A possible solution to the gallium anomaly moving beyond the leptonic wave function factorizationFor over thirty years, a 20\% deficit, now exceeding 5σ, has persisted between measured and predicted neutrino capture rates on 71Ga, as observed in radioactive source experiments…M. Cadeddu, N. Cargioli, F. Dordei et al.·Jun 17, 2026SaveLearn
Do SN 1987A data yield the three neutrino masses?Currently only upper limits are known for the neutrino masses based on cosmological constraints and direct neutrino mass experiments. This review explores the possibility that SN 1987A might provide…Robert Ehrlich·Jun 17, 2026SaveLearn
Digit anomalies in the hadronic mass spectrum, classical and quantum information entropies, and the dynamical QCD scaleQuantum Chromodynamics (QCD) has an emergent dynamical energy scale Λ QCD which sets the threshold between perturbative and nonperturbative regimes. This characteristic scale causes hadronic…R. da Rocha, R. D. Vilela·Jun 17, 2026SaveLearn
HadroTOPS: A Monte Carlo Event Generator For Hadron Production In Two-Photon Scattering In Electron Positron CollisionsWe present a Monte Carlo event generator specifically developed for the study of hadronic two-photon fusion events in two-photon scattering at electron-positron colliders. The code enables the…Max Lellmann, Igor Danilkin, Achim Denig et al.·Jun 17, 2026SaveLearn
Axion Quality Problem: Keep Calm and BaryonAxion models generically suffer from a severe quality problem when coupled to gravity. In this article we provide a very simple model with a high quality axion. The axion is a pseudo-Nambu-Goldstone…Prateek Agrawal, Anson Hook, Vazha Loladze et al.·Jun 17, 2026SaveLearn
Spectroscopy and Radiative Decays of Ωccc and Ωbbb Baryons in a Quark-Diquark ModelWe present a comprehensive study of the spectra and radiative decays of the triply heavy baryons Ωccc and Ωbbb within a quark-diquark framework using a screened potential model. The…Chaitanya Anil Bokade, Bhaghyesh·Jun 17, 2026SaveLearn
Deep Neural Network Driven Simulation Based Inference Method for Pole Position Estimation under Model MisspecificationSimulation Based Inference (SBI) is shown to yield more accurate resonance parameter estimates than traditional chi-squared minimization in certain cases of model misspecification, demonstrated…Daniel Sadasivan, Isaac Cordero, Andrew Graham et al.·Jun 17, 2026SaveLearn
The next-to-leading order of the differential cross-section of the subprocess of Compton scattering of quark-gluon of prompt photon production in proton-proton collisions at NICA energiesIn the presented article, the next-to-the-leading-order calculation of the differential cross-section of the Compton scattering subprocess qg → qγ for prompt photon production in…Mohsun Rasim Alizada, Azar Inshalla Ahmadov·Jun 16, 2026SaveLearn
π0-γ mixing in the presence of a strong magnetic fieldWe analyze the mixing between the π0 meson and the photon in the presence of a strong uniform magnetic field, in the context of a two-flavor Nambu-Jona-Lasinio model. It is shown that only one…D. Gomez Dumm, S. Noguera, N. N. Scoccola·Jun 16, 2026SaveLearn
Stress testing of fast reconstruction pipelines using machine learningThe fast reconstruction and detector-simulation pipelines are widely used in different scientific domains, such as, in High Energy Physics (HEP) and medical imaging, where the full experimental or…Swagata Ghosh·Jun 16, 2026SaveLearn
The Landscape of Composite Higgs ModelsWhile the Standard Model (SM) of particle physics contains the most precise set of predictions ever devised by humanity, that precision comes at a cost. The strange nature of the Higgs particle…Daniel Murnane·Jun 16, 2026SaveLearn
Self-Calibration of the Neutrino-Argon Cross Section with Solar NeutrinosThe success of DUNE's MeV physics program depends upon high-precision knowledge of the charged-current (CC) νe+40Ar cross section. While there are indirect constraints at the 10%…Rasmi Hajjar, Obada Nairat, John F. Beacom·Jun 16, 2026SaveLearn
Standard Candles for Supernova Neutrino Detection at DUNEThe Deep Underground Neutrino Experiment (DUNE) far detector is sensitive to O(10) MeV electron neutrinos through νe charged-current reaction with argon. This capability is a unique…Ting Cheng, Matheus Hostert, Pedro A. N. Machado et al.·Jun 16, 2026SaveLearn
Weak corrections to Minimal Dark Matter annihilationsWe compute the one-loop weak corrections to the annihilation cross sections of fermionic Minimal Dark Matter multiplets. Infrared divergences cancel in the dominant s-wave combination relevant for…Dario Buttazzo, Mateusz Duch, Pier Paolo Giardino et al.·Jun 16, 2026SaveLearn
Twist-3 contributions to γγπ0π0,\,KS0KS0 in kT factorizationWe compute the cross sections for the two-photon processes γγπ0π0 and γγ KS0KS0 in kT factorization, including the chirally enhanced two-parton twist-3 light-cone distribution…Jun-Kang He, Cong Wang·Jun 16, 2026SaveLearn
Ultra-High-Energy Cosmic Ray Boosted Relic NeutrinosUltra-high-energy cosmic rays (UHECRs) can boost relic neutrinos to high energies through Standard Model (SM) neutral-current interactions, providing an indirect probe of the cosmic neutrino…Jiajie Zhang, Jiajun Liao·Jun 16, 2026SaveLearn
From target to projectile: CSS evolution of quark TMD in different light-cone gaugesWe calculate the one-loop corrections to the quark TMD in the projectile light-cone gauge using the background field formalism, with the Mandelstam-Leibbrandt (ML) prescription for the extra…Tolga Altinoluk, Guillaume Beuf, Jamal Jalilian-Marian et al.·Jun 16, 2026SaveLearn
Semi-analytical results for e+e- J/ψ+ X non\,cc up to O(αs v2) at B factoriesWithin the NRQCD factorization framework, we investigate the color-singlet contribution to e+e- J/ψ+ X non\,cc at B factories, computing the O(αs),…Cong Li, Hao-Yang Liu, Xu-Dong Huang et al.·Jun 16, 2026SaveLearn
Description of the process e+ e- π0π0 γ in the extended NJL modelThe cross section of the process e+ e- π0π0 γ is calculated in the extended NJL quark model. The vector channel with the intermediate ρ, ω, ρ' and ω' mesons is considered.…M. K. Volkov, A. A. Pivovarov, K. Nurlan·Jun 16, 2026SaveLearn
Search for a Time-Dependent Z' Resonance in the Dimuon ChannelWe present a time-domain search strategy for resonances with periodically varying masses in high-energy collider data. Conventional resonance searches rely on time-integrated event samples and are…Marlon P. Brade, Jeremiah D. Juevesano, Venus Abbegaile S. Carbonel et al.·Jun 16, 2026SaveLearn
Fourier-Preconditioned Path Deformations for Multi-Field Vacuum TunnellingWe present an endpoint-safe Fourier method for multi-field vacuum tunnelling. The field-space tunnelling path is written as a straight-line interpolation between the false and true vacua, plus…Suriyah R. Kannagi, Aadarsh Singh, Sudhir K Vempati·Jun 16, 2026SaveLearn
Lepton g-2 non-universality of hadronic contributions and a sub-GeV window to New PhysicsWe propose the linear combination of the anomalous magnetic moments of the muon and electron, aμ-e aμ- (mμ/me)2 ae, as a natural low-energy window quantity that may directly probe…Siyuan Li, Vladimir Pascalutsa, Maxim Pospelov·Jun 16, 2026SaveLearn
Pion structure in Holographic QCDWe employ a holographic model with a modified background that incorporates effective descriptions of key QCD features, including linear confinement and gluon condensation, to study the pion's…Jiali Deng, Defu Hou, Xiaolong Wang et al.·Jun 16, 2026SaveLearn
Flavor as an Incomplete Structure: Conceptual Questions and the Role of DUNEFlavor remains one of the most successful yet least understood structures of the Standard Model. The discovery of the Higgs boson completed the electroweak account of mass generation, but did not…Claudio S. Montanari·Jun 16, 2026SaveLearn
QCD sum rules: Borel parameter vs. Euclidean timeWe explore a modification of QCD sum rules where, instead of Borel transforms of current correlators, one considers the correlators in coordinate space as functions of Euclidean time. Taking the…A. V. Smilga·Jun 16, 2026SaveLearn