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1.
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
2.
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^{-}$, where H denotes the Higgs boson, and V denotes the W or Z boson. [...]
arXiv:1808.01365; CMS-B2G-17-006; CERN-EP-2018-182; CMS-B2G-17-006-003.- Geneva : CERN, 2019-01-07 - 38 p. - Published in : JHEP 1901 (2019) 051 Article from SCOAP3: PDF; Fulltext: PDF; External link: Figures, tables and other information
3.
Precision measurement of the structure of the CMS inner tracking system using nuclear interactions / CMS Collaboration
The structure of the CMS inner tracking system has been studied using nuclear interactions of hadrons striking its material. Data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded in 2015 at the LHC are used to reconstruct millions of secondary vertices from these nuclear interactions. [...]
arXiv:1807.03289; CMS-TRK-17-001; CERN-EP-2018-144; CMS-TRK-17-001-003.- Geneva : CERN, 2018-10-29 - 41 p. - Published in : JINST 13 (2018) P10034 Fulltext: 1807.03289 - PDF; fulltext1682069 - PDF; Fulltext from Publisher: PDF; External link: Figures, tables and other information
4.
Search for resonant pair production of Higgs bosons decaying to bottom quark-antiquark pairs in proton-proton collisions at 13 TeV / CMS Collaboration
A search for a narrow-width resonance decaying into two Higgs bosons, each decaying into a bottom quark-antiquark pair, is presented. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 35.9 fb$^{-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
5.
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
6.
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
7.
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
8.
Front-side biasing of n-in-p silicon strip detectors / Baselga Bacardit, Marta (KIT, Karlsruhe, EKP) ; Bergauer, Thomas (Vienna, OAW) ; Dierlamm, Alexander Hermann (KIT, Karlsruhe, EKP) ; Dragicevic, Marko Gerhart (Vienna, OAW) ; Konig, Axel (Vienna, OAW) ; Pree, Elias (Vienna, OAW) ; Metzler, Marius (KIT, Karlsruhe, EKP)
Front-side biasing is an alternative method to bias a silicon sensor. Instead of directly applying high voltage to the back-side, one can exploit the conductive properties of the edge region to bias a detector exclusively via top-side connections. [...]
CMS-NOTE-2018-002; CERN-CMS-NOTE-2018-002.- Geneva : CERN, 2018 - 23 p. Fulltext: PDF;
9.
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
10.
Measurements of Higgs boson properties in the diphoton decay channel in proton-proton collisions at $\sqrt{s} = $ 13 TeV / CMS Collaboration
Measurements of Higgs boson properties in the H$\to\gamma\gamma$ decay channel are reported. The analysis is based on data collected by the CMS experiment in proton-proton collisions at $\sqrt{s}=$ 13 TeV during the 2016 LHC running period, corresponding to an integrated luminosity of 35.6 fb$^{-1}$. [...]
arXiv:1804.02716; CMS-HIG-16-040; CERN-EP-2018-060; CMS-HIG-16-040-003.- Geneva : CERN, 2018-11-29 - 56 p. - Published in : JHEP 11 (2018) 185 Article from SCOAP3: PDF; Fulltext: PDF; External link: Figures, tables and other information

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31 Konig, A
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31 König, A
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