Showing 241–260 of 478 results
/ Date/ Name
Jan 17, 2020Beam energy dependence of net-$Λ$ fluctuations measured by the STAR experiment at RHICJan 9, 2020Non-monotonic energy dependence of net-proton number fluctuationsJan 6, 2020A search for IceCube events in the direction of ANITA neutrino candidatesJan 3, 2020A Joint Fermi-GBM and LIGO/Virgo Analysis of Compact Binary Mergers From the First and Second Gravitational-wave Observing RunsDec 25, 2019Open data from the first and second observing runs of Advanced LIGO and Advanced VirgoDec 24, 2019Measurement of the $e^+e^-\toπ^+π^-π^0$ cross section from 0.7 GeV to 3.0 GeV via initial-state radiationNov 27, 2019Measurement of D$^0$-meson + hadron two-dimensional angular correlations in Au+Au collisions at $\sqrt{s_{\rm NN}} = $ 200 GeVNov 11, 2019Multiple Magnetic Bilayers and Unconventional Criticality without Frustration in BaCuSi$_2$O$_6$Nov 6, 2019Neutrino astronomy with the next generation IceCube Neutrino ObservatoryNov 1, 2019Methods for a blind analysis of isobar data collected by the STAR collaborationOct 31, 2019First measurement of $Λ_c$ baryon production in Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 200 GeVOct 23, 2019Supplementary information for "Quantum supremacy using a programmable superconducting processor"Oct 15, 2019Design and Performance of the first IceAct Demonstrator at the South PoleOct 14, 2019Reflectivity and PDE of VUV4 Hamamatsu SiPMs in Liquid XenonSep 27, 2019Study of $e^{+}e^{-} \to D^{+} D^{-} π^{+} π^{-} $ at center-of-mass energies from 4.36 to 4.60 GeVSep 26, 2019First observation of the decay $χ_{cJ}\to Σ^{+}\bar{p}K_{S}^{0}+c.c. ~(J = 0, 1, 2)$Sep 4, 2019Efficient propagation of systematic uncertainties from calibration to analysis with the SnowStorm method in IceCubeAug 27, 2019A Search for MeV to TeV Neutrinos from Fast Radio Bursts with IceCubeAug 26, 2019Search for PeV Gamma-Ray Emission from the Southern Hemisphere with 5 Years of Data from the IceCube ObservatoryAug 23, 2019Observation of the leptonic decay $D^+ \to τ^+ ν_τ$