83BR 83SE B- DECAY (70.1 S) 1973FE08,1976KR20 15NDS 201503
83BR H TYP=FUL$AUT=E.A. MCCUTCHAN$CIT=NDS 125, 201 (2015)$CUT=31-Dec-2014$
83BR c 1976Kr20: {+83}Se activity from {+82}Se(n,|g), E=thermal. Measured
83BR2c E|g, I|g, |g|g using two coaxial Ge(Li) detectors
83BR c 1973Fe08: {+83}Se activity from {+82}Se(n,|g), E=thermal. Measured
83BR2c E|g, I|g, |g|g using two Ge(Li) detectors.
83BR c Others: 1986Sc10, 1967Ma35, 1958Co57
83BR c A total energy release of 3940 keV {I40} is calculated for this decay
83BR2c scheme using the RADLST code, in good agreement with the Q value of
83BR3c 3902 keV {I5}.
83BR cG E,RI$Weighted average of 1973Fe08 and 1976Kr20, except where noted.
83BR cG E(A)$From 1976Kr20. 1973Fe08 could not place this |g.
83BR cG E(B)$Seen by 1976Kr20 only.
83BR cG M,MR$From the Adopted Gammas.
83BR cL E$From a least-squares fit to E|g, by evaluator.
83BR cL J,T$From the Adopted Levels.
83BR D 1986Mu15 GIVES NR=0.170 4. VALUE OF 0.175 4 WAS DEDUCED BY E. BROWNE
83BR2D USING PROGRAM GABS.
83BR D CC$FROM BrIcc v2.3 (29-Mar-2013) 2008Ki07, "Frozen Orbitals" appr.
83SE P 228.92 7 1/2- 70.1 S 4 3673 5
83BR N 0.170 4 1.0 1.0 1.0
83BR cN NR$From |SI(|g+ce) to g.s.=100 - 31.0% {I7} with I|b(g.s)=31.0% {I7}
83BR2cN from 1968Sc10.
83BR PN 3
83BR G 322.2 3 0.15 15
83BR G 371.66 12 0.56 7
83BR G 698.9 3 0.5 1
83BR G 812.6 3 1.1 4
83BRX G FLAG=B
83BR G 1549.3 8 0.3 1
83BR G 1642.8 6 1.0 5
83BRX G FLAG=B
83BR G 2022.5 3 0.52 11
83BR G 2944.8 5 0.15 3
83BR L 0 3/2- 2.374 H 4
83BR B 31.0 7 6.0 1
83BRS B EAV=1705.1 26
83BR cB IB$from 1968Sc10.
83BR L 356.69 4 5/2-
83BR G 356.69 5 100 6 M1(+E2) +0.02 16 0.0042816 C
83BRS G KC=0.00381 14$LC=0.000407 16$MC=6.47E-5 25$NC=6.05E-6 22
83BR cG RI$|DI|g from 1976Kr20.
83BR L 799.12 6 (5/2,7/2)-
83BR G 442.4 1 0.37 7 C
83BR G 799.15 15 7.2 3 C
83BR B 0.20 LT 7.7 GT
83BRS B EAV=1322.5 26
83BR L 866.80 11 7/2-
83BR G 510.1 1 1.2 4 M1(+E2) -0.04 12 0.001844
83BRS G KC=0.00164 3$LC=0.000174 4$MC=2.76E-5 6$NC=2.59E-6 5
83BR cG RI$from 1976Kr20. 1973Fe08 give an upper limit of I|g<2.1
83BR B 0.27 LT 7.5 GT
83BRS B EAV=1290.3 26
83BR L 987.96 7 1/2-,3/2-
83BR G 188.9 1 1.03 10
83BR G 631.2 1 2.65 15 C
83BR G 988.05 12 92 4 C
83BR B 12.8 8 5.8 1
83BRS B EAV=1232.7 26
83BR L 1030.65 6 (3/2)-
83BR G 231.5 1 1.86 10 C
83BR G 673.98 11 87 3 C
83BR G 1030.6 1 121 4 C
83BR B 33.2 11 5.4 1
83BRS B EAV=1212.5 26
83BR L 1053.78 8 1/2-,3/2-
83BR G 1053.7 1 9.1 4 C
83BR B 0.36 10 7.3 1
83BRS B EAV=1201.5 26
83BR L 1660.08 9 1/2-,3/2-
83BR G 1303.3 3 5.0 3 C
83BR G 1660.1 1 11.2 11
83BR B 2.63 20 6.0 1
83BRS B EAV=916.0 26
83BR L 1915.45 10 1/2(-),3/2
83BR cL E$reported by 1976Kr20 only.
83BR G 884.5 5 1.2 4 C
83BRF G FLAG=B
83BR G 1116.3 1 4.0 3 C
83BRF G FLAG=A
83BR cG E$unplaced transition with E|g=1116.0 {I1}, I|g=3.1 {I2} observed by
83BR2cG 1973Fe08.
83BR G 1558.9 2 7.0 4 C
83BRF G FLAG=A
83BR cG E$unplaced transition with E|g=1558.5 {I3}, I|g=6.9 {I4} observed by
83BR2cG 1973Fe08.
83BR B 2.07 11 5.9 1
83BRS B EAV=797.5 25
83BR L 2051.45 8 1/2-,3/2-
83BR G 391.5 2 0.70 9 C
83BR G 997.6 1 7.0 3 C
83BR G 1020.75 15 12.4 9 C
83BR G 1063.7 2 20.4 6 C
83BR G 1694.7 2 4.5 3 C
83BR G 2051.5 2 64.3 17
83BR B 18.6 4 4.8 1
83BRS B EAV=734.9 25
83BR L 2809.71 19 1/2-,3/2-
83BR G 1779.0 2 1.7 LE C
83BR cG RI$from 1976Kr20. 1973Fe08 give I|g=4.1 {I3}.
83BR G 2453.2 7 0.29 8
83BR G 2809.9 7 0.09 2
83BR B 0.21 15 5.9 4
83BRS B EAV=396.9 24
83BR L 3091.3 3 1/2-,3/2-
83BR G 2734.7 3 0.31 6
83BR G 3090.7 5 0.25 4
83BR B 0.095 12 5.7 1
83BRS B EAV=279.2 22