139SB 9BE(238U,F):T1/2:XUNDL-2 2020WU04 202101 139SB c Compiled (unevaluated) dataset from 2020Wu04: 139SB2c Phys Rev C 101, 042801(R) (2020) 139SB c Compiled by B. Singh (McMaster), Jan 23, 2021 139SB c 2020Wu04: {+139}Sb nuclide produced at the RIBF-RIKEN facility in 139SB2c {+9}Be({+238}U,F) reaction at E=345 MeV/nucleon and an intensity of 139SB3c 5pnA. Identification of fission fragments of interest was made based on 139SB4c time-of-flight (tof), magnetic rigidity (B|r), and energy loss (|DE) 139SB5c using the BigRIPS spectrometer, determining atomic Z and mass-to-charge 139SB6c ratio A/Q, where Q=charge state of the ions. The separated nuclei 139SB7c were implanted at a rate of 100 ions/s in the beta counting system 139SB8c of the Wide range Active Silicon-Strip Stopper Array for Beta and 139SB9c ion detection (WAS3ABi), which included a stack of five Double Sided 139SBAc Silicon Strip Detectors (DSSSDs). The WAS3ABi setup was surrounded 139SBBc by Euroball RIken Cluster Array (EURICA) array of 84 HPGe detectors 139SBCc for |g detection. Half-life of the separated and implanted ions 139SBDc was determined by fitting the time distribution of |b(implants)- and/or 139SBEc |b|g(implants)-correlated decay curves to the sum of activities of 139SBFc parent nuclei, daughter nuclei, grand-daughter nuclei, |b-delayed 139SBGc neutron daughter and grand-daughter nuclei, and a constant background. 139SBHc Comparison of measured half-lives with FRDM+QRPA (2003), FRDM+QRPA 139SBIc (2019), KTUY+GT2, RHB+pn-RQRPA, and DF+CQRPA theoretical calculations. 139SB L 0 182 MS 9 139SB2 L %B-=100 $ %B-N=90 10 (2020Li32) $ %B-2N=? 139SB cL %B-$only the |b{+-} decay mode is expected and detected, followed by 139SB2cL |b-delayed neutron decay 139SB cL E$the observed activity is assumed to correspond to {+139}Sb g.s. 139SB cL T$from 2020Wu04, fitting the time distribution of 139SB2cL (implanted ions)|b|g-correlated decay curves to the sum of activities 139SB3cL of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n 139SB4cL daughter and grand-daughter nuclei, and a constant background. Authors 139SB5cL compared their result with T{-1/2}=93 ms {I+14-3} from 2011Ar18: 139SB6cL Phys. Rev. C 84, 061307; same value adopted in Oct 2016 ENSDF update 139SB7cL of {+139}Sb, but with an uncertainty of 13 ms. 139SB cL $2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020).