Electron Energy Regression in the CMS High-Granularity Calorimeter PrototypeWe present a new publicly available dataset that contains simulated data of a novel calorimeter to be installed at the CERN Large Hadron Collider. This detector will have more than six-million…Roger Rusack, Bhargav Joshi, Alpana Alpana et al.·Sep 12, 2023SaveLearn
Measurements of the absolute branching fractions of - decays and test of the I = 1/2 ruleBased on a data set of (27.120.10)× 108 (3686) events collected at the BESIII experiment, the absolute branching fractions of the three dominant - decays are measured to be…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 12, 2023SaveLearn
Event-by-Event Direction Reconstruction of Solar Neutrinos in a High Light-Yield Liquid ScintillatorThe direction of individual 8B solar neutrinos has been reconstructed using the SNO+ liquid scintillator detector. Prompt, directional Cherenkov light was separated from the slower, isotropic…A. Allega, M. R. Anderson, S. Andringa et al.·Sep 12, 2023SaveLearn
Latest results from Daya Bay using the full datasetThe Daya Bay Reactor Neutrino Experiment was designed with the primary goal of precisely measuring the neutrino mixing parameter, θ13. Eight identically-designed gadolinium-doped liquid…Zhiyuan Chen·Sep 12, 2023SaveLearn
Workshop on a future muon program at FNALThe Snowmass report on rare processes and precision measurements recommended Mu2e-II and a next generation muon facility at Fermilab (Advanced Muon Facility) as priorities for the frontier. The…S. Corrodi, Y. Oksuzian, A. Edmonds et al.·Sep 12, 2023SaveLearn
Measurement of Two-Point Energy Correlators Within Jets in pp Collisions at s = 200 GeV at STARJet substructure is a powerful tool to probe the time evolution of a parton shower. However, many of the analysis methods used to extract splitting formation times from jet substructure, such as Soft…Andrew Tamis·Sep 11, 2023SaveLearn
Observation of D+ KS0a0(980)+ in the amplitude analysis of D+ KS0π+ηWe perform for the first time an amplitude analysis of the decay D+ KS0π+η and report the observation of the decay D+ KS0a0(980)+ using 2.93 fb-1 of…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 11, 2023SaveLearn
Measurement of the CKM angle γ in the B0 DK*0 channel using self-conjugate D KS0 h+ h- decaysA model-independent study of CP violation in B0 DK*0 decays is presented using data corresponding to an integrated luminosity of 9fb-1 collected by the LHCb experiment at…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Sep 11, 2023SaveLearn
Observation of the Singly Cabibbo-Suppressed Decay c+ -K+π+The singly Cabibbo-suppressed decay c+ -K+π+ is observed for the first time with a statistical significance of 6.4σ by using 4.5 fb-1 of e+e-…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 11, 2023SaveLearn
Electron and photon energy calibration with the ATLAS detector using LHC Run 2 dataThis paper presents the electron and photon energy calibration obtained with the ATLAS detector using 140 fb-1 of LHC proton-proton collision data recorded at s=13 TeV between 2015 and…ATLAS Collaboration·Sep 11, 2023SaveLearn
Measurement of the neutron timelike electromagnetic form factor with the SND detectorThe results of the measurement of the e+e- n n cross section and effective neutron timelike form factor are presented. The data taking was carried out in 2020-2021 at the VEPP-2000…SND Collaboration, M. N. Achasov, A. Yu. Barnyakov et al.·Sep 11, 2023SaveLearn
The Southern Wide-field Gamma-ray ObservatoryThe Southern Wide-field Gamma-ray Observatory (SWGO) is an R&D project to plan and design the next observatory to detect gamma rays in the Southern hemisphere. The experiment, planned to be placed at…Ruben Conceição·Sep 8, 2023SaveLearn
Search for the Zγ decay mode of new high-mass resonances in pp collisions at s=13 TeV with the ATLAS detectorThis letter presents a search for narrow, high-mass resonances in the Zγ final state with the Z boson decaying into a pair of electrons or muons. The s=13 TeV pp collision data…ATLAS Collaboration·Sep 8, 2023SaveLearn
Measurement of the cross section of e+e-→-+ at center-of-mass energies between 3.510 and 4.843 GeVUsing e+e- collision data corresponding to a total integrated luminosity of 12.9 fb-1 collected with the BESIII detector at the BEPCII collider, the exclusive Born cross sections and the…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 8, 2023SaveLearn
Novel method to extract the femtometer structure of strange baryons using the vacuum polarization effectOne of the fundamental goals of particle physics is to gain microscopic understanding of the strong interaction. Electromagnetic form factors quantify the structure of hadrons in terms of charge and…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 8, 2023SaveLearn
Search for the semileptonic decays D+s K1(1270)0 e+e and D+s b1(1235)0 e+eBy analyzing 7.33\,fb-1 of e+e- collision data collected at center-of-mass energies between 4.128 and 4.226 GeV with the BESIII detector, we search for the semileptonic decays $D+s …BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 8, 2023SaveLearn
Measurement of Time Resolution of Scintillation Detectors with EQR-15 Silicon Photodetectors for the Time-of-Flight Neutron Detector of the BM@N ExperimentTo study the dependence of the equation of state of high density nuclear matter on the term characterizing the isospin (proton-neutron) asymmetry of nuclear matter, it is necessary to measure…F. Guber, A. Ivashkin, N. Karpushkin et al.·Sep 7, 2023SaveLearn
Evidence for the Higgs boson decay to a Z boson and a photon at the LHCThe first evidence for the Higgs boson decay to a Z boson and a photon is presented, with a statistical significance of 3.4 standard deviations. The result is derived from a combined analysis of…ATLAS, CMS Collaborations·Sep 7, 2023SaveLearn
Light Meson Decays at BESIIIThe world's largest sample of Jpsi events collected at BESIII detector offers a unique opportunity to investigate eta and eta' physics via the Jpsi radiative or hadronic decays with unprecedented…Guofa Xu·Sep 7, 2023SaveLearn
Measurement of jet production in deep inelastic scattering and NNLO determination of the strong coupling at ZEUSA new measurement of inclusive-jet cross sections in the Breit frame in neutral current deep inelastic scattering using the ZEUS detector at the HERA collider is presented. The data were taken in the…ZEUS Collaboration, I. Abt, R. Aggarwal et al.·Sep 6, 2023SaveLearn
First Measurement of the Decay Asymmetry in the pure W-boson-exchange Decay c+0K+Based on 4.4~fb-1 of e+e- annihilation data collected at the center-of-mass energies between 4.60 and 4.70~GeV with the BESIII detector at the BEPCII collider, the pure…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Sep 6, 2023SaveLearn
Search for charged-lepton flavor violation in (2S) τ (=e,μ) decays at BelleWe report a search for the charged-lepton flavor violation in (2S) τ (=e,μ) decays using a 25~ (2S) sample collected by the Belle detector at the…R. Dhamija, S. Nishida, A. Giri et al.·Sep 6, 2023SaveLearn
CMS detector: Run 3 status and plans for Phase-2The CMS experiment at the LHC has started data taking in Run 3 at a pp collision energy of 13.6~TeV. In preparation for Run 3, detector systems, such as Pixel Tracker, HCAL and…Srećko Morović·Sep 5, 2023SaveLearn
The acrylic vessel for JSNS2-II neutrino targetThe JSNS2 (J-PARC Sterile Neutrino Search at J-PARC Spallation Neutron Source) is an experiment designed for the search for sterile neutrinos. The experiment is currently at the stage of the…C. D. Shin, S. Ajimura, M. K. Cheoun et al.·Sep 5, 2023SaveLearn
Reconstruction of Unstable Heavy Particles Using Deep Symmetry-Preserving Attention NetworksReconstructing unstable heavy particles requires sophisticated techniques to sift through the large number of possible permutations for assignment of detector objects to the underlying partons.…Michael James Fenton, Alexander Shmakov, Hideki Okawa et al.·Sep 5, 2023SaveLearn