Detection of a particle shower at the Glashow resonance with IceCubeThe Glashow resonance describes the resonant formation of a W- boson during the interaction of a high-energy electron antineutrino with an electron, peaking at an antineutrino energy of 6.3…IceCube Collaboration, M. G. Aartsen, R. Abbasi et al.·Oct 21, 2021SaveLearn
Beyond the Standard Model Searches with the Majorana Demonstrator ExperimentThe Majorana Demonstrator experiment operated two modular arrays of p-type point contact high purity germanium (HPGe) detectors, of which 30 kg is enriched to 88% in Ge-76, to search for neutrinoless…Wenqin Xu·Oct 21, 2021SaveLearn
Convolutional Neural Networks for Shower Energy Prediction in Liquid Argon Time Projection ChambersWhen electrons with energies of O(100) MeV pass through a liquid argon time projection chamber (LArTPC), they deposit energy in the form of electromagnetic showers. Methods to reconstruct the…Kiara Carloni, Nicholas W. Kamp, Austin Schneider et al.·Oct 20, 2021SaveLearn
Search for dark photons using a multilayer dielectric haloscope equipped with a single-photon avalanche diodeWe report on the results of the search for dark photons with mass around 1.5\, eV/c2 using a multilayer dielectric haloscope equipped with an affordable and commercially available photosensor.…Laura Manenti, Umang Mishra, Gianmarco Bruno et al.·Oct 20, 2021SaveLearn
A Neural-Network-defined Gaussian Mixture Model for particle identification applied to the LHCb fixed-target programmeParticle identification in large high-energy physics experiments typically relies on classifiers obtained by combining many experimental observables. Predicting the probability density function (pdf)…Giacomo Graziani, Lucio Anderlini, Saverio Mariani et al.·Oct 19, 2021SaveLearn
Water jet space charge spectroscopy: Route to direct measurement of electron dynamics for organic systems in their natural environmentThe toolbox for time-resolved direct measurements of electron dynamics covers a variety of methods. Since the experimental effort is increasing rapidly with achievable time resolution, there is an…Michael Mittermair, Felix Martin, Martin Wörle et al.·Oct 19, 2021SaveLearn
Tests of lepton universality using B0 K0S + - and B+ K*+ + - decaysTests of lepton universality in B0 K0S + - and B+ K*+ + - decays where is either an electron or a muon are presented. The differential branching fractions…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Oct 18, 2021SaveLearn
JUNO Non-oscillation PhysicsThe JUNO observatory, a 20 kt liquid scintillator detector to be completed in 2022 in China, belongs to the next-generation of neutrino detectors, which share the common features of having a…Giulio Settanta·Oct 18, 2021SaveLearn
Feasibility Study of Ds+ τ+ τ Decay and Test of Lepton Flavor Universality with Leptonic Ds+ Decays at STCFWe report a sensitive study of Ds+ τ+ τ decay via τ+ e+ e τ with an integrated luminosity of 1 ab-1 at the center-of-mass energy of 4.009 GeV…Huijing Li, Tao Luo, Xiaodong Shi et al.·Oct 17, 2021SaveLearn
Spin Physics Detector project at JINRThe Spin Physics Detector at the constructing NICA collider (JINR, Dubna) is a universal facility to investigate the spin structure of the proton and deuteron and the other spin-related phenomena…Alexey Guskov·Oct 17, 2021SaveLearn
Dark Matter Axion Search Using a Josephson Traveling Wave Parametric AmplifierWe present a new exclusion bound of axion-like particle dark matter with axion-photon couplings above 10-13 GeV-1 over the frequency range 4796.7--4799.5 MHz,…C. Bartram, T. Braine, R. Cervantes et al.·Oct 15, 2021SaveLearn
Machine Learning for the LHCb SimulationMost of the computing resources pledged to the LHCb experiment at CERN are necessary to the production of simulated samples used to predict resolution functions on the reconstructed quantities and…Lucio Anderlini·Oct 15, 2021SaveLearn
Measurements of the branching fractions for B K*γ decays at Belle IIThis paper reports a study of B K*γ decays using 62.8 0.6 fb-1 of data collected during 2019--2020 by the Belle II experiment at the SuperKEKB e+e- asymmetric-energy…F. Abudinén, I. Adachi, R. Adak et al.·Oct 15, 2021SaveLearn
SHADOWS (Search for Hidden And Dark Objects With the SPS)We propose a new beam-dump experiment, SHADOWS, to search for a large variety of feebly-interacting particles possibly produced in the interactions of a 400 GeV proton beam with a high-Z material…W. Baldini, A. Balla, J. Bernhard et al.·Oct 15, 2021SaveLearn
Measurement of the Coherent Elastic Neutrino-Nucleus Scattering Cross Section on CsI by COHERENTWe measured the cross section of coherent elastic neutrino-nucleus scattering () using a CsI[Na] scintillating crystal in a high flux of neutrinos produced at the Spallation Neutron Source…D. Akimov, P. An, C. Awe et al.·Oct 14, 2021SaveLearn
Study of the decay Ds+ KS0KS0π+ and observation an isovector partner to f0(1710)Using e+e- annihilation data corresponding to a total integrated luminosity of 6.32 fb-1 collected at center-of-mass energies between 4.178 and 4.226 GeV with the BESIII detector, we…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 14, 2021SaveLearn
Transverse single spin asymmetries of forward neutrons in p+p, p+Al, and p+Au collisions at s_NN=200 GeV as a function of transverse and longitudinal momentaIn 2015 the PHENIX collaboration at the Relativistic Heavy Ion Collider recorded p+p, p+Al, and p+Au collision data at center of mass energies of s_NN=200 GeV with the…U. A. Acharya, C. Aidala, Y. Akiba et al.·Oct 14, 2021SaveLearn
Search for massive long-lived particles decaying semileptonically at sqrt(s)=13 TeVA search is performed for massive long-lived particles (LLP) decaying semileptonically into a muon and two quarks. Two kinds of LLP production processes were considered. In the first, a Higgs-like…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Oct 14, 2021SaveLearn
Muon to positron conversionLepton flavor violation (LFV) has been discovered in the neutrino sector by neutrino oscillation experiments. The minimally extended Standard Model (SM) to include neutrino masses allows LFV in the…MyeongJae Lee, Michael MacKenzie·Oct 14, 2021SaveLearn
Search for invisible decays of the baryonA search for invisible decays of the baryon is carried out in the process J/ based on (1.00870.0044)×1010 J/ events collected with the BESIII…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 13, 2021SaveLearn
Collective phenomena in pp interactions with high multiplicityThe latest results on the search for collective phenomena in pp interactions at the U-70 accelerator at IHEP (Protvino) are presented. This the long-term experiment has been carried out at the SVD-2…N. Barlykov, V. Dudin, V. Dunin et al.·Oct 13, 2021SaveLearn
Search for "Invisible" Axion Dark Matter in the 3.3-4.2~μeV Mass RangeWe report the results from a haloscope search for axion dark matter in the 3.3-4.2~μeV mass range. This search excludes the axion-photon coupling predicted by one of the benchmark models of…ADMX Collaboration, C. Bartram, T. Braine et al.·Oct 12, 2021SaveLearn
First search for exclusive diphoton production at high mass with tagged protons in proton-proton collisions at s = 13 TeVA search for exclusive two-photon production via photon exchange in proton-proton collisions, pp pγγp with intact protons, is presented. The data correspond to an integrated…CMS, TOTEM Collaborations·Oct 12, 2021SaveLearn
Searching for low-mass dark matter via Migdal effect in COSINE-100We report on the search for weakly interacting massive particle (WIMP) dark matter candidates in the galactic halo that interact with sodium and iodine nuclei in the COSINE-100 experiment and produce…G. Adhikari, N. Carlin, J. J. Choi et al.·Oct 12, 2021SaveLearn
Study of the process e+e- ηηγ in the energy range s = 1.17--2.00 GeV with the SND detectorThe process e+e-ηηγ is studied in the center-of-mass energy range 1.17-2.00 GeV using data with an integrated luminosity of 201 pb-1collected by the SND detector at the VEPP-2000 e+e-…SND Collaboration, M. N. Achasov, A. Yu. Barnyakov et al.·Oct 12, 2021SaveLearn