106CD    106IN EC DECAY (6.2 M)                                  08NDS    200806
106CD  H TYP=FUL$AUT=D. DE FRENNE AND A. NEGRET$CIT=NDS 109, 943 (2008)$
106CD2 H CUT=1-May-2007$
106CD c  Experimental results are considered as incomplete by the evaluators
106CD2c  as the beta decay energy is very high (6526 keV 11)
106CD3c  A number of inconsistencies in the |e feeding of some levels are
106CD3c  observed. See also decay of other {+106}In isomer
106CD c  1992Ku01: source: {+106}Cd(p,n) E not given. Measured: E|g, I|g, ce(K)
106CD2c  deduced: {+106}Cd levels, J|p, |a(K)exp, mult
106CD c  1978Hu06: source: {+106}Cd(p,n) E=11,15 MeV. Measured: |g singles,
106CD2c  |g|g and |b|g |b singles. Deduced: {+106}Cd levels, J, |p, log| {Ift}
106CD c  1984Ro10: source {+106}In from Sn(p,2pxn), on-line mass separation.
106CD3c  Measured E|g, I|g, Ice, |g|g and |g(ce). Deduced: log| {Ift},
106CD4c  {+106}Cd levels, J, |p, |a, mult
106CD c  Others: 1972Me02, 1976Fl14, 1980Wi20
106CD c  Q(|e)=6531 {I16} keV calculated from 1984Fi05
106IN  P 0.0         7+                6.2 M     1              6526      11
106CD  N 0.997                 1.0
106CD cN           (|e+|b{++}) branching to low-lying (J|<5) states is unlikely
106CD CL BAND(D)   DJ=2 g.s. band
106CD cL E(B)      Observed only by 1984Ro10
106CD cL E(F)      Observed only by 1980Wi20
106CD CL E(E)      Only one deexciting |g observed by 1984Ro10
106CD cL J         From adopted levels
106CD cG E,RI      E|g with I|g values are from 1978Hu06,
106CD2cG unless otherwise noted.
106CD2cG E|g values for transitions with no I|g are from 1984Ro10. For I|g see
106CD3cG 1984Ro10, they are not given for {+106}In(5.2 min) and
106CD4cG {+106}In(6.2 min) |e decay separately. Unassigned |g's of 1984Ro10
106CD5cG given in both decays
106CD cG E(E),RI(E)$Taken from 1980Wi20. No |DI|g given by the authors.
106CD2cG Estimated by the evaluators to be 10%
106CD cG M         From 1984Ro10; based on conversion electron data
106CD  G 308.9     2
106CD  G 314.6     2
106CD  G 390.7     2
106CD  G 395.5     2
106CD  G 438.6     2
106CD  G 636.2     2
106CD  G 690.9     2
106CD  G 802.1     2
106CD  G 808.3     2                                                         C
106CD  G 1063.7    2
106CD  G 1076.9    2
106CD  G 1145      1 3.9     10
106CD  G 1173.7    2
106CD  G 1243.3    2
106CD  G 1298.8    2
106CD  G 1373.6    2
106CD  G 1505.9    2                                                         C
106CD  G 1518.6    2
106CD  G 1524.9    2
106CD  G 1550.5    2
106CD  G 1622.1    2
106CD  G 1633.2    2
106CD  G 1757.1    2
106CD  G 1896.4    2
106CD  G 2005.3    2                                                         C
106CD  G 2046.2    2                                                         C
106CD  G 2225.7    2                                                         C
106CD  G 2390.3    2                                                         C
106CD  G 2414.1    2                                                         C
106CD  G 2449.0    2                                                         C
106CD  G 2494.3    2                                                         C
106CD  G 2551.4    2
106CD  G 2586.2    2
106CD  L 0.0         0+                                                     D
106CD  L   632.60  102+                                                     D
106CD  E                 7   LT             7.0  GT             7         LT
106CDS E EAV=2247.1 53
106CD  G 632.6     1 100       E2                      0.0030                C
106CD  L  1493.71  134+                                                     D
106CD  E                10   6              6.5   3             10        6    ?
106CDS E EAV=1835.5 53
106CD cE           Very improbable that this level is directly fed in |e decay
106CD2cE because J|p({+106}In)=7+
106CD  G 861.1     1 90      5 E2                      0.0014                C
106CD cG RI        from 1976Fl14
106CD  L  2104.52  134+
106CD  E                1.1  7              7.1   3             1.1       7    ?
106CDS E EAV=1546.1 52
106CD cE           Very improbable that this level is directly fed in |e decay
106CD2cE because J|p({+106}In)=7+
106CD  G 610.7     2 3.6      3E2                      0.0035                C
106CD cG RI        from 1976Fl14
106CD  G 1471.9    1 6.6     5                                               C
106CD cG RI        weighted average of 3.0 {I12} (1978Hu06) and 7.2 {I5}
106CDxcG (1976Fl14)
106CD  L  2305.15  214+
106CD  E               0.87  14            7.07   7             0.87      14
106CDS E EAV=1451.7 52
106CD cE           Very improbable that this level is directly fed in |e decay
106CD2cE because J|p({+106}In)=7+
106CD  G 811.1     4 1.28    9 M1,E2
106CD cG RI        weighted average of 1.2 {I2} (1978Hu06) and 1.3 {I1}
106CDxcG (1976Fl14)
106CD  G 1672.6    3 0.19    3 E2
106CD  L  2330.26  165+
106CD  E                7.0  5             6.15   4             7.0       5    ?
106CDS E EAV=1439.9 52
106CD cE           If for {+106}In g.s. J|p=7+, then |b{+-} transition to
106CD2cE 2330-keV level is second forbidden and log| {Ift}=6.21 is too small.
106CD3cE However, because several of the transitions feeding this level have no
106CD4cE intensity given they easily could account for the feeding of the
106CD5cE 2330-keV level. Also a number of |g's deexciting unobserved levels fed
106CD6cE in |e decay could have been missed
106CD  G 225.7     2 6.9     3 M1+E2                   0.051  7              C
106CD3 G EKC=0.055 6 (1992KU01)$
106CD cG RI        weighted average of 7.0 {I4} (1978Hu06) and 6.7 {I5}
106CDxcG (1976Fl14)
106CD  G 836.7     4 2.8     2 M1,E2                                         C
106CD3 G EKC=0.0026 4 (1992KU01)$
106CD  L 2468.3    5 4+
106CD  G 974.6     4 1.6     1                                               C ?
106CD cG           Observed only by 1978Hu06.
106CD  L  2485.58  174+                                                     F
106CD  E                0.5  LT             7.2  GT             0.5       LT
106CDS E EAV=1367.0 52
106CD cE           Direct feeding of this level in |e decay highly improbable
106CD2cE because J|p({+106}In)=7+. Probably an important fraction of
106CD3cE the |e decay to higher lying levels is missed
106CD  G 992.1     2 1.50    15                                             E
106CD  G 1853.0    2 0.9     1                                              E
106CD  L  2491.72  146+                                                     D
106CD  E               10.6  20            5.87   9             10.6      20C
106CDS E EAV=1364.1 52
106CD cE           E(|b{++})=2.56 MeV {I20} (1978Hu06) |b(998|g). Other:
106CD2cE 2.7 MeV {I1} (1966Ca09) |b(860|g,990|g)
106CD  G 161.0     2 0.5     1                                              E
106CD  G 186.6     2 0.6     1
106CD  G 997.8     1 41.5    17                                              C
106CD cG RI        weighted average of 48 {I3} (1978Hu06) and 38.6 {I20}
106CDxcG (1976Fl14).
106CD  L  2502.92  156+
106CD  E                8.3  14            5.97   8             8.3       14C
106CDS E EAV=1358.9 52
106CD cE           E(|b{++})=2.59 MeV {I20} (1978Hu06) |b(1009|g)
106CD  G 1009.3    1 27.5    10                                              C
106CD cG RI        weighted average of 30.4 {I15} (1978Hu06) and 25.3 {I13}
106CDxcG (1976Fl14)
106CD  L  2629.02  195-
106CD  E               2.50  23            7.75   5             2.50      23C1U
106CDS E EAV=1309.5 51
106CD  G 524.6     2 1.9     2 E1                      0.0018               E
106CD  G 1135.2    2 0.6     1
106CD cG E,RI      from 1980Wi20
106CD  L  2920.22  245                                                      B
106CD  G 1426.5    2                                                         C
106CD  L  2924.67  20 6+
106CD  E                3.5  4             6.05   5             3.5       4 C
106CDS E EAV=1162.2 51
106CD  G 433.1     2 2.3     3 E2                      0.0093               EC
106CD  G 820.3     2                                                         C ?
106CD cG E         observed only by 1984Ro10
106CD  G 1430.8    2 1.2     2                                              EC
106CD  L  3043.91  178+
106CD  E               39.8  11 0.002568   4.901 17             39.8      11
106CDS E EAV=1106.9 51$CK=6.42E-5 9$
106CD  G 541.0     3 12.5    5                                               C
106CD cG RI        weighted average of 12.7 {I7} (1978Hu06) and 12.4 {I6}
106CDxcG (1976Fl14)
106CD  G 552.4     2 25.2    9                                               C
106CD cG RI        weighted average of 25.8 {I13} (1978Hu06) and 24.7 {I13}
106CDxcG (1976Fl14)
106CD  G 558.6     2 2.2     2                                              E
106CD  L  3084.03  237+
106CD  E                6.2  4             5.68   3             6.2       4
106CDS E EAV=1088.4 51
106CD  G 580.7     5 0.7     1                                               C
106CD  G 592.1     4 3.0     3                                               C
106CD  G 753.3     4 2.5     2                                               C
106CD  L  3126.03  187+
106CD  E               2.80  23            5.99   4             2.80      23
106CDS E EAV=1069.0 51
106CD  G 623.2     2 1.8     2 M1+E2                   0.0039               EC
106CD  G 634.1     2 1.0     1                                              EC
106CD  L  3283.93  20 +                                                     B  ?
106CD  G 780.7     2           E2                      0.0016                C
106CD  G 792.5     2                                                         C
106CD  L   3357.7   3                                                       B  ?
106CD  G 1027.4    2                                                         C
106CD  L  3366.97  208+                                                     B
106CD  G 282.7     2                                                         C
106CD  G 875.2     2           E2                      0.0015                C
106CD  L  3472.71  18                                                       B
106CD  G 980.8     2                                                         C
106CD cG E         different placement given by 1978Hu06
106CD  G 1142.7    2                                                         C
106CD  G 1978.9    2                                                         C
106CD  L  3547.44  18 +                                                     B
106CD  G 421.3     2           E2                      0.015                 C
106CD  G 1217.5    2                                                         C
106CD  G 1442.7    2                                                         C
106CD  L  3641.93  17(8+)
106CD  E                2.7  7             5.53  12             2.7       7
106CDS E EAV=832.3 50
106CD  G 1139.0    2 2.7     7 (M1)                    0.0008               EC
106CD cG E,RI      from 1978Hu06
106CD cG M$From level scheme Mult=Q
106CD  G 1149.4    2                                                         C
106CD  G 2148.8    2                                                         C
106CD  L  3787.33  20                                                       B
106CD  G 1284.6    2                                                         C
106CD  G 1295.4    2                                                         C
106CD  L  4243.51  20+                                                      B  ?
106CD  G 601.4     2           M1                      0.0043                C
106CD  G 1199.7    2                                                         C
106CD  L  4282.59  20                                                       F  ?
106CD  E               1.89  20 0.0011112  4.88   5             1.89      20
106CDS E EAV=544.1 49$CK=0.000590 18$
106CD  G 1780.1    2 1.5     2                                              E
106CD  G 1790.4    2 0.40    4                                              E
106CD  L   4398.6   3                                                       B  ?
106CDF L FLAG=E
106CD  G 1031.6    2                                                         C
106CD  L  5130.67  19                                                       B
106CD  G 887.1     2                                                         C
106CD  G 1488.7    2                                                         C
106CD  G 1763.4    2                                                         C
106CD  G 2087.1    2                                                         C