139PR    139ND EC DECAY (29.7 M)       1975VY02,1971BU22,1969BE6416NDS    201610
139PR  H TYP=FUL$AUT=P.K. JOSHI, B. SINGH, S. SINGH, A.K. JAIN$
139PR2 H CIT=NDS 138, 1 (2016)$CUT=15-Oct-2016$
139PR c  1969Be64 measured |g's, prompt and delayed |g|g-coincidences
139PR2c  (Ge(Li),NaI), and |g(t) (NaI).
139PR c  1971Bu22 measured |g's and ce's and |b{++}'s; chem.
139PR c  1975Vy02 measured |g's and |b{++}'s (mag spect; Si(Li)); chem.
139PR c  All data and decay scheme are from 1971Bu22, except as noted.
139PR2c  Other: 1988IsZX.
139PR cE TI$From |g-transition intensity balances for excited states
139PR cG $Coincidences shown on drawing are from 1969Be64. See
139PR2cG 1969Be64 for possible coincidences.
139PR cG $|a(K)exp: normalized to |a(K)(231|g {+139}Nd; M4)=9.5.
139PR cG $See 5.5-h |e decay for other gammas with T{-1/2}=29.7 min or
139PR2cG 5.5 h observed but not assigned by 1975Vy02.
139PR cG M$From Adopted Gammas, mainly based on |a(K)exp in the present
139PR2cG dataset, except as noted. The |a(K)exp: normalized to |a(K)(231|g
139PR3cG {+139}Nd; M4)=9.4.
139PR cL J         From the Adopted Levels.
139ND  P 0.0         3/2+              29.7 M    5              2806      28
139ND cP J,T$From {+139}Nd Adopted Levels
139ND cP QP$ From 2012Wa38
139PR  N 0.190     27 0.190  27 1         1
139PR cN NR,NT     from I(|g{+|+})=260 {I40} relative to I|g(405|g)=36.4,
139PR2cN decay scheme, and theoretical |e/|b{++} ratios for |e,|b{++}
139PR2cN transition to the ground state
139PR PN                                                                     3
139PR  G 220.9      30.4      1
139PR  G 368.0      30.7      2
139PR  G 621.7      36.4      7
139PR  G 696.2      32.0      4                                                ?
139PR  G 1221.2     81.5      5
139PR  G 1233.3     80.7      3                                                ?
139PR  G 1246.7     81.0      4
139PR  G 1463.4     61.7      4
139PR  L 0.0         5/2+
139PR  E                24   1    61   2   5.13  2                85      2
139PRS E EAV=803 13$CK=0.604 9$CL=0.0848 13$CM+=0.0240 4
139PR cE E$2792 {I50} from measured E|b{++} (1975Vy02)
139PR cE TI$100-summed |e+|b{++} feeding to the excited states. See also comment
139PR2cE for I|g normalization. Other: I(|b{++})=16.6% {I28} from I|b+=2.38%
139PR3cE {i40} of the 5.5-h decay and IT branching ratio of 14.3% {i14}
139PR4cE (1971Bu22,1975Vy02). Value of |e/|b{++}(for g.s.)=2.51 {I20} (theory),
139PR5cE 2.5 (1969Be64), and 2.3 {I2} (1971Bu22).
139PR  L     113.86 57/2+
139PR2 L G=0.34 6 (1983AkZY)
139PR cL G         from |g|g(|q,H,t) with T{-1/2}=2.6 ns.
139PR  G 113.87    5 4.6     CA M1+E2    0.16    10    0.906  22 8.7      8  C
139PR cG E$from 5.5-h |e decay.
139PR cG RI$other: 3.7 {I3} from I(|g+ce) and |a.
139PR cG TI$from intensity balancing. Level not expected to be fed
139PR2cG directly in |e decay (|DJ|p=2,no).
139PRS G K/T=0.402 4$L/T=0.0554 9$M/T=0.01168 18$N+/T=0.00306 5
139PRS G N/T=0.00261 4$O/T=0.000420 7$P/T=3.09E-5 5
139PR  L     405.04 93/2+
139PR  E               0.43  8    2.5  4   6.4   1               2.9      5
139PRS E EAV=622 13$CK=0.720 8$CL=0.1016 11$CM+=0.0288 3
139PR  G 405.0     1 36.4       M1                     0.0288                C
139PR3 G EKC=0.025 7
139PRS G KC=0.0246 4$LC=0.00328 5$MC=0.000689 10$
139PRS G NC=0.0001542 22$OC=2.49E-5 4$PC=1.86E-6 3
139PR  L     588.82155/2+
139PR  E               0.26  5    2.3  5   6.3   1              2.6       5
139PRS E EAV=540 13$CK=0.763 6$CL=0.1079 9$CM+=0.0306 3
139PR  G 183.5     2 4.0      4 M1                     0.245  10
139PRS G KC=0.194 8$LC=0.040 13$MC=0.009 3$
139PRS G NC=0.0019 7$OC=0.00029 8$PC=1.32E-5 22
139PRS G EKC=0.45 18
139PR  G 475.5     3 6.9      6 M1                     0.0191
139PRS G KC=0.01639 23$LC=0.00217 3$MC=0.000456 7$
139PRS G NC=0.0001020 15$OC=1.648E-5 24$PC=1.236E-6 18
139PR  G 588.8      34.2      6
139PR  L 916.90    23(1/2+,3/2+,5/2+)
139PR  E               0.049 12   1.4  3   6.4   1              1.4       3
139PRS E EAV=396 13$CK=0.816 4$CL=0.1161 6$CM+=0.03295 16
139PR  G 916.9      38.0      8
139PR3 G EKC AP 0.0047
139PR  L    1074.0322(1/2+,3/2,5/2)
139PR  E               0.077 18   4.4  8   5.8   1               4.5      8
139PRS E EAV=327 13$CK=0.8307 21$CL=0.1185 4$CM+=0.03366 11
139PR  G 485.0      42.4      4
139PR  G 669.0      38.0     10                                              C
139PR  G 1074.2     413.3    14
139PR  L     1311.8 4(1/2+,3/2,5/2)
139PR  E              0.0011 4   0.30  9   6.9   2               0.30     9
139PRS E EAV=223 13$CK=0.8412 7$CL=0.12081 21$CM+=0.03435 7
139PR  G 1311.8    4 1.6     4
139PR  L    1328.4022 (3/2+,5/2)
139PR  E              0.0066 22   2.1  4   6.0   1               2.1      4
139PRS E EAV=216 13$CK=0.8415 6$CL=0.12093 20$CM+=0.03438 6
139PR  G 411.5      20.8      2
139PR  G 923.4      37.0      7
139PR3 G EKC AP 0.0054
139PR  G 1213.4    8 1.7     5
139PR  G 1328.8     61.5      4
139PR  L     1405.5 5(1/2+,3/2,5/2)
139PR  E              0.0009 4   0.61  13  6.5   1               0.61     13
139PRS E EAV=182 13$CK=0.8426 3$CL=0.12141 17$CM+=0.03453 6
139PR  G 1405.5     53.2      5
139PR  L     1449.010(1/2+,3/2,5/2)
139PR  E                         0.15  6   7.1   2               0.15     6
139PRS E CK=0.8428 2$CL=0.12165 16$CM+=0.03461 5
139PR  G 1449      1 0.8      3
139PR  L     1501.2 4(1/2+,3/2,5/2)
139PR  E                         0.63  14  6.4   1               0.63     14
139PRS E CK=0.8429$CL=0.12192 15$CM+=0.03470 5
139PR  G 1096.5     42.0      4
139PR  G 1500.5     61.3      4
139PR  L     1532.010(1/2+,3/2,5/2)
139PR  E                         0.13  6   7.1   2               0.13     6
139PRS E CK=0.84291 9$CL=0.12208 15$CM+=0.03475 5
139PR  G 1532      1 0.7      3