{"total":16,"items":[{"citing_arxiv_id":"2606.19299","ref_index":132,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Probing Long-Lived Particle Production in Muon Decays at the SNS with a Highly Capable Hydrocarbon Detector","primary_cat":"hep-ex","submitted_at":"2026-06-17T17:24:16+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Proposes a hydrocarbon detector at SNS for order-of-magnitude better sensitivity to 10-100 MeV axion-like particles and heavy neutral leptons via e+e- decays from muon decays at rest.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.18088","ref_index":60,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Ultra-High-Energy Cosmic Ray Boosted Relic Neutrinos","primary_cat":"hep-ph","submitted_at":"2026-06-16T15:54:42+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Computes the diffuse UHECR-boosted CνB flux across elastic, coherent, incoherent, resonance, and deep-inelastic channels with mixed-composition UHECR models and derives upper limits on CνB overdensity from IceCube and Auger data.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.17132","ref_index":115,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Are neutrinos Majorana? Fixed-target and high-energy astrophysical searches decide","primary_cat":"hep-ph","submitted_at":"2026-06-15T18:00:00+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Correlated HNL discovery at SHiP and flavor ratio shifts in astrophysical neutrinos at telescopes would establish neutrinos as Majorana fermions.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"(Baikal-GVD), Overview of the Baikal-GVD neutrino telescope: 2024 status, EPJ Web Conf.319, 04002 (2025). [113] R. Brocket al.(CTEQ), Handbook of perturbative QCD: Version 1.0, Rev. Mod. Phys.67, 157 (1995). [114] J. M. Conrad, M. H. Shaevitz, and T. Bolton, Precision measurements with high-energy neutrino beams, Rev. Mod. Phys.70, 1341 (1998), arXiv:hep-ex/9707015. [115] J. A. Formaggio and G. P. Zeller, From eV to EeV: Neu- trino Cross Sections Across Energy Scales, Rev. Mod. Phys.84, 1307 (2012), arXiv:1305.7513 [hep-ex]. [116] R. Abbasiet al.(IceCube), The IceCube high-energy starting event sample: Description and flux characteri- zation with 7.5 years of data, Phys. Rev. D104, 022002 (2021), arXiv:2011.03545 [astro-ph."},{"citing_arxiv_id":"2606.12155","ref_index":23,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Improving the Angular Resolution of IBD Events Using Neutron Capture Information in Super-Kamiokande","primary_cat":"hep-ph","submitted_at":"2026-06-10T14:42:04+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Geant4 simulation finds neutron capture positions statistically enhance IBD neutrino directionality in water Cherenkov detectors from ~10 MeV to hundreds of MeV despite diffusion.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.07106","ref_index":59,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Joint probes of dark matter annihilation from neutrino detectors and CMB targets","primary_cat":"hep-ph","submitted_at":"2026-06-05T10:00:53+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Joint analysis of neutrino detectors and CMB observables can constrain dark matter annihilation into neutrinos for MeV-GeV masses.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.06773","ref_index":181,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Lepton interactions from GeV to EeV","primary_cat":"hep-ph","submitted_at":"2026-06-04T23:34:44+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Phenomenological study predicting incomplete tau polarization at FASER2, observable neutrino and muon trident processes, and contributions to hadron structure from IceCube neutrino events.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.00745","ref_index":28,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Comparisons of triple-differential cross sections for quasielastic-like $\\nu_\\mu$-hydrocarbon interactions using $\\langle E_\\nu\\rangle \\sim$ 3~GeV versus $\\sim$ 6~GeV beams in MINERvA","primary_cat":"hep-ex","submitted_at":"2026-05-30T14:25:03+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"MINERvA compares quasielastic-like cross sections at two neutrino beam energies and finds discrepancies pointing to overestimated final state interactions for protons and pions.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"the key model choices are that quasielastic interactions are modeled using the Llewellyn Smith formalism [25] with BBBA05 vector form factors [26] coming from fits to electron scattering data and an axial-vector form fac- tor based on a z-expansion fit to neutrino data on deu- terium [27]. The initial state nucleons are modeled as a relativistic Fermi gas [28] and with a Bodek-Ritchie high momentum tail [29]. Multinucleon quasielastic-like in- teractions, referred to here as 2p2h, are simulated by the Valencia model described in Refs. [5, 6, 30]. Intranuclear final-state interactions of produced hadrons are modeled using the INTRANUKE-hA package [31]. There was an error in GENIE's treatment of Elastic FSI [32] which has"},{"citing_arxiv_id":"2605.24224","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"High Statistics Measurements of $\\nu_{\\mu}$ Charged-Current Single $\\pi^{+}$ Production with Zero Pion Kinetic Energy Threshold in MINERvA","primary_cat":"hep-ex","submitted_at":"2026-05-22T21:11:22+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"High-statistics measurement of νμ CC 1π+ production cross sections on scintillator with zero pion KE threshold shows modern models disagree with data by up to 20% in key regions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.20859","ref_index":46,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Impact of matter effects on the unitarity test of lepton mixing","primary_cat":"hep-ph","submitted_at":"2026-05-20T07:48:29+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"The authors examine extraction of lepton mixing matrix elements from spectral data in neutrino oscillation experiments including matter effects and test unitarity via a vanishing quantity in a four-generation model.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.16721","ref_index":59,"ref_count":2,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Towards Measuring the CP-Violating Phase with Atmospheric Neutrinos","primary_cat":"hep-ph","submitted_at":"2026-05-16T00:07:50+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Proposes a new up-down flux ratio for sub-GeV atmospheric neutrinos to measure δ_CP, potentially exceeding T2HK sensitivity near 90° and 270° at Hyper-Kamiokande.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.15642","ref_index":9,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Locating nuclear-powered submarines with antineutrinos","primary_cat":"hep-ex","submitted_at":"2026-05-15T05:46:02+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Antineutrino-based detection can function as a barrier for locating nuclear submarines, with a 20 kt detector achieving Z_A ≈ 2.54 in the Strait of Gibraltar for a 100 MW case and higher scores with multiple detectors.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.10221","ref_index":1,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"TeV-scale neutrino cross-section measurement using upward through-going muons in Super-Kamiokande","primary_cat":"hep-ex","submitted_at":"2026-05-11T09:00:54+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Super-Kamiokande measures the flux-averaged muon neutrino and antineutrino charged-current cross section at 500-5000 GeV as (0.51 ± 0.11) × 10^{-38} cm² GeV^{-1}.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Neutrino Interactions Neutrinos are unique probes of both fundamental interactions and the high-energy universe. Their weak coupling allows them to escape dense environments and traverse astronomical distances, but also makes their interaction cross sections challenging to measure precisely. Over the past decades, neutrino observations across a vast energy range [1] have established flavour oscillations [2-5], revealed aspects of nucleon structure [ 6], and opened a new window on extreme astrophysical sources [ 7-12]. Yet this broad reach is not matched by equally continuous measurements of neutrino interaction cross sections. In particular, the charged-current (CC) cross section in the TeV regime remains comparatively less known, even"},{"citing_arxiv_id":"2604.21869","ref_index":18,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Analytical and Machine Learning Methods for Model Discernment at CE$\\nu$NS Experiments","primary_cat":"hep-ph","submitted_at":"2026-04-23T17:08:40+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Shape correlations in CEνNS allow likelihood and CNN analyses to discriminate sterile neutrinos from NSI and approximately localize sterile parameters in favorable regions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2604.14409","ref_index":24,"ref_count":1,"confidence":0.9,"is_internal_anchor":false,"paper_title":"Astrophysical bounds on the high-energy evolution of neutrino mixing","primary_cat":"hep-ph","submitted_at":"2026-04-15T20:47:50+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"High-energy astrophysical neutrinos can constrain the running of neutrino mixing parameters with energy, with future multi-detector setups forecast to set strong bounds despite astrophysical uncertainties.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"RG running of the leptonic Dirac CP phase with re- actor neutrinos, Phys. Rev. D111, 115031 (2025), arXiv:2411.18251 [hep-ph]. [22] R. Brocket al.(CTEQ), Handbook of perturbative QCD: Version 1.0, Rev. Mod. Phys.67, 157 (1995). [23] J. M. Conrad, M. H. Shaevitz, and T. Bolton, Precision measurements with high-energy neutrino beams, Rev. Mod. Phys.70, 1341 (1998), arXiv:hep-ex/9707015. [24] J. A. Formaggio and G. P. Zeller, From eV to EeV: Neu- trino Cross Sections Across Energy Scales, Rev. Mod. Phys.84, 1307 (2012), arXiv:1305.7513 [hep-ex]. [25] M. Bustamante, A. M. Gago, and J. Jones P' erez, SUSY Renormalization Group Effects in Ultra High Energy Neutrinos, JHEP05, 133, arXiv:1012.2728 [hep-ph]. [26] S. R. Mir, C. A. Arg¨ uelles, K."},{"citing_arxiv_id":"2412.12076","ref_index":1,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Predictions for dimuon production in high-energy neutrino-proton collisions using the color dipole model","primary_cat":"hep-ph","submitted_at":"2024-12-16T18:46:46+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"A color-dipole-based Monte Carlo generator interfaced with Pythia8 predicts larger transverse momenta and higher yields of angularly separated dimuons in neutrino-proton collisions than standard Pythia.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2311.04206","ref_index":10,"ref_count":1,"confidence":0.98,"is_internal_anchor":true,"paper_title":"Elastic and resonance structures of the nucleon from hadronic tensor in lattice QCD: implications for neutrino-nucleon scattering and hadron physics","primary_cat":"hep-lat","submitted_at":"2023-11-07T18:44:31+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Lattice QCD computation of hadronic tensor yields consistent nucleon Sachs electric form factor and extracts transition form factors to the Roper resonance region for inclusive cross sections.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null}],"limit":50,"offset":0}