236PA    236TH B- DECAY                1984MI02                  22NDS    202205
236PA  H TYP=FUL$AUT=Shaofei Zhu$CIT=NDS 182, 2 (2022).$CUT=1-Apr-2022$
236PA c  The decay scheme of 1984Mi02 supersedes the scheme of 1973Or06
236PA2c  because of the observation of more complete |g rays in cascades.
236PA c  1984Mi02: {+236}Th decay was assigned based on the correlation of
236PA2c  {+236}Pa daughter decay in equilibrium from {+236}Th sources produced
236PA3c  by {+238}U(p,3p) followed by chemical and mass separation
236PA c  1973Or06: {+236}Th sources produced by {+238}U(p,3p)
236PA c  Other: 1973Ka10.
236PA c  x-ray: I|g(Pa K| x ray)/I|g(642|g)=0.32 {I8} from an equilibrium
236PA2c  source gives I|g(Pa K| x ray)=(0.32 {I8}) x 0.37 {I2} x 100=12% {I4}
236PA3c  (per 100 |b{+-} decays of {+236}Pa) (1973Or06).
236PA cG E,RI$From 1984Mi02, unless otherwise noted. Absolute intensity from
236PA2cG 1984Mi02 relative to I|g(642|g) in {+236}Pa at equilibrium, corrected
236PA3cG by parent/daughter ratio of 0.76 based on their lifetimes.
236PA cG M$From I(K| x ray)/I|g suggesting that most of the intense |g rays
236PA2cG with E|g>112.6 keV (the K-shell binding energy in Pa) should be M1
236PA3cG (1984Mi02).
236PA cL E$From least square fit to E|g's by evaluator.
236PA cL J$From adopted levels.
236PA D  CC$FROM BrIcc v2.3e (17-Jun-2020) 2008Ki07, "Frozen Orbitals" appr.
236TH  P 0            0+                37.5 M    2              921      20
236TH cP QP$from 2021Wa16.
236PA  N 1.00                   1.0
236PA cN NR$1984Mi02 provide absolute intensities noting "The gamma-ray
236PA2cN intensities of the parent 37-min {+236}Th were also put on an
236PA3cN absolute basis through measurements in sources in which parent
236PA4cN and daughter were in equilibrium; proper account was taken of
236PA5cN the parent/daughter ratio (0.76)."
236PA  G 131.6     10 0.56   28
236PA cG E$from 1973Or06.
236PA cG RI$from 2.0 {I10} relative to I|g(642|g)=100 (1973Or06).
236PA  G 392.4     1  0.17   3
236PA  G 414.8     3  0.13   3
236PA  G 434.3     1  0.67   9
236PA  G 586.4     2  0.09   4
236PA  G 599.7     1  0.24   3
236PA  G 719.9     1  0.21   3
236PA  L 0            1(+)              9.1 M     1
236PA  B             94.5    12          5.6     1
236PAS B EAV=293.2 74
236PA cB IB$|b{+-} intensity to g.s. + 31.5-keV level.
236PA  L 31.54     9
236PA  G 31.5                                                                  S
236PA cG E$not observed, deduced from level scheme (1984Mi02).
236PA  L 110.76    8  (0-,1)
236PA  G 110.8     1  4.2    12
236PA cG E$from 1984Mi02; other: 110.7 {I5} (1973Or06).
236PA cG RI$from 1984Mi02; other: 10.5 {I28} relative to I|g(642|g)=100
236PA2cG (1973Or06).
236PA  B             2.0     17          7.1     3
236PAS B EAV=253.1 72
236PA  L 227.42    20
236PA  G 196.0     5  0.69   14 (M1)                    3.01  5
236PAS G KC=2.40 4$LC=0.461 7$MC=0.1111 18$NC=0.0298 5$OC=0.00715 11$
236PAS G PC=0.001366 22$QC=0.0001128 18
236PA cG E,RI$from 1984Mi02.
236PA  B             2.5     6           6.8     2
236PA  L 340.20    7  (0-,1)
236PA  G 112.8     2  0.24   9
236PA cG E$from 1984Mi02; other: 112.7 {I+5-1} (1973Or06).
236PA cG RI$from 1984Mi02; other: 2.6 {I12} relative to I|g(642|g)=100
236PA2cG (1973Or06).
236PA  G 229.5     1  0.7    4  (M1)                    1.935 27
236PAS G KC=1.543 22$LC=0.296 4$MC=0.0712 10$NC=0.01910 27$OC=0.00458 6$
236PAS G PC=0.000875 12$QC=7.23E-5 10
236PA cG E$from 1984Mi02; other: 229.6 {I10} (1973Or06).
236PA cG RI$from 1984Mi02; other: 2.0 {I10} relative to I|g(642|g)=100
236PA2cG (1973Or06).
236PA  G 308.7     1  0.42   5
236PA  G 340.1     1  0.67   9
236PA  B             3.4     12          6.4     2
236PAS B EAV=173.4 68
236PA  L 580.81    11 (0-,1)
236PA  G 549.2     1  0.32   9
236PA  G 581.1     2  0.20   4
236PA  B             0.52    10          6.4     2
236PAS B EAV=95.6 62
236PA  L 678.11    8  (0-,1)
236PA  G 567.1     3  0.13   3
236PA  G 646.6     1  0.72   11
236PA  G 678.1     1  0.47   7
236PA  B             1.32    14          5.4     1
236PAS B EAV=66.3 60