87RB    87KR B- DECAY                 1971SH01,1973BLZH,1973GEYV15NDS    201510
 87RB  H TYP=FUL$AUT=T.D. Johnson and W.D. Kulp(a)$CIT=NDS 129, 1 (2015)$
 87RB2 H CUT=27-Jul-2015$
 87RB DG CC$ FROM BrIcc v2.3 (9-Dec-2011) 2008Ki07, "Frozen Orbitals" appr.
 87RB cL           The level scheme is that proposed by 1971Sh01,
 87RB2cL      with one additional level at 1389 keV from 1973BlZH.
 87RB cG           |g-ray data for about 30 |g's were measured with good
 87RB2cG      accuracy by 1971Sh01, 1973BlZH, and 1973GeYV.  They are
 87RB3cG      in good agreement even for very weak transitions.
 87RB4cG      |g|g-coincidences (Ge(Li)) were measured by 1971Sh01.  Shorter
 87RB5cG      sets of |g data are given by 1967Ho17, 1969Bo02, 1969Ly01,
 87RB6cG      1969On01, and 1 |g ray by 1979Bo26.
 87RB cL E         From least-squares fit to |g-ray energies.
 87RB cL J         From {+87}Rb Adopted Levels.
 87RB cB E         |b- energies were measured with |s=50 keV to 100 keV by
 87RB2cB      1969Bo02. For other measurements, see 1969On01 and 1969Ly01.
 87RB cB IB        A measurement in a magnetic spectrometer and detailed
 87RB2cB      analysis of the |b{+-} spectrum was carried out by 1973Wo01.
 87RB3cB      The decomposition of this spectrum was done without intensity
 87RB4cB      constraints from the decay scheme and with constraints based
 87RB5cB      on several previous decay schemes.  Their results which differ
 87RB6cB      significantly from those from the intensity balances are noted.
 87RB cB IB        The value for the decay to the ground state, 30.5, is from
 87RB2cB      1973Wo01 and those for the excited levels are from the |g-ray
 87RB3cB      intensity balances.  Where they differ significantly, the values
 87RB4cB      recommended by 1973Wo01 are given in comments.  The analysis of
 87RB5cB      1973Wo01 does not include the level at 1389 and it does not give
 87RB6cB      values for branches of less than 0.4%.
 87RB cB IB        The |b strength function has been reported by 1973Jo02 in
 87RB2cB      graphical form.  These data support the absence of any strong
 87RB3cB      |b branches to levels between 900 and 1500 keV.
 87RB cG E,RI      Weighted average of values from 1971Sh01, 1973BlZH, and
 87RB2cG      1973GeYV, unless noted otherwise.
 87RB cG E(A)      Not observed by 1973GeYV
 87RB cG E(B)      Not observed by 1971Sh01
 87RB cG E(D)      Not observed by 1973BlZH
 87RB  N 0.496     24          1.0       1.0
 87RB cN NR        calculated to give 100% feeding of ground state with
 87RB2cN      direct |b- feeding of 30.5% {I22} (1973Wo01).
 87RB PN                                                                     3
 87KR  P 0.0          5/2+             76.3 M    5              3888.27   25
 87RB  G 129.4      3 0.09    2                                             D
 87RB  G 510.78    14 0.16    4                                             A
 87RB  G 901.5      3 0.053   9                                             D
 87RB  G 1063.2     4 0.054  12                                             A
 87RB  G 1842.61   23 0.28    2                                             B
 87RB  G 3704.6    10 0.03    1
 87RB3 G FLAG=BD
 87RB  L      0.0     3/2-             4.97E10 Y 3
 87RB  B                30.5 22            7.81   4
 87RBS B EAV=1694.44
 87RB  L  402.588  12 5/2-
 87RB  B                   41 3            7.47   4
 87RBS B EAV=1501.66
 87RB cB IB        other: 42.9 (1973Wo01)
 87RB  G 402.588   12 100     4M1+E2     -0.24   12    0.0041118             C
 87RB CG E$ From 1979Bo26. Others: 402.7 {I3}, (1971Sh01), 402.60 {I10},
 87RB2CG    and 402.578 {I20}, (1973GeYV).
 87RB cG MR        from {+87}Rb Adopted Gammas.
 87RB  L   845.44   4(1/2)-
 87RB  B                  7.3 4            9.371 24                          1U
 87RBS B EAV=1293.80
 87RB  G 845.44     4 14.8    4                                              C
 87RB  L 1349.36   10
 87RB  G 946.69    13 0.26    1                                              C
 87RB  L  1389.88  12(3/2)-
 87RB  B                0.119 8            9.39   3
 87RBS B EAV=1033.36 13
 87RB  G 1389.87   12 0.24    1
 87RB  L 1578.05    61/2-,3/2-
 87RB  B                 0.12 5            9.24  18
 87RBS B EAV=945.25 12
 87RB  G 1175.41    7 2.23    8                                              C
 87RB  G 1578.03   14 0.26    2
 87RB  L 1740.58    5(3/2,5/2)-
 87RB  B                 0.62 9            8.40   7
 87RBS B EAV=869.60 12
 87RB  G 1338.00    7 1.28    7                                              C
 87RB  G 1740.51    7 4.11    9                                              C
 87RB  L 2378.38   18
 87RB  B                0.06012            8.79   9
 87RBS B EAV=578.33 14
 87RB  G 1531.2     4 0.72   11                                             DC ?
 87RB3 G FL=845.44
 87RB cG E         from 1971Sh01, but is a poor fit and not resolved by
 87RB2cG      1973GeYV from the double-escape peak of the 2554|g .  Not
 87RB3cG      included in the least-squares fit which gives E|g=1532.96
 87RB4cG      {I12} for this transition.
 87RB  G 2378.5     3 0.19    1
 87RB  L  2414.44   6(3/2-)
 87RB  B                  5.5 3            6.788 24
 87RBS B EAV=562.23 12
 87RB cB IB        other: 5.07 (1973Wo01)
 87RB  G 673.83     8 3.81   10                                              C
 87RB  G 836.38     5 1.56    4                                              C
 87RB  G 2011.88   10 5.81   23                                              C
 87RB  L 2554.82    73/2+,5/2+
 87RB  B                  9.4 7            6.38   4
 87RBS B EAV=500.05 12
 87RB cB IB        other: 8.09 (1973Wo01)
 87RB  G 814.25     6 0.33    2
 87RB  G 976.14    12 0.113   8
 87RB  G 2554.75   25 18.6    9
 87RB  L  2811.25  143/2+,5/2+
 87RB  B                 0.60 4            7.22   3
 87RBS B EAV=388.95 13
 87RB cB IB        other: 0.42 (1973Wo01)
 87RB  G 1461.3     7 0.10    1                                             D
 87RB  G 2408.46   15 0.46    4
 87RB  G 2811.36   20 0.65    3
 87RB  L 2960.62    7(3/2,5/2)+
 87RB  B                  4.4 4            6.11   4
 87RBS B EAV=326.12 11
 87RB  G 582.32    21 0.07    2                                             A
 87RB  G 1382.55    7 0.58    2                                              C
 87RB  G 1611.18   14 0.23    3                                              C
 87RB  G 2558.08   19 8.0     5                                              C
 87RB  G 2961.2     8 0.14    4                                             A
 87RB  L  3055.15  243/2,5/2,7/2(-)
 87RB  B                0.108 9            7.55   4
 87RBS B EAV=287.26 15
 87RB  G 2652.48   38 0.047   8
 87RB  G 3055.1     3 0.162  13
 87RB  L  3308.49  123/2+,5/2+
 87RB  B                 0.49 4            6.33   4
 87RBS B EAV=187.49 11
 87RB cB IB        other: 0.91 (1973Wo01); this value may include some
 87RB2cB      scattered electrons or it may indicate additional |g rays
 87RB3cB      from this level.
 87RB  G 894.02    13 0.092   7
 87RB cG E         uncertainty in energy of this weak |g seems to be
 87RB2cG      underestimated by 1973BlZH and was increased by the evaluator
 87RB3cG      from 0.1 to 0.2 keV.
 87RB  G 3308.5     2 0.90    5