# DECAY

decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
E from ({+3}He,2np|g); E|g given as 646.8 {I10} in ({+40}Ca,5pn|g) for unresolved component of doublet. 
M,MR D+Q from |g(|q) in ({+3}He,2np|g); however, 647|g is a doublet in ({+40}Ca,5pn|g), so |d may not be reliable. E1 is favored over M1 because B(M1)(W.u.)=2.55|*10{+-5} 17 would be atypically small. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E from ({+3}He,2np|g). E|g=545.0 {I10} in ({+40}Ca,5pn|g). 
M D+Q from |g(|q) in ({+3}He,2np|g); |D|p from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M Q from ({+40}Ca,5pn|g). D from unenumerated DCO ratio in ({+35}Cl,4p3n|g), where I(1067|g)/I(521|g) is much larger than in ({+40}Ca,5pn|g); this may indicate that 1067|g is a doublet in ({+35}Cl,4p3n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from ({+35}Cl,4p3n|g); however, I|g<52 {I10} from ({+40}Ca,5pn|g) (where |g is complex). 
M Q (interpreted as M2) in ({+35}Cl,4p3n|g), but D from ({+40}Ca,5pn|g). However, if M2 and I|g|?50, T{-1/2}(3563 level) exceeds |?5 ns (based on RUL). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E|g from ({+35}Cl,4p3n|g). Based on strength of this |g, the evaluator suggests that it might be a doublet in this reaction. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
I|g=57 {I6}, anisotropy ratio=0.84 {I12} for 668.5|g+668.7|g. From adopted branching from the 1355 level, I(669|g from 1355)=29 {I4} and, therefore, I(669|g from 4716)=28 {I7}. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
I|g=57 {I6}, anisotropy ratio=0.84 {I12} for 668.5|g+668.7|g. See comment on 669|g from 1355 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
1995Gh02 do not consider this |g to be a doublet; however, see comment on E(2002 levels) in Adopted Levels. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI from (|a,p2n|g). 
E weighted average of 711.09 {I11} from (|a,p2n|g) and 711.3 {I3} from |e decay (59.7 s). 


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:
CC a calculated value of 8900 is quoted in 1978Br25; this would imply B(E1)(W.u.)=4.|*10{+-8} {I4}. 
E from energy shift between prompt and delayed 750|g peaks in (|a,p2n|g). Other E|g: 0.44 {I2} (1976Br08) in (|a,2pn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2+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_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
E,RI from (|a,p2n|g). 
M possible parity-violating E2 component <6%; from ({+32}S,2n2p|g). 
0|' -180|' asymmetry A{-|g}=4.1|*10{+-4} {I20} (2005Na28), 8.4|*10{+-4} {I27} (1996Ha13) from {+45}Sc({+52}Cr,2p2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E from (|a,p2n|g); 1723.0 in ({+40}Ca,5p|g), 1722.4 in ({+31}P,2p2n|g). 
M |DJ=0 transition from ({+40}Ca,5p|g). |DJ=2 assumed in ({+31}P,2p2n|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 from (|a,p2n|g) (where |g is placed differently); 70.4 from ({+40}Ca,5p|g). 
M D from ({+40}Ca,5p|g); |D|p=(no) from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
%I|g=58.3 {I9}. 
|a(K)exp: weighted average of 0.20 {I5} (1974Ch12) and 0.31 {I7} (1953Ea04). 
K/(L+M)=5.8 {I3} (1953Ea04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 1 |ms<T{-1/2}<10 |ms for 40% of I|g (1973Gr31). 
M A{-2}=+0.247 {I6}, A{-4}=-0.043 {I10}, polarization=+0.37 {I5} (1978Br25). A{-2}=+0.17 {I2}, A{-4}=-0.02 {I4} (1973Gr31). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI 1 |ms<T{-1/2}<10 |ms for 67% of I|g (1973Gr31). 
M A{-2}=-0.086 {I11}, A{-4}=+0.155 {I17}, polarization=+0.09 {I8} (1978Br25). A{-2}=-0.15 {I3}, A{-4}=+0.11 {I4} (1973Gr31). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI 1 |ms<T{-1/2}<10 |ms for 72% of I|g (1973Gr31). 
RI Branching=48.1 {I15} (1976Br08). 
M A{-2}=-0.185 {I8}, A{-4}=+0.019 {I14}, polarization=+0.23 {I3} (1978Br25). A{-2}=-0.15 {I2}, A{-4}=0.00 {I3} (1973Gr31). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI 1 |ms<T{-1/2}<10 |ms for 73% of I|g (1973Gr31). 
RI Branching=100.0 {I15} (1976Br08). 
A{-2}=+0.312 {I6}, A{-4}=+0.002 {I10}, polarization=-0.48 {I3} (1978Br25). A{-2}=+0.10 {I2}, A{-4}=0.00 {I3} (1973Gr31). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI for doublet. 1 |ms<T{-1/2}<10 |ms for 22% of I|g(doublet) (1973Gr31). 
E from 1976Br08; E=750.38 {I20} from the difference of E(0.31|g) and E(750.7|g). 
M from |a(K)exp. A{-2}=+0.24, A{-4}=-0.05 (1978Br25). 1973Gr31 report A{-2}=+0.12 {I1}, A{-4}=-0.07 {I2} for doublet. 


decay_energy_unit: KEV
decay_multipolarity: [E1]
decay_comment:
E weighted average of 0.32 keV {I3} (1978Br16) and 0.30 keV {I3} (1978Br25), both from the energy shift of the 750|g peaks in prompt and delayed |g spectra. Other: 0.44 {I2} (1976Br08). 
Branching: from angular dependence of E(750|g doublet) in delayed spectra relative to E(756.23|g, {+94}Ru), 1978Br25 deduce that I(|g+ce)(0.31)/I(|g+ce)(750.7)=0.03 {I3}. 
CC calculated value quoted in 1978Br25. 


decay_energy_unit: KEV
decay_multipolarity: M2+E3
decay_comment:
E from 1976Br08. Others: 750.78 {I15} (1977Ha49), 750.8 {I3} (1978Br16) (for doublet). 
I(750.7|g+0.31|g):I(40|g)=26.3 {I10}:73.7 {I10} (1976Br08). 
M from |a(K)exp. Possible parity-violating E2 component <6% (1978Br25). 
A{-2}=-0.191 {I8}, A{-4}=-0.262 {I13}, polarization=+0.23 {I4} (1978Br25). 
0|' -180|' asymmetry A{-|g}=4.1|*10{+-4} {I20} (2005Na28), 8.4|*10{+-4} {I27} (1996Ha13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_uncertain: ?
decay_comment:
A{-2}=-0.11 {I8}, A{-4}=0.0 (1973Gr31). |g placed differently in Adopted Levels, Gammas. 
Not included in Adopted Gammas. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$A 680 keV peak observed from the gated prompt gammas (prompt gamma transitions depopulating compound state to 1408 keV and 1434 keV levels) spectra suggests a 513 keV transition which is inseparable from the 511 keV annihilation peak 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$A 1194 keV peak observed from the gated prompt gammas (prompt gamma transitions depopulating compound state to 1408 keV and 1434 keV levels) spectra suggests a 213 keV transition. A gate on 1194 keV transition revealed a small peak at 213 keV 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E$The 836 |g was not observed in coincidence with the 680 keV |g transition which is probably due to the very small population of this state 


decay_energy_unit: KEV
decay_uncertain: S
decay_comment:
E$deduced from adopted levels, |g has not been experimentally observed. 
TI$from I|g(76|g)/I|g(871|g, {+94}Mo)<0.1%. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 336.40 {I10} ({+95}Ru |e decay), 336.48 {I5} ({+93}Nb(|a,2n|g)), 336.40 {I4} ({+95}Mo(p,n),(p,n|g)) 
M$from {+93}Nb(|a,2n|g) 
MR$from {+95}Mo(p,n),(p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 290.38 {I10} ({+95}Ru |e decay), 290.54 {I5} ({+93}Nb(|a,2n|g)), 290.33 {I3} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 20.7 {I6} ({+95}Ru |e decay), 21.65 {I24} ({+93}Nb(|a,2n|g)) 
M$D+Q from {+93}Nb(|a,2n|g), adopting (M1+E2) from level scheme 
MR$from {+93}Nb(|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2(+M3))
decay_comment:
M$Q(+O) from |g(|q) in (|a,2n|g), |D|p=no from level scheme 
MR$from |a(K)exp in (|a,2n|g) assuming E2+M3. Sign may be negative since |d=-0.58 |@ from |g(|q) in (|a,2n|g). 
E$weighted average of 626.83 {I10} ({+95}Ru |e decay), 626.8 {I1} ({+93}Nb(|a,2n|g)), 626.73 {I6} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 607.3 {I5} ({+95}Ru |e decay), 607.82 {I15} ({+93}Nb(|a,2n|g)), 607.56 {I6} ({+95}Mo(p,n),(p,n|g)) 
M$d(+Q) in {+93}Nb(|a,2n|g), adopting (M1) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 331.39 {I9} ({+95}Ru |e decay), 331.37 {I10} ({+95}Mo(p,n),(p,n|g)) 
RI$from {+95}Mo(p,n),(p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
M,MR$from |a(K)exp in (|a,2n|g). Sign may be negative since |d=-0.11 |@ from |g(|q) in (|a,2n|g). 
E$weighted average of 629.0 {I1} ({+93}Nb(|a,2n|g)), 628.92 {I6} ({+95}Mo(p,n),(p,n|g)) 
RI$from {+95}Mo(p,n),(p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
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 x (fm)^4
decay_BM_info: ;TYPE=BM3;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM3W
decay_comment:
M,MR$from |g(|q) in (|a,2n|g) and comparison to RUL. Possibly stretched or |DJ=0 Q 
E$weighted average of 882.36 {I10} ({+93}Nb(|a,2n|g)), 882.10 {I6} ({+95}Mo(p,n),(p,n|g)), 882.3 {I4} ({+65}Cu({+36}S,|a2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M,MR$D+Q from |g(|q) in (p,n|g). |D|p=no from the level scheme 
E$weighted average of 301.01 {I10} ({+95}Ru |e decay), 301.11 {I6} ({+93}Nb(|a,2n|g)), 300.95 {I4} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 100.0 {I7} ({+93}Nb(|a,2n|g)), 100.0 {I9} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2(+M3))
decay_comment:
M$Q(+O) from |g(|q) in (p,n|g). |D|p=no from the level scheme 
E$weighted average of 591.42 {I10} ({+95}Ru |e decay), 591.36 {I7} ({+93}Nb(|a,2n|g)), 591.50 {I8} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 56.3 {I23} ({+95}Ru |e decay), 53.8 {I4} ({+93}Nb(|a,2n|g)), 51.7 {I4} ({+95}Mo(p,n),(p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$D from |g(|q) in (p,n|g). |D|p=yes from level scheme 
E$weighted average of 889.00 {I10} ({+95}Ru |e decay), 888.86 {I11} ({+93}Nb(|a,2n|g)), 888.90 {I5} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 91 {I5} ({+95}Ru |e decay), 67.5 {I11} ({+93}Nb(|a,2n|g)), 61.1 {I15} ({+95}Mo(p,n),(p,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$weighted average of 956.6 {I2} ({+95}Ru |e decay), 957.12 {I10} ({+93}Nb(|a,2n|g)), 956.6 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$from (|a,2n|g) 
M,MR$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 748.68 {I16} ({+93}Nb(|a,2n|g)), 748.55 {I5} ({+95}Mo(p,n),(p,n|g)) 
RI$from (|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:
M,MR$D+Q from |g(|q) in (p,n|g). |=E1+M2 from |d and comparison to RUL 
E$weighted average of 551.62 {I10} ({+95}Ru |e decay), 551.8 {I2} ({+93}Nb(|a,2n|g)), 551.76 {I5} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 33.1 {I12} ({+95}Ru |e decay), 47 {I3} ({+93}Nb(|a,2n|g)), 54.1 {I10} ({+95}Mo(p,n),(p,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$weighted average of 842.16 {I10} ({+95}Ru |e decay), 842.2 {I2} ({+93}Nb(|a,2n|g)), 842.19 {I8} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 24.6 {I10} ({+95}Ru |e decay), 35 {I4} ({+93}Nb(|a,2n|g)), 41.2 {I8} ({+95}Mo(p,n),(p,n|g)) 
M,MR$D+Q from |g(|q) in (p,n|g). |=E1+M2 from 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:
E$weighted average of 1178.7 {I2} ({+95}Ru |e decay), 1178.80 {I22} ({+93}Nb(|a,2n|g)), 1178.66 {I6} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 100 {I5} ({+95}Ru |e decay), 100 {I5} ({+93}Nb(|a,2n|g)), 100.0 {I14} ({+95}Mo(p,n),(p,n|g)) 
M,MR$D+Q from |g(|q) in (p,n|g). |=E1+M2 from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 876.7 {I3} ({+95}Ru |e decay), 876.8 {I2} ({+93}Nb(|a,2n|g)), 876.81 {I10} ({+95}Mo(p,n),(p,n|g)) 
RI$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1213.10 {I10} ({+93}Nb(|a,2n|g)), 1212.8 {I2} ({+95}Mo(p,n),(p,n|g)) 
RI$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
MR$from (|a,2n|g), other: |d=+0.50 {I+13-9} from |g(|q) in (p,n|g) discrepant 
E$weighted average of 546.73 {I5} ({+93}Nb(|a,2n|g)), 546.71 {I5} ({+95}Mo(p,n),(p,n|g)), 547.0 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$weighted average of 878.27 {I24} ({+93}Nb(|a,2n|g)), 878.36 {I10} ({+95}Mo(p,n),(p,n|g)) 
RI$from (|a,2n|g) 
M$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 1214.55 {I11} ({+93}Nb(|a,2n|g)), 1214.37 {I10} ({+95}Mo(p,n),(p,n|g)), 1215.1 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$from (|a,2n|g) 
M$from ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$weighted average of 1236.5 {I3} ({+95}Ru |e decay), 1236.91 {I8} ({+95}Mo(p,n),(p,n|g)) 
RI,M,MR$from {+95}Mo(p,n),(p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 613.73 {I10} ({+93}Nb(|a,2n|g)), 613.67 {I5} ({+95}Mo(p,n),(p,n|g)) 
RI$from (|a,2n|g) 
M$D from (p,n|g), adopting (M1) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$D+Q from |g(|q) in (p,n|g). |D|p=yes from level scheme 
E$weighted average of 945.06 {I6} ({+93}Nb(|a,2n|g)), 945.03 {I10} ({+95}Mo(p,n),(p,n|g)) 
RI$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$D+Q from |g(|q) in (p,n|g). |D|p=yes from level scheme 
E$weighted average of 1281.6 {I3} ({+93}Nb(|a,2n|g)), 1281.52 {I10} ({+95}Mo(p,n),(p,n|g)) 
RI$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 254.58 {I20} ({+95}Ru |e decay), 254.35 {I20} ({+95}Mo(p,n),(p,n|g)) 
RI$from {+95}Ru |e decay 
M$from |g(|q) in (p,n|g) and level scheme 


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$weighted average of 348.20 {I10} ({+95}Ru |e decay), 348.44 {I20} ({+95}Mo(p,n),(p,n|g)) 
RI$from {+95}Ru |e decay 
M$from |g(|q) in (p,n|g) and level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 504.8 {I3} ({+95}Ru |e decay), 505.4 {I3} ({+95}Mo(p,n),(p,n|g)) 
RI$from {+95}Ru |e decay 
M$from |g(|q) in (p,n|g) and level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 806.28 {I10} ({+95}Ru |e decay), 806.32 {I5} ({+95}Mo(p,n),(p,n)) 
RI$from {+95}Ru |e decay 
M$from |g(|q) in (p,n|g) and 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=GE;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GE
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GE;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GE
decay_comment:
M$D+Q from |g(|q) in (p,n|g). |=E1+M2 from |d and comparison to RUL 
E$weighted average of 1096.80 {I10} ({+95}Ru |e decay), 1096.73 {I8} ({+95}Mo(p,n),(p,n|g)) 
RI$from {+95}Ru |e 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$weighted average of 1433.28 {I10} ({+95}Ru |e decay), 1433.10 {I10} ({+95}Mo(p,n),(p,n|g)) 
RI$from {+95}Ru |e decay 
M$from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
E$weighted average of 632.88 {I18} ({+93}Nb(|a,2n|g)), 633.3 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$weighted average of 100 {I4} ({+93}Nb(|a,2n|g)), 100 {I10} ({+65}Cu({+36}S,|a2n|g)) 
M,MR$from (|a,2n|g); supported by deduced R=1.9 {i2} from ({+65}Cu({+36}S,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
E$weighted average of 592.50 {I7} ({+93}Nb(|a,2n|g)), 593.0 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$weighted average of 100 {I4} ({+93}Nb(|a,2n|g)), 100 {I10} ({+65}Cu({+36}S,|a2n|g)) 
M,MR$from deduced R=1.8 {i2} ({+65}Cu({+36}S,|a2n|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$weighted average of 667.15 {I9} ({+93}Nb(|a,2n|g)), 667.3 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$weighted average of 90 {I3} ({+93}Nb(|a,2n|g)), 83 {I10} ({+65}Cu({+36}S,|a2n|g) 
M,MR$from (|a,2n|g); supported by deduced R=1.6 {i2} from ({+65}Cu({+36}S,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 711.54 {I20} ({+95}Ru |e decay), 711.61 {I5} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 100 {I11} ({+95}Ru |e decay), 100.0 {I17} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_uncertain: ?
decay_comment:
E$weighted average of 992.3 {I7} ({+95}Ru |e decay), 992.33 {I70} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 15 {I4} ({+95}Ru |e decay), 14.9 {I23} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 606.3 {I5} ({+95}Ru |e decay), 606.3 {I5} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 10 {I4} ({+95}Ru |e decay), 11.4 {I12} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1064.39 {I10} ({+95}Ru |e decay), 1064.42 {I6} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 95 {I8} ({+95}Ru |e decay), 81.6 {I10} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1355.1 {I2} ({+95}Ru |e decay), 1354.7 {I8} ({+93}Nb(|a,2n|g)), 1355.10 {I20} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 100 {I6} ({+95}Ru |e decay), 100 {I4} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1691.4 {I2} ({+95}Ru |e decay), 1691.35 {I10} ({+95}Mo(p,n),(p,n|g 
RI$weighted average of 11.4 {I13} ({+95}Ru |e decay), 13.6 {I6} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 487.75 {I7} ({+93}Nb(|a,2n|g)), 487.0 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$from ({+93}Nb(|a,2n|g)) 
M,MR$from (|a,2n|g); supported by deduced R=1.9 {i3} from ({+65}Cu({+36}S,|a2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
E$weighted average of 744.97 {I9} ({+93}Nb(|a,2n|g)), 745.5 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$from ({+93}Nb(|a,2n|g)) 
M$from ({+65}Cu({+36}S,|a2n|g)) and level scheme; Intensity ratio R not consistent with M1 assignment 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 819.07 {I10} ({+95}Ru |e decay), 819.3 {I1} ({+95}Mo(p,n),(p,n|g)) 
RI$from {+95}Ru |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1120.11 {I10} ({+95}Ru |e decay), 1120.3 {I2} ({+95}Mo(p,n),(p,n|g)) 
RI,M$from {+95}Ru |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1410.63 {I10} ({+95}Ru |e decay), 1410.58 {I8} ({+95}Mo(p,n),(p,n|g)) 
RI$from {+95}Ru |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 893.3 {I2} ({+95}Ru |e decay), 893.86 {I10} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 6 {I3} ({+95}Ru |e decay), 16.1 {I17} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1050.68 {I10} ({+95}Ru |e decay), 1050.75 {I5} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 100 {I4} ({+95}Ru |e decay), 100.0 {I15} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1351.9 {I2} ({+95}Ru |e decay), 1351.8 {I2} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 32.7 {I23} ({+95}Ru |e decay), 30.2 {I18} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1642.0 {I2} ({+95}Ru |e decay), 1642.0 {I3} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 3.8 {I4} ({+95}Ru |e decay), 3.9 {I3} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$D in (p,n|g), (M1) assignment from level scheme 
E$weighted average of 652.81 {I10} ({+95}Ru |e decay), 652.72 {I5} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 48.6 {I19} ({+95}Ru |e decay), 49 {I4} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$D, E2 in (p,n|g), (M1+E2) assignment from level scheme 
E$weighted average of 1158.4 {I1} ({+95}Ru |e decay), 1158.38 {I4} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 40 {I9} ({+95}Ru |e decay), 78 {I7} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$D, E2 in (p,n|g), (M1+E2) assignment from level scheme 
E$weighted average of 1459.32 {I10} ({+95}Ru |e decay), 1459.10 {I6} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 100 {I6} ({+95}Ru |e decay), 100.0 {I22} ({+95}Mo(p,n),(p,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=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$D, Q in (p,n|g), (E1) from level scheme 
E$weighted average of 2047.1 {I2} ({+95}Ru |e decay), 2046.9 {I2} ({+95}Mo(p,n),(p,n|g)) 
RI$from {+95}Ru |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 735.1 {I2} ({+95}Ru |e decay), 734.85 {I6} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 66 {I3} ({+95}Ru |e decay), 78 {I3} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
E$weighted average of 989.72 {I10} ({+95}Ru |e decay), 989.77 {I6} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 100 {I4} ({+95}Ru |e decay), 100.0 {I22} ({+95}Mo(p,n),(p,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$weighted average of 1240.4 {I2} ({+95}Ru |e decay), 1240.4 {I2} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 11 {I7} ({+95}Ru |e decay), 11.3 {I13} ({+95}Mo(p,n),(p,n|g)) 
M$D,E2 from (p,n|g), adopting (E2) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
E$weighted average of 1541.3 {I2} ({+95}Ru |e decay), 1541.27 {I10} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 39 {I3} ({+95}Ru |e decay), 40.9 {I22} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
E$weighted average of 1831.9 {I2} ({+95}Ru |e decay), 1831.7 {I2} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 34 {I3} ({+95}Ru |e decay), 34.1 {I22} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
E$weighted average of 2168.1 {I3} ({+95}Ru |e decay), 2168.27 {I30} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 6.5 {I8} ({+95}Ru |e decay), 4.8 {I11} ({+95}Mo(p,n),(p,n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
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$weighted average of 634.5 {I1} ({+93}Nb(|a,2n|g)), 634.0 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$from {+93}Nb(|a,2n|g); other: 100 {I10} ({+65}Cu({+36}S,|a2n|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$weighted average of 668.57 {I9} ({+93}Nb(|a,2n|g)), 668.0 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$from {+93}Nb(|a,2n|g); other: 57 {I5} ({+65}Cu({+36}S,|a2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 755.86 {I10} ({+95}Ru |e decay), 755.8 {I1} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 30 {I3} ({+95}Ru |e decay), 37 {I5} ({+95}Mo(p,n),(p,n|g)) 
M$from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1010.57 {I10} ({+95}Ru |e decay), 1010.44 {I8} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 100 {I4} ({+95}Ru |e decay), 100 {I3} ({+95}Mo(p,n),(p,n|g)) 
M$from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1562.3 {I2} ({+95}Ru |e decay), 1562.35 {I20} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 21.9 {I14} ({+95}Ru |e decay), 12.4 {I17} ({+95}Mo(p,n),(p,n|g)) 
M$from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted average of 1852.8 {I2} ({+95}Ru |e decay), 1852.5 {I2} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 16.4 {I14} ({+95}Ru |e decay), 17.0 {I9} ({+95}Mo(p,n),(p,n|g)) 
M$from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_comment:
E$weighted average of 2189.3 {I3} ({+95}Ru |e decay), 2188.9 {I2} ({+95}Mo(p,n),(p,n|g)) 
RI$weighted average of 5.6 {I8} ({+95}Ru |e decay), 5.4 {I9} ({+95}Mo(p,n),(p,n|g)) 
M$from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$from |a(K)exp in (|a,2n|g) 
E$weighted average of 510.8 {I5} ({+93}Nb(|a,2n|g)), 511.0 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$from (|a,2n|g); other: 38 {I4} (({+36}S,|a2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_comment:
E$weighted average of 663.43 {I12} ({+93}Nb(|a,2n|g)), 663.5 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$from (|a,2n|g); other: 38 {I4} (({+36}S,|a2n|g)) 
M$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1182.8 {I3} ({+95}Ru |e decay), 1182.5 {I3} ({+95}Mo(p,n),(p,n|g)) 
RI$from |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1339.62 {I10} ({+95}Ru |e decay), 1340.02 {I12} ({+95}Mo(p,n),(p,n|g)) 
RI$from |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1697.6 {I2} ({+95}Ru |e decay), 1697.3 {I2} ({+95}Mo(p,n),(p,n|g)) 
RI$from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1988.1 {I2} ({+95}Ru |e decay), 1988.2 {I4} ({+95}Mo(p,n),(p,n|g)) 
RI$from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2324.5 {I2} ({+95}Ru |e decay), 2324.6 {I2} ({+95}Mo(p,n),(p,n|g)) 
RI$from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 363.26 {I7} ({+93}Nb(|a,2n|g)), 364.0 {I4} ({+65}Cu({+36}S,|a2n|g)) 
M,RI$from (|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$weighted average of 1031.77 {I9} ({+93}Nb(|a,2n|g)), 1032.0 {I4} ({+65}Cu({+36}S,|a2n|g)) 
M,RI$from (|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
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M,MR$D+Q, +0.46 +|@-24 from |g(|q) in (|a,2n|g). |D|p=no from level scheme; |d|<0.25 {i28} from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
E$weighted average of 811.14 {I7} ({+93}Nb(|a,2n|g)), 812.0 {I4} ({+65}Cu({+36}S,|a2n|g)) 
M,MR$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M,MR$D+Q, -0.04 {i10} if J{-i}=17/2; D+Q, +0.63 {I+5-10} if J{-i}=19/2; E2 if J{-i}=21/2+ from |g(|q) in (|a,2n|g) and comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 968.90 {I10} ({+93}Nb(|a,2n|g)), 970.1 {I4} ({+65}Cu({+36}S,|a2n|g)) 
M,MR$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
E$weighted average of 797.76 {I9} ({+93}Nb(|a,2n|g)), 798.1 {I4} ({+65}Cu({+36}S,|a2n|g)) 
M,MR$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
E$weighted average of 402.31 {I7} ({+93}Nb(|a,2n|g)), 403.1 {I4} ({+65}Cu({+36}S,|a2n|g)) 
M,MR$from (|a,2n|g); consistent with |a(K)exp 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_uncertain: ?
decay_comment:
MR$-0.8 {i29} if J{-f}=29/2- or +0.14 {i22} if J{-f}=27/2- in (|a,2n|g) 
E,RI$Observed only in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1149.5 {I1} ({+93}Nb(|a,2n|g)), 1149.1 {I4} ({+65}Cu({+36}S,|a2n|g)) 
RI$from (|a,2n|g) 
MR$from {+65}Cu({+36}S,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q(+O)
decay_comment:
M$stretched or |DJ=0 Q (1975Sa09) 
MR$from |a(K)exp assuming E2+M3 (evaluator). Sign may be negative since |d=-0.58 |@ from |g(|q) (1978Ma05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
E$other: 628.9 {i2} from weighted av of data from 1973Xe01, 1974Kr02, and 1974Sa19 (1975Sa09) 
MR$from |a(K)exp (evaluator). Sign may be negative since |d=-0.11 |@ from |g(|q) (1978Ma05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
MR$-0.25 {I+60-}Infnt 
M,MR$other solutions to |g(|q) excluded by additional decay modes from the initial state (1978Ma05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Alternate placement from 2907 state suggested by 1975Sa09 not consistent with adopted level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
E,RI$633.8 {i1}, I|g(634|g)/I|g(689|g)=1.13 {i16} (1975Sa09) discrepant probably since 634|g unresolved from 634|g from 2847 
M$stretched or |DJ=0 Q (1978Ma05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$from |a(K)exp (1978Ma05). |a(K)(M1)=0.00356, |a(K)(E2)=0.00413, |a(K)(E1)=0.00132, |a(K)(M2)=0.0114 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_comment:
M,MR$other solutions to |g(|q) excluded by additional decay modes from the initial state (1978Ma05). Evaluator's Note: M1(+E2) does does not appear to be excluded by |a(K)exp 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
M$|DJ=1 |g (1978Ma05) 
MR$+0.07 {i3} if J{-i}=17/2+ or -0.02 {i3} if J{-i}=21/2+. Other: -0.05 {I+2-3} if J{-i}=21/2+ from |g(|q) (1975Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$+0.46 +|@-24 
M,MR$other: D+Q, -0.48 {i12} if J{-i}=21/2+; D+Q, -0.24 {i4} if J{-i}=19/2+; Q(+O), +0.07 {i4} if J{-i}=17/2+ from |g(|q) (1975Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$723.2 {i1} (1978Ma05) discrepant 
M,MR$d(+Q); |d=-0.03 {I+3-5} if J{-i}=21/2+, -1.3 {I+4-13} if J{-i}=19/2+, +0.14 {I+8-10} if J{-i}=17/2+ (1975Sa09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M,MR$D+Q, -0.04 {i10} if J{-i}=17/2; D+Q, +0.63 {I+5-10} if J{-i}=19/2; E2 if J{-i}=21/2+ (comparison to RUL excludes M2) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M,MR$E2(+M3), +0.05 {i12} if J{-i}=29/2- or M1+E2, +0.36 {i17} if J{-i}=27/2-. |a(K)exp excludes M2(+E3) and E1+M2 (evaluator) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3
decay_comment:
M$|a(K)exp=1880 {i145} (1988Ch32); |a(K)exp/|a(L)exp=1.2 {i3} (1950Me21); |a(L3)exp/|a(L1)exp=1.46 {i15} (1969Ag05) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$combined for 256+256.0 
$DCO=1.8 {i4}, A{-2}=-0.020 {i5}, A{-4}=-0.069 {i7} all values for 256+256.0 doublet 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$combined for 526.0+525.9 doublet 
$DCO=0.92 {i8}, A{-2}=-0.272 {i22}, A{-4}=-0.04 {i3}, all values for 526.0+525.9 doublet 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$combined for 488.1+487.7 doublet 
$DCO=1.16 {i8}, ; A{-2}=-0.11 {i4}, A{-4}=+0.01 {i6}, all values for 488.1+487.7 doublet 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$combined for 256.0+256 doublet 
$DCO=1.8 {i4}, A{-2}=-0.020 {i5}, A{-4}=-0.069 {i7}, all values for 256.0+256 doublet 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$combined for 526.0+525.9 doublet 
$DCO=0.92 {i8}, A{-2}=-0.272 {i22}, A{-4}=-0.04 {i3} all values for 526.0+525.9 doublet 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$combined for 487.7+488.1 doublet 
$DCO=1.16 {i8}, A{-2}=-0.11 {i4}, A{-4}=+0.01 {i6}, all values for 488.1+487.7 doublet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.028 {i6}, A{-4}=-0.01 {i1}; |a(K)exp(85.1|g+85.9|g)=0.18 {i1}, |a(L)exp(85.1|g+85.9|g)=0.028 {i3} (1979Mi08) 
$|d=+0.2 {I+4-3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.0.04 {i2}, A{-4}=+0.01 {i3}; |a(K)exp(85.1|g+85.9|g)=0.18 {i1}, |a(L)exp(85.1|g+85.9|g)=0.028 {i3} (1979Mi08) 
$|d|<-0.2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.076 {i6}, A{-4}=0.000 {i6}; |a(K)exp=0.09 {i1}; |a(L)exp=0.019 {i4} (1979Mi08); pol=-0.06 {i1}; |d=+0.05 {i5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.03 {i1}, A{-4}=-0.01 {i2}; |a(K)exp=0.20 {i2}, |a(L)exp=0.031 {i3} (1979Mi08); pol=-0.36 {i14}; |d=0.0 {i2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.03 {i1}, A{-4}=-0.01 {i1}; |a(K)exp=0.036 {i4} (for 219.8|g+220.6|g); |a(L)exp=0.0049 {i7} (1979Mi08); |d=+0.2 {i3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.04 {i1}, A{-4}=+0.01 {i1}; pol=-0.02 {i2}; |a(K)exp=0.030 {i3}; |a(L)exp=0.0049 {i5} (1979Mi08) 
$|d=+0.05 {i11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$for 472.2|g+472.2|g A{-2}=-0.05 {i3}, A{-4}=+0.02 {i3}; pol=-0.08 {i8}; |a(K)exp=0.0047 {i4}; |d=0.07 {i11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$for 493.7|g+494.0|g A{-2}=-0.08 {i3}, A{-4}=-0.02 {i3}; pol=-0.19 {i20}; |d=-0.12 {i26}; |a(K)exp=0.0037 {i5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$pol=-0.11 {i12}; |d=-0.25 {i27}. For 516.4|g+517.7|g A{-2}=+0.04 {i2}, A{-4}=-0.01 {i2}; |a(K)exp=0.0023 {i6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.14 {i1}, A{-4}=+0.01 {i1}; |d=-0.05 {i4} 
M$for 255.6|g+255.6|g pol=-0.19 {i6}; |a(K)exp=0.025 {i3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M$for 505.8|g+506.1|g+506.6|g A{-2}=-0.05 {i1}, A{-4}=+0.01 {i1}; |a(K)exp=0.0024 {i3}; |d=+0.09 {I+9-29} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.11 {i6}, A{-4}=+0.09 {i8}; |a(K)exp=0.015 {i2}; |d=-0.04 {I+40-}|@. Others: |a(K)exp=0.018 {i2}, |a(L)exp=0.0025 {i6} (1979Mi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$for 493.7|g+494.0|g A{-2}=-0.08 {i3}, A{-4}=-0.02 {i3}; pol=-0.19 {i20}; |a(K)exp=0.0037 {i5} 
$|d=0.0 {I+2-21} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$for 472.2|g+472.2|g A{-2}=-0.05 {i3}, A{-4}=+0.02 {i3}; pol=-0.08 {i8}; |a(K)exp=0.0047 {i4} 
$|d=0.07 {i18} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$for 310.8|g+310.9|g A{-2}=-0.04 {i2}, A{-4}=-0.5 {i2} 
M$pol=-0.13 {i7}; |a(K)exp=0.015 {i2}; |d=-0.05 {i6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$A{-2}=-0.14 {i1}, A{-4}=+0.01 {i1}; |d=-0.05 {i4}; for 255.6|g+255.6|g pol=-0.19 {i6}; |a(K)exp=0.025 {i3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M,MR$from |g(|q), |g|g(|q), |a(K)exp and |a(exp) ratios; |d is weighted average of measurements in (p,n|g): +0.31 {I5} (1979Xe01); and {+97}Ru |e decay: +0.20 {I5} (1977Be33), and +0.27 {I2} (1976Ba39) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
M$(D) from {+94}Zr({+6}Li,3n|g) dataset, |D|p=no from level scheme; (M1+E2) from {+82}Se({+19}F,4n|g) dataset 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
M$L1/L2=5.0 {I16}, L1/L3=0.95 {I10}, L2/L3=0.21 {I7} (1969Ag04); K:L:M=1:0.48 {I5}:0.13 {I2} (1959Un01); K/LM=1.7 {I2} (1954Bo24); K/LM=1.6 {I2} (1950Me21). (theory: L1:L2:L3=0.980: 0.218: 1.00) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$other: |d=+0.20 {I5} (1977Be33, includes data from 1971Ph02 and 1974Be24); |d=+0.27 {I2} or +6.2 {I5} (1976Ba39) K:L1:L2:L3=910 {I10}: 100: 6 {I3}: 4 {I2} (1974Be24); |a(K)exp=0.0350 {I12}, K/LM=7.0 (1971Ph02); |a(K)exp=0.0340 {I30}, K/LM=5.55 (1969Gr04). Theory (|d=0.27): K:L1:L2:L3=918: 100: 6.5: 4.1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$from 1977Be33 includes results of 1971Ph02 and 1974Be24; K:L1:L2:L3=910 {I170}: 100: 44 {I7}: 50 {I8} (1974Be24). Theory (|d=1.6) K:L1:L2:L3=1068: 100: 44: 55. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$from 1977Kr03. Other: +2.8 {I5} or +0.13 {I5} (1977Be33), |d=+0.12 {I5} or >16 (1976Ba39); M1,E2 from |a(K)exp=0.00314 {I15} (1971Ph02) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$ uncertainty on A{-2} is quoted as 0.002 by 2003Bu06, which seems unrealistic. The compilers have increased it to 0.020. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$DCO corresponds to gate on |DJ=1, dipole transition 
$|g(|q) and DCO results contain contribution from a |g ray in {+95}Tc 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$DCO corresponds to gate on |DJ=1, dipole transition 
$Energy of initial level quoted as 4334.1 for this transition in Table 1 of 2003Bu06 seems a type error. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [M4]
decay_uncertain: S
decay_comment:
TI$ deduced by the compilers from intensity balance at 96.6 level, using |e feeding of 0.2 {I2}. If no |e feeding to this level, then I(|g+ce)=0.0429 {I19} 


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,MR$|d(E2/M1)=0.255 {I18} from |g+ce intensity balance of 21.8|g and 43.5|g in (|g,p|g), assuming mult(43.5|g)=M1 and using theoretical conversion coefficients from BrIcc code. But this value would require a large half-life of >0.2 |ms for the 21.8 level (lower limit is obtained at RUL=300 for B(E2)(W.u.)), contradicting to the short-lived nature of the 21.8-keV transition as stated in 1978Ba18 and to the measured value of 2.4 ns from |g(|q) in (p,n|g). RUL=300 for B(E2)(W.u.) of 21.8|g would limit |d(E2/M1) to <0.026 assuming T{-1/2}(21.8)<1 ns. 1978Ba18 have suggested mult=E1+1% M2, which, however, results in an unreasonably large B(M2)(W.u.). From these considerations, evaluators have assigned mult=M1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
$If M1, B(M1)(W.u.)=0.0080. If E2, B(E2)(W.u.)=550 
M$from RUL of 300 for B(E2)(W.u.), mult(48|g) cannot be pure E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
If M1, B(M1)(W.u.)>0.029. If E2, B(E2)(W.u.)>2500. 
M$from RUL of 300 for B(E2)(W.u.), mult(52|g) cannot be pure E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2(+E1))
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
M$evaluators consider the multipolarity uncertain, as with |d(M2/E1)>1, and with a branching ratio of |?20% and B(M2)(W.u.)=1 from RUL, the level half-life should be |?250 ns, but no such isomer has been detected in |g|g-coin data in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
RI$contribution from 658.3|g (in {+97}Mo) is estimated as 7.5 {I15} at 90|'. Other: 7.8 {I10} for the doublet at 0|' 
M$either M1 or E2 is possible from |a(K)exp. 1987Bi21 assigned M1(+E2) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$other: 34.9 {I15} at 0|' 
$R=0.65 {I4} 
M$|a(K)exp gives E2 or M1; |g(|q) consistent with |DJ=2, quadrupole, however M1 admixture cannot be ruled out. 1987Bi21 assigned E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$other: 24.8 {I13} at 0|' 
$R=0.62 {I5} 
M$|a(K)exp gives M1 or E2; |g(|q) consistent with |DJ=2, quadrupole, however dipole mixing cannot be ruled out. 1987Bi21 assigned E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average 43.55 {I10} (1982Ar12), 43.7 {I1} (1977Mi06), 43.5 {I5} (1976Fi04), 43.5 {I5} (1976We06) 
RI$Strong |g but I|g not available in 1982Ar12. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 59.80 {I10} (1982Ar12) and 60.0 {I2} (1977Mi06). other: 59.7 {I5}, placed from a 208 level in 1976Fi04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average 47.82 {I10} (1982Ar12), 47.9 {I1} (1977Mi06), 47.8 {I5} (1976Fi04) 
RI$Strong |g but I|g not available in 1982Ar12. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 65.3 {I3} (1977Mi06). |g(t) data (1978Bi09) supports placement from 138 level, and not from 204 level, as suggested by 1977Mi06. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted average of 86.66 {I3} (1982Ar12) and 86.7 {I1} (1977Mi06). Other: 86.6 {I5}, placed from the 190 level in 1976Fi04 
RI$other: 91 (1978MiZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$others: 51.8 {I1} (1977Mi06), 51.7 {I5} (1976Fi04) 
RI$deduced from average of I|g(52|g)/I|g(99|g)=15/5.7 and 12/4.4 in 1978MiZO for gate on and off d{-5/2}IAR, respectively 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted average of 99.44 {I8} (1982Ar12), 99.7 {I2} (1977Mi06), and 99.5 {I5} (1976Fi04) 
RI$other: 19 (1978MiZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$others: 117.0 {I2} (1977Mi06), 116.9 {I5} (1976Fi04, placed from a 208 level). |g(t) data in 1978Bi09 support placement from 190 level only, and not from 138 level, as suggested by 1977Mi06 
RI$other: 7 (1978MiZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 138.33 {I11} (1982Ar12), 138.7 {I2} (1977Mi06), and 138.4 {I5} (1976Fi04, placed from a 208 level) 
RI$other: 54 (1978MiZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted average of 202.69 {I8}, 203.0 {I4} (1977Mi06), and 202.8 {I5} (1976Fi04, placed from the 351 level) 
RI$other: 27 (1978MiZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 262.86 {I11} (1982Ar12), 263.3 {I2} (1977Mi06), and 262.8 {I5} (1976Fi04) 
RI$other: 52 (1978MiZO) 
M$M1(+E2),|d<0.35 from |a(K)exp in 1982Ar12, but M1 from |a(K)exp in 1979Mi08 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_uncertain: ?
decay_comment:
E$others: 309.7 {I3} (1977Mi06), 309.7 {I5} (1976Fi04, placed from the 458 level) 
RI$other: 22 (1978MiZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted average of 233.78 {I15} (1982Ar12) and 234.1 {I3} (1977Mi06) 
RI$other: 26 (1978MiZO) 
MR$from |a(K) in 1979Mi08. |a(K)exp in 1982Ar12 gives |d(E1/M2)=0.31 {I5} but it would require an unrealistic large T{-1/2} (>150 ns) for B(M2)(W.u.) not to exceed RUL. |a(K)exp in 1982Ar12 is also in marginal agreement with M1, however, |a(K)exp from 1979Mi08 is consistent only with E1(+M2), |d(M2/E1)<0.14 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 106.66 {I9} (1982Ar12) and 106.9 {I3} (1977Mi06). Other: 106.6 {I5} (1976Fi04) 
RI$other: 12 (1978MiZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted average of 294.00 {I12} (1982Ar12), 294.5 {I3} (1977Mi06), and 294.3 {I5} (1976Fi04) 
RI$other: 19 (1978MiZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 350.00 {I14} (1982Ar12) and 350.8 {I5} (1977Mi06). Other: 350 placed from a 541 level in 1976Fi04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 275.62 {I11} (1982Ar12), 276.0 {I3} (1977Mi06), and 275.8 {I5} (1976Fi04) 
RI$other: 20 (1978MiZO) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
M,MR$|d(E2/M1)=0.255 {I18} from |g+ce intensity balance of 21.8|g and 43.5|g in (|g,p|g), assuming mult(43.5|g)=M1 and using theoretical conversion coefficients from BrIcc code. But this value would require a large half-life of >0.2 |ms for the 21.8 level (lower limit is obtained at RUL=300 for B(E2)(W.u.)), contradicting to the short-lived nature of the 21.8-keV transition as stated in 1978Ba18 and to the measured value of 2.4 ns from |g(|q) in (p,n|g). RUL=300 for B(E2)(W.u.) of 21.8|g would limit |d(E2/M1) to <0.026 for adopted T{-1/2}(21.8)=2.4 ns {I6}. 1978Ba18 have suggested mult=E1+1% M2, which, however, results in an unreasonably large B(M2)(W.u.). From these considerations, evaluators have assigned mult=M1 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
K/L=7.8 {I3} (weighted average of 8.1 {I5} (1969Ba03) and 7.70 {I3} (1968Va14)); L1/L2=12 {I4}; L1/L3=18 {I7}; L2/L3=1.7 {I7} (1969Ag04). 
E from curved-crystal measurement (1981He15); value adopted in 2000He14. Others: E=140.512 {I4} (1972Ga37), 140.511 {I6} (1969Co18), 140.466 {I15} (1990Me15) 
RI E|g=140.511, I|g=744 {i11}, from I|g=704 {i45} (1969Co18), I|g=730 (1974HeYW), I|g=743 {i19} (1978MoYU), I|g=747 {i12} (1980Di16), I|g=759 {i20} (1980Ya10), I|g=686 {i49} (1982Si16), I|g=752 {i28} (1985Ch42), I|g=755 {i26} (1990Me15), and I|g=739 {i11} (1992Go22). recommended in 2014Ch12. 
RI I|g(140.5)=744 {i11} x 0.1220 {i16}=90.8% {i2}, per 100 decays of {+99}Mo in equilibrium with {+99}Tc(6.0 h). Uncertainty of 0.2% is due to the covariant relation between the relative |g-ray intensity (744) and the normalization factor (0.1220), the latter deduced from the decay scheme by evaluators. 
RI ------------------------------------------------- 
RI Calculating decay-scheme normalization factor. 
RI I(g+e)(142g)=0.183 (11)X[1+40.2(6)] = 7.5 (5) 
RI I(g+e)(140g)=744(11)X[1+0.1181(21)] = 832 (12) 
RI T1/2(99Mo)/[T1/2(99Mo) - T12/(99mTc)] = 1.1 
RI SUMOF (g+e)(GS) = 56.9 (8) 
RI At transient equilibrium: 
RI [I(g+e)(142g)/1.1+I(g+e)(140g)/1.1+SUMOF (g+e)(GS)]XN=100% 
RI That is: 
RI [7.5(5)/1.1+832(12)/1.1+56.9 (8)]XN = 820 (11) X N = 100% 
RI So the normalization factor is 
RI N = 100 / 820 (11) = 0.1220 (16) 
RI The absolute intensity of the 140-keV gamma ray is given by: 
RI g(140) = 744 (11) X N 
RI To avoid including twice the uncertainty of RI the 140-keV gamma ray: 
RI$g(140)=744(11)X100/[7.5(5)/1.1+744(11)X1.1181(21)/1.1+56.9(8)]= 
RI$=100/[7.5(5)/(744(11)X1.1) + 1.1181(21)/1.1 + 56.9(8)/744(11)]= 
RI$=100/[0.0092(6)+1.016(2)+ 0.0765(15)]= 100/1.1017(26)=90.8 (2)% 
RI$The absolute intensity of the 140-keV gama ray is: 
RI g(140) = 90.8 (2)% 
RI$Notice that if we had not included the cancellation effect the 
RI (incorrect) result would have been: 
RI g(140)%= 744 (11) X 0.1220 (16) = 90.8 (18)%, 
RI TEN TIMES LARGER UNCERTAINTY 
RI$Something similar takes place with the beta-feeding to the 142-keV 
RI level in 99TC. The correct feeding is: 
RI beta- = 82.2 (6)% 
MR unweighted average of +0.118 {I6} from |g|g(|q) (1974Ga01), 0.194 {I33} from |a(exp), and 0.07 {I7} from |a(K)exp; 0.31 {I2} (1982Si16) 
M |a(K)exp: weighted average of 0.093 {I6}, 0.096 {I6} (both 1971Vo06), 0.094 {I8} (1969Vu03), and 0.104 {I7} (1968Va14); |a(exp): weighted average of 0.118 {I3} (1973Le29), and 0.122 {I5} (1969Vu03). 


decay_energy_unit: KEV
decay_multipolarity: E3
decay_comment:
M2:M3:(M4+M5):(N2+N3):(N4+N5+O1)= 57.0 {i18}:100:47.2 {i10}:26.1 {i23}:4.4 {i5} (1981Ge05). M2:M3:(M4+M5):N=56.4 {i20}:100:47.6 {i20}:29 {i5}; M4/M5=0.56 {i13} (1971La12) 
TI 792 {I13} in equilibrium deduced from decay-scheme intensity balance. 
E from ce (1981Ge05). Others: 2.17 {I1} (1971La12), 2.15 {I3} (1957Fr35). 


decay_energy_unit: KEV
decay_multipolarity: M4
decay_comment:
E$From 1990Me15 and 1978MeZK. 
RI I|g=0.183 {i11}, from I|g=0.195 {i40}(1968Va14), I|g=0.149 {i29} (1980Di16), and I|g=189 {i11}(1990Me15), recommended in 2014Ch12. 
RI 0.15 {i2} from I|g(142.6)/I|g(140.5)=0.00020 {i2} in equilibrium deduced from K(142.6)/K(140.5)=0.075 {i8} (1969Ag04) (from {+99}Tc it decay); others: I|g(142.6|g)/I|g(140.5|g)=0.00025 {i3} (1990Me15,1978MeZK), 0.00020 {i3} (1980Di16), 0.00030 {i6} (1968Va14), from |g-spectra in equilibrium. 
M |a(K)exp=29 {i3}; K/L=2.9 {i5} (1969Ba03) 
EKC weighted average of 31 {i3} (1969Ba54) and 23 {i6} (1968Va14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI From I|g=8.68 {i27} (1980Di16), I|g=8.6 {i5} (1990Me15), I|g=8.49 {i25}(1992Go22), recommended in 2014Ch12. Other: 7.7 {i6} (1982Si16). 
E$Value adopted in 2000He14. E|g=40.5845 {I16} (1990Me15, 1978MeZK). 
M |a(K)exp=3.2 {I2} (1969Ra01). Other: 3.9 {I5} (1969Ba54); K/L=8.3 {I9} (1969Ba03) 
MR from |g|g(|q) (1974Ga01); |<0.025 (1982Si16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
RI From I|g=48.7 {i23} (1968Va14), I|g=49.9 {i34} (1969Co18), I|g=49.6 {i42} (1974HeYW), I|g=49.1 {i16} (1978MoYU), I|g=50.1 {i7} (1980Di16), I|g=49.8 (33) (1982Si16), I|g=48.7 {i13} (1985Ch42), I|g=50.3 {i17} (1980Me15), I|g=49.4 {i8} (1992Go22), I|g=49.5 {i21} (2003La27), recommended in 2014Ch12. 
MR from |g|g(|q) (1974Ga01). 
M |a(K)exp=0.126 {I7} (weighted average of 0.140 {I20} (1969Ba54), 0.130 {I12} (1968Va14) and 0.12 {I1} (1971Vo06)); K/L=6.8 {I7} (1969Ba03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI From I|g=10.6 {i8} (1968Va14), I|g=10.7 {i6} (1969Co18), I|g=10.0 {i9} (1974HeYW), I|g=9.8 {i3} (1978MoYU), I|g=9.52 {i32} (1980Di16), I|g=9.8 {i8} (1982Si16), I|g=9.92 {i25} (1990Me15), I|g=9.82 {i15} (1992Go22), I|g=9.8 {i4} (2003La27), recommended in 2014Ch12. 
M |a(K)exp=0.0076 {i10} (1969Ba54) (note obvious misprint in 1969Ba54) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI From I|g=0.073 {i22} (1974HeYW), I|g=0.067 {i15} (1978MoYU), I|g=0.078 {i13} (1982Si16), I|g=0.097 {i5} (1990Me15), I|g=0.098 {i5} (1992Go22), I|g=0.110 {i6} (2003La27), recommended in 2014Ch12. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
RI From I|g=0.39 {i5} (1968Va14), I|g=0.49 {i5} (1969Co18), I|g=0.36 {i4} (1974HeYW), I|g=0.43 {i6} (1978MoYU), I|g=0.44 {i4} (1982Si16), I|g=0.447 {i15}, I|g=0.47 {i2} (1992Go22), I|g=0.411 {i16} (2003La27), recommended in 2014Ch12. 
M |a(K)exp=0.005 {i1} (1969Ba54) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI From I|g=0.10 {i3} (1969Co18), I|g=0.095 {i30} (1974HeYW), I|g=0.112 {i15} (1978MoYU), I|g=0.11 {i4} (1982Si16), I|g=0.139 {i8} (1990Me15), I|g=0.156 {i6} (1992Go22), I|g=0.146 {i7} (2003La27), recommended in 2014Ch12. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI From I|g=0.13 {i8} (1969Co18), I|g=0.134 {i23} (1978MoYU), I|g=0.14 {i2} (1982Si16), I|g=0.120 {i6} (1990Me15), and I|g=0.118 {i30} (2003La27), recommended in 2014Ch12. 
M |a(K)exp=0.003 {I1} (1969Ba54) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M |a(K)exp=0.0016 {i3} (weighted average of 0.0017 {i4} (1969Ba54) and 0.0016 {i4} (1968Va14)); E2(+M1) from |a(K)exp but dipole excluded by J|p. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI From I|g=35.1 {i24} (1968Va14), I|g=34.9 {i20} (1969Co18), I|g=35.8 {i30} (1974HeYW), I|g=35.5 {i10} (1978MoYU), I|g=35.8 {i8} (1980Di16), I|g=34.8 {i19} (1982Si16), I|g=35.3 {i12} (1990Me15), I|g=35.1 {i5} (1992Go22), I|g=35.13 {i12} (2003La27), recommended in 2014Ch12. 
M |a(K)exp=0.00051 (1969Ba54) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI From I|g=1.04 {i8} (1968Va14), I|g=1.11 {i8} (1969Co18), I|g=1.09 {i5} (1978MoYU), I|g=1.09 {i5} (1980Di16), I|g=1.10 {i7} (1982Si16), I|g=1.06 {i4} (1970Me15), I|g=1.10 {i2} (1992Go22), I|g=1.12 {i5} (2003La27), recommended in 2014Ch12. 
M |a(K)exp=0.0004 {i1} from 1969Ba54 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI From I|g=0.21 {i3} (1968Va14), I|g=0.217 {i22} (1969Co18), I|g=0.19 {i6} (1974HeYW), I|g=0.26 {i2} (1982Si16), I|g=0.232 {i11} (1990Me15), I|g=0.24 {i4} (1992Go22), I|g=0.222 {i12} (2003La27), recommended in 2014Ch12. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E,RI observed only in 1985Ka02; I|g(625.8|g)/I|g(485.4|g)=128 {I4}/<2 
M A{-2}=+0.10 {I3}, A{-4}=-0.02 {I4} (1985Ka02) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
M A{-2}=-0.09 {I4}, A{-4}=-0.01 {I5} 
E,RI observed only in 1985Ka02; I|g(538.7|g)/I|g(761.8|g)=0.064 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
RI I|g(610.1|g)/I|g(761.9|g)=0.030 {I1} (1985Ka02) 
M A{-2}=+0.15 {I4}, A{-4}=-0.03 {I5} (1985Ka02) 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
M,RI A{-2}=-0.16 {I4}, A{-4}=+0.02 {I4}; I|g(138|g)/I|g(762|g)=0.394 {I10} (1985Ka02) 
E from 1984Ze03, 137.4 in 1985Ka02 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$From {+99}Mo |b{+-} Decay (1981He15), value adopted in 2000He14. 
RI Uncertainty in I|g has been estimated by evaluators. 
RI I|g(140.5)=100 {I3} x 0.89 {I3}=89.0% {I3}, per 100 decays of {+99}Tc(6.0 h). The very low uncertainty of 0.3% is due to the covariant relation between the relative |g-ray intensity (100) and the normalization factor (0.89), the latter deduced by evaluators from the decay scheme. 


decay_energy_unit: KEV
decay_multipolarity: E3
decay_comment:
E$From {+99}Mo |b{+-} Decay (1981Ge05). Others: 2.17 {i1} (1971La12), 2.15 {i3} (1957Fr35). 
TI deduced from I(|g+ce)(2.17)=I(|g+ce)(140.5). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
RI from ce(K)(142.6)/ce(K)(140.5)=0.075 {I8} (1969Ag04). Others: 0.021 {I3} (1980Di16), 0.032 {I6} (1968Va14), both from {+99}Mo |b{+-} decay |g-spectra in equilibrium. The prompt components have been subtracted by the evaluators. 
E. Browne recalculated RI (old value was 0.021). From K(142)/K(140)=0.075 (8), KC(140)=0.0988, KC(142)=29.5, and IG(140)=100; as shown below: K(142)= IG(142) x 29.5; K(142)=0.075 x 100 x 0.0988. IG(142) = 0.025 (2). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from ce data in (n,|g) E=thermal. From |g-ray data: 28.6 {I4} in (p,n|g) (1978Ma36) and 28.7 {I3} in (|g,p|g) (1978Ba18) 
M$from ce data in (n,|g) E=thermal and x-ray data in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$level-energy difference=103.63. Other: E|g=103.5975 {I19} and I|g=78 {I8} from (n,|g) E=thermal is uncertain 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 286.83 {I3} from (n,|g) E=thermal and 286.90 {I6} from (p,n|g). level-energy difference=287.05 
RI$weighted average of 78 {I3} from (n,|g) E=thermal and 64 {I12} from (p,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=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$from |g(|q,pol) and ce data in ce in ({+7}Li,3n|g), |d(M2/E1)<0.14 from ce data only. |g(|q) in ({+7}Li,3n|g) consistent with |DJ=1 


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$ level-energy difference=300.9171 
RI$unweighted average from (n,|g) and ({+7}Li,3n|g) 
M$from |g(|q,pol) and ce data in ({+7}Li,3n|g), with |g(|q) consistent with |DJ=0 and |d(M2/E1)=0.25 {I6} from ce data 
RI$other: 130 {I2} in ({+7}Li,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;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$|g(|q) in ({+7}Li,3n|g) suggests |DJ=1, intensity balance at 609 level gives |a(exp)|?1.4 implying M1(+E2), |d<0.4. RUL(E2)=300 gives |d<0.12 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;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$ce data in ({+7}Li,3n|g) give M1+E2 with |d(E2/M1)=0.62 {I16}. RUL(E2)=300 gives |d<0.25; |g(|q) consistent with |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;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$|g(|q) is consistent with |DJ=1 and intensity balance at 778 and 708 levels gives |a(exp)=1.3 {I6} implying M1(+E2) with |d<0.7 in ({+7}Li,3n|g). RUL(E2)=300 gives |d<0.13. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M$|g(DCO) (2005Jo04) consistent with |DJ=1, but |g(|q) (1995Bi11) suggests |DJ=2, in ({+7}Li,3n|g). This |g is not placed in level scheme by 1995Bi11. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$6264.7 to 500.02 or 500.15 level, the energy difference and J|p assignments appear to favor the placement from the latter 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI$from 1995Bi11. Other: 28 {I1} (2005Jo04). The value from 1995Bi11 agrees better with those from (n,|g) and (p,n|g) reactions 
$R(25|'/90|')=0.74 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$300.4 (2005Jo04) 
RI$I|g(300.9|g)/I|g(225.4|g)=1.30 as compared to 0.95 in (n,|g). The discrepancy may be due to incorrect division of intensity of a triplet (as in 1995Bi11) near 301 in ({+7}Li,3n|g) reaction 
$R(25|'/90|')=2.47 {I22}; POL=-0.086 {I10}; |a(K)exp(299.4|g+300.9|g)=0.0082 {I13} 
M$|a(K)exp gives |d(M2/E1)=0.25 {I6}; however, R is consistent with |DJ=0, dipole 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
M$R(25|'/90|')=0.87 {I5} (1995Bi11) suggests |DJ=1 transition. Intensity balance at 609 level gives |a(exp)|?1.4 which rules out E1 and gives |d(E2/M1)<0.4. However, RUL(E2)=300 give |d<0.12 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$R(25|'/90|')=0.71 {I4}; |a(K)exp=0.47 {I8} 
MR$|a(K)exp gives 0.62 {I16} but RUL(E2)=300 gives |d<0.25 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
M$R(25|'/90|')=0.66 {I4} suggests |DJ=1 transition. Intensity balance at 778 level gives |a(exp)=0.72 {I18} and that at 708 level gives |a(exp)=1.72 {I20} which rule out E1 and give |d(E2/M1)<0.7. However, RUL(E2)=300 gives |d<0.13 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$DCO=1.02 {I13} gated on |DJ=1, dipole 
$R(25|'/90|')=0.81 {I5}; POL=-0.080 {I9}; |a(K)exp=0.0078 {I13} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$DCO=1.53 {I14} gated on |DJ=1, dipole 
$R(25|'/90|')=1.31 {I9}; POL=+0.134 {I20}; |a(K)exp=0.0020 {I6} 
M$|a(K)exp gives M1,E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$DCO=0.93 {I23} gated on |DJ=1; DCO=0.48 {I4}; gated on |DJ=2, Q 
$R(25|'/90|')=0.63 {I5}; POL=-0.083 {I18}; |a(K)exp=0.0047 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$from 1995Bi11. Other: 12.5 {I2} (2005Jo04) 
$DCO=1.53 {I5} gated on |DJ=1 
$R(25|'/90|')=1.32 {I21}; POL=+0.08 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$DCO=0.97 {I6} gated on |DJ=1; DCO=0.40 {I4} gated on |DJ=2, Q 
$R(0|'/90|')=0.70 {I10}; POL=-0.054 {I25} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$E|g=172.21 {I3} (2004Fu30), I|g=48.8 (1978HeZQ) 
M,MR$|a(K)exp=0.072 {I4}, |a(L1)exp=0.0086 {I6}, |a(L2)exp+|a(L3)exp<0.00090, |a(M)exp=0.0018 {I2} 
$ ICE(K)=3.50 4, ICE(L1)=0.42 2, ICE(L2+L3)<0.044, ICE(M)=0.086 9 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from ce data 
RI$0.28 {I3} from I(|g+ce)=32 {I3} and |a. From |g-ray data 1978HeZQ quote 0.15 
TI$from sum of electron intensities 
M$ce(L1)=1.36 {I16}, ce(L2)=6.5 {I8}, ce(L3)=10.9 {I14}, ce(M1)=0.23 {I7}, ce(M2+M3)=3.3 {I4}, ce(N)=0.62 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$E|g=223.48 {I3} (2004Fu30), I|g=4.91 (1978HeZQ) 
M$|a(K)exp=0.0120 {I18} 
MR$<0.1 
$ ICE(K)=0.059 8 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=43.18 {I3}, I|g=2.69 {I7} (2004Fu30): corresponds to 43.2862|g+ 43.562|g doublet in 1979Pi08 
E,RI$1978HeZQ report 43.2862 (I|g=0.39) and 43.5620 (I|g=0.79), but 2004Fu30 report only one line at 43.18 (I|g=2.69 {I7}) 
M$Ice(K)=7.6 {I12}, Ice(L1)=0.82 {I10}, Ice(L3)=2.8 {I3}, Ice(M2+M3)=0.75 {I7} 
$I|g=0.39 {I4} (1978HeZQ), 0.55 from ce data in 1979Pi08 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$E|g=62.79 {I3} (2004Fu30), I|g=2.22 (1978HeZQ) 
M$|a(K)exp=0.73 {I7}, |a(L1)exp=0.086 {I9} 
$ ICE(K)=1.62 13, ICE(L1)=0.19 2 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$E|g=91.32 {I3} (2004Fu30), I|g=3.69 (1978HeZQ) 
M$|a(K)exp=0.35 {I4}, |a(L1)exp=0.041 {I6} 
MR$<0.3 from |a(K)exp 
$ ICE(K)=1.28 10, ICE(L1)=0.15 2 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=263.58 {I3} (2004Fu30), I|g=5.2 (1978HeZQ) 
M$|a(K)exp=0.034 {I3} 
MR$>2 
$ ICE(K)=0.177 9 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$E|g=86.76 {i4} (2004Fu30), I|g=1.62 (1978HeZQ) 
M$|a(K)exp=0.36 {I4} 
MR$<0.2 
$ ICE(K)=0.59 5 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$E|g=30.8 {I6} (2004Fu30), I|g=0.78 (1978HeZQ) 
M$from |a(L1)exp=1.01 {I16} 
MR$from RUL(E2)=300. |d=0.35 {I15} (from |a(L1)exp); <0.35 (from intensity balance at 263.5 level) 
$ ICE(L1)=0.79 10 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=94.58 {I5} (2004Fu30), I|g=0.010 (1978HeZQ) 
E,RI$1978HeZQ report 94.251 (I|g=0.010) and 94.7980 (I|g=0.015), but 2004Fu30 report only one line at 94.58 (I|g=0.037) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$level-energy difference=75.5343 
$E|g=75.52 {I3} (2004Fu30), I|g=2.40 (1978HeZQ) 
M$|a(K)exp=0.40 {I5} 
$ ICE(K)=0.96 10 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=118.93 {I3} (2004Fu30), I|g=0.060 (1978HeZQ) 
E,RI$1978HeZQ report 118.8233 (I|g=0.060) and 119.0423 (I|g=0.030), but 2004Fu30 report only one line at 118.93 (I|g=0.304) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|a(K)exp=0.59 {I15} 
MR$<0.2 
$E|g=71.62 {I6} (2004Fu30), I|g=0.22 (1978HeZQ) 
$ ICE(K)=0.13 3 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$level-energy difference=46.0562 
$E|g=45.84 {I8} (2004Fu30), I|g=0.19 (1978HeZQ) 
M$|a(K)exp=2.9 {I6}, |a(L1)exp=0.53 {I12} 
MR$<0.4 
$ ICE(K)=0.55 9, ICE(L1)=0.10 2 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$E|g=168.87 {I8} (2004Fu30), I|g=1.80 (1978HeZQ) 
M$|a(K)exp=0.059 {I8} 
MR$<0.3 
$ ICE(K)=0.106 12 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$E|g=105.81 {I6} (2004Fu30), I|g=2.34 (1978HeZQ) 
M$|a(K)exp=0.23 {I3} 
MR$<0.3 
$ ICE(K)=0.54 5 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$E|g=166.58 {I6} (2004Fu30), I|g=1.23 (1978HeZQ) 
M$|a(K)exp=0.048 {I12} 
$ ICE(K)=0.059 15 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=253.56 {I5} (2004Fu30), I|g=0.23 (1978HeZQ) 
E,RI$1978HeZQ report 253.532 (I|g=0.23) and 253.876 (I|g=0.130), but 2004Fu30 report only one line at 253.56 (I|g=0.96) 
$E|g=253.56 {I5}, I|g=0.96 {I5} (2004Fu30) probably corresponds to triplet: 253.29|g+253.532|g+253.876|g in 1978HeZQ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$level energy difference=141.6011 
$E|g=141.49 {I10} (2004Fu30), I|g=0.050 (1978HeZQ) 
E,RI$1978HeZQ report three |g rays near this energy with total I|g=0.080 but 2004Fu30 report only one line with I|g=0.32 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$level-energy difference=166.1675 
E,RI$1978HeZQ report 166.1707 (I|g=0.48) and 166.6825 (I|g=1.23) but 2004Fu30 report only 166.58 with I|g=3.55 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|a(K)exp=0.030 {I6} 
MR$<0.5 
E$level-energy difference=217.1353 
$E|g=217.17 {I3} (2004Fu30), I|g=1.49 (1978HeZQ) 
$ ICE(K)=0.044 9 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$ based on the least-squares fit procedure, the 260.441|g fits better from 461 level, as proposed by 1979Pi08, than the 260.9136|g as seems proposed by 2004Fu30 who reported a single line at 260.97 
$I|g=0.05 (1978HeZQ) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.047 {I10} 
$E|g=206.17 {I3} (2004Fu30), I|g=0.90 (1978HeZQ) 
$ ICE(K)=0.042 8 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$E|g=276.55 {I3} (2004Fu30), I|g=3.10 (1978HeZQ) 
M$|a(K)exp=0.015 {I3} 
MR$<0.4 
$ ICE(K)=0.047 7 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$E|g=299.48 {I3} (2004Fu30), I|g=11.5 (1978HeZQ) 
M$|a(K)exp=0.0052 {I10} 
MR$<0.14 
$ ICE(K)=0.060 11 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_uncertain: ?
decay_comment:
$E|g=39.12 {I5} (2004Fu30), I|g=0.63 (1978HeZQ) 
M$|a(L1)exp=0.37 {I8} 
MR$<0.2 
$ ICE(L1)=0.23 4 (1979Pi08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=225.38 {I3} (2004Fu30), I|g=2.24 (1978HeZQ) 
M$suggested as E1 by 1979Pi08, probably because no electron line corresponding to this |g ray was detected 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6264.4 {I2}, I|g=0.183 {I9} (1978HeZQ) 
$|g to 500.020 or 500.147 level, however, the energy difference and J|p assignments appear to favor the placement from the latter 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
E$from 1978Ma36 
M$from comparison of observed and predicted x-ray intensity (1978Ma36), also Adopted Gammas where assignment is from ce data in (n,|g) dataset 


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 ce measurements (1972Co16) 
L1:L2:L3:M=100 {i3}:11.1 {i20}:10.3 {i17}:26 {i6} (1972Co16) 
RI from I(|g+ce) and |a 
TI from intensity balance 
MR 0.015 {i2} from L1/L3 ratio data (1972Co16). Other: 0.011 {i4} from L1/L2 (1972Co16) 


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:
L1:L2:L3:M=100 {i17}:13.3 {i48}:11.2 {i48}:23 {i5} (1972Co16) 
E$from ce measurements (1972Co16) 
TI from intensity balance 
RI from I(|g+ce) and |a 
MR 0.010 {I+2-3} from L-subshell ratio data (1972Co16) 


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 ce measurements (1972Co16) 
M from L1:L2:L3=<1.6:6 {i2}:10 {i2} (1972Co16) 
RI from ratio of I(ce(L2)+ce(L3))=88 {i22} (1972Co16) to |a(L2)+|a(L3)=1194 


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:
E others: 192.00 {i8} (1972Co16), 191.93 {i4} (1972Co17), 191.89 {i5} (1975Wr01) 
M from |a(K)exp=0.30 {i6} (1956Ma72) ce(K)/I|g; 0.20 {i3} (1973Al16) ce(K)/I|g; 0.26 {i6} (1978Ba18) K| x ray/I|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E from 1972Co16. Others: 80.67 {i14} (1975Wr01), 80.92 {i3} (1972Co17) 
RI$others: 191 {i13} (1972Co16,1972Co17), 281 {i16} (1975Wr01) 
M deduced from |a(K)exp 
|a(K)exp=0.47 {i8} (1973Al16) ce(K)/I|g; 0.51 {i9} (1972Co16) ce(K)/I|g normalized to |a(K)(192|g)=0.248 (M2 theory) 
I(ce(K) 81|g)=97 {i17} from I(ce(K) 81|g)/I(ce(K) 192|g)=0.39 {i7} (1972Co16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$av from 1972Co17 and 1975Wr01 
RI$others: 310 {i30} (1975Wr01), 355 {i11} (1973Al16), 424 {i22} (1974HeYW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$|a(K)exp=0.22~{I6} in {+105}Mo |b{+-} decay (35.6~s) (1989RuZU) and |a(exp)=0.22~{I8} in {+252}Cf SF decay (2004Lu20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$|a(K)exp=1.08~{I24} in {+105}Mo |b{+-} decay (35.6~s) (1989RuZU) and |a(exp)=1.13~{I10} in {+252}Cf SF decay (2004Lu20) 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
$|a(K)exp=1.1 {I4} from fluorescence yields or |a(K)exp=1.0 {I4} from conversion electron measurements (1995Jo02) 


decay_energy_unit: KEV
decay_multipolarity: E1
decay_comment:
$|a(K)exp=0.4 {I3} from fluorescence yields or |a(K)exp=0.18 {I6} from conversion electron measurements (1995Jo02) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$(438.6|g)(72.4|g)(|q): A{-2}=-0.04 {I2}, A{-4}=0.00 {I3} 
$(438.6|g)(161.2|g)(|q): A{-2}=-0.06 {I2}, A{-4}=+0.04 {I3} 
$(438.6|g)(206.4|g)(|q): A{-2}=+0.09 {I3}, A{-4}=-0.05 {I3} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$(159.6|g)(292.7|g)(|q): A{-2}=+0.04 {I2}, A{-4}=-0.05 {I3} 
$(159.6|g)(431.0|g)(|q): A{-2}=-0.07 {I3}, A{-4}=+0.01 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$E=86.5, T{-1/2}=140 ns (1970Jo20), 117 ns (1973TaZG). 1973TaZG also observed a 10-ns component in this transition. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$E=90.0, T{-1/2}=120 ns (1970Jo20), 116 ns (1973TaZG). E=90.2, T{-1/2}=15 ns (1970Jo20), 8 ns (1973TaZG). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
M$from T{-1/2} 
E$E=176.3, T{-1/2}=110 ns (1970Jo20), 114-ns and 8-ns components observed by 1973TaZG. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$1976ChZD measured perturbed angular correlation on a 153.9|g, deduced g=0.50 {i4}. No level scheme for {+108}Tc was proposed at this time; therefore, it is not known to what level the measured g factor corresponds. 
T{-1/2}=110 ns (1970Jo20), 108 ns (1973TaZG), 110 ns {i10} (1976ChZD). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.90 {I20} and |a(exp)=0.90 {I20} in 2012Ku28. Also |a(K)exp=1.12 {i25} for 65.2|g+69.1|g in 2012Ku28. Other: |a(K)exp=2.9 {I8} in 2010Ur03 
MR$From |a(K)exp=0.90 {I20} (2012Ku28). Other: 1.9 {I9} in {+248}Cm SF decay (2010Ur03) and 0.16 {I+7-12} in {+252}Cf SF decay (2004Lu20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
M$|a(K)exp=2.2 {I7} (2010Ur03) from comparison of I|g(165|g) and I|g(K|a x rays), but the value is too large for either Mult=E1, M1 or E2. (433|g)(165|g)(|q) data (2010Ur03) are also inconclusive. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M,MR$from |a(exp)=0.19 {I9} in {+252}Cf SF decay (2004Lu20) and (437.5|g)(137.0|g)(|q) in {+248}Cm SF decay (2010Ur03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$from |a(K)exp=1.1 {i1} in {+109}Mo |b{+-} decay (2012Ku28). Also: |a(K)exp=1.12 {i25} for 65.2|g+69.1|g (2012Ku28). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 2004Lu20; placement from 2010Gu07. This gamma was placed by 2004Lu20 from a level at E=4200.8 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$|a(K)exp=0.90 {I20} and |a(exp)=0.90 {I20} in 2012Ku28. Also |a(K)exp=1.12 {i25} for 65.2|g+69.1|g in 2012Ku28. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$|a(K)exp=2.2 {I7} (2010Ur03) from comparison of I|g(165|g) and I|g(K|a x rays), but the value is too large for either Mult=E1, M1 or E2. (433|g)(165|g)(|q) data are also inconclusive. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$(131.6|g)(67.0|g)(|q): A{-2}=+0.04 {I3}, A{-4}=-0.03 {I3} 
M$|a(K)exp=1.9 {I5} from |g and K-x ray intensities 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
M$ E1 is also allowed by measured K-conversion coefficient 
$ T{-1/2}=266 ms {I60} from decay curve for 42.6|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$Uncertainty of |a(K)exp is from table ii, listed as 0.3 in text on page 2 of 2011Ku16 
$ T{-1/2}=173 ms {I17} from decay curve for 67.2|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$This |g-ray has been interchanged with 885.6 keV |g-ray by 2004Bu13 in {+58}Ni({+40}Ca,2|a|g) dataset from intensity consideration and placed above 512.2 keV |g-transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$This |g-ray has been interchanged with 946.2 keV |g-ray by 2004Bu13 in {+58}Ni({+40}Ca,2|a|g) dataset from intensity consideration and placed below 512.2 keV |g-transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
M Q from DCO ratio in ({+36}Ar,2pn|g): E=149 MeV; not M2 from RUL, based on |<20 ns |g|g-coincidence resolving time. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI weighted average of 60 {I10} from ({+36}Ar,2pn|g): E=149 MeV and 63 {I18} from ({+40}Ca,|a2pn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M DCO ratio in ({+36}Ar,2pn|g) not consistent with pure Q (as proposed based on |g anisotropy data in ({+40}Ca,|a2pn|g)). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
M Q from |g-anisotropy ratio in ({+40}Ca,|a2pn|g); however, E|g is atypically low for a crossover transition, and |g is placed as a |DJ=1, |D|p=no transition in ({+36}Ar,2pn|g): E=149 MeV. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
Anisotropy ratio (1993Ar02): 1.47 {I22}. Note that this transition is assigned as |DJ=1 in Adopted Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E placement from 'to be published' work of C. Rusu et al. (reference 26 in 2004De40); that work is still unpublished, but placement is confirmed in ({+36}Ar,2pn|g): E=111 MeV (2013Zh10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M anisotropy ratio consistent with stretched Q (or D |DJ=0); 1997Li29 adopt the latter. |D|p=no from level scheme. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E this may be the |g reported by 2000Sc31 and attributed by them to {+93}Pd |e decay; the strongest {+93}Rh lines from {+93}Pd |e decay are not observed by 2001Xu05. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E3)
decay_comment:
Anisotropy=2.0 {I5}; consistent with M2 or E3, but M2 would lead to a strongly populated 4-, 6-, 8- cascade, and that has no counterpart in other N=48 nuclei (1993Ar08). 


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 D from ({+40}Ca,4pn|g); |D|p=(yes) from level scheme. 
Order of 177|g and 168|g is reversed in (|a,3n|g) data set. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 36% prompt, 64% has T{-1/2}|?100 ns; A{-2}=+0.11 {I3}, A{-4}=-0.07 {I5} (1973Ni04). A{-2}=+0.246 {I9}, A{-4}=-0.036 {I12}, polarization=+0.41 {I10} (1978Br25). 
Other E|g: 1392.25 (1978Br25). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 18% prompt, 82% has T{-1/2}|?100 ns; A{-2}=+0.02 {I3}, A{-4}=+0.03 {I5} (1973Ni04). A{-2}=+0.220 {I7}, A{-4}=-0.05 {I5}, polarization=+0.36 {I5} (1978Br25). 
Other E|g: 544.65 (1978Br25). 


decay_energy_unit: KEV
decay_comment:
M$|DJ=0 transition, but from POL and DCO values, |DJ=0 assignment with implied M1 or M1+E2 is not obvious (compiler's note) 
$POL=+0.01 {I1}, DCO=0.58 {I12} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$Compilers obtain B(E2)=0.0151 {I20}, in disagreement with value from 2018Er01 
E$from Table 3 in 2018Er01, value is 1159 in authors' Table 1. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$Compilers obtain B(E2)=0.00222 {I38}, in disagreement with value from 2018Er01 
E$from Table 3 in 2018Er01, value is 1254 in authors' Table 1. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$Compilers obtain B(E2)=0.00185 {I+30}, in disagreement with value from 2018Er01 
E$from Table 3 in 2018Er01, value is 1269 in authors' Table 1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 941.6 {I3} ({+95}Rh |e decay (5.02 min)), 942.2 {I3} ({+64}Zn({+35}Cl,3pn|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 410.3 {I3} ({+95}Rh |e decay (5.02 min)), 410.2 {I3} ({+64}Zn({+35}Cl,3pn|g)) 
RI$weighted average of 5.2 {I5} ({+95}Rh |e decay (5.02 min)), 3.0 {I10} ({+92}Mo(|a,n|g),({+6}Li,p2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1352.0 {I3} ({+95}Rh |e decay (5.02 min)), 1352.1 {I3} ({+64}Zn({+35}Cl,3pn|g)) 
RI$weighted average of 100 {I3} ({+95}Rh |e decay (5.02 min)), 100 {I10} ({+92}Mo(|a,n|g),({+6}Li,p2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 677.6 {I3} ({+95}Rh |e decay (5.02 min)), 677.3 {I3} ({+64}Zn({+35}Cl,3pn|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2+M1)
decay_comment:
E$weighted average of 895.0 {I3} ({+95}Rh |e decay (5.02 min)), 894.8 {I3} ({+64}Zn({+35}Cl,3pn|g)) 
RI$from |e 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:
RI$I|g(1305|g)/I|g(895|g)=0.50 {i14} in ({+6}Li,p2n|g) and =0.13 {i1} in {+64}Zn({+35}Cl,3pn|g) 
RI$weighted average of 100 {I6} ({+95}Rh |e decay (5.02 min)), 16 {I5} ({+64}Zn({+35}Cl,3pn|g)) 
RI$from |e 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:
M$Q from |g(|q) in ({+6}Li,p2n|g); |=M2 from comparison to RUL 
E,RI$weighted average of 255 {I1} ({+92}Mo(|a,n|g),({+6}Li,p2n|g)), 254.7 {I3} ({+64}Zn({+35}Cl,3pn|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$from |g(|q) in ({+6}Li,p2n|g) and comparison to RUL from half life in {+64}Zn({+35}Cl,3pn|g). 
E,RI$from ({+35}Cl,3pn|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 832.52 {I10} ({+96}Rh |e decay (9.90 min)), 832.51 {I9} ((HI,xn|g)), 832.57 {I5} ({+96}Ru(p,p'|g)), 831.6 {I4} ({+65}Cu({+36}S,p4n|g)), 832.6 {I1} ({+95}Mo({+3}He,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 685.47 {I10} ({+96}Rh |e decay (9.90 min)), 685.34 {I12} ((HI,xn|g)), 685.49 {I5} ({+96}Ru(p,p'|g)), 685.1 {I4} ({+65}Cu({+36}S,p4n|g)), 685.5 {I1} ({+95}Mo({+3}He,2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 1098.2 {I2} ({+96}Rh |e decay (9.90 min)), 1098.51 {I5} ({+96}Ru(p,p'|g)), 1098.5 {I1} ({+95}Mo({+3}He,2n|g)) 
M,MR$from {+95}Mo({+3}He,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 631.73 {I10} ({+96}Rh |e decay (9.90 min)), 631.64 {I10} ((HI,xn|g)), 631.71 {I7} ({+96}Ru(p,p'|g)), 632.1 {I4} ({+65}Cu({+36}S,p4n|g)), 631.7 {I1} ({+95}Mo({+3}He,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$weighted average of 1451.2 {I2} ({+96}Rh |e decay (9.90 min)), 1451.9 {I5} ({+96}Rh |e decay (1.51 min)), 1451.6 {I3} ({+96}Ru(p,p'|g)), 1451.2 {I2} ({+95}Mo({+3}He,2n|g)) 
RI$from {+95}Mo({+3}He,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$weighted average of 2283.6 {I4} ({+96}Rh |e decay (9.90 min)), 2283.9 {I5} ({+96}Rh |e decay (1.51 min)), 2284.2 {I5} ({+96}Ru(p,p'|g)), 2283.6 {I4} ({+95}Mo({+3}He,2n|g)) 
RI$from {+95}Mo({+3}He,2n|g), other: 9 {I5} ({+96}Rh |e decay (1.51 min)), 7.5 {I22} ({+96}Ru(p,p'|g)). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 944.07 {I10} ({+96}Rh |e decay (9.90 min)), 944.33 {I9} ({+96}Ru(p,p'|g)), 944.1 {I1} ({+95}Mo({+3}He,2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 594.1 {I2} ({+96}Rh |e decay (9.90 min)), 593.8 {I2} ({+95}Mo({+3}He,2n|g)) 
RI$from {+96}Ru(p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1006.5 {I5} ({+96}Rh |e decay (9.90 min)), 1006.7 {I2} ({+96}Ru(p,p'|g)) 
RI$from {+96}Ru(p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1692.3 {I2} ({+96}Rh |e decay (9.90 min)), 1692.2 {I2} ({+96}Ru(p,p'|g)) 
RI$from {+96}Ru(p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1743.1 {I5} ({+96}Rh |e decay (9.90 min)), 1743.4 {I1} ({+96}Ru(p,p'|g)) 
RI$from (p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2576.1 {I2} ({+96}Rh |e decay (1.51 min)), 2576.2 {I3} ({+96}Ru(p,p'|g)) 
RI$from (p,p'|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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LT
decay_comment:
E$weighted average of 1070.35 {I10} ({+96}Rh |e decay (9.90 min)), 1070.26 {I12} ((HI,xn|g)), 1070.36 {I8} ({+96}Ru(p,p'|g)), 1071.1 {I4} ({+65}Cu({+36}S,p4n|g)), 1070.4 {I1} ({+95}Mo({+3}He,2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1242.14 {I10} ({+96}Rh |e decay (9.90 min)), 1242.4 {I3} ({+96}Ru(p,p'|g)), 1242.1 {I1} ({+95}Mo({+3}He,2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 644.16 {I10} ({+96}Rh |e decay (9.90 min)), 644.2 {I1} ({+95}Mo({+3}He,2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1275.76 {I10} ({+96}Rh |e decay (9.90 min)), 1275.8 {I1} ({+95}Mo({+3}He,2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 741.87 {I10} ({+96}Rh |e decay (9.90 min)), 741.8 {I3} ((HI,xn|g)), 741.9 {I1} ({+95}Mo({+3}He,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 800.70 {I10} ({+96}Rh |e decay (9.90 min)), 800.55 {I13} ((HI,xn|g)), 801.2 {I4} ({+65}Cu({+36}S,p4n|g)), 800.7 {I1} ({+95}Mo({+3}He,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 702.95 {I25} ((HI,xn|g)), 703.1 {I2} ({+95}Mo({+3}He,2n|g)). Other 703.9 {I4} {+65}Cu({+36}S,p4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$|g previously placed in level 2588.51 (1983Wa06) but not seen in coincidence, inconsistent with J|p of level. Placed here by evaluator. 


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:
$Measured Q, calculated B(M2)(W.u.) exceeds RUL excluding M2, hence E2 
E$from (HI,xn|g), other: 601.3 {I4} ({+65}Cu({+36}S,p4n|g)) 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
$I|g=3.2 {i17} in {+60}Ni({+40}Ca,4p|g) at E({+40}Ca)=140 MeV 
M$A{-2}=-0.32 {i10}, A{-4}=-0.06 {i15} 


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$from |g(|q) ({+12}C,3n|g), (|a,2n|g); not pure E2 or higher multipolarity (RUL); L=4 to L=2 transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$D+Q from ((|a,n|g),({+6}Li,p2n|g)); D from ({+12}C,3n|g), ({+7}Li,3n|g); |D|p=no from level scheme 
MR$|d=0.13 (|a,2n|g); |d=-2.3+5-8 ((|a,n|g),({+6}Li,p2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$D+Q from |g(|q) ((|a,n|g),({+6}Li,p2n|g)), (|a,2n|g); |D|p=no from level scheme 
MR$|d=-1.7 {I2} |g(|q) ((|a,n|g),({+6}Li,p2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$from |g(|q) ({+7}Li,3n|g), ((|a,n|g),({+6}Li,p2n|g)), (|a,2n|g); D,E2 from RUL; |D|p=no from level scheme 
MR$-2.0 {I+4-6} ((|a,n|g),({+6}Li,p2n|g)), 0.16 (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$from 1974Oh07; 1975Pl05 suggests that this |g is a doublet, with E|g=1310 and 1312 keV with about equal intensity, but only one |g is placed in the level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$unweighted average of 1974Oh07, 1975Pl05 and 1981Gr20 
M,MR$from |a(K)exp=0.053 {I2} (1975Pl05). (1975Pl05 obtained |a(K)exp=0.056 {I2} relative to |a(K)(216|g in {+97}Tc)=0.0350; the evaluator has recalculated |a(K)exp using adopted |a(K)(216|g in {+97}Tc)=0.0330). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$doublet; coincidence data (1974Oh07, 1975Pl05) requires both placements in level scheme. 
RI$total intensity (8.3 {I6}) divided according to the coin data of 1974Oh07. 


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$weighted average of 652.41 {I5} from {+98}Tc |b{+-} decay, 652.8 {I1} from ({+36}S,|a4n|g), 652.6 {I2} from (|a,2n|g), 652.45 {I5} from ({+3}He,2n|g), and 652.4 {I1} from Coulomb excitation. Others: 652.6 {I4} from {+98}Rh |e decay, 652.9 {I4} from ({+36}S,p2n|g), and 652.6 {I4} from (|a,4n|g) 
M$from |g(|q) and ce data in (|a,4n|g), |g(|q) and |g(pol) in ({+3}He,2n|g), |g(DCO) and |g(pol) in ({+36}S,|a4n|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$weighted average of 745.35 {I5} from {+98}Tc |b{+-} decay, 745.4 {I4} from {+98}Rh |e decay (3.6 min), 746.2 {I4} from ({+36}S,p2n|g), 745.9 {I1} from ({+36}S,|a4n|g), 745.6 {I2} from (|a,2n|g), 745.37 {I5} from ({+3}He,2n|g), 745.5 {I4} from (|a,4n|g), and 745.4 {I5} from Coulomb excitation 
M$from |g(|q) and ce data in (|a,4n|g), |g(|q) and |g(pol) in ({+3}He,2n|g), |g(DCO) and |g(pol) in ({+36}S,|a4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 761.9 {I4} from {+98}Rh |e decay (8.72 min), 761.5 {I4} from {+98}Rh |e decay (3.6 min), 762.3 {I2} from (|a,2n|g), 761.84 {I5} from ({+3}He,2n|g), 762.2 {I4} from (|a,4n|g), and 762.5 {I5} from Coulomb excitation 
M$Q+D from |g(|q) in (p,p'|g); M2+E1 ruled out by RUL 
MR$weighted average of +13 {I+4-3} from |g(|q) in (p,p'|g) and +11 {I+8-3} from |g|g(|q) in ({+3}He,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$weighted average of 1414.2 {I8} from {+98}Rh |e decay (8.72 min), 1413.4 {I4} from {+98}Rh |e decay (3.6 min), 1415.0 {I3} from (|a,2n|g), 1414.29 {I5} from ({+3}He,2n|g), 1415.1 {I4} from (|a,4n|g), and 1414.9 {I5} from Coulomb excitation 
RI$weighted average of 56 {I5} from {+98}Rh |e decay (8.72 min), 48.6 {I20} from (|a,2n|g) and 49 {I1} from ({+3}He,2n|g). Others: 36 {I3} in (|a,4n|g), 20 {I5} in Coulomb excitation, 70 {I7} in {+98}Rh |e decay (3.6 min) 
M$Q from |g(|q) in (p,p'|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 383.0 {I5} from {+98}Rh |e decay (3.6 min), 382.7 {I3} from (|a,2n|g), 382.65 {I5} from ({+3}He,2n|g), and 382.7 {I4} from (|a,4n|g) 
RI$weighted average of 25.8 {I11} from (|a,2n|g), 25.7 {I9} from ({+3}He,2n|g), and 19.5 {I25} from (|a,4n|g). Other: 42 {I8} from {+98}Rh |e decay (3.6 min) 
M$from |g(|q) and ce data in (|a,4n|g) and ({+3}He,2n|g) 
MR$weighted average of +0.4 {I+17-3} from |g(|q) in (|a,4n|g) and 0.9 {I+8-5} from ce data in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 399.1 {I3} from (|a,2n|g) and 398.9 {I2} from ({+3}He,2n|g) 
RI$weighted average of 7.0 {I11} from (|a,2n|g) and 7.1 {I9} from ({+3}He,2n|g) 
M$D+Q from |g(|q) in ({+3}He,2n|g) (2016Gi05) 
MR$or -5.2 {I+12-17} from |g(|q) in ({+3}He,2n|g) (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted average of 1144.2 {I4} from {+98}Rh |e decay (8.72 min), 1144.2 {I4} from {+98}Rh |e decay (3.6 min), 1145.1 {I2} from (|a,2n|g), 1144.52 {I5} from ({+3}He,2n|g), and 1145.0 {I4} from (|a,4n|g) 
M$from |g(|q) and ce data in (|a,4n|g) and ({+3}He,2n|g) 
MR$from |g(|q) in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1164.3 {I4} from {+98}Rh |e decay (8.72 min), 1165.3 {I3} from (|a,2n|g), and 1164.78 {I5} from ({+3}He,2n|g) 
M,MR$mult from ce and |d from |g|g(|q) data in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1817.2 {I4} from {+98}Rh |e decay (8.72 min), and 1817.1 {I3} from ({+3}He,2n|g). Others: 1818.4 {I4} tentatively assigned to {+98}Ru in (|a,2n|g), 
RI$others: 38 {I3} from {+98}Rh |e decay (8.72 min), 14.1 {I16} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
E$weighted average of 599.0 {I4} from {+98}Rh |e decay (3.6 min), 598.9 {I3} from (|a,2n|g), 598.44 {I5} from ({+3}He,2n|g), and 599.0 {I4} from (|a,4n|g) 
RI$unweighted average of 70 {I4} from ({+3}He,2n|g) and 89 {I4} from (|a,2n|g). Others: 100 {I10} from {+98}Rh |e decay (3.6 min) and (|a,4n|g) 
M$from |g(|q) and ce in (|a,4n|g) and |g|g(|q) in ({+3}He,2n|g) 
MR$from |g|g(|q) in ({+3}He,2n|g). Other: +2.8 {I12} from |g(|q) and ce in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 615.7 {I4} from {+98}Rh |e decay (3.6 min), 615.0 {I3} from (|a,2n|g), 614.87 {I5} from ({+3}He,2n|g), and 615.1 {I4} from (|a,4n|g) 
RI$from ({+3}He,2n|g) and (|a,2n|g). Others: 98 {I10} from {+98}Rh |e decay (3.6 min) and 48 {I5} from (|a,4n|g) 
M$D+Q from |g(|q) and |g|g(|q) in ({+3}He,2n|g); (E2+M1) from ce data in (|a,4n|g) 
MR$from |g|g(|q) in ({+3}He,2n|g) (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1360.9 {I5} from {+98}Rh |e decay (3.6 min), 1360.9 {I4} from (|a,2n|g), and 1360.1 {I4} from ({+3}He,2n|g) 
RI$unweighted average of 10.1 {I16} from (|a,2n|g), and 6 {I1} from ({+3}He,2n|g). Other: 16.3 {I25} from {+98}Rh |e decay (3.6 min) 


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$weighted average of 824.4 {I4} from {+98}Rh |e decay (3.6 min), 825.3 {I4} from ({+36}S,p2n|g), 825.1 {I1} from ({+36}S,|a4n|g), 825.1 {I2} from (|a,2n|g), 824.69 {I5} from ({+3}He,2n|g), and 824.9 {I4} from (|a,4n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(|q,pol) and ce data in ({+3}He,2n|g), |g(|q) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$others: 253.8 {I3} from (|a,2n|g), 253.9 {I4} from (|a,4n|g) 
RI$weighted average of 26.4 {I11} from (|a,2n|g), 21 {I2} from ({+3}He,2n|g), and 21.7 {I22} from (|a,4n|g) 
M$from |g(|q) and ce data in ({+3}He,2n|g) and |g(|q) in (|a,4n|g) 
MR$from |g(|q) in ({+3}He,2n|g). Other: +3.5 {I+20-12} from (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$others: 469.6 {I2} from (|a,2n|g), 469.7 {I4} from (|a,4n|g) 
RI$others: 100 {I4} from (|a,2n|g), 100 {I9} from (|a,4n|g) 
M$from |g(|q,pol) in ({+3}He,2n|g), |g(|q) and ce data in (|a,4n|g) 
MR$from |g(|q) and ce data in (|a,4n|g). Other: +0.45 {I+14-8} or +4.20 {I+6-13} from |g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 869.2 {I3} from (|a,2n|g) and 868.5 {I2} from ({+3}He,2n|g) 
RI$weighted average of 28.7 {I11} from (|a,2n|g) and 29 {I3} from ({+3}He,2n|g) 
M,MR$from |g|g(|q) and |g(pol) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$other: 879.6 {I3} from (|a,2n|g) 
M$M1,E2 from |g(|q,pol) and ce data in ({+3}He,2n|g), but |DJ|p requires E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 609.9 {I4} from (|a,2n|g) and 610.0 {I1} from ({+3}He,2n|g) 
RI$unweighted average of 6.5 {I10} from (|a,2n|g) and 10 {I1} from ({+3}He,2n|g) 
M,MR$from |g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 630.3 {I4} from (|a,2n|g) and 629.9 {I2} from ({+3}He,2n|g) 
RI$unweighted average of 6.0 {I10} from (|a,2n|g) and 10.3 {I15} from ({+3}He,2n|g) 
M$from |g(|q,pol) in ({+3}He,2n|g) (1988Sa01) 
MR$deduced by 2016Gi05 from A{-2} in 1988Sa01 for J(2427)=2 in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$other: 1776.4 {I6} from 2004Ca42 in (|a,2n|g), transition identified as a doublet in 2004Ca42 
M,MR$mult from |g(|q,pol) (1988Sa01) and |d from |g|g(|q) (2016Gi05) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
E$from {+98}Rh |e decay (8.72 m) only with I(670.2|g)/I(2467.6|g)=100/19.5; but its existence can not be confirmed by 2004Ca42 in (|a,2n|g) and 2016Gi05 in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$from {+98}Rh |e decay (8.72 m) only; this transition can not been seen by 2004Ca42 in (|a,2n|g) and 2016Gi05 in ({+3}He,2n|g) due detector limit 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 280.5 {I4} from (|a,2n|g) 
RI$unweighted average of 10 {I2} from ({+3}He,2n|g) and 5.4 {I9} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$others: 324.6 {I3} from (|a,2n|g), 323.9 {I10} from ({+36}S,|a4n|g) 
RI$weighted average of 21 {I2} from ({+3}He,2n|g) and 21.7 {I9} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1149.17 {I5} from ({+3}He,2n|g), 1149.7 {I2} from (|a,2n|g), 1149.6 {I4} from (|a,4n|g) and 1149.1 {I10} from ({+36}S,|a4n|g) 
M$E2 from |g(|q) and ce data in (|a,4n|g), but ce data also agree with M1; D+Q from |g|g(|q) in ({+3}He,2n|g) (2016Gi05) 
MR$from |g|g(|q) in ({+3}He,2n|g) (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
E$others: 1259.3 {I2} in (|a,2n|g), 1259.4 {I4} in (|a,4n|g) 
M,MR$from |g(|q) in (|a,2n|g). Mult=D from |g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$weighted average of 645.1 {I4} from (|a,2n|g) and 644.9 {I2} from ({+3}He,2n|g) 
RI$other: 16 {I2} from (|a,2n|g) 
M$from ce data in ({+3}He,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$unweighted average of 904.1 {I4} from ({+36}S,p2n|g), 904.7 {I1} from ({+36}S,|a4n|g), 904.1 {I2} from (|a,2n|g), 903.80 {I5} from ({+3}He,2n|g), and 904.1 {I4} from (|a,4n|g) 
M$from |g(|q,pol) in ({+3}He,2n|g), |g(pol) and |g(DCO) in ({+36}S,|a4n|g), |g(|q) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 968.5 {I3} from ({+36}S,|a4n|g), 968.0 {I2} from (|a,2n|g), 967.69 {I5} from ({+3}He,2n|g), and 968.0 {I4} from (|a,4n|g). Other: 969.4 {I4} from ({+36}S,p2n|g) 
M$from |g(|q,pol) and ce data in ({+3}He,2n|g), |g(pol) and |g(DCO) in ({+36}S,|a4n|g), |g(|q) and ce data in (|a,4n|g). But |DJ=1, dipole suggested from |g(DCO) in ({+36}S,p2n|g) (1998Kh01) is in disagreement 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E,RI$from {+98}Rh |e decay (8.72 min) only. Not seen by 2016Gi05 in ({+3}He,2n|g) probably due to detector limit 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 979.2 {I2} from (|a,2n|g) and 978.8 {I1} from ({+3}He,2n|g) 
M$E2 from ce data in ({+3}He,2n|g), but also in overlap with M1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 591.3 {I4} from (|a,2n|g) and 590.7 {I2} from ({+3}He,2n|g) 
RI$weighted average of 46 {I7} from (|a,2n|g) and 38 {I4} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 594.7 {I4} from (|a,2n|g) and 594.2 {I2} from ({+3}He,2n|g) 
RI$weighted average of 56 {I8} from (|a,2n|g) and 42 {I5} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 984.9 {I3} from (|a,2n|g) and 984.4 {I2} from ({+3}He,2n|g) 
M$from |g(|q) and ce data in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 627.1 {I3} from (|a,2n|g), 626.8 {I4} from (|a,4n|g), and 626.9 {I1} from ({+3}He,2n|g) 
RI$weighted average of 25.5 {I11} from (|a,2n|g), 29 {I4} from (|a,4n|g), and 23 {I2} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1062.6 {I10} from ({+36}S,|a4n|g), 1061.2 {I2} from (|a,2n|g), 1060.6 {I1} from ({+3}He,2n|g), and 1061.8 {I4} from (|a,4n|g) 
M$from |g(|q) and ce data in ({+3}He,2n|g). But E1 suggested from |g(|q) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1624.7 {I6} from {+98}Rh |e decay (3.6 min) and 1625.3 {I5} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 229.8 {I4} from (|a,2n|g) and 229.1 {I2} from ({+3}He,2n|g) 
RI$weighted average of 66 {I9} from (|a,2n|g) and 78 {I13} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 412.4 {I3} from (|a,2n|g), 412.1 {I1} from ({+3}He,2n|g), 412.3 {I4} from (|a,4n|g) and , 412.0 {I10} from ({+36}S,|a4n|g) 
RI$from (|a,2n|g). Others: 100 {I6} from ({+3}He,2n|g), 81 {I6} from (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 992.0 {I3} from (|a,2n|g), 991.8 {I2} from ({+3}He,2n|g), 992.3 {I4} from (|a,4n|g) and 993.0 {I10} from ({+36}S,|a4n|g) 
RI$unweighted average of 79 {I3} from (|a,2n|g) and 65 {I5} from ({+3}He,2n|g). Other: 100 {I13} from (|a,4n|g) 
M$from |g(|q) and ce data in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 295.1 {I10} from ({+36}S,|a4n|g), 295.5 {I4} from (|a,2n|g), and 295.0 {I2} from ({+3}He,2n|g) 
E$weighted average of 26 {I4} from (|a,2n|g), and 19 {I4} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 1033.7 {I10} from ({+36}S,|a4n|g), 1032.1 {I3} from (|a,2n|g), and 1031.5 {I1} from ({+3}He,2n|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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
E$unweighted average of 725.4 {I1} from ({+36}S,|a4n|g), 725.2 {I2} from (|a,2n|g), 724.7 {I1} from ({+3}He,2n|g), and 724.9 {I4} from (|a,4n|g). Other: 725.7 {I4} from ({+36}S,p2n|g), placed from a level 7626 
M$from |g(|q) and ce data in ({+3}He,2n|g). E1 from |g(DCO) and |g(pol) in (|a,4n|g) and from |g(|q,pol) in ({+3}He,2n|g) 
MR$from |g(|q) in ({+3}He,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 569.0 {I2} from ({+3}He,2n|g) and 567.4 {I10} (placed from the 3851, 9- level) from ({+36}S,|a4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 662.1 {I4} from ({+3}He,2n|g), 661.3 {I5} from ({+36}S,|a4n|g), and 661.3 {I4} from (|a,2n|g) and (|a,4n|g) (placed from the 3851, 9- level except for the first one). 


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$weighted average of 811.4 {I5} from ({+36}S,|a4n|g), 810.7 {I3} from (|a,2n|g), 810.3 {I2} from ({+3}He,2n|g), 810.5 {I4} from (|a,4n|g), and 810.9 {I4} from ({+36}S,p2n|g) 
RI$weighted average of 75 {I17} from ({+36}S,|a4n|g), 42.5 {I17} from (|a,2n|g), 38 {I4} from ({+3}He,2n|g), and 46 {I3} from (|a,4n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(|q) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$unweighted average of 875.4 {I3} from ({+36}S,|a4n|g), 874.7 {I2} from (|a,2n|g), 874.3 {I1} from ({+3}He,2n|g), and 874.6 {I4} from (|a,4n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(|q) and ce data in (|a,4n|g). In ({+36}S,p2n|g) it was suggested as |DJ=1, E1 transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 722.4 {I2} from ({+3}He,2n|g), 722.7 {I4} from (|a,4n|g), 722.9 {I3} from (|a,2n|g) 
RI$from (|a,2n|g). Others: 100 {I8} from ({+3}He,2n|g), 100 {I9} from (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 816.1 {I3} from (|a,2n|g) and 815.4 {I2} from ({+3}He,2n|g) 
RI$weighted average of 45.7 {I17} from (|a,2n|g) and 48 {I15} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2+M1)
decay_comment:
E$weighted average of 879.5 {I2} from ({+3}He,2n|g), 879.8 {I4} from (|a,4n|g), 879.6 {I3} from (|a,2n|g) 
RI$weighted average of 32 {I5} from (|a,2n|g) and 43 {I5} from ({+3}He,2n|g). Other: 85 {I7} from (|a,4n|g) 
M$from ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1033.3 {I3} from (|a,2n|g), 1032.5 {I2} from ({+3}He,2n|g), and 1033.2 {I4} from (|a,4n|g) 
RI$from (|a,2n|g). Others: 100 {I10} from ({+3}He,2n|g), 100 {I7} from (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1097.5 {I3} from (|a,2n|g), 1096.9 {I4} from ({+3}He,2n|g), and 1096.9 {I4} from (|a,4n|g) 
RI$weighted average of 49.4 {I19} from (|a,2n|g) and 33 {I9} from ({+3}He,2n|g). Other: 85 {I7} from (|a,4n|g) 
M$M1,E2 suggested from ce data in (|a,4n|g), E2 favored from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 822.0 {I1} from ({+36}S,|a4n|g), 821.3 {I2} from (|a,2n|g), 821.1 {I4} from (|a,4n|g), 821.3 {I2} from ({+36}S,p2n|g) (placed from a level at 4798) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(|q) and ce data in (|a,4n|g); also supported by |g(|q) in (|a,2n|g) and |g(DCO) in ({+36}S,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 840.7 {I3} from (|a,2n|g) and 840.4 {I4} from (|a,4n|g) 
RI$from (|a,2n|g) 
M$from |g(|q) in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 914.3 {I3} from ({+36}S,|a4n|g), 913.4 {I3} from (|a,2n|g), and 913.2 {I4} from (|a,4n|g). Other: 912.1 {I4} in ({+36}S,p2n|g) placed from a different level at 11629 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(|q) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 987.4 {I3} from ({+36}S,|a4n|g), 987.6 {I3} from (|a,2n|g), and 987.6 {I4} from (|a,4n|g). Other: 989.8 {I4} in ({+36}S,p2n|g) placed from a different level at 14948 
M$from |g(pol) in ({+36}S,|a4n|g), |g(|q) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 303.9 {I10} from ({+36}S,|a4n|g) and 303.4 {I4} from (|a,2n|g) 
RI$weighted average of 50 {I25} from ({+36}S,|a4n|g) and 72 {I12} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1218.1 {I5} from ({+36}S,|a4n|g) and 1217.3 {I4} from (|a,2n|g) 
RI$from (|a,2n|g). Other: 100 {I25} from ({+36}S,|a4n|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$weighted average of 848.5 {I1} from ({+36}S,|a4n|g), 848.0 {I3} from (|a,2n|g), 848.0 {I4} from (|a,4n|g), and 848.4 {I4} from ({+36}S,p2n|g) (placed from a level at 3977) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(|q) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 406.7 {I5} from ({+36}S,|a4n|g), 406.8 {I4} from (|a,2n|g), and 406.9 {I4} from ({+36}S,p2n|g) (placed from a level at 12941) 
RI$from ({+36}S,|a4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 904.3 {I3} from ({+36}S,|a4n|g), and 905.0 {I4} from ({+36}S,p2n|g) (placed from a level at 12534) 
RI$from ({+36}S,|a4n|g) for 904.7+904.3 doublet 
M$from |g(DCO) and |g(pol) for 904.7+904.3 doublet in ({+36}S,|a4n|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$weighted average of 1070.0 {I1} from ({+36}S,|a4n|g), 1069.3 {I4} from (|a,2n|g), 1069.9 {I4} from (|a,4n|g), and 1070.1 {I4} from ({+36}S,p2n|g) (placed from a level at 6900) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(|q) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 275.7 {I5} from ({+36}S,|a4n|g), and 277.2 {I4} from ({+36}S,p2n|g) (placed from a level at 11088) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1050.3 {I5} from ({+36}S,|a4n|g), and 1050.1 {I4} from ({+36}S,p2n|g) (placed from a level at 15998) 
RI$from ({+36}S,|a4n|g) for 904.7+904.3 doublet 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|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$unweighted average of 1032.3 {I1} from ({+36}S,|a4n|g), 1030.6 {I4} from (|a,4n|g), 1032.2 {I4} from ({+36}S,p2n|g) (placed from a level at 5831) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), also supported by |g(DCO) in ({+36}S,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 826.0 {I1} from ({+36}S,|a4n|g), and 826.1 {I4} from ({+36}S,p2n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(DCO) in ({+36}S,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1480.8 {I1} from ({+36}S,|a4n|g), and 1481.6 {I4} from ({+36}S,p2n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(DCO) in ({+36}S,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E$weighted average of 1076.0 {I3} from ({+36}S,|a4n|g), and 1075.6 {I4} from ({+36}S,p2n|g) (placed from a level at 12286) 
M$from |g(DCO) in ({+36}S,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$unweighted average of 398.1 {I3} from ({+36}S,|a4n|g), and 399.4 {I4} from ({+36}S,p2n|g) (placed from a level at 12286) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(DCO) in ({+36}S,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 1474.0 {I3} from ({+36}S,|a4n|g), and 1475.0 {I4} from ({+36}S,p2n|g) (placed from a level at 12286) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(DCO) in ({+36}S,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 877.6 {I3} from ({+36}S,|a4n|g), and 876.7 {I4} from ({+36}S,p2n|g) (placed from a level at 9329) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a4n|g), |g(DCO) in ({+36}S,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2193.6 {I5} from ({+36}S,|a4n|g), and 2192 {I1} from ({+36}S,p2n|g) (placed from a level at 17240) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 888.1 {I5} from ({+36}S,|a4n|g), and 888.8 {I4} from ({+36}S,p2n|g) (placed from a level at 12099) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$weighted average of 1024.0 {I5} from ({+36}S,|a4n|g), and 1024.3 {I4} from ({+36}S,p2n|g) (placed from a level at 13310) 
M$from |g(DCO) in ({+36}S,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
E$weighted average of 761.5 {I4} (1978Ki17) and 762.3 {I4} (1972Ba37) 
RI$other: I|g=1.8 (1972Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 1413.4 {I4} (1978Ki17) and 1414.9 {I4} (1972Ba37) 
RI$other: 1.2 (1972Ba37) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$rounded value from Adopted Gammas 
$B(E2)(W.u.)=36 {I18}, 52 {I26}, 42 {I21}, and 49 {I25}, for four different combinations of B(E2)(W.u.)(1414,2+ to 1320,0+)=1 or 0 (1 for first two B(E2) values and 0 for others) and the relative sign=same or opposite for interfering matrix elements for the excitation of the second 2+ state, respectively (2006Wi15). The weighted average is 43 {I11}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 748 {I10} (1961St02) 
$B(E2)(W.u.)=50 {I18}, 59 {I21}, 50 {I18}, and 57 {I21}, for four different combinations of B(E2)(W.u.)(1414,2+ to 1320,0+)=1 or 0 (1 for first two B(E2) values and 0 for others) and the relative sign=same or opposite for interfering matrix elements for the excitation of the second 2+ state, respectively (2006Wi15). The weighted average is 53 {I10}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$tentatively assigned to {+98}Ru as it only appears at some beam energies. The summing contribution to this line is estimated at <0.03 units of intensity. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$this |g was not observed by 2004Ca42, only an upper limit of intensity given, as shown in authors' Fig. 4 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 669.9 {I1} mentioned in the text but not adopted in Table II in 2016Gi05 
$I|g(rel)=1.7 {I3} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
M$from Adopted Gammas 
MR$from |g|g(|q) (2016Gi05). Other values from |g(|q): -0.25 {I+14-5} or +6.0 {I+23-27} (2016Gi05) 
$A{-2}=+0.01 {I1}, POL=-0.05 {I4}, I|g(rel)=10.2 {I7} (1988Sa01); A{-2}=+0.02 {I2} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$weighted average of 25.6 {I9} from 1988Sa01 and 27 {I3} from 2016Gi05 
MR$from |a(K)exp in 2016Gi05. Evaluators obtain |d=0.9 {I+7-4}. Other values from |g(|q): +0.02 {I+10-16} or -3.5 {I12} (2016Gi05) 
$A{-2}=-0.091 {I14}, POL=+0.07 {I10}, I|g(rel)=3.0 {I1} (1988Sa01); A{-2}=-0.117 {I30} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 399.1 {I3} from 1988Sa01 and 398.8 {I2} from 2016Gi05 
RI$weighted average of 6.8 {I9} from 1988Sa01 and 10 {I3} from 2016Gi05 
MR$-0.22 {I+7-16} or -5.2 {I+12-17} from |g(|q) (2016Gi05) 
$A{-2}=+0.06 {I4}, POL=+0.14 {I18}, I|g(rel)=0.8 {I1} (1988Sa01); A{-2}=+0.08 {I6} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
RI$weighted average of 100 {I7} from 1988Sa01 and 100 {I1} from 2016Gi05 
$A{-2}=+0.025 {I10}, POL=+0.01 {I5}, I|g(rel)=11.7 {I8} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from |g|g(|q) (2016Gi05). The |a(K) exp value is somewhat high for M1 or E2 
$A{-2}=-0.03 {I2}, POL=+0.07 {I21}, I|g(rel)=3.0 {I2} (1988Sa01); A{-2}=-0.01 {I3} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$weighted average of 71 {I7} from 1988Sa01 and 70 {I4} from 2016Gi05 
MR$from |g|g(|q) (2016Gi05) 
$I|g(rel)=3.2 {I3} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$weighted average of 100 {I7} from 1988Sa01 and 100 {I4} from 2016Gi05 
MR$from |g|g(|q) (2016Gi05). Other values: +0.24 {I+20-10} or >+3 from |g(|q) (2016Gi05). Note that the sign(|d) is different in |g|g(|q) and |g(|q) 
$A{-2}=-0.108 {I11}, POL=+0.03 {I8}, I|g(rel)=4.5 {I3} (1988Sa01); A{-2}=-0.111 {I36} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 843.6 {I3} from 1988Sa01 and 843.6 {I5} from 2016Gi05 
$A{-2}=+0.18 {I7}, POL=+0.5 {I4}, I|g(rel)=0.4 {I2} (1988Sa01) 
M$|g(|q) and POL data in 1988Sa01 suggest mult=E2 or E1 (if |DJ=0) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1593.4 {I3} from 1988Sa01 and 1593.4 {I2} from 2016Gi05 
MR$from |g|g(|q) (2016Gi05) 
$A{-2}=+0.06 {I14}, I|g(rel)=0.9 {I2} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$weighted average of 22 {I2} from 1988Sa01 and 20 {I3} from 2016Gi05 
$A{-2}=-0.36 {I2}, POL=-0.49 {I22}, I|g(rel)=1.1 {I1} (1988Sa01); A{-2}=-0.365 {I54} (2016Gi05) 
MR$from |g(|q) (2016Gi05). Other: |d<0.35 from |a(K)exp at 95% confidence level (2016Gi05). Evaluators obtain |d<0.16 for an uncertainty of one |s. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
RI$weighted average of 100 {I8} from 1988Sa01 and 100 {I3} from 2016Gi05 
MR$+0.45 {I+14-8} or +4.20 {I+6-13} from |g(|q) (2016Gi05), the latter is favored by |g(pol) data of 1988Sa01 
$A{-2}=+0.135 {I9}, POL=+0.20 {I9}, I|g(rel)=5.0 {I4} (1988Sa01); A{-2}=+0.114 {I42} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
E$weighted average of 868.7 {I3} from 1988Sa01 and 868.4 {I2} from 2016Gi05 
RI$weighted average of 26 {I4} from 1988Sa01 and 30 {I3} from 2016Gi05 
MR$from |g|g(|q) (2016Gi05). Others: -0.37 {I+32-12} or +2.1 {I+10-12} from |g(|q) (2016Gi05). The |g(pol) data of 1988Sa01 for |DJ=0 transitions favors dominant E2. 
$A{-2}=-0.07 {I2}, POL=-0.6 {I4}, I|g(rel)=1.3 {I2} (1988Sa01); A{-2}=+0.04 {I4} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$weighted average of 879.0 {I3} from 1988Sa01 and 879.2 {I1} from 2016Gi05 
RI$weighted average of 56 {I13} from 1988Sa01 and 57 {I3} from 2016Gi05 
$2016Gi05 state that presence of a very weak 879.5|g from 4005.6-keV level does not affect the |a(K)exp value for 879.2|g, as the intensity of the 879.5|g is approximately 4% that of the intensity of 879.2|g 
$A{-2}=+0.10 {I2}, POL=-0.15 {I63}, I|g(rel)=0.9 {I2} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1624.3 {I3} from 1988Sa01 and 1624.2 {I3} from 2016Gi05 
RI$weighted average of 100 {I25} from 1988Sa01 and 100 {I4} from 2016Gi05 
$A{-2}=+0.8 {I4}, POL=+0.5 {I3}, I|g(rel)=1.6 {I4} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 610.1 {I3} from 1988Sa01 and 610.0 {I1} from 2016Gi05 
RI$weighted average of 9.1 {I23} from 1988Sa01 and 10 {I1} from 2016Gi05 
$A{-2}=-0.11 {I8}, POL=-0.4 {I4}, I|g(rel)=0.4 {I1} (1988Sa01); A{-2}=-0.091 {I33} (2016Gi05) 
MR$from |g(|q) for J(2427)=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 630.1 {I3} from 1988Sa01 and 629.8 {I2} from 2016Gi05 
RI$weighted average of 6.8 {I23} from 1988Sa01 and 11 {I1} from 2016Gi05 
M$|g(pol) in 1988Sa01 suggests dominant M1 
MR$|d(Q/D)=-0.04 {I45} deduced by 2016Gi05 from A{-2} in 1988Sa01 for J(2427)=2 
$A{-2}=+0.17 {I7}, POL=-1.4 {I7}, I|g(rel)=0.3 {I1} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1029.4 {I3} from 1988Sa01 and 1029.0 {I1} from 2016Gi05 
RI$weighted average of 18 {I5} from 1988Sa01 and 21 {I1} from 2016Gi05 
$A{-2}=+0.09 {I20}, POL=+0.02 {I50}, I|g(rel)=0.8 {I2} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1774.5 {I3} from 1988Sa01 and 1774.5 {I3} from 2016Gi05 
RI$weighted average of 100 {I11} from 1988Sa01 and 100 {I2} from 2016Gi05 
M$dominant M1 from |g(pol) in 1988Sa01 if 1774|g is |DJ=0 transition 
MR$from |g|g(|q) (2016Gi05) 
$A{-2}=+0.28 {I19}, POL=+0.5 {I3}, I|g(rel)=4.4 {I5} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 324.5 {I3} from 1988Sa01 and 324.4 {I1} from 2016Gi05 
RI$weighted average of 22 {I2} from 1988Sa01 and 20 {I2} from 2016Gi05 
M$from |g(pol) in 1988Sa01 
$A{-2}=+0.01 {I14}, POL=-0.55 {I16}, I|g(rel)=1.0 {I1} (1988Sa01) 
$In singles, I|g(324)/I|g(1149) is larger, as the 324|g is contaminated by a 324.5 line from {+97}Tc 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$weighted average of 100 {I9} from 1988Sa01 and 100 {I4} from 2016Gi05 
$A{-2}=+0.17 {I1}, I|g(rel)=4.5 {I4} (1988Sa01); A{-2}=+0.19 {I2} (2016Gi05) 
MR$from |g|g(|q) (2016Gi05). Other values: +0.44 {I10} or +3.6 {I+5-10} from |g(|q) for J(2547)=5 (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 1322.5 {I3} from 1988Sa01 and 1322.2 {I1} from 2016Gi05 
$A{-2}=-0.05 {I4}, POL=+0.09 {I49}, I|g(rel)=0.9 {I2} (1988Sa01); A{-2}=-0.09 {I5} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 542.7 {I3} from 1988Sa01 and 542.8 {I1} from 2016Gi05 
$A{-2}=+0.18 {I4}, POL=+0.17 {I15}, I|g(rel)=0.9 {I3} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1012.2 {I3} from 1988Sa01 and 1012.4 {I1} from 2016Gi05 
$A{-2}=+0.15 {I7}, POL=+0.14 {I42}, I|g(rel)=0.7 {I2} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 320.7 {I3} from 1988Sa01 and 320.3 {I1} from 2016Gi05 
RI$weighted average of 100 {I18} from 1988Sa01 and 100 {I5} from 2016Gi05 
$A{-2}=+0.08 {I26}, POL=-0.37 {I30}, I|g(rel)=1.1 {I2} (1988Sa01); A{-2}=+0.11 {I5} (2016Gi05) 
$|d(E2/M1) from |a(K)exp 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$weighted average of 645.2 {I3} from 1988Sa01 and 644.8 {I2} from 2016Gi05 
RI$weighted average of 45 {I9} from 1988Sa01 and 52 {I3} from 2016Gi05 
$I|g(rel)=0.5 {I1} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 1667.1 {I3} from 1988Sa01 and 1667.0 {I1} from 2016Gi05 
$A{-2}=-0.08 {I5}, POL=+0.4 {I4}, I|g(rel)=1.0 {I3} (1988Sa01); A{-2}=-0.18 {I8} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.20 {I4}, POL=+0.41 {I27}, E|g=978.9 {I3}, I|g(rel)=1.1 {I3} (1988Sa01); A{-2}=+0.251 {I32} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 19 {I5} from 1988Sa01 and 24.0 {I20} from 2016Gi05 
$E|g=626.9 {I3}, I|g(rel)=0.4 {I1} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=-0.13 {I3}, POL=+0.13 {I14}, E|g=1060.9 {I3}, I|g(rel)=2.1 {I3} (1988Sa01); A{-2}=-0.115 {I29} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=+0.53 {I28}, POL=-0.86 {I67}, I|g(rel)=0.6 {I3} (1988Sa01) 
E$weighted average of 1301.2 {I2} from 2016Gi05 and 1301.0 {I3} from 1988Sa01 
$Placement of 1301.2|g from 1953 level in 1988Sa01 is rejected by 2016Gi05 based on their |g|g-coin data, thus removing the 1953-keV level in 1988Sa01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=+0.19 {I9}, POL=+0.3 {I5}, E|g=412.1 {I3}, I|g(rel)=0.5 {I1} (1988Sa01); A{-2}=+0.197 {I80} (2016Gi05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$weighted average of 725.1 {I3} from 1988Sa01 and 724.7 {I1} from 2016Gi05 
$A{-2}=-0.28 {I14}, POL=+0.66 {I53}, I|g(rel)=0.4 {I1} (1988Sa01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$|a(K)exp is too low to be consistent with M1 or E2, it is in agreement with E1, but results of other experiments do not support E1 
MR$from |g(|q) data 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$Note that negative A{-4} is inconsistent with |DJ=1 transition. The |a(K)exp value agrees with E2, and only marginally with M1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A 1032|g placed with 3255 level in 1971Le19 from (|a,2n|g) and with a 2430 level in 1988Sa01 from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
EKC Reference value for calibration of |a(K)exp. 
MR from 1974Be11. RUL rules out E1+M2. |d=+0.21 {I+14-20} or +1.1 {I+1-2} from |g|g(|q) (1976ShYU); other: 0.1<|d<1.4 from |g|g(|q) (1967Mo20). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
MR$+0.35 {I5} or 6.5 {I15} 
A{-2}=+0.260 {I14}, A{-4}=-0.062 {I26} 
M |a(K)exp=0.0016 {I3} (1981Du06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
MR$-0.04 {I6} or -5.7 {I15} 
A{-2}=-0.24 {I6}, A{-4}=+0.09 {I12} 
M |a(K)exp=0.0057 {I20} (1981Du06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$-0.54 {I16} or +1.6 {I+6-4} for 13/2 to 13/2 and +0.2 {I+7-6} or >+7 for 15/2 to 13/2 
A{-2}=+0.07 {I7}, A{-4}=-0.25 {I11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.045 {I30} for 17/2 to 15/2 and +0.04 {I+20-8} or +0.45 {I+10-20} for 15/2 to 15/2 
A{-2}=+0.348 {I20}, A{-4}=+0.07 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$>10 or +0.1 {I1} for 17/2 to 15/2 and -0.9 {I+4-7} or +2.6 {I+80-11} for 15/2 to 15/2 
A{-2}=-0.06 {I14}, A{-4}=-0.06 {I26} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
MR$+0.34 {I+4-3} or +4.6 {I+7-6} for 15/2 to 13/2 
A{-2}=+0.23 {I3}, A{-4}=-0.01 {I6} for 903.9+904.3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.32 {I+4-3} or +4.7 {I+8-6} for 19/2 to 17/2 and -0.29 {I7} for 17/2 to 17/2 
A{-2}=+0.23 {I4}, A{-4}=-0.02 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.22 {I45} or +9 {I+5-3} for 19/2 to 17/2 and -0.57 {I12} or +1.4 {I3} for 17/2 to 17/2 
A{-2}=+0.09 {I6}, A{-4}=0.00 {I11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.5 {I3} for 19/2 to 17/2 and -1.25 {I+17-20} or +3.8 {I+16-8} for 17/2 to 17/2 
A{-2}=-0.14 {I4}, A{-4}=+0.06 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
MR$-6 {I1} or -0.07 {I3} for 19/2 to 17/2 and -5.4 {I+6-8} or -0.08 {I25} for 17/2 to 15/2 
A{-2}=-0.311 {I28}, A{-4}=+0.01 {I6} 
M |a(K)exp=0.0071 {I20} (1981Du06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.01 {I6} or <-15 for 19/2 to 21/2; -1.4 {I+4-8} or >+2.5 for 19/2 to 19/2 and <-8 or +0.04 {I6} for 19/2 to 17/2 
A{-2}=-0.16 {I8}, A{-4}=-0.07 {I15} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+7 {I+2-4} or -0.04 {I5} for 19/2 to 17/2 and <-1.6 and >+7 for 17/2 to 17/2 
A{-2}=-0.26 {I7}, A{-4}=-0.08 {I16} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$-4.5 {I+26-100} or -0.12 {I+23-29} for 19/2 to 17/2 and <-1 and >+2.5 for 17/2 to 17/2 
A{-2}=-0.4 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$-7.3 {I+15-25} or -0.04 {I4} for 21/2 to 19/2 and <-2, >+13 for 19/2 to 19/2 
A{-2}=-0.28 {I5}, A{-4}=+0.08 {I10} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.53 {I+11-9} or +2.5 {I+6-5} for 19/2 to 17/2 and +0.22 {I15} for 17/2 to 17/2 
A{-2}=+0.43 {I7}, A{-4}=-0.08 {I11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.6 {I+2-1} or +2.0 {I5} for 21/2 to 19/2 and -1.0 {I4} for 17/2 to 19/2 
A{-2}=+0.50 {I7}, A{-4}=+0.15 {I11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
MR$<-7 or +0.04 {I9} for 21/2 to 19/2 and -1.4 {I+5-200} or +3.9 {I+60-19} for 19/2 to 19/2 
A{-2}=-0.15 {I13} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.42 {I+8-6} or +3.2 {I+8-6} for 21/2 to 19/2 and +0.2 {I5} for 19/2 to 19/2 
A{-2}=+0.34 {I7}, A{-4}=-0.21 {I11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.48 {I5} or +2.7 {I+4-3} for 23/2 to 21/2 and +0.18 {I22} for 21/2 to 21/2 
A{-2}=+0.40 {I3}, A{-4}=-0.16 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.35 {I4} or 4.0 {I5} for 25/2 to 23/2 and -0.28 {I+9-8} or +0.67 {I12} for 23/2 to 23/2 
A{-2}=+0.28 {I3}, A{-4}=-0.02 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.4 {I1} or +3.3 {I+8-6} for 23/2 to 21/2 and -0.15 {I+30-15} or +0.6 {I+2-4} for 21/2 to 21/2 
A{-2}=+0.33 {I6}, A{-4}=-0.20 {I11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$-0.09 {I9} or -5.6 {I+20-50} for 23/2 to 21/2 and <-2 or >+8 for 21/2 to 21/2 
A{-2}=-0.35 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.13 {I10} or >+7 for 29/2 to 27/2 and -0.9 {I+3-5} or +1.6 {I+13-6} for 27/2 to 27/2 
A{-2}=-0.01 {I14}, A{-4}=+0.01 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.51 {I+40-17} or +2.4 {I+15-11} for 29/2 to 27/2 and +0.1 {I5} for 27/2 to 27/2 
A{-2}=+0.45 {I16}, A{-4}=-0.18 {I25} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E from 1980Al02. 
RI from I|g(232.8|g)/I|g(140.5|g)=0.095|*10{+-6} {I17} (1980Al02). I|g deduced if I|g(142.6|g)/I|g(140.5|g)=2.1|*10{+-4} {I2}, |a(140.5|g)=0.114 {I3}, |a(142.6|g)=40.9 {I12} (see {+99}Tc IT decay), and Branching=3.7|*10{+-5}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E from 1970Jo24. 
RI from I|g(322.4|g)/I|g(140.5|g)=1.09|*10{+-6} {I6} (weighted average of 1.13|*10{+-6} {I9} (1980Al02), 1.10|*10{+-6} {I10} (1972De26), and 0.97|*10{+-6} {I15} (1970Jo24)) 


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$weighted average of 539.512 {I5} from {+100}Rh |e decay (20.8 h) and 539.508 {I2} from (n,|g) E=th. Others: 539.52 {I11} from {+100}Tc |b{+-} decay (15.46 s), 539.7 {I1} from ({+36}S,|a2n|g), 539.509 {I14} from (|a,2n|g), 539.7 {I3} from (|a,4n|g), 539.506 {I18} from (n,n'|g), and 539.6 {I1} from Coulomb excitation 
M$from ce data in {+100}Rh |e decay (20.8 h), |g(DCO) in ({+36}S,|a2n|g) and ({+34}S,2|a2n|g), |g(|q) in (|a,2n|g) and (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$weighted average of 590.792 {I6} from {+100}Rh |e decay (20.8 h), 590.844 {I20} from (|a,2n|g), 590.765 {I9} from (n,|g) E=th, and 590.774 {I20} from (n,n'|g). Others: 590.77 {I10} from {+100}Tc |b{+-} decay (15.46 s) and 590.8 {I5} from Coulomb excitation 
M$M1,E2 from ce data and Q from |g|g(|q) in {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E,M$from ce data in {+100}Rh |e decay (20.8 h) 
$q{-K}{+2}(E0/E2)=0.098 {I9}, X(E0/E2)=0.0104 {I9}, |r{+2}(E0)=0.0103 {I18} (2005Ki02, evaluation) 
$B(E0)(Wilkinson units)=0.048 {I8} 


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$weighted average of 686.971 {I7} from {+100}Rh |e decay (20.8 h), 686.973 {I17} from (|a,2n|g), 686.972 {I3} from (n,|g) E=th, and 686.963 {I17} from (n,n'|g). Others: 687.5 {I1} from ({+36}S,|a2n|g), 687.4 {I3} from (|a,4n|g), and 686.9 {I5} from Coulomb excitation 
M$M1,E2 from ce data and Q from |g|g(|q) in {+100}Rh |e decay (20.8 h); also from |g(DCO) and |g(pol) in ({+36}S,|a2n|g), |g(DCO) in ({+34}S,2|a2n|g), |g(|q) in (|a,2n|g), (|a,4n|g) an d(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 822.6 {I1} from {+100}Tc |b{+-} decay (15.46 s), 822.654 {I7} from {+100}Rh |e decay (20.8 h), 822.666 {I17} from (|a,2n|g), 822.614 {I10} from (n,|g) E=th, 822.672 {I16} from (n,n'|g), and 822.5 {I2} from Coulomb excitation 
RI$from (n,n'|g). Others: 100.0 {I10} from {+100}Rh |e decay (20.8 h), 100.0 {I12} from (|a,2n|g), 100 {I4} from (n,|g) E=th. 
M$from ce data and |g|g(|q) in {+100}Rh |e decay (20.8 h) and |g(|q) in (n,n'|g), 100 {I8} from (n,|g) E=res 
MR$weighted average of +3.7 {I3} (2001Ge03) from |g(|q) in (n,n'|g), +3.2 {I8} (1978Ba29) and 3.7 {I4} (1990KeZV) from |g|g(|q) in {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1362.152 {I10} from {+100}Rh |e decay (20.8 h), 1362.172 {I23} from (|a,2n|g), 1362.17 {I3} from (n,|g) E=th, and 1362.160 {I21} from (n,n'|g). Others: 1362.2 {I1} from {+100}Tc |b{+-} decay (15.46 s) and 1362.1 {I2} from Coulomb excitation 
RI$weighted average of 72.95 {I23} from {+100}Rh |e decay (20.8 h), 73.3 {I12} from (|a,2n|g), and 73.6 {I5} from (n,n'|g). Others: 68 {I4} from (n,|g) E=th; 52 {I5} in Coulomb excitation, 95 {I3} in {+100}Tc |b{+-} decay and 112 {I11} in (n,|g) E=res are in disagreement 
M$from ce data and |g|g(|q) in {+100}Rh |e decay (20.8 h) and |g(|q) in (|a,2n|g) and (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 378.7 {I1} from {+100}Tc |b{+-} decay (15.46 s), 378.79 {I5} from {+100}Rh |e decay (20.8 h), 378.81 {I11} from (|a,2n|g), 379.10 {I10} from (n,|g) E=th, and 378.94 {I3} from (n,n'|g) 
RI$weighted average of 85 {I6} from {+100}Tc |b{+-} decay (15.46 s), 75.1 {I11} from (n,n'|g), and 69 {I12} from {+100}Rh |e decay (20.8 h). Others: 130 {I18} in (n,|g) E=th; 220 {I20} in (|a,2n|g) are in disagreement 
M$from ce data and |g|g(|q) in {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E,M$from ce data in {+100}Rh |e decay (20.8 h) 
$q{-K}{+2}(E0/E2)=0.9 {I5}, X(E0/E2)=1.1 {I6}, |r{+2}(E0)<0.090 (2005Ki02, evaluation) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1201.493 {I16} from {+100}Rh |e decay (20.8 h) and 1201.54 {I3} from (n,n'|g). Others: 1201.5 {I1} from {+100}Tc |b{+-} decay (15.46 s), 1201.4 {I3} from (|a,2n|g), and 1201.44 {I14} from (n,|g) E=th 
RI$from (n,n'|g). Others: 100 {I4} from {+100}Tc |b{+-} decay (15.46 s), 100.0 {I21} from {+100}Rh |e decay (20.8 h), 100 {I17} from (|a,2n|g), 100 {I18} from (n,|g) E=th 
M$(Q) from |g|g(|q) in {+100}Rh |e decay (20.8 h); polarity from no level-parity change 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E,M$from ce data in {+100}Rh |e decay (20.8 h) 
$ q{-K}{+2}(E0/E2)=1.6 {I9}, X(E0/E2)=0.6 {I3}, |r{+2}(E0)<0.048 (2005Ki02, evaluation) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
E$weighted average of 502.907 {I18} from {+100}Rh |e decay (20.8 h), 502.7 {I3} from (|a,2n|g), 503.09 {I10} from (n,|g) E=th, and 502.83 {I6} from (n,n'|g) 
RI$weighted average of 16.0 {I14} from {+100}Rh |e decay (20.8 h), 21 {I8} from (|a,2n|g), 19.8 {I28} from (n,|g) E=th, and 13.9 {I3} from (n,n'|g) 
M$from ce data in {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 638.619 {I14} from {+100}Rh |e decay (20.8 h), 638.81 {I13} from (|a,2n|g), 638.70 {I7} from (n,|g) E=th, and 638.72 {I5} from (n,n'|g) 
RI$unweighted average of 14.2 {I5} from {+100}Rh |e decay (20.8 h), 21 {I4} from (|a,2n|g), 25 {I3} from (n,|g) E=th, and 13.0 {I3} from (n,n'|g) 
M$M1,E2 from ce data in {+100}Rh |e decay (20.8 h); |DJ=2 requires E2 


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$weighted average of 734.806 {I7} from {+100}Rh |e decay (20.8 h), 734.789 {I7} from (n,|g) E=th, and 734.810 {I21} from (n,n'|g). Others: 734.8 {I3} from {+100}Tc |b{+-} decay (15.46 s) and 734.84 {I8} from (|a,2n|g) 
RI$weighted average of 76.8 {I7} from {+100}Rh |e decay (20.8 h), 78.3 {I6} from (n,n'|g), and 69 {I4} from (|a,2n|g). Others: 114 {I14} in {+100}Tc |b{+-}; 118 {I3} in (n,|g) E=th, 104 {I5} in (n,|g) E=res are in disagreement 
M$M1,E2 from ce data in {+100}Rh |e decay (20.8 h); |DJ=2 requires 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=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$weighted average of 1325.8 {I5} from {+100}Tc |b{+-} decay (15.46 s), 1325.583 {I13} from {+100}Rh |e decay (20.8 h), 1325.56 {I7} from (|a,2n|g), 1325.45 {I6} from (n,|g) E=th, and 1325.633 {I22} from (n,n'|g) 
RI$from (n,n'|g). Others: 100.0 {I10} from {+100}Rh |e decay (20.8 h), 100 {I4} from (|a,2n|g), 100 {I13} from (n,|g) E=th, 100 {I7} from (n,|g) E=res, 100 {I33} from {+100}Tc |b{+-} decay 
M$from ce data and |g|g(|q) in {+100}Rh |e decay (20.8 h) and |g(|q) in (n,n'|g) 
MR$from |g(|q) in (n,n'|g), -2.5 {I9} is also possible. Other: -1.6 {I+14-7} from |g|g(|q) in {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1864.9 {I2} from {+100}Tc |b{+-} decay (15.46 s), 1865.12 {I15} from {+100}Rh |e decay (20.8 h), 1865.12 {I9} from (|a,2n|g), 1865.04 {I6} from (n,|g) E=th, and 1865.07 {I6} from (n,n'|g) 
RI$weighted average of 93 {I7} from {+100}Tc |b{+-} decay (15.46 s), 90 {I4} from (|a,2n|g), and 96.4 {I12} from (n,n'|g), 109 {I13} from (n,|g) E=th, and 109 {I23} from (n,|g) E=res. Other: 63 {I6} in {+100}Rh |e decay (20.8 h) is in disagreement 
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=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$weighted average of 518.882 {I5} from {+100}Rh |e decay (20.8 h), 518.88 {I6} from (|a,2n|g), 519.11 {I13} from (n,|g) E=th, and 518.82 {I3} from (n,n'|g) 
RI$weighted average of 17.2 {I2} from {+100}Rh |e decay (20.8 h), 14.2 {I13} from (|a,2n|g), 22 {I4} from (n,|g) E=th, and 16.1 {I4} from (n,n'|g). Other: 86 {I4} in (n,|g) E=res is in disagreement 
M$from ce data and |g|g(|q) in {+100}Rh |e decay (20.8 h) and |g(|q) in (n,n'|g) and (|a,2n|g) 
MR$weighted average of +0.36 {I8} from (n,n'|g) and +0.38 {I6} from (|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$weighted average of 654.571 {I6} from {+100}Rh |e decay (20.8 h), 654.587 {I17} from (n,|g) E=th, and 654.60 {I3} from (n,n'|g). Other: 654.78 {I5} from (|a,2n|g) 
RI$unweighted average of 10.5 {I1} from {+100}Rh |e decay (20.8 h), 12.7 {I5} from (|a,2n|g), 14.2 {I8} from (n,|g) E=th, and 10.9 {I3} from (n,n'|g). Other: 116 {I31} in (n,|g) E=res is in disagreement 
M,MR$ce data in {+100}Rh |e decay (20.8 h) gives mult=M1,E2; mixing ratio is weighted average of +3.2 {I6} from |g(|q) in (n,n'|g) and +2.1 {I3} from |g(|q) 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$unweighted average of 1341.515 {I9} from {+100}Rh |e decay (20.8 h), 1341.601 {I18} from (|a,2n|g), 1341.560 {I9} from (n,|g) E=th, and 1341.515 {I22} from (n,n'|g) 
RI$from (n,|g) E=th. Others: 100.0 {I10} from {+100}Rh |e decay (20.8 h), 100.0 {I13} from (|a,2n|g), and 100.0 {I8} from (n,n'|g), 100 {I16} from (n,|g) E=res 
M$from ce data and |g|g(|q) in {+100}Rh |e decay (20.8 h), |g(|q) in (|a,2n|g) and (n,n'|g) 
MR$weighted average of +6.7 {I12} in (n,n'|g) and +5.5 {I5} in (|a,2n|g). Others: ce data give |d=4.4 {I+|@-21} and |g|g(|q) gives |d=6.8 {I+13-19}; +0.37 {I10} also from (n,n'|g) and +0.35 {I2} also from (|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$from {+100}Rh |e decay (20.8 h). Others: 689.2 {I1} from {+100}Tc |b{+-} decay (15.46 s), and 689.46 {I9} from (n,n'|g) 
RI$unweighted average of 12.3 {I4} from {+100}Tc |b{+-} decay (15.46 s) and 16.0 {I12} from {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1512.1 {I1} from {+100}Tc |b{+-} decay (15.46 s), 1512.140 {I16} from {+100}Rh |e decay (20.8 h), 1512.01 {I8} from (n,|g) E=th, and 1512.13 {I4} from (n,n'|g). Other: 1512.10 {I22} from (|a,2n|g) 
RI$from {+100}Rh |e decay (20.8 h). Others: 100 {I15} from {+100}Tc |b{+-} decay (15.46 s) 
M$Q from |g|g(|q) in {+100}Tc |b{+-} decay (15.46 s) and {+100}Rh |e decay (20.8 h); 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$weighted average of 700.52 {I6} from (n,|g) E=th and 700.51 {I5} from (n,n'|g). Other: 700.7 {I6} from (|a,2n|g) 
RI$weighted average of 47 {I3} from (|a,2n|g), 44.5 {I8} from (n,n'|g), 60 {I7} from (n,|g) E=th, and 88 {I24} from (n,|g) E=res. Other: 200 {I18} in {+100}Rh |e decay (4.6 min) is in disagreement 
M$Q from |g(|q) in (|a,2n|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=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$weighted average of 836.187 {I23} from (|a,2n|g), 836.180 {I3} from (n,|g) E=th, and 836.24 {I3} from (n,n'|g) 
RI$unweighted average of 87.6 {I18} from (|a,2n|g), 104 {I2} from (n,|g) E=th, 96 {I12} from E=res. Other: 188 {I18} in {+100}Rh |e decay (4.6 min); 52.4 {I2} in (n,n'|g) are in disagreement 
M$D+Q from |g(|q) in (n,n'|g) and (|a,2n|g); M2 ruled out by RUL 
MR$weighted average of +1.5 {I3} from |g(|q) in (n,n'|g) and +1.85 {I21} from |g(|q) from (|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$unweighted average of 1523.199 {I24} from (|a,2n|g), 1523.07 {I3} from (n,|g) E=th, and 1523.08 {I6} from (n,n'|g) 
RI$from (n,n'|g). Others: 100 {I13} from {+100}Rh |e decay (4.6 min), 100.0 {I15} from (|a,2n|g), 100 {I5} from (n,|g) E=th, 100 {I48} from (n,|g) E=res 
M$Q from |g(|q) in (n,n'|g) and (|a,2n|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 849.241 {I15} from (|a,2n|g), and 849.188 {I7} from (n,|g) E=th, and 849.241 {I15} from (n,n'|g). Others: 849.9 {I1} from ({+36}S,|a2n|g), 849.9 {I3} from (|a,4n|g) 
M$from |g(DCO) and |g(lin pol) in ({+36}S,|a2n|g), ce data and |g(|q) in (|a,4n|g), |g(|q) in (|a,2n|g), |g(DCO) in ({+34}S,2|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
E$weighted average of 736.966 {I20} from {+100}Rh |e decay (20.8 h), 736.93 {I18} from (|a,2n|g), 737.20 {I13} from (n,|g) E=th, and 737.15 {I6} from (n,n'|g) 
RI$weighted average of 13.16 {I13} from {+100}Rh |e decay (20.8 h), 13.2 {I7} from (n,n'|g), and 17 {I3} from (n,|g) E=th. Others: 57 {I9} in (|a,2n|g); 89 {I20} in (n,|g) E=res are in disagreement 
M$from ce data in {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 872.62 {I5} from {+100}Rh |e decay (20.8 h), 872.71 {I5} from (n,|g) E=th, and 872.67 {I16} from (n,n'|g) 
RI$unweighted average of 2.10 {I24} from {+100}Rh |e decay (20.8 h), 3.6 {I3} from (n,|g) E=th, and 1.59 {I25} 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$weighted average of 968.85 {I3} from {+100}Rh |e decay (20.8 h), 968.80 {I5} from (n,|g) E=th, and 968.68 {I10} from (n,n'|g). Other: 969.2 {I5} from (|a,2n|g) 
RI$unweighted average of 3.95 {I24} from {+100}Rh |e decay (20.8 h), 6.4 {I4} from (n,|g) E=th, and 3.18 {I25} from (n,n'|g). Other: 22 {I13} in (|a,2n|g) is in severe disagreement 


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$weighted average of 1558.9 {I3} from {+100}Tc |b{+-} decay (15.46 s), 1559.554 {I21} from {+100}Rh |e decay (20.8 h), 1560.1 {I6} from (|a,2n|g), 1559.37 {I6} from (n,|g) E=th, and 1559.56 {I3} from (n,n'|g) 
RI$from (n,n'|g). Others: 100.0 {I10} from {+100}Rh |e decay (20.8 h), 100 {I9} from {+100}Tc |b{+-} decay (15.46 s), 100 {I13} from (|a,2n|g), 100 {I12} from (n,|g) E=th, and 100 {I23} from (n,|g) E=res 
M$from ce data in {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 2099.16 {I7} from {+100}Rh |e decay (20.8 h), 2099.4 {I5} from (n,|g) E=th, and 2099.03 {I15} from (n,n'|g) 
RI$weighted average of 3.3 {I4} from {+100}Rh |e decay (20.8 h), 10 {I4} from (n,|g) E=th, and 4.28 {I25} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
E$weighted average of 301.771 {I8} from {+100}Rh |e decay (20.8 h), 301.769 {I1} from (n,|g) E=th. Others: 301.63 {I3} from (|a,2n|g), 301.82 {I3} from (n,n'|g) 
RI$weighted average of 12.7 {I9} from {+100}Rh |e decay (20.8 h), 13.5 {I12} from (|a,2n|g), and 12.63 {I24} from (n,n'|g). Other: 21.8 {I4} in (n,|g) E=th is in disagreement 
M$D(+Q) from |g(|q) in (n,n'|g) and (|a,2n|g); polarity from level-parity change 
MR$weighted average of +0.04 {I4} from |g(|q) in (n,n'|g) and +0.03 {I6} from |g(|q) 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$unweighted average of 804.73 {I8} from {+100}Rh |e decay (20.8 h) and 804.96 {I7} from (n,|g) E=th 
RI$unweighted average of 0.93 {I9} from {+100}Rh |e decay (20.8 h) and 3.5 {I4} from (n,|g) E=th 


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$weighted average of 1627.340 {I11} from {+100}Rh |e decay (20.8 h), 1627.462 {I22} from (|a,2n|g), 1627.35 {I4} from (n,|g) E=th, 1627.34 {I4} from (n,n'|g), and 1626.4 {I5} from Coulomb excitation 
RI$from {+100}Rh |e decay (20.8 h). Others: 100.0 {I15} from (|a,2n|g), 100.0 {I7} from (n,|g) E=th, and 100.0 {I10} from (n,n'|g) 
M$from ce data and |g|g(|q) in {+100}Rh |e decay (20.8 h). |d(M2/E1)=-0.008 {I24} in (n,n'|g), +0.02 {I3} in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E3)
decay_BE_unit: e^2 x (fm)^6
decay_BE_info: ;TYPE=BE3;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE3W
decay_comment:
E$weighted average of 2166.80 {I3} from {+100}Rh |e decay (20.8 h), 2166.65 {I16} from (|a,2n|g), 2166.94 {I7} from (n,|g) E=th, and 2166.61 {I21} from (n,n'|g) 
RI$unweighted average of 4.98 {I25} from {+100}Rh |e decay (20.8 h), 7.3 {I8} from (|a,2n|g), and 5.4 {I4} from (n,n'|g). Other: 10.9 {I13} from (n,|g) E=th, is in severe disagreement. 
M$(O) from |g(|q) in (n,n'|g); polarity from level-parity change 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from (n,|g) E=th. Other: 375.73 {I9} from (n,n'|g) 
RI$unweighted average of 4.6 {I3} from (n,|g) E=th and 1.6 {I3} 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_uncertain: ?
decay_comment:
$Placement is questioned (by evaluators) since with reported intensity of |?8% in {+100}Rh |e decay, this |g should have been seen in (n,|g) E=th 


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$weighted average of 1701.0 {I10} from {+100}Tc |b{+-} decay (15.46 s), 1701.310 {I18} from {+100}Rh |e decay (20.8 h), 1701.30 {I15} from (|a,2n|g), 1701.14 {I6} from (n,|g) E=th, and 1701.28 {I3} from (n,n'|g) 
RI$from (n,n'|g). Others: 100.0 {I16} from {+100}Rh |e decay (20.8 h), 100 {I12} from (n,|g) E=th 
M$D from |g(|q) in (|a,2n|g), |d(Q/D)=-0.014 {I50} from |g(|q) in (n,n'|g), |d(Q/D)=0.12 {I40} from |g|g(|q) in {+100}Rh |e decay (20.8 h); polarity from no level-parity change 


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$weighted average of 1124.84 {I3} from (|a,2n|g), 1124.768 {I5} from (n,|g) E=th, and 1124.77 {I3} from (n,n'|g) 
RI$from (n,n'|g). Others: 100 {I3} from (|a,2n|g), 100 {I5} from (n,|g) E=th, and 100 {I30} from (n,|g) E=res 
M,MR$D+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$weighted average of 1811.79 {I8} from (|a,2n|g), 1811.53 {I6} from (n,|g) E=th, and 1811.66 {I8} from (n,n'|g) 
RI$weighted average of 62 {I3} from (|a,2n|g), 52 {I6} from (n,|g) E=th, 81 {I25} from (n,|g) E=res, and 66.4 {I18} 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_comment:
E$weighted average of 1139.8 {I7} from (|a,2n|g), 1139.96 {I7} from (n,|g) E=th, and 1139.88 {I6} from (n,n'|g). level-energy difference=1140.12 
RI$unweighted average of 15.0 {I13} from {+100}Rh |e decay (4.6 min), 8 {I7} from (|a,2n|g), 14.4 {I18} from (n,|g) E=th, and 19.8 {I7} 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$weighted average of 1827.13 {I5} from (|a,2n|g), 1827.16 {I4} from (n,|g) E=th, and 1827.04 {I6} from (n,n'|g) 
RI$from (n,n'|g). Others: 100.0 {I25} from (|a,2n|g), 100 {I8} from {+100}Rh |e decay (4.6 min) and 100 {I8} from (n,|g) E=th 
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_comment:
E$unweighted average of 1024.9 {I1} from {+100}Tc |b{+-} decay (15.46 s), 1024.98 {I3} from {+100}Rh |e decay (20.8 h), 1025.62 {I9} from (n,|g) E=th, and 1025.00 {I5} from (n,n'|g) 
RI$from (n,n'|g). Other: 100 {I22} from (n,|g) E=th, 100 {I4} from {+100}Rh |e decay (20.8 h), 100 {I4} from {+100}Tc |b{+-} decay (15.46) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$weighted average of 1847.6 {I2} from {+100}Tc |b{+-} decay (15.46 s), 1847.57 {I8} from {+100}Rh |e decay (20.8 h), 1847.76 {I7} from (n,|g) E=th, and 1847.73 {I11} from (n,n'|g) 
RI$unweighted average of 76 {I9} from {+100}Tc |b{+-} decay (15.46 s), 102 {I8} from {+100}Rh |e decay (20.8 h), and 76.7 {I20} from (n,n'|g). Other: 200 {I22} in (n,|g) E=th is in disagreement 


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$unweighted average of 1051.51 {I6} from (|a,2n|g), 1051.57 {I7} from (n,|g) E=th, and 1051.96 {I7} from (n,n'|g) 
RI$unweighted average of 9.5 {I10} from (n,|g) E=th and 15.2 {I5} from (n,n'|g). Other: 312 {I19} from (|a,2n|g) is in severe disagreement 


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$unweighted average of 1874.70 {I23} from (|a,2n|g), 1874.15 {I5} from (n,|g) E=th, and 1874.29 {I6} from (n,n'|g) 
RI$from (n,n'|g). Others: 100 {I13} from (|a,2n|g), 100 {I15} from (n,|g) E=th 
M$(Q), |DJ=2 from |g(|q) in (n,n'|g); |DJ=0 is also possible; 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=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$weighted average of 302.507 {I6} from {+100}Rh |e decay (20.8 h) and 302.522 {I8} from (n,|g) E=th 
RI$from {+100}Rh |e decay (20.8 h). Other: 8.1 {I6} from (n,|g) E=th is in disagreement 
M,MR$from ce data in {+100}Rh |e decay (20.8 h) 


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$weighted average of 370.275 {I7} from {+100}Rh |e decay (20.8 h) and 370.283 {I5} from (n,|g) E=th 
RI$from {+100}Rh |e decay (20.8 h). Other: 10.4 {I11} from (n,|g) E=th is in disagreement 
M$from ce data in {+100}Rh |e decay (20.8 h) and RUL 


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$weighted average of 588.343 {I5} from {+100}Rh |e decay (20.8 h), 588.30 {I10} from (|a,2n|g), 588.47 {I8} from (n,|g) E=th, and 588.25 {I8} from (n,n'|g) 
RI$weighted average of 36.9 {I4} from {+100}Rh |e decay (20.8 h), and 36.6 {I9} from (n,n'|g). Others: 68 {I11} from (|a,2n|g), 71 {I9} from (n,|g) E=th are in disagreement 
M$from ce data and |g|g(|q) in {+100}Rh |e decay (20.8 h), |g(|q) in (n,n'|g), and RUL. |d(Q/D)=+0.14 {I16} from (n,n'|g) would give an unreasonably large B(M2)(W.u.) exceeding RUL 


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$weighted average of 1107.223 {I8} from {+100}Rh |e decay (20.8 h), 1107.10 {I12} from (|a,2n|g), 1107.07 {I6} from (n,|g) E=th, and 1107.29 {I5} from (n,n'|g) 
RI$from {+100}Rh |e decay (20.8 h). Others: 100.0 {I16} from (n,n'|g), 100 {I11} from (|a,2n|g) and 100 {I12} from (n,|g) E=th 
M$from ce data and |g|g(|q) in {+100}Rh |e decay (20.8 h), |g(|q) in (n,n'|g), and RUL. |d(Q/D)=-0.10 {I13} from (n,n'|g) would give an unreasonably large B(M2)(W.u.) exceeding RUL 


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$weighted average of 1929.811 {I20} from {+100}Rh |e decay (20.8 h), 1929.74 {I6} from (n,|g) E=th, and 1929.80 {I7} from (n,n'|g) 
RI$weighted average of 85.6 {I8} from {+100}Rh |e decay (20.8 h) and 84.1 {I16} from (n,n'|g). Other: 111 {I13} from (n,|g) E=th 
M$from ce data and |g|g(|q) in {+100}Rh |e decay (20.8 h), |g(|q) in (n,n'|g), and RUL. |d(Q/D)=-0.8 {I9} from (n,n'|g) would give an unreasonably large B(M2)(W.u.) exceeding RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 430.34 {I4} from (|a,2n|g), 430.61 {I7} from (n,|g) E=th, and 430.32 {I6} from (n,n'|g) 
RI$from (n,n'|g). Other: 100 {I13} in (n,|g) E=th is in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 612.03 {I6} from (n,|g) E=th, and 612.01 {I5} from (n,n'|g). Other: 612.055 {I18} from (|a,2n|g) for a doublet 
RI$from (n,n'|g). Others: 37 {I4} in (n,|g) E=th; doublet in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Placement is considered suspect, since with the reported intensity in (n,|g) E=th, it should have been seen in other studies 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$unweighted average of 1266.52 {I22} from (|a,2n|g), 1266.20 {I8} from (n,|g) E=th, and 1266.66 {I10} from (n,n'|g) 
RI$from (n,n'|g). Other: 100 {I13} from (n,|g) E=th 
M,MR$from |g(|q) 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$weighted average of 413.43 {I7} from (n,|g) E=th and 413.28 {I25} from (n,n'|g) 
RI$weighted average of 24 {I4} from (n,|g) E=th and 16.4 {I7} 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$weighted average of 631.35 {I3} from {+100}Rh |e decay (20.8 h), 631.41 {I5} from (|a,2n|g), 631.393 {I20} from (n,|g) E=th, and 631.38 {I3} from (n,n'|g) 
RI$from (n,n'|g). Others: 100 {I3} from {+100}Rh |e decay (20.8 h), 100 {I6} from (n,|g) E=th, and 100 {I14} from (|a,2n|g) 
M,MR$D+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$weighted average of 1150.6 {I3} from (n,|g) E=th and 1150.42 {I10} from (n,n'|g) 
RI$unweighted average of 5.8 {I12} from (n,|g) E=th and 13.4 {I11} 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$weighted average of 1972.91 {I6} from {+100}Rh |e decay (20.8 h), 1972.83 {I25} from (|a,2n|g), 1972.96 {I7} from (n,|g) E=th, and 1972.85 {I9} from (n,n'|g) 
RI$unweighted average of 63 {I4} from {+100}Rh |e decay (20.8 h), 41 {I10} from (|a,2n|g), 36 {I5} from (n,|g) E=th, and 54.3 {I13} from (n,n'|g) 
M$(Q), |DJ=(2) from |g(|q) in |g(|q) in (n,n'|g), |DJ=0 is also possible; M2 ruled out by RUL 


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$weighted average of 465.15 {I3} from {+100}Rh |e decay (20.8 h), 465.148 {I17} from (n,|g) E=th, and 465.11 {I15} from (n,n'|g) 
RI$unweighted average of 22.7 {I2} from {+100}Rh |e decay (20.8 h), 25.7 {I19} from (n,|g) E=th, 33 {I3} from (n,n'|g) is in disagreement 


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$weighted average of 651.707 {I6} from {+100}Rh |e decay (20.8 h), 651.88 {I7} from (n,|g) E=th, and 651.72 {I4} from (n,n'|g) 
RI$from {+100}Rh |e decay (20.8 h). Others: 100 {I3} from (n,n'|g), 100 {I14} from (n,|g) E=th 
M$from ce data in {+100}Rh |e decay (20.8 h) and RUL 


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$weighted average of 775.831 {I11} from {+100}Rh |e decay (20.8 h), 775.97 {I23} from (n,|g) E=th, and 775.95 {I13} from (n,n'|g) 
RI$unweighted average of 21.0 {I3} from {+100}Rh |e decay (20.8 h), 10 {I5} from (n,|g) E=th, and 29.0 {I19} 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=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$unweighted average of 1154.680 {I10} from {+100}Rh |e decay (20.8 h), 1154.21 {I13} from (n,|g) E=th, and 1154.60 {I8} from (n,n'|g) 
RI$weighted average of 52.4 {I5} from {+100}Rh |e decay (20.8 h), 52 {I10} from (n,|g) E=th, and 49 {I3} from (n,n'|g) 
M$D from |g|g(|q) in {+100}Rh |e decay (20.8 h); polarity from level-parity change 


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$weighted average of 1386.521 {I10} from {+100}Rh |e decay (20.8 h) and 1386.43 {I6} from (n,n'|g). Other: 1385.86 {I8} from (n,|g) E=th 
RI$unweighted average of 86.0 {I7} from {+100}Rh |e decay (20.8 h) and 100 {I3} from (n,n'|g), 48 {I5} from (n,|g) E=th 
M$D from |g|g(|q) in {+100}Rh |e decay (20.8 h); polarity from level-parity change 


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$unweighted average of 1977.24 {I4} from {+100}Rh |e decay (20.8 h), 1977.69 {I13} from (n,|g) E=th, and 1977.18 {I13} from (n,n'|g) 
RI$unweighted average of 57.5 {I11} from {+100}Rh |e decay (20.8 h), 33 {I5} from (n,|g) E=th, and 61.3 {I22} from (n,n'|g) 
M$|d(Q/D)=0.11 {I15} from |g|g(|q) in {+100}Rh |e decay (20.8 h); polarity from level-parity change 


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$weighted average of 360.331 {I23} from (|a,2n|g) and 360.373 {I5} from (n,|g) E=th 
RI$unweighted average of 5.43 {I9} from (|a,2n|g) and 6.6 {I4} from (n,|g) E=th 
M$Q from |g(|q) in (|a,2n|g); M2 ruled out by RUL 


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$weighted average of 1300.792 {I12} from (|a,2n|g), 1300.764 {I18} from (n,|g) E=th, and 1300.71 {I4} from (n,n'|g). Others: 1301.3 {I3} from ({+36}S,|a2n|g) and 1301.6 {I3} from (|a,4n|g) 
RI$from (|a,2n|g) 
M$|d(Q/D)=+0.004 {I6} from |g(|q) in (|a,2n|g), +0.05 {I7} from |g(|q) in (n,n'|g); |d(M2/E1)=-0.07 {I3} from |g(|q) and |g(lin pol) in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Placement is considered suspect (by evaluators) since with the reported intensity in (n,|g) E=th, it should have been seen in other studies 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 671.3 {I6} from {+100}Rh |e decay (20.8 h) and 671.2 {I3} from (n,|g) E=th 
RI$weighted average of 1.8 {I4} from {+100}Rh |e decay (20.8 h) and 2.2 {I11} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1309.8 {I3} from {+100}Rh |e decay (20.8 h), 1309.5 {I3} from (|a,2n|g), 1309.41 {I13} from (n,|g) E=th, and 1309.94 {I14} from (n,n'|g) 
RI$weighted average of 13.5 {I25} from {+100}Rh |e decay (20.8 h), 10.0 {I11} from (n,|g) E=th, and 11.7 {I6} from (n,n'|g). Other: 42 {I8} in (|a,2n|g) is in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$weighted average of 1996.59 {I3} from {+100}Rh |e decay (20.8 h), 1996.81 {I13} from (|a,2n|g), 1996.69 {I6} from (n,|g) E=th, and 1996.62 {I8} from (n,n'|g) 
RI$from (n,n'|g). Others: 100.0 {I16} from {+100}Rh |e decay (20.8 h), 100 {I8} from (|a,2n|g) and 100 {I12} from (n,|g) E=th 
M,MR$from |g(|q) in (n,n'|g). Other: |d=-0.2 {I3} from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 662.99 {I21} from {+100}Rh |e decay (20.8 h), 662.54 {I17} from (n,|g) E=th, and 662.56 {I25} from (n,n'|g) 
RI$weighted average of 12 {I3} from {+100}Rh |e decay (20.8 h), 6.6 {I3.4} from (n,|g) E=th, and 12.3 {I22} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 678.65 {I3} from {+100}Rh |e decay (20.8 h), 678.54 {I14} from (|a,2n|g), 678.60 {I7} from (n,|g) E=th, and 678.59 {I4} from (n,n'|g) 
RI$weighted average of 78 {I6} from {+100}Rh |e decay (20.8 h), 71 {I12} from (|a,2n|g), 55 {I7} from (n,|g) E=th, and 64.0 {I22} 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$unweighted average of 1181.49 {I5} from {+100}Rh |e decay (20.8 h), 1181.43 {I12} from (|a,2n|g), 1181.21 {I7} from (n,|g) E=th, and 1181.53 {I4} from (n,n'|g) 
RI$from (n,n'|g). Others: 100 {I6} from (|a,2n|g), 100 {I14} from (n,|g) E=th, 100 {I5} from {+100}Rh |e decay (20.8 h) 
M$D+Q from |g(|q) in (n,n'|g); M2 ruled out by RUL 
MR$from |g(|q) in (n,n'|g), with +3.5 {I12} is possible 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2004.30 {I13} from {+100}Rh |e decay (20.8 h), 2004.01 {I13} from (|a,2n|g), 2004.44 {I7} from (n,|g) E=th, and 2004.20 {I12} from (n,n'|g) 
RI$unweighted average of 53 {I4} from {+100}Rh |e decay (20.8 h) and 42.6 {I17} from (n,n'|g). Others: 147 {I12} in (|a,2n|g) and 179 {I23} in (n,|g) E=th are in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2543.60 {I9} from {+100}Rh |e decay (20.8 h), 2543.5 {I3} from (n,|g) E=th, and 2543.4 {I3} from (n,n'|g) 
RI$weighted average of 49.4 {I24} from {+100}Rh |e decay (20.8 h), 36 {I7} from (n,|g) E=th, and 27.3 {I17} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 403.07 {I11} from {+100}Rh |e decay (20.8 h), 403.092 {I15} from (|a,2n|g), 403.013 {I10} from (n,|g) E=th, and 403.14 {I4} from (n,n'|g) 
RI$from (n,n'|g). Others: 100 {I5} from (n,|g) E=th, 100 {I20} from {+100}Rh |e decay (20.8 h), 100 {I13} from (n,n|g) E=res 
M$D+Q from |g(|q) in (|a,2n|g) and (n,n'|g); polarity from no level-parity change 
MR$from (|a,2n|g). Other: +0.08 {I8} or +1.36 {I20} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 470.98 {I17} from {+100}Rh |e decay (20.8 h) and 470.82 {I3} from (n,|g) E=th 
RI$weighted average of 3.7 {I8} from {+100}Rh |e decay (20.8 h) and 3.1 {I4} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 689.3 {I5} from (|a,2n|g) and 688.89 {I3} from (n,|g) E=th 
RI$from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 1207.50 {I3} from {+100}Rh |e decay (20.8 h), 1207.70 {I5} from (|a,2n|g), 1207.74 {I7} from (n,|g) E=th, and 1207.78 {I6} from (n,n'|g) 
RI$unweighted average of 52 {I7} from {+100}Rh |e decay (20.8 h), 31 {I4} from (n,|g) E=th, 90 {I30} from (n,|g) E=res, and 70.4 {I21} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1343.44 {I5} from {+100}Rh |e decay (20.8 h), 1343.49 {I3} from (n,|g) E=th, and 1343.39 {I10} from (n,n'|g) 
RI$weighted average of 60 {I12} from {+100}Rh |e decay (20.8 h), 58 {I4} from (n,|g) E=th, and 51 {I6} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2030.56 {I20} from {+100}Rh |e decay (20.8 h), 2030.54 {I8} from (n,|g) E=th, and 2030.7 {I3} from (n,n'|g) 
RI$unweighted average of 11 {I3} from {+100}Rh |e decay (20.8 h), 8.0 {I11} from (n,|g) E=th, and 12.9 {I14} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$from (n,|g) E=th. Other: 695.8 {I3} from (|a,2n|g) 
RI$unweighted average of 63 {I3} from (|a,2n|g) and 80 {I6} from (n,|g) E=th 
M$Q from |g(|q) in (n,|g) E=th, mostly likely E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1350.40 {I3} from (|a,2n|g), 1350.450 {I20} from (n,|g) E=th, and 1350.37 {I7} from (n,n'|g) 
RI$from (|a,2n|g). Other: 100 {I5} from (n,|g) E=th 
M,MR$|d(Q/D)=-3.4 {I2} or -0.12 {I4} from |g(|q) 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$from (n,|g) E=th. Others: 424.83 {I21} from (|a,2n|g), and 424.88 {I17} from (n,n'|g) 
RI$weighted average of 61 {I14} from (|a,2n|g), 54 {I6} from (n,|g) E=th, 85 {I23} from (n,|g) E=res, and 41.7 {I14} from (n,n'|g) 
M,MR$(D+Q) from |g(|q) in (|a,2n|g); M2 ruled out by RUL 


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$from (n,|g) E=th. Others: 710.82 {I5} from (|a,2n|g), and 710.80 {I3} from (n,n'|g) 
RI$from (n,n'|g). Others: 100 {I5} from (|a,2n|g), 100 {I6} from (n,|g) E=th, 100 {I12} from (n,|g) E=res 
M$D(+Q) from |g(|q) in (n,n'|g) and (|a,2n|g); polarity from level scheme 
MR$weighted average of +0.02 {I5} from (n,n'|g) and +0.05 {I8} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_uncertain: ?
decay_comment:
$this |g is considered questionable by evaluators due to unreasonably large B(M2)(W.u.) of 26 {I+25-15} 


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:
$Unusually large B(E1)(W.u.) casts some doubt on the level half-life 
E$weighted average of 1365.40 {I3} from (|a,2n|g) and 1365.416 {I12} from (n,|g) E=th. Other: 1365.49 {I9} from (n,n'|g). 
RI$unweighted average of 73.9 {I19} from (|a,2n|g), 71 {I4} from (n,|g) E=th, 96 {I8} from (n,|g) E=res, and 85.0 {I23} from (n,n'|g) 
M$D(+Q) from |g(|q) in (|a,2n|g); polarity from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M4]
decay_uncertain: ?
decay_comment:
$Placement suspect as |DJ=4 is involved 
$this |g is considered questionable by evaluators due to unreasonably large B(M4)(W.u.) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2617.07 {I4} from {+100}Rh |e decay (20.8 h), 2617.32 {I12} from (n,|g) E=th, and 2617.09 {I9} from (n,n'|g) 
RI$from {+100}Rh |e decay (20.8 h). Other: 100 {I9} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2120.61 {I7} from {+100}Rh |e decay (20.8 h), 2120.55 {I11} from (n,|g) E=th, and 2120.57 {I11} from (n,n'|g). Other: 2121.2 {I7} from {+100}Tc |b{+-} decay (15.46 s) 
RI$from (n,n'|g). Others: 100 {I20} from {+100}Tc |b{+-} decay (15.46 s), 100 {I9} from {+100}Rh |e decay (20.8 h), 100 {I10} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2660.09 {I12} from {+100}Rh |e decay (20.8 h), 2660.0 {I4} from (n,|g) E=th, and 2660.22 {I20} from (n,n'|g). Other: 2659.5 {I10} from {+100}Tc |b{+-} decay (15.46 s) 
RI$weighted average of 40 {I20} from {+100}Tc |b{+-} decay (15.46 s), 20 {I3} from {+100}Rh |e decay (20.8 h), 23 {I7} from (n,|g) E=th, and 21.7 {I11} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 598.19 {I6} from (n,|g) E=th and 598.11 {I17} from (|a,2n|g) 
RI$from (|a,2n|g), <310 from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$from (|a,2n|g). Other: 778.980 {I14} from (n,|g) E=th differs greatly with level-energy difference 
RI$from (n,|g) E=th. Other: 100 {I6} from (|a,2n|g) 
M$from |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 1434.21 {I7} from (n,|g) E=th and 1434.81 {I20} from (|a,2n|g) 
RI$weighted average of 116 {I15} from (n,|g) E=th and 78 {I22} from (|a,2n|g) 
M,MR$D+Q from |g(|q) in (|a,2n|g), most likely M1+E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$poor fit, level-energy difference=1535.82 
$Placement is considered suspect (by evaluators) since with the reported intensity in (n,|g) E=th, it should have been seen in other studies 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2126.92 {I14} from {+100}Rh |e decay (20.8 h), 2126.91 {I6} from (n,|g) E=th, and 2126.68 {I11} from (n,n'|g) 
RI$from (n,|g) E=th. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1615.29 {I5} from {+100}Rh |e decay (20.8 h) and 1615.4 {I9} from (n,n'|g) 
RI$from (n,n'|g). Other: 100 {I5} from {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2205.96 {I14} from {+100}Rh |e decay (20.8 h) and 2205.93 {I19} from (n,n'|g) 
RI$weighted average of 35 {I6} from {+100}Rh |e decay (20.8 h) and 40.8 {I14} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$from (n,|g) E=th. Other: 580.52 {I12} from (|a,2n|g) 
RI$unweighted average of 27.5 {I25} from (|a,2n|g) and 60 {I4} from (n,|g) E=th 
M,MR$D+Q from |g(|q) in (|a,2n|g), most likely M1+E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from (n,|g) E=th. Other: 866.29 {I21} from (|a,2n|g) 
RI$weighted average of 38 {I8} from (|a,2n|g) and 39.5 {I18} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
E$weighted average of 1520.83 {I12} from (|a,2n|g) and 1520.64 {I7} from (n,|g) E=th. 
RI$from (|a,2n|g). Other: 100 {I13} from (n,|g) E=th 
M,MR$from |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1538.38 {I8} from (n,n'|g) and 1538.29 {I7} from (n,|g) E=th 
RI$from (n,n'|g). Other: 100 {I13} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$from (|a,2n|g). Other: 248.11 {I7} from (n,n'|g) 
M,MR$|DJ=0, (D+Q) from |g(|q) in (|a,2n|g), with |DJ=2 also possible; most likely (M1+E2) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 2262.1 {I5} from {+100}Rh |e decay (20.8 h), 2262.32 {I7} from (n,|g) E=th, and 2261.88 {I18} from (n,n'|g) 
RI$from (n,n'|g). Others: 100 {I25} from {+100}Rh |e decay (20.8 h) 
MR$|d(Q/D)=+0.42 {I15} or +3.9 {I8} from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 2298.4 {I4} from {+100}Tc |b{+-} decay (15.46 s) and 2298.17 {I20} from (n,n'|g) 
RI$from (n,n'|g) 
MR$|d(Q/D)=+3.0 {I5} or -0.07 {I4} from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 1515.54 {I12} from (|a,2n|g) and 1515.10 {I19} from (n,n'|g) 
RI$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_uncertain: ?
decay_comment:
$This |g is considered questionable by evaluators due to unreasonably large B(M2)(W.u.)=4.0|*10{+2} {I+38-26} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$from (|a,2n|g). Others: 423.8 {I5} from ({+36}S,|a2n|g), and 424.3 {I3} from (|a,4n|g) 
RI$weighted average of 17 {I4} from ({+36}S,|a2n|g), 13.5 {I19} from (|a,2n|g), and 17.4 {I9} from (|a,4n|g) 
M$Q from |g(DCO) in ({+36}S,|a2n|g), |g(|q) in (|a,2n|g) and (|a,4n|g); ce data in (|a,4n|g) indicates (E2) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$unweighted average of 876.2 {I1} from ({+36}S,|a2n|g), 875.878 {I12} from (|a,2n|g), and 876.7 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Others: 100 {I4} from ({+36}S,|a2n|g), 100 {I9} from (|a,4n|g) 
M$from |g(|q) in (|a,2n|g), |g(DCO) and |g(pol) in ({+36}S,|a2n|g), and |g(|q,pol) and ce data in (|a,4n|g). |d(M2/E1)=-0.02 {I3} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$Q from |g(|q) in (|a,2n|g); M2 ruled out since it would require an isomeric half-life by RUL, which is unlikely. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E,RI$from (|a,2n|g). Others: E|g=436.5 {I5} and I|g=50 {I25} from ({+36}S,|a2n|g), E|g=436.4 {I3} and I|g=39.0 {I25} from (|a,4n|g) 
M,MR$from |g(|q) and ce data in (|a,4n|g). Other: |d(Q/D)=+0.69 {I25} from |g(|q) in (|a,2n|g) for a doublet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
E$unweighted average of 888.5 {I5} from ({+36}S,|a2n|g), 887.981 {I17} from (|a,2n|g), and 888.8 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Others: 100 {I5} from (|a,4n|g), 100 {I25} from ({+36}S,|a2n|g) 
M,MR$|DJ=0, |d(Q/D)=-0.08 {I10} from |g(|q) in (|a,2n|g); E1(+M2) from |g(|q,pol) and ce data in (|a,4n|g), with |d(M2/E1)=+0.4 {I7}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 984.8 {I1} from ({+36}S,|a2n|g), 984.439 {I12} from (|a,2n|g), and 985.2 {I3} from (|a,4n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a2n|g), |g(|q) and ce data in (|a,4n|g), |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3060.25 {I11} from {+100}Rh |e decay (20.8 h) and 3059.97 {I24} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E,RI$from {+100}Rh |e decay (20.8 h). Other: E|g=2530.06 {I18}, I|g=100 from (n,n'|g) 
M$from |g|g(|q) in {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_comment:
E,RI$from {+100}Rh |e decay (20.8 h). Other: a questionable strong 3070.2|g reported in (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1710.07 {I3} from {+100}Rh |e decay (20.8 h) and 1710.00 {I12} from (n,n'|g) 
RI$from {+100}Rh |e decay (20.8 h). Other: 100 {I4} 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$weighted average of 3071.80 {I12} from {+100}Rh |e decay (20.8 h) and 3071.86 {I24} from (n,n'|g) 
RI${+100}Rh |e decay (20.8 h). Other: 106 {I4} from (n,n'|g) is in disagreement 
E$level-energy difference=3072.20 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
E$weighted average of 187.5 {I5} from ({+36}S,|a2n|g), 187.760 {I13} from (|a,2n|g), and 187.4 {I3} from (|a,4n|g) 
RI$weighted average of 76 {I26} from ({+36}S,|a2n|g), 56.1 {I21} from (|a,2n|g), and 43 {I5} from (|a,4n|g) 
M,MR$from |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 612.4 {I5} from ({+36}S,|a2n|g), 612.055 {I18} from (|a,2n|g), and 612.4 {I3} from (|a,4n|g) 
RI$from (|a,2n|g) for a doublet, but most intensity belongs with 3140 level. Others: 100 {I10} from (|a,4n|g), 100 {I26} from ({+36}S,|a2n|g) 
M$from |g(|q) in (|a,2n|g), |g(|q) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$unweighted average of 1063.3 {I5} from ({+36}S,|a2n|g), 1063.67 {I3} from (|a,2n|g), and 1064.5 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Others: <81 from (|a,4n|g); 200 {I50} from ({+36}S,|a2n|g) is in disagreement 
M,MR$from |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from (|a,2n|g) only 
M$Q from |g(|q) in (|a,2n|g); M2 ruled out since it would require an isomeric half-life (>0.45 |ms) by RUL, which is unlikely 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 202.6 {I5} from ({+36}S,|a2n|g), 203.590 {I14} from (|a,2n|g), and 204.0 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Other: 100 {I15} from (|a,4n|g) 
M$|d(Q/D)=+0.18 {I20} from |g(|q) in (|a,2n|g); |DJ=0, D from |g(DCO) in ({+36}S,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1188.012 {I20} from (|a,2n|g) and 1188.1 {I10} from (|a,4n|g) 
RI$from (|a,2n|g). Other: 100 {I15} from (|a,4n|g) 
M$from |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M,MR$|d(Q/D)=0.61 {I+18-3} for J=2, and 5.1 {I+120-25} or -0.05 {I20} for J=1 from |g|g(|q) in {+100}Rh |e decay (20.8 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from (|a,2n|g). Others: 390.9 {I5} from ({+36}S,|a2n|g) and 391.0 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Others: 100 {I6} from (|a,4n|g), 100 {I17} from ({+36}S,|a2n|g) 
M$from |g(|q,pol) and ce data in (|a,4n|g), |g(DCO) in ({+36}S,|a2n|g), and |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
E$from (|a,2n|g). Others: 403.7 {I5} from ({+36}S,|a2n|g) and 403.2 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Others: 67 {I17} from ({+36}S,|a2n|g), 55 {I3} from (|a,4n|g) 
M$from |g(|q,pol) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$from (|a,2n|g). Others: 148.1 {I5} from ({+36}S,|a2n|g) and 148.6 {I3} from (|a,4n|g) 
RI$weighted average of 17 {I8} from ({+36}S,|a2n|g), 24.7 {I11} from (|a,2n|g), and 25.8 {I16} from (|a,4n|g) 
M,MR$D+Q from |g(|q) in (|a,2n|g); polarity from no level-parity change. Other: |d(Q/D)=-1.5 {I15} from |g(|q) in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from (|a,2n|g). Others: 363.7 {I5} from ({+36}S,|a2n|g) and 364.2 {I3} from (|a,4n|g) 
RI$weighted average of 42 {I8} from ({+36}S,|a2n|g), 55.5 {I7} from (|a,2n|g), and 60 {I3} from (|a,4n|g) 
M$from |g(|q,pol) and ce data in (|a,4n|g), |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
E$from (|a,2n|g). Others: 442.8 {I5} from ({+36}S,|a2n|g) and 443.3 {I3} from (|a,4n|g) 
RI$weighted average of 67 {I17} from ({+36}S,|a2n|g), 76.0 {I11} from (|a,2n|g), and 73 {I5} from (|a,4n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a2n|g), |g(|q,pol) and ce data (|a,4n|g), |g(|q) in (|a,2n|g). 
MR$from (|a,2n|g). Other: -0.11 {I5} from (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 552.3 {I3} from ({+36}S,|a2n|g), 551.881 {I14} from (|a,2n|g), and 552.2 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Others: 100 {I7} from (|a,4n|g), 100 {I8} from ({+36}S,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from (|a,2n|g). Others: 623.8 {I3} from ({+36}S,|a2n|g) and 624.2 {I3} from (|a,4n|g) 
RI$from (|a,2n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a2n|g), |g(|q,pol) and ce data (|a,4n|g), |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
E$weighted average of 489.0 {I5} from ({+36}S,|a2n|g), 488.671 {I20} from (|a,2n|g), and 489.3 {I3} from (|a,4n|g) 
RI$weighted average of 67 {I17} from ({+36}S,|a2n|g), 54.3 {I7} from (|a,2n|g), and 46 {I8} from (|a,4n|g) 
M$from |g(|q,pol) and ce data in (|a,4n|g), |g(|q) in (|a,2n|g). 
MR$from (|a,2n|g). Other: +4 {I2} from (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 637.8 {I5} from ({+36}S,|a2n|g), 637.44 {I7} from (|a,2n|g), and 637.7 {I2} from (|a,4n|g) 
RI$from (|a,4n|g). Others: 100 {I11} from (|a,2n|g), 100 {I17} from ({+36}S,|a2n|g) 
M$from |g(|q,pol) and ce data in (|a,4n|g), |g(|q) in (|a,2n|g), |g(DCO) in ({+36}S,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 821.4 {I10} from ({+36}S,|a2n|g) and 819.62 {I7} from (|a,2n|g) 
RI$weighted average of 3.7 {I19} from ({+36}S,|a2n|g) and 7.1 {I5} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 1024.0 {I1} from ({+36}S,|a2n|g), 1023.252 {I15} from (|a,2n|g), and 1024.0 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Other: 100 {I8} from ({+36}S,|a2n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a2n|g), |g(|q,pol) and ce data in (|a,4n|g), |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$from (|a,2n|g). Others: 238.5 {I10} from ({+36}S,|a2n|g) and 238.2 {I3} from (|a,4n|g) 
RI$from (|a,2n|g), but 6.7 {I33} in ({+36}S,|a2n|g) is in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 727.8 {I3} from ({+36}S,|a2n|g), 727.340 {I20} from (|a,2n|g), and 727.7 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Other: 100 {I6} from (|a,4n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a2n|g), |g(|q) and ce data in (|a,4n|g), |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$weighted average of 973.6 {I10} from ({+36}S,|a2n|g), and 973.13 {I6} from (|a,2n|g) 
RI$from (|a,2n|g), but 8 {I4} in ({+36}S,|a2n|g) is in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$from (|a,2n|g). Other: 1177.9 {I3} in ({+36}S,|a2n|g) is discrepant 
RI$from (|a,2n|g). Other: 100 {I8} from ({+36}S,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from (|a,2n|g). Others: 740.3 {I5} from ({+36}S,|a2n|g) and 740.6 {I3} from (|a,4n|g) 
RI$from (|a,2n|g) 
M$from |g(|q,pol) in (|a,4n|g), |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 564.9 {I5} from ({+36}S,|a2n|g) and 564.51 {I15} from (|a,2n|g) 
RI$weighted average of 25 {I4} from ({+36}S,|a2n|g) and 24 {I4} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 835.2 {I1} from ({+36}S,|a2n|g), 834.45 {I8} from (|a,2n|g), and 835.2 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Other: 100 {I7} from ({+36}S,|a2n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a2n|g), |g(|q) and ce data in (|a,4n|g), |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 847.5 {I5} from ({+36}S,|a2n|g) and 846.71 {I9} from (|a,2n|g) 
RI$from (|a,2n|g), but 33 {I8} in ({+36}S,|a2n|g) is in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 932.7 {I3} from ({+36}S,|a2n|g), 931.72 {I3} from (|a,2n|g), and 932.4 {I3} from (|a,4n|g) 
RI$from (|a,2n|g). Other: 100 {I8} from ({+36}S,|a2n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a2n|g), |g(|q) and ce data in (|a,4n|g), |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 959.6 {I5} from ({+36}S,|a2n|g) and 959.03 {I12}. Other: 962.1 {I3} in (|a,4n|g) seems discrepant 
RI$from (|a,2n|g) 
M$(Q) from |g(|q) in (|a,2n|g); (E2,M1) from |g(|q) and ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 795.5 {I1} from ({+36}S,|a2n|g), 795.30 {I5} from (|a,2n|g), and 795.5 {I3} from (|a,4n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a2n|g), |g(|q) and ce data in (|a,4n|g), |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from ({+36}S,|a2n|g) 
M$from |g(DCO) and |g(pol) in ({+36}S,|a2n|g), |g(DCO) in ({+34}S,2|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1036.6 {I3} from ({+36}S,|a2n|g), and 1036.3 {I3} from (|a,4n|g) 
M$Q from |g(DCO) in ({+36}S,|a2n|g) and |g(|q) in (|a,4n|g), polarity from ce data in (|a,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$from ({+36}S,|a2n|g) 
M$Q from |g(DCO) in ({+36}S,|a2n|g) and ({+34}S,2|a2n|g); E2 indicated by |g(pol) in ({+36}S,|a2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
MR$+5.5 {I5} or +0.35 {I2} 
$2000Ge01 misplace |d value at 1325.56|g in Table 1, and it should be for 1341.6|g, as quoted in 2001Ge03 of the same author in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$a part of this |g ray may be from 2414 level, as in the Adopted Gammas (placement proposed by evaluators) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from the Adopted Gammas, only a small fraction (|?0.1 units) is expected with placement from 2493 level, main placement (|?2.3 units) should be from 3139 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$from the Adopted Gammas, it is estimated that most of the intensity of this |g is from 2570 level, only a minor component is from 3355 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$-3.4 {I2} or -0.12 {I4} 
$2000Ge01 probably misplace |d value at 1344.3|g in Table 1, since there is no |g(|q) measured for 1344.3|g and it is unplaced. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$This |g is possibly also from a low-spin level near this energy. See comment for 2775 doublet in the Adopted Levels 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Placement of this |g to 2+ state is considered questionable by the evaluators, since with the reported intensity in (n,|g) E=th, it should have been seen in other studies 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Placement is considered suspect (by evaluators) since with the reported intensity in (n,|g) E=th, it should have been seen in other studies 
E$level-energy difference=1535.63 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6340.59 {I4} (1991Is05), 6340.45 {I11} (1988CoZU) 
$I|g=1.07 {I16} (1988CoZU), 1.119 {I15} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6346.95 {I5} (1991Is05), 6346.55 {I13} (1988CoZU) 
$I|g=0.34 {I5} (1988CoZU), 0.673 {I12} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6372.55 {I2} (1991Is05), 6372.36 {I13} (1988CoZU) 
$I|g=0.31 {I5} (1988CoZU), 0.305 {I15} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6656.53 {I7} (1991Is05), 6655.8 {I3} (1988CoZU) 
$I|g=0.15 {I3} (1988CoZU), 0.104 {I15} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$level-energy difference=6689.79 
$E|g=6690.15 {I2} (1991Is05), 6689.80 {I15} (1988CoZU) 
$I|g=0.56 {I9} (1988CoZU), 0.587 {I7} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6757.73 {I10} (1991Is05), 6757.59 {I18} (1988CoZU) 
$I|g=0.078 {I12} (1988CoZU), 0.101 {I3} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6795.71 {I4} (1991Is05), 6795.53 {I13} (1988CoZU) 
$I|g=0.22 {I3} (1988CoZU), 0.221 {I4} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6835.37 {I7} (1991Is05), 6835.4 {I3} (1988CoZU) 
$I|g=0.066 {I11} (1988CoZU), 0.130 {I6} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6872.08 {I10} (1991Is05), 6871.67 {I24} (1988CoZU) 
$I|g=0.066 {I11} (1988CoZU), 0.062 {I11} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6908.54 {I5} (1991Is05), 6908.27 {I23} (1988Co18) 
$I|g=0.100 {I17} (1988Co18), 0.130 {I8} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=6925.92 {I7} (1991Is05), 6925.79 {I22} (1988Co18) 
$I|g=0.066 {I11} (1988Co18), 0.079 {I9} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7006.83 {I4} (1991Is05), 7006.73 {I18} (1988Co18) 
$I|g=0.23 {I4} (1988Co18), 0.188 {I5} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$ THIS G MOST LIKLEY FEEDS THE LOW-SPIN (1,2+) LEVEL OF THE DOUBLET AT 2660, BUT FEEDING TO THE (5+) LEVEL CAN NOT BE DISCOUNTED 
$E|g=7012.9 {I3}, I|g=0.025 {I2} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7081.35 {I5} (1991Is05), 7081.14 {I16} (1988Co18) 
$I|g=0.098 {I15} (1988Co18), 0.117 {I3} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7103.26 {I23} (1991Is05), 7102.90 {I13} (1988Co18) 
$I|g=1.00 {I15} (1988Co18), 0.983 {I11} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7129.67 {I12} (1991Is05), 7129.0 {I3} (1988Co18) 
$I|g=0.049 {I9} (1988Co18), 0.056 {I7} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7137.04 {I14} (1991Is05), 7136.6 {I6} (1988Co18) 
$I|g=0.025 {I6} (1988Co18), 0.032 {I6} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7160.29 {I8} (1991Is05), 7160.30 {I21} (1988Co18) 
$I|g=0.079 {I13} (1988Co18), 0.078 {I3} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7181.01 {I7} (1991Is05), 7179.75 {I15} (1988Co18) 
$I|g=0.17 {I3} (1988Co18), 0.232 {I5} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7203.77 {I4} (1991Is05), 7203.42 {I15} (1988Co18) 
$I|g=0.18 {I3} (1988Co18), 0.239 {I6} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7261.57 {I19}, I|g=0.12 {I3} (1991Is05). Note large energy difference of 2 keV between 2000Ge01 and 1991Is05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7306.48 {I4} (1991Is05), 7306.19 {I17} (1988Co18) 
$I|g=0.18 {I3} (1988Co18), 0.171 {I5} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7506.22 {I2} (1991Is05), 7505.90 {I13} (1988Co18) 
$I|g=0.63 {I10} (1988Co18), 0.610 {I7} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7573.94 {I5} (1991Is05), 7574.06 {I19} (1988Co18) 
$I|g=0.078 {I12} (1988Co18), 0.069 {I4} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7610.43 {I2} (1991Is05), 7610.17 {I14} (1988Co18) 
$I|g=0.49 {I7} (1988Co18), 0.453 {I6} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=7808.03 {I8} (1991Is05), 7807.6 {I4} (1988Co18) 
$I|g=0.16 {I3} (1988Co18), 0.092 {I3} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=8310.96 {I2} (1991Is05), 8310.63 {I16} (1988Co18) 
$I|g=0.22 {I3} (1988Co18), 0.270 {I3} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=8446.56 {I2} (1991Is05), 8446.23 {I21} (1988Co18) 
$I|g=0.19 {I3} (1988Co18), 0.199 {I3} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=9133.39 {I4} (1991Is05), 9133.3 {I4} (1988Co18) 
$I|g=0.17 {I3} (1988Co18), 0.169 {I3} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$Pol=+0.38 {I8} 
MR$1976De33 give -1.7 {I18} which is not consistent with A{-2} and A{-4} values for 876.7|g. The value should probably be -0.17 {I18}, consistent with |d|?0 in figure 4 (1976De33) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$this |g ray is most likely the same as 1036.6|g in 2000Ti07 from 7207, (17-) level in ({+34}S,|a2n|g) reaction 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$This |g is most likely from a high-spin (5-) level near this energy. See comment for 2775 doublet in the Adopted Levels 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$5.50 {I2} per 100 decays of {+100}Tc from |b|g coin (2005Fu18,2001Fu21), 5.2 {I5} (2017Gu17) 
RI$from unweighted average of I|g(591|g)/I|g(539|g)=1.232 {I8}/1.550 {I10}= 0.795 {I7} (2004Fu30) and I|g(591|g)/I|g(539|g)=5.50 {I2}/6.60 {I3}=0.833 {I5} (2005Fu18,2001Fu21). Others: 84.7 {I21} (2001Fu21) and 82 {I6} (1969Be69) are in agreement with this value. 
$(591|g)(540|g)(|q): A{-2}=+0.36 {I5}, A{-4}=+1.13 {I9} (1969Be69) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$The ce(L) intensity is probably incorrect. K/L(theory)=8.2. |g|g(|q) in 1990KeZV also supports E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$ce data give mult=M1,E2; |g|g(|q) support E2 
$(591|g)(540|g)(|q): A{-2}=+0.33 {I8}, A{-4}=+1.06 {I24} (1991Pr08); A{-2}=+0.40 {I7}, A{-4}=+1.00 {I13} (1990KeZV) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$ce data from 1964Ko04 gives mult=M1,E2; (687|g)(540|g)(|q): A{-2}=+0.081 {I75}, A{-4}=-0.07 {I12} (1990KeZV) favors E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
M$|a(K)exp=0.00123 {I5} from 1996Gi04 gives |d(E2/M1)=3.3 +|@-29. Other ce data: 1953Ma64. The ce(L) intensity is probably incorrect in 1964Ko04 
MR$from (822|g)(540|g)(|q): A{-2}=-0.215 {I8}, A{-4}=+0.312 {I2} (1991Pr08). |d=+3.2 {I8} from A{-2}=-0.25 {I3}, A{-4}=+0.32 {I4} (1978Ba29); 3.7 {I4} from A{-2}=-0.230 {I7}, A{-4}=+0.362 {I12} (1990KeZV). Others: 1996Gi04, 1968Ka04, 1964Ko04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$378.93 {I4} (1974Ko23) 
M$|a(K)exp in 1974Ko23 gives mult=M1,E2, but |DJ|p requires E2; (378|g)(1362|g)(|q): A{-2}=-0.1 {I5}, A{-4}=+0.4 {I9} (1990KeZV) supports E2 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
TI$from ce(K)(611|g)/ce(K)(540|g)=0.00020 {I10} (1974Ko23). Uncertainty of 0.00001 quoted by 1974Ko23 is probably underestimated since the peak is very weak in the ce spectrum shown by 1974Ko23. I|g<0.03 (1974Ko23) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M$|a(K)exp in 1996Gi04 gives mult=M1,E2 
$I|g(503|g)/I|g(735|g)=0.30 {I4} (1996Gi04) 
$EG=503.1 (1996Gi04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|a(K)exp from 1996Gi04 gives M1,E2; but only E2 is consistent with transition to 4+ 
$I|g(639|g)/I|g(735|g)=0.18 {I2} (1996Gi04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$I|g(1326|g)/I|g(735|g)=1.301 {I12} (1995KeZZ), 1.46 {I6} (1996Gi04), 0.91 {I11} in (n,|g) E=th 
MR$-1.6 {I+14-7} from (1326|g)(540|g)(|q): A{-2}=+0.42 {I17}, A{-4}=+0.24 {I29} in 1990KeZV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$I|g(1865|g)/I|g(735|g)=1.8 {I3} (1996Gi04) is too high by a factor of |?2 as compared to the values available from other studies. This may be due to summing contributions 
RI$0.50 {I13} (1969Be69) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp from 1996Gi04 gives |d(E2/M1)=2.4 +|@-17 
$(519|g)(1362|g)(|q): A{-2}=+0.15 {I7}, A{-4}=+0.10 {I11} (1978Ba29); A{-2}=-0.04 {I8}, A{-4}=+0.01 {I13} (1990KeZV) gives |d(Q/D)=0.03 {I9} or 4.3 {I+29-13} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp=0.000413 {I13} from 1996Gi04 gives |d(E2/M1)=4.4 {I+|@-31}. Other ce data: 1953Ma64. 
$(1342|g)(540|g)(|q): A{-2}=+0.20 {I8}, A{-4}=+0.05 {I8} (1978Ba29); A{-2}=-0.089 {I20}, A{-4}=-0.07 {I3} (1990KeZV) gives |d(Q/D)=6.8 {I+13-10}. Others: 1968Ka04, 1964Ko04. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$689.419 quoted by 1995KeZZ is probably a misprint. E|g deduced from a least-squares procedure is 689.500 {I13} (table 6.4 in 1995KeZZ) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_uncertain: ?
decay_comment:
RI$0.10 {I2} (1978Ba29) is in severe disagreement 
$I|g(234|g)/I|g(1559|g)<0.002 (1996Gi04) 
$Placement is from 1978Ba29. E|g agrees with the level-energy difference 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$|a(K)exp from 1996Gi04 is higher by |?5% than for pure M1 
$|d(E2/M1)=-0.72 {I+25-32} from (1559|g)(540|g)(|q): A{-2}=+0.62 {I8}, A{-4}=+0.13 {I13} (1990KeZV). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$|a(K)exp from 1996Gi04 gives |d(M2/E1)=0.06 {I+19-6} 
$|d(M2/E1)=0.09 {I6} from (1627|g)(540|g)(|q): A{-2}=+0.016 {I49}, A{-4}=-0.076 {I83} (1990KeZV). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
MR$0.12 {I40} from (1701|g)(540|g)(|q): A{-2}=+0.41 {I19}, A{-4}=-0.71 {I31} for J=2 (1990KeZV). But 1990KeZV adopt |d=-6.3 {I+39-|@} for J=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp from 1996Gi04 gives |d(E2/M1)=1.8 {I+12-5} 
$A{-2}=-0.25 {I10}, A{-4}=-0.10 {I16} for (302|g)(1627|g)(540|g)(|q) and A{-2}=+0.11 {I10}, A{-4}=+0.21 {I19} for (302|g)(1627|g)(|q) (1990KeZV) gives |d(Q/D)=2.7 {I9} or 0.16 {I10} for J(2469)=2 and J(2167)=3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp=0.0039 {I9} from 1996Gi04 gives |d(M2/E1)=0.16 {I+8-16}; |a(K)exp=0.013 {I8} from 1964Ko04 is consistent with mult=D,E2. Other ce data: 1953Ma64 
$(370|g)(1560|g)(|q): A{-2}=+0.12 {I8}, A{-4}=-0.11 {I12} (1990KeZV) gives |d(Q/D)=-1.3 {I13} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$from 1974Ko23. 1969Be69 give I|g=5.3 {I3} 
M$|a(K)exp=0.00104 {I5} from 1996Gi04 gives |d(M2/E1)=0.06 {I6}. Other ce data: 1964Ko04. 
$(588|g)(1342|g)(|q): A{-2}=-0.15 {I8}, A{-4}=+0.07 {I9} (1978Ba29); A{-2}=-0.12 {I3}, A{-4}=+0.02 {I5} (1990KeZV) gives |d(M2/E1)=-0.03 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E,RI$other: E|g=604.9 {I3}, I|g=0.47 {I8} (1969Be69) 
$|a(K)exp in 1996Gi04 gives |d(M2/E1)=0.19 {I+10-19} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$Other ce data: 1964Ko04, 1953Ma64. |g|g(|q) in 1990KeZV gives |d(Q/D)=-0.016 {I22} 
$(1107|g)(822|g)(|q): A{-2}=+0.100 {I15}, A{-4}=-0.03 {I3} (1978Ba29); A{-2}=+0.125 {I12}, A{-4}=-0.03 {I2} (1990KeZV). Other: 1968Ka04 
$(1107|g)(1362|g)(|q): A{-2}=+0.22 {I3}, A{-4}=-0.02 {I3} (1978Ba29); A{-2}=+0.264 {I16}, A{-4}=0.00 {I3} (1990KeZV). Others: 1968Ka04, 1964Ko04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp in 1996Gi04 gives mult=E1. Other ce data: 1953Ma64 
$(1930|g)(540|g)(|q): A{-2}=+0.20 {I5}, A{-4}=-0.02 {I5} (1978Ba29); A{-2}=+0.175 {I19}, A{-4}=+0.138 {I3} in 1990KeZV gives |d(Q/D)=0.07 {I2}. Others: 1968Ka04, 1964Ko04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$|a(K)exp=0.00084 {I12} from 1996Gi04 gives |d(M2/E1)=0.08 {I8}; |a(K)exp=0.0022 {I6} from 1964Ko04 is for 652|g+654|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$(1155|g)(1362|g)(|q): A{-2}=-0.18 {I22}, A{-4}=+0.03 {I37} (1990KeZV) gives |d(Q/D)=-0.0 {I2} for J=1 and 0.8 {I+17-5} for J=2 with latter adopted by 1990KeZV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M,MR$|d(Q/D)=0.11 {I15} from 1990KeZV based on (1977|g)(540|g)(|q): A{-2}=-0.13 {I25}, A{-4}=-0.16 {I44} for J=1. 1990KeZV adopt |d(E2/M1)=1.3 {I+18-6} for J=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$Placement from 1995KeZZ. 1969Be69 place this |g from 3464 level 
E$level energy difference=403.03 {I1} 
RI$from |g|g. I|g(doublet)=0.232 {I24} from singles spectrum 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Placement may be suspect since with the reported intensity in {+100}Rh |e decay, this |g should have been seen in (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_comment:
$Placement from 1995KeZZ. 1969Be69 place from 3464 level 
E$level energy difference=403.13 {I3} 
RI$from |g|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$|a(K)exp=0.0054 {I3} (1996Gi04) 
$K/L=8.3 {I10}, |a(K)exp=0.0064 {I6}, |a(L)exp=0.00077 {I7} (1964Ko04) 
MR$ce data in 1996Gi04 and 1964Ko04 gives |d(E2/M1)>0.7 is inconsistent with adopted value. Other ce data: 1953Ma64 
$(446|g)(1930|g)(|q): A{-2}=+0.067 {I11}, A{-4}=-0.02 {I3} (1978Ba29) 
$A{-2}=+0.046 {I12}, A{-4}=-0.01 {I2} for (446|g)(1930|g)(|q) and A{-2}=+0.10 {I3}, A{-4}=-0.06 {I5} for (446|g)(1107|g)(|q) (1990KeZV) gives |d(E2/M1)=-0.11 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
$|a(K)exp from 1964Ko04 for 749|g+734|g+736|g. Other ce data: 1953Ma64 
$(749|g)(1627|g)(540|g)(|q): A{-2}=+0.24 {I6}, A{-4}=-0.10 {I10} (1990KeZV) gives |d(E2/M1)=-0.51 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
M,MR$(816|g)(1560|g)(540|g)(|q): A{-2}=-0.06 {I8}, A{-4}=-0.01 {I14} (1990KeZV) gives |d(Q/D)=0.7 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
$(1034|g)(1342)(|q): A{-2}=-0.19 {I4}, A{-4}=+0.02 {I4} (1978Ba29); A{-2}=-0.03 {I5}, A{-4}=0.00 {I9} gives |d(M2/E1)=-0.11 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp=0.000159 {I9} from 1996Gi04 gives |d(M2/E1)=0.10 {I+6-10}. Other ce data: 1953Ma64. |g|g(|q) in 1990KeZV gives |d(Q/D)=-0.003 {I20} 
$(1553|g)(822|g)(|q): A{-2}=+0.083 {I24}, A{-4}=+0.04 {I4} (1978Ba29); A{-2}=+0.09 {I1}, A{-4}=+0.02 {I2}. Other: 1968Ka04 
$(1553|g)(1362|g)(|q): A{-2}=+0.21 {I3}, A{-4}=0.00 {I4} (1978Ba29); A{-2}=+0.246 {I14}, A{-4}=+0.020 {I25} (1990KeZV). Others: 1968Ka04, 1964Ko04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp from 1964Ko04 gives mult=E1. Other ce data: 1953Ma64 
$(2376|g)(540|g)(|q): A{-2}=+0.23 {I3}, A{-4}=-0.03 {I4} (1978Ba29); A{-2}=+0.268 {I10}, A{-4}=+0.017 {I18} in 1990KeZV gives |d(Q/D)=-0.037 {I16}. Others: 1968Ka04, 1964Ko04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M$|a(K)exp from 1996Gi04 gives mult=M1,E2 
$Placement from 1995KeZZ. 1969Be69 and 1996Gi04 place from 2241 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1969Be69 reported only one line at 1206.0 {I10} (I|g=0.05 {I3}). 1995KeZZ report three lines at 1204.46 and 1207.50 (doublet) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1969Be69 reported only one line at 1709.0 {I5} (I|g=0.29 {I3}). 1995KeZZ report a close doublet at 1707.44 and 1710.07 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$(2530|g)(540|g)(|q): A{-2}=+0.44 {I9}, A{-4}=-0.13 {I9} (1978Ba29) gives |d(Q/D)=-0.64 {I5} for J=1; A{-2}=+0.34 {I4}, A{-4}=+0.04 {I7} (1990KeZV) gives |d(Q/D)=-0.53 {I4} for J=1, -0.14 {I6} for J=2 and 0.80 {I18} for J=3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1969Be69 reported only one line at 3071.0 {I10} (I|g=0.05 {I3}). 1995KeZZ report a close doublet at 3069.44 and 3071.80 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$(2784|g)(540|g)(|q): A{-2}=-0.01 {I14}, A{-4}=-0.51 {I24} (1990KeZV) gives |d(Q/D)=5.1 {I+120-25} or -0.05 {I20} for J=1, 0.61 {I+18-3} for J=2, and 0.16 {I3} for J=3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M from |a(K)exp=0.0130 {i5} (1973Al16) ce(K)/I|g 
MR -0.10 {i5}; 
MR from 1973Ka28 |g(|q,t) oriented 4.3-d {+101}Rh source 


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 I|g(307|g)/I|g(221|g)=1.2 {i1} (1978Ba18), |?1.1 (1964Br27) 
I(ce(K) 307|g)/I(ce(K) 221|g)=0.11 {i2} (1965Ch26) on-line s 
M$based on |a(K)exp and |a(exp)=0.2 {I1} from an intensity balance at 307 level 
|a(K)exp=0.15 {i3} from ce(K)(1965Ch26)/I|g(1978Ba18) normalized to |a(K)(307|g)=0.0136 (M1+1% E2 theory). Other |a(K)exp=0.15 deduced from I(K| x ray)/I|g(|w(K)) 
B(M2)(W.u.)=7.6; syst with h11/2 to g7/2 transitions 
Analogs: B(M2)(W.u.)=6.2, B(M2)(W.u.)=8 


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$other: |a(K)exp=0.16 {i2} (1966Wo06) via K| x ray/I|g, scin 
MR$av: +0.22 {I4} from |a(K)exp (1996La21), +0.23 {I+8-7} from K/L (1996La21), +0.17 {I3} (1977Kr13) and 0.18 {I+6-5} (1962Ri09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=AP
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$other: |a(K)exp=0.042 {i1} (1965Hi07). Others: 1960Pe05, 1963Pa24 
MR$from (198|g)(127|g)(|q): 1977Kr13 evaluated coef of 1957Go34, 1965Ev06, 1966Ch13, 1966Wo06 


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:
EKC$|a(K)exp=0.0160 {I8} (1996La21), renormalized to 0.0177 {I9} (Theory) 
M$others: |a(K)exp=0.0164 {i16} (1965Hi07), 0.0177 {i5} (1971Si16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: 545.01 {i15} (1974HeYW), 544.85 {i8} (1971Si16) 
MR from 1973Ka28 |g(|q,t) 
K/L=7.5 {i10} (1971Si16) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$from |a(K)exp=0.15 {i2} (1973Al16) ce(K)/I|g 
MR$from T{-1/2} and B(E2). Others: +0.18 {i6} from A{-2}(127|g)(|q)=+0.114 {i22} (1962Ri09), +0.17 {i4} from (pol 127|g)(198|g)(|q): measured at 0|' and 90|' (1966Wo06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$2015Ki14 give B(M1)(W.u.)=0.0138 {I3} and B(E2)(W.u.)=17.2 {I21} using |d(E2/M1)=+0.148 {I9}, conversion coefficient |a=0.167 {I3}, and level half-life=0.649 ns {I13} from data in literature. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E not observed by 1978De19 and 1980TiZX. E|g from {+102}Rh |e decay (207 d). 
RI from {+102}Rh |e decay (207 d) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
|r(E0)=0.12 {i1} (1986Gi04). Other: 0.092 (1981Ko23) 
B(E0)/B(E2)=0.013 {i2} (1986Gi04,1981Ko23) 
TI calculated by evaluator from Ice values of 1986Gi04 
E completely converted |g-transition observed by 1981Ko23, 1986Gi04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=0.48 {I10} and A{-4}=0.20 {I14} (1971Le19) 
Placement of this |g-ray is doubtful because a 681.1|g in {+100}Mo({+7}Li,p4n|g) was observed under better experimental conditions and placed elsewhere in the level scheme 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
$ Doppler broadening measured for this |g ray (2011Bo24) 
$ Note that using |d(E2/M1)=0.25 {I3} from ENSDF, compiler obtains B(E2)<0.17, rather than <0.5 as given in table I of 2011Bo24 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$ somewhat poor fit. Level-energy difference=1105.40 {I2} 
$ (1105.3|g)(475.1|g)(|q): A{-2}=+0.117 {I9}, A{-4}=+0.014 {I19} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$ (601.3|g)(638.8|g)(|q): A{-2}=+0.05 {I11}, A{-4}=+0.12 {I21} 
$ (601.3|g)(1105.3|g)(|q): A{-2}=+0.27 {I8}, A{-4}=-0.16 {I18} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
E not observed experimentally but required from the coincidence relationship 
RI from I(|g+ce) balance at 2.7 level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=AP;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_comment:
E strong I(K| x ray) observed (T{-1/2} short) implies strongly converted transition of E|g>22 keV; photon peak obscured by K| x ray lines + impurity. Not observed experimentally but required from the coincidence relationship 
RI required for I(|g+ce) balance at 213 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=-0.211 {I32}, A{-4}=0.026 {I36} (1986Ka37) 
$A{-2}/A{-0}=-0.21 {I3}, A{-4}/A{-0}=-0.06 {I3} (1975Kl04) 
RI calculated from I|g(210|g)/I|g(346|g)=0.47 {I7} in (n,|g) and doublet I|g(210|g)=1223 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=0.186 {I40}, A{-4}=-0.02 {I47} (1986Ka37) 
$A{-2}/A{-0}=+0.04 {I9}, A{-4}/A{-0}=-0.08 {I8} (1975Kl04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=-0.47 {I43}, A{-4}=0.038 {I50} (1986Ka37) 
$A{-2}/A{-0}=-0.29 {I9}, A{-4}/A{-0}=-0.05 {I9} (1975Kl04) 
MR$from 1986Ka37 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=-0.638 {I12}, A{-4}=0.072 {I19} (1986Ka37) 
$A{-2}/A{-0}=-0.54 {I6}, A{-4}/A{-0}=+0.15 {I7} (1975Kl04) 
MR$from 1986Ka37, 1975Kl04 report -1.8 {I+4-26} 
M$from |g(|q) and level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}/A{-0}=-0.20 {I6}, A{-4}/A{-0}=+0.09 {I8} (1975Kl04) 
$A{-2}=0.010 {I39}, A{-4}=-0.019 {I49} (1986Ka37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$A{-2}/A{-0}=-0.55 {I7}, A{-4}/A{-0}=-0.03 {I8} (1975Kl04) 
MR$from 1975Kl04; |d=-1.0 {I+3-5} (1986Ka37) 
$A{-2}=-0.671 {I37}, A{-4}=0.63 {I46} (1986Ka37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}/A{-0}=+0.14 {I10}, A{-4}/A{-0}=-0.07 {I10} (1975Kl04) 
$A{-2}=0.244 {I34}, A{-4}=-0.075 {I40} (1986Ka37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=-0.14 {I38}, A{-4}=0.031 {I46} (1986Ka37) 
$A{-2}/A{-0}=-0.07 {I6}, A{-4}/A{-0}=-0.15 {I5} (1975Kl04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}/A{-0}=+0.17 {I6}, A{-4}/A{-0}=-0.03 {I4} (1975Kl04) 
$A{-2}=-0.244 {I45}, A{-4}=-0.090 {I27} (1986Ka37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}/A{-0}=-0.29 {I12}, A{-4}/A{-0}=+0.05 {I17} (1975Kl04) 
$A{-2}=-0.591 {I44}, A{-4}=0.035 {I50} (1986Ka37) 
MR$from 1986Ka37 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=0.224 {I25}, A{-4}=-0.075 {I29} (1986Ka37) 
$A{-2}/A{-0}=+0.13 {I7}, A{-4}/A{-0}=-0.09 {I7} (1975Kl04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=0.226 {I26}, A{-4}=-0.015 {I31} (1986Ka37) 
$A{-2}/A{-0}=+0.34 {I24}, A{-4}/A{-0}=-0.56 {I16} (1975Kl04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
MR if J{-i}=13/2 (1975Kl04) 
$A{-2}/A{-0}=-0.12 {I28}, A{-4}/A{-0}=+0.15 {I37} (1975Kl04) 
$A{-2}=-0.30 {I40}, A{-4}=-0.094 {I43} (1986Ka37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=0.271 {I30}, A{-4}=-0.115 {I40} (1986Ka37) 
$A{-2}/A{-0}=+0.11 {I9}, A{-4}/A{-0}=+0.04 {I10} (1975Kl04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E2 matrix element (to 358,2+)=+1.43 {I4}; +1.47 {I8} (1984St08); +1.44 {I8} (1982St09); B(E2)=0.226 {I11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$from |a|g(|q) 1968Mc08 
$M1 matrix element (358,2+ to 893,2+)<0.02 
$E2 matrix element (to 358,2+)=-0.75 {I4}; -0.9 {I4} (1984St08); -1.0 {I3} (1982St09); B(E2)=0.113 {I11} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$M1 matrix element (888,4+ to 1502,4+)=-0.15 {I3} 
$E2 matrix element (to 888,4+)=-0.83 {I5}; -0.4 {I3} (1984St08); B(E2)=0.0759 {I9} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$M1 matrix element (358,2+ to 1515,2+)=+0.24 {I3} 
$E2 matrix element (to 358,2+)=0.07 {I3}; B(E2)=0.0011 {I+12-6} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$E2 matrix element (to 888,4+)=+2.04 {I8}; +2.09 {I9} (1984St08); +2.17 {I9} (1982St09); B(E2)=0.320 {I+10-26} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$E2 matrix element (to 2197,6+)=+2.0 {I4}; +2.49 {I8} (1984St08); +2.46 {I6} (1982St09); B(E2)=0.23 {I+6-9} 


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=LE;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LE
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
CC$from I(|g+ce) balance at 20.567-keV level in {+104}Ru(n,|g) E=th ; Others: 6.7~{I12} (1978Gu14) and |a|?24 (1974Hr01) 
MR$From |a and |a(M1)=4.02~{I6} and |a(E2)=409~{I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.32~{I3} and A{-4}=0.04~{I4} in {+104}Ru(n,|g) E=th (1974Hr01) 
MR$also -2.40~{I12} in {+104}Ru(n,|g) E=th (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=-0.12~{I2} and A{-4}=0.00~{I2} in {+104}Ru(n,|g) E=th (1974Hr01) 
MR$Also >12 in {+104}Ru(n,|g) E=th (1978Gu14) 


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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_uncertain: S
decay_comment:
E$Not observed, but suggested by the evaluators on the basis of observed 365|g-143|g coinc. 
M$assumed by the evaluators on the basis of 208.6-keV level T{-1/2} and decay pattern. Parity changing transitions of higher multipolarity would be unreasonably enhanced. Possible small M2 admixture. 
BE1W$>1.3|*10{+-6} is consistent with B(E1)(W.u.) (7/2- to 5/2-) =7.0|*10{+-6} in {+103}Ru (2016Ki20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from curved crystal measurements (1979Bo26) 
M$A{-22}=-0.112~{I9} and A{-44}=-0.005~{I15} in {+104}Ru(n,|g) E=th (1978Gu14) and A{-22}=-0.112~{I8} and A{-44}=0 in {+104}Ru(n,|g) E=th (1978Gu14); A{tot}=0.6~{I3} from x-|g coinc. in 1975RaZL 
MR$Also 0.45~{I4} in {+104}Ru(n,|g) E=th (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from curved crystal measurements (1979Bo26) 
M$A{-22}=-0.311~{I18} and A{-44}=0.015~{I9} in {+104}Ru(n,|g) E=th (1978Gu14) or A{-22}=-0.305~{I15} and 0 in {+104}Ru(n,|g) E=th (1978Gu14) 
MR$also -0.13~{I4} in {+104}Ru(n,|g) E=th (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.10~{I5} and A{-44}=-0.12~{I6} in {+104}Ru(n,|g) E=th (1978Gu14) or A{-22}=0.07~{I4} and A{-44}=0 in {+104}Ru(n,|g) E=th (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.352~{I29} and A{-44}=0.038~{I48} in {+104}Ru(n,|g) E=th (1978Gu14) or A{-22}=-0.340~{I25} and A{-44}=0 in {+104}Ru(n,|g) E=th (1978Gu14) 
MR$Also -3.7~{I+5-6} in {+104}Ru(n,|g) E=th (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$41~{I11} in {+105}Tc |b{+-} decay 
M$A{-22}=-0.019~{I41} and A{-44}=0.41~{I17} in {+104}Ru(n,|g) E=th (1978Gu14) or A{-22}=-0.015~{I37} and A{-44}=0 in {+104}Ru(n,|g) E=th (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$100~{I19} in {+105}Tc |b{+-} decay 
M$A{-22}=0.150~{I15} and A{-44}=0.013~{I25} in {+104}Ru(n,|g) E=th (1978Gu14) or A{-22}=0.158~{I13} and A{-44}=0 in {+104}Ru(n,|g) E=th (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.349~{I40} and A{-44}=0.019~{I59} in {+104}Ru(n,|g) E=th (1978Gu14) or A{-22}=0.353~{I38} and A{-44}=0 in {+104}Ru(n,|g) E=th (1978Gu14) 
MR$Also 0.88~{I+15-18} in {+104}Ru(n,|g) E=th (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.013~{I48} and A{-44}=-0.012~{I76} in {+104}Ru(n,|g) E=th (1978Gu14) or A{-22}=-0.017~{I43} in {+104}Ru(n,|g) E=th (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$A{-22}=-0.072~{I30} and A{-44}=-0.025~{I47} in {+104}Ru(n,|g) E=th (1978Gu14) or A{-22}=-0.081~{I27} and A{-44}=0 in {+104}Ru(n,|g) E=th (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
E$Relative intensities of 358, 472 and 631 |g's deexciting the 631-keV level are not in good agreement with those measured in (n,|g) work: I(358|g): I(472|g); I(631|g)= 1.8 {I12}: 1.0: 0.75 {I45} here, 2.4 {I16}: 1.0: 6.6 {I20} in (n,|g) work Values from (n,|g) adopted 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$relative intensities of 541 and 1004 |g's measured in (n,|g) and {+105}Tc |b{+-} decay are not consistent: I(541|g)/I(1004|g)=1.2 {I4} in (n,|g) work, 0.40 {I18} here 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.112~{I9} and A{-44}=-0.005~{I15} (1978Gu14) and A{-22}=-0.112~{I8} and A{-44}=0 (1978Gu14) 
MR$Also 0.45~{I4} (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.311~{I18} and A{-44}=0.015~{I9} (1978Gu14) or A{-22}=-0.305~{I15} and 0 (1978Gu14) 
MR$also -0.13~{I4} (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$A{-22}=0.003~{I11} and A{-44}=-0.031~{I21} (1978Gu14) or A{-22}=-0.004~{I17} and A{-44}=0 (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI 0.17 {I9} was given by 1974Hr01 which is in better agreement with I(164.4|g)/I(252|g)=0.051 {I12} as measured in {+105}Tc |b{+-} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
M$A{-22}=-0.161~{I16} and A{-44}=0.013~{I26} (1978Gu14) and A{-22}=-0.157~{I16} and A{-44}=0 (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-22}=0.205~{I16} and A{-44}=-0.015~{I25} (1978Gu14) or A{-22}=0.202~{I15} and A{-44}=0 (1978Gu14); |d=0.02~{I+5-8} (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.352~{I29} and A{-44}=0.038~{I48} (1978Gu14) or A{-22}=-0.340~{I25} and A{-44}=0 (1978Gu14) 
MR$Also -3.7~{I+5-6} (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$0.30 {I14} was measured by 1974Hr01. I(307|g)/I(446|g) ratio does not agree well with the ratio of 0.63 {I21} obtained in {+105}Tc |b{+-} decay 
M$A{-22}=-0.019~{I41} and A{-44}=0.41~{I17} (1978Gu14) or A{-22}=-0.015~{I37} and A{-44}=0 (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.150~{I15} and A{-44}=0.013~{I25} (1978Gu14) or A{-22}=0.158~{I13} and A{-44}=0 (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.349~{I40} and A{-44}=0.019~{I59} (1978Gu14) or A{-22}=0.353~{I38} and A{-44}=0 (1978Gu14) 
MR$Also 0.88~{I+15-18} (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$A{-22}=0.025~{I55} and A{-44}=-0.043~{I99} (1978Gu14) and A{-22}=0.015~{I43} and A{-44}=0 (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$714.1|g from 1180-keV level in 1974Hr01 
M$A{-22}=-0.013~{I59} and A{-44}=-0.006~{I106} (1978Gu14) or A{-22}=-0.015~{I44} and A{-44}=0 (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.003~{I15} and A{-44}=-0.023~{I23} (1978Gu14) or A{-22}=-0.008~{I14} (1978Gu14) 
MR$-0.25~{I2} (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$A{-22}=-0.072~{I30} and A{-44}=-0.025~{I47} (1978Gu14) or A{-22}=-0.081~{I27} and A{-44}=0 (1978Gu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M from |d=infinity in (444|g)(270|g)(|q). These values are consistent with pure Q but not precise enough to exclude a small D fraction 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M from J|p assignment. Consistent with |d=infinity from (720|g)(270|g)(|q). These values are consistent with pure Q but not precise enough to exclude a small D fraction 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$this transition is not seen in (SF), So the 6+ assigned to the 1218 level in {+108}Tc decay is questionable. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$from (1445.5|g)(422.5|g)(|q): A{-2}=-0.073 {I13}, A{-4}=-0.012 {I19}. The predicted values for dipole-quadrupole cascade are: A{-2}=-0.071, A{-4}=0; and for quadrupole-quadrupole cascade are: A{-2}=-0.128 and A{-4}=-0.059. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$a{-2}/a{-0}=-0.14 {i4}, a{-4}/a{-0}=0.06 {i4} for (172|g)(132|g)(|q) in {+252}Cf SF decay (1995Bu14) 


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=0.084 {i10} (1992PeZX); |d=0.20 {I3} from |a(K)exp, but B(M2)(W.u.)=250 {I80} exceeds RUL(IV)=1 by more than 3 sigma 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$from a{-2}/a{-0}=-0.16 {i2}, a{-4}/a{-0}=0.01 {i3} for (473|g)(185|g)(|q) (2009Go18). Other value: |d(E2/M1)=-2.0 {i4} (2009Go18) 


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$From 1981SeZW in {+254}Cf SF decay 
M$a{-2}/a{-0}=0.12 {i3}, a{-4}/a{-0}=0.03 {i3} for (374|g)(172|g)(|q)(1995Bu14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$Other: 72 {I6} in {+238}U(|a,F|g) (2006Wu01) 
M,MR$from a{-2}/a{-0}=-0.20 {i3},a{-4}/a{-0}=-0.03 {i2} for (540.7|g)(222.7|g)(|q) (2009Go18). Other value: |d(E2/M1)=-1.8 {i4} (2009Go18) 


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=AP;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=AP
decay_comment:
E$374.2 (1973Ho22), 374.2 (1981SeZW) 
M$a{-2}/a{-0}=0.12 {i3}, a{-4}/a{-0}=0.03 {i3} for (374|g)(172|g)(|q) and a{-2}/a{-0}=0.12 {i2}, a{-4}/a{-0}=-0.01 {i2} (541|g)(374|g)(|q) (1995Bu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$a{-2}/a{-0}=0.19 {i5}, a{-4}/a{-0}=-0.05 {i5} for (691|g)(541|g)(|q) and a{-2}/a{-0}=0.12 {i2}, a{-4}/a{-0}=-0.01 {i2} (541|g)(374|g)(|q) (1995Bu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
%I|g|?4.1, using the calculated normalization. 
E$Other: 68.7 {i3} (1990Al43) 
RI$Other: 54 {i5}, includes also I|g(69.1|g) (1990Al43) 
M$|a(K)exp=3.5 {i9} and K/L=3.0 {I2} (1992PeZX) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
%I|g|?5.5, using the calculated normalization. 
E$Other: 95.9 {i3} in 1990Al43 
RI$Other: 64 {i6} in 1990Al43 
M$|a(K)exp=0.13 {i2} (1992PeZX) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
%I|g|?3.8, using the calculated normalization. 
RI$Other: 54 {i5}, includes also I|g(68.8|g) (1990Al43) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
%I|g|?3.0, using the calculated normalization. 
E$Others:137.8 {i3} (1990Al43), 137.7 {i3} (1989Gr23) 
RI$Other: 27 {i3} (1990Al43) 
M,MR$|a(K)exp=0.084 {i10} (1992PeZX) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
%I|g|?0.32, using the calculated normalization. 
M$|a(K)exp=0.26 {i5} for both 98.2|g and 98.9|g (1992PeZX) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
%I|g|?12.4, using the calculated normalization. 
E$Others: 194.9 {i3} (1990Al43), 194.6 {i3} (1989Gr23) 
RI$Other: 100 {i5} (1990Al43) 
M$|a(K)exp=0.039 {i4} and K/L=6.6 {I20} (1992PeZX) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
%I|g|?5.6, using the calculated normalization. 
E$Other: 128.4 {i3} (1990Al43) 
RI$Other: 54 {i5} (1990Al43) 
M,MR$|a(K)exp=0.087 {i7} (1992PeZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
%I|g|?0.50, using the calculated normalization. 
M$|a(K)exp=0.26 {i5} for both 98.2|g and 98.9|g (1992PeZX) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g|?2.5, using the calculated normalization. 
E$Other: 208.0 {i3} (1990Al43) 
RI$Other: 32 {i3} (1990Al43) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$Other: 132.0 keV (1974ClZX) and 131.8 keV (1973Ho22) 
M$A{-2}/A{-0}=-0.14 {I4}, A{-4}/A{-0}=0.06 {I4} for (172|g)(132|g)(|q) (1995Bu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$ from A{-2}/A{-0}=-0.16 {I2}, A{-4}/A{-0}=0.01 {I3} for (473|g)(185|g)(|q) (2008Go18). Other value: |d(E2/M1)=-2.0 {I4} (2008Go18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$other: 172.3 keV (1973Ho22) and 172 keV (1969WiZX), 
M$A{-2}/A{-0}=0.12 {I3}, A{-4}/A{-0}=0.03 {I3} for (374|g)(172|g)(|q) (1995Bu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$ A{-2}/A{-0}=-0.20 {I3},A{-4}/A{-0}=-0.03 {I2} for (540.7|g)(222.7|g)(|q) (2008Go18). Other value: |d(E2/M1)=-1.8 {I4} (2008Go18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$others: 374.2 keV (1973Ho22) and 374 keV (1969WiZX), 
M$A{-2}/A{-0}=0.12 {I3}, A{-4}/A{-0}=0.03 {I3} for (374|g)(172|g)(|q) and A{-2}/A{-0}=0.12 {I2}, A{-4}/A{-0}=-0.01 {I2} (541|g)(374|g)(|q) (1995Bu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$A{-2}/A{-0}=0.19 {I5}, A{-4}/A{-0}=-0.05 {I5} for (691|g)(541|g)(|q) and A{-2}/A{-0}=0.12 {I2}, A{-4}/A{-0}=-0.01 {I2} for (541|g)(374|g)(|q) (1995Bu14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$A{-2}=0.229 {I101}, A{-4}=0.195 {I153} from |g(|q) in 1972Wi15. |a(K)exp/|a(L)exp|?4.0 in 1970Wa05, |a(K)exp measurements in 1990Ay02, but the value was not given by the authors 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$From {+110}Tc |b{+-} decay (1990Ay02), based on conversion electron measurements, but the value was not given by the authors 


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 {+110}Tc |b{+-} decay (1990Ay02), based on conversion electron measurements, but the value was not given by the authors and the band structure 


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 {+248}Cm SF decay (1994Sh26), based on |g|g(|q) but A{-2} and A{-4} values were not given by the authors 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$From 2009Lu18:(867.5|g)(515.5|g)(|q): A{-2}=-0.052 {I14}, A{-4}=-0.002 {I21}. In 2009Lu01, A{-4} = +0.002 {I21} is quoted. The theoretical values for a pure dipole transition are: A{-2}=-0.071, A{-4}=0; and for a pure quadrupole transition are A{-2}=-0.112 and A{-4}=-0.054. (867.5|g)(394.5|g)(|q): A{-2}=-0.079 {I14}, A{-4}=+0.023 {I20}. The theoretical values for a pure dipole transition are: A{-2}=-0.071, A{-4}=0; and for a pure quadrupole transition are A{-2}=-0.007 and A{-4}=-0.023. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$From 2009Lu18: (1187.2|g)(575.5|g)(|q): A{-2}=-0.086 {I11}, A{-4}=+0.010 {I17}. The theoretical values for a pure dipole transition are: A{-2}=-0.071, A{-4}=0; and for a pure quadrupole transition are: A{-2}=-0.102 and A{-4}=-0.051 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$Uncertainty of 0.020 quoted in table I of 2000Wa07 is probably a misprint. The evaluator has increased it by a factor of 10. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$I|g=100 
M$A{-2}=0.229 {I101}, A{-4}=0.195 {I153} from |g(|q) in 1972Wi15; |a(K)exp/|a(L)exp|?4.0 in 1970Wa05 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$I|g=9 
M$From 2009Lu18:(867.5|g)(515.5|g)(|q): A{-2}=-0.052 {I14}, A{-4}=-0.002 {I21}. In 2009Lu01, A{-4} = +0.002 {I21} is quoted. The theoretical values for a pure dipole transition are: A{-2}=-0.071, A{-4}=0; and for a pure quadrupole transition are A{-2}=-0.112 and A{-4}=-0.054. (867.5|g)(394.5|g)(|q): A{-2}=-0.079 {I14}, A{-4}=+0.023 {I20}. The theoretical values for a pure dipole transition are: A{-2}=-0.071, A{-4}=0; and for a pure quadrupole transition are A{-2}=-0.007 and A{-4}=-0.023. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$I|g=7 
M$From 2009Lu18: (1187.2|g)(575.5|g)(|q): A{-2}=-0.086 {I11}, A{-4}=+0.010 {I17}. The theoretical values for a pure dipole transition are: A{-2}=-0.071, A{-4}=0; and for a pure quadrupole transition are: A{-2}=-0.102 and A{-4}=-0.051 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=CONV
decay_comment:
$The B(E2) value was obtained independently in 2017Do01, in the sense, that the known lifetime of this level was not used as a constraining parameter in their GOSIA analysis 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$|DJ=0 transition. A multipolarity of M1 cannot be ruled out for this |g-ray. However, an M1 assignment to this transition, would imply that the admixture of an E2 component would be rather small, considering the obtained |a{-K} value. Also, the pure M1 transition of such an energy should usually be faster than the rate which was observed. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
MR$unweighted average (by compilers) of -0.48 {I5}, -0.32 {I2} and -0.51 {I7}. This |d value compares with theoretical value of -0.21 for 5/2[402] orbital. Theoretical value of |d is +0.85 for 5/2[413] orbital 
$ |d(E2/M1)=-0.48 {I5} or -1.3 {I+9-3} from (166.6|g)(150.2|g)(|q), pure E1 assumed for 166.6|g 
$ |d(E2/M1)=-0.32 {I2} or -1.73 {I9} from (103.8|g)(150.2|g)(|q), pure E1 assumed for 103.8|g 
$ |d(E2/M1)=-0.51 {I7} or -1.23 {I16} from (431.3|g)(150.2|g)(|q), pure E2 assumed for 431.3|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 the ce measurement in {+112}Tc |b{+-} decay (1990Ay02) and |g(|w) in {+248}Cm SF decay (1994Sh26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$from (1299.6|g)(544.7|g)(|q): A{-2}=-0.090 {I35}, A{-4}=-0.02 {I6} in {+252}Cf SF decay. The predicted values are a{-2}=-0.071, a{-4}=0 (for a dipole-quadrupole cascade and A{-2}=-0.102 and A{-4}=-0.051 for a quadrupole-quadrupole cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$from (1384.6|g)(544.7|g)(|q): A{-2}=-0.07 {I6}, A{-4}=-0.05 {I9} in {+252}Cf SF DECAY. The predicted values are A{-2}=-0.071, A{-4}=0 for a for dipole-quadrupole cascade and A{-2}=-0.102 and A{-4}=-0.051 for a quadrupole-quadrupole cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$from (1299.6|g)(544.7|g)(|q): A{-2}=-0.090 {I35}, A{-4}=-0.02 {I6}. The predicted values for dipole-quadrupole cascade are: A{-2}=-0.071, A{-4}=0; and for quadrupole-quadrupole cascade are: A{-2}=-0.102 and A{-4}=-0.051. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$from (1384.6|g)(544.7|g)(|q): A{-2}=-0.07 {I6}, A{-4}=-0.05 {I9}. The predicted values for dipole-quadrupole cascade are: A{-2}=-0.071, A{-4}=0; and for quadrupole-quadrupole cascade are: A{-2}=-0.102 and A{-4}=-0.051. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
RI$ deduced by XUNDL from combined I(|g+ce)=10 {I4} from mixed isomers. Note that 23 {I4} in table I of 2011Ri01 is a misprint 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
RI$ combined I(|g+ce)=15 {I6} from mixed isomers; a small fraction (|?0.3 units) may be associated with the decay of the low-spin isomer 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$ combined intensity from mixed isomers; a small fraction (|?0.5 units) may be associated with the decay of the low-spin isomer. Note that 10 {I4} in table I of 2011Ri01 is a misprint 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
RI$ deduced by Xundl from combined I(|g+ce)=10 {I4} from mixed isomers. Note that 23 {I4} in table I of 2011Ri01 is a misprint 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$ combined I(|g+ce)=23 {I4} from mixed isomers. Note that 10 {I4} in table I of 2011Ri01 is a misprint 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp=2.7 {I6} 
E$ this |g seen in singles |g only, not in |b-gated |g spectrum. This |g is correlated with 19.2-keV K{-|a} x ray of Ru. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
E$ this |g is singles |g only, not in |b-gated |g spectrum. This |g is correlated with 19.2-keV K{-|a} x ray of Ru (2010Ku25). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D,E2)
decay_comment:
M$from 2012Ka36 based on Weisskopf estimates. Other: E1 assigned by 2012LaZT based on systematics of hindrance factors, which seem to rule out M2 
CC$overlaps E1, M1 and E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D,E2)
decay_comment:
E$others: 184 {I1} (2012LaZT), 184.4 {I2} (2006ToZW) 
M$from 2012Ka36 based on Weisskopf estimates. Other: E1 assigned by 2012LaZT based on systematics of hindrance factors, which seem to rule out M2 
CC$overlaps E1, M1 and E2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
M |g anisotropy ratio=1.56 {I12}; interpreted as D, |DJ=0 by 1997Ka07, but also consistent with Q, |DJ=2. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E,RI transition not studied in this work due to expected long half-life (|?34 ns) of 235 level based on Weisskopf estimates. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E from Adopted Gammas; E|g=543.7 {I2} (I|g=2.4 {I2}) in 2004Mu30 is for a doublet comprised of the adopted 542.8|g and 545.5|g. 
RI 2.4 {I2} for doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E Placement and intensity of transition deduced in 2004Mu30 by using coincident-proton threshold of 2.5 MeV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$Q from |g(|q); assumed E2 by 1980No06 
E$weighted average of 1351.06 {I12} ({+95}Pd |e decay (13.3 s)), 1350.7 {I2} ({+58}Ni({+40}Ca,3p|g), {+64}Zn({+36}Ar,p|a|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$Q from |g(|q); assumed E2 by 1980No06 
E$weighted average of 716.6 {I1} ({+95}Pd |e decay (13.3 s)), 716.2 {I2} ({+58}Ni({+40}Ca,3p|g), {+64}Zn({+36}Ar,p|a|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 168.8 {I1} ({+95}Pd |e decay (13.3 s)), 169.0 {I2} ({+58}Ni({+40}Ca,3p|g), {+64}Zn({+36}Ar,pag 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 913.2 {I1} ({+95}Pd |e decay (13.3 s)), 912.9 {I2} ({+58}Ni({+40}Ca,3p|g), {+64}Zn({+36}Ar,p|a|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$weighted average of 185.0 {I1} ({+95}Pd |e decay (13.3 s)), 185.2 {I2} ({+58}Ni({+40}Ca,3p|g), {+64}Zn({+36}Ar,p|a|g)) 
RI$weighted average of 12.8 {I4} ({+95}Pd |e decay (13.3 s)), 11.5 {I15} ({+58}Ni({+40}Ca,3p|g), {+64}Zn({+36}Ar,p|a|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$weighted average of 381.8 {I1} ({+95}Pd |e decay (13.3 s)), 381.5 {I2} ({+58}Ni({+40}Ca,3p|g), {+64}Zn({+36}Ar,p|a|g)) 
RI$weighted average of 100 {I3} ({+95}Pd |e decay (13.3 s)), 100 {I3} ({+58}Ni({+40}Ca,3p|g), {+64}Zn({+36}Ar,p|a|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 1005.1 {I2} ({+95}Pd |e decay (13.3 s)), 1004.8 {I2} ({+58}Ni({+40}Ca,3p|g), {+64}Zn({+36}Ar,p|a|g)) 


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$weighted average of 52.0 {I1} ({+96}Rh IT decay (1.51 min)) and 51.8 3({+96}Ru(p,n|g)) 
M$from |a(K)exp in it Decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 762.3 {I2} ({+96}Pd |e decay), 762.6 {I5} ({+96}Ru(p,n|g)) and 762.1 {I3} ({+64}Zn({+40}Ca,|a3pn|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
RI$from (|a,p2n|g); ({+40}Ca,3p|g) gives I(|g+ce)=15 {I3} (I|g=10.2 {I20}); ({+36}S,4n|g) gives I|g=14.3 {I14} 
M$D |g from |g(|q) (|a,p2n|g) or D(+Q) |g from DCO ({+36}S,4n|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E,RI$from ({+40}Ca,3p|g) (also observed in ({+36}S,4n|g)) 
M$from |g(|q) ({+40}Ca,3p|g) and DCO ({+36}S,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E,RI$from ({+40}Ca,3p|g) (also observed in ({+36}S,4n|g)) 
M$from |g(|q) ({+40}Ca,3p|g), DCO ({+36}S,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 106.8 {I2} from {+98}Pd |e decay (17.7 min), 106.8 {I7} from ({+28}Si,2p3n|g), 106.8 {I3} from (|a,pn|g), 106.8 {I2} from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 112.2 {I2} from {+98}Pd |e decay (17.7 min), 112.5 {I3} from (|a,pn|g), 112.4 {I2} from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 67.7 {I2} from {+98}Pd |e decay (17.7 min), 67.7 {I3} from (|a,pn|g), 67.7 {I2} from (p,n|g) 
RI$from {+98}Pd |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 174.5 {I2} from {+98}Pd |e decay (17.7 min), 174.4 {I3} from (|a,pn|g), 174.6 {I3} from (p,n|g) 
RI$from {+98}Pd |e decay. Other: I|g(174)/I|g(67.7)=100 {I15}/65 {I12} in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 841.6 {I3} in ({+28}Si,2p3n|g), 841.6 {I4} in ({+36}S,3n|g) and 841.3 {I3} in (|a,pn|g) 
$Placement of this |g to the 56, (5+) level is from 2014Ku04; it was previously placed to (2+) ground state. See also comments for 898 and 56 levels. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 725.6 {I3} in ({+28}Si,2p3n|g), 726.5 {I4} in ({+36}S,3n|g) and 725.8 {I3} in (|a,pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 994.0 {I3} in ({+28}Si,2p3n|g) and 994.3 {I3} in (|a,pn|g). Other: 995.1 {I4} in ({+36}S,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 413.0 {I5} in ({+28}Si,2p3n|g) and 413.4 {I4} in ({+36}S,3n|g) 
RI$others: 29 {I6} in ({+32}S,3pn|g) and 46 {I5} in ({+36}S,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 979.7 {I3} in ({+28}Si,2p3n|g), 980.4 {I4} in ({+36}S,3n|g) and 979.9 {I3} in (|a,pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$other: 1152 (Mult=Q) placed from a 6346 level in ({+32}S,3pn|g), 1150.7 {I4} placed from a 8848 level in ({+36}S,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$others: 263.7 {I3} from (|a,pn|g), 265.2 {I4} from ({+36}S,3n|g) 
RI$others: 100 {I5} in ({+32}S,3pn|g), 100 in ({+36}S,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$others: 463.4 {I4} (Mult=D) placed from a 3243 level in ({+36}S,3n|g), 462 (Mult=D) placed from a 3022 level in ({+32}S,3pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 548.9 {I3} in ({+28}Si,2p3n|g) and 549.5 {I4} in ({+36}S,3n|g) 
RI$other: 100 {I8} in ({+32}S,3pn|g), 77 in ({+36}S,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$other: 815.4 {I4} (Mult=Q) in ({+36}S,3n|g) 
RI$other: 40 {I4} in ({+32}S,3pn|g), 100 in ({+36}S,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 792 (Mult=Q) placed from a 3814 level in ({+32}S,3pn|g), 792.5 {I4} (Mult=D) placed from a 4036 level in ({+36}S,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$other: 457.4 {I4} (Mult=Q) placed from a 4001 level in ({+36}S,3n|g) 
RI$other: 39 {I3} in ({+32}S,3pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 1137.3 {I4} (Mult=Q) placed from a 5496 level in ({+36}S,3n|g) 
RI$other: 100 {I7} in ({+32}S,3pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 1380 (Mult=Q) placed from a 5194 level in ({+32}S,3pn|g), 1380.9 {I4} (Mult=D) placed from a 5417 level in ({+36}S,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$In Table I of 2014Ku04, this |g is listed as feeding a 16+ level, but not clear which of the two 16+ levels: 5547 or 5611. Here the evaluators have assumed it feeds 5611 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$other: 21 {I4} in ({+32}S,3pn|g) 
M$D (|DJ=1) from |g|g(DCO) in ({+32}S,3pn|g) is inconsistent with adopted spin-change (|DJ=0) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$other: 1363.9 {I4} (Mult=Q) in ({+36}S,3n|g) 
RI$other: 100 {I13} in ({+32}S,3pn|g) 
M$other: (Q) from |g|g(DCO) in ({+32}S,3pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 933 (Mult=Q) placed from a 6127 level in ({+32}S,3pn|g), 933.1|g (Mult=D) placed from a 6350 level and 934.6 {I4} placed from a 8652 level in ({+36}S,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$weighted average of 1432.2 {I7} in ({+28}Si,2p3n|g) and 1433.1 {I4} in ({+36}S,3n|g) 
M$from |g|g(DCO) in ({+32}S,3pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$other: 1347.4 {I4} placed from a 7697 level in ({+36}S,3n|g), 1347 (Mult=(Q)) placed from a 7474 level in ({+32}S,3pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 1486 placed from a 8960 level in ({+32}S,3pn|g), 1487.5 {I4} placed from a 9185 level in ({+36}S,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 106.8 {I2} (1972Ba37), 106.5 {I5} (1978Ki17), and 106.9 {I2} (1972Ga21). Other: 106.75 (1990RyZX) 
RI$others: 25 {I2} (1978Ki17), 33 {I6} (1972Ga21), 25.5 (1972Ba37) 
M$|a(K)exp=0.30 {I5}. 1972Ga21 give 0.26 {I7} with Ice(K)/Ice(K)(112|g)=0.336 {I25} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 112.5 {I2} (1972Ba37), 112.0 {I5} (1978Ki17), 112.0 {I2}, and 112 {I1} (1969An32). Other: 112.0 (1990RyZX) 
RI$others: 100 (1972Ba37,1978Ki17,1972Ga21,1969An32) 
M$|a(K)exp=0.225 {I50} (1972Ga21) 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
E$from 1972Ga21 only. Not seen in 1990RyZX, 1978Ki17 and 1972Ba37 
M$1972Ga21 give |a(K)exp=1.00, suggesting M1 
RI$1972Ga21 give 0.18 {I7} and Ice(K)/Ice(K)(112|g)=0.004. Other: <0.5 (1978Ki17, not seen) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 67.7 {I2} (1972Ba37), 67.5 {I5} (1978Ki17), and 67.8 {I2} (1972Ga21). Other: 67.7 (1990RyZX) 
RI$others: 19 {I2} (1978Ki17), 14 {I4} (1972Ga21), 18.1 (1972Ba37) 
M$|a(K)exp=0.58 {I6}. 1972Ga21 give 0.88 {I27} with Ice(K)/Ice(K)(112|g)=0.396 {I16} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 174.5 {I2} (1972Ba37), 174.5 {I5} (1978Ki17), and 174.6 {I2} (1972Ga21). Other: 174.4 (1990RyZX) 
RI$others: 18 {I2} (1978Ki17), 6.5 (1972Ga21), 21.2 (1972Ba37) 
M$|a(K)exp=0.057 {I11}. 1972Ga21 give 0.075 {I24} with Ice(K)/Ice(K)(112|g)=0.033 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
E$weighted average of 663.0 {I4} (1972Ba37), 661.5 {I15} (1978Ki17), 661.7 {I2} (1972Ga21) and 661 {I1} (1969An32). Other: 662.2 (1990RyZX) 
RI$others: 50 {I5} (1978Ki17), 30 {I2} (1972Ga21), 52.8 (1972Ba37), 43 {I7} (1969An32) 
M$|a(K)exp=0.0036 {I8}. 1972Ga21 give 0.0027 {I7} with Ice(K)/Ice(K)(112|g)=0.0056 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 725.7 {I4} (1972Ba37) and 725.0 {I10} (1978Ki17). Other: 724.7 (1990RyZX) 
RI$others: 7.7 {I9} (1978Ki17), 10.2 (1972Ba37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 837.9 {I4} (1972Ba37) and 836.0 {I10} (1978Ki17). other: 836.8 (1990RyZX) 
RI$others: 3 {I1} (1978Ki17), 30.3 (1972Ba37). Note severe disagreement in 1972Ba37 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$a 409.1|g placed from 3563, (11+) level and a 407.6|g placed from 2390, (8+) level in Adopted Levels; not seen in 1998Ch04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$a 215.1|g placed from 4447, (14-) level and a 215.2|g placed from 7552, (20-) level in Adopted Levels; not seen in 1998Ch04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$a 456.2|g placed from 5547, (16+) level in Adopted Levels; from a 5489 level in 1998Ch04 
M$inconsistent with M1 from |g|g(DCO) and |g|g(pol) in 2014Ku04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$a 792.0|g placed from 5024, (15-) (E2) and a 792.3|g from 6404, (17-) in Adopted Levels; from 3814, (11+) in 1998Ch04 
M$inconsistent with Q from |g|g(DCO) in 1998Ch04 and E2 from |g|g(DCO) and |g|g(pol) for 792.0|g in 2014Ku04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$a 1379.7|g placed from 6404, (17-) level in Adopted Levels; from 5194, (13+) level in 1998Ch04 
M$inconsistent with Q from |g|g(DCO) in 1998Gh07 and E2 from |g|g(DCO) and |g|g(pol) in 2014Ku04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$a 933.6|g placed from 7337, (19-) level in Adopted Level; from a 6127, (15+) level in 1998Ch04 
M$inconsistent with Q from |g|g(DCO) in 1998Ch04 and E2 from |g|g(DCO) and |g|g(pol) in 2014Ku04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$discrepant with 1361.9|g placed from 6909, (17+) in Adopted Levels 
M$consistent with (Q) from |g|g(DCO) in 1998Ch04 but inconsistent with D in 2014Ku04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$a 889.6 placed from 1290, (7+) level and a 888.4 from 2512, (9+) level in Adopted Levels; not seen in 1998Ch04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$inconsistent with Q (|DJ=2) from |g|g(DCO) in 1998Gh07 and E2 (|DJ=2) from |g|g(DCO) and |g|g(pol) in 2014Ku04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$inconsistent with D (|DJ=1) from |g|g(DCO) in 1998Gh07 but consistent with E2 from |g|g(DCO) and |g|g(pol) in 2014Ku04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$|g placed from 5024, (15-) level in Adopted Levels; from a 4036, (11-) level in 1998Gh07 
M$inconsistent with D (|DJ=1) from |g|g(DCO) in 1998Gh07 but consistent with E2 from |g|g(DCO) and |g|g(pol) in 2014Ku04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
M$inconsistent with Q (|DJ=2) from |g|g(DCO) in 1998Gh07 but consistent M1 from |g|g(DCO) and |g|g(pol) in 2014Ku04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$|g placed from a 5496 level in 1998Gh07 
M$inconsistent with Q (|DJ=2) from |g|g(DCO) in 1998Gh07 and 2014Ku04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$|g placed from 6404, (17-) level in Adopted Levels; from 5417, (12-) level in 1998Gh07, 
M$inconsistent with D (|DJ=1) from |g|g(DCO) in 1998Gh07 but consistent with E2 from |g|g(DCO) and |g|g(pol) in 2014Ku04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$|g placed from a 4001 level in 1998Gh07 
M$inconsistent with Q from |g|g(DCO) in 1998Gh07 but consistent with M1 from |g|g(DCO) and |g|g(pol) in 2014Ku04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$|g placed from 7337, (19-) level in Adopted Level; from a 6350, (13-) level in 1998Gh07 
M$inconsistent with D (|DJ=1) from |g|g(DCO) in 1998Gh07 but consistent with E2 from |g|g(DCO) and |g|g(pol) in 2014Ku04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$|g placed from 3769, (12+) level in Adopted Level; from a 8848 level in 1998Gh07 
M$inconsistent with D from |g|g(DCO) in 2014Ku04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$POL=+0.10 {I2} 
$Note that this |g has been placed from a 841 level to (2)+ ground state in previous |g-spectroscopy studies based on its original placement by 1983Be63 via (|a,np|g) and (d,3n|g). In Adopted Levels, Gammas, the evaluators have adopted the placement here by 2014Ku04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$In Table I of 2014Ku04, this |g is listed as feeding a 16+ level, but not clear which of the two 16+ levels at 6747 or 6683 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$1983Be63 deduced that 841|g mainly proceeds to the g.s. based on their argument that for each 841|g there were 3.0 |e decays of g.s. but only 0.21 decay of {+98}Rh 3.6-min isomer, from intensity balance of prompt and delayed intensities. However, this argument does not take into account that the isomer decays mostly to the g.s. by %IT=89 reported in 1978Ki17 in {+98}Pd |e decay. In Adopted Gammas, this |g has been placed to a level at 56 keV with J|p=(5)+, proposed by 2014Ku04 in {+75}As({+28}Si,2p3n|g) based on a more detailed level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
|a(K)exp=0.016 {I2}. Uncertainty not given by the author but assumed by the evaluators for deducing |d. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$from level-scheme figure 1 of 2014Ku20 only. In authors' table 1, 124.9|g is listed only from 5826 level 


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 32.66 {I2} from {+100}Pd |e decay (3.63 d) and 32.70 {I2} from (p,n|g). Others: 32.7 {I2} from {+100}Rh IT decay (4.6 min) and ({+6}Li,4n|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$weighted average of 42.08 {I2} from {+100}Pd |e decay (3.63 d) and 42.10 {I2} from (p,n|g). Others: 42.1 {I2} from {+100}Rh IT decay (4.6 min) and 42.1 {I2} from ({+6}Li,4n|g) 
RI$weighted average of 14.7 {I9} from {+100}Pd |e decay (3.63 d) and 13.0 {I8} from (p,n|g). Other: 9.1 from ({+6}Li,4n|g), 13.8 from {+100}Rh IT decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from {+100}Pd |e decay (3.63 d) and (p,n|g). Others: 74.9 {I2} from ({+6}Li,4n|g) and {+100}Rh IT decay 
RI$from (p,n|g). Other: 100 {I6} from {+100}Pd |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [D]
decay_comment:
E,RI$from (p,n|g). Other: E|g=53.52 {I15} from {+100}Pd |e decay, I|g=159 {I40} in {+100}Pd |e decay is discrepant. However, 86.3 level is very weakly populated in |e decay 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E$|g required by |g|g data in (p,n|g) 
TI$estimated (evaluators) from branching ratio in (p,n|g) (1983Bi04). 


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$weighted average of 119.18 {I8} from {+100}Pd |e decay (3.63 d) and 119.2 {I1} from (p,n|g) 
RI$from {+100}Pd |e decay. Other: <43 from (p,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=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$weighted average of 151.88 {I5} from {+100}Pd |e decay (3.63 d) and 151.79 {I2} from (p,n|g) 
RI$from {+100}Pd |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
E$weighted average of 84.00 {I2} from {+100}Pd |e decay (3.63 d) and 84.02 {I2} from (p,n|g) 
RI$from (p,n|g). Other: 100 {I6} from {+100}Pd |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
E$unweighted average of 126.15 {I2} from {+100}Pd |e decay (3.63 d) and 126.05 {I3} from (p,n|g) 
RI$weighted average of 15.0 {I10} from {+100}Pd |e decay (3.63 d) and 15.8 {I7} from (p,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$from ({+7}Li,3n|g). Other: 111.9 {I2} from ({+6}Li,4n|g) 
M$Q from |g(|q) in ({+7}Li,3n|g) and M2 ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 136.0 {I1} from ({+7}Li,3n|g) and 135.7 {I2} from ({+6}Li,4n|g) 
M,MR$from |g(|q) in ({+7}Li,3n|g) and RUL. For |d=0.38, E1+M2 is ruled out by RUL since 136|g appears strongly in prompt spectrum 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$from ({+7}Li,3n|g). Other: 138.0 {I2} from ({+6}Li,4n|g) 
RI$unweighted average of 62 {I7} from ({+7}Li,3n|g) and 90 {I8} from ({+6}Li,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 81.1 {I1} from ({+7}Li,3n|g) and 81.1 {I2} from ({+6}Li,4n|g) 
RI$weighted average of 28 {I5} from ({+6}Li,4n|g) and 26 {I5} from (|a,2np|g). Other: 6.9 {I20} from ({+7}Li,3n|g) is discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted average of 195.2 {I2} from ({+7}Li,3n|g) and 195.1 {I2} from ({+6}Li,4n|g) 
RI$from ({+7}Li,3n|g) and ({+6}Li,4n|g). Other: 100 {I17} from (|a,2np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 218.8 {I3} from ({+36}S,p5n|g), 218.8 {I2} from ({+7}Li,3n|g), and 219.1 {I2} from ({+6}Li,4n|g) 
RI$weighted average of 15.7 {I20} from ({+7}Li,3n|g), 16 {I3} from ({+6}Li,4n|g), and 20 {I9} from (|a,2np|g) 
M$|DJ=0 from |g(|q) (1986Du04) in ({+7}Li,3n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 331.1 {I3} from ({+7}Li,3n|g) and 330.9 {I2} from ({+6}Li,4n|g) 
RI$weighted average of 15.7 {I20} from ({+7}Li,3n|g), 16 {I3} from ({+6}Li,4n|g), and 12 {I4} from (|a,2np|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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
E$weighted average of 383.2 {I3} from ({+7}Li,3n|g) and 383.2 {I2} from ({+6}Li,4n|g) 
RI$weighted average of 39 {I7} from ({+7}Li,3n|g), 22 {I4} from ({+6}Li,4n|g), and 31 {I13} from (|a,2np|g) 
M$|DJ=0 from |g(|q) (1986Du04) in ({+7}Li,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_mixing_ratio_info: ;ERR=LT
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
E$weighted average of 832.0 {I3} from ({+7}Li,3n|g) and 831.8 {I2} from ({+6}Li,4n|g) 
RI$unweighted average of 45 {I7} from ({+7}Li,3n|g) and 27 {I5} from ({+6}Li,4n|g) 
MR$from RUL(M2)=1 and T{-1/2}<0.1 ps. From |g(|q) data in ({+7}Li,3n|g), 1986Du04 give +0.27 {I5}, but the authors point out that the apparent large |d is probably due to a |g ray from an unidentified impurity 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
E$weighted average of 1050.4 {I3} from ({+7}Li,3n|g) and 1051.1 {I2} from ({+6}Li,4n|g) 
RI$from ({+6}Li,4n|g). Others: 100 {I10} from ({+7}Li,3n|g) and 100 {I16} from (|a,2np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$weighted average of 133.1 {I2} from ({+7}Li,3n|g) and 133.0 {I2} from ({+6}Li,4n|g) 
RI$from ({+6}Li,4n|g). Other: 100 {I12} from ({+7}Li,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$weighted average of 516.2 {I3} from ({+7}Li,3n|g) and 516.4 {I2} from ({+6}Li,4n|g) 
RI$weighted average of 23 {I3} from ({+7}Li,3n|g) and 34 {I5} from ({+6}Li,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 326.6 {I3} from ({+7}Li,3n|g) and 326.6 {I2} from ({+6}Li,4n|g) 
RI$from ({+6}Li,4n|g). Other: 100 {I13} from ({+7}Li,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 723.8 {I4} from ({+7}Li,3n|g) and 723 {I1} from ({+6}Li,4n|g) 
RI$weighted average of 53 {I7} from ({+7}Li,3n|g) and 52 {I8} from ({+6}Li,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 468.4 {I2} from ({+7}Li,3n|g) and 468.2 {I2} from ({+6}Li,4n|g) 
RI$from ({+7}Li,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 468.4 {I2} from ({+7}Li,3n|g) and 468.2 {I2} from ({+6}Li,4n|g) 
E,RI$from ({+7}Li,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 937.0 {I3} from ({+7}Li,3n|g) and 936.9 {I2} from ({+6}Li,4n|g) 
RI$from ({+7}Li,3n|g) 
M$ce data give mult=M1,E2, but E2 consistent with band assignment 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$others: 32.72 {I6} (1965Ev05), 32.4 {I2} (1964An07) 
RI$8.6 {I2} (1977KaXX) 
M,MR$from L1/L2/L3=100/57 {I10}/48 {I10} and |a(L)exp=3.4 {I17} (1970An30). Other: K/(L+M)=7.0 {I10} (1964Ro20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
E$others: 42.10 {I5} (1965Ev05), 41.9 {I5} (1964An07) 
RI$other: 17 {I3} (1977KaXX); 1965Ev05 report I(|g+ce)=51 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$others: 74.77 {I8} (1965Ev05), 74.4 {I4} (1964An07). 
RI$others: 69.8 (1965Ev05), 81.1 {I17} (1977KaXX) 
M$from |a(K)exp=0.25 {I14} (1970An30). Others: |a(K)exp=0.42 (1965Ev05), K/(L)=8.4 {I8} (1964An07), K/(L+M)=7.2 {I5} (1964Ro20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [D]
decay_comment:
E$other: 139.72 {I30}, placed from a level at 215 by 1965Ev05 
RI$others: 0.45 {I7} (1977KaXX), 1.2 (1965Ev05) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: S
decay_comment:
$|g required by |g|g data in (p,n|g) 
RI$expected to be highly converted; |a=4.22 if E1. 
TI$estimated (evaluators) from branching ratio in (p,n|g) (1983Bi04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$other: 151.55 {I30} (1965Ev05) 
RI$others: 0.81 {I4} (1977KaXX), 2.5 (1965Ev05) 
M$from the Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$others: 84.00 {I9} (1965Ev05), 83.8 {I4} (1964An07). 
M$|a(K)exp=0.54 (1965Ev05), 0.69 {I23} (1970An30). Others: K/L=9.0 {I9} (1964An07), K/(L+M)=7.1 {I5} (1964Ro20) 
$(84|g)(75|g)(|q): A{-2}=0.173 {I4} (1971Re06). Others: A{-2}=+0.18 {I3} (1965Ev05); 1965Ma34 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$others: 126.07 {I19} (1965Ev05), 126.5 {I5} (1964An07). 
RI$others: 18.0 {I15} (1977KaXX), 33.4 (1965Ev05) 
M$|a(K)exp=0.064 {I13} (1970An30) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
MR$from RUL(M2)=1 and T{-1/2}<0.1 ps. From |g(|q), 1986Du04 give +0.27 {I5}, but point out that the apparent large |d is probably due to an unidentified impurity 
$POL=+0.23 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$POL=+0.04 {I8} 
RI$deexcitation from 1401 level suggested by 1984Ma30 and 1987Bi23, which is consistent with mult=E1. 1986Du04 placed it from a 3581 level. All the intensity is assigned from the 1401 level. It is possible, however, that a weak component may also be from 3581 level 
M$from |a(K)exp 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI$total I|g=14 {I2} divided (evaluators) from intensity balance considerations at 2596 level 
$POL=-0.45 {I9} and |a(K)exp for unresolved doublet 
M$|a(K)exp gives M1,E2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E$from requirement of consistency of |g|g data 
TI$estimated by the authors of 1983Bi04 from |g|g-coin 


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 1965Ev04, 1971Si16 ce s. Others: 157.26 {i3} (1966De06), 157.42 {i5} (1974HeYW), 157.41 {i4} (1985Va15) 
RI$from 1985Va15. Others: 0.29 {i2} (1971Si16) 0.31 {i8} (1974HeYW), 0.27 {i1} (1970Ph04) 
I(ce(K) 157|g)/I(ce(K) 307|g,{+101}Ru)=4.22 {i15} (1971Si16), 4.5 (1965Ev04) 
K/L=3.17 {i5}, L1/L3+L2=1.16 {i4}, L3/L2>2 (1971Si16) 
|a(K)exp=19.9 {i16} (1971Si16). Other: 21.6 {i10} (1970Ph04) 
|a(exp)=30 {i2} (1970Ph04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI from 1970Ph04. Other: 22 {i4} (1972Ny01) calc from I(ce(L))/|a(L) 
MR$from L-subshell ratios (1972Ny01). L1/L2=13.2 {I24}, L1/L3=24 {I6}, L2/L3=1.8 {I6} and L1/M=4.8 {I6}. 
Measured I(ce(L)+ce(M)+ce(N))=61 {i5} (1972Ny01) normalized to I(ce(K) 296|g)=17.0 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from intensity balance about 305 level and I|g<0.26 from and assumption of M1 mult. For E2 one would get I|g<0.18 


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:
RI others: 30.9 {i10} (1970Ph04), 39 {i3} (1974HeYW) 
EKC$others: 0.022 {i1} (1970Ph04) ce(K)/I, K/L=8.18 {i45} (1972Ny01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
RI others: 61.6 {i10} (1970Ph04), 70 {i4} (1974HeYW) 
EKC$others: 0.0031 {i2} (1970Ph04) ce(K)/I|g, K/L=8.51 {i20} (1972Ny01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$see 722.9, doublet: 12.2 {i12} (1970Ph04) apportioned via |g|g-coin spectra. Other: 14.4 {i16} (1974HeYW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$see 1313.5, doublet: 1.5 {i3} (1970Ph04) apportioned via |g|g-coin spectra. Other: 1.4 {i16} (1974HeYW) 
M$|a(K)exp=0.00053 {i11} for the 1311+1313 |g's 


decay_energy_unit: KEV
decay_comment:
$No reliable I|g can be given as maybe contaminated with |g of tantalum observed in {+102}Ru(p,n|g) 


decay_energy_unit: KEV
decay_multipolarity: M4
decay_comment:
E from K- and L-conversion lines 
TI due to very high |a of 98.8|g only ce was observed; therefore, I(|g+ce)(98.8|g)|?Ice(98.8|g) 
M from K/L=2.1 {i2} 


decay_energy_unit: KEV
decay_multipolarity: M4
decay_comment:
Data taken from 1990BiZY. Transition not observed by 1986Du04 
E uncertainty estimated by the evaluators 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
$A{-2}=+0.32 {I8}, A{-4}=-0.03 {I10}, Pol=-0.40 {I12} 
M admixture of M2 from theoretical and systematical point of view very unlikely 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E,RI member of unresolved multiplet at 136 keV 
EKC Sum for 135.55|g and 136.71|g 
RI including contribution from 136.11|g due to tantalum 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI including contribution from 136.11|g due to tantalum 
E member of unresolved multiplet at 137 keV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E member of unresolved multiplet at 137 keV 
EKC Sum for 135.55|g and 136.71|g 
RI including contribution from 136.11|g due to tantalum 


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:
EKC {+103}Ru |b{+-} decay: 143 {I20}, {+103}Rh IT decay: 127 {I6} (1975Cz03), 148 {I18} (1979VaZE) 
ELC {+103}Ru |b{+-} decay: 1060 {I72} 
M from electron conversion coefficients in {+103}Ru |b{+-} decay and {+103}Rh IT 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 from electron conversion coefficients in {+103}Ru |b{+-} decay 
$|a(K)exp=1.74 {I17} |a(L)exp=0.18 {I2} 
$ce(L1)/ce(L2)=12 {I4}; ce(L1)/ce(L3)=41 {I20}; ce(L2)/ce(L3)=3.4 {I20} (1970Pe04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$From 2008KrZX 
MR$from 1977Kr13, 295|g(|q) in Coul. ex. Others: -0.18 {I1} (1955Mc51), -0.17 {I1} (1958Mc02), -0.189 {I10} (1970RoZS), -0.15 {I1} (1972Sa03) 
$|a(K)exp=0.0186 {I16} 


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:
$|a(K)exp=0.0048 {I5} 
MR from low temperature nuclear orientation and |g(|q) in {+103}Ru |b{+-} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp=0.0026 {I2} 
MR from low temperature nuclear orientation and |g(|q) in {+103}Ru |b{+-} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
RI$from I(|g+ce) and |a. |a=theory times 0.975 {I10} (1990Ne01). Others: 0.073 {I6} (1969Zo02), 0.072 {I8} (1970NiZV), 0.060 {I6} (1974HeYW) 
E weighted average: 39.755 {I12} (1969Ra18), 39.762 {I16} (1970Pe04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E from 1969Ra18. Other: 53.271 {I30} (1970Pe04) 
RI$others: 0.39 {I3} (1969Zo02), 0.41 {I3} (1974HeYW) 0.42 {I2} (1976Ma37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$I|g=0.280 {I9} (1976Ma37) 
E others: 294.82 {I8} (1970Pe04), 294.72 {I12} (1969Ra18), 294.89 {I8} (1974HeYW) 
CC calculated with |d=-0.17 {I1} (1977Kr13). See also adopted gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1978Mo22. Others: 496.92 {I10} (1970Pe04); 497.08 {I2} (1976Ma37) 
MR from 1983Kr01 
MR others: -0.36 {I8} (1981Ha11); -0.42 {I4} (1981Mu18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$I|g=0.93 {I3} (1976Ma37) 
E others: 557.11 {I13} (1969Ra18), 557.10 {I18} (1970Pe04), 557.08 {I7} (1974HeYW) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E others: 610.41 {I7} (1969Ra18), 610.29 {I19} (1970Pe04), 610.30 {I8} (1974HeYW) 
RI$I|g=6.30 {I20} (1976Ma37) 
RI others: 6.24 {I31} (1969Ra18), 6.2 {I6} (1969Zo02), 6.43 {I13} (1970Pe04), 6.20 {I12} (1975DeYF) 
MR$ or |d: >+11, <-6 (1983Kr01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
Others: 1972Pa10, 1970NiZV, 1969Le17 
CC 1531 {I30} (1975Cz03); 1430 {I89} (1979VaZE) 
L1:L2:L3=2.83 {I6}:70.2 {I14}:100 (1975Ma32), 0.92 {I21}:71.0 {I15}:100 (1972Br02), 1.63 {I25}:69.5 {I6}:100 (1970Pe04), 1.45 {I45}:68.2 {I11}:100 (1969Gr13), 1.26 {I5}:69.7 {I5}:100 (1968DiZZ) 
Deviation of very weak L1-subshell intensity data from E3 theory is attributed might be due to exp analysis (1975Ma32) 
K/(L+M+N+O)=0.0914 {I43} (1975Cz03), 0.0986 {I50} (1967Br04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E from 1969Gr13 
M from L1:L2:L3 ratios and K/L=0.143 {I12} (1969Gr13). Other: K/L=0.135 {I22} (1976Ma37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=-0.186 or +-0.016, A{-4}=0.011 or +-0.018 (1983Ka31) 
$A{-2}=+0.10 {I6}, A{-4}=+0.01 {I5} Pol= +0.06 {I5} (1984Ch06) given for unresolved doublet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=0.223 or +-0.015, A{-4}=-0.024 or +0.024 (1983Ka31) 
$A{-2}=+0.41 {I6}, A{-4}=+0.09 {I5} Pol= -0.6 {I1} (1984Ch06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$A{-2}=-0.175 or +-0.003, A{-4}=0.003 or +-0.045 (1983Ka31) 
$A{-2}=-0.10 {I3}, A{-4}=+0.03 {I5} (1984Ch06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=0.225 or +-0.017, A{-4}=-0.087 or +-0.022 (1983Ka31) 
$A{-2}=+0.25 {I5}, A{-4}=-0.11 {I8} Pol= +0.46 {I8} (1984Ch06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=-0.219 or +-0.041, A{-4}=0.035 or +-0.046 (1983Ka31) 
E$not given by 1984Ch06 although clearly observed by 1983Ka31, 1988De04 and in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=0.101 or +-0.082, A{-4}=-0.082 or +-0.097 (1983Ka31) 
$A{-2}=0.0 {I1} (1984Ch06) given for unresolved doublet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.34 {I6}, A{-4}=-0.10 {I7} Pol= +0.5 {I1} (1984Ch06) 
$A{-2}=0.212 or +-0.015, A{-4}=-0.083 or +-0.019 (1983Ka31) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=0.139 or +-0.028, A{-4}=0.011 or +-0.034 (1983Ka31) 
$A{-2}=+0.26 {I7}, A{-4}=0.01 {I8} Pol= -0.5 {I2} (1984Ch06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.24 {I6}, A{-4}=-0.14 {I9} Pol= +0.47 {I8} (1984Ch06) 
$A{-2}=0.240 or +-0.007, A{-4}=-0.098 or +-0.096 (1983Ka31) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=0.228 or +-0.030, A{-4}=-0.094 or +-0.035 (1983Ka31) 
$A{-2}=+0.18 {I6}, A{-4}=-0.07 {I10} Pol= +0.51 {I10} (1984Ch06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=0.250 or +-0.022, A{-4}=-0.096 or +-0.028 (1983Ka31) 
$A{-2}=+0.45 {I10}, A{-4}=-0.13 {I12} Pol= +0.56 {I12} (1984Ch06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=0.245 or +-0.037, A{-4}=-0.087 or +-0.048 (1983Ka31) 
$A{-2}=+0.45 {I12}, A{-4}=-0.10 {I15} (1984Ch06) 
1983Ka31: excit suggests possible doublet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=0.312 or +-0.060, A{-4}=-0.144 or +-0.077 (1983Ka31) 
$A{-2}=+0.27 {I9}, A{-4}=-0.06 {I12} Pol= +0.2 {I2} (1984Ch06) 
M M1+E2 cannot be excluded (1984Ch06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$A{-2}=-0.169 or +-0.014, A{-4}=0.004 or +-0.015 (1983Ka31) 
$A{-2}=-0.26 {I5}, A{-4}=-0.03 {I8} (1984Ch06) 
M in agreement with |DJ=1 (1984Ch06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=+0.09 {I5}, A{-4}=-0.07 {I5} Pol= +0.10 {I4} (1984Ch06) 
$A{-2}=+0.20 {I5}, A{-4}=-0.20 {I8} Pol= -0.55 {I15} (1984Ch06) given for unresolved doublet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$weighted average of -0.18 {I1} (1955Mc51), -0.17 {I1} (1958Mc02), -0.189 {I10} (1970RoZS), -0.15 {I1} (1972Sa03). Others: -0.58 {I+12-8} (1988Ta23); see also 1955Mc51, 1970RoZS, 1972Sa03, 1978Ba36 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI others: 73 (1971GrXO), 103 {I14} (1969WaZU) 
MR$from 1977Kr13. -0.14 {I6} or +0.21 {I8} (1988Ta23) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$ From {+103}Rh decay dataset in ENSDF database, not determined in 2010Kr05 due to impurity line from {+192}Ir. 
RI$ deduced by the compilers from adopted dataset for {+103}Rh in ENSDF database. 2010Kr05 and {+103}Ru |b{+-} decay dataset in ENSDF database give <0.01 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
M$from ce measurements in 2018Ni14 
$|a(tot)exp=1428 {I13} in {+103}Ru |b- decay 
$2018Ni14 also obtain |a(K)exp + (1+|a(tot)exp)P{-ec,K}=1383 {I28} following the |e decay of {+103}Pd 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$in {+105}Ru |b{+-}decay value is much smaller than the 9.6 value in {+100}Mo({+11}B,|a2n|g). Latter value probably contaminated by other |g-rays 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.0107 {I17} (1967Sc01), |a(K)exp=0.0131 {I78} (1980ViZV). 
M$from |a(K)exp=0.0107, 1967Sc01 conclude that 326|g is pure M1. This is impossible because J|p=5/2- for 455 keV state and J|p=1/2- for 129 keV state. E2 character in agreement with |g|g(|q) results of 1979Sa23. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
EKC$Other: 0.0017 {I3} (1980ViZV) 
MR$from |g(|q) in oriented {+105}Ru |b{+-} decay (1976Ba39). Other: |d=-0.17 {I+5-15} from I|g(|q,H,t,t) by 1981Ha11 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$>282 {I8}: total intensity of feeding |g rays divided by |a(149|g) 
M$R{-DCO}=0.74~{I16} in {+100}Mo({+11}B,|a2n|g) (2004Al03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$>12.9 {I11}: total intensity of feeding |g rays divided by |a(263|g) 
M$R{-DCO}=0.55~{I10} in {+100}Mo({+11}B,|a2n|g) (2004Al03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
M$|a(K)exp=2.58~{I26}, |a(L)exp=1.10~{I11}, |a(M)exp=0.250~{I25} in 1967Sc01; Other: 1960Ri03 
I$from I(|g+ce) and |a 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=0.062 {i11} (1992PeZX ), 0.07 {i1} (1987Ka29), and 0.09 {i4} (1977Ba57) in {+109}Ru |b{+-} 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,MR$|a(exp)=29 {i3} (1987Ka29), |a(K)exp=13 {i4} (1987Ka29), |a(K)exp=17 {i+10-6} (1992PeZX) in {+109}Ru |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
M$from |a(K)exp=0.07 {i2} (1992PeZX in {+109}Ru |b{+-} decay), but E1+M2 with |d=1.0 {i+4-3} is also possible 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
%I|g=18.4 {I12}, using the calculated normalization. 
M$|a(K)exp=0.062 {i11} (1992PeZX), 0.07 {i1} (1987Ka29), 0.09 {i4} (1977Ba57) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
%I|g=0.44 {I3}, using the calculated normalization. 
M,MR$|a(exp) 29 {i3} (1987Ka29), |a(K)exp=13 {i4} (1987Ka29) and |a(K)exp=17 {i+10-6} (1992PeZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$From 1979Bo26 
%I|g=12.8 {I9}, using the calculated normalization. 
M$|a(K)exp=0.013 {i3} (1992PeZX) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
%I|g=2.42 {I20}, using the calculated normalization. 
M$|a(K)exp=0.07 {i2} (1992PeZX), but E1+M2 with |d=1.0 {i+4-3} is also possible 


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:
M$from Fig. 3 and footnote '1' on page 5 in 2018Bu16. In {+109}Rh Adopted dataset in the ENSDF database, mult=M1+E2, |d=1.4 {I7}. Compilers' note: E-mail communication of Jan 25, 2023 between Dr. Jun Chen (one of the evaluators of A=109 in the ENSDF database) and B. Singh discussed the multipolarity based on |a(K)(exp) data from 1992PeZX (thesis) and concluded that |a(K)exp in 1992PeZX is also consistent with pure E2 within one |s, as pointed out by 2018Bu16. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$From |a(K)exp=0.19 {I4} (from ce data) and |a(K)exp=0.22 {I15} (from Ge(|g)-Ge(|g/x) coincidence data) in 1991Jo11 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$placement not shown in figure 1; also fits between levels 2417-968, the 2417 level is populated in the decay of 0.51-s isomer 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI$total transition intensity is listed as 0.6 {i2} in e-mail reply of Oct 15, 2007 from the first author of 2007Ku23 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other placement from 1945-578 level (2002Ku18) is now omitted since 578 level is populated only in the decay of 0.51-s isomer according to 2007Ku23. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
M$|d|<0.27 
EKC$from |a(K)>1.11 Mult|=E1. From an intensity balance at the 127 level Mult=M1(+E2) with |d|<0.27 


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:
$Theoretical B(E2) value is in good agreement with the experimental observation for 13|'<|g<28|'. The RTRPM calculations give a consistent description of the available experimental data only for |e{-2}=0.26 and |g|?27|'. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
RI I(196|g)/I(349|g)=0.52 {I17} from p-|g spectra gated on 1010-keV protons in {+94}Ag p decay. Other data: 1.0 {I3} from p-|g spectra gated on 790-keV protons in {+94}Ag p decay; 0.18 {I4} from ({+40}Ca,|an|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M DCO in ({+40}Ca,|an|g) suggests Q or D+Q but |g asymmetry in ({+58}Ni,|an|g) is consistent with pure D. Possibly |g is a doublet, as suggested in {+94}Ag p decay (0.39 s). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [E1]
decay_uncertain: ?
decay_comment:
E from {+94}Ag p decay (0.39 s). 
M possibly E1; connects |p=(+) and |p=(-) level sequences. However, see comment on 275|g from 2871 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (D)
decay_comment:
RI$I(196|g)/I(349|g)=1.0 {I3} (from p-|g spectra gated on 790-keV protons) and 0.52 {I17} (from p-|g spectra gated on 1010-keV protons). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M R=0.64 {I9}, implying D multipolarity; however, in {+94}Ag p decay (0.39 s), two placements are suggested for E|g|?276, so this |g may be a doublet in the present work also. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M DCO=1.03 {I13} (984|g+1096|g in gate) suggests Q multipolarity, but DCO is also consistent with a D+Q assignment. It is also possible that |g is a doublet, as suggested in {+94}Ag p decay (0.39 s). 


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$ 2011Br01 quote 100 including internal conversion, but the compilers give it as photon intensity while giving the total conversion coefficient 
$B(E2)(W.u.) deduced by the compilers, 2011Br01 give 2.1 {I1} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
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$ 2011Br01 quote 20 {I4} including internal conversion, but the compilers give it as photon intensity while giving the total conversion coefficient 
$B(E1)(W.u.) deduced by the compilers, 2011Br01 give 3|*10{+-7} {I1} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
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:
RI$ 80 {I4} adjusted to 82 {I4} by the compilers so that the total photon intensities from the 7212 level adds to 100 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
E$From 2017Pa35, but the uncertainty is assigned by the compilers 
RI$From reported I(|g+ce) in 2017Pa35 and |a (by compilers) 
$B(E1)(W.u.)=2.2|*10{+-7} {I5} (by compilers) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E3]
decay_comment:
E$From 2017Pa35, but the uncertainty is assigned by the compilers 
RI$From reported I(|g+ce) in 2017Pa35 and |a (by compilers) 
$B(E3)(W.u.)=0.24 {I4} (by compilers) 


decay_energy_unit: KEV
decay_comment:
E$from 1982Ku15, for {+95}Rh and {+95}Pd gamma rays 
RI$from Adopted Gammas branching ratios, because of the high energy of the gamma ray, conversion is expected to be negligible. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$uncertain because of nonlinear energy response of the spectrum below 100 keV and a possible intensity contribution from neighboring 87.3 keV Pb x-ray. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$summed intensity for the doublet: one from {+95}Ag decay to {+95}Pd and the second from {+95}Pd decay to {+95}Rh 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$assuming that there is no direct feeding to the 6+, |a(exp)=1.41 {I10} obtained from intensity balance and taking 325.2 |g as E2. 


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$weighted average of 862.8 {I1} from {+98}Ag |e decay (47.5 s), 862.48 {I14} from ({+32}S,2p2n|g), and 862.6 {I3} from (|a,2n|g) 
M$Q from |g(|q) in ({+32}S,2p2n|g) and (|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 678.5 {I1} from {+98}Ag |e decay (47.5 s), 678.3 {I6} from ({+32}S,2p2n|g), and 678.3 {I3} from (|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$weighted average of 571.0 {I1} from {+98}Ag |e decay (47.5 s), 570.91 {I10} from ({+32}S,2p2n|g), and 570.6 {I3} from (|a,2n|g) 
M$Q from |g(|q) in ({+32}S,2p2n|g) and (|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$weighted average of 660.7 {I1} from {+98}Ag |e decay (47.5 s), 660.41 {I24} from ({+32}S,2p2n|g), and 660.5 {I3} from (|a,2n|g) 
M$Q from |g(|q) in ({+32}S,2p2n|g) and (|a,2n|g) and M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 871.36 {I14} from ({+32}S,2p2n|g) and 871.6 {I3} from (|a,2n|g) 
M$from |g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M$intensity ratio in ({+58}Ni,2p2|a|g) (1997Ce08) indicates likely mult=stretched quadrupole, but a mixed D+Q is required by the 454|g-434|g-979|g cascade from (11-) to 8+ with mult=stretched dipole for 454|g and 434|g 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$from ({+58}Ni,2p2|a|g) 
M$1997Ce08 in ({+58}Ni,2p2|a|g) propose that it may be a non-stretched dipole based on intensity ratio 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 802.1 {I8} from ({+32}S,2p2n|g) and 801.2 {I3} from (|a,2n|g) 
RI$from ({+58}Ni,2p2|a|g) 
M$from |g(|q) in ({+32}S,2p2n|g) and (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Other: E|g=571.1 {I3}, I|g=53 {I2} (1982Ku15) 
RI$53.0 {I2} in 1982Ku15 could be a misprint, since relative uncertainty=0.2/53.0=0.4% is not realistic, while all others in 1982Ku15 are |>4%. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Other: E|g=1468.1 {I7}, I|g=2.6 {I3} unplaced in 1982Ku15 could correspond to the 1467.5+1467.4 doublet in 2001HuZZ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Other: E|g=1076.6 {I10}, I|g=3.0 {I7} unplaced in 1982Ku15 could correspond mainly to 1075.6|g from 2617 level in 2001HuZZ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$level-energy difference=1468.03 
$Other: E|g=1468.1 {I7}, I|g=2.6 {I3} unplaced in 1982Ku15 could correspond to the 1467.5+1467.4 doublet in 2001HuZZ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Other: E|g=1523.4 {I10}, I|g=1.1 {I3} unplaced in 1982Ku15 could correspond to 1522.4+1521.5 in 2001HuZZ 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$R=1.62 {I16} indicates stretched quadrupole, but |DJ=1, D+Q is likely due to the 454|g-434|g-979|g cascade from (11-) to (8+), with 454|g and 434|g as stretched dipoles (1997Ce08) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$total I|g=26.9 {I4}. Intensity divided (evaluator) on the basis of arrow thickness in figure 1 of 1997Ce08 
$R=0.86 {I2} for doublet indicates mult=dipole 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (M1+E2)
decay_comment:
M,MR$from |g|g(|q) (2009FrZZ) for J(2222)=2 
$B(M1)>0.20 {I+9-5}, B(E2)(W.u.)>1.3 {I+20-11} (2009FrZZ) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E placed between 2137.8-keV and 832.4-keV levels although not in coincidence with 832-keV transition. 


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$weighted average of 665.7 {I1} from {+100}Ag |e decay (2.01 min), 665.50 {I10} from ({+96}Ru,2|a|g), 665.5 {I3} from ({+58}Ni,4p|g), 665.4 {I1} from ({+58}Ni,4p|a|g), 665.0 {I5} from ({+35}Cl,|ap2n|g), 665.32 {I12} from ({+12}C,3n|g), and 665.4 {I2} from ({+3}He,2n|g) 
M$from |g(|q,pol) in ({+12}C,3n|g) and ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), and ce data in |e decay (2.01 m) 


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$weighted average of 750.8 {I1} from {+100}Ag |e decay (2.01 min), 750.50 {I20} from ({+96}Ru,2|a|g), 750.6 {I3} from ({+58}Ni,4p|g), 750.6 {I1} from ({+58}Ni,4p|a|g), 750.0 {I5} from ({+35}Cl,|ap2n|g), 750.48 {I12} from ({+12}C,3n|g), and 750.5 {I2} from ({+3}He,2n|g) 
M$from |g(|q,pol) in ({+12}C,3n|g) and ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2+M1)
decay_comment:
E$unweighted average of 922.3 {I1} from {+100}Ag |e decay (2.01 min), 922.3 {I1} from {+100}Ag |e decay (2.24 min), 921.70 {I10} from ({+96}Ru,2|a|g), and 922.0 {I2} from ({+3}He,2n|g) 
RI$from ({+3}He,2n|g) and ({+96}Ru,2|a|g) 
M,MR$from |g|g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1587.9 {I2} from {+100}Ag |e decay (2.01 min), 1587.3 {I3} from ({+96}Ru,2|a|g), and 1587.4 {I3} from ({+3}He,2n|g) 
RI$weighted average of 72 {I17} from {+100}Ag |e decay (2.24 min), 60 {I5} from ({+3}He,2n|g), 69 {I23} from {+100}Ag |e decay (2.01 min). Other: 33 {I3} in ({+96}Ru,2|a|g) seems discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 337.5 {I3} from ({+96}Ru,2|a|g) and 338.1 {I2} from ({+3}He,2n|g) 
RI$unweighted average of 17.5 {I20} from ({+96}Ru,2|a|g) and 11.0 {I20} from ({+3}He,2n|g) 
M,MR$from |g|g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2+M1)
decay_comment:
E$weighted average of 1260.5 {I1} from {+100}Ag |e decay (2.01 min), 1260.0 {I6} from ({+96}Ru,2|a|g), and 1260.0 {I2} from ({+3}He,2n|g) 
RI$from ({+96}Ru,2|a|g). Other: 100 {I4} from ({+3}He,2n|g) 
M,MR$from |g|g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 639.9 {I1} from {+100}Ag |e decay (2.01 min), 639.5 {I10} from ({+96}Ru,2|a|g), 638.5 {I2} from ({+58}Ni,4p|a|g), 639.0 {I5} from ({+35}Cl,|ap2n|g), and 639.6 {I2} from ({+3}He,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$weighted average of 773.3 {I1} from {+100}Ag |e decay (2.01 min), 773.0 {I7} from ({+96}Ru,2|a|g), 773.2 {I3} from ({+58}Ni,4p|g), 773.2 {I1} from ({+58}Ni,4p|a|g), 773.0 {I5} from ({+35}Cl,|ap2n|g), 773.05 {I12} from ({+12}C,3n|g), and 773.1 {I2} from ({+3}He,2n|g) 
M$from |g(|q,pol) in ({+12}C,3n|g) and ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), and ce data in |e decay (2.01 m). |d(M3/E2)=+0.01 {I5} from |g|g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$poor fit. Level-energy difference=223.06 
E$weighted average of 222.5 {I2} from {+100}Ag |e decay (2.01 min), 221.9 {I3} from ({+96}Ru,2|a|g), and 222.7 {I4} from ({+3}He,2n|g) 
RI$weighted average of 27 {I8} from {+100}Ag |e decay (2.01 min), and 20 {I8} from ({+3}He,2n|g). Other: 89 {I11} in ({+96}Ru,2|a|g) seems discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 353.0 {I5} from {+100}Ag |e decay (2.01 min), 353.6 {I5} from ({+96}Ru,2|a|g), and 352.6 {I2} from ({+3}He,2n|g) 
RI$unweighted average of 26 {I4} from {+100}Ag |e decay (2.01 min), 50 {I7} from ({+96}Ru,2|a|g), and 10 {I5} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 862.5 {I1} from {+100}Ag |e decay (2.01 min), 862.0 {I2} from ({+96}Ru,2|a|g), and 862.0 {I4} from ({+3}He,2n|g) 
RI$from ({+96}Ru,2|a|g). Other: 100 {I8} from {+100}Ag |e decay (2.01 min), 100 {I20} from ({+3}He,2n|g) 
M,MR$from |g|g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1685.8 {I3} from {+100}Ag |e decay (2.01 min), 1686.0 {I8} from ({+96}Ru,2|a|g), and 1685.5 {I4} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
E$weighted average of 1694.0 {I3} from {+100}Ag |e decay (2.24 min) and 1693.4 {I4} from ({+3}He,2n|g) 
M,MR$D(+Q) from |g|g(|q) in ({+3}He,2n|g); (M1(+E2)) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 505.30 {I10} from ({+96}Ru,2|a|g) and 504.8 {I3} from ({+3}He,2n|g) 
M,MR$from |g|g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
E$unweighted average of 190.5 {I5} from {+100}Ag |e decay (2.01 min) and 192.0 {I5} from ({+3}He,2n|g) 
RI$weighted average of 3.2 {I3} from {+100}Ag |e decay (2.01 min) and 8 {I4} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 280.7 {I2} from {+100}Ag |e decay (2.01 min), 280.90 {I20} from ({+96}Ru,2|a|g), 280.4 {I2} from ({+58}Ni,4p|a|g), 280.0 {I5} from ({+35}Cl,|ap2n|g), and 280.5 {I2} from ({+3}He,2n|g) 
RI$weighted average of 69 {I8} from {+100}Ag |e decay (2.01 min), 49 {I11} from ({+96}Ru,2|a|g), 75 {I10} from ({+58}Ni,4p|a|g), 72 {I6} from ({+35}Cl,|ap2n|g), and 72 {I3} from ({+3}He,2n|g) 
M$from ({+58}Ni,4p|a|g) with |DJ=(0), (M1) from |DJ|p 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1053.9 {I1} from {+100}Ag |e decay (2.01 min), 1053.5 {I3} from ({+96}Ru,2|a|g), 1053.8 {I2} from ({+58}Ni,4p|a|g), 1053.0 {I5} from ({+35}Cl,|ap2n|g), and 1053.5 {I2} from ({+3}He,2n|g) 
RI$from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 450.4 {I3} from ({+96}Ru,2|a|g), 450.7 {I2} from ({+58}Ni,4p|a|g), 449.0 {I5} from ({+35}Cl,|ap2n|g), and 450.6 {I5} from ({+3}He,2n|g) 
RI$unweighted average of 12 {I1} from ({+3}He,2n|g), 6.4 {I9} from ({+58}Ni,4p|a|g), and 11.5 {I10} from ({+35}Cl,|ap2n|g). Other: 43 {I5} in ({+96}Ru,2|a|g) seems discrepant. 
M$D from |g|g(|q) in ({+36}S,6n|g), consistent with |DJ=1 


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$weighted average of 1089.40 {I10} from ({+96}Ru,2|a|g), 1089.4 {I9} from ({+58}Ni,4p|g), 1089.3 {I1} from ({+58}Ni,4p|a|g), 1089.0 {I5} from ({+35}Cl,|ap2n|g), 1089.1 {I3} from ({+12}C,3n|g), and 1089.2 {I2} from ({+3}He,2n|g) 
M$from |g(|q,pol) in ({+12}C,3n|g) and ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g). |d(M2/E1)=-0.06 {I4} from |g|g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1115.8 {I2} from {+100}Ag |e decay (2.01 min) and 1115.6 {I5} from ({+3}He,2n|g) 
M$(Q) from |g|g(|q) in ({+3}He,2n|g), |d(O/Q)=-0.10 {I14}; (E2) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$weighted average of 1278.0 {I2} from {+100}Ag |e decay (2.01 min) and 1277.8 {I3} from ({+3}He,2n|g) 
M,MR$from |g|g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1405.3 {I2} from {+100}Ag |e decay (2.01 min) and 1405.2 {I5} from ({+3}He,2n|g) 
M,MR$from |g|g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 528.9 {I1} from {+100}Ag |e decay (2.01 min) and 528.7 {I4} from ({+3}He,2n|g) 
RI$from ({+3}He,2n|g). I|g=167 {I17} in {+100}Ag |e seems discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 953.3 {I5} from {+100}Ag |e decay (2.01 min) and 954.3 {I8} from ({+3}He,2n|g) 
RI$from {+100}Ag |e decay (2.01 min). Other: 5.0 {I20} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2214.3 {I3} from {+100}Ag |e decay (2.01 min) and 2214.1 {I8} from ({+3}He,2n|g) 
RI$from ({+3}He,2n|g). Other: 100 {I25} from {+100}Ag |e decay (2.01 min) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 450.2 {I1} from {+100}Ag |e decay (2.01 min) and 450.0 {I2} from ({+3}He,2n|g) 
RI$from {+100}Ag |e decay (2.01 min). Other: 100 {I10} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 569.5 {I3} from {+100}Ag |e decay (2.01 min) and 568.5 {I5} from ({+3}He,2n|g) 
RI$weighted average of 4.1 {I3} from {+100}Ag |e decay (2.01 min) and 6.0 {I20} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 730.9 {I1} from {+100}Ag |e decay (2.01 min) and 730.6 {I3} from ({+3}He,2n|g) 
RI$from {+100}Ag |e decay, where the 2920 level is strongly populated. I|g=20 {I5} in ({+3}He,2n|g) seems discrepant. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 1503.8 {I2} from {+100}Ag |e decay (2.01 min) and 1503.4 {I4} from ({+3}He,2n|g) 
RI$from {+100}Ag |e decay, where the 2920 level is strongly populated. I|g=30 {I8} in ({+3}He,2n|g) seems discrepant. 
M,MR$from |g|g(|q) in ({+3}He,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$weighted average of 798.7 {I4} from ({+58}Ni,4p|g), 798.6 {I1} from ({+58}Ni,4p|a|g), 798.0 {I5} from ({+35}Cl,|ap2n|g), 798.58 {I14} from ({+12}C,3n|g), and 798.5 {I2} from ({+3}He,2n|g) 
M$from |g(|q,pol) in ({+12}C,3n|g) and ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g). |d(M3/E2)=+0.04 {I5} from |g|g(|q) in ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 516.3 {I1} from ({+58}Ni,4p|a|g), 516.0 {I5} from ({+35}Cl,|ap2n|g), and 516.4 {I3} from ({+3}He,2n|g) 
RI$from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$weighted average of 967.0 {I1} from ({+58}Ni,4p|a|g) and 967.0 {I5} from ({+3}He,2n|g) 
RI$weighted average of 6 {I6} from ({+58}Ni,4p|a|g) and 6 {I5} from ({+3}He,2n|g) 
M$from |g(|q) in ({+58}Ni,4p|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 609.6 {I1} from {+100}Ag |e decay (2.01 min) and 609.0 {I4} from ({+3}He,2n|g) 
RI$from {+100}Ag |e decay (2.01 min). Other: 100 {I20} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 890.4 {I2} from {+100}Ag |e decay (2.01 min) and 890.5 {I4} from ({+3}He,2n|g) 
RI$weighted average of 96 {I11} from {+100}Ag |e decay (2.01 min) and 69 {I10} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 190.4 {I3} from ({+58}Ni,4p|g), 190.3 {I1} from ({+58}Ni,4p|a|g), 190.0 {I5} from ({+35}Cl,|ap2n|g), 189.6 {I3} from ({+12}C,3n|g), and 190.4 {I4} from ({+3}He,2n|g) 
RI$from ({+58}Ni,4p|a|g). Other: 100 {I5} from ({+35}Cl,|ap2n|g) and ({+3}He,2n|g), 100 {I12} from ({+12}C,3n|g) 
M$from |g(|q,pol) ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g), ({+35}Cl,|ap2n|g) and ({+12}C,3n|g), with |DJ=0. 


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$weighted average of 708.0 {I5} from ({+35}Cl,|ap2n|g) and 708.2 {I5} from ({+3}He,2n|g) 
RI$weighted average of 5.7 {I10} from ({+35}Cl,|ap2n|g) and 19 {I10} from ({+3}He,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$weighted average of 989.6 {I6} from ({+58}Ni,4p|g), 988.9 {I1} from ({+58}Ni,4p|a|g), 988.0 {I5} from ({+35}Cl,|ap2n|g), 988.6 {I6} from ({+12}C,3n|g), and 988.8 {I5} from ({+3}He,2n|g) 
RI$unweighted average of 88 {I4} from ({+58}Ni,4p|a|g), 72 {I8} from ({+35}Cl,|ap2n|g), 71 {I4} from ({+12}C,3n|g), and 89 {I8} from ({+3}He,2n|g). Other: 155 {I6} from ({+58}Ni,4p|g) is discrepant 
M$from |g(|q,pol) ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 209.3 {I2} from ({+58}Ni,4p|a|g), 209.0 {I5} from ({+35}Cl,|ap2n|g), and 209.4 {I5} from ({+3}He,2n|g) 
RI$weighted average of 14.9 {I12} from ({+58}Ni,4p|a|g), 9.5 {I24} from ({+35}Cl,|ap2n|g), and 14.0 {I20} from ({+3}He,2n|g) 
M$D from |g(|q) in ({+58}Ni,4p|a|g), |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 726.0 {I1} from ({+58}Ni,4p|a|g), 726.0 {I5} from ({+35}Cl,|ap2n|g), 725.8 {I4} from ({+12}C,3n|g), and 725.9 {I4} from ({+3}He,2n|g). Other: 726.1 {I7} from ({+58}Ni,4p|g) 
RI$from ({+3}He,2n|g). Others: 100 {I9} from ({+58}Ni,4p|a|g), 100 {I10} from ({+35}Cl,|ap2n|g) 
M$Q (|DJ=2) from |g(|DCO) in ({+58}Ni,4p|g), ({+35}Cl,|ap2n|g) and ({+58}Ni,4p|a|g); (E2) from |g(|q) and |g(pol) in ({+12}C,3n|g); M2 is ruled out by RUL, B(M2)(W.u.)<1, since it would require an isomeric half-life (T{-1/2}>5 ns) for the 3231 level which is unlikely. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1042.0 {I1} from ({+58}Ni,4p|a|g), 1042.0 {I5} from ({+35}Cl,|ap2n|g), and 1042.2 {I4} from ({+3}He,2n|g) 
RI$weighted average of 16.1 {I23} from ({+58}Ni,4p|a|g), 17.9 {I24} from ({+35}Cl,|ap2n|g), and 14 {I3} from ({+3}He,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 261.6 {I6} from ({+58}Ni,4p|g), 261.6 {I2} from ({+58}Ni,4p|a|g), 262.0 {I5} from ({+35}Cl,|ap2n|g), and 261.7 {I5} from ({+3}He,2n|g) 
RI$from ({+58}Ni,4p|a|g). Others: 100 {I21} from ({+3}He,2n|g), 100 {I11} from ({+35}Cl,|ap2n|g). 
M$from |g(DCO) in ({+58}Ni,4p|g), consistent with |DJ=(0) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 970.0 {I2} from ({+58}Ni,4p|a|g), 970.0 {I5} from ({+35}Cl,|ap2n|g), and 969.9 {I5} from ({+3}He,2n|g) 
RI$weighted average of 104 {I21} from ({+3}He,2n|g) and 79 {I7} from ({+58}Ni,4p|a|g). Other: 189 {I17} in ({+35}Cl,|ap2n|g) seems discrepant 
M$from |g(DCO) in ({+35}Cl,|ap2n|g) and |g(|q) in ({+58}Ni,4p|a|g), with |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1250.0 {I5} from ({+35}Cl,|ap2n|g) and 1250.6 {I5} from ({+3}He,2n|g) 
RI$weighted average of 72 {I16} from ({+3}He,2n|g) and 50 {I6} from ({+35}Cl,|ap2n|g). This |g is not seen in ({+58}Ni,4p|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1767.7 {I3} from {+100}Ag |e decay (2.01 min) and 1767.6 {I8} from ({+3}He,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$weighted average of 881.2 {I4} from ({+58}Ni,4p|g), 881.1 {I1} from ({+58}Ni,4p|a|g), 881.0 {I5} from ({+35}Cl,|ap2n|g), 881.33 {I18} from ({+12}C,3n|g), and 881.1 {I2} from ({+3}He,2n|g) 
M$from |g(|q,pol) in ({+12}C,3n|g) and ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 647.8 {I1} from ({+58}Ni,4p|a|g), 648.0 {I5} from ({+35}Cl,|ap2n|g), and 647.9 {I6} from ({+3}He,2n|g) 
RI$from ({+58}Ni,4p|a|g) 
M$from |g(|q) in ({+58}Ni,4p|a|g), with |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 857.4 {I1} from ({+58}Ni,4p|a|g) and 857.3 {I6} from ({+3}He,2n|g) 
RI$from ({+58}Ni,4p|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 614.8 {I3} from ({+58}Ni,4p|g), 614.3 {I2} from ({+58}Ni,4p|a|g), and 614.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$unweighted average of 2.8 {I3} from ({+58}Ni,4p|g), 6.2 {I7} from ({+58}Ni,4p|a|g), and 6.0 {I6} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|a|g), consistent with |DJ=(1) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 823.1 {I3} from ({+58}Ni,4p|g), 822.8 {I2} from ({+58}Ni,4p|a|g), 822.0 {I5} from ({+35}Cl,|ap2n|g), and 822.7 {I8} from ({+3}He,2n|g) 
RI$unweighted average of 26.9 {I10} from ({+58}Ni,4p|g), 18.2 {I11} from ({+58}Ni,4p|a|g), and 27 {I3} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |g(|q) in ({+58}Ni,4p|a|g), with |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$weighted average of 876.1 {I3} from ({+58}Ni,4p|g), 875.9 {I1} from ({+58}Ni,4p|a|g), 876.0 {I5} from ({+35}Cl,|ap2n|g), and 876.1 {I8} from ({+3}He,2n|g). Other: 875.5 {I5}, placed from a 8715 level in ({+12}C,3n|g) 
RI$from ({+58}Ni,4p|g). Others: 100 {I5} from ({+58}Ni,4p|a|g) and ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), with |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 1066.0 {I3} from ({+58}Ni,4p|g), 1065.5 {I2} from ({+58}Ni,4p|a|g), and 1066.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 6.6 {I18} from ({+58}Ni,4p|a|g), and 4.9 {I6} from ({+35}Cl,|ap2n|g). Other: 25.9 {I11} from {+46}Ti({+58}Ni,4p|g) seems discrepant 
M$from |g(DCO) and |g(|q) in ({+58}Ni,4p|g), with |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 213.7 {I1} from ({+58}Ni,4p|a|g) and 214.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 10.9 {I22} from ({+58}Ni,4p|a|g) and 5.7 {I19} from ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 861.1 {I3} from ({+58}Ni,4p|g), 861.8 {I2} from ({+58}Ni,4p|a|g), 861.0 {I5} from ({+35}Cl,|ap2n|g), and 862.1 {I3} from ({+12}C,3n|g) 
RI$from ({+58}Ni,4p|a|g). Other: 100 {I10} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g), ({+35}Cl,|ap2n|g) and ({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 276.6 {I6} from ({+58}Ni,4p|g), 276.6 {I2} from ({+58}Ni,4p|a|g), 276.0 {I5} from ({+35}Cl,|ap2n|g), and 277.3 {I5} from ({+12}C,3n|g) 
RI$from ({+58}Ni,4p|g). Others: 100 {I11} from ({+35}Cl,|ap2n|g), 100 {I16} from ({+12}C,3n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g), ({+35}Cl,|ap2n|g), and ({+12}C,3n|g), |g(|q) in ({+58}Ni,4p|a|g), consistent with |DJ=0 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$unweighted average of 967.2 {I10} from ({+58}Ni,4p|g), 967.0 {I5} from ({+35}Cl,|ap2n|g), and 969.1 {I6} from ({+12}C,3n|g) 
RI$unweighted average of 13 {I5} from ({+58}Ni,4p|g), 46 {I4} from ({+35}Cl,|ap2n|g), and 73 {I5} from ({+12}C,3n|g) 
M$from |g(DCO) and |g(|q) in ({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E$weighted average of 542.2 {I5} from ({+58}Ni,4p|g) and 542.2 {I2} from ({+58}Ni,4p|a|g). Other: 540.0 {I5} from ({+35}Cl,|ap2n|g) is discrepant 
RI$from ({+58}Ni,4p|a|g) 
M$from |g(|q) in ({+58}Ni,4p|a|g), |DJ=(1) 


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$weighted average of 616.5 {I2} from ({+58}Ni,4p|g), 615.8 {I3} from ({+58}Ni,4p|a|g), and 616.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 1.90 {I22} from ({+58}Ni,4p|g), 1.6 {I4} from ({+58}Ni,4p|a|g), and 2.2 {I4} from ({+35}Cl,|ap2n|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$weighted average of 892.5 {I4} from ({+58}Ni,4p|g), 892.4 {I1} from ({+58}Ni,4p|a|g), 892.0 {I5} from ({+35}Cl,|ap2n|g), and 891.95 {I16} from ({+12}C,3n|g) 
RI$from ({+58}Ni,4p|g). Others: 100 {I7} from ({+58}Ni,4p|a|g), and 100 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+12}C,3n|g) and ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 633.3 {I3} from ({+58}Ni,4p|g), 633.8 {I1} from ({+58}Ni,4p|a|g), and 633.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$from ({+58}Ni,4p|g). Other: 100 {I17} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+35}Cl,|ap2n|g), consistent with |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 909.8 {I3} from ({+58}Ni,4p|g) and 909.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$from ({+35}Cl,|ap2n|g) (2001Zh26). Other: <18 for an uncertain |g in ({+58}Ni,4p|g) (2000ApZY). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 718.8 {I4} from ({+58}Ni,4p|g), 717.5 {I1} from ({+58}Ni,4p|a|g), and 718.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$unweighted average of 2.35 {I22} from ({+58}Ni,4p|g), 6.8 {I3} from ({+58}Ni,4p|a|g), and 3.0 {I4} from ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$from ({+58}Ni,4p|a|g). Others: 771.0 {I10} from ({+58}Ni,4p|g), 770.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$unweighted average of 2.8 {I7} from ({+58}Ni,4p|g), 2.9 {I3} from ({+58}Ni,4p|a|g), and 4.3 {I4} from ({+35}Cl,|ap2n|g) 
M$from |g(|q) in ({+58}Ni,4p|a|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 809.6 {I4} from ({+58}Ni,4p|g), 809.4 {I1} from ({+58}Ni,4p|a|g), 809.0 {I5} from ({+35}Cl,|ap2n|g) and 809.39 {I14} from ({+12}C,3n|g) (placed from a 4792 level) 
RI$from ({+58}Ni,4p|g). Others: 100 {I5} from ({+58}Ni,4p|a|g), and ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g) and ({+12}C,3n|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 995.7 {I6} from ({+58}Ni,4p|g), 994.3 {I1} from ({+58}Ni,4p|a|g), and 994.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 4.4 {I4} from ({+58}Ni,4p|g), 5.6 {I6} from ({+58}Ni,4p|a|g), and 5.2 {I4} from ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1057.0 {I2} from ({+58}Ni,4p|a|g) and 1056.0 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(|q) in ({+58}Ni,4p|a|g) and |g(DCO) in ({+35}Cl,|ap2n|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 309.8 {I10} from ({+58}Ni,4p|g), 311.4 {I4} from ({+58}Ni,4p|a|g), and 312.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 7.0 {I16} from ({+58}Ni,4p|g), 19 {I6} from ({+58}Ni,4p|a|g), and 16 {I5} from ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 854.0 {I2} from ({+58}Ni,4p|g), 853.7 {I2} from ({+58}Ni,4p|a|g), and 853.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$from ({+58}Ni,4p|g). Others: 100 {I13} from ({+58}Ni,4p|a|g), and 100 {I11} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |g(|q) in ({+58}Ni,4p|a|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+35}Cl,|ap2n|g). Other: 298.0 {I10} from ({+58}Ni,4p|g) 
RI$from ({+58}Ni,4p|g). Other: 154 {I17} in ({+35}Cl,|ap2n|g). |g not reported in ({+58}Ni,p|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 931.1 {I10} from ({+58}Ni,4p|g) and 932.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 45 {I5} from ({+58}Ni,4p|g) and 29 {I9} from ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1207.8 {I10} from ({+58}Ni,4p|g), 1209.1 {I2} from ({+58}Ni,4p|a|g), and 1209.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$from ({+58}Ni,4p|g). Other: 100 {I9} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+35}Cl,|ap2n|g) and ({+58}Ni,4p|g), |g(|q) in ({+58}Ni,4p|a|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 376.0 {I10} from ({+58}Ni,4p|g), 374.6 {I2} from ({+58}Ni,4p|a|g), and 374.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$unweighted average of 11.2 {I7} from ({+58}Ni,4p|g) and 16.1 {I12} from ({+58}Ni,4p|a|g). Other: 26 {I3} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g) and |g(|q) in ({+58}Ni,4p|a|g), |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 526.5 {I1} from ({+58}Ni,4p|a|g) and 526.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$unweighted average of 14.9 {I12} from ({+58}Ni,4p|a|g) and 7.6 {I15} from ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 691.3 {I4} from ({+58}Ni,4p|g), 691.2 {I2} from ({+58}Ni,4p|a|g), 691.0 {I5} from ({+35}Cl,|ap2n|g), and 691.5 {I4} from ({+12}C,3n|g) 
RI$from ({+58}Ni,4p|g). Others: 100 {I6} from ({+58}Ni,4p|a|g), and 100 {I11} from ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g), ({+35}Cl,|ap2n|g) and ({+12}C,3n|g), |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 626.9 {I3} from ({+58}Ni,4p|a|g), 626.0 {I5} from ({+35}Cl,|ap2n|g), and 625.6 {I3} from ({+58}Ni,4p|g) (placed from a 6691 level) 
RI$from ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 593.3 {I10} from ({+58}Ni,4p|g), 591.2 {I2} from ({+58}Ni,4p|a|g), and 591.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 2.78 {I24} from ({+58}Ni,4p|g) and 2.9 {I7} from ({+35}Cl,|ap2n|g). Other: 0.3 {I3} from ({+58}Ni,4p|a|g), 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 805.7 {I4} from ({+58}Ni,4p|g), 805.8 {I1} from ({+58}Ni,4p|a|g), 805.0 {I5} from ({+35}Cl,|ap2n|g), and 805.43 {I18} from ({+12}C,3n|g) (placed from a 3982 level) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g) and ({+12}C,3n|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |DJ=2 
RI$from ({+58}Ni,4p|g). Others: 100 {I5} from ({+58}Ni,4p|a|g) and ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 909.3 {I5} from ({+58}Ni,4p|g), 907.9 {I2} from ({+58}Ni,4p|a|g), and 908.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$unweighted average of 6.7 {I5} from ({+58}Ni,4p|g), 3.9 {I6} from ({+58}Ni,4p|a|g), and 5.5 {I11} from ({+35}Cl,|ap2n|g) 
M$from |g(|q) in ({+58}Ni,4p|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 254.1 {I1} from ({+58}Ni,4p|a|g) and 254.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$from ({+58}Ni,4p|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 945.0 {I6} from ({+58}Ni,4p|g), 945.0 {I2} from ({+58}Ni,4p|a|g), 944.0 {I5} from ({+35}Cl,|ap2n|g), and 945.4 {I4} from ({+12}C,3n|g) 
RI$from ({+58}Ni,4p|a|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g) and ({+12}C,3n|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 466.1 {I5} from ({+58}Ni,4p|g), 465.9 {I1} from ({+58}Ni,4p|a|g), 466.0 {I5} from ({+35}Cl,|ap2n|g), and 467.4 {I5} from ({+12}C,3n|g) 
RI$from ({+58}Ni,4p|g). Others: 100 {I6} from ({+58}Ni,4p|a|g), and 100 {I11} from ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g), ({+12}C,3n|g) and ({+35}Cl,|ap2n|g), |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 992.4 {I1} from ({+58}Ni,4p|a|g) and 992.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 47 {I3} from ({+58}Ni,4p|a|g) and 44 {I4} from ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1157.3 {I10} from ({+58}Ni,4p|g), 1156.7 {I3} from ({+58}Ni,4p|a|g), and 1157.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 13.7 {I19} from ({+58}Ni,4p|g), and 15 {I4} from ({+35}Cl,|ap2n|g). Other: 29 {I5} from ({+58}Ni,4p|a|g) seems discrepant 
M$from |g(DCO) in ({+58}Ni,4p|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+35}Cl,|ap2n|g). Other: 1118.4 {I2} in ({+58}Ni,4p|g) (2000ApZY) probably corresponds to 1116.0|g and 1122.0|g in ({+35}Cl,|ap2n|g) (2001Zh26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 682.0 {I7} from ({+58}Ni,4p|g), 681.2 {I1} from ({+58}Ni,4p|a|g), and 682.0 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) and |g(|q) in ({+58}Ni,4p|g), |g(DCO) in ({+35}Cl,|ap2n|g), |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+35}Cl,|ap2n|g). Other: 323.8 {I10} from ({+58}Ni,4p|g) 
RI$available only from {+46}Ti({+58}Ni,4p|g) (2000ApZY) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 539.8 {I3} from ({+58}Ni,4p|g), 540.5 {I1} from ({+58}Ni,4p|a|g), and 540.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$unweighted average of 14.0 {I23} from ({+58}Ni,4p|g), 15 {I4} from ({+58}Ni,4p|a|g), and 22.6 {I16} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |g(|q) in ({+58}Ni,4p|a|g), |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 752.5 {I6} from ({+58}Ni,4p|g), 752.4 {I1} from ({+58}Ni,4p|a|g), and 753.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$from ({+58}Ni,4p|g). Others: 100 {I8} from ({+58}Ni,4p|a|g), and 100 {I15} from ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1006.5 {I1} from ({+58}Ni,4p|a|g) and 1006.0 {I5} from ({+35}Cl,|ap2n|g). Other: 1006.0 {I19} from ({+58}Ni,4p|g) 
RI$from ({+58}Ni,4p|a|g). Other: 2.3 {I11} from ({+58}Ni,4p|g) ) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+35}Cl,|ap2n|g). 1118.4 {I2} in {+46}Ti({+58}Ni,4p|g) probably corresponds to 1116.0|g and 1122.0|g in ({+35}Cl,|ap2n|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$weighted average of 786.1 {I3} from ({+58}Ni,4p|g), 786.0 {I2} from ({+58}Ni,4p|a|g), and 786.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$unweighted average of 2.59 {I23} from ({+58}Ni,4p|g), 5.4 {I3} from ({+58}Ni,4p|a|g), and 4.2 {I4} from ({+35}Cl,|ap2n|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$weighted average of 997.9 {I1} from ({+58}Ni,4p|a|g) and 998.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 1.7 {I3} from ({+58}Ni,4p|a|g) and 1.7 {I4} from ({+35}Cl,|ap2n|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$weighted average of 1036.1 {I4} from ({+58}Ni,4p|g), 1035.3 {I1} from ({+58}Ni,4p|a|g), 1035.0 {I5} from ({+35}Cl,|ap2n|g) and 1035.87 {I21} from ({+12}C,3n|g) (placed from a 6768 level) 
RI$from ({+58}Ni,4p|g). Others: 100 {I4} from ({+58}Ni,4p|a|g), and 100 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g) and ({+12}C,3n|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 480.2 {I6} from ({+58}Ni,4p|g), 479.4 {I1} from ({+58}Ni,4p|a|g), 479.0 {I5} from ({+35}Cl,|ap2n|g), and 479.6 {I3} from ({+12}C,3n|g) (placed from a 6186 level) 
RI$from ({+58}Ni,4p|g) and ({+58}Ni,4p|a|g). Other: 100 {I11} from ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g), ({+35}Cl,|ap2n|g) and ({+12}C,3n|g), |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+35}Cl,|ap2n|g). Other: 1020 {I3} from ({+58}Ni,4p|g) 
RI$unweighted average of 5.3 {I15} from ({+58}Ni,4p|g) and 10.6 {I21} from ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1230.9 {I6} from ({+58}Ni,4p|g), 1231.8 {I1} from ({+58}Ni,4p|a|g), and 1231.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$unweighted average of 72 {I3} from ({+58}Ni,4p|g), 83 {I4} from ({+58}Ni,4p|a|g), and 57 {I9} from ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1166.93 {I24} from ({+58}Ni,4p|a|g) and 1166.0 {I5} from ({+35}Cl,|ap2n|g). Other: 1164.0 {I10} from ({+58}Ni,4p|g) 
RI$from ({+58}Ni,4p|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E,RI$from ({+58}Ni,4p|a|g). Other: E|g=1379.0 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(|q) in ({+58}Ni,4p|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1422.3 {I6} from ({+58}Ni,4p|g), 1421.8 {I3} from ({+58}Ni,4p|a|g), and 1423.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g), |DJ=2 


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$weighted average of 707.6 {I10} from ({+58}Ni,4p|g), 706.4 {I2} from ({+58}Ni,4p|a|g), and 706.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$unweighted average of 3.3 {I3} from ({+58}Ni,4p|g), 7.1 {I3} from ({+58}Ni,4p|a|g), and 7.7 {I8} from ({+35}Cl,|ap2n|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$weighted average of 940.6 {I4} from ({+58}Ni,4p|g), 940.2 {I1} from ({+58}Ni,4p|a|g), 940.0 {I5} from ({+35}Cl,|ap2n|g), 940.2 {I3} from ({+12}C,3n|g) (placed from a 5732 level) 
RI$from ({+58}Ni,4p|g). Others: 100 {I4} from ({+58}Ni,4p|a|g), and 100 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g) and ({+12}C,3n|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 493.0 {I3} from ({+58}Ni,4p|g) and 492.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g), |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1032.3 {I4} from ({+58}Ni,4p|g), 1032.0 {I1} from ({+58}Ni,4p|a|g), and 1931.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$from |g(DCO) and |g(|q) in ({+58}Ni,4p|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$unweighted average of 1366.7 {I6} from ({+58}Ni,4p|g), 1365.0 {I1} from ({+58}Ni,4p|a|g), and 1364.0 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1071.9 {I6} from ({+58}Ni,4p|g), 1071.2 {I1} from ({+58}Ni,4p|a|g), 1071.0 {I5} from ({+35}Cl,|ap2n|g) and 1071.0 {I5} from ({+12}C,3n|g) (placed from a 7839 level) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g) and ({+12}C,3n|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$from ({+58}Ni,4p|g). Other: 1386.0 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$unweighted average of 1154.1 {I6} from ({+58}Ni,4p|g) and 1155.6 {I4} from ({+58}Ni,4p|a|g) 
M$from |g(DCO) in ({+58}Ni,4p|g), |DJ=1 


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$weighted average of 1388.9 {I6} from ({+58}Ni,4p|g), 1388.0 {I1} from ({+58}Ni,4p|a|g), and 1388.0 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g), |g(DCO) in ({+58}Ni,4p|g) and ({+35}Cl,|ap2n|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$weighted average of 1736.5 {I4} from ({+58}Ni,4p|a|g), 1736.0 {I5} from ({+35}Cl,|ap2n|g), and 1736.6 {I5} from ({+58}Ni,4p|g) (placed from a 13165 level). Other: 1736, placed from a 13159 level in ({+37}Cl,p2n|g) 
RI$from ({+35}Cl,|ap2n|g) 
M$from |g(|q,pol) in ({+58}Ni,4p|a|g), and |g(DCO) in ({+35}Cl,|ap2n|g). But Q from |g(DCO) in ({+58}Ni,4p|g) is in conflict 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 1107.1 {I8} from ({+58}Ni,4p|g), 1107.1 {I1} from ({+58}Ni,4p|a|g), and 1106.0 {I5} from ({+35}Cl,|ap2n|g) (placed from a 11816 level) 
RI$from ({+58}Ni,4p|g) 
M$from |g(DCO) in ({+58}Ni,4p|g), ({+58}Ni,4p|a|g) and ({+35}Cl,|ap2n|g), |DJ=1 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
E$weighted average of 1200.0 {I5} from ({+35}Cl,|ap2n|g), 1200.3 {I2} from ({+58}Ni,4p|a|g), and 1201.1 {I6} from ({+58}Ni,4p|g) (placed from a 9913 level). Other: 1200, placed from a 9913 level in ({+37}Cl,p2n|g) 
M$from |g(DCO) in ({+35}Cl,|ap2n|g) and ({+58}Ni,4p|g). Other: D from |g(DCO) in ({+35}Cl,|ap2n|g) is inconsistent 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$weighted average of 1581.9 {I3} from ({+58}Ni,4p|a|g) and 1582.0 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+35}Cl,|ap2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 609.9 {I6} from ({+58}Ni,4p|g), 609.9 {I1} from ({+58}Ni,4p|a|g), and 609.0 {I5} from ({+35}Cl,|ap2n|g) (placed from a 10709 level). Other: 609, placed from a 13200 level in ({+37}Cl,p2n|g) 
RI$from ({+58}Ni,4p|g). Other: 100 {I5} from ({+58}Ni,4p|a|g) 
M$from |g(DCO) and |g(|q) in ({+58}Ni,4p|g), |g(DCO) in ({+58}Ni,4p|a|g) and ({+35}Cl,|ap2n|g), |DJ=1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1718.2 {I5} from ({+58}Ni,4p|g), 1716.9 {I3} from ({+58}Ni,4p|a|g), and 1717.0 {I5} from ({+35}Cl,|ap2n|g) 
RI$weighted average of 45.5 {I20} from ({+58}Ni,4p|g), 74 {I12} from ({+58}Ni,4p|a|g), and 44 {I11} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1293.0 {I1} from ({+58}Ni,4p|a|g), 1294.1 {I3} from ({+58}Ni,4p|g) (placed from a 14459 level), and 1293.0 {I5} from ({+35}Cl,|ap2n|g) (placed from a 14451 level) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1384.0 {I1} from ({+58}Ni,4p|a|g), 1384.0 {I5} from ({+35}Cl,|ap2n|g), and 1383.9 {I5} from ({+58}Ni,4p|g). Other: 1383, placed from a 12591 level in ({+37}Cl,p2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|a|g) and ({+35}Cl,|ap2n|g), |DJ=2. But |DJ=1, D from |g(DCO) in ({+58}Ni,4p|g) is inconsistent 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 1752.6 {I5} from ({+58}Ni,4p|a|g) and 1752.0 {I5} from ({+35}Cl,|ap2n|g) 
M$from |g(DCO) in ({+35}Cl,|ap2n|g), |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 558.1 {I1} from ({+58}Ni,4p|a|g), 558.0 {I5} from ({+35}Cl,|ap2n|g) (placed from a 15009 level), and 558.7 {I7} from ({+58}Ni,4p|g) (placed from a 15016 level). 
RI$from I|g(558|g)/I|g(1851|g)=(0.84 {I5})/(0.79 {I4}) in ({+58}Ni,4p|g). Other: 100 {I16} from ({+58}Ni,4p|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1852.0 {I4} from ({+58}Ni,4p|a|g), 1852.0 {I5} from ({+35}Cl,|ap2n|g) (placed from a 15009 level), and 1850.1 {I3} from ({+58}Ni,4p|g) (placed from a 15016 level). 
RI$weighted average of 111 {I16} in ({+58}Ni,4p|a|g) and 94 {I5} in ({+58}Ni,4p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 1511.0 {I1} from ({+58}Ni,4p|a|g), 1510.5 {I5} from ({+35}Cl,|ap2n|g) (placed from a 13158 level), and 1508.9 {I6} from ({+58}Ni,4p|g) (placed from a 10227 level). Other: 1510, placed from a 11423 level in ({+37}Cl,p2n|g) 
M$from |g(DCO) in ({+58}Ni,4p|a|g) and ({+35}Cl,|ap2n|g), |DJ=1. But |DJ=2, Q from |g(DCO) in ({+58}Ni,4p|g) is inconsistent 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 1587.7 {I3} (1980Ha20). 1980Ha20 assigned this |g ray to {+100}Ag |e decay (2.24 min) only 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
$This |g is expected to exist because of the (751|g)(353|g)-coin relationship. It is obscured by the annihilation radiation 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 773.3 {I2} (1980Ha20) 
RI$weighted average of 23.0 {I11} (1980Ha20) and 24.5 {I18} (1983Ra10) 
M$|a(K)exp=0.0016 {I2} (1983Ra10) gives mult=M1,E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 353.0 {I5} (1980Ha20) and 352.9 {I6} (1983Ra10) 
RI$unweighted average of 0.6 {I2} (1980Ha20) and 1.03 {I7} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1686.0 {I3} (1980Ha20) and 1685.6 {I3} (1983Ra10) 
RI$weighted average of 8.1 {I6} (1980Ha20) and 7.1 {I7} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 280.7 {I2} (1980Ha20) and 280.6 {I2} (1983Ra10) 
RI$unweighted average of 10.5 {I5} from (1980Ha20) and 8.3 {I5} from (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 1053.8 {I2} (1980Ha20) 
RI$weighted average of 13.4 {I8} (1980Ha20) and 13.9 {I11} (1983Ra10) 
$(1054|g)(751|g)(|q) data (1983Ra10) consistent with J(2470)=4,5,6 with somewhat better |h{+2} fit for J=5,6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$other: 1115.7 {I2} (1980Ha20) 
RI$weighted average of 4.3 {I4} (1980Ha20) and 3.4 {I6} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 1956.0 {I7} (1980Ha20) 
RI$unweighted average of 1.3 {I3} (1980Ha20) and 0.5 {I2} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2013.0 {I10} (1980Ha20) and 2013.7 {I10} (1983Ra10) 
RI$weighted average of 0.3 {I2} (1980Ha20) and 0.4 {I1} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 955.0 {I5} (1980Ha20) 
RI$weighted average of 0.2 {I1} (1980Ha20) and 0.10 {I3} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2214.8 {I5} (1980Ha20) and 2214.1 {I3} (1983Ra10) 
RI$unweighted average of 1.9 {I3} (1980Ha20) and 1.2 {I2} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 450.3 {I2} (1980Ha20) 
RI$weighted average of 19.1 {I11} (1980Ha20) and 17.6 {I10} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 730.9 {I2} (1980Ha20) 
RI$weighted average of 7.9 {I12} (1980Ha20) and 7.6 {I6} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 1503.9 {I2} (1980Ha20) and 1503.7 {I2} (1983Ra10) 
RI$weighted average of 13.6 {I7} (1980Ha20) and 11.4 {I15} (1983Ra10) 
$(1504|g)(751|g)(|q) (1983Ra10) consistent with J(2921)=4,5,6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 890.5 {I2} (1980Ha20) and 890.3 {I2} (1983Ra10) 
RI$weighted average of 3.6 {I8} (1980Ha20) and 2.6 {I2} (1983Ra10) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$this |g is not reported in the decay of {+100}Ag g.s. but reported in the decay of 2.24-min isomer (2.24 min). Quoted intensity is deduced by evaluators from the branching ratio in {+100}Ag |e decay (2.24 min) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1820.8 {I8} (1980Ha20) and 1819.7 {I3} (1983Ra10) 
RI$unweighted average of 1.5 {I3} (1980Ha20) and 0.5 {I2} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1767.9 {I4} (1980Ha20) and 1767.6 {I3} (1983Ra10) 
RI$weighted average of 1.0 {I3} (1980Ha20) and 0.7 {I2} (1983Ra10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2+M1)
decay_comment:
E$other: 922.2 {I2} (1980Ha20). 
RI$weighted average of 8.4 {I26} (1983Ra10) and 11.0 {I20} (1980Ha20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 1587.7 {I3} (1980Ha20). 
RI$weighted average of 6.2 {I20} (1983Ra10) and 8.0 {I17} (1980Ha20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
E$weighted average of 1693.9 {I3} (1983Ra10) and 1694.1 {I3} (1980Ha20) 
RI$weighted average of 17.1 {I20} (1983Ra10) and 14.0 {I30} (1980Ha20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1956.0 {I4} (1983Ra10) and 1956.0 {I7} (1980Ha20). It is unplaced in 1980Ha20 
RI$weighted average of 2.3 {I15} (1983Ra10) and 4.9 {I11} (1980Ha20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2118.1 {I4} (1983Ra10) and 2119.0 {I5} (1980Ha20). It is unplaced in 1980Ha20 
RI$weighted average of 13.0 {I30} (1983Ra10) and 10.9 {I15} (1980Ha20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1819.7 {I3} (1983Ra10) and 1820.8 {I8} (1980Ha20). It is unplaced in 1980Ha20 
RI$weighted average of 4.8 {I24} (1983Ra10) and 5.6 {I11} (1980Ha20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$placement from 10452, (20)+ in the Adopted Levels, Gammas 
M$|DJ=2, quadrupole from DCO=1.1 {I2} is in conflict with |DJ=1, E1 from |g(|q,pol) in 2001Pe05 and |DJ=1 in 2001Zh26 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$doublet in the Adopted Gammas. The second component is placed from a 6457 level. 
RI$other: <99 (1981Pi02 at 56 MeV) 
$A{-2}=+0.290 {I10}, A{-4}=-0.068 {I15} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
RI$other: <17 (1981Pi02 at 56 MeV) 
M,MR$from |g(|q) and DCO, consistent with |DJ=0, dipole 
$A{-2}=+0.306 {I22}, A{-4}=-0.005 {I32} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$other: 5.25 {I21}, corrected for 4% contribution from a{+103}pd transition (1981Pi02 at 56 MeV) 
M$M2 is proposed by 1981Pi02 from Pol=-0.33 {I37}, but E2 is proposed in {+50}Cr({+58}Ni,4p|a|g),{+70}Zn({+36}S,6n|g) (2001Pe05) from POL=+1.1 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.288 {I18}, A{-4}=-0.116 {I26} 
RI$other: 41.8 {I18}, corrected for 10% contribution from a {+99}Pd transition (1981Pi02 at 56 MeV) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$A{-2}=+0.31 {I3}, A{-4}=-0.04 {I4} 
E$placement from a 5669, 13- level in the Adopted Levels, Gammas 
RI$other: 6.6, corrected for 31% contribution from a transition in {+101}Pd (1981Pi02 at 56 MeV) 
M$|g(|q,pol) and |g|g(DCO) from 1981Pi02 consistent with E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_uncertain: ?
decay_comment:
$A{-2}=+0.46 {I8}, A{-4}=-0.15 {I12} 
E$this transition is uncertain since not reported in other studies 
RI$other: 4.70 {I23}, corrected for 7% contribution from a {+103}Pd transition (1981Pi02 at 56 MeV) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$A{-2}=+0.358 {I17}, A{-4}=-0.102 {I25} 
RI$other: 20.7, corrected for 15% contribution from a {+99}Rh and 10% from {+101}Pd transitions (1981Pi02 at 56 MeV) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
$A{-2}=+0.34 {I4}, A{-4}=-0.06 {I6} 
E$placement from a 4864, 11- level in the Adopted Levels, Gammas 
RI$other: 12.4 {I4} (1981Pi02 at 56 MeV) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$A{-2}=+0.29 {I5}, A{-4}=-0.15 {I7} 
E$placement from a 7645, (17)- level in the Adopted Levels, Gammas. 
RI$other: 3.8 {I8} (1981Pi02 at 56 MeV) 
M$|g(|q,pol) and |g|g(DCO) from 1981Pi02 consistent with (E2) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_uncertain: ?
decay_comment:
$A{-2}=+0.03 {I9}, A{-4}=-0.09 {I13} 
E$placement from a 6939, (16)+ level in the Adopted Levels, Gammas. 
RI$other: 3.7 {I3} (1981Pi02 at 56 MeV) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
$A{-2}=+0.29 {I7}, A{-4}=-0.02 {I10} 
E$placement from a 6705, 15- level in the Adopted Levels, Gammas. 
RI$other: 8.0 {I4} (1981Pi02 at 56 MeV) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
E$Placement from a 8716, (19)- level in the Adopted Levels, Gammas. 
RI$other: <4 (1981Pi02 at 56 MeV) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$placement from a 4054, 9- level in the Adopted Levels, Gammas. 
RI$other: <28 (1981Pi02 at 56 MeV) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from |e decay. I|g=33 in ({+12}C,3n|g). Also placed from 1266 in ({+12}C,3n|g). If branching is correct, then I|g(327|g from 588 in |e decay)=17.4 {I16} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$the evaluator assumes that the 2396 in ({+3}He,|a|g) corresponds to the 2393 level in |e decay. So the 991,1457,1729,1808 are lowered by 3 keV to agree with the |e decay E|g value for 2131.8 


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$deduced from intensity balance at E(level)=80. Analogs: |d=+0.11 {i3} (119 keV,{+103}Pd), +0.08 {i2} (280 keV,{+105}Pd) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$from on-line nuclear orientation in 12.9-min {+102}Ag decay (1987Wo04) 
B(E2)(W.u.),|b(M1)(W.u.): deduced from B(E2) (J=2 to second 2+) in Coul. ex. and adopted decay properties of 1534 level 
|d from {+102}Ag |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
B(E2)(W.u.): deduced from B(E2) (J=2 to 2') in Coul. ex. and adopted decay properties of 1534 level 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
From Coul. ex. |r{+2}(J=second 0+ to 0)=4.0|*10{+-3} 
$ q{-K}{+2}(E0/E2) > 2, X(E0/E2) > 0.0048, |r{+2}(E0)=0.004 {I15} (2005Ki02, evaluation) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
From Coul. ex. |r{+2}(J=third 0+ to 0)<0.3|*10{+-3} 
$ q{-K}{+2}(E0/E2) < 0.0014 , X(E0/E2) < 0.00038 |r{+2}(E0) < 0.002 (2005Ki02, evaluation) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
The relative order of the 756.7|g and 701.22|g is not established, and the reverse ordering would define a level at 3945.0 rather than at 3889.5 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from |g-intensity balance at 1276 level (J|p=4+), since no (|e+|b{++})-feeding is expected to this level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$13% of the intensity is an unresolved transition in {+101}Pd 
$A{-2}/A{-0}=+0.305 {I10}, A{-4}/A{-0}=-0.092 {I10}, Pol=0.454 {I14} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}/A{-0}=-18 {I12}, A{-4}/A{-0}=+0.03 {I12} $ Pol=0.45 {I15} 
$Pol for multiplet between 600 and 700 keV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}/A{-0}=-0.09 {I4}, A{-4}/A{-0}=+0.19 {I11}, Pol=-0.16 {I20} 
RI for an unresolved multiplet. 
$Pol for multiplet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI for an unresolved multiplet. 
$A{-2}/A{-0}=+0.236 {I29}, A{-4}/A{-0}=-0.048 {I42}, Pol=0.49 {I20} 
$Pol for multiplet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$A{-2}/A{-0}=-0.042 {I21}, A{-4}/A{-0}=-0.040 {I31}, Pol=0.306 {I28} 
RI for an unresolved multiplet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}/A{-0}=+0.20 {I3}, A{-4}/A{-0}=-0.09 {I5}, Pol=0.379 {I24} 
RI$2.4% of the intensity is an unresolved transition in {+103}Pd 
$Pol for multiplet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
$A{-2}/A{-0}=+0.236 {I29}, A{-4}/A{-0}=-0.048 {I45}, Pol=0.49 {I8} 
RI for an unresolved multiplet. 
$Pol for multiplet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}/A{-0}=-0.042 {I21}, A{-4}/A{-0}=-0.040 {I31}, Pol=0.306 {I28} 
$Pol for multiplet 
RI for an unresolved multiplet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}/A{-0}=+0.236 {I29}, A{-4}/A{-0}=-0.048 {I42}, Pol=0.49 {I8} 
RI for an unresolved multiplet. 
$Pol for multiplet 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}/A{-0}=+0.226 {I66}, A{-4}/A{-0}=-0.0141 {I98}, Pol=0.39 {I25} 
RI$1.4% of the intensity is an unresolved transition in {+103}Pd and 9.0% is due to a transition in {+99}Ru 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$A{-2}/A{-0}=+0.05 {I12}, A{-4}/A{-0}=-0.14 {I17}, Pol=0.20 {I32} 
E not observed in other experiments. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Unresolved doublet (see also 1534.5-keV level) 
RI about 1/4 of the 978-keV intensity was seen to be coincident with the 835-keV transition. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2+M1
decay_comment:
|d|>15. This is the same lower limit as that from 1976Gr12 in (HI,xn|g). The second value, |d|?0.24 (1976Gr12), is excluded on the basis of (p,p'|g) results. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR from 1975Ki13 via 244|g linear pol. Other: -0.10 {I5} (1974Gr07) via |g(|q), -0.12 {I4} (1987Ja01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M$M1 excluded if J|p initial and final levels are correct 
$|a(K)exp=0.0023 {I7} 
|a(K)(M1)=0.0030; |a(K)(E2)=0.0030 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Branching: I|g(358|g)/I|g(625|g)=0.45 {I16} ({+103}Ag decay) is in disagreement with adopted value of 0.05 for the same ratio in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI computed from doublet I|g=21 and I|g(380|g)/I|g(885|g)|?0.35 
|a(K)exp=0.0096 {I9} (doublet) |a(K)=0.00957 for M1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-22}=-0.271 {I8}, A{-44}=0.019 {I6} 
$Pol=-0.18 {i6} (1974Gr07) 
MR from linear pol (1975Ki13); other: -0.10 {I5} (1974Gr07) via |g(|q) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-22}=-0.577 {I18}, A{-44}=0.054 {I12} 
$Pol=0.06 {i6} (1974Gr07) 
MR from 532|g linear pol (1975Ki13); other: -0.7 {I3} |g(|q) (1974Gr07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$Pol=0.18 {i6} (1974Gr07) 
$A{-22}=-0.452 {I26}, A{-44}=0.078 {I32} 
MR$-1.4 {I2} or -0.50 {I20} (1974Gr07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_comment:
$Pol=-0.23 {i13} (1974Gr07) 
$A{-22}=0.165 {I30}, A{-44}=-0.090 {I35} 
M from 541|g linear pol (1975Ki13) and |a(K)exp=0.0135 (1975Di09) (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g from (|a,n|g), I|g from experimental branching ratio via (|a,n|g) (1974Gr07) 0.0118 {I17} 
$Pol=0.41 {i34} (1974Gr07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-22}=-0.714 {I50}, A{-44}=0.006 {I53} 
Branching: I|g(900|g)/I|g(656|g)=0.5 {I2} ({+12}C,3n|g), 0.46 (|a,n|g); exp branching ratios via (p,n|g) and {+103}Ag |e decay are different 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$Pol=-0.39 {i10} (1974Gr07) 
$A{-22}=-0.154 {I20}, A{-44}=0.019 {I29} 
MR from 332|g linear pol (1975Ki13); other: +0.05 {I3} |g(|q) (1974Gr07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$Pol=-0.11 {i9} (1974Gr07) 
$A{-22}=-0.170 {I12}, A{-44}=0.043 {I15} 
MR from 237|g(|q) 1975Ki13; others: +0.01 {I2} (1974Gr07) |g(|q), +0.17 {I20} (1975Ki13) 237|g linear pol 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$Pol=-0.55 {i11} (1974Gr07) 
$A{-22}=-0.094 {I20}, A{-44}=0.004 {I29} 
MR other: +0.10 {I3} (1975Ki13) 311|g linear pol 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR other: -0.12 {I13} from 256|g linear pol (1975Ki13) 
$A{-22}=0.272 {I26}, A{-44}=0.012 {I35} 
$Pol=-0.21 {i15} (1974Gr07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR other: +0.07 {I5} from 446|g linear pol (1975Ki13) 
$A{-22}=-0.075 {I43}, A{-44}=0.027 {I71} 
$Pol=-0.40 {i16} (1974Gr07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$ footnote for POL value in 2012So06 is a typo 
$POL=-1.2 {I9}. Positive sign in table I is a misprint according to e-mail reply of April 20, 2012 from J. Timar (author of 2012So06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-22}=0.156 {I8}, A{-44}=0.031 {I9} in {+105}Ag |e decay (41.29~d) (1983Si08); Also A{-22}=-0.048~{I10}, A{-44}=0.015~{I10} (1977Ri05) and R{-DCO}=2.19~{I6} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
M$|a(K)exp=0.0209~{I13} in {+105}Ag |e decay (41.29~d) (1970Ka13), 0.020~{I4} (1965Pi01) 
MR$weighted average of 0.178~{I14} (1983Si08) and +0.132~{I8} (1977Wi10); Others: 0.01~{I1} (1977Ri05), +0.07~{I7} (1976Ba39), +0.013~{I3} (1972Be67), +0.035~{I22} (1962Bh03), +0.11~{I3} (1958Ra01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-22}=-0.048~{I10}, A{-44}=0.015~{I10} (1977Ri05); R{-DCO}=2.19~{I6} (1977Ri05) 
M$|a(K)exp=0.0209~{I13} (1970Ka13); 0.016~{I2} (1964Ka23) 
MR$from 1976Ba39; Other: 0.06~{I1} (1977Wi10), 0.01~{I1} (1977Ri05), +0.02~{I4} (1977Ri05) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-22}=0.21~{I4}, A{-44}=0.01~{I5} (1977Ri05); R{-DCO}=1.08~{I19} (1977Ri05) in {+96}Zr({+12}C,3n|g); Also, |a(K)exp=0.013 (1964Ka23) in {+105}Rh |b{+-} decay (35.3 h) and 0.014~{I9} (1970Ka13) in {+105}Ag |e decay (41.29~d) 
MR$weighted average of +0.137~{I9} (1981Al19), +0.11~{I1} (1977Wi10) and +0.091~{I13} (1976Ba39); 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$|a(K)exp=1.17~{I7} (1970Ka13) in {+105}Ag |e decay (41.29~d) 
MR$from (1981Al19) in {+105}Ag |e decay (41.29~d) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-22}=-0.610~{I21}, A{-44}=0.031~{I24} (1977Ri05); R{-DCO}=4.1~{I7} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$weighted average of -0.33~{I13} or -0.20~{I7} (1977Ri05) in {+96}Zr({+12}C,3n|g); Also: -0.2 or -0.3 (1977Wi10) and -0.8~{I+7-4} (1976Ba39) in {+105}Rh |b{+-} decay (35.3 h) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$A{-22}=0.03~{I4}, A{-44}=0.00~{I4} (1977Ri05) in {+96}Zr({+12}C,3n|g); Also |a(K)exp=0.40~{I5} (1970Ka13) in {+105}Ag |e decay (41.29~d) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M$A{-22}=-0.170~{I5}, 0.001~{I1} (1977Ba32); Also, |a(K)exp=0.00090~{I6} (1970Ka13) in {+105}Ag |e decay (41.29~d) 
MR$weighted average of -0.020~{I+5-6} (1977Ba32) and -0.012~{I4} (1981Al19) in {+105}Ag |e decay (41.29~d) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=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:
M$A{-22}=-0.104~{I11}, A{-44}=-0.10~{I10} (1977Ba32) in {+105}Ag |e decay (41.29~d); Also |a(K)exp=0.0122~{I8} (1970Ka13) in {+105}Ag |e decay (41.29~d) 
MR$-0.084~{I7} (1983Si08), and -0.062~{I9} (1981Al19) in {+105}Ag |e decay (41.29~d) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=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:
M$A{-22}=-0.072~{I12}, A{-44}=-0.001~{I16} (1983Si08) and A{-22}=-0.098~{I16}, A{-44}=-0.030~{I45} (1977Ba32) in {+105}Ag |e decay (41.29~d); Also |a(K)exp=0.0094~{I8} (1970Ka13) in {+105}Ag |e decay (41.29~d) 
MR$from 1983Si08 in {+105}Ag |e decay (41.29~d), based on |g-|g(|q); Other: 0.000~{I3} (1977Ba32) in {+105}Ag |e decay (41.29~d) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-22}=0.182~{I17}, A{-44}=0.020~{I25} (1983Si08) and 0.149~{I13}, -0.014~{I20} (1977Ba32) in {+105}Ag |e decay (41.29~d); Also |a(K)exp=0.0083~{I6} (1970Ka13) in {+105}Ag |e decay (41.29~d) 
MR$weighted average of 0.05~{I4} (1983Si08) and +0.10~{I7} (1981Al19) in {+105}Ag |e decay (41.29~d); Other: -0.84~{I+3-17} (1977Ba32) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M$A{-22}=0.043 (32); A{-44}=0.053 (47) (1983Si08) in {+105}Ag |e decay (41.29~d) 
MR$from 1983Si08 in {+105}Ag |e decay (41.29~d), based on |g|g(|q) 


decay_energy_unit: KEV
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-22}=-0.29~{I5}, A{-4}=0.03~{I8} (1977Ri05); R{-DCO}=2.5~{I5} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from 1977Ri05 in {+96}Zr({+12}C,3n|g), based on |g(|q) 
MR$Also: -0.08~{I8} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


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:
M$A{-22}=0.33~{I3}, A{-44}=-0.05~{I4} (1977Ri05); R{-DCO}=1.01~{I18} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.10~{I11}, A{-44}=-0.07~{I4} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from |g(|q) in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.46~{I5}, A{-44}=-0.11~{I7} (1977Ri05), and R{-DCO}=0.92~{I16} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.01~{I3}, A{-44}=0.02~{I4} (1977Ri05) and R{-DCO}=2.4~{I5} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from |g(|q) in {+96}Zr({+12}C,3n|g) (1977Ri05); Also there: -0.04~{I8} (1977Ri05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.334~{I9}, A{-44}=-0.084~{I9} (1977Ri05); R{-DCO}=0.99~{I2} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.33~{I15}, A{-44}=0.21~{I19} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from 1977Ri05 in {+96}Zr({+12}C,3n|g), based on |g(|q) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.346~{I17}, A{-44}=-0.102~{I24} (1977Ri05); R{-DCO}=0.99~{I4} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$A{-22}=-0.108 {I15}; A{-44}=-0.2 {I2} (1983Si08) in {+105}Ag |e decay (41.29~d); Also: |a(K)exp=0.00061~{I7} (1970Ka13) in {+105}Ag |e decay (41.29~d) 
MR$0.03~{I+4-3} (1983Si08) in {+105}Ag |e decay (41.29~d), based on |g|g(|q) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.46~{I5}, A{-44}=0.04~{I6} (1977Ri05) and R{-DCO}=3.1~{I10} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from 1977Ri05 in {+96}Zr({+12}C,3n|g), but also -0.05~{I8} (1977Ri05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.20~{I5}, A{-44}=-0.09~{I7} (1977Ri05) and R{-DCO}=1.2~{I4} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
M$A{-22}=-0.38~{I4}, A{-44}=-0.05~{I5} (1977Ri05) and R{-DCO}=3.9~{I11} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from 1977Ri05 in {+96}Zr({+12}C,3n|g), but also -0.19~{I11} (1977Ri05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.329~{I16}, A{-44}=-0.06~{I21} (1977Ri05) and R{-DCO}=1.15~{I20} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.353~{I10}, A{-44}=-0.104~{I11} (1977Ri05); R{-DCO}=0.96~{I2} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.28~{I4}, A{-44}, -0.08~{I6} (1977Ri05) and R{-DCO}=1.2~{I3} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from DCO measurements in 1977Ri05; Also: 1.0~{I5} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.329~{I16}, A{-44}=-0.096~{I21} (1977Ri05) and R{-DCO}=0.96~{I4} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.436~{I25}, A{-44}=0.01~{I3} (1977Ri05) and R{-DCO}=0.58~{I8} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from DCO and linear pol. in 2019Ti02; Also: +0.46~{I10} or 1.3~{I7} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=1.4~{I7}, A{-44}=-0.4~{I8} (1977Ri05) and R{-DCO}=0.8~{I3} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from {+96}Zr({+12}C,3n|g) (1977Ri05), based on DCO measurements, but also 4~{I4} (1977Ri05) can not be excluded 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.46~{I5}, A{-44}=-0.11~{I7} (1977Ri05) and R{-DCO}=0.9~{I5} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.42~{I3}, A{-44}=-0.04~{I5} (1977Ri05) and R{-DCO}=0.86~{I13} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from 1977Ri05, based on DCO measurements; Alternatively: 0.0~{I5} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.376~{I24}, A{-44}=-0.18~{I3} (1977Ri05) and R{-DCO}=1.0~{I3} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.27~{I8}, A{-44}=-0.01~{I11} (1977Ri05) and R{-DCO}=1.07~{I23} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.283~{I19}, A{-44}=-0.075~{I24} (1977Ri05) and R{-DCO}=1.12~{I4} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.42~{I4}, A{-44}=-0.08~{I5} (1977Ri05) and R{-DCO}=0.93~{I24} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from DCO measurements in 1977Ri05; Alternatively: 0.2~{I6} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.326~{I25}, A{-44}=-0.08~{I4} (1977Ri05)and R{-DCO}=1.02~{I5} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
M$A{-22}=0.28~{I8}, A{-44}=-0.05~{I11} (1977Ri05)and R{-DCO}=1.0 {I3} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from DCO measurements in {+96}Zr({+12}C,3n|g) (1977Ri05), but also 0.08~{I8} (1977Ri05) can not be excluded 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$A{-22}=0.27~{I8}, A{-44}=-0.01~{I11} (1977Ri05) and R{-DCO}=0.7~{I3} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.57~{I6}, A{-44}=0.14~{I8} (1977Ri05) and R{-DCO}=0.62~{I14} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from DCO and linear pol. in 2019Ti02; Also: +0.62~{I18} or 0.8~{I3} from DCO measurements in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.11~{I3}, A{-44}=0.04~{I4} (1977Ri05) and R{-DCO}=1.64~{I18} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from DCO measurements in {+96}Zr({+12}C,3n|g) (1977Ri05), but also 0.13~{I4} can not be excluded (1977Ri05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.37~{I19}, A{-44}=-0.3~{I3} (1977Ri05) and R{-DCO}=1.0~{I4} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.65~{I8}, A{-44}=-0.03~{I12} (1977Ri05) and R{-DCO}=0.58~{I16} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from DCO measurements in {+96}Zr({+12}C,3n|g) (1977Ri05), but also 1.6~{I11} (1977Ri05) can not be excluded 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
M$A{-22}=0.13~{I20}, A{-44}=-0.0~{I3} in {+96}Zr({+12}C,3n|g) (1977Ri05) 
MR$from {+96}Zr({+12}C,3n|g) (1977Ri05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.263~{I23}, A{-44}=-0.10~{I3} (1977Ri05) and R{-DCO}=0.91~{I9} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.05~{I3}, A{-44}=-0.01~{I4} (1977Ri05) and R{-DCO}=1.60~{I17} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from DCO measurements in {+96}Zr({+12}C,3n|g) (1977Ri05), but also 0.11~{I4} (1977Ri05) can not be excluded 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-22}=0.42~{I5}, A{-44}=-0.13~{I8} (1977Ri05) and R{-DCO}=0.8~{I3} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from DCO measurements in {+96}Zr({+12}C,3n|g) (1977Ri05), but also 0.0~{I7} (1977Ri05) can not be excluded 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.28~{I5}, A{-44}=-0.07~{I8} (1977Ri05) and R{-DCO}=1.0~{I3} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.358~{I19}, A{-44} -0.08~{I3} (1977Ri05) and R{-DCO}=1.02~{I5} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=-0.02~{I3}, A{-44}=0.01~{I5} (1977Ri05) and R{-DCO}=1.6~{I3} (1977Ri05) in {+96}Zr({+12}C,3n|g) 
MR$from DCO measurements in {+96}Zr({+12}C,3n|g) (1977Ri05), but also 0.11~{I6} (1977Ri05)can not be excluded 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.36~{I3}, A{-44}=-0.07~{I4} (1977Ri05) and R{-DCO}=1.19~{I12} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-22}=0.8~{I3}, A{-44}=-0.2~{I4} in {+96}Zr({+12}C,3n|g) (1977Ri05) 
MR$from DCO and linear pol. in 2019Ti02; Also: +1.5~{I10} in 1977Ri05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$A{-22}=0.14~{I4}, A{-44}=-0.08~{I5} (1977Ri05) and R{-DCO}=1.54~{I16} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.44~{I3}, A{-44}=-0.11~{I4} (1977Ri05) and R{-DCO}=1.04~{I6} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-22}=0.26~{I3}, A{-44}=-0.02~{I4} (1977Ri05) and R{-DCO}=0.91~{I16} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$A{-22}=0.28~{I4}, A{-44}=-0.08~{I6} (1977Ri05) and R{-DCO}=1.21~{I18} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$A{-22}=0.19~{I8}, A{-44}=-0.11~{I2} (1977Ri05) and R{-DCO}=0.43~{I23} (1977Ri05) in {+96}Zr({+12}C,3n|g) 


