Search for axion-like particles through nuclear Primakoff production using the GlueX detectorWe report on the results of the first search for the production of axion-like particles (ALP) via Primakoff production on nuclear targets using the GlueX detector. This search uses an integrated…J. R. Pybus, T. Kolar, B. Devkota et al.·Aug 11, 2023SaveLearn
Measurement of the Positive Muon Anomalous Magnetic Moment to 0.20 ppmWe present a new measurement of the positive muon magnetic anomaly, aμ (gμ - 2)/2, from the Fermilab Muon g\!-\!2 Experiment using data collected in 2019 and 2020. We have analyzed…D. P. Aguillard, T. Albahri, D. Allspach et al.·Aug 11, 2023SaveLearn
A search for rare B → D μ+ μ- decaysA search for rare B → D μ+ μ- decays is performed using proton-proton collision data collected by the LHCb experiment, corresponding to an integrated luminosity of 9 fb-1. No…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Aug 11, 2023SaveLearn
Search for scalar leptoquarks produced via τ-lepton-quark scattering in pp collisions at s = 13 TeVThe first search for scalar leptoquarks produced in τ-lepton-quark collisions is presented. It is based on a set of proton-proton collision data recorded with the CMS detector at the LHC at a…CMS Collaboration·Aug 11, 2023SaveLearn
Search for Dark Photons with the FASER detector at the LHCThe FASER experiment at the LHC is designed to search for light, weakly-interacting particles produced in proton-proton collisions at the ATLAS interaction point that travel in the far-forward…FASER Collaboration·Aug 10, 2023SaveLearn
Search for the lepton number violation decay φ π+ π+ e- e- via J/ φηUsing (1.00870.0044)×1010 J/ events collected by the BESIII detector at the BEPCII collider, we search for the lepton number violation decay φ π+ π+ e- e- via…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Aug 10, 2023SaveLearn
Spectroscopy at e+e- collidersExotic hadron states beyond the conventional qqq baryon and qq meson configurations are well expected from QCD. Having been successful in the past decades, the heavy quarkonium sector is…Zhiqing Liu·Aug 10, 2023SaveLearn
Measurement of additional radiation in the initial-state-radiation processes e+e- μ+μ-γ and e+e- π+π-γ at BABARA dedicated measurement of additional radiation in e+e-μ+μ-γ and e+e-π+π-γ initial-state-radiation events is presented using the full BABAR data sample. For the…BABAR Collaboration·Aug 9, 2023SaveLearn
Measurement of branching-fraction ratios and CP asymmetries in B DCPK decays at Belle and Belle IIWe report results from a study of B → DK decays followed by D decaying to CP~eigenstates, where D indicates a D0 or D0 meson. These decays are sensitive to the…The Belle, Belle II Collaborations, : et al.·Aug 9, 2023SaveLearn
Charm production and fragmentation fractions at midrapidity in pp collisions at s = 13 TeVMeasurements of the production cross sections of prompt D0, D+, D +, Ds+, c+, and c+ charm hadrons at midrapidity in…ALICE Collaboration·Aug 9, 2023SaveLearn
Study of flavor dependence of the baryon-to-meson ratio in proton-proton collisions at s = 13 TeVThe production cross sections of D0 and + c hadrons originating from beauty-hadron decays (i.e. non-prompt) were measured for the first time at midrapidity (|y|<0.5) by the…ALICE Collaboration·Aug 9, 2023SaveLearn
Search for magnetic monopoles and stable particles with high electric charges in s=13 TeV pp collisions with the ATLAS detectorWe present a search for magnetic monopoles and high-electric-charge objects using LHC Run 2 s =13 TeV proton-proton collisions recorded by the ATLAS detector. A total integrated luminosity…ATLAS Collaboration·Aug 9, 2023SaveLearn
Combined measurement of the Higgs boson mass from the Hγγ and H ZZ* 4 decay channels with the ATLAS detector using s = 7, 8 and 13 TeV pp collision dataA measurement of the mass of the Higgs boson combining the H ZZ* 4 and Hγγ decay channels is presented. The result is based on 140 fb-1 of proton-proton collision…The ATLAS Collaboration·Aug 9, 2023SaveLearn
Proceedings Excited QCD on recent quarkonium results at Belle IIThe Belle experiment has given a substantial contribution in the field of heavy quarkonia. Several new states were announced by Belle for the first time, in both charmonium and bottomonium spectrum,…Dmytro Meleshko, Elisabetta Prencipe, Sören Lange·Aug 8, 2023SaveLearn
First application of a liquid argon time projection chamber for the search for intranuclear neutron-antineutron transitions and annihilation in 40Ar using the MicroBooNE detectorWe present a novel methodology to search for intranuclear neutron-antineutron transition (n→n) followed by n-nucleon annihilation within an 40Ar nucleus, using the…MicroBooNE collaboration, P. Abratenko, O. Alterkait et al.·Aug 7, 2023SaveLearn
Search for Charged Lepton Flavor Violation in J/ decays at BESIIIThe observation of any charged lepton flavor violation (CLFV) process would be a clear signal of new physics beyond the Standard Model. Various decay modes, including lepton (μ, τ) decays,…Jingshu Li, Zhengyun You·Aug 7, 2023SaveLearn
Measurement of the e+e- 0 + c.c. cross sections at s from 2.3094 to 3.0800 GeVThe Born cross sections and effective form factors of the process e+e-0 + c.c. are measured at 14 center-of-mass energy points from 2.3094 to 3.0800 GeV, based on data…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Aug 7, 2023SaveLearn
Reducing model uncertainties using proton-oxygen collisions with proton/neutron tagging at the LHCA short run of proton-oxygen and oxygen-oxygen collisions is planned to take place at the Large Hadron Collider during LHC Run 3. The primary goal of this run is to improve the modeling of Cosmic-Ray…Michael Pitt·Aug 6, 2023SaveLearn
Observation of Wγγ triboson production in proton-proton collisions at s = 13 TeV with the ATLAS detectorThis letter reports the observation of W()γγ production in proton-proton collisions. This measurement uses the full Run 2 sample of events recorded at a center-of-mass energy of…ATLAS Collaboration·Aug 6, 2023SaveLearn
Heavy Flavour SpectroscopyThe discovery of hadronic states beyond the conventional two-quark meson and three-quark baryon picture in the last two decades is one of the most amazing accomplishments in fundamental physics…Chang-Zheng Yuan·Aug 6, 2023SaveLearn
Study on the accidental background of the JSNS2 experimentJSNS2 (J-PARC Sterile Neutrino Search at J-PARC Spallation Neutron Source) is an experiment which searches for sterile neutrinos via the observation of μ e…D. H. Lee, S. Ajimura, M. K. Cheoun et al.·Aug 4, 2023SaveLearn
Enhancing the hunt for new phenomena in dijet final-states using anomaly detection filters at the High-Luminosity Large Hadron ColliderIn the realm of dijet searches in high-energy physics, a significant challenge has emerged: with experiments producing more and more data, the traditional methods of using analytic functions to…Sergei V. Chekanov, Rui Zhang·Aug 4, 2023SaveLearn
First measurement of discrimination between helium and electron recoils in liquid xenon for low-mass dark matter searchesWe report the first measurement of discrimination between low-energy helium recoils and electron recoils in liquid xenon. This result is relevant to proposed low-mass dark matter searches which seek…S. J. Haselschwardt, R. Gibbons, H. Chen et al.·Aug 4, 2023SaveLearn
Recent highlights from the LHCb experimentThe Large Hadron Collider beauty (LHCb) detector is a single-arm forward spectrometer at the LHC, designed for the study of heavy flavour physics. In this proceedings, an overview of the detector…Abhijit Mathad·Aug 4, 2023SaveLearn
Measurement of the production cross section for a W boson in association with a charm quark in proton-proton collisions at s = 13 TeVThe strange quark content of the proton is probed through the measurement of the production cross section for a W boson and a charm (c) quark in proton-proton collisions at a center-of-mass energy of…CMS Collaboration·Aug 4, 2023SaveLearn