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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

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Jet Tagging with More-Interaction Particle Transformer / Wu, Yifan (Shanghai U. Sci. Tech.) ; Wang, Kun (Shanghai U. Sci. Tech.) ; Li, Congqiao (Peking U., SKLNPT) ; Qu, Huilin (CERN) ; Zhu, Jingya (Henan U.)
In this study, we introduce the More-Interaction Particle Transformer (MIParT), a novel deep learning neural network designed for jet tagging [...]
arXiv:2407.08682. - 12.
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A Lorentz-Equivariant Transformer for All of the LHC / Brehmer, Johann (Unlisted, NL) ; Bresó, Víctor (U. Heidelberg, ITP) ; de Haan, Pim (Unlisted, NL) ; Plehn, Tilman (U. Heidelberg, ITP ; U. Heidelberg (main)) ; Qu, Huilin (CERN) ; Spinner, Jonas (U. Heidelberg, ITP) ; Thaler, Jesse (MIT, Cambridge, CTP)
We show that the Lorentz-Equivariant Geometric Algebra Transformer (L-GATr) yields state-of-the-art performance for a wide range of machine learning tasks at the Large Hadron Collider. [...]
MIT-CTP/5802 ; arXiv:2411.00446. - 26.
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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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10.

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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似た著者名：
115	Qu, H
2	Qu, H M
19	Qu, H.
3	Qu, Hang
1	Qu, Hao
4	Qu, Hua Min
2	Qu, Hua-Min
2	Qu, Hua-min
4	Qu, Huamin
1	Qu, Hui-Peng
1	Qu, Hui-Xue

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