Magnetization and Magnetic Field-Induced Correction: Implications for QGP Thermal Photon Production in MagnetohydrodynamicWe investigate thermal photon emission from magnetized quark-gluon plasma (QGP) within (1+1)-dimensional relativistic magnetohydrodynamics (MHD), systematically incorporating magnetic susceptibility…Jing Jing, Duan She, Ze-Fang Jiang·Aug 13, 2026SaveLearn
Decay widths of radially excited vector mesons of the U(3) nonet with production of three pseudoscalar mesons in the extended NJL modelIn the extended NJL model, the decays of the first radially excited vector mesons ρ',ω', ϕ' and K*' with production of 3P, where P=K,π,η are calculated. The box…M. K. Volkov, A. A. Pivovarov, K. Nurlan·Aug 13, 2026SaveLearn
Newtrinos.jl: A Julia Package for Global Analysis of Neutrino DataNewtrinos.jl is an open-source Julia package for performing global analyses of neutrino data. It provides a modular, three-layer architecture that separates physics models, experiment descriptions,…Philipp Eller, David Schultheiß·Aug 13, 2026SaveLearn
Entropy from inclusive scatteringIntroduction of probabilities from multiple inclusive cross-sections is studied in the unitary pomeron exchange models with no interaction between the pomerons themselves. Discrepancy is observed…M. A. Braun·Aug 13, 2026SaveLearn
In-medium properties of D and D* mesons in magnetized isospin asymmetric nuclear matterWe investigate the impact of an external magnetic field on the in-medium properties of pseudoscalar (D0,D+,Ds) and vector (D0*,D+*,Ds*) mesons in isospin asymmetric nuclear matter…Saksham Sharma, Dhananjay Singh, Suneel Dutt et al.·Aug 13, 2026SaveLearn
Topological diagrams of Ω0c decays in the SU(3)F limitThe Ω0c baryon is unique among charmed sextet baryons because it decays through the weak interaction. In this work, we investigate the topological amplitudes of Ωc0 decays in the SU(3)F…Ying-Xin Lai, Di Wang·Aug 13, 2026SaveLearn
Scalar induced gravitational waves as probes of dark QCDWe investigate scalar induced gravitational waves (SIGWs) as probes of a dark QCD crossover. Motivated by twin Higgs and asymmetric twin baryon dark matter scenarios, we consider a dark QCD sector…Wan-Zhe Feng, Ao Li, Jing-Zhi Zhou·Aug 13, 2026SaveLearn
Massive cold hybrid stars in a modified Polyakov-Nambu-Jona-Lasinio modelWe propose a modified Polyakov-loop Nambu--Jona-Lasinio (mPNJL) model in which the Polyakov potential is given by an explicit dependence on the quark chemical potential, allowing it to remain finite…Sk Md Adil Imam, Pedro Costa, Mariana Dutra et al.·Aug 12, 2026SaveLearn
A Novel One-loop Model for Majorana Neutrino Mass and Dark MatterWe present the first complete field-theoretic realization of the finite one-loop T4-3-i topology for Majorana neutrino mass. Here, T4-3-i denotes a one-loop realization of the Weinberg operator in…Mohamed Belfkir, Mohamed Amin Loualidi, Salah Nasri·Aug 12, 2026SaveLearn
N3LO soft-gluon corrections for Zγ productionWe calculate soft-gluon corrections for Zγ production through next-to-next-to-next-to-leading-order (N3LO) in one-particle-inclusive (1PI) kinematics. We use these results to produce approximate…Nikolaos Kidonakis, Kaan Şimşek·Aug 12, 2026SaveLearn
Spontaneous Scoto-leptogenesisWe propose a low-scale spontaneous leptogenesis scenario within the dynamical minimal scotogenic model for accommodating neutrino masses and inert scalar dark matter simultaneously. Thus, we dub the…Arghyajit Datta, Hyun Min Lee, Jun-Ho Song·Aug 12, 2026SaveLearn
Singlet-Doublet fermion origin of dark matter, neutrino mass and inverse first-order electroweak phase transitionWe study the possibility of an inverse first-order electroweak phase transition (IFOEWPT) and observable gravitational waves (GW) in a radiative neutrino mass model of scotogenic type where…Debasish Borah, Indrajit Saha, Sujit Kumar Sahoo et al.·Aug 12, 2026SaveLearn
Singlet-doublet dark matter beyond freeze-outThe Singlet-Doublet fermion model of dark matter is an economical weak-scale dark matter model that realizes the dark matter abundance through interactions with the electroweak bosons of the Standard…Prudhvi N. Bhattiprolu, Aaron Pierce, Alexander Takla·Aug 12, 2026SaveLearn
Defect-Mediated Conversion: Dark Matter from Cosmological Domain-Wall ScatteringWe propose a new mechanism for dark matter genesis, Defect-Mediated Conversion (DMC). Cosmological domain walls can host a scalar condensate in their core acting as a mixing portal between the…João Paulo Pinheiro, Mohamed Younes Sassi·Aug 12, 2026SaveLearn
Soft Collinear Effective Theory for Heavy QCD AxionsWe develop a soft-collinear effective theory (SCET) framework for heavy QCD axion, considering two low-energy realizations and taking B Ka as a benchmark mode. In the first realization,…Deepanshu Bisht, Sabyasachi Chakraborty, Siddhartha Karmakar et al.·Aug 12, 2026SaveLearn
Probing CP-violating top-quark dipole moments with tomographic observablesQuantum tomography program reconstructs the full spin density matrix of top-quark pairs from dilepton angular correlations at both electron-positron and hadron colliders. We use symmetry arguments to…Maxim Perelstein, Minal Shaik, Taewook Youn·Aug 12, 2026SaveLearn
Dark matter in scale-invariant gravity with hidden-sector condensationThe origin of the electroweak scale, cosmic inflation, and dark matter are often treated as independent problems beyond the Standard Models of particle physics and cosmology. In this work, we explore…Juan P. Garcés, Jisuke Kubo, Manfred Lindner et al.·Aug 12, 2026SaveLearn
The D*D*π and B*B*π couplings from light-cone sum rulesWe revisit the calculation of the strong couplings D*D*π and B*B*π from the light-cone sum rules (LCSR) using the pion light-cone distribution amplitudes. The accuracy of the…Chao Wang·Aug 12, 2026SaveLearn
Photon emission from rotating plasmas: a generalized McLerran-Toimela formula and the onset of superradianceThe photon emission and absorption spectra of a plasma rotating with constant angular velocity Ω are derived in terms of the spectral function of the current--current correlator. In contrast to the…Kirill Tuchin·Aug 12, 2026SaveLearn
Dark sector radiation corrections to invisible dark photon production: beyond fixed orderIn this work we study invisible dark photon production at electron-positron colliders in a dark Abelian Higgs model at NLO (next-to-leading-order), and the physical distribution of squared missing…Xiangyu Deng, Yi Li, Mengchao Zhang·Aug 12, 2026SaveLearn
Higgs Mass and CP violating Phases Implications on the SUSY Breaking Scale in MSSMThe large Higgs mass mh ≈ 125 GeV can raise the values of the SUSY breaking parameters in the Minimal Supersymmetric Standard Model MSSM to the range of several TeV scale. The CP violating…Tarek Ibrahim, Anas Zorik·Aug 12, 2026SaveLearn
The decay properties of two- and three- gluon glueballsWe previously studied the decay properties of two- and three-gluon glueballs using the Fierz rearrangement method and obtained their relative branching ratios in Ref.~Tan:2026uue. In this…Wei-Han Tan, Hua-Xing Chen, Ding-Kun Lian et al.·Aug 12, 2026SaveLearn
Physics of the Electron-Ion Collider in ChinaThe Electron-Ion Collider in China (EicC), a cutting-edge facility under development, aims to unveil the internal structure of nucleons and nuclei by leveraging collisions of high-intensity polarized…Bo-Wen Xiao, Yuxiang Zhao, Jian Zhou·Aug 12, 2026SaveLearn
How to Identify a Majoron: Effective Field Theories of Spontaneous Lepton Number BreakingWe revisit the traditional Type I, II and III Seesaw mechanisms in the presence of a complex scalar field charged under a global U(1) symmetry that can be identified with lepton number and the…Carla Biggio, Marta Fuentes Zamoro, Xu Li et al.·Aug 12, 2026SaveLearn
Particle Production, Equilibration, and Quantum Recurrences from Classical FieldsWe investigate particle production from classical fields, a phenomenon central to the pre-equilibrium dynamics of relativistic heavy-ion collisions and the reheating epoch of the early Universe.…Iván Cuntín, Wenyang Qian, Bin Wu·Aug 11, 2026SaveLearn