The (2+1)-dimensional Gross-Neveu-Yukawa model at finite temperature, density, and magnetic field within the Functional Renormalization GroupWe investigate the phase diagram of the (2+1)-dimensional Gross-Neveu-Yukawa (GNY) model at finite temperature, density, and magnetic field beyond mean-field, using the Functional Renormalization…Justin L. P. Mauldin, Dirk H. Rischke·Aug 3, 2026SaveLearn
A quality-coupling relation in chiral U(1)B-L axion modelThe quality of the QCD axion can be protected by a gauge symmetry. This work considers a gauged chiral U(1)B-L. The vacuum expectation values of two complex scalars break U(1)B-L. One…Yu-Cheng Qiu·Aug 3, 2026SaveLearn
Thermal Leptogenesis in the BNT Model of Neutrino MassWe investigate neutrino mass and thermal leptogenesis in the Babu-Nandi-Tavartkiladze (BNT) model featuring a scalar quadruplet (Φ) and a pair of vector-like fermion triplets (Σ). In this…P. S. Bhupal Dev, Srubabati Goswami, Debashis Pachhar et al.·Aug 3, 2026SaveLearn
Measuring the trilinear Higgs self-coupling in Higgs boson pair production at multi-TeV muon collidersThe trilinear Higgs self-coupling determines the shape of the Higgs potential, and its measurement is a central goal of future colliders. We assess the sensitivity of multi-TeV muon colliders to the…Kingman Cheung, Jae Sik Lee, Soojin Lee et al.·Aug 3, 2026SaveLearn
Gluon condensate effects on heavy quarkonium spectral functions and thermal dissociationWe investigate how the gluon condensate modifies the thermal spectral functions and melting patterns of heavy vector mesons, specifically charmonium and bottomonium, using an improved soft-wall…Fei Wang, Zi-qiang Zhang·Aug 3, 2026SaveLearn
Odderon exchange in high-energy K0S regeneration at the LHCWe revisit the possibility of detecting the Odderon exchange through high-energy neutral-kaon regeneration, focusing on the in-matter K0L K0S conversion of (\!0.2-2)~TeV K0L mesons…P. Filip, M. Taševský, V. A. Khoze et al.·Aug 3, 2026SaveLearn
Jet-by-jet energy correlators as stochastic probes of the parton-to-hadron transitionEnergy-energy correlators are usually reported as ensemble averages and therefore do not specify how different angular regions fluctuate together from jet to jet. We retain the binned two-point…Jingyu Zhang·Aug 3, 2026SaveLearn
Magnetic field modifications to the pion-quark vertex in the Linear Sigma Model with quarksWe compute the modification to the quark-neutral pion vertex, induced by a constant and uniform magnetic field, using the Linear Sigma Model with quarks as a low energy effective theory of QCD. The…Alejandro Ayala, Flávia Fialho, Adrián Lara et al.·Aug 3, 2026SaveLearn
Improved Approximations for Collective Neutrino OscillationsA one- and two-body su(n) Hamiltonian governing the dynamics of many systems, including collective neutrino oscillations, is investigated. We start by analyzing the algebraic…Matthew Riccio, A. B. Balantekin·Aug 3, 2026SaveLearn
Investigation of fully heavy tetraquark within chiral quark modelIn the framework of the Chiral quark model (ChQM), we investigate the fully charmed and fully bottomed tetraquark with JPC=2++ including two structures: QQ-QQ and…Yuheng Wu, Xuejie Liu, Ye Yan et al.·Aug 3, 2026SaveLearn
Rephasing invariant CP phases and sum rules in TM1,2 mixingWe show that the CP phases ϕ1,2 appearing in the TM1,2 mixing are directly identified with rephasing invariants $ϕ1 = - [ Ue2 Ue3 Uμ1 Uτ1 / Ue 1 U …Masaki J. S. Yang·Aug 3, 2026SaveLearn
Approximate mass spectra of the heavy mesons under a Coulomb plus logarithmic spin-dependent potential functionIn this paper, we presented an approximate analytical treatment of the Coulomb plus logarithmic potential using perturbation theory to investigate the mass spectra of bottomonium and charmonium…E. Omugbe, E. P Inyang, K. Adegoke et al.·Aug 3, 2026SaveLearn
Two-loop leading-color QCD corrections for Higgs plus two-jet production in the heavy-top limitWe present the leading-color two-loop QCD corrections for Higgs-boson production in association with two jets through gluon fusion in the heavy-top effective theory. We provide analytic expressions…Giuseppe De Laurentis, Harald Ita, Viktor Kuschke et al.·Aug 3, 2026SaveLearn
Quantum effects on neutrino parameters from a flavored gauge bosonWe calculate the one-loop renormalization group equations of the neutrino mass matrix when the Standard Model particle content is extended with a massive gauge boson which has family-dependent…Alejandro Ibarra, Lukas Treuer·Aug 3, 2026SaveLearn
Improving parton shower predictions via precision moments of energy flow polynomialsWe study conceptual and practical aspects of using maximum-entropy reweighting to upgrade parton-shower event samples with higher-accuracy theoretical constraints. Our approach produces strictly…Benoît Assi, Kyle Lee, Jesse Thaler·Aug 3, 2026SaveLearn
From Higgs physics to lepton flavour violation: current bounds and future prospects for vector-like lepton modelsWe present a comprehensive phenomenological study of a class of six vector-like lepton models with seesaw-like mass contributions and strong modifications to Higgs and lepton phenomenology. We focus…Gregor Daberstiel, Kilian Möhling, Dominik Stöckinger et al.·Aug 3, 2026SaveLearn
Global Analyses of Generalized Parton Distributions with Diverse PDF InputsThis paper investigates the crucial role of parton distribution functions (PDFs) in high-energy physics, particularly their impact on the extraction of generalized parton distributions (GPDs) at zero…The MMGPDs Collaboration, Fatemeh Irani, Muhammad Goharipour et al.·Aug 3, 2026SaveLearn
Polarization-dependent mass modifications of ϕ meson with finite momentum in nuclear matterWe investigate the in-medium properties of the ϕ meson with finite momentum, going beyond the commonly studied case at rest. In a nuclear medium, Lorentz invariance is broken, leading to distinct…Ahmad Jafar Arifi, Philipp Gubler, Kazuo Tsushima·Aug 3, 2026SaveLearn
Quarkonium spectra with magnetically induced anisotropic confinementStrong magnetic fields modify the force that confines quarks inside hadrons and make it direction-dependent. Using quark-antiquark potentials obtained from lattice simulations as inputs to a quark…Ahmad Jafar Arifi, Kei Suzuki·Aug 3, 2026SaveLearn
On the Robustness of type-II Seesaw Collider SearchesElectroweak triplet Higgs sector extensions are well-motivated scenarios to address lepton flavour observations. These models can also be strongly constrained by combining precise, indirect…Christoph Englert, Manimala Mitra, Wrishik Naskar et al.·Aug 3, 2026SaveLearn
No room for minimal monopole dark matterThe magnetic monopole of a dark sector has been advocated as an appealing dark matter candidate. We revisit the computation of the monopole abundance ΩM, generated by a thermal phase transition in…Felix Brümmer, Giacomo Ferrante, Théodore Fischer et al.·Aug 3, 2026SaveLearn
Exploring Leptogenesis in the Era of First Order Electroweak Phase TransitionWe present a novel approach for implementing baryogenesis via leptogenesis at low scale within neutrino seesaw framework where a sufficient lepton asymmetry can be generated via out of equilibrium…Dipendu Bhandari, Arunansu Sil·Aug 3, 2026SaveLearn
Dark Baryon Black HolesWe explore a novel mechanism for dark matter production through the formation of light black holes from the collapse of dark baryons in confining SU(N) gauge theories in the large N limit. While…Stefano Profumo·Aug 3, 2026SaveLearn
Search for active-sterile neutrino transitions using Pierre Auger Observatory dataWe investigate the sensitivity of the Pierre Auger Observatory to physics beyond the Standard Model arising from magnetic-moment-induced transitions between active and heavy sterile neutrinos. Such…The Pierre Auger Collaboration, A. Abdul Halim, P. Abreu et al.·Aug 2, 2026SaveLearn
What are the consequences of independent factorization and renormalization scales?It is common for separate factorization and renormalization scales to be discussed in connection with phenomenological applications of QCD factorization theorems. We observe that simultaneously…T. C. Rogers, R. M. Whitehill·Aug 2, 2026SaveLearn