145I 9BE(238U,F):T1/2:XUNDL-1 2020WU04 202101 145I c Compiled (unevaluated) dataset from 2020Wu04: 145I 2c Phys Rev C 101, 042801(R) (2020) 145I c Compiled by B. Singh (McMaster), Jan 23, 2021 145I c 2020Wu04: {+145}I nuclide produced at the RIBF-RIKEN facility in 145I 2c {+9}Be({+238}U,F) reaction at E=345 MeV/nucleon and an intensity of 145I 3c 5pnA. Identification of fission fragments of interest was made based on 145I 4c time-of-flight (tof), magnetic rigidity (B|r), and energy loss (|DE) 145I 5c using the BigRIPS spectrometer, determining atomic Z and mass-to-charge 145I 6c ratio A/Q, where Q=charge state of the ions. The separated nuclei 145I 7c were implanted at a rate of 100 ions/s in the beta counting system 145I 8c of the Wide range Active Silicon-Strip Stopper Array for Beta and 145I 9c ion detection (WAS3ABi), which included a stack of five Double Sided 145I Ac Silicon Strip Detectors (DSSSDs). The WAS3ABi setup was surrounded 145I Bc by Euroball RIken Cluster Array (EURICA) array of 84 HPGe detectors 145I Cc for |g detection. Half-life of the separated and implanted ions 145I Dc was determined by fitting the time distribution of |b(implants)- and/or 145I Ec |b|g(implants)-correlated decay curves to the sum of activities of 145I Fc parent nuclei, daughter nuclei, grand-daughter nuclei, |b-delayed 145I Gc neutron daughter and grand-daughter nuclei, and a constant background. 145I Hc Comparison of measured half-lives with FRDM+QRPA (2003), FRDM+QRPA 145I Ic (2019), KTUY+GT2, RHB+pn-RQRPA, and DF+CQRPA theoretical calculations. 145I L 0 89.7 MS 93 145I 2 L %B-=100 $ %B-N=? $ %B-2N=? 145I cL %B-$only the |b{+-} decay mode is expected and detected, followed by 145I 2cL |b-delayed neutron decay 145I cL E$the observed activity is assumed to correspond to {+145}I g.s. 145I cL T$from 2020Wu04, fitting the time distribution of 145I 2cL (implanted ions)|b|g-correlated decay curves to the sum of activities 145I 3cL of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n 145I 4cL daughter and grand-daughter nuclei, and a constant background.