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CMS Papers

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2025-10-24
19:38
Search for dijet resonances with data scouting in proton-proton collisions at $ \sqrt{s} = $ 13 TeV
A search is presented for narrow resonances, with a mass between 0.6 and 1.8 TeV, decaying to pairs of jets, in proton-proton collisions at $ \sqrt{s} = $ 13 TeV. [...]
CERN-EP-2025-212 ; CMS-EXO-23-004-003. - 2025
Additional information for the analysis - CMS AuthorList - Fulltext - CMS HEPData

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2025-10-22
12:24
Observation of tWZ production at the CMS experiment / CMS Collaboration
The first observation of single top quark production in association with a W and a Z boson in proton-proton collisions is reported. [...]
arXiv:2510.19080 ; CMS-TOP-24-009 ; CERN-EP-2025-205 ; CMS-TOP-24-009-003. - 2025 - 37 p, 37.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext

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2025-10-14
13:52
Search for dark matter production in association with bottom quarks and a lepton pair in proton-proton collisions at $ \sqrt{s}= $ 13 TeV / CMS Collaboration
A search is performed for dark matter produced in association with bottom quarks and a pair of electrons or muons in data collected with the CMS detector at the LHC, corresponding to 138 fb$ ^{-1} $ of integrated luminosity of proton-proton collisions at a center-of-mass energy of 13 TeV. [...]
arXiv:2510.12396 ; CMS-SUS-23-018 ; CERN-EP-2025-119 ; CMS-SUS-23-018-003. - 2025 - 51.
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2025-10-11
16:58
Performance of heavy-flavour jet identification in Lorentz-boosted topologies in proton-proton collisions at $ \sqrt{s} = $ 13 TeV / CMS Collaboration
Measurements in the highly Lorentz-boosted regime provoke increased interest in probing the Higgs boson properties and in searching for particles beyond the standard model at the LHC. [...]
arXiv:2510.10228 ; CMS-BTV-22-001 ; CERN-EP-2025-161 ; CMS-BTV-22-001-003. - 2025 - 67.
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2025-10-11
08:17
Discovery of suppressed charged-particle production in ultrarelativistic oxygen-oxygen collisions / CMS Collaboration
A hot and dense state of nuclear matter, known as the quark-gluon plasma, is created in collisions of ultrarelativistic heavy nuclei. [...]
arXiv:2510.09864 ; CMS-HIN-25-008 ; CERN-EP-2025-226 ; CMS-HIN-25-008-003. - 2025 - 39.
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2025-10-09
06:32
Combination of searches for nonresonant Higgs boson pair production in proton-proton collisions at $ \sqrt{s}= $ 13 TeV
This paper presents a combination of searches for the nonresonant production of Higgs boson pairs (HH) in proton-proton collisions at a centre-of-mass energy of 13 TeV. [...]
CMS-HIG-20-011 ; CERN-EP-2025-214 ; arXiv:2510.07527 ; CMS-HIG-20-011-003. - 2025 - 60.
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2025-10-04
15:29
Observation of long-range collective flow in OO and NeNe collisions and implications for nuclear structure studies / CMS Collaboration
The long-range collective flow of particles produced in oxygen-oxygen (OO) and neon-neon (NeNe) collisions is measured with the CMS detector at the CERN LHC. [...]
arXiv:2510.02580 ; CMS-HIN-25-009 ; CERN-EP-2025-222 ; CMS-HIN-25-009-003. - 2025 - 35.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext

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2025-10-04
12:59
Wasserstein normalized autoencoder for anomaly detection / CMS Collaboration
A novel anomaly detection algorithm is presented. [...]
arXiv:2510.02168 ; CMS-MLG-24-002 ; CERN-EP-2025-209 ; CMS-MLG-24-002-003. - 2025 - 47.
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2025-10-01
00:08
Vector boson scattering and anomalous quartic couplings in final states with $ \ell\nu\mathrm{q}\mathrm{q} $ or $ \ell\ell\mathrm{q}\mathrm{q} $ plus jets using proton-proton collisions at $ \sqrt{s} = $ 13 TeV / CMS Collaboration
A measurement is presented of the electroweak vector boson scattering production of ZV (V $ = $ W, Z) boson pairs associated with two jets in proton-proton collisions at a center-of-mass energy of 13 TeV. [...]
arXiv:2510.00118 ; CMS-SMP-22-011 ; CERN-EP-2025-147 ; CMS-SMP-22-011-003. - 2025 - 45.
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2025-09-30
23:54
Measurement of the dineutrino system kinematic variables in dileptonic top quark pair production in proton-proton collisions at $ \sqrt{s}= $ 13 TeV / CMS Collaboration
Differential top quark pair production cross sections are measured in the dilepton final states $ \mathrm{e}^+\mathrm{e}^- $, $ \mu^{+}\mu^{-} $, and $ \mathrm{e}^{\pm}\mu^{\mp} $, as a function of kinematic variables of the two-neutrino system: the transverse momentum $ p_{\mathrm{T}}^{\nu\nu} $ of the dineutrino system, the minimum distance in azimuthal angle between $ {\vec p}_{\mathrm{T}}^{\,\nu\nu} $ and leptons, and in two dimensions in bins of both observables. [...]
arXiv:2510.00160 ; CMS-TOP-24-001 ; CERN-EP-2025-201 ; CMS-TOP-24-001-003. - 2025 - 47.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext

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