Binned Likelihood including Monte Carlo Statistical Uncertainty in Bayesian InferenceData analysis in HEP experiments often uses binned likelihood from data and finite Monte Carlo sample. Statistical uncertainty of Monte Carlo sample has been introduced in Frequentist Inference in…Shilin Liu, Clark McGrew·Apr 11, 2023SaveLearn
Detector signal characterization with a Bayesian network in XENONnTWe developed a detector signal characterization model based on a Bayesian network trained on the waveform attributes generated by a dual-phase xenon time projection chamber. By performing inference…XENON Collaboration, E. Aprile, K. Abe et al.·Apr 11, 2023SaveLearn
First performance measurements with the Analysis Grand ChallengeThe IRIS-HEP Analysis Grand Challenge (AGC) is designed to be a realistic environment for investigating how analysis methods scale to the demands of the HL-LHC. The analysis task is based on publicly…Oksana Shadura, Alexander Held·Apr 11, 2023SaveLearn
Probing Gluons at the Spin Physics DetectorThe Spin Physics Detector (SPD) at the Nuclotron based Ion Collider fAcility (NICA) is a multi-purpose experiment designed to study nucleon spin structure in the three dimensions. With capabilities…Alexey Guscov, Amaresh Datta, Anton Karpishkov et al.·Apr 10, 2023SaveLearn
Correction of the baseline fluctuations in the GEM-based ALICE TPCTo operate the ALICE Time Projection Chamber in continuous mode during the Run~3 and Run~4 data-taking periods of the Large Hadron Collider, the multi-wire proportional chamber-based readout was…ALICE TPC Collaboration·Apr 8, 2023SaveLearn
Nanosecond anomaly detection with decision trees and real-time application to exotic Higgs decaysWe present an interpretable implementation of the autoencoding algorithm, used as an anomaly detector, built with a forest of deep decision trees on FPGA, field programmable gate arrays. Scenarios at…Stephen Roche, Quincy Bayer, Benjamin Carlson et al.·Apr 7, 2023SaveLearn
Integrated and differential fiducial cross-section measurements for the vector boson fusion production of the Higgs boson in the H → WW→ eμ decay channel at 13 TeV with the ATLAS detectorThe vector-boson production cross-section for the Higgs boson decay in the H → WW → eμ channel is measured as a function of kinematic observables sensitive to the…ATLAS Collaboration·Apr 6, 2023SaveLearn
The indication for 40K geo-antineutrino flux with Borexino phase-III dataWe provide the indication of high flux of 40K geo-antineutrino and geo-neutrino (40K-geo-( + )) with Borexino Phase III data. This result was obtained by introducing a new…L. B. Bezrukov, I. S. Karpikov, V. V. Sinev·Apr 5, 2023SaveLearn
Comparing and improving hybrid deep learning algorithms for identifying and locating primary verticesUsing deep neural networks to identify and locate proton-proton collision points, or primary vertices, in LHCb has been studied for several years. Preliminary results demonstrated the ability for a…Simon Akar, Michael Peters, Henry Schreiner et al.·Apr 5, 2023SaveLearn
First demonstration of O(1\,ns) timing resolution in the MicroBooNE liquid argon time projection chamberMicroBooNE is a neutrino experiment located in the Booster Neutrino Beamline (BNB) at Fermilab, which collected data from 2015 to 2021. MicroBooNE's liquid argon time projection chamber (LArTPC) is…MicroBooNE collaboration, P. Abratenko, O. Alterkait et al.·Apr 4, 2023SaveLearn
Novel method for the identification of the production flavor of neutral charmed mesonsWe propose a new algorithm for the identification of the production flavor of neutral D mesons in the Belle II experiment. The algorithm exploits the correlation between the flavor of a…Belle II Collaboration, I. Adachi, L. Aggarwal et al.·Apr 4, 2023SaveLearn
Search for D*(2007)0μ+μ- in B-π-μ+μ- decaysThe very rare D*(2007)0μ+μ- decay is searched for by analysing B-π-μ+μ- decays. The analysis uses a sample of beauty mesons produced in proton-proton collisions…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Apr 4, 2023SaveLearn
Portable Programming Model Exploration for LArTPC Simulation in a Heterogeneous Computing Environment: OpenMP vs. SYCLThe evolution of the computing landscape has resulted in the proliferation of diverse hardware architectures, with different flavors of GPUs and other compute accelerators becoming more widely…Meifeng Lin, Zhihua Dong, Tianle Wang et al.·Apr 4, 2023SaveLearn
Search for top-philic heavy resonances in pp collisions at s=13 TeV with the ATLAS detectorA search for the associated production of a heavy resonance with a top-quark or a top-antitop-quark pair, and decaying into a tt pair is presented. The search uses the data recorded by the…ATLAS Collaboration·Apr 4, 2023SaveLearn
Evidence of off-shell Higgs boson production from ZZ leptonic decay channels and constraints on its total width with the ATLAS detectorThis Letter reports on a search for off-shell production of the Higgs boson using 139 fb-1 of pp collision data at s= 13 TeV collected by the ATLAS detector at the Large…ATLAS Collaboration·Apr 4, 2023SaveLearn
Search for bosonic super-weakly interacting massive particles at COSINE-100We present results of a search for bosonic super-weakly interacting massive particles (BSW) as keV scale dark matter candidates that is based on an exposure of 97.7 kg·year from the COSINE…G. Adhikari, N. Carlin, J. J. Choi et al.·Apr 4, 2023SaveLearn
Performance of the MALTA TelescopeMALTA is part of the Depleted Monolithic Active Pixel sensors designed in Tower 180nm CMOS imaging technology. A custom telescope with six MALTA planes has been developed for test beam campaigns at…Milou van Rijnbach, Giuliano Gustavino, Phil Allport et al.·Apr 3, 2023SaveLearn
The ESSnuSB design study: overview and future prospectsESSnuSB is a design study for an experiment to measure the CP violation in the leptonic sector at the second neutrino oscillation maximum using a neutrino beam driven by the uniquely powerful ESS…ESSnuSB Collaboration, A. Alekou, E. Baussan et al.·Mar 30, 2023SaveLearn
New techniques for jet calibration with the ATLAS detectorA determination of the jet energy scale is presented using proton-proton collision data with a centre-of-mass energy of s=13 TeV, corresponding to an integrated luminosity of 140…ATLAS Collaboration·Mar 30, 2023SaveLearn
First Simultaneous Determination of Inclusive and Exclusive |Vub|The first simultaneous determination of the absolute value of the Cabibbo-Kobayashi-Maskawa matrix element Vub using inclusive and exclusive decays is performed with the full Belle data set at…Belle Collaboration, L. Cao, F. Bernlochner et al.·Mar 30, 2023SaveLearn
Observation of the (3S) meson and suppression of states in PbPb collisions at sNN = 5.02 TeVThe production of (2S) and (3S) mesons in lead-lead (PbPb) and proton-proton (pp) collisions is studied in their dimuon decay channel using the CMS detector at the LHC. The…CMS Collaboration·Mar 29, 2023SaveLearn
Impact of cross-section uncertainties on supernova neutrino spectral parameter fitting in the Deep Underground Neutrino ExperimentA primary goal of the upcoming Deep Underground Neutrino Experiment (DUNE) is to measure the O(10) MeV neutrinos produced by a Galactic core-collapse supernova if one should occur during…DUNE Collaboration, A. Abed Abud, B. Abi et al.·Mar 29, 2023SaveLearn
Production of π+ and K+ mesons in argon-nucleus interactions at 3.2 AGeVFirst physics results of the BM@N experiment at the Nuclotron/NICA complex are presented on π+ and K+ meson production in interactions of an argon beam with fixed targets of C, Al, Cu, Sn and Pb…S. Afanasiev, G. Agakishiev, E. Aleksandrov et al.·Mar 28, 2023SaveLearn
The DL Advocate: Playing the devil's advocate with hidden systematic uncertaintiesWe propose a new method based on machine learning to play the devil's advocate and investigate the impact of unknown systematic effects in a quantitative way. This method proceeds by reversing…Andrei Golutvin, Aleksandr Iniukhin, Andrea Mauri et al.·Mar 28, 2023SaveLearn
STCF Conceptual Design Report: Volume 1 -- Physics & DetectorThe Super τ-Charm facility (STCF) is an electron-positron collider proposed by the Chinese particle physics community. It is designed to operate in a center-of-mass energy range from 2 to 7 GeV…M. Achasov, X. C. Ai, R. Aliberti et al.·Mar 28, 2023SaveLearn