92MO    92TC EC DECAY                 1985BE12,1976DE07,1968KOZY12NDS    201210
 92MO  H TYP=FUL$AUT=CORAL M. BAGLIN$CIT=NDS 113, 2187 (2012)$CUT=15-Sep-2012$
 92MO DG CC$ FROM BrIcc v2.2b (20-Jan-2009) 2008Ki07, "Frozen Orbitals" appr.
 92MO c  Others: 1964Lo02, 1964Va05, 1966Di01, 1971Co08, 1973Gi04, 1974Ia01.
 92MO c  The decay scheme for E(level)<2800 keV is based on that
 92MO2c  of 1964Va05. It incorporates |g|g-coin data of 1964Va05
 92MO3c  (148,329,773,1510 |g rays in prompt coin) and accounts for all known
 92MO4c  lines with I|g|>2%. No significant |e+|b{++} branch to the 2612-keV 6+
 92MO5c  level of {+92}Mo is indicated (I(|e+|b{++})=3% {I6}, log| {Ift}|>6.5),
 92MO5c  whereas the 2760-keV 8+ state of {+92}Mo is strongly fed
 92MO6c  (I(|e+|b{++})=89% {I6}, log| {Ift}=5.4), so J|p({+92}Tc g.s.) is
 92MO7c  probably not 7+. |b{++} feeding to some level(s) other than the 190-ns
 92MO8c  8+ level must occur because 1985Be12 observe |g{+|+} in prompt coin
 92MO9c  with 773|g and 1509|g. Also, a number of weak |g's have been assigned
 92MOAc  to {+92}Tc by 1968KoZY, 1976De07 (fig 1) and 1985Be12. 1968KoZY
 92MOBc  propose several levels with E>2800 keV on the basis of pairs of weak
 92MOCc  |g rays whose energy difference matches a known level-energy
 92MODc  difference but, in the absence of coin data, the evaluator has
 92MOEc  retained only those levels deexcited by pairs of |g rays whose E|g
 92MOFc  and I|g are confirmed by the data of 1985Be12. Total unplaced I|g=5%.
 92MO cE IB        1964Va05 deduce I(|b{++})=92% {I12} from
 92MO2cE I(|g{+|+})/I(1509|g).
 92MO cE E(D)      From 1964Va05. Other: 4100 {I200} (1974Ia01).
 92MO cG           1968KoZY report, but 1985Be12 do not confirm, |g rays with
 92MO2cG the following E|g: 1337.1 {I13}, 1596.0 {I10}, 1785.9 {I13}, 2511.5
 92MO3cG {I13}, 3134.3 {I15}, 4085.5 {I15}, 4135.9 {I15}, and 2873.4 {I15},
 92MO4cG 3911.9 {I15}, 4037.6 {I22}, 4577.3 {I15}; 1985Be12 report I|g|<0.02
 92MO5cG for the latter four |g rays. The evaluator considers assignment of
 92MO6cG these lines to {+92}Tc |e+|b{++} decay to be doubtful.
 92MO cG E         E(85|g) from 1968KoZY. Other E|g from 1985Be12 (|DE=0.3-0.6
 92MO2cG keV), unless indicated otherwise; evaluator assigns |DE=0.3 keV for
 92MO3cG strongest three |g rays. Except for the 1590.9|g, 2516.8|g and
 92MO4cG 2645.2|g, all lines with E|g<3200 reported in 1985Be12 are confirmed
 92MO5cG in spectrum of fig. 1 from 1976De07.
 92MO cG RI        From 1985Be12, unless noted otherwise. Relative to
 92MO2cG I(773|g)=100
 92MO cG M,MR      From Adopted Gammas.
 92MO cG RI(A)     Weighted average of data from 1976De07 and 1985Be12.
 92MO cG RI(F)     From 1976De07. Datum from 1968KoZY inconsistent.
 92MO cL J         From Adopted Levels.
 92MO cL T(C)      From weighted average of 1.51 ns {I8} (1973Gi04) and 1.54 ns
 92MO2cL {I5} (1971Co08) from 330|g-148|g(t). Other: 1.50 ns {I15} (1968KoZY)
 92MO3cL from |b|g(t).
 92MO cL T(B)      From (E|b>300)-773|g(t) data of 1964Lo02. Other: >50 ns,
 92MO2cL from 1964Va05.
 92TC  P 0.0          (8)+             4.25 M    15               7885     5
 92MO  N 0.99857               1.0       1.0
 92MO cN NR        no g.s. or 1510 level feeding by |e+|b{++} and no crossover
 92MO2cN |g to g.s. or 1510 level, so I(|g+ce)(773|g)=100%.
 92MO PN                                                                     3
 92MO  G 1567.9     60.20     5
 92MO  G 1590.9     60.24     5
 92MO  G 1702.2     60.19     5
 92MO  G 2516.8     60.10     3
 92MO  G 2645.2     60.3      2
 92MO  G 2881.0     60.07     3
 92MO  G 2899.5     60.16     3
 92MO  G 3023.4     60.54     6
 92MO  G 3128.5     60.48     6
 92MO  G 3218.0     60.12     2
 92MO  G 4028.0     60.17     2
 92MO  G 4370.1     60.07     2
 92MO  L      0.0     0+
 92MO  L   1509.6   3 2+
 92MO  G 1509.6    3 101     3  E2                                           C
 92MOS G CC=0.000408 6$KC=0.000284 4$LC=3.15E-5 5$MC=5.62E-6 8$NC+=8.78E-5 13
 92MOS G NC=8.56E-7 12$OC=4.88E-8 7$IPC=8.69E-5 13
 92MO cG           I(|g+ce)(1510|g)=100% from level scheme.
 92MO  L   2282.6   5 4+
 92MO  G 773.0     3 100        E2                                           C
 92MOS G CC=0.001434 21$KC=0.001259 18$LC=0.0001452 21$MC=2.59E-5 4$NC+=4.14E-6
 92MOS G NC=3.92E-6 6$OC=2.15E-7 3
 92MO  L   2526.6   6 5-
 92MO  G 243.7     6 13.3    5 (E1(+M2)) 0.05    LT                         A
 92MOS G CC=0.00987 21$KC=0.00869 18$LC=0.000985 22$MC=0.000175 4$NC+=2.79E-5 7
 92MOS G NC=2.65E-5 6$OC=1.43E-6 4
 92MO  L   2611.8   5 6+               1.53 NS   4                          C
 92MO  G 85.0      5 12.1    8 (E1)                    0.202  5             F
 92MOS G KC=0.177 4$LC=0.0207 5$MC=0.00366 9$NC+=0.000571 13
 92MOS G NC=0.000544 13$OC=2.67E-5 6
 92MO  G 329.3     3 79.9    26E2                      0.0177               AC
 92MOS G KC=0.01535 22$LC=0.00195 3$MC=0.000348 5$NC+=5.43E-5 8
 92MOS G NC=5.18E-5 8$OC=2.51E-6 4
 92MO  L   2760.0   7 8+               192 NS    7                          B
 92MO  E 4.1E3     1    87   6    3.4  2   5.43   4                   90   6D
 92MOS E EAV=1880.8 25$CK=0.03330 12$CL=0.004008 15$CM+=0.000921 4
 92MO  G 148.0     6 71      4 E2                      0.292  6             AC
 92MOS G KC=0.245 5$LC=0.0386 9$MC=0.00696 15$NC+=0.001039 22
 92MOS G NC=0.001002 22$OC=3.70E-5 8
 92MO  L   4917.4   7 7+
 92MO  E               1.53  9   0.59  4   5.72   3                 2.12  13
 92MOS E EAV=866.6 24$CK=0.2402 14$CL=0.02906 18$CM+=0.00668 4
 92MO  G 2157.0     6 1.2    1
 92MO  G 2305.8     6 0.92   8
 92MO  L   5462.3   7 (7,8)+
 92MO  E               0.40  5   0.44  5   5.67   6                 0.84  10
 92MOS E EAV=619.3 23$CK=0.452 3$CL=0.0548 3$CM+=0.01260 7
 92MO  G 2702.4     6 0.44    7
 92MO  G 2850.3     6 0.40    7