First measurement of neutron capture multiplicity in neutrino-oxygen neutral-current quasi-elastic-like interactions using an accelerator neutrino beamWe report the first measurement of neutron capture multiplicity in neutrino-oxygen neutral-current quasi-elastic-like interactions at the gadolinium-loaded Super-Kamiokande detector using the T2K…T2K Collaboration, K. Abe, S. Abe et al.·May 28, 2025SaveLearn
Community input to the European Strategy on particle physics: Searches for Permanent Electric Dipole MomentsSearches for electric dipole moments (EDMs) in fundamental particles and quantum systems with spin are pivotal experiments at the intersection of low-energy and high-precision particle physics. These…M. Athanasakis-Kaklamanakis, M. Au, R. Berger et al.·May 28, 2025SaveLearn
Search for a dark baryon in the -→π-+ invisible decayA search for a dark baryon is performed for the first time in the two-body decay -→π-+ invisible using (10.0870.044)×109 J/ events collected at a…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·May 28, 2025SaveLearn
Search for CP violation in events with top quarks and Z bosons at s = 13 and 13.6 TeVA search for the violation of the charge-parity (CP) symmetry in the production of top quarks in association with Z bosons is presented, using events with at least three charged leptons and…CMS Collaboration·May 27, 2025SaveLearn
Construction, Commissioning, and Installation of the Cylindrical GEM Inner Tracker of the BESIII ExperimentBESIII (BEijing Spectrometer III) is a particle physics experiment with a vast physics program centered around the study of charmonium and the τ lepton. The performance of the spectrometer's…Stefano Gramigna·May 27, 2025SaveLearn
Parametrizing the reconstruction performance of Super-Kamiokande in the Sub-GeV to TeV neutrino energy rangeSuper-Kamiokande is a paramount detector for studying atmospheric, astrophysical and accelerator neutrino physics. This work extracts and characterizes the neutrino reconstruction performance of…C. Jesús-Valls·May 27, 2025SaveLearn
Defects and acceptor removal in 60Co γ-irradiated p-type siliconBoron-doped silicon detectors used in high radiation environments like the future HL-LHC show a degradation in device performance due to the radiation induced deactivation of the active boron dopant.…Anja Himmerlich, Núria Castelló-Mor, Esteban Currás-Rivera et al.·May 27, 2025SaveLearn
Measurement of WWZ and ZH production cross sections at s = 13 and 13.6 TeVA measurement is presented of the cross section in proton-proton collisions for the production of two W bosons and one Z boson. It is based on data recorded by the CMS experiment at the CERN LHC at…CMS Collaboration·May 26, 2025SaveLearn
First measurement of +n→ p and +n→0p cross sections via +-nucleus scattering at an electron-positron colliderUsing (1.00870.0044)×1010 J/ events collected with the BESIII detector at the BEPCII storage ring, the reactions +n→ p and…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·May 26, 2025SaveLearn
Transforming jet flavour tagging at ATLASJet flavour tagging enables the identification of jets originating from heavy-flavour quarks in proton-proton collisions at the Large Hadron Collider, playing a critical role in its physics…ATLAS Collaboration·May 26, 2025SaveLearn
Low energy calibration in DUNE far detector prototypesThe Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino experiment. In addition to GeV-scale oscillation measurements (δCP, θ23 octant, mass…Emile Lavaut·May 23, 2025SaveLearn
Measurement of branching fractions of c+ decays to + η and + η'By analyzing e+e- collision data taken at center-of-mass energies s between 4.600 and 4.699 GeV with the BESIII detector at the BEPCII collider, corresponding to an integrated luminosity…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·May 23, 2025SaveLearn
Measurement of event shapes in minimum-bias events from proton-proton collisions at s = 13 TeVA measurement of event-shape variables is presented, using a data sample produced in a special run with approximately one inelastic proton-proton collision per bunch crossing. The data were collected…CMS Collaboration·May 23, 2025SaveLearn
High-β* Optics Calculus at IP2 for Forward Physics in LHC Runs 3 and 4We present a study of high-β* optics configurations at Interaction Point 2 (IP2) of the Large Hadron Collider (LHC), developed to enable forward and diffractive physics measurements with the…Sorina Popescu·May 21, 2025SaveLearn
Observation of cJ 3KS0Kπ^By analyzing (2712.414.3)×106 (3686) events collected with the BESIII detector operating at the BEPCII collider, the decays c0,1,2 3KS0Kπ are observed for…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·May 21, 2025SaveLearn
Search for Dark Photon Dark Matter with a Mass around 36.1 μeV Using a Frequency-tunable Cavity Controlled through a Coupled Superconducting QubitWe report the results of a search for dark photon dark matter using a cavity that employs a transmon qubit as a frequency tuner. The tuning mechanism utilizes the energy level shift arising from the…Kan Nakazono, Shion Chen, Hajime Fukuda et al.·May 21, 2025SaveLearn
Measurement of the Z-boson massThe first dedicated Z-boson mass measurement at the LHC with Z μ+μ- decays is reported. The dataset uses proton-proton collisions at a centre-of-mass energy of 13 TeV, recorded in…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·May 21, 2025SaveLearn
Exploring Event-by-Event p T Fluctuations in pp Collisions at s = 13 TeV: An Insight from ALICEEvent-by-event fluctuations of the mean transverse momentum (p T) of relativistic charged particles are analyzed using the two-particle correlator Cm/M(p T)m, which…Bushra Ali·May 21, 2025SaveLearn
Sensitivity of the Hyper-Kamiokande experiment to neutrino oscillation parameters using acceleration neutrinosThis paper describes the analysis to estimate the sensitivity of the Hyper-Kamiokande experiment to long-baseline neutrino oscillation parameters using accelerator (anti)neutrinos. Results are…Kamiokande Collaboration·May 21, 2025SaveLearn
Test of local realism via entangled systemThe non-locality of quantum correlations is a fundamental feature of quantum theory. The Bell inequality serves as a benchmark for distinguishing between predictions made by quantum theory and local…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·May 21, 2025SaveLearn
Measurements of charmed meson and antimeson production asymmetries at s =13.6 TeVThis article presents doubly differential measurements of the asymmetries in production rates between mesons containing a charm quark and those containing an anticharm quark in proton-proton…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·May 20, 2025SaveLearn
Performance of short and long bent crystals for the TWOCRYST experiment at the Large Hadron ColliderThis study investigates the performance of bent silicon crystals intended to channel hadrons in a fixed-target experiment at the Large Hadron Collider (LHC). The phenomenon of planar channelling in…L. Bandiera, R. Cai, S. Carsi et al.·May 20, 2025SaveLearn
Searching for Light Dark Matter and Dark Sectors with the NA64 experiment at the CERN SPSSince its approval in 2016, NA64 has pioneered light dark matter (LDM) searches with electron, positron, muon, and hadron beams. The experiment has successfully met its primary objectives, as…Yu. M. Andreev, A. Antonov, M. A. Ayala Torres et al.·May 20, 2025SaveLearn
Investigating quarkonium collectivity in heavy-ion collisionsThe quark-gluon plasma (QGP) produced in ultrarelativistic heavy-ion collisions has exhibited properties of a mostly perfect fluid. These properties can be observed through the hydrodynamic expansion…Victor Valencia Torres·May 20, 2025SaveLearn
Cosmic Ray Muon Polarization to Facilitate Atmospheric Neutrino PhysicsAtmospheric neutrinos (ATNs) offer a paradigm for understanding neutrino properties, while it is critical to quantify uncertainties in flux modeling. Since ATNs are produced simultaneously with…Ming-Chen Sun, Shi-Han Zhao, Rui-Xuan Gao et al.·May 20, 2025SaveLearn