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Performance of the CMS Level-1 trigger in proton-proton collisions at $\sqrt{s} = $ 13 TeV / CMS Collaboration
At the start of Run 2 in 2015, the LHC delivered proton-proton collisions at a center-of-mass energy of 13 TeV. During Run 2 (years 2015-2018) the LHC eventually reached a luminosity of 2.1 $\times $ 10$^{34} $ cm$^{-2}$s$^{-1}$, almost three times that reached during Run 1 (2009-2013) and a factor of two larger than the LHC design value, leading to events with up to a mean of about 50 simultaneous inelastic proton-proton collisions per bunch crossing (pileup). [...]
arXiv:2006.10165; CMS-TRG-17-001; CERN-EP-2020-065; CMS-TRG-17-001-003.- Geneva : CERN, 2020-10-19 - 63 p. - Published in : JINST 15 (2020) P10017 Fulltext: PDF; Fulltext from Publisher: PDF; Fulltext from publisher: PDF; External links: Additional information for the analysis; CMS AuthorList

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Search for a standard model-like Higgs boson in the mass range between 70 and 110 GeV in the diphoton final state in proton-proton collisions at $\sqrt{s}=$ 8 and 13 TeV / CMS Collaboration
The results of a search for a standard model-like Higgs boson in the mass range between 70 and 110 GeV decaying into two photons are presented. The analysis uses the data set collected with the CMS experiment in proton-proton collisions during the 2012 and 2016 LHC running periods. [...]
arXiv:1811.08459; CMS-HIG-17-013; CERN-EP-2018-207; CMS-HIG-17-013-003.- Geneva : CERN, 2019-06-10 - 28 p. - Published in : Phys. Lett. B 793 (2019) 320-347 Article from SCOAP3: PDF; Fulltext: PDF; External links: Additional information for the analysis; CMS AuthorList

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Measurement of exclusive $\Upsilon$ photoproduction from protons in pPb collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV / CMS Collaboration
The exclusive photoproduction of $\Upsilon$(nS) meson states from protons, $\gamma$p $ \to\Upsilon$(nS)p (with n = 1, 2, 3), is studied in ultraperipheral pPb collisions at a centre-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV. The measurement is performed using the $\Upsilon$(nS) $\to \mu^+\mu^-$ decay mode, with data collected by the CMS experiment corresponding to an integrated luminosity of 32.6 nb$^{-1}$. [...]
arXiv:1809.11080; CMS-FSQ-13-009; CERN-EP-2018-225; CMS-FSQ-13-009-003.- Geneva : CERN, 2019-03-26 - 36 p. - Published in : Eur. Phys. J. C Article from SCOAP3: PDF; Fulltext: 1809.11080 - PDF; document - PDF; erratum - PDF; Fulltext from Publisher: PDF; External link: Figures, tables and other information

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Search for heavy resonances decaying into two Higgs bosons or into a Higgs boson and a W or Z boson in proton-proton collisions at 13 TeV / CMS Collaboration
A search is presented for massive narrow resonances decaying either into two Higgs bosons, or into a Higgs boson and a W or Z boson. The decay channels considered are HH$\to \mathrm{b\overline{b}}\tau^{+}\tau^{-}$ and VH$ \to \mathrm{q\overline{q}}\tau^{+}\tau^{-}$, where H denotes the Higgs boson, and V denotes the W or Z boson. [...]
arXiv:1808.01365; CMS-B2G-17-006; CERN-EP-2018-182; CMS-B2G-17-006-003.- Geneva : CERN, 2019-01-07 - 38 p. - Published in : JHEP 1901 (2019) 051 Article from SCOAP3: PDF; Fulltext: PDF; External link: Figures, tables and other information

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Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV / CMS Collaboration
A search for a narrow-width resonance decaying into two Higgs bosons, each decaying into a bottom quark-antiquark pair, is presented. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 35.9 fb$^{-1}$ at $\sqrt{s}=$ 13 TeV recorded by the CMS detector at the LHC. [...]
arXiv:1806.03548; CMS-HIG-17-009; CERN-EP-2018-127; CMS-HIG-17-009-003.- Geneva : CERN, 2018-08-23 - 34 p. - Published in : JHEP 08 (2018) 152 Article from SCOAP3: PDF; Fulltext: PDF; External link: Figures, tables and other information

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Search for narrow and broad dijet resonances in proton-proton collisions at $ \sqrt{s}=13 $ TeV and constraints on dark matter mediators and other new particles / CMS Collaboration
Searches for resonances decaying into pairs of jets are performed using proton-proton collision data collected at $\sqrt{s} =$ 13 TeV corresponding to an integrated luminosity of up to 36 fb$^{-1}$. A low-mass search, for resonances with masses between 0.6 and 1.6 TeV, is performed based on events with dijets reconstructed at the trigger level from calorimeter information. [...]
arXiv:1806.00843; CMS-EXO-16-056; CERN-EP-2018-123; CMS-EXO-16-056-003.- Geneva : CERN, 2018-08-21 - 54 p. - Published in : JHEP 08 (2018) 130 Article from SCOAP3: PDF; Fulltext: PDF; External link: Figures, tables and other information

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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

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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

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Measurement of the production cross section for single top quarks in association with W bosons in proton-proton collisions at $\sqrt{s} = $ 13 TeV / CMS Collaboration
A measurement is presented of the associated production of a single top quark and a W boson in proton-proton collisions at $\sqrt{s}=$ 13 TeV by the CMS Collaboration at the CERN LHC. The data collected corresponds to an integrated luminosity of 35.9 fb$^{-1}$. [...]
arXiv:1805.07399; CMS-TOP-17-018; CERN-EP-2018-074; CMS-TOP-17-018-003.- Geneva : CERN, 2018-10-18 - 37 p. - Published in : JHEP 10 (2018) 117 Article from SCOAP3: PDF; Fulltext: PDF; External link: Figures, tables and other information

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10.

Measurement of the top quark mass with lepton+jets final states using $\mathrm {p}$ $\mathrm {p}$ collisions at $\sqrt{s}=13\,\text {TeV} $ / CMS Collaboration
The mass of the top quark is measured using a sample of $\mathrm{t\overline{t}}$ events collected by the CMS detector using proton-proton collisions at $\sqrt{s} =$ 13 TeV at the CERN LHC. Events are selected with one isolated muon or electron and at least four jets from data corresponding to an integrated luminosity of 35.9 fb$^{-1}$. [...]
arXiv:1805.01428; CMS-TOP-17-007; CERN-EP-2018-063; CMS-TOP-17-007-003.- Geneva : CERN, 2018-11-02 - 27 p. - Published in : Eur. Phys. J. C Article from SCOAP3: PDF; Fulltext: 1805.01428 - PDF; document - PDF; erratum - PDF; External link: Figures, tables and other information

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似た著者名：
1	FURIC, Ivan Kresimir
158	Furic, I
59	Furic, I K
116	Furic, I.
1	Furic, I. K.
8	Furic, I.K.
16	Furic, Ivan
1	Furic, Ivan K.

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