CERN Accelerating science

CERN Document Server Sök i 426 journaler efter:  1 - 10nästaslut  gå till journal: Sökningen tog 0.67 sekunder. 
1.
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
2.
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
3.
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
4.
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
5.
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: 1802.04867 - PDF; cms-bph-15-002-arxiv - PDF; External links: Additional information for the analysis; CMS AuthorList
6.
Search for single production of vector-like quarks decaying to a b quark and a Higgs boson / CMS Collaboration
A search is presented for single production of heavy vector-like quarks (B) that decay to a Higgs boson and a b quark, with the Higgs boson decaying to a highly boosted $\mathrm{b\overline{b}}$ pair reconstructed as a single collimated jet. The analysis is based on data collected by the CMS experiment in proton-proton collisions at $\sqrt{s} =$ 13 TeV, corresponding to an integrated luminosity of 35.9 fb$^{-1}$. [...]
arXiv:1802.01486; CMS-B2G-17-009; CERN-EP-2017-338; CMS-B2G-17-009-003.- Geneva : CERN, 2018-06-05 - 40 p. - Published in : JHEP 06 (2018) 031 Article from SCOAP3: PDF; Fulltext: 1802.01486 - PDF; arXiv:1802.01486 - PDF; External links: Additional information for the analysis; CMS AuthorList
7.
Search for dark matter in events with energetic, hadronically decaying top quarks and missing transverse momentum at $\sqrt{s}=$ 13 TeV / CMS Collaboration
A search for dark matter is conducted in events with large missing transverse momentum and a hadronically decaying, Lorentz-boosted top quark. This study is performed using proton-proton collisions at a center-of-mass energy of 13 TeV, in data recorded by the CMS detector in 2016 at the LHC, corresponding to an integrated luminosity of 36 fb$^{-1}$. [...]
arXiv:1801.08427; CMS-EXO-16-051; CERN-EP-2017-299; CMS-EXO-16-051-003.- Geneva : CERN, 2018-06-05 - 52 p. - Published in : JHEP 06 (2018) 027 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
8.
Observation of medium induced modifications of jet fragmentation in PbPb collisions using isolated-photon-tagged jets / CMS Collaboration
Measurements of fragmentation functions for jets associated with an isolated photon are presented for the first time in pp and PbPb collisions. The analysis uses data collected with the CMS detector at the CERN LHC at a nucleon-nucleon center-of-mass energy of 5.02 TeV. [...]
arXiv:1801.04895; CMS-HIN-16-014; CERN-EP-2017-337; CMS-HIN-16-014-003.- Geneva : CERN, 2018-12-15 - 18 p. - Published in : Phys. Rev. Lett. 121 (2018) 242301 Article from SCOAP3: PDF; Fulltext: arXiv:1801.04895 - PDF; cms-hin-16-014-arxiv - PDF; External link: Figures, tables and other information
9.
Combined search for electroweak production of charginos and neutralinos in proton-proton collisions at $\sqrt{s} =$ 13 TeV / CMS Collaboration
A statistical combination of several searches for the electroweak production of charginos and neutralinos is presented. All searches use proton-proton collision data at $\sqrt{s}=$ 13 TeV, recorded with the CMS detector at the LHC in 2016 and corresponding to an integrated luminosity of 35.9 fb$^{-1}$. [...]
arXiv:1801.03957; CMS-SUS-17-004; CERN-EP-2017-283; CMS-SUS-17-004-003.- Geneva : CERN, 2018-03-27 - 44 p. - Published in : JHEP 03 (2018) 160 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList
10.
Measurement of the $\mathrm{Z}\gamma^{*} \to \tau\tau$ cross section in pp collisions at $\sqrt{s} = $ 13 TeV and validation of $\tau$ lepton analysis techniques / CMS Collaboration
A measurement is presented of the $\mathrm{Z}/\gamma^{*} \to \tau\tau$ cross section in pp collisions at $\sqrt{s} = $ 13 TeV, using data recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 2.3 fb$^{-1}$. The product of the inclusive cross section and branching fraction is measured to be $\sigma(\mathrm{pp} \to \mathrm{Z}/\gamma^{*}\text{+X}) \, \mathcal{B}(\mathrm{Z}/\gamma^{*} \to \tau\tau) = $ 1848 $\pm$ 12 (stat) $\pm$ 67 (syst+lumi) pb, in agreement with the standard model expectation, computed at next-to-next-to-leading order accuracy in perturbative quantum chromodynamics. [...]
arXiv:1801.03535; CMS-HIG-15-007; CERN-EP-2017-307; CMS-HIG-15-007-003.- Geneva : CERN, 2018-09-03 - 68 p. - Published in : Eur. Phys. J. C 78 (2018) 708 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList

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