163TM    163YB EC DECAY (11.05 M)      1975AD09                  10NDS    201005
163TM  H TYP=FUL$AUT=C. W. REICH, BALRAJ SINGH$CIT=NDS 111, 1211 (2010)$
163TM2 H CUT=12-Apr-2010$
163TM c  1975Ad09 (and 1985Ad12): {+163}Yb isotope obtained by bombardment of
163TM2c  tantalum by a 660-MeV proton beam followed by chemical separation.
163TM3c  Measured |g, ce, prompt and delayed |g|g coin, |b|g coin. 1985Ad12
163TM4c  reanalyzed data
163TM c  Others:
163TM c  Identification and T{-1/2} of {+163}Yb: 1967Pa20, 1968GrZX, 1970DeZF,
163TMxc  1972Ch23
163TM c  |g: 1970DeZF (about 40 |g rays reported)
163TM c  The decay scheme and all data, except as noted, are from 1975Ad09 as
163TM2c  modified by 1985Ad12. The major modifications were: new
163TM3c  levels at 175 and 254, removal of levels at 224 and 288, introduction
163TM4c  of 5/2[402] and 3/2[411] bands, and changes in spins and parities
163TM5c  of the 137, 498, and 559 levels.
163TM cE $Intensity balance gives apparent %|e+|b{++} feeding of
163TM2cE 1.9 {I7} for 174.59, (9/2)- level, whereas none is expected from
163TM3cE 3/2- parent state. Also at 86.9 level, there is a negative intensity
163TM4cE balance of -4.8 {I24}. These discrepancies are most likely due to
163TM4cE missing or incorrect placements
163TM cE LOGFT,TI$All values are considered as approximate since many
163TM2cE |g rays remain unplaced and |e, |b{++} feeding of g.s. and 13.5 level
163TM3cE are not known
163TM cG $|?13% of the total transition intensity is
163TM2cG unplaced
163TM cG $|a(K)exp: normalized via theoretical |a(K)(104|g,M1)=2.16
163TM2cG from {+163}Tm decay
163TM cG TI$From |SIce, except as noted
163TM cG M,MR$From |a(exp)'s and subshell ratios. |d's derived by the evaluators
163TM cG E(A)$Questionable assignment
163TM cL $Bands: from 1977Fo08 and 1975Ad09. Modified and extended by
163TM2cL 1985Ad12, based on a reanalysis of data and systematics of odd Tm
163TM3cL nuclides (A=161 to 169). See the adopted levels for parameter values.
163TM cL $See 1985Ad12 for structure of nonrotational states (independent
163TM2cL quasiparticles and quasiparticle-phonon model)
163TM cL E$From least-squares fit to E|g's
163TM cL J$From adopted levels
163TM cL T$From 1980AlZE (ce|g(t) and |g|g(t)), unless otherwise stated
163TM CL BAND(B)$ |p1/2[411] band.
163TM2cL From configuration of g.s. and agreement with neighboring odd Tm
163TM3cL nuclides.
163TM CL BAND(C)$ |p7/2[523] band.
163TM2cL From comparison with neighboring odd-A Tm nuclides.
163TM CL BAND(G)$ |p1/2[541] band (?).
163TM CL BAND(Z)$ |p5/2[402] band.
163TM CL BAND(Y)$ Probable |p3/2[411] band.
163TM  N 0.24      6  0.24   6   1.       1.
163TM cN NR,NT$|SI(|g+ce)(to g.s.+13.5)=100-I(|e+|b)(g.s.+13.5) where
163TM2cN I(|e+|b)(g.s.+13.5)=19 {I19} based on log| {Ift}>5.9 expected
163TM3cN for first-forbidden transitions. The normalization is considered as
163TM4cN approximate since many transitions (with as much as 15% of the
163TM5cN total intensity) are still unplaced
163TM PN                                                                     3
163YB  P 0.0          3/2-             11.05 M   25             3431      17
163YB cP J,T$From the {+163}Yb adopted levels.
163YB cP QP$From 2009AuZZ, 2003Au03
163YB cP $Configuration=|n3/2[521]
163TM  G 79.96     5  1.0    2 M1+E2     0.67    47    6.4    4
163TMS G KC=3.9 9$LC=1.9 10$MC=0.45 25$NC+=0.12 7
163TMS G NC=0.10 6$OC=0.013 7$PC=0.00023 7
163TMS G L1C=0.53 15$
163TM cG $|a(K)exp=4 {I1}, K/L1|?6.7
163TM cG E$from ce spectrum. Placement from a 224 level (1975Ad09) is
163TM2cG omitted by 1985Ad12
163TM  G 152.2     5  0.40   15
163TM cG $Placement from a 288 level (1975Ad09) is omitted by 1985Ad12
163TM2cG since 152|g-123|g coin also found in a higher part of the decay scheme
163TM  G 234.45    5  7.7    4 E1                      0.0357
163TMS G KC=0.0300 5$LC=0.00444 7$MC=0.000986 14$NC+=0.000261 4
163TMS G NC=0.000228 4$OC=3.16E-5 5$PC=1.496E-6 21
163TM cG $|a(K)exp=0.026 {I5}
163TM  G 416.8     3  0.60   8
163TM  G 447.36    20 0.70   4
163TM  G 457.4     5  0.30   10                                             A
163TM  G 481.97    20 0.86   10
163TM  G 520.7     7  0.64   15
163TM  G 561.52    30 0.78   11
163TM  G 567.71    20 1.00   11
163TM  G 601.0     30 0.20   6
163TM  G 606.02    15 5.5    3
163TM  G 619.3     3  1.2    2
163TM  G 622.2     4  1.0    2
163TM  G 643.8     3  0.70   10
163TM  G 670.0     5  1.0    3
163TM  G 694.64    30 2.4    3
163TM  G 709.67    20 1.1    3
163TM  G 730.05    20 1.6    2
163TM  G 739.9     7  0.9    2                                              A
163TM  G 743.7     5  0.78   15
163TM  G 759.1     3  1.0    2
163TM  G 797.0     3  1.7    2
163TM  G 817.9     5  0.93   15
163TM  G 841.1     12 1.5    7
163TM  G 848.5     7  2.7    7
163TM  G 853.0     5  4.0    7
163TM  G 867.5     8  2.3    7
163TM  G 881.43    50 0.56   15                                             A
163TM  G 904.34    25 2.8    3
163TM  G 920.28    20 2.8    3
163TM  G 934.91    50 1.5    3
163TM  G 942.20    20 4.8    4
163TM  G 948.5     6  1.4    2
163TM  G 959.14    15 3.4    2
163TM  G 970.00    20 3.0    2
163TM  G 983.0     10 1.2    3
163TM  G 1002.68   15 2.5    2
163TM  G 1015.3    5  0.40   15
163TM  G 1019.8    5  0.5    2
163TM  G 1023.28   14 2.82   17
163TM  G 1035.9    3  1.7    2
163TM  G 1040.8    3  2.2    2
163TM  G 1045.11   20 3.0    2
163TM  G 1052.2    7  0.5    2
163TM  G 1065.3    4  1.30   17
163TM  G 1095.04   25 1.1    2
163TM  G 1102.12   17 1.0    2
163TM  G 1108.0    7  0.37   10                                             A
163TM  G 1113.9    5  0.9    2
163TM  G 1115.9    20 0.22   16                                             A
163TM  G 1124.24   20 1.22   15
163TM  G 1158.0    7  0.43   13
163TM  G 1164.80   20 1.3    3
163TM  G 1172.0    10 0.2    1
163TM  G 1178.0    15 0.6    2
163TM  G 1235.3    3  1.25   15
163TM  G 1240.88   25 1.30   15
163TM  G 1252.5    5  1.0    2
163TM  G 1284.0    5  0.40   15
163TM  G 1291.0    8  0.22   10
163TM  G 1303.6    4  0.5    2
163TM  G 1315.3    7  0.5    1
163TM  G 1364.1    3  1.7    2
163TM  G 1414.2    3  1.31   17
163TM  G 1465.6    10 0.8    3                                              A
163TM  G 1498.0    10 0.5    2                                              A
163TM  G 1506.6    3  1.18   13
163TM  G 1511.8    5  0.8    2
163TM  G 1514.0    15 0.30   15                                             A
163TM  G 1520.5    4  0.74   14
163TM  G 1545.3    5  0.40   8
163TM cG $Placement from a 1833 level (1975Ad09) is omitted by 1985Ad12
163TM  G 1560.5    3  1.0    2
163TM  G 1591.4    3  0.75   10
163TM  G 1598.5    8  0.30   12                                             A
163TM  G 1611.48   15 1.96   15
163TM  G 1619.2    5  0.51   10
163TM  G 1651.4    8  0.6    2
163TM  G 1708.3    3  0.95   11
163TM  G 1734.6    3  0.90   13
163TM  G 1788.55   20 1.20   15
163TM  G 1843.7    4  0.68   8
163TM  G 1857.1    8  0.40   8                                              A
163TM  G 1861.0    9  0.4    1                                              A
163TM  G 1871.2    4  0.7    1
163TM  G 1883.0    3  0.46   8                                              A
163TM  G 2014.4    6  0.31   6
163TM  G 2026.0    6  0.30   6
163TM  G 2052.8    6  0.25   6
163TM  G 2060.6    6  0.24   6
163TM  L 0.0          1/2+                                                  B
163TM  E                6    LE   14   LE   5.9  GE                  20   LE   ?
163TMS E EAV=1088.3 77$CK=0.574 4$CL=0.0890 6$CM+=0.02668 19
163TM cE TI$from log| {Ift}|>5.9 for first-forbidden transitions.
163TM2cE See also comment for |e feeding to 13.5 level
163TM  L 13.52     2  3/2+             0.9 NS    LT                         B
163TM  E                6    LE   14   LE   5.9  GE                20     LE   ?
163TMS E EAV=1082.2 77$CK=0.577 4$CL=0.0895 6$CM+=0.02682 19
163TM cE TI$from log| {Ift}|>5.9 for first-forbidden transitions.
163TM2cE Intensity balance gives 70 {I50}. A similar |b transition in the decay
163TM3cE of {+161}Er (1984He18) with log| {Ift}|>6.9 would imply
163TMxcE I(|e+|b+)(13.5)|<1.9%.
163TM  G 13.53     3  2.32   APM1+E2     0.04    AP    240    AP 5.8E+2   16
163TMS G L/T AP 0.773$M/T AP 0.176$N+/T AP 0.0466
163TMS G N/T AP 0.0408$O/T AP 0.00555$P/T AP 0.000239
163TM cG $E|g from ce data. I|g from I(|g+ce) and |a
163TM cG CC        assuming |D|d=50%
163TM cG $M1/M2|?4
163TM  L 23.28     5  (7/2)+
163TM cL           |p7/2[404] bandhead
163TM  E                0.8  4     5   3   7.9   2                6       3  1U?
163TMS E EAV=1075.0 75$CK=0.7217 23$CL=0.1154 4$CM+=0.03476 12
163TM  G 9.74      5 0.00118 5  E2                     1.32E+5  156       7
163TM cG $E|g from ce data. I|g from I(|g+ce) and |a
163TMS G LC=8.55E+4$MC=3.47E+4$NC+=1.16E+4 CA
163TM cG $|a(M1):|a(M2):|a(M3)=0.010:0.70:1.00
163TM cG M$from M1<