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Constraints on the ${\chi_{\mathrm{c}1}}$ versus ${\chi_{\mathrm{c}2}}$ polarizations in proton-proton collisions at $\sqrt{s} = $ 8 TeV / CMS Collaboration
The polarizations of promptly produced ${\chi_{\mathrm{c}1}}$ and ${\chi_{\mathrm{c}2}}$ mesons are studied using data collected by the CMS experiment at the LHC, in proton-proton collisions at $\sqrt{s} = $ 8 TeV. The ${\chi_{\mathrm{c}}}$ states are reconstructed via their radiative decays ${\chi_{\mathrm{c}}} \rightarrow \mathrm{J}/\psi\, \gamma$, with the photons being measured through conversions to $\mathrm{e^{+}}\mathrm{e^{-}}$, which allows the two states to be well resolved. [...]
arXiv:1912.07706; CMS-BPH-13-001; CERN-EP-2019-279; CMS-BPH-13-001-003.- Geneva : CERN, 2020-04-25 - 18 p. - Published in : Phys. Rev. Lett. 124 (2020) 162002 Article from SCOAP3: PDF; Fulltext: CMS-BPH-13-001-arXiv - PDF; 1912.07706 - PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList

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Study of dijet events with a large rapidity gap between the two leading jets in pp collisions at $\sqrt{s}$ = 7 TeV / CMS Collaboration
Events with no charged particles produced between the two leading jets are studied in proton-proton collisions at $\sqrt{s}$ = 7 TeV. The jets were required to have transverse momentum $p_\mathrm{T}^{\text{jet}}$ > 40 GeV and pseudorapidity 1.5 $<|\eta^{\text{jet}}| <$ 4.7, and to have values of $\eta^{\text{jet}}$ with opposite signs. [...]
arXiv:1710.02586; CMS-FSQ-12-001; CERN-EP-2017-141; CMS-FSQ-12-001-003.- Geneva : CERN, 2018-03-21 - 27 p. Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList

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Search for natural supersymmetry in events with top quark pairs and photons in pp collisions at $\sqrt{s} =$ 8 TeV / CMS Collaboration
Results are presented from a search for natural gauge-mediated supersymmetry (SUSY) in a scenario in which the top squark is the lightest squark, the next-to-lightest SUSY particle is a bino-like neutralino, and the lightest SUSY particle is the gravitino. The strong production of top squark pairs can produce events with pairs of top quarks and neutralinos, with each bino-like neutralino decaying to a photon and a gravitino. [...]
arXiv:1707.03325; CMS-SUS-15-009; CERN-EP-2017-124; CMS-SUS-15-009-003.- Geneva : CERN, 2018-03-27 - 36 p. - Published in : JHEP 03 (2018) 167 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList

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A search for Higgs boson pair production in the $\mathrm{ b }\mathrm{ b }\tau\tau$ final state in proton-proton collisions at $\sqrt{s} = $ 8 TeV / CMS Collaboration
Results are presented from a search for production of Higgs boson pairs (HH) where one boson decays to a pair of b quarks and the other to a $\tau$ lepton pair. This work is based on proton-proton collision data collected by the CMS experiment at $ \sqrt{s} = $ 8 TeV, corresponding to an integrated luminosity of 18.3 fb$^{-1}$. [...]
arXiv:1707.00350; CMS-HIG-15-013; CERN-EP-2017-104; CMS-HIG-15-013-005.- Geneva : CERN, 2017-10-20 - 25 p. - Published in : Phys. Rev. D 96 (2017) 072004 Fulltext: 10.1103_PhysRevD.96.072004 - PDF; arXiv:1707.00350 - PDF; cms-hig-15-013-arxiv - PDF; External link: Open Access fulltext

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Measurement of charged pion, kaon, and proton production in proton-proton collisions at $\sqrt{s} = $ 13 TeV / CMS Collaboration
Transverse momentum spectra of charged pions, kaons, and protons are measured in proton-proton collisions at sqrt(s) = 13 TeV with the CMS detector at the LHC. The particles, identified via their energy loss in the silicon tracker, are measured in the transverse momentum range of pt ~ 0.1-1.7 GeV and rapidities abs(y) < 1. [...]
arXiv:1706.10194; CMS-FSQ-16-004; CERN-EP-2017-091; CMS-FSQ-16-004-004.- Geneva : CERN, 2017-12-05 - 24 p. - Published in : Phys. Rev. D 96 (2017) 112003 Fulltext: 10.1103_PhysRevD.96.112003 - PDF; arXiv:1706.10194 - PDF; External link: Open Access fulltext

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Exclusive and semi-exclusive $\pi^{+}\pi^{-}$ production in proton-proton collisions at $\sqrt{s} = $ 7 TeV / CMS Collaboration
A measurement is presented of the exclusive and semi-exclusive production of charged pion pairs in proton-proton collisions, $\mathrm{ p p }\to\mathrm{ p }({\mathrm{p}^*} )+ \pi^{+}\pi^{-}+ \mathrm{ p } ({\mathrm{p}^*} )$, where the $\pi^{+} \pi^{-}$ pair is emitted at central rapidities, and the scattered protons stay intact ($\mathrm{p}$) or diffractively dissociate (${\mathrm{p}^*} $) without detection. [...]
arXiv:1706.08310 ; CMS-FSQ-12-004 ; CERN-EP-2016-261 ; CMS-FSQ-12-004-005. - 2017. - 34 p.
Figures, tables and other information - Full text - Fulltext

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Measurement of the semileptonic $\mathrm{ t \bar{t} }$+$\gamma$ production cross section in pp collisions at $\sqrt{s}=$ 8 TeV / CMS Collaboration
A measurement of the cross section for top quark-antiquark (tt-bar) pairs produced in association with a photon in proton-proton collisions at sqrt(s) = 8 TeV is presented. The analysis uses data collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 19.7 inverse femtobarns. [...]
arXiv:1706.08128; CMS-TOP-14-008; CERN-EP-2017-112; CMS-TOP-14-008-003.- Geneva : CERN, 2017-10-02 - 38 p. - Published in : JHEP 10 (2017) 006 Article from SCOAP3: PDF; Fulltext: PDF; External link: Figures, tables and other information

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Suppression of Excited $\Upsilon$ States Relative to the Ground State in Pb-Pb Collisions at $\sqrt{s_\mathrm{NN}}$=5.02 TeV / CMS Collaboration
The relative yields of $\Upsilon$ mesons produced in pp and PbPb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV and reconstructed via the dimuon decay channel are measured using data collected by the CMS experiment. Double ratios are formed by comparing the yields of the excited states, $\Upsilon$(2S) and $\Upsilon$(3S), to the ground state, $\Upsilon$(1S), in both PbPb and pp collisions at the same center-of-mass energy. [...]
arXiv:1706.05984; CMS-HIN-16-008; CERN-EP-2017-080; CMS-HIN-16-008-003.- Geneva : CERN, 2018-04-02 - 17 p. - Published in : Phys. Rev. Lett. 120 (2018) 142301 Article from SCOAP3: PDF; Fulltext: arXiv:1706.05984 - PDF; 10.1103_PhysRevLett.120.142301 - PDF; External links: Additional information for the analysis; CMS AuthorList

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Measurements of jet charge with dijet events in pp collisions at $\sqrt{s}=8$ TeV / CMS Collaboration
Jet charge is an estimator of the electric charge of a quark, antiquark, or gluon initiating a jet. It is based on the momentum-weighted sum of the electric charges of the jet constituents. [...]
arXiv:1706.05868; CMS-SMP-15-003; CERN-EP-2017-085; CMS-SMP-15-003-003.- Geneva : CERN, 2017-10-19 - 38 p. - Published in : JHEP 10 (2017) 131 Article from SCOAP3: PDF; Fulltext: PDF; External link: Rivet analyses reference

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10.

Particle-flow reconstruction and global event description with the CMS detector / CMS Collaboration
The CMS apparatus was identified, a few years before the start of the LHC operation at CERN, to feature properties well suited to particle-flow (PF) reconstruction: a highly-segmented tracker, a fine-grained electromagnetic calorimeter, a hermetic hadron calorimeter, a strong magnetic field, and an excellent muon spectrometer. A fully-fledged PF reconstruction algorithm tuned to the CMS detector was therefore developed and has been consistently used in physics analyses for the first time at a hadron collider. [...]
arXiv:1706.04965; CMS-PRF-14-001; CERN-EP-2017-110; CMS-PRF-14-001-004.- Geneva : CERN, 2017-10-06 - 82 p. - Published in : JINST 12 (2017) P10003 Fulltext: 10.1088_1748-0221_12_10_P10003 - PDF; arXiv:1706.04965 - PDF; External link: Open Access fulltext

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