Measurement of the νμ-Hydrogen Charged-Current Quasi-Elastic Cross Section using the NOvA Near DetectorWe report a measurement of the total cross section for muon antineutrino charged-current quasi-elastic scattering on hydrogen, νμ H μ+ n, in the NOvA near detector using a…The NOvA Collaboration·Aug 12, 2026SaveLearn
Model-independent measurement of the transversity amplitudes of the B0 K*0μ+μ- decayAn analysis of the decay amplitudes of B0 K*0( K+π-)μ+μ- is presented, using proton-proton collision data recorded by the LHCb experiment at centre-of-mass energies of 7, 8, and 13…LHCb collaboration, R. Aaij, M. Abdelfatah et al.·Aug 12, 2026SaveLearn
Laboratory constraints on peV-scale mass splitting between ordinary and sterile neutron statesSterile states of matter, represented by a parallel ``mirror'' sector, may contribute to the observed dark matter in the Universe. We investigated the parameter space of neutron (n) to…N. J. Ayres, Z. Berezhiani, G. Bison et al.·Aug 12, 2026SaveLearn
Toward a Measurement of the Higgs Boson Mass with Natural-Width Precision at FCC-eeHiggs boson mass measurements with sub-10 MeV precision enable sub-percent determinations of Higgs boson couplings and prevent the Higgs boson mass from becoming a limiting input to electroweak fits.…Jan Eysermans, Ang Li, Gregorio Bernardi et al.·Aug 12, 2026SaveLearn
A determination of the backscattering probability of low-energy antiprotonsIt is commonly assumed that antiprotons impinging on a material surface annihilate promptly with the nuclei of the material. However, at kinetic energies of a few keV, this assumption may not hold.…GBAR Collaboration, K. Park, E. Perez et al.·Aug 12, 2026SaveLearn
Particle Identification at Future CollidersParticle identification (PID) remains a key ingredient of the physics programmes of future collider experiments. While traditional collider detectors rely on calorimetry, tracking and muon systems…Roberto Preghenella·Aug 12, 2026SaveLearn
An improved direct limit on the muon electric dipole momentA limit on the permanent electric dipole moment (EDM) of the positive muon is presented based on data from the Fermilab Muon g-2 Experiment taken between 2019 and 2020. The tracking detectors measure…2 Collaboration, D. P. Aguillard, T. Albahri et al.·Aug 11, 2026SaveLearn
Particle tracking at high luminosities using a novel reconstruction approachTracking charged particles with high precision is of vital importance for collider experiment like those operating at the Large Hadron Collider (LHC), CERN. The tracking detector in the CMS…B. K. Sirasva, S. Dugad, Y. Kumar et al.·Aug 11, 2026SaveLearn
Study of muon-tagged Ds1(2460)+ and Ds1(2536)+ decays to the Ds+π+π- final stateDecays of the pseudovector Ds1(2460)+ and Ds1(2536)+ mesons to the three-body Ds+π+π- final state are studied. The data sample is based on decays of beauty hadrons into Ds1+…LHCb collaboration, R. Aaij, M. Abdelfatah et al.·Aug 11, 2026SaveLearn
A Reusable Four-Port S-Parameter to Link-Level Signal-Integrity Analysis Framework for High-Speed Detector InterconnectsA reusable MATLAB signal-integrity (SI) framework is presented that converts compatible four-port S-parameter data, measured by VNA or obtained from electromagnetic simulation, into traceable…D M S Sultan, R. Plackett, A. E. McDougall et al.·Aug 11, 2026SaveLearn
Evidence for parity violation in gravitational fieldsDiscrete symmetries in gravity have only been tested for low energy, non-relativistic matter, confirming the perfectly symmetric general relativity. A hint for high energy CP violation in…V. Gharibyan, V. Adler, P. D. Allfrey et al.·Aug 10, 2026SaveLearn
Design of ALPHA Phase I: A Plasma Haloscope for 10--20 GHz Post-Inflation AxionsThe axion is a well-motivated hypothetical particle capable of resolving both the strong CP problem and the dark matter mystery, with recent post-inflationary cosmological simulations favoring masses…ALPHA Collaboration, Xiran Bai, Rustam Balafendiev et al.·Aug 10, 2026SaveLearn
Search for a resonance in events with four top quarks decaying into two leptons and jets in proton-proton collisionsA search for a heavy resonance in events containing four top quarks is presented and interpreted in models featuring a new vector, scalar, or pseudoscalar boson that interacts exclusively with top…CMS Collaboration·Aug 10, 2026SaveLearn
Amplitude analysis for charmed meson decays at BESIIIAmplitude analysis bridges the gap between experimental measurements of multibody charmed-meson decays and theoretical predictions of intermediate two-body processes. This work presents a…Han Zhang, Zhenxuan Li, Chunyi Guan et al.·Aug 10, 2026SaveLearn
Silent coverage failures in rare-event searches and a degeneracy index that predicts themSearches for new physics in low-background experiments infer a non-negative signal strength from few events and often report an upper limit. Nominal frequentist coverage requires both a valid…Davide Pagno·Aug 10, 2026SaveLearn
SuperEM: A Sub-meV Threshold Detector Architecture for Cosmic Neutrino Background and Dark Matter DetectionExpanding the operational boundaries of radiation detection is imperative for contemporary particle physics, astrophysics, and cosmology. At this frontier, the direct detection of the Cosmic Neutrino…Zhenjie Li, Xilei Sun, Xiaoshan Jiang·Aug 9, 2026SaveLearn
Combination of Higgs boson measurements at s = 13 TeV and their interpretations by the ATLAS experimentThis paper presents combined measurements of Higgs boson production and decay using up to 140 fb-1 of proton--proton collision data collected by the ATLAS experiment at the LHC at $s =…ATLAS Collaboration·Aug 7, 2026SaveLearn
Evidence of the e+ e- f1(1285) reaction with the CMD-3 detector at VEPP-2000A search for the e+ e- f1(1285) reaction is performed with the CMD-3 detector at the VEPP-2000 collider. Data from a scan in the center-of-mass energy range Ec.m.=1.20--1.36 GeV with 109.1…E. P. Solodov, R. R. Akhmetshin, A. N. Amirkhanov et al.·Aug 7, 2026SaveLearn
Neutral kaon mass measurement with the CMD-3 derector at VEPP-2000Using more than 600 thousand KS0π+π- decays from the e+e-ϕ(1020) KS0KL0 reaction, the neutral kaon mass has been measured with the CMD-3 detector at the…E. P. Solodov, N. A. Petrov, R. R. Akhmetshin et al.·Aug 7, 2026SaveLearn
Observation of Λ+c nπ+η and search for Λ+c na0(980)+By analysing 6.1 fb-1 of data collected at center-of-mass energies between s=4.600 and 4.843 GeV with the BESIII detector at the BEPCII collider, we observe the decay…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Aug 7, 2026SaveLearn
Intrinsic Angular Momentum of the B Mesons: Proposal for a Model-Independent MeasurementThe intrinsic angular momentum ("spin") of the B mesons has not so far been measured, notwithstanding the large amount of experimental attention that these particles have received in the four…M. P. Fewell·Aug 7, 2026SaveLearn
Estimating the sensitivity of the IceCube Upgrade to probe the interior of the Earth using atmospheric neutrino oscillationsThe IceCube Upgrade is a densely instrumented central region of the IceCube Neutrino Observatory, deployed during the 2025-26 polar season. It will reduce the detector's energy threshold and…The IceCube Collaboration, R. Abbasi, M. Ackermann et al.·Aug 6, 2026SaveLearn
Quantum noise reduction schemes for KAGRA post-O5 upgradeQuantum noise, arising from the quantisation of electromagnetic field, has been a limiting noise source for current gravitational wave (GW) detectors. Squeezed vacuum modifies quantum fluctuations…Yuhang Zhao, Marc Eisenmann, Michael Page et al.·Aug 6, 2026SaveLearn
Search for the charged lepton flavour violating decay η' eμBased on (899840)×106 J/ψ events collected in e+e- collisions at s = 3.097 GeV with the BESIII detector, we present a search for the charged lepton flavour violating decay…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Aug 6, 2026SaveLearn
Spin Physics at NICA SPDThe Spin Physics Detector (SPD) is a universal detector at the NICA collider under commissioning at JINR, Dubna. The SPD is intended to study the spin structure of the proton and deuteron and other…Igor Denisenko·Aug 6, 2026SaveLearn