{"total":70,"items":[{"citing_arxiv_id":"2605.23359","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Addressing Standard Model Tensions via X17 Vector Boson","primary_cat":"hep-ph","submitted_at":"2026-05-22T08:23:39+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"A new X17 vector boson is suggested to alleviate Standard Model tensions while connecting to the dark sector.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.21870","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Deep Neural Networks for Heavy Lepton-Flavor-Violating Higgs Searches at the LHC","primary_cat":"hep-ph","submitted_at":"2026-05-21T01:32:44+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"DNN classifiers with mass-dependent thresholds reduce expected 95% CL upper limits on H to mu tau cross sections by 36-46% versus collinear mass baseline, while a regression network improves mass resolution by up to 21%.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.21721","ref_index":2,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"The Higgs-top-$Z$ mass coincidence relation after NNLO matching","primary_cat":"hep-ph","submitted_at":"2026-05-20T20:26:42+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"The pole-level ratio M_Z M_t / M_H² is 1.00362 ± 0.00261, consistent with an exact relation at 1.4 sigma, but the NNLO-matched MSbar version at the top scale deviates to 0.96714, requiring either a pole-level symmetry or a finite threshold factor of 1.034.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.21291","ref_index":8,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Impact of Hadronic Resonances on $B\\to K^{(*)}\\tau^+\\tau^-$ decays","primary_cat":"hep-ph","submitted_at":"2026-05-20T15:24:43+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Including resonant contributions from LHCb muon data enhances standard model predictions for B to K(*) tau tau decays and makes short-distance new physics comparable to or larger than resonant effects over the full q2 range.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.20048","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Gaussian Process Eigenmodes for Statistical and Systematic Uncertainties in Template Fits","primary_cat":"hep-ex","submitted_at":"2026-05-19T16:06:21+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Introduces Gaussian Process eigenmodes to unify statistical and systematic template uncertainties, replacing per-bin factors with truncated leading modes while containing Barlow-Beeston as a limiting case.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.19935","ref_index":12,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"paper_title":"Probing the Rare Four-Bottom Higgs Decay $H\\to b\\bar b b\\bar b$ at the HL-LHC and ILC","primary_cat":"hep-ph","submitted_at":"2026-05-19T14:54:29+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"The rare Higgs decay H to four bottom quarks has a branching ratio of order 1.6e-3 with relevant destructive interference and is observable at 3-5 sigma at HL-LHC and ILC via boosted decision tree analyses in WH and ZH production.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.19144","ref_index":9,"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":"2605.19016","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Measurements of the Higgs boson production, fiducial and differential cross-sections in the four lepton decay channel using 164 fb$^{-1}$ of data collected at $\\sqrt{s}$ = 13.6 TeV with the ATLAS detector","primary_cat":"hep-ex","submitted_at":"2026-05-18T18:36:51+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"ATLAS measures the fiducial cross-section for H to four leptons as 3.65 fb matching the SM prediction of 3.68 fb, with signal strength 0.99 and differential distributions all consistent with expectations.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Model Effective Field Theory, and in scenarios probing the Higgs boson self-coupling. All the results are consistent with Standard Model expectations. ©2026 CERN for the benefit of the ATLAS Collaboration. Reproduction of this article or parts of it is allowed as specified in the CC-BY-4.0 license. arXiv:2605.19016v1 [hep-ex] 18 May 2026 1 Introduction The observation of the Higgs boson by the ATLAS and CMS Collaborations [1, 2] using proton-proton (𝑝 𝑝) collisions at the Large Hadron Collider (LHC) marked a major milestone in the understanding of the electroweak (EW) symmetry-breaking mechanism [3-5]. Subsequent studies of the Higgs boson properties have established the observed particle as a scalar boson consistent with the Standard Model (SM) predictions for a Higgs boson with a mass of125."},{"citing_arxiv_id":"2605.16756","ref_index":7,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Higgs Physics with the XFEL Compton $\\boldsymbol{\\gamma\\gamma}$ Collider Concept at $\\boldsymbol{\\sqrt{s}=125}$ GeV","primary_cat":"hep-ph","submitted_at":"2026-05-16T02:11:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"An XFEL Compton gamma-gamma collider at 125 GeV with a set transformer deep learning classifier on particle-flow point clouds can achieve high-precision Higgs measurements across hadronic, semi-leptonic, and leptonic final states including H to strange quarks.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15396","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"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":"2605.15270","ref_index":12,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Light states in real 3HDMs with spontaneous CP violation and softly broken symmetries","primary_cat":"hep-ph","submitted_at":"2026-05-14T18:00:02+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"In real 3HDMs with spontaneous CP violation and discrete symmetry on quartics, perturbativity bounds keep new scalars near the electroweak scale despite large quadratic terms.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15262","ref_index":12,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"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":"2605.14245","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"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":"004; the Kavli Foundation; the Nvidia Corporation; the SuperMicro Corporation; the Welch Foundation, contract C-1845; and the Weston Havens Foundation (USA). Data availability Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS data preservation, re-use and open access policy. References [1] ATLAS Collaboration, \"Observation of a new particle in the search for the standard model Higgs boson with the ATLAS detector at the LHC\",Phys. Lett. B716(2012) 1, doi:10.1016/j.physletb.2012.08.020,arXiv:1207.7214. [2] CMS Collaboration, \"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC\",Phys. Lett. B716(2012) 30,"},{"citing_arxiv_id":"2605.13964","ref_index":2,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"A New Source of Millicharged Particles: Secondary Showers in the LHC Forward Absorber","primary_cat":"hep-ph","submitted_at":"2026-05-13T18:00:03+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Secondary cascades in the TAXN absorber produce a substantial millicharged particle flux that complements primary production and boosts FORMOSA signals by ~50% for m_χ below 0.1 GeV.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"supported by a Doctoral Dissertation Fellowship at the University of Minnesota. Z.L. is supported in part by a Sloan Research Fellowship from the Alfred P. Sloan Foundation at the University of Minnesota. [1] S. Chatrchyanet al.(CMS), Observation of a New Bo- son at a Mass of 125 GeV with the CMS Experiment at the LHC, Phys. Lett. B716, 30 (2012), arXiv:1207.7235 [hep-ex]. [2] G. Aadet al.(ATLAS), Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC, Phys. Lett. B716, 1 (2012), arXiv:1207.7214 [hep-ex]. [3] J. Alimenaet al., Searching for long-lived particles be- yond the Standard Model at the Large Hadron Collider, J. Phys. G47, 090501 (2020), arXiv:1903.04497 [hep-ex]."},{"citing_arxiv_id":"2605.08501","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"paper_title":"Lepton Flavor Violating Higgs decays at the Compact Linear Collider","primary_cat":"hep-ph","submitted_at":"2026-05-08T21:33:29+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"CLIC could place 95% CL upper limits of 10^{-4} to 10^{-5} on the branching fractions of h→eμ, h→τμ, and h→eτ with 4 ab^{-1} at 1.4 TeV and 5 ab^{-1} at 3 TeV.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Reproduction of this article or parts of it is allowed as specified in the CC-BY-4.0 license. *fmgaray@cern.ch arXiv:2605.08501v1 [hep-ph] 8 May 2026 2 The Compact Linear Collider CLIC 1 Introduction One of the primary objectives in contemporary particle physics is to explore phenomena beyond the Standard Model (BSM). The discovery of a scalar Higgs boson at the LHC [1, 2] has offered significant insights into the mechanism of electroweak symmetry breaking [3-5], thereby opening new avenues for investigating BSM physics within the Higgs sector. The Standard Model (SM) of particle physics forbids lepton flavor violation (LFV) at tree level. Such processes can only occur via loop-level contributions involving neutrinos, resulting in extremely small"},{"citing_arxiv_id":"2605.07972","ref_index":38,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"paper_title":"It Just Takes Two: Scaling Amortized Inference to Large Sets","primary_cat":"cs.LG","submitted_at":"2026-05-08T16:32:34+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"A mean-pool deep set trained on sets of size at most two produces an encoder that generalizes to arbitrary sizes, decoupling representation learning from posterior modeling and making training cost independent of deployment set size N.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.08294","ref_index":6,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"paper_title":"Completely asymptotically free chiral theories with scalars","primary_cat":"hep-th","submitted_at":"2026-05-08T10:07:49+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Complete asymptotic freedom holds in these chiral theories with scalars for particular choices of gauge group size and multiplicities of vector-like and chiral fermion families.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"interactions. Since it is a chiral gauge-Yukawa field theory, gaining a deeper theoretical understanding of these models is paramount. It is well known that the SM must be an effective field theory since it does feature neither a free nor an interacting ultraviolet fixed point for all its couplings. In fact, the Higgs doublet quartic coupling runs negative [ 6, 7], indicating a metastable vacuum, while the hypercharge hits a Landau pole at short distances 1. On the phenomenological side, several fundamental questions are left unanswered, such as the origin of dark matter, the flavour mass hierarchy, matter-antimatter asymmetry, and the interplay with quantum gravity. To partially address these limitations, extensive"},{"citing_arxiv_id":"2605.04233","ref_index":2,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Indications for New Higgs Bosons","primary_cat":"hep-ph","submitted_at":"2026-05-05T19:19:55+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Excesses in di-photon and other channels at the LHC indicate possible new scalars near 95 GeV and 152 GeV, with the 152 GeV candidate fitting an SU(2)_L triplet model that also affects top-quark distributions.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Introduction The Standard Model (SM) of particle physics is the currently accepted theory describing the knownfundamental constituentsofmatterand theirinteractions. Ithasbeen extensivelytestedand verified within the last decades by a plethora of measurements [1] and the discovery of the Higgs boson at the Large Hadron Collider (LHC) in 2012 at CERN [2, 3] confirmed the existence of its last missing ingredient; the only known fundamental scalar particle. However, the SM cannot account for the non-vanishing neutrino masses observed via oscil- lations (in its original and minimal form without right-handed neutrinos) nor for the astrophysical evidenceforDarkMatter,theacceleratedexpansionoftheuniverse(DarkEnergy)ortheindications"},{"citing_arxiv_id":"2605.04142","ref_index":224,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"paper_title":"Heterotic String Theory Suggests a QCD Axion Near 0.5 neV","primary_cat":"hep-th","submitted_at":"2026-05-05T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Heterotic string theory implies the QCD axion mass is bounded below by 0.5 neV and typically falls in [0.5, 0.8] neV across most compactifications.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.02848","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"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":"background","top_context_polarity":"background","context_text":"004; the Kavli Foundation; the Nvidia Corporation; the SuperMicro Corporation; the Welch Foundation, contract C-1845; and the Weston Havens Foundation (USA). Data availability Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS data preservation, re-use and open access policy. References [1] ATLAS Collaboration, \"Observation of a new particle in the search for the standard model Higgs boson with the ATLAS detector at the LHC\",Phys. Lett. B716(2012) 1, doi:10.1016/j.physletb.2012.08.020,arXiv:1207.7214. [2] CMS Collaboration, \"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC\",Phys. Lett. B716(2012) 30,"},{"citing_arxiv_id":"2604.27795","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"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":"background","top_context_polarity":"background","context_text":"004; the Kavli Foundation; the Nvidia Corporation; the SuperMicro Corporation; the Welch Foundation, contract C-1845; and the Weston Havens Foundation (USA). Data availability Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS data preservation, re-use and open access policy. References [1] ATLAS Collaboration, \"Observation of a new particle in the search for the standard model Higgs boson with the ATLAS detector at the LHC\",Phys. Lett. B716(2012) 1, doi:10.1016/j.physletb.2012.08.020,arXiv:1207.7214. [2] CMS Collaboration, \"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC\",Phys. Lett. B716(2012) 30,"},{"citing_arxiv_id":"2604.27471","ref_index":7,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Constraints on a Light Singlet Scalar from Combined Exotic Higgs Decays","primary_cat":"hep-ph","submitted_at":"2026-04-30T06:13:24+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Requiring exotic Higgs decays to two or three light singlet scalars not to exceed the SM Higgs width yields cos θ < 0.12-0.13 for m_φ < 40 GeV, with predicted rate limits Γ(h→φφ) < 0.06 MeV and Γ(h→φφφ) < 5×10^{-6} MeV under stronger mixing bounds.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"W. Higgs, Broken Symmetries and the Masses of Gauge Vector Mesons, Phys. Rev. Lett. 13 (1964) 508. [5] F. Englert and R. Brout, Broken Symmetry and the Masses of Gauge Vector Mesons, Phys. Rev. Lett. 13 (1964) 321. [6] G. S. Guralnik, C. R. Hagen, and T. W. B. Kibble, Global Conservation Laws and Massless Particles, Phys. Rev. Lett. 13 (1964) 585. [7] ATLAS Collaboration, G. Aad et al., Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC, Phys. Lett. B716 (2012) 1, [arXiv:1207.7214]. [8] CMS Collaboration, S. Chatrchyan et al., Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC, Phys. Lett. B716 (2012) 30,"},{"citing_arxiv_id":"2604.27044","ref_index":7,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"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":"background","top_context_polarity":"background","context_text":"These are the most stringent constraints achieved in the 4b final state to date. Submitted to Physical Review D © 2026 CERN for the benefit of the CMS Collaboration. CC-BY-4.0 license *See Appendix A for the list of collaboration members arXiv:2604.27044v1 [hep-ex] 29 Apr 2026 1 1 Introduction The discovery of the Higgs boson (H) [1-6] in 2012 by the ATLAS [7] and CMS [8] Collabora- tions at the CERN LHC prompted a broad research program to determine its properties. To date, all measured properties are found to be consistent with the standard model (SM) predic- tions [9, 10]. In the SM, after electroweak (EW) symmetry breaking the Higgs field (H) potential can be written as V(H) = 1 2m2 HH2 +λvH 3 + 1 4 λH4,"},{"citing_arxiv_id":"2604.24924","ref_index":66,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Forward backward CP asymmetry in $\\tau^- \\to K \\pi \\nu_{\\tau}$ in the Left-Right Inverse seesaw model","primary_cat":"hep-ph","submitted_at":"2026-04-27T19:05:12+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"The Left-Right Inverse Seesaw model generates a non-decoupling scalar operator that enhances the differential forward-backward CP asymmetry A_CP^FB(s) near K* and K0* resonances in τ → Kπν_τ while leaving the integrated asymmetry too small to explain the BaBar result.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"NG: The charged Yukawa coupling connectingτR, the heavy stateNi, and the charged Goldstone bosonG±. In the Left-Right model, this is dynamically generated by the right-handed scale [26]: Yτi NG≃gR√ 2 MNi vR ,(47) whereg R is theSU(2) R gauge coupling. The explicit form of the Yukawa couplings can be found in Ref. [54]. The functionI4 is the exact, dimensionless four-point scalar loop integral (the Passarino-VeltmanD0 function [66] evaluated at zero external momentum, which is the correct kinematic limit for heavy mediators). Its exact mathematical definition is I4(m2 1,m 2 2,m 2 3,m 2 4) = ∫ ∞ 0 xdx (x+m 2 1)(x+m 2 2)(x+m 2 3)(x+m 2 4).(48) 13 In the heavy neutrino limitMNi→∞, this integral simplifies to [34] I4 MNi→∞ −−−−−−→1 M2 Ni [M2 H 0 ln(M 2 H 0)−M2 G±ln(M 2 G±) M2 H 0−M2"},{"citing_arxiv_id":"2604.24531","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"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":"and PCTI (Spain); MOSTR (Sri Lanka); Swiss Funding Agencies (Switzerland); MST (Taipei); MHESI (Thailand); TUBITAK and TENMAK (T ¨urkiye); NASU (Ukraine); STFC (United King- dom); DOE and NSF (USA). Data availability Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS data preservation, re-use and open access policy. References [1] ATLAS Collaboration, \"Observation of a new particle in the search for the standard References 9 model Higgs boson with the ATLAS detector at the LHC\",Phys. Lett. B716(2012) 1, doi:10.1016/j.physletb.2012.08.020,arXiv:1207.7214. [2] CMS Collaboration, \"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC\",Phys. Lett. B716(2012) 30,"},{"citing_arxiv_id":"2604.24421","ref_index":3,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Double SM-like Higgs Production at future $ e^+ e^- $ colliders in the 3-Higgs Doublet Model under the $ S_{3} $ symmetry","primary_cat":"hep-ph","submitted_at":"2026-04-27T12:50:06+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"In the S3-symmetric three-Higgs-doublet model, double SM-like Higgs production at future e+e- colliders deviates from SM predictions by up to several orders of magnitude in the hhZ and hhνν channels.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"The S3-3H model is built by applying the permutation symmetry among three scalar doublets, which can be split into one singlet and two doublets repre- sentation under the S 3 group. The S3-3H model has been studied in different frameworks [3-10]. As well as the S 3 symmetry, a residualZ 2 symmetry can appear after electroweak symmetry breaking, which assign the charge of the scalar sector [3, 4]. The S3-3H model offers nine physical bosons, one of which act as a SM-like Higgs boson. The Higgs couplings to gauge bosons and Higgs self-coupling in the S3-3H model differ from those in the SM. The S3-3H model is quite convinient for studying double Higgs production process, due to these properties. Furthermore, the existance of additional heavy scalars can cause resonant"},{"citing_arxiv_id":"2604.17514","ref_index":1,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"paper_title":"Higgs Physics at a $\\sqrt{s} = 10$ TeV Muon Collider","primary_cat":"hep-ex","submitted_at":"2026-04-19T16:10:09+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Simulations indicate that a 10 TeV muon collider with 10 ab^{-1} luminosity can measure the Higgs trilinear self-coupling and related processes with high precision using the MUSIC detector concept.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.16679","ref_index":10,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Probing Flavor-Violating Higgs Decays in the Type-III Two-Higgs-Doublet Model at the LHC and HL-LHC","primary_cat":"hep-ph","submitted_at":"2026-04-17T20:22:37+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"In the Type-III 2HDM, neutral and heavy charged flavor-violating Higgs decays can exceed 5 sigma significance at 300 fb^{-1} luminosity while the light charged mode is more background-limited.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.15834","ref_index":2,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Comprehensive analyses of rare $ \\Lambda_b \\rightarrow \\Lambda \\ell^+ \\ell^-$, $\\Sigma_b \\rightarrow \\Sigma \\ell^+ \\ell^-$ and $\\Xi_b \\rightarrow \\Xi \\ell^+ \\ell^-$ decays in 2HDM","primary_cat":"hep-ph","submitted_at":"2026-04-17T08:36:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"The work computes differential and total branching ratios plus forward-backward asymmetries for Λ_b → Λ ℓ⁺ℓ⁻, Σ_b → Σ ℓ⁺ℓ⁻ and Ξ_b → Ξ ℓ⁺ℓ⁻ in 2HDM Type III and contrasts them with SM predictions.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Furthermore, we highlight the potential for experimental investigations of these decay channels in the near future. The soon-to-be updated LHCb and/or Belle II detectors, renowned for their capabilities in studying rare decays, present excellent opportunities for probing the predicted branching ratios. I. INTRODUCTION The discovery of a scalar particle with a mass of approximately 125 GeV at the ATLAS [1] and CMS [2] experiments aligns, within theoretical and experimental uncertainties, with the predictions of the Standard Model (SM) Higgs boson. The properties of the Higgs boson, denoted as h, continue to be extensively measured, including its mass, width, quantum numbers, couplings, and more. The search for additional Higgs bosons remains as a significant focus of the Large Hadron Collider (LHC) physics"},{"citing_arxiv_id":"2604.15425","ref_index":6,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"The $Z_3$ soft breaking in the I(2+1)HDM and its cosmological probes","primary_cat":"hep-ph","submitted_at":"2026-04-16T18:00:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Soft Z3 breaking in the I(2+1)HDM makes the lightest Z3-charged neutral scalar a dark matter candidate while allowing a long-lived opposite-CP state to contribute to relic density or yield missing-energy plus multi-lepton/jet signatures with displaced vertices at the ILC.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"NHDMs can, in particular, afford one with viable DM candidates. For example, the so-called inert 2HDM, also called the Inert Doublet Model (IDM), provides one such DM candidate. In this model, even parity is assigned to the SM fermions, there is no softly broken term acting on theZ 2 symmetry in the Higgs potential and only theZ 2 even doublet gets a Vacuum Expectation Value (VEV) [6]. Since theZ 2 is kept unbroken, the lightestZ 2 odd scalar is, therefore, stable and can be a DM if the particle is neutral. The inert sector of an NHDM with more than two doublets also provides DM candidates. In the case of a 3-Higgs Doublet Model (3HDM), there are many possibilities to impose a discrete symmetry and trigger its breaking patterns."},{"citing_arxiv_id":"2604.14284","ref_index":1,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"A Busy Higgs Signal","primary_cat":"hep-ph","submitted_at":"2026-04-15T18:00:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Higher-order Higgs couplings induce an electroweak-symmetry-breaking enhancement that makes Higgs-rich final states the dominant signals for scalar resonances and opens resonant multi-Higgs channels above a couple of TeV.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"opens resonant tri-Higgs and four-Higgs channels as well-motivated search targets. The same under- lying mechanism extends to heavy fermionic and vector resonances, where it can similarly enhance channels such asht,Zh, andγh. We present this framework in effective field theory, demonstrate possible UV completions, and discuss its implications for collider searches. I. INTRODUCTION Since the discovery of the Higgs boson [1, 2], the Higgs sector has been studied extensively, with increasing at- tention devoted to precision measurements of Higgs cou- plings [3-14]. Motivated by accessing the Higgs self inter- action, the di-Higgs final state is one of the main focuses of the physics program at the LHC [15-19]. In parallel, substantial effort has also been devoted to searches for"},{"citing_arxiv_id":"2604.12613","ref_index":64,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Next-to-next-to-next-to-leading order QCD corrections to photon-pair production","primary_cat":"hep-ph","submitted_at":"2026-04-14T11:41:25+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"N³LO QCD predictions for photon-pair production are presented, demonstrating perturbative convergence.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Diphoton production is a background process forH→γγ, which was the most important decay chan- nel for the discovery of the Higgs boson [60, 61]. Fur- thermore, it has been measured directly by ATLAS [62] and CMS [63]. In Ref. [62], measurements were com- pared with NNLO predictions forpp→γγobtained with NNLOJET. Before that, NNLO calculations had been per- formed withq T slicing [64, 65]. The calculations showed that while the prediction starts to agree with the data at NNLO, no convergence is observed when increasing the order of the approximation. Instead, both next-to- leading order (NLO) and NNLO calculations yield cross- section values well outside the theory uncertainty pre- dicted by the previous order. Furthermore, this theory"},{"citing_arxiv_id":"2604.09809","ref_index":3,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"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":"[1] CMS Collaboration, \"Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC\",Phys. Lett. B716(2012) 30, References 23 doi:10.1016/j.physletb.2012.08.021,arXiv:1207.7235. [2] CMS Collaboration, \"Observation of a new boson with mass near 125 GeV in pp collisions at √s=7 and 8 TeV\",JHEP06(2013) 081, doi:10.1007/JHEP06(2013)081,arXiv:1303.4571. [3] ATLAS Collaboration, \"Observation of a new particle in the search for the standard model Higgs boson with the ATLAS detector at the LHC\",Phys. Lett. B716(2012) 1, doi:10.1016/j.physletb.2012.08.020,arXiv:1207.7214. [4] CMS Collaboration, \"Identification of heavy, energetic, hadronically decaying particles using machine-learning techniques\",JINST15(2020) P06005,"},{"citing_arxiv_id":"2604.06530","ref_index":9,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"The non-topological $Z^\\prime$ string in the 331 model and its classical stability","primary_cat":"hep-ph","submitted_at":"2026-04-08T00:02:42+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Numerical perturbation analysis shows non-topological Z' strings in the minimal 331 model remain stable only near the semilocal limit θ_S ≈ π/2 even after tuning Higgs self-couplings.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.03382","ref_index":11,"ref_count":1,"confidence":0.9,"is_internal_anchor":true,"paper_title":"Global Electroweak Fit Constraints on the Two-Higgs-Doublet Model in Light of the CDF W -Boson Mass","primary_cat":"hep-ph","submitted_at":"2026-04-03T18:26:25+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"The CDF W mass anomaly can be accommodated in the 2HDM via enhanced ΔT from scalar mass splittings, yielding updated constraints on the model's parameter space from global electroweak fits.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"sinβcosβ − λ4 +λ 5 2 v2.(6) The CP-even mass eigenstates are obtained by diagonalizing the neutral scalar mass matrix with mixing angleα, leading to the massesm h andm H. In the phenomenologically relevant alignment limit, cos(β−α)→0,(7) the lighter CP-even statehacquires SM- like couplings, consistent with current Higgs signal-strength measurements [11, 12]. This 3 parametrization is standard in numerical stud- ies and is implemented in public tools such as 2HDMC[10]. The contributions of the extended scalar sector to electroweak precision observ- ables are governed primarily by the mass split- tings amongH,A, andH ±, which induce cor- rections to the oblique parameters, particularly ∆T. A. Oblique Parameters in the 2HDM"},{"citing_arxiv_id":"2604.02526","ref_index":56,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"paper_title":"Applied Statistics Requires Scientific Context","primary_cat":"stat.AP","submitted_at":"2026-04-02T21:24:58+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"The paper argues that statistical inference requires nuanced scientific context and that universal significance thresholds should be abandoned.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2603.15882","ref_index":6,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Probing compressed triplet scalars with ISR jets and soft leptons at the LHC","primary_cat":"hep-ph","submitted_at":"2026-03-16T20:22:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A cut-and-count analysis exploiting ISR jets and soft leptons can reach discovery sensitivity for compressed triplet scalars with 1-30 GeV splittings at 3000 fb^{-1}.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2603.13970","ref_index":5,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Shapes are not enough: CONSERVAttack and its use for finding vulnerabilities and uncertainties in machine learning applications","primary_cat":"cs.LG","submitted_at":"2026-03-14T14:53:50+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"CONSERVAttack creates adversarial perturbations in HEP ML models that respect uncertainty bounds but cause misclassifications, revealing gaps in current validation practices.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2603.11259","ref_index":57,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Comprehensive Mass Predictions: From Triply Heavy Baryons to Pentaquarks","primary_cat":"hep-ph","submitted_at":"2026-03-11T19:38:54+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Machine learning models trained on known hadron data and an extended Gürsey-Radicati mass formula predict masses for triply heavy baryons and numerous pentaquark states, agreeing with available data and forecasting unobserved states.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2602.03235","ref_index":5,"ref_count":1,"confidence":0.88,"is_internal_anchor":true,"paper_title":"Search for the production of dark Higgs in the framework of Mono-Z$^{\\prime}$ portal at the FCC-ee simulated electron-positron collisions at $\\sqrt{s} = 240$ GeV","primary_cat":"hep-ph","submitted_at":"2026-02-03T08:11:38+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Upper limits at 95% CL are placed on the mass of the dark Higgs boson in the Mono-Z' portal model from simulated FCC-ee data at 240 GeV center-of-mass energy.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2601.10984","ref_index":4,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"The Sensitivity of Higgs Factories to Composite Higgs Models via Precision Measurements","primary_cat":"hep-ph","submitted_at":"2026-01-16T04:07:41+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Precision Higgs factory measurements can probe composite Higgs models with top quark partners above 3 TeV while also predicting deviations in top-Z couplings.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2601.02808","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Two Higgs doublet model with a complex singlet scalar and Multi-critical Point Principle","primary_cat":"hep-ph","submitted_at":"2026-01-06T08:31:19+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"A 2HDM extended by a complex singlet uses tree-level MPP to motivate degenerate neutral Higgs masses, yielding viable DM phenomenology and a thermally induced strong first-order electroweak phase transition.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2601.01527","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Top-quark pair production in electron-positron collisions within the minimal noncommutative Standard Model","primary_cat":"hep-ph","submitted_at":"2026-01-04T13:35:33+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Noncommutative effects up to second order in Θ induce measurable deviations in the e+e− → tt̄ total cross section, polar and azimuthal distributions, and forward-backward asymmetry at ILC and CLIC energies.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2512.04959","ref_index":16,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"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":"Roloff, (2018), arXiv:1812.01644 [hep-ex]. [13] J. De Blas, G. Durieux, C. Grojean, J. Gu, and A. Paul, JHEP12, 117 (2019), arXiv:1907.04311 [hep-ph]. [14] J. de Blas, Y. Du, C. Grojean, J. Gu, V. Miralles, M. E. Peskin, J. Tian, M. Vos, and E. Vryonidou, inSnowmass 2021 (2022) arXiv:2206.08326 [hep-ph]. [15] J. de Blaset al., JHEP01, 139 (2020), arXiv:1905.03764 [hep-ph]. [16] P. Artoisenetet al., JHEP11, 043 (2013), arXiv:1306.6464 [hep-ph]. [17] T. Barklow, K. Fujii, S. Jung, R. Karl, J. List, T. Ogawa, M. E. Peskin, and J. Tian, Phys. Rev. D97, 053003 (2018), arXiv:1708.08912 [hep-ph]. [18] A. V. Gritsanet al., (2022), arXiv:2205.07715 [hep-ex]. [19] H. Ono and A. Miyamoto, Eur. Phys. J. C73, 2343 (2013), arXiv:1207."},{"citing_arxiv_id":"2511.23149","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Precision Measurements of Higgs Hadronic Decay Modes at the FCC-ee","primary_cat":"hep-ex","submitted_at":"2025-11-28T12:54:47+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"FCC-ee projections show percent to per-mil precision on Higgs hadronic decay rates including first sensitivity to the rare H to strange-strange mode.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.21240","ref_index":17,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Search for signatures of electroweakinos with photons, jets, and large missing transverse momentum in $\\sqrt{s}=13$ TeV pp collisions with the ATLAS detector","primary_cat":"hep-ex","submitted_at":"2025-11-26T10:16:05+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"No significant excess observed; gauginos excluded up to 1.2 TeV in specific supersymmetric decay scenarios.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.10631","ref_index":28,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"A Bayesian Perspective on Evidence for Evolving Dark Energy","primary_cat":"astro-ph.CO","submitted_at":"2025-11-13T18:54:40+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Bayesian evidence favors a constant dark energy model for DESI plus Planck data and shows that apparent support for evolving dark energy with added supernova data stems from a 2.95 sigma tension between DESI and DES-SN5YR that the flexible model resolves.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.08154","ref_index":3,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Good flavor search in SU(5): a machine learning approach","primary_cat":"hep-ph","submitted_at":"2025-11-11T12:06:14+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Machine learning optimization of a generalized SU(5) parameter y finds y ≈ 0.8 produces the closest match to the original model while resolving the fermion mass discrepancy.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2511.04796","ref_index":5,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"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":"2510.02857","ref_index":1,"ref_count":2,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Search for a resonance decaying into a scalar particle and a Higgs boson in the final state with two bottom quarks and two photons with 199 fb$^{-1}$ of data collected at $\\sqrt{s}$=13 and 13.6 TeV with the ATLAS detector","primary_cat":"hep-ex","submitted_at":"2025-10-03T09:53:41+00:00","verdict":"ACCEPT","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"No significant excess observed in search for X → S(bb)H(γγ); 95% CL limits on σ×BR set from 9 fb to 0.06 fb over m_X 170-1000 GeV and m_S 15-500 GeV in 199 fb^{-1} of ATLAS data.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}