106PD 106RH B- DECAY (131 M) 1971TA09,1966DE11 08NDS 200806
106PD H TYP=FUL$AUT=D. DE FRENNE AND A. NEGRET$CIT=NDS 109, 943 (2008)$
106PD2 H CUT=1-May-2007$
106PD c 1971Ta09: {+106}Rh activity from {+106}Pd(n,p) and {+109}Ag(n,|a).
106PD2c Measured: E|g, I|g, E|b, |g|g. Deduced: {+106}Pd levels, J|p, log|
106PDxc {Ift} and Q(|b{+-})
106PD c 1966De11: {+106}Rh activity from {+106}Pd(d,2p) and {+108}Pd(d,|a).
106PD2c Measured: E|b, I|b, E|g, I|g, Ice, |b|g, |a, Q(|b{+-}). Deduced:
106PDxc {+106}Pd levels, J|p, log| {Ift}
106PD c Others: 1955Ne03, 1958Ma39, 1960Se07, 1969An12
106PD c |g|g (see drawings) 1971Ta09 semi-scin spectra
106PD c Q(|b{+-})=3677 {I10} deduced from E|b=920 {I10} to 2757 excitation;
106PDxc see 1966De11.
106PD cG E,RI$From semi |g-singles analysis (1971Ta09), unless otherwise
106PD2cG noted. Where comparison possible, E|g systematically 0.7-1.5 keV
106PD3cG higher than in (|a,2n|g), {+106}Ag |e decay (8.46 d), and (n,n'|g) data
106PD cG RI$Only statistical uncertainty given. Evaluators
106PD2cG added quadratically an uncertainty of 5% due to the systematic
106PD3cG deviation of the gamma data compared to other similar experiments
106PD cG M$Deduced from |a(K)exp including 8.46-d {+106}Ag decay data
106PD cG $|a(K)exp=ce(K)/I|g normalized to |a(K)(511.8|g)=0.00484 {I7}
106PD2cG (E2 theory) I(ce(K)) data are from 1966De11
106PD cG CC$Calculated for |d from adopted gammas
106PD cG $For gamma branching-ratio data, see also 8.46-d {+106}Ag decay
106PD cL E$From a least squares fit to the given gamma energies
106PD cL J$From adopted levels, gammas
106RH P 137 13 (6)+ 131 M 2 3541 6
106RH cP E$Adopted Value from Q(|b{+-})-Q(|b{+-})(g.s.)
106PD N 0.855 7 1.0 1.0
106PD cN NR$for I(|g+ce)=100 to g.s.; IT decay unobserved
106PD G 319.6 4 1.0 2
106PD G 473.2 4 1.0 5
106PD L 0.0 0+
106PD L 511.52 8 2+
106PD G 511.7 1 100 5 E2 C
106PDS G KC=0.00484 $LC=0.00061 $
106PD3 G EKC=0.0049 11 (1966De11)
106PD L 1127.89 8 2+
106PD G 616.1 1 23.6 16 M1+E2 C
106PDS G KC=0.00296 $LC=0.00035 $
106PD3 G EKC=0.0029 5
106PD G 1127.7 1 16 1 E2
106PDS G KC=0.0008 $
106PD3 G EKC=0.00053 16
106PD L 1228.78 104+
106PD G 717.2 1 33.8 18 E2 C
106PDS G KC=0.00195 $LC=0.00024 $
106PD3 G EKC=0.0015 6
106PD L 1557.80 9 3+
106PD G 328.3 4 1.4 2 E2(+M1) 0.022
106PD G 429.4 1 15.5 24 M1+E2 0.00930 1 C
106PDS G KC=0.00813 $LC=0.00106 $MC=0.00020 $
106PD3 G EKC=0.009 5
106PD G 1046.7 1 35.5 18 M1+E2 C
106PDS G KC=0.00080 $
106PD3 G EKC=0.00068 16
106PD L 1932.69 124+
106PD B 2.9 LT 7.7GT
106PDS B EAV= 675 4
106PD G 374.5 0.32 3
106PD cG RI$from I|g(374|g)/I|g(804|g)=0.021 {I3} (1973In08, {+106}Ag
106PDxcG decay)
106PD G 703.1 2 5.2 5 M1+E2
106PD G 804.6 2 15.2 13 E2 C
106PD L 2076.79 236+
106PD B 1.65 19 7.84 6
106PDS B EAV= 610 4
106PD cB $E(|b{+-}) max=1700 {I50} (1966De11) s, 1750 {I50} (1971Ta09)
106PD2cB scin, 1620 {I20} (1960Se07) scin
106PD cB IB$|?0 from level intensity balance
106PD G 848.0 2 1.9 CA @
106PD cG $Doublet I|g(848|g)=4.2 {I5} minus I|g=2.3 component via 4+,
106PD2cG 2077-keV state
106PD L 2077.18 16(4)+
106PD G 848.0 2 2.3 CA E2 @
106PD cG RI from I|g(1565|g)/I|g(848|g)=0.31 (1973In08, {+106}Ag decay)
106PD G 1565.4 3 0.7 5
106PD L 2085.07 133-
106PD B 1.2 LT 8.0GT
106PDS B EAV= 607 4
106PD G 956.2 0.56 CA S
106PD G 1573.9 2 7.8 6 E1 C
106PD3 G EKC=0.00037 13
106PD L 2306.78 114-
106PD B 3.4 LT 7.3GT
106PDS B EAV= 509 4
106PD G 221.8 1 7.5 4 M1+E2 0.0444 1
106PDS G KC=0.03809 18$LC=0.00462 7$MC=0.00087 $NC+=0.00015 $
106PD3 G EKC=0.034 5
106PD G 228.6 3 2.4 16 E1 0.015
106PD G 748.5 1 22.6 12 E1 C
106PD L 2351.98 104+
106PD B 3.7 LT 7.2GT
106PDS B EAV= 489 4
106PD G 419.2 4 0.7 2
106PD G 793.8 2 6.6 11 M1+E2 C
106PD G 1122 0.8 CA S
106PD cG RI$from I|g(1122|g)/I|g(1223|g)=0.081 {I9} (1973In08, {+106}Ag
106PDxcG decay)
106PD G 1224.2 1 9.5 8 E2
106PDS G KC=0.00057 $
106PD3 G EKC=0.00061 16
106PD G 1840.6 2 2.2 4 E2
106PD L 2366.50 19(4)+
106PD B 4.4 LT 7.1GT
106PDS B EAV= 483 4
106PD G 433.9 0.2 CA S
106PD G 808.4 2 8.7 5 M1+E2 C
106PD G 1136.8 0.5 CA S
106PD L 2757.94 105+
106PD B 920 10 85 10 5.21 6
106PDS B EAV= 318 4
106PD cB E$920 {I10} (1966De11) s, 950 {I30} (1960Se07) scin
106PD G 390.8 4 4.1 3 M1+E2 0.0126
106PDS G KC=0.01083 $LC=0.00143 $MC=0.00027 $
106PD3 G EKC=0.015 6
106PD G 406.0 1 13.6 8 M1+E2 0.0110 1
106PDS G KC=0.00950 $LC=0.00124 $MC=0.00023 $
106PD3 G EKC=0.010 5
106PD G 450.8 1 28.3 15 E1
106PDS G KC=0.00216 $LC=0.00027 $
106PD3 G EKC=0.002 10
106PD G 680.6 3 2.2 1 M1,E2
106PD cG $Transition to J(final)=6+ is inferred from I(|g+ce)
106PDxcG balance
106PDF G FL=2077.18
106PD G 825.0 1 15.9 9 M1+E2
106PD G 1200.5 1 13.3 7 E2 S
106PDS G KC=0.00059 $
106PD3 G EKC=0.00069 22
106PD G 1529.4 1 20.5 18 M1+E2
106PD3 G EKC=0.00033 10
106PD L 2953.18 125+
106PD B 700 50 14.5 18 5.61 6
106PDS B EAV= 240 4
106PD cB E$700 {I50} (1966De11) s, 790 {I40} (1960Se07) scin
106PD G 195.1 4 0.7 1 M1(+E2) 0.061
106PD G 586.0 4 1.0 1 M1,E2
106PD G 601.2 3 3.5 2 M1+E2
106PD G 645.8 2 3.2 2 E1
106PD G 1020.5 3 2.3 2 M1,E2
106PD G 1395.5 1 3.3 4 [E2]
106PDS G KC=0.00043 $
106PD3 G EKC=0.0007 3
106PD G 1724.6 2 2.6 5 M1+E2 0.00026