri, P R (Bari Polytechnic ; INFN, Bari) ; Amr, M (Cairo, Acad. Sci. Res. Tech.) ; Asghar, I (NCP, Islamabad) ; Aspell, P (CERN) ; Assran, Y (Cairo, Acad. Sci. Res. Tech.) et al.
The CMS Collaboration has been developing large-area triple-gas electron multiplier (GEM) detectors to be installed in the muon Endcap regions of the CMS experiment in 2019 to maintain forward muon trigger and tracking performance at the High-Luminosity upgrade of the Large Hadron Collider (LHC); 10 preproduction detectors were built at CERN to commission the first assembly line and the quality controls (QCs). These were installed in the CMS detector in early 2017 and participated in the 2017 LHC run. [...]
2018 - 9 p. - Published in : IEEE Trans. Nucl. Sci. 65 (2018) 2808-2816
2.
Search for Higgs boson pair production in the $\gamma\gamma\mathrm{b\overline{b}}$ final state in pp collisions at $\sqrt{s}=$ 13 TeV / CMS Collaboration
A search is presented for the production of a pair of Higgs bosons, where one decays into two photons and the other one into a bottom quark-antiquark pair. The analysis is performed using proton-proton collision data at $\sqrt{s} =$ 13 TeV recorded in 2016 by the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. [...]
arXiv:1806.00408; CMS-HIG-17-008; CERN-EP-2017-343; CMS-HIG-17-008-004.- Geneva : CERN, 2019-01-10 - 30 p. - Published in : Phys. Lett. B 788 (2019) 7-36 Article from SCOAP3: PDF; Fulltext: PDF; External link: Figures, tables and other information
3.
Measurement of nuclear modification factors of $\Upsilon$(1S), $\Upsilon$(2S), and $\Upsilon$(3S) mesons in PbPb collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 TeV / CMS Collaboration
The cross sections for $ \Upsilon(\text{1S})$, $ \Upsilon(\text{2S})$, and $ \Upsilon(\text{3S})$ production in lead-lead (PbPb) and proton-proton (pp) collisions at $ {\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}} = $ 5.02 TeV have been measured using the CMS detector at the LHC. The nuclear modification factors, $ {R_{\mathrm{AA}}} $, derived from the PbPb-to-pp ratio of yields for each state, are studied as functions of meson rapidity and transverse momentum, as well as PbPb collision centrality. [...]
arXiv:1805.09215; CMS-HIN-16-023; CERN-EP-2018-110; CMS-HIN-16-023-003.- Geneva : CERN, 2019-03-10 - 24 p. - Published in : Phys. Lett. B 790 (2019) 270-293 Article from SCOAP3: PDF; Fulltext: PDF; External link: Figures, tables and other information
4.
Performance of the CMS muon detector and muon reconstruction with proton-proton collisions at $\sqrt{s}=$ 13 TeV / CMS Collaboration
The CMS muon detector system, muon reconstruction software, and high-level trigger underwent significant changes in 2013-2014 in preparation for running at higher LHC collision energy and instantaneous luminosity. The performance of the modified system is studied using proton-proton collision data at center-of-mass energy $\sqrt{s}=$ 13 TeV, collected at the LHC in 2015 and 2016. [...]
arXiv:1804.04528; CMS-MUO-16-001; CERN-EP-2018-058; CMS-MUO-16-001-003.- Geneva : CERN, 2018-06-19 - 53 p. - Published in : JINST 13 (2018) P06015 Fulltext: 1804.04528 - PDF; openaccess_Sirunyan_2018_J._Inst._13_P06015 - PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList
5.
Measurements of differential cross sections of top quark pair production as a function of kinematic event variables in proton-proton collisions at $\sqrt{s}=$ 13 TeV / CMS Collaboration
Measurements of differential $\mathrm{t\overline{t}}$ production cross sections are presented in the single-lepton decay channel, as a function of a number of kinematic event variables. The measurements are performed with proton-proton collision data at $\sqrt{s}=$ 13 TeV, collected by the CMS experiment at the LHC during 2016, with an integrated luminosity of 35.9 fb$^{-1}$. [...]
arXiv:1803.03991; CMS-TOP-16-014; CERN-EP-2018-013; CMS-TOP-16-014-003.- Geneva : CERN, 2018-06-01 - 56 p. - Published in : JHEP 06 (2018) 002 Article from SCOAP3: PDF; Fulltext: PDF; External link: Rivet analyses reference
6.
Search for a heavy resonance decaying into a Z boson and a vector boson in the $\nu\overline{\nu}\mathrm{q}\mathrm{\bar{q}}$ final state / CMS Collaboration
A search is presented for a heavy resonance decaying into either a pair of Z bosons or a Z boson and a W boson (ZZ or WZ), with a Z boson decaying into a pair of neutrinos and the other boson decaying hadronically into two collimated quarks that are reconstructed as a highly energetic large-cone jet. The search is performed using the data collected with the CMS detector at the CERN LHC during 2016 in proton-proton collisions at a center-of-mass energy of 13 TeV, corresponding to a total integrated luminosity of 35.9 fb$^{-1}$. [...]
arXiv:1803.03838; CMS-B2G-17-005; CERN-EP-2018-023; CMS-B2G-17-005-003.- Geneva : CERN, 2018-07-11 - 34 p. - Published in : JHEP 07 (2018) 075 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
7.
Search for third-generation scalar leptoquarks decaying to a top quark and a $\tau$ lepton at $\sqrt{s} = $ 13 TeVSearch for third-generation scalar leptoquarks decaying to a top quark and a $\tau$ lepton at $\sqrt{s}=$ 13 TeV / CMS Collaboration
A search for pair production of heavy scalar leptoquarks (LQs), each decaying into a top quark and a $\tau$ lepton, is presented. The search considers final states with an electron or a muon, one or two $\tau$ leptons that decayed to hadrons, and additional jets. [...]
arXiv:1803.02864; CMS-B2G-16-028; CERN-EP-2018-019; CMS-B2G-16-028-003.- Geneva : CERN, 2018-09-03 - 38 p. - Published in : Eur. Phys. J. C 78 (2018) 707 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
8.
Measurement of the $\Lambda_b$ polarization and angular parameters in $\Lambda_b\to J/\psi\, \Lambda$ decays from pp collisions at $\sqrt{s}=$ 7 and 8 TeV / CMS Collaboration
An analysis of the decay $\Lambda_b \to J/\psi(\to\mu^+\mu^-)\Lambda(\to p \pi^-)$ decay is performed to measure the $\Lambda_b$ polarization and three angular parameters in data from pp collisions at $\sqrt{s} =$ 7 and 8 TeV, collected by the CMS experiment at the LHC. The $\Lambda_b$ polarization is measured to be 0.00 $\pm$ 0.06 (stat) $\pm$ 0.06 (syst) and the parity-violating asymmetry parameter is determined to be 0.14 $\pm$ 0.14 (stat) $\pm$ 0.10 (syst). [...]
arXiv:1802.04867; CMS-BPH-15-002; CERN-EP-2017-331; CMS-BPH-15-002-003.- Geneva : CERN, 2018-04-18 - 20 p. - Published in : Phys. Rev. D 97 (2018) 072010 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
9.
Search for heavy neutral leptons in events with three charged leptons in proton-proton collisions at $\sqrt{s} =$ 13 TeV / CMS Collaboration
A search for a heavy neutral lepton N of Majorana nature decaying into a W boson and a charged lepton is performed using the CMS detector at the LHC. The targeted signature consists of three prompt charged leptons in any flavor combination of electrons and muons. [...]
arXiv:1802.02965; CMS-EXO-17-012; CERN-EP-2018-006; CMS-EXO-17-012-003.- Geneva : CERN, 2018-05-30 - 20 p. - Published in : Phys. Rev. Lett. 120 (2018) 221801 Article from SCOAP3: PDF; Fulltext: PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList
10.
Measurement of the inelastic proton-proton cross section at $\sqrt{s}=$ 13 TeV / CMS Collaboration
A measurement of the inelastic proton-proton cross section with the CMS detector at a center-of-mass energy of $\sqrt{s} =$ 13 TeV is presented. The analysis is based on events with energy deposits in the forward calorimeters, which cover pseudorapidities of -6.6 $< \eta $ 4.1 GeV and/or $M_\mathrm{Y} >$ 13 GeV, where $M_\mathrm{X}$ and $M_\mathrm{Y}$ are the masses of the diffractive dissociation systems at negative and positive pseudorapidities, respectively. [...]
arXiv:1802.02613; CMS-FSQ-15-005; CERN-EP-2018-004; CMS-FSQ-15-005-003.- Geneva : CERN, 2018-07-25 - 30 p. - Published in : JHEP 07 (2018) 161 Article from SCOAP3: PDF; Fulltext: 1802.02613 - PDF; arXiv:1802.02613 - PDF; External link: Rivet analyses reference

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