Results and Prospects of T2KT2K is a neutrino oscillation experiment with a 295 km long baseline between the far detector, Super-Kamiokande, and a suite of near detectors to study μ/μ disappearance and…T. Nosek·Oct 18, 2023SaveLearn
Novel techniques for alpha/beta pulse shape discrimination in BorexinoBorexino could efficiently distinguish between alpha and beta radiation in its liquid scintillator by the characteristic time profile of their scintillation pulse. This alpha/beta discrimination,…D. Basilico, G. Bellini, J. Benziger et al.·Oct 18, 2023SaveLearn
Overview of ATLAS forward proton detectors for LHC Run 3 and plans for the HL-LHCThe status of the ATLAS Roman Pot detectors (AFP and ALFA) for LHC Run 3 after all refurbishments and improvements done during Long Shutdown 2 is discussed.Maciej Trzebinski·Oct 18, 2023SaveLearn
Study of Z llγ decays at s~= 8 TeV with the ATLAS detectorThis paper presents a study of Z llγ~decays with the ATLAS detector at the Large Hadron Collider. The analysis uses a proton-proton data sample corresponding to an integrated luminosity of…ATLAS Collaboration·Oct 17, 2023SaveLearn
Status and first results from XENONnTXENON is a project for direct dark matter search located in the INFN underground laboratory LNGS. The previous generation of XENON detector, XENON1T, achieved an exposure of 1 ton×year,…S. E. M. Ahmed Maouloud·Oct 17, 2023SaveLearn
QUEST-DMC superfluid 3He detector for sub-GeV dark matterThe focus of dark matter searches to date has been on Weakly Interacting Massive Particles (WIMPs) in the GeV/c2-TeV/c2 mass range. The direct, indirect and collider searches in this mass range…S. Autti, A. Casey, N. Eng et al.·Oct 17, 2023SaveLearn
Search for non-resonant Higgs boson pair production in the 2b + 2 + ETmiss final state in pp collisions s = 13\,TeV with the ATLAS detectorA search for non-resonant Higgs boson pair (HH) production is presented, in which one of the Higgs bosons decays to a b-quark pair (b b) and the other decays to WW*, ZZ*, or…ATLAS Collaboration·Oct 17, 2023SaveLearn
Diffractive and photon-induced production of top quarkThe top quark plays a central role in particle physics, as many experiments at the Large Hadron Collider scrutinize its properties within the Standard Model. Although most of the measurements of the…Michael Pitt·Oct 17, 2023SaveLearn
Search for central exclusive production of top quark pairs in proton-proton collisions at s = 13 TeV with tagged protonsA search for the central exclusive production of top quark-antiquark pairs (tt) is performed for the first time using proton-tagged events in proton-proton collisions at the LHC at a…CMS, TOTEM Collaborations·Oct 17, 2023SaveLearn
Study of non-standard interaction mediated by a scalar field at ESSnuSB experimentIn this paper we study non-standard interactions mediated by a scalar field (SNSI) in the context of ESSnuSB experiment. In particular we study the capability of ESSnuSB to put bounds on the SNSI…ESSnuSB, :, J. Aguilar et al.·Oct 16, 2023SaveLearn
Flavour Physics at LHCb -- 50 years of the KM paradigmThe LHCb experiment is in operation since 2009 and has provided measurements of the KM matrix with unprecedented precision. 50 years after the original paper we are in the position of pinning down…Patrick Koppenburg·Oct 16, 2023SaveLearn
Measurement of the cross sections for e+e-ηπ+π- at center-of-mass energies between 2.00 and 3.08 GeVUsing data samples collected at center-of-mass energies between 2.000 and 3.080 GeV with the BESIII detector operating at the BEPCII collider, a partial-wave analysis is performed on the process…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Oct 16, 2023SaveLearn
Application of Machine Learning Based Top Quark and W Jet Tagging to Hadronic Four-Top Final States Induced by SM as well as BSM ProcessesWe apply gradient boosting machine learning techniques to the problem of hadronic jet substructure recognition using classical subjettiness variables available within a common parameterized detector…Petr Baroň, Jiří Kvita, Radek Přívara et al.·Oct 16, 2023SaveLearn
Light-flavor particle production in high-multiplicity pp collisions at s = 13 TeV as a function of transverse spherocityResults on the transverse spherocity dependence of light-flavor particle production (π, K, p, φ, K*0, K0S, , ) at midrapidity in high-multiplicity…ALICE Collaboration·Oct 16, 2023SaveLearn
Long Baseline Neutrino Oscillation Results (T2K and NOvA)The well-established neutrino oscillation phenomenon, which confirms neutrinos have mass and the charged and neutral leptons are mixed, has been widely exploited to investigate the physics of this…Son Cao·Oct 15, 2023SaveLearn
Study of residual artificial neural network for particle identification in the CEPC high-granularity calorimeter prototypeParticle Identification (PID) plays a central role in associating the energy depositions in calorimeter cells with the type of primary particle in a particle flow oriented detector system. In this…Siyuan Song, Jiyuan Chen, Jianbei Liu et al.·Oct 14, 2023SaveLearn
New Hadrons Discovered at BESIIIThe BESIII experiment starts to run at 2009 and has submitted 500 publications during the past 15 years. This article reviews the 26 new hadrons discovered at BESIII, dedicated to the celebration of…Zhiqing Liu, Ryan E. Mitchell·Oct 14, 2023SaveLearn
Strange-Meson Spectroscopy with COMPASSWhile the spectrum of non-strange light mesons is well known, many predicted strange mesons have not yet been observed, and many potentially observed states require further confirmation. Using the…S. Wallner·Oct 13, 2023SaveLearn
Partial-wave analysis of τ-π-π-π+τ at BelleWe present preliminary results of a partial-wave analysis of τ-π-π-π+τ in data from the Belle experiment at the KEKB e+e- collider. We demonstrate the…Andrei Rabusov, Daniel Greenwald, Stephan Paul·Oct 13, 2023SaveLearn
Non-strange light-meson spectroscopy at COMPASSLattice-QCD predicts the exotic meson π1(1600) to dominantly decay to b1π. The b1π decay channel is accessible via the ωπ-π0 final state. COMPASS recorded the so far…Philipp Haas·Oct 13, 2023SaveLearn
Optimum filter-based analysis for the characterization of a high-resolution magnetic microcalorimeter towards the DELight experimentUltra-sensitive cryogenic calorimeters have become a favored technology with widespread application where eV-scale energy resolutions are needed. In this article, we characterize the performance of…Francesco Toschi, Benedikt Maier, Greta Heine et al.·Oct 12, 2023SaveLearn
Energy deposition studies for the Upgrade II of LHCb at the CERN Large Hadron ColliderThe Upgrade II of the LHCb experiment is proposed to be installed during the CERN Long Shutdown 4, aiming to operate LHCb at 1.5x1034cm-2s-1 that is 75 times its design luminosity and…Alessia Ciccotelli, Robert B. Appleby, Francesco Cerutti et al.·Oct 12, 2023SaveLearn
Terrestrial Very-Long-Baseline Atom Interferometry: Workshop SummaryThis document presents a summary of the 2023 Terrestrial Very-Long-Baseline Atom Interferometry Workshop hosted by CERN. The workshop brought together experts from around the world to discuss the…Sven Abend, Baptiste Allard, Iván Alonso et al.·Oct 12, 2023SaveLearn
Search for direct production of electroweakinos in final states with one lepton, jets and missing transverse momentum in pp collisions at s=13 TeV with the ATLAS detectorSearches for electroweak production of chargino pairs, +1-1, and of chargino and next-to-lightest neutralino, 102, are…ATLAS Collaboration·Oct 12, 2023SaveLearn
Reconstructing jets in the Phase-2 upgrade of the CMS Level-1 Trigger with a seeded cone algorithmThe Phase-2 Upgrade of the CMS Level-1 Trigger (L1T) will reconstruct particles using the Particle Flow algorithm, connecting information from the tracker, muon, and calorimeter detectors, and…Sioni Summers, Ioannis Bestintzanos, Giovanni Petrucciani·Oct 12, 2023SaveLearn