127SB    127SN B- DECAY (4.13 M)       1995ST28                  11NDS    201108
127SB  H TYP=FUL$AUT=A. HASHIZUME$CIT=NDS 112, 1647 (2011)$CUT=1-Oct-2009$
127SB c  1995St28: {+235}U(n,F) on-line mass; semi |g, |g|g(t)
127SB c  1970HeZG: semi |g
127SB c  1977Lu06: {+235}U(n,F) on-line mass; Si(Li) |b, Si(Li)-NaI(Tl),
127SB2c  Si(Li)-Ge(Li) |b|g-coin
127SB c  It is announced that the levels confirmed only by |g|g coincidences
127SB2c  are shown in the decay scheme (1995St28). Furthermore, because of the
127SB3c  large Q(|b{+-})value of 3021 keV, many unobserved high-energy levels
127SB4c  could be populated in this decay. Consequently, th |b{+-} feedings may
127SB5c  be inaccurate (evaluator).
127SB cL E         From a least-squares fit to E(|g's)
127SB cL J         From adopted levels
127SB cG E         From 1995St28
127SB cG E(A)      Reported only by 1970HeZG.
127SB cB E(B)      The intensity of |b-ray feeding is obtained from the |g-ray
127SB2cB intensity balance to this level, assuming no |b-ray feeding to the
127SB3cB ground state.
127SN  P 5.06      6 (3/2+)            4.13 M    3              3201      24
127SB  N     0.97  19              1.00
127SB cN NR$No |b-ray feeding to the ground state was assumed.
127SB PN                                                                     3
127SB  G 860.3                                                              A
127SB  G 979.0                                                              A
127SB  G 1095.6                                                             A
127SB  G 1584.5                                                             A
127SB  L      0.0    7/2+              3.85 D    5
127SB  L 490.63    22(5/2)+
127SB  B             91                     5.6                             B
127SBS B EAV=1111 12
127SB  G 490.6     3 100
127SB CG           %IG=97.4  6, using the calculated normalization.
127SB  L 765.30    22(3/2)+
127SB  B             0.8                    7.5
127SBS B EAV=984 11
127SB  G 765.2     3 1.36
127SB CG           %IG=1.3  4, using the calculated normalization.
127SB  L 1185.6     31/2+
127SB  B             1.3                    6.9
127SBS B EAV=792 11
127SB  G 419.9     3 0.35
127SB  G 695.3     3 0.98
127SB  L 1351.6     3(5/2+)
127SB  B             0.7                    7.1
127SBS B EAV=717 11
127SB  G 1351.6    3 0.75
127SB CG           %IG=0.73 21, using the calculated normalization.
127SB  L 1471.17   24(7/2+)
127SB  G 1471.2    3 0.05
127SB CG           %IG=0.049 14, using the calculated normalization.
127SB  L 1700.3     4(1/2+,3/2,5/2)
127SB  B             1.3                    6.4
127SBS B EAV=562 11
127SB  G 1210.2    3 1.47
127SB  L 1711.16   227/2+
127SB  B             0.4                    6.9
127SBS B EAV=557 11
127SB  G 1220.51   3 0.52
127SB  L 1840.23   19(3/2+,5/2)
127SB  B             2.1                    6.1
127SBS B EAV=501 11
127SB  G 369.1     3 0.05
127SB  G 1075.2    3 0.23
127SB  G 1349.2    3 1.39
127SB  G 1840.3    3 0.46
127SB CG           %IG=0.45 13, using the calculated normalization.
127SB  L 1994.1     4                                                          ?
127SB  G 1503.5    3 0.05
127SB  L 2054.5     3(3/2+,5/2+)
127SB  B             1.7                    5.9
127SBS B EAV=410 11
127SB  G 342.3     3 0.13
127SB  G 354.8     3 0.11
127SB  G 1564.3    3 1.51
127SB  L 2150.0     4(1/2+,3/2,5/2)
127SB  B             0.2                    6.7
127SBS B EAV=370 10
127SB  G 1659.4    3 0.21
127SB  L 2303.7     4(1/2+,3/2,5/2)
127SB  B             0.1                    6.7
127SBS B EAV=307.1 97
127SB  G 1813.1    3 0.09