Observation of quantum entanglement in top quark pairs at the ATLAS experimentThe ATLAS Collaboration has recently reported the first observation of quantum entanglement in top quark pair production at the Large Hadron Collider (LHC). A brief review of the experimental status…Baptiste Ravina·Oct 6, 2024SaveLearn
Measurements of decay branching fractions of the Higgs boson to hadronic final states at the CEPCThe Circular Electron Positron Collider (CEPC) is a large-scale particle accelerator designed to collide electrons and positrons at high energies. One of the primary goals of the CEPC is to achieve…Xiaotian Ma, Zuofei Wu, Jinfei Wu et al.·Oct 6, 2024SaveLearn
Study of same-sign W boson scattering and anomalous couplings in events with one tau lepton from pp collisions at s = 13 TeVA first study is presented of the cross section for the scattering of same-sign W boson pairs via the detection of a τ lepton. The data from proton-proton collisions at the center-of-mass energy…CMS Collaboration·Oct 5, 2024SaveLearn
MicroBooNE investigations on the photon interpretation of the MiniBooNE low energy excessThe MicroBooNE experiment is a liquid argon time projection chamber with 85-ton active volume at Fermilab, operated from 2015 to 2020 to collect neutrino data from Fermilab's Booster Neutrino Beam.…Guanqun Ge·Oct 5, 2024SaveLearn
Measuring system-size and event-topology dependence of (multi-)strangeness productionMeasurements of light-flavour particle production in small collision systems at the LHC energies have shown the onset of features that resemble what is typically observed in nucleus-nucleus…Lucia Anna Tarasovicova·Oct 4, 2024SaveLearn
Real-time Position Reconstruction for the KamLAND-Zen Experiment using Hardware-AI Co-designMonolithic liquid scintillator detector technology is the workhorse for detecting neutrinos and exploring new physics. The KamLAND-Zen experiment exemplifies this detector technology and has yielded…Alexander Migala, Eugene Ku, Zepeng Li et al.·Oct 3, 2024SaveLearn
Measurement of the effective leptonic weak mixing angleUsing pp collision data at s=13 TeV, recorded by the LHCb experiment between 2016 and 2018 and corresponding to an integrated luminosity of 5.4 fb-1, the forward-backward asymmetry…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Oct 3, 2024SaveLearn
Sustainable computing workshops in high-energy physics at DESYThis perspective article details the program of sustainable computing workshops launched within the High Energy Physics department at DESY in 2023. The workshop series targets scientific users of the…J. Alimena, C. Beyer, B. Bruers et al.·Oct 3, 2024SaveLearn
Search for lepton number violating decays of Ds+ h-h0e+e+Based on 7.33 fb-1 of e+e- collision data collected by the BESIII detector operating at the BEPCII collider at center-of-mass energies from 4.128 to 4.226 GeV, a search for the Majorana…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 3, 2024SaveLearn
PyHEP.dev 2024 Workshop Summary Report, August 26-30 2024, Aachen, GermanyThe second PyHEP.dev workshop, part of the "Python in HEP Developers" series organized by the HEP Software Foundation (HSF), took place in Aachen, Germany, from August 26 to 30, 2024. This gathering…Azzah Alshehri, Jan Bürger, Saransh Chopra et al.·Oct 3, 2024SaveLearn
Search for quantum decoherence in neutrino oscillations with six detection units of KM3NeT/ORCANeutrinos described as an open quantum system may interact with the environment which introduces stochastic perturbations to their quantum phase. This mechanism leads to a loss of coherence along the…S. Aiello, A. Albert, A. R. Alhebsi et al.·Oct 2, 2024SaveLearn
Latest oscillation results from Daya BayThe Daya Bay reactor neutrino experiment, which pioneered the measurement of a non-zero value for the neutrino mixing angle θ13 in 2012, operated for nearly nine years, from Nov.~24, 2011,…Jinjing Li·Oct 1, 2024SaveLearn
Learning to Reconstruct Quirky TracksAnalysis of data from particle physics experiments traditionally sacrifices some sensitivity to new particles for the sake of practical computability, effectively ignoring some potentially striking…Qiyu Sha, Daniel Murnane, Max Fieg et al.·Sep 30, 2024SaveLearn
High Energy Particle Detection with Large Area Superconducting Microwire ArrayWe present the first detailed study of an 8-channel 2×2 mm2 WSi superconducting microwire single photon detector (SMSPD) array exposed to 120 GeV proton beam and 8 GeV electron and pion…Cristián Peña, Christina Wang, Si Xie et al.·Sep 30, 2024SaveLearn
Nanosecond hardware regression trees in FPGA at the LHCWe present a generic parallel implementation of the decision tree-based machine learning (ML) method in hardware description language (HDL) on field programmable gate arrays (FPGA). A regression…Pavel Serhiayenka, Stephen Roche, Benjamin Carlson et al.·Sep 30, 2024SaveLearn
Study of Resonance Production using Run 3 pp Collisions with ALICERecent measurements in small collision systems at the LHC show striking similarities between high multiplicity pp, p-Pb collisions and Pb-Pb collisions. In particular, study of hadronic resonances…Hirak Kumar Koley·Sep 30, 2024SaveLearn
Novel machine learning applications at the LHCMachine learning (ML) is a rapidly growing area of research in the field of particle physics, with a vast array of applications at the CERN LHC. ML has changed the way particle physicists conduct…Javier M. Duarte·Sep 30, 2024SaveLearn
Search for a light CP-odd Higgs boson decaying into a pair of τ-leptons in proton-proton collisions at s = 13 TeV with the ATLAS detectorThis paper reports a search for a light CP-odd scalar resonance with a mass of 20 GeV to 90 GeV in 13 TeV proton-proton collision data with an integrated luminosity of 140 fb-1 collected with…ATLAS Collaboration·Sep 30, 2024SaveLearn
The search for light dark matter with DAMIC-MThe DAMIC-M (DArk Matter In CCDs at Modane) experiment will use skipper CCDs to search for low mass (sub-GeV) dark matter underground at the Laboratoire Souterrain de Modane (LSM) in France. With…R. Smida·Sep 30, 2024SaveLearn
Search for single-production of vector-like quarks decaying into Wb in the fully hadronic final state in pp collisions at s = 13 TeV with the ATLAS detectorA search for T and Y vector-like quarks produced in proton-proton collisions at a centre-of-mass energy of 13\,TeV and decaying into Wb in the fully hadronic final state is presented.…ATLAS Collaboration·Sep 30, 2024SaveLearn
Testing CPT symmetry via precise mass measurements of multi-strange baryons in ALICEThese proceedings present measurements of the -, +, -, + masses and mass differences between particle and anti-particle, in pp collisions…Romain Schotter·Sep 30, 2024SaveLearn
The axion dark matter experiment MADMAXThe MAgnetized Disk and Mirror Axion eXperiment (MADMAX) is a future experiment aiming to detect dark matter axions from the galactic halo by resonant conversion to photons in a strong magnetic…Pascal Pralavorio·Sep 30, 2024SaveLearn
The TOTEM nT2 detector: architecture, operation and performanceThe TOTEM experiment at the LHC has produced a large set of measurements on diffractive processes and pp cross sections. A new detector, called nT2, has been designed to measure the inelastic…Edoardo Bossini·Sep 30, 2024SaveLearn
Status of the muEDM experiment at PSIExplaining the matter-antimatter asymmetry in the Universe requires new sources of CP violation beyond the predictions of the Standard Model (SM). Electric dipole moments (EDMs) of particles, being…Francesco Renga·Sep 30, 2024SaveLearn
Longitudinal structure optimization for the high density electromagnetic calorimeterHigh density electromagnetic sandwich calorimeters with high readout granularity are considered for many future collider and fix-target experiments. Optimization of the calorimeter structure from the…Oleksandr Borysov, Shan Huang, Kamil Zembaczyński et al.·Sep 29, 2024SaveLearn