Expanding neutrino oscillation parameter measurements in NOvA using a Bayesian approachNOvA is a long-baseline neutrino oscillation experiment that measures oscillations in charged-current μ → μ (disappearance) and μ → e…NOvA Collaboration, M. A. Acero, B. Acharya et al.·Nov 14, 2023SaveLearn
The simulation of the DarkSide-20k calibrationDarkSide-20k will be the next liquid argon TPC built to perform direct search for dark matter under the form of WIMPs. Its calibration to both signal and backgrounds is key as very few events are…Marie van Uffelen·Nov 13, 2023SaveLearn
Observation of quantum entanglement in top-quark pairs using the ATLAS detectorEntanglement is a key feature of quantum mechanics, with applications in fields such as metrology, cryptography, quantum information, and quantum computation. It has been observed in a wide variety…ATLAS Collaboration·Nov 13, 2023SaveLearn
First Measurement of R(Xτ/) as an Inclusive Test of the b c τ AnomalyWe measure the tau-to-light-lepton ratio of inclusive B-meson branching fractions R(Xτ/) B(B X τ )/B(B X ), where indicates an…Belle II Collaboration, I. Adachi, K. Adamczyk et al.·Nov 13, 2023SaveLearn
Study of the decay J/ φ π0ηBased on (10.09 0.04) × 109 J/ events collected with the BESIII detector operating at the BEPCII collider, a partial wave analysis of the decay J/ φ π0η is…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Nov 13, 2023SaveLearn
Evidence of the Singly Cabibbo Suppressed decay c+ pπ0Evidence for the singly Cabibbo suppressed decay c+ pπ0 is reported for the first time with a statistical significance of 3.7σ based on 6.0 fb-1 of e+e-…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Nov 12, 2023SaveLearn
Search for Highly-Ionizing Particles in pp Collisions During LHC Run-2 Using the Full MoEDAL DetectorThis search for Magnetic Monopoles (MMs) and High Electric Charge Objects (HECOs) with spins 0, 1/2 and 1, uses for the first time the full MoEDAL detector, exposed to 6.6 fb-1 proton-proton…MoEDAL Collaboration·Nov 11, 2023SaveLearn
Supernova and solar neutrino searches at DUNEThe Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline experiment exploiting the liquid argon TPC technology. DUNE will have sensitivity to low energy physics searches,…C. Cuesta·Nov 10, 2023SaveLearn
Observation and branching fraction measurement of the decay J\!/\! → p + KS0 + c.c.The first observation of the decays J\!/\! → p + KS0 and J\!/\! → p - KS0 is reported using (1008744)×106…M. Ablikim, M. N. Achasov, P. Adlarson et al.·Nov 10, 2023SaveLearn
Learning Broken Symmetries with Resimulation and Encouraged InvarianceRecognizing symmetries in data allows for significant boosts in neural network training. In many cases, however, the underlying symmetry is present only in an idealized dataset, and is broken in the…Edmund Witkowski, Daniel Whiteson·Nov 10, 2023SaveLearn
Hadronic resonance production with ALICE at the LHCHadronic resonance production plays an important role both in elementary and in nucleus-nucleus collisions. In heavy-ion collisions, since the lifetimes of short-lived resonances are comparable with…Sergey Kiselev·Nov 10, 2023SaveLearn
Rydberg-atom-based single-photon detection for haloscope axion searchesWe propose a Rydberg-atom-based single-photon detector for signal readout in dark matter haloscope experiments between 40 μeV and 200 μeV (10 GHz and 50 GHz). At these frequencies, standard…Eleanor Graham, Sumita Ghosh, Yuqi Zhu et al.·Nov 10, 2023SaveLearn
Measurement of the Quasi-Two-Body B DecaysWe study the contributions of the B→ (3770)K[(3770)→ DD], B→ K*(1410)π[K*(1410)→ Kπ] and $B→ X(3872)K[X(3872)→…Hossein. Mehraban, Behnam Mohammadi·Nov 9, 2023SaveLearn
Measurement of the D* longitudinal polarization in B0 D*-τ+τ decaysThe longitudinal polarization fraction of the D* meson is measured in B0 D*-τ+τ decays, where the τ lepton decays to three charged pions and a neutrino, using…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Nov 9, 2023SaveLearn
A DNN for CMS track classification and selectionThe upgrade of the track classification and selection step of the CMS tracking to a Deep Neural Network is presented. The CMS tracking follows an iterative approach: tracks are reconstructed in…CMS Collaboration·Nov 9, 2023SaveLearn
Atmospheric neutrino oscillation analysis with neutron tagging and an expanded fiducial volume in Super-Kamiokande I-VWe present a measurement of neutrino oscillation parameters with the Super-Kamiokande detector using atmospheric neutrinos from the complete pure-water SK I-V (April 1996-July 2020) data set,…Kamiokande Collaboration, T. Wester, K. Abe et al.·Nov 9, 2023SaveLearn
Two Watts is All You Need: Enabling In-Detector Real-Time Machine Learning for Neutrino Telescopes Via Edge ComputingThe use of machine learning techniques has significantly increased the physics discovery potential of neutrino telescopes. In the upcoming years, we are expecting upgrade of currently existing…Miaochen Jin, Yushi Hu, Carlos A. Argüelles·Nov 8, 2023SaveLearn
Development of time-of-flight particle identification for future Higgs factoriesWith the emergence of advanced Silicon (Si) sensor technologies such as LGADs, it is now possible to achieve exceptional time measurement precision below 50 ps. As a result, the implementation of…Bohdan Dudar, Ulrich Einhaus, Jenny List et al.·Nov 8, 2023SaveLearn
Curvature-bias corrections using a pseudomass methodMomentum measurements for very high momentum charged particles, such as muons from electroweak vector boson decays, are particularly susceptible to charge-dependent curvature biases that arise from…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Nov 8, 2023SaveLearn
New approach to finding invisible states in e+e- annihilation and application to BESIII dataWe compare precision e+e- to μ+μ- cross section measurements by BESIII in the Ecm =3.8-4.6 GeV range, to predictions based on measured Rhad data. The consistency is poor (p-value…Glennys R. Farrar, Qi-Ming Li, Chang-Zheng Yuan·Nov 8, 2023SaveLearn
Fast timing detectors with applications in cosmic ray physics and medical scienceWe discuss the use of Low Gain Avalanche (LGAD) silicon detectors for two specific applications, namely measuring cosmic rays in space in collaboration with NASA] and beam properties and received…C. Royon, F. Gautier·Nov 8, 2023SaveLearn
Search for a CP-odd Higgs boson decaying into a heavy CP-even Higgs boson and a Z boson in the +- tt and bb final states using 140 fb-1 of data collected with the ATLAS detectorA search for a heavy CP-odd Higgs boson, A, decaying into a Z boson and a heavy CP-even Higgs boson, H, is presented. It uses the full LHC Run 2 dataset of pp collisions at s=13 TeV…ATLAS Collaboration·Nov 7, 2023SaveLearn
Search for Resonant Production of Dark Quarks in the Dijet Final State with the ATLAS DetectorThis paper presents a search for a new Z resonance decaying into a pair of dark quarks which hadronise into dark hadrons before promptly decaying back as Standard Model particles. This…ATLAS Collaboration·Nov 7, 2023SaveLearn
Measurement of the neutrino-oxygen neutral-current quasielastic cross section using atmospheric neutrinos in the SK-Gd experimentWe report the first measurement of the atmospheric neutrino-oxygen neutral-current quasielastic (NCQE) cross section in the gadolinium-loaded Super-Kamiokande (SK) water Cherenkov detector. In June…S. Sakai, K. Abe, C. Bronner et al.·Nov 7, 2023SaveLearn
Associated single top production (t+X)Single top quark production in association with vector bosons provides a unique way to probe the electroweak sector of the standard model at the Large Hadron Collider. In this talk the latest…Nils Faltermann·Nov 7, 2023SaveLearn