39CL 39S B- DECAY (11.5 S) 1980HI01 18NDS 201803
39CL H TYP=FUL$AUT=JUN CHEN$CIT=NDS 149, 1 (2018)$CUT=1-Jan-2018$
39CL c 1980Hi01: Source of {+39}S was produced via {+40}Ar(n,2p) with the fast
39CL2c neutron flux generated when the 800-MeV proton beam from the LAMPF
39CL3c (Clinton P. Anderson Meson Physics Facility) accelerator is stopped by
39CL4c the main beam stop and natural Ar gas target. |g rays were detected
39CL5c with Ge(Li) detectors (FWHM=2 keV). Measured E|g, I|g, |g|g-coin,
39CL6c |g(t). Deduced levels, parent T{-1/2}, |b-decay branching ratios,
39CL7c log {Ift}. Comparisons with available data and shell-model
39CL8c calculations.
39CL c Others: production of {+39}S
39CL c 1999Ai02: {+9}Be({+55}Mn,X)
39CL c 1997Fo01: {+208}Pb({+37}Cl,X)
39CL c 1971Ar32: {+232}Th({+40}Ar,X)
39CL c Theoretical calculations: 1989Wa28
39CL cG RI$Quoted values are relative intensities normalized to
39CL2cG I|g(1696.62|g)=100 (I|g values in 1980Hi01 divided by 10)
39CL cG RI(A)$Assuming no |b-feeding to 397 level
39CL cB IB$Deduced from |g-ray intensity balance at each level
39CL cL E$From a least-squares fit to |g-ray energies
39CL cL J$From Adopted Levels
39S P 0 (7/2)- 11.5 S 5 6640 50
39S cP J,T$From Adopted Levels of {+39}S.
39S cP QP$From 2017Wa10
39CL N 0.44 3 1.00
39CL cN NR$From |S(I|g to g.s.)=100, assuming no |b-feeding to g.s. and 397
39CL2cN level
39CL PN 3
39CL L 0 3/2+
39CL L 396.51 191/2+
39CL G 396.50 20 8.0 25 @
39CL2 G %IG=3.5 11
39CLF G FLAG=A
39CL L 1300.4314 (5/2+)
39CL B 8 6 6.1 4
39CLS B EAV=2441 25
39CL G 903.8 6 8.0 25
39CL2 G %IG=3.5 11
39CLF G FLAG=A
39CL G 1300.52 16 118 11 C
39CL2 G %IG=52 3
39CL L 1696.7815 5/2-
39CL B 68 7 5.06 6
39CLS B EAV=2247 25
39CL G 396.50 20 83 7 @C
39CL2 G %IG=37 3
39CL G 1696.62 17 100 8 C
39CL2 G %IG=44 3
39CL L 1785.3 3 (7/2-)
39CL B 10.6 15 5.83 7
39CLS B EAV=2203 25
39CL G 484.85 24 24 3 C
39CL2 G %IG=10.6 14
39CL L 2571.1023 (9/2)-
39CL B 12.8 16 5.40 7
39CLS B EAV=1820 25
39CL G 874.31 18 29 3 C
39CL2 G %IG=12.8 14