Hadrophilic inelastic freeze-in dark matter in q1-q2 gauge extension and the high energy LZ eventThe recent observation of a single event at nuclear recoil energy 2482323 keV by the LZ collaboration has prompted dark matter (DM) model builders to explore new physics explanations. While…Xiao-Gang He, Xuan Hong, Sk Jeesun·Sep 14, 2026SaveLearn
Hyperon polarization in deep inelastic scatteringWe have implemented the recent extension of the string+3P0 model of spin-dependent hadronization that includes the production of spin-1/2 baryons in the Pythia event generator for the…A. Kerbizi·Sep 14, 2026SaveLearn
Xenon Isotope Filtering at the Kinematic Edge of Inelastic Dark MatterMotivated by high-energy xenon recoil searches, we study isotope-dependent endothermic dark-matter scattering near the upper speed boundary of a truncated Galactic halo. Small differences among xenon…Waqas Ahmed, Ammara Ahmad, Mansoor Ur Rehman·Sep 14, 2026SaveLearn
Effect of inelastic scalar dark matter in hidden U(1) scenario after the LZ nuclear recoilWe study a hidden U(1)H extension of the Standard Model (SM) introducing two SM singlet complex scalar fields where one of them can be considered as a viable inelastic Dark Matter (DM) candidate…Arindam Das, Takaaki Nomura·Sep 14, 2026SaveLearn
Extraction of genuine twist-3 distribution from dataThe report on an extraction of genuine twist-three parton distributions, obtained from a joint fit of the deep-inelastic scattering (DIS) structure function g2, its moment d2, and the Sivers…Alexey Vladimirov·Sep 14, 2026SaveLearn
Generalized Parton Distributions: Phenomenology, Extraction, and Hadron ImagingGeneralized Parton Distributions (GPDs) provide a framework for investigating the correlated momentum and spatial structure of quarks and gluons in hadrons and for accessing fundamental properties…Simonetta Liuti, Zaki Panjsheeri, Kemal Tezgin·Sep 14, 2026SaveLearn
Towards the new NNPDF4.1 global analysisWe review progress and plans towards a new global PDF analysis from the NNPDF Collaboration. This new release will be based on state-of-the-art theory calculations, and in particular will be based on…Felix Hekhorn·Sep 14, 2026SaveLearn
Rotational effects on the chiral crossover transition in QCD matterWe analyze the impact of rotation on the chiral crossover transition of QCD matter within the framework of a hadron resonance gas model. By extending the conventional formulation of the renormalized…Nandita Padhan, Kshitish Kumar Pradhan, Arghya Chatterjee et al.·Sep 14, 2026SaveLearn
Complex-energy spectrum and dissociation of heavy quarkonia in an anisotropic collisional quark-gluon plasmaWe solve the Schrödinger equation for heavy quarkonia using the full complex potential of a momentum-anisotropic, collisional quark-gluon plasma. The real and imaginary parts of the complex…Najmul Haque·Sep 14, 2026SaveLearn
Next-to-leading power gluon TMDs from back-to-back DIS dijets at next-to-eikonal accuracy at low xWe calculate next-to-leading power contributions to the gluon TMDs in DIS dijet production in the back-to-back limit at low x within the Color Glass Condensate (CGC) effective field theory at…Tolga Altinoluk, Guillaume Beuf, Alina Czajka et al.·Sep 14, 2026SaveLearn
Probing gluon saturation through inclusive hadron production in DISWe investigate gluon saturation effects in semi-inclusive deep inelastic scattering (SIDIS) at small-x within the Color Glass Condensate framework. We compute the SIDIS cross section at leading…Carlisle Casuga, Swaleha Mulani, Heikki Mäntysaari·Sep 14, 2026SaveLearn
One-loop renormalization of the quark TMD in projectile light-cone gaugeWe use the background field formalism to calculate next-to-leading-order corrections to a quark transverse momentum dependent parton distribution function (TMD) in the projectile light-cone gauge,…Tolga Altinoluk, Guillaume Beuf, Jamal Jalilian-Marian et al.·Sep 14, 2026SaveLearn
Probing Neutrino-Energy Reconstruction with New Superscaling-Based ObservablesIn this study, we explore the superscaling variable ψ' within the context of neutrino-nucleus charged-current quasielastic interactions. Building on the neutrino-oriented definition of the…Lounès Amziane, Soniya Samani, Lorenzo Giannessi et al.·Sep 14, 2026SaveLearn
A DM candidate indicated at Fermi-LAT and LZ ? Connection with LHC and LC prospectsRecently an analysis of Fermi-LAT data has claimed a significant excess of energetic photons centred around 20 GeV, in the halo of our galaxy but absent in dwarf galaxies. This excess can be…Alain Le-Yaouanc, François Richard·Sep 14, 2026SaveLearn
Self-field of a moving stringWe discuss the effectiveness of the recently proposed quantity Js in suppressing the contribution of a string's self-field to its spectrum, which is used in field theory simulations to track…Richard A. Battye, Lukasz P. Bunio, Steven J. Cotterill·Sep 14, 2026SaveLearn
Vertexing displaced diphoton decays with recoil photons at Belle IIWe propose a recoil-assisted strategy for vertexing displaced diphoton decays in e+e-γX, Xγγ, using only one converted daughter photon. The initial state and recoil-photon momentum define…Zeren Simon Wang, Yu Zhang·Sep 14, 2026SaveLearn
Confronting the Higgsino Interpretation of the LZ Event with Astrophysical Uncertainties and the Solar Capture ConstraintsWe investigate whether astrophysical uncertainties in the local dark matter distribution can alleviate tensions between the higgsino interpretation of the LZ event and constraints from solar-capture…Aditya Ghosh, Ilumi Chavez, Chris Kelso·Sep 14, 2026SaveLearn
Follow-up comments to searches for QCD instantons via forward proton taggingIn this short text, only the main facts are reminded from the full-fledged study~Tasevsky:2022sch and a few experimental considerations are added, reflecting developments since the publication…Marek Tasevsky, Valery A. Khoze, Misha G. Ryskin·Sep 14, 2026SaveLearn
The γZ-box correction and its impact on parity-violating deep-inelastic scatteringThe γZ-box correction is an important electroweak contribution to precision parity-violation measurements, but its conventional low-energy treatment relies on an ambiguous effective quark-mass…Balma Duch, Pere Masjuan, Hubert Spiesberger·Sep 14, 2026SaveLearn
Determination of charged pion unpolarised TMDPDFs from Drell-Yan measurementsWe present an extraction of the unpolarised transverse momentum dependent (TMD) parton distribution functions (PDFs) for the valence quarks in the pion from experimental mea- surements of the…Wen-Chen Chang, Chia-Yu Hsieh, Chung-Wen Kao et al.·Sep 14, 2026SaveLearn
Precision Sum Rule for Nucleon Isovector Polarizabilities and the Proton-Neutron Mass DifferenceThe precision of the electromagnetic proton-neutron mass difference δmQED extracted from the Cottingham formula hinges on a subtraction function whose low-energy normalization S(0)…Xiong-Hui Cao, Ling-Yun Dai, Feng-Kun Guo·Sep 14, 2026SaveLearn
Heavy-quark expansion at leading power for local QCD operators in gradient flowGradient flow provides finite-flow-time QCD operators, whose matrix elements can be computed on the lattice and related to renormalized QCD operators through perturbative matching. We develop a…Yun-Han Gui, Xin-Qiang Li, Xiang-Peng Wang et al.·Sep 14, 2026SaveLearn
Did LZ see modified gravity?We investigate whether the recently reported high-energy nuclear recoil event by the LUX-ZEPLIN (LZ) collaboration can be interpreted as a signal of freeze-in dark matter (DM) in a non-standard…Basabendu Barman·Sep 14, 2026SaveLearn
Open-channel radiation zeros and nonlinear damping of a critical-bubble internal modeWe study radiation and nonlinear damping of a spherically symmetric localized mode of an O(3) thermal critical bubble. The leading second-harmonic radiation amplitude is determined by the overlap…Tomohiro Inagaki, Yuko Murakami·Sep 14, 2026SaveLearn
Inelastic Dark Matter at LZ from Radiative Dirac Neutrino Mass ParadigmThe LUX-ZEPLIN (LZ) experiment has reported a high-energy nuclear recoil candidate, LZ230616, at ER = 248 23 stat 23 sys\,keV, which is difficult to reconcile with elastic…Pankaj Borah, Satyabrata Mahapatra, Newton Nath et al.·Sep 14, 2026SaveLearn