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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

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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

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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

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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

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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

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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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Search for rare decays of the Z and Higgs bosons to a $ \mathrm{J}/\psi $ or $\psi(2\text{S})$ meson and a photon in proton-proton collisions at $ \sqrt{s} = $ 13 TeV / CMS Collaboration
A search is presented for rare decays of the Z and Higgs bosons to a photon and a $ \mathrm{J}/\psi $ or a $\psi(2\text{S})$ meson, with the charmonium state subsequentially decaying to a pair of muons. [...]
arXiv:2411.15000 ; CMS-SMP-22-012 ; CERN-EP-2024-253 ; CMS-SMP-22-012-003. - 2024 - 39.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext

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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

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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

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10.

Precision Timing with the CMS MIP Timing Detector for High-Luminosity LHC / Cossutti, Fabio (INFN, Trieste) /CMS Collaboration
The Compact Muon Solenoid (CMS) detector at the CERN Large Hadron Collider (LHC) is undergoing an extensive Phase 2 upgrade program to prepare for the challenging conditions of the High-Luminosity LHC (HL-LHC). A new timing detector for CMS will measure minimum ionizing particles (MIPs) with a time resolution of ~30-40 ps. [...]
CMS-CR-2024-219.- Geneva : CERN, 2024 - 7 p. Fulltext: PDF;
In : 42nd International Conference on High Energy Physics (ICHEP 2024), Prague, Czech Republic, 18 - 24 Jul 2024

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576	Cossutti, F
139	Cossutti, F.

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