Charged Particle Tracking in Real-Time Using a Full-Mesh Data Delivery Architecture and Associative Memory TechniquesWe present a flexible and scalable approach to address the challenges of charged particle track reconstruction in real-time event filters (Level-1 triggers) in collider physics experiments. The…Sudha Ajuha, Ailton Akira Shinoda, Lucas Arruda Ramalho et al.·Oct 5, 2022SaveLearn
Proposal for Measurement of the Two-body Neutron Decay using MicrocalorimeterThe bound beta-decay (BoB) of neutron is also known as the two-body neutron decay, which is a rare decay mode into a hydrogen atom and an anti-neutrino. The state of neutrino can be exactly inferred…Zhang Shuo, Xavier Mougeot, Wang Song-Lin et al.·Oct 5, 2022SaveLearn
Measurement of branching fractions of c+pKS0KS0 and c+pKS0η at BelleWe present a study of a singly Cabibbo-suppressed decay c+pKS0KS0 and a Cabibbo-favored decay c+pKS0η based on 980 fb-1 of data collected by the…Belle Collaboration, L. K. Li, K. Kinoshita et al.·Oct 5, 2022SaveLearn
Simulation study of particle identification using cluster counting technique for the BESIII drift chamberThe particle identification of charged hadrons, especially for the separation of K and π, is crucial for the flavour physics study. Ionization measurement with the cluster counting technique,…Shuiting Xin, Guang Zhao, Linghui Wu et al.·Oct 4, 2022SaveLearn
Search for exotic interactions of solar neutrinos in the CDEX-10 experimentWe investigate exotic neutrino interactions using the 205.4 kg·day dataset from the CDEX-10 experiment at the China Jinping Underground Laboratory. New constraints on the mass and couplings of…X. P. Geng, L. T. Yang, Q. Yue et al.·Oct 4, 2022SaveLearn
Neutrino-induced coherent π+ production in C, CH, Fe and Pb at E 6 GeVMINERvA has measured the μ-induced coherent π+ cross section simultaneously in hydrocarbon (CH), graphite (C), iron (Fe) and lead (Pb) targets using neutrinos from 2 to 20 GeV. The…M. A. Ramírez, S. Akhter, Z. Ahmad Dar et al.·Oct 4, 2022SaveLearn
Improved Measurement of the Evolution of the Reactor Antineutrino Flux and Spectrum at Daya BayReactor neutrino experiments play a crucial role in advancing our knowledge of neutrinos. A precise measurement of reactor electron antineutrino flux and spectrum evolution can be key inputs in…The Daya Bay Collaboration·Oct 3, 2022SaveLearn
Public Education and OutreachThis article summarizes recommendations made by the Community Engagement Frontier conveners as part of the 2022 Snowmass process. It suggests that institutions involved in high energy physics (e.g.,…Sarah Demers, Kathryn Jepsen, Don Lincoln et al.·Oct 3, 2022SaveLearn
Using Artificial Intelligence in the Reconstruction of Signals from the PADME Electromagnetic CalorimeterThe PADME apparatus was built at the Frascati National Laboratory of INFN to search for a dark photon (A') produced via the process e+ e- → A' γ. The central component of the…Kalina Dimitrova·Oct 3, 2022SaveLearn
Probing the valence quark region of nucleons with Z bosons at LHCbBecause of its forward coverage, LHCb can probe the valence quark distributions of protons and nuclei at small and large Bjorken-x with high precision. This proceeding presents new LHCb measurements…Tianqi Li·Oct 3, 2022SaveLearn
Light meson spectroscopy and gluonium searches in ηc and (1S) decays at BaBarWe study the (1S) radiative decays to γ π+ π- and γ K+ K- using data recorded with the BaBar detector operating at the SLAC PEP-II asymmetric-energy e+e- collider…Antimo Palano·Oct 3, 2022SaveLearn
Deep learning for track recognition in pixel and strip-based particle detectorsThe reconstruction of charged particle trajectories in tracking detectors is a key problem in the analysis of experimental data for high-energy and nuclear physics. The amount of data in modern…O. Bakina, D. Baranov, I. Denisenko et al.·Oct 2, 2022SaveLearn
India Based Neutrino Observatory, Physics Reach and Status ReportThe India-based Neutrino Observatory (INO) is a proposed underground facility located in India that will primarily house the magnetised Iron CALorimeter (ICAL) detector to study atmospheric neutrinos…D. Indumathi·Oct 1, 2022SaveLearn
Search for new heavy resonances decaying to WW, WZ, ZZ, WH, or ZH boson pairs in the all-jets final state in proton-proton collisions at s = 13 TeVA search for new heavy resonances decaying to WW, WZ, ZZ, WH, or ZH boson pairs in the all-jets final state is presented. The analysis is based on proton-proton collision data recorded by the CMS…CMS Collaboration·Sep 30, 2022SaveLearn
Recent LHCb results on forward physics and diffractionThe LHCb detector at the LHC offers unique coverage of forward rapidities for studies of Central Exclusive Production (CEP) and soft QCD. CEP measurements allow the investigation of the nature of…Luke McConnell·Sep 30, 2022SaveLearn
Offloading electromagnetic shower transport to GPUsMaking general particle transport simulation for high-energy physics (HEP) single-instruction-multiple-thread (SIMT) friendly, to take advantage of accelerator hardware, is an important alternative…G. Amadio, J. Apostolakis, P. Buncic et al.·Sep 30, 2022SaveLearn
A search for new resonances in multiple final states with a high transverse momentum Z boson in s=13 TeV pp collisions with the ATLAS detectorA generic search for resonances is performed with events containing a Z boson with transverse momentum greater than 100 GeV, decaying into e+e- or μ+μ-. The analysed data collected with…ATLAS Collaboration·Sep 30, 2022SaveLearn
Hyperon Physics at BESIIISpin polarization and entanglement are utilized by the BESIII experiment to learn more about the production and decay properties of hyperon-antihyperon pairs in a series of recent analyses of its…Viktor Thorén·Sep 30, 2022SaveLearn
Forward Proton Measurements with ATLASThe ALFA subdetector is designed to measure elastic proton-proton scattering from which the total cross section and -parameter are determined. In 2016, special runs at a center-of-mass energy…M. Schmidt·Sep 30, 2022SaveLearn
Study of Charmonium(-like) Spectroscopy and Decay at BESIIIThe recent results on Charmonium and Charmonium-like states at BESIII are reviewed, including the observation of Zcs(3985) state, the study of the new decay modes of 2(3823) state,…Weimin Song·Sep 29, 2022SaveLearn
Search for Cosmic-ray Boosted Sub-GeV Dark Matter using Recoil Protons at Super-KamiokandeWe report a search for cosmic-ray boosted dark matter with protons using the 0.37 megaton×years data collected at Super-Kamiokande experiment during the 1996-2018 period (SKI-IV phase). We…Kamiokande Collaboration, K. Abe, Y. Hayato et al.·Sep 29, 2022SaveLearn
Detector Challenges of the strong-field QED experiment LUXE at the European XFELThe LUXE experiment aims at studying high-field QED in electron-laser and photon-laser interactions, with the 16.5 GeV electron beam of the European XFEL and a laser beam with power of up to 350 TW.…Arka Santra·Sep 29, 2022SaveLearn
Helix string fragmentation and charged particle correlations with ATLASCorrelations between charged particles provide important insight into the hadronization process. The analysis of the momentum difference between charged hadrons in pp, p-lead, and lead-lead…S. Todorova-Nova·Sep 29, 2022SaveLearn
Measurement of the polarisation of W bosons produced in top-quark decays using dilepton events at s = 13 TeV with the ATLAS experimentA measurement of the polarisation of W bosons produced in top-quark decays is presented, using proton-proton collision data at a centre-of-mass energy of s = 13 TeV. The data were…ATLAS Collaboration·Sep 29, 2022SaveLearn
Cosmogenic activation of sodium iodideThe production of radioactive isotopes by interactions of cosmic-ray particles with sodium iodide (NaI) crystals can produce radioactive backgrounds in detectors used to search for rare events.…R. Saldanha, W. G. Thompson, Y. Y. Zhong et al.·Sep 29, 2022SaveLearn