Search for Diffuse Supernova Neutrino Background of All Flavors with PandaX-4TWe present the first search for the diffuse supernova neutrino background utilizing coherent elastic neutrino-nucleus scattering with the PandaX-4T liquid xenon detector at the China Jinping…Yingxin Zhang, PandaX Collaboration·Oct 5, 2026SaveLearn
Precision measurement of ocean tides using cosmic-ray muonsCosmic-ray muons provide a natural probe of the integrated mass along their trajectories. Here we show that cosmic-ray muons can monitor ocean-tide-induced variations in seawater overburden within an…Jiwon Seo, Jongseok Chung, Chang Hyon Ha et al.·Oct 4, 2026SaveLearn
Observation of D+ K*0ρ+ and D+ K*+ρ0 in Doubly Cabibbo-Suppressed Decay D+ K+π+π-π0By analyzing an e+e- collision data sample with an integrated luminosity of 20.3 fb-1 collected with the BESIII detector at the center-of-mass energy of 3.773 GeV, we perform the first…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 4, 2026SaveLearn
Search for Higgs boson compositeness effects in high-mass dilepton final states in proton-proton collisions at s = 13 and 13.6 TeVA search for beyond the standard model effects in high-mass dielectron and dimuon final states with the CMS detector is performed, with a specific focus on Higgs boson compositeness. The search uses…CMS Collaboration·Oct 3, 2026SaveLearn
Simultaneous measurement of the Higgs boson decay rates to WW and ZZ in fully hadronic final states at FCC-eeThe precise determination of the Higgs boson couplings to electroweak gauge bosons is a key objective of the FCC-ee physics program. In particular, measurements of the Higgs boson couplings to W and…Jan Eysermans, Mila Pandurovic, Christoph Paus et al.·Oct 3, 2026SaveLearn
Search for pair-produced vector-like top quarks decaying into Lorentz-boosted top quarks and scalar bosons in proton-proton collisions at s = 13 TeVA search for pair-produced vector-like top quarks, T, decaying into a new scalar boson ϕ and a standard model (SM) top quark is presented. The search targets events containing a photon pair…CMS Collaboration·Oct 2, 2026SaveLearn
Track fitting as a language translation problemParticle physics analysis depends on information retrieved from particle tracks in a detector. Traditionally, this involves collecting individual detector hits, recombining them to form tracks, and…Deepak Samuel, Christy Elsa Koshy·Oct 2, 2026SaveLearn
First observation of electron antineutrinos from nuclear reactors at Super-KamiokandeIn 2020, Super-Kamiokande entered the SK-Gd phase, improving its sensitivity to low-energy electron antineutrinos through the detection of neutrons captured on gadolinium dissolved in the detector…K. Abe, Y. Asaoka, M. Harada et al.·Oct 2, 2026SaveLearn
Entanglement-sensitive observables in e+e- τ+τ- at STCF: a detector-level feasibility studyQuantum entanglement in τ+τ- production provides a direct probe of non-classical spin correlations in a relativistic quantum system, with the τ decay products serving as spin analyzers. We…Chentao Bao, Xi Tao, Hai Chen et al.·Oct 2, 2026SaveLearn
First measurement of the low-momentum negative-muon beam for the muon-to-electron conversion experiment at J-PARCThe COMET Phase-α experiment, the initial beam-operation stage of the COMET muon-to-electron conversion programme at J-PARC, took place in 2023 and marked the first beam operation at the COMET…The COMET Collaboration, K. Oishi, R. Abramishvili et al.·Oct 2, 2026SaveLearn
A-GHOST: High-rate streaming of trigger-level data to programmable GPU inferenceA-GHOST (A Global Heterogeneous Online Scouting Trigger) is an R&D effort investigating high-rate streaming readout architectures for high-energy physics (HEP) experiments. The central idea is to…I. Xiotidis, N. Clarke Hall, M. S. Larson et al.·Oct 1, 2026SaveLearn
Search for charged-lepton-flavour violating eμtq interactions at s=13 TeV with the ATLAS detectorA search for charged-lepton-flavour violation (cLFV) in top-quark production and decay is presented. The data analysed correspond to 140 fb-1 of proton-proton collisions recorded at a…ATLAS Collaboration·Oct 1, 2026SaveLearn
Full Event Interpretation at Belle II: Current Status and Recent DevelopmentsThe Full Event Interpretation (FEI) algorithm is a central component of the Belle II analysis framework, designed for the efficient reconstruction of exclusive B-meson decays. The FEI performs a…R. Tiwary, M. Marfoli, V. Vobbilisetti et al.·Oct 1, 2026SaveLearn
Search for dark matter produced in association with a low-multiplicity jet in proton-proton collisions at s = 13 TeVA search for dark matter particles is presented using events with large missing transverse momentum and a single energetic jet containing few constituents. The analysis uses proton-proton collision…CMS Collaboration·Oct 1, 2026SaveLearn
Scaling Collider Event Generation with Residual-Quantized TokensFull detector simulation and reconstruction of collider events are projected to become major bottlenecks at the High-Luminosity Large Hadron Collider, motivating the development of fast, ML-based…Dan Godi, Dmitrii Kobylianskii, Eilam Gross·Sep 30, 2026SaveLearn
First double-differential cross-section measurements in proton multiplicity and kinematics for mesonless νμ charged-current interactions on argon using the MicroBooNE detectorWe present the first double-differential cross-section measurements of muon neutrino charged-current interactions on argon with no mesons and one or more protons (Np ≥ 1) in the final state…MicroBooNE collaboration, P. Abratenko, D. Andrade Aldana et al.·Sep 30, 2026SaveLearn
Non-parametric and continuous extraction of amplitudes in realistic electroweak penguin decaysA novel approach to extract decay amplitudes in B V( M1M2)+- processes, where V represents a meson with either J = 0 (S-wave) or J = 1 (P-wave), was recently proposed. In…Tingzhen Xiao, Anja Beck, Eluned Smith·Sep 30, 2026SaveLearn
Measurement of prompt and non-prompt D *+-meson spin alignment in pp collisions at s = 13.6 TeV$A precise measurement of prompt and non-prompt D *+-meson spin alignment with respect to the helicity and production axes in proton-proton (pp) collisions at s = 13.6 TeV is…ALICE Collaboration·Sep 30, 2026SaveLearn
Measurement of the triple-differential cross section of Z+jet production in proton-proton collisions at s = 13 TeVA measurement is presented of the triple-differential production cross section of Z/γ*( μμ)+jet events using proton-proton collision data recorded at a center-of-mass energy of 13 TeV by…CMS Collaboration·Sep 30, 2026SaveLearn
Projected Sensitivity to Atmospheric Neutrino Oscillations using a 1725 m3 Liquid-Nitrogen Detector at CJPLIn atmospheric neutrino analyses, the usable zenith-angle range is generally restricted to upward-going events to suppress the cosmic-ray muon background. Motivated by the exceptionally low…Xiao-Yu Peng, Shin-Ted Lin, Shu-Kui Liu et al.·Sep 30, 2026SaveLearn
Particle track reconstruction in high-density collider environments with an Evolving-Geometry TransformerCharged particle track reconstruction at the High-Luminosity Large Hadron Collider is challenged by dense hit environments and combinatorial ambiguities. Existing graph-based and Transformer…Chenxiu Ou, Yan Wang, Mingjiang Liang et al.·Sep 30, 2026SaveLearn
Overview of the HL-LHC CMS outer tracker upgrade and lessons learned from 2S module productionFor operation at the High-Luminosity LHC, the CMS collaboration is developing a significantly enhanced silicon detector system with improved radiation hardness, higher granularity, and extended…F. Zhang·Sep 29, 2026SaveLearn
Search for π1(1600) in a three-pion system at GlueXThe GlueX experiment in Hall D at Jefferson Lab enables studies of the light meson spectrum in γp interactions with a linearly polarized photon beam. GlueX aims in particular to search for hybrid…Ilia Belov, Farah Afzal·Sep 29, 2026SaveLearn
Irradiation Studies and Design Optimization of the ATLAS Tile Calorimeter for the High-Luminosity LHCThe Tile Calorimeter (TileCal) is a sampling hadronic calorimeter covering the central region of the ATLAS experiment at the CERN Large Hadron Collider (LHC). It employs steel as the absorber…Róbert Astaloš·Sep 29, 2026SaveLearn
Measurement of Neutrino Oscillation Parameters at JUNO and Indication of the Neutrino Mass OrderingWe report an improved measurement of neutrino oscillation parameters at the Jiangmen Underground Neutrino Observatory (JUNO) and the consequent indication of neutrino mass ordering. The analysis is…The JUNO Collaboration·Sep 29, 2026SaveLearn