# DECAY

decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$|a(K)exp=3.2 {I8} 
$|a(K): from comparison of I|g(87|g) compared with the iodine K|a x-ray intensity in a spectrum double gated on the 135.2|g and the 69.0|g from {+109}Tc. 
M$assigned as M1+E2 in 2006Ur02 based on |a(K)exp, however, theory gives |a(K)=0.96 and 1.8 for M1 and E2 multipolarities, respectively. Thus, multipolarity assignment should be considered tentative. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp=7 {I1} 
$|a(K)exp: from intensity of iodine K|a x-ray, 42.6|g and 234|g in spectrum gated by 1111|g and 261|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$A{-2}=0.101 {I6}, A{-4}=0.009 {I10} for 260.7|g-1111.8|g cascade (2010Li03) 
E$Placement from 2010Li03. An unplaced |g ray was observed in 1972ClZN, 1970Jo20 (E|g=261.1) and 1972Ho08 (E|g=260.9). In 1970Jo20 this |g ray is reported to decay with T{-1/2}=4 ns and in 1972ClZN with T{-1/2}=3.4 ns {I6}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
RI$other: 53 {I5} (1978Ze08) 
CC$experimental value from I|g(x) (1977Sc21), corrected for 12 % {I2} contribution to I(x) from conversion of other transitions. 
M,MR$from |a(exp) in 1977Sc21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
RI$other: 13 {I2} (1978Ze08) 
M$assumed M1+E2 for the purpose of balancing intensity through the 87.3-keV level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.5 to +1.7 from |g|g(|q) and |g(lin pol) 
$pol=+0.08 {I3} 
$(554.2|g)(400.2|g)(|q): A{-2}=-0.233 {I6}, A{-4}=-0.033 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$(620.5|g)(333.9|g)(|q): A{-2}=-0.109 {I3}, A{-4}=+0.014 {I4} 
$(620.5|g)(488.2|g)(|q): A{-2}=+0.10 {I4}, A{-4}=-0.03 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$pol=+0.15 {I5} 
$(358.4|g)(295.8|g)(|q): A{-2}=-0.06 {I5}, A{-4}=-0.07 {I7} 
$(358.4|g)(400.2|g)(|q): A{-2}=+0.098 {I2}, A{-4}=-0.011 {I4} 
$(358.4|g)(724.9|g)(|q): A{-2}=+0.10 {I1}, A{-4}=+0.02 {I1} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
MR$-1.3 {I+2-1} or -0.55 {I+7-10} from |g|g(|q) (2009Li42). The value with dominant E2 component is supported by shell-model predicted value of -3.9 


decay_energy_unit: KEV
decay_multipolarity: [M1]
decay_comment:
TI$reported by 2022Mo11 as sum of gamma-ray and ce electron intensities assuming M1 multipolarity for the 118-keV transition. 


decay_energy_unit: KEV
decay_multipolarity: [E2]
decay_comment:
TI$reported by 2022Mo11 as sum of gamma-ray and ce electron intensities assuming E2 multipolarity for the 155-keV transition. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
CC$overlaps M1 and E2 
$K-conversion coefficient measured by triple |g coin technique and comparing K-x-ray intensity to |g-ray intensity 
$(198|g)(summed gates)(|q): A{-2}=-0.10 {I1}, A{-4}=+0.10 {I1} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
$(274|g)(summed gates)(|q): A{-2}=+0.03 {I1}, A{-4}=-0.06 {I2}. Sign of A{-4} is inconsistent with |DJ=1 transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$1986Ma41 placed this |g from a 289 level because the 11/2- level was not fed in {+117}Cs |b{++} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$1992JuZX propose the placement of this transition because coin between 108|g with 205|g and 386|g but the 108|g is also in coin with the 84|g in {+117}Cs decay (1986Ma41) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|a(K)exp=0.0058 {I14} for a composite peak of 586.2|g+586.0|g 
M |a(K)exp suggests E2,M1; but M1 is rejected from |g(|q) in (HI,xn|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
ce(K)=0.031 {I6}. This value is upper limit 
M from large value for ce(K) for the combined 891 transition; 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI from I(845.7|g+847.0|g)=21.0 {I16} and I(847.0|g)<3.0 
M from |g(|q) and value of I|g(150|')/I|g(80|') for the composite peak of 845.7|g and 847.0|g. These values are considered on the basis of intensities of both |g's to be mainly due to the 845.7|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$B(E2)=49 {I13}, relative to 1 for 1028.8|g. 2020Mu17 have assumed pure E2 for 438.0|g and 1028.8|g 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
$This line is barely visible in the summed spectrum and not seen in the spectra at different distances (2020Mu17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+(E2)
decay_comment:
RI$Measured value of 52.0 {I8} includes intensity from {+119}Cs |e decay (30.4 s). Value used here assumes no |e feeding to 169-keV (5/2+) from 119Cs(9/2+) parent nucleus. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$Measured value of 100 includes intensity from {+119}Cs |e decay (30.4 s). I|g=2.12 contribution from {+119}Cs |e decay (30.4 s) has been removed. |DI|g estimated by evaluators. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+(E2)
decay_comment:
RI$Measured value of 93.2 {I7} includes intensity from {+119}Cs |e decay (30.4 s). I|g=8.9 {I3} contribution from {+119}Cs |e decay (30.4 s) has been removed. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI$Measured value of 12.20 {I8} includes intensity from {+119}Cs |e decay (30.4 s). I|g=11.0 contribution from {+119}Cs |e decay (30.4 s) has been removed. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$Measured value of 1.4 {I2} includes intensity from {+119}Cs |e decay (30.4 s). I|g=1.26 contribution from {+119}Cs |e decay (30.4 s) has been removed. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
RI$Measured value of 4.0 {I2} includes intensity from {+119}Cs |e decay (30.4 s). I|g=3.6 contribution from {+119}Cs |e decay (30.4 s) has been removed. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$Measured value of 2.12 {I8} includes intensity from {+119}Cs |e decay (30.4 s). I|g=1.9 contribution from {+119}Cs |e decay (30.4 s) has been removed. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$Measured value of 1.46 {I7} includes intensity from {+119}Cs |e decay (30.4 s). I|g=1.31 contribution from {+119}Cs |e decay (30.4 s) has been removed. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$Measured value of 1.64 {I8} includes intensity from {+119}Cs |e decay (30.4 s). I|g=1.48 contribution from {+119}Cs |e decay (30.4 s) has been removed. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$Evaluators assumed the 176-keV level to be populated only through the 524 (5/2+)-keV level. Thus I(|g+ce)(176)= I(|g+ce)(348)=2.14 {I8}. Using |a(176)=0.0434 gives I|g(176)=2.05(8). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+(E2)
decay_comment:
RI$Evaluators assumed the 225-keV level to be populated only through the 476(3/2+,5/2+)- and 524(5/2+)-keV levels. Thus I(|g+ce)(225)=I(|g+ce)(250)+I(|g+ce)(299)=5.6(2)+4.2(2)=9.8(3). Using |a(225)=0.097 gives I|g(225)=8.9(3). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E given as 485.5 {I10} in authors' table, 484.5 in drawing. The 485.5 keV may be a misprint (evaluators) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E given as 849.7 {I10} in author's table, 894.9 in drawing. The 849.7 keV may be a misprint (evaluators) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
I(|g+ce)(E0)=191 {I11} relative to I|g(586|g)=100 from a measured x=B(E0; 908L to g.s.)/B(E2; 586|g)=0.018 {I1} (1990MaYX). Other: x=0.019 {I2} (1988Wa33) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_comment:
|a(K)exp=0.015 {I1}, K/L=7.5 {I12} (1990MaYX); |a(K)exp=0.012 {I4} (1977Ge03) 
RI other: 0.31 {I3} if I(949|g)=0.86 (1977Ge03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2+E0)
decay_comment:
|a(K)exp=0.0120 {I12}, K/L=7.3 {I12} (1990MaYX); |a(K)exp=0.011 {I8} (1977Ge03) 
RI other: 1.7 {I9} if (1274|g)=6.9 (1977Ge03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|a(K)exp=0.0066 {I7} (1990MaYX), 0.0073 {I19} (1977Ge03) 
RI other: 3.3 {I3} if I(561|g)=4.1 (1977Ge03) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
I(|g+ce)(E0)=2.23 {I8} relative to I|g(747|g)=100 from a measured x=B(E0; 1623L to g.s.)/B(E2; 747|g)=1.06 {I11} (1990MaYX). Other: x=1.0 {I1} (1988Wa33) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
I(|g+ce)(E0)=0.69 {I9} relative to I|g(1300|g)=56 from a measured x=B(E0; 1623L to g.s.)/B(E2; 1300|g)=0.13 {I2} (1990MaYX). Other: x=0.21 {I3} (1988Wa33) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E unplaced in 1977Ge03 
RI other: 0.18 {I5} if I(561|g)=1.3 (1977Ge03) 
|a(K)exp=0.0099 {I22} (1990MaYX) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
|a(K)exp=0.0067 {I10}, value includes contribution from annihilation radiation, but any correction is not made (1990MaYX), K/L=5.5 {I12} (1990MaYX); |a(K)exp=0.010 {I4} (1977Ge03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E from 1982Ch01. Others: 601.2 {I1} but given for a doublet (1986Lo11), 601.5 (1994To05) 
DCO=0.90 {I2}; A{-2}=0.21 {I4}, A{-4}=-0.06 {I7} 
M RUL excludes M2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E other: 1276.1 {I1}, but given for a doublet (1986Lo11) 
DCO=0.49 {I5}; A{-2}=-0.15 {I4}, A{-4}=0.02 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E other: 702.3 (1994To05) 702.3 
DCO=0.97 {I2}; A{-2}=0.26 {I5}, A{-4}=-0.09 {I6} 
M RUL excludes M2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E other: 1098.3 {I1} but given for a doublet (1986Lo11) 
DCO=0.62 {I1}; A{-2}=-0.26 {I4}, A{-4}=0.03 {I3} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E other: 667.7 {I1} but given for a doublet (1986Lo11) 
DCO=0.85 {I10}; A{-2}=0.18 {I2}, A{-4}=-0.11 {I3} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E other: 239.5 {I1} but given for a doublet (1986Lo11) 
DCO=0.85 {I5}; A{-2}=0.33 {I6}, A{-4}=-0.03 {I6} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E other: 712.8 {I1} but given for a doublet (1986Lo11) 
DCO=1.05 {I6}; A{-2}=0.20 {I2}, A{-4}=-0.17 {I4} 
M RUL excludes M2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E other: 234.0 {I1} but given for a doublet (1986Lo11) 
DCO=0.76 {I3}; A{-2}=-0.05 {I1}, A{-4}=-0.01 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E other: 714.6 {I1} but given for a doublet (1986Lo11) 
DCO=1.08 {I5}; A{-2}=0.26 {I2}, A{-4}=-0.11 {I3} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
Intensity balance at 234.5 level requires the existence of 30.3|g (I(|g+ce)|>4) as observed in {+112}Cd({+12}C,3n|g) (evaluators) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI$weighted average of 0.18 {i7} (3.70 min), 0.18 {i7} (21.18 s) and 0.09 {i3} in {+122}Te({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI from I|g(doublet)=3.7 {i7} and I(|g)/I(983|g)=0.35 {i9} in {+122}Cs |e decay (21.18 s) 
M from |a(K)exp=0.035 {i9} for the doubly placed 371||g's 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$from I|g(doublet)=15.0 {i20} and intensity balance at 1402 level; intensity balance at 842 level gives I|g=10.7 {i17} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_uncertain: ?
decay_comment:
RI $from I|g(doublet)=3.7 {i7} and I(|g) deduced for the alternate placement (see 1214 level) 
M from |a(K)exp=0.035 {i9} for the doubly placed 371|g's 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI from I|g(doublet)=15.0 {i20} and average values of intensity balances at 1214 and 1774 levels 
M from |a(K)exp=0.0055 {i14} for the doubly placed 560|g's 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$This |g belongs to 2872-keV level in 1977Ge03, but displaced referring to adopted levels (evaluator) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=497.3 {i4}, I|g=98 {i6} (1994Ti01), 
M$DCO=1.22 {i3} (1994Ti01), DCO=0.97 {i3} (1997Se06); RUL from T{-1/2}(level) (adopted levels) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=638.4 {i4}, I|g=95 {i5} (1994Ti01) 
M$DCO=1.20 {i4} (1994Ti01), DCO=0.90 {i4} (1997Se06); RUL from T{-1/2}(level) (adopted levels) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=750.5 {i4}, I|g=79 {i3} (1994Ti01) 
M $DCO=1.05 {i1} (1994Ti01), DCO=0.94 {i6} (1997Se06), RUL from T{-1/2}(level) (adopted levels) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=822.3 {i4},I|g=42.2 {i19} (1994Ti01) 
M $DCO=1.05 {i2} (1994Ti01), DCO=0.98 {i2} (1997Se06); RUL from T{-1/2}(level) (adopted levels) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)=0.284 {i8} (331-keV, 2+ to 0, 0+) (1994Pe02) 
M $A{-2}=+0.16 {I1}, A{-4}=-0.02 {I2} (1982Ha44), A{-2}=+0.337 {I2}, A{-4}=-0.088 {I3} (1987Ha03), A{-2}=+0.309 {I15}, A{-4}=-0.118 {I22} (1994Pe02) |a(K)exp=0.025 {I5} (1982Ha44) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)=0.41 {i2} (828-keV, 4+ to 333-keV, 2+) (1994Pe02) 
RI$96.4 {I9} (with a contamination <3% from Coul. ex.) in {+108}Pd({+18}O,4n|g) (1994Pe02) 
M |a(K)exp=0.0089 {i5} (1982Ha44), 0.0075 {i8} (1987Ha03); |a(K)exp indicates E2+M1 (|d>1); A{-2}=+0.25 {I2}, A{-4}=-0.06 {I3} (1982Ha44), A{-2}=+0.320 {I9}, A{-4}=-0.085 {I14} (1987Ha03), A{-2}=+0.326 {I15}, A{-4}=-0.127 {I22} (1994Pe02), the decay scheme requires |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$I|g=15 {i2} for 841|g+843.2|g+843.0|g (1987Ha03). but, 841|g is questionable to exist 
$A{-2}=+0.08 {I2}, A{-4}=+0.05 {I3} (1982Ha44); A{-2}=+0.09 {I3}, A{-4}=+0.07 {I5} (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI from I(|g+ce)(370.9|g+371.7|g)=3.2 {I4} and I(370.9|g)/I(883|g)=0.35 {I9} in 21-s {+122}Cs |e decay 
M $A{-2}=+0.280 {I16}, A{-4}=+0.01 {I2} for 370.9|g+371.7|g (1987Ha03) |a(K)exp=0.012 {I3} for 370.9|g+371.7|g; A{-2}=+0.10 {I3}, A{-4}=-0.05 {I5} (1982Ha44), |g(|q) and |a(K)exp are consistent with M1 for 370.9|g and 371.7|g transitions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
M A{-2}=-0.33 {I10}, A{-4}=+0.20 {I17} (1982Ha44); |a(K)exp=0.022 {I4} (1982Ha44) 
RI $from I|g/I|g(883|g)=0.09 {i3} (1982Ha44) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |a(K)exp=0.0014 {i3} (1982Ha44), 0.0021 {i4} (1987Ha03); A{-2}=+0.24 {I1}, A{-4}=+0.05 {I1} (1982Ha44), A{-2}=-0.1 {I3}, A{-4}=+0.8 {I4} (1987Ha03): the disagreement of these values may be due to the nearby peak of 879.7|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI from I|g(559.5|g+560.3|g)=12.0 {i20} and I(560.3|g) deduced as noted 
M $A{-2}=+0.19 {I1}, A{-4}=-0.02 {I2}(1982Ha44), A{-2}=+0.27 {I3}, A{-4}=-0.07 {I5}(1987Ha03) for 559.5|g+560.3|g; see comment for the 560.3|g; |a(K)exp=0.0048 {I6} (1982Ha44) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)=0.51 {i7} (1467-keV, 6+ to 828-keV, 4+) (1994Pe02) 
RI$86.7 {I9} in {+108}Pd({+18}O,4n|g) (1994Pe02) 
M |a(K)exp=0.0044 {i3} (1982Ha44), 0.0040 {i5} (1987Ha03); A{-2}=+0.28 {I2}, A{-4}=-0.04 {I2} (1982Ha44), A{-2}=+0.342 {I12}, A{-4}=-0.124 {I19} (1987Ha03), A{-2}=+0.347 {I16}, A{-4}=-0.166 {I23} (1994Pe02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI see comment for 370.9|g 
M $A{-2}=+0.10 {I3}, A{-4}=-0.05 {I5} (1982Ha44), A{-2}=+0.280 {I16}, A{-4}=+0.01 {I2}, (1987Ha03); see comment for 370.9|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI from I|g(559.5|g+560.3|g)=12.0 {i20} and I(|g)/I(945|g)=2.7 {i6} in 3.7-min, {+122}Cs |e decay 
M |a(K)exp=0.046 {i5} (average of 0.0048 {i6} (1982Ha44) and 0.0044 {I7}. A{-2}=+0.19 {I1}, A{-4}=-0.02 {I2}(1982Ha44), A{-2}=+0.27 {I3}, A{-4}=-0.07 {I5}(1987Ha03) for 559.5|g+560.3|g; mult.(559.5|g)=E2, mult.(560.3|g)=E2 required by the level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M $|a(K)exp=0.0029 {i6}; A{-2}=+0.33 {I5}, A{-4}=+0.12 {I6} (1982Ha44); A{-2}=+0.33 {I4}, A{-4}=-0.09 {I5} (1987Ha03) for 654.0|g+655.7|g E2 for 654.0|g and E1 for 655.7|g were deduced from |g(|q) and |a(K)exp measurements for 654.0|g+655.7|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)=0.49 {i14} (2217-keV, 8+ to 1467-keV, 6+) (1994Pe02) 
RI 69.7 {i7} in {+108}Pd({+18}O,4n|g) (1994Pe02) 
M |a(K)exp=0.0028 {i2} (1982Ha44), 0.0032 {i5} (1987Ha03); A{-2}=+0.30 {I2}, A{-4}=-0.03 {I2} (1982Ha44), A{-2}=+0.33 {I3}, A{-4}=-0.12 {I5} (1987Ha03), A{-2}=+0.350 {I16}, A{-4}=-0.169 {I22} (1994Pe02); RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M |a(K)exp=0.0051 {i8} (1982Ha44), 0.0034 {i6} (1987Ha03); A{-2}=+0.32 {I4}, A{-4}=+0.00 {I5} (1982Ha44); A{-2}=+0.30 {I4}, A{-4}=-0.12 {I6} (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$B(E1)=6|*10{+-6} {I3} (2565-keV, 7- to 1467-keV, 6+) (1994Pe02) 
RI$6.1 {I3} in {+108}Pd({+18}O,4n|g) at 55|' (1994Pe02) 
M |a(K)exp=0.0006 {i2} (1982Ha44,19987Ha03); A{-2}=-0.26 {I6}, A{-4}=+0.09 {I8} (1982Ha44); A{-2}=-0.241 {I3}, A{-4}=+0.01 {I4} (1987Ha03); RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M see comment for 654.0|g; A{-2}=+0.33 {I5}, A{-4}=+0.12 {I6} (1982Ha44); A{-2}=+0.33 {I4}, A{-4}=-0.09 {I5} (1987Ha03) for 654.0|g+655.7|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M |a(K)exp=0.0002 {i2} (1987Ha03); A{-2}=-0.41 {I4}, A{-4}=+0.29 {I6} (1982Ha44); A{-2}=-0.3 {I3}, A{-4}=-0.04 {I5} (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Not adopted in adopted gammas because it was not observed from the same level in {+96}Zr({+30}Si,4n|g) and an M2 transition to 6+ is unlikely to compete 791.6-keV [E1] |g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)=0.35 {i4} (3033-keV, 9- to 2565-keV, 7-) (1994Pe02) 
M $A{-2}=+0.42 {I9}, A{-4}=-0.16 {I1}3 (1987Ha03); RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$B(E1)=4.1|*10{+-6} {i4} (9- to 2217-keV, 8+) (1994Pe02) 
RI 19.8 {i5} in {+108}Pd({+18}O,4n|g) (1994Pe02) 
M |a(K)exp=0.0021 {i8} (1987Ha03); A{-2}=-0.14 {I5}, A{-4}=-0.09 {I9}(1982Ha44), A{-2}=-0.31 {I4}, A{-4}=+0.03 {I6} (1987Ha03), A{-2}=-0.209 {I21}, A{-4}=+0.01 {I5} (1994Pe02), 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)=0.43 {i19} (3040-keV, 10+ to 2217-keV, 8+) (1994Pe02) 
RI$34.6 {i4} (with a contribution of <10%) in {+108}Pd({+18}O,4n|g) (1994Pe02) 
M |a(K)exp=0.0023 {i7} (1987Ha03); A{-2}=+0.34 {I2}, A{-4}=-0.06 {I2}(1982Ha44), A{-2}=+0.316 {I16}, A{-4}=-0.13 {I2} (1987Ha03), A{-2}=+0.333 {I17}, A{-4}=-0.148 {I25} (1994Pe02); RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI I|g=5.1 {i2} (1024|g+1025.2|g) (1987Ha03) 
M |a(K)exp=0.0008 {i4} (1987Ha03), A{-2}=-0.23 {I3}, A{-4}=+0.01 {I6} IN {+122}Te({+3}He,3n|g) (1987Ha03), mult.(1024|g)=Q 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$B(E1)=3.2|*10{+-6} {i5} (3682-keV, 11- to 3039-keV, 10+) (1994Pe02) 
M $A{-2}=+0.17 {I2}, A{-4}=-0.06 {I3} (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)=0.41 {i6} (3682-keV, (11)- to 3033-keV, (9)-) (1994Pe02) 
RI 22.8 {i4} in {+108}Pd({+18}O,4n|g) (1994Pe02) 
M $A{-2}=+0.41 {I3}, A{-4}=-0.17 {I5} (1987Ha03); A{-2}=+0.298 {I22}, A{-4}=-0.165 {I32} (1994Pe02); RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$contaminated by impurities in {+110}Pd({16}O,4n|g) (1987Ha03); 18.6 {I3} (with a contamination) in {+108}Pd({+18}O,4n|g) (1994Pe02), 
M A{-2}=+0.291 {I22}, A{-4}=-0.109 {I31} (1994Pe02), A{-2}=0.00 {I7}, A{-4}=+0.05 {I11} (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E|g from 2003Mo27; E|g=745 in 1987Ha03 
M $A{-2}=+0.38 {I3}, A{-4}=-0.24 {I5} for 743.8|g+745|g (1987Ha03) 


decay_energy_unit: KEV
decay_multipolarity: [E1]
decay_comment:
$B(E1)=4.5|*10{+-6} {i14} (4439-keV, (13)- to 3820-keV, 12+) (1994Pe02) 
RI$no data given (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$B(E2)=0.41 {i12} (4439-keV, (13)- to 3682-keV, (11)-) (1994Pe02) 
RI$27.2 {i3} (doublet) in {+108}Pd({+18}O,4n|g) (1994Pe02) 
M $A{-2}=+0.348 {I19}, A{-4}=-0.204 {I27} (1994Pe02); RUL 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
E|g=1006.2 {I2}, I|g=1.5 {I3} (1987Ha03) 
M from DCO ratio (2003Mo27); 1987Ha03 proposed Mult.=E1 on the bases of |a(K)exp=0.0003 {i2}, A{-2}=+0.07 {I6}, A{-4}=+0.19 {I9}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E|g=177.2, I|g=3.4 relative to 331.2|g=100 (2003Mo27) 
M A{-2}=-0.19 {I10}, A{-4}=+0.11 {I15} (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
the order of 771|g and 838|g was interchanged according to the |g sequence of the band 6 in {+96}Zr({+30}Si,4n|g) 
RI $16.0 {i16} (769.1|g+770.8|g) (1987Ha03); 16.3 {I4} (769.1|g+770.8|g) in {+108}Pd({+18}O,4n|g) (1994Pe02). 
M $A{-2}=+0.381 {I33}, A{-4}=-0.166 {I53} (1994Pe02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E|g=231.5, I|g=2.8 relative to 331.2|g=100 (2003Mo27) 
M A{-2}=-0.571 {I10}, A{-4}=+0.057 {I10} (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI$I|g=15 {i2} for 841|g+843.2|g+843.0|g (1987Ha03), but, 841|g is questionable to exist 
M $A{-2}=+0.08 {I2}, A{-4}=+0.05 {I3} (1982Ha44); A{-2}=+0.30 {I3}, A{-4}=-0.08 {I5} for 841|g+843.0|g (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
M A{-2}=-0.708 {I13}, A{-4}=+0.09 {I2} (1987Ha03) 
E|g=294.6, I|g=1.7 relative to 331.2|g=100 (2003Mo27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E the order of 771|g and 838|g was interchanged according to the |g sequence of the band 6 in {+96}Zr({+30}Si,4n|g) 
RI 20 {i2} in {+108}Pd({+18}O,4n|g) (1994Pe02) 
M $A{-2}=+0.353 {I11}, A{-4}=-0.142 {I17} (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g=758.2, I|g=0.4 relative to 331.2|g=100 (2003Mo27) 
M $A{-2}=+0.35 {I4}, A{-4}=-0.18 {I6} (1987Ha03) for 757.2|g+758.4|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E from 2003Mo27; E|g=879.7, I|g=4.1 (1987Ha03) 
RI from 1987Ha03 
M A{-2}=+0.50 {I5}, A{-4}=-0.08 {I8} (1987Ha03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI 10.2 {i3} in {+108}Pd({+18}O,4n|g) (1994Pe02) 
M $A{-2}=+0.31 {I16}, A{-4}=-0.1 {I2} (1987Ha03), A{-2}=+0.396 {I34}, A{-4}=-0.193 {I47} (1994Pe02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E from 2003Mo27; E|g=980.8, I|g=3.1 (1987Ha03) 
RI from 1987Ha03 
A{-2}=+0.1 {I2}, A{-4}=0.0 {I3} (1987Ha03) 


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$other: 97.3 {I1} from ({+3}He,3n|g) 
M$from ce data in {+123}Cs |e decay. Others: D+Q with |d=+0.11 {I4} from |g(|q) in ({+12}C,3n|g) and D(+Q) from |g(|q) and |g|g(|q) in ({+3}He,3n|g), with |DJ=1. 


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$other: 83.2 {I1} with I|g=100 {I10} from ({+3}He,3n|g). 
M$from ce data in {+123}Cs |e decay; supported by |g(|q) in ({+3}He,3n|g) and ({+12}C,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$weighted average of 180.64 {I14} from {+123}Cs |e decay and 180.6 {I1} from ({+3}He,3n|g). 
RI$weighted average of 14.7 {I15} from {+123}Cs |e decay and 16 {I3} from ({+3}He,3n|g) 
M$Q from |g(|q) in ({+12}C,3n|g); M1,E2 from ce data in {+123}Cs |e decay 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
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_uncertain: ?
decay_comment:
E$from level-energy difference; not observed. This transition is inferred by 1981Lu01 from the fact that decay curves of the 180.5|g and 83.3|g from 185 level and the 97.3|g from 97.3 level were observed to follow the isomeric 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$1981Lu01 in ({+3}He,3n|g) states the intensity balance require the same character for the 21|g as the 57|g, which is pure M1 proposed by 1981Lu01 based on |g(|q) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$other: 71.3 {I3} from ({+3}He,3n|g) 
M,MR$D+Q, |DJ=1 from |g(|q) in ({+3}He,3n|g); M1+E2 required by level scheme 


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$D+Q from |g(|q) in ({+3}He,3n|g) and ({+12}C,3n|g); M2 ruled out by RUL 
MR$weighted average of 0.06 {I+2-3} from |g(|q) in ({+3}He,3n|g) (1981Lu01) and +0.09 {I4} from |g(|q) in ({+12}C,3n|g) (1982Ze05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2,M1
decay_comment:
E$others: 209.5 {I10} from ({+48}Ca,5n|g), 209.9 from ({+3}He,3n|g) 
RI$weighted average of 4.5 {I5} from {+123}Cs |e decay and 5.0 {I10} from ({+3}He,3n|g) 
M$from ce data in {+123}Cs |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E,RI$others: 307.2 {I2} with I|g=100 {I10} in ({+3}He,3n|g); 306.9 {I10} from ({+48}Ca,5n|g) 
M$from ce data and |g(|q) (|DJ=2) in ({+3}He,3n|g) and ce data in {+123}Cs |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$from ({+3}He,3n|g). Other: 131.2 {I10} from ({+48}Ca,5n|g) 
M,MR$from ({+3}He,3n|g). Mult and |d from |g(|q) giving |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 340.1 {I2} from {+123}Cs |e decay and 340.2 {I2} from ({+3}He,3n|g). Other: 340.2 {I10} from ({+48}Ca,5n|g) 
M$from ce data and |g(|q) (|DJ=2) in ({+3}He,3n|g) and |g(|q) in ({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$weighted average of 261.8 {I1} from {+123}Cs |e decay and 261.9 {I2} from ({+3}He,3n|g) 
RI$from ({+3}He,3n|g). Other: 100 {I16} from {+123}Cs |e decay 
M$from ce data in {+123}Cs |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$also from {+123}Cs |e decay 
RI$unweighted average of 9.7 {I18} from {+123}Cs |e decay and 21 {I5} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 442.8 from ({+3}He,3n|g) 
RI$weighted average of 26 {I4} from {+123}Cs |e decay and 32 {I4} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from ce data and |g(|q) (|DJ=1) in ({+3}He,3n|g) and |g(|q) (|DJ=1) in ({+12}C,3n|g) 
MR$from |g(|q) in ({+3}He,3n|g). Other: <0 from ({+12}C,3n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$from ({+3}He,3n|g). Other: 255.1 {I10} from ({+48}Ca,5n|g) 
M,MR$from ({+3}He,3n|g). Mult and |d from |g|g(|q) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from ({+3}He,3n|g). Other: 266.2 {I10} from ({+48}Ca,5n|g) 
M$from ce data, |g(|q) (|DJ=1) and |g|g(|q) in ({+3}He,3n|g) and |g(|q) (|DJ=1) in ({+12}C,3n|g) 
MR$from |g(|q) and |g|g(|q) in ({+3}He,3n|g). Others: <-0.18 from |g(|q) in ({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from {+123}Cs |e decay. Other: 333.8 from ({+3}He,3n|g) 
RI$weighted average of 63 {I13} from {+123}Cs |e decay and 77 {I10} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from {+123}Cs |e decay. Other: 405.1 from ({+3}He,3n|g) 
RI$from ({+3}He,3n|g). Other: 100 {I19} from {+123}Cs |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from {+123}Cs |e decay. Other: 448.4 from ({+3}He,3n|g) 
RI$weighted average of 94 {I19} from {+123}Cs |e decay and 74 {I11} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from ({+3}He,3n|g). Other: 399.0 {I10} from ({+48}Ca,5n|g) 
M,MR$from |g(|q), |g|g(|q) and ce data in ({+3}He,3n|g), with |DJ=1 and |d from |g(|q). Other: |d<-0.4, |DJ=1 from |g(|q) in ({+12}C,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$from ({+3}He,3n|g). Other: 455.6 {I10} from ({+48}Ca,5n|g) 
M$from |g(|q) in ({+12}C,3n|g) and ({+3}He,3n|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$from ({+3}He,3n|g). Other: 249.0 {I10} from ({+48}Ca,5n|g) 
M,MR$from |g(|q) and |g|g(|q) in ({+3}He,3n|g), with |d from |g|g(|q). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$from ({+3}He,3n|g). Other: 613.7 {I10} from ({+48}Ca,5n|g) 
M,MR$from |g(|q) and |g|g(|q) in ({+3}He,3n|g), with |d and |DJ=1 from |g(|q). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$from ({+3}He,3n|g). Other: 314.2 {I10} from ({+48}Ca,5n|g) 
MR$from |g(|q) and |g|g(|q) in ({+3}He,3n|g), with |DJ=1 and |d from |g(|q) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 607.7 {I10} from ({+48}Ca,5n|g) 
M,MR$from |g(|q) and |g|g(|q) in ({+3}He,3n|g), with |DJ=1 from |g(|q) and |d from |g|g(|q). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
E$other: 631.6 {I10} from ({+48}Ca,5n|g) 
M,MR$from |g(|q) and ce data in ({+3}He,3n|g); Q from |g(|q) in ({+48}Ca,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 616.6 {I2} from ({+48}Ca,5n|g) and 617.0 {I2} from ({+3}He,3n|g) 
M$Q from |g(|q) in ({+12}C,3n|g) and ({+3}He,3n|g); M2 ruled out by RUL. Other: |d(O/Q)=-0.05 {I6} from |g|g(|q) in ({+3}He,3n|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$other: 1038.3 {I10} from ({+48}Ca,5n|g) 
M,MR$from |g|g(|q) in ({+3}He,3n|g). Other: D from |g(|q) in ({+48}Ca,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 753.8 {I2} from ({+48}Ca,5n|g) and 753.3 {I2} from ({+3}He,3n|g) 
M$from ce data and |g(|q) in ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$from ({+48}Ca,5n|g). Other: 739.7 from ({+3}He,3n|g) 
RI$from ({+3}He,3n|g). Other: 100 {I13} from ({+48}Ca,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+48}Ca,5n|g). Other: 1161.5 from ({+3}He,3n|g) 
RI$weighted average of 57 {I8} from ({+48}Ca,5n|g) and 48 {I5} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$from ({+48}Ca,5n|g). Other: 868.3 from ({+3}He,3n|g) 
RI$from ({+3}He,3n|g). Other: 100 {I11} from ({+48}Ca,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+48}Ca,5n|g). Other: 205.1 from ({+3}He,3n|g) 
RI$unweighted average of 41 {I6} from ({+48}Ca,5n|g) and 20.0 {I20} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$from ({+48}Ca,5n|g). Other: 286.8 from ({+3}He,3n|g) 
RI$unweighted average of 28 {I4} from ({+48}Ca,5n|g) and 13.0 {I10} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+48}Ca,5n|g). Other: 347.1 from ({+3}He,3n|g) 
RI$unweighted average of 7.3 {I12} from ({+48}Ca,5n|g) and 3.0 {I10} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$from ({+48}Ca,5n|g). Other: 480.2 from ({+3}He,3n|g) 
RI$unweighted average of 26 {I4} from ({+48}Ca,5n|g) and 16.0 {I20} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+48}Ca,5n|g). Other: 671.6 from ({+3}He,3n|g) 
RI$weighted average of 61 {I7} from ({+48}Ca,5n|g) and 76 {I8} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$from ({+48}Ca,5n|g). Other: 1079.9 from ({+3}He,3n|g) 
RI$from ({+3}He,3n|g). Other: 100 {I12} from ({+48}Ca,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$from ({+48}Ca,5n|g). Other: 713.0 from ({+3}He,3n|g) 
RI$from ({+3}He,3n|g). Other: 100 {I13} from ({+48}Ca,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+48}Ca,5n|g). Other: 1121.1 from ({+3}He,3n|g) 
RI$weighted average of 43 {I5} from ({+48}Ca,5n|g) and 50 {I7} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$from ({+48}Ca,5n|g). Other: 139.0 from ({+3}He,3n|g) 
RI$weighted average of 20.0 {I26} from ({+48}Ca,5n|g) and 15.0 {I20} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$from ({+48}Ca,5n|g). Other: 180.5 from ({+3}He,3n|g) 
RI$from ({+3}He,3n|g). Other: 100 {I11} from ({+48}Ca,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+48}Ca,5n|g). Other: 385.5 from ({+3}He,3n|g) 
RI$weighted average of 16.8 {I21} from ({+48}Ca,5n|g) and 14.0 {I10} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+48}Ca,5n|g). Other: 467.0 from ({+3}He,3n|g) 
RI$weighted average of 7.4 {I11} from ({+48}Ca,5n|g) and 10.0 {I10} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 97.3 {I1} from 1981Ma01 and 97.39 {I3} from 1981So06. Other: 100 {I1} (1975We23) 
M$supported by ce(K)/ce(L+M+N)=6.8 {I7} (1987Fr10), |a(K)exp=0.9 {I1} (1981So06), |a(K)exp=0.74 {I15}, |a(L)exp=0.13 {I4}, |a(M)exp=0.029 {I10} (1981Ma01), |a(K)exp=0.80 {I2} (1966Da09). |d(E2/M1)<0.2 calculated using BrIccMixing based on all ce data above. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 83.3 {I1} from 1981Ma01 and 83.38 {I2} from 1981So06 
RI$weighted average of 18.0 {I20} from 1981Ma01 and 21 {I1} from 1981So06 
M$supported by ce(K)/ce(L+M+N)=7.2 {I8} (1987Fr10), |a(K)exp=1.30 {I6} (1981So06), |a(K)exp=1.3 {I3}, |a(L)exp=0.22 {I6}, |a(M)=0.033 {I8} (1981Ma01). |d(E2/M1)<0.17 calculated using BrIccMixing based on all ce data above. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 180.5 {I1} from 1981Ma01 and 180.77 {I3} from 1981So06. Other: 177 {I1} (1975We23) 
RI$weighted average of 2.8 {I5} from 1981Ma01 and 3.1 {I3} from 1981So06. 
M$|a(K)exp=0.17 {I4} (1981Ma01) and ce(K)(97.4|g)/ce(K)(180.6|g)=30 {I10} (1987Fr10) give M1,E2 (1981Ma01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 71.5 {I3} from 1981Ma01 and 71.26 {I3} from 1981So06 
RI$unweighted average of 2.2 {I4} from 1981Ma01 and 1.2 {I1} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$this quoted intensity from Table IV of 1981So06 is inconsistent I(252|g)/I(71|g)=0.23/0.41 in Fig.11. Also, this |g is seen neither by 1981Ma01 and in other studies. So the placement of this |g is considered as questionable by the evaluator and is not included in Adopted Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2,M1
decay_comment:
E$weighted average of 209.5 {I2} from 1981Ma01 and 209.7 {I2} from 1981So06 
RI$weighted average of 0.9 {I1} from 1981Ma01 and 0.7 {I2} from 1981So06 
M$from |a(K)exp=0.14 {I6} (1981Ma01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 307.0 {I1} from 1981Ma01 and 307.1 {I1} from 1981So06. Other: 306 {I1} (1975We23) 
RI$weighted average of 17.0 {I20} from 1981Ma01 and 21 {I1} from 1981So06 
M$|a(K)exp=0.037 {I6}, |a(L)exp=0.005 {I2} (1981Ma01) give M1,E2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$seen and placed only by 1981Ma01, with J(437)=(1/2,3/2). But the adopted J|p(437)=7/2(+) would require Mult=M3 for this transition to 1/2(+) ground state, which is very unlikely since it would require an isomeric T{-1/2}>2 ms for the 437 level in order for B(M3)(W.u.) not to exceed RUL=10. So this placement is considered as questionable by the evaluator and this |g is not included in Adopted Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$weighted average of 261.7 {I1} from 1981Ma01 and 261.9 {I1} from 1981So06 
RI$unweighted average of 9.5 {I10} from 1981Ma01 and 13 {I1} from 1981So06 
M$from |a(K)exp=0.050 {I8}, |a(L)exp=0.006 {I2} (1981Ma01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$1981So06 place a |g of E=405.0 {I5} from the 848 level, with I|g=1.1 {I2}. See comments for that |g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$could be the same as 345.3|g, placed from 442 level in 1981Ma01 and other studies. This placement by 1981So06 is considered as questionable by the evaluator and is not included in Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2,M1
decay_comment:
E$weighted average of 499.3 {I1} from 1981Ma01 and 498.9 {I2} from 1981So06 
RI$weighted average of 6.2 {I8} from 1981Ma01 and 6 {I2} from 1981So06 
M$from |a(K)exp=0.007 {I3} (1981Ma01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$weighted average of 596.7 {I1} from 1981Ma01 and 596.4 {I2} from 1981So06. Other: 598 {I1} (1975We23) 
RI$weighted average of 45 {I6} from 1981Ma01 and 57 {I3} from 1981So06 
M$from |a(K)exp=0.006 {I2} (1981Ma01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$from 1981So06. Other: 304.0 {I2} (1981Ma01) 
RI$weighted average of 3.0 {I5} from 1981Ma01 and 5 {I1} from 1981So06 
M$from |a(K)exp=0.033 {I10} (1981Ma01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 430.6 {I2} from 1981Ma01 and 430.0 {I5} from 1981So06 
RI$weighted average of 1.1 {I2} from 1981Ma01 and 0.8 {I2} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$Masked by the strong 511-keV line. I|g estimated from ce spectrum by assuming mult=M1,E2 (1981Ma01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 611.2 {I2} from 1981Ma01 and 610.9 {I2} from 1981So06. Other: 612 {I1} (1975We23) 
RI$weighted average of 14.0 {I20} from 1981Ma01 and 16.7 {I19} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 693.8 {I2} from 1981Ma01 and 693.6 {I4} from 1981So06 
RI$weighted average of 5.7 {I8} from 1981Ma01 and 8 {I2} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$other: 434.3 {I2} (1981So06) 
RI$other: 4.7 {I7} (1981So06) 
M$from |a(K)exp=0.014 {I5} (1981Ma01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 644.2 {I2} from 1981Ma01 and 644.1 {I1} from 1981So06. Other: 645 {I1} (1975We23) 
RI$unweighted average of 10.0 {I15} from 1981Ma01 and 15 {I2} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1981So06. Other: 741.5 {I2} (1981Ma01), 743 {I1} (1975We23) 
RI$weighted average of 13.0 {I20} from 1981Ma01 and 17 {I2} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E$weighted average of 237.4 {I3} from 1981Ma01 and 238.0 {I5} from 1981So06 
RI$unweighted average of 0.45 {I5} from 1981Ma01 and 2.2 {I6} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Placed by 1981So06, listed as seen in coincidence with 261.8|g in Table V. But a peak at this energy is barely seen in the coincidence spectrum of 261.8|g in Fig.8 of 1981So06. 1981Ma01 place a |g of E=405.0 {I2} from the 586 level with I|g=1.6, and this |g is listed as seen in coincidence with 83.4|g and 97.4|g, but not with 261.8|g. 2001Ga25 in {+123}Te({+3}He,3n|g) also place a 405.1|g from the 586 level but not from the 848 level. So the placement by 1981So06 is considered as questionable (by the evaluator) and this |g could be the same |g seen from 586 level in 1981Ma01 and 2001Ga25. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 541.5 {I2} from 1981Ma01 and 540.5 {I5} from 1981So06 
RI$unweighted average of 1.8 {I3} from 1981Ma01 and 4 {I1} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 667.9 {I2} from 1981Ma01 and 667.6 {I4} from 1981So06 
RI$unweighted average of 4.5 {I7} from 1981Ma01 and 7 {I1} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 750.9 {I3} from 1981Ma01 and 750.7 {I2} from 1981So06 
RI$weighted average of 3.5 {I5} from 1981Ma01 and 4.8 {I7} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 848.9 {I5} from 1981Ma01 and 849.0 {I5} from 1981So06 
RI$weighted average of 0.8 {I2} from 1981Ma01 and 0.7 {I4} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 725.1 {I3} from 1981Ma01 and 725.0 {I5} from 1981So06 
RI$weighted average of 0.9 {I2} from 1981Ma01 and 1.3 {I3} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 711.4 {I2} from 1981Ma01 and 711.0 {I2} from 1981So06 
RI$unweighted average of 2.0 {I3} from 1981Ma01 and 4 {I1} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 841.9 {I4} from 1981Ma01 and 841.8 {I2} from 1981So06 
RI$weighted average of 1.5 {I3} from 1981Ma01 and 1.8 {I5} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1356.2 {I5} from 1981Ma01 and 1355.6 {I5} from 1981So06 
RI$weighted average of 3.0 {I8} from 1981Ma01 and 5 {I2} from 1981So06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$weighted average of 97.3 {I1} (1970Ke01) and 97.4 {I2} (1981Lu01). Other: 97.5 (2001Ga25) 
$Relative I|g=100 (1981Lu01 and 1997Sa09), 100 {I8} (1970Ke01). 
MR$all possible solutions: 0.00 {I15}, +0.23 {I12}, or -2.2 {I+6-10} from 340.3|g-97.5|g(|q) (2001Ga25). Isotropic from |g(|q) in 1997Sa09 
$A{-2}=-0.02 (1981Lu01); A{-2}=0.00 {I2} (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 83.2 {I1} (1970Ke01) and 83.4 {I2} (1981Lu01). Other: 83.4 (2001Ga25) 
RI$other: 100 {I10} (1981Lu01) 
M$Isotropic from |g(|q) in 1997Sa09 
$Relative I|g=67 {I7} (1981Lu01), 81 {I7} (1970Ke01), 77.3 (1997Sa09) 
$A{-2}=-0.02 {I2} (1981Lu01); A{-2}=-0.02 {I3} (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 180.5 {I1} (1970Ke01) and 180.8 {I2} (1981Lu01). Other: 180.8 (2001Ga25) 
RI$weighted average of 11 {I3} from 2001Ga25 and 17.2 {I18} from 1981Lu01 
$Relative I|g=11.5 {I12} (1981Lu01), 15 {I2} (1970Ke01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_uncertain: S
decay_comment:
E$from level-energy difference; not observed. This transition is inferred by 1981Lu01 from the fact that decay curves of the 180.8|g and 83.4|g from 180.6 level and the 97.3|g from 97.3 level were observed to follow the isomeric decay. 
M$If E1, hindrance factor=7.2|*10{+4} is consistent with observed values in cerium and barium. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$other: 21.1 (2001Ga25) 
M$1981Lu01 states the intensity balance require the same character for the 21|g as the 57|g, which is proposed to be pure M1 from |g(|q) in 1981Lu01 
$Relative I|g=9.0 {I9} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 66.8 (2001Ga25) 
RI$from 1981Lu01. Other: <20 (2001Ga25) 
$Relative I|g=1.0 {I3} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 71.4 (2001Ga25) 
RI$from 2001Ga25 and 1981Lu01 
$A{-2}=-0.17 {I4}, A{-4}=-0.04 {I6} (1981Lu01) 
$Relative I|g=9.0 {I9} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 57.0 (2001Ga25) 
RI$from relative I|g in 1981Lu01 
MR$other: -0.15 {I10} from |g(|q) in 1997Sa09 
$A{-2}=-0.12 {I3}, A{-4}=-0.02 {I4} (1981Lu01); A{-2}=-0.36 {I4} (1997Sa09) 
$Relative I|g=18.0 {I18} (1981Lu01), 23.9 (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 307.2 (2001Ga25) 
M$|a(K)exp=0.026 {I4} (1981Lu01) 
$A{-2}=+0.13 {I1}, A{-4}=-0.01 {I1} (1981Lu01); A{-2}=+0.31 {I15} (1997Sa09) 
$Relative I|g=9.6 {I10} (1981Lu01), 3.6 (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 130.6 (2001Ga25) 
RI$other: 15 {I5} (1981Lu01) 
MR$weighted average of 0.05 {I4} (1981Lu01) and 0.07 {I5} from 130.5|g-307.2|g(|q) (2001Ga25). Other: 0.02 {I+6-13} or -5 {I+2-11} from 497.1|g-130.5|g(|q) in 2001Ga25 
$A{-2}=-0.10 {I1}, A{-4}=+0.02 {I1} (1981Lu01) 
$Relative I|g=1.8 {I6} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 340.3 (2001Ga25) 
RI$from 2001Ga25 and 1981Lu01 
M$|a(K)exp=0.018 {I3} (1981Lu01) 
$A{-2}=+0.21 {I1}, A{-4}=-0.02 {I1} (1981Lu01); A{-2}=+0.32 {I3} (1997Sa09) 
$Relative I|g=11.8 {I12} (1981Lu01), 41.0 (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 345.3 (2001Ga25) 
RI$weighted average of 20 {I3} from 2001Ga25 and 45 {I14} from 1981Lu01 
$Relative I|g=0.50 {I15} (1981Lu01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$from 2001Ga25. Not reported in 1981Lu01, but an unlabelled apparent peak can be seen at this energy in the |g-ray spectrum in Fig.1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$other: 215.1 (2001Ga25) 
RI$other: 18 {I6} (1981Lu01) 
$A{-2}=+0.27 {I9}, A{-4}=-0.06 {I3} (1981Lu01) 
$Relative I|g=1.3 {I4} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$other: 286.5 (2001Ga25) 
RI$from 2001Ga25 and 1981Lu01 
M$|a(K)exp=0.026 {I4} (1981Lu01) 
MR$others: -0.31 {I7}, -1.80 {I+24-30} from 584.0|g-286.5|g(|q), -1.62 {I11}, -0.36 {I3}, -0.22 {I2}, -2.13 {I+11-3} from 264.4|g-286.5|g(|q), in 2001Ga25, none of them adopted by the authors. 
$A{-2}=-0.33 {I1}, A{-4}=+0.04 {I2} (1981Lu01) 
$Relative I|g=7.3 {I7} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$other: 255.2 (2001Ga25) 
RI$weighted average of 26 {I3} from 2001Ga25 and 22 {I6} from 1981Lu01 
MR$other: <-8 also from 2001Ga25 
$Relative I|g=1.4 {I4} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$other: 266.5 (2001Ga25) 
RI$100 {I11} from 1981Lu01 
M$|a(K)exp=0.046 {I5} (1981Lu01) 
MR$from 563.7|g-266.4|g(|q) in 2001Ga25; -0.9 {I3} from |g(|q) in 1981Lu01. Others: -0.61 {I8}, -0.47 {I3}, -1.14 {I7}, -1.33 {I6} from 249.3|g-266.4|g(|q) in 2001Ga25 
$A{-2}=-0.59 {I1}, A{-4}=+0.07 {I1} (1981Lu01). 
$Relative I|g=6.5 {I7} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$other: 398.9 (2001Ga25) 
RI$from 2001Ga25 and 1981Lu01 
M$|a(K)exp=0.013 {I7} (1981Lu01) 
MR$others: -0.62 {I9}, -1.3 {I2} from 631.7|g-398.7|g(|q) in 2001Ga25; -0.8 {I+4-9} from |g(|q) in 1997Sa09 
$A{-2}=-0.69 {I1}, A{-4}=+0.04 {I1} (1981Lu01); A{-2}=-0.82 {I5} (1997Sa09). 
$Relative I|g=18.0 {I18} (1981Lu01), 21.2 (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$other: 455.8 (2001Ga25) 
M$A{-2}=+0.30 {I1}, A{-4}=-0.06 {I1} (1981Lu01); A{-2}=+0.29 {I5}, A{-4}=-0.14 {I6} for the doublet (1997Sa09) 
$Relative I|g=47 {I5} (1981Lu01), 86.6 for the doublet (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 264.4 (2001Ga25) 
MR$others: -0.34 {I4}, -3.2 {I3} from 264.3|g-286.5|g(|q) (2001Ga25) 
RI$other: 140 {I40} (1981Lu01) 
$A{-2}=-0.44 {I5}, A{-4}=-0.09 {I9} (1981Lu01) 
$Relative I|g=1.4 {I4} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 249.3 (2001Ga25) 
RI$weighted average of 16.0 {I20} from 2001Ga25 and 12 {I4} from 1981Lu01 
MR$others: -0.64 {I3}, -1.35 {I15}, -1.6 {I1} also from 249.2|g-266.5|g(|q), -1.9 {I5}, -0.46 {I+11-21} from 630.2|g-249.2|g(|q), -0.46 {I+15-30}, -2.5 {I+11-14} from 249.2|g-333.3|g(|q) in 2001Ga25, and -0.4 {I+3-31} from |g(|q) in 1981Lu01 
$A{-2}=-0.54 {I2}, A{-4}=-0.07 {I20} (1981Lu01) 
$Relative I|g=1.2 {I4} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$other: 517.2 (2001Ga25) 
M$A{-2}=+0.29 {I4}, A{-4}=-0.03 {I5} (1981Lu01) 
$Relative I|g=10.3 {I10} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q(+O)
decay_comment:
E$other: 490.4 (2001Ga25) 
MR$other: 1.80 {I+30-24} also from 2001Ga25 
$Relative I|g=1.0 {I3} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 613.8 (2001Ga25) 
RI$100 {I11} (1981Lu01) 
MR$others: >+16, +0.08 {I3} from 644.5|g-613.8|g(|q) (2001Ga25). 
$A{-2}=+0.06 {I1}, A{-4}=+0.13 {I1} (1981Lu01) 
$Relative I|g=8.5 {I9} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$other: 670.7 (2001Ga25) 
RI$other: 106 {I11} (1981Lu01) 
M$from |g(|q) in 1997Sa09 
$A{-2}=+0.30 {I4} (1997Sa09) 
$Relative I|g=9.0 {I9} (1981Lu01), 43.1 (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 532.7 (2001Ga25) 
MR$-5.04 {I+57-73}, or -0.26 {I2} from 532.7|g-266.5|g(|q) (2001Ga25). 
$Relative I|g=2.0 {I6} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 314.6 (2001Ga25) 
MR$others: -0.46 {I+11-16}, -2.1 {I7} from 314.5|g-515.7|g(|q) (2001Ga25). 
$A{-2}=-0.89 {I8}, A{-4}=+0.10 {I5} (1981Lu01) 
$Relative I|g=0.70 {I21} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
E$other: 392.7 (2001Ga25) 
RI$weighted average of 23 {I3} from 2001Ga25 and 28 {I8} from 1981Lu01 
$A{-2}<0 (1981Lu01) 
$Relative I|g=1.4 {I4} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 550.6 (2001Ga25) 
RI$weighted average of 26 {I3} from 2001Ga25 and 50 {I16} from 1981Lu01 
MR$other: 0.98 {I+29-17} also from 2001Ga25 
$Relative I|g=2.5 {I8} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 607.6 (2001Ga25) 
RI$from 2001Ga25 and 1981Lu01 
MR$others: -2.9 {I+9-18} from |g(|q) in 1981Lu01, -2.62 from |g(|q) in 1997Sa09 
$A{-2}=-0.48 {I7}, A{-4}=+0.17 {I11} (1981Lu01); A{-2}=-0.68 {I12} (1997Sa09) 
$Relative I|g=5.0 {I5} (1981Lu01), 15.0 (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 574.8 (2001Ga25). 547.8 in Table 3 of 2001Ga25 is a misprint 
RI$weighted average of 79 {I8} from 2001Ga25 and 68 {I7} from 1981Lu01 
MR$unweighted average of -0.58 {I4} (2001Ga25) and -0.23 {I6} (1981Lu01). Other: -1.94 {I+27-16} in 2001Ga25 
$A{-2}=-0.52 {I1}, A{-4}=+0.06 {I2} (1981Lu01) 
$Relative I|g=5.0 {I5} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
E$other: 631.7 (2001Ga25) 
RI$other: 100 {I11} from 1981Lu01 
M$|a(K)exp=0.0042 {I9} for 630.2|g+631.9|g (1981Lu01) 
MR$other: -3.05 {I+81-55} also from 2001Ga25 
$A{-2}=+0.31 {I1}, A{-4}=-0.07 {I1} (1981Lu01) 
$Relative I|g=7.4 {I8} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q(+O)
decay_comment:
E$other: 616.9 (2001Ga25) 
M$other: mult=Q from |g(|q) in 1981Lu01 
MR$other: 2.8 {I3} also from 2001Ga25 
$A{-2}=+0.27 {I4}, A{-4}=-0.07 {I1} (1981Lu01); A{-2}=+0.33 {I3} (1997Sa09) 
$Relative I|g=18.0 {I18} (1981Lu01), 56.7 (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 630.0 (2001Ga25) 
M$|a(K)exp=0.0042 {I9} for 630.2|g +631.9|g (1981Lu01) 
$A{-2}=+0.33 {I1}, A{-4}=-0.02 {I1} (1981Lu01); A{-2}=+0.26 {I5} for 630|g+632|g (1997Sa09) 
$Relative I|g=5.5 {I6} (1981Lu01), 23.0 for 630|g+632|g (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$other: 802.6 (2001Ga25) 
RI$unweighted average of 63 {I7} from 2001Ga25 and 34 {I11} from 1981Lu01 
MR$other: -0.02 {I3} also from 2001Ga25 
$Relative I|g=1.6 {I5} (1981Lu01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 878.9 (2001Ga25) 
MR$others: -1.67 {I6} or -0.58 {I11} from |g|g(|q) in 2001Ga25 
$A{-2}=-0.58 {I5}, A{-4}=+0.11 {I8} (1981Lu01) 
$Relative I|g=1.4 {I4} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$other: 619.2 (2001Ga25) 
$A{-2}=+0.22 {I4}, A{-4}=-0.10 {I5} (1981Lu01) 
$Relative I|g=3.5 {I11} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$other: 769.0 (2001Ga25) 
$A{-2}=+0.26 {I3}, A{-4}=-0.01 {I4} (1981Lu01) 
$Relative I|g=2.5 {I8} (1981Lu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 753.4 (2001Ga25) 
M$|a(K)exp=0.0024 {I5} (1981Lu01) 
$A{-2}=+0.24 {I6}, A{-4}=-0.12 {I8} (1981Lu01); A{-2}=+0.12 {I4} (1997Sa09) 
$Relative I|g=3.0 {I9} (1981Lu01), 45.5 (1997Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$other: 714.7 (2001Ga25) 
M$A{-2}=+0.25 {I2}, A{-4}=-0.09 {I3}, half of the intensity from 715.2|g in {+122}Xe (1981Lu01) 
$Relative I|g=2.0 {I6} (1981Lu01) 


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 |g|g(|q) in {+124}Cs |e decay (1979Si11). Others: |d=+100 {I+|@-90} or -0.42 {I8} (1982Ha44); 6.3 {I+5.3-2.0} (1975Ku05); +8 {i+8-2}(2001We13). 
|a(K)exp=0.0068 {I4} 


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 2001We13. Others: |d=+5 {I+5-1} or -0.7 {I2}, from |g(|q) and |a(K)exp 
|a(K)exp=0.0077 {I5}; 


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 2001We13; other: -0.14 {I8} (from |g(|q) and |a(K)exp), -1.8(1997ScZU). 
|a(K)exp=0.105 {I20} 


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 2001We13. Others: -2.1(1997ScZU), -1.1 {I+7-11} (from |g(|q) and |a(K)exp). 
|a(K)exp=0.030 {I5} 


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(K)exp in 1984Ga21, but |a(K)exp in 1982Ha44 indicated M1+E2. 
|a(K)exp=0.00074 {I30} (1984Ga21). Other: 0.0019 {I4}. (1982Ha44) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
1984Ga21 assigned 606.2|g to the transition from 6739 level to 6133 level, but evaluators assume the two |g's are the same 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$ other: 0.31(1997ScZU). 1997ScZU and 1999Sc20 were from the same experiment, but the values are different. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI Not observed in 1988We07. The intensity ratio to 894 keV |g is inconsistent with that of (HI,xn|g). There is a possibility that too large intensity is given. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR from 2001We13. others:+100 {I+|@-90} or -0.42 {I8} (1982Ha44); +6.3 {I+5.3-2.0} (1975Ku05); -0.38 {I+25-55} (1998Sa25). 
|a(K)exp=0.0068 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
MR$+0.21 {I3} or +3.85 {I+57-45}(2001We13). |d listed as +0.21 {I19} in table 4 of 2001We13 is a misprint. See also {+123}Te({+3}He,2n|g):XUNDL-2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others:+16 {I+16-8} or +7.8 {I+79-26} (2001We13), 0.14 {I+43-3} (1998Sa25). 
|a(K)exp=0.016 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR from 2001We13. other: |d=+0.35 {I5}(from |g(|q) and |a(K)exp); |d=-0.08 {I+8-24}(1998Sa25). 
|a(K)exp=0.017 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E from 2001We13 and assumed an uncertainty of 0.3 keV 
M,MR from 2001We13; |d=+0.08 {I+3-6} or 11 {I+21-3} 
|a(K)exp=0.0014 {I3} for |g942.8+|g942.9. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from 2001We13. Others: -2.1(1997ScZU), -1.1 {I+7-11} (from |g(|q) and |a(K)exp), -0.32 {I+20-54} (1998Sa25). 
|a(K)exp=0.030 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M from |a(K)exp in 1984Ga21, but |a(K)exp in 1982Ha44 indicated M1+E2. 
|a(K)exp=0.00074 {I30} (1984Ga21). other: 0.0019 {I4}. (1982Ha44) 


decay_energy_unit: KEV
decay_comment:
E average from 1987Ha03 and 1984Ga21 assuming uncertainties of 1 keV and 0.3 keV, respectively 
1984Ga21 assigned 606.2|g to the transition from 6739 level to 6133 level, but evaluators assume the two |g's are the same 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$ 2010Ra05 quote an uncertainty of 79 units 
$B(E2)(W.u.)=57.7 {I15} (2010Ra05 used as normalization) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$Recommended in 2001We13 with |d=+7.84 +7.90-2.65 being the second solution. |d=+0.32 {I5} in Adopted gammas for {+124}Xe in ENSDF 


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_comment:
RI$From 2001We13, as used in 2010Ra05. Other: 20.8 {I22} in Adopted levels for {+124}Xe in ENSDF 
$B(E2)(W.u.)=62 {I36} (2010Ra05) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$new |g ray according to decay scheme Fig. 3 in 2107Ra20, but compilers note that this gamma from 1248 level had earlier been observed in several reaction studies, but not in the decay of {+124}Cs g.s. activity where the 1248 level is also populated. It is listed as 368.09 {I16} in {+124}Xe Adopted dataset in the ENSDF database (April 2008 update) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR From {+125}Cs decay. Others: |d<0.32 from |a(K)exp=0.47 {I7} (1968WiZY), |d<0.52 from |a(K)exp=0.51 {I7} (1968Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
RI From the decay scheme. An unweighted average of values from 1968WiZY and 1968Sc14 gives I|g(141|g)/I|g(111|g)=0.318 {I9} 
M From |a(K)exp=1.96 {I25}, |a(exp)=4.4 {I4} (1968Sc14), |a(L+...)exp=1.83 {I22} (1968WiZY) 
CC E3 CC(THEORY)'S MULT. BY 0.975 10 (Cf. 1990Ne01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.065 {I7}, A{-4}=+0.069 {I9}, pol.=+0.46 {I8}, R(DCO)=1.4 {I3} (1991Gr02) 
Doublet in 1991Gr02 with |g ray from 3487-keV level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=-0.63 {I1}, A{-4}=-0.01 {I1}, Pol.=+0.05 {I6} (1991Gr02) 
Doublet in 1991Gr02 with |g ray from 1310-keV level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=-0.17 {I2}, A{-4}=-0.08 {I2}, pol.=+0.13 {I8} (1991Gr02) 
Doublet in 1991Gr02 with |g ray from 2006-keV level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M 1991Gr02 assign this transition as (E1) but this assignment is inconsistent with band assignment. 
A{-2}=+0.14 {I3}, A{-4}=+0.04 {I4}, pol.=+0.8 {I2} R(DCO)=0.9 {I1} (1991Gr02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=-0.01 {I4}, A{-4}=+0.09 {I5}, pol.=+0.12 {I7} (1991Gr02) 
Doublet in 1991Gr02 with |g ray from 837-keV level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR From adopted levels, gammas 
A{-2}=+0.090 {I7}, A{-4}=-0.002 {I7} (1983Ir02); |a(exp)=0.75 {I15} estimated from intensity balance (1978Gi16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
M From adopted gammas 
A{-2}=+0.004 {I11}, A{-4}=+0.007 {I12} (1983Ir02) 
CC E3 CC(THEORY)'S MULT. BY 0.975 10 (Cf. 1990Ne01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E From 1979He15 
RI From I|g(43|g)/I|g(184|g)=0.12 {I4} (1979He15) measured at 125|'. Uncertainties are assumed to be 30 % for 43|g and 10 % for 184|g. 
M From intensity-balance and T{-1/2} of 296-keV level (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI From 1979He15 
M From intensity-balance and T{-1/2} of 296-keV level (1979He15). |g(|q) data disagree with (E2) assignment. 
A{-2}=+0.052 {I7}, A{-4}=+0.020 {I7} (1983Ir02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E From 1978Gi16 
MR -0.25 |< |d |< -0.07 from |g(|q) and estimated |a(exp) (1978Gi16) 
A{-2}=-0.32 {I2}, A{-4}=-0.03 {I3} (1979He15); A{-2}=-0.36 {I10}, |a(exp)=4.4 {I3} estimated from intensity balance (1978Gi16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
A{-2}=+0.16 {I1}, A{-4}=-0.12 {I5}, pol.=+0.26 {I5} (1995Wi06) A{-2}=+0.181 {I5}, A{-4}=-0.012 {I5}, pol.=+0.28 {I3} (1983Ir02). A{-2}=+0.14 {I2}, A{-4}=+0.03 {I3} (1979He15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.05 {I1}, A{-4}=-0.01 {I2}, pol.=+0.01 {I2} (1995Wi06). A{-2}=+0.02 {I5}, A{-4}=-0.04 {I5} (1983Ir02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR From 1983Ir02. Phase convention was changed by evaluators from Rose-Brink phase convention to Krane-Steffen one. 
A{-2}=-0.274 {I15}, A{-4}=+0.033 {I18}, pol.=+0.10 {I4} (1983Ir02). A{-2}=-0.04 {I3}, A{-4}=+0.07 {I5} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M D+Q and relevant levels 
A{-2}=-0.13 {I10}, A{-4}=+0.27 {I12} (1983Ir02). A{-2}=-0.02 {I2}, A{-4}=+0.06 {I3} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
A{-2}=+0.187 {I5}, A{-4}=-0.032 {I5}, pol.=+0.20 {I3} (1983Ir02). A{-2}=+0.14 {I2}, A{-4}=-0.00 {I2} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR From 1983Ir02. Phase convention was changed by evaluators from Rose-Brink phase convention to Krane-Steffen one. 
A{-2}=-0.211 {I8}, A{-4}=+0.018 {I9}, pol.=-0.14 {I6} (1983Ir02). A{-2}=-0.10 {I3}, A{-4}=+0.08 {I5} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
A{-2}=-0.18 {I1}, A{-4}=+0.02 {I1}, pol.=-0.08 {I2} (1995Wi06). A{-2}=-0.033 {I22}, A{-4}=+0.023 {I25}, pol.=-0.2 {I5} (1983Ir02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=-0.32 {I1}, A{-4}=+0.14 {I1}, pol.=+0.14 {I2} (1995Wi06). A{-2}=-0.23 {I2}, A{-4}=+0.10 {I3} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=-0.86 {I6}, A{-4}=+0.08 {I1}, pol.=+0.01 {I1} (1995Wi06). A{-2}=-0.68 {I2}, A{-4}=+0.06 {I3} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=+0.29 {I2}, A{-4}=+0.01 {I3}, pol.=+0.23 {I5} (1995Wi06). A{-2}=+0.13 {I4}, A{-4}=+0.03 {I7} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E From 1979He15 
RI From I|g(60|g)/I|g(486|g)=0.008 {I2} measured at 125|' (1979He15). Uncertainties are assumed to be 30 % for 60|g and 10 % for 486|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
A{-2}=+0.171 {I12}, A{-4}=-0.009 {I13}, pol.=+0.062 {I3} (1983Ir02). A{-2}=+0.22 {I2}, A{-4}=-0.00 {I3} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M D+Q with large |d 
A{-2}=+0.04 {I1}, A{-4}=+0.22 {I1} (1995Wi06). A{-2}=+0.05 {I2}, A{-4}=+0.20 {I3} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
A{-2}=+0.31 {I1}, A{-4}=-0.08 {I1}, pol.=+0.50 {I1} (1995Wi06). A{-2}=+0.29 {I4}, A{-4}=-0.03 {I6} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=-0.53 {I2}, A{-4}=+0.04 {I2}, pol.=-0.08 {I4} (1995Wi06). A{-2}=-0.54 {I13}, A{-4}=+0.02 {I19} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
A{-2}=+0.25 {I1}, A{-4}=-0.04 {I2}, pol.=+0.34 {I6} (1995Wi06). A{-2}=+0.32 {I2}, A{-4}=-0.04 {I3} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=-0.46 {I3}, A{-4}=+0.12 {I5}, pol.=+0.18 {I6} (1995Wi06). A{-2}=-0.61 {I3}, A{-4}=+0.13 {I5} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR -1.4 {I1} or -0.6 {I+1-2} 
A{-2}=-0.83 {I2}, A{-4}=+0.15 {I2}, pol.=-0.13 {I5}, DCO-intensities (1995Wi06). A{-2}=-0.76 {I2}, A{-4}=+0.09 {I3} (1979He15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=?
decay_comment:
M D+Q with large |d 
MR Uncertainty exceeds |D|d columns. Authors give {I+24-260}. 
A{-2}=-0.25 {I6}, A{-4}=+0.13 {I10}, DCO-intensities (1995Wi06). 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
|g energy is not reported in authors' Table 2, but the transition is indicated in the figure of the level scheme. Energy is calculated from the difference of the level energy by evaluator 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
M D+Q with large |d 
MR -2.3 {I+1-2} or -9 {I+6-7} 
A{-2}=-0.75 {I2}, A{-4}=+0.30 {I3}, pol.=+0.08 {I11} (1995Wi06) 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
|g energy is not reported but the transition is indicated in the figure of the level scheme in 1995Wi06. Energy is calculated from the difference of the level energy by evaluator 


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 {+126}Cs |e decay 
RI weighted av from all datasets with |g's except({+13}C,3n|g); other: I|g(929)/I|g(438)=1.65 {I13} in ({+13}C,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:
E from {+126}Cs |e decay 
RI from {+126}Xe(|g,|g'); other: I|g(1970)/I|g(2359)=0.73 {I22} in {+126}Cs |e decay 


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 and |g(|q) in {+126}Te({+3}He,3n|g) 
MR from (|a,n|g). Other: -7.1 {I11} in ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
RI from ({+13}C,3n|g); others: I|g(382)/I|g(688)=0.27 {I7} in (|a,n|g), 0.66 {I4} in {+82}Se({+48}Ca,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR from |g|g(|q) in {+126}I |b{+-} decay (1971Ta04). |a(K)exp=0.0112 {I9}, |a(L)exp=0.0017 {I1}, |a(M)exp=0.00046 {I5} (1992Ma08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
A{-2}=-0.96 {I2}, A{-4}=+0.182 {I2}; pol.=-0.3 {I1} (1993Se01) 
1993Se01 gives A{-4}=+0.182 {I2} but it is likely 0.18 {I2}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=-0.008 {I2}, A{-4}=-0.003 {I2}; pol.=+0.252 {I6} (1993Se01) 
MR from 2000Ga08. Other: 14 +|@-8 or -0.35 {I+7-13} or |<-16 (1993Se01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR +13 +|@-13 (1993Se01). +5.4 {I+10-8} or +0.11 {I3} (2000Ga08) 
A{-2}=-0.228 {I9}, A{-4}=+0.02 {I1}; pol.=+0.2 {I7} (1993Se01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=+0.093 {I3}, A{-4}=+0.054 {I4}; pol.=+0.33 {I1} (1993Se01) 
MR from 2000Ga08. Other: +21 {I+18-13} (1993Se01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=+0.331 {I3}, A{-4}=+0.045 {I5}; pol.=+0.31 {I2} (1993Se01) 
MR from 2000Ga08. Other: +2.3 {I+13-18} (1993Se01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=-0.018 {I4}, A{-4}=-0.064 {I6}; pol.=+0.22 {I2} (1993Se01) 
MR from 2000Ga08. Other: +3.5 {I+9-6} (1993Se01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=+0.06 {I2}, A{-4}=+0.08 {I2}; pol.=+0.3 {I2} (1993Se01) 
MR +0.16 {I8} or +21 {I+52-13} (2000Ga08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
A{-2}=-0.05 {I6}, A{-44}=-0.06 {I8}; pol.=+0.8 {I2} (1993Se01) 
MR +0.7 {I+70-9} or +0.14 {I18} or +1.7 {I+10-5} (2000Ga08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=+0.23 {I2}, A{-4}=-0.06 {I3}; pol.=+0.5 {I1} (1993Se01) 
MR from 2000Ga08. Other: +0.92 {I+34-50} or -0.27 {I+36-4} (1993Se01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=+0.2 {I3}, A{-4}=-0.09 {I5}; pol.=+0.6 {I2} (1993Se01) 
MR -0.04 {I20} or +0.00 {I8} (2000Ga08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=+0.22 {I4}, A{-4}=-0.01 {I6}; pol.=-0.02 {I9} (1993Se01) 
MR +0.09 {I8} for J=3 or -0.39 {I6} for J=4 (2000Ga08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=+0.13 {I5}, A{-4}=-0.24 {I8} (1993Se01) 
MR +0.6 {I+6-4} or +0.3 {I2} or +1.2 {I+9-5} (2000Ga08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI 100 {I3} in (|a,4n|g) (1983Ku04) 
A{-2}=+0.12 {I1}, A{-4}=-0.02 {I1} (1982Ha44), A{-2}=+0.255 {I6}, A{-4}=-0.009 {I10} (1983Ku04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_comment:
RI 8.0 {I19} in (|a,4n|g) (1983Ku04) 
|a(K)exp=0.007 {I1} 
A{-2}=-0.03 {I1}, A{-4}=+0.00 {I1} (1982Ha44) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 87 {I3} in (|a,4n|g) (1983Ku04) 
|a(K)exp=0.0055 {I2} 
A{-2}=+0.20 {I2}, A{-4}=-0.03 {I2} (1982Ha44), A{-2}=+0.278 {I7}, A{-4}=-0.042 {I11} (1983Ku04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 67.6 {I25} in (|a,4n|g) (1983Ku04) 
|a(K)exp=0.0029 {I3} 
A{-2}=+0.24 {I2}, A{-4}=-0.01 {I2} (1982Ha44), A{-2}=+0.293 {I8}, A{-4}=-0.062 {I13} (1983Ku04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 41.6 {I18} in (|a,4n|g) (1983Ku04) 
|a(K)exp=0.0025 {I3} 
A{-2}=+0.28 {I2}, A{-4}=-0.4 {I3} (1982Ha44), A{-2}=+0.313 {I12}, A{-4}=-0.085 {I19} (1983Ku04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
|a(K)exp=0.0024 {I4}. 
A{-2}=+0.16 {I3}, A{-4}=+0.01 {I4} (1982Ha44) 
M 1982Ha44 suggests (E2) from |g(|q) and |a(exp), which is in conflict with E1 from |g(|q) and pol. in {+123}Te(|a,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
RI 16.8 {I12} in (|a,4n|g) (1983Ku04) 
|a(K)exp=0.0007 {I2}. 
A{-2}=-0.13 {I1}, A{-4}=+0.02 {I2} (1982Ha44), A{-2}=-0.173 {I24}, A{-4}=+0.03 {I5} (1983Ku04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
|a(K)exp=0.0005 {I2} 
A{-2}=-0.13 {I3}, A{-4}=-0.08 {I4} (1982Ha44) 
I|g, |a(K)exp, A{-2}, A{-4}: contain about 30% impurity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI 17.0 {I12} in (|a,4n|g) (1983Ku04) 
A{-2}=+0.302 {I25}, A{-4}=-0.04 {I4} (1983Ku04) 
E from 1983Ku04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=+0.070 {I13}, A{-4}=+0.018 {I20} 
MR +10.2 {I+60-25} or +0.35 {I+6-3} 
K/L=4.8 {I20} (1965Sa11) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.13 {I3}, A{-4}=-0.02 {I5} 
M 1975Ku05 suggests Q from |g(|q) which is in conflict with E1 from |g(|q) and pol. In {+123}Te(|a,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$others: 19 {I4} (|a,n|g), 42 {I17} (|a,2n|g), 46 {I14} ({+3}He,4n|g), 35 (|a,3n|g) 
M,MR from {+127}Cs |b{++} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR -0.32 {I5} (|a,3n|g), -0.38 {I4} ({+3}He,4n), 0.45 {I+11-8} (|a,n|g). These values are probably for a composite peak of 483.4|g and 483.3|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR weighted av of 0.21 {I11}(|a,2n|g), -0.26 {I4}(|a,3n|g) and -0.16 {I9} ({+3}He,4n|g). Other: -3.5 {I+9-17} (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
CC E3 CC(THEORY)'S MULT. BY 0.975 10 (Cf. 1990Ne01) 
$L/M+N+O=3.3 (1967Ge15), K/L+M=1.3 {I1} (1969Ha03) 
CC E3 CC(THEORY)'S MULT. BY 0.975 10 (Cf. 1990Ne01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
CC E3 CC(THEORY)'S MULT. BY 0.975 10 (Cf. 1990Ne01) 
CC E3 CC(THEORY)'S MULT. BY 0.975 10 (Cf. 1990Ne01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
K:L:M=9.1 {I13}:1.4 {I2}:0.55 {I8}. Others: |a(K)exp 0.0124 {I50}, K/L=6.3 (1967Sp08) 
MR from (462.3|g)(124.5|g)(|q) (1990Ga02) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E Introduced on the basis of the observation that the 1156.5|g has a delayed component with intensity ratio of I(1156.5|g)/I(486.6|g)|?3. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
$DCO gate on 124.8|g 
$|D{-asym}=-0.062 {I35} 
M$2018Ch24 give E1 multipolarity, which compiler assumes is a typo due to the |DJ=3, |D|p=yes character of the transition based on known J|p assignments. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$DCO gate on 596.0|g 
$|D{-asym}=+0.029 {I44} 
M$2018Ch24 give E2/M1, but M1 is inconsistent with |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$I|g=12.61 {I8} per 100 decays of the parent (1994Mi35). Others: 14.0 {I14} (1961La16), 16.1 {I16} (1956Be18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$doublet. The branching ratio was determined by the authors of 2009Co24 using ENSDF database (2001Ka61) however the data do not match. B(E2)(W.u.) uncertain. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LE;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LE
decay_comment:
E$doublet. The branching ratio was determined by the authors of 2009Co24 using ENSDF database (2001Ka61). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=+0.25 {I7} from |g(|q). A{-2}=0.16 {I2} or 0.11 {I3} from |g(|q,H,t) for 442.9|g+590.2|g (1984Lo07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$A{-2}=+0.26 {I6} from |g(|q). A{-2}=0.16 {I2} or 0.11 {I3} from |g(|q,H,t) for 442.9|g+590.2|g (1984Lo07) 


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:
$A{-2}=0.111 {I5}, A{-4}=-0.014 {I7} (1996Ne04) 
$A{-2}=0.14 {I1}, A{-4}=-0.02 {I1} in ({+3}He,3n|g) (1981Go04) 
$A{-2}=0.21 {I2}, A{-4}=-0.04 {I3} in (|a,n|g) (1981Go04) 
M$Q from |g(|q), E2 from RUL 


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:
CC$|a(K)exp=0.0059 {I12} (1981Go04); |a(K)(E2)=0.00660, |a(K)(M1)=0.00855 
MR$others: 8 {I+6-3} (1996Ne04); +5.7 {I+24-17} or |d=-0.25 {I+5-7} (1981Go04) 
$A{-2}=0.006 {I3}, A{-4}=0.002 {I4} (1996Ne04) 
$A{-2}=0.03 {I3}, A{-4}=0.03 {I3} in (|a,n|g) (1981Go04) 


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:
$A{-2}=0.092 {I6}, A{-4}=-0.015 {I8} (1996Ne04) 
$A{-2}=0.13 {I12}, A{-4}=-0.08 {I15} in (|a,n|g) (1981Go04) 
M$Q from |g(|q), E2 from RUL 


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:
$|a(K)exp=0.0046 {I5} (1981Go04); |a(K)(E2)=0.00488, |a(K)(M1)=0.00647 
$A{-2}=0.211 {I3}, A{-4}=-0.038 {I3} (1996Ne04) 
$A{-2}=0.21 {I2}, A{-4}=-0.03 {I2} in ({+3}He,3n|g) (1981Go04) 
$A{-2}=0.28 {I2}, A{-4}=-0.04 {I3} in (|a,n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp=0.023 {I8} (1981Go04); |a(K)(E2)=0.0147, |a(K)(M1)=0.0173 
MR$others: +1.0 {I+17-5} (1996Ne04), |>+0.11 (1981Go04) 
$A{-2}=-0.305 {I21}, A{-4}=-0.07 {I3} (1996Ne04) 
$A{-2}=-0.31 {I5}, A{-4}=0.11 {I6} in ({+3}He,3n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$others: +7.9 {I+11-17} (1996Ne04); +6.3 {I+32-18} or +0.45 {I+8-5} (1981Go04) 
$A{-2}=0.113 {I5}, A{-4}=0.038 {I7} (1996Ne04) 
$A{-2}=0.21 {I5}, A{-4}=0.08 {I6} in (|a,n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others: +1.3 {I3} (1996Ne04); +1.3 {I+9-5} (1981Go04) 
$|a(K)exp=0.0020 {I5} (1981Go04); |a(K)(E2)=0.001440, |a(K)(M1)=0.001935 
$A{-2}=0.304 {I6}, A{-4}=0.013 {I8} (1996Ne04) 
$A{-2}=0.46 {I6}, A{-4}=0.08 {I7} in (|a,n|g) (1981Go04) 


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:
$|a(K)exp=0.0058 {I17} (1981Go04); |a(K)(E2)=0.00534, |a(K)(M1)=0.00704 
MR$others: +1.7 {I3} (1996Ne04); -0.25 {I9} or +1.5 {I+4-3} (1981Go04) 
$A{-2}=0.101 {I9}, A{-4}=-0.052 {I13} (1996Ne04) 
$A{-2}=0.12 {I1}, A{-4}=-0.03 {I2} in ({+3}He,3n|g) (1981Go04) 


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:
$|a(K)exp=0.0037 {I9} (1981Go04); |a(K)(E2)=0.00336, |a(K)(M1)=0.00454 
$A{-2}=0.255 {I10}, A{-4}=0.003 {I13} (1996Ne04) 
$A{-2}=0.17 {I4}, A{-4}=-0.02 {I5} in ({+3}He,3n|g) (1981Go04) 
$A{-2}=0.27 {I3}, A{-4}=-0.02 {I4} in (|a,n|g) (1981Go04) 


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:
$|a(K)exp=0.0027 {I3} (1981Go04); |a(K)(E2)=0.00312, |a(K)(M1)=0.00423 
$A{-2}=0.263 {I4}, A{-4}=-0.063 {I6} (1996Ne04) 
$A{-2}=0.21 {I3}, A{-4}=-0.02 {I4} in ({+3}He,3n|g) (1981Go04) 
$A{-2}=0.31 {I2}, A{-4}=-0.04 {I3} in (|a,n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.0053 {I13} (1981Go04); |a(K)(E2)=0.00542, |a(K)(M1)=0.00713 
$A{-2}=0.234 {I8}, A{-4}=-0.041 {I11} (1996Ne04) 
$A{-2}=0.16 {I2}, A{-4}=-0.01 {I2} in ({+3}He,3n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
$|a(K)exp<0.0027 (1981Go04); |a(K)(E1)=0.00154, |a(K)(M2)=0.0163 
MR$other: 0.0 {I1} (1996Ne04) 
$A{-2}=-0.15 {I3}, A{-4}=-0.06 {I4} (1996Ne04) 
$A{-2}=0.14 {I7}, A{-4}=-0.02 {I9} in ({+3}He,3n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$|a(K)exp=0.00047 {I15} (1981Go04); |a(K)(E1)=0.000427, |a(K)(M2)=0.00291 
$A{-2}=-0.180 {I7}, A{-4}=-0.011 {I10} (1996Ne04) 
$A{-2}=-0.33 {I4}, A{-4}=0.04 {I4} in (|a,n|g) (1981Go04) 


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:
$|a(K)exp=0.0054 {I16} (1981Go04); |a(K)(E2)=0.00606, |a(K)(M1)=0.00791 
MR$other: 0.0 {I+8-15} (1996Ne04) 
$A{-2}=0.137 {I14}, A{-4}=0.002 {I19} (1996Ne04) 
$A{-2}=0.28 {I3}, A{-4}=-0.03 {I4} in ({+3}He,3n|g) (1981Go04) 
$A{-2}=0.34 {I13}, A{-4}=0.06 {I15} in (|a,n|g) (1981Go04) 


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:
$|a(K)exp=0.045 {I9} (1981Go04); |a(K)(E2)=0.0473, |a(K)(M1)=0.0459 
MR$other: -0.5 {I+1-15} (1996Ne04) 
$A{-2}=-0.618 {I21}, A{-4}=0.04 {I3} (1996Ne04) 
$A{-2}=-0.45 {I1}, A{-4}=0.01 {I1} in ({+3}He,3n|g) (1981Go04) 


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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
$|a(K)exp<0.003 (1981Go04); |a(K)(E1)=0.00251, |a(K)(M2)=0.0304 
MR$other: +0.1 {I+1-2} (1996Ne04) 
$A{-2}=-0.10 {I3}, A{-4}=-0.01 {I4} (1996Ne04); 
$A{-2}=-0.10 {I7}, A{-4}=-0.02 {I9} in ({+3}He,3n|g) (1981Go04) 


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:
$|a(K)exp=0.0019 {I3} (1981Go04); |a(K)(E2)=0.00248, |a(K)(M1)=0.00337 
$A{-2}=0.308 {I18}, A{-4}=-0.126 {I25} (1996Ne04) 
$A{-2}=0.28 {I3}, A{-4}=-0.03 {I4} in ({+3}He,3n|g) (1981Go04) 
$A{-2}=0.35 {I2}, A{-4}=-0.07 {I3} in (|a,n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.025 {I8} (1981Go04); |a(K)(E2)=0.0207, |a(K)(M1)=0.0231 
$A{-2}=0.45 {I9}, A{-4}=0.06 {I12} (1996Ne04); A{-2}=0.20 {I5}, A{-4}=-0.03 {I6} in ({+3}He,3n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
$|a(K)exp<0.0009 (1981Go04); |a(K)(E1)=0.000821, |a(K)(M2)=0.00711 
$A{-2}=-0.21 {I4}, A{-4}=0.15 {I6} (1996Ne04) 


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:
$|a(K)exp=0.011 {I4} (1981Go04); |a(K)(E2)=0.00799, |a(K)(M1)=0.0102 
$A{-2}=-0.78 {I3}, A{-4}=0.05 {I4} (1996Ne04) 
$A{-2}=-0.43 {I3}, A{-4}=-0.02 {I4} in ({+3}He,3n|g) (1981Go04) 
$A{-2}=-0.87 {I9}, A{-4}=0.17 {I10} in (|a,n|g) (1981Go04) 
MR$from |g(|q) (1981Go04) 
RI$other: 12.0 {I15} (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_comment:
$|a(K)exp=0.030 {I10} (1981Go04); |a(K)(E2)=0.0401, |a(K)(M1)=0.0400 
$A{-2}=-0.04 {I14}, A{-4}=0.02 {I19} (1996Ne04) 
$A{-2}=-0.02 {I7}, A{-4}=0.12 {I7} in (|a,n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.014 {I5} (1981Go04); |a(K)(E2)=0.0117, |a(K)(M1)=0.0142 
$A{-2}=0.37 {I7}, A{-4}=0.02 {I10} (1996Ne04) 
$A{-2}=0.18 {I1}, A{-4}=0.02 {I1} in ({+3}He,3n|g) (1981Go04) 
$A{-2}=0.35 {I10}, A{-4}=-0.18 {I14} in (|a,n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.008 {I3} (1981Go04); |a(K)(E2)=0.00588, |a(K)(M1)=0.00769 
$A{-2}=-0.10 {I6}, A{-4}=-0.01 {I8} (1996Ne04) 
$A{-2}=0.05 {I2}, A{-4}=-0.04 {I2} in ({+3}He,3n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$from 1981Go04, 0.07 {I3} (1996Ne04) 
$|a(K)exp=0.022 {I8} (1981Go04); |a(K)(E2)=0.0261, |a(K)(M1)=0.0281 
$A{-2}=-0.91 {I5}, A{-4}=0.12 {I6} in ({+3}He,3n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$from 1981Go04 
$|a(K)exp=0.008 {I3} (1981Go04); |a(K)(E2)=0.00642, |a(K)(M1)=0.00834 
$A{-2}=0.26 {I6}, A{-4}=-0.06 {I7} in ({+3}He,3n|g) (1981Go04) 


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:
$|a(K)exp=0.0048 {I12} (1981Go04); |a(K)(E2)=0.00406, |a(K)(M1)=0.00545 
$A{-2}=0.29 {I3}, A{-4}=-0.07 {I3} in ({+3}He,3n|g) (1981Go04) 
$A{-2}=0.20 {I15}, A{-4}=-0.13 {I19} in (|a,n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp=0.075 {I25} (1981Go04); |a(K)(E2)=0.0471, |a(K)(M1)=0.0457 
$A{-2}=-0.69 {I5}, A{-4}=0.02 {I7} in ({+3}He,3n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.0019 {I5} (1981Go04); |a(K)(E2)=0.00200, |a(K)(M1)=0.00271 
$A{-2}=0.11 {I8}, A{-4}=-0.15 {I11} (1996Ne04) 
$A{-2}=0.27 {I2}, A{-4}=-0.02 {I3} in ({+3}He,3n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.0043 {I15} (1981Go04); |a(K)(E2)=0.00443, |a(K)(M1)=0.00952 
$A{-2}=0.26 {I4}, A{-4}=-0.03 {I5} in ({+3}He,3n|g) (1981Go04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 1985Ba73. 
RI$from |a(t) and I(|g+ce)=100 (1985Ba73). 
M$from |a(K)exp=10.2 {I5}, K/L|?8.2 (1977Ra23). Others: |a(K)exp=10.60 {I44} (1985Ba73), 10.2 {I4} (1970SaZI), 10.6 (1968ReZY), 21.0 {I10} (1965Wa13), 22 {I4} (1954De17); K/L|?10 (1954De17). 
MR$from {+129}Cs |e decay (1965Ge04,1974Ma24). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 1985Ba73. 
MR$from L subshell ratios (1965Ge04), sign from |g|g(|q) and K/L (371.9|g) (1974Ma24). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=+0.18 {I16}, A{-4}=-0.03 {I2} (1983Lo08) 
$A{-2}=+0.13 {I2}, A{-4}=-0.01 {I2} (1981He04). 
$A{-2}=+0.20 {I2}, A{-4}=0.00 {I2}, POL=+0.36 {I3} (1979Ir01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=-0.12 {I13}, A{-4}=0.00 {I2} (1983Lo08) 
$A{-2}=-0.10 {I4}, A{-4}=+0.02 {I6} (1981He04). 
$A{-2}=-0.12 {I2}, A{-4}=0.00 {I2}, POL=+0.26 {I3} (1979Ir01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=-0.39 {I1}, A{-4}=+0.02 {I2} (1983Lo08) 
$A{-2}=-0.34 {I3}, A{-4}=-0.01 {I4} (1981He04). 
$A{-2}=-0.40 {I1}, A{-4}=+0.02 {I1}, POL=+0.09 {I1} (1979Ir01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.19 {I1}, A{-4}=-0.02 {I1} (1983Lo08) 
$A{-2}=+0.17 {I4}, A{-4}=-0.01 {I5} (1981He04). 
$A{-2}=+0.18 {I1}, A{-4}=0.00 {I1}, POL=+0.26 {I5}, |d(M3/E2)=+0.03 {I+5-4} (1979Ir01) 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
$A{-2}=-0.41 {I5}, A{-4}=-0.28 {I8} (1983Lo08). For J|p(411 level)=1/2+, isotropic |g(|q) is expected 
$A{-2}=-0.01 {I4}, A{-4}=+0.01 {I4}, POL=-0.05 {I2} (1979Ir01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.21 {I3}, A{-4}=-0.02 {I4} (1981He04). 
$A{-2}=+0.27 {I1}, A{-4}=-0.08 {I1}, POL=+0.42 {I2}, |d(M3/E2)=+0.01 {I+2-4} (1979Ir01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=+0.53 {I2}, A{-4}=-0.01 {I3} (1983Lo08) 
$A{-2}=+0.25 {I2}, A{-4}=+0.09 {I3} (1981He04). 
$A{-2}=+0.46 {I2}, A{-4}=+0.03 {I2}, POL=-0.22 {I9} (1979Ir01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.26 {I3}, A{-4}=-0.08 {I4} (1983Lo08) 
$A{-2}=+0.17 {I5}, A{-4}=0.06 {I6} (1981He04). 
$A{-2}=+0.21 {I2}, A{-4}=-0.04 {I2}, POL=+0.43 {I6}, |d(M3/E2)=0.11 {I+3-9} (1979Ir01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=-0.38 {I3}, A{-4}=-0.03 {I5} (1981He04). 
$A{-2}=-0.52 {I2}, A{-4}=+0.05 {I3}, POL=-0.23 {I8} (1979Ir01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.18 {I3}, A{-4}=-0.03 {I5} (1981He04). 
$A{-2}=+0.26 {I1}, A{-4}=-0.06 {I1}, POL=+0.47 {I3}, |d(M3/E2)=+0.09 {I2} (1979Ir01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=-0.05 {I2}, A{-4}=-0.07 {I2} (1983Lo08) 
$A{-2}=-0.11 {I2}, A{-4}=-0.01 {I2}, POL=+0.42 {I9} (1979Ir01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.27 {I3}, A{-4}=-0.06 {I4} (1981He04). 
$A{-2}=+0.27 {I1}, A{-4}=-0.07 {I1}, POL=0.42 {I6} (1979Ir01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from 12.36-h {+130}I decay 
B(E2)(W.u.)=0.013 {I3}, B(M1)(W.u.)=3.4|*10{+-4} {I2} if |d=0.28; B(E2)(W.u.)=0.16 {I5}, B(M1)(W.u.)=4.5|*10{+-5} {I9} if |d=2.7 
MR +0.28 {I3} or +2.7 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+4.41 {I+42-51} or -0.160 {I+18-15} 
$B(E2)(W.u.)=40 {I+10-7} for |d=+4.41 {I+42-51}, 1.06 {I+49-35} for |d=-0.160 {I+18-15} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+3.0 {I+15-10} or +0.51 {I+17-13} 
$B(E2)(W.u.)=57 {I+59-42} for |d=+3.0 {I+15-10}, 13 {I+25-11} for |d=+0.51 {I+17-13} 


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:
MR$determined from 1096.6|g. This |g is contaminated by a known |g ray from background but which does not exhibit Doppler shift 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+2.4 {I+13-7} or -0.37 {I+18-20} 
$B(E2)(W.u.)=42 {I+48-35} for |d=+2.4 {I+13-7}, 6 {I+18-6} for |d=-0.37 {I+18-20} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from spectra at angles |>90|' due to contamination from a line in {+65}Cu from (n,n'|g) 
MR$+2.95 {I+30-31} or -0.068 {I+37-42} 
$B(E2)(W.u.)=6.7 {I+22-19} for |d=+2.95 {I+30-31}, 0.034 {I+81-9} for |d=-0.068 {I+37-42} 


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 summed spectra at all the angles |>90|' in the 2.5-MeV |g(|q) data since this |g was not observed in the single-angle spectra 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$E2 matrix element (5366,2+ to 0,0+)=+0.79 eb {I4}, B(E2)(W.u.)=32 {I3} (2020Mo35). Other: B(E2)(W.u.)=30 {I+2-7} (2020Mu35), when B(E2)(W.u.)=16.0 {I4} and Q{-s}=-0.13 {I8} values (from {+94}Mo Adopted dataset in the ENSDF database, Jan 2006 update) for the Coulomb excited first 2+ state in {+94}Mo were used as constraints in the GOSIA analysis. 
$Number of counts: 5710 {I286} for |q(c.m.)=62-131|'; 754 {I29} for |q(c.m.)=111-131|'; 1294 {I65} for |q(c.m.)=94-110|'; 1018 {I51} for |q(c.m.)=85-93|'; 1039 {I52} for |q(c.m.)=74-84|'; 1540 {I77} for |q(c.m.)=62-73|' (2020Mo35. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
$E2 matrix element (1122,2+ to 536,2+)=+0.85 eb {I4}, B(E2)(W.u.)=37 {I3} (2020Mo35) 
$M1 matrix element (1122,2+ to 536,2+)=+0.11 |m {I1}, B(M1)(W.u.)=0.0014 {I2} (2020Mo35) 
$Number of counts: 298 {I24} for |q(c.m.)=62-131|'; 81 {I11} for |q(c.m.)=111-131|'; 81 {I12} for |q(c.m.)=94-110|'; 63 {I10} for |q(c.m.)=85-93|'; 44 {I10} for |q(c.m.)=74-84|'; 45 {I11} for |q(c.m.)=62-73|' (2020Mo35). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$E2 matrix element (1122,2+ to 0.0+)=+0.067 eb {I3}, B(E2)(W.u.)=0.23 {I2} (2020Mo35) 
$Number of counts: 51 {I9} for |q(c.m.)=62-131|' (2020Mo35) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$E2 matrix element (1205,4+ to 536,2+)=+1.29 eb {I6}, B(E2)(W.u.)=47 {I4} (2020Mo35) 
$Number of counts: 900 {I45} for |q(c.m.)=62-131|'; 195 {I15} for |q(c.m.)=111-131|'; 260 {I18} for |q(c.m.)=94-110|'; 198 {I16} for |q(c.m.)=85-93|'; 121 {I13} for |q(c.m.)=74-84|'; 111 {I13} for |q(c.m.)=62-73|' (2020Mo35) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$E2 matrix element (1944,6+ to 1205,4+)=+1.74 eb {I+21-18}, B(E2)(W.u.)=60 {I+14-12} (2020Mo35) 
$Number of counts: 151 {I22} for |q(c.m.)=62-131|'; 39 {I9} for |q(c.m.)=111-131|' (2020Mo35) 


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:
$|a(K)exp=0.0192 {I11} 
MR$weighted average of -4.0 {I10} (1961Ha08), -3.4 {I6} (1970La19), -3.3 {I6} (1972Kr07), -4.53 {I12} (1974Ko02), -3.8 {I3}(1979Ir01); other: -6.7{I5} (1960Jo11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$|g(|q) from oriented {+131}I (1974Ko02). Others: |d=-6.7 {I5} (1971Kr07), |d=-4.7 {I3} (1964Da19) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
E from 1974Me21 
$$ K:L1:L2:L3=100 {I2}:23.8 {I7}:5.5 {I3}:19.6 {I6} (1962Ge09) 
$Other:L1:L2:L3=100 {I3}:24.1 {I9}:77.2 {I22} (1969Fr04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(31/2)- |) 27/2- in Table I of 2018Ka27 should be 27/2- |) 23/2-, as confirmed in e-mail reply of August 26, 2018 from the first author 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$27/2- |) 23/2- in Table I of 2018Ka27 should be (31/2-) |) 27/2-, as confirmed in e-mail reply of August 26, 2018 from the first author 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$double placement in {+132}I |b{+-} (2.295 h); but (n,|g) results suggest main placement from 2187 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$ 630.22 9 (1978Ne08) 
MR$others: +6.1 {I+65-25} (1983So04); +4.5 {I+20-10} (1980Gi07); +2 {I+3-2} (1972Kr07); +5.3 {I+21-10} (1971Kr16). Alternative |d=-0.180 {I9} from |g(|q) (1980Gi07) is inconsistent with |g|g(|q) data 
$|g(|q): A{-2}=-0.187 {I12}, A{-4}=-0.2 {I9} (1980Gi07); A{-2}=+0.45 {I32} (1972Kr07) 
$ |g(|q): B{-2}U{-2}A{-2}=-0.04 {I3}, B{-4}U{-4}A{-4}=-0.04 {I3} (1972Kr07) 
$(630|g)(668|g)(|q): A{-2}=-0.27 {I3}, A{-4}=+0.26 {I5} 
$(630|g)(668|g)(|q): A2=-0.19 3, A4=+0.31 4 (1971Kr16) 
$(668|g)(630|g)(|q): A2=-0.16 4, A4=+0.29 5 
$(630|g)(668|g)(|q): A2=-0.18 5, A4=+0.23 8 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$ 772.61 8 (1978Ne08) 
$ |g(|q): B{-2}U{-2}A{-2}=-0.063 {I5}, B{-4}U{-4}A{-4}=-0.007 {I6} (1972Kr07) 
$(773|g)(668|g)(|q): A{-2}=+0.092 {I11}, A{-4}=+0.023 {I16} 
$(773|g)(668|g)(|q): A2=+0.093 9, A4=+0.004 11 (1971Kr16) 
$(668|g)(773|g)(|q): A2=+0.095 7, A4=+0.018 9 
$(668|g)(773|g)(|q): A2=+0.096 9, A4=+0.001 11 (1971Kr16) 
$(773|g)(668|g)(|q): A2=+0.081 10, A4=+0.010 1 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$ 363.5 4 (1978Ne08) 
MR$other: -0.23 {I2} (1983So04) 
$|g(|q): A{-2}=+1.11 {I7}, A{-4}=+0.2 {I11} 
$(363|g)(773|g)(|q): A{-2}=-0.12 {I2}, A{-4}=-0.02 {I4} (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$ 505.90 13 (1978Ne08) 
MR$others: -0.1 to -3 (1972Kr07), -1.3 {I4} (1971Kr16). Alternative |d=+0.40 {I2} (1980Gi07) from |g(|q) is inconsistent with |g|g(|q) data 
$|g(|q): A{-2}=-0.366 {I24}, A{-4}=+0.4 {I24} 
$(506|g)[630|g](668|g)(|q): A{-2}=+0.13 {I3}, A{-4}=+0.04 {I4} (1971Kr16) 
$ |g(|q): B{-2}U{-2}A{-2}=+0.13 7, B{-4}U{-4}A{-4}=+0.06 7 (1972Kr07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$ 1136.03 12 (1978Ne08) 
MR$others: +0.45 {I5} (1983So04); +0.22 {I+15-11} (1980Gi07); +0.9 {I3} (1971Kr16) 
$|g(|q): A{-2}=-0.29 {I3}, A{-4}=-0.01 {I7} 
$(1136|g)(668|g)(|q): A{-2}=+0.09 {I8}, A{-4}=+0.18 {I12} 
$(1136|g+1143|g)(668|g)(|q): A2=+0.21 4, A4=0.00 6 (1971Kr16) 
$(1136|g)(668|g)(|q): A2=+0.195 18, A4=+0.03 3 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others: -0.23 {I16} (1983So04), -0.28 to -0.54 (1980Gi07); -0.25 {I15} (1971Kr16) 
$|g(|q): A{-2}=-0.369 {I8}, A{-4}=-0.042 {I25} 
$ |g(|q): B{-2}U{-2}A{-2}=-0.120 24, B{-4}U{-4}A{-4}=+0.06 3 (1972Kr07) 
$(523|g)[773|g](668|g)(|q): A{-2}=+0.27 {I5}, A{-4}=-0.06 {I7} 
$(523|g)(773|g)(|q): A{-2}=+0.270 {I20}, A{-4}=+0.028 {I24} 
$(523|g)[773|g](668|g)(|q): A2=+0.25 3, A4=-0.04 4 (1971Kr16) 
$(523|g)(773|g)(|q): A2=+0.249 25, A4=-0.03 3 (1971Kr16) 
$(523|g)[773|g](668|g)(|q): A2=+0.20 3, A4=+0.12 5 (1983So04) 
$(523|g)(773|g)(|q): A2=+0.29 3, A4=-0.01 5 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$|g(|q): A{-2}=-0.437 {I8}, A{-4}=-0.31 {I5} 
$(1295|g)(668|g)(|q): A{-2}=+0.12 {I9}, A{-4}=+0.26 {I14} 
$(1295|g+1291|g)(668|g)(|q): A2=+0.11 4, A4=-0.03 7 (1971Kr16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR$+3.7 {I+10-6} is inconsistent with that from |g|g(|q) in (n,|g) 
$|g(|q): A{-2}=-0.22 {I7}, A{-4}=-0.2 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|g(|q): A{-2}=-0.450 {I10}, A{-4}=-0.36 {I6} 
$(812|g)[630|g](668|g)(|q): A{-2}=+0.04 {I5}, A{-4}=+0.05 {I7} 
$(812|g)(630|g)(|q): A{-2}=+0.07 {I6}, A{-4}=+0.02 {I8} 
$(812|g+810|g)[630|g](668|g)(|q): A2=0.00 3, A4=-0.05 5 (1971Kr16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
MR$ -0.02 3 (1983So04) 
$|g(|q): A{-2}=-0.455 {I10}, A{-4}=-0.32 {I7} 
$(1443|g)(668|g)(|q): A{-2}=+0.16 {I11}, A{-4}=-0.28 {I16} 
$(1443|g)(668|g)(|q): A2=+0.13 5, A4=+0.01 9 (1971Kr16) 
$(1443|g)(668|g)(|q): A2=+0.09 2, A4=-0.1 4 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$3.2 {I6} for 727.0 and 2.2 {I6} for 727.2 quoted in 1978Ne08 are reverse of those in 1973Si29, from which the values are adopted 
$|a(K)exp=0.0032 {I7} for a doublet: 727.0+727.2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$|g(|q): A{-2}=+1.02 {I6}, A{-4}=+0.29 {I12} 
$(910|g)[773|g](668|g)(|q): A{-2}=-0.32 {I20}, A{-4}=+0.05 {I31} 
$(910|g)(773|g)(|q): A{-2}=-0.33 {I12}, A{-4}=-0.11 {I16} 
$(910|g)[773|g](668|g)(|q): A2=-0.18 11, A4=-0.08 16 (1983So04) 
$(630|g)(773|g)(|q): A2=-0.20 16, A4=-0.1 4 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others: -0.03 {I3} (1983So04); -0.12 {I6} (1980Gi07); -0.15 {I5} (1971Kr16) 
$|g(|q): A{-2}=-0.386 {I6}, A{-4}=-0.03 {I4} 
$ |g(|q): B{-2}U{-2}A{-2}=-0.087 16, B{-4}U{-4}A{-4}=-0.008 18 (1972Kr07) 
$(955|g)[773|g](668|g)(|q): A{-2}=+0.28 {I4}, A{-4}=+0.01 {I6} 
$(955|g)(773|g)(|q): A{-2}=+0.222 {I13}, A{-4}=+0.005 {I16} 
$(955|g)[773|g](668|g)(|q): A2=+0.225 14, A4=-0.002 17 (1971Kr16) 
$(955|g)(773|g)(|q): A2=+0.237 13, A4=-0.004 16 (1971Kr16) 
$(955|g)[773|g](668|g)(|q): A2=+0.19 3, A4=+0.03 4 (1983So04) 
$(955|g)(773|g)(|q): A2=+0.209 11, A4=-0.005 18 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others: -0.04 {I+4-9} (1971Kr16); -0.22 {I11} (1980Gi07) 
$|g(|q): A{-2}=+0.64 {I3}, A{-4}=+0.03 {I4} 
$(1143|g)[773|g](668|g)(|q): A{-2}=-0.24 {I12}, A{-4}=-0.16 {I18} 
$(1143|g)(773|g)(|q): A{-2}=-0.21 {I8}, A{-4}=+0.04 {I10} 
$(1136|g+1143|g)(773|g)(|q): A2=-0.10 5, A4=-0.03 8 (1971Kr16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
MR$ +0.01 8 (1971Kr16) FOR J(2589)=3 
$|g(|q): A{-2}=-0.455 {I12}, A{-4}=-0.31 {I9} 
$(1291|g)[630|g](668|g)(|q): A{-2}=+0.09 {I11}, A{-4}=-0.12 {I12} 
$(1291|g)(630|g)(|q): A{-2}=+0.17 {I13}, A{-4}=+0.10 {I16} 
$(1291|g+1295|g)(668|g)(|q): A2=+0.11 4, A4=-0.03 7 (1971Kr16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$ -0.16 11 (1983So04) 
$|g(|q): A{-2}=+0.85 {I3}, A{-4}=+0.10 {I4} 
$(650|g)[523|g](773|g)(|q): A2=-0.15 6, A4=+0.01 10 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|g(|q): A{-2}=-0.429 {I23}, A{-4}=-0.25 {I10} 
$(810|g+812|g)(668|g)(|q): A2=0.00 3, A4=-0.05 5 (1971Kr16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others: -0.6 {I4} or -2.0 {I+9-60} (1983So04); -0.53 {I+22-11} (1980Gi07); -0.40 {I15} (1971Kr16) 
$|g(|q): A{-2}=+1.025 {I12}, A{-4}=+0.16 {I6} 
$(1173|g)[773|g](668|g)(|q): A{-2}=-0.48 {I14}, A{-4}=+0.16 {I28} 
$(1173|g)(773|g)(|q): A{-2}=-0.42 {I11}, A{-4}=-0.16 {I14} 
$(1173|g)[773|g](668|g)(|q): A2=-0.31 11, A4=+0.05 13 (1971Kr16) 
$(1173|g)(773|g)(|q): A2=-0.31 8, A4=-0.04 10 (1971Kr16) 
$(1173|g)(773|g)(|q): A2=-0.39 18, A4=+0.16 27 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$ +0.02 7 (1983So04) 
$|g(|q): A{-2}=+0.583 {I6}, A{-4}=+0.009 {I25} 
$(1372|g)[630|g](668|g)(|q): A{-2}=-0.07 {I5}, A{-4}=+0.01 {I7} (1971Kr16) 
$(1372|g)[630|g](668|g)(|q): A2=+0.010 11, A4=-0.015 17 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp=0.0032 {I7} for a doublet 
MR$1971Kr16 give -0.32 {I4}, but 727|g is a doublet: 727.0+727.2 
$(727|g)[671|g+773|g](668|g)(|q): A2=+0.11 3, A4=+0.04 5 (1971Kr16) 
$(727|g)[671|g](773|g)(|q): A{-2}=+0.11 {I4}, A{-4}=0.00 {I5} (1971Kr16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others: +0.04 {I2} (1983So04); +0.08 {I3} (1980Gi07); +0.07 {I2} (1971Kr16) 
$|g(|q): A{-2}=+0.162 {I12}, A{-4}=0.00 {I6} 
$(1399|g)[773|g](668|g)(|q): A{-2}=-0.06 {I4}, A{-4}=+0.04 {I6} 
$(1399|g)(773|g)(|q): A{-2}=-0.009 {I23}, A{-4}=-0.01 {I3} 
$(1399|g)[773|g](668|g)(|q): A2=-0.035 16, A4=-0.01 3 (1971Kr16) 
$(1399|g)(773|g)(|q): A2=-0.020 14, A4=+0.006 25 (1971Kr16) 
$(1399|g)[773|g](668|g)(|q): A2=-0.049 15, A4=+0.059 25 (1983So04) 
$(1399|g)(773|g)(|q): A2=-0.03 3, A4=+0.04 4 (1983So04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others: +3.70 {I17} (1990Da09); +5.0 {I+8-6} (1987De33); +18 {I+50-9} (1971Ta21) 
$(630|g)(668|g)(|q): A{-2}=-0.241 {I6}, A{-4}=+0.313 {I13} (1990Da09) 
$(630|g)(668|g)(|q): A2=-0.18 4, A4=+0.22 6 (1987De33) 
$(630|g)(668|g)(|q): A2=-0.16 5, A4=+0.36 9 (1971Ta21) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR$other: +1.59 {I13} (1990Da09) 
$(363|g)(773|g)(|q): A{-2}=-0.396 {I20}, A{-4}=-0.18 {I4} (1990Da09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others: +3.6 {I5} or +0.09 {I4} (1990Da09); +1.5 {I+13-6} (1987De33) 
$(506|g)(1298|g)(|q): A{-2}=+0.01 {I3}, A{-4}=-0.07 {I5} (1990Da09) 
$(506|g)[630|g](668|g)(|q): A2=+0.01 3, A4=+0.10 6 (1987De33) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others: +0.34 {I3} (1990Da09); -4.5 {I+15-25} (1987De33) 
$(1136|g)(668|g)(|q): A{-2}=+0.156 {I13}, A{-4}=-0.02 {I3} (1990Da09) 
$(1136|g)(668|g)(|q): A2=+0.10 7, A4=+0.27 11 (1987De33) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$ 1317.927 7 (1979Gr01) 
MR$others: -0.123 {I15} (1990Da09); +0.085 {I20} (1987De33) 
$(1318|g)(668|g)(|q): A{-2}=+0.329 {I10}, A{-4}=+0.047 {I20} (1990Da09) 
$(1318|g)(668|g)(|q): A2=+0.38 6, A4=+0.06 11 (1987De33) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$+0.15 {I+22-19} disagrees with +4.07 {I16} from adopted gammas 
A{-2}=-0.191 {I18}, A{-4}=+0.288 {I28} 
$ A2=-0.14 6, A4=+0.14 15 (1971Ke13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
A{-2}=+0.115 {I19}, A{-4}=+0.095 {I24} 
$ SIGN OF A4 SHOULD BE NEGATIVE FOR DJ=2, Q TRANSITION 
$ A2=+0.18 1, A4=-0.01 2 (1971Ke13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$ (630|g)(668|g)(|q): A{-2}=-0.23 {I1}, A{-4}=+0.24 {I9} 
$ (668|g)(630|g)(|q): A{-2}=-0.24 {I1}, A{-4}=+0.25 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$ (773|g)(668|g)(|q): A{-2}=+0.10 {I1}, A{-4}=-0.01 {I2} 
$(668|g)(773|g)(|q): A{-2}=+0.10 {I1}, A{-4}=-0.01 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.35 {I+32-16} is also possible which is the preferred value by 1988Ha28. |d=+7.5 {I6} in adopted gammas 
$ (506|g)(630|g)(|q): A{-2}=+0.05 {I5}, A{-4}=-0.07 {I6} 
$ (506|g)(630|g)(668|g)(|q): A{-2}=+0.04 {I5}, A{-4}=-0.05 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$ (523|g)(727|g)(|q): A{-2}=+0.24 {I6}, A{-4}=-0.09 {I10} 
$ (523|g)[773|g](668|g)(|q): A{-2}=+0.22 {I5}, A{-4}=+0.01 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_comment:
$ (600|g)(773|g)(|q): A{-2}=-0.075 {I25}, A{-4}=-0.003 {I3} 
$ (600|g)[773|g](668|g)(|q): A{-2}=-0.013 {I3}, A{-4}=-0.015 {I35} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_comment:
$ (1029|g)(773|g)(|q): A{-2}=-0.095 {I3}, A{-4}=-0.057 {I74} 
$ (1029|g)[773|g](668|g)(|q): A{-2}=-0.02 {I7}, A{-4}=-0.06 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$ +0.65 {I+41-30} if J=2; -0.11 {I12} if J=3 from (570|g)[1318|g](668|g)(|q): A{-2}=-0.08 {I9}, A{-4}=-0.08 {I10} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
RI$ doublet with 667|g from first 2+ to 0+. Since its branching ratio is not known, the yield of 1963, 4+ state could not be determined 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$B(E2)(W.u.)<5 if |d=+0.7 {I+23-2}, <13 if |d=+2.0 {I+10-16} (2016Pe13). Compilers obtain <15 in both cases. 
MR$+0.7 {I+23-2} or +2.0 {I+10-16} 


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$poor fit in the level scheme. In an e-mail reply of Sept 23, 2016 from E.E. Peters, it was mentioned that the 1295 peak was part of complex structure and that it was possible that quoted uncertainty was underestimated. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
MR$from measured (727|g)(773|g)(|q) (2017Vo06). This value agrees with |d=+0.41 {I+7-8} in {+132}Xe Adopted dataset in the ENSDF database. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4+E5
decay_comment:
RI$isomeric transition. I|g is calculated by evaluators, assuming the isomer population equal 2.88% {I3} in {+133}I |b{+-} decay (1976Me16) 
M,MR$adopted level, gammas 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from level scheme. E|g=418.047 {I15} of 1976Me16 is probably a misprint 
MR$-0.3|<|d|<+2.2 
$A{-2}G{-2}=+1.2 {I8} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from level scheme. E|g=1236.411 {I6} in Table 1 (1976Me16) is probably a misprint 
$A{-2}G{-2}=-0.92 {I8}, A{-4}G{-4}=-1.3 {I10} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4+E5
decay_comment:
E$from (1976Me16). Others: 233.2 {I4} (1972Ac02), 232.8 {I3} (1952Be55) 
$L1:L2:L3=100 {I3}:25.0 {I12}:52.6 {I16} (1969Fr04) 
MR$calculated in 2006Ra03 from subshell ratios of 1969Fr04. |d=0.12 {I9} calculated by evaluators with BrIccMixing program from K/L+ ratios 


decay_energy_unit: KEV
decay_comment:
E$from {+133}Xe Adopted dataset in the ENSDF database. This |g not seen in 2017Vo06 as it is highly converted 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
MR$|d(Q/D)=-0.69 {I11} for J(2123)=19/2 as the best fit (|h{+2}=0.8) of (247|g)(947.7|g)(|q) data in 2017Vo06. Less likely choices are |d(Q/D)=+0.24 {I3} (|h{+2}=3.7) for J(2123)=21/2, and |d(E3/M2)=-0.32 {I6} (|h{+2}=5.4) for J|p(2123)=23/2+. For J|p=23/2-, |h{+2}=20.7, which is rejected. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M2+(E3)
decay_comment:
$|a{-T}=0.49 {I9} computed from the intensity balance in {+130}Te({+9}Be,2p4n) experiment in 2018Ka47. Comparison with the theoretical |a yields a good agreement with M2 or E3. Other: |a{-T}=0.421 {I6} calculated employing |d deduced in 2018Ka47. 
MR$from the 948|g gated |g(|q)-|g(|q) measurements in {+130}Te({+9}Be,2p4n). 
$B(M2)(W.u)=0.000209 {I3}, B(E3)(W.u) = 0.0017 {I16} measured in 2018Ka47. 
M$based on deduced |a, measured |d and comparison of the reduced transition probabilities with the shell model calculations in 2018Ka47. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$See comment on 2136 keV level. This |g ray was seen in coincidence with both 405 keV |g and 217 keV |g, as a result, it could be a doublet of 2 |g-rays very close in energy 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.119 {I7}, A{-4}=-0.006 {I9} 
$B(E2)(W.u.)=15.3 {I11} (2009Ah01 quote value from ENSDF database) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.262 {I8}, A{-4}=-0.01 {I1} 
$B(E2)(W.u.)=20 {I2} and B(M1)=0.015 {I1} (2009Ah01) 
$B(E2)(W.u.)=20.1 {I19} and B(M1)=0.015 {I3} (B(M1)(W.u.)=0.0083 {I16}) (deduced by compiler using the program ruler) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=+0.28 {I1}, A{-4}=-0.06 {I2} 
$B(E2)(W.u.)=0.74 {I5} (2009Ah01) 
$B(E2)(W.u.)=0.74 {I4} (deduced by compiler using the program ruler) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E,M$from Adopted gammas in ENSDF database. Not reported in 2009Ah01 
RI$deduced by compiler from branching ratio in adopted gammas in ENSDF database 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=+0.27 {I1}, A{-4}=+0.01 {I1} 
$B(E2)(W.u.)=0.56 {I4} and B(M1)=0.30 {I2} (2009Ah01) 
$B(E2)(W.u.)=0.6 {I3} and B(M1)=0.297 {I18} (B(M1)(W.u.)=0.166 {I10}) (deduced by compiler using the program ruler) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$A{-2}=+0.306, A{-4}=-0.074 (calcualted from theory of Coulomb excitation) 
$B(E2)(W.u.)=0.72 {I7} (2009Ah01) 
$B(E2)(W.u.)=0.75 {I5} (deduced by compiler using the program ruler) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=+0.33 {I2}, A{-4}=+0.07 {I2} 
MR$+0.14 {I2} or +1.6 {I1} 
$B(E2)(W.u.)=0.14 {I1} and B(M1)=0.041 {I3} (2009Ah01, using |d=0.14 {I2}) 
$B(E2)(W.u.)=0.15 {I5} and B(M1)=0.0423 {I19} (B(M1)(W.u.)=0.0236 {I11}) (deduced by compiler using the program ruler, |d=0.14 {I2} and |a=0.00103) 
$B(E2)(W.u.)=5.6 {I4} and B(M1)=0.012 {I1} (2009Ah01, using |d=1.6 {I1}) 
$B(E2)(W.u.)=5.5 {I3} and B(M1)=0.0121 {I12} (B(M1)(W.u.)=0.0068 {I7}) (deduced by compiler using the program ruler, |d=1.6 {I1} and |a=0.00089) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$A{-2}=+0.322, A{-4}=-0.091 (calculated from theory of Coulomb excitation) 
$B(E2)(W.u.)=0.63 {I6} (2009Ah01) 
$B(E2)(W.u.)=0.63 {I3} (deduced by compiler using the program ruler) 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
$W(|q(161{+|o} to 180{+|o}))/W(|q(150{+|o} to 161{+|o})) = 0.56 {I1} read by the compiler from Figure 4 in 2016Vo04. 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
$W(|q(161{+|o}) to 180{+|o}))/W(|q(150{+|o} to 161{+|o})) = 0.50 {I2} read by the compiler from Figure 4 in 2016Vo04. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$from the measured angular distribution ratio W(|q(161{+|o} to 180{+|o}))/W(|q(150{+|o} to 161{+|o})) = 0.54 {I3} read by the compiler from Figure 4 in 2016Vo04. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$from the measured angular distribution ratio W(|q(161{+|o} to 180{+|o}))/W(|q(150{+|o} to 161{+|o})) = 0.73 {I3} read by the compiler from Figure 4 in 2016Vo04. 


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:
MR$second solution with higher |h{+2}: -2.37 {I+74-71} 
$B(E2)(W.u.)=25.5 {I+86-91}, B(M1)=0.0076 {I+96-40} for |d(E2/M1)=-2.37 {I+74-71} 


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:
MR$second solution with higher |h{+2}: +2.86 {I+39-34} 
$B(E2)(W.u.)=75.6 {I+76-75}, B(M1)=0.032 {I+11-8} for |d(E2/M1)=+2.86 {I+39-34} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
$This |g observed in the delayed spectrum in the present experiment. Multipolarity from {+134}Xe Adopted dataset in the ENSDF database. 


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:
MR$second solution with higher |h{+2}: -2.43 {I+61-65} 
$B(E2)(W.u.)=6.3 {I18}, B(M1)=0.0049 {I+47-24} for |d(E2/M1)=-2.43 {I+61-65} 


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:
MR$second solution with higher |h{+2}: +2.02 {I+29-26} 
$B(E2)(W.u.)=6.5 {I+13-11}, B(M1)=0.0091 {I+38-27} for |d(E2/M1)=+2.02 {I+29-26} 


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:
MR$second solution with higher |h{+2}: -0.01 {I+11-10} 
$B(E2)(W.u.)=0.0003 {I+350-3}, B(M1)=0.0179 {I+43-38} for |d(E2/M1)=-0.01 {I+11-10} 


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_comment:
MR$second solution with higher |h{+2}: +1.76 {I+55-38} 
$B(E2)(W.u.)<20, B(M1)<0.01 for |d(E2/M1)=+1.76 {I+55-38} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$According to e-mail reply of July 24, 2017 from E.E. Peters, this |g ray was observed but due to a doublet with a line from the background, its intensity and precise energy could not be measured. 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
$Branching ratio, B(E2)(W.u.) and B(M1) values listed in authors' Table I should be omitted according to e-mail replies of July 24 and 25, 2017 from E.E. Peters, as the gamma-ray branching ratio for the 1040|g could not be measured in the present work. 


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:
MR$second solution with higher |h{+2}: +1.2 {I13} 
$B(E2)(W.u.)=0.56 {I+58-56}, B(M1)=0.005 {I+13-4} for |d(E2/M1)=+1.2 {i13} 


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:
MR$second solution with higher |h{+2}: -0.19 {I+16-17} 
$B(E2)(W.u.)=0.12 {I+42-12}, B(M1)=0.052 {I+23-17} for |d(E2/M1)=-0.19 {I+16-17} 


decay_energy_unit: KEV
decay_multipolarity: M4
decay_comment:
M$from {+135}Xe IT decay 
RI$transient equilibrium value=46.6 {I3} (1982Wa21) for isomeric transition 
E$526.58 {I7} (bent-crystal spectrometer (1979Bo26)) 
CC M4 CC(THEORY)'S MULT. BY 0.975 5 (1990Ne01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$220.51 {I3} (bent-crystal spectrometer (1979Bo26)) 
M$from |a(K)exp=0.07 {I3} 
(221|g)(1458|g)(|q): A{-2}=+0.29 {I2}, A{-4}=+0.07 {I3} 
(221|g)(1458|g)(THETA): A2=+0.31 6, A4=-0.01 10 (1971Ma37) 
(221|g)(1458|g)(THETA): A2=+0.205 20, A4=-0.024 9 (1972Be90) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from |a(K)exp=0.015 {I9} 
(418|g)(1260|g)(|q): A{-2}=-0.50 {I2}, A{-4}=+0.02 {I3} 
(418|g)(1260|g)(THETA): A2=-0.55 6, A4=+0.04 9 (1971Ma37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
(547|g)(1132|g)(|q): A{-2}=+0.24 {I1}, A{-4}=-0.002 {I20} 
(547|g)(1132|g)(THETA): A2=+0.25 4, A4=-0.04 7 (1971Ma37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
(837|g)(1132|g)(|q): A{-2}=+0.05 {I2}, A{-4}=-0.08 {I3} 
(837|g)(1132|g)(THETA): A2=+0.11 6, A4=-0.22 9 (1971Ma37) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
|d(M3/E2)=-0.01 {I5} from (973)(1260)(|q): A{-2}=+0.10 {I4}, A{-4}=+0.02 {I7} 
(973|g)(1260|g)(THETA): A2=+0.09 3, A4=+0.04 3 (1972Be90) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
(1124|g)(1132|g)(|q): A{-2}=+0.21 {I3}, A{-4}=+0.09 {I4} 
(1124|g)(1132|g)(THETA): A2=+0.09 8, A4=+0.13 13 (1971Ma37) 
$ (1124|g)(1132|g)(THETA): A2=+0.145 25, A4=-0.022 13 (1972Be90) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
|d(Q/D)=-0.06 {I10} for 9/2; +0.89 {I10} for 7/2 (1991Go09) 
(1240|g)(1132|g)(|q): A{-2}=-0.11 {I6}, A{-4}=+0.03 {I10} (1991Go09). (1240|g)(1132|g)(|q): A{-2}=+0.16 {I7}, A{-4}=+0.06 {I5} (1972Be90). Note sign of A{-2} is different in two studies 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from |a(K)exp,|a(L)exp in {+136}I |b{+-} decay. Transition is |DJ=0 from |g|g(|q) in {+238}U({+12}C,F|g),{+208}Pb({+18}O,F|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1313.4 {I4} (1974Su04) and 1313.3 {I2} (1970Jo20). 
RI$from 1974Su04. 
$(381|g)(1313|g)(|q): A{-2}=0.023 {I3}, A{-4}=0.001 with A{-4} held fixed (2009Go09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 381.6 {I4} (1974Su04) and 380.7 {I2} (1970Jo20). 
RI$other: 0.86 {I17} (1974Su04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 197.4 {I4} (1974Su04) and 197.3 {I2} (1970Jo20). 
M$from |a(K)exp 
EKC$From I|g(K| x ray) and I|g(197|g) assuming |a(K)(382|g; E2) (1972ClZN) 
RI$other: 0.92 {I14} (1974Su04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$from |a(K)exp 
M$other: A{-2}=0.083 {I15}, A{-4}=-0.02 {I2} for (381|g)(1313|g)(|q) consistent with Q(|b{+-})Q cascade (1985Be04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$M1,E2 from |a(K)exp; Q from |g|g(|q). Other: |a(K)exp=0.018 {I4} (1972Ac02). 
E$other: 381.37 {I6} (1977We04). 
M$other: A{-2}=0.083 {I15}, A{-4}=-0.02 {I2} for (381|g)(1313|g)(|q) consistent with Q(|b{+-})Q cascade (1985Be04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 197.33 {I5} (1977We04). 
M$from |a(K)exp, |a(L)exp, and |a(M)exp. Also |a(K)exp=0.158 {I25}, K/L+=3.8 {I8} (1972Ac02) 
M$other: A{-2}=0.080 {I20}, A{-4}=0.004 {I20} for (197|g)(381|g)(|q) consistent with Q(|b{+-})Q cascade (1985Be04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$A{-2}=-0.410 {I10}, A{-4}=0.003 {I30} for (750|g)(381|g)(|q) consistent with D-Q cascade (1985Be04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$R(22|')=1.5 {I3}, R(46|')=1.2 {I1}, R(75|')=1.00 {I6} for (968|g)(370|g)(|q) consistent with |DJ=2, quadrupole (E2) and |DJ=0, dipole cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$R(22|')=1.1 {I1}, R(46|')=1.0 {I1}, R(75|')=1.00 {I5} for (255|g)(968|g)(|q) consistent with |DJ=2, quadrupole- |DJ=2, quadrupole (E2) cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Observed T{-1/2}=5.1 ns {I11} (1974ClZX) disagrees with T{-1/2}<0.4 ns measured by 1980Fo09. T{-1/2}<0.25 ns may belong to precursor higher levels 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
$ (400.1|g)(1220.2|g)(|q): A{-2}=+0.103 {I5}; A{-4}=+0.012 {I8} (2010Li03) consistent with E2-E2 cascade and 15/2- --> 11/2- --> 7/2- spin sequence 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
$ (314.2|g)(400.1|g)(|q): A{-2}=+0.072 {I7}; A{-4}=+0.014 {I10} (2010Li03) consistent with E2-E2 cascade and 19/2- --> 15/2- --> 11/2- spin sequence 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
$ (311.7|g)(1046.6|g)(|q): A{-2}=+0.091 {I13}; A{-4}=+0.009 {I19} (2010Li03) consistent with E2-E2 cascade and 27/2- --> 23/2- --> 19/2- spin sequence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M,MR$D+Q from |g|g(|q) (1992Co26) in {+138}I |b{+-} decay; positive parity for the 1464 level based on systematics of N=84 nuclei; mult=E1+M2 with such a large |d is highly unlikely. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from 1979Bo26. Others: 588.86 {I20} from 1992Co26, 588.83 {I8} from 1979Ho21, 588.87 {I8} from 1976We20 
RI$from 1992Co26. Other: 1000 {I35} from 1979Ho21 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$from 1979Bo26. Others: 483.68 {I20} from 1992Co26, 483.62 {I9} from 1979Ho21, 483.67 {I10} from 1976We20 
RI$weighted average of 59.7 {I19} from 1992Co26 and 63 {I3} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 875.23 {I20} from 1992Co26, 875.23 {I13} from 1979Ho21 and 875.29 {I15} from 1976We20. 
RI$weighted average of 168 {I4} from 1992Co26 and 165 {I14} from 1979Ho21. 
M,MR$from 1992Co26, obtained assuming a positive parity for the 1464 level from systematics of N=84 nuclei; adopted in Adopted Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1463.95 {I21} from 1992Co26 and 1464.0 {I2} from 1979Ho21. Other: 1463.2 {I12} from 1976We20 
RI$weighted average of 14.2 {I7} from 1992Co26 and 11.0 {I12} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1277.43 {I20} from 1992Co26 and 1277.45 {I11} from 1979Ho21. Other: 1277.7 {I3} from 1976We20 
RI$weighted average of 42.6 {I12} from 1992Co26 and 42.4 {I21} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1866.10 {I25} from 1992Co26 and 1866.25 {I17} from 1979Ho21. 
RI$weighted average of 7.1 {I6} from 1992Co26 and 6.0 {I5} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 830.67 {I20} from 1992Co26 and 830.69 {I8} from 1979Ho21. Other: 830.8 {I3} from 1976We20 
RI$weighted average of 28.7 {I8} from 1992Co26 and 28.9 {I18} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1314.41 {I21} from 1992Co26 and 1314.28 {I10} from 1979Ho21. 
RI$unweighted average of 15.8 {I7} from 1992Co26 and 17.9 {I6} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 942.74 {I21} from 1992Co26 and 942.91 {I8} from 1979Ho21. 
RI$weighted average of 12.1 {I6} from 1992Co26 and 11.8 {I6} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1426.69 {I21} from 1992Co26 and 1426.9 {I3} from 1979Ho21. 
RI$weighted average of 19.6 {I8} from 1992Co26 and 21 {I6} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 650.90 {I22} from 1992Co26 and 650.8 {I5} from 1979Ho21. 
RI$weighted average of 4.0 {I4} from 1992Co26 and 4.2 {I10} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1525.85 {I22} from 1992Co26 and 1525.82 {I13} from 1979Ho21. 
RI$weighted average of 15.7 {I8} from 1992Co26 and 15.1 {I12} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2114.7 {I3} from 1992Co26 and 2114.7 {I5} from 1979Ho21. 
RI$weighted average of 3.6 {I5} from 1992Co26 and 2.7 {I5} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1528.41 {I20} from 1992Co26 and 1528.37 {I15} from 1979Ho21. 
RI$weighted average of 11.8 {I8} from 1992Co26 and 11.8 {I7} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1673.28 {I22} from 1992Co26 and 1673.28 {I9} from 1979Ho21. 
RI$weighted average of 21.7 {I8} from 1992Co26 and 21.9 {I8} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2262.26 {I25} from 1992Co26 and 2262.19 {I11} from 1979Ho21. 
RI$weighted average of 69.7 {I21} from 1992Co26 and 69 {I2} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 1259.41 {I23} from 1992Co26 and 1258.84 {I14} from 1979Ho21. 
RI$unweighted average of 9.1 {I7} from 1992Co26 and 13.0 {I8} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 869.89 {I21} from 1992Co26 and 870.2 {I2} from 1979Ho21. 
RI$weighted average of 42.6 {I13} from 1992Co26 and 58 {I9} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 1745.39 {I24} from 1992Co26 and 1744.6 {I2} from 1979Ho21. 
RI$unweighted average of 12.4 {I10} from 1992Co26 and 19.1 {I20} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1809.23 {I22} from 1992Co26 and 1809.30 {I14} from 1979Ho21. Other: 1809.5 {I5} from 1976We20 
RI$weighted average of 34.6 {I11} from 1992Co26 and 36.6 {I18} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2398.2 {I3} from 1992Co26 and 2398.15 {I15} from 1979Ho21. Other: 2398.3 {I5} from 1976We20 
RI$unweighted average of 14.6 {I8} from 1992Co26 and 11.9 {I5} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1954.80 {I23} from 1992Co26 and 1954.90 {I12} from 1979Ho21. 
RI$unweighted average of 15.6 {I8} from 1992Co26 and 13.2 {I4} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2543.7 {I3} from 1992Co26 and 2543.73 {I14} from 1979Ho21. 
RI$weighted average of 13.7 {I7} from 1992Co26 and 14.2 {I4} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1108.31 {I22} from 1992Co26 and 1108.28 {I18} from 1979Ho21. 
RI$weighted average of 7.5 {I6} from 1992Co26 and 7.0 {I5} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2572.4 {I3} from 1992Co26 and 2572.38 {I14} from 1979Ho21. 
RI$weighted average of 21.8 {I10} from 1992Co26 and 21.4 {I6} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2085.49 {I24} from 1992Co26 and 2085.42 {I12} from 1979Ho21. 
RI$weighted average of 13.6 {I5} from 1992Co26 and 13.8 {I6} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2673.8 {I5} from 1992Co26 and 2674.1 {I3} from 1979Ho21. 
RI$weighted average of 2.0 {I4} from 1992Co26 and 2.1 {I3} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1371.60 {I23} from 1992Co26 and 1371.4 {I5} from 1979Ho21. 
RI$weighted average of 5.9 {I5} from 1992Co26 and 4.7 {I10} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2835.6 {I4} from 1992Co26 and 2835.65 {I19} from 1979Ho21. 
RI$weighted average of 21.6 {I11} from 1992Co26 and 22.2 {I8} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 987.3 {I3} from 1992Co26 and 987.5 {I5} from 1979Ho21. 
RI$weighted average of 2.4 {I5} from 1992Co26 and 2.8 {I8} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 837.87 {I25} from 1992Co26 and 837.5 {I5} from 1979Ho21. 
RI$weighted average of 3.1 {I4} from 1992Co26 and 2.3 {I8} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2363.5 {I3} from 1992Co26 and 2363.74 {I16} from 1979Ho21. 
RI$weighted average of 5.7 {I5} from 1992Co26 and 5.0 {I3} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 849.76 {I24} from 1992Co26 and 849.9 {I5} from 1979Ho21. 
RI$weighted average of 2.3 {I5} from 1992Co26 and 2.4 {I5} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1500.49 {I21} from 1992Co26 and 1500.40 {I11} from 1979Ho21. 
RI$weighted average of 16.5 {I7} from 1992Co26 and 16.3 {I9} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 2376.2 {I4} from 1992Co26 and 2375.9 {I2} from 1979Ho21. 
RI$weighted average of 3.6 {I5} from 1992Co26 and 2.8 {I3} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2964.4 {I5} from 1992Co26 and 2964.4 {I3} from 1979Ho21. 
RI$weighted average of 2.6 {I4} from 1992Co26 and 2.8 {I2} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2032.79 {I24} from 1992Co26 and 2032.79 {I15} from 1979Ho21. 
RI$weighted average of 13.7 {I7} from 1992Co26 and 15.6 {I9} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3496.4 {I6} from 1992Co26 and 3496.3 {I2} from 1979Ho21. 
RI$weighted average of 13.1 {I9} from 1992Co26 and 13.1 {I7} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2928.6 {I5} from 1992Co26 and 2927.77 {I13} from 1979Ho21. 
RI$weighted average of 2.0 {I4} from 1992Co26 and 2.1 {I1} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3516.3 {I7} from 1992Co26 and 3516.3 {I2} from 1979Ho21. 
RI$weighted average of 2.6 {I4} from 1992Co26 and 2.9 {I3} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 1355.77 {I24} from 1992Co26 and 1355.81 {I11} from 1979Ho21. 
RI$weighted average of 5.7 {I5} from 1992Co26 and 7.1 {I6} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 1567.22 {I25} from 1992Co26 and 1567.1 {I5} from 1979Ho21. 
RI$weighted average of 5.7 {I6} from 1992Co26 and 4.1 {I10} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3310.3 {I5} from 1992Co26 and 3310.28 {I15} from 1979Ho21. 
RI$weighted average of 19.0 {I12} from 1992Co26 and 19.5 {I8} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1946.2 {I3} from 1992Co26 and 1946.27 {I13} from 1979Ho21. Placed by 1992Co26 based on observed 1946|g-1427|g-589|g-coin; no evidence for the placement by 1979Ho21 from a level at E=2535. 
RI$weighted average of 6.9 {I6} from 1992Co26 and 7.3 {I3} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2058.8 {I3} from 1992Co26 and 2058.85 {I14} from 1979Ho21. Placed by 1992Co26 based on observed 2059|g-831|g-coin; no evidence for the placement by 1979Ho21 from a level at E=3131. 
RI$unweighted average of 11.3 {I8} from 1992Co26 and 14.3 {I7} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1835.2 {I3} from 1992Co26 and 1835.52 {I17} from 1979Ho21. Placed by 1992Co26; unplaced in 1979Ho21 
RI$weighted average of 3.1 {I5} from 1992Co26 and 4.4 {I4} from 1979Ho21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2301.6 {I3} from 1992Co26 and 2301.56 {I16} from 1979Ho21. Placed by 1992Co26 based on observed 2302|g-1277|g-589|g-coin; no evidence for the placement by 1979Ho21 from the 2890 level. 
RI$weighted average of 17.3 {I8} from 1992Co26 and 18.3 {I8} from 1979Ho21. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$E2 is quoted for the 482.1-483.6 doublet 
$A{-2}=+0.089 {I1}, A{-4}=+0.035 {I1} for the 482.1-483.6 doublet (2000Ko15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1988FiZV 
RI$% intensities: I|g({+235}U, E=3.0 keV)=4.7 {I6}, I|g({+238}U)=2.3 {I5}, I|g({+235}U, E=th)=5.03 (1988FiZV) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1988FiZV 
RI$% intensities: I|g({+235}U, E=3.0 keV)=4.6 {I6}, I|g({+238}U)=2.2 {I6} (1988FiZV) 


decay_energy_unit: KEV
decay_multipolarity: [E2]
decay_uncertain: S
decay_comment:
$Obscured by x rays and 31.7|g in |b{+-} decay 
M$[E2] leads to an intensity balancing problem for the 22.8 level in |b{+-} decay. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(492|g)(571|g)(|q): A{-2}=-0.03 {I1}, A{-4}=+0.01 {I1}. Pol=-0.22 {I11} for 491 doublet (gated at 585|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$(397|g)(571|g)(|q): A{-2}=+0.08 {I1}, A{-4}=0.00 {I1}. Pol=-0.10 {I6} (gated at 585|g and 581.9|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$from e-mail reply of Oct. 11, 2002 from one of the authors (W. Urban). E|g=667.0 in Table 1 and Figure 1 of 2000Ur04 is a misprint. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
TI$deduced by the evaluators from |b feeding of |?21% and total |g feeding. Other: I(|g+ce)<292 from I|g<0.4 deduced from estimate by 1985Ro13 and mult=E2 is low since |g feeding from higher levels gives I(|g+ce)=332 {I5}. In addition, from systematics of neighboring nuclides, strong |b feeding is expected to this level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
ECC$>27 from intensity balance at 31.86 level, if no |b feeding 
TI$226 {I4} from intensity balancing at the 32 level, if no direct |b feeding to this level. With 22% |b feeding, I(|g+ce)|?500 
M,MR$from |g intensity balance at 31.9 level, using |b feeding of |?22% and I|g=8.0 {I3}. Assumption of no |b feeding to 31.86 level rules out E1 and implies |d(E2/M1)>0.48 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$total intensity for doublet=14.2 {I5}. Based on I|g(647)/I|g(656)=0.38 {I15} from SF decay (2002Ur04), almost all the intensity of 647.1|g belongs with the decay of 678 level, and almost none from the decay of 670 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$deduced in SF decay: E2,M2 for this |g, M2 excluded by non-observance of T{-1/2}>10 ns for the octupole band 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
M,MR$contradictorily assigned in {+252}Cf decay dataset as (M1+E2) with |d=+0.21 {I11} or or +3.9 {I15} (2017Na15), and (E1) (2016Hu10), neither of which being adopted here (see general disagreement comment) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$98.2 {I1} (1999Li18) adjusted for a slightly different total conversion coefficient value 
E$from 1979Bo26. Others: 377.1 {I4} (1971Kr22), 377.1 (1985RoZR) 
M$|a(K)exp slightly favors E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from 1979Bo26. Others: 457.7 {I2} (1985RoZR,1971Kr22) 
M$from |a(K)exp; the theoretical |a(K) values are mistakenly listed in Table 1 of 1999Li18 - should be interchanged 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$%I(377|g)=1.5 with 15% uncertainty (per 100 fissions of {+252}Cf) (1971Ch44) 
$({+140}Xe fragment)(377)(|q): A{-2}=+0.61 {I11}, A{-4}=-0.24 {I12} (1976Wo04) 
$({+140}Xe fragment)(377)(|q): A{-2}=+0.077 {I15} (2010SmZZ) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$%I(458|g)=1.29 with 15% uncertainty (per 100 fissions of {+252}Cf) (1971Ch44) 
$A{-2}=+0.104 {I5}, A{-4}=+0.000 {I7} for 457.8-376.7 cascade (2017Na15) 
$attenuated (458)(377)(|q): A{-2}=+0.095 {I4}, A{-4}=+0.010 {I6} (2009Go09) 
$({+140}Xe fragment)(457)(|q): A{-2}=+0.46 {I12}, A{-4}=+0.07 {I15} (1976Wo04) 
$({+140}Xe fragment)(457)(|q): A{-2}=+0.111 {I14} (2010SmZZ) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$or +1.3 {I2} (2016Hu10; +0.66 {I20} (2017Na17) 
$A{-2}=+0.203 {I22}, A{-4}=-0.070 {I34} for 927.7-376.7 cascade (2016Hu10) 
$A{-2}=+0.254 {I20}, A{-4}=+0.003 {I29} for 927.9-376.7 cascade (2017Na17) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=+0.203 {I8}, A{-4}=+0.003 {I13} for 738.6-457.7 cascade, 
$A{-2}=+0.189 {I5}, A{-4}=-0.017 {I8} for 738.6-sum cascade, A{-2}=+0.128 {I11}, A{-4}=-0.003 {I17} for 381.6-738.6 cascade (2016Hu10) 
$A{-2}=+0.117 {I11}, A{-4}=-0.007 {I16} for 738.6-457.8 cascade (2017Na15) 
MR$or +3.0 {I3} for 381.6-738.6 cascade, +0.53 {I3} or +1.6 {I1} for 3|s on A{-4} (2016Hu10); +0.48 {I4} or +3.4 {I4} (2017Na15) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$A{-2}=+0.064 {I23}, A{-4}=-0.005 {I36} for 308.8-582.5 cascade 
MR$or -1.5 {I2} (2016Hu10, for 2|s on A{-4}) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.117 {I25}, A{-4}=-0.014 {I39} for 891.3-457.7 cascade (2016Hu10) 
$A{-2}=+0.092 {I17}, A{-4}=+0.007 {I23} for 891.2-sum cascade (2017Na15) 
M$2016Hu10 give (M1/E2) in Table I, however this is in disagreement with the 891|g corresponding to a 6+ to 4+ transition and the angular correlations results. 2017Na15 gives E2 with |d(Q/D)=0 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
MR$or 1.3 {I2} (2016Hu10) 
$A{-2}=+0.128 {I11}, A{-4}=-0.003 {I17} for 381.6-738.6 cascade (2016Hu10) 
$A{-2}=+0.117 {I11}, A{-4}=-0.007 {I16} for 381.5-738.6 cascade (2017Na15) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
$A{-2}=-0.066 {I34}, A{-4}=+0.019 {I53} for 537.7-582.5 cascade; A{-2}=-0.086 {I23}, A{-4}=+0.002 {I35} for 537.7-457.7 cascade (2016Hu10) 
MR$0 or +18 for 1.5|s on A{-4} for 537.7-582.5 cascade; 0 or +40 for 1.5|s for 537.7-457.7 cascade (2016Hu10) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.116 {I32}, A{-4}=+0.003 {I49} for 839.7-582.5 cascade 
M$2016Hu10 give (M1/E2) in Table I, however this is in disagreement with the 840|g corresponding to a 8+ to 6+ transition and the angular correlations results 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M,MR$(M1+E2) with |d=+0.21 {I11} or or +3.9 {I15} (2017Na15), (E1) (2016Hu10), neither of which being adopted here (see general disagreement comment) 
$A{-2}=+0.057 {I60}, A{-4}=+0.038 {I93} 820.8-3815 cascade (2017Na15) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$2016Hu10 give (M1/E2) in Table I, however this is in disagreement with the 982|g corresponding to a (10+) to 8+ transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.103 {I5}, A{-4}=+0.022 {I8}. Other: A{-2}=+0.104 {I6}, A{-4}=+0.015 {I9} for 582.4|g-457.8|g cascade (2016Ur01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$|DJ=1 from |g|g(|q) (2003Ur02) adopted as (E1) as interband |D|p=yes transition 
$(1136)(377)(|q): A{-2}=-0.11 {I2}, A{-4}=-0.06 {I4} (2003Ur02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=+0.189 {I5}, A{-4}=-0.017 {I8}. Other: A{-2}=+0.125 {I8}, A{-4}=-0.010 {I11} for 738.6|g-381.5|g cascade (2016Ur01) 
MR$also +50 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
$A{-2}=-0.062 {I14}, A{-4}=-0.005 {I23} 
$(937)(413)(|q): A{-2}=-0.05 {I2}, A{-4}=-0.07 {I3}, $ (937)(sum)(|q): A{-2}=-0.10 {I3}, A{-4}=+0.02 {I4} (2003Ur02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
$A{-2}=-0.065 {I9}, A{-4}=-0.008 {I16} 
$(768)(552)(|q): A{-2}=-0.04 {I3}, A{-4}=-0.02 {I1}, (768)(sum)(|q): A{-2}=-0.07 {I3}, A{-4}=+0.01 {I1}, POL=+0.08 {I4} (2003Ur02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
$A{-2}=-0.066 {I11}, A{-4}=+0.016 {I17} 
$(753)(510)(|q): A{-2}=-0.07 {I2}, A{-4}=-0.01 {I3}, (753)(sum)(|q): A{-2}=-0.13 {I2}, A{-4}=-0.02 {I1}, POL=+0.16 {I8} (2003Ur02) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 2000Ur04 and 1996Be06 ({+248}Cm SF decay) 
M$from |a(K)exp=14 {I1} (2000Ur04). 
MR$from |a(K)exp 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (E2)
decay_comment:
M$stretched Q from |g|g(|q), most likely E2 
$A{-2}=+0.10 {I2}, A{-4}=-0.06 {I2} for 370-112 cascade 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1(+E2)
decay_comment:
M$stretched D from |g|g(|q), lin pol=-0.30 {I15} 
$A{-2}=+0.01 {I2}, A{-4}=-0.02 {I2} for 548-370 cascade 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$from |g|g(|q), lin pol=+0.20 {I10} 
$A{-2}=+0.12 {I4}, A{-4}=-0.04 {I4} for 682-(370+516) cascade 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (E2)
decay_comment:
$|g-|g(|q): A{-2}=-0.10 {I5}, A{-4}=0.00 {I5} 
No half-life longer than 10 ns was observed for 2891-kev level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
$|a(total) for 37.2 {I1} keV, as 36.7 keV is within 1 keV of L-shell binding energy 
M$(M1+E2) in 2021Zh57 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$I|g(580.1|g)+I|g(580.2|g) 
M$anisotropy ratio(|a)=1.5 {I2} for 580.1|g+580.2|g, anisotropy ratio(|b)=1.9 {I2}, RUL favors (E2) assignment 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
M$anisotropy ratio(|a)=1.6 {I2} for doubly placed 708|g, anisotropy ratio(|b)=1.5 {I1} for this transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI$I|g(726.2|g)+I|g(727|g)=99 {I8} 
M$anisotropy ratio(|a)=1.7 {I2} for 726.2|g+727|g, anisotropy ratio(|b)=1.6 {I1} for 727|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI$I|g(757|g)+I|g(757.1|g)=34 {I3} 
M$anisotropy ratio(|a)=2.0 {I3} for 757|g+757.1|g, anisotropy ratio(|b)=1.2 {I1} for 757|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI$I|g(757|g)+I|g(757.1|g)=34 {I3} 
M$anisotropy ratio(|a)=2.0 {I3} for 757|g+757.1|g, anisotropy ratio(|b)=1.4 {I3} for 757.1|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI$I|g(726.2|g)+I|g(727|g)=99 {I8} 
M$anisotropy ratio(|a)=1.7 {I2} for 726.2|g+727|g, anisotropy ratio(|b)=1.5 {I1} for 726.2|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI$I|g(894.0|g)+I|g(895|g)=52 {I4} 
M$anisotropy ratio(|a)=1.5 {I2} for 894.0|g+895|g, anisotropy ratio(|b)=1.2 {I1} for 894.0|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|a(L)exp=16.6 {I+30-23}, L:M=253 {I8}:60 {I5}. Evaluator assumes the L/M ratio could be much near to the theoretical value (33.7) than the presented value 4.6. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_comment:
$|a(K)exp=11.6 {I8}, |a(M)exp=0.86 {I9}, K/L=3.25 {I15}. Evaluator assumes |a(K)exp(81.2)=12.8, K/L(81.2)=3.59 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$evaluator assumes the DCO value given as 2.3 by 2000Mo16 is DCO(d) value because 225.6|g is parallel with 132.3 E1 gating |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$other: E|g=64.0 {I7}, I|g=15 {I2} from ({+28}Si,p4n|g) 
M$also supported by ce data in {+123}IT 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$others: 94.6 {I1} from {+123}Cs IT decay, 94.5 {I7} from ({+28}Si,p4n|g), 95.0 {I3} from ({+19}F,4n|g), and 94.7 {I3} from ({+10}B,3n|g) 
M$from ce data in {+123}Cs IT decay (1981Ma01,1972Dr06); also supported by ce data in {+123}Ba |e decay (2000Gi12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$others: 137.0 {I5} from ({+28}Si,p4n|g), 136.7 {I3} from ({+19}F,4n|g), and 136.9 {I3} from ({+10}B,3n|g) 
RI$others: 35 {I3} from ({+28}Si,p4n|g), and 49 {I4} from ({+19}F,4n|g) 
MR$from |g(|q) in ({+19}F,4n|g) (1992Hu02). Other: <0.6 from ce data in {+123}Ba |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$others: 201.0 {I5} from ({+28}Si,p4n|g), 200.7 {I3} from ({+19}F,4n|g), and 201.2 {I3} from ({+10}B,3n|g) 
RI$others: 100 {I5} from ({+28}Si,p4n|g), 100 {I7} from ({+19}F,4n|g) 
M$also supported by |g|g(DCO) in ({+28}Si,p4n|g) and |g(|q) in ({+19}F,4n|g) and ({+10}B,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$weighted average of 320.4 {I2} from ({+64}Ni,p4n|g), 321 {I1} from ({+34}S,3p|g), 320.6 {I5} from ({+28}Si,p4n|g), 320.6 {I2} from ({+19}F,4n|g), and 320.5 {I3} from ({+10}B,3n|g) 
M$also supported by |g(|q) in ({+10}B,3n|g) and ({+19}F,4n|g), and |g anisotropy in ({+34}S,3p|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$weighted average of 268.8 {I2} from ({+64}Ni,p4n|g), 269 {I1} from ({+34}S,3p|g), 268.9 {I5} from ({+28}Si,p4n|g), 269.0 {I2} from ({+19}F,4n|g), and 269.0 {I3} from ({+10}B,3n|g) 
M,MR$from |g(|q) in ({+19}F,4n|g) and RUL; |DJ=1 from |g|g(DCO) in ({+64}Ni,p4n|g) and ({+28}Si,p4n|g), and |g-anisotropy in ({+34}S,3p|g) Other: |d=|?0.2 from |g(|q) in ({+10}B,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$weighted average of 428.0 {I2} from ({+64}Ni,p4n|g), 428.2 {I5} from ({+28}Si,p4n|g), 428.3 {I2} from ({+19}F,4n|g), and 428.0 {I3} from ({+10}B,3n|g) 
M$also supported by |g(|q) in ({+10}B,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:
E$weighted average of 303.5 {I2} from ({+64}Ni,p4n|g), 304 {I1} from ({+34}S,3p|g), 303.5 {I5} from ({+28}Si,p4n|g), 303.7 {I3} from ({+19}F,4n|g), and 303.3 {I3} from ({+10}B,3n|g) 
RI$from ({+64}Ni,p4n|g). Others: 100 {I11} from ({+28}Si,p4n|g), 100 {I7} from ({+19}F,4n|g), 9.5 from ({+34}S,3p|g), 56 from ({+10}Be,3n|g) 
M,MR$from |g(|q) in ({+19}F,4n|g) and RUL; |DJ=1 from |g|g(DCO) in ({+64}Ni,p4n|g) and ({+28}Si,p4n|g), |g anisotropy in ({+34}S,3p|g). Other: |d|?+0.2 from |g(|q) in ({+10}Be,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$weighted average of 572.3 {I4} from ({+64}Ni,p4n|g), 572 {I1} from ({+34}S,3p|g), 572.4 {I7} from ({+28}Si,p4n|g), 572.4 {I3} from ({+19}F,4n|g), and 572.8 {I3} from ({+10}B,3n|g) 
RI$from ({+64}Ni,p4n|g). Others: 27 {I5} from ({+28}Si,p4n|g), <7 from ({+19}F,4n|g) 
M$also supported by |g(|q) in ({+10}Be,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 522.3 {I2} from ({+64}Ni,p4n|g), 522 {I1} from ({+34}S,3p|g), 522.3 {I5} from ({+28}Si,p4n|g), 522.5 {I2} from ({+19}F,4n|g), and 522.2 {I3} from ({+10}B,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 682.7 {I4} from ({+64}Ni,p4n|g), 682.7 {I5} from ({+28}Si,p4n|g), 682.7 {I3} from ({+19}F,4n|g), and 682.5 {I3} from ({+10}B,3n|g) 
M,MR$from |g(|q) in ({+19}F,4n|g); magnetic/electric character from level scheme. |DJ=1 from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 336.7 {I2} from ({+64}Ni,p4n|g), 337 {I1} from ({+34}S,3p|g), 336.9 {I5} from ({+28}Si,p4n|g), 336.9 {I3} from ({+19}F,4n|g), and 337.0 {I3} from ({+10}B,3n|g) 
M,MR$from |g(|q) in ({+19}F,4n|g); |DJ=1 from |g|g(DCO) in ({+64}Ni,p4n|g) and ({+28}Si,p4n|g), |g anisotropy in ({+34}S,3p|g). Other: |d|?+0.2 from |g(|q) in ({+10}Be,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 640.2 {I4} from ({+64}Ni,p4n|g), 642 {I1} from ({+34}S,3p|g), 640.5 {I5} from ({+28}Si,p4n|g), 640.5 {I3} from ({+19}F,4n|g), and 640.3 {I3} from ({+10}B,3n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g), supported by |g(|q) in ({+10}B,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 367.8 {I4} from ({+64}Ni,p4n|g), 368 {I1} from ({+34}S,3p|g), 368.0 {I5} from ({+28}Si,p4n|g), 367.9 {I3} from ({+19}F,4n|g), and 367.4 {I3} from ({+10}B,3n|g) 
RI$from ({+64}Ni,p4n|g) and ({+28}Si,p4n|g). Other: 100 {I25} from ({+19}F,4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 704.5 {I4} from ({+64}Ni,p4n|g), 706 {I1} from ({+34}S,3p|g), 704.5 {I5} from ({+28}Si,p4n|g), and 704.5 {I3} from ({+19}F,4n|g) 
RI$weighted average of 66 {I8} from ({+64}Ni,p4n|g), 67 {I7} from ({+28}Si,p4n|g), and 50 {I25} from ({+19}F,4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|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 685.5 {I2} from ({+64}Ni,p4n|g), 686 {I1} from ({+34}S,3p|g), 685.5 {I5} from ({+28}Si,p4n|g), 685.6 {I2} from ({+19}F,4n|g), and 685.2 {I3} from ({+10}B,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 570.0 {I6} from ({+64}Ni,p4n|g), 570.3 {I7} from ({+28}Si,p4n|g), and 570.0 {I3} from ({+19}F,4n|g) 
RI$weighted average of 30 {I5} from ({+64}Ni,p4n|g), 33 {I7} from ({+28}Si,p4n|g), and 40 {I20} from ({+19}F,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
E$weighted average of 730.4 {I4} from ({+64}Ni,p4n|g), 730.9 {I5} from ({+28}Si,p4n|g), 730.7 {I2} from ({+19}F,4n|g), and 730.2 {I3} from ({+10}B,3n|g) 
RI$from ({+64}Ni,p4n|g). Others: 100 {I11} from ({+28}Si,p4n|g), and 100 {I20} from ({+19}F,4n|g) 
M,MR$from |g(|q) in ({+10}B,3n|g) and RUL. |DJ=1 from |g|g(DCO) in ({+64}Ni,p4n|g) and ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 389.7 {I4} from ({+64}Ni,p4n|g), 389 {I1} from ({+34}S,3p|g), 389.5 {I7} from ({+28}Si,p4n|g), 389.5 {I3} from ({+19}F,4n|g), and 388.6 {I3} from ({+10}B,3n|g) 
RI$weighted average of 72 {I4} from ({+28}Si,p4n|g) and 97 {I10} from ({+64}Ni,p4n|g). Others: 100 {I50} from ({+19}F,4n|g), 200 from ({+34}S,3p|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 734.6 {I4} from ({+64}Ni,p4n|g), 734.9 {I7} from ({+28}Si,p4n|g), and 734.2 {I3} from ({+19}F,4n|g) 
RI$from ({+28}Si,p4n|g). Others: 102 {I20} from ({+64}Ni,p4n|g), 250 {I100} from ({+19}F,4n|g) seem discrepant 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 757.5 {I4} from ({+64}Ni,p4n|g), 757 {I1} from ({+34}S,3p|g), 757.5 {I5} from ({+28}Si,p4n|g), and 757.9 {I3} from ({+19}F,4n|g) 
RI$from ({+28}Si,p4n|g). Others: 100 {I12} from ({+64}Ni,p4n|g), 100 {I50} from ({+19}F,4n|g), 100 from ({+34}S,3p|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 398.6 {I4} from ({+64}Ni,p4n|g) and 398.4 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 159 {I33} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 743.5 {I4} from ({+64}Ni,p4n|g), 744.0 {I7} from ({+28}Si,p4n|g), and 743.2 {I3} from ({+19}F,4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I20} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 766.5 {I6} from ({+64}Ni,p4n|g) and 766.4 {I7} from ({+28}Si,p4n|g) 
RI$weighted average of 51 {I11} from ({+64}Ni,p4n|g) and 46 {I13} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 466.5 {I6} from ({+64}Ni,p4n|g), 466.9 {I7} from ({+28}Si,p4n|g), and 466.6 {I3} from ({+19}F,4n|g) 
RI$from ({+64}Ni,p4n|g). Others: 100 {I24} from ({+28}Si,p4n|g), and |?50 from ({+19}F,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 603.0 {I6} from ({+64}Ni,p4n|g), 603.0 {I7} from ({+28}Si,p4n|g), and 602.9 {I3} from ({+19}F,4n|g) 
RI$from ({+64}Ni,p4n|g). Others: 100 {I24} from ({+28}Si,p4n|g), and 100 {I50} from ({+19}F,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1196.9 {I6} from ({+64}Ni,p4n|g), 1198.0 {I7} from ({+28}Si,p4n|g), and 1197.7 {I3} from ({+19}F,4n|g) 
RI$from ({+64}Ni,p4n|g). Others: 118 {I24} from ({+28}Si,p4n|g), and |?50 from ({+19}F,4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 406.9 {I6} from ({+64}Ni,p4n|g) and 406.5 {I7} from ({+28}Si,p4n|g). 
RI$weighted average of 60 {I10} from ({+64}Ni,p4n|g) and 42 {I8} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 415.8 {I6} from ({+64}Ni,p4n|g), 415.4 {I7} from ({+28}Si,p4n|g), and 416.2 {I3} from ({+19}F,4n|g) 
RI$unweighted average of 60 {I10} from ({+64}Ni,p4n|g) and 25 {I8} from ({+28}Si,p4n|g). Other: |?50 from ({+19}F,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 805.5 {I6} from ({+64}Ni,p4n|g), 804.9 {I7} from ({+28}Si,p4n|g), and 805.7 {I3} from ({+19}F,4n|g) 
RI$from ({+64}Ni,p4n|g). Others: 100 {I21} from ({+28}Si,p4n|g), 100 {I50} from ({+19}F,4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 706.9 {I4} from ({+64}Ni,p4n|g), 706.6 {I5} from ({+28}Si,p4n|g), and 706.9 {I3} from ({+19}F,4n|g) 
RI$unweighted average of 52 {I6} from ({+64}Ni,p4n|g), 95 {I9} from ({+28}Si,p4n|g), and 67 {I34} from ({+19}F,4n|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|g) and ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 751.8 {I4} from ({+64}Ni,p4n|g), 751.9 {I5} from ({+28}Si,p4n|g), and 751.5 {I3} from ({+19}F,4n|g) 
RI$from ({+28}Si,p4n|g). Others: 100 {I11} from ({+64}Ni,p4n|g), 100 {I34} from ({+19}F,4n|g) 
M$D from |g|g(DCO) in ({+64}Ni,p4n|g) and ({+28}Si,p4n|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 800.5 {I2} from ({+64}Ni,p4n|g), 801 {I1} from ({+34}S,3p|g), 800.5 {I5} from ({+28}Si,p4n|g), 800.6 {I3} from ({+19}F,4n|g), and 800.1 {I3} from ({+10}B,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$weighted average of 1021.6 {I6} from ({+64}Ni,p4n|g) and 1022.2 {I7} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 410.8 {I6} from ({+64}Ni,p4n|g), 411.0 {I7} from ({+28}Si,p4n|g), and 410.5 {I3} from ({+19}F,4n|g) 
RI$unweighted average of 90 {I10} from ({+64}Ni,p4n|g) and 56 {I12} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 817.7 {I6} from ({+64}Ni,p4n|g) and 818.0 {I7} from ({+28}Si,p4n|g) 
RI$from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 826.6 {I6} from ({+64}Ni,p4n|g), 826.5 {I7} from ({+28}Si,p4n|g), and 826.7 {I3} from ({+19}F,4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I20} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 432.7 {I6} from ({+64}Ni,p4n|g) and 433.5 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I21} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 839.6 {I6} from ({+64}Ni,p4n|g) and 839.8 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 159 {I30} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 848.6 {I6} from ({+64}Ni,p4n|g) and 849.8 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I21} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 721.0 {I6} from ({+64}Ni,p4n|g), 720.9 {I7} from ({+28}Si,p4n|g), and 721.0 {I3} from ({+19}F,4n|g) 
RI$({+64}Ni,p4n|g). Others: 100 {I22} from ({+28}Si,p4n|g), 100 {I50} from ({+19}F,4n|g). 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1232.4 {I6} from ({+64}Ni,p4n|g), 1233.0 {I7} from ({+28}Si,p4n|g), and 1233.3 {I3} from ({+19}F,4n|g) 
RI$weighted average of 70 {I20} from ({+64}Ni,p4n|g) and 50 {I11} from ({+28}Si,p4n|g). Other: ?50 from ({+19}F,4n|g). 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$weighted average of 1288.5 {I4} from ({+64}Ni,p4n|g) and 1288.7 {I5} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 224.2 {I4} from ({+64}Ni,p4n|g) and 223.9 {I7} from ({+28}Si,p4n|g) 
RI$weighted average of 65 {I10} from ({+64}Ni,p4n|g) and 80 {I16} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
RI$from ({+64}Ni,p4n|g). Other: 100 {I20} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 742.0 {I4} from ({+64}Ni,p4n|g), 742.9 {I7} from ({+28}Si,p4n|g), and 741.4 {I3} from ({+19}F,4n|g) 
RI$from ({+28}Si,p4n|g). Others: 143 {I17} from ({+64}Ni,p4n|g), |?50 from ({+19}F,4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 790.7 {I4} from ({+64}Ni,p4n|g), 790.8 {I5} from ({+28}Si,p4n|g), and 791.0 {I3} from ({+19}F,4n|g) 
RI$from ({+28}Si,p4n|g). Others: 100 {I16} from ({+64}Ni,p4n|g), 100 {I20} from ({+19}F,4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 259.2 {I6} from ({+64}Ni,p4n|g) and 259.5 {I7} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I22} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 331.6 {I6} from ({+64}Ni,p4n|g) and 331.3 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g), normalized to I(259.3|g)=100. Other: 32 {I7} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 284.2 {I6} from ({+64}Ni,p4n|g) and 284.5 {I7} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 
RI$unweighted average of 76 {I10} from ({+64}Ni,p4n|g) and 156 {I31} from ({+28}Si,p4n|g), normalized to I(623.5|g)=100. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 356.5 {I6} from ({+64}Ni,p4n|g) and 356.0 {I7} from ({+28}Si,p4n|g) 
RI$unweighted average of 14 {I4} from ({+64}Ni,p4n|g) and 31 {I6} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 623.5 {I6} from ({+64}Ni,p4n|g) and 623.5 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I19} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|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 868.3 {I2} from ({+64}Ni,p4n|g), 869 {I1} from ({+34}S,3p|g), 868.4 {I5} from ({+28}Si,p4n|g), 868.3 {I3} from ({+19}F,4n|g), and 868.0 {I4} from ({+10}B,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 288.2 {I6} from ({+64}Ni,p4n|g) and 288.5 {I7} from ({+28}Si,p4n|g) 
RI$unweighted average of 19 {I4} from ({+64}Ni,p4n|g) and 36 {I8} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 313.2 {I4} from ({+64}Ni,p4n|g) and 313.0 {I7} from ({+28}Si,p4n|g) 
RI$weighted average of 90 {I11} from ({+64}Ni,p4n|g) and 96 {I20} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 644.7 {I4} from ({+64}Ni,p4n|g) and 644.5 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I20} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$weighted average of 1132.8 {I4} from ({+64}Ni,p4n|g) and 1133.1 {I7} from ({+28}Si,p4n|g) 
RI$weighted average of 65 {I11} from ({+64}Ni,p4n|g) and 60 {I12} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 811.5 {I6} from ({+64}Ni,p4n|g), 811.1 {I7} from ({+28}Si,p4n|g), and 811.4 {I3} from ({+19}F,4n|g) 
RI$from ({+64}Ni,p4n|g) and ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1243.4 {I6} from ({+64}Ni,p4n|g), 1243.2 {I7} from ({+28}Si,p4n|g), and 1243.8 {I3} from ({+19}F,4n|g) 
RI$weighted average of 50 {I13} from ({+64}Ni,p4n|g) and 88 {I18} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 377.1 {I4} from ({+64}Ni,p4n|g) and 377.3 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I19} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 690.3 {I4} from ({+64}Ni,p4n|g) and 690.3 {I7} from ({+28}Si,p4n|g) 
RI$weighted average of 74 {I9} from ({+64}Ni,p4n|g) and 69 {I15} from ({+28}Si,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 701.9 {I4} from ({+64}Ni,p4n|g), 701.5 {I7} from ({+28}Si,p4n|g), and 701.7 {I3} from ({+19}F,4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I24} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 828.2 {I6} from ({+64}Ni,p4n|g), 828.5 {I7} from ({+28}Si,p4n|g), and 828.4 {I3} from ({+19}F,4n|g) 
RI$weighted average of 68 {I11} from ({+64}Ni,p4n|g) and 94 {I18} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|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 904.9 {I2} from ({+64}Ni,p4n|g), 906 {I1} from ({+34}S,3p|g), 904.8 {I5} from ({+28}Si,p4n|g), and 904.63 {I3} from ({+19}F,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 413.0 {I6} from ({+64}Ni,p4n|g) and 413.4 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I24} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 790.1 {I6} from ({+64}Ni,p4n|g) and 790.8 {I7} from ({+28}Si,p4n|g) 
RI$unweighted average of 123 {I19} from ({+64}Ni,p4n|g) and 82 {I18} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 892.0 {I6} from ({+64}Ni,p4n|g), 891.9 {I7} from ({+28}Si,p4n|g), and 891.8 {I3} from ({+19}F,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 425.6 {I6} from ({+64}Ni,p4n|g) and 426.0 {I7} from ({+28}Si,p4n|g) 
RI$unweighted average of 64 {I12} from ({+64}Ni,p4n|g) and 32 {I11} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 838.6 {I6} from ({+64}Ni,p4n|g) and 839.4 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I21} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 817.8 {I4} from ({+64}Ni,p4n|g) and 818.0 {I5} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 675.5 {I6} from ({+64}Ni,p4n|g) and 675.8 {I7} from ({+28}Si,p4n|g) 
RI$from ({+64}Ni,p4n|g). Other: 100 {I24} from ({+28}Si,p4n|g) 
M$D from |g|g(DCO) in ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 878.5 {I6} from ({+64}Ni,p4n|g) and 878.0 {I7} from ({+28}Si,p4n|g) 
RI$weighted average of 89 {I14} from ({+64}Ni,p4n|g) and 65 {I12} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|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 955.8 {I2} from ({+64}Ni,p4n|g), 955 {I1} from ({+34}S,3p|g), 955.0 {I7} from ({+28}Si,p4n|g), and 955.5 {I3} from ({+19}F,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 888.4 {I4} from ({+64}Ni,p4n|g) and 889.0 {I7} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 971.8 {I6} from ({+64}Ni,p4n|g) and 972.1 {I7} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|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$unweighted average of 1025.9 {I2} from ({+64}Ni,p4n|g), 1026 {I1} from ({+34}S,3p|g), 1026.0 {I7} from ({+28}Si,p4n|g), and 1024.0 {I3} from ({+19}F,4n|g) 
RI$from ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 918.9 {I4} from ({+64}Ni,p4n|g) and 919.0 {I7} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+28}Si,p4n|g) and ({+64}Ni,p4n|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$weighted average of 1112.9 {I4} from ({+64}Ni,p4n|g), 1113 {I1} from ({+34}S,3p|g), and 1113.0 {I7} from ({+28}Si,p4n|g). Other: 1108 from ({+19}F,4n|g) 
RI$from ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 976.3 {I4} from ({+64}Ni,p4n|g) and 976.0 {I7} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|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$weighted average of 1206.8 {I4} from ({+64}Ni,p4n|g) and 1206 {I1} from ({+34}S,3p|g) 
RI$from ({+64}Ni,p4n|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1052.9 {I6} from ({+64}Ni,p4n|g) and 1053.2 {I7} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1188.3 {I6} from ({+64}Ni,p4n|g) and 1188.2 {I7} from ({+28}Si,p4n|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1371.0 {I6} from ({+64}Ni,p4n|g) and 1372 {I1} from ({+34}S,3p|g) 
M$Q from |g|g(DCO) in ({+64}Ni,p4n|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E$transition not observed, but expected from proposed decay scheme (1981Ma01). 
TI$from intensity balance 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$other: 63 (1972Dr06) 
RI$other: 345 {I+182-88} from I(95|g/62|g)=2.9 {I10} (1972Dr06) seems discrepant 
M$D or M1+E2 (|d|<0.47) from |a(L)exp<1.5 and intensity balance (1981Ma01) 
$I(ce(L))(64|g)/I(ce(K))(95|g)=1.6 {I5} (1972Dr06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 95.5 (1972Dr06) 
M$E2 from |a(K)exp=1.4 {I5}, |a(L)exp=0.6 {I1}, |a(M)exp=0.16 {I6} (1981Ma01), and K/L=2.5 {I10} (1972Dr06) 
$I(K x ray)/I(95|g)=2.5 {I6} (1972Dr06), 1.3 {I2} (1981Ma01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1978Bo32. Not seen in 2000Gi12 
RI$from I|g/I(K x-ray) ratios of 30.6|g and 63.97|g in 1978Bo32 and I(63.97|g)=16.6 {I1} in 2000Gi12 
$I(30.6|g)/I(K x-ray)=0.10 {I2} (1978Bo32). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$others: 64.1 {I5} from 1978Bo32, 63.9 {I6} (1975Ar31) 
RI$Other: 14 {I4} (1975Ar31) 
M$|a(K)exp=3.5 {I4}; K/L>9 
$I|g(63.9|g)/I(K x-ray)=0.025 {I5} (1978Bo32). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 94.5 {I6} (1975Ar31) 
RI$other: 100 (1975Ar31) 
M$E2 from Adopted Gammas, based on ce data in {+123}Cs IT decay; E2(+M1) proposed in 2000Gi12 based on |a(K)exp=1.2 {I1} and K/L=3 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$58.3 {I5} from 1978Bo32 
M$|a(L)exp=4.5 {I9}; K/L<1 
$I|g(58.3|g)/I(K x-ray)=0.004 {I1} (1978Bo32). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$other: 137.0 {I6} (1975Ar31) 
RI$other: 23 {I7} (1975Ar31) 
M$|a(K)exp=0.35 {I5}; K/L=8 {I2} 
MR$from Adopted Gammas. Other: |d<0.6 from ce data in 2000Gi12 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 320.5 {I3} (1992Hu02) and 320.7 {I2} (1992Dr05) 
M$Q from A{-2}=+0.297 {I28}, A{-4}=-0.043 {I45}; M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 303.8 {I3} (1992Hu02) and 303.6 {I4} (1992Dr05) 
M$A{-2}=-0.013 {I49}, A{-4}=+0.039 {I63} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from 1992Dr05. Other: 522.6 {I3} (1992Hu02) 
M$Q from A{-2}=+0.280 {I40}, A{-4}=-0.024 {I46}; M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 303.8 {I3} (1992Hu02) and 303.6 {I4} (1992Dr05) 
M$Q from A{-2}=+0.429 {I45}, A{-4}=+0.033 {I51}; M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 320.6 {I3} (1979Ga02) and 320.4 {I4} (1978Ti01). Other: 320.6 (1978Yo03) 
RI$other: 100 (1978Yo03) 
$A{-2}=+0.34 {I8}, A{-4}=-0.04 {I10} (1979Ga02) 
$A{-2}=+0.32 {I4} (1978Yo03) 
$A{-2}=+0.50 {I10}, A{-4}=-0.22 {I13} (1978Ti01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
E,RI$other: E|g=269.1, I|g=16 (1978Yo03) 
M,MR$A{-2}=+0.13 {I4}, A{-4}=+0.02 {I5} (1979Ga02) 
$A{-2}=+0.19 {I7} (1978Yo03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
E,RI$other: E|g=303.7, I|g=9 (1978Yo03) 
M,MR$A{-2}=+0.08 {I5}, A{-4}=-0.08 {I7} (1979Ga02) 
$A{-2}=+0.12 {I6} (1978Yo03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 522.2 {I3} (1979Ga02) and 522.3 {I4} (1978Ti01). Other: 522.4 (1978Yo03) 
RI$other: 71 (1978Yo03) 
$A{-2}=+0.35 {I4}, A{-4}=-0.08 {I5} (1979Ga02) 
$A{-2}=+0.36 {I4} (1979Ga02) 
$A{-2}=+0.38 {I3}, A{-4}=-0.10 {I4} (1978Ti01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
E,RI$other: E|g=337.0, I|g=7 (1978Yo03) 
M,MR$A{-2}=+0.03 {I4}, A{-4}=-0.02 {I6} (1979Ga02) 
$A{-2}=+0.15 {I7} (1978Yo03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 685.2 {I3} (1979Ga02) and 685.3 {I4} (1978Ti01). Other: 685.5 (1978Yo03) 
RI$other: 36 (1978Yo03) 
$A{-2}=+0.30 {I4}, A{-4}=-0.03 {I5} (1979Ga02) 
$A{-2}=+0.31 {I1} (1978Yo03) 
$A{-2}=+0.46 {I5}, A{-4}=-0.10 {I6} (1978Ti01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
E,RI$other: E|g=730.7, I|g=14 (1978Yo03) 
M$A{-2}=-0.60 {I5}, A{-4}=+0.17 {I9} (1979Ga02) 
$A{-2}=-0.51 {I3} (1978Yo03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 800.0 {I3} (1979Ga02) and 800.3 {I4} (1978Ti01). Other: 800.7 (1978Yo03) 
RI$other: 20 (1978Yo03) 
$A{-2}=+0.23 {I5}, A{-4}=-0.09 {I7} (1979Ga02) 
$A{-2}=+0.13 {I20} (1978Yo03) 
$A{-2}=+0.40 {I7}, A{-4}=+0.22 {I9} (1978Ti01) (A{-4}>0 inconsistent with |DJ=2) 


decay_energy_unit: KEV
decay_comment:
E$from 1978Ti01. Other: 870 from 1978Yo03 
RI$7 (1978Yo03) 
$A{-2}=+0.37 {I18} (1978Yo03) 
$A{-2}=+0.30 {I16}, A{-4}=+0.21 {I19} (1978Ti01) (A{-4}>0 inconsistent with |DJ=2) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E3)
decay_comment:
CC E3 CC(THEORY)'S MULT. BY 0.975 10 (Cf. 1990Ne01) 
RI from ce(K)(161|g)/ce(K)(65|g)=44 {I4}/4350 {I150} 
K/L=1.0 {I3} 
M from K/L 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
|a(K)exp=0.063 {I+5-4}, K/L=5.8 {I+26-14}, L/M=5.0 {I14} 
RI From the intensity in the figure in 1986We01. I|g=13.3 {I3} for a triplet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
RI From the intensity in the figure in 1986We01. I|g=0.64 {I4} for a doublet. 
|a(K)exp=0.96 {I+11-9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI From the intensity in the figure in 1986We01. I|g=1.69 {I15} for a doublet. 
|a(K)exp=0.23 {I3}, K/L=4.2 {I4} for a doublet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E complex line (1986We01). 
RI From the intensity (|?0.06) in the figure in 1986We01. I|g=0.17 {I4} for a doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI From the intensity in the figure in 1986We01. I|g=5.35 {I10} for a doublet 
|a(K)exp=0.25 {I1}, K/L=5.1 {I+27-14}, L/M>2.4 for a doublet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI From the intensity in the figure in 1986We01. I|g=0.29 {I3} for a doublet. 
|a(K)exp|?0.8, K/L|?7.1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI this |g is multiplet including 2+ to 0+ transition in {+124}Xe. Values are from authors' drawing. 


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_uncertain: ?
decay_comment:
E$From Table II in 2015Se17. From level scheme, |DE=463.5 and the |g transition is not shown in Fig. 1 (2015Se17) nor is it given in 2016KuZZ. Compilers have considered this transition as tentative. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
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_uncertain: S
decay_comment:
M Reduced transition probabilities are consistent only with mult=E2 or M2. The level scheme requires M2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M From Ice(85.4K)/Ice(140.9K)=17 {I4} (1987Fr10). |a(84.5K) |a(84.5K)=0.11+6-4 deduced from the ratio rules out all mults excepting E1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M From adopted gammas. A{-2}, A{-4} values suggest D+Q and |d=+24 {I2} which is inconsistent with (7/2+) to 3/2(+) transition. Long T{-1/2} of 266 level could result in large attenuation in |g(|q) through 13-keV transition. 
A{-2}=+0.115 {I13}, A{-4}=+0.019 {I16} (1991Hu09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
Placed by 1988Ma49 as deexciting the 43/2-member of yrast band. 2006Si16 place it from the 47/2-member of this band, with a 1002|g, not reported by 1988Ma49, being the 43/2- to 39/2-transition. 


decay_energy_unit: KEV
decay_uncertain: S
decay_comment:
E$The "*" marked for this gamma in Table 1 (2016Su14) indicating observed for the first time is a typo. Email reply from second author (Ying-Jun Ma) on 1 July, 2016 confirms this and state that the uncertainty for the unobserved 41|g was estimated based on uncertainties of 430.2, 1023.2, 648.3 , 1695.9 and 365.8 keV gamma transitions. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$R{-ADO}=1.37 {I19} 
E$Contaminated by the 478.1 |g in {+126}Cs and by the 475.6 and 480.3 |g transitions in {+125}Cs 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$R{-ADO}=0.81 {I8} 
E$Assigned as a transition from the 540 keV level in the Adopted Levels of {+125}Cs in the ENSDF database 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Transition was indicated as depopulating level 2554.8 which compilers believe was a typo and should instead be 2454.8 (Table 1, 2016Su14). In this XUNDL compilation with the least-squares fit to E|g data, the depopulating level is 2454.6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Transition was indicated as depopulating level 4685.3 which compilers believe was a typo and should instead be 4635.3 (Table 1, 2016Su14). In this XUNDL compilation with the least-squares fit to E|g data, the depopulating level is 4634.9 keV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$Clarification provided by second author (Ying-Jun Ma) in email reply on 1 July, 2016 that the 842|g placement in the level scheme is uncertain due to severe contamination from {+126}Cs and that the results from 2006Si16: Eur.Phys.J. A 27, 321 (2006) that its placement is immediately between the 832.6 and 871.5-keV |g transitions cannot be refuted. In 2016Su26 (which appears) the 842.8 transition is placed between the 832.6 and 871.5-keV gammas. 
$R{-ADO}=1.37 {I19} 


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:
RI from {+127}Cs IT decay 
M M2 from |a(exp)=0.93 {I10}, obtained by intensity balance in {+127}Cs IT decay. RUL also rules out E3. 


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:
|a(K)exp=3.6 {I3} if mult(72.8|g)=M1 (1977Pa10) 
M |a(K)exp gives E2(+M1) with |d>1.0. From transition intensity balance, |a(exp) in IT decay gives |d>1.2. From adopted J|p values, |DJ=2 is required 


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:
Ice(K)/Ice(L+M+N+)=6.8 {I7} (1987Fr10) 
|a(K)exp=0.5 {I1} and K/L=5.6 {I+19-15} normalized to |a(L)(66.3|g E2) 


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 from K/L (1987Fr10) 
|a(K)exp=0.14 {I3} and K/L=3.5 {I+14-10} normalized to |a(L)(66.3|g E2) 
Ice(K)/Ice(L+M+N+)=5.2 {I5} (1987Fr10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$given for doubly placed |g, and A{-2}, A{-4} and DCO values are also given 
$A{-2}=-0.36 {I6}, A{-4}=-0.15 {I5}; R(DCO)=0.24 {I3} 
M$from internal conversion coefficient based on intensity balance (1989Pa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=-0.33 {I4}, A{-4}=-0.08 {I5}; R(DCO)=0.34 {I3} 
M$from internal conversion coefficient based on intensity balance (1989Pa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$from internal conversion coefficient based on intensity balance (1989Pa09) 
$A{-2}=-0.14 {I4}, A{-4}=-0.11 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=-0.33 {I4}, A{-4}=-0.06 {I5}; R(DCO)=0.49 {I6} (2003Ko23) 
M$from internal conversion coefficient based on intensity balance (1989Pa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$from 1991Hi12 in in-beam |g-ray work. Others: 5.3 {I6} (2009Si08), 28 (1977Ch23) in in-beam |g-ray work seems discrepant. Values from the |e decay cannot be used since 420|g is doubly placed 


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:
RI$branching ratios are from in-beam |g-ray data where this level is populated more intensely than in |e decay. Values from |e decay are in general agreement 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [M4]
decay_uncertain: ?
decay_comment:
E$|g reported only by 1983TaZI in |e decay with an upper limit of intensity. It is neither seen in any other decay study (1972Ta02, 1973Is04) nor in in-beam |g-ray data; thus it is considered as questionable by the evaluators 


decay_energy_unit: KEV
decay_multipolarity: [E3]
decay_uncertain: ?
decay_comment:
E$|g not reported in in-beam |g-ray data; B(E3)(W.u.)=400 {I50} is a factor of 4 larger than RUL, thus this transition is considered suspect 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
RI$from {+122}Sn({+11}B,4n|g),{+124}Sn({+11}B,6n|g); doublet in |e decay with total intensity=18.9 {I10} 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
E$from ce(L2), ce(L3) measurements (1973Is04) relative to the ce(K) line of 182.32 {I5} |g. Other: 6.48 {i15} from differences of pairs |g-ray transitions feeding g.s. and 6.54-keV isomer (1972Ta02) 
TI$from total I|g+ce feeding this level from higher levels, no direct |e or |b feeding is expected due to J|p difference 
M$L3/L2=1.79 {I28} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$EG=129.1 1, IG=51 (1972Ta02); |?40 units of intensity are from {+129}Ba g.s. decay; remaining |?11 units of intensity are from isomer decay 
$EG=129.1, IG=14.3 (1973Is04) 
$EG=129.1, ICE(K)=42.0, K/|SL>5.6; K, L1, M1, N1 observed (1961Ar05) 
$EG=129.14 (1983TaZI) 
M$L1:L2:L3::100.0 {I26}:13.4 {I13}:5.4 {I11}. Other: K/|SL>5.6 (1961Ar05) gives |d(E2/M1)<0.5 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$EG=135.6 3, IG=8.0 (1972Ta02); |?6 units of intensity are from {+129}Ba g.s. decay; remaining |?2 units of intensity are from isomer decay 
$EG=135.6, IG=2.06 (1973Is04) 
$EG=135.7, ICE(K)=5.5, K/|SL>6.1; K, L1, M1 observed (1961Ar05) 
$EG=135.61 (1983TaZI) 
M,MR$from K/|SL>6.1 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$uncertainty based on |g intensity in isomer decay 
$EG=202.3 1, IG=39 (1972Ta02); |?38 units of intensity are from isomer decay 
$EG=202.4, IG=35.6 (1973Is04); mostly from isomer decay 
$EG=202.3, ICE(K)=25.5, K/|SL=6.9; K, L1 observed (1961Ar05) 
M$L1:L2:L3::100.0 {I44}:7.0 {I19}:4.5 {I16} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$EG=214.3 1, IG=87 (1972Ta02); |?78 units of intensity are from {+129}Ba g.s. decay; remaining |?9 units of intensity are from isomer decay 
$EG=214.3, IG=19.8 (1973Is04) 
$EG=214.2, ICE(K)=13.7, K/|SL=6.9; K, L1, M1 observed (1961Ar05) 
$EG=214.30 (1983TaZI) 
M$|a(K)exp=0.097 {I3}. Other: K/|SL=6.9 (1961Ar05) gives |d(E2/M1)<0.75 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
M,MR$from |a(K)exp AND K/|SL=6.7 (1961Ar05) 
$EG=220.8 1, IG=53 (1972Ta02); |?47 units of intensity are from {+129}Ba g.s. decay; remaining |?6 units of intensity are from isomer decay 
$EG=220.8, IG=13.1 (1973Is04) 
$EG=220.6, ICE(K)=6.5, K/|SL=6.7; K, L1, M1 observed (1961Ar05) 
$EG=220.83 (1983TaZI) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M$from |a(K)exp=0.035 (1961Ar05) 
$EG=333.9 7, IG=0.34 (1972Ta02) 
$EG=334.0, IG=0.95 (1973Is04) 
$EG=333.6, ICE(K)=0.23 (1961Ar05) 
$EG=333.9 (1983TaZI) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
M$from |a(K)exp=0.016 (1961Ar05) 
$EG=554.1 2, IG=15.5 (1972Ta02) 
$EG=553.9, IG=2.28 (1973Is04, unplaced) 
$EG=554.3, ICE(K)=0.25 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
M$from |a(K)exp=0.0024 (1961Ar05) 
$EG=1164.6 2, IG=8.8 (1972Ta02) 
$EG=1164.2, IG=1.83 (1973Is04, placed from 1812 level) 
$EG=1163.3, ICE(K)=0.03 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=1473.7 4, IG=1.4 (1972Ta02, placed from 1681 level). G not in 1916Ar05 
$EG=1472.9, IG=0.88 (1973Is04, placed from 1681 level) 
$EG=1473.6 (1983TaZI) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=1693.8 5, IG=0.25 (1972Ta02, unplaced). A 1693.8|g is placed also from 1701 level. G not in 1973Is04 
$EG=1694.3 (1983TaZI) 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
E$from ce(L2), ce(L3) (1973Is04) measurements relative to the ce(K) line of 182.32 {I5} |g. 
TI$from total I|g+ce feeding the 6.5-keV level, assuming no direct |e+|b{++} feeding 
M$L3/L2=1.79 {I28}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$EG=129.1 1, IG=51 (1972Ta02); |?40 units of intensity are from {+129}Ba g.s. decay; remaining |?11 units of intensity are from isomer decay 
$EG=129.1, IG=14.3 (1973Is04) 
$EG=129.1, ICE(K)=42.0, K/L>5.6; K, L1, M1, N1 observed (1961Ar05) 
M$L1:L2:L3=100.0 {I26}:13.4 {I13}:5.4 {I11}. Other: K/L>5.6 (1961Ar05) gives |d(E2/M1)<0.5 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$EG=135.6 3, IG=8.0 (1972Ta02); |?6 units of intensity are from {+129}Ba g.s. decay; remaining |?2 units of intensity are from isomer decay 
$EG=135.6, IG=2.06 (1973Is04) 
$EG=135.7, ICE(K)=5.5, K/L>6.1; K, L1, M1 observed (1961Ar05) 
M,MR$|a(K)exp=0.39, K/L>6.1 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$EG=53.2, IG=0.23 (1973Is04). 
$EG=53.2, ICE(K)=12.0, K/L=0.5; K, L1, L2, L3, M2, N2 observed (1961Ar05) 
M$L1:L2:L3=14.9 {I29}:81.9 {I42}:100 {I5}. Also E2 from K/L=0.5 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$EG=182.3 1, IG=100 (1972Ta02) 
$EG=182.3, IG=100 (1973Is04) 
$EG=182.3, ICE(K)=100, K/L=7.0; K, L1, M1 observed (1961Ar05) 
E$from ce data in 1973Is04. 
M$L1:L2:L3=100.0 {I9}:9.79 {I42}:5.41 {I39}. Other: K/L=7.0 (1961Ar05) gives |d(E2/M1)<0.5 
MR$0.32 {I5} if penetration effect is included (1973Is04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$EG=73.2, IG=0.21 (1973Is04) 
$EG=73.2, ICE(K)=3.0, K/L=5.5; K, L1, M1 observed (1961Ar05) 
M,MR$from |a(K)exp=2.1, K/L=5.5 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$EG=202.3 1, IG=39 (1972Ta02); |?38 units of intensity are from {+129}Ba isomer decay; remaining |?1 unit of intensity is from g.s. decay 
$EG=202.4, IG=35.6 (1973Is04) 
$EG=202.3, ICE(K)=25.5, K/L=6.9; K, L1 observed (1961Ar05) 
M$L1:L2:L3=100.0 {I44}:7.0 {I19}:4.5 {I16}. Other: K/L=6.9 (1961Ar05) gives |d(E2/M1)<0.7 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$EG=214.3 1, IG=87 (1972Ta02); |?78 units of intensity are from {+129}Ba g.s. decay; remaining |?9 units of intensity are from isomer decay 
$EG=214.3, IG=19.8 (1973Is04) 
$EG=214.2, ICE(K)=13.7, K/L=6.9; K, L1, M1 observed (1961Ar05) 
M$|a(K)exp=0.097 {I3}. Other: K/L=6.9 (1961Ar05) gives |d(E2/M1)<0.75 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$EG=220.8 1, IG=53 (1972Ta02); |?47 units of intensity are from {+129}Ba g.s. decay; remaining |?6 units of intensity are from isomer decay 
$EG=220.8, IG=13.1 (1973Is04) 
$EG=220.6, ICE(K)=6.5, K/L=6.7; K, L1, M1 observed (1961Ar05) 
M,MR$from |a(K)exp=0.073, K/L=6.7 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$EG=238.3 6, IG=1.6 (1972Ta02) 
$EG=237.7, IG=2.84 (1973Is04) 
$EG=237.4, ICE(K)=1.9, K/L=9; K line mixed with that of 202|g, L1 observed (1961Ar05) 
$EG=237.65 (1983TaZI) 
M$K/L=9, |a(K)exp=0.098 (1961Ar05); and |g(|q) in in-beam |g ray studies 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$total I|g=26.7 {I13} divided based on branching ratios in Adopted Gammas 
$EG=420.2 2, IG=25 (1972Ta02, placed only from 426 level 
$EG=419.8, IG=25.0 (1973Is04) 
$EG=419.5, ICE(K)=2.7, K/L=6.4; K, L1, M1 observed (1961Ar05) 
$EG=419.83 (1983TaZI) 
M$|a(K)exp=0.016, K/L=6.4 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
$EG=333.9 7, IG=0.34 (1972Ta02) 
$EG=334.0, IG=0.95 (1973Is04) 
$EG=333.6, ICE(K)=0.23 (1961Ar05) 
M$|a(K)exp=0.035 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$poor fit, level-energy difference=346.3 
$EG=345.3, IG=0.20 (1973Is04). G not in 1972Ta02, 1961Ar05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
RI$1.65 from 366 level and 0.50 from 575 level added 
$EG=366.4 2, IG=2.0 (1972Ta02, placed from 969 level) 
$EG=365.9, IG=1.94 (1973Is04) 
$EG=365.6, ICE(K)=0.35 (1961Ar05) 
$EG=365.86 (1983TaZI) 
M$|a(K)exp=0.026 (1961Ar05) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [M4]
decay_uncertain: ?
decay_comment:
RI$1983TaZI report |<2.7. |g not seen in 1972Ta02 and 1961Ar05. RI|<0.15 in 1973Is04. Based on decay data and in-beam |g-ray studies, the evaluators consider this |g ray either non-existent or very weak 


decay_energy_unit: KEV
decay_multipolarity: [E3]
decay_uncertain: ?
decay_comment:
E,RI$this |g is not reported in any of the three in-beam |g-ray studies, even though the 575, (11/2-) isomer is very strongly populated in these studies. It is possible that a small component of 366|g belongs in this location 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2)
decay_comment:
M$|a(K)exp=0.116 (1961Ar05) 
$EG=386.7, IG=0.43 (1973Is04). G not in 1972Ta02 
$EG=386.3, ICE(K)=0.34 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E3]
decay_comment:
RI$from branching in-beam |g-ray study (1977Ch23), where this |g is seen very weakly with only 7% branching ratio, consistent with its high multipolarity. In 1983TaZI, with I|g=1.19, branching is 34%. In 1972Ta02 this |g was not placed. Main component of this |g ray must belong somewhere else 
$EG=569.1 4, IG=2.2 (1972Ta02, unplaced) 
$EG=569.3, IG=1.32 (1973Is04). G not in 1961Ar05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$EG=176.9 3, IG=12 (1972Ta02) 
$EG=177.0, IG=7.69 (1973Is04) 
$EG=176.9, ICE(K)=6.6, K/L=7.0; K, L1 observed (1961Ar05) 
$EG=177.02 (1983TaZI) 
M$|a(K)exp=0.126, K/L=7.0 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=468.0 2, IG=2.8 (1972Ta02). G not in 1961Ar05 
$EG=467.8, IG=3.41 (1973Is04) 
$EG=475.2, ICE(K)=0.32; K, L1 observed (1961Ar05). Seems energy is is incorrectly quoted 
$EG=467.76 (1983TaZI) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
$EG=596.9 1, IG=16 (1972Ta02) 
$EG=596.8, IG=14.2 (1973Is04) 
$EG=597.0, ICE(K)=1.03, K/L=6; K, L, M observed (1961Ar05) 
$EG=596.78 (1983TaZI) 
M$|a(K)exp=0.0106, K/L=6 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$EG=459.6 2, IG=14 (1972Ta02) 
$EG=459.4, IG=13.8 (1973Is04) 
$EG=459.3, ICE(K)=1.2, K, L1 observed (1961Ar05) 
$EG=459.43 (1983TaZI) 
M$|a(K)exp=0.013 gives M1,E2 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
RI$total intensity of 1.80 {I9} based on branching ratios in Adopted Gammas 
$EG=264.0 4 (1972Ta02, unplaced but seen in |g|g coin) 
$EG=263.8, IG=1.69 (1973Is04) 
$EG=263.6, ICE(K)=0.72 (1961Ar05) 
$EG=263.78 (1983TaZI) 
MR$|a(K)exp=0.062 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$EG=481.6 2, IG=8.2 (1972Ta02) 
$EG=481.3, IG=8.24 (1973Is04) 
$EG=481.5, ICE(K)=0.91, K/L=6.3; K, L, M observed (1961Ar05) 
M$|a(K)exp=0.016, K/L=6.3 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$EG=501.4 4, IG=3.7 (1972Ta02) 
$EG=501.4, IG=4.68 (1973Is04) 
$EG=501.4, ICE(K)=0.42 (1961Ar05) 
$EG=501.38 (1983TaZI) 
M$|a(K)exp=0.013 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
$EG=328.4, IG=0.49 (1973Is04). G not in 1972Ta02 
$EG=328.2, ICE(K)=0.09 (1961Ar05) 
M$|a(K)exp=0.027 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$EG=534.6 3, IG=2.5 (1972Ta02) 
$EG=534.3, IG=2.55 (1973Is04) 
$EG=534.2, ICE(K)=0.20 (1961Ar05) 
M$|a(K)exp=0.011 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$EG=546.8 3, IG=10.5 (1972Ta02) 
$EG=546.4, IG=10.6 (1973Is04) 
$EG=546.6, ICE(K)=1.0, K/L=8; K, L observed (1961Ar05) 
M$|a(K)exp=0.014, K/L=8 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=566.1 3, IG=6.8 (1972Ta02) 
$EG=566.2, IG=2.14 (1973Is04) 
$EG=561.2, ICE(K)=0.48, K/L=8; K, L observed (1961Ar05). Seems energy is incorrectly quoted 
$EG=566.21 (1983TaZI) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
$EG=748.6 2, IG=6.8 (1972Ta02) 
$EG=748.5, IG=5.75 (1973Is04) 
$EG=748.5, ICE(K)=0.25 (1961Ar05) 
E$placement from 1972Ta02 and 1973Is04; not given in level-scheme figure 1 of 1983TaZI 
M$|a(K)exp=0.0064 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=744.9 4, IG=0.90 (1972Ta02, placed from a 1299 level) 
$EG=743.9, IG=0.19 (1973Is04). G NOT IN 1961Ar05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
$EG=872.5 1, IG=5.9 (1972Ta02, placed from a 1299 level) 
$EG=872.5, IG=4.67 (1973Is04) 
$EG=872.0, ICE(K)=0.13 (1961Ar05) 
M$|a(K)exp=0.0041 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
$EG=543.2 2, IG=4.2 (1972Ta02) 
$EG=542.6, IG=3.09 (1973Is04) 
$EG=543.0, ICE(K)=0.28 (1961Ar05) 
M$|a(K)exp=0.013 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
$EG=802.5 3, IG=5.9 (1972Ta02, placed from a 1451 level) 
$EG=803.0, IG=7.96 (1973Is04) 
$EG=802.4, ICE(K)=0.28 (1961Ar05) 
M$|a(K)exp=0.0051 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
$EG=285.7 9, IG=0.14 (1972Ta02, placed from a 1451 level) 
$EG=286.6, IG=0.66 (1973Is04) 
$EG=286.0, ICE(K)=0.12 (1961Ar05) 
M$|a(K)exp=0.027 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=700.6 3, IG=2.4 (1972Ta02, unplaced) 
$EG=700.6, IG=2.42 (1973Is04) 
$EG=700.3, ICE(K)=0.12, K/L=6; K, L observed (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
$EG=1035.1 3, IG=9.0 (1972Ta02) 
$EG=1034.6, IG=8.49 (1973Is04) 
$EG=1034.8, ICE(K)=0.14, K/L=7.4; K, L observed (1961Ar05) 
M$|a(K)exp=0.0024, K/L=7.4 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1973Is04; large uncertainty of 0.6 keV in 1972Ta02 
$EG=1047.6 6, IG=5.7 (1972Ta02) 
$EG=1047.1, IG=5.44 (1973Is04). G NOT IN 1961Ar05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$EG=392.4 4, IG=13 (1972Ta02) 
$EG=392.3, IG=21.3 (1973Is04) 
$EG=392.0, ICE(K)=3.5, K/L=8.0; K, L1 observed (1961Ar05) 
$EG=392.33 (1983TaZI) 
M$|a(K)exp=0.024, K/L=8.0 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=656.4 3, IG=4.5 (1972Ta02, placed from a 2144 level) 
$EG=656.1, IG=3.28 (1973Is04). G NOT IN 1961Ar05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$EG=678.9 1, IG=15 (1972Ta02) 
$EG=678.8, IG=12.6 (1973Is04) 
$EG=679.0, ICE(K)=0.65, K/L=6.5; K, L, M observed (1961Ar05) 
M$|a(K)exp=0.0075, K/L=6.5 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$EG=768.6 3, IG=2.8 (1972Ta02, placed from a 1459 level) 
$EG=769.0, IG=2.48 (1973Is04) 
$EG=768.5, ICE(K)=0.09 (1961Ar05) 
M$|a(K)exp=0.0053 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$EG=892.7 1, IG=21 (1972Ta02) 
$EG=892.6, IG=18.9 (1973Is04) 
$EG=892.4, ICE(K)=0.42, K/L=6.4; K, L observed (1961Ar05) 
M$|a(K)exp=0.0032, K/L=6.4 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=957.3 3, IG=5.4 (1972Ta02) 
$EG=957.7, IG=4.55 (1973Is04) 
$EG=956.7, ICE(K)=0.14, K/L=5; K, L observed (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=999.7 1, IG=7.9 (1972Ta02, placed from a 1208 level) 
$EG=999.4, IG=6.83 (1973Is04) 
$EG=1000.0, ICE(K)=0.15, K/L=6; K, L observed (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=1044.7 3, IG=16 (1972Ta02) 
$EG=1044.7, IG=17.0 (1973Is04) 
$EG=1044.7, ICE(K)=0.38, K/L=6.2; K, L observed (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=1073.0 4, IG=0.54 (1972Ta02, placed from a 1208 level) 
$EG=1072.7, IG=0.54 (1973Is04). G NOT IN 1961Ar05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=1221.8 1, IG=8.5 (1972Ta02) 
$EG=1221.6, IG=6.22 (1973Is04) 
$EG=1221.3, ICE(K)=0.07 (1961Ar05) 
M$|a(K)exp=0.0016 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=1459.3 1, IG=56 (1972Ta02) 
$EG=1459.1, IG=48.5 (1973Is04) 
$EG=1458.4, ICE(K)=0.44, K/L=6.3; K, L observed (1961Ar05) 
M$from |a(K)exp=4|*10{+-4} {I1} (in figure 7 of 1973Is04) suggests E1, but (M1,E2) from |a(K)exp=0.0013 and K/L=6.3 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$EG=426.7 4, IG=0.96 (1972Ta02) 
$EG=425.7, IG=1.19 (1973Is04) 
$EG=425.8, ICE(K)=0.15 (1961Ar05) 
M$|a(K)exp=0.018 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=689.4 2, IG=4.0 (1972Ta02) 
$EG=689.0, IG=1.86 (1973Is04) 
$EG=689.6, ICE(K)=0.20, K/L=6; K, L observed (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=712.2 3, IG=2.8 (1972Ta02) 
$EG=712.0, IG=2.38 (1973Is04) 
$EG=712.5, ICE(K)=0.15, K/L|?5; K, L observed (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=820.3 3, IG=4.2 (1972Ta02, placed from a 2076 level) 
$EG=820.7, IG=2.30 (1973Is04) 
$EG=819.6, ICE(K)=0.09 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=933.4 3, IG=2.8 (1972Ta02, placed from a 1487 level) 
$EG=933.1, IG=1.94 (1973Is04) 
$EG=933.0, ICE(K)=0.08 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=1122.4 2, IG=7.1 (1972Ta02) 
$EG=1122.2, IG=6.00 (1973Is04) 
$EG=1122.1, ICE(K)=0.08, K/L=6.2; K, L observed (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=1164.6 2, IG=8.8 (1972Ta02, G belongs mainly with 129BA GS decay) 
$EG=1164.2, IG=1.83 (1973Is04, G belongs mainly with 129BA GS decay) 
$EG=1163.3, ICE(K)=0.03 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=1209.2 2, IG=9.0 (1972Ta02) 
$EG=1209.0, IG=6.81 (1973Is04) 
$EG=1208.3, ICE(K)=0.08 (1961Ar05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$EG=1250.8 3, IG=1.9 (1972Ta02, placed from a 1459 level) 
$EG=1250.3, IG=1.22 (1973Is04) 
$EG=1252.0, ICE(K)=0.03 (1961Ar05) 


decay_energy_unit: KEV
decay_comment:
E$From figure 1 of 2005Si13; not listed in authors' tables 1 or 2. |DE|g=0.3 keV assumed by the compilers 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$questionable placement on the base of energy relations only; mult.=D,E2 from RUL is inconsistent with |DJ|p=2, yes 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|d=0.52 {I3} (1969Fe02) 
$K:L1:L2:L3=44.3 {I9}:5.24 {I11}:1.62 {I5}:1.42 {I5} (1975Mo12) 
$Possible B(E0)/B(E2)=0.015 {I5} (1978Vo11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 496.321 {I12} (1980VyZZ), 496.326 {I13}, (1982KhZW), 496.30 {I1} (1990Su07), 496.326 {I5} (2003Sa62). Other: 496.280 {I16} (1995Ku32) 
$A{-2}=-0.001 {I2}, A{-4}=+0.001 {I3}, |g(lin pol) P{-1}(90|')=+0.012 {I16} (1969Fe02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$questionable placement on the base of energy relations only; |g from J|p=11/2- to J|p=7/2+ have to be of mult.=M2 that is unlikely 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 534.4 {I3} (2005Ku10) and 538.0 {I5} (1997FuZY). Other: 536.7 {I5} (1979Ga01) 
M$DCO=1.02 {I8}; A{-2}=+0.20 {I5}, A{-4}=-0.03 {I6}$ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
M$DCO=0.40 {I6}; A{-2}=-0.56 {I3}, A{-4}=0.02 {I4} 
MR$from (1979Ga01), mult.=M1 has been set by 2005Ku01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
M$DCO=0.34 {I9}; A{-2}=-0.44 {I4}, A{-4}=-0.11 {I8} 
MR$from (1979Ga01), mult.=M1 has been set by 2005Ku01 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
E$placement from figure 1 in 2008Si26, the placement shown in authors' Table I from 4386 level seems a misprint 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$K:L1:L2:L3:M1:M2:M3:N1:N2+= 100:12.9 {I4}:1.94 {I6}:1.44 {I5}:3.0 {I2}:0.56 {I7}:0.37 {I5}: 0.64 {I5}:0.08 {I3} averages of 1961Br09, 1961Er04, 1964Si21 and 1969Fr04 (evaluated by 1982KhZW). |a(K)=1.43 {I4}, weighted average of |a(K)exp=1.39 {I6} (1961Er04) and 1.46 {I5} (1970Av01) (absolute K| x ray and |g-ray counting) 
MR$Others: 0.161 {I9} calculated by evaluators using the BrIccMixing program from shell intensities cited 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$K:L1:L2:L3=0.57 {I7}:0.060 {I8}:|<0.009:|<0.009 (1969Fr04) 
MR$Others: <0.16 (1969Fr04); 0.14 {I3} calculated by evaluators with BrIccMixing program from known shell intensities 
RI$average of 0.8 {I1} (1961Er04) and 1.6 {I7} (1968Al16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from branching ratio in adopted gammas. Others: 0.242 {I25} (1992Ma05), 0.109 {I10} (1961Er04) and 0.174 {I9} (1968Al16) 
M$ce(K)=0.025 {I6} (1980VyZZ) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from branching ratio in adopted gammas. Others: 0.0004 {I4} (1961Er04), 0.00065 {I61} (1968Al16) and 0.00044 {I18} (1992Ma05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$unweighted average of 0.0123 {I12} (1992Ma05), 0.0135 {I4} (1961Er04) and 0.0193 {I7} (1968Al16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$from branching ratio in adopted gammas. Others: 0.00090 {I4} (1992Ma05), 0.00618 {I19} (1961Er04) and 0.0062 {I9} (1961Er04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$K:L1:L2:L3=100 {I4}:12.8 {I8}:1.93 {I14}:1.43 {I11} 
MR$Others: 0.169 (1986Po04); -0.151 {I2} from |g|g(|q); penetration parameter |l(M1)=6.5 {I23} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2(+E0)
decay_comment:
ce(K)(E0)/ce(K)(E2)|<0.3 (1982Si17) 
$K:L1:L2:L3=100 {I7}:12.6 {I4}:1.5 {I3}:0.98 {I23} 
MR$Others: 0.171 (1985Po04); -0.03 {I3} from |g|g(|q); penetration parameter |l(M1)=4 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$K:L1:L2:L3=100 {I3}:9.6 {I9}:4.9 {I5}:4.6 {I4} 
MR$Others: +1.28 {I13} from |g|g(|q); penetration parameter |l(M1)=4 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$K:L1:L2=100 {I19}:10.1 {I3}:1.4 {I5} 
MR$-0.15 {I+6-5} from |g|g(|q); penetration parameter |l(M1)=7 {I7} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$uncertainty of 0.3 in Table 1 of 2018Xu08 seems too low to be realistic. Compiler has increased it by a factor of 10 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$uncertainty of 0.2 in Table 1 of 2018Xu08 seems too low to be realistic. Compiler has increased it by a factor of 10 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$uncertainty of 0.1 in Table 1 of 2018Xu08 seems too low to be realistic. Compiler has increased it by a factor of 10 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$I|g(abs)=62.4 {I7} 
$I(ceK)=100, I(ceL)=17.1 {I11}, 3.5 {I6} 
$|a{-K}(theory)=0.0211 is assumed in 2021De18 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from the intensity balance 
M,MR$M1:M2:M3=1.0:0.131 {I8}:0.084 {I11}, M1:N1:O1:P1=4.38 {I19}:1.0:0.162 {I9}: <0.0068 (1973MaVM) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
$K:L1:L2:L3=1.89 {I5}:0.176 {I6}:1.03 {I1}:1.0, M1:M2:M3:M45:N:L3=0.034 6:0.258 {I4}:0.216 {I3}:0.0053 {I8}:0.105 {I4}:1.0 (1973Ma68) 


decay_energy_unit: KEV
decay_multipolarity: E3
decay_comment:
EKC$ from measured I(K x ray)/I|g(127.5)=2.6609 {I4}} (2007Ni04), measured I(K x ray)/I|g(165.9|g in {+139}La)=0.2419 {I8}} (2008Ni02), and theoretical |a{-K}}=0.2229 {I3}} for 165.9|g in {+139}La. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
TI$from intensity balance 
M$assuming a cascade of 413-105-keV transitions, intensity balance is consistent only with an E2 transition for the 105|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
$|a(M+N)=0.0031 {I11}, K/L=4.0 {I6}, L/(M+N)=4.0 {I15} (2011Wi09) 
M$from experimental conversion coefficients and subshell ratios 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
RI$in spectra gated by transitions belonging to the complementary fragment, the uncertainty on I|g(66|g) is very large; no value provided by 2013As05. 
ECC$from intensity balance 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from supplemental material. Text mentions a 104.8 {I3} transition. 
RI$total intensity, delayed intensity is 4.7 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$(487|g)(1184|g)(|q): R(22|')=1.19 {I9}, R(46|')=1.07 {I8}, R(75|')=1.00 {I6} consistent with |DJ=2, quadrupole (E2) and |DJ=2, quadrupole (E2) cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$(222|g)(1184|g)(|q): R(22|')=0.93 {I7}, R(46|')=0.99 {I6}, R(75|')=1.00 {I5} consistent with |DJ=1, dipole and |DJ=2, quadrupole (E2) cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$(890|g)(1184|g)(|q): R(22|')=1.09 {I9}, R(46|')=1.07 {I7}, R(75|')=1.00 {I6} consistent with |DJ=2, quadrupole (E2) and |DJ=2, quadrupole (E2) cascade 
$(890|g)(487|g)(|q): R(22|')=1.20 {I8}, R(46|')=1.08 {I7}, R(75|')=1.00 {I4} consistent with |DJ=2, quadrupole (E2) and |DJ=2, quadrupole (E2) cascade 


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$from {+138}Cs IT decay 
M$T{-1/2}=2.91 min requires Mult=M3 or E3; M3 (|a(K)=119, calculated using the BrIcc program) would account for observed K x-ray intensity in {+138}Cs IT decay (1971Ca21) whereas E3 (|a(K)=12.5) would not 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M3)
decay_comment:
E$1971Ca21 assign 79.9|g as the isomeric transition on the basis that it is the only |g seen in {+138}Cs (2.91 min) decay and not seen in the decay of {+138}Cs g.s. 
RI$1971Ca21 measure I|g(79.9|g)/I|g(1436|g in {+138}Ba)=0.020 {I5} 
M$T{-1/2}=2.91 min requires Mult=M3 or E3 if the 79.9|g is the isomeric transition; M3 (|a(K)=119, calculated using the BrIcc program) would account for observed K x-ray intensity whereas E3 (|a(K)=12.5 from BrIcc) would not (1971Ca21). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$from 1972Mo33 
TI$from |g+ce intensity imbalance at ground state assuming no g.s. |b feeding. The total |g+ce feeding to g.s. from levels above 10.86 keV is 37.4% {I15} with total relative I(|g+ce)=1096 {I22}, leaving the rest 62.6% {I15} feeding to be accounted for by |g+ce intensity of this transition. 
RI$deduced from I(|g+ce) and |a(total). 
M$from L1:L2:L3=100:7 {I2}:1.5 {I10} (1972Mo33) and |a(L)=150 {I70} (1973Ac01) based on X(L)/|g. (authors' value in 1973Ac01 is obtained using |w(L)=0.143 from 1970Ma01 (Appendix III). 
M$In previous evaluation (2003So13,1976Pa04), it states that the recommended |w(L)=0.11, which is indicated from 1972Bb16. But 1972Bb16 give no recommended |w(L) and only list measured |w(L)=0.089(13) for Cs element. It is seen in the same table that a value of |w(L)=0.11 is for Xe element. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$from 1972Mo33 
TI$from intensity balance at 10.9 and 15.8 levels. The combined |b feeding to 10.9 and 15.8 level is 7.1% {I26} from intensity balances. 
RI$deduced from I(|g+ce) and |a(total) 
M$from ce(M1)/ce(M2)>11 (1972Mo33). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from 1979Bo26 
RI$2013Xi08 measured absolute emission probability=34.9 {I10}, 1972Mo33 report 32.5 {I15}. 
M$|a(K)exp=0.056 {I5} (1973Ac01), 0.058 {I20} (1972Mo33) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$observed by 1973Ac01, difficult to detect due to {+138}Cs contaminant, this g.s. feeding |g-ray helps to define J|p(412)=1- and M(401)=M1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$from 1979Bo26 
RI$2013Xi08 measured absolute emission probability=22.2 {I6} 
M$|a(K)exp=0.015 {I2} (1973Ac01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
M$|g|g(|q) consistent with M1 for 174.5|g and E2 for 1156.9|g 
$(1156.9|g)(174.5|g)(|q): A{-2}=-0.07 {I1}, A{-4}=-0.02 {I2} (quoted by 2007Li21 from a paper to be published; ref 26 in 2007Li21). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$M1+E2 or M1,E2 from |a(exp) deduced from intensity balance. 
$(185.5|g)(1156.9|g)(|q): A{-2}=-0.076 {I23}; A{-4}=0.007 {I34} (2010Li03) consistent with M1,E2-E2 cascade and 10- --> 9- --> 7- spin sequence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR$-4.2 {I+4-5} or -0.07 {I2} from |g|g(|q) (2009Li42), shell-model predicted value of -3.6 favors higher value. From RUL, large |d(Q/D) is consistent with M1+E2 rather than E1+M2, assuming level half-life is less than 10 ns 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$|a(K)exp=0.079 {I25} is too large for M1 and E2, barely overlaps M2 or E3 
CC$deduced from |a(K)exp 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (M1+E2)
decay_comment:
M$from total conversion coefficient deduced from intensity balance considerations in |g|g-coincidence analysis in {+252}Cf SF decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$1972Ac02 suggest M2,E3, but |a(K)=0.519 for M2 and 0.515 for E3 barely overlap the experimental value. High value of |a(K)exp may be due to E0 admixture in the 356.7 transition 
CC$deduced from |a(K)exp 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_uncertain: ?
decay_comment:
M,MR$M1(+E2), |d|<0.5 {I3} or E1(+M2), |d|<0.28 {I6} from I(|g+ce) and I|g. 
TI$|<15.4 {I14} from intensity balancing at the 2064 level and |>4.0 {I11} from |a(E1)=1.096 and I|g. 
ECC$upper limit from I(|g+ce) and I|g; lower limit from |a(E1)=1.105. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
TI$|<51.2 {I18} from intensity balancing at the 2186 level and |>1.4 {I5} from |a(E1)=0.134 and I|g. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (M1+E2)
decay_comment:
M$from total conversion coefficient deduced from intensity balance considerations in |g|g-coincidence analysis (2009Li42) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2,M1)
decay_comment:
$|DJ=1 for 454.7|g, |DJ=2 for 594.3|g from (454.7|g)(594.3|g)(|q): A{-2}=-0.09 {I3}, A{-4}=-0.01 {I4} 
MR$ +0.07 {I+14-13} or +4.4 {I+60-18} (2010Li10) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$|DJ=2 (probable E2) for 594.3|g and 640.9|g from (640.9|g)(594.3|g)(|q): A{-2}=+0.096 {I17}, A{-4}=-0.005 {I25} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M |a(K)exp=1.8 {I5} (1981Ot02), |a(K)exp=1.20 {I19} (1974Ad08); 1981Ot02 quote K/L+M=0.30 {I25}, which appears to be a misprint 
E 80.109 {I3} (1979Bo26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M |a(K)exp(103.9|g+104.52|g)=0.66 {I10}; K/L=3.2 {I6} (1981Ot02); |a(K)exp(103.9|g+104.52|g)=0.87 {I12} (1974Ad08) 
E 103.080 {I4} (1979Bo26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
M |a(K)exp=0.70 {I10}; K/L=12.0 {I7} (1981Ot02); |a(K)exp=0.74 {I9} (1974Ad08) 
MR from M1(<45%E2) (1981Ot02); other: E2(|?40%M1) (1974Ad08) 
E 112.606 {I4} (1979Bo26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M |a(K)exp(103.9|g+104.52|g)=0.66 {I10}; K/L=3.2 {I6} (1981Ot02); |a(K)exp(103.9|g+104.52|g)=0.87 {I12} (1974Ad08) 
E 104.398 {I3} (1979Bo26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M |a(K)exp=0.67 {I10}; K/L=13 {I7} (1981Ot02); |a(K)exp=0.50 {I6} (1974Ad08) 
E 118.310 {I3} (1979Bo26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+(E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E 211.887 {I20} (1979Bo26) 
M |a(K)exp=0.14 {I3}, K/L=3.8 {I8} (1981Ot02); |a(K)exp=0.134 {I20} (1974Ad08) 
MR M1(<29%E2) (1981Ot02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
M |a(K)exp=0.17 {I3}; K/L=3.2 {I6} (1981Ot02); | a(K)exp=0.17 {I3} (1974Ad08) 
MR E2(+|?25%M1) (1981Ot02) 
E 167.092 {I10} (1979Bo26; two |g's with same energy and uncertainty, possible typographical error) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2,M1)
decay_comment:
M |a(K)exp=0.0024 {I7}; |a(K)exp is consistent with E1 for |g from 1427 keV level, and M1,E2 for |g from 653 keV level (1974Ad08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M |a(K)exp=0.0024 {I7}; |a(K)exp is consistent with E1 for |g from 1427 keV level, and M1,E2 for |g from 653 keV level (1974Ad08) 
RI analysis of |g-|g coin (1981Ot02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
The discrepancy between T{-1/2} for 89.9|g in {+141}Xe |b decay (T{-1/2}<2.1 ns) and in {+252}Cf SF decay (T{-1/2}=12 ns) suggests that this |g may be a doublet in SF decay with unknown placement of T{-1/2}=12 ns component. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E E|g=68.994 is reported by 1979Bo26; however, 1988Fa06, on the basis of cascade and crossover sums, conclude that this transition is misassigned 
M from balance of I(69|g) and I(119|g) in |g|g and fact that 119|g is M1+(E2) (1988Fa06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M |a(K)exp=0.20 {I8} from which 1976Ot03 adopted M1,E2 while E1(+M2) is a better match (not adopted because it would contradict parity conservation) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(exp) from intensity balance consistent with mult=M1+E2 (2004Ur01); |DJ=2 transition given in table I of 2004Ur01 seems a misprint since negative A{-2} is expected for |DJ=1 transition; A{-2}=-0.10 {I3}, A{-4}=+0.07 {I4} for (105|g)(283|g)(|q) (2004Ur01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$|DJ=0,1 transition from A{-2}=-0.07 {I2}, A{-4}=+0.06 {I4} for (389|g)(473|g)(|q) (2004Ur01); A{-2}=-0.090 {I11}, A{-4}=-0.014 {I17} (2010Lu02, same cascade) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|DJ=2 transition from A{-2}=+0.101 {I9}, A{-4}=+0.013 {I14} for (481.0|g)(369.7|g)(|q) (2010Lu02), and from A{-2}=+0.09 {I2}, A{-4}=-0.04 {I2} for (481|g)(370|g)(|q) (2004Ur01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|DJ=2 transition from A{-2}=+0.105 {I12}, A{-4}=+0.023 {I19} for (632.2|g)(481.0|g)(|q) (2010Lu02), and from A{-2}=+0.10 {I2}, A{-4}=-0.07 {I4} for (632|g)(summed |g)(|q) (2004Ur01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|DJ=2 transition from A{-2}=+0.105 {I21}, A{-4}=+0.03 {I3} for (626.5|g)(473.4|g)(|q) (2010Lu02), and A{-2}=+0.08 {I2}, A{-4}=-0.04 {I4} for (626|g)(summed |g)(|q) (2004Ur01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$ |DJ=0,1 transition from A{-2}=-0.08 {I4}, A{-4}=+0.05 {I6} for (452.6|g)(626.5|g)(|q) (2010Lu02), and A{-2}=-0.06 {I2}, A{-4}=+0.04 {I4} for (453|g)(626|g)(|q) (2004Ur01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$|DJ=1, D transition from A{-2}=-0.11 {I3}, A{-4}=0.00 {I4} for (603.9|g)(632.2|g)(|q) (2010Lu02); other: A{-2}=-0.07 {I2}, A{-4}=+0.01 {I3} for (604|g)(summed |g)(|q) (2004Ur01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|DJ=2 transition from A{-2}=+0.095 {I14}, A{-4}=+0.017 {I21} for (648.4|g)(632.2|g)(|q) (2010Lu02), and A{-2}=+0.11 {I3}, A{-4}=-0.03 {I3} from (648|g)(summed |g)(|q) (2004Ur01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$(M1+E2) is proposed in 2009Rz02 from ambiguous results of angular correlation measurements. E2 from |g|g(|q) in 2010Li14 is also preferable due to the systematics of J|p's values. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
M$A{-2} and A{-4} for (90|g)(282|g)(|q) suggest E1,M1. However, multipolarity should be E2 from level scheme. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (M1+E2)
decay_comment:
M$ M1 or E2 from I(x ray)/I|g |? 7 in {+248}Cm SF decay, when gated on ce(L)(49|g), but pure E2 assignment is excluded from intensity balance considerations, thus M1+E2 is most likely 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$ placement is preferred here from {+252}Cf SF decay due to somewhat better statistics in double-gated coincidence spectra. In {+248}Cm SF decay, this |g is placed as 405-474-535 cascade 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (M1+E2)
decay_comment:
M$ M1 or E2 from I(x ray)/I|g |? 7, when gated on L-conversion line of 49-keV transition, but pure E2 assignment is excluded from intensity balance considerations, thus M1+E2 is most likely 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$E|g=195.9, I|g=100 in {+107}Ag({+19}F,4n|g), E|g=197, I|g=100 in {+108}Cd({+16}O,2n|g) 
M I(0|')/I(90|')|?1.2 (1974Co36); RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
$E|g=512.9, I|g=61 in {+107}Ag({+19}F,4n|g), E|g=513 in {+108}Cd({+16}O,2n|g) 
M I(0|')/I(90|')|?1.2 (1974Co36) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$I|g(1216.7)/I|g(415.2)=35.0 {I12}/100.0 in {+112}Sn({+12}C,2n|g); E|g=1122.8, I|g=5.8 in {+107}Ag({+19}F,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q(+O)
decay_comment:
$I|g(435.6)/I|g(938.5)=40.2 {I7}/100.0 {I7} in {+112}Sn({+12}C,2n|g); E|g=435.1, I|g=4.5 in {+107}Ag({+19}F,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$I|g(785.3)/I|g(540.7)=28.5 {I9}/100.0 {I12} in {+112}Sn({+12}C,2n|g); E|g=784.9, I|g=2.6 in {+107}Ag({+19}F,4n|g) 
M$from DCO (2001Zh22) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q(+O)
decay_comment:
$E|g=735.4, I|g=12 in {+107}Ag({+19}F,4n|g); E|g=745 was shown in decay scheme only in {+112}Sn({+12}C,2n|g), but E|g differs 10 keV from other reactions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$weighted average of 92.5 {I3} from {+123}La |e decay, 92.5 {I2} from ({+19}F,3np|g), and 92.7 {I1} from ({+12}C,3n|g) 
M$D from |g|g(DCO) in ({+19}F,3np|g); (E1) from level scheme. Other: (D+Q) from |g(|q) in ({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 153.6 {I3} from {+123}La |e decay and 153.6 {I5} from ({+19}F,3np|g) 
M$M1,E2 from ce data in {+123}La |e decay; D from |g|g(DCO) in ({+19}F,3np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 169.0 {I3} from {+123}La |e decay, 169.0 {I2} from ({+19}F,3np|g), and 169.6 {I10} from ({+12}C,3n|g) 
M$D from |g|g(DCO) in ({+19}F,3np|g); (M1) from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
E$weighted average of 109.8 {I3} from {+123}La |e decay, 109.8 {I2} from ({+19}F,3np|g), and 110.0 {I1} from ({+12}C,3n|g) 
M$(D+Q) from |g(|q) in ({+12}C,3n|g) and |g|g(DCO) in ({+19}F,3np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
E$weighted average of 133.2 {I3} from {+123}La |e decay, 133.3 {I2} from ({+19}F,3np|g), and 133.3 {I10} from ({+12}C,3n|g) 
RI$other: 100 {I13} from {+123}La |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 243.1 {I3} from {+123}La |e decay and 243.1 {I5} from ({+19}F,3np|g) 
RI$also from {+123}La |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
E$weighted average of 205.2 {I3} from {+123}La |e decay, 205.2 {I2} from ({+19}F,3np|g), and 205.3 {I2} from ({+12}C,3n|g) 
M$from |g(|q) in ({+12}C,3n|g) and |g|g(DCO) in ({+19}F,2np|g) 
RI$other: 100 {I8} from ({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 374.3 {I3} from {+123}La |e decay and 374.2 {I5} from ({+19}F,3np|g) 
RI$unweighted average of 42 {I4} from {+123}La |e decay and 53.2 {I12} from ({+19}F,3np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 243.9 {I3} from {+123}La |e decay and 243.4 {I2} from ({+19}F,3np|g) 
M$M1,E2 from ce data in {+123}La |e decay; (E2) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
E$weighted average of 246.7 {I3} from {+123}La |e decay, 246.7 {I2} from ({+19}F,3np|g), and 247.0 {I3} from ({+12}C,3n|g) 
RI$others: 100 {I8} from {+123}La |e decay, 100 {I14} from ({+12}C,3n|g) 
M$from |g(|q) in ({+12}C,3n|g) and |g|g(DCO) in ({+19}F,2np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 380.0 {I3} from {+123}La |e decay, 380.0 {I2} from ({+19}F,3np|g), and 380.1 {I10} from ({+12}C,3n|g) 
RI$weighted average of 71 {I8} from {+123}La |e decay and 61 {I3} from ({+19}F,3np|g). Other: 123 {I24} from ({+12}C,3n|g) is in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
E$weighted average of 238.4 {I3} from {+123}La |e decay, 237.7 {I2} from ({+19}F,3np|g), and 238.1 {I3} from ({+12}C,3n|g) 
RI$weighted average of 86 {I10} from {+123}La |e decay and 94 {I5} from ({+19}F,3np|g) 
M$from |g(|q) in ({+12}C,3n|g) and |g|g(DCO) in ({+19}F,2np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 443.5 {I3} from {+123}La |e decay and 442.9 {I2} from ({+19}F,3np|g) 
RI$other: 100 {I10} from {+123}La |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
E$weighted average of 174.2 {I2} from ({+19}F,3np|g) and 174.4 {I10} from ({+12}C,3n|g) 
RI$other: |?20 in ({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 380.0 {I2} from ({+19}F,3np|g) and 380.1 {I10} from ({+12}C,3n|g) 
RI$other: 123 {I24} from ({+12}C,3n|g) is in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$weighted average of 554.2 {I2} from ({+19}F,3np|g) and 553.7 {I6} from ({+12}C,3n|g) 
RI$other: 100 {I17} from ({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 188.9 {I5} from ({+19}F,3np|g) and 189.1 {I10} from ({+12}C,3n|g) 
RI$from ({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 568.9 {I2} from ({+19}F,3np|g) and 569.0 {I6} from ({+12}C,3n|g) 
RI$from ({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$E2 or M1+E2 from |a{-K}(exp); M1 mixing was estimated to be 0 or very small on the basis of Weisskopt hindrance factor for the measured T{-1/2} (1991Ii02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|a(K)exp=0.016 {I4} 
Ice(K) deduced after subtraction of Ice(L) of the 421.5-keV transition. 
M From adopted gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
|a(K)exp=0.0026 {I6} 
M From adopted gammas. 1992Id01 assigned M1, but M1 assignment contradicts the mult.=Q assignment in {+64}Ni({+64}Ni,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
|a(K)exp=0.0055 {I12} 
M From adopted gammas. 1992Id01 assigned E1, but the assignment contradicts the spin assignment of {+64}Ni({+64}Ni,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) and linear polarization (1988Ma49): A{-2}=+0.26 {I4}, A{-4}=-0.35 {I10}, pol=0.46 {I9} in {+96}Zr({+34}S,6n|g), A{-2}=+0.41 {I3} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.2533 {I23}, A{-4}=-0.038 {I4} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=1.06 {I2}, A{-2}=-0.22 {I2} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from |g(|q) and linear polarization (1988Ma49): A{-2}=+0.30 {I5}, A{-4}=-0.15 {I5}, pol=0.47 {I9} in {+96}Zr({+34}S,6n|g), A{-2}=+0.31 {I2} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.321 {I3}, A{-4}=-0.050 {I4} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=1.03 {I2}, A{-2}=-0.24 {I2} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=0.00 {I5}, A{-4}=-0.13 {I8} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.95 {I13} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from I(643.4|g)/I(873.3|g)=1.6 {I5}/0.7 {I3} in {+111}Cd({+16}O,3n|g) (1989Ko19); other: I|g=0.4 from I(642.7|g)/I(872.5|g)=2.3/0.6 in {+110}Cd({+16}O,2n|g) (1990Pi11) 
A{-2}=+0.06 {I5}, A{-4}=-0.04 {I7} in {+110}Cd({+16}O,3n|g) (1989Ko19) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g=1.1 for 509.9|g+510.9|g doublet (1990Pi11) 
A{-2}=+0.15 {I3}, A{-4}=+0.02 {I4} in {+110}Cd({+16}O,3n|g) (1989Ko19) DCO=1.12 {I14} and A{-2}=-0.07 {I4} for 509.9|g+510.9|g in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.17 {I20} in {+110}Cd({+18}O,4n|g) (1988Ma49) DCO=0.78 {I17} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from |g(|q) and linear polarization (1988Ma49): A{-2}=+0.23 {I2} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.314 {I3}, A{-4}=-0.071 {I4} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.92 {I4}, A{-2}=-0.07 {I4} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g=3.7 for 451.4|g+452.0|g doublet (1990Pi11) 
A{-2}=0.36 {I3} for a complex peak in {+110}Cd({+18}O,4n|g) (1988Ma49) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
A{-2}=+0.11 {I2} in {+110}Cd({+18}O,4n|g) (1988Ma49) A{-2}=+0.15 {I3}, A{-4}=-0.11 {I4} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.87 {I9}, A{-2}=-0.20 {I2} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
RI from I(444.4|g)/I(1020.8|g)=1.1/3.7 in {+110}Cd({+16}O,2n|g) (1990Pi11) 
A{-2}=+0.54 {I6}, A{-4}=+0.19 {I9} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.96 {I15} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_comment:
Observed in coincidence with 345 keV and (326 keV or 312 keV) |g. Intensity is not given. Uncertainty of energy is given by evaluator. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.35 {I15} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.15 {I3}, A{-4}=-0.08 {I5} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=1.12 {I16} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI from I(534.4|g)/I(629.7|g)=3.0 {I2}/3.2 {I6} in {+111}Cd({+16}O,3n|g) (1989Ko19); other: I|g=0.4 from I(533.2|g)/I(629.6|g)=3.0/0.6 in {+110}Cd({+16}O,2n|g) (1990Pi11) 
A{-2}=-0.4 {I4} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=-0.02 {I4}, A{-4}=+0.09 {I5} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.89 {I12} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
A{-2}=-0.08 {I6} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=0.89 {I18} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M from |g(|q) and linear polarization (1988Ma49): A{-2}=-0.45 {I10}, A{-4}=+0.4 {I3}, pol=0.37>in {+96}Zr({+34}S,6n|g), A{-2}=-0.25 {I12} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=-0.19 {I4}, A{-4}=+0.06 {I6} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.55 {I7}, A{-2}=+0.18 {I13} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=0.28 {I2} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.280 {I6}, A{-4}=-0.064 {I9} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.95 {I8}, A{-2}=-0.25 {I2} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_comment:
Observed in coincidence with 345 keV and 326 keV |g. Intensity is not given. Uncertainty of energy is given by evaluator. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
A{-2}=+0.31 {I20} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.35 {I9}, A{-4}=+0.09 {I13} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.91 {I21} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M from |g(|q) and linear polarization (1988Ma49): A{-2}=-0.41 {I10}, A{-4}=0.0 {I2}, pol=0.62 {I25} in {+96}Zr({+34}S,6n|g), A{-2}=-0.23 {I6} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=-0.238 {I19}, A{-4}=+0.03 {I3} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.56 {I5}, A{-2}=+0.22 {I5} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI from I(354.0|g)/I(942.4|g)=0.7/1.6 in {+110}Cd({+16}O,2n|g) (1990Pi11) 
A{-2}=+0.23 {I5} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=1.10 {I18} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
A{-2}=+0.26 {I11} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=-0.10 {I7}, A{-4}=-0.11 {I11} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.83 {I17} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
A{-2}=-0.23 {I23} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=0.8 {I3} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
A{-2}=-0.3 {I3} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=0.73 {I23} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.81 {I8}, A{-4}=-0.09 {I11} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=1.10 {I14}, A{-2}=-0.20 {I3} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
RI from I(612.2|g)/I(1056.6|g)=3.6/1.4 in {+110}Cd({+16}O,2n|g) (1990Pi11) 
DCO=1.0 {I3} in {+110}Cd({+16}O,2n|g) (1990Pi11) A{-2}=+0.22 {I9}, A{-4}=+0.20 {I13} in {+110}Cd({+16}O,3n|g) (1989Ko19) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.38 {I7}, A{-4}=-0.16 {I10} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=1.22 {I14} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
A{-2}=-0.5 {I3} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=-0.50 {I4}, A{-4}=+0.08 {I6} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.31 {I4}, A{-2}=+0.52 {I5} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
A{-2}=+0.43 {I18} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.25 {I4}, A{-4}=+0.03 {I6} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=1.06 {I7}, A{-2}=-0.21 {I8} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g=4.6 for 555.7|g+555.9|g doublet (1990Pi11). 
DCO=1.07 {I20} for 555.7|g+555.9|g in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI composite line. Other components were not given by authors. 
DCO=0.46 {I8} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
RI from I(288.1|g)/I(385.7|g)=0.6/2.0 in {+110}Cd({+16}O,2n|g) (1990Pi11) 
DCO=0.35 {I12}, A{-2}=+0.34 {I5} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI from I(385.7|g)/I(789.3|g)=2.0/0.9 in {+110}Cd({+16}O,2n|g) (1990Pi11) 
DCO=0.55 {I16} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.33 {I3} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.295 {I10}, A{-4}=-0.108 {I15} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.95 {I5}, A{-2}=-0.29 {I2} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
A{-2}=-0.30 {I7} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=-0.390 {I4}, A{-4}=+0.002 {I5} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.53 {I4}, A{-2}=+0.19 {I3} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.53 {I13} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.28 {I3}, A{-4}=-0.09 {I4} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=1.07 {I4}, A{-2}=-0.22 {I3} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g=0.9 for 442.9|g+444.4|g doublet (1990Pi11) 
DCO=0.94 {I8} for 442.9|g+444.4|g in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g=5.7 for 781.2|g+781.3|g doublet (1990Pi11) 
A{-2}=+0.22 {I3}, A{-4}=-0.10 {I5} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.89 {I15} for 781.2|g+781.3 in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.39 {I8} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.325 {I18}, A{-4}=0.00 {I3} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.96 {I6}, A{-2}=-0.21 {I3} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M from |g(|q) and linear polarization (1988Ma49) 
Pol=+0.36 {I15} in {+96}Zr({+34}S,6n|g), A{-2}=-0.35 {I7} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=-0.203 {I14}, A{-4}=+0.037 {I21} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.58 {I5}, A{-2}=+0.28 {I4} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
A{-2}=-0.35 {I19} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=-0.639 {I3}, A{-4}=+0.072 {I4} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.45 {I4}, A{-2}=+0.25 {I2} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.21 {I18} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=1.18 {I23} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g=3.7 for 451.4|g+452.0|g doublet (1990Pi11) 
DCO=1.25 {I19} and A{-2}=-0.19 {I2} for 451.4|g+452.0|g in {+110}Cd({+16}O,2n|g) (1990Pi11) A{-2}=+0.39 {I9} in {+110}Cd({+18}O,4n|g) (1988Ma49) A{-2}=+0.333 {I10}, A{-4}=-0.025 {I16} in {+110}Cd({+16}O,3n|g) (1989Ko19) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from |g(|q) and linear polarization (1988Ma49): 
A{-2}=+0.18 {I6}, A{-4}=-0.02 {I8}, pol=0.50 {I19} in {+96}Zr({+34}S,6n|g), A{-2}=+0.26 {I4} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.288 {I15}, A{-4}=-0.064 {I22} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.96 {I6}, A{-2}=-0.13 {I2} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
A{-2}=-0.15 {I19} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.30 {I4}, A{-4}=+0.09 {I6} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.89 {I22} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.34 {I3} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.271 {I14}, A{-4}=-0.070 {I21} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.91 {I6}, A{-2}=-0.30 {I3} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI composite line. Other components were not given by authors. 
A{-2}=+0.42 {I3} for a complex line in {+110}Cd({+18}O,4n|g) (1988Ma49) DCO=1.09 {I8}, A{-2}=-0.08 {I3} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
A{-2}=+0.20 {I15} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=0.98 {I13} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=-0.07 {I3} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=1.07 {I14} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=-0.20 {I7} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=0.62 {I9} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from |g(|q) and linear polarization (1988Ma49): pol=+0.52 {I18} in {+96}Zr({+34}S,6n|g), A{-2}=+0.28 {I8} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.194 {I25}, A{-4}=-0.11 {I4} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.91 {I13}, A{-2}=-0.20 {I2} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI composite line. Other components were not given by authors. 
M from |g(|q), |g|g(|q), DCO and linear polarization (1988Ma49) 
A{-2}=+0.32 {I4}, A{-4}=-0.30 {I5}, pol=+0.58 {I18} in {+96}Zr({+34}S,6n|g), A{-2}=+0.27 {I3} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.42 {I3}, A{-4}=-0.05 {I4} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=1.08 {I9}, A{-2}=-0.26 {I2} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.30 {I15} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=0.90 {I23} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=-0.21 {I12} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=0.69 {I20} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.25 {I6} in {+110}Cd({+18}O,4n|g) (1988Ma49); A{-2}=+0.22 {I3}, A{-4}=+0.08 {I5} in {+110}Cd({+16}O,3n|g) (1989Ko19); DCO=0.82 {I17}, A{-2}=-0.36 {I7} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.15 {I3} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=0.95 {I18}, A{-2}=-0.26 {I3} in {+110}Cd({+16}O,2n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g=5.7 for 781.2|g+781.3|g doublet (1990Pi11) 
A{-2}=+0.15 {I6} in {+110}Cd({+18}O,4n|g) (1988Ma49) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=+0.16 {I3} in {+110}Cd({+18}O,4n|g) (1988Ma49); DCO=1.09 {I13} in 94Zr({+34}S,4n|g) (1990Pi11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
-1.97|<|d|<-1.46 or -0.46|<|d|<-0.29 
A{-2}=-0.48 {I4}, A{-4}=-0.04 {I6} (1978Gi08) 
M From |g(|q) and |a(K)exp in {+125}La |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
-2.25|<|d|<-0.274 
A{-2}=-0.592 {I16}, A{-4}=0.067 {I14} (1978Gi08); A{-2}=-0.19 {I2} (1988Ma49) 
M From |g(|q) and |a(K)exp in {+125}La |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
-2.71|<|d|<-2.29 or -0.23|<|d|<-0.176 
A{-2}=-0.59 {I4}, A{-4}=0.05 {I4} (1978Gi08) 
M From |g(|q) and |a(K)exp in {+125}La |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
-4.00|<|d|<-1.94 or -0.38|<|d|<-0.12 
A{-2}=-0.34 {I5}, A{-4}=0.02 {I5} (1978Gi08); A{-2}=-0.34 {I9} (1988Ma49) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI Multiply placed, undivided intensity given 
A{-2}=-0.01 {I4}, A{-4}=-0.08 {I5} (1978Gi08); A{-2}=-0.13 {I3} (1988Ma49) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
-2.84|<|d|<-1.88 or -0.42|<|d|<-0.10 
A{-2}=-0.39 {I5}, A{-4}=-0.04 {I8} (1978Gi08); -0.71 {I10} (1988Ma49) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
|a(K)exp<0.0058. Authors assigned multipolarity of E2, but this assignment is not consitent with |a(K)(E2)=0.00659. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|a(K)exp=0.0250 {I23} for 312.5K+313.3K 
MR from |g(|q) in (HI,xn|g), other: -0.8 {I+1-11} or -1.7 {I+10-2} (2002Ko02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 108 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20); (100) in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
Spin orientation ratio=1.43 {I3} (1991Wa20); A{-2}=+0.199 {I4}, A{-4}=-0.036 {I7}, pol.=+1.41 {I4} (1976Fl11); A{-2}=+0.245 {I10}, A{-4}=-0.081 {I14} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 100 in ({+34}S,4n) at 155 MeV (1991Wa20); 97 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=1.01 {I5}, spin orientation ratio=1.41 {I5} (1991Wa20); A{-2}=+0.273 {I6}, A{-4}=-0.078 {I11}, pol.=+1.62 {I5} (1976Fl11); A{-2}=+0.299 {I18}, A{-4}=-0.08 {I3} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI other: 2.9 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
M from adopted gammas 
MR from 1987Sc14; others: 1>(1991Wa20), +5.1 {I+10-20} (1993LuZX) 
DCO=0.66 {I4}, spin orientation ratio=1.02 {I5} (1991Wa20); A{-2}=+0.106 {I18}, A{-4}=-0.13 {I3} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI other: 1.0 {I3} in ({+34}S,4n) at 155 MeV (1991Wa20). 
M from adopted gammas 
MR from 1993LuZX 
DCO=0.9 {I1} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 86 {I4} in ({+34}S,4n) at 155 MeV (1991Wa20); 72 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=1.00 {I5}, spin orientation ratio=1.47 {I6} (1991Wa20); A{-2}=+0.286 {I11}, A{-4}=-0.032 {I17}, pol.=+1.50 {I4} (1976Fl11); A{-2}=+0.332 {I12}, A{-4}=-0.102 {I16} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
RI other: 4 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20). 
M from adopted gammas 
MR other: >+4.1 (1993LuZX) 
DCO=0.74 {I4}, spin orientation ratio=0.86 {I4} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 4.8 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.95 {I6}, spin orientation ratio=1.46 {I6} (1991Wa20); A{-2}=+0.30 {I4}, A{-4}=-0.16 {I5} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI others: 9 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20); 6 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=0.63 {I4}, spin orientation ratio=0.85 {I5} (1991Wa20); A{-2}=-0.25 {I4}, A{-4}=+0.11 {I12}, pol.=+0.72 {I21} (1976Fl11); A{-2}=+0.18 {I5}, A{-4}=+0.04 {I7} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI other: 1.5 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
M from adopted gammas 
MR from 1987Sc14 
DCO=0.37 {I3}, spin orientation ratio=0.55 {I4} (1991Wa20); A{-2}=-0.68 {I13}, A{-4}=+0.24 {I18} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI other: 4.6 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=1.1 {I6}, spin orientation ratio=1.6 {I2} (1991Wa20); A{-2}=+0.45 {I7}, A{-4}=+0.07 {I11} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 62 {I4} in ({+34}S,4n) at 155 MeV (1991Wa20); 46 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=0.99 {I5}, spin orientation ratio=1.46 {I6} (1991Wa20); A{-2}=+0.271 {I17}, A{-4}=-0.064 {I2}, pol.=+1.44 {I7} (1976Fl11); A{-2}=+0.348 {I17}, A{-4}=-0.106 {I20} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI other: 4.6 {I8} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.69 {I3}, spin orientation ratio=1.28 {I7} (1991Wa20); A{-2}=+0.29 {I12}, A{-4}=+0.07 {I20} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI others: 19 {I2} in ({+34}S,4n) at 155 MeV (1991Wa20); 15 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=0.56 {I3}, spin orientation ratio=0.77 {I4} (1991Wa20); A{-2}=-0.20 {I2}, A{-4}=-0.01 {I3}, pol.=+1.14 {I10} (1976Fl11); A{-2}=-0.273 {I15}, A{-4}=+0.04 {I4} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 1.3 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=1.18 {I5}, spin orientation ratio=1.63 {I8} (1991Wa20); A{-2}=+0.21 {I4}, A{-4}=-0.08 {I6} (1987Sc14) 


decay_energy_unit: KEV
decay_comment:
RI 1991Wa20 gives I|g=5.0 {I5} for the 469.2+469.4|g's. other: 4.5 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.52 {I3}, spin orientation ratio=0.84 {I4} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
RI other: 2.0 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
MR other: +0.01 {I10} (1987Sc14). 
DCO=0.65 {I4}, spin orientation ratio=0.80 {I4} (1991Wa20); A{-2}=-0.17 {I5}, A{-4}=-0.02 {I6} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 2.4 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.94 {I5}, spin orientation ratio=1.45 {I7} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI other: 1.8 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.33 {I3}, spin orientation ratio=0.58 {I4} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 6 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=1.03 {I5}, spin orientation ratio=1.02 {I5} (1991Wa20); A{-2}=+0.18 {I4}, A{-4}=-0.09 {I5} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI other: 7 {I2} in ({+34}S,4n) at 155 MeV (1991Wa20). 
MR other: -0.07 {I4} (1987Sc14). 
DCO=0.45 {I5}, spin orientation ratio=0.77 {I4} (1991Wa20); A{-2}=-0.40 {I3}, A{-4}=-0.01 {I4} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 16 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20); 21 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=1.01 {I5}, spin orientation ratio=1.30 {I6} (1991Wa20); A{-2}=+0.29 {I2}, A{-4}=-0.01 {I4}, pol.=+1.34 {I18} (1976Fl11); A{-2}=+0.35 {I3}, A{-4}=-0.13 {I4} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI others: 15 {I2} in ({+34}S,4n) at 155 MeV (1991Wa20); 9 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=0.54 {I3}, spin orientation ratio=0.78 {I4} (1991Wa20); A{-2}=-033 {I3}, A{-4}=+0.05 {I5}, pol.=+1.38 {I20} (1976Fl11); A{-2}=+0.34 {I4}, A{-4}=-0.01 {I7} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI other: 7 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20). 
MR other: -1.0 {I5} (1987Sc14). 
DCO=0.34 {I4}, spin orientation ratio=0.65 {I4} (1991Wa20); A{-2}=-0.55 {I4}, A{-4}=+0.03 {I6} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 45 {I4} in ({+34}S,4n) at 155 MeV (1991Wa20); 29 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=0.98 {I5}, spin orientation ratio=1.45 {I6} (1991Wa20); A{-2}=+0.28 {I2}, A{-4}=-0.04 {I3}, pol.=+1.44 {I10} (1976Fl11); A{-2}=+0.321 {I20}, A{-4}=-0.06 {I3} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI other: 4 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20). 
MR other: -1.5 {I+12-7} (1987Sc14). 
DCO=0.33 {I4}, spin orientation ratio=0.63 {I4} (1991Wa20); A{-2}=-0.64 {I7}, A{-4}=+0.09 {I7} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 2.6 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.98 {I5} (1991Wa20); A{-2}=+0.56 {I16}, A{-4}=+0.23 {I24} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 6.3 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=1.16 {I6}, spin orientation ratio=1.29 {I6} (1991Wa20); A{-2}=+0.33 {I4}, A{-4}=-0.05 {I6} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 4 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=1.06 {I7} (1991Wa20); A{-2}=+0.38 {I9}, A{-4}=+0.01 {I12} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI others: 2.0 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20); (4) in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=0.52 {I3}, spin orientation ratio=0.82 {I4} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 26 {I3} in ({+34}S,4n) at 155 MeV (1991Wa20); 17 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=1.00 {I5}, spin orientation ratio=1.41 {I6} (1991Wa20); A{-2}=+0.32 {I2}, A{-4}=-0.11 {I3}, pol.=+1.9 {I3} (1976Fl11); A{-2}=+0.34 {I5}, A{-4}=-0.09 {I7} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI other: 3.1 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.30 {I3}, spin orientation ratio=0.57 {I4} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI other: 1.0 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.32 {I4}, spin orientation ratio=0.58 {I4} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 5.2 {I8} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.99 {I5}, spin orientation ratio=1.29 {I5} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 30 {I2} in ({+34}S,4n) at 155 MeV (1991Wa20); 18 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=1.02 {I5}, spin orientation ratio=1.40 {I6} (1991Wa20); A{-2}=+0.34 {I5}, A{-4}=-0.11 {I7}, pol.=+1.62 {I21} (1976Fl11); A{-2}=+0.38 {I5}, A{-4}=-0.07 {I6} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 6.5 {I10} in ({+34}S,4n) at 155 MeV (1991Wa20); 7 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=0.98 {I5}, spin orientation ratio=1.60 {I8} (1991Wa20); A{-2}=+0.27 {I10}, A{-4}=-0.10 {I12}, pol.=+1.43 {I20} (1976Fl11); A{-2}=+0.35 {I6}, A{-4}=-0.04 {I8} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 23 {I3} in ({+34}S,4n) at 155 MeV (1991Wa20); 11 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=1.00 {I5}, spin orientation ratio=1.44 {I5} (1991Wa20); A{-2}=+0.46 {I5}, A{-4}=-0.22 {I6}, pol.=+1.8 {I3} (1976Fl11); A{-2}=+0.28 {I6}, A{-4}=+0.04 {I7} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 4 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=1.22 {I7}, spin orientation ratio=1.57 {I9} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI other: 4 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.96 {I9}, spin orientation ratio=1.3 {I1} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 26 {I3} in ({+34}S,4n) at 155 MeV (1991Wa20); 12 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=0.99 {I5}, spin orientation ratio=1.39 {I6} (1991Wa20); A{-2}=+0.35 {I5}, A{-4}=-0.13 {I7}, pol.=+1.44 {I14} (1976Fl11); A{-2}=+0.35 {I4}, A{-4}=-0.11 {I6} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 6 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.98 {I7}, spin orientation ratio=1.27 {I6} (1991Wa20); A{-2}=+0.43 {I13}, A{-4}=-0.13 {I19} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 13 {I2} in ({+34}S,4n) at 155 MeV (1991Wa20); 9 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=1.09 {I6}, spin orientation ratio=1.44 {I6} (1991Wa20); A{-2}=+0.44 {I10}, A{-4}=-0.05 {I15}, pol.=+2.3 {I8} (1976Fl11); A{-2}=+0.35 {I11}, A{-4}=-0.14 {I16} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 20 {I3} in ({+34}S,4n) at 155 MeV (1991Wa20); 9 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=1.06 {I5}, spin orientation ratio=1.44 {I6} (1991Wa20); A{-2}=+0.40 {I9}, A{-4}=-0.26 {I15}, pol.=+1.37 {I23} (1976Fl11); A{-2}=+0.42 {I12}, A{-4}=-0.24 {I18} (1987Sc14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 5 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.91 {I7}, spin orientation ratio=1.21 {I6} (1991Wa20) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 1.3 {I2} in ({+34}S,4n) at 155 MeV (1991Wa20). 
Spin orientation ratio=1.37 {I7} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI other: 10 {I2} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=1.06 {I8}, spin orientation ratio=1.48 {I6} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI others: 19 {I3} in ({+34}S,4n) at 155 MeV (1991Wa20); 4 in ({+16}O,4n|g) at 83 MeV (1976Fl11). 
DCO=0.91 {I9}, spin orientation ratio=1.45 {I7} (1991Wa20); A{-2}=+0.27 {I17}, A{-4}=-0.02 {I25}, pol.=+1.2 {I3} (1976Fl11) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 2.0 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=0.95 {I15}, spin orientation ratio=1.32 {I6} (1991Wa20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 13 {I2} in ({+34}S,4n) at 155 MeV (1991Wa20). 
DCO=1.04 {I15}, spin orientation ratio=1.59 {I8} (1991Wa20) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 11.5 {I2} in ({+34}S,4n) at 155 MeV (1991Wa20). 
Spin orientation ratio=1.49 {I7} (1991Wa20) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 4.5 {I5} in ({+34}S,4n) at 155 MeV (1991Wa20). 
Spin orientation ratio=1.61 {I8} (1991Wa20) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI other: 4.5 {I1} in ({+34}S,4n) at 155 MeV (1991Wa20). 
Spin orientation ratio=1.5 {I1} (1991Wa20) 


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:
CC E3 CC(THEORY)'S MULT. BY 0.975 10 (Cf. 1990Ne01) 
M$From |g-X and |g-e coincidence in IT decay (1981Li08,1981LiZK) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$|a(K)exp=0.10 {I3} for 213.3+213.7 
RI The relative intensities for 134.28 and 213.5 |g from {+127}La |b{++} decay (5.1 min) are 100 and 11.4 (2002Sh01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI The relative intensities for 91.6, 220.35 and 334.4 |g from {+127}La |b{++} decay (5.1 min) are 5.7, 100 and 36 respectively (2002Sh01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from DCO, |a(K)exp and K/L 
|a(K)exp=0.291 {I67}, K/L=6.8 {I22} (1993Co09) 
|a(K)(M1)=0.371, |a(K)(E2)=0.487, K/L=7.48 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from DCO and |a(K)exp 
|a(K)exp=0.094 {I22} (1993Co09) 
|a(K)(M1)=0.0658, |a(K)(E2)=0.629 
RI I/I(473|g)=48/49 in 1977Gi05 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$rounded value from energy difference of relevant levels. 945 in authors' drawing (1997Vo12) but not plotted in the drawing of 1998Wi20 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$(479|g)(284|g)(|q): A{-2}=+0.107 {I5}, A{-4}=+0.016 {I8}; A{-2}=+0.100 {I4}, A{-4}=+0.016 {I7} (2001As02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from 2002Wo10. Other: 1/|d=0.002 {I17} (2001As02) 
$(601|g)(284|g)(|q): A{-2}=-0.12 {I2}, A{-4}=+0.29 {I4} (2002Wo10); A{-2}=-0.093 {I15}, A{-4}=+0.36 {I3} (2001As02) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
$(659|g)(284|g)(|q): A{-2}=+0.36 {I7}, A{-4}=+1.05 {I13} (2002Wo10) 
$(659|g)(284|g)(|q lin pol) also measured by 2002Wo10 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from 2002Wo10. Other: +6.7 {I+80-25} (2001As02) 
$(1040|g)(284|g)(|q): A{-2}=-0.032 {I13}, A{-4}=-0.099 {I21} (2002Wo10); A{-2}=-0.081 {I17}, A{-4}=-0.10 {I3} (2001As02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from 2002Wo10. Others: -19 {I+11-}|@ (2001As02) 
$(609|g)(284|g)(|q): A{-2}=-0.09 {I3}, A{-4}=+0.13 {I4} (2002Wo10). 
$(609|g)(479|g)(|q): A{-2}=-0.12 {I2}, A{-4}=+0.15(3) (2002Wo10); A{-2}=-0.104 {I18}, A{-4}=+0.16 {I3} (2001As02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from |g|g(|q) and (|g)(|g)(|q lin pol) results of 2002Wo10. 
$(1070|g)(284|g)(|q): A{-2}=-0.033 {I22}, A{-4}=+0.09 {I4} (2002Wo10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$large negative A{-2} in |g(|q) data suggests significant quadrupole admixture, favoring M1+E2 over E1+M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2+E3
decay_comment:
ICE/ICE(357G)=0.24 3 (1966Br14) 
MR$from |a(K)exp=0.0058 {I6} (weighted average of 0.0075 {I8} (1969Ro23) and 0.0052 {I5} (1969WaZX)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
(822|g)(357|g)(|q): R=0.507 {I10} 
(822|g)(357|g)(|q): A{-2}=+0.32 {I4}, A{-4}=+1.03 {I8} (1997As05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
(367|g)(1120|g)(|q): R=1.02 {I10} 
(367|g)(569|g)(|q): R=1.07 {I7} 
|d(Q/D)=-1.0 {I8} or +213 {I167} (1995Ki06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
(869|g)(1120|g)(|q): R=0.89 {I4} 
(869|g)(569|g)(|q): R=0.89 {I3} 
|d(Q/D)=+0.47 {I11} or +3.8 {I14} (1995Ki06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
(801|g)(1486|g)(|q): R=1.1 {I1} 
(801|g)(936|g)(|q): R=1.2 {I1} 
|d(Q/D)=-0.2 {I2} or -2.4 {I13} (1995Ki06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
$|a(K)exp=0.0232 {I25} (recalculated by evaluators); |a(K)exp=0.058 {i15} in 1979En06 apparently, is a misprint 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |g(|q): A{-2}=-0.56 {I4}, A{-4}=0.12 {I6} 
MR +0.02 {I4} obtained by 1977Kr13 from data of 1975Gi11 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |g(|q): A{-2}=-0.73 {I4}, A{-4}=0.06 {I6} 
MR -0.25 {I12} obtained by 1977Kr13 from data of 1975Gi11 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |g(|q): A{-2}=-0.48 {I6}, A{-4}=0.10 {I8} 
MR +0.12 {I8} obtained by 1977Kr13 from data of 1975Gi11 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M,MR$(M1+E2) with |d=-0.56 {I8} (for J=1) from |g|g(|q) data is in contradiction with E1 for 3199|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from |g|g(|q) (1990Da09). Others: +9 {I+7-3} (1971Ta21), >14 (1962Ro07) 
$ A2=-0.18 3, A4=+0.30 6 (1971Ta21) 
$ A2=-0.07 5, A4=+0.39 9 (1962Ro07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI$I|g(1533.6)/I|g(1998.3)=3.3 {I5} (1996Ku01) suggests that most of the intensity belongs with placement from 1998 level; the component from 3219 level must be very weak 
$|a(K)exp=0.00069 {I25} for a doublet 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI$8 (2002Ga01) 
$(383.4|g)(663.1|g)(|q): R(90|'/180|')=1.54 {I13} 
$ E|g=383.28 {I11}, I|g=0.55 {I8} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(697.7|g)(567.3|g)(|q): R(90|'/180|')=1.02 {I4} 
$(697.7|g)(1031.7|g)(|q): R(90|'/180|')=0.89 {I4} 
$ E|g=697.68 {I3}, I|g=1.24 {I8} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(912.7|g)(567.3|g)(|q): R(90|'/180|')=0.86 {I9} 
$(912.7|g)(1031.7|g)(|q): R(90|'/180|')=0.83 {I18} 
$ E|g=912.50 {I12}, I|g=0.073 {I14} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(1479.7|g)(464.5|g)(|q): R(90|'/180|')=0.82 {I23} 
$ E|g=1479.7 {I5}, I|g=0.020 {I13} (deleted by 1975WiZJ) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$32 {I4} (2002Ga01, as per e-mail reply from A. Gade on Jan 16/02). I|g=100 quoted in table 5 of 2002Ga01 is a misprint 
$ E|g=1998.38 {I6}, I|g=0.61 {I4} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(1014.7|g)(567.3|g)(|q): R(90|'/180|')=0.99 {I9} 
$(1014.7|g)(1031.7|g)(|q): R(90|'/180|')=1.02 {I19} 
$ E|g=1014.59 {I19}, I|g=0.060 {I15} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_comment:
$(1036.8|g)(567.3|g)(|q): R(90|'/180|')=1.05 {I8} 
$(1036.8|g)(1031.7|g)(|q): R(90|'/180|')=1.06 {I13} 
$ E|g=1036.92 {I9}, I|g=0.42 {I4} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_comment:
$(175.2|g)(816.6|g)(|q): R(90|'/180|')=1.11 {I70} 
$(175.2|g)(912.7|g)(|q): R(90|'/180|')=1.08 {I16} 
$(175.2|g)(1479.7|g)(|q): R(90|'/180|')=1.4 {I4} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
$(991.9|g)(601.7|g)(|q): R(90|'/180|')=0.94 {I4} 
$(991.9|g)(663.1|g)(|q): R(90|'/180|')=1.10 {I5} 
$(991.9|g)(697.7|g)(|q): R(90|'/180|')=1.15 {I5} 
$ E|g=991.95 {I9}, I|g=0.18 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(511.1|g)(601.7|g)(|q): R(90|'/180|')=1.13 {I11} 
$(511.1|g)(697.7|g)(|q): R(90|'/180|')=0.99 {I9} 
$J|p labels in the cascade are misprinted in 1996Ku01 
$(511.1|g)(1264.8|g)(|q): R(90|'/180|')=0.83 {I10} 
$J|p labels in the cascade are misprinted in 1996Ku01 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(265.9|g)(918.8|g)(|q): R(90|'/180|')=1.16 {I12} 
$(265.9|g)(1014.7|g)(|q): R(90|'/180|')=1.36 {I25} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(131.7|g)(496.4|g)(|q): R(90|'/180|')=1.3 {I7} 
$(131.7|g)(714.7|g)(|q): R(90|'/180|')=1.08 {I9} 
$(131.7|g)(1098.1|g)(|q): R(90|'/180|')=1.38 {I22} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(330.5|g)(297.5|g)(|q): R(90|'/180|')=0.90 {I12} 
$(330.5|g)(515.9|g)(|q): R(90|'/180|')=1.07 {I7} 
$(330.5|g)(899.2|g)(|q): R(90|'/180|')=0.85 {I6} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
$(645.0|g)(601.7|g)(|q): R(90|'/180|')=0.95 {I11} 
$(645.0|g)(697.7|g)(|q): R(90|'/180|')=1.28 {I12} 
$ E|g=645.05 {I4}, I|g=0.41 {I3} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
$(1342.7|g)(567.3|g)(|q): R(90|'/180|')=1.15 {I9} 
$(1342.7|g)(1031.7|g)(|q): R(90|'/180|')=1.25 {I14} 
$ E|g=1342.81 {I7}, I|g=0.47 {I4} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(395.6|g)(515.9|g)(|q): R(90|'/180|')=1.10 {I7} 
$(395.6|g)(899.2|g)(|q): R(90|'/180|')=0.88 {I6} 
$(395.6|g)(297.5|g)(|q): R(90|'/180|')=0.81 {I11} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(363.3|g)(175.2|g)(|q): R(90|'/180|')=0.98 {I13} 
$(363.3|g)(187.6|g)(|q): R(90|'/180|')=0.94 {I13} 
$(363.3|g)(390.2|g)(|q): R(90|'/180|')=1.09 {I6} 
$(363.3|g)(991.9|g)(|q): R(90|'/180|')=1.08 {I8} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(548.0|g)(816.6|g)(|q): R(90|'/180|')=0.96 {I12} 
$Final J|p=4 {-1} - in the cascade seems misprinted in 1996Ku01. The parity should be positive 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$uncertainty of 0.06 quoted in table 3 of 2002Ga01 is a misprint (as per e-mail reply from A. Gade on Jan 16/02) 
$(2040.7|g)(464.5|g)(|q): R(90|'/180|')=0.77 {I5} 
$ E|g=2040.79 {I5}, I|g=1.11 {I7} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(192.9|g)(1909.8|g)(|q): R(90|'/180|')=0.9 {I4} 
$(192.9|g)(1342.7|g)(|q): R(90|'/180|')=1.18 {I23} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
$(569.1|g)(1533.6|g)(|q): R(90|'/180|')=1.05 {I6} 
$(569.1|g)(1998.3|g)(|q): R(90|'/180|')=1.23 {I13} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(126.6|g)(242.3|g)(|q): R(90|'/180|')=0.98 {I12} 
$(126.6|g)(363.3|g)(|q): R(90|'/180|')=1.13 {I10} 
$(126.6|g)(551.1|g)(|q): R(90|'/180|')=0.9 {I3} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(252.0|g)(131.7|g)(|q): R(90|'/180|')=1.20 {I23} 
$(252.0|g)(330.5|g)(|q): R(90|'/180|')=0.85 {I10} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(490.0|g)(175.2|g)(|q): R(90|'/180|')=1.05 {I12} 
$(490.0|g)(187.6|g)(|q): R(90|'/180|')=1.20 {I13} 
$(490.0|g)(390.2|g)(|q): R(90|'/180|')=1.15 {I5} 
$(490.0|g)(991.9|g)(|q): R(90|'/180|')=1.12 {I7} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$(573.7|g)(991.9|g)(|q): R(90|'/180|')=0.87 {I13} 
$(573.7|g)(390.2|g)(|q): R(90|'/180|')=1.04 {I13} 
$ E|g=573.64 {I19}, I|g=0.20 {I4} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$(652.8|g)(390.2|g)(|q): R(90|'/180|')=0.67 {I7} 
$(652.8|g)(991.9|g)(|q): R(90|'/180|')=0.80 {I14} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$(671.8|g)(390.2|g)(|q): R(90|'/180|')=1.15 {I28} 
$(671.8|g)(991.9|g)(|q): R(90|'/180|')=0.84 {I20} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$(929.7|g)(1533.6|g)(|q): R(90|'/180|')=1.22 {I17} 
$(929.7|g)(1998.3|g)(|q): R(90|'/180|')=0.87 {I19} 
$ E|g=929.68 {I5}, I|g=0.260 {I21} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$(588.7|g)(237.9|g)(|q): R(90|'/180|')=0.41 {I4} 
$(588.7|g)(330.5|g)(|q): R(90|'/180|')=1.2 {I4} 
$ E|g=588.1 {I3}, I|g=0.046 {I19} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$|d(E2/M1)=-0.56 {I8} (2002Ga01) for J|p=1+ for 3664.7 level. But 1+ is inconsistent with mult=E1 for 3199.8|g from ce data 
$ E|g=2631.63 {I7}, I|g=0.315 {I22} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$for 464.4+463; <8 units assigned to 463|g 
$ A{-2}=+0.24 {I6}, A{-4}=-0.03 {I6} for doublet. DCO=1.06 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$According to 1995Ju09, this transition does not deexcite |DJ=1 band member, instead, it deexcites a 13- level at 5033. However, |g(|q) and |g|g(|q) data imply a |DJ=1 transition, which is inconsistent with |DJ=2 transition implied by |g|g(|q) data of 1995Ju09 
A{-2}=-0.06 {I7}, A{-4}=-0.06 {I9}. DCO=0.79 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_uncertain: ?
decay_comment:
$Placement is from 2901, 8- to 2423, 6- level in 1995Ju09. I|g(478)/I|g(417)=0.40 {I6} (1975Gi11) marginally agrees with 0.28 {I4} from 1995Ju09 
A{-2}=+0.18 {I10} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
DCO=1.34 {I11} 
E$placement seems suspect in 1995Ju09, 6+ |g-vibration level is at 2241 with a 1113.5|g from this level to 4+ level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=LE
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=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M,MR$L1:L2:L3=100:9.6 {I20}:3.1 {I15} (1965Th05); |a(exp)=65 {I3} (1980Mi13); maximum possible E2 admixture of |d{+2}=1.6|*10{+-4}. 


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:
M$other: K:L:M:N=100.0 {I11}:31.5 {I4}:6.68 {I12}:1.78 {I7} (1980VyZZ); |a(K)exp=3.45 {I20} and K/L+=2.55 {I10} (1965Th05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$calculated by evaluators with BrIccMixing program from ce(K)=1000 {I150}, ce(L)=145 {I25}, and ce(M)=35 {I6} (1966Ha23) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$Calculated by evaluators with BrIccMixing program from ce(K)=520 {I80}, ce(L1)=70 {I10} and ce(M)=18 {I3} (1966Ha23) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
M,MR$from 'adopted levels and gammas' 
RI$from I(|g+ce)=3976 {I164} deduced using I|g({+|+})=458 {I11} (1976He11), |e/|b{++}=15.2 (theory 1972Dz09 with assumed uncertainty of 3%) and |SI(|g+ce)=266 {I4}, the total intensity feeding this state 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$Calculated by evaluators with BrIccMixing program from ce(K)=520 {I80}, ce(L1)=70 {I10} and ce(M)=18 {I3} (1966Ha23) 
E$level energy difference is 290.044 {I8}; 290.275 {I22} in 1980VyZZ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_uncertain: ?
decay_comment:
E$this transition questionably populates the 630.567-keV level (1976He11), poor fit, the level energy difference = 293.388 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$this transition questionably populates the 862.80-keV level in 1976He11, however, the level energy difference (158.78 {I9}) fits 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$this transition questionably populates the 676.486-keV level in 1976He11, however, the level energy difference (345.098 {I25}) fits 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$this transition questionably populates the g.s. in 1976He11, the level energy difference = 1112.344 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$this transition populates the 1/2+, g.s.; in {+132}Ba(pol d,p) L=1 for the 1283.9-keV state. Comparison of I|g and ce for 1283.9- and 1199.5-keV (M1) transitions point at mult.=(E1) for the former 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$this transition questionably populates the 887.134-keV level in 1976He11, the level energy difference = 442.182 {I19} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$ poor fit, the level energy difference = 445.93 {I5} 
M M1,E2 from conversion data. M1 ruled out from placement in level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other transition questionably populates the 291.186-keV level from the 1620.56-keV level (1976He11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$428.53 {I9} is placed from the 1351-keV (3/2+,5/2+) level (1980VyZZ), but this level is not supported by others, the level energy difference is equal to 428.74 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$this transition populates the 858.499-keV level questionably (1976He11), the level energy difference = 494.20 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$poor fit: the level energy difference is equal to 733.36 {I3} 
M$|a(K)exp value does not correspond to mult.=D or E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$questionable population in 1976He11, the level energy difference = 1329.38 {I4}; other transition populates the g.s. from the 1329.3-keV level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$this transition questionably populates the 577.553-keV level (1976He11), the level energy difference = 1112.19 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
$L1:L2:L3=100:9.6 {I20}:3.1 {I15} (1965Th05) 
RI$calculated by evaluators from intensity balance with 275.9-keV transition and |a=69.5 {I19}; others: 0.086 {I5} (1980Mi13), 0.0515 {I25} (1980VyZZ) 
M,MR$from 1965Th05, 1980Mi13; maximum possible E2 admixture of |d{+2}=1.6|*10{+-4}. 
MR$=0.007 {I5} calculated with BrIccMixing program by evaluators using the L-subshell ratio of 1965Th05; |a=68.9 {I20} with that |d 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E5]
decay_comment:
E$from 2011Gr01 and 1980AnZG: |DE|g=1 keV (assigned by evaluators) 
RI$from 2011Gr01. Other: 0.036 {I25} (1980AnZG) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|d(E2/M1)=-0.15 {I2} given in Table 2; M1 adopted by the authors 
$R{-DCO}=0.37 {I3}, |D{-asym}=-0.050 {I42} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|d: +0.01 {I12} or +2.2 {I+12-7} 
$B(M1)(W.u.)=0.041 {I4}, B(E2)(W.u.)<0.08 if |d=+0.01 {I12}; B(M1)(W.u.)=0.007 {I7}, B(E2)(W.u.)=25 {I6} if |d=+2.2 {I+12-7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|d: -0.80 {I+10-16} or -5.5 {I+9-14} 
$B(M1)(W.u.)=0.0044 {I21}, B(E2)(W.u.)=0.6 {I3} if |d=-0.80 {I+10-16}; B(M1)(W.u.)=0.00023 {I13}, B(E2)(W.u.)=1.4 {I4} if |d=-5.5 {I+9-14} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From 1972Be45. If one assumes E0 and E2 components, then the ratio of E0 to E2 intensities is estimated to be |<0.06 (1998Ga24) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$|a(K)exp: average for 2564|g and 2570|g consistent with E1, M1, or E2 for either or both transitions. Placement requires |D|p=no 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$|a(K)exp: average for 2564|g and 2570|g consistent with E1, M1 or E2 for either or both transitions. 


decay_energy_unit: KEV
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:
$Relative branching ratio=100.0 {I34} from (n,n'|g) in 1995De64 (Phys. Atomic Nuclei 58, 2001) 
$B(E1)(W.u.) deduced by compiler, assuming absence of 16-keV transition 


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:
$Relative branching ratio=14.5 {I6} from (n,n'|g) in 1995De64 
$B(E3)(W.u.) deduced by compiler, assuming absence of 16-keV transition 


decay_energy_unit: KEV
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 {+134}Ba Adopted dataset in the ENSDF database (July 2004 update) 
$B(E2)(W.u.) deduced by compiler 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}=1.10 {I8}, |D=0.026 {I55} 
RI$sum intensity of 969.9 and 970.8 gamma rays, where the sum of the 970.8 gamma is <10% of sum intensity (2020Ne01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$unplaced |g rays of E|g=1130.89 {I11} and E|g=1130.6 {I6} were reported in {+135}La |e decay and (n,n'|g), respectively 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
E$average of 268.238 {I18} (1971Ba18) and 268.198 {I16} (1980VyZZ) 
M$from |a(exp)=5.42 {I11} (1973LeYP), |a(K)exp=3.84 {I11} 
|a(exp): from absolute ce and |g-ray counting (1973LeYP) 
|a(K)exp: weighted average of 3.68 {I20} (1958Mi88) and 3.91 {I13} (1973LeYP) 
K/L+M+=2.6 {I1} (1973LeYP) 


decay_energy_unit: KEV
decay_comment:
E$ from 'adopted gammas', not observed by 2006Ch51 due to its high multipolarity and subsequent large internal conversion 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$|g assigned (by evaluators) with both 980 and 1239 levels on the basis of 'adopted gammas'. Total I|g=0.63 {I11} split in two places based on branching ratios in 'adopted gammas' 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
This transition is considered uncertain since it is not reported in (n,n'|g) where the 1446 level is fed strongly 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$|g assigned (by evaluators) with both 980 and 1239 levels on the basis of 'adopted gammas'. Total I|g=8.8 {I4} split according to branching ratios in 'adopted gammas'. It should be noted, however, that E|g=758.99 is required for placement from 980 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$based on e-mail reply of June 29, 2010 from the first author of 2010Ku15, E|g should be 1080.3, not 1080.6 as listed in authors' table I 
$ POL=+0.06 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$based on e-mail reply of June 29, 2010 from the first author of 2010Ku15, E|g should be 1154.5, not 1154.9 as listed in authors' table I 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M2+(E3)
decay_comment:
E$not observed in {+208}Pb({+136}Xe,X|g) experiment may be due to the selection of the width of the time difference between Prisma and Agatha used in the analysis. 
$|a{-T}=0.32 {I7} computed from the intensity balance in {+130}Te({+9}Be,4n) experiment in 2018Ka47. Comparison with the theoretical |a yields a good agreement with M2 or E3. Other: |a{-T}=0.364 {I5} calculated employing |d deduced in 2018Ka47. 
MR$from the 1184|g gated |g(|q)-|g(|q) measurements in {+130}Te({+9}Be,4n). 
$B(M2)(W.u)=0.001053 {I40}, B(E3)(W.u) = 0.0012 {I11} measured in 2018Ka47. 
M$based on deduced |a, measured |d and cmparison of the reduced transition probabilities with the shell model calculations in 2018Ka47. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
TI$from {+135}Ba(n,|g), E=thermal 
M$from {+135}Ba(n,|g), E=thermal; ce(K) observed but not |g 
$B(E0)/B(E2 to 2+, 818 level)=0.173 {I15} (1987PaZS) 
$B(E2 to 2+, 1551 level)/B(E2 to 2+, 818 level)|?0 (1987PaZS) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [E0]
decay_comment:
E$from {+136}La |e decay only 
$B(E0)/B(E2 to 2+, 818 level)=0.125 {I15} (1987PaZS) 
$B(E2 to 2+, 1551 level)/B(E2 to 2+, 818 level)|?0 (1987PaZS) 


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$from relative branchings for transitions from the 2356.5 level in (n,n'|g) from 2008Mu19. 
M$Q from |g(|q) in {+136}Ba(n,n'|g); M2 excluded by comparison to RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from relative photon branchings for transitions from the 2694.4 level in (n,n'|g) from 2008Mu19. 


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$Q from |g(|q) in {+136}Ba(n,n'|g); M2 excluded by comparison to RUL. 
RI$from 1994Al17 in (n,n'|g). In 2008Mu19, also (n,n'|g) the branching ratio I|g(2773|g):I|g(1955|g) is given as 78 {I10}: 22 {I10}, and no observation of 1222|g is reported. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$D+Q from |g(|q) in {+136}Ba(n,n'|g); nonzero value of |d excludes E1+M2. 
MR$-2.0 {I2} or -0.26 {I4} (1994Al17); 2 {I1} or 0.3 {I1} (2008Mu19), both from |g(|q) in {+136}Ba(n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from branching ratio measurements in (n,n'|g) (2008Mu19) 
MR$0.3 {I+5-3} or 6.9 {I+10-50} from |g(|q) in {+136}Ba(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from branching ratio measurements in (n,n'|g) (2008Mu19) 
MR$0.2 {I2} or 12 {I+1-8} from |g(|q) in {+136}Ba(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_comment:
RI$from branching ratio measurements in (n,n'|g) (2008Mu19) 
M$D+Q from |g(|q) in {+136}Ba(n,n'|g), large, non-zero value of delta and RUL exclude E1+M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from branching ratio measurements in (n,n'|g) (2008Mu19) 
MR$+4 {I+4-1} or -0.13 {I14} (1994Al17); 3 {I+6-1} or 0.04 {I+25-20} (2008Mu19), both from |g(|q) in {+136}Ba(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:
RI$from branching ratio measurements in (n,n'|g) (2008Mu19) 
M$Q from |g(|q) in {+136}Ba(n,n'|g); M2 excluded by comparison to RUL. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
E$from 1980GeZU. Note that energies cited by 1980GeZU are |?0.2 keV higher than those cited by 1983BrZK 
M$no |g of this energy observed (1980GeZU) 
TI$from ce(K) and ce(K)/ce (evaluator) 
$ce(K)=1066; ce(K)/ce=0.89 
$B(E0)(1580|g)/B(E2)(761|g)=0.11 {I2} (1985CoZR,1980GeZU) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from 2008Mu19. Others: 818.51 {I2} (1994Al17), 818.54 {I4} (1985Di10) 
RI$|DI|g from 1985Di10. 
M$A{-2}=0.210 {I5}, A{-4}=-0.088 {I7}, POL=2.0 {I+3-2} (1994Al17); A{-2}=0.18 {I1}, A{-4}=-0.09 {I2} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g{+rel}=0.48 {I1} 
E$weighted average of 732.39 {I1} (2008Mu19), 732.46 {I2} (1994Al17), 732.48 {I5} (1985Di10). 
RI$other: 7.3 {I3} (1985Di10). 
M$A{-2}=-0.205 {I6}, A{-4}=-0.018 {I9}, POL=1.6 {I+23-14} (1994Al17); A{-2}=-0.21 {I2}, A{-4}=0.01 {I2} (1985Di10). 
MR$others:-1.5 {I+7-4} (2008Mu19), -1.5 {I+6-10} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$I|g{+rel}=0.52 {I1} 
E$weighted average of 1551.00 {I1} (2008Mu19), 1550.96 {I2} (1994Al17), 1550.95 {I4} (1985Di10). 
RI$other: 8.2 {I2} (1985Di10). 
M$A{-2}=0.260 {I7}, A{-4}=-0.102 {I8}, POL=2.3 {I+4-2} (1994Al17); A{-2}=0.26 {I2}, A{-4}=-0.10 {I2} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 760.44 {I1} (2008Mu19), 760.49 {I2} (1994Al17), 760.51 {I6} (1985Di10). 
RI$other: 2.8 {I2} (1985Di10). 
M$A{-2}=-0.01 {I2}, A{-4}=0.00 {I3} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1047.98 {I5} (2008Mu19), 1048.07 {I2} (1994Al17), 1048.08 {I4} (1985Di10). 
RI$other: 13.5 {I5} (1985Di10). 
M$A{-2}=0.277 {I5}, A{-4}=-0.054 {I7}, POL=2.6 {I+5-3} (1994Al17); A{-2}=0.33 {I4}, A{-4}=0.06 {I5} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 163.95 {I5} (1994Al17) and 164.02 {I12} (1985Di10). 
RI$other: 3 {I1} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M$A{-2}=0.27 {I4}, A{-4}=-0.04 {I6} (1994Al17). 
MR$from 2008Mu19. Other: -0.04 {I6} or +1.07 {I13} (1994Al17). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1235.41 {I1} (2008Mu19), 1235.26 {I3} (1994Al17), 1235.33 {I4} (1985Di10). 
RI$other: 6.8 {I2} (1985Di10). 
M$A{-2}=0.304 {I7}, A{-4}=-0.069 {I9}, POL=3.2 {I+9-4} (1994Al17); A{-2}=0.28 {I3}, A{-4}=-0.06 {I4} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 528.94 {I8} (1994Al17) and 529.1 {I2} (1985Di10). 
RI$other: 0.2 {I1} (1985Di10). 
M$A{-2}=0.00 {I3}, A{-4}=-0.08 {I5} (1994Al17). 
MR$-0.28 {I5} or +7 {I+4-2} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g{+rel}=0.62 {I1} 
E$weighted average of 1261.67 {I1} (2008Mu19), 1261.49 {I3} (1994Al17), 1261.55 {I5} (1985Di10). 
RI$other: 1.9 {I1} (1985Di10). 
M$A{-2}=-0.211 {I5}, A{-4}=-0.019 {I7}, POL=1.6 {I+3-2} (1994Al17); A{-2}=-0.23 {I4}, A{-4}=-0.02 {I5} (1985Di10). 
MR$others: -1.3 {I+14-3} (2008Mu19), -1.5 {I+6-15} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$I|g{+rel}=0.38 {I1} 
E$weighted average of 2080.25 {I4} (2008Mu19), 2080.04 {I3} (1994Al17), 2080.0 {I2} (1985Di10). 
RI$other: 1.1 {I1} (1985Di10). 
M$A{-2}=0.277 {I8}, A{-4}=-0.093 {I10} (1994Al17); A{-2}=0.32 {I5}, A{-4}=-0.07 {I7} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$I|g{+rel}=0.69 {I1} 
E$weighted average of 1310.34 {I1} (2008Mu19), 1310.33 {I3} (1994Al17), 1310.31 {I5} (1985Di10). 
RI$other: 2.0 {I1} (1985Di10). 
M$A{-2}=0.200 {I7}, A{-4}=-0.012 {I9}, POL=2.0 {I+5-3} (1994Al17); A{-2}=0.22 {I7}, A{-4}=0.06 {I8} (1985Di10). 
MR$others: -0.002 {I31} (2008Mu19), 0.03 {I+18-15} or 2.2 {I+16-8} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$I|g{+rel}=0.31 {I1} 
E$weighted average of 2128.94 {I3} (2008Mu19), 2128.81 {I4} (1994Al17), 2128.75 {I9} (1985Di10). 
RI$other: 1.0 {I1} (1985Di10). 
M$A{-2}=0.288 {I8}, A{-4}=-0.121 {I12} (1994Al17); A{-2}=0.38 {I4}, A{-4}=0.03 {I5} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$weighted average of 273.53 {I1} (2008Mu19), 273.65 {I2} (1994Al17), 273.81 {I6} (1985Di10). 
RI$other: 2.4 {I2} (1985Di10). 
M$A{-2}=-0.205 {I9}, A{-4}=0.010 {I13} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1322.86 {I3} (2008Mu19), 1322.87 {I4} (1994Al17), 1322.76 {I7} (1985Di10). 
RI$other: 0.6 {I1} (1985Di10). 
M$A{-2}=0.008 {I10}, A{-4}=-0.008 {I12}, POL=1.0 {I+4-3} (1994Al17); A{-2}=0.08 {I9}, A{-4}=0.13 {I10} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$weighted average of 176.68 {I5} (1994Al17) and 176.9 {I2} (1985Di10). 
RI$other: 0.3 {I1} (1985Di10). 
M$A{-2}=-0.11 {I2}, A{-4}=0.00 {I3} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 340.42 {I4} (2008Mu19), 340.55 {I3} (1994Al17), 340.75 {I7} (1985Di10). 
RI$other: 1.1 {I1} (1985Di10). 
M$A{-2}=0.282 {I12}, A{-4}=-0.106 {I17}, POL=2.6 {I7} (1994Al17); A{-2}=0.29 {I3}, A{-4}=0.05 {I3} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$I|g{+rel}=0.47 {I2} 
E$weighted average of 671.64 {I1} (2008Mu19), 671.73 {I3} (1994Al17), 671.76 {I7} (1985Di10). 
RI$other: 0.9 {I2} (1985Di10). 
M$A{-2}=0.197 {I6}, A{-4}=-0.012 {I12}, POL=2.0 {I+6-4} (1994Al17); A{-2}=0.19 {I7}, A{-4}=0.02 {I10} (1985Di10). 
MR$others: +0.03 {I+3-100} or +2 {I1} (2008Mu19), -0.01 {I+11-12} or 2.5 {I+12-8} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g{+rel}=0.53 {I2} 
E$weighted average of 1404.22 {I2} (2008Mu19), 1404.20 {I3} (1994Al17), 1404.19 {I9} (1985Di10). 
RI$other: 0.9 {I1} (1985Di10). 
M$A{-2}=0.251 {I8}, A{-4}=0.010 {I11}, POL=0.9 {I+4-3} (1994Al17); A{-2}=0.15 {I9}, A{-4}=-0.02 {I12} (1985Di10). 
MR$others: +1.5 {I1} or +0.22 {I10} (2008Mu19), 0.01 {I+9} or 2.3 {I+7-5} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 158.44 {I2} (1994Al17) and 158.59 {I8} (1985Di10). 
RI$other: 0.9 {I2} (1985Di10). 
M$A{-2}=-0.052 {I7}, A{-4}=0.004 {I10} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1496.71 {I3} (2008Mu19), 1496.82 {I7} (1994Al17), 1496.7 {I2} (1985Di10). 
RI$other: 0.4 {I1} (1985Di10). 
M$A{-2}=-0.00 {I2}, A{-4}=0.02 {I3} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$I|g{+rel}=0.16 {I1} 
E$weighted average of 302.33 {I3} (2008Mu19), 302.61 {I8} (1994Al17), 302.9 {I2} (1985Di10). 
RI$other: 0.3 {I1} (1985Di10). 
M$A{-2}=0.33 {I3}, A{-4}=0.03 {I4}, POL=1.4 {I+15-7} (1994Al17) 
MR$other: 0.00 {I6} or +1.07 {I12} (1994Al17). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g{+rel}=0.26 {I1} 
E$weighted average of 489.64 {I2} (2008Mu19), 489.93 {I5} (1994Al17), 489.9 {I7} (1985Di10). 
RI$other: 0.6 {I2} (1985Di10). 
M$A{-2}=0.377 {I17}, A{-4}=-0.004 {I20} (1994Al17) 
MR$=+0.14 {I4} or +0.79 (1994Al17); 0.02 {I+19-13} or 1.0 {I+4-3} (2008Mu19). 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
$I|g{+rel}=0.18 {I1} 
E$from 2008Mu19. A 805.55 {I16} transition is observed by 1994Al17 and tentatively placed from a level at 2934 keV. In their excitation function, 2008Mu19 observe a threshold below 2.5 MeV for the 805.5|g. 
M$from |g(|q) in 2008Mu19 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$I|g{+rel}=0.40 {I1} 
E$weighted average of 1537.95 {I3} (2008Mu19), 1537.98 {I4} (1994Al17), 1537.90 {I7} (1985Di10). 
RI$other: 0.8 {I1} (1985Di10). 
M$A{-2}=0.326 {I12}, A{-4}=-0.074 {I15}, POL=2.8 {I+28-10} (1994Al17); A{-2}=0.32 {I4}, A{-4}=-0.06 {I5} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 166.61 {I4} (1994Al17) and 166.7 {I2} (1985Di10). 
RI$other: 0.2 {I1} (1985Di10). 
M$A{-2}=-0.05 {I2}, A{-4}=-0.06 {I4} (1994Al17) 
MR$-0.08 {I4} or -5.9 {I20} (1994Al17). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 319.72 {I4} (2008Mu19), 319.88 {I4} (1994Al17), 320.1 {I2} (1985Di10). 
RI$other: 0.4 {I1} (1985Di10). 
M$A{-2}=-0.07 {I2}, A{-4}=0.06 {I3}, POL=0.9 {I+4-3} (1994Al17) 
MR$from 2008Mu19. Other: +0.09 {I4} or 1/|d=0.00 {I1} (1994Al17). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 506.91 {I1} (2008Mu19) and 507.12 {I7} (1994Al17) 
M,MR$from |g(|q) in 2008Mu19 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
$I|g{+rel}=0.16 {I1} 
E$weighted average of 336.68 {I4} (2008Mu19) and 336.97 {I7} (1994Al17) 
M,MR$A{-2}=-0.09 {I5}, A{-4}=0, POL=1.6 {I+17-5} (1994Al17). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
E$weighted average of 1572.29 {I2} (2008Mu19), 1572.28 {I3} (1994Al17), 1572.25 {I8} (1985Di10). 
RI$other: 1.2 {I1} (1985Di10). 
M,MR$A{-2}=-0.286 {I6}, A{-4}=-0.007 {I9}, POL=1.3 {I+4-3} (1994Al17), A{-2}=-0.33 {I5}, A{-4}=0.12 {I4} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1581.44 {I3} (2008Mu19), 1581.36 {I4} (1994Al17), 1581.34 {I9} (1985Di10). 
RI$other: 0.8 {I1} (1985Di10). 
M$A{-2}=-0.027 {I6}, A{-4}=-0.012 {I8}, POL=0.6 {I3} (1994Al17), A{-2}=-0.10 {I2}, A{-4}=-0.03 {I3} (1985Di10). 
MR$1/|d=0.019 {I17} (1994Al17); -2 {I+6-2} or -0.2{I+60-4} (2008Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g{+rel}=0.52 {I1} 
E$weighted average of 879.94 {I2} (2008Mu19), 879.93 {I3} (1994Al17), 879.99 {I6} (1985Di10). 
RI$other: 0.6 {I1} (1985Di10). 
M$A{-2}=-0.37 {I2}, A{-4}=0.09 {I3}, POL=1.7 {I+6-4} (1994Al17), A{-2}=-0.43 {I7}, A{-4}=0.12 {I5} (1985Di10). 
MR$weighted average of -1.4 {I5} (2008Mu19) and -2.3 {I4} (1994Al17). Other: -0.27 {I8} or -2.1 {I2} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g{+rel}=0.48 {I1} 
E$weighted average of 1612.51 {I3} (2008Mu19), 1612.37 {I4} (1994Al17), 1612.5 {I1} (1985Di10). 
RI$other: 0.5 {I1} (1985Di10). 
M$A{-2}=-0.193 {I13}, A{-4}=0.111 {I17}, POL=1.8 {I+12-2} (1994Al17), A{-2}=-0.31 {I7}, A{-4}=0.16 {I7} (1985Di10). 
MR$others: -3 {I1} (2008Mu19); -0.15 {I9} or -2.8 {I6} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g{+rel}=0.43 {I8} 
E$weighted average of 1666.60 {I2} (2008Mu19), 1666.44 {I4} (1994Al17), 1666.5 {I2} (1985Di10). 
RI$other: 0.7 {I1} (1985Di10). 
M$A{-2}=0.200 {I9}, A{-4}=-0.002 {I12}, POL=1.6 {I+13-4} (1994Al17), A{-2}=0.29 {I8}, A{-4}=0.12 {I10} (1985Di10). 
MR$others: 0.10 {I7} or 2 {I1} (2008Mu19); 0.07 {I+36-20} or 1.9 {I+20-13} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$I|g{+rel}=0.57 {I8} 
E$weighted average of 2485.11 {I6} (2008Mu19), 2484.94 {I10} (1994Al17), 2484.3 {I2} (1985Di10). 
RI$other: 0.3 {I1} (1985Di10). 
M$A{-2}=0.179 {I15}, A{-4}=-0.079 {I21} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
$I|g{+rel}=0.34 {I1} 
E$weighted average of 981.66 {I2} (2008Mu19), 981.60 {I6} (1994Al17), 981.54 {I9} (1985Di10). 
RI$other: 0.6 {I1} (1985Di10). 
M,MR$A{-2}=-0.078 {I14}, A{-4}=0.002 {I20}, POL=3.7 {I+35-11} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
$I|g{+rel}=0.65 {I1} 
E$weighted average of 1714.24 {I2} (2008Mu19), 1714.10 {I4} (1994Al17), 1713.90 {I8} (1985Di10). 
RI$other: 1.1 {I1} (1985Di10). 
M,MR$A{-2}=-0.197 {I4}, A{-4}=0.004 {I19}, POL=2.1 {I+30-4} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 993.50 {I2} (2008Mu19), 993.44 {I4} (1994Al17), 993.50 {I8} (1985Di10). 
E$1985Di10 place the 993.50|g as depopulating a tentative level at 1812.0 keV. 
RI$other: 0.9 {I1} (1985Di10). 
M$A{-2}=0.328 {I10}, A{-4}=-0.042 {I13}, POL=3.8 {I+35-12} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 720.46 {I1} (2008Mu19), 720.54 {I4} (1994Al17), 720.6 {I2} (1985Di10). 
E$a 720.6|g is unplaced in 1985Di10. 
RI$other: 0.5 {I1} (1985Di10). 
M,MR$A{-2}=0.239 {I11}, A{-4}=-0.020 {I16}, POL=3.7 {I+36-11} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1822.29 {I4} (2008Mu19), 1822.20 {I6} (1994Al17), 1822.2 {I2} (1985Di10). 
RI$other: 0.5 {I1} (1985Di10). 
M$A{-2}=-0.076 {I15}, A{-4}=0.020 {I20}, POL=3.7 {I+36-11} (1994Al17) 
MR$from 2008Mu19. Other: -0.64 {I7} or -13 {I+9-4} (1994Al17). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 793.00 {I3} (2008Mu19), 793.16 {I5} (1994Al17), 793.1 {I2} (1985Di10). 
RI$other: 0.4 {I1} (1985Di10). 
E$a 793.1|g is unplaced in 1985Di10. 
M,MR$A{-2}=0.272 {I15}, A{-4}=-0.010 {I22}, POL=4.0 {I+160-2} (1994Al17) 


decay_energy_unit: KEV
decay_comment:
$I|g{+rel}=0.19 {I2} 
E$placement from 2008Mu19. A 1110.26 {I14} transition with I|g=0.25 {I2} is placed from the 2977-keV level by 1994Al17. 
M$|g(|q) is consistent with Q or D+Q with |d=+8 {I5} or +0.3 {I3} (2008Mu19). 
E$from 2008Mu19. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g{+rel}=0.81 {I2} 
E$weighted average of 1843.00 {I1} (2008Mu19), 1842.85 {I5} (1994Al17), 1843.1 {I1} (1985Di10). 
RI$other: 0.7 {I1} (1985Di10). 
M,MR$A{-2}=0.25 {I2}, A{-4}=0.01 {I3}, POL=4.0 {I+160-2} (1994Al17) 
M,MR$other: |g(|q) is consistent with Q or D+Q with |d=+1.7 {I4} or +0.2 {I1} (2008Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 1142.37 {I13} (1994Al17) and 1142.6 {I4} (1985Di10). 
RI$other: 0.2 {I1} (1985Di10). 
E$placement from 1985Di10 and 1994Al17 could not be confirmed in 2008Mu19. Excitation function for 1142-keV transition yields threshold of 3.0 MeV suggesting transition originates from a level at higher excitation energy (2008Mu19); transition not included in Adopted Levels, Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g{+rel}=0.15 {I7} 
E$weighted average of 1875.36 {I5} (2008Mu19), 1875.15 {I8} (1994Al17), 1875.1 {I2} (1985Di10). 
RI$other: 0.3 {I1} (1985Di10). 
M$A{-2}=0.00 {I2}, A{-4}=0.01 {I2} (1994Al17) 
MR$from 2008Mu19. Other: -2.6 {I+30-9} or -0.07 {I+25-17} (1994Al17). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$I|g{+rel}=0.85 {I7} 
E$weighted average of 2693.92 {I7} (2008Mu19), 2694.0 {I4} (1994Al17), 2693.7 {I4} (1985Di10). 
RI$other: 0.2 {I1} (1985Di10). 
M$A{-2}=-0.10 {I3}, A{-4}=0.01 {I4} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g{+rel}=0.42 {I3} 
E$weighted average of 487.15 {I2} (2008Mu19) and 487.47 {I7} (1994Al17) 
M$A{-2}=-0.28 {I4}, A{-4}=0.07 {I6} (1994Al17) 
MR$+0.12 {I3} or 1/|d=+0.03 {I2} (1994Al17). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g{+rel}=0.58 {I3} 
E$weighted average of 640.55 {I2} (2008Mu19), 640.72 {I6} (1994Al17), 640.7 {I2} (1985Di10). 
RI$other: 0.3 {I1} for unplaced 640.7|g (1985Di10). 
M$A{-2}=-0.69 {I3}, A{-4}=-0.01 {I4}, POL=0.8 {I3} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1222.6 {I2} (1994Al17) and 1221.4 {I3} (1985Di10). 
RI$other: 0.2 {I1} (1985Di10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g{+rel}=0.22 {I10} 
E$weighted average of 1955.03 {I5} (2008Mu19), 1955.05 {I8} (1994Al17), 1954.8 {I3} (1985Di10). 
RI$other: 0.4 {I1} (1985Di10). 
M,MR$A{-2}=0.236 {I17}, A{-4}=-0.043 {I26} (1994Al17) 
MR$other: 0.4 {I+10-2} or 0.8 {I+5-8} (2008Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$I|g{+rel}=0.78 {I10} 
E$weighted average of 2773.66 {I4} (2008Mu19) and 2773.53 {I25} (1994Al17) 
M$A{-2}=0.18 {I3}, A{-4}=-0.07 {I5} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g{+rel}=0.39 {I3} 
E$weighted average of 1229.18 {I5} (2008Mu19) and 1228.87 {I14} (1994Al17). Other: 1229.0 {I3} for unplaced transition with I|g=0.1 {I1} (1985Di10). 
M$A{-2}=0.05 {I4}, A{-4}=0.00 {I5} (1994Al17) 
MR$+5 {I+3-1} or -0.20 {I12} (1994Al17); -0.3 {I2} or 16 {I5} (2008Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g{+rel}=0.61 {I2} 
E$weighted average of 1961.39 {I6} (2008Mu19) and 1961.42 {I11} (1994Al17) 
M$A{-2}=0.183 {I15}, A{-4}=-0.013 {I20} (1994Al17) 
MR$+1.50 {I17} or +0.20 {I6} (1994Al17); 5 {I+27-3} or -0.2 {I2} (2008Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1965.88 {I6} (2008Mu19) and 1965.90 {I13} (1994Al17) 
M$A{-2}=0.01 {I5}, A{-4}=0.0 {I20} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1993.57 {I7} (2008Mu19), 1993.42 {I7} (1994Al17), 1993.3 {I2} (1985Di10). 
RI$other: 0.3 {I1} (1985Di10). 
M$A{-2}=-0.445 {I15}, A{-4}=0.103 {I21} (1994Al17) 
MR$-2.0 {I2} or -0.26 {I4} (1994Al17); 2 {I1} or 0.3 {I1} (2008Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 287.23 {I7} (2008Mu19) and 287.56 {I6} (1994Al17). Other: 287.61 {I8} for unplaced transition with I|g=0.2 {I1} (1985Di10). 
$A{-2}=0.30 {I2}, A{-4}=0.03 {I3} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$I|g{+rel}=0.41 {I3} 
E$weighted average of 974.3 {I6} (2008Mu19) and 974.10 {I15} (1994Al17). Other: 974.2 {I2} for unplaced transition with I|g=0.2 {I1} (1985Di10). 
M$A{-2}=0.16 {I3}, A{-4}=-0.13 {I4}, POL=9 {I+75-6} (1994Al17) 
MR$+0.05 {I15} or +1.0 {I2} (1994Al17). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$I|g{+rel}=0.59 {I3} 
E$weighted average of 2022.32 {I8} (2008Mu19), 2022.15 {I12} (1994Al17), 2021.7 {I2} (1985Di10). 
RI$other: 0.2 {I1} (1985Di10). 
M$A{-2}=0.21 {I3}, A{-4}=-0.05 {I4} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1118.41 {I6} (2008Mu19) and 1118.32 {I14} (1994Al17). Other: 1118.1 {I3} for unplaced transition with I|g=0.1 {I1} (1985Di10). 
$A{-2}=-0.01 {I3}, A{-4}=0.03 {I4} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2203.63 {I5} (2008Mu19) and 2203.40 {I12} (1994Al17). 
$A{-2}=0.00 {I3}, A{-4}=-0.01 {I4} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3044.49 {I5} (2008Mu19) and 3044.39 {I17} (1994Al17). 
$A{-2}=-0.14 {I3}, A{-4}=0.00 {I4} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$I|g{+rel}=0.37 {I4} 
E$weighted average of 1210.70 {I6} (2008Mu19) and 1210.72 {I18} (1994Al17). 
MR$0.2 {I2} or 12 {I+1-8} (2008Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g{+rel}=0.48 {I5} 
E$weighted average of 2258.73 {I9} (2008Mu19) and 2258.9 {I2} (1994Al17). 
M$A{-2}=-0.20 {I7}, A{-4}=0.16 {I9} (1994Al17) 
MR$other: -2.9 {I+50-17} (2008Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g{+rel}=0.18 {I13} 
E$weighted average of 2291.13 {I12} (2008Mu19) and 2291.1 {I4} (1994Al17). 
M$A{-2}=0.04 {I6}, A{-4}=-0.07 {I8} (1994Al17) 
MR$+4 {I+4-1} or -0.13 {I14} (1994Al17); 3 {I+6-1} or 0.04 {I+25-20} (2008Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$I|g{+rel}=0.81 {I13} 
E$weighted average of 3109.41 {I14} (2008Mu19) and 3109.5 {I3} (1994Al17). 
M$A{-2}=0.17 {I5}, A{-4}=-0.09 {I7} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 3116.06 {I5} (2008Mu19) and 3115.8 {I2} (1994Al17). 
M$A{-2}=0.20 {I6}, A{-4}=-0.08 {I7} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2423.28 {I10} (2008Mu19) and 2423.6 {I2} (1994Al17). 
$A{-2}=0.31 {I6}, A{-4}=-0.02 {I8} (1994Al17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$multiply placed from a 3551-keV level or a 3866-keV level (1994Al17) 
$A{-2}=0.32 {I6}, A{-4}=-0.09 {I8} (1994Al17) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$Observed in coincidence with scattered {+32}S (1980Br01) and scattered C (2002Ra21); energy not explicitly given 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$weighted average of 79.9 {I8} (1975Gr31) and 81 {I4} (1973Ba24). Other: 80 {I3} (1977OhZO) 
EKC$other: 0.0016 {I2} (1967Fu05). 
$K/L=7.50 {I26} (1977OhZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
EKC$Other: 0.46 {I4} (1965Re07) 
RI$weighted average of 4.62 {I10} (1975Gr31) and 5.2 {I3} (1973Ba24). Other: 3.40 {I12} (1977OhZO) 
$K/L=1.25 {I3} (1977OhZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$weighted average of 0.60 {I6} (1975Gr31) and 0.50 {I5} (1973Ba24). Other: 0.36 {I4} (1977OhZO) 
$K/L=5.7 {I7} (1977OhZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$weighted average of 19.8 {I8} (1975Gr31) and 19 {I1} (1973Ba24). Other: 80 {I3} (1977OhZO) 
EKC$other: 0.00089 {I14} (1967Fu05). 
$K/L=7.8 {I6} (1977OhZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$weighted average of 6.3 {I3} (1975Gr31) and 4.8 {I5} (1973Ba24). Other: 5.2 {I2} (1977OhZO) 
$K/L=7.24 {I3} (1977OhZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$weighted average of 0.40 {I4} (1975Gr31) and 0.41 {I2} (1973Ba24). Other: 0.21 {I3} (1977OhZO) 
$K/L=2.45 {I15} (1977OhZO) 
MR$|d(O/Q)<0.05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
RI$weighted average of 12.7 {I2} (1975Gr31) and 12.6 {I5} (1973Ba24). Other: 11.1 {I4} (1977OhZO) 
$K/L=7.50 {I26} (1977OhZO) 
EKC$other: 0.011 {I4} (1967Fu05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
M$from |a(L)exp. 
MR$from comparison to RUL. BrIcc mixing using |a(L)exp and L23/L1 ratio gives |d=0.100 {I6} 
RI$other: 12.5 {I1} (1975Gr31), 7.3 {I11} 1973Ba24) 
$L23/L1=0.353 {I11} (1977OhZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
EKC$Other: 0.15 {I3} (1965Re07) 
RI$weighted average of 7.48 {I16} (1975Gr31) and 9.0 {I4} (1973Ba24). Other: 5.77 {I18} (1977OhZO) 
$K/L=3.60 {I10} (1977OhZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
EKC$Other: 0.011 {I8} (1965Re07) 
RI$weighted average of 13.6 {I2} (1975Gr31) and 14.9 {I7} (1973Ba24). Other: 10.0 {I4} (1977OhZO) 
$K/L=8.8 {I7} (1977OhZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$weighted average of 46.8 {I5} (1975Gr31) and 49 {I2} (1973Ba24). Other: 42.3 {I13} (1977OhZO) 
$K/L=5.94 {I11} (1977OhZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$weighted average of 0.63 {I3} (1975Gr31) and 0.62 {I5} (1973Ba24). Other: 0.37 {I4} (1977OhZO) 
$K/L=6.9 {I9} (1977OhZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$weighted average of 0.60 {I6} (1975Gr31) and 0.45 {I4} (1973Ba24). Other: 0.50 {I5} (1977OhZO) 
M$from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$weighted average of 0.98 {I5} (1975Gr31) and 1.1 {I1} (1973Ba24). Other: 0.97 {I3} (1977OhZO) 
M$from |a(K)exp. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
$B(E0)/B(E2 to 2+, 818 level)=0.173 {I15} (1987PaZS); B(E2 to 2+, 1551 level)/B(E2 to 2+, 818 level)|?0 (1987PaZS) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [E0]
decay_comment:
$B(E0)/B(E2 to 2+, 818 level)=0.125 {I15} (1987PaZS); B(E2 to 2+, 1551 level)/B(E2 to 2+, 818 level)|?0 (1987PaZS) 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
$N{-|g}(90|')/N{-|g}(127|')=0.91 {I16} 
$N{-|g}(126|')/N{-|g}(96|')=1.27 {I14}, POL=+0.09 {I14} (1978Me18) 


decay_energy_unit: KEV
decay_multipolarity: E1
decay_comment:
$N{-|g}(90|')/N{-|g}(127|')=0.81 {I5} 
$N{-|g}(126|')/N{-|g}(96|')=1.28 {I12}, POL=+0.066 {I32} (1978Me18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$based on placement in level scheme as 6+ to 4+ transition, E2 is suggested for the 153|g, while the DCO ratio is characteristic of a stretched dipole transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI$other: 100 in {+9}Be+{+130}Te experiment 
M$pure D with J=11 for the 3707-keV level provides best agreement with |g(|q) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$other: 63 {I7} in {+9}Be+{+130}Te experiment 
M,MR$from (510|g)(349|g)(|q) and taking |d=0 for 349|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
RI$other: 35 {I3} in {+9}Be+{+130}Te experiment 
M,MR$from (1214|g)(349|g)(|q) and taking |d=0 for 349|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1997WaZZ in (n,n'|g). 1997WaZZ in both (n,n'|g) and {+137}Cs |b{+-} decay and 1996Bi23 in {+137}Cs |b{+-} decay confirm this energy and did not find any evidence for a possible doublet at previously reported 279.96|g (1973Ke07,1973Ke22) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
RI$probably multiply placed as only a small intensity can be assigned to this placement, as the transition has to be an M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$E|g from 1997Wa37, %I|g average of 5.3|*10{+-4} {I14} (1996Bi23), 6.1|*10{+-4} {I10} (1997Wa37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
E$from 1995HeZZ 
RI$recommended by 1991BaZS on the basis of following values: 85.21 {I7} (1983Be18), 84.3 {I5} (1978Gr09), 84.7 {I7} (1978MeZM), 85.1 {I4} (1975Go28), 84.56 {I8} (1973LeZJ), 85.1 {I4} (1969Ha05) 
Mult.,|a: see {+137}Ba IT decay 


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$from 1995HeZZ 
CC$evaluated by 1991BaZS based on the following values: 0.1083 {I3} (1983Be18), 0.1100 {I3} (1975Go28), 0.1105 {I4} (1973LeZJ), 0.1124 {I6} (1969Ha05), 0.1100 {I11} (1965Me03) 
$|a(K)exp=0.0904 {I5} (1992Ne04). Also |a(K)exp: 0.0900 {I6} from 1992Ne04 given as weighted mean of |a(K)exp=0.0901 {I4} (1973LeZJ), 0.0922 {I22} (1973Wi10), 0.0894 {I10} (1965Me03). Others: |a(K)exp=0.0881 {I2} (1983Be18), 0.0888 {I7} (1978Ch22), 0.0916 {I4} (1969Ha05) 
M K:L1:L2:L3=1000 {I20}:151 {I4}:22 {I1}:19 {I1} (1962Ge09), K/L=5.29 {I23}, L1:L2:L3=341 {I10}:100:50 {I3} (1967Ka24) 
RI$from I(|g+ce)/(1+|a) 
Double-decay processes: see 1971Lj02, 1971Lj01, 1971Po04, 1969Lj01. Probability ratio of two-ce(K)/one-ce(K)=8|*10{+-5} {I4} (1999Vi15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1997WaZZ; the authors find no evidence for previously reported 279|g 
M A{-2}=0.0 {I7}, A{-4}=0.0 {I7} 


decay_energy_unit: KEV
decay_multipolarity: M4
decay_comment:
EKC$ from measured I(K x ray)/I|g(661.6)=0.2559 {I6} (2007Ni04), measured I(K x ray)/I|g(165.9|g in {+139}La)=0.2419 {I8} (2008Ni02), and theoretical |a{-K}=0.2229 {I3} for 165.9|g in {+139}La. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E5
decay_BE_unit: e^2 x (fm)^10
decay_BE_info: ;TYPE=BE5;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE5W
decay_comment:
E$from measured E|g1-E|g2=|+94.5 {I4} for the |g rays in the 11/2 -> 1/2 -> 3/2 cascade and E|g1+E|g2=661.659 {I3} (from ENSDF database for {+137}Ba). E|g1-E|g2=|+94.5 {I4} is obtained from the average of E|g1-E|g2=+94.1 {I4} and -94.8 {I4}. Only detectors with opening angles between 53|' and 130|' were considered in the analysis. 
E$value of E|g=377.9 {I3} given in the abstract is a typo, per email communication with first author to XUNDL compiler on Nov 13, 2014. 
RI$see general comment. 
M$proposed in 2014Mo32 based on |DJ|p of level scheme. Authors argue that M6 contribution is negligible since partial widths decrease by about two orders of magnitude per multipole and magnetic widths are generally two orders of magnitude smaller than corresponding electric widths. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M4
decay_comment:
$Measured I(two |g)/I(single |g)=2.05|*10{+-6} {I37} from Gaussian peaks observed with 693 {I95} counts at 661.6 keV {I16} for the 72|' group and with 307 {I78} counts at 664.2 keV {I28} for the 144|' group of detector pairs (2015Wa29). 2015Wa29 correct small contribution from the 378|g-283|g cascade based on measured intensity of this decay branch by 2014Mo32 as 1.12|*10{+-7} {I9} (2014Mo32), which is <6% of the I(two |g)/I(single |g) value measured in the present work. Theoretical I(two |g)/I(single |g)=2.69|*10{+-6} (QPM,2015Wa29) 
$Coefficient |a{-E2M2}(expt)=+33.9 e{+2}fm{+4}MeV{+-1} {I28} compared to theoretical value of +42.60 e{+2}fm{+4}MeV{+-1} from the matrix element coupling the lowest 7/2+ state at 1252 keV 
$Coefficient |a{-M1E3}(expt)=+10.1 e{+2}fm{+4}MeV{+-1} {I42} compared to theoretical value of +9.50 e{+2}fm{+4}MeV{+-1} from the matrix element coupling possibly the lowest 5/2+ state at 1294 keV 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
M$|DJ=1 transition from |g(|q). In |g|g(|q) measurements of the 275|g-289|g cascade, solutions with both transitions having zero mixing are incompatible with the data, leading 2019Ka04 to conclude that both transitions are non-parity changing. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M4
decay_comment:
$Measured I(two |g)/I(single |g)=2.62|*10{+-6} {I30} from Gaussian peak observed with 960 {I100} counts at 662 keV for condition | E|g1-E|g2 | < 300 keV and | E|g1-E|g2 | < 960 keV - (E|g1+E|g2), the latter to remove cosmic-ray induced background. 
$Coefficient |a{-E2M2}(expt)=8.8 e{+2}fm{+4}MeV{+-1} {I50} 
$Coefficient |a{-M1E3}(expt)=36.4 e{+2}fm{+4}MeV{+-1} {I20} 


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$from {+138}La |e decay 
M$from ce data in {+138}La |e decay, |g(|q) and |g(pol) in (n,n'|g), and |g(|q) in (|a,2n|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$from {+138}Cs |b{+-} decay (32.5 m) 
M$from ce data in {+138}Cs |b{+-} decay (32.5 m), |g(|q) and |g(pol) in (n,n'|g), and |g(|q) in (|a,2n|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 (n,n'|g). Others: 191.96 {I6} from {+138}Cs |b{+-} decay (32.5 m), 191.94 {I9} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$observed only in singles spectrum by 1995Bo05 in (n,|g) E=thermal, not observed by 2003Go02 in (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:
E$weighted average of 112.50 {I10} from {+138}Cs |b{+-} decay (32.5 m), 112.5 {I3} from {+138}Cs |b{+-} decay (2.91 m), 112.6 {I3} from (|a,2n|g), 112.84 {I17} from (n,|g) E=thermal, 112.51 {I3} from (n,n'|g), and 112.1 {I5} from {+238}U({+12}C,F|g),{+208}Pb({+18}O,F|g). 
RI$from (n,n'|g) 
M$from ce data in |b{+-} decay (32.5 m) and |g(|q) in (|a,2n|g) and (n,n'|g) 
MR$from |g(|q) in (|a,2n|g). Other: -0.27 {I+12-10} from (n,n'|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:
E$weighted average of 782.08 {I9} from {+138}Cs|b{+-} decay (32.5 m), 782.8 {I4} from (n,|g) E=thermal, and 782.06 {I10} from (n,n'|g). 
RI$unweighted average of 2.16 {I20} from {+138}Cs |b{+-} decay (32.5 m), 2.57 {I14} from (n,|g) E=thermal, and 3.07 {I23} from (n,n'|g). 
MR$or +2.5 {I+7-4} (2003Go02) in (n,n'|g) 
M,MR$from |g(|q) and |g(pol) in (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:
E$from (n,n'|g). Others: 2218.00 {I10} from {+138}Cs |b{+-} decay (32.5 m), 2217.76 {I7} from (n,|g) E=thermal, 2218.0 {I10} from (|g,|g'), and 2217.86 {I2} from (n,n'|g). 
RI$from {+138}Cs|b{+-} decay (32.5 m) 
M$from (n,n'|g) based on |g(|q) and RUL 


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$weighted average of 408.98 {I6} from {+138}Cs |b{+-} decay (32.5 m), 408.8 {I2} from {+138}Cs |b{+-} decay (2.91 m), 408.9 {I3} from (|a,2n|g), 409.02 {I6} from (n,|g) E=thermal, and 408.96 {I2} from (n,n'|g). 
RI$weighted average of 91.2 {I18} from {+138}Cs |b{+-} decay (32.5 m) and 86 {I4} from (n,n'|g). Others: 76.9 {I4} from (n,|g) E=thermal, 52 {I3} from (|a,2n|g) 
M$from ce data in {+138}Cs |b{+-} decay (32.5 m), |g(|q) and |g(pol) in (n,n'|g), |g(|q) in (|a,2n|g) 
MR$from (n,n'|g). Others: -0.23 {I7} in (|a,2n|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$weighted average of 871.74 {I9} from (n,|g) E=thermal, 871.68 {I2} from (n,n'|g), 871.72 {I7} from {+138}Cs |b{+-} decay (32.5 m) 
RI$from {+138}Cs |b{+-} decay (32.5 m) 
M$from ce data in {+138}Cs |b{+-} decay (32.5 m), |g(|q) and |g(pol) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from (n,n'|g). Others: 107.5 {I3} from {+138}Cs |b{+-} decay (2.91 m), 107.3 {I3} (|a,2n|g) 
RI$weighted average of 16 {I8} from {+138}Cs |b{+-} decay, 7.1 {I24} from {+136}Xe(|a,2n|g), and 7.8 {I12} from {+138}Ba(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:
E$from (n,n'|g). Others: 212.34 {I8} from {+138}Cs |b{+-} decay (32.5 m), 212.0 {I3} from {+138}Cs |b{+-} decay (2.91 m), 212.3 {I3} from (|a,2n|g), 212.20 {I19} from (n,|g) E=thermal, 
RI$weighted average of 41 {I3} from {+138}Cs |b{+-} decay (32.5 m), 45 {I8} from {+138}Cs |b{+-} decay (2.91 m), and 34.9 {I28} from (n,n'|g). Others: 16.7 {I24} from (|a,2n|g), 16.7 {I9} (n,|g) E=thermal 
M,MR$D+Q from |g(|q) in (n,n'|g), polarity from no level-parity change determined from other experimental evidence 


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$unweighted average of 325.16 {I8} from (n,|g) E=thermal, 324.83 {I2} from (n,n'|g), 324.90 {I8} from {+138}Cs |b{+-} decay (32.5 m), 324.5 {I3} from {+138}Cs |b{+-} decay (2.91 m), 324.8 {I3} from (|a,2n|g) 
RI$unweighted average of 44 {I3} from (n,|g) E=thermal, 64 {I4} from (n,n'|g), 68 {I4} from {+138}Cs |b{+-} decay (32.5 m), 40.5 {I24} from (|a,2n|g) 
M$from ce data in {+138}Cs |b{+-} decay (32.5 m),|g(|q) and |g(pol) in (n,n'|g) 
MR$or -7.8 {I+16-18} in (n,n'|g). Others: -0.08 {I3} or -7.5 {I15} in (|a,2n|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$from (n,n'|g). Others: 516.71 {I12} from (n,|g) E=thermal, 516.74 {I12} from {+138}Cs |b{+-} decay (32.5 m), 516.7 {I4} from {+238}U({+12}C,F|g), 516.2 {I5} from {+138}Cs |b{+-} decay (2.91 m), 516.6 {I3} from (|a,2n|g) 
RI$from (|a,2n|g) 
M$from |g(|q) and |g(pol) in (n,n'|g) and (|a,2n|g) 
MR$from (|a,2n|g). Other: +0.059 {I7} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$weighted average of 138.08 {I6} from {+138}Cs |b{+-} decay (32.5 m), and 138.13 {I7} from (n,n'|g). 
E$unweighted average of 5.0 {I3} from {+138}Cs |b{+-} decay (32.5 m), and 10 {I1} from (n,n'|g). 
M$from ce data in {+138}Cs |b{+-} decay (32.5 m) 


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:
E$weighted average of 227.76 {I6} from {+138}Cs |b{+-} decay (32.5 m), 227.7 {I3} from (|a,2n|g), 227.7 {I3} from (n,|g) E=thermal, and 227.71 {I6} from (n,n'|g). 
RI$weighted average of 5.06 {I13} from {+138}Cs |b{+-} decay (32.5 m), 4 {I4} from (|a,2n|g), 4.4 {I4} from (n,|g) E=thermal, and 6.4 {I5} from (n,n'|g). 
M$from ce data in {+138}Cs |b{+-} decay (32.5 m) and |g(|q) in (n,n'|g) 
MR$or -5.6 {I+18-46} from (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:
E$weighted average of 546.990 {I15} from {+138}Cs |b{+-} decay (32.5 m), 546.9 {I3} from (|a,2n|g), 546.89 {I8} from (n,|g) E=thermal, and 546.93 {I3} from (n,n'|g). 
RI$weighted average of 36.1 {I8} from {+138}Cs |b{+-} decay (32.5 m), 24 {I4} from (|a,2n|g), 35.1 {I18} from (n,|g) E=thermal, and 39 {I3} from (n,n'|g). 
M$from ce data and |g(|q) in {+138}Cs |b{+-} decay (32.5 m), |g(|q) and |g(pol) in (n,n'|g) 
MR$from (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:
E$from (n,n'|g). Others: 1009.78 {I7} from {+138}Cs |b{+-} decay (32.5 m), 1009.80 {I8} from (n,|g) E=thermal, 1009.7 {I3} from (|a,2n|g) 
RI$from {+138}Cs |b{+-} decay (32.5 m) 
M$from ce data in {+138}Cs |b{+-} decay (32.5 m), |g(|q) in (|a,2n|g), |g(|q) and |g(pol) in (n,n'|g) 
MR$or -0.14 {I3} from (|a,2n|g). Others: -2.9 {I1} (1984Di03) and +0.018 {I7} (2003Go02) in (n,n'|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:
E$weighted average of 365.29 {I13} from {+138}Cs |b{+-} decay (32.5 m), and 365.10 {I11} from (n,n'|g). Other: 364.65 {I7} from (n,|g) E=thermal 
RI$weighted average of 15.3 {I19} from {+138}Cs |b{+-} decay (32.5 m), and 14.0 {I12} from (n,n'|g). Other: 26.5 {I14} from (n,|g) E=thermal for doublet (also placed from 2779 level) 
M$D(+Q) from |g(|q) in (n,n'|g), polarity from no level-parity change determined from other experimental evidence. 
MR$or |d= -2.6 {I+18-}|@ in (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:
E$weighted average of 1147.22 {I9} from {+138}Cs |b{+-} decay (32.5 m), 1147.1 {I3} from (|a,2n|g), 1147.20 {I13} from (n,|g) E=thermal, and 1147.16 {I3} from (n,n'|g). 
RI$from (n,|g) E=thermal. 
M,MR$from |g(|q) and |g(pol) in (n,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$weighted average of 2583.15 {I13} from {+138}Cs |b{+-} decay (32.5 m), 2583.02 {I16} from (n,|g) E=thermal, and 2582.96 {I10} from (n,n'|g). 
RI$weighted average of 19.2 {I12} from {+138}Cs |b{+-} decay (32.5 m), 25 {I5} from (n,|g) E=thermal, and 22.2 {I19} from (n,n'|g). 
M$D from |g(|q) in (n,n'|g), polarity from no level-parity change determined from other experimental evidence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E$from {+138}Cs |b{+-} decay (32.5 m). Other: 193.9 {I2} from (n,n'|g) 
RI$weighted average of 4.3 {I3} from {+138}Cs |b{+-} decay (32.5 m) and 4.9 {I4} from {+138}Ba(n,n'|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:
E$unweighted average of 421.59 {I7} from {+138}Cs |b{+-} decay (32.5 m), 421.87 {I13} from (n,|g) E=thermal, and 421.41 {I11} from (n,n'|g). 
RI$unweighted average of 5.6 {I3} from {+138}Cs |b{+-} decay (32.5 m), 5.1 {I6} from (n,|g) E=thermal, and 8.7 {I7} from (n,n'|g). 
M$D(+Q) from |g(|q) in (n,n'|g), polarity from no level-parity change determined from other experimental evidence 
MR$or +2.9 {I+18-9} in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1203.69 {I13} from {+138}Cs |b{+-} decay (32.5 m), 1204.4 {I3} from (|a,2n|g), 1203.1 {I20} from (n,|g) E=thermal, 1204.0 {I4} from (n,n'|g) 
RI$weighted average of 5.2 {I5} from {+138}Cs |b{+-} decay (32.5 m), 5.1 {I17} from (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:
E$weighted average of 2639.59 {I13} from {+138}Cs |b{+-} decay (32.5 m), 2639.26 {I4} from (n,|g) E=thermal, 2639.7 {I10} from (|g,|g'), and 2639.38 {I3} from (n,n'|g). 
RI$from {+138}Cs |b{+-} decay (32.5 m) 
M$Q from |g(|q) in (n,n'|g), M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 333.86 {I16} from {+138}Cs |b{+-} decay (32.5 m), 334.01 {I12} from (n,|g) E=thermal, and 333.68 {I8} from (n,n'|g). 
RI$weighted average of 7.8 {I13} from {+138}Cs |b{+-} decay (32.5 m), 13 {I7} from (n,|g) E=thermal, and 9.8 {I8} from (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=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:
E$weighted average of 363.93 {I8} from {+138}Cs |b{+-} decay (32.5 m), 363.9 {I3} from (|a,2n|g), and 363.90 {I4} from (n,n'|g). Other: 364.65 {I7} from (n,|g) E=thermal 
RI$weighted average of 21.3 {I20} from {+138}Cs |b{+-} decay (32.5 m), and 26 {I4} from (n,n'|g). Other: 48 {I3} from (n,|g) E=thermal for doublet (also placed from 2583 level), 10 {I3} from (|a,2n|g) 
M$D+Q from |g(|q) in (n,n'|g), polarity from no level-parity change determined from other experimental evidence 
MR$or -4.7 {I+6-9} in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 880.8 {I3} from {+138}Cs |b{+-} decay (32.5 m), 880.62 {I23} from (n,|g) E=thermal, and 880.77 {I10} from (n,n'|g). 
RI$weighted average of 10 {I3} from {+138}Cs |b{+-} decay (32.5 m), 9.3 {I17} from (n,|g) E=thermal, and 11.3 {I15} from (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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
E$weighted average of 1343.59 {I9} from {+138}Cs |b{+-} decay (32.5 m), 1343.4 {I3} from (|a,2n|g), 1343.43 {I10} from (n,|g) E=thermal, and 1343.54 {I3} from (n,n'|g). This peak could be an unresolved doublet with the second line associated with the de-excitation of the 3242 level, but that placement is uncertain. 
RI$from {+138}Cs |b{+-} decay (32.5 m) 
M$from |g(|q) and |g(pol) in (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=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:
E$weighted average of 953.0 {I3} from {+138}Cs |b{+-} decay (32.5 m), 952.7 {I3} from (|a,2n|g), 952.87 {I17} from (n,|g) E=thermal, and 952.85 {I11} from (n,n'|g). 
RI$weighted average of 14 {I4} from {+138}Cs |b{+-} decay (32.5 m), 17 {I4} from (|a,2n|g), 15.1 {I12} from (n,|g) E=thermal, and 14.2 {I12} from (n,n'|g). 
M$from |g(|q) and |g(pol) in (n,n'|g) 
MR$or -5 {I+2-9} in (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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
E$weighted average of 1415.68 {I13} from {+138}Cs |b{+-} decay (32.5 m), 1415.7 {I3} from (|a,2n|g), 1415.66 {I11} from (n,|g) E=thermal, and 1415.71 {I3} from (n,n'|g). 
RI$from (n,|g) E=thermal 
M$from |g(|q) and |g(pol) in (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_comment:
E$weighted average of 1445.04 {I25} from {+138}Cs |b{+-} decay (32.5 m), 1444.8 {I3} from (|a,2n|g), 1444.97 {I6} from (n,|g) E=thermal, and 1444.86 {I2} from (n,n'|g). 
RI$from (n,|g) E=thermal 
M$from |g(|q) and |g(pol) in (n,n'|g) 
MR$others: -0.14 {I6} or -3.0 {I4} from 1984Di03 in (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:
E$weighted average of 1495.63 {I23} from {+138}Cs |b{+-} decay (32.5 m), 1495.5 {I3} from (|a,2n|g), 1495.69 {I11} from (n,|g) E=thermal, and 1495.58 {I3} from (n,n'|g). 
RI$from (n,n'|g) 
M,MR$from |g(|q) and |g(pol) in (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:
E$weighted average of 2931.4 {I4} from {+138}Cs |b{+-} decay (32.5 m), 2930.9 {I8} from (n,|g) E=thermal, and 2931.3 {I3} from (n,n'|g). 
RI$unweighted average of 10.8 {I21} from {+138}Cs |b{+-} decay (32.5 m), 12.4 {I18} from (n,|g) E=thermal, and 7.2 {I11} from (n,n'|g). 
M$Q from |g(|q) in (n,n'|g), M2 ruled out by RUL 


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:
E$weighted average of 683.59 {I15} from {+138}Cs |b{+-} decay (32.5 m), 683.69 {I15} from (n,|g) E=thermal, and 683.78 {I13} from (n,n'|g). 
RI$unweighted average of 30 {I4} from {+138}Cs |b{+-} decay (32.5 m), 18.3 {I17} from (n,|g) E=thermal, and 48 {I3} from (n,n'|g). 
M$D+Q from |g(|q) in (n,n'|g), polarity from no level-parity change determined from other experimental evidence in (n,n'|g) 
MR$or -0.27 {I6} in (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=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:
E$weighted average of 773.31 {I10} from {+138}Cs |b{+-} decay (32.5 m), 773.42 {I15} from (n,|g) E=thermal, and 773.15 {I5} from (n,n'|g). 
RI$weighted average of 64 {I5} from {+138}Cs |b{+-} decay (32.5 m), 53 {I3} from (n,|g) E=thermal, and 58 {I5} from (n,n'|g). 
M$from |g(|q) and |g(pol) in (n,n'|g) 
MR$or -0.18 {I4} (2003Go02) in (n,n'|g). Other: -2.0 {I+4-6} (1984Di03) in (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=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:
E$weighted average of 1555.31 {I10} from {+138}Cs |b{+-} decay (32.5 m), 1555.54 {I18} from (n,|g) E=thermal, and 1555.24 {I3} from (n,n'|g). 
RI$from (n,|g) E=thermal 
M$from |g(|q) and |g(pol) in (n,n'|g) 
MR$from (n,n'|g) (2003Go02). Other: or 0.21 {I+4-3} (1984Di03) in (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:
E$weighted average of 1614.09 {I20} from {+138}Cs |b{+-} decay (32.5 m), 1614.0 {I3} from (|a,2n|g), 1614.26 {I12} from (n,|g) E=thermal, and 1614.07 {I3} from (n,n'|g). This |g is also placed from 3911 level in (n,|g) E=thermal, but that placement is not confirmed in other |g studies. 
RI$from (n,|g) E=thermal 
M$from |g(|q) and |g(pol) in (n,n'|g) 
MR$from 2003Go02 in (n,n'|g). Other: -008 {I5} or 3.1 {I+6-5} from from 1984Di03 in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 3049.9 {I3} from {+138}Cs |b{+-} decay (32.5 m) and 3049.27 {I5} from (n,|g) E=thermal. 
RI$weighted average of 23 {I3} from {+138}Cs |b{+-} decay (32.5 m) and 26.5 {I10} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 739.0 {I3} from (n,|g) E=thermal and 739.44 {I19} from (n,n'|g). 
RI$unweighted average of 34 {I8} from (n,|g) E=thermal and 54 {I5} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1064.0 {I3} from (|a,2n|g), 1064.5 {I3} from (n,|g) E=thermal, and 1064.11 {I10} from (n,n'|g). 
RI$unweighted average of 63 {I5} from (n,|g) E=thermal and 87 {I12} from (n,n'|g). 1995Bo05 in (n,|g) E=thermal also place this transition from the 4707 and 4115 levels but those placements are not confirmed in other |g studies. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1256.3 {I3} from (n,|g) E=thermal and 1256.22 {I10} from (n,n'|g). 
RI$from (n,n'|g), 100 {I8} from (n,|g) E=thermal 
M,MR$D+Q from |g(|q) in (n,n'|g), polarity from no level-parity change determined from other experimental evidence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 717.7 {I3} from {+138}Cs |b{+-} decay (32.5 m), 717.56 {I13} from (n,|g) E=thermal, and 717.67 {I17} from (n,n'|g). 
RI$weighted average of 16.9 {I13} from (n,|g) E=thermal, and 15.8 {I17} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 855.6 {I5} from {+138}Cs |b{+-} decay (32.5 m), 855.6 {I4} from (n,|g) E=thermal, and 855.7 {I3} from (n,n'|g). 
RI$weighted average of 9.2 {I8} from (n,|g) E=thermal, and 11.1 {I14} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 946.0 {I5} from {+138}Cs |b{+-} decay (32.5 m) and 945.3 {I3} from (n,|g) E=thermal. Not observed in (n,n'|g) 
RI$from (n,|g) E=thermal 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$weighted average of 1264.94 {I16} from {+138}Cs |b{+-} decay (32.5 m), 1264.7 {I3} from (|a,2n|g), 1264.29 {I25} from (n,|g) E=thermal, and 1264.67 {I10} from (n,n'|g). 
RI$weighted average of 64 {I4} from (n,|g) E=thermal, and 51 {I6} from (n,n'|g). This transition is observed as the strongest one in {+138}Cs |b{+-} decay (32.5 m), with I(1264.7|g)/I(1727.3|g)=123 {I15}/100 {I12} 
M$from |g(|q) in (n,n'|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:
E$unweighted average of 1727.68 {I18} from {+138}Cs |b{+-} decay (32.5 m), 1727.2 {I2} from (n,|g) E=thermal, and 1727.02 {I6} from (n,n'|g). 
RI$from (n,|g) E=thermal. Others: 100 {I9} from (n,n'|g) 
M$from |g(|q) and |g(pol) in (n,n'|g). 
MR$or 2.0 {I+5-3} in (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:
E$weighted average of 980.7 {I3} from (|a,2n|g), 980.7 {I3} from (n,n'|g), and 980.3 {I3} from {+238}U({+12}C,F|g),{+208}Pb({+18}O,F|g). 
RI$weighted average of 31.7 {I20} from (|a,2n|g), 42 {I7} from (n,n'|g), and 32 {I7} from {+238}U({+12}C,F|g),{+208}Pb({+18}O,F|g). 
M$Q from |g(|q) in (|a,2n|g) and M2 ruled out by RUL 


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$weighted average of 1093.3 {I3} from (|a,2n|g), 1093.1 {I3} from (n,n'|g), and 1092.7 {I3} from {+238}U({+12}C,F|g),{+208}Pb({+18}O,F|g). 
RI$from (|a,2n|g) 
M$Q from |g(|q) and |g(pol) in (|a,2n|g), M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 935.03 {I12} from {+138}Cs |b{+-} decay (32.5 m), 934.81 {I12} from (n,|g) E=thermal, and 934.78 {I9} from (n,n'|g). 
RI$from (n,n'|g). Others: 100 {I6} from (n,|g) E=thermal, 100 {I9} from {+138}Cs |b{+-} decay (32.5 m) 
M$from |g(|q) in (n,n'|g) 
MR$or +8 {I+6-3} in (n,n'|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$observed in the coincidence spectrum (1995Bo05) in (n,|g) E=thermal, could be unresolved with the 1343.54|g from 2779 level; placed by 1995Bo05 in (n,|g) E=thermal and 2003Go02 in (n,n'|g) but it is uncertain. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1806.65 {I18} from {+138}Cs |b{+-} decay (32.5 m), 1807.1 {I2} from (n,|g) E=thermal, and 1806.77 {I18} from (n,n'|g). 
RI$unweighted average of 51 {I6} from {+138}Cs |b{+-} decay (32.5 m), 79 {I6} from (n,n'|g). Other: 106 {I10} from (n,n'|g) E=thermal 
M$from |g(|q) in (n,n'|g) 
MR$or -28 {I+6-}|@ in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1359.1 {I5} from {+138}Cs |b{+-} decay (32.5 m), 1358.6 {I3} from (|a,2n|g), 1359.4 {I3} from (n,|g) E=thermal, and 1358.75 {I9} from (n,n'|g). 1995Bo05 in (n,|g) E=thermal also place this transition from a level at 4872 level, but it is not confirmed in other |g studies 
RI$weighted average of 62 {I25} from (|a,2n|g), 50 {I4} from (n,|g) E=thermal, and 65 {I4} from (n,n'|g). 
M$from |g(|q) in (n,n'|g) 
MR$or -50 {I+40-600} in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1821.7 {I3} from {+138}Cs |b{+-} decay (32.5 m), 1821.2 {I3} from (|a,2n|g), 1821.4 {I2} from (n,|g) E=thermal, and 1821.30 {I8} from (n,n'|g). 1995Bo05 in (n,|g) E=thermal also place this transition from a level at 2794 level, but it is not confirmed in other |g studies 
RI$from (n,n'|g) 
M$from |g(|q) in (n,n'|g) 
MR$or +4.2 {I+7-6} in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1903.2 {I4} from {+138}Cs |b{+-} decay (32.5 m), 1902.6 {I2} from (n,|g) E=thermal, and 1903.0 {I4} from (n,n'|g). 
RI$weighted average of 30 {I9} from {+138}Cs |b{+-} decay (32.5 m), 14.3 {I14} from (n,|g) E=thermal, and 11.0 {I15} from (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:
E$weighted average of 3339.01 {I25} from {+138}Cs |b{+-} decay (32.5 m), 3338.62 {I5} from (n,|g) E=thermal, 3338.4 {I15} from (|g,|g'),(pol |g,|g'), and 3338.81 {I8} from (n,n'|g). 
RI$from {+138}Cs |b{+-} decay (32.5 m) 
M$Q from |g(|q) in (n,n'|g), M2 ruled out by RUL 


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$weighted average of 944.2 {I3} from (|a,2n|g), 944.7 {I3} from (n,n'|g) and 944.0 {I5} from {+238}U({+12}C,F|g),{+208}Pb({+18}O,F|g) 
M$Q from |g(|q) in (|a,2n|g) and (n,n'|g), M2 ruled out by RUL 


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$weighted average of 3366.98 {I25} from {+138}Cs |b{+-} decay (32.5 m), 3366.67 {I10} from (n,|g) E=thermal, 3365.4 {I15} from (|g,|g'),(pol|g,|g'), and 3366.73 {I7} from (n,n'|g). 
RI$from (n,|g) E=thermal 
M$Q from |g(|q) in (n,n'|g) and M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1940.67 {I19} from (n,|g) E=thermal and 1940.76 {I9} from (n,n'|g). It is also placed from the 4131 level in (n,|g) E=thermal, but not confirmed in (n,n'|g) 
RI$from (n,n'|g) 
M,MR$from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 3442.6 {I6} from {+138}Cs |b{+-} decay (32.5 m), 3442.30 {I13} from (n,|g) E=thermal, and 3442.12 {I18} from (n,n'|g). 
RI$from (n,n'|g) 
M$from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2068.16 {I15} from (n,|g) E=thermal and 2068.1 {I4} from (n,n'|g). Also placed from 4707 level 
RI$from 39 {I13}, unweighted average of 26 {I4} from (n,|g) E=thermal and 52 {I6} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 3504.5 {25} from (n,|g) E=thermal and 3504.1 {I2} from (n,n'|g). 
RI$from (n,n'|g) 
M$Q from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
E,RI$from (n,n'|g) only 
M,MR$D+Q from |g(|q) in (n,n'|g), polarity from level-parity change determined by L(d,p)=3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2164.99 {I12} from (n,|g) E=thermal and 2164.8 {I3} from (n,n'|g). 
RI$from (n,n'|g). Other: I(2164.96|g)/I(3600.56|g)=56 {I10}/100 {I12} from (n,|g) E=thermal 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 3600.52 {I17} from (n,|g) E=thermal and 3600.7 {I3} from (n,n'|g). 
RI$from (n,n'|g) 
M$from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_comment:
E$weighted average of 1406.9 {I3} from (|a,2n|g) and 1407.1 {I4} from (n,n'|g). 
M$from |g(|q) in (|a,2n|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$weighted average of 438.6 {I3} from (|a,2n|g) and 438.3 {I3} from (n,n'|g). 
M$from |g(|q) and |g(pol) in (|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$weighted average of 449.2 {I3} from (|a,2n|g), 449.2 {I3} from (n,n'|g), and 449.1 {I3} from ({+12}C,F|g),({+18}O,F|g). 
M$from |g(|q) and |g(pol) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1744.6 {I2} from (n,|g) E=thermal and 1743.95 {I18} from (n,n'|g). 
RI$from (n,|g) E=thermal 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$from (n,|g) E=thermal only 
RI$from I|g in (n,|g) E=thermal only for unresolved 2207+2212 doublet 


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$unweighted average of 3643.3 {I4} from {+138}Cs |b{+-} decay (32.5 m), 3643.61 {I3} from (n,|g) E=thermal, 3642.7 {I15} from (|g,|g'),(pol |g,|g'), and 3642.8 {I2} from (n,n'|g) 
RI$from (n,|g) E=thermal, possible contribution due to strong 3641|g in {+139}Ba 
M$Q from |g(|q) in (n,n'|g), M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 766.10 {I12} from {+138}Cs |b{+-} decay (32.5 m), 766.09 {I21} from (n,|g) E=thermal, and 765.90 {I14} from (n,n'|g). 
RI$from (n,n'|g) 
M$from |g(|q) in (n,n'|g), polarity from level-parity change determined by L(d,p)=3 
MR$or +1.5 {I5} in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$from {+138}Cs |b{+-} decay (32.5 m), not observed in (n,n'|g). I|g is normalized to I|g(766.03|g)=100 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2210.7 {I4} from {+138}Cs |b{+-} decay (32.5 m), and 2210.9 {I3} from (n,n'|g). 
RI$from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 813.0 {I3} from {+138}Cs |b{+-} decay (32.5 m), 813.2 {I4} from (n,|g) E=thermal, and 813.0 {I4} from (n,n'|g). 
RI$from {+138}Cs |b{+-} decay (32.5 m) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 842.21 {I16} from {+138}Cs |b{+-} decay (32.5 m) and 842.8 {I3} from (n,|g) E=thermal. 
RI$from {+138}Cs |b{+-} decay (32.5 m) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1386.39 {I21} from {+138}Cs |b{+-} decay (32.5 m) and 1387.0 {I4} from (n,n'|g). 
RI$from {+138}Cs |b{+-} decay (32.5 m) 


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:
E$weighted average of 288.5 {I3} from (|a,2n|g) and 288.2 {I3} from ({+12}C,F|g),({+18}O,F|g). 
RI$unweighted average of 12 {I4} from (|a,2n|g) and 34 {I12} from ({+12}C,F|g),({+18}O,F|g). 
M,MR$from |g(|q) in (|a,2n|g), polarity from level-parity change determined fro other experimental evidence. 


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:
E$weighted average of 727.1 {I3} from (|a,2n|g) and 726.7 {I3} from ({+12}C,F|g),({+18}O,F|g). 
RI$from (|a,2n|g) 
M$from |g(|q) and |g(pol) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1041.4 {I3} from {+138}Cs |b{+-} decay (32.5 m) and 1041.51 {I11} from (n,|g) E=thermal. 
RI$weighted average of 54 {I14} from {+138}Cs |b{+-} decay (32.5 m) and 37 {I2} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$weighted average of 2023.93 {I20} from {+138}Cs |b{+-} decay (32.5 m), 2023.59 {I7} from (n,|g) E=thermal, and 2023.5 {I3} from (n,n'|g). 
RI$from (n,n'|g) E=thermal 
M$(D) from |g(|q) in (n,n'|g), polarity from level-parity change determined by L(d,p)=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2487.1 {I6} from {+138}Cs |b{+-} decay (32.5 m), 2486.48 {I17} from (n,|g) E=thermal, and 2486.1 {I8} from (n,n'|g). 
RI$weighted average of 19 {I7} from {+138}Cs |b{+-} decay (32.5 m), 17 {I2} from (n,|g) E=thermal, and 16 {I5} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1054.32 {I15} from {+138}Cs |b{+-} decay (32.5 m), 1054.9 {I3} from (n,|g) E=thermal, and 1054.2 {I2} from (n,n'|g). 
RI$from (n,n'|g). Others: 105 {I28} from {+138}Cs |b{+-} decay (32.5 m) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2499.4 {I3} from {+138}Cs |b{+-} decay (32.5 m), 2499.8 {I5} from (n,|g) E=thermal, and 2499.3 {I3} from (n,n'|g). 
RI$from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 4001.41 {I11} from (n,|g) E=thermal and 4001.2 {I4} from (n,n'|g). 
RI$from (n,n'|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:
E,RI$from (n,|g) E=thermal, also placed as primary transition 
M$from |g(lin pol) in (pol |g,|g') and |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 2806.57 {I17} from {+138}Cs |b{+-} decay (32.5 m), 2805.97 {I10} from (n,|g) E=thermal, and 2806.3 {I11} from (n,n'|g). 
RI$from (n,|g) E=thermal 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 4323.37 {I7} from (n,|g) E=thermal, 4323.0 {I7} from (|g,|g') and 4323.2 {I4} from (n,n'|g). 
M$from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 2062.34 {I17} from {+138}Cs |b{+-} decay (32.5 m) and 2061.5 {I4} from (n,|g) E=thermal. Also placed from 4280 level in (n,|g) E=thermal 
RI$from {+138}Cs |b{+-} decay (32.5 m) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2609.3 {I3} from {+138}Cs |b{+-} decay (32.5 m) and 2609.61 {I16} from (n,|g) E=thermal. 
RI$from {+138}Cs |b{+-} decay (32.5 m) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 3072.5 {I4} from {+138}Cs |b{+-} decay (32.5 m) and 3074.25 {I11} from (n,|g) E=thermal. 
RI$from {+138}Cs |b{+-} decay (32.5 m) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$placed only in (n,|g) E=thermal. Poor fit, inconsistent with level-energy difference=3100. The evaluator has considered this placement questionable. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4535.94 {I6} from (n,|g) E=thermal and 4535.1 {I6} from (|g,|g'),(pol |g,|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:
E$weighted average of 778.6 {I3} from (|a,2n|g) and 778.4 {I3} from ({+12}C,F|g),({+18}O,F|g). 
M$Q from |g(|q) in (|a,2n|g), M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$placed only by 1995Bo05 in (n,|g) E=thermal, not confirmed in other |g studies. See also 1821|g from 3258 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$placed only by 1995Bo05 in (n,|g) E=thermal, not confirmed in other |g studies. See also 3436|g from 3436 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$1435.8 {I4} (1977Ce04), 1435.70 {I7} (1979Ta21) 
M$(L+M+...)/K capture ratio=0.48 {I16} (1984Ma46); L/K=0.391 {I3}, M/K=0.102 {I3}, M/L=0.261 {I9} (2016Qu01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$others: 1000 {I44} (E|a=22 MeV), 1000 {I44} (E|a=24 MeV), 1000 {I46} (E|a=27 MeV) 
$A{-2}=+0.03 {I4}, A{-4}=+0.01 {I5} (1987Pr06); A{-2}=+0.09 {I12}, A{-4}=+0.09 {I13} (1973Ke07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$others: 472 {I14} (E|a=22 MeV), 547 {I16} (E|a=24 MeV), 546 {I16} (E|a=27 MeV) 
$POL1=+0.02 {I2}, POL2=+0.03 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$others: 29 {I1} (E|a=22 MeV), 34 {I1} (E|a=24 MeV), 37 {I1} (E|a=27 MeV) 
$A{-2}=+0.26 {I1}, A{-4}=-0.01 {I2} (1987Pr06); A{-2}=+0.23 {I8}, A{-4}=-0.19 {I9} (1973Ke07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$others: 13 {I1} (E|a=22 MeV), 10 {I1} (E|a=24 MeV), 11 {I1} (E|a=27 MeV) 
$A{-2}=+0.20 {I4}, A{-4}=+0.04 {I4} (1987Pr06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
RI$others: 6 {I1} (E|a=22 MeV), 5 {I1} (E|a=24 MeV), 4 {I1} (E|a=27 MeV) 
$A{-2}=-0.14 {I3}, A{-4}=-0.01 {I5} (1987Pr06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$others: 15 {I1} (E|a=22 MeV), 13 {I1} (E|a=24 MeV), 15 {I1} (E|a=27 MeV) 
$A{-2}=-0.04 {I3}, A{-4}=+0.04 {I4} (1987Pr06) 
MR$or -7.5 {I15} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$others: 41 {I2} (E|a=22 MeV), 33 {I1} (E|a=24 MeV), 28 {I5} (E|a=27 MeV) 
$A{-2}=-0.41 {I5}, A{-4}=-0.12 {I8} (1987Pr06) 
$POL1=-0.31 {I8}, POL2=-0.24 {I21} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$others: 20 {I2} (E|a=22 MeV), 12 {I1} (E|a=24 MeV), 10 {I3} (E|a=27 MeV) 
$A{-2}=-0.21 {I13}, A{-4}=+0.04 {I19} (1987Pr06) 
MR$or -0.14 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$others: 53 {I2} (E|a=22 MeV), 92 {I4} (E|a=24 MeV), 104 {I5} (E|a=27 MeV) 
M$Q from |g(|q) and M2 ruled out by RUL 
$A{-2}=+0.28 {I4}, A{-4}=-0.20 {I7} (1987Pr06); A{-2}=+0.3 {I2} (1973Ke07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$others: 153 {I6} (E|a=22 MeV), 281 {I11} (E|a=24 MeV), 315 {I1} (E|a=27 MeV) 
$A{-2}=+0.26 {I2}, A{-4}=-0.16 {I3} (1987Pr06); A{-2}=+0.15 {I10}, A{-4}=-0.02 {I2} (1973Ke07) 
$POL1=+0.36 {I5}, POL2=+0.41 {I13} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_comment:
RI$others: 15 {I1} (E|a=22 MeV), 16 {I1} (E|a=24 MeV), 10 {I3} (E|a=27 MeV) 
$A{-2}=-0.15 {I14}, A{-4}=+0.08 {I21} (1987Pr06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$others: 18 {I2} (E|a=22 MeV), 18 {I1} (E|a=24 MeV), 18 {I2} (E|a=27 MeV) 
M$Q from |g(|q) and M2 ruled out by RUL 
$A{-2}=+0.30 {I12}, A{-4}=-0.06 {I14} (1987Pr06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_comment:
RI$others: 19 {I2} (E|a=22 MeV), 23 {I3} (E|a=24 MeV), 34 {I5} (E|a=27 MeV) 
$A{-2}=+0.43 {I17}, A{-4}=+0.06 {I22} (1987Pr06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$others: 39 {I2} (E|a=22 MeV), 81 {I3} (E|a=24 MeV), 109 {I4} (E|a=27 MeV) 
$A{-2}=+0.22 {I1}, A{-4}=-0.05 {I2} (1987Pr06); A{-2}=+0.43 {I7}, A{-4}=+0.62 {I8} (1973Ke07). Note that A{-4} from 1973Ke07 indicates |DJ=1, inconsistent with Mult=E2, |DJ=2 
$POL1=+0.34 {I2}, POL2=+0.44 {I10} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$others: 24 {I1} (E|a=22 MeV), 44 {I2} (E|a=24 MeV), 50 {I3} (E|a=27 MeV) 
$A{-2}=-0.34 {I3}, A{-4}=-0.00 {I3} (1987Pr06) 
$POL1=-0.44 {I3}, POL2=+0.30 {I10} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$others: 5 {I1} (E|a=22 MeV), 7 {I1} (E|a=24 MeV), 9 {I1} (E|a=27 MeV) 
$A{-2}=-0.37 {I6}, A{-4}=+0.10 {I8} (1987Pr06) 
$POL1=-0.40 {I9} (E|a=22 MeV), POL2=+0.57 {I37} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$others: 6 {I1} (E|a=22 MeV), 13 {I1} (E|a=24 MeV), 20 {I1} (E|a=27 MeV) 
$A{-2}=+0.24 {I5}, A{-4}=-0.21 {I7} (1987Pr06); A{-2}=-0.4 {I4} (1973Ke07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$others: 51 {I2} (E|a=22 MeV), 68 {I3} (E|a=24 MeV), 114 {I5} (E|a=27 MeV) 
M$Q from |g(|q) and M2 ruled out by RUL 
$A{-2}=+0.24 {I11}, A{-4}=-0.07 {I14} (1987Pr06) 
$POL1=+0.37 {I23}, POL2=+0.45 {I62} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_comment:
RI$others: 2 {I1} (E|a=22 MeV), 6 {I1} (E|a=24 MeV), 7 {I2} (E|a=27 MeV) 
$A{-2}=-0.08 {I12}, A{-4}=+0.19 {I17} (1987Pr06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_comment:
RI$others: 2 {I1} (E|a=22 MeV), 2 {I1} (E|a=24 MeV), 2 {I1} (E|a=27 MeV) 
$A{-2}=-0.16 {I13}, A{-4}=-0.72 {I24} (1987Pr06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$others: 10 {I1} (E|a=22 MeV), 38 {I2} (E|a=24 MeV), 74 {I3} (E|a=27 MeV) 
M$Q from |g(|q) and M2 ruled out by RUL 
$A{-2}=+0.34 {I9}, A{-4}=-0.13 {I11} (1987Pr06); A{-2}=+0.3 {I2} (1973Ke07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1435.88 {I4} from 1990Is07 and 1435.82 {I7} from 1995Bo05. 
RI$from 1990Is07. 1995Bo05 normalize their I|g with respect to 1436|g, 5730|g of 1990Is07 and get I|g(1436|g)=417 {I23} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2217.73 {I5} from 1990Is07 and 2217.92 {I11} from 1995Bo05. 
RI$unweighted average of 80 {I3} from 1990Is07 and 60 {I6} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 2582.86 {I8} from 1990Is07 and 2583.18 {I8} from 1995Bo05. 
RI$weighted average of 7.3 {I13} from 1990Is07 and 4.7 {I7} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2639.27 {I4} from 1990Is07 and 2639.24 {I8} from 1995Bo05. 
RI$weighted average of 32.2 {I8} from 1990Is07 and 28.8 {I18} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 2795.68 {I14} from 1990Is07 and 2794.02 {I14} from 1995Bo05. 
RI$weighted average of 2.1 {I5} from 1990Is07 and 1.2 {I4} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1444.99 {I6} from 1990Is07 and 1444.90 {I12} from 1995Bo05. 
RI$unweighted average of 85 {I4} from 1990Is07 and 111 {I7} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2916.86 {I18} from 1990Is07 and 2917.3 {I3} from 1995Bo05. 
RI$unweighted average of 2.4 {I4} from 1990Is07 and 0.71 {I19} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1495.82 {I15} from 1990Is07 and 1495.62 {I11} from 1995Bo05. 
RI$unweighted average of 23 {I5} from 1990Is07 and 11.3 {I6} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 2931.69 {I21} from 1990Is07 and 2930.12 {I16} from 1995Bo05. 
RI$weighted average of 1.9 {I3} from 1990Is07 and 2.4 {I4} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3049.28 {I5} from 1990Is07 and 3049.12 {I17} from 1995Bo05. 
RI$weighted average of 5.28 {I22} from 1990Is07 and 5.5 {I7} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$placement indicated in Table 1 of 1995Bo05, but not placed by authors into the level scheme in Table 2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3338.60 {I5} from 1990Is07 and 3338.72 {I10} from 1995Bo05. 
RI$unweighted average of 16.8 {I8} from 1990Is07 and 11.6 {I14} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3366.74 {I9} from 1990Is07 and 3366.53 {I13} from 1995Bo05. 
RI$unweighted average of 5.8 {I5} from 1990Is07 and 3.9 {I5} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 3436.18 {I9} from 1990Is07 and 3436.61 {I19} from 1995Bo05. 
RI$from 1995Bo05. Other: 8.2 {I13} from 1990Is07 but it may have interference with {+136}Ba. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3442.34 {I13} from 1990Is07 and 3442.24 {I16} from 1995Bo05. 
RI$weighted average of 3.7 {I13} from 1990Is07 and 2.6 {I3} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 3504.02 {I6} from 1990Is07 and 3504.91 {I18} from 1995Bo05. 
RI$weighted average of 8.3 {I5} from 1990Is07 and 6.6 {I8} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3600.53 {I17} from 1990Is07 and 3600.5 {I3} from 1995Bo05. 
RI$weighted average of 1.9 {I3} from 1990Is07 and 2.01 {I24} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 2402.10 {I8} from 1990Is07 and 2401.46 {I11} from 1995Bo05. 
RI$9.1 {I11} from singles spectrum. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2023.55 {I7} from 1990Is07 and 2023.70 {I11} from 1995Bo05. 
RI$weighted average of 15.7 {I13} from 1990Is07 and 13.9 {I17} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 2500.27 {I32} from 1990Is07 and 2499.38 {I25} from 1995Bo05 
RI$5.7 {I32} from 1990Is07 (renormalized by 1995Bo05) and 1.64 {I19} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4001.37 {I8} from 1990Is07 and 4001.71 {I21} from 1995Bo05. Unassigned by 1990Is07 
RI$from 1995Bo05. Other: 6.0 {I7} from 1990Is07 (renormalized by 1995Bo05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 2577.45 {I22} from 1990Is07 and 2578.12 {I26} from 1995Bo05 
RI$2.8{I9} from 1990Is07 (renormalized by 1995Bo05) and 2.7 {I3} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4011.54 {I20} from 1990Is07 and 4012.7 {I6} from 1995Bo05. Unassigned by 1990Is07 
RI$1.7 {I3} from 1990Is07 (renormalized by 1995Bo05) and 1.64 {I22} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4025.85 {I7} from 1990Is07 and 4025.54 {I15} from 1995Bo05. 
RI$weighted average of 6.4 {I5} from 1990Is07 and 5.2 {I5} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 4082.95 {I6} from 1990Is07 and 4083.66 {I12} from 1995Bo05. 
RI$unweighted average of 6.6 {I4} from 1990Is07 and 9.2 {I6} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2679.64 {I8} from 1990Is07 and 2679.84 {I31} from 1995Bo05 
RI$from 1995Bo05. Other: 4.4{I7} from 1990Is07 (renormalized by 1995Bo05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 4114.76 {I10} from 1990Is07 and 4114.17 {I15} from 1995Bo05. 
RI$weighted average of 5.2 {I4} from 1990Is07 and 4.5 {I3} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4142.15 {I20} from 1990Is07 and 4143.0 {I6} from 1995Bo05. 
RI$weighted average of 0.84 {I16} from 1990Is07 and 0.88 {I17} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2762.34 {I8} from 1990Is07 and 2761.8 {I4} from 1995Bo05 
RI$from 1995Bo05. Other: 3.8 {I4} from 1990Is07 (renormalized by 1995Bo05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2806.14 {I22} from 1990Is07 and 2805.93 {I10} from 1995Bo05 
RI$5.0 {I5} from 1990Is07 (renormalized by 1995Bo05) and 4.8 {I8} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 2061.12 {I18} from 1990Is07 and 2061.84 {I12} from 1995Bo05. 
RI$weighted average of 2.7 {I7} from 1990Is07 and 3.3 {I4} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4280.28 {I8} from 1990Is07 and 4280.42 {I15} from 1995Bo05. 
E,RI$This |g is also placed as a primary transition in (n,|g) E=thermal. 1995Bo05 in (n,|g) E=thermal state that I|g(4280.31) in 4232-4280 cascade is less than 1 per 1000 neutron captures 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4323.39 {I7} from 1990Is07 and 4323.31 {I13} from 1995Bo05. 
E$weighted average of 2923.37 {I14} from 1990Is07 and 2923.96 {I11} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2895.67 {I9} from 1990Is07 and 2895.50 {I14} from 1995Bo05 
RI$3.3 {I3} from 1990Is07 (renormalized by 1995Bo05) and 3.8 {I5} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4332.21 {I6} from 1990Is07 and 4332.30 {I11} from 1995Bo05. 
RI$weighted average of 13.5 {I6} from 1990Is07 and 12.4 {I6} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 2923.37 {I14} from 1990Is07 and 2923.96 {I11} from 1995Bo05. 
RI$weighted average of 2.5 {I5} from 1990Is07 and 2.8 {I7} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4445.38 {I5} from 1990Is07 and 4445.61 {I16} from 1995Bo05. 
RI$weighted average of 5.9 {I3} from 1990Is07 and 5.2 {I6} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2609.56 {I16} from 1990Is07 and 2609.8 {I3} from 1995Bo05. 
RI$weighted average of 1.1 {I3} from 1990Is07 and 1.14 {I14} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 3074.29 {I11} from 1990Is07 and 3074.1 {I2} from 1995Bo05. Placed by 1990Is07; not placed by 1995Bo05. 
RI$weighted average of 2.01 {I21} from 1990Is07 and 2.6 {I5} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$poor fit, inconsistent with level-energy difference=3100. The placement is considered questionable. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4535.93 {I6} from 1990Is07 and 4536.02 {I24} from 1995Bo05. 
RI$weighted average of 3.85 {I15} from 1990Is07 and 4.10 {I25} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3129.5 {I7} from 1990Is07 and 3129.5 {I5} from 1995Bo05. Unassigned by 1990Is07 
RI$1.5 {I8} from 1990Is07 (renormalized by 1995Bo05) and 2.3 {I3} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3144.28 {I21} from 1990Is07 and 3143.84 {I14} from 1995Bo05. Unassigned by 1990Is07 
RI$2.0 {I5} from 1990Is07 (renormalized by 1995Bo05) and 4.0 {I10} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3230.01 {I9} from 1990Is07 and 3230.00 {I14} from 1995Bo05. Unassigned by 1990Is07 
RI$from 1995Bo05. Other: 2.8 {I7} from 1990Is07 (renormalized by 1995Bo05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4664.12 {I11} from 1990Is07 and 4664.3 {I15} from 1995Bo05. Unassigned by 1990Is07 
RI$from 1995Bo05. Other: 0.99 {I11} from 1990Is07 (renormalized by 1995Bo05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3359.9 {I3} from 1990Is07 and 3360.5 {I4} from 1995Bo05. Unassigned by 1990Is07 
RI$1.1 {I3} from 1990Is07 (renormalized by 1995Bo05) and 1.12 {I15} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4855.11 {I14} from 1990Is07 and 4855.1 {I5} from 1995Bo05. Unassigned by 1990Is07 
RI$weighted average of 1.55 {I29} from 1990Is07 (renormalized by 1995Bo05) and 1.7 {I13} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 3436.18 {I9} from 1990Is07 and 3436.61 {I19} from 1995Bo05. Placement is made by 1995Bo05 only 
RI$from 1995Bo05. Other: 8.2 {I13} from 1990Is07 but it may have interference with {+136}Ba. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 3738.22 {I7} from 1990Is07 and 3739.53 {I15} from 1995Bo05. 
RI$unweighted average of 5.5 {I3} from 1990Is07 and 2.7 {I8} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 3815.59 {I8} from 1990Is07 and 3813.29 {I17} from 1995Bo05. 
RI$weighted average of 3.5 {I3} from 1990Is07 and 3.9 {I6} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3868.54 {I17} from 1990Is07 and 3867.9 {I6} from 1995Bo05. 
RI$weighted average of 1.8 {I5} from 1990Is07 and 1.81 {I23} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 3945.81 {I8} from 1990Is07 and 3946.17 {I15} from 1995Bo05. 
RI$unweighted average of 6.0 {I6} from 1990Is07 and 3.7 {I7} from 1995Bo05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 3965.28 {I6} from 1990Is07 and 3964.92 {I14} from 1995Bo05. 
RI$weighted average of 4.31 {I18} from 1990Is07 and 4.7 {I3} from 1995Bo05. 


