80RB 80SR EC DECAY (106.3 M) 1973BR32 05NDS 200508
80RB H TYP=FUL$AUT=BALRAJ SINGH$CIT=NDS 105, 223 (2005)$CUT=22-Jun-2005$
80RB c 1973Br32: Measured |g, |g|g, T{-1/2}. Source produced by
80RB2c {+65}Cu({+20}Ne,5n){+80}Y. {+80}Y decays by |e to {+80}Sr
80RB c 1961Ho13, measured |g, T{-1/2}({+80}Sr)
80RB cL E$From least-squares fit to E|g's
80RB cL J$From 'adopted levels'
80SR P 0 0+ 106.3 M 15 1865 10
80RB N 0.39 3 1.0 1.0
80RB cN NR$from I|g(589|g)(absolute)=39 {I3} deduced by 1973Br32 from
80RB2cN I(|g{+|+})/I|g(617|g from {+80}Rb |e)=7.95, I|g(617|g) and I|g(589|g)
80RB3cN when {+80}Sr and {+80}Rb were in equilibrium
80RB PN 4
80RB L 0.0 1+
80RB E 9.2 16 31 5 4.79 8 40 7
80RBS E EAV=368.2 44$CK=0.674 7$CL=0.0789 8$CM+=0.01667 16
80RB cE TI$from I|g(589|g)(absolute)=39 {I3} (1973Br32) deduced from
80RB2cE intensities of annihilation radiation, 617|g and 589|g when
80RB3cE {+80}Sr and {+80}Rb were in equilibrium
80RB L 174.9 4 (2-)
80RB E 0.32 15 2.4 11 5.81 21 2.7 13
80RBS E EAV=292.5 43$CK=0.772 5$CL=0.0906 6$CM+=0.01914 13
80RB G 175.0 5 26 3
80RB L 236.1 8 ?
80RB E 0.27 5 2.8 5 5.70 7 3.1 5 ?
80RBS E EAV=266.2 43$CK=0.800 5$CL=0.0938 5$CM+=0.01983 11
80RB G 235.9 8 10.7 11 ?
80RB L 553.5 4 1+
80RB E 0.070 13 12.0 13 4.89 5 12.1 13
80RBS E EAV=131.0 43$CK=0.8700 7$CL=0.1025 1$CM+=0.02168 3
80RB G 316.0 15 2.7 3 ?
80RB G 378.8 5 10.7 11
80RB G 553.4 5 17.6 18
80RB L 589.0 4 1+
80RB E 0.14 3 42 5 4.32 6 42 5
80RBS E EAV=115.9 43$CK=0.8720 5$CL=0.10280 8$CM+=0.02174 2
80RB G 414.1 5 8.3 8
80RB G 589.0 5 100 10