Flavor, transverse momentum, and azimuthal dependence of charged pion multiplicities in SIDIS with 10.6 GeV electronsMeasurements of SIDIS multiplicities for π+ and π- from proton and deuteron targets are reported on a grid of hadron kinematic variables z, PT, and ϕ* for leptonic kinematic…Hall C SIDIS Collaboration, P. Bosted, H. Bhatt et al.·Jun 22, 2026SaveLearn
Searches for resonant and nonresonant multi-Higgs production in ATLAS and CMSThe measurement of the Higgs boson self-coupling is one of the key physics goals of the LHC program, providing direct access to the shape of the Higgs potential and offering sensitivity to physics…Emmanouil Vourliotis·Jun 21, 2026SaveLearn
Search for the charged lepton flavor violating decay η eμ^Based on (10.087 0.044) × 109~J/ψ events collected at the center-of-mass energy s = 3.097~GeV with the BESIII detector, we search for the charged lepton flavor violating decay…M. Ablikim, M. N. Achasov, P. Adlarson et al.·Jun 21, 2026SaveLearn
Optomechanical Accelerometer Search for Ultralight Dark MatterCavity optomechanical systems have recently been proposed as detectors for ultralight dark matter, leveraging their ability to cool and probe mechanical oscillators at the quantum limit. Here we…M. Dey Chowdhury, J. P. Manley, C. A. Condos et al.·Jun 21, 2026SaveLearn
Accelerating Discovery: Model-Agnostic Likelihoods for the Reinterpretation of Particle Physics Results and their Application to the Belle II B+ K+νν MeasurementExperimental results in high-energy physics are inherently hypothesis-dependent, as collider analyses are designed to test specific theoretical frameworks. The proliferation of theoretical models…Lorenz Gärtner·Jun 20, 2026SaveLearn
AI Agents Can Already Autonomously Perform Experimental High Energy PhysicsLarge language model-based AI agents are now able to autonomously execute substantial portions of a high energy physics (HEP) analysis pipeline with minimal expert-curated input. Given access to a…Eric A. Moreno, Samuel Bright-Thonney, Andrzej Novak et al.·Jun 20, 2026SaveLearn
Towards LLM-Powered Automation of a Dark Matter Constraint RepositoryDark matter constraint repositories are critical community infrastructure, giving experimentalists and theorists a shared landscape of existing bounds. Yet the most widely-used repositories are…Lanqing Yuan, Karthik Ramanathan·Jun 19, 2026SaveLearn
Analysis note: Long-range near-side correlation in e+e- with W-boson-pair events at 183-209 GeV with ALEPH archived dataEvents characterized by a high multiplicity of charged particles have been a central focus in the study of collective behavior across both large and small collision systems. A previous measurement of…Tzu-An Sheng, Yu-Chen Chen, Yi Chen et al.·Jun 19, 2026SaveLearn
A frontend ASIC for MicrodosimetryRecent clinical evidence shows a correlation between linear energy transfer (LET) and tumor control in carbon ion radiotherapy. This prompts the direct inclusion of LET into the treatment planning.…Simon Waid, Matthias Knopf, Giulio Magrin et al.·Jun 19, 2026SaveLearn
Measurement of mixing-induced CP violation in the decay B0 π0 π0Measurements of charge-parity (CP) violation in quark transitions provide stringent tests of the current theory and sensitive probes of particles or interactions beyond it. We report the first…Belle II Collaboration, M. Abumusabh, I. Adachi et al.·Jun 18, 2026SaveLearn
Observation of electroweak production of pairs of Z bosons in proton-proton collisions at 13 TeVThe first evidence of electroweak (EW) production of pairs of Z bosons in association with two jets (jj) in the final state ZZjj ννjj, where = e, μ, is reported by the CMS…CMS Collaboration·Jun 18, 2026SaveLearn
HEPTv2: End-to-End Efficient Point Transformer for Charged Particle ReconstructionCharged-particle tracking -- reconstructing trajectories from sparse detector measurements -- is a fundamental high-energy-physics inference problem and a canonical example of learning under extreme…Siqi Miao, Shitij Govil, Jack P. Rodgers et al.·Jun 18, 2026SaveLearn
Measurements of the Higgs boson production, fiducial and differential cross-sections in the four lepton decay channel using 164 fb-1 of data collected at s = 13.6 TeV with the ATLAS detectorInclusive, differential and production-mode cross-section measurements of the Higgs boson are performed in the H ZZ* 4 decay channel. The analysis uses proton-proton collision data…ATLAS Collaboration·Jun 18, 2026SaveLearn
ADAMOS: Axion Daily Modulation Searches for Dark Matter at 20 GHzThe ADAMOS (Axion Daily Modulation Searches) project aims to explore the nature of dark matter (DM) through a novel axion haloscope experiment. We propose to construct a fixed-frequency cavity…Marios Maroudas, Toma-Stefan Cezar, Antonios Gardikiotis et al.·Jun 18, 2026SaveLearn
Charged kaon and proton multiplicities in semi-inclusive deep-inelastic scattering with 11 GeV electronsMeasurements of SIDIS multiplicities for charged kaons and protons from proton and deuteron targets are reported on a grid of hadron kinematic variables 0.3<z<0.7 and Pt<0.6 GeV for leptonic…P. Bosted, W. Armstrong, H. Bhatt et al.·Jun 17, 2026SaveLearn
Probing Long-Lived Particle Production in Muon Decays at the SNS with a Highly Capable Hydrocarbon DetectorThe Spallation Neutron Source (SNS) at Oak Ridge National Laboratory (ORNL) is a prolific muon producer, making it an ideal location for studying dark sector particles produced in muon decays at…M. Andriamirado, A. B. Balantekin, C. D. Bass et al.·Jun 17, 2026SaveLearn
High-p T physics and jet productionJet production is the dominant high-p T process at hadron colliders and provides a central testing ground for perturbative QCD, parton distribution functions and determinations of the strong…Francesco Giuli·Jun 17, 2026SaveLearn
QCD studies and precision physics at the LHeCThe Large Hadron electron Collider (LHeC) would add a high-current Energy Recovery Linac to the HL-LHC, delivering electron-proton collisions at centre-of-mass energies around the TeV scale. This…Francesco Giuli·Jun 17, 2026SaveLearn
Gluon dominance model and multiparticle productionThe gluon dominance model describes multiparticle production of secondary particles at high energies in lepton and hadron interactions, including annihilation processes and heavy quarkonium decays.…E. S. Kokoulina, A. Ya. Kutov, V. A. Nikitin et al.·Jun 17, 2026SaveLearn
Radon-induced backgrounds in the NEXT-100 experimentThe NEXT-100 detector at the LSC aims at the first competitive search for the decay using a high-pressure 136 electroluminescent time projection chamber. The first low-background run of…NEXT Collaboration, C. Cortes-Parra, P. Novella et al.·Jun 17, 2026SaveLearn
Neutron Reconstruction via Blips in Liquid Argon Time Projection ChambersNeutrons are important final-state particles in neutrino interactions, yet they are not considered or reconstructed in most current neutrino LArTPC physics analyses. In this paper, we present a…Miguel Hernandez Morquecho, Bryce Littlejohn, Paola Sala et al.·Jun 17, 2026SaveLearn
Observation of the radiative decay Ds (2317)+ Ds* γWe observe the radiative decay D*s0(2317)+ Ds*+ γ for the first time, with a significance exceeding 10 standard deviations. The signal is found in the continuum $e+ e- …Belle II Collaboration, M. Abumusabh, I. Adachi et al.·Jun 17, 2026SaveLearn
Search for dark matter production in association with bottom quarks and a lepton pair in proton-proton collisions at s = 13 TeVA search is performed for dark matter produced in association with bottom quarks and a pair of electrons or muons in data collected with the CMS detector at the LHC, corresponding to 138 fb-1 of…CMS Collaboration·Jun 17, 2026SaveLearn
The ESSnuSB ExperimentIn this proceedings, we will describe the physics program of the ESSnuSBplus, phase-I of the ESSnuSB project. ESSnuSB is a future long-baseline neutrino oscillation experiment in Europe which aims to…Monojit Ghosh·Jun 16, 2026SaveLearn
Electromagnetic Shower Reconstruction and Identification in FASER's Emulsion Detector for LHC Forward Neutrino MeasurementsWe present methods for electromagnetic shower reconstruction and identification in the FASERnu emulsion detector using 100 GeV and 200 GeV electron test-beam data from the CERN SPS H4 beamline. The…FASER Collaboration, Roshan Mammen Abraham, Xiaocong Ai et al.·Jun 16, 2026SaveLearn