Modeling and characterization of TES-based detectors for the Ricochet experimentCoherent elastic neutrino-nucleus scattering (CE) offers a valuable approach in searching for physics beyond the Standard Model. The Ricochet experiment aims to perform a precision measurement…R. Chen, E. Figueroa-Feliciano, G. Bratrud et al.·Nov 21, 2023SaveLearn
Measurement of the muon magnetic anomaly aμ in the Muon g-2 experiment at FermilabThe Fermilab Muon g-2 experiment measures the muon anomalous magnetic moment with high precision. Together with recent improvements on the theory front, the first results of the experiment confirm…Marco Incagli·Nov 21, 2023SaveLearn
Search for the decay Bs0 J/π0 at Belle experimentWe have analyzed 121.4 fb-1 of data collected at the (5S) resonance by the Belle experiment using the KEKB asymmetric-energy e+e- collider to search for the decay $Bs0…Belle Collaboration, D. Kumar, B. Bhuyan et al.·Nov 21, 2023SaveLearn
DeepTreeGAN: Fast Generation of High Dimensional Point CloudsIn High Energy Physics, detailed and time-consuming simulations are used for particle interactions with detectors. To bypass these simulations with a generative model, the generation of large point…Moritz Alfons Wilhelm Scham, Dirk Krücker, Benno Käch et al.·Nov 21, 2023SaveLearn
Distilling particle knowledge for fast reconstruction at high-energy physics experimentsKnowledge distillation is a form of model compression that allows artificial neural networks of different sizes to learn from one another. Its main application is the compactification of large deep…Aritra Bal, Tristan Brandes, Fabio Iemmi et al.·Nov 21, 2023SaveLearn
First observation of c+→ K+π0 and evidence of c+→ K+π+π-We present the first observation of the singly Cabibbo-suppressed decay c+ → K+π0 with a significance of 5.7σ and the first evidence of $c+…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Nov 21, 2023SaveLearn
Improved measurement of the decays η' π+π-π+(0)π-(0) and search for the rare decay η' 4π0Using a sample of 10 billion J/ events collected with the BESIII detector, the decays η' π+π-π+π-, η' π+π-π0π0 and $η' 4…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Nov 21, 2023SaveLearn
Measurements and EFT fits on detector levelThe framework of standard model effective field theory (SMEFT) provides a relatively model-agnostic tool with which to parameterize the off-shell effects of potential heavy new physics. In the top…Kelci Mohrman·Nov 20, 2023SaveLearn
PAIReD jet: A multi-pronged resonance tagging strategy across all Lorentz boostsWe propose a new approach of jet-based event reconstruction that aims to optimally exploit correlations between the products of a hadronic multi-pronged decay across all Lorentz boost regimes. The…Spandan Mondal, Gaetano Barone, Alexander Schmidt·Nov 18, 2023SaveLearn
Anomalous spin precession systematic effects in the search for a muon EDM using the frozen-spin techniqueAt the Paul Scherrer Institut (PSI), we are currently working on the development of a high-precision apparatus with the aim of searching for the muon electric dipole moment (EDM) with unprecedented…G. Cavoto, R. Chakraborty, A. Doinaki et al.·Nov 17, 2023SaveLearn
The polarimeter vector for τ → 3 πτ decaysThe polarimeter vector of the τ represents an optimal observable for the measurement of the τ spin. In this paper we present an algorithm for the computation of the τ polarimeter…Vladimir Cherepanov, Christian Veelken·Nov 17, 2023SaveLearn
A model-independent measurement of the CKM angle γ in partially reconstructed B D* h decays with D KS0 h+h- (h=π, K)A measurement of C\!P-violating observables in B D* K and B D* π decays is made where the photon or neutral pion from the D* Dγ or $D*…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Nov 17, 2023SaveLearn
ALICE 3: a next-generation heavy-ion detector for LHC Run 5 and beyondThe ALICE Collaboration proposes a completely new apparatus, ALICE 3, for the LHC Runs 5 and 6. The detector consists of a large pixel-based tracking system covering eight units of pseudorapidity,…Nicola Nicassio·Nov 16, 2023SaveLearn
Status of Dual-Readout Calorimetry for Future High-Energy Physics ExperimentsFuture experiments at high energy e+e- colliders will focus on extremely precise Standard Model measurements. Among the most important physics benchmarks, there is the capability to resolve the…Andrea Pareti·Nov 16, 2023SaveLearn
Probing EFT models using top quark production in multilepton final statesUsing data consisting of top quarks produced with additional final leptons collected by the CMS detector at a center-of-mass energy of s=13 TeV from 2016 to 2018 (138 fb-1), a search…Aashwin Basnet·Nov 16, 2023SaveLearn
Physics Opportunities at a Beam Dump Facility at PIP-II at Fermilab and BeyondThe Fermilab Proton-Improvement-Plan-II (PIP-II) is being implemented in order to support the precision neutrino oscillation measurements at the Deep Underground Neutrino Experiment, the U.S.…A. A. Aguilar-Arevalo, J. L. Barrow, C. Bhat et al.·Nov 16, 2023SaveLearn
Searches for New High-Mass Resonances Decaying to Fermions at the LHCAccelerator searches for new resonances have a long-standing history of discoveries that have driven advances in our understanding of nature. Since 2010, the Large Hadron Collider (LHC) has probed…Barbara Clerbaux, Carl Gwilliam·Nov 16, 2023SaveLearn
Measurement of ZZ production cross-sections in the four-lepton final state in pp collisions at s=13.6 TeV with the ATLAS experimentThis paper reports cross-section measurements of ZZ production in pp collisions at s=13.6 TeV at the Large Hadron Collider. The data were collected by the ATLAS detector in 2022, and…ATLAS Collaboration·Nov 16, 2023SaveLearn
Search for Charged Excited States of Dark Matter with KamLAND-ZenParticle dark matter could belong to a multiplet that includes an electrically charged state. WIMP dark matter (0) accompanied by a negatively charged excited state (-) with a small…Zen collaboration, S. Abe, M. Eizuka et al.·Nov 16, 2023SaveLearn
The International Large Detector (ILD) for a future electron-positron collider: Status and PlansThis work presents the status and plans of the International Large Detector (ILD) concept, one of the most detailed and comprehensive detector concepts for a future Higgs factory. Most hardware…Ulrich Einhaus·Nov 15, 2023SaveLearn
Implementation, performance and physics impact of particle identification at Higgs factoriesThis work introduces the software tool Comprehensive Particle Identification (CPID). It is a modular approach to combined PID for future Higgs factories and implemented in the Key4hep framework. Its…Ulrich Einhaus, Matthew Basso, Mikael Berggren et al.·Nov 15, 2023SaveLearn
Simultaneous energy and mass calibration of large-radius jets with the ATLAS detector using a deep neural networkThe energy and mass measurements of jets are crucial tasks for the Large Hadron Collider experiments. This paper presents a new calibration method to simultaneously calibrate these quantities for…ATLAS Collaboration·Nov 15, 2023SaveLearn
Observation of strangeness enhancement with charmed mesons in high-multiplicity pPb collisions at sNN=8.16\,TeVThe production of prompt D+s and D+ mesons is measured by the LHCb experiment in proton-lead (pPb) collisions in both the forward (1.5<y*<4.0) and backward (-5.0<y*<-2.5)…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Nov 14, 2023SaveLearn
New results from the Muon g-2 ExperimentThe Muon g-2 experiment at Fermilab has published the first result on Run-1 dataset in 2021 showing a good agreement with the previous experimental result at Brookhaven National Laboratory at…Graziano Venanzoni·Nov 14, 2023SaveLearn
High Intensity Kaon Experiments (HIKE) at the CERN SPS Proposal for Phases 1 and 2A timely and long-term programme of kaon decay measurements at an unprecedented level of precision is presented, leveraging the capabilities of the CERN Super Proton Synchrotron (SPS). The proposed…The HIKE Collaboration·Nov 14, 2023SaveLearn