Track-based alignment for the BESIII CGEM detector in the cosmic-ray testThe Beijing Electron Spectrometer III (BESIII) is a multipurpose detector operating on the Beijing Electron Positron Collider II (BEPCII). After more than ten year's operation, the efficiency of the…A. Q. Guo, L. H. Wu, L. L. Wang et al.·Nov 2, 2022SaveLearn
Study of the B- c+ c- K- decayThe decay B- c+ c- K- is studied in proton-proton collisions at a center-of-mass energy of s=13 TeV using data corresponding to an integrated…LHCb collaboration·Nov 2, 2022SaveLearn
Exploration of different parameter optimization algorithms within the context of ACTS software frameworkParticle track reconstruction, in which the trajectories of charged particles are determined, is a critical and time consuming component of the full event reconstruction chain. The underlying…Rocky Bala Garg, Elyssa Hofgard, Lauren Tompkins et al.·Nov 1, 2022SaveLearn
Construction of Precision sMDT Detector for ATLAS Muon Spectrometer UpgradeThis paper describes the small-diameter monitored drift-tube detector construction at the University of Michigan as a contribution to the ATLAS Muon Spectrometer upgrade for the high-luminosity Large…D. Amidei, N. Anderson, A. Chen et al.·Nov 1, 2022SaveLearn
FASER Tracker Detector Commissioning, Installation, and FunctionalityFASER (ForwArd Search ExpeRiment) fills the axial blindspot of other, radially arranged LHC experiments. It is installed 480 meters from the ATLAS interaction point, along the collision axis. FASER…Savannah Shively·Nov 1, 2022SaveLearn
Measurements of K0S, and production in 120 GeV/c p + C interactionsThis paper presents multiplicity measurements of K0S, , and produced in 120 GeV/c proton-carbon interactions. The measurements were made using data collected…SHINE Collaboration, H. Adhikary, K. K. Allison et al.·Oct 31, 2022SaveLearn
Collins and Sivers transverse-spin asymmetries in inclusive muoproduction of 0 mesonsThe production of vector mesons in deep inelastic scattering is an interesting yet scarsely explored channel to study the transverse spin structure of the nucleon and the related phenomena. The…G. D. Alexeev, M. G. Alexeev, C. Alice et al.·Oct 31, 2022SaveLearn
Advanced LIGO, LISA, and Cosmic Explorer as dark matter transducersWe present a method to search for scalar field ultralight dark matter directly interacting with gravitational-wave interferometers via a modulation of the fine structure constant and the electron…Evan Hall, Nancy Aggarwal·Oct 31, 2022SaveLearn
Spin Density Matrix Elements in Exclusive 0 Meson MuoproductionWe report on a measurement of Spin Density Matrix Elements (SDMEs) in hard exclusive 0 meson muoproduction at COMPASS using 160~GeV/c polarised μ + and μ - beams impinging…G. D. Alexeev, M. G. Alexeev, C. Alice et al.·Oct 30, 2022SaveLearn
Study of e+e- → 0 0 and +- by Initial State Radiation Method at BelleThe processes e+e-→ 00 and e+e-→+- are studied using initial-state-radiation events in a sample of 980…Belle Collaboration, G. Gong, L. K. Li et al.·Oct 30, 2022SaveLearn
Correlation of heavy-flavour hadron production and charged-particle multiplicity in pp collisions measured by ALICEHeavy-flavour (HF) quarks, i.e. charm and beauty, are produced in the early stages of ultra-relativistic collisions via hard scattering processes. The measurement of heavy flavour as a function of…ALICE Collaboration, Joyful Elma Mdhluli·Oct 29, 2022SaveLearn
Azimuthal correlations in Z+jets events in proton-proton collisions at s = 13 TeVThe production of Z bosons associated with jets is measured in pp collisions at s = 13 TeV with data recorded with the CMS experiment at the LHC corresponding to an integrated luminosity of…CMS Collaboration·Oct 28, 2022SaveLearn
Measurement of T-odd asymmetry in radiative K+ -> pi0 e+ nu gamma decay using OKA detectorThe paper presents a measurement of the T-odd correlation in radiation decay K+ → π0 e+ e γ performed on the installation of the 101200 candidate events of…A. Yu. Polyarush, S. A. Akimenko, A. V. Artamonov et al.·Oct 27, 2022SaveLearn
NaNu: Proposal for a Neutrino Experiment at the SPS Collider located at the North Area of CERNSeveral experiments have been proposed in the recent years to study the nature of tau neutrinos, in particular aiming for a first observation of tau anti-neutrinos, more stringent upper limit on its…Friedemann Neuhaus, Matthias Schott, Chen Wang et al.·Oct 27, 2022SaveLearn
Timing and Synchronization of the DUNE Neutrino DetectorThe DUNE neutrino experiment far detector has a fiducial mass of 40 kt. The O(1M) readout channels are distributed over the four 10 kt modules and need to be synchronized with respect to each other…A. Barcock, D. Cussans, D. Lindebaum et al.·Oct 27, 2022SaveLearn
Search for pair-production of vector-like quarks in pp collision events at s=13 TeV with at least one leptonically decaying Z boson and a third-generation quark with the ATLAS detectorA search for the pair-production of vector-like quarks optimized for decays into a Z boson and a third-generation Standard Model quark is presented, using the full Run 2 dataset corresponding to…ATLAS Collaboration·Oct 27, 2022SaveLearn
Observation of a resonant structure near the Ds+ Ds- threshold in the B+ Ds+ Ds- K+ decayAn amplitude analysis of the B+ Ds+ Ds- K+ decay is carried out to study for the first time its intermediate resonant contributions, using proton-proton collision data collected with the…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Oct 27, 2022SaveLearn
Observation of the B0s\! D*+D*- decayThe first observation of the B0s\! D*+D*- decay and the measurement of its branching ratio relative to the B0\! D*+D*- decay are presented. The data sample used corresponds…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Oct 26, 2022SaveLearn
Cross-section measurement of two-photon annihilation in-flight of positrons at s=20 MeV with the PADME detectorThe inclusive cross-section of annihilation in flight e+e-→γγ of 430 MeV positrons with atomic electrons of a thin diamond target has been measured with the PADME detector at…F. Bossi, P. Branchini, B. Buonomo et al.·Oct 26, 2022SaveLearn
A multidimensional study of the structure function ratio σLT'/σ0 from hard exclusive π+ electro-production off protons in the GPD regimeA multidimensional extraction of the structure function ratio σLT'/σ0 from the hard exclusive e p e n π+ reaction above the resonance region has been…S. Diehl, A. Kim, K. Joo et al.·Oct 26, 2022SaveLearn
The Mu2e Experiment -- Searching for Charged Lepton Flavor ViolationThe Mu2e experiment will search for a Standard Model violating rate of neutrinoless conversion of a muon into an electron in the presence of an aluminum nucleus. Observation of this charged lepton…Michael Thomas Hedges·Oct 25, 2022SaveLearn
Rare decays at LHCbFlavour-changing neutral-current processes, such as b s +-, are forbidden at tree level in the Standard Model and hence might receive comparatively large corrections from new…M. Santimaria·Oct 25, 2022SaveLearn
The LHCspin projectThe goal of LHCspin is to develop, in the next few years, innovative solutions and cutting-edge technologies to access spin physics in polarised fixed-target collisions at high energy, exploring the…M. Santimaria, V. Carassiti, G. Ciullo et al.·Oct 25, 2022SaveLearn
Revision of results on (1S), (2S), and (3S) massesWe have reconsidered the results on the masses of the narrow bottomonium states (1S)--(3S) obtained in 1982--1986 at CESR, DORIS and VEPP-4 colliders in order to fix shortcomings…A. G. Shamov, O. L. Rezanova·Oct 25, 2022SaveLearn
Search for central exclusive production of top quark pairs with the CMS and TOTEM experimentsA search for central exclusive production of top quark pairs (tt) is presented using collision data collected by CMS and the CMS-TOTEM Precision Proton Spectrometer in 2017.…Beatriz Ribeiro Lopes·Oct 25, 2022SaveLearn