40CL 40S B- DECAY (8.8 S) 2006WI10 17NDS 201702
40CL H TYP=FUL$AUT=JUN CHEN$CIT=NDS 140, 1 (2017)$CUT=30-Sep-2015$
40CL c 2006Wi10 (also 1998WiZX,1998WiZV): {+40}S isotope was obtained from the
40CL2c decay of {+40}P isotope produced by fragmentation of a {+48}Ca beam
40CL3c at 70 MeV/nucleon bombarding a 254 mg/cm{+2} {+9}Be target at NSCL,
40CL4c Michigan facility. The fragments were separated by A1200 fragment
40CL5c separator and identified using energy loss (|DE) versus time-of-flight
40CL6c (TOF) measured by a 500-|mm Si PIN diode (|DE) and a thin plastic
40CL7c scintillator (TOF), and implanted into 17-mil targets on a rotatable
40CL8c wheel. |b particles were detected with a 1-mm-thick plastic
40CL9c scintillator directly downstream of the Al targets and |g rays were
40CLac detected by two Ge detectors (FWHM=2.5 and 2.9 keV at 1332 keV).
40CLbc Measured E|g, I|g, E|b, I|b, |g|g-coin, |b|g-coin. Deduced levels,
40CLcc J, |p, |b-decay branching ratios, log| {Ift}. Comparisons with
40CLdc shell-model calculations.
40CL c 1986Du07: {+40}S ions were produced by fragmentation of a 60
40CL2c MeV/nucleon {+40}Ar beam on a 190 mg/cm{+2} Be target at GANIL.
40CL3c Fragments were separated by the LISE spectrometer. |b particles were
40CL4c detected with a 1-mm-thick plastic scintillator and |g rays were
40CL5c detected with a 174 cm{+3} intrinsic Ge detector. Measured E|g, I|g,
40CL6c decay curves. Deduced T{-1/2}, |g-ray branching ratios. Reported four
40CL7c |g rays at 211.6, 431.9, 677.5 and 888.6.
40CL cG E,RI$From 2006Wi10
40CL cB IB$Deduced by evaluator based on |g-ray intensity imbalance at
40CL2cB each level with a normalization of 0.52 {I3} from 2006Wi10, unless
40CL3cB otherwise noted.
40CL cL E$From a least-squares fit to |g-ray energies
40CL cL J$From Adopted Levels
40S P 0 0+ 8.8 S 22 4720 30
40S cP T$From Adopted Levels of {+40}S, taken from 1986Du07.
40S cP QP$From 2012Wa38.
40CL N 0.52 3 1 1
40CL cN NR$Deduced by 2006Wi10 from relative intensities of strong |g rays from
40CL2cN {+40}Cl |b{+-} decay observed in the saturation spectra. The value is
40CL3cN 0.54 {I2} deduced by evaluator assuming |S(I|g to g.s.)=100.
40CL PN 3
40CL L 0 2-
40CL B 0.5 LT 8.8 GT 1U?
40CLS B EAV=2136 69
40CL cB IB$from 2006Wi10, shell-model prediction; intensity balance gives
40CL2cB 3 {I7} (or <10)
40CL L 211.56 9 1-
40CL G 211.59 11 100 3 C
40CL DG $ EG=211.6 4, RI=100 10 (1986Du07)
40CL L 431.61 7 (1-,2)
40CL G 431.57 7 49 5 C
40CL DG $ EG=431.9 4, RI=51 10 (1986Du07)
40CL L 889.02 10 1+
40CL B 35 5 4.7 2
40CLS B EAV=1690 68
40CL cB IB$2006Wi10 give 36 {I4}
40CL G 457.4 6 7.7 19 C
40CL G 677.41 12 52 7 C
40CL DG $ EG=677.5 5, RI=38 10 (1986Du07)
40CL G 889.04 17 21 3 C
40CL DG $ EG=888.6 4, RI=50 12 (1986Du07)
40CL L 1292.75 11 (1+)
40CL B 5 4 5.4 4
40CLS B EAV=1494 68
40CL cB IB$2006Wi10 give 6 {I3}
40CL G 403.70 12 12.6 15 C
40CL G 1081.33 18 38 5 C
40CL G 1292.87 21 16.4 24 C
40CL L 1998.02 21 (1+)
40CL B 10 2 4.6 2
40CLS B EAV=1155 67
40CL G 705.20 23 9.5 20 ?
40CL G 1786.6 3 9.6 21 C
40CL L 2306.23 13 1+
40CL B 46 4 3.7 2
40CLS B EAV=1009 67
40CL cB IB$2006Wi10 give 47 {I4}
40CL G 1013.57 13 47 3 C
40CL G 1874.41 19 42 5 C