CERN Accelerating science

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1.
Search for resonant pair production of Higgs bosons in the $ \mathrm{b}\overline{\mathrm{b}}\mathrm{b}\overline{\mathrm{b}} $ final state using large-area jets in proton-proton collisions at $ \sqrt{s}= $ 13 TeV / CMS Collaboration
A search is presented for the resonant production of a pair of standard model-like Higgs bosons using data from proton-proton collisions at a centre-of-mass energy of 13 TeV, collected by the CMS experiment at the CERN LHC in 2016-2018, corresponding to an integrated luminosity of 138 fb$ ^{-1} $. [...]
arXiv:2407.13872 ; CMS-B2G-20-004 ; CERN-EP-2024-030 ; CMS-B2G-20-004-003.
- 2024 - 42.
Fermilab Library Server - Fulltext - Fulltext - Fulltext
2.
Status of QCD precision predictions for Drell-Yan processes / Alekhin, S. (Hamburg U., Inst. Theor. Phys. II) ; Amoroso, S. (DESY) ; Buonocore, L. (CERN) ; Huss, A. (CERN) ; Kallweit, S. (Zurich U.) ; Kardos, A. (U. Debrecen, Inst. Phys. ; MTA-DE, Debrecen ; Eotvos U.) ; Michel, J. (Amsterdam U. ; NIKHEF, Amsterdam) ; Moch, S. (Hamburg U., Inst. Theor. Phys. II) ; Petriello, F. (Northwestern U. ; Argonne) ; Rottoli, L. (Zurich U.) et al.
We compute differential distributions for Drell-Yan processes at the LHC and the Tevatron colliders at next-to-next-to-leading order in perturbative QCD, including fiducial cuts on the decay leptons in the final state. [...]
arXiv:2405.19714 ; DESY 24-073 ; CERN-TH-2024-068 ; ZU-TH 26/24 ; MPP-2024-106.
- 31 p.
Fulltext
3.
First measurement of the forward rapidity gap distribution in pPb collisions at $ \sqrt{\smash[b]{s_{_{\mathrm{NN}}}}} = $ 8.16 TeV / CMS Collaboration
For the first time at LHC energies, the forward rapidity gap spectra from proton-lead collisions for both proton and lead dissociation processes are presented. The analysis is performed over 10.4 units of pseudorapidity at a center-of-mass energy per nucleon pair of $ \sqrt{\smash[b]{s_{_{\mathrm{NN}}}}} = $ 8.16 TeV, almost 300 times higher than in previous measurements of diffractive production in proton-nucleus collisions. [...]
arXiv:2301.07630; CMS-HIN-18-019; CERN-EP-2022-164; CMS-HIN-18-019-003.- Geneva : CERN, 2023-11-01 - 25 p. - Published in : Phys. Rev. D 108 (2023) 092004 Fulltext: CMS-HIN-18-019-arXiv - PDF; 2301.07630 - PDF; Fulltext from Publisher: PDF; External links: Additional information for the analysis; CMS AuthorList
4.
Azimuthal correlations in Z+jets events in proton-proton collisions at $\sqrt{s}$ = 13 TeV / CMS Collaboration
The production of Z bosons associated with jets is measured in pp collisions at $ \sqrt{s}= $ 13 TeV with data recorded with the CMS experiment at the LHC corresponding to an integrated luminosity of 36.3 fb$ ^{-1} $. The multiplicity of jets with transverse momentum $ p_{\mathrm{T}} > $ 30 GeV is measured for different regions of the Z boson's $ p_{\mathrm{T}}(\mathrm{Z}) $, from lower than 10 GeV to higher than 100 GeV. [...]
arXiv:2210.16139; CMS-SMP-21-003; CERN-EP-2022-178; CMS-SMP-21-003-003.- Geneva : CERN, 2023-08-11 - 28 p. - Published in : Eur. Phys. J. C 83 (2023) 722 Fulltext: c60c1a67a239a0bbb60cebd10f1df446 - PDF; CMS-SMP-21-003-arXiv - PDF; 2210.16139 - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
5.
Measurements of jet multiplicity and jet transverse momentum in multijet events in proton-proton collisions at $ \sqrt{s}= $ 13 TeV / CMS Collaboration
Multijet events at large transverse momentum ($ p_{\mathrm{T}} $) are measured at $ \sqrt{s}= $ 13 TeV using data recorded with the CMS detector at the LHC, corresponding to an integrated luminosity of 36.3 fb$^{-1}$. The multiplicity of jets with $ p_{\mathrm{T}} > $ 50 GeV that are produced in association with a high-$ p_{\mathrm{T}} $ dijet system is measured in various ranges of the $ p_{\mathrm{T}} $ of the jet with the highest transverse momentum and as a function of the azimuthal angle difference $ \Delta\phi_{1,2} $ between the two highest $ p_{\mathrm{T}} $ jets in the dijet system. [...]
arXiv:2210.13557; CMS-SMP-21-006; CERN-EP-2022-144; CMS-SMP-21-006-003.- Geneva : CERN, 2023-08-22 - 25 p. - Published in : Eur. Phys. J. C 83 (2023) 742 Fulltext: CMS-SMP-21-006-arXiv - PDF; 803f4ed4711aa3d9018f9864b52cb6b8 - PDF; 2210.13557 - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
6.
Search for the exotic decay of the Higgs boson into two light pseudoscalars with four photons in the final state in proton-proton collisions at $ \sqrt{s} $ = 13 TeV / CMS Collaboration
A search for the exotic decay of the Higgs boson to a pair of light pseudoscalars, each of which subsequently decays into a pair of photons, is presented. The search uses data from proton-proton collisions at $\sqrt{s} = $ 13 TeV recorded with the CMS detector at the LHC that corresponds to an integrated luminosity of 132 fb$^{-1}$. [...]
arXiv:2208.01469; CMS-HIG-21-003; CERN-EP-2022-095; CMS-HIG-21-003-003.- Geneva : CERN, 2023-07-19 - 21 p. - Published in : JHEP 2307 (2023) 148 Fulltext: 2208.01469 - PDF; CMS-HIG-21-003-arXiv - PDF; cdef9798d8b4b639348f1bf1a1f1baef - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
7.
Search for direct pair production of supersymmetric partners of $\tau$ leptons in the final state with two hadronically decaying $\tau$ leptons and missing transverse momentum in proton-proton collisions at $\sqrt{s} = $ 13 TeV / CMS Collaboration
A search for the direct production of a pair of $\tau$ sleptons, the supersymmetric partners of $\tau$ leptons, is presented. Each $\tau$ slepton is assumed to decay to a $\tau$ lepton and the lightest supersymmetric particle (LSP), which is assumed to be stable and to not interact in the detector, leading to an imbalance in the total reconstructed transverse momentum. [...]
arXiv:2207.02254; CMS-SUS-21-001; CERN-EP-2022-032; CMS-SUS-21-001-003.- Geneva : CERN, 2023-07-01 - 30 p. - Published in : Phys. Rev. D 108 (2023) 012011 Fulltext: 2207.02254 - PDF; 9a6c32e7e91069453efa307bd98cb187 - PDF; CMS-SUS-21-001-arsiv - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
8.
Precision measurement of the Z boson invisible width in pp collisions at $\sqrt{s}$ = 13 TeV / CMS Collaboration
A precise measurement of the invisible width of the Z boson produced in proton-proton collisions at a center-of-mass energy of 13 TeV is presented using data recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 36.3 fb$^{-1}$. The result is obtained from a simultaneous fit to kinematic distributions for two data samples of Z boson plus jets: one dominated by Z boson decays to invisible particles and the other by Z boson decays to muon and electron pairs. [...]
arXiv:2206.07110; CMS-SMP-18-014; CERN-EP-2022-088; CMS-SMP-18-014-003.- 2023-05-22 - 14 p. - Published in : Phys. Lett. B 842 (2023) 137563 Fulltext: 2206.07110 - PDF; d8ee8d323b9ab80b63f3837ca02ace0c - PDF; CMS-SMP-18-014-arXiv - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
9.
Search for Higgs boson decays into Z and J/$\psi$ and for Higgs and Z boson decays into J/$\psi$ or $\Upsilon$ pairs in pp collisions at $\sqrt{s}$ = 13 TeV / CMS Collaboration
Decays of the Higgs boson into a Z boson and a J/$\psi$ or $\psi$(2S) meson are searched for in four-lepton final states with the CMS detector at the LHC. A data set of proton-proton collisions corresponding to an integrated luminosity of 138 fb$^{-1}$ is used. [...]
arXiv:2206.03525; CMS-HIG-20-008; CERN-EP-2022-074; CMS-HIG-20-008-003.- Geneva : CERN, 2023-05-18 - 25 p. - Published in : Phys. Lett. B 842 (2023) 137534 Fulltext: 2ece6549fd6ff60ed7e5af6a730bfbb4 - PDF; Publication - PDF; CMS-HIG-20-008-arXiv - PDF; 2206.03525 - PDF; Fulltext from Publisher: PDF; External link: Fermilab Library Server
10.
Combination of inclusive top-quark pair production cross-section measurements using ATLAS and CMS data at $\sqrt{s}= 7$ and 8 TeV / ATLAS Collaboration
A combination of measurements of the inclusive top-quark pair production cross-section performed by ATLAS and CMS in proton-proton collisions at centre-of-mass energies of 7 and 8 TeV at the LHC is presented. The cross-sections are obtained using top-quark pair decays with an opposite-charge electron-muon pair in the final state and with data corresponding to an integrated luminosity of about 5 fb$^{-1}$ at $\sqrt{s}=7$ TeV and about 20 fb$^{-1}$ at $\sqrt{s}=8$ TeV for each experiment. [...]
arXiv:2205.13830; CERN-EP-2021-222; CMS-TOP-18-014; CERN-LPCC-2022-03.- 2023-07-27 - 59 p. - Published in : JHEP 2307 (2023) 213 Fulltext: PDF; Fulltext from Publisher: PDF; External link: Previous draft version

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1151 TROCSANYI, Zoltan Laszlo
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