Solar Capture Tests of Inelastic Dark Matter after the LZ High-Recoil EventThe LUX-ZEPLIN (LZ) Collaboration has reported a 248 keV nuclear-recoil candidate for which endothermic dark matter (DM) gives some of the largest local significances. We study Solar-capture…Mattia Di Mauro, Halim Shaikh·Sep 6, 2026SaveLearn
LZ Nuclear-Recoil Excess from Boosted Light Magnetic Dipole-dipole Dark MatterThe LZ collaboration has reported a nuclear-recoil excess near 248 keV with a global significance of 2.6σ. Although halo dark matter with a magnetic dipole-dipole interaction and a TeV-scale mass…Jin-Han Liang, Zuowei Liu, Van Que Tran et al.·Sep 6, 2026SaveLearn
GUT-induced FCC signatures of the LUX-ZEPLIN eventThe recent observation of an event with large recoil energy at LUX-ZEPLIN has found a possible explanation in terms of the inelastic scattering of a pseudo-Dirac particle like the Higgsino of the…Wojciech Kotlarski, Kamila Kowalska, Enrico Maria Sessolo·Sep 6, 2026SaveLearn
Inverse seesaw and inflation in a supersymmetric 331 model from SU(6)We propose a N=1 supersymmetric SU(6) theory with an intermediate (SU(3)C× SU(3)L× U(1)X) phase, in which common fields and operators relate the neutrinos, gauge mediation,…Imtiaz Khan, Tianjun Li·Sep 6, 2026SaveLearn
Multi-Messenger and Paleo-Detector Probes of the LZ Dark Matter SignalThe LUX-ZEPLIN collaboration recently reported a 2.6σ excess at a nuclear recoil energy of 248\ keV, challenging the standard elastic WIMP paradigm. We show that a leptophobic inelastic…Meiwen Yang, Quan-feng Wu, Yue-Lin Sming Tsai et al.·Sep 6, 2026SaveLearn
The Inert Doublet Model of Dark Matter and the LUX-ZEPLIN High-Recoil EventThe recent LUX-ZEPLIN (LZ) search reported a nuclear-recoil event near 248~ keV. Such a high-recoil event can be interpreted in terms of endothermic inelastic dark matter scattering, which…Lei Wang, Yang Xiao·Sep 6, 2026SaveLearn
Radiative double inverse seesaw and dark matter in an alternative gauged U(1)B-L modelWe propose a concrete theoretical framework for the double inverse seesaw mechanism within an alternative gauged U(1)B-L model, where the tiny neutrino masses emerge radiatively at the loop…Hiroshi Okada, Labh Singh·Sep 6, 2026SaveLearn
A Mean-Field Approach to the Dielectric Response of Bulk Superconductors for Light Dark Matter Direct DetectionThe dielectric function is central to describing many-body screening effects in dark matter (DM) direct detection with condensed matter targets. Current superconducting detector analyses employ the…Chengyao Gan, Hui Li, Wenjing Li et al.·Sep 6, 2026SaveLearn
Nodal filtering in open-charm decays of the ψ(4040)--ψ(4160) systemHadronic decay channels can provide direct information on the momentum-space structure of confined quark systems. We investigate this possibility in the ψ(4040)--ψ(4160) system using an…Bing-Dong Wan·Sep 6, 2026SaveLearn
On the analytic continuation and matching of threshold singularities from Vacuum AmplitudesWe provide a detailed discussion for all kinematical configurations of the analytic continuation to negative values of initial-state on-shell energies used to generate interferences of scattering…Selomit Ram\'ırez-Uribe, Prasanna K. Dhani, German F. R. Sborlini et al.·Sep 5, 2026SaveLearn
Planck-Scale Signatures in Vacuum Neutrino OscillationsWe present a closed-form perturbative framework for two-flavour vacuum neutrino oscillations in the presence of a weak, flavour-blind Planck-scale mass correction generated by the dimension-five…Bipin Singh Koranga, Imran Khan·Sep 5, 2026SaveLearn
Inelastic dark matter and baryon flavor symmetry in light of LUX-ZEPLIN (LZ) experimentWe present a novel model for inelastic dark matter in a simple extension of the Standard Model (SM) with a local U(1)' baryon flavor symmetry, such as U(1)Bi-Bj with i≠ j. In this…Hyun Min Lee·Sep 5, 2026SaveLearn
Exothermic dark matter and the 248 keV nuclear recoil in LUX-ZEPLINThe single 248-keV nuclear-recoil candidate reported by LZ is reproduced by dark matter that downscatters, with the relic in the excited state of a pseudo-Dirac pair and a splitting δ-350.…Howard Baer, Vernon Barger·Sep 5, 2026SaveLearn
Improved analyses of the electroweak phase transition and its phenomenology in the Georgi-Machacek modelThe Georgi-Machacek model is a promising new physics scenario with isospin-triplet scalar fields, whose effects can qualitatively change the nature of the electroweak phase transition compared with…Cheng-Wei Chiang, Kazuki Enomoto·Sep 5, 2026SaveLearn
Mass Generation for Axion Like ParticlesThe most widely accepted solution to the Strong CP problem is the QCD axion, whose traditional parameter space is relatively constrained. However, recent studies on exotic axion models have shown…Luca Merlo·Sep 5, 2026SaveLearn
Decipher the nature of glueball candidate X(2370)As a unique form of matter composed entirely of gauge bosons, glueballs are an important low-energy prediction of QCD. After decades of searches, the BESIII Collaboration recently suggested that…Sheng-Qi Zhang, Bing-Dong Wan, Cong-Feng Qiao·Sep 5, 2026SaveLearn
Deconfining Phase Transition under Real Rotation: A Matrix Model StudyWe construct a matrix model to study the deconfining phase transition for a pure gluon plasma that is confined in a cylinder of radius R and rotating rigidly at a real-valued angular…Qianqian Du, Jing He, Yun Guo et al.·Sep 5, 2026SaveLearn
The Masses of Bosons and Usual Fermions on Supersymmetric SU(3)C× SU(4)L× U(1)X ModelWe will study in details the masses spectrum of bosons and usual fermions of the Minimal Supersymmetric SU(3)C× SU(4)L× U(1)X Model.M. C. Rodriguez·Sep 4, 2026SaveLearn
Fermion mass hierarchy and flavor signals from a D4 dihedral symmetry within a 2HDM-Tx with four-zero texturesWe propose an extended Texturized Two-Higgs Doublet Model (2HDM-Tx) where a discrete D4 symmetry predicts a four-zero texture in the fermion mass matrices. In contrast to the standard ansatz where…M. A. Arroyo-Ureña, E. Díaz, J. L. Díaz-Cruz et al.·Sep 4, 2026SaveLearn
Agnostic search for a vector-like top partner at a lepton collider via the recoil mass techniqueA study of the single production of a vector-like top partner T at a s=3 TeV e+e- collider is presented, using a decay-mode and mass-agnostic event selection built around the…Higinio Valle, Cristina Oropeza Barrera, Oscar Ochoa-Valeriano·Sep 4, 2026SaveLearn
Macroscopic dark matter constraints for extended mass functionsWe compile and recompute a subset of the landscape of constraints for macroscopic dark matter (macros), explicitly including the dependence on the fraction of dark matter in macros f dm. This…Zachary S. C. Picker, Andrew Buchanan, Melissa Diamond et al.·Sep 4, 2026SaveLearn
High-sensitivity Ultralight Dark Matter detector: Parametrically Amplified Casimir DevicesWe propose the use of sphere-and-plate Casimir force measurement setups to detect ultralight vector dark matter. We demonstrate that sub-picometer signals can be parametrically amplified to be…Muping Chen, Hideo Iizuka, Kyohei Mukaida et al.·Sep 4, 2026SaveLearn
Energy-energy correlators and color decoherence from a generating functionalUsing jet calculus at leading-logarithmic accuracy, we develop a generating-functional approach to describe the hard-collinear sector of jets propagating through the quark-gluon plasma. This…Yacine Mehtar-Tani·Sep 4, 2026SaveLearn
The Colors of Jet QuenchingWe combine inclusive jet nuclear modification factors with energy-energy correlators to perform a data-driven extraction of the quark and gluon quenching factors and the medium resolution scale from…Hannah Bossi, Maxence Larose, Yacine Mehtar-Tani·Sep 4, 2026SaveLearn
Minimal spontaneous baryogenesis from flavorIn its minimal realization, the Froggatt-Nielsen (FN) mechanism addresses the Standard Model (SM) flavor puzzle via the spontaneous breaking of a horizontal U(1)H symmetry. If U(1)H is global…Martin A. Mojahed, Alfredo Stanzione·Sep 4, 2026SaveLearn