Search for black holes and sphalerons using novel machine learning techniques at CMSA comprehensive search for microscopic black holes and electroweak sphalerons is presented, using proton-proton collision data collected by the CMS detector during 2016-2018, corresponding to an…Tamas Almos Vami, Danyi Zhang·Nov 5, 2025SaveLearn
Studies of hadron spectroscopy at Belle and Belle IIThe Belle and Belle II experiments have collected a 1.6\,ab-1 sample of e+e- collision data at center-of-mass energies near the (nS) resonances. We conduct searches for…S. Wallner·Nov 4, 2025SaveLearn
GPU-based track-finding for the J-PARC muon g-2/EDM experimentThe muon g-2/EDM experiment at J-PARC is designed to precisely measure the muon's magnetic moment and electric dipole moment, driven by discrepancies between theory and previous experiments.…Hridey Chetri, Deepak Samuel, Saurabh Sandilya et al.·Nov 4, 2025SaveLearn
First Displaced Vertex Search for Electroproduced Dark-Sector Strongly Interacting Massive Particles by the HPS ExperimentThe Heavy Photon Search experiment (HPS) is a fixed-target, electron beam experiment designed to search for e+e- mass resonances and displaced decays using a forward acceptance spectrometer. This…The HPS Collaboration·Nov 4, 2025SaveLearn
Search for KS(L)0 → π+π-μ+μ- decays at LHCbA search for KS(L)0 → π+π-μ+μ- decays is performed using proton-proton collision data collected by the LHCb experiment at a centre-of-mass energy of…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Nov 4, 2025SaveLearn
Machine learning in LHCb Simulation: From fast to flashMonte Carlo simulations are essential for physics analyses in high-energy physics, but their computational demands are continuously increasing. In LHCb, 90 % of computing resources are used for…Michał Mazurek·Nov 3, 2025SaveLearn
Inclusive and differential measurements of the ttγ cross section and the ttγ / tt cross section ratio in proton-proton collisions at s = 13 TeVInclusive and differential cross section measurements of top quark pair (tt) production in association with a photon (γ) are performed as a function of lepton, photon, top…CMS Collaboration·Nov 3, 2025SaveLearn
First results of the NEXT-100 detector using 83mKr decaysThe NEXT collaboration is investigating the double beta decay of 136Xe using high-pressure gas electroluminescent time projection chambers, which provide excellent energy resolution together…NEXT Collaboration, G. Martínez-Lema, C. Hervés Carrete et al.·Nov 3, 2025SaveLearn
Beam-Beam Backgrounds for the Cool Copper ColliderIn this paper, we present a comprehensive characterization of beam-beam backgrounds for the Cool Copper Collider (C3), a proposed linear e+e- collider designed for precision Higgs studies…Dimitrios Ntounis, Laith Gordon, Lindsey Gray et al.·Nov 2, 2025SaveLearn
Prospects for Measuring the Higgs Boson Decay to WW* in Fully Hadronic Final States at the ILC Using Multivariate TechniquesIn this paper, the statistical potential of the measurement of Higgs to WW* decay at the International Linear Collider (ILC) is presented. The Higgs boson with a mass of 125 GeV is produced…M. Pandurović·Nov 2, 2025SaveLearn
Search for Baryon/Lepton number violation processes at BESIIIThe observed matter-antimatter asymmetry in the universe is a serious challenge to our understanding of nature. Baryon/lepton number violation (BNV/LNV) decays have been searched for in many…Xudong Yu·Nov 1, 2025SaveLearn
Single-Point Search for eV-scale Axion-like particles with Variable-Angle Three-Beam Stimulated Resonant Photon ColliderWe report a laboratory search for axion-like particles (ALPs) in the eV-mass range using a variable-angle three-beam stimulated resonant photon collider. The scheme independently focuses and collides…Takumi Hasada, Kensuke Homma, Airi Kodama et al.·Nov 1, 2025SaveLearn
The ANUBIS detector and its sensitivity to neutral long-lived particlesLong-lived particles (LLPs), i.e., particles with macroscopic lifetimes τ>10~ns, appear in various extensions of the Standard Model (SM) that address fundamental questions like the particulate…ANUBIS Collaboration·Oct 30, 2025SaveLearn
Baryon-antibaryon photoproduction cross sections off the protonThe GlueX experiment at Jefferson Lab has observed pp and, for the first time, and p photoproduction from a proton target at photon energies up to 11.6…GlueX Collaboration, F. Afzal, M. Albrecht et al.·Oct 30, 2025SaveLearn
Differential cross-section measurements of coherent production of singly and doubly resonant top-quark in WWbb events with one lepton at s = 13 TeV with the ATLAS detectorThis paper presents differential cross-section measurements of events containing a charged lepton, missing transverse momentum, two b-jets, and two light jets, consistent with the…ATLAS Collaboration·Oct 30, 2025SaveLearn
Observation of the decay ηcγγ at BESIIIIn the decays of ηcγγ and J/γηc, there are discrepancies between the theoretical calculations and the PDG experimental values, referred to as the charmonium QCD…Zhijun Li, Zhengyun You·Oct 30, 2025SaveLearn
Search for dark sector at BESIIIBESIII experiment has collected a large data sample of charmonium, charm mesons, hyperons, and other light mesons. These data provide a unique opportunity to explore the dark sector beyond the…Zhijun Li, Zhengyun You·Oct 30, 2025SaveLearn
Analytically Optimising Muon Diffusion Experiments with Fisher informationOne of the key challenges in performing muon experiments is knowing which temperatures and applied fields to measure at, and how many muon decays should be measured at each temperature/field…Alex Sampson, Peter J. Baker, Lucas Wilkins et al.·Oct 30, 2025SaveLearn
Searching for the X17 with the PADME experimentThe PADME experiment was originally designed to test dark matter theories predicting the existence of a ''Dark Sector'' composed of particles that interact with Standard Model ones exclusively…V. Kozhuharov·Oct 30, 2025SaveLearn
Search for nucleon decay via p→π+ and n→π0 in 0.484 Mton-year of Super-Kamiokande dataWe present the results of searches for nucleon decays via p→π+ and n→π0 using a 0.484 Mt·yr exposure of Super-Kamiokande I-V data covering the entire…Kamiokande Collaboration, S. Jung, K. Abe et al.·Oct 30, 2025SaveLearn
Reconstruction of neutrino events in the Accelerator Neutrino Neutron Interaction Experiment: Part IThe Accelerator Neutrino Neutron Interaction Experiment (ANNIE) was designed to reconstruct neutrino events from the Fermilab Booster Neutrino Beam (BNB) with the parallel goals of measuring neutron…S. Abubakar, M. Acsencio-Sosa, D. Ajana et al.·Oct 30, 2025SaveLearn
Letter of Intent: The Forward Physics FacilityThe Forward Physics Facility (FPF) is a proposed extension of the HL-LHC program designed to exploit the unique scientific opportunities offered by the intense flux of high energy neutrinos, and…Luis A. Anchordoqui, John K. Anders, Akitaka Ariga et al.·Oct 30, 2025SaveLearn
Infrared narrow band emitting quantum dots for high energy physics, medicine and space applicationsInfrared quantum dots, operating in the near-infrared (NIR, 700-1400 nm), short-wavelength infrared (SWIR, 1400-3000 nm), mid-infrared (MIR, 3000-8000 nm) and long-wavelength infrared (LWIR,…Tribikram Choudhury, Yacine Haddad, Michael Doser·Oct 29, 2025SaveLearn
Improved measurement of Born cross sections for bJ\,ω and bJ\,(π+π-π0) non-ω (J = 0, 1, 2) at Belle and Belle IIWe study the processes bJ\,ω and bJ\,(π+π-π0) non-ω (J = 0, 1, 2) at center-of-mass energies s from 10.73 to 11.02 GeV using a…Belle, Belle II Collaborations, : et al.·Oct 29, 2025SaveLearn
Test of CP Symmetry in the Neutral Decays of via J/Using (1008744)×106 J/ events collected with the BESIII detector, a full angular distribution analysis is carried out on the process…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 28, 2025SaveLearn