CERN Accelerating science

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83.
Proton reconstruction with the TOTEM Roman pot detectors for high-$ \beta^* $ LHC data / Hayrapetyan, Aram (Yerevan Phys. Inst.) ; Tumasyan, Armen (Yerevan Phys. Inst.) ; Adam, Wolfgang (Vienna, OAW) ; Andrejkovic, Janik Walter (Vienna, OAW) ; Benato, Lisa (Vienna, OAW) ; Bergauer, Thomas (Vienna, OAW) ; Chatterjee, Suman (Vienna, OAW) ; Damanakis, Konstantinos (Vienna, OAW) ; Dragicevic, Marko (Vienna, OAW) ; Hussain, Priya Sajid (Vienna, OAW) et al.
The TOTEM Roman pot detectors are used to reconstruct the transverse momentum of scattered protons and to estimate the transverse location of the primary interaction. This paper presents new methods of track reconstruction, measurements of strip-level detection efficiencies, cross-checks of the LHC beam optics, and detector alignment techniques, along with their application in the selection of signal collision events. [...]
arXiv:2411.19749; CMS-SMP-23-006; CERN-EP-2024-273; TOTEM-2024-002; CMS-SMP-23-006-003.- Geneva : CERN, 2025-04-10 - 58 p. - Published in : JINST 20 (2025) P04012 Fulltext: PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList
84.
Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $ \to \mathrm{b}\overline{\mathrm{b}} $ decay channel in proton-proton collisions at $ \sqrt{s} = $ 13 TeV / CMS Collaboration
A standard model effective field theory (SMEFT) analysis with dimension-six operators probing nonresonant new physics effects is performed in the Higgs-strahlung process, where the Higgs boson is produced in association with a W or Z boson, in proton-proton collisions at a center-of-mass energy of 13 TeV. The final states in which the W or Z boson decays leptonically and the Higgs boson decays to a pair of bottom quarks are considered. [...]
arXiv:2411.16907; CMS-HIG-23-016; CERN-EP-2024-294; CMS-HIG-23-016-004.- Geneva : CERN, 2025-03-14 - 63 p. Fulltext: CMS-HIG-23-016-arXiv - PDF; 2411.16907 - PDF; e1e09eecbc10eda1f2cb2b575bea1939 - PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList; CMS HEPData
85.
Angular analysis of the $ {\mathrm{B}^0}\to \mathrm{ K^*(892)^0 } \mu^{+}\mu^{-} $ decay in proton-proton collisions at $ \sqrt{s}= $ 13 TeV / CMS Collaboration
A full set of optimized observables is measured in an angular analysis of the decay $ {\mathrm{B}^0}\to \mathrm{ K^*(892)^0 } \mu^{+}\mu^{-} $ using a sample of proton-proton collisions at $ \sqrt{s}= $ 13 TeV, collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 140 fb$ ^{-1} $. The analysis is performed in six bins of the squared invariant mass of the dimuon system, $ q^{2} $, over the range 1.1 $ < q^{2} < $ 16 GeV$^2 $. [...]
arXiv:2411.11820; CMS-BPH-21-002; CERN-EP-2024-268; CMS-BPH-21-002-003.- Geneva : CERN, 2025-03-21 - 39 p. - Published in : Phys. Lett. B 864 (2025) 139406 Fulltext: CMS-BPH-21-002-arXiv - PDF; 2411.11820 - PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList; CMS HEPData
86.
Reweighting simulated events using machine-learning techniques in the CMS experiment / CMS Collaboration
Data analyses in particle physics rely on an accurate simulation of particle collisions and a detailed simulation of detector effects to extract physics knowledge from the recorded data. Event generators together with a GEANT -based simulation of the detectors are used to produce large samples of simulated events for analysis by the LHC experiments. [...]
arXiv:2411.03023; CMS-MLG-24-001; CERN-EP-2024-269; CMS-MLG-24-001-003.- Geneva : CERN, 2025-05-06 - 49 p. - Published in : Eur. Phys. J. C 85 (2025) 495 Fulltext: CMS-MLG-24-001-arXiv - PDF; 2411.03023 - PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList
87.
Search for excited tau leptons in the $ \tau\tau\gamma $ final state in proton-proton collisions at $ \sqrt{s} = $ 13 TeV / CMS Collaboration
Results are presented for a test of the compositeness of the heaviest charged lepton, $ \tau $, using data collected by the CMS experiment in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC. The data were collected in 2016--2018 and correspond to an integrated luminosity of 138 fb$ ^{-1} $. [...]
arXiv:2410.21137; CMS-EXO-22-007; CERN-EP-2024-249; CMS-EXO-22-007; CERN-EP-2024-249; CMS-EXO-22-007-003.- Geneva : CERN, 2025-06-03 - 37 p. - Published in : 10.1007/JHEP06(2025)006 Fulltext: CMS-EXO-22-007-arXiv - PDF; 2410.21137 - PDF; publication - PDF; Fulltext from Publisher: PDF; Publication: PDF; External link: Preprint
88.
Search for pair production of heavy particles decaying to a top quark and a gluon in the lepton+jets final state in proton-proton collisions at $ \sqrt{s}= $ 13 TeV / CMS Collaboration
A search is presented for the pair production of new heavy resonances, each decaying into a top quark (t) or antiquark and a gluon ($ \mathrm{g} $). The analysis uses data recorded with the CMS detector from proton-proton collisions at a center-of-mass energy of 13 TeV at the LHC, corresponding to an integrated luminosity of 138 fb$ ^{-1} $. [...]
arXiv:2410.20601; CMS-B2G-22-005; CERN-EP-2024-266; CMS-B2G-22-005-004.- Geneva : CERN, 2025-03-25 - 43 p. - Published in : Eur. Phys. J. C 85 (2025) 342 Fulltext: 2410.20601 - PDF; d53716dcd9aab5a232f2ea74b8631efa - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
89.
Search for the Higgs boson decays to a $ \rho^{0} $, $ \phi $, or $ \mathrm{K}^{*0} $ meson and a photon in proton-proton collisions at $ \sqrt{s}= $ 13 TeV / CMS Collaboration
Three rare decay processes of the Higgs boson to a $ \rho(770) $, $ \phi(1020) $, or $ \mathrm{K}^{*}(892)^{0} $ meson and a photon are searched for using $ \sqrt{s}= $ 13 TeV proton-proton collision data collected by the CMS experiment at the LHC. Events are selected assuming the mesons decay into a pair of charged pions, a pair of charged kaons, or a charged kaon and pion, respectively. [...]
arXiv:2410.18289; CMS-HIG-23-005; CERN-EP-2024-252; CMS-HIG-23-005-003.- Geneva : CERN, 2025-02-03 - 28 p. - Published in : Phys. Lett. B 862 (2025) 139296 Fulltext: PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList
90.
Search for high-mass resonances in a final state comprising a gluon and two hadronically decaying W bosons in proton-proton collisions at $ \sqrt{s} = $ 13 TeV / CMS Collaboration
A search for high-mass resonances decaying into a gluon, $ \mathrm{g} $, and two W bosons is presented. A Kaluza-Klein gluon, $ \mathrm{g}_\text{KK} $, decaying in cascade via a scalar radion R, $ \mathrm{g}_\text{KK}\to\mathrm{g}\mathrm{R}\to\mathrm{g}\mathrm{W}\mathrm{W} $, is considered. [...]
arXiv:2410.17303; CMS-B2G-23-004; CERN-EP-2024-250; CMS-B2G-23-004-003.- Geneva : CERN, 2025-02-27 - 43 p. - Published in : JHEP 2502 (2025) 199 Fulltext: 2410.17303 - PDF; 5bc31d406d3f0b3c953ab304fb13ec91 - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
91.
Performance of the CMS high-level trigger during LHC Run 2 / CMS Collaboration
The CERN LHC provided proton and heavy ion collisions during its Run 2 operation period from 2015 to 2018. Proton-proton collisions reached a peak instantaneous luminosity of 2.1 $ \times $ 10$^{34}$ cm$^{-2}$s$^{-1} $, twice the initial design value, at $ \sqrt{s}= $ 13 TeV. [...]
arXiv:2410.17038; CMS-TRG-19-001; CERN-EP-2024-259; CMS-TRG-19-001-003.- Geneva : CERN, 2024-11-22 - 62 p. - Published in : JINST 19 (2024) P11021 Fulltext: 2410.17038 - PDF; FERMILAB-PUB-24-0717-CMS - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
92.
Search for heavy long-lived charged particles with large ionization energy loss in proton-proton collisions at $ \sqrt{s} $ = 13 TeV / CMS Collaboration
A search for heavy, long-lived, charged particles with large ionization energy loss within the silicon tracker of the CMS experiment is presented. A data set of proton-proton collisions at a center of mass energy at $ \sqrt{s} = $ 13 TeV, collected in 2017 and 2018 at the CERN LHC, corresponding to an integrated luminosity of 101 fb$ ^{-1} $, is used in this analysis. [...]
arXiv:2410.09164; CMS-EXO-18-002; CERN-EP-2024-254; CMS-EXO-18-002-003.- Geneva : CERN, 2025-04-15 - 43 p. - Published in : JHEP 2504 (2025) 109 Fulltext: 14038be844d8a0ed61334973e6cae878 - PDF; 2410.09164 - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server

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