AMBER -- A Strong-Interaction Facility at CERNAMBER (NA66) is a fixed-target facility at the M2 beam line of CERN SPS, which performs worldwide unique research on the internal structure and the excitation spectrum of hadrons. The approved first…Bernhard Ketzer, Michela Chiosso·Jan 10, 2026SaveLearn
The hadronic decays of charmed mesons at BESIIIIn this presentation, we discuss the recent hadronic decays of charmed mesons observed in the BESIII experiment, specifically focusing on the decay processes D+ KS0 π+ η, $D0 …Hui Li·Jan 10, 2026SaveLearn
Rare and Experimentally Challenging Supersymmetry SignaturesSupersymmetry has long played a central role in the search for physics beyond the Standard Model at colliders, providing a comprehensive and internally consistent framework for generating…Laura Jeanty, Lawrence Lee·Jan 9, 2026SaveLearn
Shedding Light on Dark Matter via the Higgs PortalA selection of new results from the CMS experiment that probe Higgs-portal frameworks are presented. These searches target scenarios in which dark matter particles are produced in association with…Shivani Lomte·Jan 9, 2026SaveLearn
Measuring high-precision luminosity at the CEPCPurpose: Luminosity measurement at the Circular Electron-Positron Collider (CEPC) is required to achieve 10-4 precision when operating at the center-of-mass energy of the Z-pole. Approximately…Jiading Gong, Jun He, Rongyan He et al.·Jan 9, 2026SaveLearn
Reconstruction of atmospheric neutrinos in DUNE's horizontal-drift far-detector moduleThis paper reports on the capabilities in reconstructing and identifying atmospheric neutrino interactions in one of the Deep Underground Neutrino Experiment's (DUNE) far detector modules, a…DUNE Collaboration, S. Abbaslu, F. Abd Alrahman et al.·Jan 9, 2026SaveLearn
Differential measurements of ttZ and tttt at large Q2 at FCC-hhThis contribution presents studies of differential top-quark measurements at the Future Circular Collider in its proton-proton stage (FCC-hh). The analyses target the leptonic final states of the…Louise Beriet, Matteo Defranchis, Birgit Stapf et al.·Jan 8, 2026SaveLearn
Measurement of spin correlation and entanglement in ATLAS and CMSThe Large Hadron Collider has delivered exceptionally large proton-proton collision datasets at centre-of-mass energies of up to 13.6 TeV. These datasets, collected by the ATLAS and CMS detectors,…Fiona Ann Jolly·Jan 8, 2026SaveLearn
Probes of lepton flavor symmetry and violation with top quarks in ATLAS and CMSMeasurements of lepton flavor universality (LFU) and searches for charged lepton flavor violation (cLFV) are one of the most straightforward ways of searching for Beyond Standard Model (BSM) physics.…Normunds Ralfs Strautnieks·Jan 7, 2026SaveLearn
Electron identification and hadron discrimination using Cherenkov radiation in air and SiPMsThis paper presents a method to identify electrons using the Cherenkov light emitted when a charged particle travels in air and photons are detected with a Silicon PhotoMultiplier (SiPM). The…A. Alici, F. Carnesecchi, B. R. Achari et al.·Jan 6, 2026SaveLearn
First comments on a descoped/staged FCC-eeIn response to its remit, the European Strategy Group (ESG) recommended the electron-positron Future Circular Collider (FCC-ee) as the preferred option for the next flagship collider at CERN; and a…Alain Blondel, Christophe Grojean, Patrick Janot et al.·Jan 6, 2026SaveLearn
First evidence of the Bs0→ K-π+γ decayThe first search for the Bs0→ K-π+γ decay in the range 796<m(K-π+)<1800\,MeV/c2 is performed using data from proton-proton collisions collected by the LHCb…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Jan 6, 2026SaveLearn
EFT results in the top quark sector in CMSThe CMS programme of indirect searches in the top-quark sector interprets precision measurements in the Standard Model Effective Field Theory (SMEFT) framework. These proceedings summarize recent CMS…Andrea Piccinelli·Jan 6, 2026SaveLearn
Measurements of the branching fractions of cJ 2K+ 2K- ω and φ K+ K- ω decaysUsing a data sample of (2712.4 14.3) × 106 (3686) events collected with the BESIII detector operating at the BEPCII collider, we report the first observation of the decays…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jan 5, 2026SaveLearn
Cross section measurement of e+e-→ π0π0ψ(3686) from s= 4.008 GeV to 4.951 GeVUsing data samples with a total integrated luminosity of 22.1~ fb-1 at center-of-mass energies between 4.008 and 4.951~GeV collected with the BESIII detector, the cross sections of…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jan 5, 2026SaveLearn
Tau lepton reconstruction at the Muon Collider: Cross section measurement of the H→τ+τ- processStudies of Higgs boson properties are crucial for the understanding the Standard Model (SM), as it could couple to new particles and provide hints to physics Beyond the Standard Model (BSM).…Kevin Dewyspelaere, Giacomo Da Molin, Giovanni Battista Marozzo et al.·Jan 4, 2026SaveLearn
Measurements of the absolute branching fractions of the c+ hadronic decaysBased on 4.5 fb-1 of e+e- collision data collected at center-of-mass energies between 4599.53 MeV and 4698.82 MeV with the BESIII detector, the absolute branching fractions of twelve…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jan 4, 2026SaveLearn
Electron Identification using Machine Learning in the MPD Experiment at NICAWe present studies of electron identification (eID) in the MPD experiment at NICA using machine learning techniques. The goal is to improve electron identification efficiency while preserving high…Sudhir Pandurang Rode·Jan 3, 2026SaveLearn
Improved liquid argon ionization model and its impact on the DarkSide low-mass WIMP search programmeDarkSide-50 achieved leading WIMP limits down to 1.2 GeV/c2 with an ionization-only analysis, despite its small active mass of 46 kg compared to multi-ton noble-liquid detectors. Accurate modelling…Davide Franco·Jan 2, 2026SaveLearn
Search for charged Higgs bosons decaying into top and bottom quarks in lepton+jets final states in proton-proton collisions at s = 13 TeVA search is presented for charged Higgs bosons (H) in proton-proton (pp) collision events via the pp (b)H processes, with H decaying into top (t) and bottom (b) quarks. The…CMS Collaboration·Dec 30, 2025SaveLearn
Thirty years after the discovery of the top quark: the field enters an age of refinement and subtletyThirty years after the first observation of on-shell top quarks the investigation of the heaviest elementary particle remains a thriving field of basic research, as was illustrated by the 18th…Wolfgang Wagner·Dec 30, 2025SaveLearn
Charmed Baryons at Belle and Belle IIWe present the recent results on charm baryon production and decays at Belle and Belle II experiments using a 1.4 ab-1 data sample of e+ e- collision collected at center-of-mass energies…Alena Mufazalova·Dec 30, 2025SaveLearn
Prospect for measurement of CP-violating parameters of Bs0 φγ at the Tera Z factoryb sγ transition is a critical flavor-changing neutral current (FCNC) process that could be used to probe CP violation (CPV) and new physics (NP). We quantify the anticipated precision for…Hengyu Wang, Hanhua Cui, Yongfeng Zhu et al.·Dec 30, 2025SaveLearn
Large Language Model Integration for Knowledge Retrieval and Interaction for the DUNE ExperimentThe Deep Underground Neutrino Experiment (DUNE) is a next-generation neutrino experiment that will generate an unprecedented volume of heterogeneous information-from documentation and technical notes…A. Rafique, A. Singh, R. Srinivas·Dec 30, 2025SaveLearn
Study of K*(892)0 η and KS0 a0(980)0 in the D0 KS0π0η decayWe perform an amplitude analysis of the decay D0 KS0 π0 η and measure its absolute branching fraction to be (1.016 0.013 stat. 0.014 syst.)\%. The…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Dec 29, 2025SaveLearn