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1.
The CMS Phase-1 Pixel Detector Upgrade / CMS Tracker Group of the CMS Collaboration
The CMS detector at the CERN LHC features a silicon pixel detector as its innermost subdetector. The original CMS pixel detector has been replaced with an upgraded pixel system (CMS Phase-1 pixel detector) in the extended year-end technical stop of the LHC in 2016/2017. [...]
arXiv:2012.14304.- 2021-02-22 - 84 p. - Published in : JINST 16 (2021) P02027 Fulltext: 2012.14304 - PDF; fermilab-pub-20-697-cms - PDF; Fulltext from Publisher: PDF; Fulltext from publisher: PDF; External link: Fermilab Accepted Manuscript
2.
Dependence of inclusive jet production on the anti-${k_{\mathrm{T}}}$ distance parameter in pp collisions at $\sqrt{s} = $ 13 TeV / CMS Collaboration
The dependence of inclusive jet production in proton-proton collisions with a center-of-mass energy of 13 TeV on the distance parameter $R$ of the anti-${k_{\mathrm{T}}}$ algorithm is studied using data corresponding to integrated luminosities up to 35.9 fb$^{-1}$ collected by the CMS experiment in 2016. The ratios of the inclusive cross sections as functions of transverse momentum ${p_{\mathrm{T}}}$ and rapidity $y$, for $R$ in the range 0.1 to 1.2 to those using $R= $ 0.4 are presented in the region 84 $ < {p_{\mathrm{T}}} < $ 1588 GeV and $|y| < $ 2.0. [...]
arXiv:2005.05159; CMS-SMP-19-003; CERN-EP-2020-040; CMS-SMP-19-003-003.- Geneva : CERN, 2020-12-11 - 43 p. - Published in : JHEP 2012 (2020) 082 Article from SCOAP3: PDF; Fulltext: SMP-19-003-arXiv - PDF; 2005.05159 - PDF; External links: Additional information for the analysis; CMS AuthorList
3.
Beam test performance of prototype silicon detectors for the Outer Tracker for the Phase-2 Upgrade of CMS / CMS Tracker Group Collaboration
A new CMS tracker detector will be installed for operation at the High Luminosity LHC (HL-LHC). This detector comprises modules with two closely spaced parallel sensor plates and front-end ASICs capable of transmitting tracking information to the CMS Level-1 (L1) trigger at the 40 MHz beam crossing rate. [...]
2020 - 32 p. - Published in : JINST 15 (2020) P03014 Fulltext: PDF;
4.
Identification of heavy, energetic, hadronically decaying particles using machine-learning techniques / CMS Collaboration
Machine-learning (ML) techniques are explored to identify and classify hadronic decays of highly Lorentz-boosted W/Z/Higgs bosons and top quarks. Techniques without ML have also been evaluated and are included for comparison. [...]
arXiv:2004.08262; CMS-JME-18-002; CERN-EP-2020-037; CMS-JME-18-002-005.- Geneva : CERN, 2020-06-03 - 87 p. - Published in : JINST 15 (2020) P06005 Fulltext: 2004.08262 - PDF; CMS-JME-18-002-arXiv - PDF; Fulltext from publisher: PDF; External link: Open Access fulltext
5.
Measurement of quark- and gluon-like jet fractions using jet charge in PbPb and pp collisions at 5.02 TeV / CMS Collaboration
The momentum-weighted sum of the electric charges of particles inside a jet, known as jet charge, is sensitive to the electric charge of the particle initiating the parton shower. This paper presents jet charge distributions in ${\sqrt {\smash [b]{s_{_{\mathrm {NN}}}}}}=$ 5.02 TeV lead-lead (PbPb) and proton-proton (pp) collisions recorded with the CMS detector at the LHC. [...]
arXiv:2004.00602; CMS-HIN-18-018; CERN-EP-2020-019; CMS-HIN-18-018-004.- Geneva : CERN, 2020-07-17 - 37 p. - Published in : JHEP 2007 (2020) 115 Article from SCOAP3: PDF; Fulltext: CMS-HIN0-18-018-arXiv - PDF; 2004.00602 - PDF; External links: Additional information for the analysis; CMS AuthorList
6.
Measurement of the cross section for $\mathrm{t\bar{t}}$ production with additional jets and b jets in pp collisions at $\sqrt{s} = $ 13 TeV / CMS Collaboration
Measurements of the cross section for the production of top quark pairs in association with a pair of jets from bottom quarks (${\sigma_{{\mathrm{t\bar{t}}\mathrm{b\bar{b}}} }} $) and in association with a pair of jets from quarks of any flavor or gluons (${\sigma_{{\mathrm{t\bar{t}} \mathrm{jj}} }} $) and their ratio are presented. The data were collected in proton-proton collisions at a center-of-mass energy of 13 TeV by the CMS experiment at the LHC in 2016 and correspond to an integrated luminosity of 35.9 fb$^{-1}$. [...]
arXiv:2003.06467; CMS-TOP-18-002; CERN-EP-2020-011; CMS-TOP-18-002-003.- Geneva : CERN, 2020-07-20 - 46 p. - Published in : JHEP 2007 (2020) 125 Article from SCOAP3: PDF; Fulltext: CMS-TOP-18-002-arXiv - PDF; 2003.06467 - PDF; External links: Additional information for the analysis; CMS AuthorList
7.
Study of central exclusive $\pi^{+}\pi^{-}$ production in proton-proton collisions at $\sqrt{s} = $ 5.02 and 13 TeV / CMS Collaboration
Central exclusive production of $\pi^{+}\pi^{-}$ pairs is measured with the CMS detector in proton-proton collisions at the LHC at center-of-mass energies of 5.02 and 13 TeV. The theoretical description of these nonperturbative processes, which have not yet been measured in detail at the LHC, poses a significant challenge to models. [...]
arXiv:2003.02811; CMS-FSQ-16-006; CERN-EP-2020-005; CMS-FSQ-16-006-003.- Geneva : CERN, 2020-08-10 - 28 p. - Published in : Eur. Phys. J. C 80 (2020) 718 Article from SCOAP3: PDF; Fulltext: 2003.02811 - PDF; CMS-FSQ-16-006-arXIv - PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList
8.
Pileup mitigation at CMS in 13 TeV data / CMS Collaboration
With increasing instantaneous luminosity at the LHC come additional reconstruction challenges. At high luminosity, many collisions occur simultaneously within one proton-proton bunch crossing. [...]
arXiv:2003.00503; CMS-JME-18-001; CERN-EP-2020-017; CMS-JME-18-001-003.- Geneva : CERN, 2020-09-15 - 57 p. - Published in : JINST 15 (2020) P09018 Fulltext: CMS-JME-18-001-arXiv - PDF; 2003.00503 - PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList
9.
Measurement of single-diffractive dijet production in proton-proton collisions at $\sqrt{s} =$ 8 TeV with the CMS and TOTEM experiments / CMS and TOTEM Collaborations
Measurements are presented of the single-diffractive dijet cross section and the diffractive cross section as a function of the proton fractional momentum loss $\xi$ and the four-momentum transfer squared $t$. Both processes ${\mathrm{p}}{\mathrm{p}} \to {\mathrm{p}}\mathrm{X}$ and ${\mathrm{p}}{\mathrm{p}} \to \mathrm{X}{\mathrm{p}}$, ie with the proton scattering to either side of the interaction point, are measured, where $\mathrm{X}$ includes at least two jets; the results of the two processes are averaged [...]
arXiv:2002.12146; CMS-FSQ-12-033; TOTEM-2020-001; CERN-EP-2019-260; CMS-FSQ-12-033-003.- Geneva : CERN, 2020-12-17 - 42 p. - Published in : Eur. Phys. J. C Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
10.
Measurement of the cross section for electroweak production of a Z boson, a photon and two jets in proton-proton collisions at $\sqrt{s} = $ 13 TeV and constraints on anomalous quartic couplings / CMS Collaboration
A measurement is presented of the cross section for electroweak production of a Z boson and a photon in association with two jets ( $\mathrm{Z \gamma jj}$) in proton-proton collisions. The Z boson candidates are selected through their decay into a pair of electrons or muons. [...]
arXiv:2002.09902; CMS-SMP-18-007; CERN-EP-2020-007; CMS-SMP-18-007-003.- Geneva : CERN, 2020-06-10 - 39 p. - Published in : JHEP 2006 (2020) 076 Article from SCOAP3: PDF; Fulltext: 2002.09902 - PDF; CMS-SMP-18-007-arXiv - PDF; External links: Additional information for the analysis; CMS AuthorList

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