RTL Fault Injection of a Deployed Graph Neural Network Trigger for Belle IIAs particle physics detectors grow in scale, High Energy Physics experiments must process ever-increasing data volumes. Level-1 trigger systems, implemented on Field-Programmable Gate Arrays and…Georgios Sotiropoulos, Marc Neu, Tanja Harbaum et al.·Jul 17, 2026SaveLearn
CaloTrilogy: Toward a Breakthrough in One-Step, End-to-End, Physics-Guided Shower Generation for Modern CalorimetersHigh-precision calorimeter simulation at current and future colliders imposes rapidly growing computational demands, motivating the development of machine-learning surrogates for traditional Monte…Cheng Jiang, Sitian Qian, Kevin Pedro et al.·Jul 17, 2026SaveLearn
Searches for Light Dark Matter and Evidence of Coherent Elastic Neutrino-Nucleus Scattering of Solar Neutrinos with the LUX-ZEPLIN (LZ) ExperimentWe present searches for light dark matter (DM) with masses 3-9 GeV/c2 in the presence of coherent elastic neutrino-nucleus scattering (CEνNS) from 8B solar neutrinos with the LUX-ZEPLIN…D. S. Akerib, A. K. Al Musalhi, F. Alder et al.·Jul 17, 2026SaveLearn
Demonstration of deuterium's enhanced sensitivity to symmetry violations governed by the Standard-Model ExtensionWe have performed hyperfine spectroscopy of two transitions in ground-state deuterium and searched for violations of CPT and Lorentz symmetry that would manifest as sidereal variations of the…Amit Nanda, Daniel Comparat, Olivier Dulieu et al.·Jul 17, 2026SaveLearn
Mitigating Detector Ageing Effects with Graph-Based Multi-Modal Track Reconstruction at Belle IILarge backgrounds that can lead to hardware failures and the degradation of detector gain impact the track finding in the Belle II central drift chamber. These conditions lead to spatially…Lea Reuter, Tristan Brandes, Giacomo De Pietro et al.·Jul 16, 2026SaveLearn
A Differential Neutral-to-Charged Current Double-Proton Observable for Studying Short-Range Correlations in Neutrino--Argon ScatteringTwo-nucleon emission is a leading uncertainty in neutrino--nucleus interaction modeling, and no neutrino measurement constrains its short-range-correlation (SRC) component. We propose such a…A. Bueno, D. Garcia-Gamez, C. Martin-Morales·Jul 16, 2026SaveLearn
Probing unexplored spin-dependent dark matter-proton coupling with few-photoelectron threshold in COSINE-100We report new constraints on the spin-dependent scattering cross section between low-mass dark matter and protons using data collected by the COSINE-100 experiment. By implementing a specialized…W. K. Kim, N. Carlin, J. Y. Cho et al.·Jul 16, 2026SaveLearn
Observation of CP violation in B0\!J-3mu/-2muψρ(770)0 decaysThe time-dependent CP asymmetry in B0\!J-3mu/-2muψρ(770)0 decays is measured using proton-proton collision data corresponding to an integrated luminosity of…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Jul 16, 2026SaveLearn
Measurement of forward photon production cross-section in pp collisions at s = 510 GeV with RHICf detectorThis study reported the inclusive differential production cross-section of photons in six pseudorapidity regions: 6.1 < η < 6.5, 6.5 < η < 7.0, 7.0 < η <7.5, 7.5 < η <8.0, 8.0 < η < 8.5,…O. Adriani, E. Berti, L. Bonechi et al.·Jul 16, 2026SaveLearn
A Low-energy Threshold and Multi-messenger Trigger System for the JUNO ExperimentThe Jiangmen Underground Neutrino Observatory (JUNO) is a 20-kiloton liquid scintillator neutrino detector, located 650 meters (1800 m.w.e.) underground in Jiangmen, Guangdong, China. JUNO is…Thomas Adam, Fengpeng An, Costas Andreopoulos et al.·Jul 15, 2026SaveLearn
Measurement of the double Dalitz decay η e+e-e+e-Using a data sample of (1.0087 0.0044) × 1010 J/ψ events collected with the BESIII detector, we study the rare double Dalitz decay of η→ e+e-e+e- through the…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jul 15, 2026SaveLearn
Search for long-lived particles using displaced vertices of oppositely charged leptons in 140 fb-1 of pp collisions at s = 13 TeV with the ATLAS detectorA search is presented for long-lived particles decaying into an oppositely charged lepton pair, μ+μ-, e+e-, or eμ, that form a vertex within the inner tracking system of…ATLAS Collaboration·Jul 15, 2026SaveLearn
Search for emerging jets in pp collisions at s = 13 TeV with the ATLAS experimentA search is presented for emerging jets using 140 fb-1 of proton-proton collision data at s = 13 TeV, collected by the ATLAS experiment between 2015 and 2018. The search looks for the…ATLAS Collaboration·Jul 15, 2026SaveLearn
Search for decays of the Higgs boson into scalar particles decaying into four or six b-quarks using pp collisions at s= 13\,TeV with the ATLAS detectorA search for exotic decays of the Higgs boson H into new scalar or pseudoscalar particles that subsequently decay into b-quarks is presented. The search considers ZH production with several…ATLAS Collaboration·Jul 15, 2026SaveLearn
Electroweak diboson production in association with a high-mass dijet system in semileptonic final states from pp collisions at s = 13 TeV with the ATLAS detectorThis paper reports the observation of electroweak diboson (WW/WZ/ZZ) production in association with a high-mass dijet system, in which final states with one boson decaying leptonically and the…ATLAS Collaboration·Jul 15, 2026SaveLearn
Open Charm production in proton-proton collisions at s = 13.6 TeV with Pythia event generatorCharm and beauty are heavy quarks with observed masses of 1.28 GeV/c2 and 4.18 GeV/c2 respectively. They are produced in initial hard scattering processes. Due to their small…Randhir Singh·Jul 15, 2026SaveLearn
Observation of pair production of longitudinally polarized Z bosons in four-lepton final state with the ATLAS detectorThe production of two longitudinally polarized Z bosons is measured using proton-proton collision data recorded by the ATLAS experiment at a center-of-mass energy s=13.6 TeV and with an…ATLAS Collaboration·Jul 14, 2026SaveLearn
Search for the decays B+(c) μ+ νμγA search for the radiative leptonic decays B+μ+νμγ and B+cμ+νμγ is performed using proton-proton collision data collected with the LHCb experiment at a center-of-mass energy of…LHCb collaboration, R. Aaij, M. Abdelfatah et al.·Jul 14, 2026SaveLearn
First double-differential measurement of pionless charged-current muon neutrino interactions using kinematic imbalance observables on carbon and oxygen with the T2K experimentWe report the first measurement of muon-neutrino charged-current cross section as a function of kinematic imbalance (KI) observables on oxygen with no pions and at least one proton in the final…K. Abe, S. Abe, H. Adhikary et al.·Jul 14, 2026SaveLearn
Improved muon energy estimation using a detailed model of multiple Coulomb scattering in the MicroBooNE LArTPCWe present an improved technique for estimating a muon's energy by measuring the deflections along its path inside the MicroBooNE detector from multiple Coulomb scattering (MCS). This approach…MicroBooNE Collaboration, P. Abratenko, D. Andrade Aldana et al.·Jul 14, 2026SaveLearn
Combined effective field theory interpretation of measurements sensitive to quartic gauge boson couplings in pp collisions at s=13 TeV with the ATLAS detectorA combination of measurements sensitive to anomalous quartic electroweak gauge boson couplings is presented using proton-proton collision data collected by the ATLAS detector at s = 13 TeV…ATLAS Collaboration·Jul 14, 2026SaveLearn
Lepton and photon energy scale and resolution corrections based on the minimization of an analytical likelihood: IJazZ2.0We present a novel method to determine lepton energy scale and resolution corrections by means of an analytical likelihood maximization applied to Drell--Yan \(Z \) events. The approach…F. Couderc, P. Gaigne, M. Ö. Sahin·Jul 14, 2026SaveLearn
Analytical Markov Chain for Spatiotemporal Flux Evolution of the Inner Filter Effect in Fluorescent MediaCharacterizing emission and decay time spectra in multi-component fluorescent media is essential for identifying intrinsic material properties and optimizing detectors. However, wavelength evolution…Xuhui Yang, Guofu Cao·Jul 13, 2026SaveLearn
Machine Learning-Based Reconstruction for Resistive Silicon SensorsLow-Gain Avalanche Diodes (LGADs) and AC-coupled Low-Gain Avalanche Diodes (AC-LGADs) are promising technologies for precision timing and four-dimensional tracking. In AC-LGADs, the AC pad is coupled…Alexander Aoki, Gaetano Barone, Leena Diehl et al.·Jul 13, 2026SaveLearn
Study of the proccess e+e- π+π-π0π0η in the c.m. energy range 1.6--2.0 GeV with the CMD-3 detectorThe cross section of the process e+e- π+π-π0π0η has been measured using a data sample with the integrated luminosity of 372 pb-1 collected with the CMD-3 detector at the VEPP-2000…R. R. Akhmetshin, A. N. Amirkhanov, A. V. Anisenkova et al.·Jul 13, 2026SaveLearn