Measurement of the Z boson invisible width at s=13 TeV with the ATLAS detectorA measurement of the invisible width of the Z boson using events with jets and missing transverse momentum is presented using 37 fb\(-1\) of 13 TeV proton-proton data collected by the…ATLAS Collaboration·Dec 5, 2023SaveLearn
Track finding with deep neural networksHigh-energy physics experiments require fast and efficient methods for reconstructing the tracks of charged particles. The commonly used algorithms are sequential, and the required CPU power…Marcin Kucharczyk, Marcin Wolter·Dec 5, 2023SaveLearn
Search for the semileptonic decays c0 0+- at BelleUsing the full data sample of 980 fb-1 collected with the Belle detector at the KEKB asymmetric energy electron-positron collider, we report the results of the first search for the rare…Belle Collaboration, J. X. Cui, Y. B. Li et al.·Dec 5, 2023SaveLearn
Amplitude Analysis of the Decays D0π+π-π+π- and π+π-π0π0Using e+e- annihilation data corresponding to an integrated luminosity of 2.93 fb-1 taken at the center-of-mass energy s=3.773~GeV with the BESIII detector, a joint amplitude…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 5, 2023SaveLearn
Measurement of the VH, H→ ττ process with the ATLAS detector at 13 TeVA measurement of the Standard Model Higgs boson produced in association with a W or Z boson and decaying into a pair of τ-leptons is presented. This search is based on proton-proton…ATLAS Collaboration·Dec 4, 2023SaveLearn
Search for the lepton flavor violating τ 3μ decay in proton-proton collisions at s = 13 TeVA search for the lepton flavor violating τ 3μ decay is performed using proton-proton collision events at a center-of-mass energy of 13 TeV collected by the CMS experiment at the LHC in…CMS Collaboration·Dec 4, 2023SaveLearn
First Constraints on WIMP-Nucleon Effective Field Theory Couplings in an Extended Energy Region From LUX-ZEPLINFollowing the first science results of the LUX-ZEPLIN (LZ) experiment, a dual-phase xenon time projection chamber operating from the Sanford Underground Research Facility in Lead, South Dakota, USA,…LZ Collaboration, J. Aalbers, D. S. Akerib et al.·Dec 4, 2023SaveLearn
Search for the decay of the Higgs boson to a Z boson and a light pseudoscalar particle decaying to two photonsA search for the decay of the Higgs boson to a Z boson and a light, pseudoscalar particle, a, decaying respectively to two leptons and to two photons is reported. The search uses the full LHC Run…ATLAS Collaboration·Dec 4, 2023SaveLearn
Momentum scale calibration of the LHCb spectrometerFor accurate determination of particle masses accurate knowledge of the momentum scale of the detectors is crucial. The procedure used to calibrate the momentum scale of the LHCb spectrometer is…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Dec 4, 2023SaveLearn
Strangeness production in double gap events in ALICEThe ALICE detector at the LHC was upgraded in the long shutdown of 2019-2021 in order to take data at much-increased Run 3 and 4 rates. The various challenges of this upgrade are presented, and the…R. Schicker·Dec 3, 2023SaveLearn
Development of a Monte Carlo tool for simulating electron transport in noble liquidsThis study presents a Monte Carlo simulation tool for modeling the transportation processes of thermal electrons in noble liquids, specifically focusing on liquid argon and liquid xenon. The study…Yijun Xie, Yi Wang·Dec 3, 2023SaveLearn
The Targets of Opportunity Source Catalog for the EUSO-SPB2 MissionThe Extreme Universe Space Observatory on a Super Pressure Balloon 2, EUSO SPB2, mission was designed to take optical measurements of extensive air showers, EASs, from suborbital space. The EUSO SPB2…Hannah Wistrand, Tobias Heibges, Jonatan Posligua et al.·Dec 1, 2023SaveLearn
Inclusive and differential results of top quark pair production from the ATLAS and CMS experimentsThis report summarizes recent results of inclusive and differential tt cross section measurements from the ATLAS and CMS Collaborations at the LHC. Measurements at $s=7,\ 8,\…David Walter·Dec 1, 2023SaveLearn
The U.S. CMS HL-LHC R&D Strategic PlanThe HL-LHC run is anticipated to start at the end of this decade and will pose a significant challenge for the scale of the HEP software and computing infrastructure. The mission of the U.S. CMS…Oliver Gutsche, Tulika Bose, Margaret Votava et al.·Dec 1, 2023SaveLearn
Machine learning approaches for parameter reweighting in MC samples of top quark production in CMSIn particle physics, Monte Carlo (MC) event generators are needed to compare theory to the measured data. Many MC samples have to be generated to account for theoretical systematic uncertainties, at…Valentina Guglielmi·Dec 1, 2023SaveLearn
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detectorThis paper presents the measurement of fiducial and differential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets ($W…The ATLAS Collaboration·Dec 1, 2023SaveLearn
Status and Prospects of Exotic Hadrons at Belle IIIn the past twenty years, many new hadrons that are difficult to be explained within the conventional quark model have been discovered in the quarkonium region, which are called exotic hadrons. Belle…Sen Jia, Weitao Xiong, Chengping Shen·Dec 1, 2023SaveLearn
Long-term temporal stability of the DarkSide-50 dark matter detectorThe stability of a dark matter detector on the timescale of a few years is a key requirement due to the large exposure needed to achieve a competitive sensitivity. It is especially crucial to enable…50 Collaboration, P. Agnes, I. F. M. Albuquerque et al.·Nov 30, 2023SaveLearn
Observation of structures at 17 and 38 MeV/c2 in the γγ invariant mass spectra in pC, dC, and dCu collisions at plab of a few GeV/c per nucleonThe results of an analysis of the invariant mass spectra of photon pairs produced in dC, pC and dCu interactions at momenta of 2.75, 5.5 and 3.83 GeV/c per nucleon respectively, are presented.…Kh. U. Abraamyan, Ch. Austin, M. I. Baznat et al.·Nov 30, 2023SaveLearn
Search for Hidden Neutrinos at the European Spallation Source: the SHiNESS experimentThe upcoming European Spallation Source (ESS) will soon provide the most intense neutrino source in the world. We propose the Search for Hidden Neutrinos at the ESS (SHiNESS) experiment, highlighting…Stefano Roberto Soleti, Pilar Coloma, Juan Jose Gómez Cadenas et al.·Nov 30, 2023SaveLearn
Search for light long-lived neutral particles from Higgs boson decays via vector-boson-fusion production from pp collisions at s=13 TeV with the ATLAS detectorA search is reported for long-lived dark photons with masses between 0.1 GeV and 15 GeV, from exotic decays of Higgs bosons produced via vector-boson-fusion. Events that contain displaced collimated…ATLAS Collaboration·Nov 30, 2023SaveLearn
Reconstruction of electromagnetic showers in calorimeters using Deep LearningThe precise reconstruction of properties of photons and electrons in modern high energy physics detectors, such as the CMS or Atlas experiments, plays a crucial role in numerous physics results.…Polina Simkina, Fabrice Couderc, Julie Malclès et al.·Nov 29, 2023SaveLearn
Exploring Photoproduction with the GlueX ExperimentThe GlueX experiment at Jefferson Lab (Newport News, VA USA) is designed to explore the spectrum of mesons up to about 3 GeV. We present results on the production of light-quark resonances with…Matthew Shepherd·Nov 29, 2023SaveLearn
Status of e+e- Higgs Factory ProjectsAn electron-positron collider designed for precision studies of the Higgs boson, a so-called Higgs factory is the highest-priority next collider of the particle physics community. This contribution…Jenny List·Nov 29, 2023SaveLearn
Magnetic field simulations and measurements on the mini-ICAL detectorThe ICAL (Iron Calorimeter) is a 51 kTon magnetized detector proposed by the INO collaboration. It is designed to detect muons with energies in the 1-20 GeV range. A magnetic field of about 1.5 T in…Honey Khindri, B. Satyanarayana, D. Indumathi et al.·Nov 29, 2023SaveLearn