Jet tagging algorithm of graph network with HaarPooling message passingRecently methods of graph neural networks (GNNs) have been applied to solving the problems in high energy physics (HEP) and have shown its great potential for quark-gluon tagging with graph…Fei Ma, Feiyi Liu, Wei Li·Oct 25, 2022SaveLearn
Tevatron Greatest HitsThe Tevatron collider led the World energy frontier program in particle physics during the late 20th and early 21st centuries. During this exciting period the standard model of particle physics was…Dmitri Denisov, Costas Vellidis·Oct 24, 2022SaveLearn
Measurements of jet multiplicity and jet transverse momentum in multijet events in proton-proton collisions at s = 13 TeVMultijet events at large transverse momentum (pT) are measured at s = 13 TeV using data recorded with the CMS detector at the LHC, corresponding to an integrated luminosity of…CMS Collaboration·Oct 24, 2022SaveLearn
Proceedings of the IFJ PAN Particle Physics Summer Student Alumni Conference 2022IFJ PAN PPSS Alumni Conference is organized by the Institute of Nuclear Physics Polish Academy of Sciences (IFJ PAN). It is addressed to: participants of previous editions of Particle Physics Summer…Derendarz Dominik, Rafal Staszewski, Maciej Trzebinski et al.·Oct 24, 2022SaveLearn
Determination of |Vcb| from B D decays using 2019-2021 Belle II dataWe present a determination of the magnitude of the Cabibbo-Kobayashi-Maskawa (CKM) matrix element Vcb using B D decays. The result is based on e+e-(4S) data recorded…Belle II collaboration, F. Abudinén, I. Adachi et al.·Oct 24, 2022SaveLearn
Study of e+e-γφ J/ from s=4.600 to 4.951 GeVUsing data samples with an integrated luminosity of 6.4~fb-1 collected by the BESIII detector operating at the BEPCII storage ring, the process of e+e-γφ J/ is studied. The…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 24, 2022SaveLearn
Track reconstruction at the LUXE experiment using quantum algorithmsLUXE (Laser Und XFEL Experiment) is a proposed experiment at DESY which will study Quantum Electrodynamics (QED) in the strong-field regime, where QED becomes non-perturbative. Measuring the rate of…Arianna Crippa, Lena Funcke, Tobias Hartung et al.·Oct 24, 2022SaveLearn
Measurement of the ratio of branching fractions B(Bc+ Bs0 π+)/B(Bc+ J/ π+)The ratio of branching fractions of Bc+ Bs0 π+ and Bc+ J/ π+ decays is measured with proton-proton collision data of a centre-of-mass energy of 13TeV. The data…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Oct 21, 2022SaveLearn
Uncovering the neutrino mass ordering with the next galactic core-collapse supernova neutrino burst using water Cherenkov detectorsA major challenge of particle physics is determining the neutrino mass ordering (MO). Due to matter effects, the flavor content of the neutrino flux from a Core-Collapse Supernova (CCSN) depends on…César Jesús-Valls·Oct 21, 2022SaveLearn
Mu2e Run I Sensitivity Projections for the Neutrinoless μ- e- Conversion Search in AluminumThe Mu2e experiment at Fermilab will search for the neutrinoless μ- e- conversion in the field of an aluminum nucleus. The Mu2e data-taking plan assumes two running periods, Run I and Run…Mu2e Collaboration·Oct 20, 2022SaveLearn
Snowmass Early CareerThe Snowmass 2021 strategic planning process provided an essential opportunity for the United States high energy physics and astroparticle (HEPA) community to come together and discuss upcoming…Garvita Agarwal, Joshua L. Barrow, Mateus F. Carneiro et al.·Oct 20, 2022SaveLearn
Utilizing Theory and Experiment to Search for new structures of Fundamental ParticlesOur current understanding of the Big Bang indicates that the universe was not a dimensionless point at t=0 but already had four dimensions. This work, exploring physics beyond the Standard Model,…Jürgen Ulbricht, Minghui Liu·Oct 20, 2022SaveLearn
Axion Dark Matter Search around 4.55 μeV with Dine-Fischler-Srednicki-Zhitnitskii SensitivityWe report an axion dark matter search at Dine-Fischler-Srednicki-Zhitnitskii sensitivity with the CAPP-12TB haloscope, assuming axions contribute 100\% of the local dark matter density. The search…Andrew K. Yi, Saebyeok Ahn, Çağlar Kutlu et al.·Oct 20, 2022SaveLearn
Search for the baryon- and lepton-number violating decays B0 pμ- and B0s pμ-A search for the baryon- and lepton-number violating decays B0 pμ- and B0s pμ- is performed at the LHCb experiment using data collected in proton-proton collisions at s =…LHCb collaboration·Oct 19, 2022SaveLearn
Observation of a J/ resonance consistent with a strange pentaquark candidate in B- J/p decaysAn amplitude analysis of B- J/p decays is performed using about 4400 signal candidates selected on a data sample of pp collisions recorded at center-of-mass energies of 7, 8…LHCb collaboration·Oct 19, 2022SaveLearn
Jet-Flavour Tagging at FCC-eeJet-flavour identification algorithms are of paramount importance to maximise the physics potential of the Future Circular Collider (FCC). Out of the extensive FCC-ee physics program, flavour tagging…Kunal Gautam·Oct 19, 2022SaveLearn
Measurement of the photon-energy spectrum in inclusive B→ Xsγ decays identified using hadronic decays of the recoil B meson in 2019-2021 Belle II dataWe measure the photon-energy spectrum in radiative bottom-meson (B) decays into inclusive final states involving a strange hadron and a photon. We use SuperKEKB electron-positron collisions…Belle II Collaboration, F. Abudinén, I. Adachi et al.·Oct 19, 2022SaveLearn
First constraints on light sterile neutrino oscillations from combined appearance and disappearance searches with the MicroBooNE detectorWe present a search for eV-scale sterile neutrino oscillations in the MicroBooNE liquid argon detector, simultaneously considering all possible appearance and disappearance effects within the 3+1…MicroBooNE collaboration, P. Abratenko, D. Andrade Aldana et al.·Oct 18, 2022SaveLearn
Flavour-changing neutral scalar interactions of the top quarkA study of the top quark interactions via flavour-changing neutral current (FCNC) processes provides an intriguing connection between the heaviest elementary particle of the standard model (SM) of…Nuno Castro, Kirill Skovpen·Oct 18, 2022SaveLearn
Observation of the J/ and (3686) decays into η+-The decays J/η+- and (3686)η+- are observed for the first time, using (10087 44)× 106 J/ and $(448.1 …BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 18, 2022SaveLearn
Measurement of the absolute branching fraction of the inclusive decay c- n + XBased on e+e- collision data corresponding to an integrated luminosity of 4.5 fb-1 collected at the center-of-mass energies between 4.600 and 4.699 GeV with the BESIII detector at BEPCII,…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 18, 2022SaveLearn
Through Iron & Ice: Searching for Sterile Neutrinos at the IceCube Neutrino ObservatoryDespite the rapid progression in our understanding of neutrinos over the last half century, much is left unknown about their properties. This leaves neutrinos as the most promising portal for Beyond…Alejandro Diaz·Oct 17, 2022SaveLearn
Optimizing XW → h0i Reconstruction Efficiency with Small-R (R = 0.4) and Large-R (R = 1.0) JetsMany Beyond the Standard Model searches at ATLAS employ jets to simplify event reconstruction. These jets cluster particle shower products into calculable objects, which are then used to obtain…Sophie Kadan, Evelyn Thomson·Oct 17, 2022SaveLearn
Rock Neutron Backgrounds from FNAL Neutrino Beamlines in the -DRIFT DetectorThe -DRIFT collaboration seeks to detect low-energy nuclear recoils from CE or BSM interactions at FNAL. Backgrounds due to rock neutrons are an important concern. We present…D. Aristizabal Sierra, J. L. Barrow, B. Dutta et al.·Oct 16, 2022SaveLearn
Search for medium effects using jets from bottom quarks in PbPb collisions at sNN = 5.02 TeVThe first study of the shapes of jets arising from bottom (b) quarks in heavy ion collisions is presented. Jet shapes are studied using charged hadron constituents as a function of their radial…CMS Collaboration·Oct 16, 2022SaveLearn