Endpoint Logarithms in the NLO Mueller-Navelet Jet Vertex: Threshold Matching and BLM/MOM Prescription SensitivityThe endpoint region ζ1 of the NLO forward jet vertex has not been systematically separated from BFKL energy-scale terms in Mueller-Navelet phenomenology. Starting from the small-cone NLO vertex,…Lei Wang·Jul 6, 2026SaveLearn
Maximum phase-space density of linearly polarized gluon TMDs in the saturation regionWe calculate the Sudakov-limited maximum phase-space density associated with the linearly polarized gluon TMD coefficient h1 g in the saturation region. Using Mueller's occupancy…Lei Wang·Jul 6, 2026SaveLearn
Toward Charge-Dependent Tests of the Equivalence Principle: A Phenomenological Parameter and an Unexplored FrontierWe introduce and define the phenomenological parameter κ, defined by Δa/g = κ\, Δ(q/m), to quantify potential linear coupling between electric charge and gravitational acceleration. A synthesis…Renato Vieira dos Santos·Jul 6, 2026SaveLearn
Multimodal Fragmentation of All-Heavy Pentaquarks: Uncertainty-Aware Predictions for Hadron CollidersWe present an uncertainty-aware description of leading-power fragmentation for all-charm pentaquark states (S-wave |ccccc) at hadron colliders. We construct a multimodal set of…Francesco Giovanni Celiberto·Jul 6, 2026SaveLearn
Quantum Fisher Information as a Probe of Sterile Neutrino New Physics:Geometric Advantage of KM3NeT over IceCubeWe investigate a reported discrepancy between a high-energy neutrino detection at KM3NeT and its non-observation at IceCube, which suggests a statistical tension of up to 3.5 standard deviations.…Baktiar Wasir Farooq, Bipin Singh Koranga, Aritro Chatterjee·Jul 6, 2026SaveLearn
Boltzmann Equation Solver for ThermalizationWe present BEST (Boltzmann Equation Solver for Thermalization), a Python framework for solving the momentum-resolved Boltzmann equation for arbitrary n in n out scattering…Jong-Hyun Yoon·Jul 6, 2026SaveLearn
One-loop matching of the LEFT to the QCD gradient flowWe present the complete one-loop matching of the baryon- and lepton-number-conserving low-energy effective field theory (LEFT) to the QCD gradient flow. Using Euclidean conventions and the…Òscar L. Crosas, Peter Stoffer·Jul 6, 2026SaveLearn
Energy Correlators of Spinning SourcesThe N-point energy correlator measures the energy flux through N detectors. We present a general framework that characterizes its full angular dependence in a series of spinning energy…Marc Riembau, Minho Son·Jul 6, 2026SaveLearn
Timelike showers with jet recoilsWe propose a new way to impose four-momentum conservation on timelike parton-shower branchings, allowing for recoil to be imparted not only to individual partons but also to groups of partons,…Jack Helliwell, Ludovic Scyboz, Peter Skands·Jul 6, 2026SaveLearn
Symmetry Constraints on Pion Valence StructureThe profile of the pion valence quark distribution function (DF) remains controversial. Working from the concepts of QCD effective charges and generalised parton distributions, we show that since the…Xiaobin Wang, Lei Chang, Minghui Ding et al.·Jul 6, 2026SaveLearn
Dynamically generated tilt of isocurvature fluctuationsLight scalar fields acquire isocurvature fluctuations during inflation. While these fluctuations could lead to interesting observable signatures at small scales, they are strongly constrained on…Saarik Kalia·Jul 6, 2026SaveLearn
Semileptonic Ωb*→Ωc* ν transition in QCDWe employ the QCD sum rule method to study the semileptonic weak decay of the single bottom baryon Ωb* with spin 32 into the single charmed baryon Ωc* with spin…A. Amiri, P. Eslami, K. Azizi et al.·Jul 6, 2026SaveLearn
Photonic Freeze-InWe present a new scenario of freeze-in, where the dark matter is produced exclusively via the annihilation of photons. We study fermionic and scalar dark matter models with a focus on cosmological…Peter Cox, Matthew J. Dolan, Frederick J. Hiskens·Jul 6, 2026SaveLearn
Shifted Hybrid Realization of Non-Minimal Higgs Inflation in Light of ACT DR6 and Planck DataWe investigate non-minimal Higgs inflation in a no-scale-inspired supergravity framework and confront its predictions with the latest CMB constraints from ACT DR6 and Planck. Working within a…Nadir Ijaz, Pirzada, Mansoor Ur Rehman·Jul 5, 2026SaveLearn
Implications of exclusive photon leptoproduction measurements for the proton charge-radius puzzleIn the present study, we extend our previous analysis of the proton electromagnetic form factors (FFs) extracted from exclusive photon leptoproduction (EP) measurements in kinematic regions where the…The MMGPDs Collaboration, Muhammad Goharipour, Anoushiravan Moradi et al.·Jul 5, 2026SaveLearn
Probing Neutrinophilic Long-Range Forces at DUNENeutrino oscillations provide compelling evidence for physics beyond the Standard Model, while the weakly interacting nature of neutrinos makes them powerful probes of new interactions and hidden…Sudip Jana, Pragyanprasu Swain·Jul 5, 2026SaveLearn
Charting doubly strange hidden-charm pentaquarks: An electromagnetic mapping of spin-12 and 32 statesWe calculate the magnetic dipole moments of doubly strange hidden-charm pentaquark states with spin-parity JP = 1/2- and 3/2- using QCD light-cone sum rules (LCSR), presenting the first…Ulaş Özdem·Jul 5, 2026SaveLearn
Quantum interference effects enhanced in π+p femtoscopic correlation functionsWe present a comprehensive analysis of the π+p femtoscopic correlation functions measured by the ALICE Collaboration in high-multiplicity pp collisions at s=13 TeV. Using the…Zhi-Wei Liu, Jun-Xu Lu, Duo-Lun Ge et al.·Jul 5, 2026SaveLearn
Anomalous triple gauge couplings in the light of dimension-8 operators in W+W-We compare the size of dimension-8 effects on W+W- production at the LHC arising from the q q and γγ initial states. In particular, we consider bosonic operators, which contribute to the…Daniel Gillies, Andrea Banfi, Adam Martin·Jul 5, 2026SaveLearn
Updated analysis of minimal supersymmetric SO(10) with a universal soft spectrumWe update the analysis of minimal supersymmetric 10 grand unification with a universal, constrained-MSSM-like soft-breaking spectrum. A pair of Yukawa matrices in the…Cheng-Wei Chiang, Takeshi Fukuyama·Jul 5, 2026SaveLearn
Double strange hybrid baryonWe investigate the spectroscopic properties of the double strange hybrid baryon with quark content ssqg within the framework of QCD sum rule. Using an interpolating current with explicit gluonic…B. Barsbay, K. Azizi, H. Sundu·Jul 5, 2026SaveLearn
Vector meson photoproduction on the nucleus and the extraction of the nuclear suppression factor using asymmetric beamsThe cross-section for photoproduction of a vector meson on a nucleus is usually determined in nucleus-nucleus collisions, which introduces a two-fold ambiguity as to which nucleus emitted the photon.…Ronan McNulty, Wolfgang Schafer·Jul 5, 2026SaveLearn
Anatomy of the Quasi-PDF with a Transverse-Momentum CutoffThe quasi-PDF is fundamentally different from the light-cone PDF, and large-momentum effective theory relates the two through perturbative matching. This has required considerable effort. One of the…Junegone Chay·Jul 5, 2026SaveLearn
Advancing axion detection: Photon regeneration in high-sensitivity Penning trap experimentsThe axion, a hypothetical particle proposed to solve the strong CP problem and considered a viable candidate for dark matter, has prompted extensive experimental efforts for its detection. This study…Yao Chen, Ju Guo, Libo Zhao et al.·Jul 5, 2026SaveLearn
A MeV-Scale Dark QCD Solution to the Axion Domain Wall ProblemPQ solution to the strong CP problem probably encounters the axion domain wall problem. In this article, we propose a simple and testable solution, assuming that the U(1) PQ possesses mixed…Jun Guo, Zhaofeng Kang, Jiang Zhu·Jul 5, 2026SaveLearn