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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

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

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

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

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

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

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

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} $. [...]
arXiv:2411.11820 ; CMS-BPH-21-002 ; CERN-EP-2024-268 ; CMS-BPH-21-002-003. - 2024 - 39.
Additional information for the analysis - CMS AuthorList - Fulltext - CMS HEPData - Fulltext

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. [...]
arXiv:2411.03023 ; CMS-MLG-24-001 ; CERN-EP-2024-269 ; CMS-MLG-24-001-003. - 2024 - 49.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext

10.

Measurements of inclusive and differential cross sections for top quark production in association with a Z boson in proton-proton collisions at $ \sqrt{s}= $ 13 TeV / CMS Collaboration
Measurements are presented of inclusive and differential cross sections for Z boson associated production of top quark pairs ($ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $) and single top quarks ($ \mathrm{t}\mathrm{Z}\mathrm{q} $ or $ \mathrm{t}\mathrm{W}\mathrm{Z} $). [...]
arXiv:2410.23475 ; CMS-TOP-23-004 ; CERN-EP-2024-251 ; CMS-TOP-23-004-003. - 2024 - 52.
Fermilab Library Server - Fulltext - Fulltext - Fulltext

Se också: liknande författarnamn
3	Devetak, D
4	Devetak, D.

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