Search for the FCNC charmonium decay J/ D0 μ+ μ- + c.c.Based on a data sample of (10087 44) × 106 J/ events taken with the BESIII detector, we search for the flavor-changing neutral current charmonium decay $J/ D0 μ+…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jan 14, 2025SaveLearn
Search for the production of Higgs-portal scalar bosons in the NuMI beam using the MicroBooNE detectorWe present the strongest experimental limits to date on the mixing angle, θ, with which a new scalar particle, S, mixes with the Higgs field in the mass range $110 MeV<mS<155…MicroBooNE collaboration, P. Abratenko, D. Andrade Aldana et al.·Jan 14, 2025SaveLearn
Overview of the latest ATLAS and ATLAS-AFP photoproduction resultsA key focus of the physics program at the LHC is the study of head-on proton-proton collisions. However, an important class of physics can be studied for cases where the protons narrowly miss one…Andre Sopczak·Jan 13, 2025SaveLearn
Efficient cosmic ray generator for particle detector simulationsTraditional cosmic ray simulations make use of the Montecarlo method in a very naive way to randomise energy and direction for each simulated particle. The flux of cosmic rays is modelled as a rain…David Díez Ibáñez, Luis Obis Aparicio·Jan 13, 2025SaveLearn
Study of light-meson resonances decaying to K0 S K π in the B (K0 S K π) K channelsA study is presented of B+ K0 S K- π+ K- and B+ K0 S K+ π- K+ decays based on the analysis of proton-proton collision data collected with the LHCb detector at…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Jan 11, 2025SaveLearn
Search for K0S invisible decaysBased on (1.00870.0044)×1010 J/ events collected with the BESIII detector at the BEPCII e+e- storage ring, we search for KS0 invisible decays via the $J/ φ…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jan 11, 2025SaveLearn
Towards An Updated Simulation of the Booster Neutrino BeamPrecise, accurate neutrino flux predictions for neutrino beam experiments are crucial for physics results. Flux predictions for the Booster Neutrino Beam at Fermilab were first published in 2009 by…Josephine L Paton·Jan 10, 2025SaveLearn
Detecting LHC Neutrinos at Surface LevelThe first direct detection of neutrinos at the LHC not only marks the beginning of a novel collider neutrino program at CERN but also motivates considering additional neutrino detectors to fully…Akitaka Ariga, Steven Barwick, Jamie Boyd et al.·Jan 10, 2025SaveLearn
Searches for Top-associated Dark Matter Production at the LHCRecent searches for dark matter (DM) produced in association with top quarks from the ATLAS and CMS experiments using data collected between 2015 and 2018 are presented. These comprise searches from…Dominic Stafford·Jan 10, 2025SaveLearn
First simultaneous measurement of single and pair production of top quarks in association with a Z boson at the LHCThe first simultaneous measurement of single and pair production of top quarks in association with a Z boson (tZq, tWZ and ttZ) is presented, including both inclusive and differential…Konstantin Sharko·Jan 10, 2025SaveLearn
Collective effects in strong interaction processes: experimental highlightsCollective effects are reviewed for collisions of various systems - from proton-proton to heavy ion - in wide energy range. In proton-proton interactions studies of hadron jets devote to the better…V. A. Okorokov·Jan 10, 2025SaveLearn
Evidential Deep Learning for Uncertainty Quantification and Out-of-Distribution Detection in Jet Identification using Deep Neural NetworksCurrent methods commonly used for uncertainty quantification (UQ) in deep learning (DL) models utilize Bayesian methods which are computationally expensive and time-consuming. In this paper, we…Ayush Khot, Xiwei Wang, Avik Roy et al.·Jan 10, 2025SaveLearn
Direct observation of coherent elastic antineutrino-nucleus scatteringNeutrinos are elementary particles that interact only very weakly with matter. Neutrino experiments are, therefore, usually big, with masses in the multi-tonne range. The thresholdless interaction of…N. Ackermann, H. Bonet, A. Bonhomme et al.·Jan 9, 2025SaveLearn
Search for the leptonic decay D+ e+eWe search for the leptonic decay D+ e+e using an e+e- collision data sample with an integrated luminosity of 20.3~fb-1 collected with the BESIII detector at the center-of-mass…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jan 8, 2025SaveLearn
The ENUBET monitored neutrino beam and its implementation at CERNThe ENUBET project recently concluded the R&D for a site independent design of a monitored neutrino beam for high precision cross section measurements, in which the neutrino flux is inferred from the…ENUBET collaboration, L. Halić, F. Acerbi et al.·Jan 8, 2025SaveLearn
Observation of the W-annihilation process Ds+ ω+ and measurement of Ds+ φ+ in D+s π+π+π-π0π0 decaysWe present the first amplitude analysis and branching fraction measurement of the decay D+s π+π+π-π0π0, using e+e- collision data collected with the BESIII detector at…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jan 8, 2025SaveLearn
AI-assisted design of experiments at the frontiers of computation: methods and new perspectivesDesigning the next generation colliders and detectors involves solving optimization problems in high-dimensional spaces where the optimal solutions may nest in regions that even a team of expert…Pietro Vischia·Jan 8, 2025SaveLearn
Study of the electromagnetic Dalitz decay J/ e+e- π0We report the first measurement of the di-electron invariant mass dependent transition form factor in the electromagnetic Dalitz decay J/ e+e- π0 using (10087 44) × 106…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jan 8, 2025SaveLearn
GraphNeT 2.0 -- A Deep Learning Library for Neutrino TelescopesNeutrino telescopes, an extension of traditional multiwavelength astronomy, provide a complementary view of the universe using neutrinos. Differences in detector geometry and detection medium mean…Rasmus F. Ørsøe, Aske Rosted, GraphNeT Team·Jan 7, 2025SaveLearn
Search for double beta decay of 106Cd Monte Carlo simulation and cosmogenic activation of the CdWO4 detectrosThe thesis describes the experimental setup designed to study the decay spectrum of 106Cd, a candidate for positive double-β decay and the Monte Carlo simulation used to estimate the background…Ester Ricci·Jan 7, 2025SaveLearn
Top quark spin and quantum entanglement in the ATLAS experimentTop quark pair spin correlation measurements performed by the ATLAS experiment using pp collisions at the CERN Large Hadron Collider are summarized. Moreover, the measurement of a specific…Roman Lysak·Jan 7, 2025SaveLearn
Design, Construction, and Testing of the APOLLO ATCA Blades for Use at the HL-LHCThe Apollo Advanced Telecommunications Computing Architecture (ATCA) platform is an open-source design consisting of a generic "Service Module" (SM) and a customizable "Command Module" (CM), allowing…Alp Akpinar, Aymeric Blaizot, Serhii Cholak et al.·Jan 7, 2025SaveLearn
Search potential for direct slepton pair production at the CEPC with s = 360 GeVThe Circular Electron Positron Collider (CEPC) is designed to operate at the key center-of-mass energies: 91.2 GeV as a Z factory for precision Z boson studies,≈ 160 GeV at the threshold for…Feng Lyu, Jiarong Yuan, Huajie Cheng et al.·Jan 7, 2025SaveLearn
CMS Upgrades for the High-Luminosity LHC EraThe High-Luminosity LHC (HL-LHC) era, set to begin in 2029, will provide the general-purpose experiments with an instantaneous luminosity of up to L = 7.5 × 1034 cm-2…Thiago R. F. P. Tomei·Jan 6, 2025SaveLearn
Design and Implementation of the Cosmic Ray Tagger System for the ICARUS detector at FNALThe ICARUS-T600 Liquid Argon Time Projection Chamber is operating at Fermilab at shallow depth and thus exposed to a high flux of cosmic rays that can fake neutrino interactions. A cosmic ray tagging…A. Aduszkiewicz, L. Bagby, B. Behera et al.·Jan 6, 2025SaveLearn