Perturbative and nonperturbative properties of heavy quark transport in a thermal SU(3) gluon plasmaWe investigate the perturbative and nonperturbative aspects of heavy quark transport in a thermal SU(3) gluon plasma. Based on the soft-hard factorized model, we extend the original perturbative…Jiazhen Peng, Yage Zhen, Jiale Lou et al.·Jul 7, 2026SaveLearn
Finite-temperature effects on the threshold cusps in ππ and DD scatterings from relativistic heavy-ion collisionsWe investigate how the temperature influences the threshold cusps in meson-meson scatterings, i.e., ππ and DD (or DD) scatterings, using the production rates and…Ying Zhang, Atsushi Hosaka, Qian Wang et al.·Jul 7, 2026SaveLearn
Generic framework for non-perturbative QCD in light hadronsIn this paper, we review several topological aspects of the QCD vacuum and recent progress on this quantitative unifying framework for the low-lying hadron physics rooted in QCD by introducing the…Wei-Yang Liu·Jul 7, 2026SaveLearn
Amplitude of H γZ process via one W loop in unitary gauge (I. Details of calculation with Dyson scheme)Decay amplitude of H γZ process via one W loop in the unitary gauge is presented. The divergent integrals including those of high divergence orders typical of unitary gauge are arranged to…Shi-Yuan Li·Jul 7, 2026SaveLearn
Can blind spots save neutralino dark matter in natural supersymmetry models?Natural supersymmetry (SUSY) models remain viable even in the face of LHC Run 2 sparticle search limits. However, the LZ experiment has placed strong limits on light higgsino dark matter even when…Howard Baer, Vernon Barger, Dibyashree Sengupta·Jul 6, 2026SaveLearn
Linear Breit-Wheeler pair production in the search for axion-like particlesAssuming the existence of axion-like particles (ALPs), the standard Quantum Electrodynamics (QED) amplitudes for the linear Breit-Wheeler (BW) pair production process are shown to be supplemented by…Thomas Rook, Wei Wu, Stuart P. D. Mangles et al.·Jul 6, 2026SaveLearn
Precision Study of Semileptonic and Non-Leptonic Bc Decays to ηc and P Wave CharmoniaWe analyse semileptonic and non-leptonic decays of the Bc meson into P wave charmonium states. The analytic expressions for the transition form factors are taken from NRQCD, while their…Aritra Biswas, Soumitra Nandi, Shantanu Sahoo·Jul 6, 2026SaveLearn
Constant Scaling Fails for Global Monopole NetworksGlobal monopoles, which can also be understood as the zero-gauge-coupling limit of gauged monopoles, can form in the early Universe and evolve following a scaling network, as do other topological…Wakutaka Nakano, Wen Yin·Jul 6, 2026SaveLearn
Searching for charged Higgs bosons in top decays via the t*b channelRare top-quark decays offer a sensitive probe of charged Higgs bosons with masses below the top mass, owing to the large t t production rate at the LHC and the distinctive final states…Saiyad Ashanujjaman, Guglielmo Coloretti, Andreas Crivellin et al.·Jul 6, 2026SaveLearn
Galactic Center Neutrinos from Cosmic Ray-Dark Matter InteractionsThe IceCube and ANTARES collaborations have recently reported evidence for high-energy neutrinos associated with the Galactic plane and the Galactic Ridge, offering a new pathway to search for dark…Jorge Terol Calvo, Pedro de la Torre Luque, Mainak Mukhopadhyay et al.·Jul 6, 2026SaveLearn
Parametric Resonance of Higgsed Vector Dark Matter: Inflationary Initial Conditions and Sourced DisplacementsParametric resonance in a Higgsed Abelian sector provides an efficient mechanism for producing vector dark matter, but its viability depends crucially on the origin of the initial dark-Higgs…Imtiaz Khan, Salvatore Capozziello, G. Mustafa et al.·Jul 6, 2026SaveLearn
The variable flavor number scheme to three-loop orderWe describe the variable flavor number scheme to three-loop order, which modifies the massless parton densities by single- and two-mass effects and introduces heavy-quark parton distribution…J. Ablinger, A. Behring, J. Blümlein et al.·Jul 6, 2026SaveLearn
Pathways and impediments towards a detection of the relic neutrino windA direct detection of the cosmic neutrino background (CNB) in laboratories on Earth has been called the ``holy grail'' of experimental neutrino physics, but a still more glorious prize…Andrew J. Long, Michiru Uwabo-Niibo, Masahide Yamaguchi·Jul 6, 2026SaveLearn
Insight on confinement from the QCD effective chargeLike the Gell-Mann--Low coupling α of QED, the effective charge αg1 is a physical, observable-defined running coupling that can serve as the QCD coupling αs. It can be represented by an…A. Deur·Jul 6, 2026SaveLearn
Flavor decomposition of the gravitational form factors and mechanical structure of the protonWe review in the present talk a series of recent works on the flavor decomposition of the gravitational form factors of the proton and its mechanical properties within the framework of the chiral…Hyun-Chul Kim, June-Young Kim, Ho-Yeon Won·Jul 6, 2026SaveLearn
Beyond Half-Life Limits: Robust Operator-Level Interpretation of Multi-Isotope Neutrinoless Double-Beta DecayCurrent and future neutrinoless double-beta decay (0νββ) searches are usually characterized by half-life limits or projected sensitivities. For operator-level interpretation, however, the relevant…K. Ishidoshiro·Jul 6, 2026SaveLearn
Gluon radiation from a QCD antenna with realistic parton-medium interactionsThe spectrum of coherent gluon radiation from a quark-antiquark pair undergoing multiple scatterings within a colored medium is central for understanding in-medium parton cascades. However, current…Carlota Andrés, Liliana Apolinário, Néstor Armesto et al.·Jul 6, 2026SaveLearn
Sub-eikonal stress and model dependence of the small-x gluon D-termThe leading-eikonal small-x dipole gives a compact representation of the gluon momentum form factor Ag(t). We show that the same information is not sufficient to determine the gluon stress form…Lei Wang·Jul 6, 2026SaveLearn
Classifying the hidden-charm pentaquarks via a flavor mixing schemeIn this work, we propose a scheme to classify the molecular states consisting of ground single-charm baryons (Λc, Ξc, Σc(*), Ξc(*), Ωc(*)) and…Kan Chen, Bo Wang·Jul 6, 2026SaveLearn
Emergent Local Phase-Space Scaling in Small-x Gluon EvolutionGeometric scaling is a central output of nonlinear small-x evolution, but it is less clear whether the same dynamics fixes a probability distribution in transverse phase space. Using fixed-coupling…Lei Wang·Jul 6, 2026SaveLearn
Collinearly Improved Balitsky-Kovchegov Evolution of the Gluon Wigner DistributionWe study how collinearly improved small-x evolution modifies the elliptic gluon Wigner distribution and its coherent diffractive dijet 2ϕ signal. Starting from the SO(3)-symmetric Gubser…Lei Wang·Jul 6, 2026SaveLearn
Energy-Flow Moments for Elliptic Gluon Wigner TomographyThe elliptic small-x gluon Wigner distribution correlates transverse momentum with impact parameter, but it is usually accessed through exclusive diffractive dijets whose recoil is sensitive to…Lei Wang·Jul 6, 2026SaveLearn
Nuclear Gluon Gravitational Form Factors and Neutron Skins at the Electron-Ion ColliderCoherent quarkonium production at the Electron--Ion Collider can image the average small-x gluon radius of nuclei, providing a reaction mechanism complementary to parity-violating electron…Lei Wang·Jul 6, 2026SaveLearn
Hyperon-pair spin tomography beyond scalar spin correlationsSpin correlations measured after hadronization probe how quantum information is transported through confinement. We formulate a process-independent spin-tomography framework for ΛΛ pairs in…Lei Wang·Jul 6, 2026SaveLearn
Multiplicity-dependent forward jet production in proton-nucleus collisionsForward jet production in proton--nucleus collisions probes a dilute projectile scattering from a dense small-x nuclear gluon field, while the charged-particle multiplicity inside the jet probes…Lei Wang·Jul 6, 2026SaveLearn