{"total":91,"items":[{"citing_arxiv_id":"2606.28272","ref_index":36,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Neutrino oscillation data and a pseudo-Dirac heavy neutral lepton","primary_cat":"hep-ph","submitted_at":"2026-06-26T17:13:23+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"In the minimal pseudo-Dirac HNL scenario, light-neutrino oscillation data fixes an ellipse in the active flavour simplex for leading active-heavy interactions via a single complex amplitude and Majorana phase.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.28212","ref_index":102,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Real poles with opposite-sign residues in the non-perturbative quark 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Sources","primary_cat":"astro-ph.HE","submitted_at":"2026-06-24T15:07:36+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Feasibility proposal for SKA-Low radio detection of PeV gamma-ray air showers from galactic PeVatrons.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.26182","ref_index":55,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Gravitational Wave Signatures from Periodic Orbits around a Non--commutative Schwarzschild Black Hole","primary_cat":"gr-qc","submitted_at":"2026-06-24T13:04:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Non-commutative corrections move periodic orbits inward, lower the energy needed for a given orbit shape, and generate gravitational waves with phase shifts plus higher amplitude; a bound Θ/M² < 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radiation","primary_cat":"gr-qc","submitted_at":"2026-06-03T16:33:27+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":4.0,"formal_verification":"none","one_line_summary":"Derives general solution to □R=0 in R² gravity plus radiation in flat FLRW and establishes integrability of the scalar-field and conformal chiral versions.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2606.03703","ref_index":25,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Phase structure of strong interaction matter from Functional QCD","primary_cat":"hep-ph","submitted_at":"2026-06-02T14:21:51+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"A pedagogical review introducing functional QCD methods for studying the phase diagram of strong interaction matter at finite temperature and 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saturation at scale m_V, normalizes the coupling to the deuteron, and substitutes CD-Bonn couplings to obtain B_ΔΔ ≃ 96 MeV, within 14% of the experimental 84 MeV.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.30419","ref_index":65,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"New quantum information perspectives in the axion--photon and neutrino systems","primary_cat":"hep-ph","submitted_at":"2026-05-28T18:00:02+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":5.0,"formal_verification":"none","one_line_summary":"Axion-photon oscillations generate bipartite mode entanglement with maximal values at resonance, and quantum speed limits are derived for both axion-photon and neutrino 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transverse mass, with the Levy index alpha falling at higher energies.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.13498","ref_index":4,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Pulse shape discrimination for $\\alpha$ event rejection in BEGe-type high-purity germanium detectors","primary_cat":"physics.ins-det","submitted_at":"2026-05-13T13:20:52+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Gamma-only trained multilayer perceptron and likelihood classifiers achieve >2.71e4 alpha rejection in BEGe detectors with >80% signal survival and <20% background survival.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.13903","ref_index":131,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Radiative decays of the 1$P$, 1$D$, 2$S$, and 2$P$ $\\Lambda_c$ and 1$D$, 2$S$, and 2$P$ $\\Xi_c$ charmed baryons","primary_cat":"hep-ph","submitted_at":"2026-05-12T23:16:02+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Constituent quark model calculations of electromagnetic transitions for 1P, 1D, 2S, and 2P states in flavor anti-triplet charmed baryons yield branching ratios to identify specific resonances.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.12767","ref_index":34,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Radioactive Molecules as Laboratories of Fundamental 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m_eff.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"n,κ>0|>|E ± n,κ<0|, or yet|E ↓ n,l|>|E ↑ n|). It is interesting to highlight that in the case of the modified metric forκ <0, the spectrum does not depend on the parameterβ − (see (56)), that is, it is as if the DO \"lived\" in the Minkowski spacetime. So, analogous to what happens with the DO or DE [20-23, 56-58] (and even with the Klein-Gordon equation [85]) in the cosmic string spacetime (or Bonnor- Melvin-Lambda spacetime), where the angular momentum (or total magnetic quantum number) is modified by the topological/curvature parameter, here, this also happens, given byj α+ (orl/α +) andj β− (orl/β −). Consequently, the spectra (55) and (56) forj=l−1/2 (κ >0) also has its degeneracy broken (\"undefined\" or not \"well-defined\"),"},{"citing_arxiv_id":"2605.11278","ref_index":28,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Detection of Gravitons by Measuring Excess of Photon Luminosities from Interstellar and Intergalactic Hydrogen","primary_cat":"hep-ph","submitted_at":"2026-05-11T22:02:11+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"B 71 (1977) 133-134.doi:10.1016/0370-2693(77)90759-6. [26] S. G. Matinyan, G. K. Savvidy, Vacuum Polarization Induced by the Intense Gauge Field, Nucl. Phys. B 134 (1978) 539-545.doi:10.1016/0550-3213(78)90463-7. [27] I. A. Batalin, S. G. Matinyan, G. K. Savvidy, Vacuum Polarization by a Source-Free Gauge Field, Sov. J. Nucl. Phys. 26 (1977) 214. [28] G. Savvidy, From Heisenberg-Euler Lagrangian to the discovery of Chromomagnetic Gluon Condensation, Eur. Phys. J. C 80 (2) (2020) 165.arXiv:1910.00654,doi:10.1140/epjc/ s10052-020-7711-6. [29] M. B. Green, J. H. Schwarz, E. Witten, Superstring theory. Vol. 1: Introduction, Cambridge Monographs on Mathematical Physics, 1988. 24 [30] M. B. Green, J."},{"citing_arxiv_id":"2605.07095","ref_index":24,"ref_count":1,"confidence":0.5,"is_internal_anchor":false,"paper_title":"Baryon Bethe-Salpeter Equation in Minkowski-Space QCD$_2$","primary_cat":"hep-ph","submitted_at":"2026-05-08T01:21:49+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"In 1+1D QCD the baryon Bethe-Salpeter equation reduces to the Bars-Durgut equation under valence truncation and is solved numerically for the spectrum and parton distributions.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"dimensional QCD and the infinitely long pion, Phys. Rev. D 105 (3) (2022) 036009.arXiv:2111.03194, doi:10.1103/PhysRevD.105.036009. [23] M. Ahmady, H. Dahiya, S. Kaur, C. Mondal, R. San- dapen, N. Sharma, Extending light-front holographic QCD using the 't Hooft Equation, Phys. Lett. B 823 (2021) 136754.arXiv:2105.01018,doi:10.1016/j. physletb.2021.136754. 9 [24] M. Rinaldi, F. A. Ceccopieri, V. Vento, The pion in the graviton soft-wall model: phenomeno- logical applications, Eur. Phys. J. C 82 (7) (2022) 626.arXiv:2204.09974,doi:10.1140/epjc/ s10052-022-10538-z. [25] B. Gurjar, C. Mondal, S. Kaur,ϕ-meson spectroscopy and diffractive production using two Schrödinger-like equations on the light front, Phys."},{"citing_arxiv_id":"2605.05936","ref_index":10,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Analysis of Mixed Radiation Fields at the MoEDAL Experiment Based on Real-Time Data from a Timepix Detector Network","primary_cat":"physics.ins-det","submitted_at":"2026-05-07T09:43:35+00:00","verdict":null,"verdict_confidence":null,"novelty_score":null,"formal_verification":null,"one_line_summary":null,"context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.03831","ref_index":26,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Reply to Comment on \"Controlling the Dynamical Evolution of Quantum Coherence and Quantum Correlations in $e^{+}e^{-} \\to \\Lambda\\bar{\\Lambda}$ Processes at BESIII\"","primary_cat":"quant-ph","submitted_at":"2026-05-05T15:01:23+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"The authors clarify that their quantum information analysis of Lambda pair production is grounded in QCD dynamics and prior experimental work rather than lacking physical basis.","context_count":0,"top_context_role":null,"top_context_polarity":null,"context_text":null},{"citing_arxiv_id":"2605.03745","ref_index":219,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"The LHCb Experiment","primary_cat":"hep-ex","submitted_at":"2026-05-04T13:29:57+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"This review summarizes the historical motivation, detector design, experimental techniques, and major physics results of the LHCb experiment at the LHC.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"complementary measurements to those performed by the central detectors, LHCb strengthens the LHC's collective efforts in exploring QGP properties, heavy quark dynamics, and nuclear structure. Finally, the fixed-target program offers valuable measurements to the understanding of cosmic ray spectra by measuring the production rate of anti-protons in p-He collisions [219; 220]. 58The LHCb Experiment 12 Complementarity with other experiments in the field Over the years, multiple experimental facilities have been designed and built to exploit the opportunity of scrutinizing the Standard Model through precision measurements of flavour processes. For example, the NA62 and KOTO experiments aim to measure rare kaon decays from"},{"citing_arxiv_id":"2605.00502","ref_index":52,"ref_count":2,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Multiplicative matching of neutral current deep-inelastic scattering processes at next-to-leading order in PYTHIA 8","primary_cat":"hep-ph","submitted_at":"2026-05-01T08:25:34+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"A multiplicative matching scheme reweights Born-level events in PYTHIA 8 so the first parton shower emission follows the real NLO matrix element, improving agreement with HERA DIS data.","context_count":1,"top_context_role":"method","top_context_polarity":"use_method","context_text":"is to compare the distributions of the DIS quantitiesx,y,Q 2 andW 2. We use a fixed value for the electromagnetic cou- pling with 1/α=137.036. We derive the electroweak pa- rameters from the input ofα(M Z), electroweak mixing an- gle sin2 θW =0.2312, and theZ-boson massM Z =91.1876 GeV . We use the PDF setNNPDF31_nlo_as_0118_luxqed [51] provided by the LHAPDF library [52]. The running of the strong coupling is handled by the PDF set. Setting up the event generation with beam energies cor- responding to the HERA experiments, 27.5 GeV for the elec- tron and 920 GeV for the proton, we generate events with the three generators at process level; without parton show- ers, beam remnants or hadronization. To focus solely on the higher-order effects, all partons"},{"citing_arxiv_id":"2605.00115","ref_index":158,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Crossing into the $m_a > f_a$ Region for Leptophilic ALPs","primary_cat":"hep-ph","submitted_at":"2026-04-30T18:10:39+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":6.0,"formal_verification":"none","one_line_summary":"Leptophilic ALPs with m_a > f_a can explain the electron anomalous magnetic moment tension over a large parameter space and are testable via μ→e conversion.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"Observable SM prediction+m ν Experimental limits (g−2) e/2 Cs: 0.00115965218161(23) [146] Rb: 0.001159652180252(95) [147] 0.00115965218062(12) [145] (g−2) µ/2 0.00116592033(62) [148] 0.00116592059(22) [149] BR(µ→eγ) ≲O(10 −55) [150-152] <1.5·10 −13 [153] (<6·10 −14 [153, 154]) BR(µ→3e) ≲O(10 −55) [150, 155] <1.0·10 −12 [156] (Mu3e:<5·10 −16 [157]) BR(µ+N→e+N) ≲O(10 −54) [158] BRAu <7·10 −13 [159] (Mu2e:BR Al <2.87·10 −17 [160]) (COMET:BR Al <2·10 −17 [161]) BR(τ→eγ) ≲O(10 −49) [151] <3.3·10 −8 [145] BR(τ→µγ) ≲O(10 −49) [151] <4.2·10 −8 [145] BR(τ→3e) ≲O(10 −56) [150, 155] <2.7·10 −8 [145] BR(τ→3µ) ≲O(10 −55) [150, 155] <1.9·10 −8 [145] BR(τ − →e −µ+µ−) ≲O(10 −56) [150, 155] <2.7·10 −8 [145] BR(τ − →µ −e+e−) ≲O(10 −55) [150, 155] <1."},{"citing_arxiv_id":"2604.27993","ref_index":92,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Hadron properties at finite temperature","primary_cat":"nucl-th","submitted_at":"2026-04-30T15:21:01+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"A review of thermal modifications to light and heavy hadron properties via imaginary-time formalism, effective field theories, unitarized approaches, and lattice QCD, with links to heavy-ion phenomenology.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"of chiral partners that are otherwise split by the anomaly, such as the isovectors(π, a0)and isoscalar(σ, η)pairs. Recent lattice-QCDanalysesandeffectivemodelssuggestthatwhileU(1) A breakingeffectspersistatT c [89], theyaresignificantly suppressed, leading to a decrease of theη′mass and a narrowing of the mass splitting between parity partners [89, 90]. In the context of ChPT at low temperatures, this sector has been studied, e.g., in Refs. [91, 92]. Increasing temperature or density can lead to partial restoration of chiral symmetry, potentially through a phase 16 /DownTriangle/DownTriangle /DownTriangle /DownTriangle/DownTriangle /DownTriangle/DownTriangle /DownTriangle /DownTriangle /DownTriangle /DownTriangle /DownTriangle/DownTriangle /DownTriangle/DownTriangle/DownTriangle/DownTriangle/DownTriangle/DownTriangle"},{"citing_arxiv_id":"2604.27706","ref_index":10,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"The impact of experimental conditions on the observation of channeling and crystalline undulator radiation","primary_cat":"physics.acc-ph","submitted_at":"2026-04-30T10:50:17+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":3.0,"formal_verification":"none","one_line_summary":"Simulations of 855 MeV electrons in a boron-doped diamond hetero-crystal show that angular divergence, beam orientation, radiation detection direction, and doping profiles strongly affect channeling and crystalline undulator radiation intensity, achieving good agreement with experiment while noting ","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"This particular motion, known as channelling, is due to the collective action of the electrostatic fields of the lattice atoms [1]. The study of the channelling process of ultra-relativistic projectiles in oriented crystals has become a broad research field [2-6], with applications including beam steering [7], collimation [8], focusing [9], and extraction [10]. When irradiated by beams of ultra-relativistic electrons and positrons, oriented crystals of various geometries have the potential to serve as advanced, versatile crystal-based light sources (CLS). These structures can generate gamma radiation of high intensity spanning a broad range of photon energies from MeV to GeV [6, 11, 12]. Recent research [13] has"},{"citing_arxiv_id":"2604.27541","ref_index":5,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Low mass scalars at $e^+e-$ colliders","primary_cat":"hep-ph","submitted_at":"2026-04-30T07:48:15+00:00","verdict":"UNVERDICTED","verdict_confidence":"LOW","novelty_score":2.0,"formal_verification":"none","one_line_summary":"The paper summarizes new developments in models and experimental searches for low-mass scalars at Higgs factories since prior reviews.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"focus on center-of-mass energies of 240 to 250 GeV. Higher center of mass energies, although also of interest, will not be mentioned here and I refer the reader to [ 3] for more details. 1 arXiv:2604.27541v1 [hep-ph] 30 Apr 2026 2 Processes at Higgs factories At the center-of-mass (com) energies of Higgs factories, Higgs strahlung is the domi- nant production mode for single scalar production [ 5]. Leading-order predictions for Zh production at e+e− colliders for low mass scalars which are Standard Model (SM)- like, using Madgraph5 [ 6], are shown in figure 1 for a center-of-mass energy of 250 GeV. The e+e− → h νℓ ¯νℓ process contains contributions from both scalar strahlung and VBF type topologies, so we also display the expected rates from the former for"},{"citing_arxiv_id":"2604.25748","ref_index":32,"ref_count":1,"confidence":0.88,"is_internal_anchor":false,"paper_title":"Sub-keV energy calibration of CONUS+ via 71Ge M-shell neutron activation","primary_cat":"hep-ex","submitted_at":"2026-04-28T15:12:54+00:00","verdict":"CONDITIONAL","verdict_confidence":"LOW","novelty_score":7.0,"formal_verification":"none","one_line_summary":"Neutron activation resolves the 71Ge M-shell X-ray line at 158.7 eVee in a CONUS+ germanium detector, reducing CEvNS signal prediction uncertainty below 4%.","context_count":1,"top_context_role":"background","top_context_polarity":"background","context_text":"teraction with beryllium nuclei: 241Am→ 237Np +α 9Be +α→ 12C +n (4) Additional reaction channels, such as 9Be(α, n)8Be+α, contribute at the few percent level. The source has an activity of 3.84 GBq corre- sponding to a neutron emission rate of approximately 105 n/s. It emits neutrons with an average energy of about 4.5 MeV and a maximum energy up to 6 11 MeV [32-34]. This energy range is particularly well suited for the activation of 71Ge via neutron capture on 70Ge, while avoiding the production of long-lived radioactive isotopes in the surrounding detector ma- terials, in particular copper. The activation products from copper, 64Cu (half-life 12.7 h) and 66Cu (half-life 5.12 min [35]), decay rapidly and their contributions"},{"citing_arxiv_id":"2604.25557","ref_index":188,"ref_count":1,"confidence":0.88,"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":"background","top_context_polarity":"background","context_text":"GAMBIT, PoS ICHEP2018 (2019) 402.arXiv: 1807.03208,doi:10.22323/1.340.0402. [186] A. Kvellestad, First SUSY results with GAM- BIT, PoS EPS-HEP2017 (2017) 299.arXiv: 1710.02503,doi:10.22323/1.314.0299. 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