232U 232NP EC DECAY 1972WE16 06NDS 200610
232U H TYP=FUL$AUT=E. BROWNE$CIT=NDS 107, 2579 (2006)$CUT=1-Nov-2004$
232U CE %|b{++}<0.1% from |g{+|+} (1972We16)
232U CE TI$Deduced by evaluator from decay-scheme transition intensity balance
232U 2CE at each level.
232U CG From 1972We16. Other: 1970Ho27
232U CG E Comparison with {+232}Pa |b{+-} decay suggests that all
232U 2CG E|g's in 1972We16 are |?1 keV too high.
232U CG K| x ray=57.8% of intensity of all observed |g's (1970Ho27)
232U CG M From adopted gammas
232U CL E$Deduced by evaluator from a least-squares fit to G-ray energies.
232U CL BAND(A) KPI=0+ GS rotational band
232U CL BAND(E) KPI=2+ G vibrational band
232U CL BAND(G) KPI=2-
232U CL BAND(H) KPI=2+
232U CL BAND(I) KPI=(1-)
232NP P 0 (4+) 14.7 M 3 2750 99
232U N 0.53 2 1.0 1.0
232U CN NR$Deduced by evaluator from sum of G-ray transition intensities
232U 2CN to GS = 99.5 % 5.
232U PN 3
232U G 377.0 3 2.4 2
232U G 1016.8 4 1.1 1
232U L 0 0+ A
232U E 0.01 1 1 LT 8.0 1 LT ?
232U 2 E EAV=790 43 $CK=0.757 4 $CL=0.1601 12 $CM+=0.0556 5
232U CE I|e<1% to g.s. band of {+232}U, based on K| x ray of
232U 2CE 1972We16 and |a(K).
232U L 47.57 2 2+ A
232U G 47.57 2 E2 460 S
232U CG E$From Adopted Gammas
232U 2 G LC= 339 $MC= 93.6 $
232U L 156.52 3 4+ A
232U G 108.95 2 E2 9.1 S
232U CG E$From Adopted Gammas
232U 2 G LC= 6.62 $MC= 1.838 $NC+= 0.692 $
232U L 321.5 5 6+ A
232U G 165.0 5 0.6 2 E2 1.60
232U 2 G KC= 0.2054 $LC= 1.015 $MC= 0.281 $NC+= 0.1044 $
232U L 867.1 2 2+ E
232U G 710.7 6 1.1 2 [E2]
232U G 819.5 4 64 3 E2 0.017
232U 2 G KC=0.01205 $LC=0.00340 $
232U G 867.2 6 47 3 E2 0.015
232U 2 G KC=0.01091 $LC=0.00295 $
232U L 911.9 3 3+ E
232U G 755.0 4 8.1 6 [M1+E2]
232U G 864.3 5 39 2 E2 0.014
232U 2 G KC=0.01097 $LC=0.00297 $
232U L 971.3 2 (4+) E
232U E 0.0027 18 1.7 5 7.1 1.7 5 ?
232U 2 E EAV=367 44 $CK=0.7698 $CL=0.1694 10 $CM+=0.0592 4
232U G 814.8 4 7.9 6 [M1+E2]
232U G 924.4 4 1.8 2 [E2]
232U L 1017.9 2 2- G
232U G 970.9 3 0.6 1 [E1]
232U 2 G FL=47.57
232U G 1016.8 4
232U cG RI$from {+232}Pa |b{+-} decay I|g(970.9)/I|g(1016.8)=3000
232U L 1051.2 4 3- G
232U G 895.1 5 1.6 2 [E1]
232U L 1098.1 4 4- G
232U E 0.0012 10 1.6 3 7.0 1.6 3 ?
232U 2 E EAV=311 45 $CK=0.7688 12 $CL=0.1707 11 $CM+=0.0597 5
232U G 941.6 4 3.1 5 [E1]
232U L 1133.0 3 (2+) H
232U E 0.0012 10 1.9 1 6.9 1.9 1 ?
232U 2 E EAV=295 45 $CK=0.7684 13 $CL=0.1711 12 $CM+=0.0599 5
232U G 1085.4 4 1.9 1
232U G 1133.1 4 1.7 2
232U L 1146.3 10 (1-) I
232U G 1146.3 0.7 1 & ?
232U L 1173.6 4 (2)- I
232U E 1.5 2 7.0 1.5 2
232U 2 E CK=0.7679 15 $CL=0.1715 12 $CM+=0.0601 5
232U G 1126.0 4 2.8 3 [E1]
232U L 1194.3 2 (3+,4+)
232U E 0.04 4 94 4 5.2 94 4
232U 2 E EAV=268 46 $CK=0.7676 15 $CL=0.1718 13 $CM+=0.0602 6
232U G 143.4 5 0.8 2 [E1] .22
232U 2 G KC= 0.1686 $LC= 0.0373 $MC=0.00908 $NC+=0.00321 $
232U G 223.6 4 4.3 3 [E2] .51
232U 2 G KC= 0.1302 $LC= 0.276 $MC= 0.0756 $NC+= 0.0280 $
232U G 282.0 4 38 2 [E2] 0.23
232U 2 G KC= 0.0855 $LC= 0.1079 $MC= 0.0292 $NC+=0.01086 $
232U DG Only E1 or E2 are allowed by intensity balance
232U G 327.3 3 100 [E2] 0.148
232U 2 G KC= 0.0646 $LC= 0.0608 $MC=0.01636 $NC+=0.00608 $
232U DG Only E1 or E2 are allowed by intensity balance
232U G 1037.4 5 6.3 4
232U G 1146.3 5 0.7 1 & ?
232U G 1193.9 6 0.7 2 ?
232U L 1983.6 5 ?
232U E 0.42 5 6.9 0.42 6 ?
232U 2 E CK=0.740 9 $CL=0.191 7 $CM+=0.068 3
232U G 1936.0 5 0.8 1 ?