137TE 9BE(238U,F):T1/2:XUNDL-2 2020WU04 202101 137TE c Compiled (unevaluated) dataset from 2020Wu04: 137TE2c Phys Rev C 101, 042801(R) (2020) 137TE c Compiled by B. Singh (McMaster), Jan 23, 2021 137TE c 2020Wu04: {+137}Te nuclide produced at the RIBF-RIKEN facility in 137TE2c {+9}Be({+238}U,F) reaction at E=345 MeV/nucleon and an intensity of 137TE3c 5pnA. Identification of fission fragments of interest was made based on 137TE4c time-of-flight (tof), magnetic rigidity (B|r), and energy loss (|DE) 137TE5c using the BigRIPS spectrometer, determining atomic Z and mass-to-charge 137TE6c ratio A/Q, where Q=charge state of the ions. The separated nuclei 137TE7c were implanted at a rate of 100 ions/s in the beta counting system 137TE8c of the Wide range Active Silicon-Strip Stopper Array for Beta and 137TE9c ion detection (WAS3ABi), which included a stack of five Double Sided 137TEAc Silicon Strip Detectors (DSSSDs). The WAS3ABi setup was surrounded 137TEBc by Euroball RIken Cluster Array (EURICA) array of 84 HPGe detectors 137TECc for |g detection. Half-life of the separated and implanted ions 137TEDc was determined by fitting the time distribution of |b(implants)- and/or 137TEEc |b|g(implants)-correlated decay curves to the sum of activities of 137TEFc parent nuclei, daughter nuclei, grand-daughter nuclei, |b-delayed 137TEGc neutron daughter and grand-daughter nuclei, and a constant background. 137TEHc Comparison of measured half-lives with FRDM+QRPA (2003), FRDM+QRPA 137TEIc (2019), KTUY+GT2, RHB+pn-RQRPA, and DF+CQRPA theoretical calculations. 137TE L 0 2080 MS 400 137TE2 L %B-=100 $ %B-N=2.91 16 (2020Li32) 137TE cL %B-$only the |b{+-} decay mode is expected and detected, followed by 137TE2cL |b-delayed neutron decay 137TE cL E$the observed activity is assumed to correspond to {+137}Te g.s. 137TE cL T$from 2020Wu04, fitting the time distribution of 137TE2cL (implanted ions)|b-correlated decay curves to the sum of activities 137TE3cL of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n 137TE4cL daughter and grand-daughter nuclei, and a constant background. Authors 137TE5cL compared with half-life of 2490 ms {I50} from 1985Sa15 137TE6cL (Zeit. Phys. A321, 255), the same value adopted in Oct 2006 ENSDF 137TE7cL update of {+137}Te. 137TE cL $2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 137TE 138SB B-N DECAY:XUNDL-3 2021MO10 202109 137TE c Compiled (unevaluated) dataset from 2021Mo10: 137TE2c Phys Rev C 103, 034320 (2021) 137TE c Compiled by J. Chen (NSCL, MSU), April 22, 2021 137TE c 2021Mo10: {+138}Sb source ions are produced by in-flight fragmentation 137TE2c of 345 MeV {+238}U beam from RIBF at RIKEN on a {+9}Be target. 137TE3c Fragments were identified and selected in the first stage of the 137TE4c BigRIPS spectrometer by the B|r-|DE-tof method along the second stage 137TE5c of the BigRIPS and the Zero-Degree Spectrometer. Selected ions were 137TE6c implanted into the Wide-range Active Silicon Strip Stopper Array for 137TE7c |b and ion detector (WAS3ABi) consisting of multiple layers of 137TE8c double-sided silicon strip detectors (DSSSDs); |g rays were detected 137TE9c with the EUROBALL-RIKEN Cluster Array (EURICA) of 12 cluster detectors 137TEAc each consisting of 7 hexagonal-tapered HPGe crystals. Measured E|g, 137TEBc I|g, E|b, |g|g-coin, |b|g-coin, |b|g(t), implant-|b-correlation. 137TECc Deduced levels, J, |p, T{-1/2}, |b-decay branching ratios, log {Ift}. 137TEDc Comparisons with large-scale shell-model calculations. 137TE cDNIP$Deduced by 2021Mo10 from |g-ray intensity balance 137TE cG E,RI$From 2021Mo10. Intensity is relative to I|g=100 for 460.8|g 137TE2cG from {+138}Sb |b{+-} decay. For absolute intensity per 100 {+138}Sb 137TE3cG decays, multiply by 0.62 {I5} (2021Mo10). 137TE cG E(X)$Newly identified transition in 2021Mo10 137TE cL E$From a least-squares fit to |g-ray energies (by compiler) 137TE cL J$As given in 2021Mo10 137TE cL E(Y)$Newly identified level in 2021Mo10 138SB P 0.0 (3-) 313 MS 4 7.0E3 11 138SB cP J$From Adopted Levels of {+138}Sb in ENSDF database 138SB cP T$From |b|g(t) of 461|g+442|g in the decay of {+138}Sb (2021Mo10) 138SB cP QP$7010 {I1060} (2017Wa10) 137TE N 0.253 GE 1.0 137TE cN BR$%|b{+-}n|>29.0 {I37} (2021Mo10) 137TE PN 0.62 5 4 137TE L 0.0 (7/2-) 137TE L 61.6 3 (5/2-) Y 137TE DN 18.1 33 137TE G 61.6 3 7.9 15 [M1] 2.69 14 29.0 55X 137TE cG RI$deduced by compiler from I(|g+ce)=29.0 {I55} and |a(total)=2.69 137TE2cG {I14} assuming M1 in 2021Mo10 137TE L 608.0 10 (11/2-) 137TE DN 2.0 5 137TE G 608.0 10 3.2 8 137TE L 633.3 3 (9/2-) Y 137TE DN 2.0 4 137TE G 633.3 3 3.2 7 X 137TE L 798.9 4 Y 137TE DN 2.5 11 137TE G 798.9 4 3.9 18 X 137TE L 973.7 5 Y 137TE DN 1.7 9 137TE G 973.7 5 2.7 15 X 137TE L 998.3 4 Y 137TE DN 1.7 7 137TE G 998.3 4 2.8 11 X 137TE L 1137.3 4 Y 137TE DN 1.1 4 137TE G 1137.3 4 1.76 60 X 137TE 137SB B- DECAY:XUNDL-4 2021MO10 202109 137TE c Compiled (unevaluated) dataset from 2021Mo10: 137TE2c Phys Rev C 103, 034320 (2021) 137TE c Compiled by J. Chen (NSCL, MSU), April 22, 2021 137TE c 2021Mo10: {+137}Sb source ions are produced by in-flight fragmentation 137TE2c of 345 MeV {+238}U beam from RIBF at RIKEN on a {+9}Be target. 137TE3c Fragments were identified and selected in the first stage of the 137TE4c BigRIPS spectrometer by the B|r-|DE-tof method along the second stage 137TE5c of the BigRIPS and the Zero-Degree Spectrometer. Selected ions were 137TE6c implanted into the Wide-range Active Silicon Strip Stopper Array for 137TE7c |b and ion detector (WAS3ABi) consisting of multiple layers of 137TE8c double-sided silicon strip detectors (DSSSDs); |g rays were detected 137TE9c with the EUROBALL-RIKEN Cluster Array (EURICA) of 12 cluster detectors 137TEAc each consisting of 7 hexagonal-tapered HPGe crystals. Measured E|g, 137TEBc I|g, E|b, |g|g-coin, |b|g-coin, |b|g(t), implant-|b-correlation. 137TECc Deduced levels, J, |p, T{-1/2}, |b-decay branching ratios, log {Ift}. 137TEDc Comparisons with large-scale shell-model calculations. 137TE cB IB$Deduced by 2021Mo10 from |g+ce intensity balance 137TE cB LOGFT$From the log| {Ift} code, same as values in 2021Mo10 137TE cG E,RI$From 2021Mo10. Intensity is relative to I|g=100 for 606.2|g from 137TE2cG {+137}Sb |b{+-}n decay. For absolute intensity per 100 {+137}Sb decays, 137TE3cG multiply by 0.229 (2021Mo10) 137TE cG E(X)$Newly identified transition in 2021Mo10 137TE cG CC$As quoted by 2021Mo10 and used for |g+ce intensity balance. Value 137TE2cG from BrIcc is 2.71 {I6} for 61.8|g 137TE cL E$From a least-squares fit to |g-ray energies (by compiler) 137TE cL J$As given in 2021Mo10 137TE cL E(Y)$Newly identified level in 2021Mo10 137SB P 0.0 (7/2+) 507 MS 27 9240 50 137SB cP J$From Adopted Levels of {+137}Sb in ENSDF database 137SB cP T$From |b|g(t) of 606|g, 608|g, 633|g and 974|g in the decay of 137SB2cP {+137}Sb (2021Mo10) 137SB cP QP$From 2017Wa10 137TE N 0.525 GE 137TE cN BR$%|b{+-}|>60.1 {I76} (2021Mo10) 137TE PN 0.23 2 1.0 4 137TE L 0.0 (7/2-) 137TE L 61.80 21 (5/2-) Y 137TE B 14 6 6.1 2 137TES B EAV=4151 24 137TE G 61.8 3 25 7 [M1] 2.69 14 93 26X 137TE cG RI$deduced by compiler from I(|g+ce)=93 {I26} and |a(total)=2.69 {I14} 137TE2cG assuming M1 in 2021Mo10 137TE L 608.1 4 (11/2-) 137TE B 7.2 15 6.2 1 137TES B EAV=3895 24 137TE G 608.1 4 31.3 64 137TE L 633.31 22 (9/2-) Y 137TE B 10.0 25 6.1 1 137TES B EAV=3883 24 137TE G 571.1 4 12 7 X 137TE G 633.2 3 52 8 X 137TE L 799.3 3 (5/2-,7/2-,9/2-) Y 137TE B 3.9 10 6.5 1 137TES B EAV=3805 24 137TE G 799.3 3 17.1 42 X 137TE L 973.84 24 (5/2-,7/2-,9/2-) Y 137TE B 4.3 14 6.4 2 137TES B EAV=3723 24 137TE G 912.4 4 7.8 34 X 137TE G 973.8 3 18.7 43 X 137TE L 998.3 4 (5/2-,7/2-,9/2-) Y 137TE B 2.2 8 6.7 2 137TES B EAV=3711 24 137TE G 998.3 4 9.7 35 X 137TE L 1136.6 4 (5/2-,7/2-,9/2-) Y 137TE B 3.0 13 6.5 2 137TES B EAV=3646 24 137TE G 1136.6 4 13 6 X 137TE L 1725.56 21 (7/2) Y 137TE B 15.2 25 5.6 1 137TES B EAV=3369 24 137TE G 752.2 5 7.8 22 X 137TE G 1091.9 3 20.5 44 X 137TE G 1663.8 4 10.3 37 X 137TE G 1725.7 3 28 7 X 137TE 235U(N,F):T1/2:XUNDL-5 2022Si16 202210 137TE c Compiled (unevaluated) dataset from 2022Si16: 137TE2c Phys Rev C 106, 014302 (2022) 137TE c Compiled by J. Chen (FRIB, MSU), July 28, 2022 137TE c 2022Si16: {+137}Te source ions were produced by thermal neutron-induced 137TE2c fission of a {+235}U target in the ILL reactor, separated according to 137TE3c mass-to-charge ratio by the LOHENGRIN separator and transported to the 137TE4c |b-decay station of plastic detectors in 4|p geometry from the LOENIE 137TE5c |b-delayed neutron detector. |g rays were detected with two Clover 137TE6c detectors with BGO shields and one coaxial HPGe detector. Measured E|g, 137TE7c |g(t). Deduced T{-1/2}, |b-delayed neutron emission probability 137TE L 0.0 (7/2-) 2.46 S 5 137TE2 L %B-=100 $%B-N=2.63 85 (2022Si16) 137TE cL J$from Adopted Levels of {+137}Te in ENSDF database 137TE cL T$from |g(t) in 2022Si16. 137TE cL %B-N$deduced by 2022Si16 from measured I|g of 87.3|g in {+136}I, 137TE2cL assumed from |b{+-}n decay of {+137}Te; considered as a lower limit by 137TE3cL 2022Si16 due to possible unobserved weak transitions.