Measurement of the branching fraction of Ds*+ e+e-Ds+The branching fraction of the electromagnetic Dalitz decay D*+s e+e-D+s is measured with an e+e- collision data sample collected by the BESIII experiment at…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jun 9, 2026SaveLearn
Atmospheric Neutrino Oscillations: the Full PictureWe present the first combined oscillation analysis of multiple atmospheric neutrino datasets, featuring data from Super-Kamiokande, IceCube-DeepCore, and KM3NeT/ORCA together with reactor data from…Philipp Eller·Jun 9, 2026SaveLearn
New high-statistics measurement of the π0 e+e-γ Dalitz decay at the Mainz MicrotronThe Dalitz decay π0 e+e-γ has been measured with the highest statistical accuracy obtained so far in the γp π0 p reaction with the A2 tagged-photon facility at the Mainz Microtron,…S. Prakhov, L. Heijkenskjöld, S. Abt et al.·Jun 9, 2026SaveLearn
Performance of the Eos detector with waterIn this manuscript we present the first results from Eos, a four tonne optical detector located at the University of California, Berkeley. The primary goal of Eos is to demonstrate the performance…Eos Collaboration, S. Arora, M. Askins et al.·Jun 8, 2026SaveLearn
Measurement of the ratio of branching fractions B(Bc+ J/ψτ+ ντ)/B(Bc+ J/ψμ+ νμ)A measurement of the ratio of semileptonic branching fractions R(Jψ), defined as R(J/ψ) B(Bc+ J/ψτ+ ντ)/B(Bc+ J/ψμ+ νμ), is reported…LHCb collaboration, R. Aaij, M. Abdelfatah et al.·Jun 8, 2026SaveLearn
Testing Heavy Dark Matter Decay as the Origin of KM3-230213AThis work explores the hypothesis that the ultra-high-energy neutrino event KM3-230213A originates from the decay of a heavy dark matter particle with a mass above PeV scale. The analysis exploits…KM3NeT Collaboration, O. Adriani, J. A. Aguilar et al.·Jun 8, 2026SaveLearn
Search for new physics using single-lepton events with high multiplicities of jets and b jets in proton-proton collisions at s = 13 TeVThis paper presents a search for beyond the standard model physics using single-lepton events with a high multiplicity of jets, including those identified as bottom quark jets, without a requirement…CMS Collaboration·Jun 8, 2026SaveLearn
Measurement of differential t-channel single top (anti)quark production cross-sections at 13 TeV with the ATLAS detectorThe production of single top quarks and top antiquarks via the t-channel exchange of a virtual W boson is measured in proton-proton collisions at a centre-of-mass energy of 13 TeV at the Large…ATLAS Collaboration·Jun 8, 2026SaveLearn
Search for the isospin-violating decays χcJΛΣ0+c.c. and ηcΛΣ0+c.c.Using a sample of (2712.414.3)×106~ψ(3686) events collected with the BESIII detector, we perform a search for the isospin-violating decays χcJΛΣ0+c.c.~(J=0,1,2) and…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jun 6, 2026SaveLearn
A homodyne detection scheme for all-optical photon-photon scattering experiments using 2D detectorsLow signal-to-noise ratios are a common problem in experiments attempting to measure photon-photon scattering. In the optical regime, where petawatt lasers with femtosecond pulse durations are used,…Timo Pohle, Leonard Doyle, Paul Ihde et al.·Jun 5, 2026SaveLearn
Mountain Muography for China Jinping Underground LaboratoryThe China Jinping Underground Laboratory (CJPL), located 2,400~m beneath Jinping Mountain, is one of the world's deepest and largest ( 300,000~m3) underground facilities,…Xinshun Zhang, Shaomin Chen, Wei Dou et al.·Jun 4, 2026SaveLearn
Higgs CP studies and other Higgs properties at ATLAS and CMSRecent measurements of Higgs boson properties using proton-proton collision data recorded at s=13 TeV and s=13.6 TeV with the ATLAS and CMS detectors at the LHC are presented. CMS…Lucas Russell·Jun 4, 2026SaveLearn
Associated Z + J/ψ production as a probe of multiparton interactions in the forward regionThis letter reports a study of associated Z boson and prompt J/ψ production in proton-proton collisions at s=13 TeV with the LHCb detector in the forward rapidity region, using a data…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Jun 4, 2026SaveLearn
Searching for vector-like leptons decaying into an electron and missing transverse energy in e+e- collisions with s = 240 GeV at the FCC-eeThis analysis delves into the lepton portal dark matter by utilizing Monte Carlo simulated samples from electron-positron collisions at the Future Circular Collider (FCC-ee), operating at a center of…S. Elgammal·Jun 4, 2026SaveLearn
Search for the charmonium weak decay ψ(2S) Ds-π+ + c.c. and ψ(2S) Ds-ρ+ + c.c.We search for the weak decays ψ(2S) Ds-π+ + c.c. and ψ(2S) Ds-ρ+ + c.c. for the first time. The search is based on (2712.414.3)× 106 events containing the charmonium state…BESIII Collaboration, M. Ablikim, M. N. Achasov et al.·Jun 4, 2026SaveLearn
Measurement of the solar neutrino interaction rate below 3.49 MeV in Super-Kamiokande-IVSuper-Kamiokande (SK) has observed 8B solar neutrino elastic scattering at recoil electron kinetic energies (Ekin) as low as 3.49 MeV to study neutrino flavor conversion…Kamiokande Collaboration, A. Yankelevich, K. Abe et al.·Jun 4, 2026SaveLearn
Feasibility Study of Pion and Kaon Structure via the Sullivan Process at EicCThe Electron--Ion Collider in China (EicC) provides an excellent opportunity to explore the internal structure of pions and kaons via the Sullivan process in deep-inelastic scattering (DIS). In this…Zongyang Lu, Zihan Yu, Ting Lin et al.·Jun 4, 2026SaveLearn
Probing the Higgs-top Yukawa interaction in the ttH and tH processes using H→γγ with the ATLAS detectorA study of the structure of the coupling between the Higgs boson and the top quark is performed using events from ttH and tH production in the H→γγ decay channel, with 164…ATLAS Collaboration·Jun 3, 2026SaveLearn
Archi: Agentic Operations at the CMS ExperimentWe present Archi, an open-source, end-to-end framework for scientific collaborations that combines the systematic ingestion and organization of heterogeneous data sources with the deployment of…Pietro Lugato, Luca Lavezzo, Jason Mohoney et al.·Jun 3, 2026SaveLearn
Measurement of time-dependent CP violation parameters in B0 KS0 π0 γ decays at Belle and Belle IIWe perform a measurement of time-dependent CP violation parameters in B0 KS0 π0 γ decays using a dataset of approximately 772 × 106 and 521 × 106 Υ(4S) decays…Belle, Belle II Collaborations, : et al.·Jun 3, 2026SaveLearn
HS3: A Descriptive, Interoperable Serialization Standard for Statistical Models in High-Energy PhysicsStatistical models in high-energy physics formally encode the relationship between observed data, physics parameters of interest, and experimental and theoretical uncertainties. Likelihood-based…Carsten Burgard, Oliver Schulz, Giordon Stark et al.·Jun 3, 2026SaveLearn
Refined Global Fit of KamLAND Data and the Daya Bay Antineutrino Energy SpectrumRecently, the JUNO experiment published its measurement of the solar neutrino oscillation parameters Δm221 and 2θ12 based on 59 days of data, with central values differing by 0.2σ…Guihong Huang·Jun 3, 2026SaveLearn
Measurement of the top-quark production cross-section and charge asymmetry at LHCbThe first measurements of the top- and antitop-quark differential production cross-sections and the top-quark charge asymmetry in the forward region are presented, using proton-proton collision data…LHCb collaboration, R. Aaij, A. S. W. Abdelmotteleb et al.·Jun 3, 2026SaveLearn
Particle Detection Using Magnetic Avalanches in Single-Molecule Magnet CrystalsThe detection of a single quantum of energy with high efficiency and a low false positive rate is of considerable scientific interest, from serving as single quantum sensors of optical and infra-red…Bailey Kohn, Hao Chen, Rupak Mahapatra et al.·Jun 3, 2026SaveLearn
Analysis of the C\!P structure of the Yukawa coupling between the Higgs boson and tau leptons in proton-proton collisions at s = 13.6 TeVThis paper presents a measurement of the charge-parity (C\!P) structure of the Yukawa coupling between the Higgs boson (H) and tau leptons, using proton-proton collision data at s = 13.6…CMS Collaboration·Jun 2, 2026SaveLearn