{"total":45,"items":[{"citing_arxiv_id":"2606.26832","ref_index":19,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Precision luminosity measurement in proton-proton collisions at a center-of-mass energy of 13 TeV with the CMS detector at the Large Hadron Collider","primary_cat":"hep-ex","submitted_at":"2026-06-25T10:14:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"CMS reports 0.73% precision on integrated luminosity for the full 13 TeV dataset by calibrating multiple monitors via beam-separation scans and validating stability with Z boson rates.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.25840","ref_index":32,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for long-lived particles decaying into muons in proton-proton collisions at $\\sqrt{s}$ = 13.6 TeV using data scouting","primary_cat":"hep-ex","submitted_at":"2026-06-24T13:51:53+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Null result from dimuon scouting search at 13.6 TeV sets 95% CL limits on long-lived particle production in Higgs and b-hadron decay channels across multiple BSM models.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.20558","ref_index":12,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Observation of electroweak production of pairs of Z bosons in proton-proton collisions at 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-06-18T17:59:33+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"CMS provides first evidence for electroweak ZZjj production in the ℓℓννjj final state with measured cross section 0.37 fb agreeing with SM prediction 0.39 fb at 3.1σ (5.0σ combined), plus limits on anomalous quartic gauge couplings.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.09567","ref_index":33,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for new physics using single-lepton events with high multiplicities of jets and b jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-06-08T14:41:05+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"No significant excess found in single-lepton high-multiplicity jet events; gluino masses below 1890 GeV excluded at 95% CL in R-parity violating SUSY model.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.03510","ref_index":45,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Analysis of the $C\\!P$ structure of the Yukawa coupling between the Higgs boson and tau leptons in proton-proton collisions at $\\sqrt{s}$ = 13.6 TeV","primary_cat":"hep-ex","submitted_at":"2026-06-02T11:28:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Combined CMS result gives α^{Hττ} = 7 ± 16° for the CP mixing angle in H→ττ, consistent with SM expectation of 0 ± 14°.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[42] ATLAS Collaboration, \"Measurement of the CP properties of Higgs boson interactions withτ-leptons with the ATLAS detector\",Eur. Phys. J. C83(2023) 563, doi:10.1140/epjc/s10052-023-11583-y,arXiv:2212.05833. [43] \"HEPData record for this analysis\", 2026.doi:10.17182/hepdata.172938. [44] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [45] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [46] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165. [47] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2606.02285","ref_index":37,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Centrality dependence of charged-hadron pseudorapidity distributions in oxygen-oxygen collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.36 TeV","primary_cat":"nucl-ex","submitted_at":"2026-06-01T14:07:59+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"First measurement of dNch/dη in OO collisions at 5.36 TeV yields midrapidity densities of 41.8 overall and 135 in central events, consistent with PbPb per participant but showing deviations from simple scaling.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.01423","ref_index":19,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for single production of a vector-like B' quark decaying to a top quark and a W boson in the single-lepton final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-05-31T19:46:24+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"CMS excludes narrow-width singlet vector-like B' quarks with masses 0.8-1.23 TeV in the tW channel using neural-network tagging and data-driven background modeling.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.27875","ref_index":35,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for light scalar particles produced in Higgs boson decays in exclusive final states with two muons and two hadrons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-05-27T02:51:39+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"CMS obtains O(10^{-4}) upper limits on Higgs branching fraction to light scalars (0.4-2 GeV) decaying to muon-hadron pairs with lifetimes up to ~1 mm.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.19144","ref_index":60,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for Higgs boson decays into two neutral scalars with unequal masses in final states with b quarks and tau leptons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-05-18T21:51:39+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"No statistically significant excess is observed in the search for Higgs decays to two neutral scalars with unequal masses, setting 95% CL upper limits between 0.9 and 36.8 pb depending on mass and decay scenario.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15396","ref_index":33,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"First measurements of vector boson scattering in W$^\\pm$W$^{\\pm}$ and WZ production in all-leptonic final states at $\\sqrt{s}$ = 13.6 TeV","primary_cat":"hep-ex","submitted_at":"2026-05-14T20:29:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"CMS observes electroweak W±W± and WZ production with two jets at 13.6 TeV with >5σ significance in all-leptonic final states using 171 fb⁻¹ of data.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15023","ref_index":14,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for new physics in triple boson production in proton-proton collisions at $\\sqrt{s}$ = 13 TeV using the effective field theory approach","primary_cat":"hep-ex","submitted_at":"2026-05-14T16:22:47+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"No excess in VVV production; bounds set on c_W/Λ² (-0.13 to 0.12 TeV^{-2}) and c_Hq3/Λ² (-0.24 to 0.21 TeV^{-2}) at 95% CL.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.14245","ref_index":34,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Constraints on anomalous Higgs boson couplings to vector bosons and fermions using the $\\gamma\\gamma$ final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-05-14T01:22:19+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Updated constraints from the full Run 2 dataset show no evidence for anomalous Higgs couplings in gluon fusion, vector boson fusion, and associated production modes decaying to two photons.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"arXiv:2109.13808. Published inEur. Phys. J. C. [32] J. F. Gunion and X.-G. He, \"Determining the cp nature of a neutral higgs boson at the cern large hadron collider\",Phys. Rev. Lett.76(Jun, 1996) 4468, doi:10.1103/PhysRevLett.76.4468. [33] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [34] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [35] CMS Collaboration, \"Constraints on anomalous Higgs boson couplings from its production and decay using the WW channel in proton-proton collisions at√s=13 TeV\",Eur. Phys. J. C84(2024) 779, doi:10."},{"citing_arxiv_id":"2605.13649","ref_index":16,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for single vector-like quark production in opposite-sign dilepton final states in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-05-13T15:07:25+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"No excess observed in search for vector-like top quark T to tH in opposite-sign dilepton final states; 95% CL upper limits on sigma times BR range from 2.0 pb at 600 GeV to 0.1 pb at 1000 GeV.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[13] CMS Collaboration, \"Search for production of a single vector-like quark decaying to tH or tZ in the all-hadronic final state in pp collisions at √s=13 TeV\",Phys. Rev. D110 (2024) 072012,doi:10.1103/PhysRevD.110.072012,arXiv:2405.05071. [14] HEPData record for this analysis, 2026.doi:10.17182/hepdata.166760. [15] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [16] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [17] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020, doi:10.1088/1748-0221/12/01/P01020,arXiv:1609.02366. [18] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions"},{"citing_arxiv_id":"2605.13614","ref_index":49,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for pair production of additional neutral scalars within the Inert Doublet Model in a final state with two electrons or two muons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV and 13.6 TeV","primary_cat":"hep-ex","submitted_at":"2026-05-13T14:45:01+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"No significant excess found; new exclusion limits reach m_H = 108 GeV for m_H - m_A = 78 GeV in the Inert Doublet Model.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"the high-level trigger (HLT), is a software-based system that runs a version of the full event reconstruction optimised for fast processing, reducing the event rate to about 1 to 5 kHz. A detailed description of the CMS detector, together with a definition of the coordinate system used and the relevant kinematic variables, is given in Ref. [48]. The upgraded configuration of the detector for the LHC Run 3 is given in Ref. [49]. 4 Data and simulated samples Data were recorded with several triggers, as detailed in Section 6, during the LHC Run 2 (2016-2018) and part of Run 3 (2022), for integrated luminosities corresponding to 138 fb −1 and 35 fb−1, respectively. The IDM signal samples were generated at LO using MADGRAPH5 aMC@NLOv2.6.7 [50]. The input model is taken from Ref."},{"citing_arxiv_id":"2605.02848","ref_index":35,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for a new heavy scalar resonance decaying into the Higgs boson and a new scalar particle in the $\\mathrm{b}\\bar{\\mathrm{b}}\\mathrm{b}\\bar{\\mathrm{b}}$ final state using proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-05-04T17:25:03+00:00","verdict":"ACCEPT","verdict_confidence":"MODERATE","novelty_score":5.0,"formal_verification":"none","one_line_summary":"No evidence found for a new heavy scalar resonance X decaying to Higgs plus new scalar Y in the four-bottom-quark final state; 95% CL upper limits set on cross section times branching fraction.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"[32] ATLAS Collaboration, \"Combination of searches for Higgs boson pair production in pp collisions at √s= 13 TeV with the ATLAS detector\",Phys. Rev. Lett.133(2024) 101801, doi:10.1103/PhysRevLett.133.101801,arXiv:2406.09971. References 19 [33] HEPData record for this analysis, 2026.doi:10.17182/hepdata.154245. [34] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [35] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [36] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165. [37] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2605.00615","ref_index":22,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Observation of the rare decay $\\eta$ $\\to$ $\\mu^+\\mu^-$e$^+$e$^-$","primary_cat":"hep-ex","submitted_at":"2026-05-01T12:32:29+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"CMS observes η → μ⁺μ⁻e⁺e⁻ for the first time and measures its branching fraction as (2.4 ± 0.8) × 10^{-6}.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[19] CELSIUS/WASA Collaboration, \"Measurement ofηmeson decays into lepton-antilepton pairs\",Phys. Rev. D77(2008) 032004,doi:10.1103/PhysRevD.77.032004, arXiv:0711.3531. [20] HEPData record for this analysis, 2026.doi:10.17182/hepdata.168684. [21] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [22] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. 10 [23] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165. [24] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2604.27795","ref_index":23,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for light charged Higgs bosons decaying to charm and strange quarks in $\\mathrm{t\\bar{t}}$ events in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-04-30T12:40:10+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"No evidence found for light charged Higgs bosons in ttbar events; upper limits set on B(t to H±b) of 0.07-1.12% at 95% CL for masses 40-160 GeV assuming 100% decay to cs.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"H± →cs, in pp collisions at √s=13 TeV with the ATLAS detector\",Eur. Phys. J. C85 (2025) 112,doi:10.1140/epjc/s10052-024-13715-4,arXiv:2407.10096. [21] HEPData record for this analysis, 2026.doi:10.17182/hepdata.167415. [22] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2003) S08004, doi:10.1088/1748-0221/3/08/S08004,arXiv:0803.2024. [23] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064. [24] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165. [25] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2604.27091","ref_index":14,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Measurement of the top quark pair production cross section in PbPb collisions at $\\sqrt{s_\\mathrm{NN}}$ = 5.36 TeV","primary_cat":"nucl-ex","submitted_at":"2026-04-29T18:36:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"The ttbar production cross section in PbPb collisions at 5.36 TeV is measured as 3.42 +0.54-0.51 (stat) +0.50-0.43 (syst) μb and is consistent with NNLO pQCD predictions using nuclear PDFs.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[11] ATLAS Collaboration, \"Observation of t t production in Pb+Pb collisions at√sNN =5.02 TeV with the ATLAS detector\",Phys. Rev. Lett.134(2025) 142301, doi:10.1103/PhysRevLett.134.142301,arXiv:2411.10186. [12] HEPData record for this analysis, 2026.doi:10.17182/hepdata.168317. [13] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [14] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024), no. 05, P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [15] CMS Collaboration, \"Performance of the CMS level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165. [16] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2604.27044","ref_index":35,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Improved results on Higgs boson pair production in the 4b final state","primary_cat":"hep-ex","submitted_at":"2026-04-29T17:54:15+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"CMS sets an observed upper limit of 4.4 on the HH signal strength μ_HH in the 4b final state at 13.6 TeV, improving prior LHC results by more than a factor of two in the resolved topology.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"5, with at least two of them identified as b jets by means of a selection on their PNET@HLTb jet output score,P b. In 2022, this trigger operated at a data output rate of ap- proximately 60 Hz, with jetp T thresholds at 70, 50, 40, and 35 GeV on the fourp T-leading AK4 jets, respectively. In 2023, a larger allocated rate, up to 150 Hz, was made possible by the development of a dedicated data parking stream, denoted \"ParkingHH\" [35, 81, 82]. The ParkingHH trigger was re-optimized with looser jetp T thresholds, set at 30 GeV for all four leading AK4 jets, as well as a looser selection on theP b score. With the ParkingHH strategy, the absolute trigger acceptance for the SM HH→4b signal increased by about 22% relative to the 2022 data-taking conditions, at a cost of more than twice the background rate."},{"citing_arxiv_id":"2604.25604","ref_index":25,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for electroweakinos in compressed-spectrum scenarios with low-momentum isolated tracks in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-04-28T13:09:44+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"No significant excess observed; 95% CL exclusion of higgsino electroweakinos with mass splittings 0.28-1.15 GeV and chargino masses up to 185 GeV using soft-track and neural-network selection.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"1103/PhysRevLett.132.221801,arXiv:2401.14046. [23] ATLAS Collaboration, \"Search for higgsinos in compressed mass spectra using low-momentum tracks in pp collisions at √s=13 TeV with the ATLAS detector\", 2025. arXiv:2511.20042. Submitted toJHEP. [24] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [25] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [26] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017,doi:10.1088/1748-0221/15/10/P10017, arXiv:2006.10165. [27] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2604.25538","ref_index":53,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Simultaneous measurements of $N$-subjettiness observables in jets from gluons and light-flavour quarks, and in decays of boosted W bosons and top quarks","primary_cat":"hep-ex","submitted_at":"2026-04-28T12:04:54+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"CMS reports a simultaneous measurement of 25 N-subjettiness observables in 1-, 2-, and 3-prong jets, unfolded to stable particles with particle-level correlations for QCD modeling.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Thaler, \"Jet shapes with the broadening axis\",JHEP04 (2014) 017,doi:10.1007/JHEP04(2014)017,arXiv:1401.2158. [51] A. J. Larkoski and J. Thaler, \"Aspects of jets at 100 TeV\",Phys. Rev. D90(2014) 034010, doi:10.1103/PhysRevD.90.034010,arXiv:1406.7011. [52] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [53] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [54] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165. [55] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2604.24531","ref_index":11,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for associated production of a Higgs boson and two vector bosons via vector boson scattering at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-04-27T14:30:10+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"CMS excludes κ_VV outside 0.40-1.60 at 95% CL and constrains κ_2W and κ_2Z using VBS events with a boosted Higgs to bb decay.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"1007/JHEP07(2014)079,arXiv:1405.0301. [9] CMS Collaboration, \"Search for Higgs boson pair production with one associated vector boson in proton-proton collisions at √s=13 TeV\",JHEP10(2024) 061, doi:10.1007/JHEP10(2024)061,arXiv:2404.08462. [10] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [11] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [12] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017,doi:10.1088/1748-0221/15/10/P10017, arXiv:2006.10165. [13] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2604.20999","ref_index":19,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for dark matter produced in association with a dark Higgs boson decaying into a bottom quark-antiquark pair in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-04-22T18:41:48+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"New upper limits exclude mediator masses up to 4.5 TeV for a 50 GeV dark Higgs and up to 2.5 TeV for 150 GeV in a spin-1 mediator dark matter model, the most stringent to date for these masses.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"To avoid events with anomalousUdue to reconstruction failures of the PF algorithm, events are required to have|p miss T (PF)−p miss T (calorimeter)|/U<0.5, wherep miss T (PF)refers to the standardp miss T computed from PF candidates as defined in Section 2, whilepmiss T (calorimeter)is thep miss T calculated using only information from the calorimeters. To mitigate mismeasurement from a nonfunctioning HCAL section in the 2018 data [19], events with jets in that region or withϕ( ⃗p miss T )∈[−1.62,−0.62]atp miss T <470 GeV are rejected. As shown in Table 1, even after the full SR selection is applied, the selected data sample still 7 has a large contamination from Z+jets, W+jets, and tt production. In order to characterize and constrain these background processes, dedicated control regions (CRs) are used."},{"citing_arxiv_id":"2604.17564","ref_index":26,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for the single production of vector-like quarks decaying into a W boson and a b quark using single-lepton final states in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-04-19T18:10:43+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"No significant excess observed in search for vector-like quark single production to Wb, setting 95% CL upper limits on κ_W as low as 0.086 near 1.4 TeV mass and excluding masses below 2.4 TeV at κ_W=0.2.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"arXiv:2409.20273v2. [24] ATLAS Collaboration, \"Search for single production of vector-like quarks decaying into W(ℓν)b in pp collisions at √s=13 TeV with the ATLAS detector\",JHEP12(2025) 012, doi:10.1007/JHEP12(2025)012,arXiv:2506.15515. [25] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [26] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [27] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165. [28] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2604.14236","ref_index":10,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for heavy resonances decaying into four-lepton final states via light bosons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-04-14T22:17:26+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"No significant excess observed in four-lepton events from heavy resonances, setting upper limits on production cross sections for dilepton masses 0.4-15 GeV using novel merged-object techniques.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"References 9 [8] ATLAS Collaboration, \"Search for a new scalar decaying into new spin-1 bosons in four-lepton final states with the ATLAS detector\",Phys. Lett. B865(2025) 139472, doi:10.1016/j.physletb.2025.139472,arXiv:2410.16781. [9] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [10] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064. [11] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020, doi:10.1088/1748-0221/12/01/P01020,arXiv:1609.02366. [12] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions"},{"citing_arxiv_id":"2604.13320","ref_index":10,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Highly boosted dielectron identification in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-04-14T21:56:57+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"CMS develops two multivariate models for identifying boosted dielectrons with γ_L > 20, reporting 80% efficiency for two-track cases from J/ψ data and 60% for single-track from Z conversions, plus an energy correction.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"1007/JHEP06(2023)036,arXiv:2209.15345. 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[12] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2604.10732","ref_index":28,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"A search for microscopic black holes, string balls, and sphalerons in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-04-12T17:12:30+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"No evidence found; excludes semiclassical black holes below 8.4-11.4 TeV and string balls below 9.0-10.7 TeV at 95% CL, and caps the quark-quark sphaleron fraction above 9 TeV at 0.0034.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"[25] CMS Collaboration, \"Search for black holes in high-multiplicity final states in proton-proton collisions at √s=13 TeV\",Phys. Lett. B774(2017) 279, doi:10.1016/j.physletb.2017.09.053,arXiv:1705.01403. 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[16] HEPData record for this analysis, 2026.doi:10.17182/hepdata.167416. [17] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [18] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [19] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165. [20] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2604.09809","ref_index":33,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Particle transformers for identifying Lorentz-boosted Higgs bosons decaying to a pair of W bosons","primary_cat":"hep-ex","submitted_at":"2026-04-10T18:33:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"PaRT achieves >50% tagging efficiency for boosted H->WW jets at 1% background efficiency, decorrelated from jet mass, with data-to-simulation scale factors of 0.9-1.0 on 138 fb^{-1} of 13 TeV collisions.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"the Lund jet plane\",JHEP11(2025) 038,doi:10.1007/JHEP11(2025)038, arXiv:2507.07775. 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[35] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2604.02594","ref_index":15,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Evidence of ZZ$\\gamma$ production and observation of $4\\ell\\gamma$ in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-04-03T00:11:48+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"First evidence for ZZ gamma production at 3.7 sigma and observation of 4 lepton gamma at 5.0 sigma in CMS data at 13 TeV, with measured fiducial cross sections consistent with predictions.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[12] CMS Collaboration, \"Stairway to discovery: a report on the CMS programme of cross section measurements from millibarns to femtobarns\",Phys. Rep.1115(2025) 3, doi:10.1016/j.physrep.2024.11.005,arXiv:2405.18661. [13] HEPData record for this analysis, 2026.doi:10.17182/hepdata.167735. [14] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [15] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [16] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017,doi:10.1088/1748-0221/15/10/P10017, arXiv:2006.10165. [17] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2602.11359","ref_index":17,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"High-level hadronic tau lepton triggers of the CMS experiment in proton-proton collisions at $\\sqrt{s}$ = 13.6 TeV","primary_cat":"physics.ins-det","submitted_at":"2026-02-11T20:46:53+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"CMS deployed ML-based high-level triggers for hadronic tau leptons with high efficiency and low compute cost, validated on 62 fb^{-1} of 2022-2023 data.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2512.00502","ref_index":19,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Measurements of electroweak production of a photon in association with two jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2025-11-29T14:16:21+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"First observation of electroweak photon plus two jets production yields a cross section of 202 fb consistent with the standard model prediction of 177 fb at greater than 5 sigma significance.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.19563","ref_index":19,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for light pseudoscalar bosons, pair-produced in Higgs boson decays in the four-electron final state in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2025-11-24T15:36:17+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"No excess observed; first LHC search sets 95% CL upper limits on H to AA to 4e branching fraction down to 10^{-5} for 10-100 MeV masses and short lifetimes.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.17310","ref_index":14,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for new physics in the final state with a single photon and large missing transverse momentum in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2025-11-21T15:25:58+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Combined LHC data shows no deviation from the standard model in single-photon plus missing momentum events, establishing the strongest limits to date on simplified dark matter models and large extra dimensions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.16394","ref_index":41,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for Higgsinos in final states with low-momentum lepton-track pairs at 13 TeV","primary_cat":"hep-ex","submitted_at":"2025-11-20T14:13:31+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.10666","ref_index":33,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Jet fragmentation function and groomed substructure of bottom quark jets in proton-proton collisions at 5.02 TeV","primary_cat":"hep-ex","submitted_at":"2025-11-06T19:14:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"CMS measures soft-drop groomed radius and momentum balance plus a charged fragmentation function for b jets, observing dead-cone suppression compared to inclusive jets.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.01995","ref_index":22,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Inclusive and differential measurements of the $\\mathrm{t\\bar{t}}\\gamma$ cross section and the $\\mathrm{t\\bar{t}}\\gamma$ / $\\mathrm{t\\bar{t}}$ cross section ratio in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2025-11-03T19:08:32+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"CMS reports fiducial and differential ttγ cross sections plus ttγ/tt ratios at 13 TeV that agree with Standard Model expectations within uncertainties.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.21641","ref_index":40,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for dijet resonances with data scouting in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2025-10-24T16:54:45+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Search for narrow dijet resonances in the 0.6-1.8 TeV mass range with data scouting in 117 fb^{-1} of 13 TeV data finds no significant signal and sets model-independent upper limits on various resonance types and dark matter mediator couplings.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.09864","ref_index":85,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Observation of suppressed charged-particle production in ultrarelativistic oxygen-oxygen collisions","primary_cat":"nucl-ex","submitted_at":"2025-10-10T20:56:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"First measurement of the nuclear modification factor R_AA in OO collisions at 5.36 TeV shows suppression with a minimum of 0.69 at p_T around 6 GeV, favoring models with parton energy loss.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.00160","ref_index":31,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Measurement of the dineutrino system kinematic variables in dileptonic top quark pair production in proton-proton collisions at$\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2025-09-30T18:29:48+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Differential cross sections for ttbar production in e+e-, mu+mu-, and e mu channels measured versus dineutrino pT and azimuthal separation using 138 fb-1 of 13 TeV CMS data, unfolded to particle level with unregularized least squares and found consistent with SM and MC predictions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2509.08626","ref_index":22,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Measurement of D$^0$ meson photoproduction in ultraperipheral heavy ion collisions","primary_cat":"nucl-ex","submitted_at":"2025-09-10T14:21:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":8.0,"formal_verification":"none","one_line_summary":"First measurement of photonuclear D0 production cross section in ultraperipheral PbPb collisions as a function of pT and rapidity, compared to NLO pQCD with nuclear PDFs and CGC predictions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2508.06947","ref_index":37,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for light pseudoscalar boson pairs produced from Higgs boson decays using the 4$\\tau$ and 2$\\mu$2$\\tau$ final states in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2025-08-09T11:43:00+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"No excess observed in search for Higgs to a1 a1 decays; 95% CL upper limits on branching ratio range 0.007-0.079 for a1 masses 4-15 GeV, excluding >16% in Type III 2HD+S for tan beta >2.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2504.13081","ref_index":18,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Combination and interpretation of differential Higgs boson production cross sections in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2025-04-17T16:48:08+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Combined differential and total Higgs boson production cross sections at 13 TeV are measured and found consistent with Standard Model expectations, with a total cross section of 53.4 pb.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2504.02958","ref_index":42,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Combined effective field theory interpretation of Higgs boson, electroweak vector boson, top quark, and multi-jet measurements","primary_cat":"hep-ex","submitted_at":"2025-04-03T18:27:21+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"CMS performs a combined SMEFT fit to multiple LHC measurements and precision data, yielding individual constraints on 64 Wilson coefficients and 43 linear combinations.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Mildner, \"An EWPD SMEFT likelihood for the LHC - and how to improve it with measurements of W and Z boson properties\",JHEP07(2025) 089, doi:10.1007/JHEP07(2025)089,arXiv:2412.07651. [40] HEPData record for this analysis, 2025.doi:10.17182/hepdata.157866. [41] CMS Collaboration, \"The CMS experiment at the CERN LHC\",JINST3(2008) S08004, doi:10.1088/1748-0221/3/08/S08004. [42] CMS Collaboration, \"Development of the CMS detector for the CERN LHC Run 3\", JINST19(2024) P05064,doi:10.1088/1748-0221/19/05/P05064, arXiv:2309.05466. [43] CMS Collaboration, \"Performance of the CMS Level-1 trigger in proton-proton collisions at √s=13 TeV\",JINST15(2020) P10017, doi:10.1088/1748-0221/15/10/P10017,arXiv:2006.10165. [44] CMS Collaboration, \"The CMS trigger system\",JINST12(2017) P01020,"},{"citing_arxiv_id":"2412.19952","ref_index":28,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"First evidence for mixing-induced $CP$ violation in B$^0_\\mathrm{s}$ $\\to$ J/$\\psi\\,\\phi$(1020) decays in pp collisions at $\\sqrt{s} = $ 13 TeV","primary_cat":"hep-ex","submitted_at":"2024-12-27T23:21:20+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"First evidence for non-zero φ_s in B_s^0 → J/ψ φ decays at 3.2σ from CMS 13 TeV data combined with prior 8 TeV result.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}