Simulation Software of the JUNO ExperimentThe Jiangmen Underground Neutrino Observatory (JUNO) is a multi-purpose experiment, under construction in southeast China, that is designed to determine the neutrino mass ordering and precisely…Tao Lin, Yuxiang Hu, Miao Yu et al.·Dec 21, 2022SaveLearn
New determination of the branching ratio of the structure dependent radiative K+ e+ e γ decayThe branching ratio of the structure dependent (SD) radiative K+ e+ e γ decay relative to that of the K+→ e+ e (γ) decay including the internal…A. Kobayashi, H. Ito, S. Bianchin et al.·Dec 21, 2022SaveLearn
Searching for Prompt and Long-Lived Dark Photons in Electro-Produced e+e- Pairs with the Heavy Photon Search Experiment at JLabThe Heavy Photon Search experiment (HPS) at the Thomas Jefferson National Accelerator Facility searches for electro-produced dark photons. We report results from the 2016 Engineering Run consisting…P. H. Adrian, N. A. Baltzell, M. Battaglieri et al.·Dec 20, 2022SaveLearn
Measurement of the charge asymmetry in top-quark pair production in association with a photon with the ATLAS experimentA measurement of the charge asymmetry in top-quark pair (tt) production in association with a photon is presented. The measurement is performed in the single-lepton tt decay channel…The ATLAS Collaboration·Dec 20, 2022SaveLearn
Looking forward: Photon induced processes with tagged protons at the CMS experimentPhoton induced processes can be used as a sensitive probe of new physics searches and can be studied using exclusive processes. These processes lead to unprecedented sensitivities on quartic…Michele Gallinaro·Dec 20, 2022SaveLearn
Measurement of the B0S μ+μ- decay properties and search for the B0 μ+μ- decay in proton-proton collisions at s = 13 TeVMeasurements are presented of the B0S μ+μ- branching fraction and effective lifetime, as well as results of a search for the B0 μ+μ- decay in proton-proton…CMS Collaboration·Dec 20, 2022SaveLearn
Search for a heavy neutrino in τ decays at BelleWe report on a search for a heavy neutrino in the decays τ- π- h, h π -+, = e, μ. The results are obtained using the full data sample collected with the…Belle Collaboration, D. Liventsev, I. Adachi et al.·Dec 20, 2022SaveLearn
Search for light dark matter with ionization signals in the PandaX-4T ExperimentWe report the search results of light dark matter through its interactions with shell electrons and nuclei, using the commissioning data from the PandaX-4T liquid xenon detector. Low energy events…PandaX Collaboration·Dec 20, 2022SaveLearn
Search for dark photons from Higgs boson decays via ZH production with a photon plus missing transverse momentum signature from pp collisions at s = 13 TeV with the ATLAS detectorThis paper describes a search for dark photons (γd) in proton-proton collisions at s=13 TeV at the Large Hadron Collider (LHC). The dark photons are searched for in the decay of…Atlas Collaboration·Dec 19, 2022SaveLearn
Luminosity determination in pp collisions at s=13 TeV using the ATLAS detector at the LHCThe luminosity determination for the ATLAS detector at the LHC during Run 2 is presented, with pp collisions at s=13 TeV. The absolute luminosity scale is determined using van der Meer…ATLAS Collaboration·Dec 19, 2022SaveLearn
Input of the Belle II Collaboration to the NuPECC Long Range Plan 2024The Belle II physics potential for hadron spectroscopy, inputs to g-2, fragmentation functions, proton form factors, measurements of αs and hadronic τ decays is outlined.B. G. Fulsom, J. S. Lange, J. Libby et al.·Dec 18, 2022SaveLearn
Measurement of lepton universality parameters in B+ K++- and B0 K*0+- decaysA simultaneous analysis of the B+ K++- and B0 K*0+- decays is performed to test muon-electron universality in two ranges of the square of the dilepton invariant…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Dec 18, 2022SaveLearn
Test of lepton universality in b → s + - decaysThe first simultaneous test of muon-electron universality using B+→ K++- and B0→ K*0+- decays is performed, in two ranges of the…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Dec 18, 2022SaveLearn
The NA60+ experiment at the CERN SPS to study dilepton and heavy quark production at large μBThe region of high baryonic densities of the QCD phase diagram is the object of several studies focused on the investigation of the order of the phase transition and the search for the critical…Maryna Borysova·Dec 18, 2022SaveLearn
Determination of U-spin breaking parameters with an amplitude analysis of the decay D0 K L0π+π-We present a study of the resonant structure of the decay D0 K L0π+π-, using quantum-correlated D0D0 data produced at s=3.773 GeV. The data sample was collected…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 18, 2022SaveLearn
Decay-aware neural network for event classification in collider physicsThe goal of event classification in collider physics is to distinguish signal events of interest from background events to the extent possible to search for new phenomena in nature. We propose a…Tomoe Kishimoto, Masahiro Morinaga, Masahiko Saito et al.·Dec 17, 2022SaveLearn
Adding Stroboscopic Muon Information For Reduction of Systematic Uncertainties in DUNEMuons have a similar latency/energy correlation from pion decay as do the neutrinos, and hence in each time-slice in a stroboscopic analysis measurements of their momentum spectra can reduce…Henry J. Frisch·Dec 16, 2022SaveLearn
JUNO Sensitivity on Proton Decay p K+ SearchesThe Jiangmen Underground Neutrino Observatory (JUNO) is a large liquid scintillator detector designed to explore many topics in fundamental physics. In this paper, the potential on searching for…JUNO Collaboration, Angel Abusleme, Thomas Adam et al.·Dec 16, 2022SaveLearn
Measurement of Br(H Zγ) at the 250 GeV ILCThe e+e- HZ process with the subsequent decay of the Higgs boson H Zγ is studied, where both Z bosons are reconstructed in the final states with two jets. The analysis is…E. Antonov, A. Drutskoy·Dec 15, 2022SaveLearn
First measurement of quasi-elastic baryon production in muon anti-neutrino interactions in the MicroBooNE detectorWe present the first measurement of the cross section of Cabibbo-suppressed baryon production, using data collected with the MicroBooNE detector when exposed to the neutrinos from the Main…MicroBooNE collaboration, P. Abratenko, D. Andrade Aldana et al.·Dec 15, 2022SaveLearn
Fast way to determine pp-collision time at the SPD experimentThe main task of this work is to find a fast and robust way to determine pp-collision time t0 at the SPD experiment. Using physics motivations, from the input flux of reconstructed particles' tracks…P. G. Filonchik, M. V. Zhabitsky·Dec 15, 2022SaveLearn
Lorentz group equivariant autoencodersThere has been significant work recently in developing machine learning (ML) models in high energy physics (HEP) for tasks such as classification, simulation, and anomaly detection. Often these…Zichun Hao, Raghav Kansal, Javier Duarte et al.·Dec 14, 2022SaveLearn
Studies of the muon momentum calibration and performance of the ATLAS detector with pp collisions at s=13 TeVThis paper presents the muon momentum calibration and performance studies for the ATLAS detector based on the pp collisions data sample produced at s=13 TeV at the LHC during Run 2 and…ATLAS Collaboration·Dec 14, 2022SaveLearn
Observation of a New X(3872) Production Process e+e-ω X(3872)Using 4.7~ fb-1 of e+e- collision data at center-of-mass energies from 4.661 to 4.951 GeV collected by the BESIII detector at the BEPCII collider, we observe the X(3872) production…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 14, 2022SaveLearn
Reconstructing charged particle track segments with a quantum-enhanced support vector machineReconstructing the trajectories of charged particles from the collection of hits they leave in the detectors of collider experiments like those at the Large Hadron Collider (LHC) is a challenging…Philippa Duckett, Gabriel Facini, Marcin Jastrzebski et al.·Dec 14, 2022SaveLearn