PineAPPLv1: fast and flexible theory predictions for present and future collidersWe present PineAPPLv1, a library designed to provide accurate and flexible interpolation tables of partonic cross sections that can be convolved with parton distribution functions (PDFs) and…Tomáš Ježo, Emanuele R. Nocera, Tanjona R. Rabemananjara et al.·Jun 15, 2026SaveLearn
Short-Range Correlations Between Partons in a ProtonA principal lesson from recreating droplets of quark-gluon plasma (QGP) in heavy ion collisions is that it is a strongly coupled liquid, not a plasma of partons. The energy density and pressure of…Jen-Chieh Peng, Krishna Rajagopal, John Terry·Jun 15, 2026SaveLearn
Are neutrinos Majorana? Fixed-target and high-energy astrophysical searches decideDetermining whether the neutrino is a Dirac or Majorana fermion remains a fundamental open question. Conventional searches rely on neutrinoless double beta decay, but this electron-only channel…Gabriela Barenboim, Mauricio Bustamante, Qinrui Liu·Jun 15, 2026SaveLearn
First Experimental Limit on the Thermal Solar Neutrino FluxThe neutrino sky below 165\,keV is yet to be explored. This region provides a unique probe of stellar cooling mechanisms through the detection of thermal solar neutrinos and the low-energy tail of…Cecilia Ferrari, Gonzalo Herrera, Brooke Russell·Jun 15, 2026SaveLearn
A scaling non-compact QCD axionWe present a dynamical mechanism for the erasure of inflationary isocurvature perturbations of the non-compact QCD axion. The key ingredient is an early-time runaway exponential potential, which…Georgios K. Karananas, Mikhail Shaposhnikov·Jun 15, 2026SaveLearn
Scalar D(*)K(*) and D(*)π(ρ) molecular states from B meson decaysIn this paper, we investigate the production of scalar singly charmed four-quark states from B meson decays, employing phenomenological SU(3) flavor symmetry analysis and final-state interaction…Jing-Rui Shi, Jiang-Tao Zhang, Ye Xing·Jun 15, 2026SaveLearn
Hadronic tensor in lattice gauge theories by quantum computingThe hadronic tensor encodes crucial information regarding the internal structure of hadrons, reflecting the non-perturbative features of quantum chromodynamics (QCD). In this work, we directly…Dairui Zou, Tianyin Li, Jian Liang et al.·Jun 15, 2026SaveLearn
Threshold cusp effects to measure masses of radiatively decaying hadrons: The Bs0* mass from the Υϕ spectrumHadrons that decay predominantly into final states containing photons are notoriously difficult to detect at hadron colliders. Prominent examples are the yet-unobserved Bs0* and Bs1, the…Hai-Long Fu, Xu Zhang, Feng-Kun Guo et al.·Jun 15, 2026SaveLearn
QCD-like theories at next-to-next-to-leading order with NF=2 non-degenerate fermionsQCD-like theories with NF=2 fermion flavours in real and pseudoreal representations are studied within Chiral Perturbation Theory. For the pseudoreal symmetry-breaking pattern SU(4)/Sp(4), the…Johan Bijnens, Daniil Krichevskiy·Jun 15, 2026SaveLearn
Modern Determination of Pion and Kaon Fragmentation Functions from SIA and High-Precision COMPASS SIDIS MultiplicitiesWe present a combined determination of charged-pion and charged-kaon fragmentation functions (FFs), denoted HAPS-PiFF1.0 and HAPS-KaFF1.0, at next-to-leading order (NLO) and within a…HAPS Collaboration, Maryam Soleymaninia, Hamzeh Khanpour et al.·Jun 15, 2026SaveLearn
Revealing the nature of double-strangeness pentaquark states via femtoscopic correlation functionsRecent discoveries of exotic hadrons, which cannot be classified within the conventional quark model of q q mesons and qqq baryons, strongly imply the existence of dynamically generated…Zheng-Ting Lai, Jun-Xu Lu, Zhi-Wei Liu et al.·Jun 15, 2026SaveLearn
Diffractive structure functions from JIMWLK evolutionWe compute diffractive structure functions from Wilson line configurations whose energy evolution is given by the JIMWLK equation. We use a JIMWLK evolution setup that has already been constrained…Tuomas Lappi, Heikki Mäntysaari, Pyry Runko·Jun 15, 2026SaveLearn
A Minimal Dark U(1)D Framework for Inverse Seesaw Neutrino Masses and Dark MatterWe propose a minimal framework based on a dark U(1)D gauge symmetry that simultaneously accounts for neutrino masses and dark matter within an inverse seesaw realization. In this setup, the…D. T. Huong, N. T. Duy, Phung Van Dong·Jun 15, 2026SaveLearn
High-quality Axion Strings from Monopole StringsFive-dimensional 't Hooft-Polyakov monopole strings whose cores restore a non-abelian gauge symmetry become axion strings for extra-dimensional axions. The parametric separation between the…Nathaniel Craig, Amalia Madden·Jun 15, 2026SaveLearn
Sommerfeld Enhancement in Spin-1 Electroweak Dark MatterWe study a renormalizable spin-1 electroweakly interacting dark matter (DM) model in which the DM particle is the neutral component of a Z2-odd SU(2)L triplet vector boson. The model…Tomohiro Abe, Motoko Fujiwara, Junji Hisano·Jun 15, 2026SaveLearn
Chiral-odd structure of the N Δ transition: tensor form factors from QCD light-cone sum rulesWe report the first calculation of the tensor transition form factors of the N Δ transition within QCD light-cone sum rules, and use them to construct the transverse multipole structure of this…Ulaş Özdem·Jun 15, 2026SaveLearn
Static linear response of hot and dense QCD matter to electromagnetic fields: Leading hard and soft QCD correctionsWe compute the static electromagnetic susceptibilities of a hot and dense quark-gluon plasma using perturbative Quantum Chromodynamics (QCD). Our evaluation includes the leading O(αs)…Osvaldo Ferreira, Eduardo S. Fraga, Tyler Gorda et al.·Jun 15, 2026SaveLearn
Determining the Spin Density Matrix via Its Rank and Probing the Quantum Entanglement and Bell Non-Locality at the Lepton CollidersConsidering two-fermion Fa Fb productions and decays via one scalar or photon exchange at the e+e- collider, we show that the rank rρ of spin density matrix ρ is equal to the number of…Liwei Liu, Xiqing Hao, Dianwei Wang et al.·Jun 15, 2026SaveLearn
Search for Invisibly Decaying Light Scalars at the FCC-eeWe investigate the production of invisibly decaying light scalars in association with hadronically decaying Z bosons at the Future Circular Collider-ee at a centre-of-mass energy s=240…Aman Desai, Tania Robens·Jun 15, 2026SaveLearn
Modular S4 Scotogenic Model with Flavored Resonant LeptogenesisWe construct a radiative neutrino mass model that combines the scotogenic mechanism with modular S4 flavour symmetry. The entire lepton flavour structure is governed by holomorphic modular forms…Abhishek, V. Suryanarayana Mummidi·Jun 15, 2026SaveLearn
Dark Matter Attenuation inside the Earth: A Boltzmann Equation ApproachFor strongly interacting or boosted dark matter, propagation through the Earth can involve sizable scattering and energy loss, reshaping the underground flux in energy, direction, and normalization.…Chuan-Yang Xing, Chen Xia·Jun 15, 2026SaveLearn
LIGO, LISA and Ultralight Axion-like Dark MatterA coherent cosmic background of axion-like particles (ALPs) coupled to photons can produce a small periodic differential phase or polarization modulation for photons traversing separate arms in…Lawrence M. Krauss·Jun 15, 2026SaveLearn
Resolving the CP Asymmetry Puzzle in B Decays with Unitarized Final-State InteractionsA reliable description of direct CP asymmetries in hadronic B decays, among the most sensitive probes of the CKM mechanism and of physics beyond the Standard Model, remains unresolved. Conventional…Xin-Yue Hu, Pengyu Niu, Qian Wang et al.·Jun 15, 2026SaveLearn
Heavy fermionic dark matter in a secluded Z4 frameworkWe investigate heavy Majorana dark matter χ in a secluded scalar sector with a spontaneously broken Z4 symmetry. The symmetry forbids a bare Majorana mass, providing a dynamical origin for the…XinXin Qi, Hao Sun·Jun 15, 2026SaveLearn
Does the Weinberg angle allow a local hidden-variable description for the leptonic decays of an entangled ZZ pair?Quantum entanglement in di-boson systems offers a useful testing ground for exploring the boundary between quantum-mechanical correlations and classical descriptions based on local hidden variables.…Junle Pei·Jun 15, 2026SaveLearn