142SM    142EU EC DECAY (2.34 S)       1991FI03,1975KE08         11NDS    201108
142SM  H TYP=FUL$AUT=T.D. Johnson, D. Symochko(a), M. Fadil(b), and J.K. Tuli$
142SM2 H CIT=NDS 112, 1949 (2011)$CUT=1-Jun-2010$
142SM c  Measured: |g, |b{++} (1975Ke08); others: 1973VaYZ, 1987FiZW
142SM c  Decay scheme is given by 1991Fi03 based on earlier work of 1975Ke08.
142SM c  1991Fi03 obtained source in {+142}Gd decay and measured x-ray, |g,
142SM2c  |g(t). From two component fit to 768|g(t), assuming
142SM3c  T{-1/2}({+142}Gd)=70.2 s {I6}, they determined T{-1/2}({+142}Eu
142SM4c  g.s.)=2.34 s {I12}. I(|e+|b{++}) values of 1991Fi03 determined from
142SM5c  I|b{++}/I(768|g)=8.8 {I6} (1991Fi03) are given. Other:
142SMxc  I|b{++}/I(768|g)=8.4 {I11} (1975Ke08)
142SM cE           E|b+=7000 {I300} (1975Ke08), 6651 {I30} (1994Po26)
142SM DG CC$ FROM BrIcc v2.2b (20-Jan-2009) 2008Ki07, "Frozen Orbitals" appr.
142SM cL E$From least-squares fit to E|g.
142SM cL J         Adopted values
142EU  P 0.0         1+                2.34 S    12             7670      30
142SM  N 0.102     7 0.102   7 1.0       1.0
142SM PN                                                                     4
142SM  L 0.0         0+
142SM  E               81.0      5.12       4.3                 86.1
142SMS E EAV=3083 15$CK=0.0503 7$CL=0.00715 9$CM+=0.00205 3
142SM  L     768.11 82+
142SM  E                3.4      0.31       5.4                 3.7
142SMS E EAV=2715 15$CK=0.0699 10$CL=0.00995 14$CM+=0.00286 4
142SM  G 768.1      1100       E2
142SMS G CC=0.00444 7$KC=0.00373 6$LC=0.000556 8$MC=0.0001201 17$NC+=3.13E-5 5
142SMS G NC=2.71E-5 4$OC=3.97E-6 6$PC=2.20E-7 3
142SM cG M$from adopted gammas
142SM  L    1451.1113(0+)
142SM  E                0.5      0.07       6.0                 0.6
142SMS E EAV=2389 15$CK=0.0965 15$CL=0.01375 21$CM+=0.00395 6
142SM  G 683.0      14.1      4
142SM  G 1451.1                (E0)                             2         AP   S
142SM cG $Transition not observed. I(|g+ce) from excess I(K| x ray)
142SM  L    1657.90 8(2)+
142SM  E               2.39      0.347      5.3                 2.74
142SMS E EAV=2291 15$CK=0.1070 17$CL=0.01525 24$CM+=0.00438 7
142SM  G 889.8      110.4    7
142SM  G 1657.9    1 17.2    13
142SM  L    2055.52132+
142SM  E               1.36      0.251      5.3                 1.61
142SMS E EAV=2103 15$CK=0.1316 22$CL=0.0188 3$CM+=0.00540 9
142SM  G 1287.4    1 11.4    8
142SM  G 2055.8    204.4     4
142SM  L    2173.52130+
142SM  E               0.34      0.068      5.9                 0.41
142SMS E EAV=2047 15$CK=0.1403 23$CL=0.0200 4$CM+=0.00575 10
142SM  G 1405.4     14.0     4
142SM  L     2353.7 3(2+)
142SM  E               0.43      0.097      5.7                 0.53
142SMS E EAV=1962 15$CK=0.155 3$CL=0.0221 4$CM+=0.00636 11
142SM  G 2353.7    3 5.2     10
142SM  L     2373.9 3(2+)
142SM  E               0.63      0.14       5.5                 0.77
142SMS E EAV=1953 15$CK=0.157 3$CL=0.0224 4$CM+=0.00643 11
142SM  G 2373.9     37.5     9
142SM  L     2439.410(0+)
142SM  E               1.04      0.248      5.3                 1.29
142SMS E EAV=1922 15$CK=0.162 3$CL=0.0232 4$CM+=0.00667 12
142SM  G 1671.3      12.6
142SM  L    2522.2412(0+)
142SM  E               1.25      0.316      5.2                 1.57
142SMS E EAV=1883 14$CK=0.170 3$CL=0.0243 5$CM+=0.00699 12
142SM  G 864.4     2 0.84    18
142SM  G 1754.1    1 14.6    12
142SM  L     3031.8 4(0+)
142SM  E               0.36      0.14       5.4                 0.50
142SMS E EAV=1645 14$CK=0.229 5$CL=0.0328 6$CM+=0.00942 17
142SM  G 2263.7    4 4.9     11
142SM  L    3187.8322(0+)
142SM  E               0.17      0.071      5.7                 0.24
142SMS E EAV=1572 14$CK=0.251 5$CL=0.0360 7$CM+=0.01035 19
142SM  G 2419.7    2 2.4     9