Conceptual Design Report of the SUPAX ExperimentThe SUPerconduction AXion search experiment (Supax) is a haloscope designed to probe axion-like particles (ALPs) as candidates for dark matter and solutions to the strong CP problem. ALPs are…Dhruv Chouhan, Tim Schneemann, Kristof Schmieden et al.·May 12, 2025SaveLearn
Resolution Studies for Future DIRC DetectorsThe resolution of Cherenkov detectors using the DIRC method is mainly limited by three components: photon loss due to steep angles of incidence, dispersion effects, and angle straggling due to the…Mustafa Schmidt, Afaf Wasili·May 12, 2025SaveLearn
Detector Requirements, Design, and Technologies for the FCC-ee Higgs, electroweak, and top factoryThe proposed high-luminosity, circular electron-positron collider, FCC-ee, provides unparalleled opportunities for precise exploration of Higgs, electroweak, top, flavour, and beyond standard model…Mogens Dam·May 10, 2025SaveLearn
Adjusting optical cavity birefringence with wavelength tunable laser for axion searchesAxions have attracted attention as promising candidates for dark matter (DM). Although axions have been intensively searched for, they have not been observed yet. Recently, novel experiments to…Hinata Takidera, Hiroki Fujimoto, Yuka Oshima et al.·May 10, 2025SaveLearn
Particle Identification with Deep Neural Networks Across Collision Energies in Simulated Proton-Proton CollisionsThis study demonstrates a proof-of-concept application of a deep neural network for particle identification in simulated high transverse momentum proton-proton collisions, with a focus on evaluating…Omar M. Khalaf, Ahmed M. Hamed·May 10, 2025SaveLearn
Neutrinos from Stored Muons (nuSTORM)The Neutrinos from Stored Muons, nuSTORM, facility has been designed to deliver a definitive neutrino-nucleus scattering programme using beams of ,e- and ,μ- from the decay of muons…L. Alvarez Ruso, W. Chang, J. Franklin et al.·May 9, 2025SaveLearn
CODEX-b: Opening New Windows to the Long-Lived Particle Frontier at the LHCThis document is written as a contribution to the European Strategy of Particle Physics (ESPP) update. We offer a detailed overview of current developments and future directions for the CODEX-b…Giulio Aielli, Juliette Alimena, Saul Balcarcel-Salazar et al.·May 9, 2025SaveLearn
Search for solar axions produced through the axion-electron coupling gae using a new GridPix detector at CASTWe present a search for solar axions produced through the axion-electron coupling (gae) using data from a novel 7-GridPix detector installed at the CERN Axion Solar Telescope (CAST). The…K. Altenmüller, V. Anastassopoulos, S. Arguedas-Cuendis et al.·May 9, 2025SaveLearn
Measurement of the phase between strong and electromagnetic amplitudes in the decay J/φηThe first direct measurement of the relative phase between the strong and electromagnetic amplitudes for a J/ decaying into a vector-pseudoscalar final state is performed using 26 energy points…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·May 9, 2025SaveLearn
Physics Opportunity at the Electron-Ion Collider (EIC)The Electron-Ion Collider (EIC) is a next-generation facility under construction at Brookhaven National Laboratory, uniquely designed to collide polarized electrons with polarized protons and ions.…Satoshi Yano·May 9, 2025SaveLearn
Low metallicity solar model finds the prove in Borexino dataThe Borexino Collaboration interprets its data within the framework of Bulk Silicate Earth model and the model of the Sun with high metallicity. Other authors have given a different interpretation of…L. B. Bezrukov, A. S. Bykovsky, V. V. Sinev·May 8, 2025SaveLearn
Search for dark matter produced in association with one or two top quarks in proton-proton collisions at s = 13 TeVA search is performed for dark matter (DM) produced in association with a single top quark or a pair of top quarks using the data collected with the CMS detector at the LHC from proton-proton…CMS Collaboration·May 8, 2025SaveLearn
Three-dimensional femtoscopy for proton pairs in heavy-ion collisionsFemtoscopy, a technique of measuring the size and the dynamics of the system created in heavy-ion collisions is used extensively in experiments at RHIC, LHC, SPS, and the FAIR/GSI. Analysis for pairs…Adam Kisiel·May 8, 2025SaveLearn
Recent results of (semi)leptonic decays of charm hadrons at BESIIIIn this talk, we report the recent measurements of (semi)leptonic decays of charm mesons from the BESIII experiment, including D+μ+μ, D+τ+τ,…Xiang Pan·May 8, 2025SaveLearn
Axion Dark Matter Search with Near-KSVZ Sensitivity Using the TM020 ModeDark matter remains one of the most profound mysteries in modern physics, with axions, a hypothetical particle proposed to resolve the strong CP problem, standing as a compelling candidate. Among…Sungjae Bae, Junu Jeong, Younggeun Kim et al.·May 8, 2025SaveLearn
Charged Lepton Flavor Violating Experiments with MuonsWe report on the status of charged lepton flavor violating (CLFV) experiments with muons. We focus on the three "golden channels": μ+ → e+ γ, $μ+ → e+ e-…Dylan Palo·May 7, 2025SaveLearn
Measurement of reactor antineutrino oscillation at SNO+The SNO+ collaboration reports its second spectral analysis of reactor antineutrino oscillation using 286 tonne-years of new data. The measured energies of reactor antineutrino candidates were fitted…SNO+ Collaboration, :, M. Abreu et al.·May 7, 2025SaveLearn
Measurement of neutron production in atmospheric neutrino interactions at Super-KamiokandeWe present measurements of total neutron production from atmospheric neutrino interactions in water, analyzed as a function of electron-equivalent visible energy over a range of 30 MeV to 10 GeV.…Kamiokande collaboration, S. Han, K. Abe et al.·May 7, 2025SaveLearn
Probing light nuclei production mechanism by measuring nucleus production in and out of jetsThe production mechanism of (anti)nuclei in ultrarelativistic hadronic collisions is under debate in the scientific community. Two successful models used for the description of the experimental…Chiara Pinto·May 7, 2025SaveLearn
Measurement of the branching fraction ratio RK at large dilepton invariant massA test of lepton universality between muons and electrons is performed using B+ K++- decays (where = e, μ), in the dilepton invariant-mass-squared region above 14.3…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·May 6, 2025SaveLearn
Simulation-based performance comparison of varied pitch sizes GEM detectorsGas Electron Multiplier (GEM) detectors, typically featuring a standard pitch size of 140 μm and an inner hole diameter of 50 μm, are extensively utilized in high-energy physics experiments…Rajiv Gupta, Gauri Devi, Sunidhi Saxena et al.·May 6, 2025SaveLearn
Stability study of GEM chamber using radioactive sourceGas Electron Multiplier (GEM) is a cutting edge Micro Pattern Gaseous detector (MPGD) technology suitable as tracking device in high rate Heavy-Ion (HI) experiments for their good spatial resolution…S. Mandal, S. Gope, S. Das et al.·May 6, 2025SaveLearn
Observation of resonant contribution to the e+e- -+ around 4.2 GeV and evidence of (3770) -+Using e+e- collision data corresponding to a total integrated luminosity of 22.7 fb-1, collected at center-of-mass energies between 3.7 and 4.7 GeV with the BESIII detector, we present a…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·May 6, 2025SaveLearn
First Measurement of the Muon Neutrino Interaction Cross Section and Flux as a Function of Energy at the LHC with FASERThis letter presents the measurement of the energy-dependent neutrino-nucleon cross section in tungsten and the differential flux of muon neutrinos and anti-neutrinos. The analysis is performed using…FASER Collaboration, Roshan Mammen Abraham, Xiaocong Ai et al.·May 6, 2025SaveLearn
Fast and Precise Track Fitting with Machine LearningEfficient and accurate particle tracking is crucial for measuring Standard Model parameters and searching for new physics. This task consists of two major computational steps: track finding, the…Ryan Miller, Alexander Shmakov, Kyuho Oh et al.·May 5, 2025SaveLearn