102Y 102SR B- DECAY 1986HI02 09NDS 200908
102Y H TYP=FUL$AUT=D. DE FRENNE$CIT=NDS 110, 1745 (2009)$CUT=31-Dec-2008$
102Y c Mass assignment from mass-separated A=102 source from {+235}U(n,F).
102Y 2c Z assignment from yield, systematics, T{-1/2} and level scheme.
102Y 3c Measured: E|g, I|g, |g|g, T{-1/2}. Deduced: {+102}Y levels, log|
102Y xc {Ift}, J|p. Structure information in relation with this work can be
102Y yc found in 1986Pe04
102Y cB From |g-ray transition intensity balance. M1 multipolarity
102Y 2cB assumed for all low-energy |g rays, except the 93|g for which E2 was
102Y 3cB assumed because otherwise negative level feeding. As a consequence of
102Y 4cB that assumption the logft values are only approximate values and should
102Y 5cB be treated as such
102Y 4cB |?3% of {+102}Sr decay unobserved
102Y cL J log| {Ift}<4.5 suggests J|p-1+
102Y CL $LOGFT due to the incompleteness of the decay scheme due to the large
102Y 2CL ^Q value all LOGFT values should be considered as lower limits
102SR P 0.0 0+ 69 MS 6 8810 70
102Y N 0.53 16 1.0 1.0
102Y cN From absolute intensity I(243|g)=50 {I15} per 100 {+102}Tc
102Y 2cN g.s. decays and delayed-neutron emission probabilities of 4.8% {I23}
102Y 3cN for {+102}Sr and 6.0% {I12} for {+102}Y. Unobserved 3% of {+102}Sr
102Y 4cN decay not taken into account. An absolute intensity for the 475|g of
102Y 5cN 6.7 per 100 decays of the {+102}Tc 1+ isomer was used (1986Hi02).
102Y PN 0.53 16 1.0 5
102Y G 814.4 3 5.3 10
102Y L 0.0 0.36 S 4
102Y B 3 LT 5.6 GT
102Y 2 B EAV= 4052 385
102Y L 93.80 6
102Y B 3.3 24 5.6 4
102Y 2 B EAV= 4007 385
102Y G 93.89 8 25.3 14[E2] 1.348 C
102Y L 208.23 9
102Y B 6 4 5.3 4
102Y 2 B EAV= 3952 385
102Y G 114.46 154.7 5 [M1] 0.1256 C
102Y G 208.16 1314.9 11[M1] 0.0257 C
102Y L 243.85 61+
102Y B 35 12 4.4925
102Y 2 B EAV= 3935 385
102Y G 35.58 181.0 14[M1] 3.53
102Y G 150.15 1034.0 18[M1] 0.0608 C
102Y G 243.80 8 100 5 [M1] 0.01713 C
102Y L 311.70 9
102Y B 3.9 20 5.4 3
102Y 2 B EAV= 3903 385
102Y G 67.89 1414.9 9 [M1] 0.542 C
102Y G 103.4 2 1.8 3 [M1] 0.1660 ?
102Y G 217.92 157.0 6 [M1] 0.02285 C
102Y G 311.6 2 2.7 5
102Y L 497.81 10
102Y B 5.2 23 5.3 3
102Y 2 B EAV= 3813 385
102Y G 186.15 157.0 7 [M1] 0.0344 C
102Y G 253.95 1523.8 15[M1] 0.01543 C
102Y G 404.2 2 1.1 5
102Y G 498.4 6 1.6 9
102Y L 645.4 4 ?
102Y B 1.0 5 5.9 3
102Y 2 B EAV= 3742 385
102Y G 437.2 3 1.9 7 C
102Y L 898.63 22
102Y B 3.9 14 5.3 3
102Y 2 B EAV= 3620 386
102Y G 655.1 3 3.6 8 C
102Y G 804.5 3 3.8 9 C
102Y L 1347.92 141+
102Y B 21 7 4.4 3
102Y 2 B EAV= 3404 386
102Y G 850.4 2 6.7 11 C
102Y G 1036.0 2 14.0 18 C
102Y G 1104.0 2 19 2 C
102Y L 1689.58 151+
102Y B 17 6 4.4 3
102Y 2 B EAV= 3240 386
102Y G 1191.8 2 17 2 C
102Y G 1378.1 3 6.5 17 C
102Y G 1445.5 3 6.1 14 ?
102Y G 1689.4 4 3.0 11