CERN Accelerating science

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1.
Measurement of light-by-light scattering and the Breit-Wheeler process, and search for axion-like particles in ultraperipheral PbPb collisions at $ \sqrt{\smash[b]{s_{_{\mathrm{NN}}}}} = $ 5.02 TeV / CMS Collaboration
Measurements of light-by-light scattering (LbL, $ \gamma\gamma\to\gamma\gamma $) and the Breit-Wheeler process (BW, $ \gamma\gamma\to\mathrm{e}^+\mathrm{e}^- $) are reported in ultraperipheral PbPb collisions at a centre-of-mass energy per nucleon pair of 5.02 TeV. [...]
CMS-HIN-21-015 ; CERN-EP-2024-284 ; arXiv:2412.15413 ; CMS-HIN-21-015-003.
- 2024
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
2.
CMS RPC performance and operation in LHC Run 3 / CMS Collaboration
The CMS experiment has collected more than 180 fb$^{-1}$ of proton-proton collision data at a 13.6 TeV center-of-mass energy in Run 3 data taking (2022, 2023 and 2024). The CMS RPC system faces the challenge of the LHC delivered instantaneous luminosity of up to 2 x 10$^{34}$ cm$^{-2}$s$^{-1}$, providing redundant information for robust muon triggering, reconstruction and identification. [...]
CMS-CR-2024-336.- Geneva : CERN, 2024 - 8 p. Fulltext: PDF;
In : 17th International Conference on Resistive Plate Chambers and Related Detectors, Santiago de Compostela, 09 - 13 Sep 2024
3.
High-precision measurement of the W boson mass with the CMS experiment at the LHC / CMS Collaboration
In the standard model of particle physics, the masses of the carriers of the weak interaction, the W and Z bosons, are uniquely related. [...]
arXiv:2412.13872 ; CMS-SMP-23-002 ; CERN-EP-2024-308 ; CMS-SMP-23-002-003.
- 2024 - 73.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
4.
R&D; of the cluster finding algorithm for CMS iRPC detector / CMS Muon Collaboration
The Compact Muon Solenoid (CMS) experiment will undergo phase-II upgrade to enhance the capacity of detectors in the High-Luminosity Large Hadron Collider era. An important extension involves the installation of the Improved Resistive Plate Chambers (iRPC) in the most forward part of the endcap muon system. [...]
2024 - 12 p. - Published in : JINST 19 (2024) T12001
5.
Search for heavy neutral resonances decaying to tau lepton pairs in proton-proton collisions at $ \sqrt{s} = $ 13 TeV / CMS Collaboration
A search for heavy neutral gauge bosons (Z') decaying into a pair of tau leptons is performed in proton-proton collisions at $ \sqrt{s}= $ 13 TeV at the CERN LHC. [...]
arXiv:2412.04357 ; CMS-EXO-21-016 ; CERN-EP-2024-292 ; CMS-EXO-21-016-003.
- 2024 - 43.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
6.
Model-agnostic search for dijet resonances with anomalous jet substructure in proton-proton collisions at $ \sqrt{s} $ = 13 TeV / CMS Collaboration
This paper presents a model-agnostic search for narrow resonances in the dijet final state in the mass range 1.8-6 TeV. [...]
arXiv:2412.03747 ; CMS-EXO-22-026 ; CERN-EP-2024-291 ; CMS-EXO-22-026-003.
- 2024 - 55.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
7.
Measurement of the inclusive WZ production cross section in pp collisions at $ \sqrt{s}= $ 13.6 TeV / CMS Collaboration
The inclusive WZ production cross section is measured in proton-proton collisions at a centre-of-mass energy of 13.6 TeV, using data collected during 2022 with the CMS detector, corresponding to an integrated luminosity of 34.7 fb$ ^{-1} $. [...]
arXiv:2412.02477 ; CMS-SMP-24-005 ; CERN-EP-2024-293 ; CMS-SMP-24-005-003.
- 2024 - 45.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
8.
Search for heavy neutral Higgs bosons A and H in the $ {\mathrm{t}\overline{\mathrm{t}}} $Z channel in proton-proton collisions at 13 TeV / CMS Collaboration
A direct search for new heavy neutral Higgs bosons A and H in the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ channel is presented, targeting the process $ \mathrm{p}\mathrm{p}\to\mathrm{A}\to\mathrm{Z}\mathrm{H} $ with $ \mathrm{H}\to{\mathrm{t}\overline{\mathrm{t}}} $. [...]
arXiv:2412.00570 ; CMS-B2G-23-006 ; CERN-EP-2024-301 ; CMS-B2G-23-006-003.
- 2024 - 43.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
9.
Proton reconstruction with the TOTEM Roman pot detectors for high-$ \beta^* $ LHC data / CMS and TOTEM Collaboration
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. [...]
arXiv:2411.19749 ; CMS-SMP-23-006 ; CERN-EP-2024-273 ; TOTEM-2024-002 ; CMS-SMP-23-006-003.
- 2024 - 58.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
10.
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. [...]
arXiv:2411.16907 ; CMS-HIG-23-016 ; CERN-EP-2024-294 ; CMS-HIG-23-016-004.
- 2024 - 63.
Additional information for the analysis - CMS AuthorList - Fulltext - CMS HEPData - Fulltext - Fulltext

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89 Abbrescia, M.
1373 Abbrescia, Marcello
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