Search for e+e- K+ K- (3770) at center-of-mass energies from 4.84 to 4.95 GeVUsing e+e- collision data, corresponding to an integrated luminosity of 892\, pb-1 collected at center-of-mass energies from 4.84 to 4.95\,GeV with the BESIII detector, we search for the…BESIII Collaboration·Apr 18, 2024SaveLearn
Top-quark spin properties at LHCDue to its high mass top quarks decay before top-flavoured hadrons can be formed. This feature yields experimental access to the top quark polarization and production asymmetries. The large top quark…Nello Bruscino·Apr 17, 2024SaveLearn
Strategies for Machine Learning Applied to Noisy HEP Datasets: Modular Solid State Detectors from SuperCDMSBackground reduction in the SuperCDMS dark matter experiment depends on removing surface events within individual detectors by identifying the location of each incident particle interaction. Position…P. B. Cushman, M. C. Fritts, A. D. Chambers et al.·Apr 17, 2024SaveLearn
First double-differential cross section measurement of neutral-current π0 production in neutrino-argon scattering in the MicroBooNE detectorWe report the first double-differential cross section measurement of neutral-current neutral pion (NCπ0) production in neutrino-argon scattering, as well as single-differential measurements of…MicroBooNE collaboration, P. Abratenko, O. Alterkait et al.·Apr 16, 2024SaveLearn
Measurement of the branching fraction of the decay B- D0 (770)- at Belle IIWe measure the branching fraction of the decay B- D0 (770)- using data collected with the Belle II detector. The data contain 387 million BB pairs produced in e+e-…Belle II Collaboration, I. Adachi, L. Aggarwal et al.·Apr 16, 2024SaveLearn
Climbing to the Top of the ATLAS 13 TeV dataThe large amount of data recorded with the ATLAS detector at the Large Hadron Collider, corresponding to 140 fb-1 of pp collisions at a centre-of-mass energy of s=13 TeV, has brought…ATLAS Collaboration·Apr 16, 2024SaveLearn
Calibration of the Cryogenic Measurement System of a Resonant Haloscope CavityPossible light bosonic dark matter interactions with the Standard Model photon have been searched by microwave resonant cavities. In this paper, we demonstrate the cryogenic readout system…Dong He, Jie Fan, Xin Gao et al.·Apr 16, 2024SaveLearn
Measurement of the differential cross section for neutral pion production in charged-current muon neutrino interactions on argon with the MicroBooNE detectorWe present a measurement of neutral pion production in charged-current interactions using data recorded with the MicroBooNE detector exposed to Fermilab's booster neutrino beam. The signal comprises…MicroBooNE collaboration, P. Abratenko, O. Alterkait et al.·Apr 15, 2024SaveLearn
Combined Pre-Supernova Alert System with Kamland and Super-KamiokandePreceding a core-collapse supernova, various processes produce an increasing amount of neutrinos of all flavors characterized by mounting energies from the interior of massive stars. Among them, the…KamLAND, Super-Kamiokande Collaborations, : et al.·Apr 15, 2024SaveLearn
First search for light fermionic dark matter absorption on electrons using germanium detector in CDEX-10 experimentWe present the first results of the search for sub-MeV fermionic dark matter absorbed by electron targets of germanium using the 205.4~kg·day data collected by the CDEX-10 experiment, with the…J. X. Liu, L. T. Yang, Q. Yue et al.·Apr 15, 2024SaveLearn
Observation of D a0(980)π in the decays D0 → π+π-η and D+ → π+π0ηWe report the first amplitude analysis of the decays D0 π+ π- η and D+ → π+π0η using a data sample taken with the BESIII detector at the…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Apr 14, 2024SaveLearn
First combined tuning on transverse kinematic imbalance data with and without pion production constraintsWe present the first combined tuning, using GENIE, of four transverse kinematic imbalance measurements of neutrino-hydrocarbon scattering, both with and without pion final states, from the T2K and…Weijun Li, Marco Roda, Julia Tena-Vidal et al.·Apr 12, 2024SaveLearn
Search for Higgs boson pair production with one associated vector boson in proton-proton collisions at s = 13 TeVA search for Higgs boson pair (HH) production in association with a vector boson V (W or Z boson) is presented. The search is based on proton-proton collision data at a center-of-mass energy of 13…CMS Collaboration·Apr 12, 2024SaveLearn
Technical Design Report of the Spin Physics Detector at NICAThe Spin Physics Detector collaboration proposes to install a universal detector in the second interaction point of the NICA collider under construction (JINR, Dubna) to study the spin structure of…The SPD Collaboration, V. Abazov, V. Abramov et al.·Apr 12, 2024SaveLearn
Search for Rare b d+- Transitions at BelleWe present the results of a search for the b d+- flavor-changing neutral-current rare decays B+, 0 (η, ω, π+,0, +, 0) e+e- and $B+, 0 (η,…Belle, Belle II Collaborations, : et al.·Apr 11, 2024SaveLearn
Silicon-Photomultiplier (SiPM) Protection Against Over-Current and Over-IlluminationSiPMs operate in Geiger mode, wherein photodiode cells are reverse-biased to the breakdown by even a single photon. Each cell is connected in series with a quenching resistor, which prevents cell…Gholamreza Fardipour Raki, Mohsen Khakzad·Apr 11, 2024SaveLearn
Thirty years of the Beauty ConferenceThis paper remembers thirty years of the Beauty conference series and celebrates its 20th meeting. The conference highlights are reviewed.Neville Harnew·Apr 11, 2024SaveLearn
Measurement of e+e- ωη cross sections at s= 2.000 to 3.080 GeVThe Born cross sections for the process e+e- ωη are measured at 22 center-of-mass energies from 2.000 to 3.080 GeV using data collected with the BESIII detector at the…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Apr 11, 2024SaveLearn
Search for prompt production of pentaquarks in charm hadron final statesA search for hidden-charm pentaquark states decaying to a range of cD and cD final states, as well as doubly-charmed pentaquark states to cD and…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Apr 10, 2024SaveLearn
First constraints on the Lμ-Lτ explanation of the muon g-2 anomaly from NA64-e at CERNThe inclusion of an additional U(1) gauge Lμ-Lτ symmetry would release the tension between the measured and the predicted value of the anomalous muon magnetic moment: this paradigm assumes…Yu. M. Andreev, A. Antonov, D. Banerjee et al.·Apr 10, 2024SaveLearn
Electroweak, QCD and flavour physics studies with ATLAS data from Run 2 of the LHCA summary of precision measurements sensitive to electroweak, QCD and quark-flavour effects performed by the ATLAS Collaboration at the Large Hadron Collider is reported. The measurements are…ATLAS Collaboration·Apr 10, 2024SaveLearn
Measurement of the Born cross section for e+e- η hc at center-of-mass energies between 4.1 and 4.6\,GeVWe measure the Born cross section for the reaction e+e- → η hc from s = 4.129 to 4.600~GeV using data sets collected by the BESIII detector running at the BEPCII…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Apr 10, 2024SaveLearn
A Beehive Haloscope for High-mass Axion Dark MatterWe propose a new haloscope geometry that can arbitrarily increase the resonator volume for a given target axion mass. This geometry consists of closely packed, overlapping coaxial cavities operating…Matthew O. Withers, Chao-Lin Kuo·Apr 9, 2024SaveLearn
Software and computing for Run 3 of the ATLAS experiment at the LHCThe ATLAS experiment has developed extensive software and distributed computing systems for Run 3 of the LHC. These systems are described in detail, including software infrastructure and workflows,…ATLAS Collaboration·Apr 9, 2024SaveLearn
Precise measurements of W- and Z-boson transverse momentum spectra with the ATLAS detector using pp collisions at s = 5.02 TeV and 13 TeVThis paper describes measurements of the transverse momentum spectra of W and Z bosons produced in proton-proton collisions at centre-of-mass energies of s=5.02 TeV and s=13 TeV…ATLAS Collaboration·Apr 9, 2024SaveLearn