156W 156W B-:T:XUNDL-1 2023Br10 202403 156W c Compiled (unevaluated) dataset from 2023Br10: 156W c Phys Lett. B 847, 138310 (2023) 156W c Compiled by E.A. McCutchan (NNDC,BNL) November 28, 2023 156W c {+160}Os activity from {+106}Cd({+58}Ni,4n) reaction. Measured Ep, 156W 2c E|a, Ip, |a-recoil (coin). 156W 3c The recoiling fusion-evaporation residues were 156W 4c separated from the beam by the MARA gas-filled recoil 156W 5c separator and deposited in a DSSD at the focal plane surrounded by 156W 6c 8 silicon detectors arranged in a box configuration. 156W L 0.0 0+ 157 MS +57-34 156W cL T$from time difference between {+160}Os |a decays and subsequent 156W 2cL {+156}Ta proton decays or {+156}Hf isomer |a decays (2023Br10). 156W 156W B-:T:XUNDL-2 2024Ya04 202403 156W c Compiled (unevaluated) dataset from 2024Ya04: 156W c Phys Rev. Lett. 132, 072502 (2024) 156W c Compiled by E.A. McCutchan (NNDC,BNL) February 28, 2024 156W c {+160}Os activity from {+106}Cd({+58}Ni,4n) reaction. 156W 2c Measured Ep, E|a, Ip, |a-recoil (coin) using 156W 3c three 300-|mm thick position-sensitive Si strip detectors. 156W 4c The recoiling fusion-evaporation residues were 156W 5c separated from the beam by the SHANS recoil 156W 6c separator and deposited in a PSSD at the focal plane surrounded by 156W 7c 8 silicon detectors arranged in a box configuration. 156W 8c Measured E|g, recoil-|g using two HPGe detectors. 156W L 0.0 0+ 291 MS +86-61 156W cL T$from time difference between {+160}Os |a decays and subsequent 156W 2cL {+156}Ta decays (2024Ya04). Authors state that the half-life 156W 3cL was roughly estimated.