On the Charged Fragments Tagging in the ATLAS Detector during the 2025 Oxygen CampaignDuring the Summer of 2025 the LHC collided protons with oxygen, oxygen with oxygen and neon with neon. The ATLAS experiment recorded these data with its Forward Proton detectors (AFP) inserted on…Weronika Sobien, Maciej Trzebinski·Jun 2, 2026SaveLearn
Search for electroweak scale dijet resonances in pile-up collisions at s=13 TeV with the ATLAS detectorA search for dijet resonances in the mass range of 100-250 GeV is presented using proton-proton collision data recorded by the ATLAS experiment at the Large Hadron Collider at a centre-of-mass energy…ATLAS Collaboration·Jun 2, 2026SaveLearn
Nuclear Recoil Migdal Effect in Liquid Xenon Dark Matter ExperimentsThe Migdal effect predicts that a nuclear recoil can be accompanied by detectable atomic ionization or excitation signals, even at the low energies expected from interactions of sub-GeV dark matter…Jingke Xu, Jeonghwa Kim, Duncan Adams et al.·Jun 2, 2026SaveLearn
Probing Quantum Entanglement in τ+τ- Pairs via the ππ Channel at STCFQuantum entanglement and Bell-inequality violation in τ+τ- pairs provide a sensitive probe of quantum correlations in high-energy interactions. We present a feasibility study of $e+e- …Xiaokang Li, Chentao Bao, Hai Chen et al.·Jun 2, 2026SaveLearn
Study of Central Exclusive Production of π+π-, K+K- and p p Pairs in Proton-Proton Collisions at s = 510 GeV with the STAR Detector at RHICWe report on the first measurement of the Central Exclusive Production process in proton-proton collisions: pp \ → \ p h+ h- p (where h = π, K, p) at the center-of-mass energy…STAR Collaboration, B. E. Aboona, J. Adam et al.·Jun 2, 2026SaveLearn
Precision Measurement of Ds*+-Ds+ Mass DifferenceWe measure the mass difference between Ds*+ and Ds+, Δms, using the decay chain Ds*+ Ds+( K+ K- π+)π0, utilizing e+e- annihilation data…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jun 2, 2026SaveLearn
Search for a leptoquark in events with a hadronically decaying τ-lepton and missing transverse momentum using pp collisions at s=13 TeV with the ATLAS detectorA search for leptoquark signals is performed in final states with a hadronically decaying τ-lepton and missing transverse momentum, using data from proton--proton collisions at a centre-of-mass…ATLAS Collaboration·Jun 1, 2026SaveLearn
Searching for Anomalies with Foundation ModelsFoundation models have the potential to extend the discovery reach for anomaly detection searches. When studying the large OmniLearned foundation model on data from the CMS experiment, unexpected…Vinicius Mikuni, Benjamin Nachman·Jun 1, 2026SaveLearn
Search for single production of a vector-like B' quark decaying to a top quark and a W boson in the single-lepton final state in proton-proton collisions at s = 13 TeVA search is presented for the single production of a narrow-width vector-like B' quark that decays to a t quark and a W boson, with one of the decay products yielding an electron or muon. The…CMS Collaboration·May 31, 2026SaveLearn
Expected Sensitivity of the Light Dark Matter eXperiment to Long-Lived Dark Photons and Axion-Like ParticlesThe Light Dark Matter eXperiment (LDMX) is an electron-beam fixed-target experiment primarily designed to achieve world-leading, model-independent sensitivity to sub-GeV dark matter particles. LDMX…Torsten Akesson, Clay Barton, Charles Bell et al.·May 31, 2026SaveLearn
Radiation Resistance of Ge-doped Multi-Mode Fiber for Optical Links in Collider ExperimentsThe applications of optical links in collider experiments provide the advantage of high-speed data transmission with low mass fibers over distances of a few hundred meters. Ge-doped multi-mode fibers…Datao Gong, Suen Hou, Bo-Jing Juang et al.·May 31, 2026SaveLearn
Comparisons of triple-differential cross sections for quasielastic-like νμ-hydrocarbon interactions using Eν 3~GeV versus 6~GeV beams in MINERvANeutrino charged-current quasielastic-like scattering, a reaction category extensively used in neutrino oscillation measurements, receives contributions from single nucleon knockout processes,…D. Ruterbories, S. Akhter, Z. Ahmad Dar et al.·May 30, 2026SaveLearn
Probing the nature of the χc1(3872) state using radiative decaysThe radiative decays χc1(3872)→ψ(2S)γ and χc1(3872)→ J/ψγ are used to probe the~nature of the~χc1(3872) state using proton-proton collision data collected with the…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·May 30, 2026SaveLearn
An AI-ready, Polarized Electron-Positron Collision DatasetWe present a modernized, AI-ready release of reconstructed data from the SLD experiment at the SLAC Linear Collider (SLC). The dataset comprises approximately 660,000 reconstructed events collected…Chi Lung Cheng, Simon Corrodi, T. J. Hobbs et al.·May 29, 2026SaveLearn
Measurement of the cross-section for the production of a W boson in association with b-jets in pp collisions at s=13 TeV with the ATLAS detectorThis paper presents a measurement of the production cross-section of a W boson associated with one or two jets, where at least one jet originates from a b-quark. The data are collected with the…ATLAS Collaboration·May 29, 2026SaveLearn
Phast: Simultaneous reconstruction of photoelectron count and time profiles from PMT waveforms via machine learningPhotomultiplier tubes (PMTs) are widely used in particle and nuclear physics experiments. The reconstruction of PMT waveforms is a fundamental task in these experiments, where accurate extraction of…Yiming Xu, Youwen Fan, Siyu Chen et al.·May 28, 2026SaveLearn
Enhanced evidence of X(7200) and improved measurements of X(6900) parameters from a combined LHCb-ATLAS-CMS analysisWe report stronger evidence for the X(7200) state and markedly improved measurements of the X(6900) resonance parameters based on a combined analysis of the di-J/ψ mass spectrum using published…Yuan Wang, Ran Li, Bin Zhong et al.·May 28, 2026SaveLearn
Electromagnetic deflection effects in the integrated luminosity measurement at the CEPCIn order to ensure measurement of the integrated luminosity with a relative precision of 10-4 at the Z0 pole at CEPC, numerous systematic effects have to be quantified…Ivan Smiljanić, Ivanka Božović, Ivana Vidaković et al.·May 28, 2026SaveLearn
Wasserstein normalized autoencoder for anomaly detectionA novel anomaly detection algorithm is presented. The Wasserstein normalized autoencoder (WNAE) is a normalized probabilistic model that minimizes the Wasserstein distance between the learned…CMS Collaboration·May 28, 2026SaveLearn
Characterising the role of final state interactions on neutrino energy estimation in the DUNE and Hyper-K eraThe Deep Underground Neutrino Experiment (DUNE) and Hyper-Kamiokande (Hyper-K) will measure neutrino oscillation parameters with an unprecedented precision that requires neutrino energy estimation to…Stephen Dolan, Jake McKean, Laura Munteanu·May 27, 2026SaveLearn
CP-violation or Nuclear Excitation: Reviewing the Role of Neutrino Interaction Model Uncertainties on Accelerator-Based Neutrino Oscillation MeasurementsAccelerator-based neutrino oscillation experiments have the potential to revolutionise our understanding of fundamental physics, offering an opportunity to characterise charge-parity violation in the…Stephen Dolan, Luke Pickering, Patrick Stowell et al.·May 27, 2026SaveLearn
Search for pair-produced vector-like T-quarks decaying into Ht final states in the lepton-plus-jets channel in pp collisions at s=13 TeV with the ATLAS detectorA search for pair-produced vector-like T-quarks in 139 fb-1 of pp collisions recorded by the ATLAS detector at a centre-of-mass energy s=13 TeV is presented. The search targets…The ATLAS Collaboration·May 27, 2026SaveLearn
Search for light scalar particles produced in Higgs boson decays in exclusive final states with two muons and two hadrons in proton-proton collisions at s = 13 TeVA search for new scalar particles of O(GeV) mass in exclusive final states with muons and light hadrons is presented. The analysis uses proton-proton collision data produced at a…CMS Collaboration·May 27, 2026SaveLearn
Search for heavy long-lived charged particles with level-1 trigger scouting data from proton-proton collisions at s = 13.6 TeVA search for heavy long-lived charged particles at the LHC is presented. Particles interacting with the CMS muon detector across several bunch crossings are searched for using a data sample of…CMS Collaboration·May 27, 2026SaveLearn
Measurement of the Higgs boson total decay width using the H WW eνμν decay channel in proton-proton collisions at s = 13 TeVThe Higgs boson (H) decay width is determined from the ratio of off- and on-shell production of H WW eνμν using proton-proton collision data corresponding to an integrated luminosity of…CMS Collaboration·May 27, 2026SaveLearn