121I     121XE EC DECAY                1972MU03,1971HO02         10NDS    201006
121I   H TYP=FUL$AUT=S. OHYA$CIT=NDS 111, 1619 (2010)$CUT=20-Jan-2009$
121I  c  1972Mu03: Ce(p,5pxn) E=600 MeV, on-line mass separation, semi |g, |g|g,
121I 2c  semi and magnetic spectrometer ce (1972Mu03)
121I  c  1971Ho02: |g|g(t), |gce(t)
121I  c  The decay scheme is that proposed by 1972Mu03
121I  c  Others: 1969Bu07, 1971ShZY {+120}Te(|a,3n) E=40 MeV, semi |g
121I  c  The |g placements in the present decay scheme are
121I 2c  inconsistent with the J|p=(9/2)+ assignment of 433.6, 529.2, and 649.7
121I 3c  levels deduced from {+121}Sb({+3}He,3n|g) data. The evaluators noted
121I 4c  that inconsistencies of several |b feedings with low log| {Ift} values
121I 5c  (7.0-7.5) can be reduced by placing several gammas from higher
121I 6c  lying levels with consistent energies
121I  cL E         E(levels) are based on a least-squares fit to
121I 2cL E(|g's) from 1972Mu03
121I  cL J         From adopted levels
121I  cL T$T{-1/2} are from |g|g(t) (1970Sc21) and |g-ce(t) (1971Ho02), unless
121I 2cL noted otherwise
121I  cG E$From 1972Mu03
121I  cG RI$From 1972Mu03. I|g are relative to I(252.7|g)=100
121I  cG M,MR $From |a(K)exp, |a(L)exp, unless noted otherwise;
121I 2cG multipolarities of the following |g's were assumed to deduce |a:
121I 4cG [M1]: 77.0|g; and [E2]: 192.6|g, 214.6|g
121I  cG RI(B)$Transition intensities of multiply placed gammas and doublet
121I 2cG shown in their decay scheme by 1972Mu03 were estimated from
121I 3cG |g|g-coincidence (1972Mu03)
121I  cG E(A)      Possible doublet
121I  cE LOGFT(B),TI(B)$The evaluator noted that inconsistency of |b feedings
121I 2cE with low log| {Ift} value can be reduced by of several
121I 3cE gammas from higher lying levels with consistent energies
121XE  P 0.0          5/2(+)           40.1 M    20             3776      12
121I   N 0.126     121.0       1.0       1.00    10
121I  cN NR        from sum I(|g+ce) to g.s.=72% {I9}.
121I  PN                                                                     3
121I   G 72.6      3 1.2     2
121I   G 743.2     3 0.7     1
121I   G 860.7     5 1.2     2
121I   G 899.3     5 0.4     1
121I   G 978.7     5 0.9     2
121I   G 1096.3    5 1.0     3
121I   G 1128.1    4 1.3     2
121I   G 1273.3    4 1.2     2
121I   G 1306.8    4 1.0     2
121I   G 1358.4    4 1.4     2
121I   G 1566.0    5 1.3     3
121I   G 1695.5    5 0.6     2
121I   G 1710.2    4 1.7     3
121I   G 1740.4    4 1.8     3
121I   G 2265.7    4 0.8     2
121I   G 2302.7    5 0.7     2
121I   G 2365.8    6 0.7     2
121I   G 2434.2    6 1.1     3
121I   G 2495.7    6 0.6     2
121I   G 2607.6    6 0.50    15
121I   G 2718.3    6 1.1     3
121I   G 2763.2    6 0.5     2
121I   G 2926.6    5 0.50    15
121I   G 2950.8    6 0.40    15
121I   G 2996.6    6 0.3     1
121I   G 3052.1    5 0.6     2
121I   G 3126.4    5 0.50    15
121I   L 0.0         5/2+              2.12 H    1
121I  cL T         from adopted levels
121I   E                20   6    7.7  22  6.21  14             28        8
121I S E EAV=1244.7 56$CK=0.2367 23$CL=0.0313 3$CM+=0.00835 8
121I   L      95.71101/2+              8.3 NS    4
121I  cL T         from (80|g + |g{+|+} + 843|g)(96|g)(t) (1970Sc21)
121I   E               0.91  LE  0.39  LE   7.5  GE             1.3       LE
121I S E EAV=1200.3 56$CK=0.2555 25$CL=0.0338 4$CM+=0.00902 9
121I   G 95.7      2 36      3 E2                      2.05   4              C
121I S G KC=1.372 22$LC=0.540 9$MC=0.1143 20$NC+=0.0241 4
121I S G NC=0.0220 4$OC=0.00205 4
121I  cG M         from |a(K)exp=1.40 {I15}, |a(L)exp=0.56 {I7}, |a(M)exp=0.17
121I xcG {I5}
121I   L     132.8710 7/2+             0.35 NS   2
121I  cL T         from (600