Near-Quantum-Noise Axion Dark Matter Search at CAPP around 9.5 μeVWe report the results of an axion dark matter search over an axion mass range of 9.39-9.51 μeV. A flux-driven Josephson parametric amplifier (JPA) was added to the cryogenic receiver chain. A…Jinsu Kim, Ohjoon Kwon, Çağlar Kutlu et al.·Jul 27, 2022SaveLearn
LUXE: A new experiment to study non-perturbative QED in electron-laser and photon-laser collisionsThe LUXE experiment (Laser Und XFEL Experiment) is an experiment in planning at DESY Hamburg using the electron beam of the European XFEL (Eu.XFEL). LUXE is intended to study collisions between a…Aharon Levy·Jul 27, 2022SaveLearn
Measurement of the top quark pole mass using tt+jet events in the dilepton final state at s= 13 TeV with the CMS experimentIn this contribution, a measurement of the top quark pole mass mtpole is presented. Events where a top quark-antiquark pair (tt) is produced in association…Sebastian Wuchterl·Jul 27, 2022SaveLearn
Measurement of the top quark pole mass using tt+jet events in the dilepton final state at s=13 TeVIn these proceedings, a measurement of the differential cross section of top quark-antiquark pair (tt) production in association with one additional jet…Sebastian Wuchterl·Jul 27, 2022SaveLearn
Hadronic D(s) decays at BESIIICharm hadronic decays are an important tool for understanding the the hadron spectroscopy and dynamics of the strong interaction in the low energy regime. BESIII experiment has collected a huge…Zehui Lu·Jul 27, 2022SaveLearn
c+ decays at BESIIIBESIII has made great progress in taking data which is the largest data samples near the c+c- threshold. We have measured the branching fraction of…Yang Gao·Jul 27, 2022SaveLearn
Measurement of the total cross section and -parameter from elastic scattering in pp collisions at s=13 TeV with the ATLAS detectorIn a special run of the LHC with β = 2.5~km, proton-proton elastic-scattering events were recorded at s = 13~TeV with an integrated luminosity of 340~μ b-1 using…ATLAS Collaboration·Jul 25, 2022SaveLearn
Top quark mass measurements at the tt threshold with CEPCWe present a study of top quark mass measurements at the tt threshold based on CEPC. A centre-of-mass energy scan near two times of the top mass is performed and the measurement precision of…Zhan Li, Xiaohu Sun, Yaquan Fang et al.·Jul 25, 2022SaveLearn
Search for dark matter particle interactions with electron final states with DarkSide-50We present a search for dark matter particles with sub-GeV/c2 masses whose interactions have final state electrons using the DarkSide-50 experiment's (12306 184) kg d low-radioactivity…50 Collaboration, P. Agnes, I. F. M. Albuquerque et al.·Jul 25, 2022SaveLearn
Search for dark matter-nucleon interactions via Migdal effect with DarkSide-50Dark matter elastic scattering off nuclei can result in the excitation and ionization of the recoiling atom through the so-called Migdal effect. The energy deposition from the ionization electron…50 Collaboration, P. Agnes, I. F. M. Albuquerque et al.·Jul 25, 2022SaveLearn
Search for low-mass dark matter WIMPs with 12 ton-day exposure of DarkSide-50We report on the search for dark matter WIMPs in the mass range below 10 GeV/c2, from the analysis of the entire dataset acquired with a low-radioactivity argon target by the DarkSide-50…50 Collaboration, P. Agnes, I. F. M. Albuquerque et al.·Jul 25, 2022SaveLearn
Large-Scale Deep Learning for Multi-Jet Event ClassificationWe report the largest scale deep learning with High Performance Computing (HPC) to physics analysis with the CMS simulation data in proton-proton collisions at 13 TeV. We build a Convolutional Neural…Jiwoong Kim, Dongsung Bae, Kihyeon Cho et al.·Jul 24, 2022SaveLearn
Study of (3686)→ωBased on a data sample of (448.12.9)×106 (3686) events collected with the BESIII detector at the BEPCII collider, the branching fraction of…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jul 24, 2022SaveLearn
First Observation of the Semileptonic Decay c+→ pK- e+eUsing 4.5~fb-1 of e+e- annihilation data samples collected at the center-of-mass energies ranging from 4.600~GeV to 4.699~GeV with the BESIII detector at the BEPCII collider, a…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jul 23, 2022SaveLearn
Design of axion and axion dark matter searches based on ultra high Q SRF cavitiesThe Superconducting Quantum Materials and Systems center is developing searches for dark photons, axions and ALPs with the goal of improving upon the current state-of-the-art sensitivity. These…Bianca Giaccone, Asher Berlin, Ivan Gonin et al.·Jul 22, 2022SaveLearn
Search for New Physics in Electronic Recoil Data from XENONnTWe report on a blinded analysis of low-energy electronic-recoil data from the first science run of the XENONnT dark matter experiment. Novel subsystems and the increased 5.9 tonne liquid xenon target…E. Aprile, K. Abe, F. Agostini et al.·Jul 22, 2022SaveLearn
Measurements of the branching fraction, isospin asymmetry, and lepton-universality ratio in B J/ K decays at Belle IIWe report a study of B J/(+-)K decays, where represents an electron or a muon, using e+e- collisions at the (4S) resonance. The data were collected by…Belle II Collaboration, F. Abudinén, I. Adachi et al.·Jul 22, 2022SaveLearn
High precision in CKM unitarity tests in b and c decaysThis article surveys the important questions attached to unitarity tests of the Cabibbo-Kobayashi-Maskawa matrix, with a focus on the direct determinations of the magnitude of CKM matrix elements.…Alexander Lenz, Stephane Monteil·Jul 22, 2022SaveLearn
Improved FIFRELIN de-excitation model for neutrino applicationsThe precise modeling of the de-excitation of Gd isotopes is of great interest for experimental studies of neutrinos using Gd-loaded organic liquid scintillators. The FIFRELIN code was recently used…H. Almazan, L. Bernard, A. Blanchet et al.·Jul 22, 2022SaveLearn
Measurement of Branching Fractions of Singly Cabibbo-suppressed Decays c+ → 0 K+ and + KS0Based on a sample of 4.4 fb-1 of e+e- annihilation data collected in the energy region between 4.6 GeV and 4.7 GeV with the BESIII detector at BEPCII, two singly…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jul 22, 2022SaveLearn
ECCE unpolarized TMD measurementsWe performed feasibility studies for various measurements that are related to unpolarized TMD distribution and fragmentation functions. The processes studied include semi-inclusive Deep inelastic…R. Seidl, A. Vladimirov, J. K. Adkins et al.·Jul 22, 2022SaveLearn
ECCE Sensitivity Studies for Single Hadron Transverse Single Spin Asymmetry MeasurementsWe performed feasibility studies for various single transverse spin measurements that are related to the Sivers effect, transversity and the tensor charge, and the Collins fragmentation function. The…R. Seidl, A. Vladimirov, D. Pitonyak et al.·Jul 22, 2022SaveLearn
Search for the weak decay (3686) c+ - +c.cUsing (448.1 2.9) × 106 (3686) events collected with the BESIII detector, we perform the first search for the weak baryonic decay $(3686) c+ -…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jul 22, 2022SaveLearn
Search for invisible Higgs bosons produced via vector boson fusion at the LHC using the ATLAS detectorDespite dark matter abundance, its nature remains elusive. Many searches of dark matter particles are carried out using different technologies either via direct detection, indirect detection, or…Mohamed Zaazoua, Farida Fassi, Kétévi Adiklè Assamagan et al.·Jul 21, 2022SaveLearn
Study of the reactions e+e- K+K-π0π0π0, e+e- K0SKππ0π0, and e+e- K0SKππ+π- at center-of-mass energies from threshold to 4.5 GeV using ISRWe study the processes e+e- K+K-π0π0π0γ, K0SKππ0π0γ, and K0SKππ+π-γ in which an energetic photon is radiated…BaBar Collaboration·Jul 21, 2022SaveLearn