Search for a new resonance decaying into two spin-0 bosons in a final state with two photons and two bottom quarks in proton-proton collisions at s = 13 TeVA search for a new boson X is presented using CERN LHC proton-proton collision data collected by the CMS experiment at s = 13 TeV in 2016-2018, and corresponding to an integrated luminosity…CMS Collaboration·Oct 2, 2023SaveLearn
Measurement of t-channel single-top-quark production in pp collisions at s = 5.02 TeV with the ATLAS detectorThe observation of the electroweak production of single-top-quarks is made using 255 pb-1 of proton-proton collision data recorded at s = 5.02 TeV with the ATLAS detector at the…ATLAS Collaboration·Oct 2, 2023SaveLearn
Determination of |Vcb| using B0 D*+- decays with Belle IIWe determine the CKM matrix-element magnitude |Vcb| using B0 D*+- decays reconstructed in 189 \, fb-1 of collision data collected by the Belle…Belle II Collaboration, I. Adachi, K. Adamczyk et al.·Oct 2, 2023SaveLearn
Exclusion of ALP Cogenesis Dark Matter in a Mass Window Above 100 μeVWe report the results of Phase 1b of The ORGAN Experiment, a microwave cavity haloscope searching for dark matter axions in the 107.42-111.93~μeV mass range. The search excludes axions with…Aaron Quiskamp, Ben T. McAllister, Paul Altin et al.·Oct 2, 2023SaveLearn
Design Challenges for a Future Liquid Xenon ObservatoryAn ultimate liquid xenon experiment would be limited in its dark matter science reach by irreducible neutrino backgrounds, which are an exciting signal in their own right. To achieve such…Abigail Kopec·Oct 1, 2023SaveLearn
Ecological transition for the gas mixtures of the MRPC cosmic ray telescopes of the EEE ProjectThe Extreme Energy Events (EEE) Collaboration is fully involved in an ecological transition. The use of the standard gas mixture, C2H2F4+ SF6, has stopped in favor of an…C. Ripoli, M. Abbrescia, C. Avanzini et al.·Sep 29, 2023SaveLearn
Polyglot Jet FindingThe evaluation of new computing languages for a large community, like HEP, involves comparison of many aspects of the languages' behaviour, ecosystem and interactions with other languages. In this…Graeme Andrew Stewart, Philippe Gras, Benedikt Hegner et al.·Sep 29, 2023SaveLearn
Measurement of the production cross-section of J/ and (2S) mesons in pp collisions at s = 13 TeV with the ATLAS detectorMeasurements of the differential production cross-sections of prompt and non-prompt J/ and (2S) mesons with transverse momenta between 8 and 360 GeV and rapidity in the range |y|<2…ATLAS Collaboration·Sep 29, 2023SaveLearn
Search for supersymmetry in final states with disappearing tracks in proton-proton collisions at s = 13 TeVA search is presented for charged, long-lived supersymmetric particles in final states with one or more disappearing tracks. The search is based on data from proton-proton collisions at a…CMS Collaboration·Sep 28, 2023SaveLearn
Results on Elastic Cross Sections in Proton-Proton Collisions at s = 510 GeV with the STAR Detector at RHICWe report results on an elastic cross section measurement in proton-proton collisions at a center-of-mass energy s=510 GeV, obtained with the Roman Pot setup of the STAR experiment at the…STAR Collaboration, M. I. Abdulhamid, B. E. Aboona et al.·Sep 28, 2023SaveLearn
Search for direct production of GeV-scale resonances decaying to a pair of muons in proton-proton collisions at s = 13 TeVA search for direct production of low-mass dimuon resonances is performed using s = 13 TeV proton-proton collision data collected by the CMS experiment during the 2017-2018 operation of the…CMS Collaboration·Sep 27, 2023SaveLearn
Search for the exclusive W boson hadronic decays Wπγ, W Kγ and W^γ with the ATLAS detectorA search for the exclusive hadronic decays W πγ, W Kγ and W γ is performed using up to 140\, fb-1 of proton-proton…ATLAS Collaboration·Sep 27, 2023SaveLearn
MicroBooNE Public Data Sets: a Collaborative Tool for LArTPC Software DevelopmentAmong liquid argon time projection chamber (LArTPC) experiments MicroBooNE is the one that continually took physics data for the longest time (2015-2021), and represents the state of the art for…Giuseppe Cerati·Sep 27, 2023SaveLearn
Experimental Limits on Solar Reflected Dark Matter with a New Approach on Accelerated-Dark-Matter-Electron Analysis in SemiconductorsRecently a dark matter-electron (DM-electron) paradigm has drawn much attention. Models beyond the standard halo model describing DM accelerated by high energy celestial bodies are under intense…Z. Y. Zhang, L. T. Yang, Q. Yue et al.·Sep 26, 2023SaveLearn
Multi-Messenger Measurements of the Static Structure of Shock-Compressed Liquid Silicon at 100 GPaIonic structure of high pressure, high temperature fluids is a challenging theoretical problem with applications to planetary interiors and fusion capsules. Here we report a multi-messenger platform…H. Poole, M. K. Ginnane, M. Millot et al.·Sep 26, 2023SaveLearn
Fraction Constraint in Partial Wave AnalysisTo resolve the non-convex optimization problem in partial wave analysis, this paper introduces a novel approach that incorporates fraction constraints into the likelihood function. This method offers…Xiang Dong, Chu-Cheng Pan, Yu-Chang Sun et al.·Sep 26, 2023SaveLearn
Updated measurements of the M1 transition (3686) γ ηc(2S) with ηc(2S) K K πBased on a data sample of (27.08 0.14 ) × 108~(3686) events collected with the BESIII detector at the BEPCII collider, the M1 transition (3686) γ ηc(2S) with…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 26, 2023SaveLearn
Investigation of the I = 1/2 rule and test of CP violation through the measurement of decay asymmetry parameters in - decaysUsing (1008744)× 106 J/ events collected with the BESIII detector, numerous - and decay asymmetry parameters are simultaneously determined from the process $J/…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 26, 2023SaveLearn
Software Citation in HEP: Current State and Recommendations for the FutureIn November 2022, the HEP Software Foundation and the Institute for Research and Innovation for Software in High-Energy Physics organized a workshop on the topic of Software Citation and Recognition…Matthew Feickert, Daniel S. Katz, Mark S. Neubauer et al.·Sep 25, 2023SaveLearn
Inclusive and differential cross section measurements of ttbb production in the lepton+jets channel at s = 13 TeVMeasurements of inclusive and normalized differential cross sections of the associated production of top quark-antiquark and bottom quark-antiquark pairs, ttbb, are presented. The results are based…CMS Collaboration·Sep 25, 2023SaveLearn
Longitudinal and transverse spin transfer to and hyperons in polarized p+p collisions at s = 200 GeVThe longitudinal and transverse spin transfers to () hyperons in polarized proton-proton collisions are expected to be sensitive to the helicity and transversity…STAR Collaboration, M. I. Abdulhamid, B. E. Aboona et al.·Sep 25, 2023SaveLearn
Measurement of prompt D+ and D+s production in pPb collisions at sNN=5.02\,TeVThe production of prompt D+ and D+s mesons is studied in proton-lead collisions at a centre-of-mass energy of sNN=5.02\,TeV. The data sample corresponding to an…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Sep 25, 2023SaveLearn
Challenges for the directional dark matter direct detectionDirectional methods have been considered to provide a solid proof for the direct detection of the dark matter. Gaseous time-projection-chambers (TPCs) are the most mature devices for directional dark…Kentaro Miuchi·Sep 25, 2023SaveLearn
Measurement of the e+e- KS0 KL0 π0 cross sections from s= 2.000 to 3.080 GeVBased on e+e- collision data collected at center-of-mass energies from 2.000 to 3.080 GeV by the BESIII detector at the BEPCII collider, a partial wave analysis is performed for the process…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 25, 2023SaveLearn
Observation of (3686) → η decayUsing a sample of (27.12 0.14) × 108 (3686) events collected with the BESIII detector, the decay (3686) η' with η' subsequently decaying…M. Ablikim·Sep 25, 2023SaveLearn