{"total":22,"items":[{"citing_arxiv_id":"2606.20558","ref_index":25,"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":"2606.01423","ref_index":47,"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":"2605.19144","ref_index":97,"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":"2605.16655","ref_index":36,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for the nonresonant production of a pair of additional Higgs bosons in the Type-X two-Higgs-doublet model in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-05-15T21:49:47+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"No evidence found for additional Higgs boson pairs in Type-X 2HDM; new limits exclude the model for explaining the muon anomalous magnetic moment anomaly.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15023","ref_index":35,"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":"2605.13649","ref_index":27,"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":"method","top_context_polarity":"use_method","context_text":"[25] CMS Collaboration, \"Pileup mitigation at CMS in 13 TeV data\",JINST15(2020) P09018, doi:10.1088/1748-0221/15/09/P09018,arXiv:2003.00503. [26] CMS Collaboration, \"Performance of missing transverse momentum reconstruction in proton-proton collisions at √s=13 TeV using the CMS detector\",JINST14(2019) P07004,doi:10.1088/1748-0221/14/07/P07004,arXiv:1903.06078. [27] E. Bols et al., \"Jet flavour classification usingDEEPJET\",JINST15(2020) P12012, doi:10.1088/1748-0221/15/12/P12012,arXiv:2008.10519. [28] CMS Collaboration, \"Performance summary of AK4 jet b tagging with data from proton-proton collisions at 13 TeV with the CMS detector\", CMS Detector Performance Summary CMS-DP-2023-005, 2023. [29] CMS Collaboration, \"Identification of heavy-flavour jets with the CMS detector in pp"},{"citing_arxiv_id":"2605.13614","ref_index":81,"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":"method","top_context_polarity":"use_method","context_text":"Specific event filters have been designed to reduce events with spuriousp miss T arising from reconstruction failures or from genuine showers not originating from the pp collisions [80]. The specific features of heavy-flavoured jets, in particular the presence of displaced vertices, are used in a multivariate jet tagging method. A working point of the DEEPJETalgorithm [81] is used to tag b quark jets withpT >20 GeV and|η|<2.4, corresponding to a 90% efficiency for correctly identifying b jets and a 40 (4)% probability of misidentifying a charm jet (light-flavour or gluon jet) as a bottom jet. 6 Event selection Events are selected in three steps. First, events are required to pass criteria based on HLT algorithms that require the presence of at least one electron (muon), satisfying isolation and"},{"citing_arxiv_id":"2605.02848","ref_index":50,"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":"are vetoed if they contain an isolated electron (muon) candidate withp T >15(10)GeV and |η|<2.4. Criteria for identifying these objects include passing a multivariate identification dis- criminant and passing selections on isolation and impact parameter with respect to the primary interaction vertex observables [38, 39]. Jets originating from a bottom quark (b jets) are identified using the DEEPJETalgorithm [50] and the loose or medium b tagging working point [51]. The working points are defined by the rate of jets that are initiated from light flavor (up, down, or strange) quarks or gluons, but are incorrectly identified as b jets. The loose and medium working points are defined such that the misidentification rates of light flavor and gluon (charm) jets are about 10 and 1 (40 and"},{"citing_arxiv_id":"2604.27795","ref_index":51,"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":"at 100 GeV, and 5% at 1 TeV. Jets are required to be isolated from selected charged leptons by ∆R>0.4. The missing transverse momentum vector ⃗p miss T is computed as the negative vector sum of the transverse momenta of all PF candidates, and its magnitude is denoted asp miss T . It includes corrections to the JES [50]. Flavor tagging is performed using the DEEPJETalgorithm [51], which employs a deep neural network to identify jets originating from b, c, or light-flavor quarks or gluons. The discrimi- nator distributions in simulation are calibrated to data using scale factors derived from control samples in data [52]. At the medium working point, the identification efficiency for b jets is approximately 80%, with a light-jet mistag rate below 1%."},{"citing_arxiv_id":"2604.27044","ref_index":89,"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":"Three b tagging working points (WPs) are used, the loose (L), medium (M), and tight (T), corresponding to misidentification rates for light-flavor quark and gluon jets of about 10%, 1% and 0.1%, and b tagging efficiencies of approximately 92%, 83%, and 70%, respectively. For the analysis using Run 2 data, discussed in Section 5.4, jets are tagged with the DEEPJET[89, 90] b tagging algorithm. For a fixed misidentification rate,PNETimproves the absolute b tagging efficiency with respect to the Run 2 DEEPJETalgorithm by 3-7%, depending on the WP and jet pT. The b tagging efficiency in simulated events is corrected to match the one observed in data with correction factors applied to the simulation [90, 91]. These correction factors are derived"},{"citing_arxiv_id":"2604.25604","ref_index":51,"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":"method","top_context_polarity":"use_method","context_text":"with larger∆m ±, while the transverse displacement, measured by the impact parameter, IP xy, decreases, as shown by the colored open histograms in the main panels of Fig. 2. A parame- terized feedforward NN is trained to classify simulated tracks that are geometrically matched to stable generator-level particles. The NN has a three-layer architecture with 256 hidden units per layer, LeakyReLU activations [51], and preprocessing layers for input normalization. There are five output nodes corresponding to five track classes: signal tracks; secondary tracks from hadronicτlepton decays in W→τ hνevents; other secondary tracks from particles created at the PV; prompt tracks from the PV (together with the previous class referred to as \"PV- associated\"); and spurious tracks."},{"citing_arxiv_id":"2604.24531","ref_index":35,"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":"method","top_context_polarity":"use_method","context_text":"Rubin, and G. P . Salam, \"Jet substructure as a new Higgs search channel at the LHC\",Phys. Rev. Lett.100(2008) 242001, doi:10.1103/PhysRevLett.100.242001,arXiv:0802.2470. [34] CMS Collaboration, \"Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV\",JINST13(2018) P05011, doi:10.1088/1748-0221/13/05/P05011,arXiv:1712.07158. [35] E. Bols et al., \"Jet flavour classification using DeepJet\",JINST15(2020) P12012, doi:10.1088/1748-0221/15/12/P12012,arXiv:2008.10519. [36] CMS Collaboration, \"Performance of the DeepJet b tagging algorithm using 41.9 fb −1 of data from proton-proton collisions at 13 TeV with Phase 1 CMS detector\", CMS Detector Performance Summary CMS-DP-2018-058, 2018."},{"citing_arxiv_id":"2604.20999","ref_index":38,"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":"method","top_context_polarity":"use_method","context_text":"primary interaction vertex deduced from the local shape variable, superseding the need for jet-based pileup corrections [36]. The AK4 jets used in this search are further required to have ap T >30 GeV and|η|<2.5. Jets with∆R<0.4 with respect to a well-identified and isolated lepton or photon are removed. To identify jets originated by the hadronization of b quarks (hereafter referred to as \"b jets\"), the DEEPJETalgorithm [38] is employed. A loose working point is used, defined for each data- taking year as the minimum requirement in the DEEPJETdiscriminator distribution, which returns a 10% rate of misidentifying a jet originated by a light-flavor quark or gluon. The loose working point corresponds to an efficiency of correctly identifying jets originated by b quarks (i."},{"citing_arxiv_id":"2604.17564","ref_index":39,"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":"method","top_context_polarity":"use_method","context_text":"calorimeter response [38]. The corrected jetp T must be>200 GeV for the highestp T (leading) jet, and>30 GeV for the remaining jets with|η|<2.4. For the final event selection, at least one jet is required withp T >30 GeV and 2.4<|η|<5.0. Jets are identified as b tagged (called b jets), meaning they come from the hadronization of b quarks, using the DEEPJETalgorithm [39] based on secondary vertex and track impact parame- ter information. The b-tagged jets are required to be within the acceptance of the silicon tracker (|η|<2.4). We use both medium and tight working points (WPs) for the algorithm [40]. Events with at least one medium WP b-tagged jet are selected. The algorithm correctly identifies b jets with efficiencies of approximately 70% and 40% for the medium and tight WPs, respectively."},{"citing_arxiv_id":"2604.09809","ref_index":57,"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":"method","top_context_polarity":"use_method","context_text":"be the SD mass (m SD). The second is a mass regression algorithm using the PARTICLENET architecture, which leverages PF candidate and SV information in a GNN to predict the jet mass (m reg), and has demonstrated improved mass resolution of two-pronged jets compared with the SD mass with the aforementioned parameters [10]. The DEEPJETrecurrent neural network algorithm [57] is used to identify AK4 jets originating from b quarks, as discussed in Section 6. The missing transverse momentum vector ⃗p miss T is computed as the negative vector sum of the transverse momenta of all the PF candidates in an event, and its magnitude is denoted as pmiss T [58]. The ⃗p miss T is modified to account for corrections to the energy scale of the recon-"},{"citing_arxiv_id":"2604.05996","ref_index":43,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Search for soft unclustered energy patterns produced in association with a W or Z boson in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","primary_cat":"hep-ex","submitted_at":"2026-04-07T15:21:23+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"No significant excess is observed in leptonic W/Z plus high-multiplicity soft-particle events, setting limits on Higgs to SUEP decays across a range of model parameters.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"the data-taking year and lepton flavor. Uncertainties in the jet energy corrections [40] are prop- agated through the event selection and account for effects of up to 1 (2)% for the scale (reso- lution). The b tagging efficiency is corrected separately for light- and heavy-flavor jets, with uncertainties of up to 3% depending on the data-taking year [43]. The PF candidate selection efficiency is varied down by 3% [49] for models with fully hadronic SUEP decays and 4.5% for signal models with leptons from SUEP decays to account for the lower tracking efficiency for low-pT electrons, with a resulting effect of up to 30% in somenSUEP constituent bins. The uncertainty in the pileup modeling is assessed by varying the total inelastic pp cross section by 5% [50], result-"},{"citing_arxiv_id":"2604.02604","ref_index":51,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Probing Freeze-In Dark Matter via a Spin-2 Portal at the LHC with Vector Boson Fusion and Machine Learning","primary_cat":"hep-ph","submitted_at":"2026-04-03T00:47:19+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"LHC vector boson fusion searches enhanced by machine learning can probe substantial regions of cosmologically viable parameter space for freeze-in dark matter mediated by a spin-2 particle.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"65% with a corresponding misidentification probability of 0.5% at the edge of the tracker acceptance. Such re- ductions, primarily induced by pileup, lead to a mod- est deterioration in the resolution of reconstructed lepton kinematics. Forb-jet identification, we follow Ref. [50] and adapt theDelphescard to implement the \"Loose\" working point of the DeepCSV algorithm [51]. This choice cor- responds to ap T-dependentb-tagging efficiency in the range 70-85%, with an associated light-flavor mistag rate of approximately 10%. The operating points for both lep- ton andb-jet identification are selected through an op- timization procedure designed to maximize the expected signal significance while suppressing SM backgrounds."},{"citing_arxiv_id":"2511.01995","ref_index":65,"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":"2510.00160","ref_index":76,"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":"2508.06947","ref_index":59,"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":"2504.02958","ref_index":53,"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":"1088/1126-6708/2008/04/063,arXiv:0802.1189. [51] M. Cacciari, G. P . Salam, and G. Soyez, \"FastJet user manual\",Eur. Phys. J. C72(2012) 1896,doi:10.1140/epjc/s10052-012-1896-2,arXiv:1111.6097. [52] CMS Collaboration, \"Identification of heavy-flavour jets with the CMS detector in pp collisions at 13 TeV\",JINST13(2018) P05011, doi:10.1088/1748-0221/13/05/P05011,arXiv:1712.07158. [53] E. Bols et al., \"Jet flavour classification using DeepJet\",JINST15(2020) P12012, doi:10.1088/1748-0221/15/12/P12012,arXiv:2008.10519. [54] CMS Collaboration, \"Performance of the DeepJet b tagging algorithm using 41.9/fb of data from proton-proton collisions at 13 TeV with Phase 1 CMS detector\", CMS Detector Performance Note CMS-DP-2018-058, 2018."},{"citing_arxiv_id":"2303.14511","ref_index":3,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Improving robustness of jet tagging algorithms with adversarial training: exploring the loss surface","primary_cat":"hep-ex","submitted_at":"2023-03-25T16:23:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Adversarial training enhances robustness of jet tagging classifiers while preserving performance, with loss surface geometry providing insights into correlations and vulnerability.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}