{"total":18,"items":[{"citing_arxiv_id":"2606.20558","ref_index":55,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"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":"2605.28538","ref_index":57,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Search for pair-produced vector-like $T$-quarks decaying into $Ht$ final states in the lepton-plus-jets channel in $pp$ collisions at $\\sqrt{s}$=13 TeV with the ATLAS detector","primary_cat":"hep-ex","submitted_at":"2026-05-27T14:33:13+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"No excess observed in search for vector-like T-quarks in Ht channel; 95% CL mass limits set at 1.40 TeV (SU(2) singlet), 1.56 TeV (doublet), and 1.66 TeV (100% BR to Ht).","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.19918","ref_index":40,"ref_count":2,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Redetermination of proton sea distributions","primary_cat":"hep-ph","submitted_at":"2026-05-19T14:43:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"NNLO global fits to HERA and ATLAS data extract \bar u > \bar d asymmetry in the proton sea and yield a revised Gottfried sum rule.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.19144","ref_index":90,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"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":"2605.18360","ref_index":24,"ref_count":2,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Nested-GPT for variable-multiplicity parton showers: A case study in the resummation of non-global logarithms","primary_cat":"hep-ph","submitted_at":"2026-05-18T13:13:28+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Nested-GPT is an autoregressive Transformer surrogate that generates variable-multiplicity parton showers while enforcing ordered Markovian branching and matches reference Monte Carlo results for leading-log non-global logarithm resummation in the large-Nc limit.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15853","ref_index":62,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Numerical Study of MRW-Type Unintegrated Double Parton Distribution Functions from Non-Factorized DPDFs","primary_cat":"hep-ph","submitted_at":"2026-05-15T11:11:50+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Numerical study of MRW-type unintegrated DPDFs constructed from GS09 non-factorized collinear DPDFs via double DGLAP evolution, comparing DMKMRW, DVO-MRW and matched variants.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.12755","ref_index":41,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Probing muon anomaly and lepton flavor violation with scalar leptoquarks in the 331LHN model","primary_cat":"hep-ph","submitted_at":"2026-04-14T14:02:08+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"A singlet scalar leptoquark in the 331LHN model can fully account for the muon anomalous magnetic moment discrepancy with mass above 1.8 TeV (or 6 TeV using 2025 data) while obeying LFV constraints and showing suppressed LHC signals.","context_count":1,"top_context_role":"background","top_context_polarity":"support","context_text":"[39] I. Bigaran and R. R. Volkas,Getting chirality right: Single scalar leptoquark solutions to the(g−2) e,µ puzzle,Phys. Rev. D102(2020) 075037 [2002.12544]. [40] E. C. Leskow, G. D'Ambrosio, A. Crivellin and D. M¨ uller, (g−2) µ, lepton flavor violation, andz decays with leptoquarks: Correlations and future prospects,Phys. Rev. D95(2017) 055018. [41] A. Crivellin and M. Hoferichter,The anomalous magnetic moment of the muon: Beyond the Standard Model via chiral enhancement,Nuovo Cim. C46(2022) 10 [2207.01912]. [42] I. Dorˇ sner, S. Fajfer and O. Sumensari,Muong−2and scalar leptoquark mixing,JHEP06(2020) 089 [1910.03877]. [43] S.-P. He,Leptoquark and vectorlike quark extended models as the explanation of the muong−2"},{"citing_arxiv_id":"2604.07161","ref_index":64,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Impact of hidden heavy Higgs channels of VLB-Quarks below 1 TeV in 2HDM","primary_cat":"hep-ph","submitted_at":"2026-04-08T14:51:12+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Hidden BSM decays of vector-like bottom quarks in 2HDM-II relax LHC mass limits from ~1.5 TeV to 1.34 TeV for singlets and 0.98 TeV for doublets.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"[61]Particle Data Groupcollaboration,Review of Particle Physics,PTEP2020(2020) 083C01. [62] D. Eriksson, J. Rathsman and O. Stal,2HDMC: Two-Higgs-Doublet Model Calculator Physics and Manual,Comput. Phys. Commun.181(2010) 189 [0902.0851]. [63]A TLAScollaboration,Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector usingppcollisions at √s= 13TeV,Phys. Rev. Lett.125(2020) 051801 [2002.12223]. [64]CMScollaboration,Searches for additional Higgs bosons and for vector leptoquarks inτ τfinal states in proton-proton collisions at √s= 13 TeV,JHEP07(2023) 073 [2208.02717]. [65]A TLAScollaboration,Search for a heavy Higgs boson decaying into a Z boson and another heavy Higgs boson in theℓℓbbandℓℓW Wfinal states inppcollisions at √s= 13TeV with the ATLAS detector,Eur."},{"citing_arxiv_id":"2602.19072","ref_index":40,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Charmonium suppression in fixed target proton-nucleus collisions","primary_cat":"nucl-th","submitted_at":"2026-02-22T07:11:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Models initial-state energy loss, nuclear shadowing, and final-state absorption on J/ψ and ψ(2S) production in p+A collisions, compares to SPS/Fermilab/HERA-B data, and extrapolates absorption levels for NA60+ and CBM.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2602.02688","ref_index":58,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Generalized Neutrino Interactions: constraints and parametrizations","primary_cat":"hep-ph","submitted_at":"2026-02-02T19:04:52+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Relating two GNI parametrizations shows scalar neutrino-quark interactions are more tightly constrained by COHERENT while tensor interactions are better bounded by deep inelastic scattering.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2510.11809","ref_index":43,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Modeling the TMD shape function in $J/\\psi$ electroproduction","primary_cat":"hep-ph","submitted_at":"2025-10-13T18:06:13+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"NLO hard function in TMD factorization for quarkonium electroproduction with predictions for unpolarized J/ψ cross section at EIC.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2508.05171","ref_index":9,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"An analysis of nuclear parton distribution function based on relative entropy","primary_cat":"hep-ph","submitted_at":"2025-08-07T09:04:39+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"A relative-entropy method with a minimum-relative-entropy hypothesis reproduces quark nPDF shapes from global fits and indicates that EPPS21 gluon central values align more closely with the hypothesis than nNNPDF3.0.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1912.10053","ref_index":166,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"New CTEQ global analysis of quantum chromodynamics with high-precision data from the LHC","primary_cat":"hep-ph","submitted_at":"2019-12-20T19:00:05+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"New CT18 PDFs at NLO and NNLO from global fit to HERA plus LHC jet, Drell-Yan, top-pair and Z data, with Hessian errors, Lagrange-multiplier studies, and alternate sets for data tensions and scale choices.","context_count":1,"top_context_role":"other","top_context_polarity":"background","context_text":"against the ATLAS (544) and CMS 7 TeV (542) jet production, as well as measurements by CDHSW (108), CCFR (110), and BCDMS (102) of the DIS structure function F2(x,Q ) on various targets. An extensive collection of the L2 sensitivity plots for CT18(Z) PDFs and PDF ratios, reflecting the interplay and competing pulls among the CT18 data sets, can be viewed at [166]. Analogous calculations are shown for the alternative CT18Z fit in Sec. A 4. In Fig. 26, we show the L2 sensitivity of the CT18 data on the gluon PDF at fixed Q=100 GeV, plotting curves for those experiments that satisfy |Sf,L2(E)| ≥ 4 for any value of x. This criterion generally identifies the leading 5 − 10 experiments with strongest pulls on the PDF in the kinematical region under consideration."},{"citing_arxiv_id":"1907.11165","ref_index":16,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Applications of the WW-type approximation to SIDIS","primary_cat":"hep-ph","submitted_at":"2019-07-25T16:16:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Applies the WW-type approximation to relate TMDs and FFs and approximate the complete SIDIS cross-section up to power-suppressed terms.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1907.10368","ref_index":25,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Inclusive Jet Longitudinal Double-spin Asymmetry $A_{LL}$ Measurements in 510 GeV Polarized $pp$ Collisions at STAR","primary_cat":"hep-ex","submitted_at":"2019-07-24T11:18:20+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"First measurement of inclusive jet A_LL at √s=510 GeV in polarized pp collisions at STAR, found consistent with global polarized PDF analyses and prior 200 GeV data.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1907.04324","ref_index":226,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Dark Matter Energy Deposition and Production from the Table-Top to the Cosmos","primary_cat":"hep-ph","submitted_at":"2019-07-09T15:47:40+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"The thesis presents a new 3-to-2 freezeout mechanism, bound-state effects on searches, a new axion interferometric search, reionization assessments, 21-cm constraints, and the DarkHistory code for ionization and thermal histories.","context_count":1,"top_context_role":"dataset","top_context_polarity":"use_dataset","context_text":"𝜁(𝑠) is the Riemann 𝜁-function, which takes into account the cross section for the production of all of the excited states of the bound state. Here 𝜏ℬ ≡ 𝑚2 ℬ/𝑠, 𝑚ℬ is the mass of the bound state, and√𝑠 is the collider center-of-mass energy. ℒ𝑞¯𝑞 is the parton luminosity function defined as ℒ𝑞𝑞(𝜏) = 𝜏 ∫︁1 𝜏 𝑑𝑥 𝑥 𝑓𝑞(𝑥)𝑓𝑞(𝜏 /𝑥) , (3.6) with 𝑓𝑞(𝑥) being the parton distribution functions (PDF), taken from [226] for calcu- lations in this chapter. In the perturbative limit, we can write 𝜎ℬ ≈ ∑︁ 𝑞 8𝜋𝜁(3) 3𝑚ℬ 𝑔2 𝑞 𝑔2 𝜒|𝜓(0)|2ℒ𝑞¯𝑞 (𝜏ℬ) (𝑚2 ℬ − 𝑚2 𝑉 )2 + Γ2 𝑉 (𝑠 = 𝑚2 ℬ)𝑚2 𝑉 , (3.7) where 𝑔𝑞 (𝑔𝜒) sets the coupling of the mediator𝑉 to quarks(DM) and 𝜓(0) is the wave function of the bound state at the origin. For a Coulomb-like potential with coupling 𝛼ℬ (i.e. where the mass of the bound state mediator𝑚𝑌 can be neglected),"},{"citing_arxiv_id":"1906.08681","ref_index":12,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Off-shell initial state effects and gauge invariance in the Drell-Yan process","primary_cat":"hep-ph","submitted_at":"2019-06-20T15:02:32+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Helicity structure functions in Drell-Yan are analyzed in the Parton Reggeization Approach with gauge-invariant inclusion of initial-state transverse momentum, clarifying relations to the TMD Parton Model.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"1405.0301","ref_index":219,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations","primary_cat":"hep-ph","submitted_at":"2014-05-01T20:24:46+00:00","verdict":"ACCEPT","verdict_confidence":"MODERATE","novelty_score":7.0,"formal_verification":"none","one_line_summary":"MadGraph5_aMC@NLO automates tree-level, NLO, shower-matched, and merged cross-section computations for collider processes in a unified flexible framework.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}