# DECAY

decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$A{-22}=0.02~{I9}, A{-44}=0.04~{I14} (1977Ri05) and R{-DCO}=0.9~{I3} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.156 {I8}, A{-44}=0.031 {I9} (1983Si08) 
MR$0.178~{I14} in 1983Si08 
$|a(K)exp=0.0209~{I13} (1970Ka13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.064 {I17}, A{-44}=-0.081 {I24} (1983Si08); Other: A{-22}=-0.200~{I33}, A{-44}=0.043~{I71} (1977Ba32) 
M$|a(K)exp=0.0142~{I14} (1970Ka13) 
MR$0.02~{I4} (1983Si08), -0.39~{I+13-6} from |g|g(|q) in 1977Ba32 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.157 {I8}; A{-44}=0.026 {I11} (1983Si08) 
MR$Also, -0.007~{I20} (1983Si08),-0.16~{I3} from |g|g(|q) in 1977Ba32; +0.137 (9) from |g|g(|q) in 1981Al19; 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
MR$-0.020~{I+5-6} from |g|g(|q) in 1977Ba32; Other: -0.012~{I4} from |g|g(|q) in 1981Al19 
M$A{-22}=-0.170~{I5}, 0.001~{I1} (1977Ba32) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.104~{I11}, A{-44}=-0.10~{I10} (1977Ba32); Also |a(K)exp=0.0122~{I8} (1970Ka13) 
MR$-0.084~{I7} from |g-|g(|q) in 1983Si08, and -0.062~{I9} from |g-|g(|q) in 1981Al19 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.072~{I12}, A{-44}=-0.001~{I16} (1983Si08); Other: A{-22}=-0.098~{I16} A{-44}=-0.030~{I45} (1977Ba32); Also |a(K)exp=0.0094~{I8} (1970Ka13) 
MR$Also: 0.000~{I3} (1977Ba32) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.182~{I17}, A{-44}=0.020~{I25} (1983Si08); Other: 0.149~{I13}, -0.014~{I20} (1977Ba32); Also |a(K)exp=0.0083~{I6} (1970Ka13) 
MR$0.05~{I4} in 1983Si08 from |g-|g(|q), -0.84~{I+3-17} from |g|g(|q) in 1977Ba32; and +0.10~{I7} from |g-|g(|q) in 1981Al19 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.11~{I3} in 1958Ra01, +0.035~{I22} in 1962Bh03, +0.013~{I3} in 1972Be67 and +0.07~{I7} in 1976Ba39 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$Other: +0.055 {I2} (1976Ba39) and 0.06 {I1} (1977Wi10) 
EKC$0.016~{I2} from Ice/I|g and comparison with low energy I|b (1964Ka23) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from the adopted gammas; Others: +0.11~{I1} (1977Wi10), +0.091~{I13} or +1.35~{I3} (1976Ba39), -0.11 (1962Me07) 
EKC$From Ice/I|g and comparison with low-energy I|b (1964Ka23) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-22}=-0.048~{I10}, A{-44}=0.015~{I10} (1977Ri05); R{-DCO}=2.19~{I6} (1977Ri05) 
MR$Also: 0.01~{I1} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.21~{I4}, A{-44}=0.01~{I5} (1977Ri05); R{-DCO}=1.08~{I19} (1977Ri05) 
MR$other: 1.9~{I7} (1977Ri05); Also: -0.05~{I17} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.610~{I21}, A{-44}=0.031~{I24} (1977Ri05); R{-DCO}=4.1~{I7} (1977Ri05) 
MR$Also, -0.20~{I7} from DCO in 1977Ri05 and -0.37~{I8} from DCO in 2019Ti02 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-22}=-0.29~{I5}, A{-4}=0.03~{I8} (1977Ri05); R{-DCO}=2.5~{I5} (1977Ri05) 
MR$Also: -0.08~{I8} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.01~{I3}, A{-44}=0.02~{I4} (1977Ri05); R{-DCO}=2.4~{I5} (1977Ri05) 
MR$Also: -0.04~{I8} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.46~{I5}, A{-44}=0.04~{I6} (1977Ri05); R{-DCO}=3.1~{I10} (1977Ri05) 
MR$Also: -0.05~{I8} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.38~{I4}, A{-44}=-0.05~{I5} (1977Ri05); R{-DCO}=3.9~{I11} (1977Ri05) 
MR$Also: -0.19~{I11} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.28~{I4}, A{-44}, -0.08~{I6} (1977Ri05); R{-DCO}=1.2~{I3} (1977Ri05) 
MR$Also: 1.0~{I5} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.436~{I25}, A{-44}=0.01~{I3} (1977Ri05); R{-DCO}=0.58~{I8} (1977Ri05) 
MR$from DCO and linear pol. in 2019Ti02; Also: +0.46~{I10} or 1.3~{I7} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=1.4~{I7}, A{-44}=-0.4~{I8} (1977Ri05); R{-DCO}=0.8~{I3} 
MR$Also: 4~{I4} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.42~{I3}, A{-44}=-0.04~{I5} (1977Ri05); R{-DCO}=0.86~{I13} (1977Ri05) 
MR$Also: 0.0~{I5} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.42~{I4}, A{-44}=-0.08~{I5} (1977Ri05); R{-DCO}=0.93~{I24} (1977Ri05) 
MR$Also: 0.2~{I6} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
M$A{-22}=0.28~{I8}, A{-44}=-0.05~{I11} (1977Ri05); R{-DCO}1.0 {I3} (1977Ri05) 
MR$Also: 0.08~{I8} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.57~{I6}, A{-44}=0.14~{I8} (1977Ri05); R{-DCO}=0.62~{I14} (1977Ri05) 
MR$from DCO and linear pol. in 2019Ti02; Also: +0.62~{I18} or 0.8~{I3} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.11~{I3}, A{-44}=0.04~{I4} (1977Ri05); R{-DCO}=1.64~{I18} (1977Ri05) 
MR$Also: 0.13~{I4} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.65~{I8}, A{-44}=-0.03~{I12} (1977Ri05); R{-DCO}=0.58~{I16} (1977Ri05) 
MR$Also: 1.6~{I11} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.05~{I3}, A{-44}=-0.01~{I4} (1977Ri05); R{-DCO}=1.60~{I17} (1977Ri05) 
MR$Also: 0.11~{I4} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-22}=0.42~{I5}, A{-44}=-0.13~{I8} (1977Ri05); R{-DCO}=0.8~{I3} (1977Ri05) 
MR$Also: 0.0~{I7} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.02~{I3}, A{-44}=0.01~{I5} (1977Ri05); R{-DCO}=1.6~{I3} (1977Ri05) 
MR$Also: 0.11~{I6} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.8~{I3}, A{-44}=-0.2~{I4} (1977Ri05) 
MR$from DCO and linear pol. in 2019Ti02; Also: +1.5~{I10} in 1977Ri05 


decay_energy_unit: KEV
decay_multipolarity: [E2]
decay_comment:
E$ Deduced from level scheme in Coul. ex. (1995Sv01) 
$B(E2)(W.u.)=19 {I+7-3} in Coul. ex. (1995Sv01) 


decay_energy_unit: KEV
decay_comment:
E$Deduced by evaluators from level scheme in Coul. ex. (1995Sv01) 
$B(E2)(W.u.)=5.3 +2.5-1.4 in Coul. ex. (1995Sv01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M from |a(K)exp in (n,|g). M1 excluded if J|p for the initial and final states are correct 
$B(E2)(W.u.)=2.4 +0.4-0.3 in Coul. ex. (1995Sv01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M from |a(K)exp=0.0041 {I10} for the 346.59+347.14 |g transitions 
E No final level within 0.48 keV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$No final level within 0.13 keV 
$E1 suggested in {+106}Rh |b{+-} decay (131 m) but impossible if J|p(2305)=4- and J|p(2077)=6+ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI taken from {+106}Rh |b{+-} decay using the ratio I|g(2309 from 2309) /I|g(1180|g+1797|g)|<0.051 {I8} from |e decay but taking into account the division of the I(2309|g) of the doublet of 2309|g between 2308 and 2821 levels 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M deduced under the assumption J|p(2365)=4+. |g|g(|q) also consistent with mult(808|g)=E2 and J|p(2365)=5+. M1 fraction impossible if J|p(2566)=5+ and J|p(1557)=3+ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Discrepancies exist for branching ratios of the 2626 and 3054 keV levels in (n,|g) and (n,n'|g) due to unresolved doublet of 1498|g deexciting both levels 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$No final level within 0.89 keV 
Discrepancies exist for branching ratios of the 2626 and 3054 keV levels in (n,|g) and (n,n'|g) due to unresolved doublet of 1498|g deexciting both levels 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E semi 1976Sh25 measurement rel to E(|g{+|+})=511.0034 {I14}; other; 511.85 {I1} (1977Ok02) 
Absolute I|g(512|g)=20.6% {I6} (1969Od01), 21% {I2} (1966Ov01), 22.0% {I11} (1975Ge06), 20.5% (1953Ka47) I|g/summed |b{+-} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR taken from 1968Ha35 via |g|g(|q) 
Branching: I|g(616|g)/I|g(1128|g)=1.88 {I38} (1977Ok02), 1.95 {I29} (1975Hs02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
EKC Other: 0.0030 {I7} (1967Vr05) 
(622|g)(512|g)(|q): 1972Av03, 1971Az02, 1968Ha35, 1953Kl51, 1953Kr07 
|b(622|g)(512|g)(|q): 1974Ra29, 1968Pe12 
Branching: I(ce(K))(1134|g)/I|g(622|g)=0.00049 {I5} (1977Ok03) 
Absolute I|g(616+622|g)=10.6% {I3} (1969Od01), 10% {I1} (1966Ov01), 10.4% (1953Ka47) I|g/summed |b{+-} 
Absolute I|g(622|g)=11.0 {I10} (1975Ge06) I|g/summed |b{+-}; |g-peak is corrected for unresolved I|g(616|g) fraction 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
E from 1977Ok03 (s); other: 1133.9 (1973Gr25) 
|a(K)exp|>0.18 if I|g(1134|g)|<1.3 (1977Ok03,1973Gr25) 
I(ce(K) 1134|g)/I(ce(K) 512|g)=0.048 {I4} (1977Ok03), 0.07 {I2} (1973Gr25), 0.044 {I5} (1974BeZH) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Branching: I|g(1909|g)/I|g(1398|g)=0.40 {I6} (1976SaYX, {+106}Ag decay) is used to apportion doublet I|g(1909|g)=0.060 {I5} (1977Ok02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
|a(K)exp|?0.0015 deduced from I(ce(K) 1114|g)/I(ce(K) 1194|g)|?0.5 (1973Av01). |D|p=no from decay scheme 
MR taken from (1973Av01). Obtained via |g|g(|q) in {+106}Rh |b{+-} decay (30.07 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI deduced from (K| x ray)(512|g)/(K| x ray)(616+622|g) (1967Ra11) and theoretical |e/|b{++}, |eL/|eK, yielding I|g(616+622|g)/I|g(512|g)=0.0269. Other: 809 (1967Ra11) normalized to I|g(622|g)=12.7 
Doublet I|g(511.9|g+|g{+|+})=1000 (1976SaYX) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E other: 511.8605 {I31} (1976Sh25, {+106}Ru source) semi, relative to E(|g{+|+})=511.0034 {I14} 
RI |g{+|+} is negligible; unobserved |b{++}<0.1% (1953Be42) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1+E2
decay_comment:
EKC Weighted average of 0.00306 {I14} (1973In08) and 0.00308 {I14} (1990Ka35) 
M from electron conversion data of 1990Ka35 
MR from 1977Ti01. Other: -10 {I+4-2} from |g(|q) (1975Sc38); -14 {I8} or -0.53 {I6} from NMR on oriented nuclei (1984Ed02); or 14 {I+17-4} from 1990Ka35. 
$L1:L2:L3=100:8.5 {I8}:6.0 {I7} (1978Sh25) 
|r(E0)=0.16 {I8} (1990Ka35) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR weighted average: -7.4 {I7} from |g(|q) (1975Sc38) and -9 {I1} from NMR on oriented nuclei (1984Ed02) 
$L1:L2:L3=100:13 {I4}:5.8 {I15} (1978Sh25) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR weighted average of: -4.7 {I8}, -5.5 {I15}, -2.4 {I8} from |g|g(|q) (1977Ti01) and -3.8 {I3} from NMR on oriented nuclei (1984Ed02) 
$L1:L2:L3=100:4.4 {I16}:1.5 {I9} (1978Sh25) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M |D|p=no from decay scheme 
MR from 1977Ok03. Others: +0.20 {I2} (1968We16), +0.19 {I2} (1968Ha35), +0.21 {I1} (1953Kl51), +0.30 {I7} (1975Hs02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|a(K)exp: other: 0.00202 {I24} (1990Ka35) 
MR from 1977Ti01; others: -1.1 {I4} (1975Sc38); -1.7 {I11} (1984Ed02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|a(K)exp(doublet)=0.0014 {I4} 
E from 1978IdZZ 
RI doublet I|g(848|g)=50 {I2} (1973In08) minus I|g=18 {I6} component via 4+, 2077.4-keV state 
M |a(K)exp=0.0014 {I4} for 847|g doublet is consistent with mult (847.03|g)=M1,E2 and with mult (841.27|g)=M1,E2 or possibly E1. The placement in the decay scheme requires mult=E2 and |D|p=no, respectively 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
E from 1978IdZZ 
RI |g|g measurement (1977Ti01); other: I|g(847.27|g)=I|g(847.43|g) (1978IdZZ) suggests component I|g=25 
M |a(K)exp=0.0014 {I4} for 847|g doublet is consistent with mult (847.03|g)=M1,E2 and with mult (841.27|g)=M1,E2 or possibly E1.the placement in the decay scheme requires mult=E2 and |D|p=no, respectively 
From |a(K)exp=0.0014 {I4} for 847|g doublet M1 or E2 most likely although E1 cannot be excluded 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E3]
decay_comment:
RI from 1977Ti01; others: 0.34 {I11} (1978IdZZ), 0.19 {I15} (1973In08), 0.20 {I6} (1968Mo02), 0.31 (1967Ra11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR weighted average of: -0.13 {I2} from |g(|q) oriented nuclei (1975Sc38); -0.08 {I8} from |g|g(|q) (1977Ti01) and -0.08 {I2} from NMR on oriented nuclei (1984Ed02) 
$L1:L2:L3=100:7.6 {I4}:4.2 {I2} (1978Sh25) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR weighted average: -7.0 {I20} from |g(|q) (1975Sc38); -4.3 {I15} from |g|g(|q) (1977Ti01) and -8.0 {I20} from NMR on oriented nuclei (1984Ed02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
RI other: 1.1 {I2} (1977Ti01) 
M$D+Q from |g|g(|q). E1+M2 from linear pol in {+96}Zr({+13}C,3n|g) 
MR from 1976Gr12 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
$|a(K)exp=0.0109 {I9} and also 0.00104 {I9} (1990Ka35) 
|d|?-16 from |g(|q) (1975Sc38); |?-33 or -1.7 {I6} from NMR on oriented nuclei (1984Ed02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR weighted average: -3.2 {I2} from |g(|q) (1975Sc38) and -3.5 {I2} from NMR on oriented nuclei (1984Ed02). Other: -7 {I4} (1977Ti01) 
$L1:L2:L3=100:20 {I4}:12 {I2} (1978Sh25) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E doublet decomposed by 1978IdZZ 
RI from doublet I|g=24.9 {I9} (1973In08) and I|g(680.4|g)/I|g(679.6|g)=2.4 {I1} (1978IdZZ) 
M |a(K)exp=0.0017 {I3} for the 680 doublet consistent with mult(679.64|g)=E1 and mult(680.42|g)=M1,E2. Placement in the decay scheme |D|p=no for both placements.This requirement leads to |S I(ce(K))=0.057 {I4}, compared with |SI(ce(K))exp=0.042 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
|a(K)(M1)=0.0024; |a(K)(E2)=0.0022 
|a(K)exp=0.0017 {I3} doublet 
RI from doublet I|g=24.9 {I9} (1973In08) and I|g(680.4|g)/I|g(679.6|g)=2.4 {I1} (1978IdZZ) 
M |a(K)exp=0.0017 {I3} for the 680 doublet consistent with mult(679.64|g)=E1 and mult(680.42|g)=M1,E2. Placement in the decay scheme |D|p=no for both placements. This requirement leads to |S I(ce(K))=0.057 {I4}, compared with |SI(ce(K))exp=0.042 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR weighted average: -5.7 {I+13-8} from |g(|q) 1975Sc38 and -6.8 {I6} from NMR on oriented nuclei (1984Ed02). Other: -0.04 {I+2-4} (1975Sc38) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$D+Q from |g|g(|q). M1+E2 from linear pol in {+96}Zr({+13}C,3n|g) 
MR weighted average: -2.3 {I2} from |g(|q) (1975Sc38); -2.5 {I1} from NMR on oriented nuclei (1984Ed02) and -2.3 {I8} from |g|g(|q) (1977Ti01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI |g-singles I|g(512|g+|g{+|+})=137; I|g(512|g)=100 is derived from summed I|g to 512 level + 2% unobserved feeding 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI from |g|g; |g-singles I|g(1000|g+1001|g)=5.4 {I3} 
M Q from |g|g(|q). Transition is possibly Doppler broadened 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI calculated from ce measurement. I|g is obscured in the singles spectrum by interference with 511|g annihilation radiation. Therefore the intensity of that |g was calculated from the conversion electron spectra. No uncertainty on I|g was given in the paper 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI calculated based upon I|g(428|g from 1562 level)/I|g(1050|g)= 0.0453 {I15} and I|g(429|g from 1557 level0/I|g(1045|g)=0.445 {I19} in adopted gammas. However, a large fraction of the 429 peak, with I|g=102 {I12} remains unassigned 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI calculated based upon I|g(428|g from 1562 level)/I|g(1050|g)= 0.0453 {I15} and I|g(429|g from 1557 level)/I|g(1045|g)=0.445 {I19} in adopted gammas. However, a large fraction of the 429 peak, with I|g=102 {I12}, remains unassigned 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI I|g=7.9 {I10} for 346.59|g +347.14|g doublet in (n,|g) 
M from |a(K)exp=0.0041 {I10} for the 346.59+347.14 |g transitions 
E$no final level within 0.49 keV 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI deduced from I|g(848|g from 2077)/I|g(949|g+1565|g)=2.3 {I8} in {+106}Ag |e decay and I|g=38 {I5} for the doubly placed 848 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1+E2
decay_comment:
MR$+0.24 {I1} from the Adopted Gammas for {+106}Pd in the ENSDF database was used in the calculation to determine |r{+2}(E0) as it had a smaller uncertainty by authors (2016Pe06) 
$|W{-K}(E0) |*10{+-9}= 2.966 from BrIcc calculations by authors (2016Pe06) 
$|r{+2}(E0) |*10{+3}= 34 {I22} with |a{-K}= 1.12 |*10{+-3} {I15} (1987Co03) 
$|r{+2}(E0) |*10{+3}= 97 {I39} with |a{-K}= 1.56 |*10{+-3} {I24} (1987Fa07) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1+E2
decay_comment:
MR$Two values were given for |d, +1.32 {I+11-25} and +0.25 {I+6-5}, as the authors could not differentiate between them. 
$|W{-K}(E0)|*10{+-9}= 4.189 from BrIcc calculations by authors (2016Pe06) 
$|r{+2}(E0) |*10{+3}= 21 {I+10-21} with |a{-K}= 0.68 |*10{+-3} {I9} (1987Co03) and |d=+1.32 {I+11-25} 
$|r{+2}(E0)|*10{+3}= 18 {I+10-18} with |a{-K}= 0.68 |*10{+-3} {I9} (1987Co03) and |d=+0.25 {I+6-5} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1+E2
decay_comment:
$|W{-K}(E0) |*10{+-9}= 3.177 from BrIcc calculations by authors 
$|r{+2}(E0) |*10{+3}= 96 {I+43-61} with |a{-K} = 1.46 |*10{+-3} {I26} (1987Co03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$B(E2)(W.u.)=+0.0002 {I+52-2} (overlaps zero) for other |d value. 
MR$Other value (first): -0.03 {I+12-11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$B(E2)(W.u.) calculated by compiler. In 2017Pr03: 0.003 {I+11-3} (overlaps zero) and 1.00 {I+49-43} for other |d value. 
MR$Other value: +2.7 {i3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$B(E2)(W.u.) calculated by compiler. In 2017Pr03: 0.02 {I+11-2} (overlaps zero) and 0.61 {I+49-34} for other |d value. 
MR$Other value: +4 {I+12-2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_comment:
$q{+2}(E0/E2)=0.027 {I38}; |r{+2}<0.005 {I8} (2022Ma24); using branching ratio=64.7 {I24} for 616.2|g from 2017Pr03 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2+E0)
decay_comment:
$q{+2}(E0/E2)=4.2 {I18}; |r{+2}=0.026 {I11} (2022Ma24); using branching ratio=85.3 {I34} for 1050.4|g from 2017Pr03 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [E0]
decay_comment:
$q{+2}(E0/E2)=0.09 {I15}; |r{+2}=0.002 {I4} (2022Ma24); using branching ratio=85.7 {I34} for 1194.5|g from 2017Pr03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E others: 115.7 (1978Fr16), 115.6 (1978Ho06), 115.8 (1976Kl01) 
M |a(K)exp=0.70 {I9} (1969Gr18) K| x ray/I|g via (452|g)(K| x ray,116|g)(t) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,(E2)
decay_comment:
E others: 302.79 {I37} (1969WiZX) semi, 302.86 {I6} (1979Bo26) cryst 
M |a(K)exp|<0.016 (1969Gr18) is compatible with dipole radiation. (303|g)(|q) via (|a,n|g) favors M1+E2 mixture. |a(K)=0.017 (M1), 0.0059 (E1), 0.025 (E2) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E from 1976Kl01 (|a,n|g). Others: 216 {I5} (1957St87), 214 {I1} (1969Gr18) 
M |a(K)exp=0.41 {I2} (1964We09), 0.30 {I5} (1957St87); K| x ray/I|g, scin 
|a(exp)|?0.4 (1952Fl10) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR +1.73|<|d|<-0.05 from A{-2}=0.35 {I9}, A{-4}=-0.05 {I9}. Deexcites a 696 level in (HI,xn|g) and adopted levels. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI doublet from observed line width 
M A{-2}=0.67 {I6}, A{-4}=0.01 {I5}; (|g doublet)(|q) suggests strong E2 component 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI doublet deduced from level intensity balance 
A{-2}=-0.586 {I13}, A{-4}=0.084 {I23}; (|g doublet)(|q) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E|g=643.9 {I8} also observed in {+107}Rh decay (1969Gr18) 
M E2 deduced from A{-2}=0.41 {I12}, A{-4}=-0.13 {I11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$E=472.5 {I1} with I|g=110 {I2} (1994Ju05) 
M$anisotropy=-0.23 {I5}. Substate alignment=0.47 {I10} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$anistropy=0.62 {I27}. Substate alignment=(0.9) 
MR$045<|d<1.9 
E$E=627 {I1} with I|g=3.0 {I5} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$estimated by evaluator from spectrum in |e decay where the insert in fig. 1 of 1973Si02 shows no evidence for a 393|g. This strongly suggests that the value of 25 {I+6-4} in Coulomb excitation is too large. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$weighted average of I|g/I|g (1007|g) from |e decay and (n,n'|g) 
E$E=1441.60 {i10} reported in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E other: 497.47 {i45} (1969WiZX) 
M$|d from Adopted levels and Coul ex. 
RI others: 17 {i3} (1969WiZX), 15 (1975Fe12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$I|g=54.6 (1969Pi08). Value of 36 seems to be a misprint in 1984Bh02. From the authors' decay scheme, an intensity balance gives I|g>58 {I6}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E from energy level difference 
RI from intensity balance at the 931 level. From the 511 peak in coin with the 434|g the authors estimate I(510.1|g)=0.7 {i5}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$|a=0.0091 
E$from 1994HeZZ. Others: 433.939 {i4} (1978MeZZ), 433.935 {I4} (1975Mo34). 
M$from decay scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from 1994HeZZ. Others: 614.281 {I6} (1978MeZZ), 614.37 {i10} (1969Br03), 614.3 {i1} (1973Be08), 614.27 {i5} (1974HeYW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from 1994HeZZ. Others: 722.938 {I8} (1978MeZZ), 722.95 {i8} (1969Br03), 722.9 {i1} (1973Be08), 722.90 {i5} (1974HeYW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$-10|<|d|<-3 or |d=-0.48 {I16}; the former is consistent with the known value of |d=-3.1 {I4} from {+108}Pd in ENSDF. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$DCO value for 693+695 peaks. Separate analysis leads to less reliable 1.8 {I3} and 1.1 {I3} values, respectively (authors' note). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from |e decay. The value of 1441.60 {I12} given by 1975Go11 appears to be a misprint. The author's value of E|g=1007.21 for the |g to the 434 level (1007.22 {I6} in |e decay) gives E(level)=1441.14. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$authors place 1957|g deexciting the 2889 level and alternatively, from the 2391 level. However, the energy fit is bad for the former placement. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$from (497|g)(434|g)(|q) (1971Ro09). Other: -(5.2 {I+25-14}) from 497|g(|q) (1969Ro05). |D|p=no from decay scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=0.7 {I2} in {+109}Rh |b{+-} decay (1977Ba57); |a(K)exp=0.56 {I8}, |a(L1)exp=0.053 {I8}, |a(L2)exp=0.031 {I4}, |a(L3)exp=0.039 {I6}, |a(M)exp=0.010 {I2} in {+108}Pd(n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_BE_unit: e^2 x (fm)^6
decay_BE_info: ;TYPE=BE3;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE3W
decay_comment:
M$|a(K)exp=0.52 {i4} (1964We09), 0.60 {i1} (1957St87) in {+109}Rh |b{+-} decay; |a(K)exp=0.50 {I5}, |a(L1)exp=0.049 {I7}, |a(L2)exp=0.055 {I9}, |a(L3)exp=0.046 {I8}, |a(M)exp=0.022 {I5} in {+108}Pd(n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$weighted average of 100 {I11} in (n,|g) E=thermal, 100 {I10} in (n,|g) E= 2.96 eV, and 100 {I8} in {+109}Rh |b{+-} decay. 
M$|a(K)exp=0.095 {I10}, |a(L1)exp=0.010 {I2}, |a(M)exp=0.002 {I5} in {+108}Pd(n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$weighted average of 29 {I3} in (n,|g) E=thermal, 31 {I3} in (n,|g) E=2.96 eV, and 42 {I8} in {+109}Rh |b{+-} decay. 
M$|a(K)exp=0.040 {I4} in {+108}Pd(n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$weighted average of 100 {I10} in (n,|g) E=thermal, 100 {I10} in (n,|g) E=2.96 eV, and 100 {I5} in {+109}Rh |b{+-} decay. 
M$|a(K)exp=0.063 {I6}, |a(L1)exp=0.006 {I1} in {+108}Pd(n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$weighted average of 83 {I8} in (n,|g) E=thermal, 82 {I8} in (n,|g) E=2.96 eV, and 99 {I6} in {+109}Rh |b{+-} decay. 
M,MR$|a(K)exp=0.021 {I2}, |a(L1)exp=0.004 {I2} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$weighted average of 28 {I3} in (n,|g) E=thermal, 25 {I3} in (n,|g) E=2.96 eV, and 44 {I8} in {+109}Rh |b{+-} decay. 
M,MR$|a(K)exp=0.044 {I5}, |a(L1)exp=0.007 {I2} in {+108}Pd(n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$weighted average of 100 {I10} in (n,|g) E=thermal, 100 {I10} in (n,|g) E=2.96 eV, and 100 {I19} in {+109}Rh |b{+-} decay. 
M,MR$|a(K)exp=0.015 {I1}, |a(L1)exp=0.002 {I1} in {+108}Pd(n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
RI$from {+109}Rh |b{+-} decay 
M,MR$D+Q from |a(K)exp=0.7 {I6} in {+109}Rh |b{+-} decay (1978Ka10), change in parity between two levels indicates E1(+M2). 1978Ka10 report M1(+E2). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_comment:
E$Note 326.450 {I10} in {+109}Rh |b{+-} decay (1979Bo26) is discrepant with the value from the {+108}Pd(n,|g) E=thermal data 
RI$from {+109}Rh |b{+-} decay 
M$|a(K)exp=0.020 {I2} in {+108}Pd(n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$|a(K)exp=0.43 {I9}, |a(L1)exp=0.044 {I6}, |a(L2)exp=0.014 {I6}, |a(L3)exp=0.018 {I8}, |a(M)exp=0.018 {I8} in {+108}Pd(n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 8.5 {I9} in (n,|g) E=thermal, 6.7 {I8} in (n,|g) E=2.96 eV, and 7.7 {I7} in {+109}Rh |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$weighted average of 100 {I10} in (n,|g) E=thermal, 100 {I11} in (n,|g) E=2.96 eV, and 100 {I9} in {+109}Rh |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$weighted average of 47 {I5} in (n,|g) E=thermal and 54 {I5} in (n,|g) E=2.96 eV (1980Ca02) 
M$|a(K)exp=0.013 {I3} in (n,|g) E=thermal(1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$weighted average of 100 {I10} in (n,|g) E=thermal and 100 {I9} in (n,|g) E=2.96 eV (1980Ca02) 
M$|a(K)exp=0.0065 {I8} in (n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 9.1 {I17} in (n,|g) E=thermal, 10.7 {I23} in (n,|g) E=2.96 eV, and 4.4 {I22} in {+109}Rh |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$weighted average of 49 {I5} in (n,|g) E=thermal, 55 {I6} in (n,|g) E=2.96 eV, and 39 {I4} in {+109}Rh |b{+-} decay. 
M$|a(K)exp=0.041 {I10} in (n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$weighted average of 100 {I10} in (n,|g) E=thermal, 100 {I10} in (n,|g) E=2.96 eV, and 100 {I9} in {+109}Rh |b{+-} decay. 
M$|a(K)exp=0.012 {I3} in (n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 40 {I4} in (n,|g) E=thermal, 40 {I4} in (n,|g) E=2.96 eV, and 30 {I4} in {+109}Rh |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 9.3 {I16} in (n,|g) E=thermal, 7.9 {I11} in (n,|g) E=2.96 eV, and 9.3 {I19} in {+109}Rh |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$weighted average of 35 {I4} in (n,|g) E=thermal, 33 {I3} in (n,|g) E=2.96 eV, and 29.6 {I19} in {+109}Rh |b{+-} decay. 
M$|a(K)exp=0.039 {I5} in (n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$weighted average of 100 {I10} in (n,|g) E=thermal, 100 {I10} in (n,|g) E=2.96 eV, and 100 {I6} in {+109}Rh |b{+-} decay. 
M$|a(K)exp=0.027 {I3} in (n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 7.2 {I21} in (n,|g) E=thermal, 5 {I5} in (n,|g) E=2.96 eV, and 6.5 {I19} in {+109}Rh |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 3.1 {I5} in (n,|g) E=thermal, 3.9 {I11} in (n,|g) E=2.96 eV, and 1.9 {I9} in {+109}Rh |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 7.2 {I16} in (n,|g) E=thermal, 4.5 {I11} in (n,|g) E=2.96 eV, and 5.6 {I9} in {+109}Rh |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 16 {I4} in (n,|g) E=thermal, 15 {I8} in (n,|g) E=2.96 eV, and 8.3 {I9} in {+109}Rh |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$weighted average of 19.4 {I19} in (n,|g) E=thermal and 17.5 {I19} in (n,|g) E=2.96 eV (1980Ca02) 
M,MR$|a(K)exp=0.030 {I5} in (n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
RI$weighted average of 100 {I10} in (n,|g) E=thermal and 100 {I10} in (n,|g) E=2.96 eV (1980Ca02) 
M,MR$|a(K)exp=0.019 {I6} in (n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$weighted average of 100 {I10} in (n,|g) E=thermal and 100 {I10} in (n,|g) E=2.96 eV (1980Ca02) 
M,MR$|a(K)exp=0.013 {I2} in (n,|g) E=thermal (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
%I|g=5.7 {I6}, using the calculated normalization. 
E$113.35 {I5} (1978Ka10) 
RI$others: 10.0 {I7} (1978Fr21), 12.0 {I11} (1977Ba57) 
M$|a(K)exp=0.7 {I2} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
%I|g=1.30 {I16}, using the calculated normalization. 
E$245.03 {I7} (1978Ka10) 
RI$others: 2.1 {I2} (1978Fr21), 2.5 {I3} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=0.65 {I8}, using the calculated normalization. 
E$152.91 {I7} (1978Ka10) 
E$placed by 1977Ba57 and 1978Fr21 from a level at E=694 keV that is not in Adopted Levels 
RI$others: 1.0 {I1} (1978Fr21), 1.3 {I3} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
%I|g=0.27 {I6}, using the calculated normalization. 
E$266.26 {I10} (1978Ka10) 
E$placed by 1978Fr21 from a level at E=806.8 keV that is not in Adopted Levels 
RI$others: 0.48 {I7} (1978Fr21), 0.9 {I2} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
%I|g=2.2 {I3}, using the calculated normalization. 
E$276.26 {I7} (1978Ka10) 
E$placed by 1977Ba57 from a level at E=389.7 keV that is not in Adopted Levels 
RI$others: 3.9 {I3} (1978Fr21), 4.3 {I6} (1977Ba57) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_mixing_ratio_info: ;ERR=LE
decay_uncertain: ?
decay_comment:
%I|g=0.03 {I3}, using the calculated normalization. 
E$this |g was not observed in the singles spectra but was inferred from |g|g-coincidence measurements (1978Ka10). 
M$measurements by 1978Ka10 indicate the 25.1|g may be M1 (+0-50% E2) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=7.6 {I8}, using the calculated normalization. 
E$178.03 {I5} (1978Ka10) 
RI$others: 12.1 {I8} (1978Fr21), 14.7 {I8} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
%I|g=7.5 {I8}, using the calculated normalization. 
E$291.36 {I7} (1978Ka10) 
RI$others: 13.2 {I9} (1978Fr21), 12.8 {I14} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=1.30 {I19}, using the calculated normalization. 
E$35.34 {I10} (1978Ka10) 
RI$others: 2.8 {I10} (1978Fr21), 0.7 {I2} (1977Ba57) 
M$|a(K)exp=9 {I5} (1978Ka10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
%I|g=0.70 {I9}, using the calculated normalization. 
E$81.78 {I5} (1978Ka10) 
RI$others: 1.3 {I1} (1978Fr21), 1.1 {I2} (1977Ba57) 
M$|a(K)exp=0.7 {I6} (1978Ka10) 
MR$the authors report M1(+E2) with |d=0.3 {I+21-3} which is not compatible with change in parity between the two levels. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_comment:
%I|g=54 {I5}, using the calculated normalization. 
E$326.450 {I10} (1979Bo26) and 326.83 {I5} (1978Ka10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.59 {I8}, using the calculated normalization. 
E$149.82 {I7} (1978Ka10) 
E$placed by 1977Ba57 from a level at E=263.1 keV that is not in Adopted Levels 
RI$others: 1.1 {I1} (1978Fr21), 1.1 {I3} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=7.7 {I10}, using the calculated normalization. 
E$426.14 {I7} (1978Ka10) 
RI$others: 15.2 {I11} (1978Fr21), 14.0 {I14} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=0.49 {I7}, using the calculated normalization. 
E$200.13 {I7} (1978Ka10) 
RI$others: 0.83 {I7} (1978Fr21), 0.9 {I2} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
%I|g=1.24 {I16}, using the calculated normalization. 
E$378.05 {I7} (1978Ka10) 
RI$others: 1.7 {I2} (1978Fr21), 1.9 {I3} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.38 {I7}, using the calculated normalization. 
E$491.7 {I2} (1978Ka10) 
RI$others: 0.95 {I8} (1978Fr21), 0.7 {I2} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.54 {I12}, using the calculated normalization. 
E$213.81 {I10} (1978Ka10) 
E$placed by 1977Ba57 and 1978Fr21 from the 326.7-keV level 
RI$others: 0.97 {I9} (1978Fr21), 4.4 {I14} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=1.73 {I20}, using the calculated normalization. 
E$215.28 {I7} (1978Ka10) 
RI$others: 2.9 {I2} (1978Fr21), 4.5 {I14} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=5.8 {I7}, using the calculated normalization. 
E$249.16 {I5} (1978Ka10) 
RI$others: 9.1 {I6} (1978Fr21), 11.3 {I11} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.38 {I12}, using the calculated normalization. 
E$264.33 {I10} (1978Ka10) 
E$1977Ba57 place a transition of E|g=263.1 {I2} from a level at E=263.1 keV level that is not in Adopted Levels 
RI$others: 0.59 {I7} (1978Fr21), 0.9 {I2} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.32 {I7}, using the calculated normalization. 
E$295.54 {I10} (1978Ka10) 
RI$others: 0.60 {I7} (1978Fr21), 0.9 {I2} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.49 {I7}, using the calculated normalization. 
E$540.7 {I2} (1978Ka10) 
RI$others: 2.4 {I2} (1978Fr21), 1.4 {I3} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.05 {I3}, using the calculated normalization. 
E$from 1978Ka10. A 320.164|g de-excites a 3/2+ level at E=433.56 in Adopted Levels 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
%I|g=0.05 {I3}, using the calculated normalization. 
E$weighted average of 391 {I1} (1978Ka10) and 389.7 {I2} (1977Ba57). 1977Ba57 place this |g ray from a E=389.7 keV level. 
RI$others: 0.8 {I2} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.032 {I17}, using the calculated normalization. 
RI$normalized to I|g(690.3|g)=0.2 {I1} based on I|g(555.614|g)/I|g(630.3|g)=32 {I4}/100 {I7} in Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.038 {I22}, using the calculated normalization. 
RI$normalized to I|g(690.3|g)=0.2 {I1} based on I|g(654.892|g)/I|g(630.3|g)=37 {I4}/100 {I7} in Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
%I|g=0.11 {I6}, using the calculated normalization. 
E$690.6 {I5} from weighted average of 692 {I2} (1978Ka10) and 690.5 {I5} (1978Fr21). 
RI$others: 0.23 {I1} (1978Fr21) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.016 {I11}, using the calculated normalization. 
RI$normalized to I|g(690.3|g)=0.2 {I1} based on I|g(705.43|g)/I|g(630.3|g)=17 {I3}/100 {I7} in Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.11 {I6}, using the calculated normalization. 
E$1317.1 {I2} (1978Ka10) 
E$weighted average of 1318 {I1} (1978Ka10) and 1317.1 {I2} (1977Ba57). 1977Ba57 place this |g ray from a level at E=1857.8 keV 
RI$others: 0.4 {I2} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$171 {I12} from |s=1.266 b {I19} in 2008Kr05 
$I(ce)(K)=166 {I17}, I(ce)(L1)=15.7 {I16}, I(ce)(L2)=9.21 {I92}, I(ce)(L3)=11.6 {I12}, I(ce)(M1)=2.97 {I30}, I(ce)(M2+M3)=4.16 {I42} (1980Ca02) 
M$|a(K)exp=0.56 {I8}, |a(L1)exp=0.053 {I8}, |a(L2)exp=0.031 {I4}, |a(L3)exp=0.039 {I6}, |a(M)exp=0.010 {I2} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
RI$13.9 {I12} from |s=0.103 b {I6} in 2008Kr05 
$I(ce)(K)=8.32 {I25}, I(ce)(L1)=0.809 {I81}, I(ce)(L2)=0.91 {I14}, I(ce)(L3)=0.76 {I12}, I(ce)(M)=0.363 {I73} (1980Ca02) 
M$|a(K)exp=0.50 {I5}, |a(L1)exp=0.049 {I7}, |a(L2)exp=0.055 {I9}, |a(L3)exp=0.046 {I8}, |a(M)exp=0.022 {I5} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$128 {I9} from |s=0.945 b {I15} in 2008Kr05 
$I(ce)(K)=1.54 {I5}, I(ce)(L1)=0.231 {I46} (1980Ca02) 
M$|a(K)exp=0.010 {I1}, |a(L1)exp=0.0015 {I3} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$74 {I5} from |s=0.549 b {I8} in 2008Kr05 
$I(ce)(K)=9.04 {I45}, I(ce)(L1)=0.952 {I95}, I(ce)(M)=0.190 {I32} (1980Ca02) 
M$|a(K)exp=0.095 {I10}, |a(L1)exp=0.010 {I2}, |a(M)exp=0.002 {I5} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$26.4 {I19} from |s=0.195 b {I4} in 2008Kr05 
$I(ce)(K)=1.10 {I3} (1980Ca02) 
M$|a(K)exp=0.040 {I4} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$28.6 {I22} from |s=0.212 b {I7} in 2008Kr05 
$I(ce)(K)=0.782 {I23} (1980Ca02) 
M$|a(K)exp=0.024 {I2} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$11.1 {I11} from |s=0.082 b {I6} in 2008Kr05 
$I(ce)(K)=4.7 {I7} I(ce)(L1)=0.73 {I15} (1980Ca02) 
M$|a(K)exp=0.29 {I5}, |a(L1)exp=0.044 {I10} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$56 {I4} from |s=0.413 b {I8} in 2008Kr05 
$I(ce)(K)=4.54 {I14}, I(ce)(L1)=0.432 {I86} (1980Ca02) 
M$|a(K)exp=0.063 {I6}, |a(L1)exp=0.006 {I1} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$53 {I4} from |s=0.393 b {I8} in 2008Kr05 
$I(ce)(K)=1.27 {I4}, I(ce)(L1)=0.24 {I12} (1980Ca02) 
M$|a(K)exp=0.021 {I2}, |a(L1)exp=0.004 {I2} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$27.6 {I21} from |s=0.204 b {I7} in 2008Kr05 
$I(ce)(K)=1.48 {I6}, I(ce)(L1)=0.235 {I71} (1980Ca02) 
M$|a(K)exp=0.044 {I5}, |a(L1)exp=0.007 {I2} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$106 {I7} from |s=0.786 b {I11} in 2008Kr05 
$I(ce)(K)=1.83 {I6}, I(ce)(L1)=0.244 {I41} (1980Ca02) 
M$|a(K)exp=0.015 {I1}, |a(L1)exp=0.002 {I1} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$41 {I3} from |s=0.300 b {I8} in 2008Kr05 
$I(ce)(K)=0.978 {I39} (1980Ca02) 
M$|a(K)exp=0.020 {I2} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$19.6 {I17} from |s=0.145 b {I8} in 2008Kr05 
$I(ce)(K)=15.0 {I23}, I(ce)(L1)=1.53 {I15}, I(ce)(L2)=0.49 {I19}, I(ce)(L3)=0.63 {I25}, I(ce)(M)=0.63 {I25} (1980Ca02) 
M$|a(K)exp=0.43 {I9}, |a(L1)exp=0.044 {I6}, |a(L2)exp=0.014 {I6}, |a(L3)exp=0.018 {I8}, |a(M)exp=0.018 {I8} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
RI$100 {I7} from |s=0.737 b {I11} in 2008Kr05 
$I(ce)(K)=0.570 {I57} (1980Ca02) 
M$|a(K)exp=0.005 {I1} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$8.1 {I11} from |s=0.060 b {I7} in 2008Kr05 
$I(ce)(K)=0.064 {I16} (1980Ca02) 
M$|a(K)exp=0.0055 {I20} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$20 {I6} from |s=0.15 b {I4} in 2008Kr05 
$I(ce)(K)=0.361 {I65} (1980Ca02) 
M$|a(K)exp=0.013 {I3} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$50 {I4} from |s=0.367 b {I11} in 2008Kr05 
$I(ce)(K)=0.383 {I31} (1980Ca02) 
M$|a(K)exp=0.0065 {I8} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$9.9 {I10} from |s=0.073 b {I5} in 2008Kr05 
$I(ce)(K)=0.49 {I10} (1980Ca02) 
M$|a(K)exp=0.041 {I10} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$20.9 {I18} from |s=0.155 b {I8} in 2008Kr05 
$I(ce)(K)=0.292 {I58} (1980Ca02) 
M$|a(K)exp=0.012 {I3} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$7.8 {I9} from |s=0.058 b {I5} in 2008Kr05 
$I(ce)(K)=0.261 {I26} (1980Ca02) 
M$|a(K)exp=0.039 {I5} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$17.3 {I16} from |s=0.128 b {I8} in 2008Kr05 
$I(ce)(K)=0.524 {I42} (1980Ca02) 
M$|a(K)exp=0.027 {I3} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$11.4 {I9} from |s=0.084 b {I3} in 2008Kr05 
$I(ce)(K)=0.402 {I60} (1980Ca02) 
M$|a(K)exp=0.030 {I5} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$61 {I4} from |s=0.453 b {I11} in 2008Kr05 
$I(ce)(K)=0.687 {I27} (1980Ca02) 
M$|a(K)exp=0.010 {I1} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
RI$9.7 {I10} from |s=0.072 b {I6} in 2008Kr05 
$I(ce)(K)=0.239 {I72} (1980Ca02) 
M$|a(K)exp=0.019 {I6} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$29.7 {I23} from |s=0.220 b {I9} in 2008Kr05 
$I(ce)(K)=0.897 {I27} (1980Ca02) 
M$|a(K)exp=0.014 {I1} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$1.4 {I3} from |s=0.010 b {I2} in 2008Kr05 
$I(ce)(K)=0.152 {I15} (1980Ca02) 
M$|a(K)exp=0.008 {I1} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$17.4 {I15} from |s=0.129 b {I7} in 2008Kr05 
$I(ce)(K)=0.273 {I19} (1980Ca02) 
M$|a(K)exp=0.013 {I2} (1980Ca02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$57 {I7} from |s=0.42 b {I4} in 2008Kr05 
E$weighted average of 4794.0 {I8} (1980Ca02) and 4793.79 {I24} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$16.4 {I19} from |s=0.121 b {I11} in 2008Kr05 
E$weighted average of 4920.3 {I8} (1980Ca02) and 4920.2 {I3} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$6.1 {I15} from |s=0.045 b {I11} in 2008Kr05 
E$weighted average of 5006.1 {I8} (1980Ca02) and 5006.3 {I5} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$7.3 {I16} from |s=0.054 b {I11} in 2008Kr05 
E$weighted average of 5018.9 {I8} (1980Ca02) and 5018.8 {I6} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$3.5 {I15} from |s=0.026 b {I11} in 2008Kr05 
E$weighted average of 5099.7 {I8} (1980Ca02) and 5100.1 {I6} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$31 {I3} from |s=0.231 b {I19} in 2008Kr05 
E$weighted average of 5211.8 {I8} (1980Ca02) and 5211.8 {I3} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$8.6 {I16} from |s=0.064 b {I11} in 2008Kr05 
E$weighted average of 5431.7 {I8} (1980Ca02) and 5432.0 {I5} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$7.4 {I13} from |s=0.055 b {I9} in 2008Kr05 
E$weighted average of 5480.3 {I8} (1980Ca02) and 5479.7 {I3} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$16.4 {I23} from |s=0.121 b {I15} in 2008Kr05 
E$weighted average of 5720.3 {I8} (1980Ca02) and 5719.4 {I3} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$16.4 {I19} from |s=0.121 b {I11} in 2008Kr05 
E$weighted average of 5828.6 {I8} (1980Ca02) and 5829.0 {I3} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$6 {I3} from |s=0.042 b {I19} in 2008Kr05 
E$weighted average of 5887.5 {I8} (1980Ca02) and 5887.2 {I7} (2008Kr05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E$weighted average of 188.9 {I1} (1969Sc12) and 189.1 {I3} (1967Na18). Other: 188 {I5} (1957St87). 
RI$deduced from I(|g+ce)=100 and |a=0.785 
M$|a(K)exp=0.52 {i4} (1964We09), 0.60 {i1} (1957St87) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
M$A{-2}=-0.214 {I37} using |g(|q) in 1969Ro05; |g|g(|q) in 1969Ro03 
MR$From |g|g(|q) in 1969Ro03. Other:-6.0 {I+15-16} (1989SvZZ) 
$E2 matrix element of 0.919 {I+12-35} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)=0.277 {I+1-13} from E2 matrix element of 1.579 {I+4-37} in 1989SvZZ and 0.31 {i4} in 1969Ro05 
M$A{-2}=0.36 {i7} and -0.31 {i11} from |g(|q) in 1962Ec01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$from E2 matrix element of 0.297 {I+13-3} in 1989SvZZ and 0.115 {i20} 0.115 {i20} from Coulomb excitation in 1969Ro05 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$B(E2)=0.237 {I+8-41} from matrix element of 1.09 {I+2-10} if |d(841|g)=1.2 B(E2)=0.189 {I+11-18} from matrix element of 0.97 {I+3-5} if |d(841|g)=-0.21 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$B(E2)=0.0038 {I+6-5} from matrix element of -0.138 if |d=1.2 B(E2)=0.00029 {I+8-25} from matrix element of -0.038 {I+23-5} if |d=-0.21. Origin of |d value not given by 1989SvZZ 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$B(E2)=0.099 {I+8-10} from E2 matrix element of -0.94 {I+8-10} if |d(477)=11 B(E2)=0.064 {I+24-2} from E2 matrix element of -0.76 {I+1-14} if |d(477)=-1.3 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$B(E2)=0.36 {I+5-3} from E2 matrix element of 1.81 {I+11-8} if |d(841|g)=1.2 B(E2)=0.44 {I2} from E2 matrix element of 1.98 {I4} if |d(841|g)=-0.21 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
$B(E2)=0.00084 {I+19-25} from E2 matrix element of -0.065 {I+11-7} if |d(477|g)=11, B(E2)=0.0020 {I+8-2} from E2 matrix element of -0.100 {I+4-19} if |d(477|g)=-1.3 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$B(E2)=0.37 {I+4-8} from E2 matrix element of 2.20 {I+11-24} if |d(841|g)=1.2 B(E2)=0.30 {I+2-4} from E2 matrix element of 1.97 {I+7-15} if |d(841|g)=-0.21 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From 1988Ay02, the conversion electrons were measured but the value of |a(exp) was not given by the authors 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From adopted gammas 
RI$The authors give 100 {i38} (1999Lh01), but the quoted uncertainty may be a typo 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
M$based on |a(exp)=1.32 {I14} I|g(172|g)/I|b(2170|b): 1965Na01, scin; mult=E3 with <2% M4 (1969Be11) from |a(K)exp based on K| x ray/|g. 1969Be11 do not give the |a(K)exp explicitly. 
E$from 1977Kr14. Others: 172.2 {I5} (1969Be11), 172.0 {I1} (1969Sc12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
RI$relative to 100 for 694.088-keV |g ray in {+111}Ag from |b{+-} decay of 5.563-h {+111}Pd. Absolute intensity=35.4% {I5} (2015Kr07) 
M$From {+111}Pd Adopted dataset in the ENSDF database 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_comment:
M$A{-2}=0.08 {I4}; A{-4}=0.28 {I5}, gated on 388.0|g and 348.8|g in {+252}Cf SF decay (1999Bu32); A{-22}=0.089 {I34} gated on 348.7|g and 388.0|g in 1999Lh01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.14 {I2}; A{-4}=-0.01 {I2}, gated on 534.3|g and 348.8|g in {+252}Cf SF (1999Bu32); A{-22}=0.105 {I34} gated on 348.7|g and 534.3|g in 1999Lh01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.16 {I7}; A{-4}=-0.06 {I8}, gated on 359.4|g and 736.8|g in {+252}Cf SF (1999Bu32); A{-22}=0.041 {I35} gated on 348.7|g and 359.6|g in 1999Lh01 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
E$from {+110}Pd(t,p|g) 
M$from I(E0,K)/I(tot)>58|*10{+6} (1987Es01) and I(ce(K) 1125)/I|g(777|g)=1.26|*10{+-4} in 110Pd(t,p|g) (1987Es01,1986HeZT) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.13 {I2}; A{-4}=-0.03 {I3}, gated on 667.3|g and 534.3 in {+252}Cf SF (1999Bu32); A{-22}=0.097 {I45} gated on 348.7|g and 667.5|g in {+112}Rh |b{+-} decay (6.76 s) (1999Lh01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$A{-2}=0.07 {I5}; A{-4}=0.03 {I6}, gated on 1098.6|g and 359.4|g in {+252}Cf SF (1999Bu32); A{-22}=0.014 {I40} gated on 359.6|g and 1098.3|g in {+112}Rh |b{+-} decay (6.76 s) (1999Lh01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$A{-22}=-0.105 {I89} gated on 359.6|g and 1658.5|g in 1999Lh01 would suggest D, but the level scheme requires |DJ=2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
M$Based on ce measurements (1987Es01,1986HeZT). 
I(E0,K)/I(tot)>58|*10{+6} (1987Es01). I(ce(K) 1125)/I|g(777|g)=1.26|*10{+-4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_comment:
RI$From adopted gammas using I|g(747.6|g)/I|g(359.6|g)=0.79 {I10} 
M$A{-22}=-0.485 {I47} gated on 348.7|g and 747.6|g in 1999Lh01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$New placement (7/2- to 5/2+) compared to that proposed (11/2- to 9/2-) in 2009Fo09 (Phys. Rev. C 72, 014315). 
M$From |a(K)exp=0.12 {I3} in 1993Pe11 (Nucl. Phys. A561, 416). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$placement in Table III of 2014Ku28, absent in authors' level scheme Fig. 10. 
E$poor fit, level-energy difference=159.65 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$new placement (7/2- to 5/2+) compared to that proposed (11/2- to 9/2-) in 2009Fo09 (Phys. Rev. C 72, 014315). 
M$From |a(K)exp=0.12 {i3} in 1993Pe11 (Nucl. Phys. A561, 416). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$(362.1|g)(332.8|g)(|q): A{-2}=-0.038 {I6}, A{-4}=+0.31 {I1} consistent with cascade of |DJ=0, quadrupole and |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$(520.1|g)(332.8|g)(|q): A{-2}=0.102 {I4}, A{-4}=+0.013 {I6} consistent with cascade of |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$(679.3|g)(332.8|g)(|q): A{-2}=-0.372 {I8}, A{-4}=-0.098 {I11} consistent with cascade of |DJ=1, quadrupole and |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$(1331.7|g)[520.1|g](332.8|g)(|q): A{-2}=-0.067 {I15}, A{-4}=-0.004 {I23} consistent with cascade of |DJ=1, dipole and |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$(1098.0|g)[648.4|g][520.1|g](332.8|g)(|q): A{-2}=-0.069 {I10}, A{-4}=+0.035 {I15} consistent with cascade of |DJ=1, dipole and |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$(1288.8|g)(648.4|g)(|q): A{-2}=-0.079 {I16}, A{-4}=-0.032 {I24} consistent with cascade of |DJ=1, dipole and |DJ=2, quadrupole transitions 
M$(1288.8|g)[648.4|g](520.1|g)(|q): A{-2}=-0.069 {I16}, A{-4}=-0.024 {I29} consistent with cascade of |DJ=1, dipole and |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$(1022.2|g)[715.5|g][648.4|g](520.1|g)(|q): A{-2}=-0.059 {I36}, A{-4}=-0.019 {I55} consistent with cascade of |DJ=1, dipole and |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$(619.2|g)(317.2|g)(|q): A{-2}=+0.021 {I7}, A{-4}=+0.010 {I10} consistent with |DJ=2, E2 -> |DJ=1, E2 cascade (2016Hu16). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$(627.2|g)(317.2|g)(|q): A{-2}=+0.012 {I83}, A{-4}=+0.12 {I13} consistent with |DJ=1, E2 -> |DJ=1, E2 cascade (2016Hu16). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
$B(E2)=0.174 {I7} and B(E2)(W.u.)=53 {I2} (2019Ga29), for mean lifetime |t=113 ps {I5}, a recommended value as confirmed by the corresponding author of 2019Ga29 in e-mail reply of March 19, 2020 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
$B(E2)=0.140 {I73}, B(E2)(W.u.)=43 {I27} (2019Ga29) for |t=21 ps {I11}. Authors have taken the average of upper and lower limits, as confirmed by the corresponding author of 2019Ga29 in e-mail reply of March 19, 2020 
$Compiler obtains B(E2)=0.102 {I+112-35} and B(E2)(W.u.)=31 {I+34-11}. Symmetrizing these results gives nearly the same result as in authors' Table II 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_uncertain: ?
decay_comment:
E$From text of 2004Ur04; not shown in authors' figure 2. now for 2005Fo09, this |g is deexisting a 127.9 level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E1
decay_comment:
M$M2 multipolarity for this |g-ray is unlikely, considering the prompt character of this transition. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: Q
decay_comment:
M$(488.9|g)(340.5|g)(|q): A{-2}=+0.128 {I27}, A{-4}=+0.016 {I42} consistent with cascade of |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: Q
decay_comment:
M$(579.9|g)(394.7|g)(|q): A{-2}=+0.097 {I15}, A{-4}=+0.045 {I23} consistent with cascade of |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: Q
decay_comment:
M$(642.8|g)(530.5|g)(|q): A{-2}=+0.068 {I48}, A{-4}=+0.036 {I75} consistent with cascade of |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: Q
decay_comment:
M$(743.4|g)(394.7|g)(|q): A{-2}=+0.080 {I18}, A{-4}=+0.036 {I27} consistent with cascade of |DJ=2, quadrupole transitions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$(1105.8|g)(537.6|g)(|q): A{-2}=-0.064 {I12}, A{-4}=-0.005 {I18} consistent with |DJ=1, dipole and |DJ=2, quadrupole cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$352.7 listed in Table 3 of 2013Lu18 is incorrect, correct energy is 382.3, as in Erratum to 2013Lu18 in Nucl. Phys. A983, 321 (2019) 
RI$7.8 in 2013Lu18 is incorrect, correct value is <15 as in Erratum to 2013Lu18 in Nucl. Phys. A983, 321 (2019) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$(877.0|g)(681.7|g)(|q): A{-2}=-0.078 {I16}, A{-4}=+0.025 {I25} consistent with |DJ=1, dipole and |DJ=2, quadrupole cascade 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$(1095.9|g)(681.7|g)(|q): A{-2}=-0.090 {I43}, A{-4}=+0.013 {I67} consistent with |DJ=1, dipole and |DJ=2, quadrupole cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
MR$from {+117}Pd Adopted dataset in the ENSDF database, based on conversion electron data in 1991Pe10 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
M$E2 is not possible as it would give large negative intensity imbalance at the 207.7 level, and also would violate RUL for E2 transitions, assuming the 225.4 level is short-lived. A third argument for mult=M1 comes from the requirement of an intensity balance at the 207.69 level, which gives |d<0.09. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Ordering of the 412.5|g |) 539.3|g cascade in {+252}Cf SF decay (2013Lu18) is determined from the intensity of the 539.3|g as 18% {I3} stronger than that of the 412.5|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Ordering of the 412.5|g |) 539.3|g cascade in 2013Lu18 is determined from the intensity of the 539.3|g as 18% {I3} stronger than that of the 412.5|g. This ordering is given in the Adopted dataset 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$E|g=821.5 (2001Zh05) 
M$(821.4|g)(718.3|g)(|q): A{-2}=+0.15 {I10}, A{-4}=+0.13 {I15} consistent with cascades of |DJ=2, quadrupole transitions. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$tentative placement; no (438|g)(618|g) evidence observed, but |g near this energy confirmed by 2007St19 and 2013Wa28 in reaction based |g-ray spectroscopy 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Order of 757|g and 825|g based on comparison to level energies in {+126}Pd, however, possibility of reversing the ordering cannot be ruled out. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E3]
decay_comment:
$The 297-keV |g peak is seen in coincidence with conversion electrons for the 86-keV transition, and with other |g rays such as 693|g in {+126}Pd and 598|g in {+126}Ag 


decay_energy_unit: KEV
decay_multipolarity: (M1)
decay_comment:
M$from shell-model it is expected |D|p=0. The experimental value for |g(77.4)/I|g(255.8)=15 {I8}/12 {I6}=1.25 {I91} favors M1 assignment since this ratio will be equal to 0.638 for M1 and equal to 0.259 for E2. 


decay_energy_unit: KEV
decay_multipolarity: (E3)
decay_comment:
M$supported by shell-model calculations and by the fact that B(E3)(W.u.)>0.039 if Mult.=(E3), B(E2)(W.u.)>2.7|*10{+-8} if Mult.=(E2) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$expected from shell-model; also, because I|g(163.8) is very similar to I|g(427.8), transition can only be dipole. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$expected from shell-model, also, because I|g(163.8) is very similar to I|g(427.8), transition can only be dipole. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$expected from shell-model; also, because I|g(158.8) is about 73 % of I|g(1294.5), transition can only be dipole or E2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E,RI$From 2017Pa35. 
M$From |a{-T}=33 {I6} in 2017Pa35, based on intensity balances 
$B(E2)(W.u.)=3.00 {I10} (by compilers) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$98 keV reported in 2017Pa35 
RI$From reported I(|g+ce) in 2017Pa35 and |a (by compilers) 
$B(E2)(W.u.)=4.8 {I16} (by compilers) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E4)
decay_comment:
E$4265 keV reported in 2017Pa35 
RI$From reported I(|g+ce) in 2017Pa35 and |a (by compilers) 
$B(E4)(W.u.)=0.8 {I4} (by compilers) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$Value has been corrected by 2019Pa16 to include conversion assuming M1 multipolarity. 
RI$I|g{-rel}=100 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
$DCO is for 289.4 doublet 
$Placements and intensity division from 1998Ce03 
RI$other: 100 {I30} for doublet (1995Sc50) 
$Total I|g(289|g)=75 (1998Ce03), 100 {I30} (1995Sc50) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M,MR$from |a(K)exp. Note that Mult=M1+E2 with |d(E2/M1)=0.27 {I8} deduced from |a(K)exp=1.80 {I4} would give a larger |a{-T}=2.23, resulting in a total (|g+ce) intensity much greater than that of 107|g, which is expected to be equal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
M |a(K)exp=0.7 {I4}, K/L=2.6 {I3} (1988BaZS); |a(K)exp=1.5 {I3}; K/L=2.5 {I3} (1981Hu03); |a(K)exp=3.8 {I20} (1980Ka05); |a(exp)=1.75 {I22} from I(|g+ce) balance 
RI I|g=39 from I(|g+ce)=100. Other: 30 {I2} (1982Ku15). This value is too small since it requires |a=2.4 {I2}, |d=0.18 {I3} to fulfill intensity balance. 
MR <0.002 if B(M4)(W.u.)<30 (RUL). |d=0.08+4-8 if I|g=37 {I3}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From |a(K)exp=0.47 {I5} in IT decay, 0.56 {I9} in |e decay and K/L=6.0 {I3} in |e decay. K/LM=3.9 in IT decay is discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$From intensity balance at the 750 level, |a|<1.8, Compared with theory of 1.44 for E1, 3.44 for M1, this suggests E1, The author suggest |p(750)=-, which requires mult=M1,so d is adopted 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E member of complex multiplet together with 555.1|g and {+101,102}Pd impurities at almost the same energy 


decay_energy_unit: KEV
decay_multipolarity: (M3)
decay_uncertain: S
decay_comment:
E the energy of this unobserved transition is deduced from energy differences of |g-rays observed in the {+102}Cd |e decay (1970Hn02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
$|a(K)(M1)=0.00585 {I9}; |a(K)(E2)=0.00610 {I9} 
$|a(L)(M1)=0.000694 {I10}; |a(L)(E2)=0.000791 {I12} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
R(dcom)=0.58 {i2} 
R(DCOQ)=0.91 {i11} 
$A{-22}=+0.54 {i3}; a{-44}=+0.07 {i4}; Pol=-0.52 {i9} 
MR$Other: |d|>-1.7 or |<-0.7 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1
decay_comment:
M$d from a{-22}, a{-44} and M1 from observed band structure 
$A{-22}=-0.33 {I9}; a{-44}=-0.01 {I10} 
MR$Other: |d|>-0.14 or |<0.18 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
R(dcom)=1.26 {I20} 
M from R(DCO) in {+89}y({+16}O,3n) 
$A{-22}=-0.09 {I3}; a{-44}=-0.10 {I4} 
MR$Other: |d|>-1.7 or |<-0.7 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
R(dcom)=0.98 {i10} 
R(DCOQ)=2.04 {i24} 
M from |a(K)exp and R(DCO) in {+89}y({+16}O,3n) 
$A{-22}=-0.10 {i5}; a{-44}=-0.04 {i6}; Pol=-0.17 {i21} 
MR$Other: |d=0|?(1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
R(dcom)=1.12 {i14} 
R(DCOQ)=1.61 {i21} 
M from |a(K)exp and R(DCO) in {+89}y({+16}O,3n) 
$A{-22}=-0.25 {i3}; a{-44}=-0.04 {i3} 
M$Other: M1(+E2) (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1
decay_comment:
R(dcom)=0.31 {i4} 
R(DCOQ)=0.68 {i22} 
$A{-22}=-0.22 {i4}; a{-44}=-0.03 {i5}; Pol=-0.33 {i10} 
MR$Other: |d|>-0.08 or |<+0.08 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
R(dcom)=0.59 {i5} 
$A{-22}=+0.55 {i5}; a{-44}=-0.04 {i6}; Pol=-0.52 {i9} 
MR$Other: |d|>-1.7 or |<+0.08 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
R(dcom)=0.92 {i16} 
$A{-22}=-0.10 {i3}; a{-44}=-0.05 {i4}; Pol=-0.06 {i4} 
M$No |d given in (HI,xn|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
R(dcom)=1.58 {i27} 
R(DCOQ)=1.35 {i22} 
$A{-22}=-0.24 {i10}; a{-44}=-0.03 {i13}; Pol=-0.94 {i12} 
MR$Other: |d|>-0.08 or |<+0.360.7 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
R(dcom)=1.26 {i20} 
$A{-22}=-0.24 {i4}; a{-44}=-0.03 {i4}; Pol=-0.29 {i7} 
MR$Other: |d|>-0.08or |<+0.08 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$A{-22}=-0.30 {i3}; a{-44}=-0.02 {i3}; Pol=+0.33 {i9} 
R(dcom)=1.07 {i13} 
MR$|d|>0 or |<+0.05 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
R(dcom)=1.06 {i10} 
R(DCOQ)=2.50 {i40} 
M$d from R(DCO) in {+89}y({+16}O,3n) and (E2) from a{-22}=+0.25 {I2}; a{-44}=-0.12 {I3}; Pol=+0.36 {I5} (1983Tr01) From observed band structure E1 is most likely 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
R(dcom)=0.98 {i4} 
$A{-22}=-0.09 {i4}; a{-44}=-0.03 {i3}; Pol=-0.32 {i4} 
MR$Other: |d|>0 or |<+0.12 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
Observed in {+89}y({+16}O,3n) as an unresolved multiplet also containing impurities due to {+101}Pd and {+102}Pd. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
R(dcom)=1.08 {i4} 
R(DCOQ)=2.38 {i45} 
$A{-22}=-0.18 {i4}; a{-44}=-0.07 {i4}; Pol=-0.29 {i6} 
MR$Other: |d|>-0.08 or |<-0.08 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1
decay_comment:
R(dcom)=1.06 {i10} 
R(DCOQ)=1.72 {i21} 
$A{-22}=-0.12 {i3}; a{-44}=-0.01 {i4}; Pol=-0.28 {i5} 
M$Other: M1,E2 (1983Tr01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
R(dcom)=1.19 {i5} 
R(DCOQ)=2.70 {i29} 
$A{-22}=-0.24 {i3}; a{-44}=-0.02 {i3}; Pol=-0.32 {i5} 
$A{-22} and a{-44}for unresolved doublet 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
R(dcom)=1.01 {I7} 
E I|g is not reliable because 554.8 is a member of a complex multiplet together with 555.1|g and {+101,102}Pd impurities of almost the same energy 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1
decay_comment:
R(dcom)=1.19 {i5} 
R(DCOQ)=2.70 {i29} 
$A{-22}=-0.24 {i3}; a{-44}=-0.02 {i3}; Pol=-0.32 {i5} 
$Pol is for unresolved multiplet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M from |a(K)exp. If J|p's of 590 and 134 keV levels are correct M1 is excluded 
$|a(K)exp=0.0074 {I11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M from |a(K)exp. M1 excluded if J|p=7/2+. If J|p's of 590 and 1311 keV levels are correct M1 is excluded 
$|a(K)exp=0.0025 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$(E1) from {+72}Ge({+35}Cl,2p2n|g) 
M$M1+E2 from {+94}Mo({+12}C,2np|g) but more evidence for (E1) from DCO value 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$From {+94}Mo({+12}C,2np|g). Other: 32.8 {I21} ({+76}Ge({+35}Cl,|a4n|g)) 
M from 839|g(|q) and linear pol 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from 1980Lu07, based on conversion electron measurements. No |d given. DCO also compatible with M1+E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
Composite line. E1,E2 is given as multipolarity in {+94}Mo({+12}C,2np) (1980Tr05) but 3599 level is band member of |DJ=1 band on 21/2- 3439 keV level, so E2 is excluded 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
$A{-2}=-0.02{I5}; A{-4}=-0.04 {I6}; Pol=0.49 {I13} 
Composite line. E1,E2 is given as multipolarity by 1980Tr05. If 3599 level is band member of |DJ=1 band on 21/2- 3439 keV level, E2 is excluded 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=-0.21{I6}; A{-4}=+0.10 {I8}; Pol=-0.39 {I10} 
Composite line. M1+E2 is given with |d=+0.03 {I6} in ({+12}C,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=-0.21{I6}; A{-4}=+0.10 {I8}; Pol=-0.39 {I10} 
Composite line. M1+E2 given with |d=+0.03 {I6} in ({+12}C,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=-0.02{I5}; A{-4}=-0.04 {I17}; Pol=0.49 {I13} 
Composite line. E1,E2 given as multipolarity in ({+12}C,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Positive parities for initial and final levels as listed in table i of 2004Da14 seem to be misprints. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_BE_unit: e^2 x (fm)^6
decay_BE_info: ;TYPE=BE3;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE3W
decay_comment:
E$weighted average of 25.53~{I3} (1978Sh08) and 25.47~{I1} (1976Sv04); Others:|?25 (1969Ho36) 
M$from |a(L1)exp:|a(L2)exp:|a(L3)exp=0.002<:1:1.47~{I4} and |a(L)exp:|a(M)exp:|a(N)exp=1:0.22~{I2}:0.09~{I2} in 1978Sh08; Other: 1953Jo20 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$from the intensity balance in {+105}Cd |e decay, assu 
MR$from Ice(M1)/(Ice(M2)+Ice(M3))= (100~{I5})/(22~{I3}) in 1976Sv04, and M1+25% E2 in 1976Ja05; 
CC$Other: 46~{I7} from I|g balance leading to |d=0.51~{I7} and unreasonably high B(E2)(W.u.)=2200 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.12~{I4}, A{-4}=0.03~{I5} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.08~{I9}, A{-4}=0.18~{I14} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-31~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=-0.92~{I52}, P{-a.d.}=-0.12~{I15} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.014~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); Other: 0.0|<|d|<0.30 in {+103}Rh(|a,2n|g) (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
MR$from |g linear pol measurement in {+103}Rh(|a,2n|g) (1979KeZW); Other: 0.0|>|d|>-1.0 in {+103}Rh(|a,2n|g) (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.20~{I2}, A{-4}=-0.11~{I3} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.19~{I2}, A{-4}=-0.02~{I3} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=32~{I3} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.92~{I11}, P{-a.d.}=0.30~{I4} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.0079~{I24} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.31~{I1}, A{-4}=0.04~{I1} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.25~{I2}, A{-4}=0.03~{I2} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-56~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=-0.50~{I9}, P{-a.d.}=-0.50~{I9} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.0039~{I12} (1979Ka05); 0.34|<|d |< 0.40 in {+103}Rh(|a,2n|g) (1985Ke09); Others: +0.35~{I4} (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.34~{I5}, A{-4}=0.12~{I7} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.11~{I11}, A{-4}=-0.03~{I18} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=57~{I13} in {+103}Rh(|a,2n|g) (1979Ka05); 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.11~{I1}, A{-4}=-0.03~{I2} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.10~{I1}, A{-4}=-0.02~{I2} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-30~{I4} in {+103}Rh(|a,2n|g) (1979Ka05) P{-c.p.}=-0.41~{I13}, P{-a.d.}=-0.38~{I2} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.030~{I9} in {+103}Rh(|a,2n|g) (1979Ka05); Other: 0.07|<|d |< 0.09 in {+103}Rh(|a,2n|g) (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.29~{I2}, A{-4}=-0.13~{I2} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.31~{I2}, A{-4}=-0.09~{I3} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=60~{I5} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.43~{I13}, P{-a.d.}=0.50~{I5} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.0012~{I4} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=-0.62~{I31}, A{-4}=-0.46~{I34} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.43~{I22}, A{-4}=0.09~{I36} in {+103}Rh(|a,2n|g) (1985Ke09); 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$A{-2}=0.27~{I5}, A{-4}=-0.13~{I7} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.26~{I3}, A{-4}=-0.09~{I5} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=50~{I17} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.35~{I17}, P{-a.d.}=0.40~{I7} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.0018~{I6} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.69~{I5}, A{-4}=0.23~{I7} in {+103}Rh(|a,2n|g) (1979Ka05); P{-exp}=-92~{I24} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.19~{I3}, A{-4}=0.04~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.21~{I2}, A{-4}=-0.01~{I3} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-49~{I6} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=-0.46~{I16}, P{-a.d.}=-0.57~{I5} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.0020~{I6} (1979Ka05); Other: 0.27|<|d|<0.33 in {+103}Rh(|a,2n|g) (1985Ke09); Other: +0.25~{I4} in {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.28~{I8}, A{-4}=-0.25~{I11} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.27~{I7}, A{-4}=-0.20~{I10} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=59~{I8} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.44~{I30}, P{-a.d.}=0.35~{I16} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.00065~{I22} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=-0.92~{I6}, A{-4}=0.10~{I6} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.76~{I5}, A{-4}=0.13~{I7} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=18~{I5} in {+103}Rh(|a,2n|g) (1979Ka05) P{-c.p.}=0.16~{I9}, P{-a.d.}=0.09~{I6} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.0016~{I5} (1979Ka05); Other: -0.35|>|d|>-1.10 in {+103}Rh(|a,2n|g) (1985Ke09); -1.01~{I17} in {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$A{-2}=0.36~{I4}, A{-4}=-0.05~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.32~{I3}, A{-4}=-0.09~{I4} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=46~{I7} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.37~{I17}, P{-a.d.}=0.53~{I8} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.00059~{I19} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.094~{I53}; A{-44}=0.017~{I70} in {+92}Zr({+16}O,p2n|g) (1979Po13); R{-DCO}=0.72~{I12} in {+100}Mo({+10}B,5n|g) (2007Ti07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.322~{I32}; A{-44}=-0.15~{I5} in {+92}Zr({+16}O,p2n|g) (1979Po13); R{-DCO}=0.65 {I6} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12); R{-DCO}=1.00~{I9} in {+100}Mo({+10}B,5n|g) (2007Ti07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.01~{I5}, A{-4}=0.05~{I7} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.14~{I20}, A{-4}=0.14~{I36} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-19~{I6} in {+103}Rh(|a,2n|g) (1979Ka05) 
MR$|a(K)exp=0.015~{I5} in {+103}Rh(|a,2n|g) (1979Ka05); Other: -7~{I5} in {+103}Rh(|a,2n|g) (1979KeZW); +0.09~{I5} in {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.30~{I2}, A{-4}=-0.10~{I2} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.34~{I3}, A{-4}=-0.08~{I4} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=46~{I8} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.58~{I17}, P{-a.d.}=0.57~{I7} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.00058~{I18} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.24~{I4}, A{-4}=-0.10~{I6} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.24~{I2}, A{-4}=0.05~{I4} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=30~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.32~{I15}, P{-a.d.}=-0.29~{I4} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.0012~{I5} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.77~{I3}, A{-4}=0.44~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.78~{I3}, A{-4}=0.18~{I5} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=27~{I6} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.87~{I63}, P{-a.d.}=0.20~{I4} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.026~{I8} in {+103}Rh(|a,2n|g) (1979Ka05); Other: -2.3|<|d|<-1.8 in {+103}Rh(|a,2n|g) (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.37~{I4}, A{-4}=-0.07~{I6} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.30~{I3}, A{-4}=-0.10~{I5} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=83~{I7} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.56~{I14}, P{-a.d.}=0.48~{I8} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.0031~{I10} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.31~{I3}, A{-4}=-0.07~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.23~{I4}, A{-4}=0.04~{I6} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=10~{I9} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.3~{I4}, P{-a.d.}=-0.30~{I7} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.00015~{I7} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.24~{I2}, A{-4}=0.03~{I3} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.29~{I3}, A{-4}=-0.05~{I5} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=10~{I6} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.2~{I2}, P{-a.d.}=-0.41~{I6} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$|a(K)exp=0.00014~{I6} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.23~{I1}; A{-4}=-0.02~{I2} in {+103}Rh(|a,2n|g) (1979Ka05) A{-2}=-0.21~{I3}, A{-4}=0.09~{I5} in {+103}Rh(|a,2n|g) (1985Ke09); P{-a.d.}=-0.39~{I6} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$Other: 0.0|<|d|<0.04 in {+103}Rh(|a,2n|g) (1985Ke09); -0.12~{I5} {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.09~{I9}; A{-4}=0.00~{I6} in {+103}Rh(|a,2n|g) (1979Ka05) A{-2}=-0.13~{I3}, A{-4}=0.03~{I5} in {+103}Rh(|a,2n|g) (1985Ke09); P{-a.d.}=-0.37~{I5} in {+103}Rh(|a,2n|g) (1985Ke09); 
MR$Other: 0.02|<|d|<0.09 in {+103}Rh(|a,2n|g) (1985Ke09), and -0.12~{I5} {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.22~{I30}, A{-4}=-0.02~{I34} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.17~{I7}, A{-4}=0.18~{I11} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=66~{I12} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.64~{I27}, P{-a.d.}=-0.12~{I11} in {+103}Rh(|a,2n|g) (1985Ke09); 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.17~{I1}; A{-4}=0.00~{I1} in {+103}Rh(|a,2n|g) (1979Ka05) A{-2}=-0.17~{I2}, A{-4}=0.05~{I2} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-0.68~{I35}, P{-a.d.}=-0.41~{I4} in {+103}Rh(|a,2n|g) (1985Ke09); R{-DCO}=0.56~{I6} in {+100}Mo({+10}B,5n|g) (2007Ti07) 
MR$Other: 0.02|<|d|<0.08 in {+103}Rh(|a,2n|g) (1985Ke09); +0.04~{I1} {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.23~{I6}, A{-4}=-0.09~{I8} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=0.37~{I6}, A{-4}=0.01~{I9} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-80~{I9} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=-0.84~{I35}, P{-a.d.}=-0.81~{I15} in {+103}Rh(|a,2n|g) (1985Ke09); R{-DCO}=0.67~{I17} in {+100}Mo({+10}B,5n|g) (2007Ti07) 
MR$|a(K)exp=0.0059~{I19} in {+103}Rh(|a,2n|g) (1979Ka05); Other: 0.30|<|d|<0.44 in {+103}Rh(|a,2n|g) (1985Ke09); +0.26~{I4} in {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-2}=-0.18~{I11}, A{-4}=-0.04~{I16} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.16~{I3}, A{-4}=-0.09~{I5} in {+103}Rh(|a,2n|g) (1985Ke09); R{-DCO}=0.95~{I14} in {+100}Mo({+10}B,5n|g) (2007Ti07) +0.06~{I1} in {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.18~{I7}, A{-4}=-0.09~{I11} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=29~{I14} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=0.2~{I5}, P{-a.d.}=-0.44~{I12} in {+103}Rh(|a,2n|g) (1985Ke09); R{-DCO}=0.57~{I17} in {+100}Mo({+10}B,5n|g) (2007Ti07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.16~{I1}, A{-4}=0.00~{I1} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.14~{I2}, A{-4}=-0.07~{I2} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-39~{I11} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=-0.38~{I27}, P{-a.d.}=-0.47~{I3} in {+103}Rh(|a,2n|g) (1985Ke09); R{-DCO}=0.62~{I7} in {+100}Mo({+10}B,5n|g) (2007Ti07) R{-DCO}=0.99~{I2} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) 
MR$others: 0.05|<|d|<0.08 in {+103}Rh(|a,2n|g) (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-2}=-0.25~{I2}, A{-4}=-0.02~{I3} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.23~{I2}, A{-4}=-0.01~{I2} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-0.37~{I33}, P{-a.d.}=-0.36~{I3} in {+103}Rh(|a,2n|g) (1985Ke09); R{-DCO}=0.62~{I7} in {+100}Mo({+10}B,5n|g) (2007Ti07) 
MR$others: 0.0|<|d|<0.03 in {+103}Rh(|a,2n|g) (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.44~{I16}, A{-4}=-0.03~{I21} in {+103}Rh(|a,2n|g) (1979Ka05); R{-DCO}=1.05~{I19} in {+100}Mo({+10}B,5n|g) (2007Ti07) P{-exp}=70~{I18} in {+103}Rh(|a,2n|g) (1979Ka05) 
MR$|a(K)exp=0.00038~{I14} in {+103}Rh(|a,2n|g) (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-2}=-0.17~{I1}, A{-4}=-0.03~{I2} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.14~{I2}, A{-4}=-0.04~{I3} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-25~{I5} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=-0.35~{I26}, P{-a.d.}=-0.45~{I3} in {+103}Rh(|a,2n|g) (1985Ke09); R{-DCO}=0.52~{I5} in {+100}Mo({+10}B,5n|g) (2007Ti07) 
MR$|a(K)exp=0.039~{I12} in {+103}Rh(|a,2n|g) (1979Ka05); Other: 0.04|<|d|<0.07 in {+103}Rh(|a,2n|g) (1985Ke09); +0.05~{I1} in {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-2}=-0.20~{I2}, A{-4}=0.00~{I3} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.21~{I2}, A{-4}=-0.07~{I3} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-30~{I8} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=-0.46~{I35}, P{-a.d.}=-0.45~{I3} in {+103}Rh(|a,2n|g) (1985Ke09); R{-DCO}=0.52~{I6} in {+100}Mo({+10}B,5n|g) (2007Ti07) 
MR$|a(K)exp=0.027~{I9} in {+103}Rh(|a,2n|g) (1979Ka05); Other: 0.01|<|d|<0.04 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.18~{I11}, A{-4}=-0.04~{I16} in {+103}Rh(|a,2n|g) (1979Ka05) R{-DCO}=1.02~{I8} in {+100}Mo({+10}B,5n|g) (2007Ti07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=-0.19~{I3}, A{-4}=0.10~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.16~{I5}, A{-4}=-0.03~{I7} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-40~{I5} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=-0.40~{I28}, P{-a.d.}=-0.39~{I8} in {+103}Rh(|a,2n|g) (1985Ke09); R{-DCO}=1.01~{I5} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) R{-DCO}=0.57~{I6} {+100}Mo({+10}B,5n|g) (2007Ti07) 
MR$|a(K)exp=0.012~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); Other: 0.02|<|d|<0.08 in {+103}Rh(|a,2n|g) (1985Ke09); +0.085~{I10} in {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$A{-22}=-0.105~{I14}; A{-44}=-0.009~{I19} in {+92}Zr({+16}O,p2n|g) (1979Po13) R{-DCO}=1.1~{I3} in {+100}Mo({+10}B,5n|g) (2007Ti07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=0.01~{I14}, A{-4}=0.05~{I16} in {+103}Rh(|a,2n|g) (1979Ka05); A{-2}=-0.05~{I6}, A{-4}=-0.16~{I11} in {+103}Rh(|a,2n|g) (1985Ke09); P{-exp}=-65~{I12} in {+103}Rh(|a,2n|g) (1979Ka05); P{-c.p.}=-0.73~{I35}, P{-a.d.}=-0.65~{I12} in {+103}Rh(|a,2n|g) (1985Ke09); R{-DCO}=0.60~{I5} in {+100}Mo({+10}B,5n|g) (2007Ti07) 
MR$|a(K)exp=0.011~{I4} in {+103}Rh(|a,2n|g) (1979Ka05); Other: 0.08|<|d|<0.15 in {+103}Rh(|a,2n|g) (1985Ke09); +0.06~{I2} in {+92}Zr({+16}O,p2n|g) (1979Po13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.49~{I6} in {+100}Mo({+10}B,5n|g) (2007Ti07); R{-DCO}=1.05~{I4} or 0.54~{I3} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.52~{I6} in {+100}Mo({+10}B,5n|g) (2007Ti07); R{-DCO}=0.99~{I4} or 0.51~{I14} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$R{-DCO}=0.93~{I16} in {+100}Mo({+10}B,5n|g) (2007Ti07); 
M$R{-DCO}=0.54~{I17} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.50~{I6} in {+100}Mo({+10}B,5n|g) (2007Ti07); R{-DCO}=1.00~{I7} or 0.42~{I16} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.47~{I8} in {+100}Mo({+10}B,5n|g) (2007Ti07); R{-DCO}=1.10~{I8} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$R{-DCO}=1.79~{I25} in {+100}Mo({+10}B,5n|g) (2007Ti07); 
M$R{-DCO}=0.64~{I17} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.48~{I5} in {+100}Mo({+10}B,5n|g) (2007Ti07); R{-DCO}=1.06~{I9} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$R{-DCO}=0.94~{I17} in {+100}Mo({+10}B,5n|g) (2007Ti07); R{-DCO}=0.56~{I14} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.46~{I9} in {+100}Mo({+10}B,5n|g) (2007Ti07); 
M$R{-DCO}=1.06~{I9} in {+76}Ge({+37}Cl,|a4n|g) (1994Je12) 


decay_energy_unit: KEV
decay_multipolarity: E3
decay_comment:
E$weighted average of 25.53~{I3} (1978Sh08) and 25.47~{I1} (1976Sv04); Other: 25.5 in 1969Ho36 
M$from |a(L)exp:|a(M)exp:|a(N)exp=1:(0.22 +/- 2):(0.09 +/- 2) in 1978Sh08; |a(L1)exp:|a(L2)exp:|a(L3)exp<0.002:1:(1.47 +/- 4) in 1978Sh08 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E$weighted average of 25.53~{I3} (1978Sh08) and 25.47~{I1} (1976Sv04) 
RI$0.76~{I6} calculated by requiring the sum of all transition intensities to g.s. to be 100% 
M$from |a(L1)exp:|a(L2)exp:|a(L3)exp=0.002<:1:1.47~{I4} and |a(L)exp:|a(M)exp:|a(N)exp=1:0.22~{I2}:0.09~{I2} in 1978Sh08; Other: 1953Jo20 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$from 1976Sv04 
MR$from Ice(M1)/(Ice(M2)+Ice(M3))= (100~{I5})/(22~{I3}) in 1976Sv04, and M1+25% E2 in 1976Ja05; 
CC$Other: 46~{I7} from I|g balance leading to |d=0.51~{I7} and unreasonably high B(E2)(W.u.)=2200 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.12~{I4}, A{-4}=0.03~{I5} (1979Ka05); 
M$A{-2}=-0.08~{I9}, A{-4}=0.18~{I14} (1985Ke09); 
M$P{-exp}=-31~{I4} (1979Ka05); 
M$P{-c.p.}=-0.92~{I52}, P{-a.d.}=-0.12~{I15} (1985Ke09) 
MR$|a(K)exp=0.014~{I4} (1979Ka05); Other: 0.0|<|d|<0.30 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.20~{I2}, A{-4}=-0.11~{I3} (1979Ka05); 
M$A{-2}=0.19~{I2}, A{-4}=-0.02~{I3} (1985Ke09); 
M$P{-exp}=32~{I3} (1979Ka05) 
M$P{-c.p.}=0.92~{I11}, P{-a.d.}=0.30~{I4} (1985Ke09) 
MR$|a(K)exp=0.0079~{I24} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.31~{I1}, A{-4}=0.04~{I1} (1979Ka05); 
M$A{-2}=0.25~{I2}, A{-4}=0.03~{I2} (1985Ke09); 
M$P{-exp}=-56~{I4} (1979Ka05); 
M$P{-c.p.}=-0.50~{I9}, P{-a.d.}=-0.50~{I9} (1985Ke09); 
MR$|a(K)exp=0.0039~{I12} (1979Ka05); 0.34|<|d |< 0.40 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.34~{I5}, A{-4}=0.12~{I7} (1979Ka05); 
M$A{-2}=0.11~{I11}, A{-4}=-0.03~{I18} (1985Ke09); 
M$P{-exp}=57~{I13} (1979Ka05); 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.11~{I1}, A{-4}=-0.03~{I2} (1979Ka05); 
M$A{-2}=-0.10~{I1}, A{-4}=-0.02~{I2} (1985Ke09); 
M$P{-exp}=-30~{I4} (1979Ka05) 
M$P{-c.p.}=-0.41~{I13}, P{-a.d.}=-0.38~{I2} (1985Ke09); 
MR$|a(K)exp=0.030~{I9} (1979Ka05); Other: 0.07|<|d |< 0.09 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.29~{I2}, A{-4}=-0.13~{I2} (1979Ka05); 
M$A{-2}=0.31~{I2}, A{-4}=-0.09~{I3} (1985Ke09); 
M$P{-exp}=60~{I5} (1979Ka05); 
M$P{-c.p.}=0.43~{I13}, P{-a.d.}=0.50~{I5} (1985Ke09); 
MR$|a(K)exp=0.0012~{I4} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.62~{I31}, A{-4}=-0.46~{I34} (1979Ka05); 
M$A{-2}=-0.43~{I22}, A{-4}=0.09~{I36} (1985Ke09); 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.27~{I5}, A{-4}=-0.13~{I7} (1979Ka05); 
M$A{-2}=0.26~{I3}, A{-4}=-0.09~{I5} (1985Ke09); 
M$P{-exp}=50~{I17} (1979Ka05) 
M$P{-c.p.}=0.35~{I17}, P{-a.d.}=0.40~{I7} (1985Ke09); 
MR$|a(K)exp=0.0018~{I6} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.19~{I3}, A{-4}=0.04~{I4} (1979Ka05); 
M$A{-2}=0.21~{I2}, A{-4}=-0.01~{I3} (1985Ke09); 
M$P{-exp}=-49~{I6} (1979Ka05); 
M$P{-c.p.}=-0.46~{I16}, P{-a.d.}=-0.57~{I5} (1985Ke09); 
MR$|a(K)exp=0.0020~{I6} (1979Ka05); Other: 0.27|<|d|<0.33 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.28~{I8}, A{-4}=-0.25~{I11} (1979Ka05); 
M$A{-2}=0.27~{I7}, A{-4}=-0.20~{I10} (1985Ke09); 
M$P{-exp}=59~{I8} (1979Ka05); 
M$P{-c.p.}=0.44~{I30}, P{-a.d.}=0.35~{I16} (1985Ke09); 
MR$|a(K)exp=0.00065~{I22} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.92~{I6}, A{-4}=0.10~{I6} (1979Ka05); 
M$A{-2}=-0.76~{I5}, A{-4}=0.13~{I7} (1985Ke09); 
M$P{-exp}=18~{I5} (1979Ka05) 
M$P{-c.p.}=0.16~{I9}, P{-a.d.}=0.09~{I6} (1985Ke09); 
MR$|a(K)exp=0.0016~{I5} (1979Ka05); Other: -0.35|>|d|>-1.10 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.36~{I4}, A{-4}=-0.05~{I4} (1979Ka05); 
M$A{-2}=0.32~{I3}, A{-4}=-0.09~{I4} (1985Ke09); 
M$P{-exp}=46~{I7} (1979Ka05); 
M$P{-c.p.}=0.37~{I17}, P{-a.d.}=0.53~{I8} (1985Ke09); 
MR$|a(K)exp=0.00059~{I19} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.37~{I4}, A{-4}=0.00~{I4} (1979Ka05); 
M$A{-2}=0.33~{I3}, A{-4}=-0.09~{I4} (1985Ke09); 
M$P{-exp}=45~{I7} (1979Ka05); 
M$P{-c.p.}=0.56~{I18}, P{-a.d.}=0.55~{I8} (1985Ke09); 
MR$|a(K)exp=0.00057~{I18} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.01~{I5}, A{-4}=0.05~{I7} (1979Ka05); 
M$A{-2}=-0.14~{I20}, A{-4}=0.14~{I36} (1985Ke09); 
M$P{-exp}=-19~{I6} (1979Ka05) 
MR$|a(K)exp=0.015~{I5} (1979Ka05); Other: -7~{I5} (1979KeZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.30~{I2}, A{-4}=-0.10~{I2} (1979Ka05); 
M$A{-2}=0.34~{I3}, A{-4}=-0.08~{I4} (1985Ke09); 
M$P{-exp}=46~{I8} (1979Ka05); 
M$P{-c.p.}=0.58~{I17}, P{-a.d.}=0.57~{I7} (1985Ke09); 
MR$|a(K)exp=0.00058~{I18} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.24~{I4}, A{-4}=-0.10~{I6} (1979Ka05); 
M$A{-2}=-0.24~{I2}, A{-4}=0.05~{I4} (1985Ke09); 
M$P{-exp}=30~{I4} (1979Ka05); 
M$P{-c.p.}=0.32~{I15}, P{-a.d.}=-0.29~{I4} (1985Ke09); 
MR$|a(K)exp=0.0012~{I5} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.77~{I3}, A{-4}=0.44~{I4} (1979Ka05); 
M$A{-2}=-0.78~{I3}, A{-4}=0.18~{I5} (1985Ke09); 
M$P{-exp}=27~{I6} (1979Ka05); 
M$P{-c.p.}=0.87~{I63}, P{-a.d.}=0.20~{I4} (1985Ke09); 
MR$|a(K)exp=0.026~{I8} (1979Ka05); Other: -2.3|<|d|<-1.8 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.37~{I4}, A{-4}=-0.07~{I6} (1979Ka05); 
M$A{-2}=0.30~{I3}, A{-4}=-0.10~{I5} (1985Ke09); 
M$P{-exp}=83~{I7} (1979Ka05); 
M$P{-c.p.}=0.56~{I14}, P{-a.d.}=0.48~{I8} (1985Ke09); 
MR$|a(K)exp=0.0031~{I10} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.31~{I3}, A{-4}=-0.07~{I4} (1979Ka05); 
M$A{-2}=-0.23~{I4}, A{-4}=0.04~{I6} (1985Ke09); 
M$P{-exp}=10~{I9} (1979Ka05); 
M$P{-c.p.}=0.3~{I4}, P{-a.d.}=-0.30~{I7} (1985Ke09); 
MR$|a(K)exp=0.00015~{I7} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.24~{I2}, A{-4}=0.03~{I3} (1979Ka05); 
M$A{-2}=-0.29~{I3}, A{-4}=-0.05~{I5} (1985Ke09); 
M$P{-exp}=10~{I6} (1979Ka05); 
M$P{-c.p.}=0.2~{I2}, P{-a.d.}=-0.41~{I6} (1985Ke09); 
MR$|a(K)exp=0.00014~{I6} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.23~{I1}; A{-4}=-0.02~{I2} (1979Ka05) 
M$A{-2}=-0.21~{I3}, A{-4}=0.09~{I5} (1985Ke09); 
M$P{-a.d.}=-0.39~{I6} (1985Ke09); 
MR$Other: 0.0|<|d|<0.04 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.09~{I9}; A{-4}=0.00~{I6} (1979Ka05) 
M$A{-2}=-0.13~{I3}, A{-4}=0.03~{I5} (1985Ke09); 
M$P{-a.d.}=-0.37~{I5} (1985Ke09); 
MR$Other: 0.02|<|d|<0.09 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.22~{I30}, A{-4}=-0.02~{I34} (1979Ka05); 
M$A{-2}=-0.17~{I7}, A{-4}=0.18~{I11} (1985Ke09); 
M$P{-exp}=66~{I12} (1979Ka05); 
M$P{-c.p.}=0.64~{I27}, P{-a.d.}=-0.12~{I11} (1985Ke09); 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.17~{I1}; A{-4}=0.00~{I1} (1979Ka05) 
M$A{-2}=-0.17~{I2}, A{-4}=0.05~{I2} (1985Ke09); 
M$P{-exp}=-0.68~{I35}, P{-a.d.}=-0.41~{I4} (1985Ke09); 
MR$Other: 0.02|<|d|<0.08 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.23~{I6}, A{-4}=-0.09~{I8} (1979Ka05); 
M$A{-2}=0.37~{I6}, A{-4}=0.01~{I9} (1985Ke09); 
M$P{-exp}=-80~{I9} (1979Ka05); 
M$P{-c.p.}=-0.84~{I35}, P{-a.d.}=-0.81~{I15} (1985Ke09); 
MR$|a(K)exp=0.0059~{I19} (1979Ka05); Other: 0.30|<|d|<0.44 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.18~{I11}, A{-4}=-0.04~{I16} (1979Ka05); 
M$A{-2}=-0.16~{I3}, A{-4}=-0.09~{I5} (1985Ke09); 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$A{-2}=-0.18~{I7}, A{-4}=-0.09~{I11} (1985Ke09); 
M$P{-exp}=29~{I14} (1979Ka05); 
M$P{-c.p.}=0.2~{I5}, P{-a.d.}=-0.44~{I12} (1985Ke09); 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.16~{I1}, A{-4}=0.00~{I1} (1979Ka05); 
M$A{-2}=-0.14~{I2}, A{-4}=-0.07~{I2} (1985Ke09); 
M$P{-exp}=-39~{I11} (1979Ka05); 
M$P{-c.p.}=-0.38~{I27}, P{-a.d.}=-0.47~{I3} (1985Ke09); 
MR$others: 0.05|<|d|<0.08 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-2}=-0.25~{I2}, A{-4}=-0.02~{I3} (1979Ka05); 
M$A{-2}=-0.23~{I2}, A{-4}=-0.01~{I2} (1985Ke09); 
M$P{-exp}=-0.37~{I33}, P{-a.d.}=-0.36~{I3} (1985Ke09); 
MR$others: 0.0|<|d|<0.03 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.44~{I16}, A{-4}=-0.03~{I21} (1979Ka05); 
M$P{-exp}=70~{I18} (1979Ka05) 
MR$|a(K)exp=0.00038~{I14} (1979Ka05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.17~{I1}, A{-4}=-0.03~{I2} (1979Ka05); 
M$A{-2}=-0.14~{I2}, A{-4}=-0.04~{I3} (1985Ke09); 
M$P{-exp}=-25~{I5} (1979Ka05); 
M$P{-c.p.}=-0.35~{I26}, P{-a.d.}=-0.45~{I3} (1985Ke09); 
MR$|a(K)exp=0.039~{I12} (1979Ka05); Other: 0.04|<|d|<0.07 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.20~{I2}, A{-4}=0.00~{I3} (1979Ka05); 
M$A{-2}=-0.21~{I2}, A{-4}=-0.07~{I3} (1985Ke09); 
M$P{-exp}=-30~{I8} (1979Ka05); 
M$P{-c.p.}=-0.46~{I35}, P{-a.d.}=-0.45~{I3} (1985Ke09); 
MR$|a(K)exp=0.027~{I9} (1979Ka05); Other: 0.01|<|d|<0.04 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.19~{I3}, A{-4}=0.10~{I4} (1979Ka05); 
M$A{-2}=-0.16~{I5}, A{-4}=-0.03~{I7} (1985Ke09); 
M$P{-exp}=-40~{I5} (1979Ka05); 
M$P{-c.p.}=-0.40~{I28}, P{-a.d.}=-0.39~{I8} (1985Ke09); 
MR$|a(K)exp=0.012~{I4} (1979Ka05); Other: 0.02|<|d|<0.08 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.01~{I14}, A{-4}=0.05~{I16} (1979Ka05); 
M$A{-2}=-0.05~{I6}, A{-4}=-0.16~{I11} (1985Ke09); 
M$P{-exp}=-65~{I12} (1979Ka05); 
M$P{-c.p.}=-0.73~{I35}, P{-a.d.}=-0.65~{I12} (1985Ke09); 
MR$|a(K)exp=0.011~{I4} (1979Ka05); Other: 0.08|<|d|<0.15 (1985Ke09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Placement is by evaluators based on |e decay data. Placed from 1543.5 by 1977Mi16. I|g/I|g(530|g) in |e decay leads to an expected I|g(877|g)=27 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E taken from {+103}Rh(|a,n|g). Considered by the evaluators to be identical to the 439.9-keV |g transition observed in {+96}Zr({+14}N,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E,RI,M,MR$from 1981Po06 in {+96}Zr({+14}N,4n) 
M,MR$if J|p of 2441.60 (11-), 2033.48 (9-) levels are correct D+Q is impossible 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from branching I|g(675.5|g)/I|g(432.4|g)=34 {I7} if fraction I|g(675|g from 765 level) is the same in both 13.4- and 16.7-MeV data 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from coincidence data 
RI doublet=251 {I9} minus I|g(675.5|g)=235 
Considered doubtful by the evaluators. Observed only in {+103}Rh(|a,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
RI$ 86 {I4} units contributed by positive parity states, and 43 {I5} units by negative parity states. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A=+0.46 {I9}. POL=-0.5 {I3}. Values corrected for contribution from 1014.4|g in {+27}Al(n,n'|g) shifted to 1021.5 keV 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
$B(M1)(W.u) and B(E2)(W.u) calculated by compiler. 2016Da03 gives B(M1)(W.u)=2.01 {I19} and B(E2)(W.u)=114 {I10} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
$B(M1)(W.u) and B(E2)(W.u) calculated by compiler. 2016Da03 gives B(M1)(W.u)=1.22 {I12} and B(E2)(W.u)=80 {I7} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
$B(M1)(W.u) and B(E2)(W.u) calculated by compiler. 2016Da03 gives B(M1)(W.u)=0.92 {I13} and B(E2)(W.u)=64 {I10} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
$B(M1)(W.u) and B(E2)(W.u) calculated by compiler. 2016Da03 gives B(M1)(W.u)=0.46 {I9} and B(E2)(W.u)=37 {I7} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
$B(M1)(W.u) and B(E2)(W.u) calculated by compiler. 2016Da03 gives B(M1)(W.u)=0.87 {I11} and B(E2)(W.u)=50 {I13} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
$B(M1)(W.u) and B(E2)(W.u) calculated by compiler. 2016Da03 gives B(M1)(W.u)=0.49 {I17} and B(E2)(W.u)=47 {I17} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E 93.124 {I20} (1974HeYW). Others: 93.06 {I4} (1953Jo20,1972Br02), 93.10 {I5} (1962La10), 93.13 {I3} (1974Pa15), 93.16 {I2} (1978Sh08) 
M L1:L2:L3=18.0 {I11}:90.0 {I35}:100 (1958Sc40), 17.7 {I11}:86.6 {I27}:100 (1972Br02), 17.1 {I14}:84.0 {I15}:100 (1978Sh08) 
K/L=1.09 {I4} (1958Sc40), 1.08 {I3} (1962La10), 0.95 {I4} (1978Sh08) 
|a(K)exp=9.5 {I10} (1953Br73) ce(K)/I|g, 9.1 {I5} (1962La10) K| x ray/I|g, 9.3 {I4} (1974Pa15) K| x ray/I|g. K/L2=2.30 {I15}, L1/L2=0.20 {I1}, L2/L3=0.90 {I2} (1981Tr07). 1981Tr07 extract a value for the penetration factor, |l=-0.7 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
RI$I|g is the intensity in equilibrium 
E from 1974HeYW. Others: 93.13 {I3} (1974Pa15), 93.16 {I2} (1978Sh08) 
RI others: 2290 {I300} (1962La10), 2560 {I180} (1967Bl08), 2400 {I250} (1974Bu15), 3510 {I300} (1974HeYW) 
M from |a(K)exp, K/L, L-subshell ratios; see {+107}Ag IT decay (44.3 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1976Sv04. Others: 32.3 {I1} (1974Pa15), 32.6 {I4} (1962La10) 
MR from L1:L2:L3=100 {I8}:17 {I4}: <14 (1976Sv04) 
|a(K)exp=10.1 {I4} from I(K| x ray)/I|g(32|g) via (796|g)(32|g)-coin (1974Pa15) 
(796|g)(32|g)-coin: I(K| x ray)/I|g(32|g)=20 {I8} (1962La10), 18.0 {I13} (1974Pa15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 1974HeYW. Other: 324.8 {I1} (1974Pa15) 
RI$others: 18 {I1} (1967Bl08), 16 {I2} (1974Bu15), 20 {I2} (1974HeYW) 
MR$from 325|g(|q) Coul. ex. (1970RoZS). Other: 0.205 {I6} (1977Kr13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$from Coul. ex. (1970Ro14). Other: 98.2 (1974Pa15) 
RI$from branching: I|g(98|g)/I|g(423|g)=0.046 {I5} (1970Ro14, Coul. ex.) 
MR$from 98|g(|q) Coul. ex. (1970Ro14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from 1974HeYW. Other: 423.0 {I1} (1974Pa15) 
RI$others: 18.1 {I30} (1962La10), 18.6 {I17} (1974HeYW) 
|a(K)exp=0.0095 {I12} if normalized to |a(K)(93|g)=9.4 (E3 theory) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$|a(K)exp is consistent with M1 or E2; level scheme requires E2. 
E$from 1974HeYW. Other: 796.7 {I1} (1974Pa15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from 526|g(|q) Coul. ex. (1970Ro14). Others: -0.25 {I3} (1969Ro03), -0.17 +7 -10 (1974Pa15), -0.18 {I3} (1977Kr13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 1974HeYW. Other: 625.0 {I1} (1974Pa15) 
MR$from 625|g(|q) Coul. ex. (1970Ro14). Other: 0.24 {I3} (1977Kr13), -0.09 {I6} (1974Pa15) via (625|g)(325|g)(|q) 
M$the |a(K)exp is discrepant with M1 or E2 theory values. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 1974HeYW. Other: 720.0 {I1} (1974Pa15) 
MR$(720|g)(423|g)(|q): -1.1 {I2} (1974Pa15), -0.9 {I4} (1967Bl08). Other: 1977Kr13 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E from 1974HeYW. Other: 818.5 {I4} (1974Pa15) 
MR +2.0 {I+2-5} or +0.26 {I+14-11} (1974Pa15) via (818|g)(325|g)(|q) 
Doublet |a(K)exp=0.007 {I3}, E(ce(K) 818|g)=E(ce(L) 796|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E other: 324.4 {I2} (1973Co10) 
MR$from 1970Ro14. Others: -0.21 {I1} (1958Mc02), -0.207 {I10} (1970RoZS) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
RI from I|g(330|g)-branching excit (1973Co10). Others: 0.26 {I8} prompt |g singles (1973Co10), 0.4 {I2} (1970Ro14), |?0.5 (1954Hu57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR av: -0.05 {I13} |g(|q), -0.11 {I3} |g|g(|q), -0.19 {I6} |g|g(|q) (1970Ro14) 
E existence questionable 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
E$from 1982Ma13. Uncertainty is given at 2|s confidence level. K|a| x ray lines of Pb (energy from 1967Be73) were used for calibration. Others: 1972Sc42, 1973Be08, 1979Da05 
M$from |a(K)exp based on Ice(K)/I|g of 1966Ki03 normalized so that |a(K)exp(434|g, {+108}Pd)=0.00789 (E2 theory) 


decay_energy_unit: KEV
decay_multipolarity: M4
decay_BM_unit: mu^2 x (fm)^6
decay_BM_info: ;TYPE=BM4;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM4W
decay_comment:
E$from 1966Ki03, s ce 
M$from ce(L1)/ce(L23), |a(K)/(1+|a) (1966Ki03) 
CC$for E|g=30.332 (adopted value) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|DJ=0, dipole transition. R{-IPDCO}=-0.23 {I3}, R{-DCO}=1.86 {I1} with gate on a stretched dipole |g ray (according to email reply from R. Palit on August 1, 2013 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E$unobserved transition below the 40 keV experimental threshold; existence is suggested by the observation of both the 206|g and 215|g in a spectrum double gated on the 75|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI$Combined intensity for the 74.6|g and 74.8|g. 
$R{-DCO}=0.52 {I5} measured by gating on |DI = 2 178|g which feeds the 74.6|g from the top. 
RI$>7.3 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$from assigned J{+|p} in 2016Se01, 329.4|g is a |DJ = 0 transition. R{-DCO}=1.86 {I1}, R{-IPDCO}=-0.23 {I3}. See also the XUNDL-2 compilation for 2013Se12; an email exchange with one of the co-authors about the same multipolarity assignment. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=1.02 {I2}, R{-IPDCO}=0.046 {I12} measured by gating on |DI = 2 755|g. Authors stated in the text that 413.1|g is a mixed M1+E2 transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$from R{-DCO}=0.96 {I4}, R{-IPDCO}=0.0990 {I17} and 755|g(|q) (A{-2}=0.26 {I6} and A{-4}=-0.025 {I10}). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_BE_unit: e^2 x (fm)^6
decay_BE_info: ;TYPE=BE3;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE3W
decay_comment:
E$From {+109}Cd |e decay (2000He14) 
M$from ce data in {+109}Pd |b{+-} decay. |a(K)exp=10.6 {I5} (1970Ba37); |a(K)exp=11.6, K:L:M:N=(0.98 {I5}):1:(0.20 {I1}):(0.050 {I5}), L1:L2:L3=(0.185 {I15}):1:(1.163 {I27}) (1978Sh08) and ce data in {+109}Cd |e decay 
RI$Double photon decay: I(|g|g)/I(|g)<6|*10{+-7} (1988Il01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from |g(|q): A{-2}=-0.395 {I16} (1970Ro14), -0.39 {I2} (1955Mc51), -0.388 {I7} (1958Mc02), A{-2}=-0.710 {I7} (1970RoZS), -0.654 {I36} (1989Lo08) in Coulomb Excitation and |a(K)exp=0.019 {I2} from {+109}Pd |b{+-} decay (1970Ba37) 
MR$weighted average of 0.193 {i10} (1970RoZS), -0.196 {i27} (1970Ro14), and 0.19 {i1} (1958Mc02). Others: 0.19 (1955Mc51) in Coulomb Excitation and |d=0.35 {I5} from |g|g(|q) in {+109}Pd |b{+-} decay (1975El10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$Others: 5.1 {I4} in Coulomb Excitation (weighted average of 5.4 {I5} (1989Lo08), 4.9 {I5} 1970Ro14 and 4.6 {I11}, deduced from I(|g+ce) in 1973Co10) 
M$|a(K)exp=0.44 {I5} in {+109}Pd |b{+-} decay (1970Ba37); A{-2}=-0.239 {I17} in Coulomb Excitation (1970Ro14) 
MR$From |g(|q) in Coulomb excitation 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=0.010 {I1} from {+109}Pd |b{+-} decay (1970Ba37); A{-2}=+0.124 {I23} (1970Ro14), A{-2}=+0.248 {I4}, A{-4}=-0.039 {I9} (1955Mc51) in Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.095 {I2} (1970Ba37); |g|g(|q) in {+109}Pd |b{+-} decay 
MR$weighted average of |d=0.19 {I6} (1977Bo04) and +0.23 {I5} (1988Br31) using |g|g(|q) in {+109}Pd |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.0023 {I5} from {+109}Pd |b{+-} decay (1970Ba37); A{-2}=-0.32 {I6} (|g(|q)) in Coulomb excitation (1970Ro14) 
MR$from |g(|q) in Coulomb excitation (1970Ro14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$|a(K)exp=0.006 {I1} from {+109}Pd |b{+-} decay (1970Ba37) 
MR$|g|g(|q) in {+109}Pd |b{+-} decay (1988Br31) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
M$|a(K)exp=0.0030 {I3} (1970Ba37) and |g|g(|q) (1977Bo04) in {+109}Pd |b{+-} decay. 
MR$|g|g(|q) in {+109}Pd |b{+-} decay (1977Bo04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$|a(K)exp=0.0030 {I5} (1970Ba37) and |g|g(|q) in {+109}Pd |b{+-} decay 
MR$from |g|g(|q) in 1988Br31; Other: |d=-0.27 {I3} in (1977Bo04)  


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$|a(K)exp=0.0070 {I8} from {+109}Pd |b{+-} decay (1970Ba37); A{-2}=+0.124 {I23} (1970Ro14), A{-2}=+0.32 {I10}, A{-4}=-0.11 {I15} (1989Lo08) 
MR$From |g(|q) in Coulomb excitation (1970Ro14); Other: -0.12 {I14} in Coulomb excitation (1988Br31) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.441 {I29} in Coulomb excitation (1970Ro14); ; |g|g(|q) in {+109}Pd |b{+-} decay (1988Br31) 
MR$weighted average of -0.28 {I4} from |g(|q) in Coulomb excitation (1970Ro14), -0.28 {I4} (1977Bo04) and -0.26 {I7} (1988Br31) from |g|g(|q) in {+109}Pd |b{+-} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$|a(K)exp=0.15 {I2} (1970Ba37) and |d=0.13 {I2} from |g|g(|q) (1975El10) in {+109}Pd |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
M,MR$|a(K)exp=0.0012 {I3} (1970Ba37) and |d=-0.26 {I5} from |g|g(|q) (1977Bo04) in {+109}Pd |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from Coulomb excitation. 
M$A{-2}=+0.48 {I5}, A{-4}=-0.26 {I7} from Coulomb excitation (1989Lo08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E$From adopted gammas. Others in {+109}Pd |b{+-} decay: 88.022 {I10} (2015Kr07), 88.04 {I5} (1969Sc12), 88.04 {I10} (1982Aw03), 88.06 {I2} (1978Sh08), 88.1 {I2} (1968Be22), 88.2 {I5}(1968Gr02), 88.0 {I4} (1970Ba37), 88.1 {I5} (1975El10), and 88 {I1} (1978Pr08) 
RI$Others: 1.37E4 16 (1968Gr02), 1.48E4 18 (1969Sc12), 1.17E4 12 (1970Ba37), 1.43E4 19 (1975El10), 1.46E4 13 (1978Pr08) and 1.20E4 8 (1982Aw03). 
M$From adopted gammas. ce data in {+109}Pd |b{+-} decay: |a(K)exp=10.6 {I5} (1970Ba37); |a(K)exp=11.6, K:L:M:N=(0.98 {I5}):1:(0.20 {I1}):(0.050 {I5}), L1:L2:L3=(0.185 {I15}):1:(1.163 {I27}) (1978Sh08) 
$Double K-shell vacancy per K-shell internal conversion: 13.0|*10{+-5} 11 (1979Va04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 44.7 {I2} (1968Be22), 44.8 {I6} (1968Gr02), 44.8 {I4} (1970Ba37), 44.0 {I5} ( 1975El10) and 44.98 {I21} (1982Aw03). Other: 45.8 {I2} (1978Sh08) 
RI$weighted average of 5.5 {I17} (1968Gr02), 4.8 {I5} (1970Ba37) and 4.5 {I6} (1982Aw03). Other: 4.5 (1968Be22) 
MR$From 1984ShZL 
M$|a(K)exp=3.6 {I5}, |a(L)exp=0.7 {I3} (1978Sh08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: 311.3 {I1} (1968Be22), 311.5 {I5} (1968Gr02), 311.4 {I1} (1969Sc12), 311.4 {I2} (1970Ba37), 311.0 {I2} (1975El10), 311.4 {I1} (1978Pr08) and 311.4 {I1} (1982Aw03). 
RI$Others: 154 {I12} (1968Gr02), 91 {I8} (1970Ba37), 123 {I12} (1975El10), 124 {I6} (1978Pr08) and 121 {I9} (1982Aw03). 
M$|a(K)exp=0.019 {I2} (1970Ba37) 
MR$Other: 0.35 {I5} from |g|g(|q) in 1975El10 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: 103.7 {I2} (1968Be22), 103.6 {I7} (1968Gr02), 103.9 {I4} (1969Sc12), 103.6 {I4} (1970Ba37), 103.5 {I5} (1975El10), 103.6 {I2} (1978Pr08) and 103.73 {I25} (1982Aw03). 
RI$Others: 3.4 {I11} (1968Gr02), 3.8 {I12} (1969Sc12), 1.9 {I2} (1970Ba37), 2.7 {I6} (1975El10), 2.8 {I5} (1978Pr08) and 2.7 {I5} (1982Aw03). 
M$|a(K)exp=0.44 {I5} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Others: 415.0 {I1} (1968Be22), 415.2 {I6} (1968Gr02), 415.2 {I3} (1969Sc12), 415.1 {I2} (1970Ba37), 415.2 {I1} (1975El10), 415.19 {I7} (1978Pr08) and 415.3 {I1} (1982Aw03). 
RI$Others: 35 {I11} (1968Gr02), 43 {I12} (1969Sc12), 45 {I4} (1970Ba37), 43 {I4} (1975El10), 42 {I3} (1978Pr08) and 48 {I6} (1982Aw03). 
M$|a(K)exp=0.010 {I1} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$Weighted average of 564.4 {I5} (1975El10) and 564.2 {I3} (1982Aw03). Seen only in 1975El10 and 1982Aw03. 
RI$weighted average of 0.43 {I7} (1975El10) and 0.8 {I5} (1982Aw03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$Weighted average of 609.2 {I4} (1975El10), 609.40 {I21} (1982Aw03) and 609.5 {I5} (1969Sc12). It is not placed in 1969Sc12 and evaluators have assigned it to this level. 
RI$Others: 0.7 {I5} (1975El10) and 0.6 {I3} (1969Sc12). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
E$Others: 286.3 {I5} (1969Sc12), 286.0 {I5} (1975El10), 286.8 {I2} (1978Pr08) and 286.5 {I3} (1982Aw03). 
RI$Others:0.6 {I2} (1969Sc12), 0.8 {I1} (1975El10) and 0.5 {I1} (1978Pr08). 1.7 {I5} from 1982Aw03. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: 390.5 {I3} (1968Be22), 390.9 {I8} (1968Gr02), 390.6 {I2} (1969Sc12), 390.7 {I5} (1970Ba37), 391.0 {I3} (1975El10), 390.6 {I2} (1978Pr08) and 390.4 {I2} (1982Aw03). 
RI$Others: 3.9 {I8} (1968Gr02), 3.8 {I12} (1969Sc12), 3.2 {I3} (1970Ba37), 3.9 {I6} (1975El10), 3.6 {I3} (1978Pr08). 8.1 {I11} from 1982Aw03 
MR$0.19 {I6} from |g|g(|q) in 1977Bo04, +0.23 {I5} from |g|g(|q) in 1988Br31. 
M$|a(K)exp=0.095 {I2} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: 702.0 {I2} (1968Be22), 701.8 {I8} (1968Gr02), 701.9 {I2} (1969Sc12), 702.0 {I3} (1970Ba37), 701.9 {I3} (1975El10), 701.8 {I1} (1978Pr08) and 701.80 {I15} (1982Aw03). 
RI$Others: 14.2 {I19} (1968Gr02), 13 {I3} (1969Sc12), 14.7 {I12} (1970Ba37), 13.8 {I14} (1975El10), 13.5 {I18} (1978Pr08) and 14.2 {I12} (1982Aw03) 
M$|a(K)exp=0.0023 {I5} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Others: 395.6 {I5} (1969Sc12), 395.6 {I3} (1975El10), 395.8 {I9} (1978Pr08) and 396.3 {I3} (1982Aw03). 
RI$Others: 0.27 {I13} (1969Sc12), 0.7 {I3} (1975El10), 0.27 {I5} (1978Pr08) and 0.50 {I5} (1982Aw03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Others: 706.9 {I3} (1968Be22), 707.0 {I2} (1969Sc12), 707.1 {I4} (1970Ba37), 707.1 {I2} (1975El10), 706.9 {I1} (1978Pr08) and 707.7 {I2} (1982Aw03). 
RI$Others: 6.5 {I18} (1969Sc12), 7.1 {I7} (1970Ba37), 7.1 {I10} (1975El10), 6.3 {I9} (1978Pr08) and 5.3 {I6} (1982Aw03) 
$|a(K)exp=0.0020 {I6} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
E$Others: 309.3 {I5} (1968Be22), 309.1 {I5} (1969Sc12), 309.1 {I7} (1970Ba37), 109.0 {I5} (1975El10), 309.3 {I4} (1978Pr08) and 309.30 {I15} (1982Aw03). 
RI$Others: 19 {I8} (1969Sc12), 21.0 {I9} (1970Ba37), 16.4 {I16} (1975El10), 20 {I6} (1978Pr08) and 20 {I2} (1982Aw03) 
MR$|g|g(|q) in 1988Br31 
M$|a(K)exp=0.006 {I1} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
E$Others: 413.0 {I1} (1968Be22), 413.5 {I10} (1968Gr02), 413.0 {I4} (1969Sc12), 413.2 {I2} (1970Ba37), 413.0 {I1} (1975El10), 413.0 {I1} (1978Pr08) and 413.05 {I10} (1982Aw03). 
RI$Others: 40 {I12} (1968Gr02), 27 {I8} (1969Sc12), 23 {I2} (1970Ba37), 29 {I3} (1975El10), 29 {I2} (1978Pr08) and 24 {I3} (1982Aw03) 
MR$from |g|g(|q) in 1977Bo04. 
M$|a(K)exp=0.0030 {I3} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Others: 636.4 {I2} (1968Be22), 636.1 {I5} (1968Gr02), 636.3 {I1} (1969Sc12), 636.3 {I3} (1970Ba37), 636.5 {I4} (1975El10), 636.25 {I9} (1978Pr08) and 636.3 {I1} (1982Aw03). 
RI$Others: 42 {I6} (1968Gr02), 41 {I10} (1969Sc12), 41 {I4} (1970Ba37), 40 {I4} (1975El10), 42 {I3} (1978Pr08) and 42.6 {I21} (1982Aw03) 
M$|a(K)exp=0.0026 {I5} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Others: 724.6 {I3} (1968Be22), 724.4 {I3} (1969Sc12), 724.4 {I5} (1970Ba37), 724.6 {I2} (1975El10), 724.1 {I3} (1978Pr08) and 724.4 {I3} (1982Aw03). 
RI$Others: 0.8 {I3} (1969Sc12), 1.1 {I1} (1970Ba37), 1.0 {I3} (1975El10), 0.4 {I4} (1978Pr08) and 1.1 {I3} (1982Aw03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
E$Others: 423.9 {I3} (1968Be22), 424.7 {I8} (1968Gr02), 423.9 {I2} (1969Sc12), 424.0 {I4} (1970Ba37), 424.1 {I3} (1975El10), 424.0 {I2} (1978Pr08) and 424.0 {I2} (1982Aw03). 
RI$Others: 2.8 {I7} (1968Gr02), 3.8 {I12} (1969Sc12), 3.9 {I3} (1970Ba37), 3.8 {I5} (1975El10), 3.5 {I3} (1978Pr08) and 3.4 {I5} (1982Aw03) 
M$|a(K)exp=0.0030 {I5} (1970Ba37) 
MR$from |g|g(|q) in 1988Br31; Other: -0.27 {I3} from |g|g(|q) in 1977Bo04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Others: 602.5 {I1} (1968Be22), 602.4 {I5} (1968Gr02), 602.5 {I1} (1969Sc12), 602.4 {I2} (1970Ba37), 602.3 {I5} (1975El10), 602.49 {I9} (1978Pr08) and 602.6 {I1} (1982Aw03). 
RI$Others: 33 {I4} (1968Gr02), 33 {I8} (1969Sc12), 34 {I3} (1970Ba37), 35 {I4} (1975El10), 35 {I2} (1978Pr08) and 31 {I3} (1982Aw03) 
M$|a(K)exp=0.0030 {I5} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$Others: 647.3 {I1} (1968Be22), 647.3 {I6} (1968Gr02), 647.3 {I1} (1969Sc12), 647.3 {I2} (1970Ba37), 647.21 {I7} (1978Pr08) and 647.3 {I1} (1982Aw03). 646.4 {I1} from 1975El10 
M$|a(K)exp=0.0027 {I4} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$Weighted average of 114.2 {I3} (1975El10) and 114.30 {I25} (1982Aw03). Seen only in 1975El10 and 1982Aw03. 
RI$from 1975El10. 2.8 {I6} from 1982Aw03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$Weighted average of 500.6 {I5} (1975El10) and 500.6 {I3} (1982Aw03). Seen only in 1975El10 and 1982Aw03. 
RI$from 1975El10. 1.2 {I3} from 1982Aw03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: 447.5 {I2} (1968Be22), 448.2 {I8} (1968Gr02), 447.6 {I2} (1969Sc12), 447.4 {I3} (1970Ba37), 447.8 {I3} (1975El10), 447.5 {I2} (1978Pr08) and 447.02 {I20} (1982Aw03). 
RI$Others: 4 {I1} (1968Gr02), 3.3 {I12} (1969Sc12), 3.3 {I3} (1970Ba37), 3.0 {I5} (1975El10), 3.5 {I3} (1978Pr08) and 3.0 {I5} (1982Aw03) 
MR$-0.12 {I14} from |g|g(|q) in 1988Br31 
M$|a(K)exp=0.0070 {I8} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: 551.3 {I2} (1968Be22), 551.3 {I8} (1968Gr02), 551.4 {I4} (1969Sc12), 551.2 {I3} (1970Ba37), 551.2 {I5} (1975El10), 551.2 {I1} (1978Pr08) and 551.2 {I2} (1982Aw03). 
RI$Others: 2.3 {I8} (1968Gr02), 2.5 {I9} (1969Sc12), 2.5 {I3} (1970Ba37), 2.6 {I5} (1975El10), 2.7 {I2} (1978Pr08) and 3.1 {I3} (1982Aw03) 
MR$-0.28 {I4} from |g|g(|q) in 1977Bo04, -0.26 {I7} from |g|g(|q) in 1988Br31 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Others:862.8 {I5} (1968Be22), 862.5 {I4} (1969Sc12), 863.0 {I7} (1970Ba37), 862.9 {I1} (1975El10), 862.5 {I3} (1978Pr08) and 862.6 {I3} (1982Aw03). 
RI$Others: 0.54 {I18} (1969Sc12), 0.3 {I1} (1970Ba37), 0.5 {I2} (1975El10), 0.66 {I11} (1978Pr08) and 0.44 {I5} (1982Aw03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: 134.3 {I2} (1968Be22), 134.7 {I7} (1968Gr02), 134.2 {I2} (1969Sc12), 134.5 {I3} (1970Ba37), 134.4 {I2} (1975El10), 134.0 {I2} (1978Pr08) and 134.1 {I2} (1982Aw03). 
RI$Others: 4.9 {I15} (1968Gr02), 5.4 {I18} (1969Sc12), 4.0 {I4} (1970Ba37), 4.7 {I7} (1975El10), 6.1 {I9} (1978Pr08) and 5.7 {I6} (1982Aw03) 
M$|a(K)exp=0.20 {I2} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: 145.4 {I3} (1968Be22), 145.9 {I7} (1968Gr02), 145.1 {I2} (1969Sc12), 145.5 {I3} (1970Ba37), 145.4 {I2} (1975El10), 145.0 {I2} (1978Pr08) and 145.20 {I21} (1982Aw03). 
RI$Others: 4.2 {I13} (1968Gr02), 4.6 {I14} (1969Sc12), 3.1 {I3} (1970Ba37), 3.5 {I5} (1975El10), 3.8 {I8} (1978Pr08) and 3.9 {I5} (1982Aw03) 
MR$0.13 {I2} from |g|g(|q) in 1975El10 
M$|a(K)exp=0.15 {I2} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
E$Others: 454.3 {I2} (1968Be22), 454.3 {I3} (1969Sc12), 454.1 {I3} (1970Ba37), 454.0 {I3} (1975El10), 454.2 {I2} (1978Pr08) and 454.40 {I25} (1982Aw03). 
RI$Others: 2.2 {I11} (1969Sc12), 2.3 {I2} (1970Ba37), 2.2 {I4} (1975El10), 1.7 {I2} (1978Pr08) and 2.2 {I5} (1982Aw03) 
MR$-0.14 {I+36-17} from |g|g(|q) in 1988Br31 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
E$Others: 558.1 {I1} (1968Be22), 557.8 {I5} (1968Gr02), 558.1 {I2} (1969Sc12), 558.5 {I2} (1970Ba37), 558.0 {I3} (1975El10), 558.05 {I7} (1978Pr08) and 558.10 {I15} (1982Aw03). 
RI$Others: 9.5 {I14} (1968Gr02), 10 {I3} (1969Sc12), 9.6 {I9} (1970Ba37), 10.7 {I16} (1975El10), 9.9 {I7} (1978Pr08) and 11.0 {I7} (1982Aw03) 
MR$-0.26 {I5} from |g|g(|q) in 1977Bo04, -0.026 {I23} from |g|g(|q) in 1988Br31. 
M$|a(K)exp=0.0012 {I3} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Others: 736.7 {I2} (1968Be22), 736.7 {I7} (1968Gr02), 736.7 {I2} (1969Sc12), 736.8 {I4} (1970Ba37), 736.7 {I2} (1975El10), 736.6 {I1} (1978Pr08) and 736.50 {I25} (1982Aw03). 
RI$Others: 7.7 {I11} (1968Gr02), 6.9 {I19} (1969Sc12), 7.7 {I7} (1970Ba37), 7.5 {I12} (1975El10), 6.8 {I9} (1978Pr08) and 7.5 {I6} (1982Aw03) 
M$|a(K)exp=0.0018 {I5} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: 781.4 {I2} (1968Be22), 781.8 {I7} (1968Gr02), 781.4 {I2} (1969Sc12), 781.5 {I3} (1970Ba37), 782.1 {I4} (1975El10), 781.3 {I1} (1978Pr08) and 781.4 {I1} (1982Aw03). 
RI$Others: 51 {I6} (1968Gr02), 45 {I12} (1969Sc12), 50 {I4} (1970Ba37), 49 {I7} (1975El10), 48 {I3} (1978Pr08) and 43 {I3} (1982Aw03) 
M$|a(K)exp=0.0017 {I5} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$Others: 778.3 {I5} (1968Be22), 778.3 {I5} (1969Sc12), 778.4 {I7} (1970Ba37), 778.2 {I2} (1975El10), 778.2 {I3} (1978Pr08), 778.3 {I5} (1982Aw03) and 778.3 {I5} (1988Br31) 
RI$Others: 6.2 {I25} (1969Sc12), 4.0 {I4} (1970Ba37), 5.8 {I9} (1975El10), 7.3 {I25} (1978Pr08) and 4.0 {I5} (1982Aw03) 
M$|a(K)exp=0.0018 {I5} (1970Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
E$Others: 822.9 {I3} (1968Be22), 822.9 {I4} (1969Sc12), 822.7 {I5} (1970Ba37), 823.1 {I2} (1975El10), 822.8 {I2} (1978Pr08) and 822.9 {I3} (1982Aw03). 
RI$Others: 0.77 {I22} (1969Sc12), 0.5 {I1} (1970Ba37), 0.77 {I11} (1978Pr08) and 0.8 {I5} (1982Aw03). 1.5 {I4} from 1975El10. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$Others: 496.9 {I5} (1968Be22), 496.7 {I7} (1970Ba37), and 496.9 {I6} (1978Pr08) 
RI$Others: 0.15 {I3} (1970Ba37) and 0.31 {I6} (1978Pr08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 402.2 {I5} (1975El10) and 402.0 {I3} (1982Aw03). Seen only in 1975El10 and 1982Aw03. 
RI$from 1975El10. 1.9 {I5} from 1982Aw03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Others: 966.3 {I5} (1968Be22), 966.4 {I7} (1970Ba37), 966.2 {I3} (1975El10), 966.2 {I5} (1978Pr08) and 966.1 {I3} (1982Aw03). 
RI$Others: 0.37 {I13} (1975El10), 0.25 {I4} (1978Pr08) and 0.43 {I5} (1982Aw03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Others: 1010.5 {I5} (1968Be22), 1010.6 {I9} (1970Ba37), 1010.0 {I3} (1975El10), 1010.8 {I6} (1978Pr08) and 1010.5 {I3} (1982Aw03). 
RI$Others: 0.25 {I8} (1975El10), 0.11 {I4} (1978Pr08) and 0.38 {I4} (1982Aw03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E$from relative wavelength measurement in 2000He14. Other values are given in the table above 
RI$From I(|g+ce)=100 and |a=26.3 {I4}. Other values are given in the table above 
M$from ce data listed in the table above. Others: L1:L2:L3=0.148 {I7}:0.86 {I2}:1 (1980Da23); |a(K)exp=11.4 {I3} (1979Pl04); L1:L2:L3=0.159 {I13}:0.860 {I20}:1 and K/L/M/N=0.98 {I5}:1:0.20 {I1}:0.050 {I5} (1978Sh08); |a(K)exp=11.4 {I3}, |a(L1)exp=0.63 {I13}, |a(L2)exp=5.48 {I18}, |a(L3)exp=6.11 {I20}, |a(M)exp=2.40 {I8} (1976Dr07); L1:L2=0.994 {I12}, L1:L3=1.020 {I14} and L2:L3=0.99 {I2} (1975Ma32); L1:L2:L3=0.132 {I8}:0.830 {I20}:1 (1972Br02); |a(K)exp=10.6 {I5} (1970Ba37); K/(L+M+N)=0.76 {I2} (1969Pl08); |a(K)exp=12.7 {I9}, and K/(L+M)=0.76 {I2} (1968Fo03); |a(K)exp=11.3 {I4} K/(L+M)=0.866 {I27} (1965Se08); |a(K)exp=11.0 {I3}, |a(L)exp=11.7 {I8} and (|a(M)exp + |a(N)exp)=2.0 {I11} (1965Le06); K/L=0.95 {I3} (1964Bo12); |a(K)exp=10.3 {I5} (1957Wa05); |a(K)exp=9.5 {I1} and K/(L+M+N)=0.80 {I4} (1954Wa15); |a(K)exp=8.6 {I1} (1953Av25); |a(K)exp=12.4 {I10} and K/(L+M+N)=0.85 {I2} (1953Br73) 
$Double K-shell vacancy per K-shell internal conversion: 2.8|*10{+-5} 7 (1977Va05), 1.02|*10{+-5} 36 (1977Va05) and 1.53|*10{+-4} 24 (1975Na01). 
$Double photon decay: I(|g|g)/I(|g)<6|*10{+-7} (1988Il01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from |g(|q): A{-2}=-0.395 {I16} (1970Ro14), -0.39 {I2} (1955Mc51), -0.388 {I7} (1958Mc02), A{-2}=-0.710 {I7} (1970RoZS), and -0.654 {I36} (1989Lo08) 
MR$weighted average of 0.193 {i10} (1970RoZS), -0.196 {i27} (1970Ro14), and 0.19 {i1} (1958Mc02). Others: 0.19 (1955Mc51) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$Others: I(103.5|g)/I(415.1|g)=0.054 {i5} from 1989Lo08, 0.09 {i1} from 1967Bl08; I(103.5|g)=4.9 {i5} and I(415.1|g)=95.3 {i5} from 1970Ro14 
MR$from |g(|q) in 1970Ro14 
M$A{-2}=-0.239 {I17} (1970Ro14) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_uncertain: ?
decay_comment:
E$from level energy difference, weak branch seen by 1973Co10. 
RI$1970Ro14 set upper limit for branching of this |g as <0.2% 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.124 {I23} (1970Ro14), A{-2}=+0.248 {I4}, A{-4}=-0.039 {I9} (1955Mc51). Other values: A{-2}=+0.556 {I15}, A{-4}=-0.432 {I28} (1989Lo08), A{-2}=-0.515 {I10}, A{-4}=-0.401 {I11} (1970RoZS). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$Other: 43 {I3} (1967Bl08) 
M$A{-2}=+0.124 {I23} (1970Ro14), A{-2}=+0.32 {I10}, A{-4}=-0.11 {I15} (1989Lo08) 
MR$From |g(|q) in 1970Ro14; Other: -0.12 {I14} (1988Br31) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$From energy level differences 
CC$933 {I66}, calculated with the RAINE code using the same atomic and nuclear parameters as BRICC (T. Kibedi, private communication) 
M$From M1/M2/M3=0.3 {I1}/1.0/2.1 {I4}, N1/N2/N3=0.25 {I10}/1.00/2.0 {I6} 1993Ka37). Theoretical |a ratios for E1 transition (calculated by T. Kibedi with the RAINE code using the same atomic and nuclear parameters as BRICC by T. Kibedi): M1/M2/M3=0.3/1.0/2.2, N1/N2/N3=0.43/1.00/2.11 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_BM_unit: mu^2 x (fm)^6
decay_BM_info: ;TYPE=BM4;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM4W
decay_comment:
E$From {+110}Ag IT decay (249.83 d) (1990Me15) 
M$From conversion electron intensity ratios, K/L=2.04 {I6}, L1/L2=4.8 {I5}, L1/L3=1.02 {I2} (1965Ge01). Other: K/L=2.1 {I2} (1963Su07), K/L=1.95 {I10} (1965Ha07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$A{-2}=-0.142 {I5}, A{-4}=+0.019 {I8} (for E(p)=3.5 MeV), A{-2}=-0.149 {I16}, A{-4}=+0.019 {I8} (for E(p)=3.0 MeV) (1976Ha57); |a(K)exp=0.088, |a(L1)exp=0.0073 (1968El03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$From A{-2}=+0.235 {I13}, A{-4}=-0.030 {I22} (1976Ha57). Authors of 1976Ha57 assign this transition as Q(O), based on the measured |d=+0.034 {I61} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M$A{-2}=-0.084 {I4}, A{-4}=+0.014 {I6} (1976Ha57) and from |a(K)exp=0.048 {I3}, |a(L1)exp=0.0055 {I8} (1968El03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M$A{-2}=+0.013 {I9}, A{-4}=+0.026 {I16} (1976Ha57), coefficient of summed angular distribution for 265.7|g and 267.0|g and from |a(K)exp=0.017 {I1} (1968El03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$From |a(K)exp=0.00639 {I6} calculated by the evaluators using I|g and I{-e} in 1968El03. Note that I|g quoted by the authors are same for both 235.75|g and 237.05|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
E,RI$266.95 {I10} (I|g(266.95)=57) and 268.77 {20} (I|g(268.77)=14) were reported in 1971Gu05 but depopulating state(s) were not specified by the authors. Evaluators adopted I|g(268.77) (assuming that this transition in 1971Gu05 corresponded 267.22 keV transition in 1979Bo41). See 1970Ka05 for different intensities 
M$|a(K)exp=0.017 {I1}. |a(K)exp was measured for 266.95 keV transition in 1968El03. The authors did not observe any close |g-ray transition and placed it depopulating 270.2 keV level. Evaluators assigned (M1) mult for 267.22|g based on the decay pattern 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$From 1993Ka37 
RI$Estimated by the evaluators using I(|g+ce) and |a 
M$M1/M2/M3=0.3 {I1}/1.0/2.1 {I4}, N1/N2/N3=0.25 {I10}/1.00/2.0 {I6} (1993Ka37). Theoretical Ice ratios (calculated by T. Kibedi, priv. communication) with the RAINE code using the same atomic and nuclear parameters as BRICC by T. Kibedi): M1/M2/M3=0.3/1.0/2.2, N1/N2/N3=0.43/1.00/2.11 
CC$933 {I66}, calculated with the RAINE code using the same atomic and nuclear parameters as BRICC (T. Kibedi, private communication) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
E$From 1990Me15 
RI$From I(|g+ce) and |a. Other: 0.0085 {I3} in 1990Me15 relative to I|g(658)=100 
M$From K/L=2.04 {I6}, L1/L2=4.8 {I5}, L1/L3=1.02 {I2} (1965Ge01). Other: K/L=2.1 {I2} (1963Su07), K/L=1.95 {I10} (1965Ha07) 


decay_energy_unit: KEV
decay_multipolarity: D+Q
decay_comment:
E$From 1976Ha57. Other: 117 keV {i1} in 1974Be47 
M$A{-2}=-0.142 {I5}, A{-4}=+0.019 {I8} (for E(p)=3.5 MeV), A{-2}=-0.149 {I16}, A{-4}=+0.019 {I8} (for E(p)=3.0 MeV) 


decay_energy_unit: KEV
decay_comment:
M$A{-2}=+0.115 {I4}, A{-4}=+0.003 {I6}, coefficient of summed angular distribution for 235.35|g, 235.55|g and 236.66|g from 1976Ha57 (no mult assignment) 


decay_energy_unit: KEV
decay_comment:
M$A{-2}=+0.013 {I9}, A{-4}=+0.026 {I16}, coefficient of summed angular distribution for 265.7|g and 267.0|g 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E$transition not observed. Energy estimated by 2018Da15 from level-energy difference, and consistency with 7- to 6- transitions in odd-odd Ag isotopes, for example E|g=64.2 keV in {+106}Ag and 59.0 keV in {+108}Ag. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
RI$from 1969Be11. Others: 43 {i5} (1977Kr14), 79 {i21} (1969Sc12) 
M$from L1/L2/L3=7.0 {i15}/100/130 {i2}, K/L=0.64 {i20} (1978Sh08) HF(E3,59.8|g)=21 W.u. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+(E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
RI$from I(|g+ce) and |a. Others: 80 {i5} (1969Be11), 106 {i21} (1969Sc12), 50 {i8} (1977Kr14). |d|<0.12 deduced by 1976Sv04 from L-subshell ratios 
TI$from an intensity balance at the 130 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$the placement of this |g and the two levels (568.5,568.8) are based on coincidence work of 1987Ze04 in ({+3}He,pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$assigned also to 1062.2 level; however, branching in ({+3}He,pn|g) suggests that all the intensity belongs with the 1085.7 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$assigned also to 1120 level by 1969Be11 but branching in ({+3}He,pn|g) is consistent with placement entirely from 1190 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$I|g:I|g(834|g):I|g(921|g)=1.09 {I24}: 1.0 {I7}: 2.90 {I12} in ({+3}He,pn|g) suggests that only part of the 603|g should be assigned as deexciting the 1210 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$placement from 1974Bu15; deexcites 1705 and/or 1519 levels (1969Be11,1969Sc12), placement in ({+3}He,pn|g) is from 1210 and 642 levels 
RI$from I|g=7.0 {I5} for the doubly placed 641.9|g and I|g deduced for placement from the 642 level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$from I|g=3.2 {I4} for the doubly placed 809|g (weighted average of 3.4 {i5} (1977Kr14), 3.0 {i15} (1969Be11), 2.6 {i8} (1969Sc12) and I|g deduced for placement from the 809 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E$from 1978Sh08 (ce). Others: 59.9 {i1} (1969Be11), 59.8 {i1} (1969Sc12), 59.8 {i3} (1977Kr14) 
TI$calc to achieve intensity balance about 59.8 level. 
RI$from I(|g+ce) and |a. Measured I|g=35 {i8} (1969Be11,1977Kr14) for equilibrium 5.5-h + 23-min source 
M$from L1:L2:L3=7.0 {i15}:100:130 {i2}, K/L=0.64 {i20} (1978Sh08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
E$from 1976Sv04. Other: 70.4 {i3} (1977Kr14) 
RI$from 1969Be11. Others: 414 {i60} (1977Kr14), 486 {i100} (1969Sc12) 
M,MR$from L1:L2:L3=100 {i8}:11 {i8}: <8 (1976Sv04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from 1988Br31. |d=-0.014 {i46} or +8.1 +4.9-2.3. The measured |g(|q) gives a strong preference for the larger value. 
RI$69 {i6} doublet resolved via |g|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$assigned by 1977Kr14 to the 1987 level. Reassigned by the evaluator to the 876 level, on the basis of branching in 23-min |b{+-} decay and in ({+3}He,pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$other: |d=-20 {I+28-6}. The negative anisotropy favors the smaller value in agreement with 1987Ze04. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$assigned to 1549.5 by 1974Bu15 and 1969Sc12; however, a 724.52 in ({+3}He,pn|g) is assigned to a 1748 level. This placement is consistent with the (724.8|g)(633|g) coin reported by 1977Kr14 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from I|g=8.7 {I16} for the doubly placed 828|g and value deduced for placement from the 959 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$I|g=0.7 {I22} from I|g=3 {I2} for the doubly placed 1029|g and I|g=2.3 {I9} deduced for placement from the 1159.5 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E$from 1978Sh08 (ce). Other: 59.82 {I8} (1977Kr14) 
M$from K/L, L-subshell ratio data (1978Sh08) in {+111}Pd decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
RI$the decay of the 64.8-s isomer in {+111}Ag is assumed to be in secular equilibrium with the decay of 23.6-min {+111}Pd 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E$from decay of 23.6-min {+111}Ag (2015Kr07). In the decay of isomer decay, 2015Kr07 give 59.7 {I2} 
RI$deduced by compiler from I(|g+ce) intensity=993 {I80} deduced from I(|g+ce)=1000 {I80} feeding the 59.85 level, %IT=99.3 {I2} for the decay of the 59.85 isomer, and conversion coefficient for E3 multipolarity of 59.85|g. 2015Kr07 give 5 {I3} from direct, but imprecise, |g-ray measurement in the decay of the isomer 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$2015Kr07 assign this transition from 808.8 level based on comparison of |g-branching ratios with results from ({+3}He,pn|g) study by 1987Ze04 (Phys. Rev. C36, 939) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Previous placement from 1964 to 824 level is inconsistent with the transition energy. 2015Kr07 place it tentatively from 1821 level to 683 level due to its better fit 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
RI$total intensity of the doublet and division of intensity in 2015Kr07 is different from those in previous studies. Results in 2015Kr07 are an improvement due to better resolution 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: S
decay_comment:
E$from {+111}Ag Adopted dataset in the ENSDF database. This |g, listed in Table VIII of 2017La17, was not observed in the present experiment 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
RI$from I(|g+ce) and |a=2.71. 
RI$|?0.08 photons per 617|g in {+112}Ag reported by 1955Nu11 corresponds to I|g(18.5|g)=3.4 which is much smaller than the value of 27 obtained with the assumption of a pure E1. 
TI$from the assumption that 100% of the decay of {+112}Pd passes through the 18.5-keV level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$Branching ratio: I|g(631)/I|g(97)=100.0/28.5 (from Table VIII in 2017La17); same as deduced from I|g values in authors' Table III. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI$ 14 {I4}, combined intensity in 2012Ri05. It seems I|g=14 is a misprint in paper, it should probably be 4 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI$ 14 {I4}, combined intensity in 2012Ri05 It seems I|g=14 is a misprint in paper, it should probably be 4 {I4} 


decay_energy_unit: KEV
decay_multipolarity: E3
decay_BE_unit: e^2 x (fm)^6
decay_BE_info: ;TYPE=BE3;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE3W
decay_comment:
E$the isomeric transition was identified by decomposing a complex line where the x-rays are dominant. 
M$from K/L 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 382.4 {I5} (2013La11) and 383.8 {I3} (2006ToZW). Others: 385.3 {I2} (unplaced in 2009St28), 383.1 (2019Ch24) 
RI$weighted average of 5.5 {I7} (2013La11), 4 {I1} (2009St28), and 6 {I2} (2006ToZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 2013La11. Others: 597.6 {I6} (unplaced in 2009St28), 594.0 (2019Ch24). This |g is not reported in 2006ToZW but an unlabelled peak around this energy is seen in the |g spectrum in Fig 4.33. 
RI$weighted average of 6.5 {I8} (2013La11) and 7 {I2} (2009St28). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 389.5 {I5} (2013La11) and 390.8 {I3} (2006ToZW). Others: 391.2 {I3} (unplaced in 2009St28), 390.1 (2019Ch24) 
RI$unweighted average of 8.8 {I9} (2013La11), 4 {I1} (2009St28), and 3 {I3} (2006ToZW). In the level scheme of 2019Ch24, this |g is indicated much weaker than both 593|g and 383|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 629.1 {I5} (2013La11) and 630.1 {I1} (2006ToZW). Other: 632.9 {I1} (2009St28) 
RI$weighted average of 32.7 {I15} (2013La11), 37 {I4} (2009St28), and 33 {I3} (2006ToZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 713.2 {I5} (2013La11) and 714.0 {I1} (2006ToZW). Other: 716.7 {I2} and 714 with combined I|g=100 {I7} in 2009St28. Doublet at 713 keV was not confirmed by 2013La11, who place the 713|g above the 27 level, whereas 2009St28 placed a 714|g as a ground-state transition, and 717|g from a 1430 level. 
RI$other: 100 {I4} in 2006ToZW 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$others: 1049.3 {I6} (2006ToZW), 1052.1 {I5} (2009St28) 
RI$weighted average of 9.1 {I9} (2013La11), 17 {I3} (2009St28), and 11 {I5} (2006ToZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1076.3 {I5} (2013La11) and 1076.6 {I3} (2006ToZW). Other: 1079.4 {I5} (2009St28) 
RI$weighted average of 19.5 {I13} (2013La11), 22 {I3} (2009St28), and 16 {I3} (2006ToZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 348.7 {I5} (2013La11) and 349.5 {I1} (2006ToZW). Other: 351.4 {I1} (2009St28) 
RI$unweighted average of 42.8 {I14} (2013La11), 36 {I3} (2009St28), and 37 {I2} (2006ToZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 684.7 {I5} (2013La11) and 685.6 {I1} (2006ToZW). Other: 687.3 {I1} placed from 714 level (2009St28) 
RI$weighted average of 84.5 {I23} (2013La11), 78 {I6} (2009St28), and 80 {I7} (2006ToZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 768.8 {I5} (2013La11) and 769.8 {I1} (2006ToZW). Other: 771.6 {I4} (2009St28) 
RI$weighted average of 29.5 {I15} (2013La11), 31 {I4} (2009St28), and 26 {I2} (2006ToZW) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_uncertain: S
decay_comment:
TI$deduced by evaluator from |g+ce intensity balance at 1426 level, with negligible contributions from internal conversion of |g rays de-exciting 1426 level 
RI$|g not observed experimentally, I|g deduced from the intensity balance at the 1426-keV level, and conversion coefficient=19.9 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_comment:
E$weighted average of 732.1 {I5} (2013La11) and 732.9 {I3} (2006ToZW). Other: 735.1 {I3} unplaced in 2009St28 
RI$unweighted average of 15.4 {I11} (2013La11), 8 {I2} (2009St28), and 6 {I3} (2006ToZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
$E|g=75, I|g=74 {I38} (2013La11) 
$|a(exp)=0.8 {I10} if mult(155|g)=E2, 0.4 {I8} if mult(155|g)=E2 (2013La11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=669.8 5, IG=90 3 (2013La11) 
$EG=669.8 5, IG=77 9 (2012Ka36) placed from a 1398, (13/2-) level 
$EG=672.1 3, IG=77 18 (2009St28); earlier values: EG=670.1 3, IG=69 19 (2006ToZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=714.1 5, IG=100 (2013La11) 
$EG=714.5 5, IG=100 11 (2012Ka36) 
$EG=716.6 4, IG=90 22 (2009St28) placed from 1398 level; earlier values: EG=713.9 2, 49 13 (2006ToZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=683.4 5, IG=73 3 (2013La11) 
$EG=684.0 5, IG=76 9 (2012Ka36) 
$EG=686.3 4, IG=100 22 (2009St28) placed from a 686, (11/2+) level; earlier values: EG=684.4 3, IG=100 24 (2006ToZW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=728.3 5, IG=80 3 (2013La11) 
$EG=728.4 5, IG=76 10 (2012Ka36) placed from a 728, (11/2-) level 
$EG=731.9 2, IG=75 19 (2009St28); earlier values: EG=729.1 2, IG=77 16 (2006ToZW) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$this |g ray is proposed by the evaluator to be the same as 254.8 in 2012Ka36 and 254 in 2013La11, placed from a 254.8+x level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$150 {I+14-20} from measured E(ce) in the ce spectrum gated by the sum of all subsequent |g transitions (2021Wa49) 
RI$3.3 {I+14-15} estimated from |g+ce intensity balance (2021Wa49) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1395.5 {I2} in {+98}In decay (0.89 s), 1394.8 {I2} in ({+58}Ni,|a2n|g) and 1395.1 {I3} in ({+46}Ti,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 687.8 {I2} in {+98}In decay (0.89 s), 687.7 {I3} in ({+58}Ni,|a2n|g) and 687.7 {I2} in ({+46}Ti,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 198.4 {I1} in {+98}In decay (0.89 s) and 198.1 {I2} in ({+58}Ni,|a2n|g). Other: 197.6 {I1} in ({+46}Ti,|a2n|g), seems low in energy as compared to the other two values. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 147.2 {I1} in {+98}In decay (0.89 s) and 147.2 {I2} in ({+58}Ni,|a2n|g). Other: 146.5 {I2} in ({+46}Ti,|a2n|g), seems low in energy as compared to the other two values. 
M$from |a(K)exp in ({+58}Ni,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1394.9 {I2} (2004Bl10) and 1394.7 {I3} (1997Go18) 
RI$from 1997Go18 and 2004Bl10 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 687.8 {I3} (2004Bl10) and 687.6 {I3} (1997Go18) 
RI$weighted average of 105 {I15} (2004Bl10) and 102 {I15} (1997Go18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$weighted average of 198.2 {I2} (2004Bl10) and 197.9 {I3} (1997Go18) 
RI$weighted average of 80 {I15} (2004Bl10) and 87 {I11} (1997Go18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 147.1 {I2} (2004Bl10) and 147.3 {I3} (1997Go18) 
RI$weighted average of 70 {I15} (2004Bl10) and 75 {I10} (1997Go18) 
M$from |a(K)exp. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
$This |g not observed by 2019Pa16. From the upper limit of 8% for |e+|b{++} feeding quoted in 2019Pa16, I|g<14 


decay_energy_unit: KEV
decay_comment:
E$4157.9 {I2} with statistical uncertainty, and 4158 {I2} with systematic uncertainty considered (priv. comm. Dec 14, 2019 from J. Park, first author of 2017Pa35). Other: 4157 {I3} (2010Bl13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_uncertain: S
decay_comment:
$B(E2)(W.u.)=1.99 {I25} in 2017Pa35 is based on E|g=49.2 {I2} and corresponding conversion coefficient. Based on E|g=49 {I2}, value is 2.0 {I9} in the Adopted dataset. 
E$this |g is not observed in 2017Pa35, its energy of 49.2 {I2} given by the authors was deduced from the difference in energy of the 4207.0 {I1} and 4157.9 {I2} with statistical uncertainty. Inclusion of the systematic uncertainty gives E|g=49 {I2} keV (priv. comm. Dec 14, 2019 from J. Park, first author of 2017Pa35). 
TI$from the observed ratio I|g(4158|g)/I|g(4207|g), and equating the intensity of the 4158|g with the transition intensity of the 49-keV |g ray (priv. comm. Dec 14, 2019 from J. Park, first author of 2017Pa35) 
RI$deduced from I(|g+ce) and |a 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E4]
decay_BE_unit: e^2 x (fm)^8
decay_BE_info: ;TYPE=BE4;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE4W
decay_comment:
E$4207.0 {I1} with statistical uncertainty, and 4207 {I2} with systematic uncertainty considered (priv. comm. Dec 14, 2019 from J. Park, first author of 2017Pa35) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$search for depopulating transition of 4157 keV did not reveal a statistically significant peak (2019Pa16). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 1004.1 {I1} from {+100}In |e decay (5.8 s), 1004.2 {I2} from ({+58}Ni,2p2n|g), and 1004.03 {I17} from ({+40}Ca,2p2n|g). Other: 1004 {I15} from ({+102}Cd,{+100}Cd|g) 
M$supported by |g(|q) in ({+40}Ca,2p2n|g) and level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 794.9 {I1} from {+100}In |e decay (5.8 s), 795.1 {I2} from ({+58}Ni,2p2n|g), and 795.02 {I21} from ({+40}Ca,2p2n|g). Other: 760 {I15} from ({+102}Cd,{+100}Cd|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1041.9 {I2} from {+100}In |e decay (5.8 s) and 1042.3 {I2} from ({+58}Ni,2p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 296.8 {I1} from {+100}In |e decay (5.8 s), 296.1 {I1} from ({+58}Ni,2p2n|g), and 296.27 {I17} from ({+40}Ca,2p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 362.7 {I1} from {+100}In |e decay (5.8 s) and 362.4 {I1} from ({+58}Ni,2p2n|g) 
RI$other: 100 {I11} from {+100}In |e decay 
RI$weighted average of 31 {I5} from {+100}In |e decay (5.8 s) and 32 {I4} from ({+58}Ni,2p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 411.7 {I3} from {+100}In |e decay (5.8 s) and 411.5 {I1} from ({+58}Ni,2p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 658.2 {I3} from {+100}In |e decay (5.8 s) and 658.5 {I2} from ({+58}Ni,2p2n|g) 
RI$weighted average of 47 {I5} from {+100}In |e decay (5.8 s) and 43 {I5} from ({+58}Ni,2p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 452.8 {I1} from {+100}In |e decay (5.8 s), 452.5 {I1} from ({+58}Ni,2p2n|g), and 452.56 {I17} from ({+40}Ca,2p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1004.1 {I2} (2000Cl01) and 1004.5 {I3} (1994Go38) 
RI$from 1994Go38. Other: 100 {I4} (2000Cl01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 795.0 {I2} (2000Cl01) and 795.2 {I3} (1994Go38) 
RI$weighted average of 94 {I3} (2000Cl01) and 98 {I3} (1994Go38). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 247.3 {I1} (2000Cl01) and 247.1 {I3} (1994Go38) 
RI$weighted average of 1.0 {I3} (2000Cl01) and 0.4 {I2} (1994Go38). 
$I|g(247|g)/I|g(1042|g)=0.4 {I2}/1.9 {I11} (1994Go38) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1042.2 {I2} (2000Cl01) and 1042.5 {I3} (1994Go38) 
RI$weighted average of 2.6 {I6} (2000Cl01) and 1.9 {I11} (1994Go38). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 296.1 {I1} (2000Cl01) and 296.1 {I3} (1994Go38) 
RI$weighted average of 88 {I3} (2000Cl01), 95 {I3} (1994Go38) and 102 {I10} (1992Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 362.4 {I1} (2000Cl01) and 362.2 {I3} (1994Go38) 
RI$weighted average of 8.6 {I9} (2000Cl01) and 10.3 {I8} (1994Go38). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 411.5 {I1} (2000Cl01) and 411.5 {I3} (1994Go38) 
RI$weighted average of 3.1 {I4} (2000Cl01) and 2.4 {I8} (1994Go38). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 658.5 {I2} (2000Cl01) and 658.5 {I3} (1994Go38) 
RI$weighted average of 4.2 {I5} (2000Cl01) and 3.8 {I9} (1994Go38). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$weighted average of 90.7 {I1} (2000Cl01) and 90.4 {I3} (1994Go38) 
RI$unweighted average of 5.6 {I8} (2000Cl01) and 2.3 {I4} (1994Go38). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 452.5 {I1} (2000Cl01) and 452.5 {I3} (1994Go38) 
RI$unweighted average of 85 {I3} (2000Cl01) and 87.4 {I25} (1994Go38). Other: 111 {I11} (1992Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$from 1992Al17 
$Ordering of 1108.6-461.7 is reversed in earlier (1994Go38) studies 
$EG=1111 (1994Go38, 1992Al17) 
$R=0.85 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$Ordering of 1108.6-461.7 is reversed in earlier (1994Go38) studies 
$E|g=463 (1994Go38). I|g=86 {I9} (1992Al17) 
$R=1.30 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$Other: 49 {I15} (1996Ra23) 
M$From 2001Li24, no |d given. M1/E2 from (1997Pe25) 
M$Measured short lifetime excludes parity change (2001Li24) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$From (HI,xn|g) in 2001Li24. Other: d from (HI,xn|g) in 1997Pe25. Measured short lifetime excludes parity change (2001Li24) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From (HI,xn|g) 2001Li24, . Other d (1997Pe25) 
M$Measured short lifetime excludes parity change (2001Li24) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From (HI,xn|g) 2001Li24. Other d (1997Pe25) 
M$Measured short lifetime excludes parity change (2001Li24) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
R=1.16 {i4} 
$A{-22}=+0.09 {i4}; a{-44}=+0.03 {i5}; Pol=-0.06 {i6} 
M$A{-22}, A{-44} and Pol for multiplet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=+0.34 {I4}; A{-4}=-0.21 {I6}; Pol=+0.2 {I2} 
J{-i}-J{-f}=0,-2 from |g(|q) and linear polarization 


decay_energy_unit: KEV
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E,M,MR$ from Adopted Gammas for {+103}Cd in ENSDF database 
$Compilers get B(M1)(W.u.)=0.0082 {I7}, B(E2)(W.u.)<2.3. 2011Ki17 did not seem to include conversion coefficient of 188|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.20 {I10} or (+0.84 {I18}) 
A{-2}=+0.20 {I4} 
A{-4}=-0.05 {I5} 
E$level-energy difference=308.4 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=-0.176~{I14} and A{-4}=-0.033~{I16} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=0.56~{I3} in {+92}Mo({+16}O,2pn|g) (2015Ra02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.61~{I7} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=0.176~{I10}; A{-44}=0.000~{I13} and Pol{-exp}/Pol{-ad}=0.56~{I38} in {+94}Zr({+16}O,5n|g) (1978St01); A{-2}=+0.20~{I2}; A{-4}=+0.030~{I26} in {+102}Pd(|a,n|g) (1978Ge05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.62~{I14} (2015Ra02); Pol=-0.004~{I8} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=-0.704~{I29} and A{-44}=0.17~{I4} in {+94}Zr({+16}O,5n|g) (1978St01) and Pol{-exp}/Pol{-ad}=0.9~{I11} in {+94}Zr({+16}O,5n|g) (1978St01); A{-2}=-0.73~{I3}; A{-4}=+0.10~{I5} in {+102}Pd(|a,n|g) (1978Ge05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.52~{I3} and Pol=-0.03~{I3} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=-0.185~{I12} and A{-44}=0.139~{I18} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=0.63~{I38} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.35~{I5} and A{-4}=-0.13~{I9} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=1.11~{I5} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=0.190~{I32} and A{-44}=-0.06~{I4} in {+94}Zr({+16}O,5n|g) (1978St01) and Pol{-exp}/Pol{-ad}=1.0~{I7} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.30~{I2} and A{-4}=-0.12~{I3} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=0.98~{I4} and Pol=+0.12~{I3} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}= 0.212~{I10} and A{-44}=-0.041~{I14} in {+94}Zr({+16}O,5n|g) (1978St01) and Pol{-exp}/Pol{-ad}=1.17~{I19} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
M$A{-2}=-0.31~{I9}; A{-4}=0.000~{I14} in {+102}Pd(|a,n|g) (1978Ge05); Also, R{-DCO}=0.55~{I4} in {+92}Mo({+16}O,2pn|g) (2015Ra02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.82~{I10} and A{-4}=-0.13~{I15} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=0.65~{I11} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=-0.50~{I5} and A{-44}=0.13~{I8} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=1.7~{I8} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.30~{I3} and A{-4}=-0.08~{I4} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=0.97~{I6} and Pol=+0.09~{I4} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=0.267~{I12} and A{-44}=-0.088~{I17} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=0.92~{I32} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.28~{I2} and A{-4}=-0.01~{I4} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=1.29~{I10} and Pol=+0.07~{I3} in {+92}Mo({+16}O,2pn|g) (2015Ra02). Also, A{-22}=-0.251~{I9} and A{-44}=0.024~{I9} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=-0.97~{I25} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$A{-2}=-0.27~{I3}; A{-4}=-0.02~{I4} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=0.55~{I3} and Pol=+0.07~{I3} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=-0.239~{I12} and A{-44}=0.025~{I13} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=-1.08~{I22} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.85~{I15} and A{-4}=+0.1~{I2} in {+102}Pd(|a,n|g) (1978Ge05); Also, R{-DCO}=0.63~{I7} (2015Ra02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.30~{I4} and A{-4}=-0.12~{I6} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=0.99~{I3} and Pol=+0.04~{I4} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=0.155~{I18} and A{-44}=-0.065~{I25} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=1.4~{I6} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.29~{I3} and A{-4}=-0.07~{I4} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=0.96~{I6} and Pol=+0.13~{I3} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=0.231~{I16} and A{-44}=-0.042~{I26} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=1.36~{I30} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.28~{I3}; A{-4}=-0.13~{I4} in {+102}Pd(|a,n|g) (1978Ge05); Pol=+0.13~{I2} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=0.281~{I8} and A{-44}=-0.097~{I10} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=0.87~{I10} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+(E2)
decay_comment:
M$A{-2}=-0.73~{I30} and A{-4}=+0.4~{I4} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=0.59~{I7} and Pol=-0.03~{I4} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=-0.12~{I4} and A{-44}=0.05~{I5} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=1.0~{I15} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.14~{I11} and A{-4}=-0.13~{I18} in {+102}Pd(|a,n|g) (1978Ge05); Also, R{-DCO}=1.19~{I11} in {+92}Mo({+16}O,2pn|g) (2015Ra02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.29~{I5} and A{-4}=-0.14~{I8} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=0.98~{I3} (2015Ra02) and Pol=+0.07~{I3} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=0.277~{I10} and A{-44}=-0.106~{I13} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=0.99~{I20} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$A{-2}=+0.02~{I9} and A{-4}=-0.14~{I16} in {+102}Pd(|a,n|g) (1978Ge05); Also, R{-DCO}=0.97~{I3} in {+92}Mo({+16}O,2pn|g) (2015Ra02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$A{-2}=+0.38~{I10} and A{-4}=-0.29~{I17} in {+102}Pd(|a,n|g) (1978Ge05); R{-DCO}=0.97~{I8} and Pol=+0.08~{I2} in {+92}Mo({+16}O,2pn|g) (2015Ra02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=-0.20~{I17} and A{-4}=-0.16~{I27} in {+102}Pd(|a,n|g) (1978Ge05) R{-DCO}=0.95~{I5} and Pol=+0.10~{I3} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=0.331~{I16} and A{-44}=-0.113~{I23} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=0.43~{I25} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=0.96~{I5} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Pol=+0.04~{I2} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Also, A{-22}=0.185~{I29}; A{-44}=-0.03~{I4} in {+92}Mo({+16}O,2pn|g) (1978St01); Pol{-exp}/Pol{-ad}=1.2~{I7} in {+92}Mo({+16}O,2pn|g) (1978St01); 
M$R{-DCO}=1.06~{I11} in {+76}Ge({+34}S,5n|g) (1995Je04) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=1.12~{I16} in {+76}Ge({+34}S,5n|g) (1995Je04); Also, R{-DCO}=0.98~{I6} and Pol=+0.12~{I7} in {+92}Mo({+16}O,2pn|g) (2015Ra02); Others: A{-22}=0.22~{I4} and A{-44}=-0.08~{I6} in {+94}Zr({+16}O,5n|g) (1978St01); Pol{-exp}/Pol{-ad}=1.0~{I15} in {+94}Zr({+16}O,5n|g) (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$E2 in 1995Je04, from R{-DCO}=0.91~{I30}. M1 in 2015Ra02, from R{-DCO}=0.48~{I11} and Pol=-0.02~{I8} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=1.11~{I23} in {+76}Ge({+34}S,5n|g) (1995Je04); Also, R{-DCO}=1.05~{I11} and Pol=+0.08~{I5} in {+92}Mo({+16}O,2pn|g) (2015Ra02) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from the adopted gammas; Also, R{-DCO}=0.61~{I7} (2015Ra02); A{-22}=0.176~{I10}, A{-44}=0.000~{I13} (1978St01) and Pol{-exp}/Pol{-ad}=0.56~{I38} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.62~{I14} (2015Ra02); Pol=-0.004~{I8} (2015Ra02) 
$Also, A{-22}=-0.704~{I29}; A{-44}=0.17~{I4} (1978St01); Pol{-exp}/Pol{-ad}=0.9~{I11} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.52~{I3} (2015Ra02); Pol=-0.03~{I3} (2015Ra02) 
$Also, A{-22}=-0.185~{I12}; A{-44}=0.139~{I18} (1978St01); Pol{-exp}/Pol{-ad}=0.63~{I38} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=1.11~{I5} (2015Ra02) 
$Also, A{-22}=0.190~{I32}; A{-44}=-0.06~{I4} (1978St01); Pol{-exp}/Pol{-ad}=1.0~{I7} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=0.98~{I4} (2015Ra02); Pol=+0.12~{I3} (2015Ra02); 
$Also, A{-22}= 0.212~{I10}; A{-44}=-0.041~{I14} (1978St01); Pol{-exp}/Pol{-ad}=1.17~{I19} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$R{-DCO}=0.65~{I11} (2015Ra02) 
$Also, A{-22}=-0.50~{I5}; A{-44}=0.13~{I8} (1978St01); Pol{-exp}/Pol{-ad}=1.7~{I8} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=0.97~{I6} (2015Ra02); Pol=+0.09~{I4} (2015Ra02) 
$Also, A{-22}=0.267~{I12}; A{-44}=-0.088~{I17} (1978St01); Pol{-exp}/Pol{-ad}=0.92~{I32} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$R{-DCO}=1.29~{I10} (2015Ra02); Pol=+0.07~{I3} (2015Ra02) 
$Also, A{-22}=-0.251~{I9}; A{-44}=0.024~{I9} (1978St01); Pol{-exp}/Pol{-ad}=-0.97~{I25} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$R{-DCO}=0.55~{I3} (2015Ra02); Pol=+0.07~{I3} (2015Ra02) 
$Also, A{-22}=-0.239~{I12}; A{-44}=0.025~{I13} (1978St01); Pol{-exp}/Pol{-ad}=-1.08~{I22} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=0.99~{I3} (2015Ra02); Pol=+0.04~{I4} (2015Ra02) 
$Also, A{-22}=0.155~{I18}; A{-44}=-0.065~{I25} (1978St01); Pol{-exp}/Pol{-ad}=1.4~{I6} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=0.96~{I6} (2015Ra02); Pol=+0.13~{I3} (2015Ra02) 
$Also, A{-22}=0.231~{I16}; A{-44}=-0.042~{I26} (1978St01); Pol{-exp}/Pol{-ad}=1.36~{I30} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$Pol=+0.13~{I2} (2015Ra02) 
$Also, A{-22}=0.281~{I8}; A{-44}=-0.097~{I10} (1978St01); Pol{-exp}/Pol{-ad}=0.87~{I10} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$R{-DCO}=0.59~{I7} (2015Ra02); Pol=-0.03~{I4} (2015Ra02) 
$Also, A{-22}=-0.12~{I4}; A{-44}=0.05~{I5} (1978St01); Pol{-exp}/Pol{-ad}=1.0~{I15} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=1.19~{I11} (2015Ra02); 
$Also, A{-22}=0.128~{I22}; A{-44}=-0.005~{I31} (1978St01); Pol{-exp}/Pol{-ad}=2.0~{I7} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=0.98~{I3} (2015Ra02); Pol=+0.07~{I3} (2015Ra02) 
$Also, A{-22}=0.277~{I10}; A{-44}=-0.106~{I13} (1978St01); Pol{-exp}/Pol{-ad}=0.99~{I20} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=0.95~{I5} (2015Ra02); Pol=+0.10~{I3} (2015Ra02) 
$Also, A{-22}=0.331~{I16}; A{-44}=-0.113~{I23} (1978St01); Pol{-exp}/Pol{-ad}=0.43~{I25} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=0.96~{I5} (2015Ra02); Pol=+0.04~{I2} (2015Ra02) 
$Also, A{-22}=0.185~{I29}; A{-44}=-0.03~{I4} (1978St01); Pol{-exp}/Pol{-ad}=1.2~{I7} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$R{-DCO}=0.79~{I10} (2015Ra02); Pol=-0.12~{I4} (2015Ra02) 
$DCO is lower than expected value of |?1 for |DJ=0, dipole 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$R{-DCO}=0.98~{I6} (2015Ra02); Pol=+0.12~{I7} (2015Ra02) 
$Also, A{-22}=0.22~{I4}; A{-44}=-0.08~{I6} (1978St01); Pol{-exp}/Pol{-ad}=1.0~{I15} (1978St01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI$Uncertinaty increased by the evaluators, since 0.05 quoted by the authors seems unrealistically low 
M$R{-DCO}=0.97~{I9} (2015Ra02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR from (n,n'|g). Others: -0.85 {I20} from |g(|q) in {+106}Cd(|a,|a'|g|g) (1973Gr16) and -0.60 {I+20-15} 1084|g(|q) in {+106}Cd(p,p'|g) (1969Mi07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
MR weighted average of |d=-0.31 {I5} from {+94}Zr({+16}O,4n|g); -0.34 {I4} from {+96}Mo({+13}C,3n|g); -0.4 {I6} from {+97}Mo({+12}C,3n|g); -0.30 {I3} from {+106}Cd(n,n'|g) 
M other: E2 from conversion electron data in {+106}In |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from |g(|q) and |g linear pol in (n,n'|g) 
MR weighted average of |d=-0.5 {I9} from |g|g(|q) in {+97}Mo({+12}C,3n|g) |d=0.00 {I22} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) and from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|d=-0.58 {I12} from |g(|q) in {+96}Mo({+13}C,3n|g); -0.27 {I4} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or -0.57 {I12} from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|d=-0.24 {I19} from |g|g(|q) in {+97}Mo({+12}C,3n|g); -0.03 {I5} or -5.4 {I+21-12} from |g(|q) in (n,n'|g); |d=-0.18 {I5} from |g(|q) in {+96}Mo({+13}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M from conversion electron data in {+106}In |e decay (5.2 min) and from change in sign of 525|g pol via |g(|q) versus |g-ray linear pol in {+94}Zr({+16}O,4n|g). Others: D+Q and |d=-0.046 {I15} from |g(|q) in {+96}Mo({+13}C,3n|g); |d=+0.076 {I18} from |g|g(|q) in {+97}Mo({+12}C,3n|g); |d=-0.05 {I3} from |g(|q) in (n,n'|g) and |d=0.00 {I5} from {+94}Zr({+16}O,4n|g). From RUL, one expects |d<0.012 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR weighted average of |d=+0.02 {I9} from |g|g(|q) in {+97}Mo({+12}C,3n|g) and |d=+0.063 {I27} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E,RI taken from {+106}In |e decay (6.2 min) 
M from conversion electron data in {+106}In |e decay (6.2 min). Others: D+Q and |d=-0.29 {I17} from |g(|q) in {+96}Mo({+13}C,3n|g) and |d=+0.06 {I27} from |g|g(|q) in {+97}Mo({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|d=-0.27 {I17} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=-0.16 {I5} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR other: +0.03 {I8} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or -0.03 {I2} from |g(|q) in {+96}Mo({+13}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E,RI from {+106}In |e (6.2 min) 
|d=+0.13 {I21} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=+0.039 {I6} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Weighted average of |d=+0.57 {I22} from linear |g pol in ({+16}O,xn); +1.22 {I28} from |g(|q) in {+97}Mo({+12}C,3n|g) or |d=+0.71 {I7} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
|d=+0.10 {I19} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=+0.09 {I18} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|d=-0.28 {I16} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=-0.02 {I6} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|d=+0.23 {I10} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=+0.02 {I23} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|d=+0.026 {I54} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=-0.014 {I32} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|d=-0.02 {I10} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=-0.023 {I29} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|d=+0.043 {I37} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=-0.016 {I10} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|d=-0.11 {I34} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=+0.25 {I36} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M M2 ruled out by RUL 
MR from |g(|q) in {+96}Mo({+13}C,3n|g). Other: |d=+0.15 {I2} from |g|g(|q) in {+97}Mo({+12}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
|d=+0.15 {I14} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=0.00 {I6} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|d=-0.02 {I6} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=-0.038 {I28} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
MR weighted average of |d=+0.26 {I34} from {+96}Mo({+13}C,3n|g) and |d=+0.3 {I3} from {+97}Mo({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR weighted average of |d=+0.45 {I15} from |g|g(|q) in {+97}Mo({+12}C,3n|g) and |d=+0.35 {I15} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|d=-0.10 {I4} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=+0.10 {I4} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|d=-0.05 {I3} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or |d=-0.019 {I11} from |g(|q) in {+96}Mo({+13}C,3n|g) (1979Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Weighted average of 1716.4 {I1} (1978Hu06),1716.7 {I2} (1984Ro10) and 1716.5 {I2} (2007Li07) 
RI calculated based on the weighted average of the ratio I|g(1084|g)/I|g(1716|g)=0.81 {I8} obtained from 0.70 {I9} (Coul. Ex); 1.02 {I19} (n,n'|g); 1.17 {I25} (p,p'|g) and 0.91 {I20} (p,2n|g). 
M$From 2007Li07 


decay_energy_unit: KEV
decay_comment:
E from 1992Ku01 
EKC |a(K)exp=0.00034 {I5} for doublet of 1619.6|g + 1621.4|g 
RI a value of 5.4 {I3} for the doublet of 1619.6|g + 1621.4|g is given for the decay of the two isomers together by (1992Ku01) 


decay_energy_unit: KEV
decay_comment:
EKC |a(K)exp=0.00034 {I5} for doublet of 1619.6|g + 1621.4|g 
RI a value of 5.4 {I3} for the doublet of 1619.6|g + 1621.4|g is given for the decay of the two isomers together by (1992Ku01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E from 1984Ro10. Others: 1714.7 {I3} (1992Ku01), 1716.4 (1978Hu06) 
RI obtained from I|g(doublet 1715|g)=20.3 - I|g(1716|g from 1716 level)=4.2 {I5} (1978Hu06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Weighted average of 2256.9 {I3} (1978Hu06 and 2256.8 {I3} (2007Li07) 
RI other: 4.9 {I9} (1976Fl14) 


decay_energy_unit: KEV
decay_comment:
$I|g(553)/I|g(557)/I|g(748)/I|g(1324)/I|g(1402)/I|g(2486)/ I|g(3118)= 12/4/15/3/7/100/96 (2007Li07) 
E$From 2007Li07 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Unassigned by 1988BeYC, but placed from the 2252 level in (p,p'|g). This placement is also suggested by 1993GoZZ (see also comment on 536|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E |h{+2}=15.6 when peak at 1620 keV analyzed as a single peak |h{+2}=3.5 if analyzed as a (1619.71|g 3 + 1621.27|g 3) doublet 
RI I|g(1619.71|g 3 + 1621.27|g 3)=4.6 {I6} 
MR |d=-11.2 {I+22-10} for (1619.71|g 3 + 1621.27|g 3) doublet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Transition is unassigned by 1988BeYC, but is placed from the 2254 level in (p,p'|g). 1993GoZZ suggest placement from the 2252 level, along with the 758|g, but these transitions have different excitation functions in (p,p'|g) so that even if the energy fit is much better with the 536|g deexciting the 2252.4 level (1716.5 + 536.2= 2252.7 {I3}) the 536|g and 758|g cannot deexcite the same level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E |h{+2}=15.6 when peak at 1620 keV analyzed as a single peak |h{+2}=3.5 if analyzed as a (1619.71|g 3 + 1621.27|g 3) doublet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI relative photon branchings in % from 1977Da08 (|a,2n|g) 
E from 1977Da08 (|a,2n|g). Other: 1085 {I1} (1969Mi07) 
MR from 1084|g(633|g)(|q) (1973Gr16); other: -0.60 {I+20-15} (1969Mi07) 1084|g(|q) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
M$Other: M1+E2 with |d=-0.03 {I2} (1979Sa01) 
$ J|p=7- for the initial level shown in table of 1995Re07 showing level energies seems a misprint. There is only one level at this energy 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1+M2]
decay_comment:
M$|d=+0.10 {I19} from |g|g(|q) in {+97}Mo({+12}C,3n|g) or +0.09 {I18} in {+96}Mo({+13}C,n|g) (1979Sa01) 
M$Other: D+Q with |d=+0.08 {I17} (1979Sa01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=CONV
decay_comment:
$Compiler obtains B(E2)|_=0.0295 {I23}. Value in 2021Si26 is higher by a factor 5, which is (2J+1) for J=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$Priv. communication by T. Gray to F.G. Kondev (December 12, 2022) 
MR$From <2+{-1}|| E2 ||2+{-2}>/<2+{-1}|| M1 ||2+{-2}> in 2022Gr08 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from |a(K)exp=0.074 {I15} via (|a,2n|g) associated with K/L=7.9 {I5} 
MR +0.25 {I1} from anisotropy ratio A{-2}(205|g)/A{-2}(640|g)=0.31 {I3} (1974Be17). Other: <0.48 from K/L=7.9 {I5} (1973Ny03) 
K/L=7.9 {I5} (1973Ny03). Others: 9.2 {I2} (1971Ri05), 8.6 {I7} (1973Jo06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from |a(K)exp=0.0052 {I7} via (p,n|g) and 505|g(|q) A{-2}=-0.49 {I9} via (|a,2n|g) 
MR -0.28 {I8} from 505|g(|q) via ({+16}O,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from |a(K)exp=0.0032 {I6} and 604|g(|q) A{-2}=-0.58 {I4} via (|a,2n|g) 
MR -2.3 {I3} from 604|g(|q) via ({+16}O,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M consistent with |a(K)exp=0.0017 {I3} (p,n|g), 0.0014 {I3} (|a,2n|g); supported by 809|g(|q) A{-2}=0.30 {I6} via (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M consistent with |a(K)exp=0.0025 {I3} (p,n|g), 0.0023 {I4} (|a,2n|g); supported by 728|g(|q) A{-2}=0.35 {I6} via (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M from |a(K)exp=0.00097 {I21} via (p,n|g) 
RI from doublet=2.59 {I12} and I|g from placement from 2875 (1973Ny03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from |a(K)exp=0.074 {I15} (1974Ha41) 
MR +0.25 {I1} from measured anisotropy ratio A{-2}(205|g)/A{-2}(640|g)=0.31 {I3} (1974Be17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M from |a(K)exp=0.018 {I3} and 321|g(|q) A{-2}=0.21 {I6} (1974Ha41) 
MR 321|g(|q) A{-2}=0.21 {I6} via (|a,2n|g) suggests a highly mixed (|DJ=0) transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M from |a(K)exp=0.0144 {I12} (p,n|g), 0.007 {I3} (|a,2n|g), and 365|g(|q) A{-2}=-0.08 {I7} (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from |a(K)exp=0.0052 {I7} (p,n|g), 0.0032 {I6} (|a,2n|g), and 505|g(|q) A{-2}=-0.49 {I9} (|a,2n|g) 
MR -0.28 {I8} from 505|g(|q) A{-2}=-0.430 {I26} via ({+16}O,3n|g) |d=-0.39 {I12} (1991Vi07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from |a(K)exp=0.0032 {I6} and 604|g(|q) A{-2}=-0.58 {I4} (1974Ha41) 
MR -2.3 {I3} from 604|g(|q) via ({+16}O,3n|g) |d=-1.9 {I3} (1991Vi07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M consistent with |a(exp)=2.7 {I10} (1974Ha41) deduced from I(|g+ce) balance about 809 level via delayed |g-spectra 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M from |a(K)exp=0.0081 {I12} (p,n|g), 0.0062 {I14} (|a,2n|g), and 416|g(|q) A{-2}=-0.36 {I6} (|a,2n|g) 
MR$from 1991Vi07 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
E other: 1185.1 {I4} (1979Oh02) 
MR from A{-2}=0.61 (1974Ha41); evaluated by 1979Oh02. Analogous 17/2- to 15/2- transitions: |d(1180|g,{+109}Cd)=+1.2 {I5}, |d(1179|g,{+111}Cd)=+1.1 {I5},|d=0.70 {I14} (1991Vi07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
K/L=8.6 {I7} via (p,n|g) includes anisotropy effects; compare K/L=7.9 {I5} from chem separated {+107}In activity (1973Jo06,1973Ny03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_uncertain: S
decay_comment:
E from (|a,2n|g) (1974Ha41) 
RI from branching; I|g(36|g)/I|g(640|g)=0.11 {I1} (|a,2n|g) (1974Ha41) 
M$from adopted gammas. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=-0.324 {I19}, A{-4}=0.11 {I2} 
MR from 604|g(|q). Other: -27|<|d|<-1.6 from |g-ray linear pol 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_uncertain: S
decay_comment:
RI from branching: I|g(37|g)/I|g(640|g)=0.11 {I1} via (|a,2n|g) 
M based on |a(exp)=2.7 {I10} from I(|g+ce) balance about E(level)=809 via (|a,2n|g)(t) (1974Ha41) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_comment:
A{-2}=0.154 {I7}, A{-4}=-0.041 {I7} 
M from |a(K)exp=0.0112 {I12} via (p,n|g); consistent with change in sign of 641|g pol via |g(|q) versus |g-ray linear pol 
-0.016|<|d|<+0.08 from 641|g linear pol 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
A{-2}=-0.144 {I12}, A{-4}=0.00 {I2} 
E$from 1978St01. Not seen by 1992Je02 
M$E1 inferred from change in sign of 521|g pol via |g(|q) versus |g-ray linear pol (1978St01) 
-0.008|<|d|<+0.04 from 521|g linear pol 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=0.445 {I34}, A{-4}=0.07 {I5} 
MR$from 891|g(|q). Other: +0.6|<|d|<+5 from |g-ray linear pol 
E$from 1978St01. 1992Je02 gives a pure E2 from DCO ratio and an other placement (4009 level) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
A{-2}=-0.208 {I32}, A{-4}=0.02 {I4} 
M$E1 inferred from change in sign of 1076|g pol and from DCO 
-0.022|<|d|<+0.03 from 1076|g(|q) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=CONV
decay_comment:
$B(E2) value is for 100% branching ratio for 728.9|g (compilers' note); does not consider branching ratio for 355|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$from E(level) difference, placed by 1992Ku01 from this level, but the placement in (n,n'|g) is not consistent in energy 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from 1993Th05 in (HI,xn|g). 1978Sa13 report 39 {I3}. 1980Wi20 report 74 in |e decay, a value inconsistent with non observation by 1984Ro13. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
MR$-0.36 {I21} from (|a,n). |d=-0.5 {I2} in table III is a misprint (E-mail from A. Gade, November 30, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E from (HI,xn|g) 
RI from I|g/I(374|g)=0.34 {i5} in (HI,xn|g). Transition in {+108}In decay is masked by 266|g from 2808 level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$from I|g/I|g(3748)=0.097 {I15} in adopted |g's. 1980Wi20 report I|g=0.74. The |g is not seen by 1984Ro10. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$from I|g/I|g(350|g+455|g)=0.313 {I21} in (HI,xn|g). 1980Wi20 report I|g/I|g(350|g)=1.55, in disagreement with (HI,xn|g) and with non observation by 1984Ro10. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.82 {I7} in (|a,n|g); also -1.9 {I2} in |e decay. |d=-0.78 {I7} in table III is a misprint (e-mail reply from A. Gade Nov. 30, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
MR$+0.07 {I8} in (|a,n|g). In table IV |d=-0.03 {I9} should be listed from |e decay (E-mail reply from A. Gade November 30, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$positive sign in table IV of 2002Ga35 is a misprint (E-mail reply from A. Gade, November 30, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
MR$uncertainty=0.004 in table III of 2002Ga35 is a misprint (E-mail reply from A. Gade, November 30, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
MR$-0.36 {I21} from (|a,n). |d=-0.5 {I2} in table III is a misprint (E-mail reply from A. Gade, November 30, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Placement from 3171.2 level as given in 2002Ga35 is incorrect (e-mail reply from A. Gade, Dec. 8, 2002). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$Placement from 3221.9 level as given in 2002Ga35 is incorrect (e-mail reply from A. Gade, Dec. 8, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$Placement from 3489.4 level as given in 2002Ga35 is incorrect (e-mail reply from A. Gade, Dec. 8, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from table IV of 2002Ga35. |d=+0.49 {I8} in table III is a misprint (e-mail reply from A. Gade, November 30, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$Placement from 3605.5 level also as shown in 2002Ga35 is incorrect (e-mail reply from A. Gade, Dec. 8, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from table IV of 2002Ga35. |d=-0.49 {I6} in table III is a misprint (e-mail reply from A. Gade, November 30, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Placement from 4323.4 level as shown in 2002Ga35 is incorrect (e-mail reply from A. Gade, Dec. 8, 2002) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Placement from 4640.4 level as shown in 2002Ga35 is incorrect (e-mail reply from A. Gade, Dec. 8, 2002) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
RI$pure E0 gives I|g=0, so I|g=0.13 {i3} from 1975Fl01 probably is an error. I|g<0.1 (1984Ro10) 
M$|a(K)exp>0.012 (1984Ro10), >0.025 (1992Ku01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$1984Ro10 determine |a(K)exp=0.00019 which indicates E1. This mult is not confirmed by new measurement of 1990Ku01 or by data in (n,n'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
B(M1)=1.00 {I12} (2010Ro15) 
$ Uncertainty of 1.2 in B(M1) listed in table I of 2010Ro15 is a misprint 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 59.6 {I2} from {+109}In |e decay, 59.9 {I5} from {+109}Cd IT decay (12 |ms), and 59.5 {I5} from {+109}Ag(p,n|g) (1983Ch34). 
M$|a(exp)=13 {I3} (1956Pe56), K/L=0.85 {I8} (1956Pe56), 1.3 {I5} (1962No06) in {+109}In |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$|a(exp)=0.07 {I1} and K/L=7.6 {i4} (1956Pe56), K/(L+M)=7 {I1} (1962No06) from {+109}In |e decay; |a(K)exp(259.5|g)/|a(K)exp(203.2|g)=2.06 {i23} (1969Be37) and I|g(259.g|g)/I|g(203.2|g)=0.9 (1966Mc06 and 1964Br27) from {+109}Cd IT decay (10.9 |ms) are consistent with mul(203|g)=M1 and mul(259|g)=M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$weighted average of 77 {I3} from {+109}In |e decay and 71 {I5} from {+109}Ag(p,n|g). 
M$|a(exp)=0.04 {I1}, K/L=5.0 (1956Pe56), K/(L+M)=6.6 {I15} (1962No06) from {+109}In |e decay; a{-2}/a{-0}=+0.03 {i3}, a{-4}/a{-0}=-0.06 {i4} (1994Ju05) in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(exp)=0.020 {I8} from K/L=5.1 {i5} (1956Pe56), K/(L+M)=7 {I5} (1962No06) from {+109}In |e decay; a{-2}/a{-0}=+0.01 {i2}, a{-4}/a{-0}=-0.06 {i4} (1994Ju05) in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from {+109}In |e decay. Other: 100 {I6} from (p,n|g) 
M$|a(exp)=0.014 {I5} from K/L=8 {i1} (1956Pe56), K/(L+M)=8 {I2} (1962No06) from {+109}In |e decay; a{-2}/a{-0}=+0.10 {i4}, a{-4}/a{-0}=+0.01 {i5} (1994Ju05) in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$|a(K)exp(259.5|g)/|a(K)exp(203.2|g)=2.06 {i23} (1969Be37) and I|g(259.5|g)/I|g(203.2|g)=0.9 (1966Mc06 and 1964Br27) from {+109}Cd IT decay (10.9 |ms) are consistent with mul(203|g)=M1 and mul(259|g)=M2; K/(L+M)=2.4 {I8} (1962No06) from {+109}In |e decay. A{-2}/a{-0}=+0.045 {i6}, a{-4}/a{-0}=-0.005 {i6}, pol=-0.13 {i5} from {+96}Zr({+16}O,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$weighted average of 14.7 {I13} from {+109}In |e decay and 17.2 {I13} from {+109}Ag(p,n|g). 
M$a{-2}/a{-0}=+0.22 {i1}, a{-4}/a{-0}=+0.06 {i2} (1994Ju05) in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$from {+109}In |e decay. Other: 100 {I7} from (p,n|g) 
M$|a(exp)=0.0032 {I15} (1956Pe56) from {+109}In |e decay; a{-2}/a{-0}=-0.41 {i3}, a{-4}/a{-0}=-0.08 {i4} (1994Ju05) in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$a{-2}/a{-0}=+0.09 {i2}, a{-4}/a{-0}=-0.06 {i6} (1994Ju05) in (p,n|g), mul=Q is ruled out by T{-1/2}, polarity from level-parity change based L(d,t)=2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$from {+109}In |e decay 
M$R(angular)=0.64 {i7} from {+96}Zr({+18}O,5n|g), a{-2}/a{-0}=-0.67 {i3}, a{-4}/a{-0}=-0.10 {i5} (1994Ju05) in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from {+109}In |e decay 
RI$weighted average of 67 {I2} in {+109}In |e decay and 72 {I6} in (p,n|g) Others: 44 {I8} from (|a,3n|g), 29 {I5} from {+100}Mo({+13}C,4n|g) 
M$Q from a{-2}/a{-0}=+0.24 {i4}, a{-4}/a{-0}=+0.03 {i6} (p,n|g), M2 is ruled out by T{-1/2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 522.0 {I5} from {+96}Zr({+16}O,3n|g), 522.4 {I1} from {+96}Zr({+18}O,5n|g), 522.4 {I1} from {+100}Mo({+13}C,4n|g), 522.2 {I2} from {+108}Pd(|a,3n|g), and 522.2 {I4} from {+109}Ag(p,n|g). 
M$a{-2}/a{-0}=+0.304 {i10}, a{-4}/a{-0}=-0.094 {i11} (1978St01) in {+96}Zr({+16}O,3n|g); a{-2}/a{-0}=+0.292 {i3}, a{-4}/a{-0}=-0.108 {i4} (1975Me22) in (|a,3n|g); T{-1/2} rules out M2; R(angular)=1.33 {i2}, DCO(Q)=1.01 {i1} in {+96}Zr({+18}O,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from {+109}In |e decay. 
RI$weighted average of 12.8 {I5} from {+109}In |e decay and 13.3 {I10} from {+109}Ag(p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
E$weighted average of 570.4 {I5} from {+109}In |e decay (1970Ri06) and 571.2 {I3} from {+109}Ag(p,n|g) (1988Vi03). 
RI$from (p,n|g). Other: 2.2 {I10} from {+109}In |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI$weighted average of 8.3 {I17} from {+96}Zr({+18}O,5n|g) and 7.8 {I9} from {+100}Mo({+13}C,4n|g). 
M$R(angular)=1.00 {i10} from {+96}Zr({+18}O,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$from {+100}Mo({+13}C,4n|g). 
M$a{-2}/a{-0}=+0.32 {i6}, a{-4}/a{-0}=-0.02 {i8} (1975Me22) in (|a,3n|g); a{-2}/a{-0}=+0.27 {i6}, a{-4}/a{-0}=-0.01{i8} (1994Ju05) in (p,n|g); R(angular)=1.33 {i8}, DCO(Q)=0.93 {i14} in {+96}Zr({+18}O,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from {+96}Zr({+18}O,5n|g) (1994Ju05) 
M$a{-2}/a{-0}=+0.284 {i8}, a{-4}/a{-0}=-0.079 {i8} in {+96}Zr({+16}O,3n|g); a{-2}/a{-0}=+0.284 {i8}, a{-4}/a{-0}=-0.079 {i8} in {+96}Zr({+18}O,5n|g); a{-2}/a{-0}=+0.274 {i5}, a{-4}/a{-0}=-0.093 {i8} in (|a,3n|g). T{-1/2} rules out M2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1075.7 {I5} from {+100}Mo({+13}C,4n|g) (1994Ju05), 1075.3 {I3} from {+96}Zr({+18}O,5n|g) (1994Re06) and 1075.1 {I4} from (|a,3n|g) 
M$R(angular)=1.40 {i7}, DCO(Q)=1.06 {i22} in {+96}Zr({+18}O,5n|g), a{-2}/a{-0}=+0.20 {i8}, a{-4}/a{-0}=-0.04 {i12} in (p,n|g), a{-2}/a{-0}=+0.23 {i9}, a{-4}/a{-0}=+0.30 {i16} in (|a,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 740.7 {I3} from {+96}Zr({+18}O,5n|g) and 740.9 {I4} from (|a,3n|g). A 740.3|g deexcites the 1563 level in (p,n|g) 
RI$from {+96}Zr({+18}O,5n|g). Others: 23 {I2} from {+100}Mo({+13}C,4n|g), 25 {I8} from (|a,3n|g) 
M$DCO(Q)=0.86 {i19} in {+96}Zr({+18}O,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 1180.4 {I2} from {+96}Zr({+18}O,5n|g), 1180.9 {I5} from {+100}Mo({+13}C,4n|g and 1179.6 {I3} from (|a,3n|g). Not seen in (p,n|g) 
RI$from {+96}Zr({+18}O,5n|g). 
M$R(angular)=2.0 {i2}, DCO(Q)=0.71 {i26} in {+96}Zr({+18}O,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
M$a{-2}/a{-0}=+0.295 {i15},a{-4}/a{-0}=-0.096 {i18}, pol=+0.44 {i12} in {+96}Zr({+16}O,3n|g), a{-2}/a{-0}=+0.26 {i4}, a{-4}/a{-0}=-0.09 {i5} in (|a,3n|g), R(angular)=1.36 {i3}, DCO(Q)=0.96 {i5} in {+96}Zr({+18}O,5n|g), T{-1/2} rules out M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from {+100}Mo({+13}C,4n|g) 
M$R(angular)=0.80 {i14} in {+96}Zr({+18}O,5n|g) and a{-2}/a{-0}=-0.06 {i2}, a{-4}/a{-0}=-0.06 in (|a,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$a{-2}/a{-0}=-0.257 {i15}, a{-4}/a{-0}=-0.005 {i17}, pol=+0.4 {i3} in {+96}Zr({+16}O,3n|g), a{-2}/a{-0}=-0.29 {i2}, a{-4}/a{-0}=+0.05 {i3} in (|a,3n|g), R(angular)=0.81 {i3}, DCO(Q)=0.53 {i3} in {+96}Zr({+18}O,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$from {+96}Zr({+16}O,3n|g) 
M$a{-2}/a{-0}=-0.25 {i4}, a{-4}/a{-0}=+0.12 {i5}, pol=-0.5 {i4} in {+96}Zr({+16}O,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M,MR$R(angular)=1.19 {i3}, DCO(Q)=0.89 {i5} in {+96}Zr({+18}O,5n|g), a{-2}/a{-0}=+0.13 {i3}, a{-4}/a{-0}=-0.08 {i4} from (|a,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$a{-2}/a{-0}=+0.303 {i16}, a{-4}/a{-0}=-0.109 {i19}, pol=+0.25 {i9} in {+96}Zr({+16}O,3n|g), a{-2}/a{-0}=+0.29 {i2}, a{-4}/a{-0}=-0.13 {i2} in (|a,3n|g), R(angular)=1.33 {i5}, DCO(Q)=1.04 {i3} in {+96}Zr({+18}O,5n|g), T{-1/2} rules out M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$a{-2}/a{-0}=+0.04 {i3}, a{-4}/a{-0}=-0.02 {i5} from (|a,3n|g), R(angular)=1.30 {i6}, DCO(Q)=0.87 {i5} in {+96}Zr({+18}O,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$a{-2}/a{-0}=+0.35 {i3}, a{-4}/a{-0}=-0.19 {i4} from (|a,3n|g), R(angular)=1.50 {i7}, DCO(Q)=1.01 {i6} in {+96}Zr({+18}O,5n|g), T{-1/2} rules out M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$a{-2}/a{-0}=+0.26 {i5}, a{-4}/a{-0}=-0.10 {i6}, pol=+1.3 {i9} from {+96}Zr({+16}O,3n|g), a{-2}/a{-0}=+0.18 {i5}, a{-4}/a{-0}=-0.04 {i7} from (|a,3n|g), R(angular)=1.44 {i5}, DCO(Q)=0.96 {i10} from {+96}Zr({+18}O,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
M$a{-2}/a{-0}=+0.255 {i20}, a{-4}/a{-0}=-0.111 {i26}, pol=+29 {i15} from {+96}Zr({+16}O,3n|g), a{-2}/a{-0}=+0.37 {i3}, a{-4}/a{-0}=-0.16 {i5} from (|a,3n|g), R(angular)=1.37 {i5}, DCO(Q)=1.06 {i7} in {+96}Zr({+18}O,5n|g), T{-1/2} limit rules out M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
%I|g=0.19 {I5}, using the calculated normalization. 
E$59.6 {I2} from weighted average of 59.9 {I5} (1970Ri06), 59.5 {I3} (1971Ba08), 59.6 {I5} (1972Ch56) and 60 {I1} (1969Di16) 
RI$from 1969Di16. 
M$|a(exp)=13 {I3} (1956Pe56), K/L=0.85 {i8} (1956Pe56), 1.3 {I5} (1962No06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=74.2 {I5}, using the calculated normalization. 
E$203.4 {I1} from weighted average of 204.6 {I4} (1969Di16), 203.5 {I2} (1970Ri06), 203.3 {I3} (1971Ba08), 203.6 {I5} (1972Ch56) and 203.3 {I1} (1988Vi03) 
M$|a(exp)=0.07 {I1} and K/L=7.6 {i4} (1956Pe56), K/(L+M)=7 {I1} (1962No06). |d=-0.13 {I4} (1977Be19, Hyperfine field) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$288.1 {I1} from weighted average of 289.1 {I4} (1969Di16), 288.4 {I8} (1970Ri06), 287.7 {I3} (1971Ba08), 287.8 {I5} (1972Ch56), and 288.1 {I1} (1988Vi03). 
RI$2.10 {I7} from weighted average of 2.29 {I18} (1969Di16), 2.4 {I2} (1970Ri06), 2.10 {I11} (1971Ba08), 1.98 {I23} (1972Ch56), and 2.0 {I1} (1988Vi03). 
M$|a(exp)=0.04 {I1}, K/L=5.0 (1956Pe56), K/(L+M)=6.6 {I15} (1962No06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
%I|g=2.02 {I8}, using the calculated normalization. 
E$347.5 {I1} from weighted average of 348.3 {I5} (1969Di16), 347.5 {I3} (1970Ri06), 347.4 {I3} (1971Ba08), 347.5 {I5} (1972Ch56), and 347.5 {I1} (1988Vi03). 
RI$weighted average of 2.54 {I16} (1969Di16), 3.0 {I2} (1970Ri06), 2.7 {I15} (1971Ba08), 2.5 {I3} (1972Ch56), and 2.8 {I2} (1988Vi03). 
M$|a(exp)=0.020 {I8}, |a(exp)=0.020 {I8} from K/L=5.1 {i5} (1956Pe56), K/(L+M)=7 {I5} (1962No06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$223.0 {I1} from weighted average of 223.1 {I2} (1970Ri06), 223.0 {I3} (1971Ba08), and 223.0 {I1} (1988Vi03). 
RI$0.16 {I5} from weighted average of 0.10 {I2} (1970Ri06), 0.20 {I3} (1971Ba08), and 0.21 {I2} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
%I|g=4.05 {I12}, using the calculated normalization. 
E$426.3 {I1} from weighted average of 427.0 {I5} (1969Di16), 426.2 {I3} (1970Ri06), 426.2 {I3} (1971Ba08), 426.4 {I5} (1972Ch56), and 426.3 {I1} (1988Vi03). 
RI$weighted average of 4.9 {I3} (1969Di16), 5.75 {I20} (1970Ri06), 5.3 {I3} (1971Ba08), 5.7 {I4} (1972Ch56), and 5.4 {I3} (1988Vi03). 
M$|a(exp)=0.014 {I5} from K/L=8 {i1} (1956Pe56), K/(L+M)=8 {I2} (1962No06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_comment:
E$259.6 {I1} from weighted average of 259 {I2} (1970Ri06), 259.1 {I3} (1971Ba08), and 259.7 {I1} (1988Vi03). 
RI$weighted average of 0.08 {I1} (1971Ba08) and 0.04 {I2} (1988Vi03). 
M$|a(K)exp=0.12 {I2} from ratio |a(K)exp(259.5|g)/|a(K)exp(203.5|g)= 2.06 {i23} (1969Be37). K/(L+M)=2.4 {I8} (1962No06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$420.6 {I1} from weighted average of 420.5 {I4} (1970Ri06), 420.5 {I3} (1971Ba08), 420.9 {I5} (1972Ch56), and 420.6 {I1} (1988Vi03). 
RI$1.12 {I10} from weighted average of 1.35 {I10} (1970Ri06), 1.00 {I6} (1971Ba08), 1.63 {I19} (1972Ch56), and 1.10 {I8} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=5.64 {I22}, using the calculated normalization. 
E$623.8 {I1} from weighted average of 623.0 {I5} (1969Di16), 623.5 {I4} (1970Ri06), 623.8 {I5} (1971Ba08), 623.7 {I10} (1972Ch56), and 623.8 {I1} (1988Vi03). 
RI$weighted average of 7.9 {I8} (1969Di16), 8.2 {I4} (1970Ri06), 7.1 {I6} (1971Ba08), 7.3 {I6} (1972Ch56), and 6.9 {I6} (1988Vi03). 
M$|a(exp)=0.0032 {I15} (1956Pe56) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$326.3 {I2} from weighted average of 326.6 {I5} (1970Ri06), 326.3 {I3} (1971Ba08), and 326.3 {I2} (1988Vi03). 
RI$0.73 {I3} from weighted average of 0.73 {I4} (1971Ba08) and 0.72 {I5} (1988Vi03). Others: 1.2 {I1} for the 324.3+326.6 doublet (1970Ri06), 1.39 {I28} (1972Ch56) for the doublet, 1.24 {I14} (1969Di16) for the doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$613.6 {I1} from weighted average of 614 {I1} (1969Di16), 613.6 {I4} (1970Ri06), 614.0 {I5} (1971Ba08), and 613.6 {I1} (1988Vi03). 
RI$weighted average of 2.8 {I4} (1969Di16), 3.4 {I3} (1970Ri06), 2.8 {I4} (1971Ba08), and 2.8 {I3} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.73 {I5}, using the calculated normalization. 
E$721.8 {I1} from weighted average of 721.0 {I5} (1969Di16), 721.5 {I4} (1970Ri06), 721.5 {I5} (1971Ba08), 721.9 {I10} (1972Ch56), and 721.8 {I1} (1988Vi03). 
RI$weighted average of 0.93 {I8} (1969Di16), 1.22 {I10} (1970Ri06), 0.91 {I5} (1971Ba08), 1.4 {I3} (1972Ch56), and 1.05 {I8} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$618.5 {I1} from weighted average of 619.0 {I5} (1970Ri06), 619.3 {I5} (1971Ba08), 618.8 {I10} (1972Ch56), and 618.4 {I1} (1988Vi03). 
RI$weighted average of 2.4 {I3} (1970Ri06), 2.6 {I4} (1971Ba08), 3.0 {I3} (1972Ch56), and 2.3 {I3} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
%I|g=1.31 {I14}, using the calculated normalization. 
E$822.0 {I1} from weighted average of 822 {I1} (1969Di16), 822.5 {I5} (1970Ri06), 822.5 {I5} (1971Ba08), 823.1 {I7} (1972Ch56), and 821.9 {I1} (1988Vi03). 
RI$1.75 {I6} from weighted average of 1.68 {I15} (1969Di16), 1.9 {I1} (1970Ri06), 1.74 {I8} (1971Ba08), 2.1 {I3} (1972Ch56), and 1.6 {I1} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$831.7 {I1} from weighted average of 832 {I1} (1969Di16), 832.2 {I10} (1970Ri06), 831.5 {I5} (1971Ba08), 831.8 {I10} (1972Ch56), and 831.7 {I1} (1988Vi03). 
RI$weighted average of 0.34 {I5} (1970Ri06) and 0.34 {I3} (1971Ba08). Others: 0.18 {I2} (1969Di16), 0.24 {I2} (1988Vi03), 0.8 {I3} (1972Ch56) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.193 {I23}, using the calculated normalization. 
E$891.2 {I1} from weighted average of 890 {I1} (1969Di16), 890.5 {I6} (1970Ri06), 890.8 {I5} (1971Ba08), and 891.2 {I1} (1988Vi03). 
RI$0.31 {I3} from weighted average of 0.29 {I3} (1969Di16), 0.38 {I7} (1970Ri06), 0.28 {I3} (1971Ba08), and 0.35 {I3} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$324.4 {I2} from weighted average of 324.3 {I5} (1970Ri06), 324.4 {I3} (1971Ba08), 324.7 {I5} (1972Ch56), and 324.4 {I3} (1988Vi03). Other: 325.3 {I5} from 1969Di16. 
RI$0.51 {I2} from weighted average of 0.50 {I3} (1971Ba08) and and 0.51 {I3} (1988Vi03). Others: 1.2 {I1} for the 324.3+326.6 doublet (1970Ri06), 1.39 {I28} (1972Ch56) for the doublet, 1.24 {I14} (1969Di16) for the doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$650.0 {I1} from weighted average of 651.0 {I5} (1969Di16), 649.8 {I4} (1970Ri06), 650.1 {I5} (1971Ba08), 650.1 {I10} (1972Ch56), and 650.0 {I1} (1988Vi03). 
RI$weighted average of 4.1 {I3} (1970Ri06), 3.8 {I4} (1971Ba08), 4.4 {I4} (1972Ch56), and 3.7 {I3} (1988Vi03). Other: 5.9 {I4} (1969Di16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$794.0 {I3} from weighted average of 793.9 {I4} (1970Ri06), 794.0 {I5} (1971Ba08), and 794.7 {I10} (1972Ch56). Other: 792.5 {I5} (1969Di16) 
RI$0.80 {I8} from weighted average of 0.8 {I2} (1970Ri06), 0.74 {I6} (1971Ba08), 0.99 {I13} (1969Di16), and 1.4 {I3} (1972Ch56). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.65 {I6}, using the calculated normalization. 
E$998.5 {I3} from weighted average of 998 {I1} (1969Di16), 998.5 {I6} (1970Ri06), 998.7 {I5} (1971Ba08), 998.2 {I10} (1972Ch56), and 998.5 {I4} (1988Vi03). 
RI$0.87 {I5} from weighted average of 0.99 {I13} (1969Di16), 0.97 {I5} (1970Ri06), 0.77 {I5} (1971Ba08), 1.1 {I3} (1972Ch56), and 0.8 {I1} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$862.7 {I1} from weighted average of 864 {I1} (1969Di16), 862.2 {I6} (1970Ri06), 863.2 {I5} (1971Ba08), 863.2 {I10} (1972Ch56), and 862.7 {I1} (1988Vi03). 
E$this placement is proposed by 1988Vi03 based on observed 203|g-862|g-coin in (p,n|g); 1970Ri06 placed this transition from the 1861 level. 
RI$weighted average of 0.15 {I12} (1969Di16), 0.23 {I7} (1970Ri06), 0.24 {I3} (1971Ba08), 0.4 {I3} (1972Ch56), and 0.29 {I3} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$482.3 {I2} from weighted average of 482.2 {I4} (1970Ri06), 482.6 {I3} (1971Ba08), and 482.2 {I2} (1988Vi03). 
RI$0.12 {I2} from weighted average of 0.17 {I3} (1970Ri06), 0.11 {I2} (1971Ba08), and 0.11 {I2} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$901.7 {I2} from weighted average of 901 {I1} (1969Di16), 900.7 {I6} (1970Ri06), 901.6 {I5} (1971Ba08), 901.9 {I10} (1972Ch56) and 901.8 {I2} (1988Vi03). Also placed as a transition from E=1622 level. 
RI$0.50 {I3} from weighted average of 0.44 {I5} (1969Di16), 0.64 {I10} (1970Ri06), 0.50 {I4} (1971Ba08), 0.7 {I3} (1972Ch56) and 0.6 {I1} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
%I|g=0.289 {I15}, using the calculated normalization. 
E$1105.9 {I1} from weighted average of 1106.0 {I5} (1969Di16), 1106.2 {I8} (1970Ri06), 1106.0 {I5} (1971Ba08), 1105.9 {I10} (1972Ch56), and 1105.9 {I1} (1988Vi03). 
RI$weighted average of 0.43 {I4} (1970Ri06), 0.38 {I4} (1971Ba08), 0.4 {I3} (1972Ch56), and 0.36 {I4} (1988Vi03). Other: 0.74 {I7} (1969Di16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$929.5 {I2} from weighted average of 930.3 {I5} (1970Ri06), 930.4 {I5} (1971Ba08), 931.3 {I10} (1972Ch56), and 929.4 {I1} (1988Vi03). 1988Vi03 placed this transition from the 930 level in (p,n|g) 
RI$weighted average of 0.4 {I1} (1970Ri06), 0.27 {I5} (1971Ba08), and 0.3 {I1} (1988Vi03). Other: 1.0 {I3} (1972Ch56) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$normalized to I(549.2|g)=0.02 {I1} based on I(746.9|g)/I(549.4|g)=(33 {I4})/(79 {I4}) in Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$normalized to I(549.2|g)=0.02 {I1} based on I(826.2|g)/I(549.4|g)=(100 {I8})/(79 {I4}) in Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$529.9 {I2} from weighted average of 530.8 {I5} (1969Di16), 529.3 {I4} (1970Ri06), 529.7 {I5} (1971Ba08), 529.7 {I7} (1972Ch56), and 530.1 {I3} (1988Vi03). 
RI$0.75 {I5} from weighted average of 0.93 {I8} (1969Di16), 0.80 {I4} (1970Ri06), 0.69 {I5} (1971Ba08), 1.02 {I19} (1972Ch56), and 0.65 {I5} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$630.3 {I3} from weighted average of 629.9 {I6} (1970Ri06), 630.8 {I5} (1971Ba08), and 630.2 {I4} (1988Vi03). 
RI$0.10 {I1} from weighted average of 0.10 {I3} (1970Ri06), 0.10 {I1} (1971Ba08), and 0.10 {I2} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$678.6 {I2} from weighted average of 677.5 {I5} (1969Di16), 678.8 {I4} (1970Ri06), 678.9 {I5} (1971Ba08), 679.0 {I7} (1972Ch56), and 678.8 {I3} (1988Vi03). 
RI$1.12 {I7} from weighted average of 0.93 {I8} (1969Di16), 1.35 {I10} (1970Ri06), 1.12 {I7} (1971Ba08), 1.19 {I24} (1972Ch56), and 1.2 {I1} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$728.1 {I3} from weighted average of 727.4 {I5} (1970Ri06), 728.2 {I5} (1971Ba08), 728.8 {I10} (1972Ch56), and 728.3 {I4} (1988Vi03). 
RI$0.36 {I2} from weighted average of 0.35 {I5} (1970Ri06), 0.34 {I3} (1971Ba08), 0.56 {I18} (1972Ch56), and 0.38 {I3} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$925.6 {I3} from weighted average of 925.8 {I5} (1970Ri06), 925.8 {I5} (1971Ba08), 926.4 {I10} (1972Ch56), and 925.3 {I4} (1988Vi03). 
RI$0.96 {I7} from weighted average of 1.2 {I2} (1970Ri06), 1.00 {I7} (1971Ba08), 1.2 {I3} (1972Ch56), and 0.8 {I1} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1004.8 {I3} from weighted average of 1004.1 {I7} (1970Ri06), 1005.0 {I5} (1971Ba08), 1004.9 {I10} (1972Ch56), and 1005.0 {I6} (1988Vi03). 
RI$0.30 {I2} from weighted average of 0.30 {I3} (1970Ri06), 0.30 {I3} (1971Ba08), 0.35 {I20} (1972Ch56), and 0.25 {I6} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1148.5 {I2} from weighted average of 1148.0 {I5} (1969Di16), 1149.1 {I6} (1970Ri06), 1148.8 {I5} (1971Ba08), 1148.6 {I10} (1972Ch56), and 1148.5 {I2} (1988Vi03). 1971Ba08 also placed this |g from the 1773 level 
RI$weighted average of 6.2 {I4} (1969Di16), 5.9 {I5} (1970Ri06), 7.0 {I4} (1971Ba08), 6.4 {I6} (1972Ch56), and 6.0 {I4} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.71 {I3}, using the calculated normalization. 
E$1352.3 {I1} from weighted average of 1352.3 {I7} (1970Ri06), 1352.2 {I5} (1971Ba08), 1351.9 {I15} (1972Ch56), and 1352.3 {I1} (1988Vi03). 
RI$0.96 {I4} from weighted average of 1.0 {I1} (1970Ri06), 0.99 {I6} (1971Ba08), 1.2 {I3} (1972Ch56), and 0.86 {I8} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$962.2 {I2} from weighted average of 962.2 {I3} (1988Vi03) and 962.6 {I7} (1970I|g)6). Placed by 1988Vi03, this |g was unplaced in 1970Ri06. 1988Vi03 also also placed this |g from the 1425 level in (p,n|g) 
RI$0.03 {I2} from 1988Vi03. Other: 0.13 {I3} (1970Ri06). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1186.8 {I10} from 1970Ri06 only. This |g was not seen by 1988Vi03 in {+109}In |e decay but seen in their (p,n|g) measurements. Placed by evaluators based on (p,n|g) 
RI$<0.4 from 1970Ri06 in this dataset 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.059 {I15}, using the calculated normalization. 
E$1388.8 {I3} from weighted average of 1388.2 {I10} (1970Ri06), 1389.9 {I5} (1971Ba08), and 1388.6 {I2} (1988Vi03). Placed by 1988Vi03, but 1970Ri06 placed this |g from a level at 1847 
RI$weighted average of 0.05 {I2} (1970Ri06), 0.11 {I2} (1971Ba08), and 0.07 {I4} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.06 {I3}, using the calculated normalization. 
E$1430.1 {I4} from weighted average of 1429.8 {I10} (1970Ri06) and 1430.2 {I4} (1988Vi03). Seen by 1988Vi03 in both {+109}In |e decay and (p,n|g) but 1988Vi03 placed this |g from the 1633 level in (p,n|g), which is not populated in {+109}In |e decay. 
RI$unweighted average of 0.12 {I3} (1970Ri06) and 0.04 {I2} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$584.3 {I2} from weighted average of 583.8 {I5} (1970Ri06), 584.2 {I5} (1971Ba08), and 584.6 {I3} (1988Vi03). 
RI$0.30 {I5} from unweighted average of 0.40 {I3} (1970Ri06), 0.24 {I2} (1971Ba08), and 0.25 {I2} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$653.4 {I2} from weighted average of 652.9 {I4} (1970Ri06), 653.4 {I5} (1971Ba08), 653.5 {I10} (1972Ch56), and 653.6 {I3} (1988Vi03). 
RI$unweighted average of 2.6 {I2} (1970Ri06), 1.9 {I4} (1971Ba08), 2.3 {I3} (1972Ch56), and 1.8 {I1} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$753.8 {I4} from weighted average of 752.5 {I5} (1969Di16), 753.9 {I6} (1970Ri06), 754.4 {I5} (1971Ba08), 754.6 {I7} (1972Ch56), and 754.0 {I6} (1988Vi03). 
RI$0.51 {I3} from weighted average of 0.41 {I6} (1969Di16), 0.6 {I1} (1970Ri06), 0.55 {I4} (1971Ba08), 0.6 {I3} (1972Ch56), and 0.49 {I4} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$851.8 {I3} from weighted average of 851 {I1} (1969Di16), 852.3 {I5} (1970Ri06), 851.6 {I5} (1971Ba08), 851.5 {I10} (1972Ch56), and 851.9 {I5} (1988Vi03). 
RI$0.19 {I1} from weighted average of 0.18 {I2} (1969Di16), 0.35 {I10} (1970Ri06), 0.23 {I4} (1971Ba08), 0.4 {I3} (1972Ch56), and 0.19 {I2} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1049.4 {I2} from weighted average of 1048.5 {I5} (1969Di16), 1049.7 {I6} (1970Ri06), 1049.8 {I5} (1971Ba08), 1049.6 {I10} (1972Ch56), and 1049.5 {I3} (1988Vi03). 
RI$1.58 {I5} from weighted average of 1.76 {I18} (1969Di16), 1.58 {I8} (1970Ri06), 1.5 {I1} (1971Ba08), 1.5 {I3} (1972Ch56), and 1.6 {I1} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1272.6 {I2} from weighted average of 1272.9 {I7} (1970Ri06), 1272.6 {I5} (1971Ba08), 1272 {I1} (1972Ch56), 1271 {I2} (1969Di16) and 1272.6 {I3} (1988Vi03). 1972Ch56 also placed this |g from a level at 1272 
RI$0.77 {I3} from weighted average of 0.80 {I5} (1970Ri06), 0.77 {I5} (1971Ba08), 0.8 {I3} (1972Ch56), 0.81 {I8} (1969Di16) and 0.72 {I6} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.49 {I3}, using the calculated normalization. 
E$1475.6 {I2} from weighted average of 1473 {I1} (1969Di16), 1475.8 {I7} (1970Ri06), 1475.6 {I5} (1971Ba08), 1475.6 {I10} (1972Ch56), and 1475.7 {I2} (1988Vi03). 
RI$0.66 {I4} from weighted average of 0.74 {I15} (1969Di16), 0.6 {I1} (1970Ri06), 0.69 {I5} (1971Ba08), 0.74 {I22} (1972Ch56), and 0.61 {I7} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.119 {I15}, using the calculated normalization. 
E$1539.4 {I2} from weighted average of 1539.3 {I10} (1970Ri06), 1539.8 {I5} (1971Ba08), 1539.0 {I15} (1972Ch56), and 1539.3 {I2} (1988Vi03). 
RI$weighted average of 0.19 {I3} (1970Ri06), 0.15 {I2} (1971Ba08), 0.33 {I16} (1972Ch56), and 0.13 {I5} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$731.0 {I4} from weighted average of 729.7 {I5} (1969Di16), 730.9 {I5} (1970Ri06), 731.6 {I5} (1971Ba08), 732.2 {I10} (1972Ch56), and 731.6 {I6} (1988Vi03). 
RI$0.46 {I4} from weighted average of 0.68 {I7} (1969Di16), 0.53 {I5} (1970Ri06), 0.40 {I3} (1971Ba08), 0.64 {I23} (1972Ch56), and 0.45 {I4} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$800.3 {I3} from weighted average of 800.0 {I6} (1970Ri06), 800.3 {I5} (1971Ba08), 800.4 {I10} (1972Ch56), 800.4 {I6} (1988Vi03) and 800 {I2} (1969Di16). 
RI$0.40 {I3} from weighted average of 0.48 {I5} (1970Ri06), 0.42 {I4} (1971Ba08), 0.5 {I3} (1972Ch56) and 0.35 {I4} (1988Vi03). Other: 0.12 {I3} (1969Di16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$948.9 {I2} from weighted average of 949.1 {I5} (1970Ri06), 949.2 {I5} (1971Ba08), and 949.3 {I10} (1972Ch56). 
RI$1.96 {I7} from weighted average of 2.1 {I3} (1970Ri06), 2.00 {I12} (1971Ba08), and 2.1 {I3} (1972Ch56). Other: 1.24 {I9} (1969Di16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$998.5 {I3} from weighted average of 998 {I1} (1969Di16), 998.5 {I6} (1970Ri06), 998.7 {I5} (1971Ba08), 998.2 {I10} (1972Ch56), and 998.5 {I4} (1988Vi03). 
RI$0.87 {I5} from weighted average of 0.99 {I13} (1969Di16), 0.97 {I5} (1970Ri06), 0.77 {I5} (1971Ba08), 1.1 {I3} (1972Ch56), and 0.8 {I1} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1195.7 {I2} from weighted average of 1195 {I1} (1969Di16), 1196.5 {I6} (1970Ri06), 1196.2 {I5} (1971Ba08), 1196.1 {I10} (1972Ch56), and 1195.6 {I2} (1988Vi03). 
RI$2.21 {I8} from weighted average of 2.5 {I2} (1969Di16), 2.4 {I3} (1970Ri06), 2.20 {I12} (1971Ba08), 2.6 {I4} (1972Ch56), and 2.1 {I1} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1419.0 {I1} from weighted average of 1418 {I1} (1969Di16), 1419.2 {I7} (1970Ri06), 1419.1 {I5} (1971Ba08), 1419.3 {I10} (1972Ch56), and 1419.0 {I1} (1988Vi03). 
RI$1.68 {I6} from weighted average of 1.47 {I15} (1969Di16), 1.8 {I2} (1970Ri06), 1.74 {I11} (1971Ba08), 1.9 {I3} (1972Ch56), and 1.66 {I10} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=2.08 {I8}, using the calculated normalization. 
E$1622.3 {I3} from weighted average of 1620 {I1} (1969Di16), 1622.3 {I8} (1970Ri06), 1622.5 {I5} (1971Ba08), 1621.6 {I10} (1972Ch56), and 1622.5 {I3} (1988Vi03). 
RI$weighted average of 2.9 {I2} (1969Di16), 2.8 {I3} (1970Ri06), 3.0 {I2} (1971Ba08), 3.2 {I5} (1972Ch56), and 2.6 {I2} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1346.4 {I1} from weighted average of 1346.9 {I7} (1970Ri06), 1346.6 {I5} (1971Ba08), 1346.3 {I15} (1972Ch56), and 1346.4 {I1} (1988Vi03). 
RI$weighted average of 0.80 {I5} (1970Ri06), 1.0 {I3} (1972Ch56), and 0.72 {I10} (1988Vi03). Other: 0.28 {I3} (1971Ba08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1569.9 {I4} from weighted average of 1567 {I2} (1969Di16), 1569 {I1} (1970Ri06), 1570.7 {I5} (1971Ba08), 1570.0 {I15} (1972Ch56), and 1569.5 {I5} (1988Vi03). 
RI$0.15 {I2} from weighted average of 0.12 {I2} (1969Di16), 0.18 {I3} (1970Ri06), 0.18 {I3} (1971Ba08), 0.18 {I12} (1972Ch56), and 0.15 {I5} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.423 {I23}, using the calculated normalization. 
E$1772.5 {I2} from weighted average of 1774 {I2} (1969Di16), 1771.9 {I8} (1970Ri06), 1772.6 {I5} (1971Ba08), 1772.1 {I10} (1972Ch56), and 1772.6 {I3} (1988Vi03). 
RI$0.57 {I3} from weighted average of 0.57 {I4} (1969Di16), 0.6 {I1} (1970Ri06), 0.60 {I5} (1971Ba08), 0.65 {I16} (1972Ch56), and 0.54 {I5} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.033 {I6}, using the calculated normalization. 
E$1861.4 {I1} from 1988Vi03. Others: 1860.6 {I10} (1970Ri06), 1863 {I3} (1969Di16) 
RI$weighted average of 0.047 {I9} (1969Di16), 0.04 {I2} (1970Ri06), and 0.04 {I2} (1988Vi03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 1040.8 {i3} (1994Re06) 
M$R(angular)=1.36 {i3}, DCO(Q)=0.96 {i5}, R(angular) is for 1039|g+1040.7|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$other: 1037.9 {i2} (1994Re06) 
M$R(angular)=1.36 {i3}, DCO(Q)=0.87 {i20}; R(angular) is for 1039|g+1040.7|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$placed by 1994Ju05 in {+100}Mo({+13}C,4n|g), but not observed in {+96}Zr({+18}O,5n|g) by the same authors. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1044.8 {I5} in 1975Me22 
RI$46 {I9} in 1975Me22 
M$a{-2}/a{-0}=-0.06 {i2}, a{-4}/a{-0}=-0.06 {i3},|DJ=0,|+1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$721.8 {i4} in 1975Me22 
RI$31 {i4} in 1975Me22 
M$a{-2}/a{-0}=+0.37 {i3}, a{-4}/a{-0}=-0.16 {i5}, |DJ=0,-2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$other: 203.3 {I1} (1994Ju05), 203.4 {i2} (1988Ch35), 203.4 {I3} (1983Ch34), 203.2 {I3} (1969Be37) 
M$from Adopted Gammas 
$A{-2}/A{-0}=-0.10 {I4}, A{-4}/A{-0}=-0.02 {I5} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$others: 287.5 {I1} (1994Ju05), 287.9 {i2} (1988Ch35), 287.9 {I3} (1983Ch34) 
RI$others: 7.2 {I2} (1994Ju05), 32.5 {I33} (1988Ch35), 42.9 (1983Ch34) 
$A{-2}/A{-0}=+0.03 {I3}, A{-4}/A{-0}=-0.06 {I4} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$others: 347.4 {I1} (1994Ju05), 347.6 {I2} (1988Ch35), 347.5 {I3} (1983Ch34) 
RI$others: 9.2 {I1} (1994Ju05), 49 {I5} (1988Ch35), 58.3 (1983Ch34) 
$A{-2}/A{-0}=+0.01 {I2}, A{-4}/A{-0}=-0.06 {I4} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$others: 426.2 {I1} (1994Ju05), 426.4 {I2} (1988Ch35), 426.4 {I3} (1983Ch34) 
RI$others: 12.2 {I3} (1994Ju05), 55 {I6} (1988Ch35), 51 (1983Ch34) 
$A{-2}/A{-0}=+0.10 {I4}, A{-4}/A{-0}=+0.01 {I5} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_comment:
E$others: 259.6 {I1} (1994Ju05), 259.9 {i2} (1988Ch35), 259.7 {I3} (1983Ch34), 259.5 {I3} (1969Be37) 
RI$others: 36.0 {I10} (1994Ju05), 15.7 {I17} (1988Ch35), 20.7 (1983Ch34) 
M$from measured |a{-K}(260|g)/|a{-K}(203|g)=2.06 {I23} in 1969Be37 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$other: 420.5 {I1} (1994Ju05) 
RI$other: 2.3 {I1} (1994Ju05) 
$A{-2}/A{-0}=+0.22 {I1}, A{-4}/A{-0}=+0.06 {I2} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$others: 623.8 {I1} (1994Ju05), 623.2 {i5} (1988Ch35), 623.9 {I5} (1983Ch34) 
RI$others: 12.1 {I3} (1994Ju05), 33 {I4} (1988Ch35), 34.1 (1983Ch34) 
$A{-2}/A{-0}=-0.41 {I3}, A{-4}/A{-0}=-0.08 {I4} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$others: 325.5 {I1} (1994Ju05), 325.7 {i2} (1988Ch35) 
RI$others: 2.3 {I5} (1994Ju05), 9.5 {I11} (1988Ch35) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$others: 614.2 {I1} (1994Ju05), 614.0 {I5} (1988Ch35), 613.6 {I2} (1982Av07), 614.0 {I3} (1983Ch34) 
RI$others: 6.3 {I4} (1994Ju05), 40 {I4} (1988Ch35), 41.5 (1983Ch34) 
$A{-2}/A{-0}=+0.09 {I2}, A{-4}/A{-0}=-0.06 {I6} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$others: 721.7 {I5} (1988Ch35), 721.2 {I2} (1982Av07), 721.8 {I5} (1983Ch34) 
RI$other: 29 {I3} (1988Ch35), 27.9 (1983Ch34) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$others: 619.3 {I1} (1994Ju05), 619.2 {i5} (1988Ch35), 619.4 {I5} (1983Ch34) 
RI$others: 6.8 {I3} (1994Ju05), 8.1 {I13} (1988Ch35), 10.5 (1983Ch34) 
$ A{-2}/A{-0}=-0.67 {I3}, A{-4}/A{-0}=-0.10 {I5} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$others: 822.5 {I1} (1994Ju05), 821.0 {I3} (1982Av07), 821.9 {I5} (1983Ch34) 
RI$other: 2.0 {I2} (1994Ju05), 13.5 (1983Ch34) 
M$ Q from A{-2}/A{-0}=+0.24 {I4}, A{-4}/A{-0}=+0.03 {I6} (1994Ju05), M2 is ruled out by T{-1/2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 831.0 {I3} (1982Av07). 1988Ch35 report a |g ray at E|g=833.1 {I2} with I|g=28 {I3} and 1983Ch34 report E|g=833.1 {I5} with I|g=31.7 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$others: 891.7 {i5} (1988Ch35), 890.6 {I3} (1982Av07), 891.6 {I5} (1983Ch34) 
RI$other: 13.5 {I17} (1988Ch35), 15.5 (1983Ch34) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$others: 649.9 {I1} (1994Ju05), 649.8 {i5} (1988Ch35), 650.2 {I5} (1983Ch34) 
RI$others: 4.9 {I2} (1994Ju05), 10.1 {I14} (1988Ch35), 7.2 (1983Ch34) 
M$ Q from A{-2}/A{-0}=+0.18 {I4}, A{-4}/A{-0}=-0.06 {I6} (1994Ju05), T{-1/2} rules out M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$others: 794.0 {I5} (1994Ju05), 794.2 {I2} (1982Av07), 794.3 {I5} (1983Ch34) 
RI$other: 0.8 {I2} (1994Ju05), 2.3 (1983Ch34) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 863.1 {I1} in 1994Ju05 
RI$other: 6.9 {I3} (1994Ju05) 
M$ Q from A{-2}/A{-0}=+0.27 {I6}, A{-4}/A{-0}=-0.01 {I8} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$other: 482.0 {I5} (1994Ju05) 
RI$other: 1.1 {I2} (1994Ju05) 
$ A{-2}/A{-0}=-0.31 {I5}, A{-4}/A{-0}=+0.11 {I6} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$other: 902.6 {I0}.5 (1994Ju05) 
RI$other: 1.4 {I2} (1994Ju05) 
$ A{-2}/A{-0}=+0.33 {I12}, A{-4}/A{-0}=+0.1 {I2} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$others: 1106.1 {I1} (1994Ju05), 1105.6 {i5} (1988Ch35), 1106.2 {i3} (1982Av07) 
RI$others: 2.5 {I2} (1994Ju05), 5.0 {I10} (1988Ch35) 
$ Q from A{-2}/A{-0}=+0.22 {I4}, A{-4}/A{-0}=-0.03 {I5} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Placed by evaluators. 1988Vi03 has seen this |g-ray in coincidence with 623.8|g but not placed it. 1983Ch34 report a |g ray at E|g=998.4 {I5} with I|g=17.2 and place it from 998 level and they also assign it to {+107}Cd 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$placed by 1994Ju05. A 998.5|g is seen by 1988Vi03 in coincidence with 623.8|g but not placed 
$A{-2}=-0.15 {I19} (1994Ju05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E,M$from Adopted Gammas 
RI$from I(|g+ce)=100 and conversion coefficient calculated by the BrICC program based on adopted multipolarity. Uncertainty is from |D|a(th)=0.4 by BrICC. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
M$A{-2}/A{-0}=-0.257 {I15}, A{-4}/A{-0}=-0.005 {I17}, pol=+0.4 {i3}. -0.16|<|d|<0.06 from pol (1978St01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=0.00264 {I10} (1964Ne05), K/L=8.1 {I7}, (M+N)/L=0.23 {I6} in {+110}Ag |b{+-} decay (249.83 d) (1993Ka37). Other: A{-2}=+0.23 {I2}, A{-4}=-0.15 {I3} (1992Ku01) from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|a(K)exp=0.0016 {I2}, sum of 815.31 keV and 818.05 keV transitions in {+110}In |e decay (69.1 min) (1992Ku01). Other: A{-2}=0.277 {I30}, A{-4}=0.990 {I50}, 657.76|g gated (0-2-0 spin sequence) in {+110}Ag |b{+-} decay (24.56 s) (1972Ka34) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E,M$From {+110}In |e decay (69.1 min) (1990Gi01). The uncertainty of the electron energy was estimated by the evaluators based on the energy resolution (2.6 keV at 1450 keV electron energy) given by the authors. Mult. from ce 
$I|g(1473|g)/Ice(K)(1473|g)<3.4|*10{+-4} (1990Gi01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From |a(K)exp=0.00172 {I19} (1967Mo12). Other:0.00191 {I15} (1980Ba58) from {+110}In |e decay (4.92 h); A{-2}=-0.23 {I1}, A{-4}=-0.10 {I1} (1992Ku01) 
MR$Weighted average of -1.20 {I15} (1970Kr03), -1.36 {I10} (1973Jo08), -1.2 {I5} (1978Wa07), -1.25 {I+22-10} (1979Ve03), and -1.44 {I10} (1980Ru03) (from {+110}Ag |b{+-} decay (249.83 d)), -1.5 {I+9-4} (1969Mi07) (from Coulomb excitation), -1.4 {I+10-4} (1992De41), -1.4 {I+4-10} (1990Ar20), 1.5 {I+3-4} (2001Co01) (from {+110}Cd(n,n'|g)), and -1.5 {I4} (1990Ke02) (from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From |a(K)exp=0.00043 {I6} (1967Mo12) in {+110}Ag |b{+-} decay (249.83 d) and 0.00036 {I7} (1980Ba58) from {+110}In |e decay (4.92 h)). Other: A{-2}=0.18 {I3}, A{-4}=-0.11 {I4} (1992Ku01) from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From |a(K)exp=0.00126 {I6} (1964Ne05) and K/L=7.6 (1963Su07) in {+110}Ag |b{+-} decay (249.83 d). K/(L+M)=7.7 {I13} (1962Ka08) from {+110}In |e decay (4.9 h). Other: A{-2}=0.289, A{-4}=-0.069 {I10} in (HI,xn|g) (1974Lu01) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$From {+110}In |e decay (69.1 min) (1992Ku01). The uncertainty of the electron energy was estimated from another close transition given by the authors 
$I|g(258|g)/Ice(K)(258|g)<6.5|*10{+-3} from {+110}In |e decay (69.1 min) (1990Gi01) 
M$From {+110}In |e decay (69.1 min) (1990Gi01) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$From {+110}In |e decay (69.1 min) (1992Ku01). The uncertainty of the electron energy was estimated by the evaluators based on the energy resolution (2.6 keV at 1450 keV electron energy) given by the authors 
$I|g(1731|g)/Ice(K)(1731|g)<2.1|*10{+-4} (1990Gi01) 
M$From {+110}In |e decay (69.1 min) (1990Gi01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From |a(K)exp=0.0009 {I2} (1979Sy02) in {+110}In |e decay (4.9 h), from A{-2}=+0.36 {I2}, A{-4}=+0.02 {I4} (1992De41) in {+110}Cd(n,n'|g) and from A{-2}=0.21 {I10}, A{-4}=-0.07 {I14}, 657.50|g gated (2-2-0 spin sequence) in {+110}Ag |b{+-} decay (24.56 s) (1972Ka34). Other: |a(K)exp=0.00043 {I5} (1992Ku01) in {+110}In |e decay (69.1 min) 
MR$Weighted average of +0.13 {I+3-2} (2001Co01), +0.33 {I+7-4} (1992De41), +0.33 {I8} (1990Ar20) (from {+110}Cd(n,n'|g)), -0.06 {I+7-12} (1972Ka34) (from {+110}Ag |b{+-} decay (24.56 s)) and 0.3 {I2} (1976De23). Other: 1.7 {I3} (1976De23). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From A{-2}=+0.29 {I3}, A{-4}=-0.07 {I4} (1992De41) in {+110}Cd(n,n'|g) and from |a(K)exp=0.00018 {I3} (1992Ku01) in {+110}In |e decay (69.1 min) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$From A{-2}=-0.3 {I2}, A{-4}=-0.3 {I3} (1992Ku01) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
MR$From 1990Ke02 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$|a(K)exp=0.00019 {I2} (1992Ku01) in {+110}In |e decay (69.1 min) and from A{-2}=-0.28 {I3}, A{-4}=-0.04 {I5} (1992Ku01) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
MR$From 1990Ke02 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E,RI$From {+110}Ag |b{+-} decay (24.56 s) 
M$From |a(K)exp=0.028 {I5} in {+110}In |e decay (69.1 min) (1992Ku01) and A{-2}=0.259 {I17}, A{-4}=0.753 {I26}, 1783.6|g gated (0-2-0 spin sequence) in {+110}Ag |b{+-} decay (24.56 s) (1972Ka34) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From |a(K)exp=0.0031 {I6} (1967Mo12) 
MR$Weighted average of -0.50 {I8} (1980Ru03), -0.8 {I5} (1970Kr03), -0.85 {I25} (1979Ve03) (from {+110}Ag |b{+-} decay (249.83 d)) and -0.46 {I+7-6} (2001Co01) (from {+110}Cd(n,n'|g)). Others: -1.2 {I5} or -0.7 {I3} (1978Wa07) (from {+110}Ag |b{+-} decay (249.83 d)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From |a(K)exp=0.0022 {I5} and from A{-2}=-0.70 {I5}, A{-4}=-0.01 {I2} (1992Ku01, in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g)) 
MR$Weighted average of -1.80 {I5} (1973Jo08), -1.65 {I9} (1978Wa07), and -1.27 {I38} (1980Ru03), -1.1 {I+8-4} (1970Kr03) and -1.5 {I+6-22} (1979Ve03) (from {+110}Ag |b{+-} decay (249.83 d)), -1.66 {I+9-8} (2001Co01), -1.48 {I10} (1992De41), -1.48 {I15} (1990Ar20), and -1.3 {I4} (1992Ku01) (from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g)). Others: 0.4 {I+1-2} (1976De23) (from {+110}Cd(n,n'|g)), -0.40 {I4} (1992De41) (from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g)). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From |a(K)exp=0.00046 {I4} (1967Mo12) 
MR$Weighted average of -1.05 {I16} (1988Kr03), -1.24 {I7} (1988Kr03), -1.24 {I20} (1980Ru03), -1.09 {I9} (1978Wa07), and -1.26 {I6} (1973Jo08) (from {+110}Ag |b{+-} decay (249.83 d)), -1.37 {I8} (1992De41), -1.37 {I15} (1990Ar20), -1.52 {I+11-14} (2001Co01) from {+110}Cd(n,n'|g)), -1.48 {I23} (1990Ke02) (from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g)). Others: -0.55 {I10} (1970Kr03), -0.48 {I3} (1973Jo08), -0.40 {I+9-17} (1979Ve03) (from {+110}Ag |b{+-} decay (249.83 d)), -0.30 {I7} (1980Ba58) (from {+110}In |e decay (4.92 h)), -0.1 {I1} or 3 {I+2-1} (1976De23) (from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From |a(K)exp=0.0025 {I4} (1967Mo12) 
MR$Unweighted average of -0.25 {I20} (1970Kr03), -0.44 {I5} (1973Jo08), -0.36 {I3} (1978Wa07), -0.25 {I15} (1979Ve03), -0.28 {I5} (1980Ru03) from {+110}Ag |b{+-} decay (249.83 d), -0.40 {I7} (1990Ke02) from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g), -0.34 {I3} (1992De41), -0.34 {I4} (1990Ar20), -0.41 {I2} (2001Co01) from {+110}Cd(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From |a(K)exp=0.0021 {I4} in {+110}Ag |b{+-} decay (249.83 d) (1967Mo12); A{-2}=0.28 {I1}, A{-4}=-0.27 {I1} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From A{-2}=0.22 {I6}, A{-4}=-0.19 {I8} (1992Ku01) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) and from |a(K)exp=0.00046 {I7} (1967Mo12). Other: E2(+M3) with |d=-0.10 {I+2-3} from |g|g(|q) in {+110}Ag |b{+-} Decay (249.83 d) (1979Ve03). |d= Infinite (1970Kr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From A{-2}=+0.22 {I6}, A{-4}=-0.10 {I8} (1992De41) in {+110}Cd(n,n'|g) and from |a(K)exp=0.013 {I4} (1979Sy02) in {+110}In |e Decay (4.9 h) (1979Sy02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From A{-2}=+0.22 {I6}, A{-4}=-0.10 {I8} (1992De41) from {+110}Cd(n,n'|g) 
MR$Weighted average of -0.15 {I9} (1992De41), -0.15 {I9} (1990Ar20), 0.13 {I+4-3} (2001Co01) (from {+110}Cd(n,n'|g)). Other: -0.7 {I3} (1990Ke02) from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From |g(|q) in {+110}Cd(n,n'|g) but A{-2} and A{-4} coefficients were not given by the authors of 1992De41 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From A{-2}=+0.24 {I3}, A{-4}=+0.01 {I4} (1992De41) in {+110}Cd(n,n'|g) 
MR$From 1992De41 and 1990Ar20 using |g(|q) in {+110}Cd(n,n'|g). Other: -0.01 {I2} (2001Co01) from {+110}Cd(n,n'|g) 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
E$From {+110}Cd(n,n'|g) (2001Co01) 
M$From |g(|q) in {+110}Cd(n,n'|g) but A{-2} and A{-4} coefficients were not given by the authors of 2001Co01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From A{-2}=+0.27 {I3}, A{-4}=-0.01 {I3} (1992De41) in {+110}Cd(n,n'|g) 
MR$From 1992De41. Others: +0.11 {I4} (1992De41), 0.1 {I+2-1} or 1.7 {I+6-5} (1976De23), 1.8 {I2} or +0.10 {I5} (1990Ar20) in {+110}Cd(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From A{-2}=-0.58 {I3}, A{-4}=+0.07 {I3} (1992De41) in {+110}Cd(n,n'|g) 
MR$Others: -0.45 {I5} or -1.38 {I14} (1992De41), -0.43 {I8} or -1.38 {I20} (1990Ar20) in {+110}Cd(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From A{-2}=-0.56 {I8}, A{-4}=0.00 {I3} (1992De41) in {+110}Cd(n,n'|g) 
MR$-0.35 {I10} or -1.6 {I3} (1992De41), -0.35 {I10} or -1.6 {I4} (1990Ar20) in {+110}Cd(n,n'|g) 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
M$From |g(|q) in {+110}Cd(n,n'|g) but A{-2} and A{-4} coefficients were not given by the authors of 2001Co01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From |a(K)exp=0.0012 {I8} (1964Ne05) in {+110}Ag |b{+-} Decay (249.83 d) and 0.00114 {I8} (1980Ba58) in {+110}In |e Decay (4.92 h)). K/(L+M)=6.6 {I14} from {+110}In |e decay (4.92 h) (1962Ka08) and A{-2}=+0.34 {I2}, A{-4}=-0.08 {I3} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_multipolarity: (E1)
decay_comment:
E$From {+110}Cd(n,n'|g) 
M$From |g(|q) in {+110}Cd(n,n'|g) but A{-2} and A{-4} coefficients were not given by the authors (2001Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From A{-2}=+0.07 {I3} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
MR$From 1992De41 in {+110}Cd(n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From A{-2}=-0.15 {I3}, A{-4}=0.02 {I4} in {+110}Cd(n,n'|g) (1992De41) 
MR$-0.70 {I9} or -4.9 {I+24-11} (1992De41), -0.70 {I10} or -5.2 {I20} (1990Ar20) in {+110}Cd(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$|a(K)exp=0.00041 {I5} (1980Ba58) in {+110}In |e decay (4.92 h) 
MR$From 1990Ke02 in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From A{-2}=+0.01 {I6} (1990Ke02) {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g). 
MR$Other: -0.49 {I+16-19} in {+110}Cd(n,n'|g) (2001Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From A{-2}=+0.36 {I4}, A{-4}=-0.10 {I5} (1992De41) in {+110}Cd(n,n'|g) and |a(K)exp=0.0008 {I2} in {+110}In |e decay (4.9 h) (1980Ba58) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$From A{-2}=-0.09 {I4}, A{-4}=0.00 {I5} (1992De41) in {+110}Cd(n,n'|g) and from {+110}Cd(|g,|g') (2005Ko32), deduced using |g(|q) and |p from linear polarization measurements 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$Other: 58 {I10} in {+110}Cd(n,n'|g) 
M$From A{-2}=0.26 {I13} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$From |a(K)exp=0.0027 {I10} (1970Ko12) in {+110}In |e decay (4.9 h) and A{-2}=-0.25 {I2} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1990Ke02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$From |a(K)exp=0.00033 {I7} (1990Ke02) in {+110}In |e decay (4.9 h) (1980Ba58) and A{-2}=-0.18 {I2} in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E,RI$From {+110}Ag |b{+-} decay (24.56 s) 
M$From A{-2}=0.177 {I28}, A{-4}=0.986 {I47}, 657.50|g gated (0-2-0 spin sequence) (1972Ka34) in {+110}Ag |b{+-} decay (24.56 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From A{-2}=+0.32 {I5}, A{-4}=-0.03 {I6} (1992De41) in {+110}Cd(n,n'|g). 
MR$From |g(|q) in {+110}Cd(n,n'|g) (1992De41) 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
E$From measured Ice in {+110}Ag |b{+-} decay (249.83 d) 
M$From M1/M2/M3=10 {I2}/1.0/0.35 {I10} in {+110}Ag |b{+-} decay (249.83 d) (1993Ka37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$Other: 62 {I3} in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g), 56 {I5} in {+110}Cd(n,n'|g) 
M$From A{-2}=+0.02 {I5} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g). 
MR$Other:-0.03 {I5} or -5.5 {I+24-10} (1992De41) from {+110}Cd(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
M$From A{-2}=+0.17 {I5} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g). Other: A{-2}=+0.39 {I11}, A{-4}=+0.02 {I14} (1992De41) from {+110}Cd(n,n'|g) 
MR$Other:-0.07 {I+10-7} (1992De41) from {+110}Cd(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From A{-2}=+0.39 {I11}, A{-4}=+0.02 {I14} (1992De41) in {+110}Cd(n,n'|g) 
MR$From |g(|q) in {+110}Cd(n,n'|g) (1992De41) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From A{-2}=-0.31 {I5}, A{-4}=-0.02 {I5} (1992De41) in {+110}Cd(n,n'|g) 
MR$+0.18 {I+10-7} or +1.5 {I3} (1992De41) in {+110}Cd(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$Other: 17.4 {I14} in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g), <63 in {+110}Cd(n,n'|g) 
M$From A{-2}=+0.10 {I14} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$From A{-2}=-0.21 {I2} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) and from |g(|q) in {+110}Cd(n,n'|g) (2001Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
M$From |g(|q) in {+110}Cd(n,n'|g), but A{-2} and A{-4} coefficients were not given by the authors (2001Co01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From |g(|q) in {+110}Cd(n,n'|g) but A{-2} and A{-4} coefficients were not given by the authors (1992De41) 
MR$+1.8 {I7} or +0.10 {I+22-13} (1992De41) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From |a(K)exp=3.0|*10{+-3} {I4} (1980Ba58) in {+110}In |e decay (4.92 h) and from A{-2}=+0.35 {I2}, A{-4}=-0.04 {I3} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From A{-2}=+0.37 {I3}, A{-4}=-0.09 {I4} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) and from DCO=1.38 {I13} (1994Ju04) in (HI,xn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$From A{-2}=-0.25 {I1} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
MR$Other:<0.06 in (HI,xn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$From DCO=0.66 {I5} in (HI,xn|g); A{-2}=-0.35 {I1} with |d=-0.09 {I4} in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$Other:3.2 {I3} in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
M$From |a(K)exp=0.0070 {I11} (1967Mo12) 
MR$Weighted average of -0.40 {I6} (1978Wa07), -0.39 {I+2-1} (1979Ve03), -0.35 {I5} (1980Ru03) and -0.45 {I20} (1970Kr03) from {+110}Ag |b{+-} decay (249.83 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From |a(K)exp=0.00262 {I23} (1967Mo12). K/L=4.7 (1963Su07) 
MR$Weighted average of -1.42 {I7} (1978Wa07), -1.0 {I3} (1970Kr03), -0.58 {I2} (1973Jo08), -1.8 {I+7-9} (1979Ve03) and -1.1 {I3} (1980Ru03) from {+110}Ag |b{+-} decay (249.83 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From A{-2}=+0.31 {I1}, A{-4}=-0.13 {I1} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g). Other:E2(+M3) with |d=-0.10 {I+2-3} (1979Ve03) in {+110}Ag |b{+-} decay (249.83 d). Other |d=Infinite (1970Kr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From |a(K)exp=0.00055 {I4} (1967Mo12) 
MR$Weighted average of -0.37 {I3} (1970Kr03), -0.46 {I1} (1973Jo08), -0.39 {I2} (1978Wa07), -0.42 {I+7-6} (1979Ve03), and -0.44 {I2} (1980Ru03) in {+110}Ag |b{+-} decay (249.83 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From A{-2}=-0.50 {I18}, A{-4}=+0.02 {I18} (1992De41) in {+110}Cd(n,n'|g) 
MR$-1.9 {I+12-7} or -0.3 {I+3-2} (1992De41) in {+110}Cd(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$From A{-2}=-0.17 {I4} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
MR$-0.01 {I9} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$From A{-2}=-0.27 {I3} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
MR$From {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1990Ke02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E,RI$E|g from {+110}Cd(n,n'|g), I|g from {+110}Cd(|g,|g') 
M$From |g(|q) and linear polarization in {+110}Cd(|g,|g') (2005Ko32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$K/(L+M)=9 {I3} in {+110}In |e decay (4.9 h)(1962Ka08). Other: A{-2}=+0.29 {I2}, A{-4}=+0.19 {I4} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
MR$From |g|g(|q) in {+110}In |e decay (4.92 h) (1980Ba58) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$From A{-2}=-0.19 {I7} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
MR$From 1990Ke02 in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$|a(K)exp=2.96|*10{+-3} {I21} (1980Ba58) from {+110}In |e decay (4.9 h). Other: From A{-2}=+0.39 {I5}, A{-4}=+0.11 {I8} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=2.61|*10{+-3} {I16} (1980Ba58), 2.9|*10{+-3} {I6} (1970Ko12). K/(L+M)=6.0 {I5} (1962Ka08). DCO=1.47 {I6} (1994Ju04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From A{-2}=+0.36 (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g). M1 from |a(K)exp=2.2|*10{+-3} {I1} (1980Ba58) in {+110}In |e decay (4.9 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From A{-2}=+0.36 {I2}, A{-4}=-0.10 {I2} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1990Ke02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_uncertain: ?
decay_comment:
M$From A{-2}=+0.30 {I11} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g). No |d given by 1990Ke02 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$16.7 {I9} in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
M$From A{-2}=+0.28 {I5} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$From A{-2}=0.42 {I4} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) Other:DCO=1.39 {I9} in (HI,xn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From |a(K)exp=4.2|*10{+-3} {I12} (1979Sy02) in {+110}In |e decay (4.9 h) 
MR$From |g|g(|q) in {+110}In |e decay (4.9 h) (1980Ba58) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$From |a(K)exp=1.0|*10{+-3} {I2} (1980Ba58) 
MR$From |g|g(|q) in {+110}In |e decay (4.9 h) (1980Ba58) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$From {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
RI$From (HI,xn|g) 
M$From A{-2}=+0.22 {I2}, A{-4}=-0.08 {I3} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
E$From {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
RI$From (HI,xn|g) 
M$From A{-2}=-0.27 {I2} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$From {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
RI$From (HI,xn|g) 
M$From A{-2}=+0.35 {I2}, A{-4}=-0.10 {I3} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) and A{-2}=0.333 {I11}, A{-4}=-0.093 {I16} in (HI,xn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From A{-2}=+0.67 {I9} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g). No reliable |d could be obtained by 1990Ke02 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From DCO=0.90 {I10} in (HI,xn|g) and A{-2}=-0.57 {I4} (1990Ke02), in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$Other: 100 {I12} in (HI,xn|g) 
M$From A{-2}=+0.36 {I2}, A{-4}=-0.18 {I3} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$Other: 14.8 {I9} in (HI,xn|g) 
M$From DCO=0.60 {I6} in (HI,xn|g) and A{-2}=-0.61 {I4}, A{-4}=+0.13 {I6} in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1990Ke02) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E,RI$From {+110}Cd(|g,|g') 
M$Deduced from |g(|q) and linear polarization measurements in {+110}Cd(|g,|g') (2005Ko32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$Other: 33 {I7} from (HI,xn|g) 
M$From DCO=0.46 {I4} in (HI,xn|g) and A{-2}=-0.66 {I4} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From DCO=1.6 {I2}. Other: M1+E2 from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1990Ke02). |d=0.57 {I12} reported by 1990Ke02 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
RI$From (HI,xn|g). Other: 17.4 {I14} in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 
M$From DCO=0.73 {I14} in (HI,xn|g) and A{-2}=-0.37 {I5} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$Note that mult.=M1+E2 was suggested in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1990Ke02), while the decay scheme requires mult.=E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From DCO=1.7 {I4} in (HI,xn|g) and A{-2}=+0.35 {I5}, A{-4}=-0.11 {I7} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From DCO=1.46 {I6} in (HI,xn|g) and A{-2}=+0.35 {I2}, A{-4}=-0.10 {I3} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From DCO=1.41 {I3} in (HI,xn|g) and A{-2}=+0.32 {I2}, A{-4}=-0.14 {I3} (1990Ke02) in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: D
decay_comment:
E,M$From {+110}Cd(|g,|g'). I|g(150|')/I|g(90|')=1.66 {I8}, 1.75 expected for 0(1)1(1)0 transition (1969Mi13) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$From 1990Gi01. The uncertainty of the electron energy was estimated by the evaluators based on the energy resolution (2.6 keV at 1450 keV electron energy) given by the authors 
$I|g(1473|g)/Ice(K)(1473|g)<3.4|*10{+-4} (1990Gi01) 
M$From 1990Gi01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From adopted gammas. |a(K)exp=0.0016 {I2}, sum of the 815.31 keV and 818.05 keV transitions in {+110}In |e Decay (69 min) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$From 1990Gi01. The uncertainty of the electron energy was estimated from another close transition given by the authors 
$I|g(258|g)/Ice(K)(258|g)<6.5|*10{+-3} (1990Gi01) 
M$From 1990Gi01 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$From 1990Gi01. The uncertainty of the electron energy was estimated by the evaluators based on the energy resolution (2.6 keV at 1450 keV electron energy) given by the authors 
M$From 1990Gi01 
$I|g(1731|g)/Ice(K)(1731|g)<2.1|*10{+-4} (1990Gi01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$From adopted gammas. 0.111 {I9} in {+110}In |e decay (69.1 min) 
M$Deduced from |g(|q) using (|a,2n|g) (A{-2}=-0.70 {I15}, A{-4}=-0.01 {I2}) in 1992Ku01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.23 {I2}, A{-4}=-0.15 {I3} (1992Ku01). Other: A{-2}=+0.29 {I2}, A{-4}=-0.06 {I3} (1990Ke02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.28 {I3}, A{-4}=-0.22 {I3} (1992Ku01). Other: A{-2}=+0.32 {I2}, A{-4}=-0.07 {I3} (1990Ke02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$An unresolved doublet at 295.42 keV depopulating 2078.8 keV level, observed by 1990Ke02. 295.3 keV reported by 1992Ku01 
M$A{-2}=-0.06 {I4}, A{-4}=-0.18 {I5} (1992Ku01). Other: A{-2}=0.04 {I5} (1990Ke02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$Unresolved doublet at 295.42 keV observed by 1990Ke02. 295.3 keV reported (depopulating 2078.57 keV J|p=0+ state) 
RI$Undivided intensity for unresolved doublet in 1990Ke02 
M$From decay pattern and from A{-2}=0.04 {I5} (1990Ke02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
E$602.9 keV {i3} in 1992Ku01 
M$A{-2}=-0.3 {I2}, A{-4}=-0.3 {I3} (1992Ku01). Other: A{-2}=-0.20 {I7} (1990Ke02) 
MR$From 1990Ke02 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
E$1421.2 keV {i3} in 1992Ku01 
M$A{-2}=-0.28 {I3}, A{-4}=-0.04 {I5} (1992Ku01). Other: A{-2}=-0.13 {I2} (1990Ke02) 
MR$From 1990Ke02 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.55 {I4}, A{-4}=-0.03 {I7} (1992Ku01). Other: A{-2}=-0.45 {I2}, A{-4}=+0.04 {I2} (1990Ke02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.22 {I6}, A{-4}=-0.19 {I8} (1992Ku01). Other: A{-2}=+0.45 {I7}, A{-4}=-0.24 {I11} (1990Ke02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.22 {I3}, A{-4}=-0.16 {I4} (1992Ku01). Other: A{-2}=+0.42 {I6}, A{-4}=-0.20 {I10} (1990Ke02) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$4695 keV was measured to populate 1.795 MeV state but authors stated that 1.795 MeV state is in fair agreement with 1.78 MeV state in {+110}Cd. 4707 keV was adopted by the evaluators using the adopted level energy ~ 1783 keV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=+0.36 {i2}, A{-4}=+0.02 {i4} 
MR$From |g(|q) in 1990Ar20. Others: +0.33 {I+7-4} (1992De41), 0.3 {I2} or 1.7 {I3} (1976De23), +0.13 {I+3-2} (2001Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$0.74 {i2} in 2001Co01 
M$Other: A{-2}=-0.55 {I3}, A{-4}=+0.09 {I4} (1992De41) 
MR$From 2001Co01. Others: -1.48 {i10} or -0.40 {i4} (1992De41), -1.48 {I15} (1990Ar20), 0.4 {I+1-2} (1976De23). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.590 {I17}, A{-4}=+0.06 {I3} 
MR$Others: -0.1 {I1} or 3 {I+2-1} (1976De23), -1.37 {I15} (1990Ar20), -1.52 {I+11-14} (2001Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=+0.27 {i3}, A{-4}=-0.01 {i3} 
MR$+0.11 {i4} or +1.75 {i15} (1992De41), 0.1 {I+2-1} or 1.7 {I+6-5} (1976De23), 1.8 {i2} or +0.10 {i5} (1990Ar20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.58 {I3}, A{-4}=+0.07 {I3} 
MR$-0.45 {I5} or -1.38 {I14} (1992De41), -0.43 {I8} or -1.38 {I20} (1990Ar20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.56 {I8}, A{-4}=0.00 {I3} 
MR$-0.35 {I10} or -1.6 {I3} (1992De41), -0.35 {I10} or -1.6 {I4} (1990Ar20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.15 {I3}, A{-4}=0.02 {I4} 
MR$-0.70 {I9} or -4.9 {I+24-11} (1992De41), -0.70 {I10} or -5.2 {I20} (1990Ar20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$0.17 {i1} in 2001Co01 
M$A{-2}=-0.28 {I10}, A{-4}=+0.01 {I12} 
MR$-0.03 {i5} or -5.5 {I+24-10} (1992De41) 


decay_energy_unit: KEV
decay_uncertain: S
decay_comment:
E$From 2001Co01. Not observed by the authors due to the attenuation of low-energy |g-rays in the sample but taken from literature 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$Not observed in 2001Co01 
M$A{-2}=-0.50 {I18}, A{-4}=+0.02 {I18} 
MR$-1.9 {I+12-7} or -0.3 {I+3-2} (1992De41) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$A{-2}=0.30 {I3}, A{-4}=-0.08 {I4}. Because of the more intense 335|g, the polarity of the 339|g could not be determined in the linear polarization measurements in 1974Lu01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$The authors of 1974Lu01 stated that polarization measurement was not much influenced by presence of weak unresolved 339|g, because of its similar angular distribution and its expected E2 character 
M$A{-2}=0.333 {I11}, A{-4}=-0.093 {I16} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$From adopted gammas. A{-2}=0.416 {I41}, A{-4}=0.075 {I50} (1979Ve03) and A{-2}=0.481 {I82}, A{-4}=0.155 {I112} (1970Kr03), 657.51|g gated 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$From adopted gammas. |d=-0.06 {I+7-12} (1972Ka34) from |g|g(|q) in 110Ag |b{+-} Decay (24.56 s) 
M$A{-2}=0.21 {I10}, A{-4}=-0.07 {I14}, 657.51|g gated (2-2-0 spin sequence) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|a(K)exp=0.00264 {I10}, directly measured by 1964Ne05. K/L=8.1 {I7}, (M+N)/L=0.23 {I6} (1993Ka37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.00172 {I19} (1967Mo12) 
MR$From adopted gammas. |d=-1.20 {I15} (1970Kr03), -1.36 {I10} (1973Jo08), -1.2 {I5} (1978Wa07), -1.25 {I+22-10} (1979Ve03), and -1.44 {I10} (1980Ru03) in {+110}Ag |b{+-} decay (249.83 d)) Other: -0.27 {I10} (1979Ve03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.0031 {I6} 
MR$From adopted gammas. Other: -0.54 {I8} (weighted average of -0.50 {I8} (1980Ru03), -0.8 {I5} (1970Kr03) and -0.85 {I25} (1979Ve03)) and -1.2 {I5} or -0.7 {I3} (1978Wa07) in {+110}Ag |b{+-} Decay (249.83 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.0022 {I5} 
MR$From adopted gammas. Others: -1.80 {I5} (1973Jo08), -1.65 {I9} (1978Wa07), -1.27 {I38} (1980Ru03), -1.1 {I+8-4} (1970Kr03) and -1.5 {I+6-22} (1979Ve03) in {+110}Ag |b{+-} Decay (249.83 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.00046 {I4} 
MR$From adopted gammas. Others: -1.05 {I16} (1988Kr03), -1.24 {I7} (1988Kr03), -1.24 {I20} (1980Ru03), -1.09 {I9} (1978Wa07), -1.26 {I6} (1973Jo08), -0.55 {I10} (1970Kr03), -0.48 {I3} (1973Jo08), and -0.40 {I+9-17} (1979Ve03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From |a(K)exp=0.0025 {I4} 
MR$From adopted gammas. Others: -0.25 {I20} (1970Kr03), -0.44 {I5} (1973Jo08), -0.36 {I3} (1978Wa07), -0.25 {I15} (1979Ve03), and -0.28 {I5} (1980Ru03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From adopted gammas. Other: E2(+M3) (1979Ve03) with -0.0 {I+16-10} (1979Ve03) and (E2) from |a(K)exp=0.0021 {I4} (1967Mo12) in {+110}Ag |b{+-} Decay (249.83 d). |d=Infinite (1970Kr03) in {+110}Ag |b{+-} Decay (249.83 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From adopted gammas. Other: E2(+M3) (1979Ve03) with -0.10 {I+2-3} (1979Ve03) and (E2) from |a(K)exp=0.00046 {I7} (1967Mo12) in {+110}Ag |b{+-} Decay (249.83 d). |d=Infinite (1970Kr03) in {+110}Ag |b{+-} Decay (249.83 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From adopted gammas. Other: From |a(K)exp=0.0012 {I8} (1964Ne05) and E2 from 1967Mo12. M3+E2 with |d=-0.07 {I+7-3} (1979Ve03) in 110Ag |b{+-} Decay (249.53 d). Other |d=Infinite (1970Kr03) in 110Ag |b{+-} Decay (249.53 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.0070 {I11} 
MR$Weighted average of -0.40 {I6} (1978Wa07), -0.39 {I+2-1} (1979Ve03), -0.35 {I5} (1980Ru03) and -0.45 {I20} (1970Kr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.00262 {I23}. K/L=4.7 (1963Su07) 
MR$Weighted average of -1.42 {I7} (1978Wa07), -1.0 {I3} (1970Kr03), -0.58 {I2} (1973Jo08), -1.8 {I+7-9} (1979Ve03) and -1.1 {I3} (1980Ru03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From adopted gammas. Other: E2 from |a(K)exp=0.00184 {I17} (1967Mo12). E2(+M3) from 1979Ve03 with |d=-0.10 {I+2-3} in {+110}Ag |b{+-} Decay (249.83 d). |d=Infinite (1970Kr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.00055 {I4} 
MR$Weighted average of -0.37 {I3} (1970Kr03), -0.46 {I1} (1973Jo08), -0.39 {I2} (1978Wa07), -0.42 {I+7-6} (1979Ve03), and -0.44 {I2} (1980Ru03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From the decay pattern. |a(K)exp=0.0021 {I2}. Other: 0.0022 {I9} (1970Ko12). Mult=M1+E2 by 1980Ba58 and 1970Ko12 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$From adopted gammas. Mult=E1(+M2) and |d=-0.03 {I+4-8} from I|g(|q,H,T) results of 1977Be19 in {+110}In |e Decay (4.9 h). |a(K)exp=4.1|*10{+-4} {I5} in {+110}In |e Decay (4.9 h). Other: |a(K)exp=4.7|*10{+-4} {I19} (1970Ko12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From adopted gammas. From |a(K)exp=0.5|*10{+-3} {I2} (1970Ko12) M1,E2 is favored in {+110}In |e Decay (4.9 h). If |a(K)exp=0.33|*10{+-3} {I9} (1980Ba58) is accepted, then multipolarity is E1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$ No final level within 5 sigmas. Uncertainty on energy probably underestimated. Least-squares fit gives 584.76 {i3} 
$K/(L+M)=9 {I3} (1962Ka08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$|a(K)exp=2.96|*10{+-3} {I21}. Other: 3.5|*10{+-3} {I8} (1970Ko12). |d -0.05 {I+16-10} or +0.74 {I+17-25} (1977Be19) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From |a(K)exp=2.61|*10{+-3} {I16}. E2+M1 with |d=+0.52 {I+12-10} reported in 1980Ba58 See also 1977Be19. If J|p=8+ M1 component is impossible. Other: |a(K)exp=2.9|*10{+-3} {I6} (1970Ko12). K/(L+M)=6.0 {I5} (1962Ka08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$ No final level within 4 sigmas. Uncertainty on energy probably underestimated. Least-squares fit gives 759.60 {I3} 
M,MR$From adopted gammas. |a(K)exp=2.2|*10{+-3} {I1} in {+110}In |e Decay (4.92 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$From adopted gammas. E2(+M1) from |a(K)exp=1.0|*10{+-3} {I2} in {+110}In |e Decay (4.9 h). Other: 8|*10{+-4} {I3} (1970Ko12) 
MR$From adopted gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$ 818.323 in table I of 2012Ga41 is a misprint according to e-mail reply of May 16, 2013 from P. Garrete 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$|d=-0.050 {I+34-45} also possible but less favored 
$B(E2)(W.u.)=0.009 {I+23-8} for |d=-0.050 {I+34-45} 


decay_energy_unit: KEV
decay_multipolarity: M1+E2+E0
decay_comment:
M$|a(K)exp=0.00292 {I30} 
$|r{+2}(E0)|*10{+3}=106 {I+98-91} in 2016Ji02, using |t=1080 fs {I+450-250}, Branching{-|g}=0.813 {I5}, |W{-K}=2.723|*10{+9} and |d=-0.14 {I3} 


decay_energy_unit: KEV
decay_multipolarity: M1+E2+E0
decay_comment:
M$K/L=7.53 {I38}; |a(K)exp=0.00348 {I19}. 
MR$|d(M1/E2)|<1.2 is deduced by the compiler from K/L and |a(K)exp, and by assuming no E0 component 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
$B(E2)(W.u.)=27.0 {I8} in Table III of 2020Ga10 from {+110}Cd Adopted dataset in the ENSDF database 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 2012Ga41, however, 818.323 in authors' Table I is a misprint according to e-mail reply of May 16, 2013 from P. Garrett, value should be 818.023 keV, instead 
RI$from 2012Ga41 
$B(E2)(W.u.)=30 {I5} in Table III of 2020Ga10 from {+110}Cd Adopted dataset in the ENSDF database, which is based on T{-1/2}(1476 level) of 0.68 ps {I10} and |d(818|g)=1.36 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)(W.u.)=1.35 {I20} in Table III of 2020Ga10 from {+110}Cd Adopted dataset in the ENSDF database, which is based on T{-1/2}(1476 level) of 0.68 ps {I10} and |d(818|g)=1.36 {I6} 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
$B(E2)(W.u.)=42 {I7} in Table III of 2020Ga10 from {+110}Cd Adopted dataset in the ENSDF database, which is based on T{-1/2}(1542 level) of 0.80 ps {I+17-16} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.186 {I+38-28} or +1.52 {I+12-9} from 2012Ga41 
$B(E2)(W.u.)=0.32 {I+10-14} for smaller |d, 6.7 {I+10-9} for larger |d in Table III of 2020Ga10 from 2012Ga41 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$|g from 2012Ga41, where E|g is form level-energy difference 
$Relative B(E2)(W.u.)<0.65 (2020Ga10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.36 {I+4-5} or -1.93 {I+24-28} (2012Ga41) 
$B(E2)(W.u.)=2.9 {I+9-8} in 2020Ga10 and 2.4 {I+9-8} in 2012Ga41 for lower |d, 39 {I12} for higher |d in Table III of 2020Ga10 taken from from 2012Ga41 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|d(E2/M1)=+2.22 {I+19-18} or +0.020 {I+27-36} (2020Ga10) 
$B(E2)(W.u.)=4.78 {I35} for larger |d, 0.0023 {I9} for smaller |d (2020Ga10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+2.7 {I3} or -0.050 {I+34-45} (2012Ga41) 
$B(E2)(W.u.)=3.2 {I3} for larger |d, 0.009 {I+23-8} for smaller |d in Table III of 2020Ga10 from 2012Ga41 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$somewhat poor fit, level-energy difference=782.890 
$|d(E2/M1)=-25 {I+12-|@} or +0.15 {I4} (2020Ga10) 
$B(E2)(W.u.)=11 {I2} for larger |d, 0.25 {I+12-15} for smaller |d (2020Ga10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|d(E2/M1)=+1.18 {I+20-18} or -0.04 {I7} (2020Ga10) 
$B(E2)(W.u.)=31 {I9} for larger |d, 0.09 {I+56-9} for smaller |d (2020Ga10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from {+110}Cd Adopted dataset in the ENSDF database. 2020Ga10 mention that the value is from 1990Ke02 (Nucl. Phys. A512, 1). But in 1990Ke02, it is stated that no |d value could be extracted 
$B(E2)(W.u.)<58 {I+46-39} (2020Ga10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$somewhat poor fit, level-energy difference=1384.31 
MR$-0.44 {I1} from {+110}Cd Adopted dataset in the ENSDF database 
$B(E2)(W.u.)<7 {I+6-5} (2020Ga10), assuming E2 for 1384.557|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
E$somewhat poor fit, level-energy difference=131.73 
$Relative B(E2)(W.u.)<8400 {I600} (2020Ga10), assuming pure E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from |b{+-} decay. Others: I|g(509|g)/I|g(755|g)=10 {i6} ({+3}He,2n|g), 1.8 (1968Mc04 in Coul ex.), and 0.98 (1975AnYZ) in Coul ex. these values are strongly affected by |g|+. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 245.43 {I4} (1974ShZQ) 
RI$weighted av: 19.1 {I13} (1975PuZZ), 16.9 (1974HeYW), 15.8 {I6} (1974ShZQ), 18.4 {I4} (1975Sh29),20.6 {I2} (1970Hn04) 
M$from K:L1:L2:L3=100:8.7 {I2}:2.4 {I1}:2.1 {I1} (1975Sh29) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from (1975Sh29) 
RI$from I(ce) data of 1975Sh29. Directly measured values are: 4.2 {I1} (1970Hn04), 1.6 (1974HeYW), 3.8 (1974BuZU), 3.4 {I2} (1975PuZZ), 1.8 {I2} (1975Sh29) 
M$from |a(K)exp=0.25 {I4}, L1/L2=100/8.5 {I22} (1975Sh29) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 1974HeYW. Others: 342.13 {I2} (1975Sh29), 342.24 {I4} (1974ShZQ) 
RI$absolute I|g/decay=0.0668 {I33} (1977Ne10) 4|p|b|g, 0.068 {I6} (1976Th07), 0.046 {I5} (1970Hn04), 0.060 {I15} (1958Ro62) 
M$deduced from |a(K)exp, |a(L)exp, and L-subshell ratio data K:L1:L2:L3=90 {I2}:10 {I1}:1.6 {I2}:0.67 {I6} (1975Sh29) 
MR$from adopted |g's. +0.74 {I+10-7} from L1/L3 ratio, sign from |g(|q) (1958Mc02) Coul. ex. penetration effects may account for exp L1/L2/L3 ratios (1975Sh29). Incompatible with predictions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1970Hn04. 1975Sh29 report 276.8 {I2}. E|g=278.04 {I5} in (n,n'|g) 
RI$from 1970Hn04. Others: 0.038 {I19} (1975Sh29), <0.02 (1975PuZZ) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted av: 374.6 (1974BuZU) and 374.4 {I4} (1970Hn04). Other: 373.9 {I2} (1975Sh29), E|g=374.75 {I5} in (n,n'|g) 
RI$weighted av: 0.048 {I2} (1970Hn04), 0.043 {I4} (1975PuZZ), 0.04 (1974BuZU) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$others: 620.1 {I3} (1977Kr14), 64.8-s {+111}Ag decay 
RI$triplet I|g(619|g+620|g+622|g)=0.42 {I4} (1975Sh29) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted av from 1975Sh29, 1975PuZZ, and 1970Hn04. The values for 1975PuZZ and 1970Hn04 are deduced 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
RI$from I|g(865|g/I|g(865+867|g's)=0.30 {I6} (1976ShYW) and I|g(865+867|g's) =0.077 {I2} (1970Hn04). Others: I|g(865+867|g's)=0.077 {I10}(1975PuZZ) and I|g(865|g)=0.050 {I11} (1976ShYW) and I|g(861|g)=0.116 {I15} (1976ShYW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
E$Others: 866.6 {i2} (1975PuZZ), 867.0 {i4} (1976ShYW), 866.7 {i4} (1970Hn04) 
RI$see 865|g. Others: 0.116 {I15} (1976ShYW), 0.08 (1974BuZU) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_uncertain: S
decay_comment:
RI$from I(|g+ce) balance at 342 level and adopted branching: I|g(96.7|g)/I|g(342|g)=0.0173 {I9}, and adopted |a's 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from 1974HeYW. Other: 245.40 {I2} (1975Sh29) 
M$from ce-ratio data (1975Sh29), {+111}Ag g.s. decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E$from 1974HeYW. Others: 150.81 {I3} (1975Sh29), 150.6 {I2} (1970Hn04) 
RI$from 1974HeYW. Others: 32.2 from I(|g+ce)(151|g)=I(|g+ce)(245|g), 24 {I2} (1975Sh29), 33 (1968Da24), 34 {I6} (1951Mc11), 31 {I5} (1951Su73) 
M$ce(K)(151|g)/ce(K)(245|g)=8.55 {I20} (1975Sh29) s from K:L1:L2:L3:M=100:10.4 {I9}:22.0 {I18}:20.0 {I18}:11.0 {I16} (1975Sh29) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI from 100.0/[1.0 + |a(245)] = 100.0 / 1.0628 {I19} where an uncertainty of 3% has been assigned to |a(245). 
M from K:L1:L2:L3:M=100 {I1}:10.2 {I2}:2.30 {I15}:2.21 {I15}:2.73 {I10} (1966Sp04), 100/11.5 {I16}/2.06 {I25}/1.9 {I3}/2.7 {I4} (1975Sh29) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
RI from 1975Sh29; other: 0.0028 deduced from %|e=0.0086 (1972MeZD) and < 0.003 from limit of 1972MeZD 
M from {+111}Cd IT decay (48.50 min) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI from I{-|g} = [100.0 - I{-|b}(396)] / [1.0 + |a(171)] = 99.995 {I5} / 1.103 {I3} 
MR average of -0.146 {I3} (1956St64) |g|g(|q), -0.141 {I3} (1973Bu31) |g|g(|q); 0.145 (1974Kr03) |g|g(|q, linear pol) sign inconsistent. |d=0.196 {I+46-55} from L3/L1=0.042 {I12} (1966Sp04,1975Sh29). Penetration effects may account for exp L1/L2/L3 ratios (1966Sp04,1975Sh29); incompatible with predictions 
M other |a(K)exp: 0.110 {I5} (1975Sh29), 0.10 {I1} (1951Mc61) normalized to |a(K)(245|g)=0.0536 (E2 theory) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$alternate value of -0.10 {I5} is ruled out since it leads via T{-1/2} to RUL(524.4|g) greater than 740 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$from I|g=3.1 {I6} for the doubly placed 1054|g and value deduced for placement from the 1298 level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 1985Si01 
RI$D+Q from |g(|q). |D|p=+ from direct excitation of 755 level in Coul. ex. 
MR$|d=+0.087 {i18} or -2.14 {i10} (1985Si01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$absolute I|g=0.00883 % {I14} (2014Co08). 
E,RI$corrected for contribution from 620.3|g from {+110m}Ag decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
RI$absolute I|g=0.0161 % {I4} (2014Co08). 
E,RI$corrected for contribution from 620.3|g from {+110m}Ag decay. 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
E$from {+111}Cd Adopted dataset in the ENSDF database 
TI$deduced by compiler from intensity balance at 417 level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E3
decay_comment:
EKC$Agrees well with Dirac-Fock calculation with K-shell vacancy and disagrees by |?1.5|s when vacancy is ignored. |a(K)exp value was determined by taking into consideration the |a(K)th for the 245|g calculated using the Dirac-Fock formalism for both the options with an average |a(K)th=0.05326 {I17}. 
ECC$Disagrees with Dirac-Fock calculation by up to |?2|s with vacancy accounted for. |a(th) value for the 245|g was calculated using the Dirac-Fock formalism for both the vacancy and no vacancy options with an average |a(th)=0.06351 {I17}. No definitive conclusion can be drawn for the discrepancy but authors suggest it may be from penetration effects due to the 150-keV |g transition being hindered by a factor of 10{+4} relative to the single particle Weisskopf estimate 
EKC,ECC$Measured by 2016Ni05 from precisely determined intensities and detector efficiencies. For X-rays; peak counts from contribution of impurities, x-ray peak shape, coincidence-summing and attenuation from finite thickness of samples were corrected. For |g-rays; only the summing corrections were done. Details of these corrections are given in the paper. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=0.00317 {I16}, |a(L)exp=0.00039 {I4}, and |a(M)exp=0.000138 {I15} in {+111}Cd(n,|g) E=th:secondary (1997Dr03); |a(K)exp=0.0038 {I7} in {+112}In |e decay (14.88 min) (1962Ru05); A{-2}=+0.44 {I2}, A{-4}=-0.05 {I2} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=0.0034 {I3} in {+111}Cd(n,|g) E=th:secondary (1997Dr03); A{-2}=-0.02 {I7}; A{-4}=-0.08 {I10} in {+110}Pd(|a,2n|g) (1992Ku01) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$transition energy from level energy differences 
M$from ce measurements 1979Gi05, 1980Ju05 and 1997Dr03; Ice(K)(1224.341|g)/Ice(K)(606.821|g)=0.300 {I22}, weighted average of 0.30 {I4} (1979Gi05), 0.33 {I5} (1980Ju05) and 0.29 {I3} (1997Dr03) 
TI$from Ice(K)(1224.341|g)/Ice(K)(606.821|g)=0.300 {I22} |a(K)(606.84|g)=0.00336 {I5} and |W{-K}/|W{-T}=0.8961 (2008Ki07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$|a(K)exp=0.00242 {I18} in {+111}Cd(n,|g) E=th:secondary (1997Dr03); A{-2}=-0.224 {I7}; A{-4}=0.008 {I10} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$From |g|g(|q) in {+112}Ag |b{+-} decay (1972Wa03); Others (|g(|q)): -1.6 {I+5-8} (1997Dr03), -2.6 {I+4-3} in (2001Ga44), -0.77 {I6} in {+111}Cd(d,p|g) and -0.87 {I10} or -3.5 {I9} (1969Mi07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=0.00052 {I6} in {+111}Cd(n,|g) E=th:secondary (1997Dr03); A{-2}=+0.46 {I2}, A{-4}=-0.04 {I3} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=0.00155 {I15} in {+111}Cd(n,|g) E=th:secondary (1997Dr03); A{-2}=+0.58 {I4}, A{-4}=-0.15 {I5} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$transition energy from level energy differences 
M$from |a measurements in 1980Ju05 and 1997Dr03 
TI$from Ice(K)(208.93|g):Ice(K)(815.79|g)=45 {I5} (1997Dr03), |a(K)(815.79|g)=0.001589 {I23}, I|g(815.79|g)=100 {I11} and |W{-K}/|W{-T}=0.8941 (2008Ki07); Other: Ice(K)(208.93|g):Ice(K)(815.79|g)=25 {I9} (1980Ju05), is probably affected by the uncertainties in the ce spectrum around the 183-keV line 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$transition energy from level energy differences 
M$from |a measurements in 1980Ju05 and 1997Dr03 
TI$from Ice(K)(1433.27|g):Ice(K)(815.79|g)=19.0 {I17} (1997Dr03), |a(K)(815.57|g)=0.001589 {I23}, I|g(815.57|g)=100 {I11} and |W{-K}/|W{-T}=0.8962 (2008Ki07) Other: Ice(K)(1433.27|g):Ice(K)(815.79|g)=7.9 {I25} (1980Ju05), but the value is probably affected by the weak population of this level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$from |a(K)exp=0.00235 {I18} in {+111}Cd(n,|g) E=th (1997Dr03) and |a(K)exp=0.00234 {I12} in {+112}In |e decay (14.88 min) (1991Gi05); A{-2}=0.50 {I2} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03); Others: A{-2}=0.07 {I7} and A{-4}=0.03 {I16} in {+112}Ag |b{+-} decay (3.130 h) (1972Wa03) 
MR$Weighted average of 0.053 {I30} in 1997De03 and 0.048 {I22} in 1991Gi05. Others: +0.14 {I5} from |g(|q) in {+112}Cd(n,n'|g) (2001Ga44), +0.23 {I13} or +1.4 {I5} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03), +0.10 {I7} (1973Gr16); 0.05 or +2.0 {I+7-5} (1969Mi07) in Coulomb excitation; +0.22 {I5} in {+112}Ag |b{+-} decay (3.130 h) (1972Wa03) 
CC$0.00195 {I4}, using q{+2}=9.7 {I35}, weighted average of 9.4 {I54} (1997Dr03) and 9.9 {I46}(1991Gi05), and |a from 2008Ki07. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=0.00050 {I7} in {+111}Cd(n,|g) E=th (1997Dr03) 
M$a{-0}=15.6 {I2}; A{-2}=0.210 {I13}; A{-4}=-0.036 {I19} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.06 {I23}, A{-4}=-0.41 {I24} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 
MR$Other: 2.43 {I15} or -0.45 {I14} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$A{-2}=-0.07 {I6} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03); Also, A{-2}=-0.11 {I3} and A{-4}=-0.02 {I5} in {+112}Ag |b{+-} decay (3.130 h) (1972Wa03). Possible M2 admixture; |d=-0.06 {I2} from {+112}Ag |b{+-} decay (3.130 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=+0.45 {I7} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 
MR$Also: -1.6 {I3} or -0.50 {I15} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=0.303 {I6}; A{-4}=-0.092 {I8} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Also: -1.5 {I5} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=-0.47 {I6}, A{-4}=+0.10 {I10} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 
MR$Also: -1.24 {I15} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=+0.36 {I2} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 
MR$Also: -0.47 {I5} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$seen as 1507.3 keV {I3} in {+112}In |e decay (14.97 min) 
M$|a(K)exp=0.00030 {I10} in {+111}Cd(n,|g) E=th (1997Dr03); A{-2}=0.16 {I4} from |g|g(|q) in (1993De09) 
MR$Also: +0.15 {I5} or +1.6 {I3} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=-0.02 {I7} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Also: -0.33 {I15} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=-0.05 {I3} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Also: -0.6 {I+2-4} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=0.09 {I5} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Also: 0.33 {I10} from |g|g(|q) in 1997Dr03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=-0.26 {I4} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$-0.25 {I20} from |g(|q) in 1997Dr03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$From {+112}Ag |b{+-} decay (3.130 h) 
M$A{-2}=0.46 {I9}; A{-4}=0.19 {I13} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Also: +4.2 +|@-20 from |g|g(|q) in {+112}Cd(n,n'|g) (2001Ga44); 0.50 {I25} or 2.7 {I10} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=+0.47 {I23} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 
MR$Also: -0.03 {I25} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
RI$100 in {+110}Pd(|a,2n|g) (1997Dr03) 
M$A{-2}=+0.61 {I13} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09); possible E2 admixture with |d=0.00 {I15} in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
M$A{-2}=-0.21 {I5} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09); possible M2 admixture with |d=0.02 {I5} in {+110}Pd(|a,2n|g) (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
M$A{-2}=-0.35 {I10} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09); Possible M2 admixture with |d=-0.13 {I13} in {+110}Pd(|a,2n|g) (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
M,MR$A{-2}=0.048 {I22}; A{-4}=-0.3 {I3} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Others: +1.8 {I8} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
M$A{-2}=-0.13 {I3} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09); possible M2 admixture with |d=0.03 {I5} (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
M$A{-2}=0.09 {I6} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Other: +0.27 {I15} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
M$A{-2}=-0.58 {I5}; A{-4}=0.19 {I6} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Other: -2.0 {I5} or -0.30 {I12} in 1997Dr03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=0.09 {I3} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Other: -0.33 {I9} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.73 {I2}; A{-4}=0.05 {I2} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Other: -0.45 {I18} from |g(|q) in 1997Dr03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
M$A{-2}=-0.33 {I2} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Other: -0.11 {I8} |g|g(|q) in {+110}Pd(|a,2n|g) in 1997Dr03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$A{-2}=-0.29 {I3}; A{-4}=0.07 {I4} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
M$stretched transition; |d=+0.014 {I+33-30} from |g(|q) in 2001Ga44 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=-0.55 {I8} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Other: -0.33 {I15} from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.15 {I5}; A{-4}=0.10 {I8} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Also: +1.3 {I2} from |g(|q) in 1997Dr03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.42 {I3}; A{-4}=-0.03 {I4} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Also: -0.09 {I12} from |g|g(|q) in {+110}Pd(|a,2n|g) in 1997Dr03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=+0.68 {I4} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Also: +0.54 {I+30-15} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$a{-0}=0.96 {I6}; A{-2}=-0.40 {I10}; A{-4}=0.15 {I16} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Other: +7 {I4} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.32 {I6}; A{-4}=0.17 {I8} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Also: -0.42 {I+15-40} from |g(|q) in 1997Dr03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=+0.23 5from |g|g(|q) in {+110}Pd(|a,2n|g) (1997Dr03) 
MR$Other: +0.62 {i12} in {+110}Pd(|a,2n|g) (1997dr3) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.28 {I4}; A{-4}=-0.11 {I5} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Other: -0.33 {i14} in {+110}Pd(|a,2n|g) (1997Dr03) 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.46 {I9}; A{-4}=0.19 {I13} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$from {+110}Pd(|a,2n|g) (1993De09); Other: 2.7 {I10} in {+110}Pd(|a,2n|g) (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.39 {I5} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$possible M2 admixture of |d=-0.08 {I5} {+110}Pd(|a,2n|g) (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$A{-2}=0.35 {I10}; A{-4}=0.17 {I12} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 
MR$Other: 3.6 {I+20-10} from |g|g(|q) in {+110}Pd(|a,2n|g) (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_comment:
M,MR$A{-2}=0.07 {I7}, A{-4}=0.03 {I16} and |d=+0.22 {I5} (1972Wa03) 
CC$0.00195 {I4} from adopted gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
placed in the level scheme in 1992Ku01 
RI$from 1992Ku01 and normalized using I|g(815,57|g)=3.5 
M$A{-0}=1.2 {I1}; A{-2}/A{-0}=0.02 {I2} (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,(E2)
decay_comment:
M$A{-2}=0.14 {I14} (1997Dr03) 
M$D,(E2) sin 1997Dr03 in contradiction with adopted value 
Level energy difference=1007.21 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-0}=213.4 {I10}; A{-2}/A{-0}=-0.233 {I7} (1993De09) 
possible M2 admixture; |d=-0.02 {I2} (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$a{-0}=1.9 {I1}; A{-2}/A{-0}=0.46 {I9}; A{-4}/A{-0}=0.19 {I13} (1993De09) 
MR$Also: 2.7 {I10} (1993De09) 


decay_energy_unit: KEV
decay_multipolarity: D
decay_uncertain: ?
decay_comment:
E$ambiguous transition, reported only in 1993De09. It is not reported in the following paper 1997Dr03 and not confirmed in (n,n'|g) 2001Ga44. Instead, it was suggested to de-excite the 2403.28-keV level 
M$A{-0}=3.1 {I1}; A{-2}/A{-0}=0.24 (1993De09) 
possible Q admixture; |d=0.05 {I25} (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-0}=8.8 {I3}; A{-2}/A{-0}=-0.21 {I5} (1993De09) 
possible M2 admixture; |d:-0.02 {I5} (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-0}=11.4 {I5}; A{-2}/A{-0}=-0.35 {I10} (1993De09) Possible M2 admixture; |d=-0.13 {I13} (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-0}=3.7 {I1}; A{-2}/A{-0}=0.048 {I22}; A{-4}/A{-0}=-0.3 {I3} (1993De09) 
MR$Also: +1.8 {i8} (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-0}=3.6 {I2}; A{-2}/A{-0}=-0.13 {I3} (1993De09) 
possible M2 admixture; |d=0.03 {I5} (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-0}=6.9 {I2}; A{-2}/A{-0}=-0.58 {I5}; A{-4}/A{-0}=0.19 {I6} (1993De09) 
MR$Also: -0.30 {i12} (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-0}=106.05; A{-2}/A{-0}=-0.250 {I6} (1993De09) 
stretched E1 transition; |d=-0.008 {I12} (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$A{-0}=2.95 {I6}; A{-2}/A{-0}=-0.18 {I4} (1993De09) 
possible quadrupole admixture; |d=+0.03 {I3} (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$A{-0}=6.2 {I2}; A{-2}/A{-0}=-0.29 {I3}; A{-4}/A{-0}=0.07 {I4} (1993De09) 
possible quadrupole admixture; |d=-0.07 {I11} (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-0}=26.3 {I2}; A{-2}/A{-0}=-0.249 {I14} (1993De09) 
possible M2 admixture; |d=-0.01 {I2} (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-0}=1.8 {I1}; A{-2}/A{-0}=0.15 {I5}; A{-4}/A{-0}=0.10 {I8} (1993De09) 
MR$Also: +1.3 {i2} (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$A{-0}=3.2 {I1}; A{-2}/A{-0}=-0.20 {I6} (1993De09) 
possible quadrupole admixture; |d=0.00 {I6} (1997Dr03) 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
E$observed only in 1993De09 
M$A{-0}=6.8 {I1}; A{-2}/A{-0}=0.350 {I14}; A{-4}/A{-0}=-0.11 {I2} (1993De09) 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
Transition reported only in 1993De09 
M$A{-2}=2.75 {I5}; A{-2}/A{-0}=0.33 {I2}; A{-4}/A{-0}=-0.06 {I4} (1993De09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-0}=6.8 {I1}; A{-2}/A{-0}=0.42 {I3}; A{-4}/A{-0}=-0.03 {I4} (1993De09) 
MR$Also: -0.09 {i12} (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-0}=0.96 {I6}; A{-2}/A{-0}=-0.40 {I10}; A{-4}/A{-0}=0.15 {I16} (1993De09) 
MR$Also: +7 {i4} (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$A{-0}=12.0 {I20}; A{-2}/A{-0}=-0.281 {I12} (1993De09) 
possible quadrupole admixture; |d=-0.2 {I3} (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-0}=1.12 {I5}; A{-2}/A{-0}=0.32 {I6}; A{-4}/A{-0}=0.17 {I8} (1993De09) 
MR$Also: -0.42 {I+15-40} (1997Dr03) 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_uncertain: ?
decay_comment:
transition reported only in 1993De09 
M$A{-0}=3.9 {I1}; A{-2}/A{-0}=0.25 {I4} (1993De09) 
MR$from 1993De09 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-0}=2.32 {I5}; A{-2}/A{-0}=0.28 {I4}; A{-4}/A{-0}=-0.11 {I5} (1993De09) 
MR$Also: -0.33 {i14} (1997Dr03) 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_uncertain: ?
decay_comment:
transition seen only in 1993De09 
M$A{-0}=3.74 {I15}; A{-2}/A{-0}=-0.43 {I8} (1993De09) 
MR$from 1993De09 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
M$A{-0}=1.9 {I1}; A{-2}/A{-0}=0.46 {I9}; A{-4}/A{-0}=0.19 {I13} (1993De09) 
MR$from 1993De09; Also: 2.7 {I10} (1993De09) 


decay_energy_unit: KEV
decay_multipolarity: E1
decay_comment:
M$A{-0}=2.6 {I1}; A{-2}/A{-0}=-0.39 {I5} (1993De09) 
possible M2 admixture; |d=-0.08 {I5} (1993De09) 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
M$A{-0}=4.3 {I1}; A{-2}/A{-0}=0.35 {I10}; A{-4}/A{-0}=0.17 {I12} (1993De09) 
MR$from 1993De09; Also: 3.6 {I+20-10} (1993De09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$ as per e-mail reply (Aug 14/01) from the lead author (P. Garrett) of 2001Ga44, listed experimental energy of 1248.14 {I12} should be replaced by level-energy difference. Since this peak lies on the tail of a strong 1253 peak, experimental energy is not reliable 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1398.7 in table 1 of 2001Ga44 is a misprint (as per e-mail reply Aug 14/01 from the lead author (P. Garrett)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_comment:
ECC$0.00267 {I13}, using weighted average of |a(K)exp=0.00235 {I18} (1997Dr03) and 0.00234 {I12} (1991Gi05), and |a/|eK=1.143 {I24} (2008Ki07) 
MR$Others: +0.10 {I7} (1973Gr16); 0.05 or +2.0 {I+7-5} (1969Mi07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$From I|g(233.86|g)/I|g(851.285|g)=0.010 {I3} and I|g(851.285|g) from from {+112}In |e decay (14.88 min) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_comment:
M$|a(K)exp=2.34|*10{+-3} {I12} (1991Gi05); A{-2}=0.086 {I45}; A{-4}=-0.081 {I100} (1972Ka34) 
MR$Other: 0.048 {I22} from |g(|w) in 1991Gi05, -0.21 {I+5-6} in |g|g(|w) in 1972Ka34 
$Ice(K)(E0,2+ to 2+)/Ice(K)(M1,2+ to 2+)=0.41 {I7}, B(E0)/B(E2)=2.7 {I13}, B(E0)/B(M1)=2555 {I472} and |r{+2}(E0)=0.031 {I20} (1991Gi05) 
CC$From adopted gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$From 2009Gr10; |DE estimated by the evaluators 
RI$from the adopted I|g branching ratio and I|g(1253.56|g)=4.7 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|a(K)exp=0.00317 {I16} (1997Dr03); |a(L)exp=0.00039 {I4} (1997Dr03); |a(M)exp=0.000138 {I15} (1997Dr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_comment:
M$|a(K)exp=0.00235 {I18} (1997Dr03) 
MR$From |g(|w) in 1997Dr03. Other solution: |d=1.96 {I70} 
$Ice(K)(E0,2+ to 2+)/Ice(K)(M1,2+ to 2+)=0.43 {I11}, B(E0)/B(E2)=2.6 {I15}, and B(E0)/B(M1)=2700 {I700} (1991Gi05) 


decay_energy_unit: KEV
decay_multipolarity: E1
decay_comment:
$|G{-0}/|G=85.4 {I8} 
M$|e=-0.10 {i8} from polarization measurements in {+112}Cd(|g,pol |g') (2005Ko32) 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
$|G{-0}/|G=49.9 {I9} 
M$|e=+0.08 {i10} from polarization measurements in {+112}Cd(|g,pol |g') (2005Ko32) 
RI$70 {I4} in 1999Le31 


decay_energy_unit: KEV
decay_multipolarity: E1
decay_comment:
$|G{-0}/|G=72.1 {I8} 
M$|e=-0.13 {i6} from polarization measurements in {+112}Cd(|g,pol |g') (2005Ko32) 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
$|G{-0}/|G=72.0 {I11} 
M$|e=+0.27 {i12} from polarization measurements in {+112}Cd(|g,pol |g') (2005Ko32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-2.3 {I+19-|@} in 2001Ga44; -2.3 {I19} in the ENSDF dataset 
$B(E2)(W.u.)=21 {I+5-18} (2020Ga10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E,RI,MR$from 2001Ga44 
E$somewhat poor fit, level-energy difference=532.07 
$B(E2)(W.u.)=16 {I+40-15} (2020Ga10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$|d from 1987BaYW in (n,n'|g) is discrepant with |d>1.1 in |b{+-} decay, but agrees with |d=0.29 {i1} (1958Mc02) in Coul. ex. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$obtained by low-energy photon spectrometer. 
TI$from I(|g+ce)(17.7|g)/I(|g+ce)(316.3|g) in {+113}Ag |b{+-} decay (68.7 s). 
M$from I|g and I(|g+ce) 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
TI$calculated from the decay scheme with assumption of no |b{+-} feeding of the 298 level. 
RI$from I(|g+ce) and |a 
M$from {+113}Ag |b{+-} decay (5.37 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$from 1972An28. |d=0.29 (1958Mc02) from |g(|q) and linear polarization. |d=0.26 {I+5-5} or -3.6 {I+6-10} (1991KrZR) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E5
decay_comment:
RI$ measured in 2011Ko01 as intensity/100 decays of {+113m}Cd 
M$ From Adopted Gammas of {+113}Cd in ENSDF database 
$ Theoretical conversion coefficients are from BrIcc code 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI$reported by 1976De42 in (n,n'|g) with I|g=56 {i28}, not reported in (n,|g); evaluator estimates I|g<13 in (n,|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI$reported by 1976De42 in (n,n'|g) with I|g=124 {i11}, not reported in (n,|g); evaluator estimates I|g<43 in (n,|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|d from 1976De42. 1982Hu08 give +0.19 {I+22-16} discrepant with -2.20 {I15} reported by 1987Ar24 in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E others: 131.39 {I6} (1969WiZX), 131.4 {I2} (1970Hn01) 
RI 23 {I3} (1981Me17) 
M from |a(K)exp=0.16 {I5} 
RI 24 {I3} (1981Me17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E others: 213.5 {I2} (1970Hn01), 213.3 (1973BrXC) 
RI 25.7 {I20} (1981Me17) 
M from |a(K)exp=0.071 {I15} 
RI 25.7 {I20} (1981Me17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
EKC$Uncertainty of 0.00001 in Table I of 2009Ba52 seems unrealistic, the compilers have increased the uncertainty by a factor of 10 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$M1 proposed by 2009Ba52 is inconsistent with |DJ|p 
$|a(K)exp=8|*10{+-3} {i2} is also listed in the text on page 9 of 2009Ba52 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$|d from 1990Ar20. Others: -0.30 {I+5-6} (1976De42), 0.6 {I+8-5} (1977Ne01), -2.05 {I26} (2003Ka45) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$or +0.44 {I10} for J=3 (1991Ar17). |d=0.0 or +2.3 {I+10-5} for J=2 (1977Ne01). |d=+0.40 {I5} for J=3 (1976De42) 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
M$|DJ=0,D from A{-2}=+0.181 {I38} and A{-4}=+0.023 {I58} from 800.4|g-727.9|g(|q). Theoretical values for a |DJ=0, dipole transition and a 19/2 -> 19/2 ->15/2 cascade are A{-2}=+0.165 and A{-4}=0.0, while those for a mixed |DJ=1, M1+E2 transition (|d=0.55) and 21/2- ->19/2- ->15/2 cascade are A{-2}=+0.183 and A{-4}=-0.011. Theoretical values of A{-2}=+0.176 and A{-4}=+0.03 for a mixed |DJ=0, M1+E2 transition (|d=-0.20) and 19/2- ->19/2- ->15/2 cascade are also consistent with the observations, but the non-observation of |g-ray transition to the 15/2- level would argue against 19/2- assignment. 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
M$from A{-2}=-0.065 {I11} and A{-4}=+0.022 {I16} using 1058.3|g-677.0|g(|q). Theoretical values for a pure dipole, |DJ=1 transition and 5 ->4 ->2 cascade are A{-2}=-0.071 and A{-4}=0.0 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
M$from A{-2}=-0.049 {I23} and A{-4}=-0.018 using 704.7|g-770.8|g(|q). Theoretical values for a pure dipole, |DJ=1 transition and 7 ->6 ->4 cascade are A{-2}=-0.071 and A{-4}=0.0 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
EKC from I(K| x ray)/I|g 
TI from intensity balance 
RI$Deduced by evaluators from |g-ray transition intensity balance at 27-keV level using I(|g+ce)(26.9|g)=410 {I10} (from |g rays feeding the 27-keV level) and assuming no |b{+-} feeding to this level. Thus I|g(26.9|g)=(410 {I10})/1 + |a=(410 {I10})/1 + (21.2 {I6})=18.5 {I7}. Other value: 21 {I4} (experimental, 1975Ka09). 
M |a(K)exp is consistent with |a(K)(M1) and also |a(K)(E2). But, E2 is ruled out since |a(E2) leads to a larger (and inconsistent) value for I(|g+ce) due to the large L-shell conversion for an E2 multipolarity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
EKC given for 399.1|g+400.1|g 
M if 400.1|g is E2 from decay scheme, the combined |a(K)exp suggests the 399.1|g to be E1, or possibly M1,E2. 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
M$|DJ=0 D from A{-2}=+0.194 {I35} and A{-4}=-0.057 {I78} from 759.8|g-749.8|g(|q). Theoretical values for a pure |DJ=0 dipole transition and a 19/2 -> 19/2 ->15/2 cascade are A{-2}=+0.165 and A{-4}=0.0, while those for a mixed |DJ=1, M1+E2 transition (|d=0.60) and 21/2- ->19/2- ->15/2 cascade are A{-2}=+0.194 and A{-4}=-0.012. J|p=19/2+ is preferred by 2010Lu01 from comparison with level structure in {+117}Cd 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
M$from A{-2}=+0.120 {I16} and A{-4}=-0.005 {I24} using 829.7|g-697.6|g(|q). Theoretical values for a pure quadrupole transition and 6 ->4 ->2 cascade are A{-2}=+0.102 and A{-4}=0.009 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
M$from A{-2}=-0.100 {I25} and A{-4}=-0.040 {I39} using 925.6|g-697.6|g(|q). Theoretical values for a pure dipole transition and 5 ->4 ->2 cascade are A{-2}=-0.071 and A{-4}=0.0. Other: A{-2}=-0.087 {I20} and A{-4}=-0.023 {I31} using 925.6|g-505.9|g(|q). Theoretical values for a pure dipole transition and 5 ->4 ->2 ->0 cascade are A{-2}=-0.071 and A{-4}=0.0. 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
M$from A{-2}=-0.095 {I35} and A{-4}=-0.021 {I54} using 491.8|g-829.7|g(|q). Theoretical values for a pure dipole transition and 7 ->6 ->4 cascade are A{-2}=-0.071 and A{-4}=0.0. Other: A{-2}=-0.123 {I11} and A{-4}=+0.013 {I18} using 570.2|g-491.8|g(|q). Theoretical values for a pure dipole transition and 9 ->7 ->6 cascade are A{-2}=-0.118 and A{-4}=0.0. 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
M$from A{-2}=+0.098 {I28} and A{-4}=+0.010 {I42} using 852.8|g-829.7|g(|q). Theoretical values for a pure quadrupole transition and 8 ->6 ->4 cascade are A{-2}=+0.102 and A{-4}=+0.009 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$ |g not listed in Table I of 2012Ba58, included here based on e-mail reply of Jan 17, 2013 from J.C. Batchelder 
RI$ deduced by compilers from listed I|b value=0.3 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$ form table II of 2012Ba58; not listed in authors' table I. 2515.7 listed as level in authors' table II seems a misprint 


decay_energy_unit: KEV
decay_multipolarity: [M1,E2]
decay_comment:
CC$|a=127 {i6} for M1, 9.90|*10{+4} {i8} for E2 
E$deduced from the level scheme 
TI$from an intensity balance at the 7.52 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$from A{-2}=+0.58 {I14}, A{-4}=+0.45 {I19} for (1135|g)(569|g)(|q) (1995Za01): 0-2-0 spin sequence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$from A{-2}=+0.29 {I15}, A{-4}=+0.56 {I21} for (1422|g)(569|g)(|q) (1995Za01): 0-2-0 spin sequence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_uncertain: ?
decay_comment:
E,M$the placements of 123.67|g and 263.87|g from the same level are proposed by 2013Ka08, with the 123.67|g feeding the 11/2- isomer at 144 keV {I4} from their direct mass measurement. However, such placement of 123.67|g results in J|p=(7/2+), thus Mult=[M2], and consequently an unreasonably large B(M2)(W.u.)=56 {+17-11} greatly exceeding RUL=1. This |g is placed from a 440, (9/2-) level to feed the 11/2- isomer at E=316 keV proposed in 1989Hu10. It could also be implied that the 123.67|g could de-excite a different level with a very close energy. It is the evaluator's opinion that the further investigation is needed to firmly make the placement of the 123.67|g and the level scheme as well. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_uncertain: ?
decay_comment:
E$the placements of 123.67|g and 263.87|g from the same level are proposed by 2013Ka08, with the 123.67|g feeding the 11/2- isomer at 144 keV {I4} from their direct mass measurement. However, such placement of 123.67|g results in J|p=(7/2+), thus Mult=[M2] and consequently an unreasonably large B(M2)(W.u.)=56 {+17-11} greatly exceeding RUL=1. This |g is placed from a 440, (9/2-) level to feed the 11/2- isomer at E=316 keV proposed in 1989Hu10. It could also be implied that the 123.67|g could de-excite a different level with a very close energy. It is the evaluator's option that the further investigation is needed to firmly make the placement of the 123.67|g and the level scheme as well. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$I|g(537.1)/I|g(796.5|g)=0.154 from I|g data, 0.12 from branching ratio in Fig. 6, both data from |g|g-coin 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$I|g(309.1)/I|g(1247.8|g)=0.74 from I|g data, 0.76 from branching ratio in Fig. 6, both data from |g|g-coin 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$compiler's note: 2021Ba34 assign (E2) in Table IV, but from |DJ|p, it can be (M1+E2) which is assigned here. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$2014Ba18 placed the 827 keV |g as the transition from 2695 keV level to 1869 keV level in low spin {+126}Ag decay, but no |g is reported from 1868 keV level. The placement of the 827 keV |g is uncertain. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(exp)=6.4 {I9} 
ECC$from |g|g coincidence data with gate on 238|g in ({+136}Xe,X|g) 
M$from |a(exp) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
TI$1098 {I160} (e-mail reply from authors of 2019Lu08) 
$Absolute I(|g+ce)=100 {I31} for 141|g (2012Hi07), implying I|g=84 {I26} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
RI$637 {I123} (e-mail reply from authors of 2019Lu08) 
$Absolute I|g=72 {I26} for 1297|g (2012Hi07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
$When gated on 2048|g, only one event was seen at 95 keV in 2019Lu08. 
RI$365 {I114} (e-mail reply from authors of 2019Lu08) 
$Absolute I|g=53 {I26} for 2048|g (2012Hi07) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$From best fit for the tas spectrum in {+102}Sn |e decay obtained with 94 keV |g being E2 and 69 keV |g being M1 


decay_energy_unit: KEV
decay_multipolarity: (M4)
decay_comment:
M suggested from comparable situation in {+105,107,109,111}In and similar B(M4)(W.u.) values, e.g. 11.0 for {+103}In and 13.7 for {+105}In where M4 character of this transition is well established 


decay_energy_unit: KEV
decay_multipolarity: (M4)
decay_BM_unit: mu^2 x (fm)^6
decay_BM_info: ;TYPE=BM4;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM4W
decay_comment:
M suggested from comparable situation in {+105,107,109,111}In and similar B(M4)(W.u.) values, e.g. 11.4 for {+107}In and 10.0 for {+109}In where M4 character of this transition is well established 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
RI$Deduced by the evaluators from I(tot)=720 given by the authors assuming transition is M4 
M$from |a(exp)=0.055 {I6} (2006Ka44) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$the |g-ray peak was contaminated by the 8+ to 6+ transition in {+104}Cd. I|g, A{-2} and A{-4} values were obtained by subtraction of the component of {+104}Cd, assuming that |g in {+104}Cd shows |g(|q) with A{-2}=+0.28 and A{-4}=-0.08. 
M$pol>1 
$A{-2}=-0.04~{I8}; A{-4}=0.05~{I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
CC$|a(K)exp measured using a mini-orange spect. |a(K)exp=0.049 {I6} ce(K)/I|g (1973Ny03) normalized to |a(K)exp(662|g,{+137}Ba)=0.092 
E$av: 678.6 {I4} (1972Ri16), 678.3 {I3} (1975Di12). Others: 678 (1973Ny03), 678.8 (1976Hs01) 
M$based on |a(K)exp and HF(M4) systematics 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
E$from 1972Ri16. Other: 678.8 (1976Hs01) 
RI$from 1972Ri16, 1976BuZF, could be erroneous because equilibrium. T{-1/2}(Parent)/(isomer)=3.5 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_comment:
|a(K)exp=0.00085 {I26}, A{-2}=0.13 {I3} 
MR undetermined; for analogous 11/2+ to 9/2+ transitions, |d(1153|g,{+111}In)=+0.4 {I1} (1978He10), |d(1133|g,{+115}In)=+0.51 {I4} (1977Kr13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
A{-2}=-0.12 {I4} 
MR undetermined; for analogous 3/2- to 1/2- transition, |d(261|g,{+115}In)=-0.09 {I6} (1973Ba29) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$this transition connects the the 4213 and 3357 keV levels in 1997Ko51. Placed from this level by 1998Ta26 on coincidence arguments. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$ initial level=5042.0 listed in authors' table I seems a misprint. it should be the final level as shown in authors' level-scheme figure 2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+(E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
TI$from int. balance at the 266 level. 
RI$I|g from 1977Va14 
M 1978Hs01 estimate I(|g+ce)(36.6|g)/I|g(396|g)|?0.10 on the basis of coincidence data although the transition is not seen in their singles spectrum; thus, |a|?14. The requirement of an intensity balance at the 266 level leads to |a=14 {i4}. |a(theory)=60.4(E2), 9.5(M1); thus, |d<0.45. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from 1977Va14 corrected for contribution from summing of 396 and 104|g's. 1978Hs01 report I|g=2.7 {i2}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from 1977Va14 who established that most of the intensity in the 565 peak is from summing of the 396.3 and 168.2|g's. 1978Hs01 report I|g=3.0 {i4}, 1981Bu20 report I|g=2.1 {i6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Level-energy difference=150.8 
$DCO=1.68 {i6} 
$DCO(|DJ=2,Q gated)=0.98 {i6} 
$Other I|g=8.3 {i8} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_uncertain: ?
decay_comment:
$DCO=1.07 {i1} 
E$Uncertainty of 0.1 keV quoted by 2001Ch71 seems to be underestimated since the least-squares adjustment gives E|g=528.4 keV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$this transition is not given in the authors' table but is shown in their level scheme 
RI$I|g deduced from I|g/I|g(811.3|g)=0.033 {I2} in authors' level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_BM_unit: mu^2 x (fm)^6
decay_BM_info: ;TYPE=BM4;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM4W
decay_comment:
E$Other: 650.1 {I3} from {+108}Cd(d,n|g), and 649.8 {I3} from {+107}Ag(|a,2n|g). 
M$|a(exp)=0.07 {i2}(1956Pe56), |a(exp)=0.08 {i3}, K/L=6.2 {i9} (1965Kh04) from {+109}Sn |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$Other: 331.2 {I3} from {+108}Cd(d,n|g) and 331.0 {I4} from {+107}Ag(|a,2n|g). 
M$a{-2}/a{-0}=-0.14 {i4}, a{-4}/a{-0}=+0.08 {i5}(1979Va13) in {+107}Ag(|a,2n|g); |a(K)exp=12|*10{+-3} (1965Kh04),|a(K)exp=28|*10{+-3} (1970Sh05) in {+109}Sn |e decay; a{-2}/a{-0}=-0.08 {i4} (1975Di12) in {+108}Cd(d,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$Other: 1026.0 {I5} from {+108}Cd(d,n|g), 1026.35 {I8} from {+107}Ag(|a,2n|g), 1026.2 {I5} from {+96}Zr({+19}F,6n|g), 1025.3 {I6} (1994ByZZ) in {+109}In IT decay (0.210 s), 1027.6 {I1} (1997Ko51) in {+92}Mo({+19}F,2p|g). 
M$|a(K)exp=1.1|*10{+-3} {I3}, pol=-0.47 {i5}, |d=+0.40 {I+9-4}, a{-2}/a{-0}=+0.25 {i1}, a{-4}/a{-0}=-0.04 {i2} (1979Va13) in {+107}Ag(|a,2n|g); R=0.65 {i3} (1997Ko51) in {+92}Mo({+19}F,2p|g); |a(K)exp=1.08|*10{+-3} {i10}, a{-2}/a{-0}=+0.15 {i3} (1975Di12) in {+108}Cd(d,n|g); |a(K)exp=0.0046 (1970Sh05) in {+109}Sn |e decay 
MR$deduced by evaluators using experimental conversion coefficients and mixing ratio from |g(|q) using the BrIccMixing program. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$Other: 1099.2 {I5} from {+108}Cd(d,n|g), and 1099.5 {I3} from {+107}Ag(|a,2n|g) 
M$|a(K)exp=0.79|*10{+-3} {i14}, a{-2}/a{-0}=+0.01 {i3} (1975Di12) in {+108}Cd(d,n|g); |a(K)exp=0.89|*10{+-3} {I20}, pol=0.11 {i13}, a{-2}/a{-0}=+0.01 {i2}, a{-4}/a{-0}=-0.03{i3} (1979Va13) in {+107}Ag(|a,2n|g); |a(K)exp=0.0013 (1970Sh05) in {+109}Sn |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$Other: 522.2 {I3} in {+108}Cd(d,n|g). 
M$|a(K)exp=1.5|*10{+-3} {i3}, a{-2}/a{-0}=+0.004 {i30} (1975Di12) in {+108}Cd(d,n|g); |a(K)exp=0.012 (1970Sh05) in {+109}Sn |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Other: 1320.8 {I5} in {+108}Cd(d,n|g). 
M$|a(K)exp=0.59|*10{+-3} {i20}, a{-2}/a{-0}=+0.04 {i3} (1975Di12) in {+108}Cd(d,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from {+107}Ag(|a,2n|g). Others: 402.2 {I5} from {+109}In IT decay (0.210 s), 401.6 {I4} from {+108}Cd(d,n|g), 402 {I1} from {+76}Ge({+37}Cl,4n|g), 402.0 {I2} from {+92}Mo({+19}F,2p|g), and 402.2 {I5} from {+96}Zr({+19}F,6n|g). 
RI$weighted average of 26 {I7} from {+109}In IT decay (0.210 s), 23.1 {I23} from {+108}Cd(d,n|g), 23.8 {I10} from {+107}Ag(|a,2n|g), and 19.5 {I14} from {+96}Zr({+19}F,6n|g). Other: 19.0 {I5} from {+92}Mo({+19}F,2p|g) 
M$|a(K)exp=10|*10{+-3} {I4}, pol=-0.25 {i3}, |d=+0.07 {i03}, a{-2}/a{-0}=-0.11 {i2}, a{-4}/a{-0}=-0.03 {i3}(1979Va13) in {+107}Ag(|a,2n|g); |a(K)exp=15|*10{+-3} {I5} (1975Di12) in {+108}Cd(d,n|g), R=1.10 {i3} (1997Ko51) in {+92}Mo({+19}F,2p|g) 
MR$deduced by evaluators using experimental conversion coefficient and mixing ratio from |g(|q) using the BrIccMixing program. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from {+107}Ag(|a,2n|g). Others: 1427.5 {I5} from {+109}In IT decay (0.210 s), 1428.4 {I6} from {+108}Cd(d,n|g), 1428 {I1} from {+76}Ge({+37}Cl,4n|g), 1429.4 {I1} from {+92}Mo({+19}F,2p|g), and 1428.4 {I5} from {+96}Zr({+19}F,6n|g). 
RI$weighted average of 100 {I20} from {+109}In IT decay (0.210 s), 100 {I19} from {+108}Cd(d,n|g), 100.0 {I3} from {+92}Mo({+19}F,2p|g), and 100 {I6} from {+96}Zr({+19}F,6n|g). 
M$|a(K)exp=0.53|*10{+-3} {I8}, pol=+0.33 {i6}, a{-2}/a{-0}=+0.32 {i1}, a{-4}/a{-0}=-0.16 {i2} (1979Va13) in {+107}Ag(|a,2n|g); R=1.56 {i2} (1997Ko51) in {+92}Mo({+19}F,2p|g); a{-2}/a{-0}=+0.32 {i12} (1975Di12) in {+108}Cd(d,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$Other: 460.1 {I5} in {+108}Cd(d,n|g). 
RI$weighted average of 13 {I6} from {+109}Sn |e decay and 7.9 {I26} from {+108}Cd(d,n|g). 
M$|a(K)exp=8|*10{+-3} {i4} (1975Di12) in {+108}Cd(d,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 790.9 {I3} from {+109}Sn |e decay and 791.2 {I5} from {+108}Cd(d,n|g). 
RI$weighted average of 100 {I4} from {+109}Sn |e decay and 100 {I13} from {+108}Cd(d,n|g). 
M$|a(K)exp=1.4|*10{+-3} {i4}, a{-2}/a{-0}=+0.09 {i8} (1975Di12) in {+108}Cd(d,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$Others: 437.6 {I5} in {+108}Cd(d,n|g) and 437.0 {I2} in {+107}Ag(|a,2n|g). 
RI$weighted average of 50 {I13} from {+109}Sn |e decay, 55 {I7} from {+108}Cd(d,n|g) 
M$|a(K)exp=10|*10{+-3} {i4}, a{-2}/a{-0}=-0.25 {i7} (1975Di12) in {+108}Cd(d,n|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$Other: 1463.4 {I5} from {+108}Cd(d,n|g). 
RI$weighted average of 100 {I30} from {+109}Sn |e decay and 100 {I17} from {+108}Cd(d,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Other: 311.6 {I5} from {+108}Cd(d,n|g). 
RI$Other: 9 {I3} in {+108}Cd(d,n|g). Other: 25 {I3} from {+109}Sn |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$Other: 384.2 {I3} from {+108}Cd(d,n|g). 
RI$from {+108}Cd(d,n|g) 
M$|a(K)exp=12.4|*10{+-3} {i13}, a{-2}/a{-0}=-0.07 {i4} (1975Di12) in {+108}Cd(d,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$from {+108}Cd(d,n|g) only. This |g could correspond to the 501.2|g from the 1482.2 level observed in {+109}Sn |e decay 
M$|a(K)exp|?3.6|*10{+-3}, 1975Di12 in {+108}Cd(d,n|g) suggest (M1,E2), but not compatible with parity 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Others: 614.2 {I4} from {+108}Cd(d,n|g), and 614.2 {I3} from {+107}Ag(|a,2n|g). 
M$M1 or E2 from |a(K)exp=2.5|*10{+-3} {i9} (1975Di12) in {+108}Cd(d,n|g), |DJ=2 based on J|p(1713)=9/2+ deduced from |g transitions to 5/2+ and 13/2+ rules out M1. A{-2}/a{-0}=-0.12 {i6}, a{-4}/a{-0}=+0.02{i4} (1979Va13) in {+107}Ag(|a,2n|g) is for an unresolved doublet with transition in {+109}Cd produced in {+109}In decay and in the (|a, pn|g) reaction. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$Other: 623.6 {I4} from {+108}Cd(d,n|g). 
M$|a(K)exp=3.5|*10{+-3} {i13} (1975Di12) in {+108}Cd(d,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$Other: 833.0 {I5} from {+108}Cd(d,n|g) 
M$|a(K)exp=1.7|*10{+-3} {i7} (1975Di12) in {+108}Cd(d,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Other: 874.0 {I5} from {+96}Zr({+19}F,6n|g) 
M$|a(K)exp=1.3|*10{+-3} {I3}, pol=-0.48 {i6}, a{-2}/a{-0}=0.19 {i2}, a{-4}/a{-0}=0.00{i3}, |d=+0.32 {I+17-7} (1979Va13) in {+107}Ag(|a,2n|g); 
MR$deduced by evaluators using experimental conversion coefficient and mixing ratio from |g(|q) using the BrIccMixing program 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3
decay_BM_unit: mu^2 x (fm)^4
decay_BM_info: ;TYPE=BM3;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM3W
decay_comment:
E$from 1979Va13 in {+107}Ag(|a,2n|g). Others: 673.5 {I1} from {+109}In IT decay (0.210 s), 673.2 from {+96}Zr({+19}F,6n|g) (2012Ne03), 674 {I1} from {+76}Ge({+37}Cl,4n|g) (1997VaZS). 1979Va13 also report a unplaced prompt |g ray at E|g=673.85 with mult=E2. This prompt |g ray is also reported by 2012Ne03 in {+96}Zr({+19}F,6n|g) and by 1997Ko51 in {+92}Mo({+19}F,2p|g), and is placed from a J|p=17/2+ level, slightly above the E=2101.8 level. 
M$|a(K)exp=19.9|*10{+-3} {I20}, K/L=7.5 {i7} (1979Va13) in {+107}Ag(|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$placement as suggested in by 1997Ko51 and 2012Ne03. Unplaced in 1979Va13. Others: 673.9 {I3} (1997Ko51) in {+92}Mo({+19}F,2p|g), 673.8 {I5} (2012Ne03) in {+96}Zr({+19}F,6n|g). 1997VaZS in {+76}Ge({+37}Cl,4n|g) has placed an unresolved doublet of E|g=674 {I1} from the isomer at E=2101.8 (J|p=19/2+) and from a level at E=2995.4 (J|p=17/2+). The evaluators have adopted the placement here for the latter 
M$|a(K)exp=2.4|*10{+-3} {I5}, a{-2}/a{-0}=+0.26 {i2}, a{-4}/a{-0}=-0.18 {i3} (1979Va13) in {+107}Ag(|a,2n|g), DCO(Q)=1.13 {I14} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$|a(K)exp=2.1|*10{+-3} {I4}, pol=-0.85 {i9}, |d=+0.19 {i+1-3}, a{-2}/a{-0}=+0.05 {i2}, a{-4}/a{-0}=-0.04{i3} (1979Va13) in {+107}Ag(|a,2n|g) 
MR$deduced by evaluators from the experimental conversion coefficient and mixing ratio from |g(|q) using the BrIccMixing program. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$from {+107}Ag(|a,2n|g). Other: 1245.7 {I5} from {+96}Zr({+19}F,6n|g), 1246 {I1} from {+76}Ge({+37}Cl,4n|g) 
M$|a(K)exp<0.34|*10{+-3}, pol=+0.14 {i5}, a{-2}/a{-0}=-0.26 {i3}, a{-4}/a{-0}=-0.09 {i6} (1979Va13) in {+107}Ag(|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$others: 893 {I1} from 1997VaZS in {+76}Ge({+37}Cl,4n|g). 2012Ne03 in {+96}Zr({+19}F,6n|g) have tentatively placed a |g-ray of E|g=893.7 {I5} from a level at E=2996. The evaluators has adopted the placement here. 
M$|a(K)exp=1.7|*10{+-3} {I4}, pol=-0.51 {i8}, a{-2}/a{-0}=+0.10 {i2}, a{-4}/a{-0}=-0.06{i3} (1979Va13) in {+107}Ag(|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E,RI$other: E|g=984.3 {I10}, I|g=100 {I43} from {+108}Cd(d,n|g) 
M$|a(K)exp=1.08|*10{+-3} {i10} (1975Di12) in {+108}Cd(d,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 259.0 {I4} from {+107}Ag(|a,2n|g), 260 {I1} from {+76}Ge({+37}Cl,4n|g), and 260.4 {I5} from {+96}Zr({+19}F,6n|g). 
RI$from {+96}Zr({+19}F,6n|g). Other: 7 {I4} from {+107}Ag(|a,2n|g) 
M$a{-2}/a{-0}=-0.14 {i7}, a{-4}/a{-0}=-0.16 {i14} (1979Va13) in {+107}Ag(|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$others: 1104.0 {I10} from {+92}Mo({+19}F,2p|g), and 1103.8 {I5} from {+96}Zr({+19}F,6n|g), 1104 {I1} from {+76}Ge({+37}Cl,4n|g) 
M$|a(K)exp=0.38|*10{+-3} {I9}, pol=+0.35 {i5}, a{-2}/a{-0}=-0.266 {i10}, a{-4}/a{-0}=-0.022 {i17} (1979Va13) in {+107}Ag(|a,2n|g); R=0.77 {i2} (1997Ko51) in {+92}Mo({+19}F,2p|g); DCO(Q)=0.50 {i5} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$others: 336 {I1} from {+76}Ge({+37}Cl,4n|g), 335.9 {I1} from {+92}Mo({+19}F,2p|g), and 336.6 {I5} from {+96}Zr({+19}F,6n|g). 
M,MR$|a(K)exp=18|*10{+-3} {I8}, pol=-0.14 {i4},|d=0.03 {i3} from |g(|q), a{-2}/a{-0}=-0.113 {i8}, a{-4}/a{-0}=-0.033 {i14} (1979Va13) in {+107}Ag(|a,2n|g); R=0.98 {i3} (1997Ko51) in {+92}Mo({+19}F,2p|g); DCO(Q)=0.69 {i4} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
E$other: 88.9 {I5} from {+96}Zr({+19}F,6n|g), 89 {I1} from {+76}Ge({+37}Cl,4n|g) 
M,MR$a{-2}/a{-0}=-0.206 {i9}, a{-4}/a{-0}=+0.01 {i2}, |d=0.01 {i4} (1979Va13) in {+107}Ag(|a,2n|g); R=1.02 {i1} (1997Ko51) in {+92}Mo({+19}F,2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$others: 856.2 {I5} from {+96}Zr({+19}F,6n|g), 856 {I1} from {+76}Ge({+37}Cl,4n|g) 
RI$other: 19.8 {I13} from {+96}Zr({+19}F,6n|g) 
M$|a(K)exp|<1.0|*10{+-3}, pol=-0.48 {i6}, a{-2}/a{-0}=+0.38 {i3}, a{-4}/a{-0}=-0.04 {i5} (1979Va13) in {+107}Ag(|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$pol=-0.64 {i15}, |d=0.14 {i7}, a{-2}/a{-0}=-0.04 {i3}, a{-4}/a{-0}=-0.06 {i5} (1979Va13) in {+107}Ag(|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 223.4 {I3} from {+107}Ag(|a,2n|g), 223 {I1} from {+76}Ge({+37}Cl,4n|g), 223.5 {I2} from {+92}Mo({+19}F,2p|g), and 223.1 {I5} from {+96}Zr({+19}F,6n|g). 
M$|a(K)exp=24|*10{+-3} {I12}, a{-2}/a{-0}=-0.18 {i3}, a{-4}/a{-0}=+0.09 {i5} (1979Va13) in {+107}Ag(|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$others: 990 {I1} from {+76}Ge({+37}Cl,4n|g), 989.4 {I10} from {+92}Mo({+19}F,2p|g), and 990.4 {I5} from {+96}Zr({+19}F,6n|g). 
M$|a(K)exp=0.45|*10{+-3} {I15}, pol=-0.62 {i14}, a{-2}/a{-0}=+0.32 {i3}, a{-4}/a{-0}=-0.01 {i5} (1979Va13) in {+107}Ag(|a,2n|g); R=0.85 {i7} (1997Ko51) in {+92}Mo({+19}F,2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
E$others: 164 {I1} from {+76}Ge({+37}Cl,4n|g), 164.7 {I2} from {+92}Mo({+19}F,2p|g), and 164.6 {I5} from {+96}Zr({+19}F,6n|g). 
M$|a(K)exp=159|*10{+-3} {i50}, |d=0.01 {i5}, a{-2}/a{-0}=-0.197 {i9}, a{-4}/a{-0}=-0.017 {i15} (1979Va13) in {+107}Ag(|a,2n|g); R=0.82 {i2} (1997Ko51) in {+92}Mo({+19}F,2p|g); DCO(Q)=0.78 {I8} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
E$others: 110 {I1} from {+76}Ge({+37}Cl,4n|g), 110.1 {I3} from {+92}Mo({+19}F,2p|g), and 110.4 {I5} from {+96}Zr({+19}F,6n|g). 
RI$others: 23.5 {I6} from {+92}Mo({+19}F,2p|g), 89 {I5} from {+96}Zr({+19}F,6n|g) 
M,MR$a{-2}/a{-0}=-0.24 {i2}, a{-4}/a{-0}=+0.04 {i2},|d=-0.05 {i7} (1979Va13) in; R=0.73 {i1} (1997Ko51); DCO(D)=0.99 {i21} (2012Ne03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
E$weighted average of 244.5 {I3} from {+107}Ag(|a,2n|g), 244 {I1} from {+76}Ge({+37}Cl,4n|g), 244.7 {I2} from {+92}Mo({+19}F,2p|g), and 244.6 {I5} from {+96}Zr({+19}F,6n|g). 
RI$others: 100 {I1} from {+92}Mo({+19}F,2p|g), and 100 {I5} from {+96}Zr({+19}F,6n|g) 
M$|a(K)exp=34|*10{+-3} {I12}, pol=-0.27 {i13}, |d=0.00 {i4}, a{-2}/a{-0}=-0.21 {i2}, a{-4}/a{-0}=0.01 {i2} (1979Va13) {+107}Ag(|a,2n|g); R=0.76 {i1} (1997Ko51) in {+92}Mo({+19}F,2p|g; DCO(Q)=0.70 {i10} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
M$|a(K)exp=36|*10{+-3} {I18}, a{-2}/a{-0}=-0.18 {i3}, a{-4}/a{-0}=+0.13 {i4} (1979Va13) in {+107}Ag(|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$others: 208 {I1} from {+76}Ge({+37}Cl,4n|g), 207.9 {I1} from {+92}Mo({+19}F,2p|g), and 208.0 {I5} from {+96}Zr({+19}F,6n|g). 
RI$others: 100.0 {I2} from {+92}Mo({+19}F,2p|g), and 100 {I5} from {+96}Zr({+19}F,6n|g). 
M,MR$|a(K)exp=59|*10{+-3} {I20}, pol=-0.42 {i15}, |d=-0.02 {i7}, a{-2}/a{-0}=-0.217 {i10}, a{-4}/a{-0}=-0.032 {i17}(1979Va13) in {+107}Ag(|a,2n|g); R=0.82 {i2} (1997Ko51) in {+92}Mo({+19}F,2p|g); DCO(Q)=0.75 {i14} (2012Ne03) {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$others: 288 {I1} from {+76}Ge({+37}Cl,4n|g), 287.9 {I3} from {+92}Mo({+19}F,2p|g), and 288.0 {I5} from {+96}Zr({+19}F,6n|g). 
RI$from {+92}Mo({+19}F,2p|g). Other: 17 {I3} in {+107}Ag(|a,2n|g) and 10.8 {I13} in {+96}Zr({+19}F,6n|g). 
M$a{-2}/a{-0}=-0.13 {i5}, a{-4}/a{-0}=-0.02 {i8} (1979Va13) in {+107}Ag(|a,2n|g); DCO(D)=1.0 {i3} (2012Ne03) {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$others: 339 {I1} from {+76}Ge({+37}Cl,4n|g), 339.4 {I2} from {+92}Mo({+19}F,2p|g), and 339.7 {I5} from {+96}Zr({+19}F,6n|g). 
M,MR$|a(K)exp=19|*10{+-3} {I8}, pol=-0.26 {i10}, |d=+0.05 {i3} a{-2}/a{-0}=-0.097 {i11}, a{-4}/a{-0}=-0.018 {i9} (1979Va13) in {+107}Ag(|a,2n|g); R=1.05 {i4} (1997Ko51) in {+92}Mo({+19}F,2p|g); DCO(Q)=0.56 {i5} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E,RI$from {+92}Mo({+19}F,2p|g) (1997Ko51). 2012Ne03 in {+96}Zr({+19}F,6n|g) tentatively place a |g ray of 211.4 keV 5 from a level at E=4686 while 1997VaZS in {+76}Ge({+37}Cl,4n|g) place a |g ray of 211 keV 1 from the level at E=4565 keV. 
M$DCO(Q)=0.56 {I17}, DCO(D)=1.15 {I20} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_uncertain: ?
decay_comment:
E,RI$from {+92}Mo({+19}F,2p|g) (1997Ko51). Other: E|g=363.5 {I5} from {+96}Zr({+19}F,6n|g) (2012Ne03). 1997VaZS in {+76}Ge({+37}Cl,4n|g) have placed a |g ray of 362 from the level at E=4928 
M$DCO(Q)=0.63 {I10} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E,RI$from {+92}Mo({+19}F,2p|g). Other: E|g=338.4 {I5}, I|g=13.1 {I18} from {+96}Zr({+19}F,6n|g) 
M$DCO(Q)=0.56 {I5} for 339.7+338.4 (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$others: 390 {I1} from {+76}Ge({+37}Cl,4n|g), 389.8 {I2} from {+92}Mo({+19}F,2p|g), and 390.1 {I5} from {+96}Zr({+19}F,6n|g). 
RI$weighted average of 100 {I4} from {+107}Ag(|a,2n|g), 100 {I1} from {+92}Mo({+19}F,2p|g), and 100 {I6} from {+96}Zr({+19}F,6n|g). 
M,MR$|a(K)exp=13|*10{+-3} {I4}, pol=-0.35 {i6}, |d=+0.04 {i3}, a{-2}/a{-0}=-0.151 {i12}, a{-4}/a{-0}=-0.027 {i20} (1979Va13) in {+107}Ag(|a,2n|g); R=1.02 {i6} (1997Ko51) in {+92}Mo({+19}F,2p|g; DCO(Q)=0.61 {i8} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$others: 576 {I1} from {+76}Ge({+37}Cl,4n|g), 575.4 {I4} from {+92}Mo({+19}F,2p|g), and 575.6 {I5} from {+96}Zr({+19}F,6n|g). 
M$|a(K)exp=3.0|*10{+-3} {I15}, a{-2}/a{-0}=-0.29 {i4}, a{-4}/a{-0}=-0.09 {i6} (1979Va13) in {+107}Ag(|a,2n|g); DCO(D)=1.04 {i17} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E,RI$from {+92}Mo({+19}F,2p|g). Other: E|g=470.9 {I5}, I|g=41 {I4} from {+96}Zr({+19}F,6n|g) 
M$DCO(D)=0.93 {I14} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E,RI$from {+92}Mo({+19}F,2p|g). Other: E|g=708.1 {I5}, I|g=100 {I4} from {+96}Zr({+19}F,6n|g) 
M$R=0.95 {i6} (1997Ko51) in {+92}Mo({+19}F,2p|g), DCO(D)=1.28 {I19} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_multipolarity: (M1)
decay_comment:
E$2012Ne03 in {+96}Zr({+19}F,6n|g) tentatively place a |g ray of 211.4 keV 5 from a level at E=4686; 1997Ko51 in {+92}Mo({+19}F,2p|g) tentatively place a |g ray of 211.0 keV 2 from a level at E=3485 keV. The evaluators have adopted the placement here by 1997VaZS in {+76}Ge({+37}Cl,4n|g). 
M$DCO(Q)=0.56 {I17}, DCO(D)=1.15 {I20} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$from {+92}Mo({+19}F,2p|g). Others: 324.4 {I5} from {+96}Zr({+19}F,6n|g), 324 {I1} from {+76}Ge({+37}Cl,4n|g) 
RI$from {+96}Zr({+19}F,6n|g) 
M$R=0.90 {i4} (1997Ko51) in {+92}Mo({+19}F,2p|g); DCO(Q)=0.73 {i18} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_multipolarity: (M1)
decay_comment:
E$2012Ne03 in {+96}Zr({+19}F,6n|g) tentatively place a |g ray of 354.8 keV 5 from a level at E=5408; 1997Ko51 in {+92}Mo({+19}F,2p|g) tentatively place a |g ray of 353.9.9 keV 2 from a level at E=(6259) keV. The evaluators have adopted the placement here by 1997VaZS in {+76}Ge({+37}Cl,4n|g). 1997VaZS also place a |g ray of E|g=354 {I1} from the level at E=6272. 
M$DCO(D)=1.2 {i4} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_multipolarity: (M1)
decay_comment:
E$2012Ne03 in {+96}Zr({+19}F,6n|g) tentatively place a |g ray of 362.5 keV 5 from a level at E=3485; 1997Ko51 in {+92}Mo({+19}F,2p|g) tentatively place a |g ray of 361.9 keV 2 from a level at E=3485 keV. The evaluators have adopted the placement here by 1997VaZS in {+76}Ge({+37}Cl,4n|g). 
M$DCO(Q)=0.63 {i10} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$from {+96}Zr({+19}F,6n|g). Other: 589 {I1} from {+76}Ge({+37}Cl,4n|g) 
M$DCO(D)=1.0 {i5} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
M$R=0.96 {i4} (1997Ko51) in {+92}Mo({+19}F,2p|g); DCO(D)=1.19 {i23} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$2012Ne03 in {+96}Zr({+19}F,6n|g) have tentatively placed a |g-ray of E|g=497.2 {I5} from a level at E=3982 and 1997Ko51 in {+92}Mo({+19}F,2p|g) have tentatively placed a |g-ray of E|g=497.0 {I3} from a level at E=4474. The evaluators have adopted the placement here by 1997VaZS in {+76}Ge({+37}Cl,4n|g). 
M$DCO(D)=1.03 {I16} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$from {+92}Mo({+19}F,2p|g) (1997Ko51). Other: 555 {I1} from {+76}Ge({+37}Cl,4n|g) (1997VaZS) and 554.7 {I5} in {+96}Zr({+19}F,6n|g) (2012Ne03). 2012Ne03 also report a |g ray of E|g=555.4 {I5} from a level at E=5581. 
M$DCO(D)=0.9 {i3} for 555.4+554.7 (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$2012Ne03 in {+96}Zr({+19}F,6n|g) have tentatively placed a |g-ray of E|g=492.9 {I5} from a level at E=4475 and 1997Ko51 in {+92}Mo({+19}F,2p|g) have tentatively placed a |g-ray of E|g=492.0 {I2} from a level at E=3977. The evaluators have adopted the placement here by 1997VaZS in {+76}Ge({+37}Cl,4n|g). 
M$DCO(D)=1.20 {I22} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_multipolarity: (M1)
decay_comment:
E$2012Ne03 in {+96}Zr({+19}F,6n|g) have tentatively placed a |g-ray of E|g=581.3 {I5} from a level at E=5990 and 1997Ko51 in {+92}Mo({+19}F,2p|g) have tentatively placed a |g-ray of E|g=581.8 {I3} from a level at E=5905. The evaluators have adopted the placement here by 1997VaZS in {+76}Ge({+37}Cl,4n|g). 1997VaZS also place a |g ray of E|g=582 {I1} from the level at E=8005. 
M$DCO(D)=1.1 {I4} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$2012Ne03 in {+96}Zr({+19}F,6n|g) have tentatively placed a |g-ray of E|g=367.1 {I5} from a level at E=5054 and 1997Ko51 in {+92}Mo({+19}F,2p|g) have tentatively placed a |g-ray of E|g=367.6 {I2} from a level at E=5423. The evaluators have adopted the placement here by 1997VaZS in {+76}Ge({+37}Cl,4n|g). 
M$DCO(D)=1.0 {I3} (2012Ne03) in {+96}Zr({+19}F,6n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
%I|g=29.6 {I9}, using the calculated normalization. 
RI$from Table 3 in 1981Bu17, while I|g=93 from Table 4. 
M$|a(exp)=0.07 {i2}(1956Pe56), |a(exp)=0.08 {i3}, K/L=6.2 {I9} (1965Kh04), 0.07 (1970Sh05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=9.4 {I4}, using the calculated normalization. 
M$|a(K)exp=0.012 (1965Kh04), |a(K)exp=0.028 (1970Sh05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
%I|g=3.98 {I21}, using the calculated normalization. 
RI$from 17.6 {I7} for the doublet placed from levels at E=1026 and 2126, and individual intensity of I|g|?13 and I|g=4, respectively, in 1981Bu17 
M$|a(K)exp=0.0046 (1970Sh05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
%I|g=0.064 {I21}, using the calculated normalization. 
E,M,MR$From Adopted gammas 
RI$From I(|g+ce)=1.2 {I4} (from intensity balances) and branching from adopted gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
%I|g=0.287 {I10}, using the calculated normalization. 
E,M$From Adopted gammas 
RI$From I(|g+ce)=1.2 {I4} (from intensity balances) and branching from adopted gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
%I|g=0.13 {I4}, using the calculated normalization. 
RI$From adopted gammas and I|g(790.9|g)=5.2. I|g=0.7 {I3} in 1991Bu17 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g=1.61 {I18}, using the calculated normalization. 
RI$From adopted gammas. Other: 8.6 {I13} for 437.2|g+437.4|g, I(437.2|g)=5 and I(437.4|g)=3.6 in 1981Bu17 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.41 {I9}, using the calculated normalization. 
E$it is indicated in Table 3 of 1981Bu17 that this |g is assigned in the decay scheme but no specific placement is made. Evaluators have made this placement based on |g-ray energy. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=1.1 {I4}, using the calculated normalization. 
RI$from 8.6 {I13} for 437.2|g+437.4|g, I(437.2|g)=5 and I(437.4|g)=3.6 in 1981Bu17 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=1.17 {I21}, using the calculated normalization. 
RI$from 17.6 {I7} for the doublet placed from levels at E=1026 and 2126, and individual intensity of I|g|?13 and I|g=4, respectively, in 1981Bu17 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
%I|g=0.47 {I9}, using the calculated normalization. 
E,RI$unresolved with 1107.7|g from E=2924 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=0.47 {I9}, using the calculated normalization. 
E,RI$unresolved with 1107.2|g from E=2592 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$for prompt+delayed components of this transition, 50 {I3} for the prompt component only 
M$|a(K)exp=1.1|*10{+-3} {I3}, pol=-0.47 {i5}, a{-2}/a{-0}=+0.215 {i9}, a{-4}/a{-0}=-0.030{i13} for prompt+delayed components, a{-2}/a{-0}=+0.25 {i1}, a{-4}/a{-0}=-0.04 {i2} for prompt component only (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$|a(K)exp=0.89|*10{+-3} {I20}, pol=+0.11 {i13}, a{-2}/a{-0}=+0.01 {i2}, a{-4}/a{-0}=-0.03{i3} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$for prompt+delayed components of this transition, 14 {I4} for the prompt component only 
M$|a(K)exp=10|*10{+-3} {I4}, pol=-0.25 {i3}, a{-2}/a{-0}=-0.080 {i8}, a{-4}/a{-0}=-0.017 {i14} for prompt+delayed components, a{-2}/a{-0}=-0.11 {i2}, a{-4}/a{-0}=-0.03 {i3} for prompt component only (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$for prompt+delayed components of this transition, 61 {I3} for the prompt component only 
M$|a(K)exp=0.53|*10{+-3} {I8}, pol=+0.33 {i6}, a{-2}/a{-0}=+0.191 {i11}, a{-4}/a{-0}=-0.097{i11} for prompt+delayed components, a{-2}/a{-0}=+0.32 {i1}, a{-4}/a{-0}=-0.16 {i2} for prompt component only (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=1.3|*10{+-3} {I3}, pol=-0.48 {i6}, a{-2}/a{-0}=+0.19 {i2}, a{-4}/a{-0}=0.00 {i3} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=2.1|*10{+-3} {I4}, pol=-0.85 {i9}, a{-2}/a{-0}=+0.05 {i2}, a{-4}/a{-0}=-0.04 {i3} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp<0.34|*10{+-3}, pol=+0.14 {i5}, a{-2}/a{-0}=-0.26 {i3}, a{-4}/a{-0}=-0.09 {i6} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$|a(K)exp=1.7|*10{+-3} {I4}, pol=-0.51 {i8}, a{-2}/a{-0}=+0.10 {i2}, a{-4}/a{-0}=-0.06 {i3} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp=0.38|*10{+-3} {I9}, pol=+0.35 {i5}, a{-2}/a{-0}=-0.266 {i10}, a{-4}/a{-0}=-0.022 {i17} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=18|*10{+-3} {I8}, pol=-0.14 {i4}, a{-2}/a{-0}=-0.113 {i8}, a{-4}/a{-0}=-0.033 {i14} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp|<1.0|*10{+-3}, pol=-0.48 {i6}, a{-2}/a{-0}=+0.38 {i3}, a{-4}/a{-0}=-0.04 {i5} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp=0.45|*10{+-3} {I15}, pol=-0.62 {i14}, a{-2}/a{-0}=+0.32 {i3}, a{-4}/a{-0}=-0.01 {i5} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=34|*10{+-3} {I12}, pol=-0.27 {i13}, a{-2}/a{-0}=-0.21 {i2}, a{-4}/a{-0}=+0.01 {i2} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=59|*10{+-3} {I20}, pol=-0.42 {i15}, a{-2}/a{-0}=-0.217 {i10}, a{-4}/a{-0}=-0.032 {i17} (1979Va13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=19|*10{+-3} {I8}, pol=-0.26 {i10}, a{-2}/a{-0}=-0.097 {i11}, a{-4}/a{-0}=-0.018 {i9} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=13|*10{+-3} {I4}, pol=-0.35 {i6}, a{-2}/a{-0}=-0.151 {i12}, a{-4}/a{-0}=-0.027 {i20} (1979Va13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$|a(K)exp|?3.6|*10{+-3}. 1975Di12 suggest (M1,E2), not compatible with parity change of the level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$other: 20 {I5} (1965Al15) and 25 (1994ByZZ) 
$DRI=0.5 in RI=0.20+/0.5 in 1965Al15 could be a typo 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$497.1 listed in figure 1 of 2012Ne03. Transition shown from 27/2 to 25/2 in table I of 2012Ne03 
M$DCO(D)=1.03 {I16} (2012Ne03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$|a(K)exp=0.18 {I4} and A{-2}=-0.192 {I19}, A{-4}=0.069 {I23} (1987Kr15). Other: |a(K)exp=0.133 {I9} (1989Kr12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.19 {I5} and A{-2}=-0.31 {I4}, A{-4}=-0.05 {I5} (1987Kr15). Other: M1 from |a(K)exp=0.14 {I3} (1989Kr12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
M$|a(K)exp=0.005 {I3} (1989Kr12) in {+107}Ag(|a,n|g) and from DCO=2.14 {I16} (2001Ch71) in {+96}Zr({+19}F,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
M$|a(K)exp=0.00082 {I4} (1989Kr12) in {+107}Ag(|a,n|g) and from DCO=2.04 {I10} in {+96}Zr({+19}F,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
RI$Other: 40 {I4} in {+110}Cd(p,n|g) 
M$|a(K)exp=0.0058 {I19} and A{-2}=0.03 {I6}, A{-4}=0.17 {I11} (1987Kr15) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E,M$From level-energy difference, transition shown in {+96}Zr({+19}F,5n|g). mult=[M2] suggested by the authors 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$Others: 283 keV (1956Me94), 281 keV (1973Ka45) 
RI$Deduced from I(|g+ce) 
M$K/L=8 {I1} in 1956Me94 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$From |a(K)exp=0.18 {I4} and A{-2}=-0.192 {I19}, A{-4}=0.069 {I23} at Ep=5.6 MeV. Others: A{-2}=-0.22 {I5} at Ep=5.2 MeV, A{-2}=-0.170 {I13}, A{-4}=0.003 {I16} at Ep=6 MeV 
MR$From E(p)=5.6 MeV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$From A{-2}=-0.23 {I4}, A{-4}=0.03 {I5} at 5.6 MeV and |a(K)exp=0.31 {I6}. Other: A{-2}=-0.21 {I3}, A{-4}=-0.01 {I3} at Ep=6 MeV 
MR$From Ep=5.6 MeV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$From |a(K)exp=0.032 {I3} and A{-2}=-0.193 {I11}, A{-4}=-0.009 {I13} at Ep=5.6 MeV. Other: A{-2}=0.172 {I17}, A{-4}=-0.014 {I21} at Ep=6 MeV 
MR$From Ep=5.6 MeV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$From |a(K)exp=0.0291 {I23} and A{-2}=-0.004 {I13}, A{-4}=-0.011 {I15} at Ep=5.6 MeV 
MR$From Ep=5.6 MeV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$From |a(K)exp=0.19 {I5} and A{-2}=-0.31 {I4}, A{-4}=-0.05 {I5} at Ep=5.6 MeV. Other: A{-2}=-0.207 {I30}, A{-4}=0.004 {I34} at Ep=6 MeV 
MR$From Ep=5.6 MeV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$From |a(K)exp=0.066 {I16} and A{-2}=-0.155 {I13}, A{-4}=-0.006 {I17} 
MR$+0.03 {I2} deduced from |g(|q) reported 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$From |a(K)exp=0.0067 {I4} and A{-2}=-0.164 {I18}, A{-4}=-0.021 {I25}. Other: A{-2}=-0.35 {I16}, A{-4}=-0.12 {I21} at Ep=5.6 MeV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Least-squares fit gives 209.88 {I6} 
DCO=1.04 {I2} 
DCO(|DJ=2,Q gated)=0.63 {I13} 
$Other I|g=100 {I3} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$A dotted transition (involving |DJ=3) to 1396.3 keV, (9+) level that is shown in figure 3 of 2001Ch71 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$A dotted transition (involving |DJ=4) to 1396.3 keV, (9+) level that is shown in figure 3 of 2001Ch71 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$misprinted as 1.1 {i8} in authors' table 1. See authors' table 2. Others: 9.7 {i6} (1972Bu41), 7.9 (1976MeZD) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=+0.27 {i3}, A{-4}=+0.01 {i3}. Others: |a(K)exp=0.00085 {i15}, A{-2}=+0.46 {i4}, K/L=10 {I5} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from table I of 2011Ba05; +0.20 {I10} in authors' table ii 
$ DCO=1.4 {I3} gated on |DJ=1, dipole 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from table I of 2011Ba05; +0.18 {I+8-7} in authors' table ii 
$ DCO=0.98 {I11} gated on 371|g (|DJ=1,M1+E2, |d=+0.20 {I10}) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from table I of 2011Ba05; +0.25 {I+8-9} in authors' table ii 
$ DCO=1.07 {I12} gated on 371|g (|DJ=1,M1+E2, |d=+0.20 {I10}) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
$Absolute I|g=0.25% {I4} (ENSDF dataset, also NuDat) 
$I|g(relative)=8.9 {I5} (2022Ch11), 9.5 {I8} (ENSDF dataset) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$Absolute I|g=0.64% {I11} (ENSDF dataset, also NuDat) 
$I|g(relative)=23.2 {I26} (2022Ch11), 24 {I2} (ENSDF dataset) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
$Absolute I|g=2.65% {I40} (ENSDF dataset, rounded to 2.7 in NuDat) 
$I|g(relative)=100 {I10} (2022Ch11), 100 (ENSDF dataset) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$Absolute I|g=0.38% {I6} (ENSDF dataset, also NuDat) 
$I|g(relative)=14.2 {I16} (2022Ch11), 14.4 {I8} (ENSDF dataset) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Absolute I|g=1.31% {I20} (ENSDF dataset, also NuDat) 
$I|g(relative)=48.4 {I47} (2022Ch11), 49.5 {I18} (ENSDF dataset) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Absolute I|g=0.42% {I7} (ENSDF dataset, also NuDat) 
$I|g(relative)=17.4 {I11} (2022Ch11), 16.0 {I8} (ENSDF dataset) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Absolute I|g=1.48% {I23} (ENSDF dataset, also NuDat) 
$I|g(relative)=57.4 {I53} (2022Ch11), 55.8 {I19} (ENSDF dataset) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Absolute I|g=1.99% {I31} (ENSDF dataset, rounded to 2.0 {I3} in NuDat) 
$I|g(relative)=73.7 {I68} (2022Ch11), 75 {I3} (ENSDF dataset) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Absolute I|g=0.30% {I5} (ENSDF dataset, also NuDat) 
$I|g(relative)=10.5 {I11} (2022Ch11), 11.5 {I8} (ENSDF dataset) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Absolute I|g=0.51% {I8} (ENSDF dataset, also NuDat) 
$I|g(relative)=22.1 {I16} (2022Ch11), 19.2 {I8} (ENSDF dataset) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3
decay_BM_unit: mu^2 x (fm)^4
decay_BM_info: ;TYPE=BM3;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM3W
decay_comment:
M$|a(K)exp=5.4 {I5} in {+112}Cd(p,n|g) (1988Ki04), 5.8 {I12} in {+112}In IT decay (20.56 min) (1962Ru05) and 4.8 {I3} in {+109}Ag(|a,n|g) (1991Kr14); |a(L)exp=1.36 {I12} in {+112}Cd(p,n|g) (1988Ki04); K/LM=3.3 {I7} (1962Ru05) and 3.7 {I4} in {+112}In IT decay (20.5 min) (1953Bl44) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
E$not observed experimentally. Obtained from energy level difference by the evaluators 
M$From J|p difference 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.130 {I4}; A{-4}=0.022 {I6} in {+112}Cd(p,n|g) (1983Ko12); |a(K)exp=0.066 {I5}, weighted average of 0.059 {I7} in {+109}Ag(|a,n|g) (1988Ki04) and 0.072 {I6} in {+112}Cd(p,n|g) (1988Ki04); |a(L)exp=0.0068 {I7} in {+109}Ag(|a,n|g) (1988Ki04) and 0.0075 {I6} in {+112}Cd(p,n|g) (1988Ki04); |a(M)exp=0.0015 {I4} in {+109}Ag(|a,n|g) (1988Ki04) and 0.0013 {I1} in {+112}Cd(p,n|g) (1988Ki04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.203 {I9}; A{-4}=-0.007 {I11} in {+112}Cd(p,n|g) (1983Ko12); |a(K)exp=0.036 {I4} in {+109}Ag(|a,n|g) (1988Ki04) and 0.041 {I3} {+112}Cd(p,n|g) (1988Ki04); |a(L)exp=0.0054 {I10} in {+112}Cd(p,n|g) (1988Ki04); |a(M)exp=0.0013 {I3} in {+112}Cd(p,n|g) (1988Ki04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.287 {I52}; A{-4}=0.005 {I66} in {+112}Cd(p,n|g) (1983Ko12); |a(K)exp=0.18 {I2} in {+109}Ag(|a,n|g) (1988Ki04) and 0.20 {I4} in {+112}Cd(p,n|g) (1988Ki04); |d=0.01 {I10} in {+112}Cd(p,n|g) (1983Ko12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=0.156 {I25}; A{-4}=-0.020 {I30} in {+112}Cd(p,n|g) (1983Ko12); 
M$|a(K)exp=0.0111 {I11} in {+109}Ag(|a,n|g) (1988Ki04) and 0.0127 {I12} in {+112}Cd(p,n|g) (1988Ki04); |d=0.05 {I5} in {+112}Cd(p,n|g) (1983Ko12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.082 {I11}; A{-4}=0.032 {I14} in (1983Ko12) and p{-exp}=-0.19 {I4} in {+112}Cd(p,n|g) (1983Ko12); |a(K)exp=0.0046 {I6} in {+109}Ag(|a,n|g) (1988Ki04) and 0.0045 {I4} in {+112}Cd(p,n|g) (1988Ki04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$DCO=1.17 {I10} in {+100}Mo({+16}O,p3n|g) (2012Tr01); |a(K)exp=0.015 {I2} and |a(L)exp=0.0015 {I2} in {+109}Ag(|a,n|g) (1988Ki04) 
MR$from PAC measurements (1987Iw04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|a(K)exp=0.022 {I3}; |a(L)exp=0.0019 {I3} in {+109}Ag(|a,n|g) (1988Ki04); DCO=0.42 {I15} in {+110}Pd({+7}Li,5n|g) (2011He04); Others: DCO=1.06 {I7} in {+100}Mo({+16}O,p3n|g) (2012Tr01); pol=-0.079 {I28} in {+100}Mo({+16}O,p3n|g) (2012Tr01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.092 {I18} and A{-4}=0.004 {I23} in {+112}Cd(p,n|g) (1983Ko12); Also: A{-2}=-0.079 {I7} and A{-4}=0.010 {I9} in {+112}Cd(p,n|g) (1983Ko12) pol=-0.10 {I10} in {+112}Cd(p,n|g) (1983Ko12); |a(K)exp=0.0042 {I10} {+109}Ag(|a,n|g) (1988Ki04) and 0.00099 {I15} in {+112}Cd(p,n|g) (1988Ki04) 
MR$from {+112}Cd(p,n|g) (1983Ko12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-2}=-0.238 {I69}; A{-4}=0.033 {I91} in {+112}Cd(p,n|g) (1983Ko12); |a(K)exp=0.072 {I12}; |a(L)exp=0.0097 {I10} in {+109}Ag(|a,n|g) (1988Ki04); 
MR$from {+112}Cd(p,n|g) (1983Ko12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.171 {I14}; A{-4}=0.006 {I18} in {+112}Cd(p,n|g) (1983Ko12); pol=-0.35 {I6} in {+112}Cd(p,n|g) (1983Ko12); |a(K)exp=0.024 {I5} in {+112}Cd(p,n|g) (1988Ki04) 
MR$from {+112}Cd(p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp=0.0065 {I14}, weighted average of 0.007 {I2} in {+109}Ag(|a,n|g) (1988Ki04) and 0.006 {I2} in {+112}Cd(p,n|g) (1988Ki04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=0.086 {I20}; A{-4}=0.029 {I27} in {+112}Cd(p,n|g) (1983Ko12); pol=-0.20 {I10} in {+112}Cd(p,n|g) (1983Ko12); |a(K)exp=0.00063 {I7} in {+112}Cd(p,n|g) (1988Ki04); |d=0.00 {I12} or -0.31 {I7} in {+112}Cd(p,n|g) (1983Ko12); 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|a(K)exp=0.067 {I7}, weighted average of 0.060 {I6} in {+109}Ag(|a,n|g) (1988Ki04) 0.073 {I6} in {+112}Cd(p,n|g) (1988Ki04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=0.159 {I19}; A{-4}=0.009 {I25} in {+112}Cd(p,n|g) (1983Ko12); pol=-0.24 {I11} in {+112}Cd(p,n|g) (1983Ko12); |a(K)exp=0.009 {I1} in {+112}Cd(p,n|g) (1988Ki04); 


