140TE 9BE(238U,F):T1/2:XUNDL-3 2020WU04 202101 140TE c Compiled (unevaluated) dataset from 2020Wu04: 140TE2c Phys Rev C 101, 042801(R) (2020) 140TE c Compiled by B. Singh (McMaster), Jan 23, 2021 140TE c 2020Wu04: {+140}Te nuclide produced at the RIBF-RIKEN facility in 140TE2c {+9}Be({+238}U,F) reaction at E=345 MeV/nucleon and an intensity of 140TE3c 5pnA. Identification of fission fragments of interest was made based on 140TE4c time-of-flight (tof), magnetic rigidity (B|r), and energy loss (|DE) 140TE5c using the BigRIPS spectrometer, determining atomic Z and mass-to-charge 140TE6c ratio A/Q, where Q=charge state of the ions. The separated nuclei 140TE7c were implanted at a rate of 100 ions/s in the beta counting system 140TE8c of the Wide range Active Silicon-Strip Stopper Array for Beta and 140TE9c ion detection (WAS3ABi), which included a stack of five Double Sided 140TEAc Silicon Strip Detectors (DSSSDs). The WAS3ABi setup was surrounded 140TEBc by Euroball RIken Cluster Array (EURICA) array of 84 HPGe detectors 140TECc for |g detection. Half-life of the separated and implanted ions 140TEDc was determined by fitting the time distribution of |b(implants)- and/or 140TEEc |b|g(implants)-correlated decay curves to the sum of activities of 140TEFc parent nuclei, daughter nuclei, grand-daughter nuclei, |b-delayed 140TEGc neutron daughter and grand-daughter nuclei, and a constant background. 140TEHc Comparison of measured half-lives with FRDM+QRPA (2003), FRDM+QRPA 140TEIc (2019), KTUY+GT2, RHB+pn-RQRPA, and DF+CQRPA theoretical calculations. 140TE L 0 0+ 360 MS 21 140TE2 L %B-=100 $ %B-N=? $ %B-2N=? 140TE cL %B-$only the |b{+-} decay mode is expected and detected, followed by 140TE2cL |b-delayed neutron decay 140TE cL T$from 2020Wu04, fitting the time distribution of 140TE2cL (implanted ions)|b|g-correlated decay curves to the sum of activities 140TE3cL of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n 140TE4cL daughter and grand-daughter nuclei, and a constant background. 140TE5cL Half-life of 348 ms {I5} is adopted in Nov 2018 ENSDF update of 140TE6cL {+140}Te, based on 350 ms {I5} from 2017Mo19 (Phys. Rev. C 96, 140TE7cL 014325); a value derived from the same experiment as in 2020Wu04 140TE8cL (see caption for Table I in 2020Wu04); and and a tentative value of 140TE9cL 335 ms {I14} from 2006KeZZ (Annual Rept. GSI 2006-1, p154) 140TE cL $2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020).