Model Independent Approach of the JUNO 8B Solar Neutrino ProgramThe physics potential of detecting 8B solar neutrinos will be exploited at the Jiangmen Underground Neutrino Observatory (JUNO), in a model independent manner by using three distinct channels of…JUNO Collaboration, Jie Zhao, Baobiao Yue et al.·Oct 16, 2022SaveLearn
Azimuthal anisotropy of dijet events in PbPb collisions at sNN = 5.02 TeVThe path-length dependent parton energy loss within the dense partonic medium created in lead-lead collisions at a nucleon-nucleon center-of-mass energy of sNN = 5.02 TeV is…CMS Collaboration·Oct 15, 2022SaveLearn
Strangeness production in small-collision systems with ALICEWe present the new studies which are performed with the aim of better understanding the production mechanisms for strange particles, and hence the strangeness enhancement phenomenon, in…Anju Bhasin, Meenakshi Sharma·Oct 15, 2022SaveLearn
Stereo neutrino spectrum of 235U fission rejects sterile neutrino hypothesisAnomalies in past neutrino measurements have led to the discovery that these particles have non-zero mass and oscillate between their three flavors when they propagate. In the 2010's, similar…H. Almazán, L. Bernard, A. Blanchet et al.·Oct 14, 2022SaveLearn
Effective field theory and inelastic dark matter results from XENON1TIn this work, we expand on the XENON1T nuclear recoil searches to study the individual signals of dark matter interactions from operators up to dimension-eight in a Chiral Effective Field Theory…E. Aprile, K. Abe, F. Agostini et al.·Oct 14, 2022SaveLearn
An approximate likelihood for nuclear recoil searches with XENON1T dataThe XENON collaboration has published stringent limits on specific dark matter -nucleon recoil spectra from dark matter recoiling on the liquid xenon detector target. In this paper, we present an…E. Aprile, K. Abe, F. Agostini et al.·Oct 13, 2022SaveLearn
Status of DMRadio-50L and DMRadio-m3Recent theoretical advancements have made the QCD axion a stronger dark matter candidate, especially in the sub-μeV range. While cavity haloscopes have made significant progress in…Nicholas M. Rapidis·Oct 13, 2022SaveLearn
Measurement of e+ e- → φ η cross sections at center-of-mass energies between 3.508 and 4.600 GeVWe present a measurement of the dressed cross sections for e+ e- → φ η at different center-of-mass energies between 3.508 and 4.600 GeV based on 15.1 fb-1 of $e+…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 13, 2022SaveLearn
Measurement of the c+ to D0 production cross-section ratio in peripheral PbPb collisionsWe report on a measurement of the c+ to D0 production ratio in PbPb collisions at s NN= 5.02 TeV with the LHCb detector in the forward rapidity region 2 <y< 4.5. The…LHCb collaboration·Oct 13, 2022SaveLearn
Deep generative models for fast photon shower simulation in ATLASThe need for large-scale production of highly accurate simulated event samples for the extensive physics programme of the ATLAS experiment at the Large Hadron Collider motivates the development of…ATLAS Collaboration·Oct 12, 2022SaveLearn
Proton reconstruction with the CMS-TOTEM Precision Proton SpectrometerThe Precision Proton Spectrometer (PPS) of the CMS and TOTEM experiments collected 107.7 fb-1 in proton-proton (pp) collisions at the LHC at 13 TeV (Run 2). This paper describes the key features…CMS, TOTEM Collaborations·Oct 12, 2022SaveLearn
The Future of High Energy Physics Software and ComputingSoftware and Computing (S&C) are essential to all High Energy Physics (HEP) experiments and many theoretical studies. The size and complexity of S&C are now commensurate with that of experimental…V. Daniel Elvira, Steven Gottlieb, Oliver Gutsche et al.·Oct 11, 2022SaveLearn
The DAMIC-M Experiment: Status and First ResultsThe DAMIC-M (DArk Matter In CCDs at Modane) experiment employs thick, fully depleted silicon charged-coupled devices (CCDs) to search for dark matter particles with a target exposure of 1 kg-year. A…I. Arnquist, N. Avalos, P. Bailly et al.·Oct 11, 2022SaveLearn
Search for Higgs boson pair production in association with a vector boson in pp collisions at s= 13 TeV with the ATLAS detectorThis paper reports a search for Higgs boson pair (hh) production in association with a vector boson (W or Z) using 139 fb-1 of proton-proton collision data at s= 13 TeV recorded…ATLAS Collaboration·Oct 11, 2022SaveLearn
Directional Neutrino Searches for Galactic Center Dark Matter at Large Underground LArTPCsWe investigate the sensitivity of a large, underground LArTPC-based neutrino detector to dark matter in the Galactic Center annihilating into neutrinos. Such a detector could have the ability to…Matthew R. Buckley, Andrew Mastbaum, Gopolang Mohlabeng·Oct 10, 2022SaveLearn
Report of the Frontier For Rare Processes and Precision MeasurementsThis is the Snowmass 2021 Rare and Precision Frontier Report. The Rare Processes and Precision Measurements Frontier, referred to as the ``Rare and Precision Frontier", or RPF, encompasses searches…Marina Artuso, Robert H. Bernstein, Alexey A. Petrov·Oct 10, 2022SaveLearn
Search for pair-produced scalar and vector leptoquarks decaying into third-generation quarks and first- or second-generation leptons in pp collisions with the ATLAS detectorA search for pair-produced scalar and vector leptoquarks decaying into quarks and leptons of different generations is presented. It uses the full LHC Run 2 (2015-2018) data set of 139 fb-1…ATLAS Collaboration·Oct 10, 2022SaveLearn
Multiplicity dependence of charged-particle jet production in pp collisions at 13 TeV with ALICEMeasurements of jet production and jet properties in pp collisions provide a test of perturbative quantum chromodynamics (pQCD) and form a baseline for similar measurements in heavy ion (A--A)…Debjani Banerjee·Oct 10, 2022SaveLearn
A Detailed Study of Interpretability of Deep Neural Network based Top TaggersRecent developments in the methods of explainable AI (XAI) allow researchers to explore the inner workings of deep neural networks (DNNs), revealing crucial information about input-output…Ayush Khot, Mark S. Neubauer, Avik Roy·Oct 9, 2022SaveLearn
Determination of |Vub| from untagged B0π- + decays using 2019-2021 Belle II dataWe present an analysis of the charmless semileptonic decay B0π- + , where = e, μ, from 198.0 million pairs of BB mesons recorded by the Belle II detector at…Belle II Collaboration, K. Adamczyk, L. Aggarwal et al.·Oct 9, 2022SaveLearn
Observations of the Cabibbo-Suppressed decays c+ nπ+π0, nπ+π-π+ and the Cabibbo-Favored decay c+ nK-π+π+Using electron-positron annihilation data samples corresponding to an integrated luminosity of 4.5 fb-1, collected by the BESIII detector in the energy region between 4600 MeV and…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 7, 2022SaveLearn
Snowmass 2021 Topical Report on Synergies in Research at Underground FacilitiesThis is a Snowmass 2021 Topical Report for the Underground Facilities and Infrastructure Frontier on Synergies in Research at Underground Facilities: A broad range of scientific and engineering…Catalina Curceanu, Derek Elsworth, Joe Formaggio et al.·Oct 6, 2022SaveLearn
Search for a heavy composite Majorana neutrino in events with dilepton signatures from proton-proton collisions at s = 13 TeVResults are presented of a search for a heavy Majorana neutrino N decaying into two same-flavor leptons (electrons or muons) and a quark-pair jet. A model is considered in which the…CMS Collaboration·Oct 6, 2022SaveLearn
SND@LHC: The Scattering and Neutrino Detector at the LHCSND@LHC is a compact and stand-alone experiment designed to perform measurements with neutrinos produced at the LHC in the pseudo-rapidity region of 7.2 < η < 8.4. The experiment is located…LHC Collaboration·Oct 6, 2022SaveLearn
Precision measurements of jet and photon production at the ATLAS experimentThe production of jets and prompt isolated photons at hadron colliders provides stringent tests of perturbative QCD. We present the latest measurements of photon+jets and diphoton production using…Giuseppe Callea·Oct 5, 2022SaveLearn