Search for solar axions by Primakoff effect with the full dataset of the CDEX-1B ExperimentWe present the first limit on gAγ coupling constant using the Bragg-Primakoff conversion based on an exposure of 1107.5 kg days of data from the CDEX-1B experiment at the China Jinping…L. T. Yang, S. K. Liu, Q. Yue et al.·May 12, 2024SaveLearn
Characterization of the PADME positron beam for the X17 measurementThis paper presents a detailed characterization of the positron beam delivered by the Beam Test Facility at Laboratori Nazionali of Frascati to the PADME experiment during Run III, which took place…S. Bertelli, F. Bossi, B. Buonomo et al.·May 12, 2024SaveLearn
Search for exotic physics at BESIIIExotic physics typically encompasses two categories of exotic particles: ``dark" particles beyond the standard model and exotic hadrons within the extended standard model. We present a summary of the…Zhijun Li, Zhengyun You·May 12, 2024SaveLearn
Inclusive and differential cross-section measurements in tW with CMS in Run 3The first measurements of the inclusive and normalised differential cross sections for the production of single top quarks in association with a W boson in proton-proton collisions at a…Alejandro Soto Rodríguez·May 11, 2024SaveLearn
Search for time-dependent CP violation in D0 → π+ π- π0 decaysA measurement of time-dependent CP violation in D0 → π+ π- π0 decays using a pp collision data sample collected by the LHCb experiment in 2012 and from 2015 to 2018,…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·May 10, 2024SaveLearn
Measurement of the e+e- p pπ0 cross section at s=2.1000-3.0800 GeVThe process e+e- ppπ0 is studied at 20 center-of-mass energies ranging from 2.1000 to 3.0800 GeV using 636.8 pb-1 of data collected with the BESIII detector operating at…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·May 10, 2024SaveLearn
In-medium changes of nucleon cross sections tested in neutrino-induced reactionsHistorically studied in the context of heavy-ion collisions, the extent to which free nucleon-nucleon cross sections are modified in-medium remains undetermined by these data sets. Therefore, we…B. Bogart, K. Gallmeister, U. Mosel·May 9, 2024SaveLearn
Daily modulations and broadband strategy in axion searches. An application with CAST-CAPP detectorIt has been previously advocated that the presence of the daily and annual modulations of the axion flux on the Earth's surface may dramatically change the strategy of the axion searches. The…F. Caspers, C. M. Adair, K. Altenmüller et al.·May 9, 2024SaveLearn
Probing CPV mixing in the Higgs sector in VBF at 1 TeV ILCWith the current precision of measurements by the ATLAS and CMS experiments, it cannot be excluded that a SM-like Higgs boson is a CP violating mixture of CP-even and CP-odd states. We explore this…N. Vukašinović, I. Božović-Jelisavčić, G. Kačarević et al.·May 9, 2024SaveLearn
Development, Characterization and Production of a novel Water-based Liquid Scintillator based on the Surfactant TRITON X-100Water-based Liquid Scintillator (WbLS) is a novel detector medium for particle physics experiments. Applications range from the use as hybrid Cherenkov/scintillation target in low-energy and…Hans Th. J. Steiger, Manuel Böhles, Matthias Raphael Stock et al.·May 9, 2024SaveLearn
Reactor neutrino liquid xenon coherent elastic scattering experimentCoherent elastic neutrino-nucleus scattering (CEvNS) provides a unique probe for neutrino properties Beyond the Standard Model (BSM) physics. REactor neutrino LIquid xenon Coherent Scattering…Chang Cai, Guocai Chen, Jiangyu Chen et al.·May 9, 2024SaveLearn
Comparative Analysis of Single Charged Particle Production in Proton-Carbon Interactions at High EnergiesThe generation of charged pions, kaons, and protons from proton beam incident on Carbon at 31 GeV/c is calculated and compared with the results of the NA61/SHINE experiment. Predictions of the single…R Lalnuntluanga, A Giri·May 8, 2024SaveLearn
Search for production of a single vector-like quark decaying to tH or tZ in the all-hadronic final state in pp collisions at s = 13 TeVA search for electroweak production of a single vector-like T quark in association with a bottom (b) quark in the all-hadronic decay channel is presented. This search uses proton-proton collision…CMS Collaboration·May 8, 2024SaveLearn
Underlying-event studies with strange hadrons in pp collisions at s = 13 TeV with the ATLAS detectorProperties of the underlying-event in pp interactions are investigated primarily via the strange hadrons KS0, and , as reconstructed using the ATLAS detector at the…ATLAS Collaboration·May 8, 2024SaveLearn
ATLAS searches for additional scalars and exotic Higgs boson decays with the LHC Run 2 datasetThis report reviews the published results of searches for possible additional scalar particles and exotic decays of the Higgs boson performed by the ATLAS Collaboration using up to 140 fb-1 of…ATLAS Collaboration·May 8, 2024SaveLearn
Calibration of a soft secondary vertex tagger using proton-proton collisions at s=13 TeV with the ATLAS detectorSeveral processes studied by the ATLAS experiment at the Large Hadron Collider produce low-momentum b-flavored hadrons in the final state. This paper describes the calibration of a dedicated…ATLAS Collaboration·May 6, 2024SaveLearn
SSLG4: A Novel Scintillator Simulation Library for Geant4This study introduces a new Scintillator Simulation Library called SSLG4 for the Geant4 Monte Carlo simulation package. With SSLG4, we aim to enhance efficiency and accelerate progress in optical…Mustafa Kandemir, Emrah Tiras, Burcu Kirezli et al.·May 3, 2024SaveLearn
Measurement of atmospheric neutrino oscillation parameters using convolutional neural networks with 9.3 years of data in IceCube DeepCoreThe DeepCore sub-detector of the IceCube Neutrino Observatory provides access to neutrinos with energies above approximately 5 GeV. Data taken between 2012-2021 (3,387 days) are utilized for an…IceCube Collaboration·May 3, 2024SaveLearn
Echo-free quality factor of a multilayer axion haloscopeWe report a methodology to determine the quality factor (Q) in implementations of the so-called dielectric haloscope, a new concept of wavy dark matter detector equipped with a multilayered…Juan F. Hernández-Cabrera, Javier De Miguel, E. Hernández-Suárez et al.·May 2, 2024SaveLearn
Properties of Charge Recombination in Liquid ArgonLiquid argon is an excellent medium for detecting particles, given its yields and transport properties of light and charge. The technology of liquid argon time projection chambers has reached its…Ettore Segreto·May 1, 2024SaveLearn
Search for new resonances decaying to pairs of merged diphotons in proton-proton collisions at s = 13 TeVA search is presented for an extended Higgs sector with two new particles, X and φ, in the process X φφ (γγ)(γγ). Novel neural networks classify events…CMS Collaboration·May 1, 2024SaveLearn
Search for charged lepton flavor violation in J/ decays at BESIIIIn the Standard Model, charged lepton flavor violation (CLFV) is heavily suppressed by tiny neutrino mass, while many theoretical models can enhance CLFV effects up to a detectable level. The…Xudong Yu·May 1, 2024SaveLearn
Amplitude analysis and branching fraction measurement of B+ D*-D+sπ+ decaysThe decays of the B+ meson to the final state D*-D+sπ+ are studied in proton-proton collision data collected with the LHCb detector at centre-of-mass energies of 7, 8, and 13…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Apr 30, 2024SaveLearn
First observation of b0 → c(*)++ D(*)- K- decaysThe four decays, b0 → c(*)++ D(*)- K-, are observed for the first time using proton-proton collision data collected with the LHCb detector at a centre-of-mass…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Apr 30, 2024SaveLearn
Search for heavy neutral Higgs bosons decaying into a top quark pair in 140 fb-1 of proton-proton collision data at s=13 TeV with the ATLAS detectorA search for heavy pseudo-scalar (A) and scalar (H) Higgs bosons decaying into a top-quark pair (tt) has been performed with 140 fb-1 of proton-proton collision data collected by the…ATLAS Collaboration·Apr 29, 2024SaveLearn