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CMS Physics Analysis Summaries

Latest additions:
2025-08-23
18:51
Search for s-channel production of lepton-enriched semivisible jets in proton-proton collisions at 13 TeV /CMS Collaboration
A search for resonant production of strongly-coupled dark matter manifesting as lepton-enriched semivisible jets in proton-proton collisions at the LHC is presented. The search is performed using data collected by the CMS experiment during 2016--2018 at a center-of-mass energy of 13 TeV corresponding to a total integrated luminosity of 138 fb1138 fb1. [...]
CMS-PAS-EXO-24-029.- Geneva : CERN, 2025 Figure_001: PDF; Figure_002: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)

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2025-08-23
18:00
Precision luminosity measurement in proton-proton collisions at sqrt{s} = 13 TeV with the CMS detector /CMS Collaboration
The measurement of the integrated luminosity recorded by the CMS detector at the LHC in proton-proton collisions at s=13 TeVs=13 TeV in 2017 and 2018 is reported. The absolute luminosity calibration is obtained with the van der Meer (vdM) method through beam-separation scans that were performed in special accelerator conditions. [...]
CMS-PAS-LUM-20-001.- Geneva : CERN, 2025 Figure_001-a: PDF; Figure_001-b: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: PDF; Figure_005: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_010-a: PDF; Figure_010-b: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Figure_012: PDF; Figure_013: PDF; Figure_014: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_015-c: PDF; Figure_015-d: PDF; Figure_016: PDF; Figure_017: PDF; Figure_018: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)

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2025-08-22
19:39
Search for charged Higgs bosons decaying into a top and a bottom quark in proton-proton collisions at sqrt{s} = 13 TeV /CMS Collaboration
A search is presented for charged Higgs bosons (H±H±) in proton-proton (pppp) collision events via the pp(q)H±pp(q)H± processes with H±tbH±tb decays. The analysis is based on the data collected at a center-of-mass energy of 13 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 138 fb1fb1. [...]
CMS-PAS-B2G-24-008.- Geneva : CERN, 2025 Figure_001-a: PDF; Figure_001-b: PDF; Figure_001-c: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_005-c: PDF; Figure_005-d: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)

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2025-08-14
19:30
Search for dark matter produced in association with a dark Higgs boson decaying into a bottom quark pair in proton-proton collisions at 13 TeV /CMS Collaboration
A search for dark matter produced in association with a dark Higgs boson decaying into a bottom quark pair has been performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector during the 2016-2018 data-taking period at the CERN LHC. The analyzed data sample corresponds to an integrated luminosity of 138 fb1fb1. [...]
CMS-PAS-SUS-23-013.- Geneva : CERN, 2025 Figure_001: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004: PDF; Figure_005: PDF; Figure_006: PDF; Figure_007: PDF; Figure_008: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)

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2025-08-02
14:42
Simultaneous measurements of NN-subjettiness observables in light-flavour quark and gluon jets, and in hadronic decays of boosted W bosons and top quarks /CMS Collaboration
A simultaneous measurement of twenty-five jet substructure observables is presented using large-radius jets with high transverse momentum from proton-proton collisions at s=13s=13 TeV. The measurement is carried out on QCD dijet events and t¯tt¯t events enriched in boosted, hadronic decays of W bosons and top quarks. [...]
CMS-PAS-SMP-22-003.- Geneva : CERN, 2025 Figure_001-a: PDF; Figure_001-b: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007: PDF; Figure_008: PDF; Figure_009: PDF; Figure_010: PDF; Figure_011: PDF; Figure_012: PDF; Figure_013-a: PDF; Figure_013-b: PDF; Figure_014-a: PDF; Figure_014-b: PDF; Figure_015-a: PDF; Figure_015-b: PDF; Figure_016-a: PDF; Figure_016-b: PDF; Figure_017-a: PDF; Figure_017-b: PDF; Figure_017-c: PDF; Figure_017-d: PDF; Figure_018-a: PDF; Figure_018-b: PDF; Figure_018-c: PDF; Figure_018-d: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)

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2025-08-02
09:45
Particle transformers for identifying Lorentz-boosted Higgs bosons decaying to a pair of W bosonsn /CMS Collaboration
A novel deep neural network classifier, the "particle transformer" (ParT), is introduced for the identification of highly Lorentz-boosted, multi-pronged jets in measurements and searches performed with the CMS detector at the LHC. Based on a self-attention mechanism that allows the model to weigh the importance of different particles, ParT is trained on a wide variety of topologies, notably demonstrating strong performance for the first time on jets originating from boosted Higgs boson decays to W bosons. [...]
CMS-PAS-JME-25-001.- Geneva : CERN, 2025 Figure_001: PDF; Figure_002: PDF; Figure_003: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_004-c: PDF; Figure_004-d: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_007: PDF; Figure_008-a: PDF; Figure_008-b: PDF; Figure_008-c: PDF; Figure_008-d: PDF; Figure_008-e: PDF; Figure_008-f: PDF; Figure_009-a: PDF; Figure_009-b: PDF; Figure_010: PDF; Figure_011-a: PDF; Figure_011-b: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)

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2025-07-27
20:29
A search for a heavy resonance decaying to a top quark and a new scalar in the boosted all-hadronic final state at s=s= 13 TeV /CMS Collaboration
A search for a heavy resonance decaying to a top quark and a neutral scalar boson ϕϕ in the all-hadronic final state is presented, where the ϕϕ boson candidate is identified by its decay into a bottom quark-antiquark pair. The search is focused on final states in which the decay products of the highly Lorentz-boosted top quark and ϕϕ boson are each expected to be reconstructed as single, large-radius jets with distinct substructures. [...]
CMS-PAS-B2G-22-001.- Geneva : CERN, 2025 Figure_001: PDF; Figure_002: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_003-c: PDF; Figure_003-d: PDF; Figure_004: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006: PDF; Figure_007: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)

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2025-07-21
14:00
Measurement of the t-channel single top quark cross section in pp collision data at sqrt(s) = 5.02 TeV /CMS Collaboration
The single top quark tt-channel production cross section is measured in proton-proton collisions at s=5.02s=5.02 TeV using data recorded in 2017, corresponding to an integrated luminosity of 302 pb1302 pb1. Events with one electron or muon and two or more jets, among which one or more are identified as coming from a b quark, are analyzed. [...]
CMS-PAS-TOP-24-011.- Geneva : CERN, 2025 Figure_001-a: PDF; Figure_001-b: PDF; Figure_002: PDF; Figure_003-a: PDF; Figure_003-b: PDF; Figure_004-a: PDF; Figure_004-b: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006: PDF; Figure_007: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)

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2025-07-18
21:08
Search for the pair production of long-lived supersymmetric partners of the tau lepton in proton-proton collisions at sqrt{s}=13 TeV /CMS Collaboration
Gauge-mediated supersymmetry breaking models provide a strong motivation to search for a supersymmetric partner of the tau lepton (stau) with a macroscopic lifetime. Long-lived stau decays produce tau leptons that are displaced from the primary proton-proton interaction vertex, leading to unconventional signatures in the detector. This study presents the first search for the direct production of long-lived staus decaying within the tracker volume in proton-proton collisions at s=13s=13 TeV, performed with a dedicated graph network-based identification algorithm for displaced tau leptons. The data sample used, corresponding to an integrated luminosity of 138 fb11, was recorded with the CMS experiment at the CERN LHC between 2016 and 2018. This search excludes at 95%95% confidence level stau masses in the 9029090290 (9045090450) GeV range for cτ0=50cτ0=50 mm in the maximally mixed (mass degenerate) scenario, while for m˜τ=200m~τ=200 GeV, stau proper lifetimes are excluded in the range 1513015130 (53905390) mm..
CMS-PAS-EXO-24-020.- Geneva : CERN, 2025 Figure_001: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_002-c: PDF; Figure_003: PDF; Figure_004: PDF; Figure_005-a: PDF; Figure_005-b: PDF; Figure_006-a: PDF; Figure_006-b: PDF; Figure_006-c: PDF; Figure_006-d: PDF; Figure_006-e: PDF; Figure_006-f: PDF; Figure_007-a: PDF; Figure_007-b: PDF; Figure_007-c: PDF; Figure_007-d: PDF; Figure_007-e: PDF; Figure_007-f: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)

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2025-07-15
11:02
Measurement of the photon-fusion production cross section of a pair of W bosons /CMS Collaboration
A measurement of the cross section of W boson pair production in photon fusion (γγWWγγWW) is presented, using an integrated luminosity of 138 fb1138 fb1 of proton-proton collision data collected in 2016-2018 at a center-of-mass energy of s=13 TeVs=13 TeV. Events are selected in the final state with one electron, one muon, and a low multiplicity of tracks associated with the electron-muon production vertex. [...]
CMS-PAS-SMP-24-019.- Geneva : CERN, 2025 Figure_001-a: PDF; Figure_001-b: PDF; Figure_002-a: PDF; Figure_002-b: PDF; Figure_003: PDF; Figure_004: PDF; Figure_005: PDF; Fulltext in PDF: PDF; External link: Additional information for the analysis (restricted access)

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