136CE    136CE IT DECAY (1.9 US)       1991MU07,2013VA10         NDS18    201810
136CE  H TYP=FUL$AUT=E.A. MCCUTCHAN$CIT=NDS 152, 331 (2018)$CUT=1-Apr-2018$
136CE c  1991Mu07: {+9}Be({+132}Xe,5n) with E({+136}Ce)=6.3 MeV/nucleon
136CE2c  followed by recoil ion separation using gas filled GARIS. Measured
136CE3c  E|g, I|g using four Ge detectors.
136CE c  2013Va10: {+96}Zr({+48}Ca,|a4n|g) with E({+48}Ca)=180 MeV. Measured
136CE2c  recoil-|g coincidences, |g(t) using RITU gas-filled separator,
136CE3c  JUROGAM array consisting of 39 Compton-suppressed HPGe detectors, and
136CE4c  GREAT spectrometer.
136CE c  Others: 1975Yo01, 1978Mu09, 1980Ba68, 1982Ri09, 1983Da29
136CE cL E$From a least-squares fit to E|g, by evaluator.
136CE cL J$From the Adopted Levels.
136CE cG E,RI$From 1991Mu07, except where noted.
136CE cG M$From the Adopted Levels.
136CE  P 3095.0       10+               1.9 US    1
136CE  N 1.0          1.0       1.0
136CE cN NR$From |SI(|g+ce)=100. As 1991Mu07 do not provide uncertainties on
136CE2cN transition intensities, these values should be considered approximate.
136CE PN                                                                     3
136CE  L 0.0          0+
136CE  L 552.1        2+
136CE  G 552.1        100       E2                     0.00827
136CES G KC=0.00693 10$LC=0.001055 15$MC=0.000223 4$NC=4.90E-5 7$OC=7.72E-6 11$
136CES G PC=4.91E-7 7
136CE  L 1314.4       4+
136CE  G 762.3        100       E2                     0.00371
136CES G KC=0.00315 5$LC=0.000443 7$MC=9.29E-5 13$NC=2.05E-5 3$OC=3.27E-6 5$
136CES G PC=2.27E-7 4
136CE  L 1978.6       5-
136CE  G 664.2        1.9       E1                     0.00192
136CES G KC=0.001652 24$LC=0.000209 3$MC=4.33E-5 6$NC=9.59E-6 14$
136CES G OC=1.550E-6 22$PC=1.165E-7 17
136CE  L 2214.4       6+
136CE  G 900.0        37        E2                     0.00254
136CES G KC=0.00217 3$LC=0.000295 5$MC=6.18E-5 9$NC=1.366E-5 20$OC=2.19E-6 3$
136CES G PC=1.567E-7 22
136CE  L 2307.1       7-
136CE  G 328.5        1.6       E2                      0.0367
136CES G KC=0.0297 5$LC=0.00549 8$MC=0.001178 17$NC=0.000257 4$OC=3.93E-5 6$
136CES G PC=1.99E-6 3
136CE  L 2366.8       6+
136CE  G 1052.4       63        E2                     0.00181
136CES G KC=0.001548 22$LC=0.000206 3$MC=4.31E-5 6$NC=9.53E-6 14$
136CES G OC=1.534E-6 22$PC=1.124E-7 16
136CE  L 2990.1       8+
136CE  G 623.3        63        E2                     0.00605
136CES G KC=0.00510 8$LC=0.000751 11$MC=0.0001582 23$NC=3.48E-5 5$OC=5.52E-6 8$
136CES G PC=3.64E-7 5
136CE  G 683.1        1.2       [E1]                   0.00181
136CES G KC=0.001557 22$LC=0.000197 3$MC=4.08E-5 6$NC=9.03E-6 13$
136CES G OC=1.460E-6 21$PC=1.099E-7 16
136CE  G 775.7        37        E2                     0.00356
136CES G KC=0.00302 5$LC=0.000424 6$MC=8.89E-5 13$NC=1.96E-5 3$OC=3.13E-6 5$
136CES G PC=2.18E-7 3
136CE  L 3095.0       10+               1.9 US    1
136CE2 L G=-0.180 2 (1981BA69)
136CE cL T$weighted average of 552|g(t), 623|g(t), 762|g(t), and 1052|g(t)
136CE2cL (2013Va10); |g(t) for each transition fit with exponential decay
136CE3cL curve after background subtraction. Other: 2.2 |ms {I2} from |g(t) in
136CE4cL 1975Yo01.
136CE cL G$from TDPAD. Other: 0.180 {I3} (1982Ri09, TDPAD).
136CE cL MOME2$Q/Q(10+, {+138}Ce)=1.45 {I4} (1983Da29, TDPAD).
136CE  G 104.9        36.6      E2                      1.730    100
136CES G KC=1.054 15$LC=0.529 8$MC=0.1179 4$OC=0.00358 5
136CE cG RI$deduced by evaluator from I(|g+ce)=100 from intensity balance and
136CE2cG |a.