Study of MALTA2, a Depleted Monolithic Active Pixel Sensor, with grazing angles at CERN SPS 180 GeV/c hadron beamMALTA2 is a Depleted Monolithic Active Pixel Sensor designed to meet the challenging requirements of future collider experiments, in particularly extreme radiation tolerance and high hit rate. The…L. Li, P. Allport, I. Asensi Tortajada et al.·Feb 19, 2025SaveLearn
Amplitude analysis of (3686) γ KS0 KS0Using (271214)×106 (3686) events collected with the BESIII detector, we perform the first amplitude analysis of the radiative decay (3686) γ KS0 KS0 within the mass…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Feb 19, 2025SaveLearn
Partial wave analyses of ψ(3686) ppπ0 and ψ(3686) ppηUsing a sample of (271214)×106 ψ(3686) events collected with the BESIII detector, we perform partial wave analyses of the decays ψ(3686) ppπ0 and ψ(3686) ppη. The…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Feb 19, 2025SaveLearn
Measurement of the inelasticity distribution of neutrino-nucleon interactions for 80~GeV<E<560~GeV with IceCube DeepCoreWe report a study of the inelasticity distribution in the scattering of neutrinos of energy 80-560 GeV off nucleons. Using atmospheric muon neutrinos detected in IceCube's sub-array DeepCore during…IceCube Collaboration, R. Abbasi, M. Ackermann et al.·Feb 18, 2025SaveLearn
Development of systematic uncertainty-aware neural network trainings for binned-likelihood analyses at the LHCWe propose a neural network training method capable of accounting for the effects of systematic variations of the data model in the training process and describe its extension towards neural network…CMS Collaboration·Feb 18, 2025SaveLearn
Measurement of the strong-phase difference between D0 and D0 K+K-π+π- in bins of phase spaceA first determination of the strong-phase difference between D0 and D0 K+K-π+π- is performed using e+e-(3770) DD data collected by the BESIII detector…BESIII Collaboration·Feb 18, 2025SaveLearn
Neuromorphic Readout for Hadron CalorimetersWe simulate hadrons impinging on a homogeneous lead-tungstate (PbWO4) calorimeter to investigate how the resulting light yield and its temporal structure, as detected by an array of light-sensitive…Enrico Lupi, Abhishek, Max Aehle et al.·Feb 18, 2025SaveLearn
The Sliding Flux Ramp Demodulation Algorithm with High Sampling Rate in Microwave SQUID MultiplexerMicrowave SQUID Multiplexing (uMUX) is a widely used technique in the low temperature detectors community as it offers high capacity of reading out large scale Transition-Edge Sensor (TES) arrays. In…Guofu Liao, Congzhan Liu, Zhengwei Li et al.·Feb 18, 2025SaveLearn
Prospect for measurement of C\!P-violating observables in Bs0 Ds K decays at a future Z factoryA precise determination of the CKM angle γ from Bs0 oscillations in Bs0 Ds K decays offers a critical test of the Standard Model and probes for new physics. We present a…Ji Peng, Mingrui Zhao, Xiaolin Wang et al.·Feb 16, 2025SaveLearn
Search for the Cabibbo-suppressed decays c+0K+π0 and c+0K+π+π-Utilizing 4.5 fb- of e+e- annihilation data collected at center-of-mass energies ranging from 4599.53 MeV to 4698.82 MeV by the BESIII detector at the BEPCII collider, we search for the singly…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Feb 16, 2025SaveLearn
First Search for Dark Sector e+e- Explanations of the MiniBooNE Anomaly at MicroBooNEWe present MicroBooNE's first search for dark sector e+e- explanations of the long-standing MiniBooNE anomaly. The MiniBooNE anomaly has garnered significant attention over the past 20 years…MicroBooNE Collaboration, A. M. Abdullahi, P. Abratenko et al.·Feb 15, 2025SaveLearn
Implementation of a relativistic distorted wave impulse approximation model into the NEUT event generatorWe describe the implementation of a model for charged-current quasi-elastic (CCQE) neutrino-nucleus scattering in the NEUT Monte Carlo event generator. This model employs relativistic momentum…J. McKean, R. González-Jiménez, M. Kabirnezhad et al.·Feb 15, 2025SaveLearn
Recent Highlights from the Belle II ExperimentThe Belle II experiment operates at the SuperKEKB asymmetric-energy e+e- collider. During the Run 1 data taking, we have collected an integrated luminosity of 424 fb-1 of collision…Shu-Ping Lin·Feb 14, 2025SaveLearn
Angular analysis of B0→ K*0e+e- decaysAn angular analysis of B0→ K*0e+e- decays is presented using proton-proton collision data collected by the LHCb experiment at centre-of-mass energies of 7, 8 and 13 TeV,…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Feb 14, 2025SaveLearn
Reconstructing neutrinoless double beta decay event kinematics in a xenon gas detector with vertex taggingIf neutrinoless double beta decay is discovered, the next natural step would be understanding the lepton number violating physics responsible for it. Several alternatives exist beyond the exchange of…NEXT Collaboration, M. Martínez-Vara, K. Mistry et al.·Feb 14, 2025SaveLearn
Search for Pcs(4459) and Pcs(4338) in Upsilon(1S,2S) inclusive decays at BelleUsing data samples of 102 million Upsilon(1S) events and 158 million Upsilon(2S) events collected by the Belle detector at the KEKB asymmetric-energy e+e- collider, we search for [udsccbar]…I. Adachi, L. Aggarwal, H. Ahmed et al.·Feb 14, 2025SaveLearn
Weakly supervised anomaly detection for resonant new physics in the dijet final state using proton-proton collisions at s=13 TeV with the ATLAS detectorAn anomaly detection search for narrow-width resonances beyond the Standard Model that decay into a pair of jets is presented. The search is based on 139 fb-1 of proton-proton collisions at…ATLAS Collaboration·Feb 13, 2025SaveLearn
Multiple-cavities interferometric analysis for dark matter axions directional-sensitive search based on signal cross-correlation processingCurrent axion detection limits neglect the relevance of the relative velocity between the axion field and the detectors. However, this aspect can lead to a daily modulation of the detected axion…José Reina-Valero, Alejandro Díaz-Morcillo, Benito Gimeno et al.·Feb 13, 2025SaveLearn
An Automated Bandwidth Division for the LHCb Upgrade TriggerThe upgraded Large Hadron Collider beauty (LHCb) experiment is the first detector based at a hadron collider using a fully software based trigger. The first `High Level Trigger' stage (HLT1) reduces…T. Evans, C. Fitzpatrick, J. Horswill·Feb 13, 2025SaveLearn
CosmoLink: Portable Coincidence Detector for On-Site Muon Flux MeasurementThe CosmoLink project aims to develop low cost, low power, long range and portable form factor particle detectors for experimental and educational research on Cosmic Rays. Use of these detectors…Yuvaraj Elangovan·Feb 13, 2025SaveLearn
Search for Heavy Neutral Leptons with IceCube DeepCoreThe observation of neutrino oscillations has established that neutrinos have non-zero masses. This phenomenon is not explained by the Standard Model of particle physics, but one viable explanation to…R. Abbasi, M. Ackermann, J. Adams et al.·Feb 13, 2025SaveLearn
Measurement of W-boson differential cross-sections in proton-proton collisions with low pile-up data at s = 5.02 TeV and 13 TeV with the ATLAS detectorHigh precision single-differential W-boson production cross-sections as a function of electron or muon transverse momentum pT or their pseudorapity η, as well as…ATLAS Collaboration·Feb 13, 2025SaveLearn
Precise Measurement of the c0 Resonance Parameters and Branching Fractions of c0,c2π+π-/K+K-By analyzing a (3686) data sample containing (107.70.6)×106 events taken with the BESIII detector at the BEPCII storage ring in 2009, the c0 resonance parameters are…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Feb 13, 2025SaveLearn
CP violation studies at Super Tau-Charm FacilityCharge-parity (C\!P) violation in the tau-charm energy region is a promising area for sensitive tests of Standard Model (SM) predictions and searches for new, beyond the SM physics. A future…Hai-Yang Cheng, Zhi-Hui Guo, Xiao-Gang He et al.·Feb 13, 2025SaveLearn
70 Years of Hyperon Spectroscopy: A review of strange , baryons, and the spectrum of charmed and bottom baryonsThe first hyperon was discovered about 70 years ago, but the nature of these particles, particularly with regard to multistrange hyperons, and many of their properties can still be considered to be…Volker Crede, John Yelton·Feb 12, 2025SaveLearn