Axion-photon conversion in stochastic magnetic fieldsWe investigate axion-photon conversion in stochastic magnetic fields, focusing on the evolution of the photon intensity and polarizations induced by conversion into axions. Assuming Gaussian magnetic…Wataru Chiba, Ryusuke Jinno, Kimihiro Nomura·Jul 11, 2026SaveLearn
Shifting the neutrino fog: studying the Isospin-violating Dark Matter caseFirst observation of solar neutrinos through coherent elastic neutrino-nucleus scattering by dark matter (DM) direct detection (DD) experiments makes the study of the neutrino fog of the most…Laura Duque, J. M. Lamprea, Omar G. Miranda·Jul 11, 2026SaveLearn
Finite-size effects and scaling properties of chiral and baryon-number fluctuationsAn effective chiral model is introduced to illustrate finite-size effects, incorporating the standard zero-mode treatment, momentum-space discretization, and gradient effects modeled via a prescribed…Győző Kovács, Pok Man Lo, Krzysztof Redlich et al.·Jul 11, 2026SaveLearn
Charge distribution of the gauge-mediation type Q ballWe numerically study the formation of the gauge-mediation type Q balls in the logarithmic square potential on three-dimensional lattices. We obtain the broad charge distribution of the Q ball of this…Shinta Kasuya, Masahiro Kawasaki·Jul 11, 2026SaveLearn
Spontaneous baryogenesis with large misalignmentWe investigate particle production by a pseudo-Nambu-Goldstone boson (pNGB) in the spontaneous baryogenesis scenario for large misalignment angles. Since the fermionic backreaction is intrinsically…Maxim Krasnov, Ufuk Aydemir, Maxim Khlopov·Jul 11, 2026SaveLearn
One-Dimensional Simulations of the Topological Defects in a 3:1 U(1) ModelThe domain wall is a kind of topological defect that can appear when a discrete symmetry is broken. If the discrete symmetry appears as an intermediate symmetry during a U(1) symmetry breaking, the…Jianjun Hua, Bowen Fu, Yi-Lei Tang·Jul 10, 2026SaveLearn
Suppressing Extra-Dimensional Axion Isocurvature DynamicallyExtra-dimensional QCD axion is well motivated by string compactifications and enjoys enhanced protection against quality-violating effects. If present during inflation, however, its quantum…Gongjun Choi, Tony Gherghetta·Jul 10, 2026SaveLearn
Strong First-Order Electroweak Phase Transitions and Gravitational Waves in the Normal Two-Higgs-Doublet Model: A Comparative Study of the Four Yukawa Types and Thermal Resummation SchemesWe present a comprehensive global analysis of strong first-order electroweak phase transitions (SFOEWPTs) and their associated stochastic gravitational-wave (GW) backgrounds within the Normal…Jin-Hwan Cho, Dongjoo Kim, Jinheung Kim et al.·Jul 10, 2026SaveLearn
The Higgs boson through the lens of electroweak precision dataThe global electroweak fit tests the quantum structure of the Standard Model by confronting precision measurements with high-order theoretical predictions. This paper presents an updated Gfitter…Yannick Fischer, Johannes Haller, Andreas Hoecker et al.·Jul 10, 2026SaveLearn
Benchmarking the Nearside Energy-Energy Correlators with Mellin TransformWe investigate nearside energy-energy correlators (EECs) at small angles, explicitly incorporating the QCD scaling behavior in both the perturbative and post-confinement regimes through a…Yuxun Guo, Feng Yuan·Jul 10, 2026SaveLearn
Counting b-jets at the FCC-ee as a probe of top-quark flavor physicsWe explore the sensitivity of a future FCC-ee to multi-TeV new physics (NP) that can generate vector, scalar and tensor flavor-changing (FC) eetuk contact interactions (uk=u,c for k=1,2),…Shaouly Bar-Shalom, Jose Wudka·Jul 10, 2026SaveLearn
Darkly Charged ALPsThe established d=5 ALP effective Lagrangian describes the interaction of scalars with approximate shift-symmetry which carry no Standard Model (SM) charges with SM fields. It implicitly assumes…Nicolás M. Arenaza, Enrique Fernández-Martínez, Belén Gavela et al.·Jul 10, 2026SaveLearn
Searching for heavy charged relics in the EarthWe propose a method for detecting an ambient density of heavy, electrically-charged particles. Such particles would impact the Earth, lose energy in terrestrial matter, and become trapped. We study…Reza Ebadi, Peter W. Graham, Surjeet Rajendran et al.·Jul 10, 2026SaveLearn
Second-Order Perturbative Correction for Neutrino Oscillation Tomography of the EarthThe Earth's interior at depths exceeding present direct probing limit, which is just one five-hundredth of its radius, remains unknown to a significant extent due to existing ambiguities in…Dmitry Zhuridov, Wiktor Porwoł·Jul 10, 2026SaveLearn
SCET sum rules for B D1(2420) and B D1'(2430) form factors at next-to-leading orderWe present the first calculation of the B D1(2420) and B D'1(2430) transition form factors at O(αs) using light-cone sum rules within the framework of soft-collinear…Jun-Wei Zhang, Yong-Kang Huang·Jul 10, 2026SaveLearn
Disentangling short- vs. long-distance dynamics in B K*μ+μ-We present an updated data-driven analysis of short- vs. long-distance dynamics in B K*μ+μ-. The analysis is based on the recent LHCb measurement of the full angular distribution of this…Marzia Bordone, Gino Isidori, Arianna Tinari·Jul 10, 2026SaveLearn
Analysis of the hidden-charm pentaquark candidates in the J/ψΩ mass spectrum via the QCD sum rulesWe explore the diquark-diquark-antiquark type ssscc pentaquark states with the isospin-spin-parity IJP=012-, 032- and 052- via the QCD sum rules…Zhi-Gang Wang·Jul 10, 2026SaveLearn
Fully-beauty tensor tetraquarkParameters of the fully-beauty tensor tetraquark T=bbbb are computed using QCD sum rule method. The mass m and coupling Λ of this state are evaluated by means of…S. S. Agaev, K. Azizi, H. Sundu·Jul 10, 2026SaveLearn
Running coupling effects in the anti-collinear resummation in high energy evolutionWe study the effects of the running of the QCD coupling on the anti-collinear resummation in JIMWLK evolution in the linear (BFKL) regime. We determine the appropriate scale choice for the coupling…Alex Kovner, Michael Lublinsky, Maxim Nefedov et al.·Jul 10, 2026SaveLearn
Diffusion Monte Carlo study of deuteron-like fully light hexaquarksWe perform a Diffusion Monte Carlo study of fully light hexaquarks containing three u quarks and three d quarks within a constituent-quark model. Both compact and baryon--baryon-like arrangements…M. C. Gordillo, J. Segovia·Jul 10, 2026SaveLearn
Tensor-polarized parton distribution functions of the deuteron by a convolution modelTensor-polarized parton distribution functions (PDFs) are calculated for the deuteron by using a convolution formalism, where the tensor-polarized PDFs are given by the corresponding nucleon's…S. Kumano, Kenshi Kuroki·Jul 10, 2026SaveLearn
Hunting for new physics in B meson b u transitions: A fresh look with Belle II dataWe present an analysis of the decays B- - ν, B0 π+ - ν, and B- ρ0 - ν leveraging the precise measurements of binned…Pietro Colangelo, Fulvia De Fazio, Maria Letizia Di Cuia et al.·Jul 10, 2026SaveLearn
Exclusive J/ψ photoproduction in photon-proton diffractive scattering: A light-front Hamiltonian approachWe investigate the cross-section for exclusive J/ψ production in photon-proton diffractive scattering within the Basis Light-Front Quantization (BLFQ) framework. The leading-order contribution to…Xiaoyi Wu, Zhi Hu, Chandan Mondal et al.·Jul 10, 2026SaveLearn
Enhancing the sensitivity to FCNC top decays t cH and t cS in the boosted regime at CLICThe top quark, having the largest Yukawa coupling to the Higgs sector, provides a unique window into electroweak symmetry breaking and possible new physics beyond the Standard Model. Searches for…Shuo Yang, Peng-Bo Zhao, Ji-Chong Yang·Jul 10, 2026SaveLearn
Minimal Majoron Dark Matter from a Discrete ZN Gauge SymmetryWe investigate majoron dark matter in a minimal setup, where the Standard Model is extended by three right-handed neutrinos and a complex scalar field. The theory is defined by an exact discrete…Subaru Fujisawa, Qiuyue Liang, Shigeki Matsumoto et al.·Jul 10, 2026SaveLearn