Radiative Corrections to the Direct Detection of Inelastic Scattering of Higgsino-like Neutralino Dark MatterThe direct detection (DD) of Higgsino-like dark matter (DM) through inelastic scattering processes may provide a promising avenue, along with the elastic scattering, when the mass splitting between…Arindam Chatterjee, Debottam Das, Syed Adil Pasha et al.·Sep 9, 2026SaveLearn
Charmed baryon semileptonic decays in a relativistic three-quark modelWe study the spin-1/21/2 semileptonic decays of singly charmed baryons (Λc+, Ξc0,+, and Ωc0) into the light baryon octet within a relativistic three-quark model. The constituent…Ru-Hui Ni, Zhen-Yang Wang, Jia-Jun Wu et al.·Sep 9, 2026SaveLearn
More QCD Masterclass Lectures on Jet Physics and Machine LearningThese lectures were presented at the 2026 QCD Masterclass in Saint-Jacut-de-la-mer, France. They supplement the published notes from the 2024 school with presentation of a few new topics that have…Andrew J. Larkoski·Sep 9, 2026SaveLearn
Next-to-Leading-Order Calculation of the Light Tensor (JP=2+) Hybrid Correlation FunctionWe report on the QCD calculations underlying a next-to-leading-order (NLO) QCD Laplace sum-rule analysis of the light tensor (JP = 2+) hybrid meson mass and coupling. This article focuses on the…R. T. Kleiv, J. Ho, S. Li et al.·Sep 9, 2026SaveLearn
Inclusive productions of J/ψ+ηc in e+e- annihilation at BelleWe study e+e- J/ψ+ηc+X at next-to-leading order (NLO) in αs within the nonrelativistic QCD (NRQCD) framework to assess the color-octet (CO) mechanism at low energies. QCD corrections…Zhan Sun, Shu-Jian Qi, Ying-Zhao Jiang·Sep 9, 2026SaveLearn
Cutoff Scales in the Type-I 2HDM with Strongly First-Order Electroweak Phase Transitions: One-Step versus MultistepWe investigate the UV viability of strongly first-order electroweak phase transitions (SFOEWPTs) in the Type-I two-Higgs-doublet model (2HDM), considering both the Normal and Inverted Scenarios (NS…Jin-Hwan Cho, Dongjoo Kim, Jinheung Kim et al.·Sep 8, 2026SaveLearn
Heavy Higgsino Interpretation of the LZ EventThe LZ experiment has recently reported a 248 keV nuclear recoil event in a region where backgrounds are expected to be low. A pure higgsino scattering inelastically through a Z-boson is an…Kevin Langhoff·Sep 8, 2026SaveLearn
Constraints on Neutron-Electron Quantum Dark ForcesInteractions induced by dark matter particles which couple bilinearly to standard model particles through quantum fluctuations were termed quantum dark forces by Brax, Fichet, and Pignol, who…V. Kurmangaliyeva, B. Massak, O. Agyl-Mussapar et al.·Sep 8, 2026SaveLearn
Level-Four Modular Symmetry Selected by the Harmonic Pattern of Quark and Lepton MassesThe mass ratios of the quarks and charged leptons follow a simple pattern. The logarithmic generation steps come in a two to one ratio, a note to its octave, and the ordering is mirrored between the…Vernon Barger·Sep 8, 2026SaveLearn
From LUX-ZEPLIN to Colliders: Probing Higgsino Dark MatterThe high-energy nuclear recoil event with recoil energy ER ≈ 248 keV observed by the LZ collaboration provides an exciting hint toward a model with a 1.1 TeV Higgsino…Kingman Cheung, Sin Kyu Kang, Ranjeet Kumar·Sep 8, 2026SaveLearn
The transverse-spin asymmetry AϕSΛUUT in Λ production in SIDIS within the collinear frameworkWe investigate the transverse-spin asymmetry AϕSΛUUT for transversely polarized Λ production in semi-inclusive deep inelastic scattering with an unpolarized electron beam and an…Yongliang Yang, Zhun Lu·Sep 8, 2026SaveLearn
Free μ+μ- and bound-free e+e- pair production in relativistic heavy-ion collisionsIn our previous studies, we calculated the cross-section for the production of free μ+μ- pairs using a probability function dependent on the impact parameter, and also, we computed bound-free…Melek Yilmaz Şengül·Sep 8, 2026SaveLearn
Hot QCD: transport coefficients in strong and weak coupling regimesWe evaluate the transport coefficients, namely the shear viscosity η and the spatial diffusion coefficient of heavy quarks Ds, within a Quasi-Particle Model (QPM). In particular, for the first…Gabriele Parisi·Sep 8, 2026SaveLearn
A distance-independent constraint on the axion-electron coupling from RGB starsInterest in axions and axion-like particles has resurged, driven by their role in solving the strong CP problem and their appeal as dark matter candidates. The luminosity of the tip of the red giant…Thomas Levasseur, Oscar Straniero, Andrea Caputo·Sep 8, 2026SaveLearn
Gravitational transverse momentum dependent distributions for the gluonsWe investigate the momentum-space structure of the gauge-invariant gluon energy-momentum tensor (EMT) for spin-0 and spin-12 hadrons in the light-front formalism. We parameterize the…Kauship Saha, Dipansu Mishra, Dipankar Chakrabarti et al.·Sep 8, 2026SaveLearn
Nonperturbative functional renormalization group for Higgs-singlet models with physics-informed neural networksWe develop a nonperturbative functional renormalization group framework within the LPA' to solve the Wetterich flow equation for the Z2-symmetric real singlet extension of the Standard Model…Norimi Yokozaki·Sep 8, 2026SaveLearn
Inclusive electron-nucleus cross section models from domain adaptationWe apply transfer learning (TL) to construct data-driven models of inclusive electron-nucleus cross sections. Starting from an ensemble of deep neural networks pretrained on \(12\)C data, we…Krzysztof M. Graczyk, Beata E. Kowal, Rwik Dharmapal Banerjee et al.·Sep 8, 2026SaveLearn
Time evolution of scalar condensate decayA scalar field, which oscillates coherently over the space and decays through production of daughter particles, plays an important role in cosmology. It was recently shown that the…Ayuki Kamada, Kodai Sakurai·Sep 8, 2026SaveLearn
Light cone distributions of P-wave quarkoniaMotivated by renewed interest in the light-cone distributions of P-wave quarkonia, we investigate the leading-twist distribution amplitudes of these states within the basis light-front quantization…Yang Li, Tianyang Hu, Xianghui Cao et al.·Sep 8, 2026SaveLearn
Top-quark flavor-changing neutral currents and charged-lepton flavor violation in a generational three-Higgs-doublet modelIn this work, we systematically investigate top-quark flavor-changing neutral-current decays, charged-lepton flavor-violating processes, and coherent μ-e conversion in the CP-conserving…Hao-Ran Ma, Ti-Bin Hou, Yu-Ju Peng et al.·Sep 8, 2026SaveLearn
Probing the B0 meson in a hot medium with finite baryon chemical potentialWe perform a quantitative analysis of the B0 meson spectroscopic parameters in a hot and dense medium. Within the framework of QCD two-point sum rules, we calculate the mass and decay constant…A. Türkan, G. Bozkır, K. Azizi·Sep 8, 2026SaveLearn
Near-Threshold Dynamics of hic1(3872) and T+cc(3875) States via Effective Range Expansion and Monte Carlo Uncertainty PropagationWe investigate the near-threshold structure of the exotic tetraquark candidates χc1(3872) and Tcc+(3875) using the effective-range expansion (ERE) and resonance compositeness relations.…A. A. Atangana Likéné, A. Franck Rothen, J. M. Ema'a Ema'a et al.·Sep 8, 2026SaveLearn
Nuclear interference versus dark sector excitation in the 248 keV LUX-ZEPLIN recoil candidateThe 2026 LUX-ZEPLIN (LZ) high energy nuclear recoil search reports one event at 24823 stat23 sys~keV and finds the elastic isovector interaction L6v locally…Imtiaz Khan, Salvatore Capozziello, G. Mustafa et al.·Sep 7, 2026SaveLearn
Revisiting two-body charmed anti-charmed baryonic B decaysThe study of two-body charmed anti-charmed baryonic B Bc Bc decays using the topological amplitude approach is revisited. We include the b u u q…Chun-Khiang Chua·Sep 7, 2026SaveLearn
Recent applications of the gradient flowThe gradient flow provides a gauge- and O(4)-invariant ultraviolet regulator for QCD. This opens new opportunities for combining non-perturbative lattice calculations with perturbative results, in…R. Harlander, A. Shindler·Sep 7, 2026SaveLearn