Measurement of integrated luminosities at BESIII for data samples at center-of-mass energies between 4.0 and 4.6 GeVThe integrated luminosities of the data samples collected in the BESIII experiment in 2016--2017 at center-of-mass energies between 4.19 and 4.28 GeV are measured with a precision better than 1% by…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Mar 7, 2022SaveLearn
Deep Learning From Four VectorsAn early example of the ability of deep networks to improve the statistical power of data collected in particle physics experiments was the demonstration that such networks operating on lists of…Pierre Baldi, Peter Sadowski, Daniel Whiteson·Mar 6, 2022SaveLearn
Review of sterile neutrino searches at very short-baseline reactor experimentsSearch for New Physics beyond the Standard Model is the main direction in particle physics nowadays. There are several experimental hints of New Physics. The most statistically significant…Mikhail Danilov·Mar 6, 2022SaveLearn
The odderon discovery by the D0 and TOTEM collaborationsWe describe the discovery of the colorless C-odd gluonic compound, the odderon, by the D0 and TOTEM Collaborations by comparing elastic differential cross sections measured in pp and p p…Christophe Royon·Mar 6, 2022SaveLearn
Deep Regression of Muon Energy with a K-Nearest Neighbor AlgorithmWithin the context of studies for novel measurement solutions for future particle physics experiments, we developed a performant kNN-based regressor to infer the energy of highly-relativistic muons…T. Dorigo, Sofia Guglielmini, Jan Kieseler et al.·Mar 6, 2022SaveLearn
Cross section measurements of the processes e+e- → ωπ0 and ωη at center-of-mass energies between 3.773 and 4.701 GeVThe Born cross sections of the processes e+e- → ωπ0 and e+e- → ωη are measured at center-of-mass energies between 3.773 and 4.701 GeV using a total…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Mar 5, 2022SaveLearn
A Search for Low-mass Dark Matter via Bremsstrahlung Radiation and the Migdal Effect in SuperCDMSIn this paper, we present a re-analysis of SuperCDMS data using a profile likelihood approach to search for sub-GeV dark matter particles (DM) through two inelastic scattering channels:…SuperCDMS Collaboration, Musaab Al-Bakry, Imran Alkhatib et al.·Mar 4, 2022SaveLearn
Low Energy Event Reconstruction in IceCube DeepCoreThe reconstruction of event-level information, such as the direction or energy of a neutrino interacting in IceCube DeepCore, is a crucial ingredient to many physics analyses. Algorithms to extract…R. Abbasi, M. Ackermann, J. Adams et al.·Mar 4, 2022SaveLearn
Search for the Majorana Nature of Neutrinos in the Inverted Mass Ordering Region with KamLAND-ZenThe KamLAND-Zen experiment has provided stringent constraints on the neutrinoless double-beta (0ββ) decay half-life in 136Xe using a xenon-loaded liquid scintillator. We report an…Zen Collaboration, S. Abe, S. Asami et al.·Mar 4, 2022SaveLearn
Hyper-Kamiokande Experiment: A Snowmass White PaperHyper-Kamiokande (HK) is the next generation underground water Cherenkov detector that builds on the highly successful Super-Kamiokande (SK) experiment. The 260,000-ton detector has an 8.4 times…J. Bian, F. Di Lodovico, S. Horiuchi et al.·Mar 3, 2022SaveLearn
Beam dynamics corrections to the Run-1 measurement of the muon anomaly aμ at FermilabThe Fermi National Accelerator Laboratory (FNAL) Muon g-2 Experiment has measured the positive muon magnetic anomaly aμ (gμ-2)/2 with a precision of 0.46 parts per million, with…Alessandra Lucà·Mar 3, 2022SaveLearn
PIONEER: Studies of Rare Pion DecaysA next-generation rare pion decay experiment, PIONEER, is strongly motivated by several inconsistencies between Standard Model (SM) predictions and data pointing towards the potential violation of…PIONEER Collaboration, W. Altmannshofer, H. Binney et al.·Mar 3, 2022SaveLearn
The Potential to Probe Solar Neutrino Physics with LiCl Water SolutionLithium chloride water solution is a good option for solar neutrino detection. The e charged-current (CC) interaction cross-section on 7Li is evaluated with new B(GT) experimental…Wenhui Shao, Weiran Xu, Ye Liang et al.·Mar 3, 2022SaveLearn
Study of Bc+ J/ Ds+ and Bc+ J/ Ds*+ decays in pp collisions at s = 13 TeV with the ATLAS detectorA study of Bc+ J/ Ds+ and Bc+ J/ Ds*+ decays using 139 fb-1 of integrated luminosity collected with the ATLAS detector from s = 13 TeV pp collisions at the…ATLAS Collaboration·Mar 3, 2022SaveLearn
First measurement of the Z→ μ+ μ- angular coefficients in the forward region of pp collisions at s=13 TeVThe first study of the angular distribution of μ+ μ- pairs produced in the forward rapidity region via the Drell-Yan reaction pp → γ*/Z +X → l+ l- + X is…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Mar 3, 2022SaveLearn
Measurement of the branching fraction of the doubly Cabibbo-suppressed decay D0 K+π-π0 and search for D0 K+π-π0π0Using 2.93\, fb-1 of e+e- collision data collected at a center-of-mass energy of 3.773\,GeV with the BESIII detector, we present a measurement of the branching fraction of the doubly…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Mar 3, 2022SaveLearn
The Higgs bb, cc, gg measurement at CEPCAccurately measuring the properties of the Higgs boson is one of the core physics objectives of the Circular Electron Positron Collider (CEPC). As a Higgs factory, the CEPC is expected to operate at…Yongfeng Zhu, Hanhua Cui, Manqi Ruan·Mar 3, 2022SaveLearn
Search for neutral long-lived particles in pp collisions at s=13 TeV that decay into displaced hadronic jets in the ATLAS calorimeterA search for decays of pair-produced neutral long-lived particles (LLPs) is presented using 139 fb-1 of proton-proton collision data collected by the ATLAS detector at the LHC in 2015-2018 at a…ATLAS Collaboration·Mar 2, 2022SaveLearn
Search for events with a pair of displaced vertices from long-lived neutral particles decaying into hadronic jets in the ATLAS muon spectrometer in pp collisions at s=13 TeVA search for events with two displaced vertices from long-lived particles (LLP) pairs using data collected by the ATLAS detector at the LHC is presented. This analysis uses 139~fb-1 of…ATLAS Collaboration·Mar 1, 2022SaveLearn
Search for new particles in an extended Higgs sector with four b quarks in the final state at s = 13 TeVA search for an extended Higgs sector, characterized by a massive resonance X decaying to a pair of spin-0 bosons φ that themselves decay to pairs of bottom quarks, is presented. The analysis is…CMS Collaboration·Mar 1, 2022SaveLearn
Constraints on future analysis metadata systems in High Energy PhysicsIn High Energy Physics (HEP), analysis metadata comes in many forms -- from theoretical cross-sections, to calibration corrections, to details about file processing. Correctly applying metadata is a…T. J. Khoo, A. Reinsvold Hall, N. Skidmore et al.·Mar 1, 2022SaveLearn
Exploring the Quark Transversity and the Collins Fragmentation Functions using Polarized pp Collisions at STARUnderstanding the internal spin structure of the nucleon still remains a challenge in strong interaction physics. Transversity, which describes the transverse spin structure of quarks in a…Ting Lin·Mar 1, 2022SaveLearn
Quantum Machine Learning for b-jet charge identificationMachine Learning algorithms have played an important role in hadronic jet classification problems. The large variety of models applied to Large Hadron Collider data has demonstrated that there is…Alessio Gianelle, Patrick Koppenburg, Donatella Lucchesi et al.·Feb 28, 2022SaveLearn
Measurements of jet observables sensitive to b-quark fragmentation in tt events at the LHC with the ATLAS detectorSeveral observables sensitive to the fragmentation of b-quarks into b-hadrons are measured using 36 fb-1 of s = 13 TeV proton-proton collision data collected with the ATLAS…ATLAS Collaboration·Feb 28, 2022SaveLearn
Measurements of Absolute Branching Fractions of D0 KL0φ, KL0η, KL0ω, and KL0η^We report the first measurements of the absolute branching fractions of D0 KL0φ, D0 KL0η, D0 KL0ω, and D0 KL0η, obtained by analyzing $2.93\,…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Feb 28, 2022SaveLearn