{"total":20,"items":[{"citing_arxiv_id":"2606.17134","ref_index":9,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"PineAPPLv1: fast and flexible theory predictions for present and future colliders","primary_cat":"hep-ph","submitted_at":"2026-06-15T18:00:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"PineAPPLv1 provides interpolation tables supporting multiple convolutions with polarised and unpolarised PDFs and FFs for fast collider observable predictions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.04826","ref_index":85,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Kinematic Riffs and Interference Effects in Triple Higgs Production in the N2HDM","primary_cat":"hep-ph","submitted_at":"2026-06-03T12:49:53+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Interference effects and extra decay channels in N2HDM resonant triple Higgs production significantly alter kinematic distributions, limiting simplified approximations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.01681","ref_index":65,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Probing pair production of long-lived scalars via an off-shell Standard-Model-like Higgs boson at the LHC","primary_cat":"hep-ph","submitted_at":"2026-06-01T04:43:11+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Pair production of long-lived scalars via off-shell Higgs at the LHC is probed with displaced-vertex searches, excluding masses up to ~230 GeV with current ATLAS data for a benchmark coupling.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.29289","ref_index":35,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Hiding in the Shadow of the Upsilon: Ditaus from a Light Pseudoscalar","primary_cat":"hep-ph","submitted_at":"2026-05-28T03:12:28+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"A light pseudoscalar near the Υ(1S) mass, mixing with two Higgs doublets in the alignment limit, accounts for the anomalous ditau rate while evading existing constraints.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.28667","ref_index":64,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Towards the two-loop electroweak corrections to the Drell-Yan process: the complete fermionic contributions","primary_cat":"hep-ph","submitted_at":"2026-05-27T16:01:05+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"The authors present the finite two-loop fermionic virtual corrections to the Drell-Yan cross section after renormalization and infrared subtraction using an automated methodology.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15286","ref_index":25,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Predicting Three Generations of Fermions: Discovery Prospects of the Bilepton Model","primary_cat":"hep-ph","submitted_at":"2026-05-14T18:01:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Bilepton Model predicts observable pairs of doubly-charged bileptons at HL-LHC up to m_D ~2.5 TeV or m_Y ~2 TeV through background-free four-lepton final states in two complementary channels.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15262","ref_index":67,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"USMEFT as a tool for discovery of universal new physics at high luminosity LHC","primary_cat":"hep-ph","submitted_at":"2026-05-14T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Universal SMEFT fits to pseudo-data from neutral and charged Drell-Yan processes at HL-LHC can detect universal new physics and extract its properties stably across EFT truncation orders.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.05880","ref_index":9,"ref_count":2,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Top-associated Higgs-boson production using perturbative fragmentation functions at next-to-leading-order","primary_cat":"hep-ph","submitted_at":"2026-05-07T08:47:26+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Perturbative fragmentation functions approximate ttH production at NLO and yield reliable results in the hybrid prescription at LHC energies.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Jackson, L.H. Orr, L. Reina and D. Wackeroth,Associated Higgs production with top quarks at the large hadron collider: NLO QCD corrections,Phys. Rev. D68(2003) 034022 [hep-ph/0305087]. [8] S. Frixione, V. Hirschi, D. Pagani, H.S. Shao and M. Zaro,Weak corrections to Higgs hadroproduction in association with a top-quark pair,JHEP09(2014) 065 [1407.0823]. [9] Y. Zhang, W.-G. Ma, R.-Y. Zhang, C. Chen and L. Guo,QCD NLO and EW NLO corrections tot ¯tH production with top quark decays at hadron collider,Phys. Lett. B738(2014) 1 [1407.1110]. [10] S. Frixione, V. Hirschi, D. Pagani, H.S. Shao and M. Zaro,Electroweak and QCD corrections to top-pair hadroproduction in association with heavy bosons,JHEP06(2015) 184 [1504."},{"citing_arxiv_id":"2605.01488","ref_index":18,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Multi-Lepton Probes of the Drell-Yan Production of Triplet Higgses","primary_cat":"hep-ph","submitted_at":"2026-05-02T15:22:57+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"The ΔSM real Higgs triplet model is consistent with LHC triboson excesses but predicts more events than observed and is not preferred over the Standard Model.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"c e-mail:andreas.crivellin@cern.ch d e-mail:mukesh.kumar@cern.ch e e-mail:rachid.mazini@cern.ch f e-mail:bmellado@mail.cern.ch in di-photon [9, 10],Zγ[11, 12], andW W[13-15] final states, providing strong indications in support of a new scalar particle with a mass 152±1 GeV [16, 17]. Interest- ingly, no corresponding excess has been seen in theZZ channel [18,19], a pattern that poses a challenge for mod- els involving a standard Higgs doublet or singlet exten- sion. However, this pattern is naturally obtained if the new scalar is the neutral component of a hypercharge Y= 0 triplet [20, 21] and, in fact, the observed excesses can be partially explained by the Drell-Yan production of the triplet [22-25]."},{"citing_arxiv_id":"2605.00549","ref_index":159,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Bounds on massive graviton-like particles from searches for axion-like particles coupling to photons","primary_cat":"hep-ph","submitted_at":"2026-05-01T10:04:25+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Limits on axion-like particles from photon-coupling searches are recast as constraints on massive graviton-like particles across lab, astrophysical, and cosmological experiments using analogous Primakoff and Gertsenshtein conversion mechanisms.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"this threshold, hadronic modes open up and quickly dominate, reducing the diphoton branching ratio toB GÑγγ «0.05 (Fig. 2). 25 A. Beam-dumps and fixed-target collisions Searches for ALPs in fixed-target collisions performed at beam-dump or collider facilities, include data from the following setups: SLAC E141 [152] and E137 [153]; Fermilab MiniBooNE [154-156]; U70's NuCal [38]; CERN CHARM [157], NA64 [158], FASER [159], and SHiP [160] (future); and Fermilab SeaQuest [53] (future). In beam-dump experiments, a high-intensity proton or electron beam strikes a thick target (\"dump\") where the quasireal photon field of the charged beam particles, or the real photons from secondary photons from decays of neutral mesons produced in hadronic interactions of the beam with the target material, interact with the Coulomb field of the target"},{"citing_arxiv_id":"2604.25557","ref_index":71,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Jarvis-HEP: A lightweight Python framework for workflow composition and parameter scans in high-energy physics","primary_cat":"hep-ph","submitted_at":"2026-04-28T12:28:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Jarvis-HEP introduces a YAML-based Python framework for composing workflows and performing parameter scans in high-energy physics.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"1140/epjc/s10052-013-2588-2. [70] J. Alwall, R. Frederix, S. Frixione, V . Hirschi, F. Maltoni, O. Mattelaer, H. S. Shao, T. Stelzer, P. Torrielli, M. Zaro, The automated com- putation of tree-level and next-to-leading or- der differential cross sections, and their match- ing to parton shower simulations, JHEP 07 (2014) 079.arXiv:1405.0301,doi:10.1007/ JHEP07(2014)079. [71] R. Frederix, S. Frixione, V . Hirschi, D. Pa- gani, H. S. Shao, M. Zaro, The automation of next-to-leading order electroweak calculations, JHEP 07 (2018) 185, [Erratum: JHEP 11, 085 (2021)].arXiv:1804.10017,doi:10.1007/ JHEP11(2021)085. [72] T. Sjostrand, S. Mrenna, P. Z. Skands, PYTHIA 6.4 Physics and Manual, JHEP 05 (2006) 026.arXiv:hep-ph/0603175,doi:10."},{"citing_arxiv_id":"2604.18025","ref_index":14,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Precision calculations for electroweak multi-boson processes","primary_cat":"hep-ph","submitted_at":"2026-04-20T09:50:50+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"Electroweak corrections reach about -16% for like-sign WW scattering and -7% for triple-W production at the LHC, even for integrated cross sections, and the paper discusses approximations to full off-shell calculations.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.16218","ref_index":101,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Quantum Tomography and Entanglement in Semi-Leptonic $h\\to VV^*$ Decays at Higher Orders","primary_cat":"hep-ph","submitted_at":"2026-04-17T16:28:40+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Semi-leptonic h to VV* decays retain an effective two-qutrit description for quantum tomography and entanglement after including finite fermion masses and NLO corrections.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"July, 2018.https://cds.cern.ch/record/2630340. [99] D. Goncalves and J. Nakamura, \"Role of theZpolarization in theH→b¯bmeasurement,\" Phys. Rev. D98no. 9, (2018) 093005,arXiv:1805.06385 [hep-ph]. [100] D. Goncalves and J. Nakamura, \"Boosting theH→invisibles searches withZboson polarization,\"Phys. Rev. D99no. 5, (2019) 055021,arXiv:1809.07327 [hep-ph]. [101]A TLASCollaboration, M. Aaboudet al., \"Measurements of top-quark pair spin correlations in theeµchannel at √s= 13TeV usingppcollisions in the ATLAS detector,\" Eur. Phys. J. C80no. 8, (2020) 754,arXiv:1903.07570 [hep-ex]. [102]CMSCollaboration, A. M. Sirunyanet al., \"Measurement of the top quark polarization andt ¯tspin correlations using dilepton final states in proton-proton collisions at√s=13"},{"citing_arxiv_id":"2604.14099","ref_index":94,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Electro-Weak Phase Transitions and Collider Signals in the Aligned 2-Higgs Doublet Model","primary_cat":"hep-ph","submitted_at":"2026-04-15T17:14:52+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"The Aligned 2HDM supports strong first-order electroweak phase transitions that yield LISA-detectable gravitational waves together with LHC-accessible signals from additional neutral and charged Higgs states.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"collider signatures that closely resemble those of charged Higgs decays into a charged lepton and a neutrino. 4 A2HDM Parameter Space For generation of parameter points compatible with all the constraints mentioned above we use the open-sourceHEPfitpackage [93] that implements a Markov-Chain Monte-Carlo (MCMC) algorithm via theBayesian Analysis Toolkit[94] and perform global fits of the A2HDM. We begin with - 10 - flat distributions of model parameters aspriors. Then, based on the experimental measurement of a large number of observables,HEPfitconstructs thelikelihood(L)of the model, according to Bayes' theorem, thereby generating theposteriordistribution. The relative quality of different fits or models is assessed using the Information Criterion (IC), defined asIC =−2logL+ 4σ 2"},{"citing_arxiv_id":"2604.11574","ref_index":36,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"SemiCharmTag: a tool for Semileptonic Charm tagging","primary_cat":"hep-ex","submitted_at":"2026-04-13T14:52:52+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"CHEP2000. [34] M. Clemencic et al., Recent developments in the LHCb software framework gaudi , Journal of Physics: Conference Series 219 (2010) 042006. [35] J. Alwall et al., The automated computation of tree-level and next-to-leading order differential cross sections, and their matching to parton shower simulations , JHEP 07 (2014) 079, arXiv:1405.0301. [36] R. Frederix et al., The automation of next-to-leading order electroweak calculations , JHEP 07 (2018) 185, arXiv:1804.10017, [Erratum: JHEP 11, 085 (2021)]. [37] R. D. Ball et al., Parton distributions for the LHC run2 , Journal of High Energy Physics 2015 (2015) . [38] M. Cacciari et al., Theoretical predictions for charm and bottom production at the"},{"citing_arxiv_id":"2601.11986","ref_index":13,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Prospects for discovering strongly decaying doubly heavy $T_{bc}$ tetraquark states at LHCb","primary_cat":"hep-ph","submitted_at":"2026-01-17T09:40:29+00:00","verdict":"CONDITIONAL","verdict_confidence":"MODERATE","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Phenomenological study calculates luminosity for 5σ discovery of T_bc tetraquark in B D channel at LHCb under three production cross-section scenarios.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2512.04959","ref_index":36,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Towards a Fully Automated Differential $\\text{NNLO}_\\text{EW}$ Generator for Lepton Colliders","primary_cat":"hep-ph","submitted_at":"2025-12-04T16:29:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"A framework based on the YFS theorem enables process-independent local IR subtraction and resummation matching for automated NNLO_EW calculations in lepton collider processes.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"for potentially large logarithms that could spoil their parametric accuracy. In full analogy to similar calculations for the LHC, this can be achieved in the collinear picture by convoluting the electron parton distribution function (PDF) [32], known to NLO [33] and recently to NNLO [34, 35], with a short distance partonic cross-section that can be calculated to higher-orders with standard techniques [36, 37]. Results of such calculations can be combined with a parton shower [38-41] to achieve fully exclusive predictions [42, 43]. While there has been significant progress in the inclusive picture [44, 45] the implementation of a fully matched NLOEW/NNLOEW parton shower for arbitrary processes is so far missing. An alternative approach to collinear resummation is available through the Yennie-Frautschi-Suura (YFS) theorem [46],"},{"citing_arxiv_id":"2511.04796","ref_index":87,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Interpretation of LHC excesses at 95 GeV and 152 GeV in an extended Georgi-Machacek model","primary_cat":"hep-ph","submitted_at":"2025-11-06T20:32:38+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"A minimally extended Georgi-Machacek model accommodates the LHC excesses at 95 GeV and 152 GeV while preserving the 125 GeV Higgs signal and the electroweak rho parameter near unity.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2509.07094","ref_index":67,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Searching for a Charged Higgs Boson in Top-Quark Decays via the $WZ$ Mode","primary_cat":"hep-ph","submitted_at":"2025-09-08T18:00:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Recasting ttZ analyses yields sub-permille constraints on Br(t→H±b)×Br(H±→WZ) and vΔ≲2 GeV in the Y=0 Higgs triplet model, accompanied by a 2σ preference for a non-zero signal.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2507.13430","ref_index":76,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Stopping Dark Mesons in Their Tracks with Long-Lived Particle and Resonant Signatures","primary_cat":"hep-ph","submitted_at":"2025-07-17T18:00:00+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Recast LHC searches yield a ~1.2 TeV lower bound on long-lived charged dark mesons and show that anomaly-driven diboson resonances can reconstruct UV parameters like dark flavor and color numbers from IR measurements.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}