232U 236PU A DECAY 1994AR08 06NDS 200610 232U H TYP=FUL$AUT=E. BROWNE$CIT=NDS 107, 2579 (2006)$CUT=1-Nov-2004$ 232U C 236PU source produced by 238U(P,3N)236NP(22.5 H), which decays to 232U 2C 236PU. Chemical separation of plutonium. Measured EG, RI, GG COIN 232U 3C using Germanium detectors. Others: 1956Hu96, 1963Le17. 232U CA E(X),IA(X)$Values recommended in 1991Ry01. Others: 1976BaZZ, 232U 2CA 1979Ry01, 1984Ry02. 232U CG M$From Adopted Gammas 232U CG RI$RI are per 100 decays of 236PU. Relative experimental values 232U 2CG normalized to an absolute scale from a decay scheme G-ray transition 232U 3CG intensity balance using IA(GS)=69.1 % 3 (1994Ar08). 232U CL BAND(A) KPI=0+ GS rotational band 232U CL BAND(B) KPI=0- Octupole vibrational band 232U CL BAND(D) KPI=0+ Beta vibrational band 232U CL BAND(E) KPI=2+ Gamma vibrational band 232U CL BAND(J) KPI=(0+) Two-phonon octupole vibrational band 236PU P 0.0 0+ 2.858 Y 8 5867.07 8 232U N 1.0 1.0 1.0 232U PN 3 232U G 927.69 20 3.6E-7 4 232U L 0.0 0+ A 232U A 5767.53 8 69.1 3 1.0 X 232U L 47.58 2 2+ 254 PS 20 A 232U CL T$delayed coincidence measurement (1960Be25) 232U A 5720.87 10 30.8 3 1.3 X 232U G 47.57 2 0.065 E2 468 232U 2 G LC=342$MC=94 232U L 156.54 3 4+ A 232U A 5613.7 0.23 44 232U G 108.95 2 0.0225 E2 9.2 232U 2 G LC=6.62$MC=1.84$NC+=0.692 232U L 322.65 6 6+ A 232U A 5450.4 1.85E-3 639 232U G 166.09 5 7.35E-4 2 E2 1.56 232U 2 G KC=0.204$LC=0.99$MC=0.273$NC+=0.101 232U L 540.7 1 8+ A 232U A 5236.1 1.3E-5 24690 232U G 218.0 1 8.4E-6 1 E2 0.558 232U 2 G KC=0.136$LC=0.307$MC=0.084$NC+=0.0312 232U L 563.2 2 1- B 232U A 5214.0 2.6E-4 1171 232U G 515.58 2 1.63E-4 5 E1 0.0127 232U 2 G KC=0.0103$LC=0.00185 232U G 563.19 2 1.14E-4 4 E1 0.0107 232U 2 G KC=0.0087$LC=0.00155 232U L 629.0 1 3- B 232U CL No alpha particle group feeds this level (IA < 1E-6 %). 232U G 472.34 10 2.5E-6 2 E1 0.0152 232U 2 G KC=0.0122$LC=0.00222$MC=0.00053$NC+=0.00019 232U G 581.41 10 4.1E-6 2 E1 0.0101 232U 2 G KC=0.00817$LC=0.00145 232U L 691.45 4 0+ D 232U A 5087.9 5.8E-4 1012 232U G 643.87 3 2.25E-4 9 [E2] 0.0270 232U 2 G KC=0.0184$LC=0.00650 232U G 691.3 1 E0 3.5E-4 10 ? 232U CG TI$From 1963Le17 232U L 734.56 6 2+ D 232U A 5045.5 1.3E-5 1286 232U G 577.95 10 1.2E-6 2 [E2] 0.0342 232U 2 G KC=0.0224$LC=0.0089 232U G 687.04 10 2.3E-6 1 E0+E2 6.8E-6 20 232U G 734.55 10 3.08E-613[E2] 0.0206 232U 2 G KC=0.0146$LC=0.00452 232U L 746.8 1 5- B 232U A 5033.5 2.46E-6 1260 232U G 423.85 20 6.3E-7 1 [E1] 0.0189 232U 2 G KC=0.0152$LC=0.00280$MC=0.00067$NC+=0.00024 232U G 590.28 10 1.8E-6 1 [E1] 0.0098 232U 2 G KC=0.00795$LC=0.00141 232U L 833.5 2 4+ D 232U A 4948.2 6E-7 1400 232U CA IA$Assuming an E0 intensity of (3.2E-7 9 %) for the 677-keV G ray, 232U 2CA and a total photon intensity of AP 2.7E-7 % for the sum of all the 232U 3CA G rays that de-excite the 833-keV level (1994Ar08). 232U G 677.0 2 9.5E-8 4 [E0]+E2 232U L 866.9 1 2+ E 232U A 4915.4 1.21E-5 641 232U G 710.1 3 3.2E-7 1 E2 0.0221 232U 2 G KC=0.0155$LC=0.00495 232U G 819.27 10 6.0E-6 2 E2 0.0166 232U 2 G KC=0.0121$LC=0.00340 232U G 866.88 10 4.9E-6 3 E2 0.0148 232U 2 G KC=0.0109$LC=0.00295 232U L 927.3 1 (0+) J 232U A 4856.0 1.33E-5 15 232U G 364.0 1 1.09E-5 15 [E1] 0.0260 232U 2 G KC=0.0208$LC=0.00392$MC=0.00094$NC+=0.00033 232U G 879.9 1 2.1E-6 1 [E2] 0.0144 232U 2 G KC=0.0106$LC=0.00284 232U L 967.6 1 (2+) J 232U A 4816.4 1.53E-5 6.7 232U G 338.5 1 7.2E-6 1 [E1] 0.0304 232U 2 G KC=0.0243$LC=0.00462$MC=0.00110$NC+=0.00039 232U G 404.46 10 5.5E-6 1 [E1] 0.0209 232U 2 G KC=0.0168$LC=0.00310$MC=0.00074$NC+=0.00026 232U G 811.26 20 9.4E-7 1 [E2] 0.0169 232U 2 G KC=0.0123$LC=0.00348 232U G 920.23 20 9.6E-7 1 M1+E2 1.14 20 0.030 4 232U 2 G KC=0.024 3$LC=0.0049 6 232U G 967.9 3 3.5E-7 8 [E2] 0.0120 232U 2 G KC=0.0090$LC=0.00226