# DECAY

decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ADO=1.12 {I32} 
$ADO ratio seems consistent with |DJ=2, quadrupole rather than with |DJ=1, dipole transition assigned in 2016Li34 (compilers' note) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ADO=1.14 {I27} 
$ADO ratio seems consistent with |DJ=2, quadrupole rather than with |DJ=1, dipole transition assigned in 2016Li34 (compilers' note) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$from |g(|q) and lin pol in {+74}Ge({+18}O,np|g),{+76}Ge({+18}O,3np|g). Other: |d=-0.68 {I5} in ({+11}B,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_uncertain: ?
decay_comment:
M,MR$from |g(|q) and lin pol in {+74}Ge({+18}O,np|g),{+76}Ge({+18}O,3np|g) 
RI$other: 68 {I5} in {+74}Ge({+18}O,np|g),{+76}Ge({+18}O,3np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$from I|g(202|g)/I|g(479|g)=1.072 {I4} (1973Ha18). See comment on 479|g for derivation of I|g(479|g) 
MR$From |a(K)exp=0.0243 {I14} and 479.5|g-202.5|g correlation with A{-2}=-0.178 {I5} and A{-4}=0.009 {I8} (1973Ha18). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4(+E5)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
RI$from I|g(682|g)/I|g(479|g)=0.0035 {I3} (1978Ra05). Other: 0.0040 {I8} (1974Kl06). 
MR$From B(E5)(W.u.)<300. 
CC$|a(exp)=0.101 {I4} from intensity balance, using |a(202)=0.0273 {I3} and measured I|g(202|g)/I|g(479|g)=1.072 {I4} (1973Ha18). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E5
decay_comment:
E$from 1978Ra05. 
RI$from I|g(682|g)/I|g(479|g)=0.0035 {I3} (1978Ra05). Other: 0.0040 {I8} (1974Kl06). 


decay_energy_unit: KEV
decay_multipolarity: M4
decay_comment:
RI 184 {I1} in transient equilibrium (1977Ho12). 
Other |a(K)exp: 0.042 {I3} (1977Ho12), 0.046 {I2} (1953Am08). 
K/(L+M)=6.00 (1953Am08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
|a(K)exp=0.0126 {I10} for the 272.6|g + 274.7|g doublet (weighted average of 0.015 {I4} (1977Ho12) and 0.0125 {I10} (1973Ha11)). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M M1,E2 from |a(K)exp; not M1 from level scheme. 
|a(K)exp: weighted average of 0.00088 {I7} (1977Ho12) and 0.00108 {I9} (1973Ha11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
|a(K)exp=0.0126 {I10} for the 272.6|g+274.7|g doublet dominated by this transition (weighted average of 0.015 {I4} (1977Ho12) and 0.0125 {I10} (1973Ha11)). 
M if 272.6|g is M1,E2 as deduced from level scheme. 


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 M1(+E2) (|d<1.4) from |a(K)exp in {+93}Sr |b{+-} decay. If present, an L=2 component would rule out J=1/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
|a(K)exp: from 1974Ac04; implies mult.=M1(+E2), |d<1.4. 
E from 1979Bo26. Others: 590.28 {I5} (1977Bi01), 590.18 {I6} (1974Ac04). 
%I|g=67.7 {I17} assuming recommended decay scheme normalization. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E from 1979Bo26. Others: 168.69 {I5} (1977Bi01), 168.45 {I6} (1974Ac04; for doublet). 
|a(K)exp: weighted average of 0.72 {I7} (1972Mc04), 0.73 {I5} (1974Sc39), 0.67 {I7} (1974Ac04), 0.81 {I7} (1986Ka20); K/(L+...)=3.62 {I23} (1974Ac04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$A{-2}=+0.12 {I4}, A{-4}=+0.02 {I8} for 584|g-306|g cascade 
MR$other: -0.89 {I30} from |g|g(|q) for 718|g-584|g cascade 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: S
decay_comment:
E,RI$transition not observed but suggested by coincidence relationships. E|g from level energy difference and I|g+ce from intensity balance. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
RI$deduced by evaluator from I(|g+ce)=100. {I55} 5 from 1996Lh03 and 50 (no unc.) from 1996Lh03 would imply I(|g+ce)>100. 
M$|a(K)exp=0.98 {I20} (from |gX/|g|g, 1986Lh01), |a(exp)=1.00 {I19} (from intensity balance at 3361.1-keV level, 1986Lh01). 


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$from {+98}Sr |b{+-} decay. Values from other reactions and decays are in agreement but much less precise. 
M$also supported by |d(Q/D)=0.0 {I2} from |g|g(|q) in SF decay (2017Ur03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
RI$unweighted average of 6.9 {I17} in {+235}U,{+241}Pu(n,F|g) and 2.9 {I12} in {+235}U(n,F|g):delayed |g 
M$|a(K)exp in 2004Br14 gives M1+E2 with |d=0.7 {I4} to 374, 4- level but it contradicts to 49.9|g E1 from 495, 4- level; E1+M2 with |d=0.5 {I2}, but it would require an unreasonably large B(M2)(W.u.) exceeding RUL=1. So it is most probable that 71.3|g is pure E1, by combining all considerations. Note that 71.3|g is very weak (the weakest transition in 2004Br14 and 2017Ur03 also states that this transition is too weak to determine its conversion in their data including {+235}U(n,f|g), {+248}Cm,{+248}Cf SF decay, and {+98}Sr |b{+-} 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:
RI$weighted average of 3.8 {I9} in {+235}U,{+241}Pu(n,F|g) and 4.9 {I7} in {+235}U(n,F|g):delayed |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$from |g|g(|q) in SF decay (2017Ur03), and RUL; (M1) from |a(K)exp in {+235}U,{+241}Pu(n,F|g) (2004Br14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
M,MR$from |a(K)exp in |b{+-} decay (2002PfZZ,1988MaYY). Other: |d(Q/D)=-0.04 {i6}, +0.2 {I2}, +0.04 {I2}, +0.4 {I2} from |g|g(|q) in SF decay (2017Ur03) 


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(total)exp in |b{+-} decay (2017Ur03). Other: |d(E2/M1)>0.22 from |a(K)exp and |a(total)exp in |b{+-} (2002PfZZ,1987Ma58) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M,MR$|a(total)exp=0.3 {I1} in |b{+-} decay (2017Ur03). Other: |d(E2/M1)=0.53 {I16} from |a(total)exp=1.5 {I7} in 2002PfZZ. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$E|g=119.3 {I1} (2017Ur03). I|g=221 {I10} (2002PfZZ), 100 for 119.4|g (1987Ma58). Measured absolute intensity=73 {I6} per 100 decays of {+98}Sr (1987Ma58) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$E|g=428.5 {I1}, I|g=84 {I4} (2002PfZZ). I|g=42 for 428.4|g (1987Ma58) 
$|d(M2/E1)<0.17 
$(428|g)(119|g)(|q): A{-2}=-0.33 {I5}, A{-4}=+0.09 {I8} (2002PfZZ, 1988MaYY,1989BeZG); A{-2}=-0.23 {I6}, A{-4}=+0.07 {I10} (2002PfZZ) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$E|g=444.7 {I1} (2017Ur03). I|g=100.0 {I10} (2002PfZZ), 54 for 444.6|g (1987Ma58). Measured absolute intensity=38 {I3} per 100 decays of {+98}Sr (1987Ma58) 
$(445|g)(119|g)(|q): A{-2}=-0.33 {I5}, A{-4}=+0.06 {I8} (2002PfZZ, TRISTAN); A{-2}=-0.20 {I2}, A{-4}=+0.06 {I3} (2002PfZZ,OSTIS) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$E|g=36.3 {I1}, I|g=32 {I5} (2002PfZZ). I|g=28 for 36.5|g (1987Ma58) 
$|d(M2/E1)<0.04 (2017Ur03,2002PfZZ) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$E|g=52.5 {I1}, I|g=11.2 {I9} (2002PfZZ). I|g=8 for 52.5|g (1987Ma58) 
M,MR$from |a(total)exp (2017Ur03). Other: |d(E2/M1)<0.22 (2002PfZZ,1987Ma58) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$E|g=66.0 {I1}, I|g=3.6 {I6} (2002PfZZ). I|g=2.1 for 66.0|g (1987Ma58) 
M$from |a(total)exp in 2017Ur03. Other: |d(E2/M1)=0.53 {I16} from |a(total)exp in 2002PfZZ, factor of |?5 higher than in 2017Ur03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$from 2002PfZZ, intensity is renormalized to 99.5 for 119.3|g. I|g=0.2 for a tentative 157.7|g in 1987Ma58. This |g is not reported by 2017Ur03, and is not included in Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$from 2002PfZZ, intensity is renormalized to 99.5 for 119.3|g. I|g=0.4 for 224.0 in 1987Ma58. This |g is not reported by 2017Ur03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$from 2002PfZZ, intensity is renormalized to 99.5 for 119.3|g. I|g=0.4 for a tentative 344.1|g in 1987Ma58. This |g is not reported by 2017Ur03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=386.0 {I1}, I|g=10.0 {I10} (2002PfZZ). I|g=6.0 for 386.0|g (1987Ma58) 
RI$uncertainty of 0.1 seems a misprint in 2002PfZZ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$This |g is not confirmed by 2017Ur03, thus treated as uncertain by evaluators, and not included in the Adopted dataset 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$This |g is not confirmed by 2017Ur03, thus treated as uncertain by evaluators, and is not included in the Adopted dataset 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$E|g=119.4 (1998Hw08) 
$|d(Q/D)=0.0 {I2} from (428.6|g)(119.4|g)(|q): A{-2}=-0.16 {I2}, A{-4}=+0.07 {I3} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
MR$from (121.1|g)(204.3|g)(|q): A{-2}=+0.22 {I2}, A{-4}=+0.09 {I4} 
M$large mixing ratio suggests mult=M1+E2 in contrast to E1+M2 
$E|g=121.0 (1998Hw08) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$|d(Q/D)=-0.04 {I6} for J(564)=1, +0.2 {I2} for J(564)=2 from (36.2|g)(444.7|g)(|q): A{-2}=+0.09 {I5}, A{-4}=-0.15 {I9} 
$|d(Q/D)=+0.04 {I2} for J(564)=1, +0.4 {I2} for J(564)=2 from (444.7|g)(119.3|g)(|q): A{-2}=-0.19 {I2}, A{-4}=-0.02 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=229.0 (1998Hw08) 
$|d(Q/D)=+0.31 {I5} or +2.5 {I3} for J(603)=5. |d(O/Q)=0.0 for J(603)=6 from (228.6|g)(204.3|g)(|q): A{-2}=+0.11 {I2}, A{-4}=-0.01 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|a(K)exp also gives E1+M2 with |d=1.1 {I+5-4}, but it would require an unreasonably large B(M2)(W.u.) exceeding RUL=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$|a(K)exp gives M1+E2 with |d=0.7 {I4} to 374, 4- level but it contradicts 49.8|g E1 from 495, 4- level; E1+M2 with |d=0.5 {I2}, but it would require an unreasonably large B(M2)(W.u.) exceeding RUL=1. So it is most probable that 71.3|g is pure E1, by combining all considerations. Note that 71.3|g is very weak (the weakest transition in 2004Br14) and 2017Ur03 also state that this transition is too weak to determine its conversion in their data including {+235}U(n,f|g), {+248}Cm,{+248}Cf SF decay, and {+98}Sr |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
M$|a(K)exp also M1+E2 with |d<0.15; it also gives E1+M2 with |d=1.22 {I4}, but it is inconsistent with |D|p=no 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$8.2 {I8} (2004Br14) 
$|a(exp) gives |d(E2/M1)>1.8; also give E1+M2 with |d=0.95 {I10}, but it would require an unreasonably large B(M2)(W.u.) exceeding RUL=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
ECC$from intensity balance at 171-keV level 
MR$deduced by evaluators from |a(total)exp using the BrIccMixing code 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
ECC$from intensity balance at 446-keV level 
$|d(M2/E1)<0.08 from |a(total)exp, deduced by evaluators 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$large |a values for multipolarities other than E1 or M1 will make this transition almost fully converted which will not allow this transition to be seen as photons. For M1 multipolarity (with |a=15.4), the required |b feeding to the 10.7-keV level would be almost 100% from intensity balance, which is highly unlikely. Thus E1 is the only choice that is consistent with the measured photon intensity of 10.68|g, and intensity balance considerations. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
RI$1985Mu07 give I|g=145. 1987Wo07 were aware of this large discrepancy. Their value of I|g=69 {I5} is a weighted average of three independent measurements. Also a larger value of I|g would imply direct |b{+-} feeding which would be inconsistent with |DJ=2 and |D|p=no 
M,MR$from |a(K)exp=0.53 {I5}, |a(L)exp=0.064 {I10} (1987Wo07) 


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
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$|d{+2}(E2/M1)=0.038 {I3} (deduced by 2017Ha12 from |g-ray branching ratios) 
$Compiler's note: B(E2)(W.u.) is larger than RUL(E2)=300, implying that |d(E2/M1) for 163|g is probably overestimated 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E Transition expected from coincidence data, but not observed in {+58}Ni({+28}Si,|an|g) by 2004Ma39. E|g from level energy difference. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E transition expected from coincidence data, but not observed by 2004Ma39. E|g is rounded value from level energy difference. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$D+Q from |g(|q) in {+58}Ni({+28}Si,2pn|g), E1+M2 excluded by comparison to RUL. 
MR$other: -0.51 from |g(|q) in {+54}Fe({+32}S,2pn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=?
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$D+Q from |g(|q) in {+54}Fe({+32}S,2pn|g), M1+E2 from assumed band structure. 
MR$from |g(|q) in {+54}Fe({+32}S,2pn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=?
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
M$D+Q from |g(|q) in {+54}Fe({+32}S,2pn|g), |D|p=no from level scheme 
MR$from |g(|q) in {+54}Fe({+32}S,2pn|g). 
RI$other: 2 {I1} in {+54}Fe({+32}S,2pn|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(exp)=18 {I10} from intensity balance (1988Hu01). 
M$|a(exp) gives E2 or M2, the latter is excluded by comparison to RUL. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
$|a(exp)= 8 {I4} from intensity balance (1988Hu01). 
M$|a(exp) gives E1 or M1, the latter is excluded by comparison to RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$100 in {+59}Co({+28}Si,p2n|g) (2003Do01) and {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=1.03 {I3}, 1.04 {I4}. A{-2}=+0.23 {I1}, A{-4}=-0.03 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI$8.9 {I6} in {+59}Co({+28}Si,p2n|g) (2003Do01) 
$DCO=1.29 {I10}, 1.02 {I11}. A{-2}=-0.12 {I6}, A{-4}=+0.02 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$79 {I2} in {+59}Co({+28}Si,p2n|g) (2003Do01); 88 {I9} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=0.83 {I2}. A{-2}=+0.36 {I2}, A{-4}=-0.18 {I2} (1993Ch41) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
RI$8.2 {I5} in {+59}Co({+28}Si,p2n|g) (2003Do01) 
$DCO=0.97 {I10}, 1.02 {I10}. A{-2}=+0.23 {I12}, A{-4}=+0.09 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$55 {I2} in {+59}Co({+28}Si,p2n|g) (2003Do01); 63 {I7} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=0.83 {I2}. A{-2}=+0.32 {I3}, A{-4}=-0.16 {I3} (1993Ch41) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$6.1 {I4} in {+59}Co({+28}Si,p2n|g) (2003Do01) 
$DCO=1.05 {I18}, 0.94 {I12}. A{-2}=+0.36 {I8}, A{-4}=-0.09 {I8} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
RI$15 {I1} in {+59}Co({+28}Si,p2n|g) (2003Do01) 
$DCO=0.54 {I7}, 0.63 {I9}. A{-2}=-0.43 {I7}, A{-4}=+0.17 {I8} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$2.8 {I3} in {+59}Co({+28}Si,p2n|g) (2003Do01) 
$DCO=1.05 {I17}. A{-2}=+0.21 {I7}, A{-4}=+0.04 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$32 {I2} in {+59}Co({+28}Si,p2n|g) (2003Do01); 43 {I4} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=0.98 {I5}, 0.95 {I7} (2003Do01). A{-2}=+0.37 {I3}, A{-4}=-0.10 {I4} (1993Ch41) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$5.0 {I5} in {+59}Co({+28}Si,p2n|g) (2003Do01) 
$DCO=1.08 {I11}, 1.15 {I19}. A{-2}=+0.35 {I10}, A{-4}=-0.22 {I10} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI$7.8 {I5} in {+59}Co({+28}Si,p2n|g) (2003Do01), 8.0 {I8} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=0.29 {I4}, 0.35 {I6}. A{-2}=-0.53 {I11}, A{-4}=-0.09 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$2.7 {I4} in {+59}Co({+28}Si,p2n|g) (2003Do01) 
$DCO=0.28 {I6}, 0.34 {I12}. A{-2}=-0.75 {I8}, A{-4}=+0.06 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$|?6 in {+59}Co({+28}Si,p2n|g) (2003Do01), 10.0 {I15} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=1.01 {I3}, 0.97 {I4} for 722.9+723.3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$24 {I2} in {+59}Co({+28}Si,p2n|g) (2003Do01); 41 {I4} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=0.87 {I3}. A{-2}=+0.37 {I3}, A{-4}=-0.10 {I4} (1993Ch41) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$7.6 {I5} in {+59}Co({+28}Si,p2n|g) (2003Do01), 14.0 {I14} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=0.99 {I9}, 0.93 {I13} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$16 {I1} in {+59}Co({+28}Si,p2n|g) (2003Do01); 35 {I4} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=0.99 {I7}, 0.94 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$7.0 {I5} in {+59}Co({+28}Si,p2n|g) (2003Do01), 19.0 {I20} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=1.00 {I9}, 1.08 {I14}. A{-2}=+0.28 {I6}, A{-4}=-0.03 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$7.4 {I7} in {+59}Co({+28}Si,p2n|g) (2003Do01), 16.0 {I16} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=0.94 {I11}, 0.92 {I17} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$5.4 {I6} in {+59}Co({+28}Si,p2n|g) (2003Do01); 18.0 {I20} in {+58}Ni({+29}Si,2pn|g) (1993Ch41) 
$DCO=0.86 {I2} (1993Ch41) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$759 quoted in level-scheme figure 1 of 2006Ch09 does not fit, it is too high by 4-5 keV. The evaluators have decreased energy to 754 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M$A{-2}=+0.27 {I18}, A{-4}=+0.34 {I31} (2006Ch09) consistent with |DJ=1, D+Q, most likely M1+E2 transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$from |a(K)exp in {+85}Nb |e decay (20.5 s); Measured K/L=9.0 {I18} (2005Ka39) gives |d(E2/M1)<0.12 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E3]
decay_comment:
E$because of the observation of 292|g and 417|g with T{-1/2}=10.9 s {I3} where the 417|g belongs to {+85}Y (see {+85}Y Adopted Gammas), this |g has been assigned to {+85}Zr. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
(234|g)(628|g)(|q): A{-2}=+0.26 {I5}, A{-4}=-0.07 {I5} 
(1028|g)(628|g)(|q): A{-2}=+0.47 {I9}, A{-4}=-0.18 {I10} 
(|g)(|q): A{-2}=+0.29 {I3}, A{-4}=-0.07 {I3} 


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$A{-2}=+0.334 {I16}, A{-4}=+0.026 {I21} consistent with |DJ=0, dipole; RUL(E2)=300 suggests |d(E2/M1)<0.17 
A2=+0.30 5, A4=-0.03 6 (1977Ko05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$A{-2}=+0.256 {I20}, A{-4}=-0.024 {I30} consistent with |DJ=0, dipole 
A2=+0.09 12, A4=+0.02 15 (1977Ko05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=?
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR |d=-0.35 or -2.6 from (HI,xn|g), but |a(exp) determined in isomeric decay deviates from |a for |d=-2.6 by more than one standard deviation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_mixing_ratio_info: ;ERR=?
decay_comment:
CC$|a(K)exp=0.049 {i5} and K/L+M=7.07 {i36} from a |b{++} study in 1991Mi15. From this, the authors infer |d=0.72 {i10}. A re-analysis yields |d=0.4 {i4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
CC$|a(K)exp=2.02 {i12} and K/L+M=3.02 {i3} from a |b{++} study in 1991Mi15. This confirms the E3 character 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI Weighted average of 74.0 {I44} (1974Vo03), 71.7 {I40} (1972Tu03), and 60 {I5} (1982DeZQ), and 67 (1986CoZQ), normalized to this value in 1977K05; other: 72 {I4} (1972Tu03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E Adopted 1683.2 {I3} (1974Vo03); others: 1686.0 {I7} (1977Ko05) and is discrepant, 1682.7 (1982De43), and 1684.1 {I23} (1986CoZQ). 
RI Weighted average of 4.2 {I21} (1977Ko05) and 2 {I1} (1982De43); others 15.2 {I5} (1974Vo03) and 2 (1986CoZQ), but with no uncertainties given. The evaluators have opted for a lower intensity values since at least 3 values have consistently low values, whereas the larger value may be due to impurities. Note that the I|g(1683)/(I|g(1067|g + 1884|g)) branching is 0.26 {I6} from 1982De43, 0.21 {I3} from 1974Vo03, 0.09 {I5} from 1977Ko05, and 0.06 from 1986CoZQ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=?
decay_comment:
M A{-2}=+0.17 {I2}, A{-4}=-0.02 {I4} (1978Ar19) 
MR -0.35 or -2.6 from (HI,xn|g) (1978Ar19), but |a(exp) determined in isomeric decay deviates from |a for |d=-2.6 by more than one standard deviation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
RI from I{-|g}(801)=6 and I{-|g}(601)=11 from 1978Ki06, 1978Ar19 give I{-|g}(600) <4. 
M A{-2}=-0.2 {I2}, A{-4}=0 (1978Ar19) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M A{-2}=+0.38 {I3}, A{-4}=-0.04 {I5} (1978Ar19) 
M$Stretched Q from angular distribution and M2 excluded by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M A{-2}=-0.34 {I12}, A{-4}=0 (1978Ar19) 
M from |g(|q), mult is definitely not Q. From tentative J|p likely E1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
M A{-2}=+0.42 {I2}, A{-4}=+0.03 {I3} (1978Ar19) 
M From |g(|q). Tentative J|p assignment is consistent with E1 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E$Used the unweighted average of 1978Ar19 and 1999Zh18 as the 673.4|g from 1978Ki06 is not only discrepant, but unplaced by the authors 
M A{-2}=-0.16 {I10}, A{-4}=0 (1978Ar19) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
$R(DCO)=0.70 {I13} gated on 239|g 
RI$sum of relative intensities of all transitions into the 201.2 level is 16.2 (2018Ba34) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$uncertainty of 0.03 likely a typo (compilers note) 
$R(DCO)=0.51 {I11} gated on 1070.5|g + 967.6|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$D+Q from |g|g(|q) in {+89}Y(p,2n|g), |D|p=no from level scheme 
MR$from |g|g(|q) in {+89}Y(p,2n|g). Other: -0.10 {I13} from |g(|q) in {+86}Sr(|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:
RI$from {+88}Nb |e decay (7.78 min). Others: 21 {I21} from {+89}Y(|a,p4n|g) and 72 from {+89}Y(p,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$D+Q from |g|g(|q) in {+89}Y(p,2n|g), |D|p=no from level scheme 
MR$from |g|g(|q) in {+89}Y(p,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$D(+Q) from |g(|q) in {+86}Sr(|a,2n|g), |D|p=no from level scheme 
MR$from |g|g(|q) in {+89}Y(p,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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
MR$from |g(|q) {+86}Sr(|a,2n|g). Others: -0.7 {I3} from {+74}Ge({+18}O,4n|g), -0.3 {I2} from {+89}Y(|a,p4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
M$A{-2}=+0.43 {I10}, A{-4}=+0.07 {I10} (1978Ki06), A{-2}=+0.431 {I7}, A{-4}=-0.015 {I10} (1979Nu02). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (E0)
decay_comment:
RI$I(|g+ce)(1521)/I(|g+ce)(464)=0.0005 {i1} deduced from Ice(K)(1521)/Ice(K)(464)=0.09 {i2} (1981Ju03) if ce(K)/(|g+ce)(1521)=0.82 |a(K)(464)=0.0046 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Compiler's note: DCO value of 0.54 with gate on stretched dipole seems too low for assigned |DJ=1 for 1221.6 transition 
$POL=+0.03 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Uncertainty of 0.01 in DCO value in table I pf 2014Sa26 seems unrealistically low, increased to 0.10 by compiler 
$POL=-0.17 {I1} 


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$|g(|q) in (|a,n|g) is consistent with |DJ=0, dipole. |d(Q/D)=+5.8 {I+35-18} from |g(|q) in (p,n|g) indicating M1+E2 is discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
RI$ unweighted average of 41 4 and 21 3 
MR$+0.12 {I15} from |g(|q) but RUL<300 for E2 requires almost pure M1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M4)
decay_comment:
E$from 1969Ro02. Others: 1971Ar18, 1968Dr02, 1964Va03, 1953Sh48 
RI$I|g(|g{+|+})/I|g(588|g)=0.0332 {I20} (1964Va03), 0.038 {I4} (1953Sh48). I|g(1507|g)/I|g(588|g)=0.072 {I8} (1969Ro02), 0.0675 {I7} (1964Va03), 0.077 {I18} (1953Sh48) 
M$from |a(exp)=0.076 {I14}, K/(L+M+..)=5.4 {I7} (1953Sh48) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$from 1975Ko21, who probably adopted from 1975HaYQ. E|g=172 {I2}, I|g|?2 (1969HaZP). |g not reported by 1974Vo08 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$861.6 (1969Li17) 
From |g(|q): |d(M3/E2)=+0.15 {I5} or +1.5 {I2} (1969Li17) 
A{-2}=+0.151 {I20}, A{-4}=-0.016 {I20} (1969Li17) 
A2=+0.23 3, A4=+0.01 3 (EP=5.973, 1969Li17) 
A2=+0.254 20, A4=+0.034 20 (EP=5.595, 1969Li17) 
I|g(|g to g.s.)<3 (1972Gi06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
From |g(|q): |d(M3/E2)=+0.16 {I+9-6} or -3.0 {I+6-8} (1969Li17) 
A{-2}=0.00 {I20} (1969Li17) 
A2=+0.011 13 (EP=5.973, 1969Li17) 
A2=+0.002 25 (EP=5.595, 1969Li17) 
I|g(|g rays to states other than g.s. and 1095)<3 to <20 (1972Gi06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
M,MR$|d(E2/M1)=+0.15 {I+7-5} or -3.0 {I+6-8}, but |DJ|p requires M1 
A{-2}=-0.034 {I20} (1969Li17) 
A2=-0.02 3 (EP=5.595, 1969Li17) 
I|g(|g rays to states other than 588)<3 to <18 (1972Gi06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
|d(M3/E2)=+0.16 {I7} 
A{-2}=+0.047 {I20} (1969Li17) 
A2=+0.027 14 (EP=5.973, 1969Li17) 
A2=+0.06 5 (EP=5.595, 1969Li17) 
I|g(|g rays to states other than g.s. and 1095)<3 to <25 (1972Gi06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.05 {I3} (at E(p)=5.973, 1969Li17) 
I|g(|g rays to states other than 588, 1095 and 1452) <3 to <15 (1972Gi06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$988.0 (1969Li17) 
A{-2}=-0.07 {I5}, A{-4}=+0.09 {I6} (1969Li17) 
A2=-0.15 6, A4=+0.24 8 (EP=5.973, 1969Li17) 
I|g(|g rays to states other than 1095 and 1628)<2 to <8 (1972Gi06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$1002.1 (1969Li17) 
A{-2}=-0.19 {I4}, A{-4}=+0.09 {I4} (1969Li17) 
A2=-0.247 22, A4=+0.09 3 (EP=5.973, 1969Li17) 
I|g(|g rays to states other than 1095 and 1452)<3 to <6 (1972Gi06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
A{-2}=-0.64 {I3}, A{-4}=+0.05 {I4} (1969Li17) 
I|g(|g rays to states other than g.s. and 1512)<10 to <30 (1972Gi06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
M,MR$M1+E2 with |d=+5.8 {I+35-15} from A{-2}=+0.26 {I7}, A{-4}=+0.22 {I9} (1969Li17), but |g(|q) in (|a,n|g) and L({+3}He,t) indicate |DJ=0, dipole (E1) transition 
I|g(|g rays to states other than g.s.)<9 to <30 (1972Gi06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
A{-2}=-0.10 {I4}, A{-4}=-0.04 {I5} (1969Li17) 
I|g(|g rays to states other than g.s. and 1512)<6 to <12 (1972Gi06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$barely resolved from a 271.8|g in {+88}Zr and 269.9|g in {+90}Zr 
A{-2}=+0.28 {I1}, A{-4}=-0.07 {I1}, POL=+0.42 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=-0.03 {I20}, A{-4}=0, POL=-0.17 {I20} for composite peak 
E$doublet with an unknown contaminant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$doublet with a 1740|g in {+87}Sr 
A{-2}=+0.20 {I3}, A{-4}=-0.06 {I3}, POL=+0.67 {I18} for composite peak 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$only partly resolved from 639|g in {+90}Zr, 642 and 645|g in {+88}Zr, 646.0|g in {+88}Y and 642.3|g in {+90}Y 
A{-2}=-0.35 {I16}, A{-4}=0, POL=-0.09 {I4} for composite peak 


decay_energy_unit: KEV
decay_comment:
E$from Adopted Gammas 
RI$the transition may be masked by the 511 |g{+|+} peak. From intensity balance I|g|>340. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from I|g(177|g)/I|g(2122|g)=1.38 {I18} (weighted average from 1979Nu03) 
A{-2}=+0.309 {I22}, A{-4}=-0.03 {I3} (1979Nu03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$|D=-0.05 {I1} 
RI$the possibility of an additional line at 507.5 keV could not be ruled out, thus 2019Sa28 quote I|g as a limit. 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$from {+90}Nb |e decay. Probability of two-photon decay is 0.040% {I5}, see {+90}Y |b{+-} decay. Other: 0.018% {I2} with a ratio <2E1>/<2M1>of 1.9 {I7} (1984Sc37). Probability of one-photon E0 transition for 1760.7 relative to internal conversion is 5|*10{+-7} {I2} (1990Zh20), see {+90}Y |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$weighted average of 329.058 {I16} ({+90}Nb |e decay) and 329.125 {I15} ({+90}Zr(n,n'|g)) 
RI$weighted average of 6.82 {I23} ({+90}Nb |e decay) and 6.6 {I3} ({+90}Zr(n,n'|g)) 
M$D from |g(|q) in (n,n'|g); |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 337.50 {I15} ({+90}Nb |e decay) and 337.8 {I2} ({+90}Zr(n,n'|g)) 
RI$weighted average of 1.4 {I5} ({+90}Nb |e decay) and 0.88 {I11} ({+90}Zr(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 757.95 {I5} ({+90}Nb |e decay) and 757.80 {I4} ({+90}Zr(n,n'|g)) 
RI$weighted average of 2.23 {I23} ({+90}Nb |e decay) and 2.76 {I11} ({+90}Zr(n,n'|g)) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$Conversion electrons observed by 1968Pe01. 
TI$From intensity balance, assuming no |e feeding. 
M$|a(K)exp > 4.8 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3(+M4)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
M$|a(K)exp=2.11 {I15}; K/L=3.22 {I16} (1968Pe01) 
M$(132.7|g)(2186.3|g)(|q): A{-2}=+0.187 {I38}, A{-4}=-0.063 {I36} (1978Be12). 
MR$+0.06 {I10} from |g|g(|q); 0.00 {I7} from ce measurements 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$|a(K)exp=0.00076 {I6} 
M$(890.6|g)(2186.3|g)(|q): A{-2}=+0.132 {I51}, A{-4}=-0.023 {I48} (1978Be12). 
MR$+0.05 {I7} from |g|g(|q); 0.0 {I1} from ce measurements; both consistent with no M3 admixture. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp=0.000197 {I11} 
M$(141.3|g)(1129.2|g)(|q): A{-2}=-0.070 {I12}, A{-4}=-0.003 {I10} (1978Be12). 
MR$-0.02 {I7} from |g|g(|q); 0.000 {I14} from ce measurements; both consistent with no M2 admixture. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|a(K)exp=0.268 {I19}; K/L=6.25 {I33} (1968Pe01) 
M$(141.3|g)(1129.2|g)(|q): A{-2}=-0.070 {I12}, A{-4}=-0.003 {I10} (1978Be12). 
MR$-0.02 {I+11-5} from |g|g(|q); 0.05 {I4} from ce measurements; both consistent with no M3 admixture. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp=0.00033 {I4} 
M$(827.7|g)(1913.2|g)(|q): A{-2}=+0.164 {I40}, A{-4}=+0.062 {I35} (1978Be12). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
M$|a(K)exp=0.000240 {I22} 
M$(1611.8|g)(1129.2|g)(|q): A{-2}=-0.088 {I20}, A{-4}=+0.013 {I18} (1978Be12). 
MR$+0.35 {I7} or +2.4 {I5} from |g|g correlation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$|a(K)exp=0.00021 {I7} 
M$(1716.2|g)(1129.2|g)(|q): A{-2}=-0.011 {I75}, A{-4}=+0.041 {I60} (1978Be12). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$Unresolved from impurity line. From intensity balance at the 3448 level, using |a(exp)=0.32 for 141 |g. 
M$A{-2}=+0.023 {I3}, A{-4}=-0.007 {I3}, Pol=+0.032 {I3} (1985Wa09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_comment:
RI$Unresolved from impurity lines. I|g is from intensity balance. 
M,MR$A{-2}=+0.004 {I4}, A{-4}=+0.030 {I5}, Pol=+0.007 {I5} (1985Wa09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI$From E. Warburton, priv. comm. 
M$No polarization data available. Mult. is from intensity arguments (|a for E1 and M1 are 3.7 and 6.8, respectively). Absence of E2 admixture is from RUL. 
M$A{-2}=-0.016 {I4} (1985Wa09). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
CC$I(ce)/I(|g)=2.38 {I8}, K/LM=7.06 {I8} (1962Ne02). 
E$For excitation function of K-electrons for E(p)=6.0-8.6 MeV, see 1970Co01. 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
TI$derived from I|b{+-} to this level, see comment on I|b{+-} 
$Probability of one-phonon E0 transition relative to internal conversion is 5|*10{+-7} {I2} (1990Zh20) 
$internal pair production of 1760.7 E0 transition, branching ratio=0.00320 {I15} pairs/100 decays (2020Pi01), 0.00326 {I4} pairs/100 decays (2020Dr01), 0.003186 {I47} pairs/100 decays (2007Se01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$From absolute counting (1976Gr16). Other: 1.12|*10{+-6} {I6} from measurement of activity in equilibrium with a {+90}Sr source (1990Zh20). The method of normalization of 1990Zh20 is however not described. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$listed as 562 keV in Figure 4 of 2015Cr02, which evaluators consider to be a typo. Figure 1 and text of 2015Cr02 describe a 425|g depopulating the 2186.3-keV level. A 562|g depopulates 2748, 3- level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$a 562|g is shown in Figure 4 of 2015Cr02 as depopulating the 3448-keV level and populating the 2739-keV level, which evaluators considers to be a typo. Figure 1 and text of 2015Cr02 describe a 1129|g depopulating the 3448-keV level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$observed in spectrum with condition on the energy of the scattered {+17}O particles which corresponds to excitation energies in {+90}Zr between 4.2 MeV and 5.2 MeV, however, absent in same spectrum gated on {+90}Zr energies between 3.0 MeV and 4.0 MeV. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E1
decay_comment:
M$dipole from observation in spectra with condition on angle between emitted |g ray and recoil direction which enhances dipole transitions. 
M$Y{-R}=1.43 {I17}, read by evaluator from Figure 3 of 2015Cr02 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$DCO(D)=1.06 {I2}, |D{-asym}=+0.021 {I3} 
M$DCO and |D{-asym} have contributions from another 1128.8|g. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$DCO(D)=0.78 {I8}, |D{-asym}=-0.043 {I65} 
M$DCO and |D{-asym} have contributions from another 429.3|g. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$DCO(D)=0.78 {I3}, DCO(Q)=0.44 {I2}, |D{-asym}=-0.042 {I5} 
M$DCO and |D{-asym} for unresolved 637.4|g and 638.3|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:
E unweighted average of 1204.67 {I8} from |e decay (60.86 d) and 1204.92 {I10} from (n,n'|g). 
M from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
B(M1)(W.u.)=0.233 {I23} if pure M1; B(E2)(W.u.)=59 {I6} if pure E2. 
MR -10<|d<+0.1 from |g(|q) in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E3)
decay_comment:
BE3W<1.9E+3 
RI from ({+6}Li,2np|g). 
M |g(|q) in ({+6}Li,2np|g) and (n,n'|g) consistent with octupole; |D|p from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR -0.20 {I+25-80} or -2.3 {I+13-37} from (n,n'|g). 
B(M1)(W.u.)=0.0060 {I+11-17}, B(E2)(W.u.)=0.053 {I+10-15} if |d=-0.20; B(M1)(W.u.)=0.00100 {I+19-28}, B(E2)(W.u.)=1.15 {I+21-32} if |d=-2.3. 


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_uncertain: ?
decay_comment:
Reported in (|a,n|g) only. I|g is average of 33 and 40 from (|a,n|g) at E(p)=11.8 and 13.5 MeV, respectively. 
M not pure E2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
M Q from |g(|q) in ({+6}Li,2np|g), not M2 from RUL. 
In (n,n'|g), this |g was tentatively placed from a 2896 level which is not adopted here. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M A{-2}=+0.44 {I3}, A{-4}=+0.01 {I3}, A{-6}=-0.03 {I3} (1976Br14), consistent with octupole transition. 


decay_energy_unit: KEV
decay_multipolarity: (M1)
decay_comment:
E uncertainty given as 0.1 keV in text of 1976Br14. 
ECC,M Apparently deduced by authors on the basis of |g|g and unenumerated I|g data. 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
MR +0.4 {I1} or |d=+1.25 {I15}. Sign from Adopted Gammas; sign convention used by 1977Me13 not stated. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$The absolute intensity was measured by 2024Gi03 by determining activity using the liquid scintillation counting technique. 


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 934.47 {I7} from |b{+-} decay, 934.44 {I10} from |e decay (10.15 d), 934.46 {I5} from (n,|g) E=thermal and 934.5 {I1} from (n,n'|g). 
M Q to 0+, from |g(|q) in ({+7}Li,2np|g); |D|p=no from RUL. E2 confirmed by |a(exp) in {+92}Nb |e decay (10.15 d). 


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 448.5 {I1} (from |b{+-} decay), 448.13 {I7}, 448.22 {I10}, 448.3 {I2} (all from (n,|g) E=thermal) and 448.3 {I1} (from (n,n'|g)). (the unweighted average is 448.29 {I6}.) 
M mult=Q to 2+, from |g|g(|q) in {+92}Y |b{+-} decay; not M2, from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E weighted average of 561.1 {I1} from |b{+-} decay and (n,n'|g), 561.0 {I2} from ({+7}Li,2np|g) and 560.93 {I5} from (n,|g) E=thermal. 
M mult=Q from |g(|q) in ({+7}Li,2np|g); not M2 from RUL. 
|d(Q,O)=+0.04 {I2} from (n,n'|g), +0.01 {I+11-9} or +1.6 {I+4-3} from |g|g(|q) in {+92}Y |b{+-} decay. B(M3)(W.u.) exceeds RUL, unless |d<0.00033. 


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 (n,n'|g). 
M mult=D(+Q) from {+92}Nb(10.15 d) |e decay; |D|p=no from level scheme. 
MR unweighted average of -0.04 {I2} in (n,n'|g), and -0.01 {I3} and +0.044 {I17} from |e decay (10.15 d). 


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 1847.3 {I1}, 1847.5 {I3}, 1847.27 {I9} and 1847.2 {I1} from |b{+-} decay, |e decay (10.15 d), (n,|g) E=thermal and (n,n'|g), respectively. 
RI unweighted average of 58 {I4}, 47.8 {I22}, 52 {I8} and 44.6 {I23} from |b{+-} decay, |e decay (10.15 d), (n,|g) E=thermal and (n,n'|g), respectively (weighted average is 47.9 {I25}). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
E weighted average of 1132.17 {I14}, 1132.11 {I6} and 1132.1 {I1} from |e decay, (n,|g) E=thermal and (n,n'|g), respectively. Other E|g: 1132.4 {I1} from |b{+-} decay. 
M D+Q from |g|g(|q) in (n,|g) and (n,n'|g); adopted |D|p=no. 
MR from |d=-3.2 {I+5-4} or +0.85 {I7} from 2005Fr17 in (n,n'|g) and -2.7 {I+8-15} from (n,|g) E=thermal. Other |d: -2.4 {I+3-4} or -1.04 {I11} (1978Gl04) in (n,n'|g). 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
E,RI E|g from (n,|g) E=thermal. Branch absent in |b{+-} decay and (n,n'|g) and one (n,|g) E=thermal study, and I|g data from the two (n,|g) E=thermal studies that report it are discrepant. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_mixing_ratio_info: ;ERR=LE
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=?;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=?
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=LE;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LE
decay_comment:
RI unweighted average of 11.7 {I7} from (n,n'|g), 10.6 {I9} from (n,|g) E=thermal and 10.1 {I6} from |b{+-} decay. Weighted average is 10.7 {I5}. 
M D(+Q) from |g(|q) in (n,n'|g), |D|p=yes from level scheme. 
MR +0.01 {I3} from (n,n'|g); however, B(M2)(W.u.) exceeds RUL, unless |d<0.009. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_mixing_ratio_info: ;ERR=LE
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GE;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GE
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=LE;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LE
decay_comment:
M D+Q from |g(|q) in (n,n'|g), |D|p=yes from level scheme. 
MR +0.13 {I4} (1978Gl04) from (n,n'|g); however, B(M2)(W.u.) exceeds RUL, unless |d<0.02. 
RI unweighted average of 32.3 {I18} from (n,n'|g), 31.1 {I22} from (n,|g) E=thermal and 26.2 {I17} from |b{+-} decay. Weighted average is 29.6 {I20}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI weighted average from (n,n'|g), (n,|g) E=thermal and |b{+-} decay. 
M mult=D(+Q) from |g|g(|q) in (n,|g), {+92}Y |b{+-} decay, and from |g(|q) in (n,n'|g); adopted |D|p=yes. 
MR -0.019 {I+21-20} from |g|g(|q) in {+92}Y |b{+-} decay. Others: +0.03 {I2} from |g(|q) in (n,n'|g); evaluator rejects value of +0.18 {I+20-15} from |g|g(|q) in (n,|g). B(M2)(W.u.) exceeds RUL, unless |d<0.04. 


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,RI from |b{+-} decay. Other E|g (I|g): 2339.4 {I22} (0.4 {I7}) in (n,|g) E=thermal. 
M from form factor in (e,e'). 
B(E3)(W.u.): from (e,e'). However, B(E3)(W.u.)=48 {I13} from adopted T{-1/2} and branching=0.30 {I7} from |b{+-} decay; a branch of 0.11 would Be required to reduce this B(E3)(W.u.) to the value obtained in (e,e'), suggesting branching may be overestimated in |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:
RI weighted average from (n,n'|g) and (n,|g) E=thermal. 
Other |d: +1.30 {I+13-30} or -0.13 {I9} from (n,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:
B(E2)(W.u.): if |d=0; see comment on |d. 
RI weighted average of 35.9 {I23} from (n,n'|g) and 27 {I7} from (n,|g) E=thermal. 
MR -0.13 {I+5-6} (2005Fr17) in (n,n'|g). However, B(M3)(W.u.) violates RUL, unless |d<0.0007. Other |d: -0.13 {I+9-5} (1978Gl04) 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=GE;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GE
decay_comment:
May also deexcite the 3057 level. 
M mult=D or D(+Q) to 4+, from |g(|q) in ({+7}Li,2np|g) and (n,n'|g), respectively; |D|p=yes from level scheme. 
MR +0.04 (1978Gl04) in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
B(M1)(W.u.): if |d=0. 
RI from (n,n'|g). 72 {I7} from (n,|g) E=thermal if I(404|g)=57. 
M D(+Q) from (n,n'|g); |D|p=no from level scheme. 
Other |d(D,Q)=+0.09 {I+8-5} or |>11.4 or |<-22.9 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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
RI from (n,n'|g). 
M D(+Q) from (n,n'|g); |D|p=no from level scheme. 
Other |d: 0.00 {I4} or -7 {I+2-16} from 1978Gl04 in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=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:
RI from (n,n'|g). 
M D(+Q) from (n,n'|g); |D|p=yes from level scheme. 
Other |d: -0.13 {I4} from 1978Gl04 in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI weighted average from |b{+-} decay, (n,n'|g) and (n,|g) E=thermal. 
M from |g(|q) in (n,n'|g), assuming |D|p from level scheme. 
MR +2.3 {I+2-1} also possible, but less likely (2005Fr17 in (n,n'|g)). Other |d: -0.18 {I4} or +4.5 {I+12-8} from 1978Gl04 in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI unweighted average of 34.2 {I19} from (n,n'|g), 41 {I4} from from (n,|g) E=thermal and 41 {I5} from |b{+-} decay. Weighted average is 36.0 {I21}. 
M D+Q from |g(|q) in (n,n'|g), |D|p=no from level scheme. 
MR -0.14 {I4} or +3.7 {I+7-5} 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 from |b{+-} decay. Other: 2819.3 {I7} from (n,n'|g). 
RI weighted average of 4.5 {I4} from (n,n'|g) and 6.1 {I18} from |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:
RI weighted average of 11.1 {I10} from (n,n'|g) and 8.0 {I22} from (n,|g) E=thermal. 
M D(+Q) from (n,n'|g); |D|p=no from level scheme. 


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:
RI unweighted average of 26.7 {I17} from (n,n'|g) and 34 {I3} from (n,|g) E=thermal. 
Other |d(Q,O)=+0.32 {I+19-28} or |>+3.73 (1978Gl04) for 1928.7|g 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=GE;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GE
decay_comment:
E weighted average of 1461.8 {I3} in (n,|g) E=thermal and 1462.3 {I5} from ({+7}Li,2np|g). 
M mult=(Q) from |g(|q) in ({+7}Li,2np|g); (6)+ to 4+ transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
Other E|g: 717.7 {I3} from (n,|g) E=thermal. 
M D(+Q) from |g(|q) in (n,n'|g); |D|p=no from level scheme. 
MR from 2005Fr17; other |d: +0.41 {I+17-14} or +4.5 {I+31-18} (1978Gl04); all |d from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E from (n,|g) E=thermal. Other E|g: 1058.0 {I3} from (n,n'|g). 
RI from (n,n'|g). 
MR -3.1 {I+15-59} or -0.02 {I20} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E|g matches that for |g placed from possible 3237 level in (n,|g) E=thermal. 
M,MR OTHER: A2=-0.24 2 (EN=3700) (1978Gl04), MR(^D,Q)=-1.09 +9-10, -0.13 +4-1, -0.04 +4-0, RESPECTIVELY, IF J=4, 3, 5, AND MR(Q,O)=-0.70 +6-7 IF J=2 IN (N,N'G); NOT ANALYZED BY 1978Gl04 FOR J=1. 


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 (n,n'|g). 
M D+Q from |g(|q) in (n,n'|g); |D|p=no from level scheme. 
MR from (2005Fr17); other |d: -0.27 {I+9-5} (1978Gl04); both from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
RI from (n,n'|g). Other I|g: 55 {I12} in (n,|g) E=thermal. 
MR +0.02 {I6} or +1.5 {I2} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI from (n,n'|g). Data from (n,|g) E=thermal are discrepant. 
MR +0.68 {I+9-7} or +2.3 {I4} 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 1441.6 {I5} from (n,n'|g) and 1441.0 {I4} from (n,|g) E=thermal. 
RI from (n,n'|g). Other: 12 {I3} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_comment:
RI average of 43.1 {I26} from (n,n'|g) and 47.0 {I26} from (n,|g) E=thermal. 
M D(+Q)) from |g(|q) in (n,n'|g), |D|p=yes from level scheme. 
MR +0.11 {I18} or -5 {I+3-27} 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:
RI unweighted average of 43 {I3} from (n,n'|g), 60 {I7} from (n,|g) E=thermal, 50 {I7} from |b{+-} decay. (weighted average is 46 {I4}.) 
M D from (|g,|g'); |D|p from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR +5.8 {I21} or +0.36 {I+6-5} if J=2 from (n,n'|g). Other |d: +1.2 {I+7-5} if J=2, -1.7 {I+7-28} if J=3, -0.13 {I4} if J=4 from |g(|q) in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_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:
Other E|g (I|g): 2473.6 {I2} (159 {I19}) from (n,|g) E=thermal. 
M D(+Q) from (n,n'|g); |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_mixing_ratio_info: ;ERR=LE
decay_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.): if pure E2. 
MR +0.11 {I10} from (n,n'|g); B(M3)(W.u.) exceeds RUL, unless |d|<0.005. 
Other I|g: 24 {I5} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI from (n,n'|g); 37 {I3} from (n,|g) E=thermal. 
MR 0.0 {I3} or -3.4 {I+17-280} from (n,n'|g); M1 from (pol |g,|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:
Other E|g (I|g): 3472.6 {I3} (100 {I16}) from (n,|g) E=thermal. 
M from (pol |g,|g'); confirmed by |g(|q) in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
RI from (n,n'|g). Other: 30 {I4} from (n,|g) E=thermal. 
M D(+Q) from |g(|q) in (n,n'|g); |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI weighted average of 56 {I6} from (n,|g) E=thermal and 50 {I5} from (n,n'|g). 
|d(D,Q)=+12 {I+52-6} or +0.22 {I+7-8} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_uncertain: ?
decay_comment:
RI from (n,n'|g); 43 {I11} from (n,|g) E=thermal. 
|d(D,Q)=-3.8 {I+9-14} or -0.08 {I8} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI from (n,n'|g); 100 {I11} from (n,|g) E=thermal. 
|d(D,Q)=-3.9 {I+7-9} or -0.12 {I4} from (n,n'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E from level-energy difference. 
M from (|g,|g'); if M1, B(M1)(W.u.)=0.0037 {I6} (2002We15 in (|g,|g')). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E from level-energy difference. 
M from (|g,|g'); if M1, B(M1)(W.u.)=0.022 {I3} (2002We15 in (|g,|g')). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from 2007Na05. Other I|g: 1000 {I80} (1979HeZT), 1000 {I40} (2007ChZX, Budapest data). 
RI 79 {I16} per 100 neutron captures (2007Eg02). 
E weighted average of 934.47 {I6} (2007ChZX, Budapest data), 934.46 {I10} (1979HeZT), 934.4 {I2} (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E unweighted average of 448.3 {I2} (2007Na05), 448.13 {I7} (2007ChZX, Budapest data), 448.22 {I10} (1979HeZT). 
RI weighted average of 52.9 {I17} (2007Na05), 53.6 {I24} (2007ChZX, Budapest data), 48 {I5} (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 560.96 {I10} (1979HeZT), 560.91 {I6} (2007ChZX, Budapest data), 561.0 {I2} (2007Na05). 
RI unweighted average of 225 {I16} (1979HeZT), 228 {I4} (2007ChZX, Budapest data), 255 {I8} (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 912.71 {I7} (2007ChZX, Budapest data), 912.7 {I2} (2007Na05), 912.76 {I10} (1979HeZT). 
RI unweighted average of 92 {I8} (1979HeZT), 107 {I3} (2007Na05), 94 {I4} (2007ChZX, Budapest data). 
Other E|g (I|g): 912.7 {I2} (107 {I3}) (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 1847.26 {I10} (1979HeZT), 1847.3 {I2} (2007Na05). 
RI unweighted average of 46 {I4} (1979HeZT), 67 {I6} (2007ChZX, Budapest Data), 41.1 {I17} (2007Na05). 
Other E|g (I|g): 1847.78 {I15} (67 {I6}) (2007ChZX, Budapest Data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 219.16 {I17} (1979HeZT) and 218.8 {I3} (2007Na05). 
RI from 1979HeZT. Other I|g: 28.5 {I17} (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 571.37 {I22} (1979HeZT) and 571.2 {I2} (2007Na05). Other E|g: 572.05 {I20} (2007ChZX, Budapest Data). 
RI from 1979HeZT. Others: 15.1 {I8} (2007Na05), 17.6 {I24} (2007ChZX, Budapest Data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E|g (I|g): weighted average of 1132.1 {I2} (79.7 {I25}) (2007Na05), 1132.10 {I7} (80 {I6}) (2007ChZX, Budapest Data), 1132.13 {I10} (76 {I7}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Other E|g (I|g): 273.08 {I11} (23 {I3}) (2007ChZX, Budapest Data), unobserved by 2007Na05, so shown as uncertain here and excluded from Adopted Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 844.2 {I2} (2007Na05), 844.08 {I7} (2007ChZX, Budapest Data), 844.19 {I10} (1979HeZT). 
RI unweighted average of 75.5 {I25} (2007Na05), 76 {I3} (2007ChZX, Budapest Data), 61 {I5} (1979HeZT) (the weighted average is 74 {I3}). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E weighted average of 1405.1 {I2} (2007Na05), 1405.02 {I6} (2007ChZX, Budapest Data), 1405.16 {I10} (1979HeZT). 
RI unweighted average of 211 {I7} (2007Na05), 241 {I8} (2007ChZX, Budapest Data), 232 {I20} (1979HeZT) (the weighted average is 225 {I10}). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 902.8 {I2} (34.4 {I17}) (2007Na05), 903.05 {I12} (38 {I4}) (2007ChZX, Budapest Data), 902.86 {I10} (34 {I3}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 1463.8 {I2} (2007Na05), 1463.82 {I12} (1979HeZT). 
RI unweighted average of 6.7 {I8} (2007Na05), 11.7 {I10} (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 990.54 {I10} (27.0 {I24}) (1979HeZT), 990.45 {I17} (23 {I4}) (2007ChZX, Budapest Data); |g unobserved by 2007Na05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 345.40 {I15} (8.6 {I19}) (2007ChZX, Budapest Data). Branch not observed by 2007Na05 or in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 403.81 {I10} (4.7 {I4}) (1979HeZT) and 403.9 {I2} (6.7 {I8}) (2007Na05). Other: 403.47 {I15} (2007ChZX, Budapest Data). 
RI unweighted average of 4.7 {I4} (1979HeZT) and 6.7 {I8} (2007Na05). Other: 11.0 {I20} (2007ChZX, Budapest Data). Unweighted average of all data is 7.5 {I19}. 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
E weighted average of 677.45 {I23} (1979HeZT), 677.7 {I2} (2007Na05). Fits placement poorly and placement requires M2 multipolarity, so shown as tentative here and branch omitted from Adopted Levels. Gammas. 
RI data are discrepant: 0.64 {I16} (1979HeZT), 8.4 {I8} (2007Na05). Branch is absent in (n,n'|g). 


decay_energy_unit: KEV
decay_comment:
E weighted average of 1248.08 {I11} (1979HeZT), 1247.76 {I13} (2007ChZX, Budapest Data), 1248.1 {I2} (2007Na05). 
RI data are discrepant: 4.7 {I4} (1979HeZT), 30 {I3} (2007ChZX, Budapest Data), 16.8 {I8} (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 972.2 {I2} (19.3 {I8}) (2007Na05) and 972.33 {I10} (17.7 {I16}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
|g unconfirmed by 2007Na05 and 2007ChZX or in either |b{+-} decay or (n,n'|g), so placement is shown as uncertain here. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 1885.07 {I12} (1979HeZT) and 1774.8 {I2} (2007Na05). 
RI from 1979HeZT, consistent with branching in (n,n'|g) and |b{+-} decay. Other: 39.4 {I17} (2007Na05); source of discrepancy unknown. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 1369.2 {I2} (13.4 {I8}) (2007Na05) and 1369.27 {I11} (14.9 {I19}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 569.46 {I21} (1979HeZT), 569.5 {I3} (2007ChZX, Budapest Data). 
RI 0.56 {I16} (1979HeZT), 10.4 {I24} (2007ChZX, Budapest Data). |g unobserved by 2007Na05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 1413.9 {I2} (8.4 {I8}) (2007Na05), 1414.05 {I13} (8.9 {I8}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 1974.90 {I12} )1979HeZT), 1975.2 {I3} (2007ChZX, Budapest Data), 1974.9 {I2} (2007Na05). 
RI unweighted average of 13.5 {I12} (1979HeZT), 19 {I4} (2007ChZX, Budapest Data), 10.9 {I8} (2007Na05). Weighted average is 11.9 {I12}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 700.0 {I2} (4.2 {I8}) (2007Na05) and 700.13 {I10} (4.8 {I5}) (1979HeZT). 
Other E|g (I|g): 700.0 {I2} (4.2 {I8}) (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 2105.13 {I10} (1979HeZT), 2105.26 {I23} (2007ChZX, Budapest Data), 2105.3 {I2} (2007Na05). 
RI unweighted average of 16.8 {I8} (2007Na05), 20 {I4} (2007ChZX, Budapest Data), 21.1 {I20} (1979HeZT). Weighted average is 17.5 {I11}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 1057.8 {I2} (3.4 {I8}) (2007Na05) and 1058.03 12 (2.96 {I24}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Placement from 2007Na05; placed from 2124 level by 1979HeZT and also in (n,n'|g), so placement shown as uncertain here. 
E|g (I|g): weighted average of 1741.8 {I2} (5.0 {I8}) (2007Na05) and 1741.66 {I12} (6.7 {I6}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 2328.4 {I2} (14.3 {I8}) (2007Na05) and 2328.10 {I11} (13.0 {I12}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 877.3 {I2} (2007Na05) and 877.51 {I12} (1979HeZT). 
RI unweighted average of 2.24 {I24} (1979HeZT) and 3.4 {I8} (2007Na05). Weighted average is 2.3 {I3}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average 1209.3 {I2} (10.1 {I8}) (2007Na05) and 1209.19 {I11} (9.0 {I8}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 379.34 {I12} (9.0 {I15}) and 379.5 {I2} (2007Na05). Other: 379.34 {I12} (2007ChZX, Budapest Data). 
RI unweighted average of 5.0 {I8} (2007Na05), 3.12 {I24} (1979HeZT). Other: 9.0 {I15} (2007ChZX, Budapest Data).379.5 {I2} (5.0 {I8}) (2007Na05), . 


decay_energy_unit: KEV
decay_comment:
E weighted average of 1222.43 {I11} (1979HeZT), 1222.37 {I19} (2007ChZX, Budapest Data), 1222.7 {I2} (2007Na05). 
RI 4.8 {I5} (1979HeZT), 14 {I3} (2007ChZX, Budapest Data), 22.7 {I8} (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 1988.75 {I12} (1979HeZT) and 1988.6 {I2} (2007Na05). 
RI unweighted average of 26.3 {I24} (1979HeZT), 20.1 {I8} (2007Na05). 
Other E|g (I|g): 1988.14 {I18} (39 {I4}) (2007ChZX, Budapest Data). 1988.6 {I2} (20.1 {I8}) (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 2437.0 {I2} (10.9 {I8}) (2007Na05) and 2436.90 {I11} (10.6 {I10}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 3371.5 {I3} (13.4 {I17}) (2007Na05) and 3370.8 {I4} (16 {I4}) (2007ChZX). 
Other E|g: 3371.2 (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI unweighted average of 1.20 {I24} (1979HeZT), 2.5 {I8} (2007Na05). 
Other E|g: 1111.9 {I3} (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 1604.9 {I2} (6.7 {I8}) (2007Na05) and 1604.85 {I11} (7.4 {I7}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 1956.6 {I2} (5.0 {I8}) (2007Na05) and 1956.60 {I15} (6.0 {I6}) (1979HeZT). 
Other E|g (I|g): 1957.35 {I23} (28 {I4}) (2007ChZX, Budapest Data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 2517.8 {I2} (7.6 {I8}) (2007Na05) and 2517.70 {I14} (8.4 {I3}) (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E fits placement poorly; excluded from least-squares fit. |g unobserved by 2007Na05 so placement shown as uncertain. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 1230.05 {I21} (1979HeZT), 1229.6 {I2} (2007Na05). 
Other I|g: 3.4 {I8} (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 2132.90 {I13} (1979HeZT), 2132.9 {I2} (2007Na05). 
RI unweighted average of 8.4 {I8} (2007Na05) and 10.1 {I5} (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 2693.8 {I1} (1979HeZT), 2694.1 {I2} (2007Na05). 
RI unweighted average of 31.9 {I17} (2007Na05) and 40 {I4} (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 821.1 {I4} (1979HeZT), 820.9 {I5} (2007Na05). 
Other |g: 0.8 {I8} (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 2705.7 {I1} (1979HeZT), 2706.0 {I2} (2007Na05). 
RI unweighted average of 10.1 {I8} (2007Na05) and 13.8 {I12} (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
|g unobserved by 2007Na05 or 2007ChZX and E|g somewhat low for this placement, so shown as tentative. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 790.74 {I13} (1979HeZT), 790.6 {I2} (2007Na05). 
RI unweighted average of 4.2 {I8} (2007Na05) and 2.88 {I24} (1979HeZT). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): unweighted average of 1490.46 {I12} (5.1 {I5}) (1979HeZT), 1491.0 {I3} (3.4 {I8}) (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E E|g (I|g): unweighted average of 5262.7 {I4} (51 {I6}) (2007ChZX, Budapest Data) and 5263.6 {I2} (41.4 {I17}) (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E E|g (I|g): weighted average of 6294.86 {I18} (223 {I16}) (2007ChZX, Budapest Data) and 6294.9 {I2} (211 {I8}) (2007Na05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|s{-|g}=1407 mb {I152} (1978Gl04). 
M,MR |d=0 (2005Fr17). A{-2}=+0.13 {I2} (E(n)=3200), A{-2}=+0.12 {I2} (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|s{-|g}=85 mb {I9} (1978Gl04). 
M,MR |d=0 (2005Fr17). A{-2}=0.0 (E(n)=3200), A{-2}=0.0 (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
|s{-|g}=336 mb {I36} (1978Gl04). 
A{-2}=+0.25 {I3} (E(n)=3200), A{-2}=+0.22 {I3} (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_uncertain: ?
decay_comment:
|s{-|g}=143 mb {I15} (1978Gl04). 
MR -0.04 {I2} or +2.6 {I2} (2005Fr17); the latter is rejected based on its inconsistency with the very small |d obtained from |g|g(|q) in {+92}Nb |e decay (10.15 d). A{-2}=+0.10 {I3} (E(n)=3200), A{-2}=+0.09 {I2} (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|s{-|g}=69 mb {I8} (1978Gl04). 
M,MR |d=0 (2005Fr17). A{-2}=+0.17 {I3} (E(n)=3200), A{-2}=+0.18 {I2} (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|s{-|g}=223 mb {I24} (1978Gl04). 
A{-2}=-0.21 {I1} (E(n)=3200), A{-2}=-0.20 {I1} (E(n)=3700) (1978Gl04). 
MR -3.2 {I+5-4} or +0.85 {I7} (2005Fr17); the former value is adopted based on its agreement with |d=-2.7 {I+8-15} from {+91}Zr(n,|g). Other |d: -2.4 {I+3-4} or -1.04 {I11} (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|s{-|g}=10 mb {I1} (1978Gl04). 
A{-2}=-0.21 {I5} (E(n)=3200), A{-2}=-0.25 {I17} (E(n)=3700), |d=+0.04 {I+4-0} (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|s{-|g}=35 mb {I4} (1978Gl04). 
M,MR from A{-2}=-0.24 {I5} (E(n)=3200), A{-2}=-0.20 {I7} (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|s{-|g}=89 mb {I10} (1978Gl04). 
A{-2}=-0.28 {I2} (E(n)=3200), A{-2}=-0.22 {I2}, A{-4}=+0.05 {I3}, |d=-0.04 {I+4-0} (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|s{-|g}=69 mb {I7} (1978Gl04). 
A{-2}=+0.31 {I6} (E(n)=3200), A{-2}=+0.26 {I3} (E(n)=3700) (1978Gl04). 
Other |d: +1.30 {I+13-30} or -0.13 {I9} (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M3
decay_comment:
|s{-|g}=25 mb {I3} (1978Gl04). 
A{-2}=+0.29 {I7} (E(n)=3200), A{-2}=+0.29 {I7} (E(n)=3700) (1978Gl04). 
Other |d: -0.13 {I+9-5} or -5.7 {I+12-173} (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_mixing_ratio_info: ;ERR=?
decay_comment:
|s{-|g}=37 mb {I10} (1978Gl04). 
M,MR from A{-2}=-0.19 {I3} (E(n)=3200), A{-2}=-0.15 {I2} (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|s{-|g}=7 mb {I1} (1978Gl04). 
M,MR from 2005Fr17. Other data: A{-2}=-0.30 {I11} (E(n)=3200), A{-2}=-0.34 {I12} (E(n)=3700), |d(D,Q): +0.09 {I+8-5} or |>+11.4 or |<-22.9 (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|s{-|g}=6 mb {I1} (1978Gl04). 
A{-2}=-0.27 {I7}, |d=0.00 {I4} or -8 {I+3-15} (E(n)=3200); A{-2}=-0.15 {I13}, A{-4}=+0.54 {I19}, |d=-0.04 {I+13-4} or -5.7 {I+12-172} (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|s{-|g}=12 mb {I1} (1978Gl04). 
A{-2}=+0.31 {I3} (E(n)=3200), A{-2}=+0.33 {I10}, |d=-0.13 {I4} (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|s{-|g}=51 mb {I6} (1978Gl04). 
MR +2.3 {I+2-1} also possible but less likely (2005Fr17). 
A{-2}=+0.11 {I3} (E(n)=3200), A{-2}=+0.14 {I4} (E(n)=3700), |d=-0.18 {I4} or +4.5 {I+12-8} (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|s{-|g}=18 mb {I2} (1978Gl04). 
MR +3.7 {I+7-5} or -0.14 {I4} (2005Fr17). Other |d: -0.22 {I+5-9} or |>+3.7 (1978Gl04). 
A{-2}=0.0 (E(n)=3200), A{-2}=0.0 (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|s{-|g}=29 mb {I3} (1978Gl04). 
A{-2}=+0.07 {I3} (E(n)=3200), A{-2}=0.0 (E(n)=3700), |d=-0.47 {I5} (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q(+O)
decay_comment:
|s{-|g}=8 mb {I1} (1978Gl04). 
A{-2}=+0.63 {I15} (E(n)=3200), |d(Q,O)=+0.32 {I+19-28} or |>+3.7 for E|g=1928.7 {I2}(1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|s{-|g}=14 mb {I1} (1978Gl04). 
M,MR |d(Q,O)=0 (2005Fr17). Other data: A{-2}=0.0 (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|s{-|g}=23 mb {I3} (1978Gl04). 
MR -0.50 {I+6-7} or -1.49 {I+16-14} (2005Fr17). Other data: A{-2}=+0.27 {I8} (E(n)=3200), A{-2}=+0.24 {I5} (E(n)=3700), |d(Q,O)=-0.5 {I+3-6} if J(2909 level)=2; |d(D,Q)=-0.41 {I+10-17} or -1.7 {I+4-7} if J(2909 level)=3 (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|s{-|g}=29 mb {I3} (1978Gl04). 
M A{-2}=-0.10 {I3} (E(n)=3200), A{-2}=0.0 (E(n)=3700) (1978Gl04). 
MR from 1978Gl04 assuming J(2909 level)=3; -0.47 {I5} or |?|@ if J(2909 level)=2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|s{-|g}=26 mb {I3} (1978Gl04). 
A{-2}=-0.35 {I8} (E(n)=3200), A{-2}=-0.34 {I5} (E(n)=3700), |d=-1.6 {I+5-8} if J(3039 level)=2, -0.04 {I+4-9} if J(3039 level)=3 (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|s{-|g}=12 mb {I1} (1978Gl04). 
A{-2}=-0.31 {I6} (E(n)=3700) (1978Gl04). Other |d: +0.41 {I+17-14} or +4.5 {I+31-18}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from I(991|g)/I(2122|g)=2.6 {I7} in 1978Gl04 and I(2123|g) in 2005Fr17. 
|s{-|g}=31 mb {I8} (1978Gl04), estimated from 4|p|s{-|g}(90|'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|s{-|g}=12 mb {I1} (1978Gl04). 
A{-2}=+0.26 {I6} (E(n)=3200), A{-2}=+0.41 {I11} (E(n)=3700), |d=+0.4 {I+12-3} for E|g=2122.4 {I7} (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|s{-|g}=13 mb {I1} (1978Gl04). 
MR -3.1 {I+15-59} or -0.02 {I20} (2005Fr17). Other data: A{-2}=0.0 (E(n)=3700) (1978Gl04), |d|<+0.32 if J(3124 level)=1 (-0.32 {I+14-21} if J(3124 level)=2). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
|s{-|g}=24 mb {I3} (1978Gl04). 
|g placed instead as sole branch from a 4+ 3236 level by 1978Gl04. 
M |d(D,Q)=0 (2005Fr17). Other: A{-2}=-0.24 {I2} (E(n)=3700) (1978Gl04); |d(D,Q)=-1.09 {I+9-10}, -0.13 {I+4-1}, -0.04 {I+4-0}, respectively, if J=4, 3, 5 and |d(Q,O)=-0.70 {I+6-7} if J=2; not analyzed for adopted J=1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|s{-|g}=14 mb {I2} (1978Gl04). 
A{-2}=+0.34 {I8} (E(n)=3700), |d=-0.09 {I13} or +1.3 {I+3-5} (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|s{-|g}=27 mb {I3} (1978Gl04). 
A{-2}=0.0 (E(n)=3700) (1978Gl04). 
MR from 2005Fr17. Other |d: -0.27 {I+9-5} (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_comment:
|s{-|g}=5 mb {I1} (1978Gl04). 
MR >+10 or +0.08 {I+4-5} (2005Fr17). 
A{-2}=0.0 (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|s{-|g}=22 mb {I2} (1978Gl04). 
M from A{-2}=-0.10 {I4} (E(n)=3700) (1978Gl04). 
MR if J(3275 level)=3; |@ or -0.52 {I+11-8} if J(3275 level)=2 (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
|s{-|g}=8 mb {I1} (1978Gl04). 
MR +0.02 {I6} or +1.5 {I2} (2005Fr17). 
A{-2}=0.0 (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|s{-|g}=10 mb {I1} (1978Gl04). 
MR +0.68 {I+9-7} or +2.31 {I35} (2005Fr17). Other |d: +0.04 to +1.92 if J(3289 level)=2, +0.52 {I+12-16} if J(3289 level)=3 (1978Gl04). 
A{-2}=+0.41 {I12} (E(n)=3700) for E|g=1225.5 {I6} (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
|s{-|g}=11 mb {I1} (1978Gl04). 
M,MR |d(D,Q)=0 (2005Fr17). Other data: A{-2}=0.0 (E(n)=3700) (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|s{-|g}=11 mb {I1} (1978Gl04). 
A{-2}=-0.50 {I7} (E(n)=3700) (1978Gl04). 
MR +5.8 {I21} or +0.36 {I+6-5} (2005Fr17). Other |d: +1.2 {I+7-5} if J=2, -1.7 {I+7-28} if J=3, -0.13 {I4} if J=4 (1978Gl04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|s{-|g}=6 mb {I1} (1978Gl04). 
A{-2}=-0.38 {I10} (E(n)=3700), |d=-1.6 {I+6-12} if J=2 for E|g=1606.2 {I8} (1978Gl04). 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
E from 1978Gl04; placement not adopted. A 569.5|g deexcites the 2909 level in (n,|g) and this |g is not reported by 2005Fr17 in (n,n'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E rounded value from Adopted Gammas; |g evident in particle-|g coin spectrum in fig. 1 of 2008We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
B(M1)(W.u.)<0.089 {I6} if pure M1, B(E2)<8.0 {I6} if pure E2 (2002We15); adopted B(E2)(W.u.)=0.063 {I9}. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1
decay_comment:
B(M1)(W.u.)=0.094 {I4} (2002We15) cf. adopted value of 0.063 {I9}. 
M R(asymmetry)=+0.94 {I3} (2004Fr30). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: Q
decay_comment:
If E2, B(E2)(W.u.)=0.17 {I1} (2002We15) cf. adopted value of 0.35 {I4}. Additional gammas are known to deexcite this level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E1
decay_comment:
M R(asymmetry)=-0.87 {I3} (2004Fr30). 
If M1, B(M1)(W.u.)=0.093 {I4} (2002We15); however, |g is now known to be E1. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
B(M1)(W.u.)<0.036 {I7} if pure M1, B(E2)<2.8 {I5} if pure E2 (2002We15). Adopted B(M1)(W.u.)=0.011 {I+31-11}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$doublet, second component is a new transition from (11-) level reported by 2017Su22 
$R(ADO)=1.29 {I8}, 1.95 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M D+Q from |b{+-} decay; adopted |D|p=no. 
MR -3.2 to -4.0 or +0.23 to +0.29 if abs[|d(267|g)]=1.2 (from |g|g(|q) in {+93}Y |b{+-} decay). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
M2 multipolarity is implied by a (15/2+) to (11/2-) placement proposed in ({+28}Si,X|g); if correct, RUL would then imply T{-1/2}(2990 level)>3.0 ns. The proposed (17/2+) to (13/2+) placement from ({+24}Mg,F|g) seems more plausible for this strong branch. 
Other I|g: 94 {I25} from {+173}Yb({+24}Mg,F|g), 75 from {+162}Dy({+36}S,F|g). Note that adopted order of 705|g and 1334|g is the reverse of that proposed in ({+24}Mg,F|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|a(K)exp from 1972Oh06; misprinted as 0.022 {I40} in 1972Oh03. Other: 0.024 (1959Kn38) (from I(267ce(K))/I|b=0.00152 and I(267|g)/I|b=0.064 {I10}). 
M,MR from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR,M |d(D,Q)=-3.2 to -4.0 or +0.23 to +0.29 if abs(|d(267))=1.2; based on A{-2}=-0.005 {I21}, A{-4}=-0.02 {I4} for 680|g-267|g(|q) (1972Oh06). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
1169-keV peak stronger than expected for 2191|g double escape peak alone (1973Ta15); unplaced by 1973Ta15. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1426.8 {I4} (10.3 {I5}) (1977Ba33). 
E placed by evaluator; |g placed by 1977Ba33 from a 2372 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1650 {I1} (2.7 {I5}) (1977Ba33). 
E placed by evaluator; 1977Ba33 placed |g from an otherwise unknown 1650 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1916.2 {I6} (1.9 {I3}) (1977Ba33). E|g misprinted as 1616.2 in table 2 of 1977Ba33. 
Placement consistent with |b{+-} decay data. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 3458.1 {I6} (1977Ba33) and 3457.4 {I5} (1972Gr23). 
RI from 1977Ba33. Other I|g: 2.5 (1972Gr23). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 4204.2 {I6} (1977Ba33) and 4203.5 {I11} (1972Gr23). 
RI from 1977Ba33. Other I|g: 1.13 (1972Gr23). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 4262.6 {I8} (1977Ba33) and 4260.5 {I11} (1972Gr23). 
RI from 1977Ba33. Other I|g: 1.6 (1972Gr23). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E unweighted average of 6470.0 {I8} (1977Ba33) and 6465.5 {I11} (1972Gr23). 
RI from 1977Ba33. Other I|g: 2.1 (1972Gr23). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E unweighted average of 6735.0 {I7} (1977Ba33) and 6732.7 {I11} (1972Gr23). 
RI from 1977Ba33. Other I|g: 2.1 (1972Gr23). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
TI |<40 {I8} from intensity balance at 3264 level, assuming negligible internal conversion for 392|g and 275|g. 
M |a(exp)|<0.6 {I7} (from I(|g+ce) and I|g) rules out E2 or higher multipolarity (|a(E2)=5.11 for 65.6|g, |a(M1)=0.67). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E unresolved multiplet. 
TI |<31 {I3} from intensity balance at 3265 level, assuming negligible internal conversion for 392|g and 275|g. 


decay_energy_unit: KEV
decay_comment:
MR$-0.8 {I+6-12} if J=1, |d=-0.22 {I+4-10} if J=2, |d=+0.22 {I+5-4} if J=3 pure E2 and J=0 also possible. 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
$1978Gl04 place this |g from a level at 3056.8 keV {i11} together with the 2140.9 keV {i25} |g. The latter one is probably identical to the 2140.6 keV {i2} |g deexciting the 3059.4 level in |b{+-} decay. However, with the smaller uncertainty from |b{+-} decay the 2140|g and 1384|g do not fit into the level scheme. The evaluator therefore concludes that the 1384|g is misplaced in (n,n'|g). Also the excitation function of the 1384|g seems to indicate a level lower than the 3056. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.19 {I+25-15} or +1.6 {I+7-6} 
$B(M1)=0.07 {I+4-3} or +0.012 {I+9-7}; B(E2)(W.u.)=7 {I+4-3} or 135 {I+115-75} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+2.90 {I+35-25} or -0.07 {I+3-4} 
$B(E2)(W.u.)=1.02 {I15} or 187 {I+55-40}; B(M1)=0.18 {I+3-2} or 0.018 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.52 {I+16-12} or +0.3 {I+17-2} 
$B(E2)(W.u.)=0.18 {I+5-4} or 0.8 {I+8-4}; B(M1)=0.004 {I1} or 0.0005 {I+3-4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.04 {I+9-8} or +2.7 {I+10-6} 
$B(E2)(W.u.)=0.3 {I+10-3} or 130 {I+74-48}; B(M1)=0.18 {I2} or 0.017 {I+7-8} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
MR$+1.6 {I+5-4} or +0.15 {I+15-8} 
$B(E2)(W.u.)=5 {I2} or 0.16 {I+6-5}; B(M1)=0.02 {I1} or 0.06 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.01 {I+9-8} or +1.24 {I+28-24} 
$B(E2)(W.u.)=0.1 {I+12-1} or 38E1 +16-12; B(M1)=0.89 {I+22-20} or 0.28 {I+11-9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
MR$+2.1 {I+8-7} or +0.9 {I+24-2} 
$B(E2)(W.u.)=46 {I+28-22} or 18 {I+36-5}; B(M1)=0.02 {I1} or 0.05 {I+2-5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.09 {I+25-14} or +1.0 {I+4-10} 
$B(E2)(W.u.)=0.14 {I+72-14} or 9 {I+3-9}; B(M1)=0.095 {I+15-14} or 0.05 {I+5-2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2295.5 {I4} ({+95}Y |b{+-} decay), 2294.0 {I6} ({+94}Zr(n,|g) E=thermal) 
E$only |g ray observed in ({+94}Zr(n,|g) E=thermal) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$from {+173}Yb({+24}Mg,F|g) 
M$suggested to be (E2) by {+173}Yb({+24}Mg,F|g); not consistent with {+176}Yb({+28}Si,X|g); adopted as (E1) following J{|pi} assignments of ({+176}Yb({+28}Si,X|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%IG$Taken as 15.9% {i7} (Ge(Li)) assuming %I|g({+95}Zr 757|g)=54.7 {i4} for current value of 54.46% {i10}. Others: 9% {i2} (1967Va03. 4|p|g, NaI), 13.0 {i10} (13.2% {i10} (1973Ca26. Ge(Li), assuming %I|g({+95}Zr 724|g)=44.7 {i7} (1969Fo01)) revised using current value of 44.17% {i9}), 19% {i2} (1975Ca12), and 11.1% {i22} (1983Ni09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$E|g=2022 was observed in 2007Sz05, which is assigned to be E3 decay of 11/2- level to g.s. on the basis of intensity ratio w.r.t. 230 keV E1 transition. 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$from {+96}Y |b{+-} decay (5.34 s) 
$|r{+2}=7.53|*10{+-3} {i14}=0.32 {i1}(SPU); from t, K,L{-I},L{-II} shell conversion factors from 1970Be87, and the K-shell conversion/pair production ratio from 1986PaZM 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
TI$ce(K)(1114)/I(469|g)=0.00015 to 0.00018 in (t,p|g) 
$X{-322}=0.037 {i6} (if 1114.6|g is M1 or E2), =0.043 {i7} (if 1114.6|g is E1) (1988HeZM) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
TI$from ce(K)(2695)/I(469|g)=0.000030 in (t,p|g) 
$X{-312}=0.0039 {i9} (1988HeZM); statistical uncertainty only, a calibration uncertainty of 50% for E{-e}>1600 keV is not included 
$|r{+2}{-32}/|r{+2}{-31}=9.4 {i26} (1988HeZM) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
$X{-412}=0.067 {i27} (1988HeZM); statistical uncertainty only; a calibration uncertainty of 50% for E{-e}>1600 keV is not included 
$|r{+2}{-42}/|r{+2}{-41}<3.0 (1988HeZM) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$this |g is designated as E1 (1987StZX,1988StZS) without giving experimental details for this assignment. If this |g is a dipole, it should be M1. 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$weighted average of 1581.4 {i5} (1988Ma01) and 1581.7 {i5} (1986VaZP) 
M$no |g corresponding to ce was seen (1975Kh05) 
TI$from 1990Ma03; other: 1.4% {i5} (1988Ma01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$from difference in energy of initial and final levels; 517.2 keV (1995HaZT, 1997RaZZ). 1987StZX report a 517.4 keV |g with I|g=12 depopulating the 4907 level which is not seen by 1995HaZT, 1997RaZZ. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$1995HaZT, 1997RaZZ show a 804.7 keV |g, I|g=18 depopulating a 3924.3 level not observed by 1987StZX 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
E$from level energy; 1588 from the ce(K) at 1570 keV (1972Bu18) 
M$internal conversion electrons observed without a |g (1972Bu18) 


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:
TI$from the coincidence gates on |g rays at the top of the 1897 level, transition intensity of the 146.6-keV transition is the same as that of the 1750.4-keV |g ray 
RI$deduced by compiler from I(|g+ce) and total conversion coefficient 
$B(E1)(W.u.) is deduced by compiler. 2019SiAA give B(E1)(W.u.)=0.00133 {I8}, which the compiler obtains if conversion coefficient of 0.0371 for E1 multipolarity is ignored. 


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:
$B(E3)=23|*10{+3} e{+2}fm{+6} {I2} (2019SiAA) or 0.023 {I2} e{+2}b{+3} 
RI$2019Is03 measured the following values in six different reactions: 13.3 {I13}, 12.7 {I13}, 13.5 {I13}, 13.4 {I27}, 12.4 {I33}, 12.9 {I30} with summed gate on 1222.7, 363.8 and 906.2 transitions. 13.5 {I6}, 13.2 {I6}, 12.8 {I6}, 13.0 {I13}, 12.3 {I11}, 12.4 {I12} with gate on 1222.7 transition. 12.5 {I5}, 12.8 {I6}, 13.2 {I6}, 13.6 {I11}, 12.8 {I11}, 13.7 {I12} with gate on 363.6 transition. Weighted averages from the three sets are: 13.1 {I7}, 13.0 {I3} and 12.9 {I3}, respectively. Weighted average of these three values is 13.0 {I3}, and after correcting for summing effect of 146 and 1750 |g rays, final value is 12.8 {I3}, relative to 100 for the 1750.4 |g ray. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$|g observed by 1996Lh03 only (in coin with 1291|g); I(189.6|g) from 4 % 2 depopulation branching of 1997 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
RI$73.0 {I8} adopted by evaluator. 73 {I8} given by 1996Lh03 seems to have a too big uncertainty, which seems to be sustained by the other intensities (much smaller) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M3]
decay_uncertain: ?
decay_comment:
$Observed by 1976MoZC but not by 1996Lh03 (possible 161|g-1103|g coincidence summing); I|g from I(161|g,1996Lh03) and |g branching ratio from 1976MoZC 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
MR$or -3.8 {I5} 
$A{-2} and A{-4}, POL for 161.5-1103.3 cascade. pol=+0.19 {I19} from 756.2-1103.3 cascade. 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
$Monopole strength |r{+2}(E0)=0.0112 {I12} (2005Ki02 evaluation), based on data in 1994Lh01 
$Energy of E0 transition from level energy difference 
M$from ce data in (t,p|g) and {+98}Y |b{+-} decay (0.548 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$other: 370.0 {I10} in (|a,F|g) 
RI$from {+98}Y |b{+-} decay (0.548 s). Others: 2.1 {I2} in (|a,F|g), 0.9 {I3} in {+248}Cm SF decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$others: 1222.7 {I2} in {+98}Zr IT decay, 1222.7 {I10} in (|a,F|g) 
RI$deduced from {+98}Y |b{+-} decay (0.548 s). Uncertainty of 0.2 is from deduced absolute |g-branching ratios to the 854 level and the ground state. 
M$|g|g(|q) in |b{+-} decay (0.548 s) and {+235}U(n,F|g), and RUL 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
M$ce data in (t,p|g) and {+98}Y |b{+-} decay (0.548 s) 
$Evaluated q{-K}{+2}(E0/E2)=1.05 {I7}, X(E0/E2)=0.054 {I3}, |r{+2}=0.076 {I6} (2005Ki02), based on data in 1994Lh01 and 1982Ka03 
$Monopole strength |r=0.274 {I15} (1994Lh01), 0.29 {I8} (1982Ka03) 
$I(E0)/I(E2)=0.065 {I4} (1994Lh01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$from |g|g(|q) in {+98}Zr |b{+-} decay (0.548 s), and (n,F|g), and |DJ|p, where J|p of each level is known independently 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$|g|g(|q) in {+235}U(n,F|g), D+Q from |g|g(|q), M1+E2 from |DJ|p, where each J|p is determined uniquely in different experiments. Other |d: +0.2 {I1} from |g|g(|q) in {+98}Y |b{+-} decay (0.548 s) 


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$others: 1.4 {I2} in (|a,F|g), 5.2 {I17} in {+248}Cm SF decay, 4.8 in {+252}Cf SF decay. Values in SF decay seem too high by a factor of |?3. 


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$other: 100 in (|a,F|g), 100 {I5} in {+248}Cm SF decay 
M$|g(|q) and |g(pol) in {+248}Cm SF decay 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
M$ce data in (t,p|g) and {+98}Y |b{+-} decay (0.548 s) 
$Evaluated q{-K}{+2}(E0/E2)=5.4 {I14}, X(E0/E2)=26 {I7}, |r{+2}=0.061 {I8} (2005Ki02), based on data in 1994Lh01 and 1982Ka03 
$Monopole strength |r=0.237 {I25} (1994Lh01), 0.29 {I15} (1982Ka03) 
$I(E0)/I(E2(269|g))=0.0130 {I16} (1994Lh01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
E$other: 240.1 {I1} from {+98}Zr IT decay 
RI$others: 100 {I14} in {+248}Cm SF decay, 100 in {+252}Cf SF decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$other: 36 {I7} in {+248}Cm SF decay. I|g=133 in {+252}Cf SF decay is discrepant 
M$|g(|q) in {+248}Cm SF decay, and |DJ|p 


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$|g(|q) and |g(pol) in {+248}Cm SF decay, also supported by |g|g(|q) in {+98}Y |b{+-} decay (2.32 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$unweighted average of 1258.9 {I1} from {+98}Y |b{+-} decay (2.32 s) and 1258.2 {I2} from {+98}Zr IT decay (1.9 |ms) 
RI$from {+248}Cm SF 
M$|g|g(|q) in IT decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from IT decay. Other: 725.3 {I2} in {+98}Y |b{+-} decay (2.32 s) 
M$|g|g(|q) and |g(pol) in {+248}Cm SF decay ,also supported by |g|g(|q) in {+252}Cf SF decay and RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from IT decay. 
RI$unweighted average of 111 {I25} in IT decay, 50 {I25} in {+248}Cm SF decay and 47 in {+252}Cf SF decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|g|g(|q) in {+98}Y |b{+-} (2.32 s), {+252}Cf SF, and {+235}U(n,F|g) 
MR$from |g|g(|q) in {+98}Y |b{+-} (2.32 s). Other: -0.77 {I12} from |g|g(|q) in (n,F|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 IT decay 
$|a(exp)=5.5 {I16} (2006Si36) 
M$from |a(expt)=5.5 {I16} (2006Si36), deduced from intensity balance. Value is consistent with E2(+M1), |d>1.25 or E2(+M3), |d<0.09. 
E$2006Si36 discussed another scenario for the placement of 63.0|g: two closely-spaced 63.0-keV gamma rays, an E1 to 6540, (16+) level (from 2004Wu08) and E2 to 6541, (15-) level, however, based on intensity-balance arguments, this scenario was considered unlikely. 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
TI$from intensity balance, corresponding to %I(|g+ce)=14.4 {I14} in agreement with 15 {I3} deduced by 1987Ma58 from ce(K)(854)/ce(K)(268|g) (1983VaZJ,1982Ka03). Others: 4.9 {I18} (1983VaZJ), 26 {I5} (1971Fo21). Values of I(E0)(absolute)=4.4 and 7.2 are also quoted by 1983VaZJ based mult(119|g) from {+98}Sr |b{+-}. This values agrees with value of 40 (relative to 100 for 1223|g) in 1984Be50, but a corresponding relative value of |?200 in 1977Si05 was grossly over estimated 
$ceK/ceL=9.7 {I19} (1975Kh05) 
$Energy of E0 transition from level energy difference 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$E|g=368.5, I|g=1.6 (1984Be50) 
$E|g=368.5 {I2}, I|g=1.5 {I4} (1977Si05) 
RI$2.5 {I2} in 2017Ur03 (Table VII) is probably the total intensity from the two activities in {+98}Y. Evaluators have subtracted 0.76 {I7} units to account for contribution from the 2.32-s isomer decay obtained from intensity balance at 1223 level in {+98}Y |b{+-} decay (2.32 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=1223.0, I|g=100 (1984Be50) 
$E|g=1222.8 {I2}, I|g=100.0 (1977Si05) 
RI$100.0 {I30} in 2017Ur03 (Table VII) is likely the total intensity from the two activities in {+98}Y. Evaluators have subtracted 30.2 {I8} units to account for contribution from the 2.32-s isomer decay obtained from intensity balance at 1223 level in {+98}Y |b{+-} decay (2.32 s). Adjusted intensity gives I|g(1223)/100 decays=37.0 {I17} consistent with measured I|g/100 decays=36 {I3} in 1987Ma58. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$213.1 {I1} from 1994Lh01. Precise E|g=213.948 {I22} (1979Bo26) from crystal spectrometer seems to be in error 
$E|g=213.1 {I2}, I|g=12.0 {I20} (1977Si05) 
$E|g=213.1, I|g=11.3 (1984Be50) 
M$(213|g)(1223|g)(|q): A{-2}=+0.36 {I12}, A{-4}=+1.19 {I19} (1984Be50), 1982Ka03 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$from ce data in 1994Lh01. Other: 1982Ka03 
TI$from I(E0)/I(E2(213|g))=0.065 {I4} (1994Lh01) and adopted I(213|g)=14.6 {I5} here. 
$Monopole strength (|r)=0.274 {I15} (1994Lh01), 0.29 {I8} (1982Ka03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
$E|g=367.5, I|g=2.4 (1984Be50) 
$E|g=367.6 {I2}, I|g=2.0 {I5} (1977Si05) 
RI$3.1 {I2} in 2017Ur03 (Table VII) is probably the total intensity from the two activities in {+98}Y. Evaluators have subtracted 0.24 {I3} units to account for contribution from the 2.32-s isomer decay obtained from intensity balance at 1591 level in {+98}Y |b{+-} decay (2.32 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$E|g=736.7, I|g=4.5 (1984Be50) 
$E|g=736.7, I|g=3.5 (1977Si05) 
RI$3.9 {I2} in 2017Ur03 (Table VII) is probably the total intensity from the two activities in {+98}Y. Evaluators have subtracted 0.30 {I3} units to account for contribution from the 2.32-s isomer decay obtained from intensity balance at 1591 level in {+98}Y |b{+-} decay (2.32 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=1590.9, I|g=40.9 (1984Be50) 
$E|g=1590.7 {I2}, I|g=40.5 {I20} (1977Si05) 
RI$26.7 {I8} in 2017Ur03 (Table VII) is probably the total intensity from the two activities in {+98}Y. Evaluators have subtracted 2.04 {I17} units to account for contribution from the 2.32-s isomer decay obtained from intensity balance at 1591 level in {+98}Y |b{+-} decay (2.32 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$E|g=521.6, I|g=3.5 (1984Be50) 
$E|g=521.6 {I2}, I|g=6.0 {I5} (1977Si05) 
$(522|g)(123|g)(|q): A{-2}=+0.01 {I16}, A{-4}=-0.28 {I28} (1984Be50), |d(E2/M1)=+0.2 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=268.7, I|g=18.6 (1984Be50) 
$E|g=268.6 {I2}, I|g=21.0 {I20} (1977Si05) 
$(269|g)(154|g)(|q): A{-2}=+0.50 {I16}, A{-4}=+1.1 {I3}; (269|g)(1591|g)(|q): A{-2}=+0.24 {I21}, A{-4}=+1.03 {I21} (1984Be50). (269|g)(737|g)(|q): A{-2}=+0.6 {I3}, A{-4}=+1.5 {I5} (1982Ka03) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$from ce data in 1994Lh01. Other: 1982Ka03 
TI$from I(E0)/I(E2(269|g))=0.0130 {I16} (1994Lh01) and adopted I(269|g)=22.6 {I7} here. 
$Monopole strength (|r)=0.237 {I25} (1994Lh01), 0.29 {I15} (1982Ka03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=636.4, I|g=3.3 (1984Be50) 
$E|g=636.2 {I2}, I|g=4.0 {I10} (1977Si05) 
$(636|g)(1223|g)(|q): A{-2}=+0.6 {I4}, A{-4}=+0.9 {I5} (1982Ka03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=2305.5, I|g=9.8 (1984Be50) 
$E|g=2305.5 {I5}, I|g=5.5 {I15} (1977Si05) 
$(2305|g)(269|g)(|q): A{-2}=-0.28 {I21}, A{-4}=+0.29 {I27} (1984Be50) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
$E|g=2941.3, I|g=46.3 (1984Be50) 
$E|g=2941.3 {I5}, I|g=48.5 {I30} (1977Si05) 
$(2941|g)(1223|g)(|q): A{-2}=-0.18 {I14}, A{-4}=+0.20 {I27} (1984Be50) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$this |g should be placed from a 5590, (14+) level, as in 2006Si36 and in the Adopted Levels, Gammas. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$from |g|g(|q) (2017Ur03). |d(Q/D)=0.00 {I2} from (583.2|g)(1222.9|g)(|q): A{-2}=-0.069 {I2}, A{-4}=-0.015 {I18} for J(1806)=3. |d=-0.16 {I1} for J(1806)=1, and no solution for |d for J(1806)=2 (2017Ur03) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(620.5|g)(1222.9|g)(|q): A{-2}=+0.095 {I7}, A{-4}=-0.006 {I11}, consistent with 4 |) 2 |) 0 sequence (2017Ur03) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(725.3|g)(1222.9|g)(|q): A{-2}=+0.089 {I13}, A{-4}=0.00 {I2} (2017Ur03) consistent with 8 |) 6 |) 4 sequence (2017Ur03) 


decay_energy_unit: KEV
decay_multipolarity: (E1)
decay_comment:
M$from |g|g(|q) (2017Ur03); |d(Q/D)=0.00 {I3} from (2942.3|g)(1222.9|g)(|q): A{-2}=-0.25 {I3}, A{-4}=+0.02 {I4} for J(4165)=1. No solution for |d for J(4165)=0 or 2. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$from |g|g(|q) and linear polarization data in 2017Ur03. Preferred |d(E2/M1) value in 2017Ur03 from three possible values for J(4292)=6: -0.77 {I12}, +0.17 {I8} or -0.80 {I14}. Polarization data is from {+235}U(n,F|g) experiment. |d(E2/M1)=-0.80 {I14} or +0.17 {I8} (2017Ur03) from (1801.6|g)(1222.9|g+620.5|g+647.1|g)(|q): A{-2}=+0.14 {I2}, A{-4}=-0.04 {I3} for J(4292)=6. |d(Q/D)=+0.38 {I6} or +2.3 {I3} for J(4292)=7 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
RI$0.4 {I1} in 2017Ur03 (Table VIII) is probably the total intensity from the two activities in {+98}Y. Evaluators have subtracted 0.044 {I12} units to account for contribution from the 0.548-s g.s. decay obtained from intensity balance at 1806 level in {+98}Y |b{+-} decay (0.548 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$E|g=583.2 {I1} (2017Ur03) 
$E|g=583.3, I|g=4.6 (1994St31,1988StZS) 
$E|g=583.3 {I2}, I|g=6.5 {I5}(1977Si05) 
RI$6.0 {I2} in 2017Ur03 (Table VIII) is probably the total intensity from the two activities in {+98}Y. Evaluators have subtracted 0.66 {I10} units to account for contribution from the 0.548-s g.s. decay obtained from intensity balance at 1806 level in {+98}Y |b{+-} decay (0.548 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$E|g=253.1 {I2}, I|g=1.5 {I10} (1977Si05), |g could also correspond to the proposed placement of a 253.4|g from 4545 level in 2017Ur03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$E|g=620.5 {I1} (2017Ur03) 
$E|g=620.7, I|g=27.6 (1994St31,1988StZS) 
$E|g=620.5 {I2}, I|g=27.0 {I20} (1977Si05) 
$(620|g)(1223|g)(|q): A{-2}=-0.09 {I3} (1988StZS) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
$E|g=241.7, I|g=2.5 (1994St31,1988StZS) 
$E|g=241.5, I|g=5.6 (1984Be50), assigned incorrectly to the decay of {+98}Y g.s. 
$E|g=241.5 {I2}, I|g=2.5 {I5} (1977Si05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$note that value from 1979Bo26 is in disagreement with 647.1 {I1} from 2017Ur03 by |?3 |s 
$E|g=647.5, I|g=23.2 (1994St31,1988StZS) 
$E|g=647.3 {I2}, I|g=20.0 {I20} (1977Si05) 
$(647|g)(620|g)(|q): A{-2}=-0.04 {I7}. (647|g)[620|g](1223|g)(|q): A{-2}=-0.06 {I3} (1988StZS) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=839.7, I|g=2.3 (1994St31,1988StZS) 
$E|g=840.3 {I2}, I|g=2.5 {I10} (1977Si05), but assigned to the decay of {+98}Y g.s. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1174.2 {I2} in 2017Ur03 fits poorly in the level scheme. Value of 1174.9 from 1994St31 with an assigned uncertainty of 0.3 keV is used here, instead. 
$E|g=1174.9, I|g=2.0 (1994St31,1988StZS) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$E|g=1801.5, I|g=17.4 (1994St31,1988StZS) 
$E|g=1801.6 {I5}, I|g=16.5 {I15} (1977Si05) 
$(1801|g)(647|g)(|q): A{-2}=-0.07 {I4}; (1801|g)[647|g](620|g)(|q): A{-2}=--0.03 {I5}; (1801|g)[647|g][620|g](1223|g)(|q): A{-2}=+0.08 {I7} (1988StZS) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$|DJ=2, Q from (1258|g)(583|g)(|q): A{-2}=-0.08 {I3}, A{-4}=+0.04 {I4}. From I|g(1221)/I|g(1258)=0.6 {I4}, 2006Si36 suggest E2 for 1258|g and E1 for 1221|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
ECC$ from intensity balance. 
E$2006Si36 discussed another scenario for the placement of 63.0|g: two closely-spaced 63.0-keV gamma rays, an E1 to 6540, (16+) level (from 2004Wu08) and E2 to 6541, (15-) level. Based on intensity-balance arguments, this scenario is considered unlikely. 
M$from |a(expt) deduced from intensity balance. Value is consistent with E2(+M1), |d>1.25 or E2(+M3), |d<0.09 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$from I|g(369)/I|g(1223)=0.76 {I7}/30.2 {I8} (2017Ur03) 
$Uncertainty in B(E2)(W.u.) is 6.0 from T{-1/2} and 2.4 from |g-branching ratio, both added in quadrature 


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:
$Uncertainty in B(E2)(W.u.) is 0.6 from T{-1/2} and 0.2 from |g-branching ratio, both added in quadrature 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$from I|g(253)/I|g(620)=0.4 {I1}/23.0 {I7} (2017Ur03: 
$Uncertainty in B(E2)(W.u.) is 13.5 from T{-1/2} and 16.9 from |g-branching ratio, both added in quadrature 


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:
$Uncertainty in B(E2)(W.u.) is 8.7 from T{-1/2} and 10.8 from |g-branching ratio, both added in quadrature 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
E$from 2017Ur03 (in {+98}Y decay) 
M$from |g|g(|q) (2017Ur03) in {+235}U(n,F|g) reaction; (213.2|g)(1222.9|g)(|q): A{-2}=+0.356 {I23}, A{-4}=+1.152 {I48} consistent with 0 |) 2 |) 0 sequence. 


decay_energy_unit: KEV
decay_multipolarity: (M1+E2)
decay_comment:
E$from 2017Ur03 (in {+98}Y decay) 
M,MR$from (521.6|g)(1222.9|g)(|q): A{-2}=-0.073 {I21}, A{-4}=+0.016 {I43} (2017Ur03) consistent with 2 |) 2 |) 0 sequence 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$from |g|g(|q) (2017Ur03). d(Q/D)=-0.01 {I2} from (583.2|g)(1222.9|g)(|q): A{-2}=-0.076 {I12}, A{-4}=-0.017 {I27} for J(1806)=3. |d=-0.15 {I1} for J(1806)=1, and no solution for |d for J(1806)=2 (2017Ur03) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(620.5|g)(1222.9|g)(|q): A{-2}=+0.102 {I12}, A{-4}=-0.037 {I28}, consistent with 4 |) 2 |) 0 sequence (2017Ur03) 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
M$from (269|g)(1591|g)(|q): A{-2}=+0.340 {I25}, A{-4}=+1.169 {I48} (2017Ur03) consistent with 0 |) 2 |) 0 sequence 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(824.8|g)(1222.9|g)(|q): A{-2}=+0.15 {I5}, A{-4}=-0.11 {I12}, consistent with 4 |) 2 |) 0 sequence (2017Ur03) 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
$(686.2|g)(1590.9|g)(|q): A{-2}=+0.13 {I4}, A{-4}=+0.01 {I8}, consistent with 4 |) 2 |) 0 sequence (2017Ur03) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(647.1|g)(1222.9|g)(|q): A{-2}=+0.105 {I10}, A{-4}=-0.069 {I22}, consistent with 6 |) 4 |) 2 sequence (2017Ur03) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$Note that this |g is doubly placed in Adopted Levels, Gammas, the second component from 4756, (12+) level, and 837|g in 2012Mu08 should be placed from a 5590, (14+) level, above the 4756 level 


decay_energy_unit: KEV
decay_multipolarity: (E1)
decay_comment:
M$from |g|g(|q) and linear polarization data (2017Ur03); |d(Q/D)=-0.03 {I3} from (2574.4|g)(1590.9|g)(|q): A{-2}=-0.213 {I28}, A{-4}=+0.051 {I56} for J(4165)=1; |d(Q/D)=+0.71 {I8} for unlikely J(4165)=2, and -0.18 {I4} for J(4165)=3. 


decay_energy_unit: KEV
decay_multipolarity: E1
decay_comment:
M$from |g|g(|q) and linear polarization data (2017Ur03); |d(Q/D)=-0.01 {I1} from (2942.3|g)(1222.9|g)(|q): A{-2}=-0.24 {I1}, A{-4}=+0.01 {I1} for J(4165)=1; |d(Q/D)=-0.21 {I15} for unlikely J(4165)=3, and no solution for |d for J(4165)=0, 2 and 4. POL(2942.3|g)=+0.2 {I1} from (2942.3|g)(1222.9|g), |d=-0.01 {I1}. (2017Ur03) 


decay_energy_unit: KEV
decay_multipolarity: (E1)
decay_comment:
M$from |g|g(|q) (2017Ur03); |d(Q/D)=-0.03 {I7} from (2680.3|g)(1590.9|g)(|q): A{-2}=-0.28 {I7}, A{-4}=0.00 {I13}. 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
M,MR$from |g|g(|q) and linear polarization data in 2017Ur03. Preferred |d(E2/M1) value in 2017Ur03 from three possible values for J(4292)=6: -0.77 {I12}, +0.17 {I8} or -0.80 {I14} 
M,MR$from (1801.6|g)(1222.9|g+620.5|g+647.1|g)(|q) and polarization data (2017Ur03); A{-2}=+0.160 {I16}, A{-4}=+0.065 {I36} for J(4292)=6. No solution for |d(Q/D) for J(1802)=7. But |d(E2/M1)=+0.17 {I8} from |g|g(|q) in SF decay preferred by 2017Ur03 
$POL(1801.6|g)=+0.4 {I15} from (1801.6|g)(1222.9|g+620.5|g+647.1|g). |d(E2/M1)=-0.78 {I9} or +0.17 {I8} for J(4292)=6, |d(E2/M1)=+0.38 {I6} or +2.3 {I3} for J(4292)=7 (2017Ur03) 


decay_energy_unit: KEV
decay_multipolarity: E1
decay_comment:
M$from |g|g(|q) and linear pol data (2017Ur03); |d(Q/D)=+0.03 {I2} from (3229.8|g)(1222.9|g)(|q), A{-2}=-0.29 {I2}, A{-4}=0.00 {I5} for J(4452)=1; |d(Q/D)=-0.29 {I4} for unlikely J(4452)=3. POL(3229.8|g)=+0.5 {I2} from (3229.8|g)(1222.9|g), |d=+0.03 {I2} for J(4452)=1, and |d=-0.29 {I4} for unlikely J(4452)=3 (2017Ur03) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$this |g should be placed from a 5590, (14+) level, as in 2006Si36, and in the Adopted dataset. See also comment for 769|g 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$B(E2)(W.u.)|>11.5 and |<71.3 (deduced by 2018Wi09 using I|g(368.8)/I|g(1222.9)=1.6 {I2}/100 {I5} taken from {+98}Zr Adopted dataset in 2003Si07 evaluation of A=98. I|g(368.8)/I|g(1222.9)=2.5 {I2}/100.0 {I2} in the present Adopted dataset gives B(E2)(W.u.)|>18.1 and |<109 (evaluators) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)(W.u.)|>1.83 and |<11 (lower limit from 2017An15 and upper limit from 2018Wi09) 
$B(E2)(W.u.)=8.9 {I20} or <11 (2018Wi09), the measured value is based on an estimated upper limit of 40 counts ascribed to the 1222.9 peak, and the uncertainty on the first value is mainly from beam composition, and with a 3|s significance limit. It should be noted that no peak corresponding to 1222.9 keV was observed by 2018Wi09, as the spectrum in this energy region was dominated by a 1230-keV |g-ray peak from the first 3- state to the first 2+ state in {+98}Mo. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$Transition not adopted. Its placement is discrepant with adopted J|p. 
$(381)(536)(|q): A{-2}=-0.09 {I4}, A{-4}=-0.04 {I5} (2003Ur01) 


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$unweighted average of 212.531 {I9} and 212.62 {I7} in {+100}Y |b{+-} decay (732 ms); and 212.67 {I3} in {+248}Cm,{+252}Cf SF decay. Others: 212.5 {I1} and 212.5 {I3} in {+100}Y |b{+-} decay (0.94 s) 
M$|g|g(|q) in {+252}Cf SF decay and 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 118.59 {I7} in {+100}Y |b{+-} decay (732 ms), 118.6 {I2} in |b{+-} decay (0.94 s) and 118.65 {I5} in {+248}Cm,{+252}Cf SF decay 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
E$from level-energy difference 
TI$from branching(118|g)=0.68 {I6} from {+100}Y |b{+-} decay (732 ms) (1986Wo01) 
$q{-K}{+2}(E0/E2)=1.7 {I3}, X(E0/E2)=0.060 {I11}, |r{+2}(E0)=0.108 {I19} (2005Ki02, evaluation) 
$B(E0)(Wilkinson units)=0.41 {I13} 


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$weighted average of 351.960 {I12} and 352.08 {I8} in {+100}Y |b{+-} decay (732 ms); and 351.99 {I3} in {+248}Cm,{+252}Cf SF decay. Others: 351.8 {I2} and 351.9 {I3} in {+100}Y |b{+-} decay (0.94 s) 
M$|g|g(|q) in {+248}Cm,{+252}Cf SF decay and RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 0.8 {I3} from {+100}Y |b{+-} decay (732 ms) and 1.0 {I5} from {+100}Y |b{+-} decay (0.94 s) 
$|g not reported in {+248}Cm,{+252}Cf SF decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 547.37 {I7} in {+100}Y |b{+-} decay (732 ms); 547.4 {I2} in {+100}Y |b{+-} decay (0.94 s); and 547.5 {I1} in {+248}Cm,{+252}Cf SF decay. 
RI$weighted average of 26 {I4} in {+100}Y |b{+-} decay (732 ms); 37 {I6} in {+100}Y |b{+-} decay (0.94 s); and 34 {I7} in {+248}Cm,{+252}Cf SF decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$unweighted average of 665.98 {I7} in {+100}Y |b{+-} decay (732 ms); 665.8 {I2} in {+100}Y |b{+-} decay (0.94 s); and 666.23 {I7} in {+248}Cm,{+252}Cf SF decay. 
M,MR$from (666|g)(213|g)(|q) (1986Wo01) in |b{+-} decay (732 ms) and |D|p=no. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 878.54 {I8} in {+100}Y |b{+-} decay (732 ms); 878.6 {I2} in {+100}Y |b{+-} decay (0.94 s); and 878.8 {I1} in {+248}Cm,{+252}Cf SF decay. 
E$other: 878.6 {I2} from |b{+-} decay (0.94 s) 
RI$weighted average of 52 {I4} from {+100}Y |b{+-} decay (732 ms); 58 {I8} from {+100}Y |b{+-} decay (0.94 s); and 48 {I7} in {+248}Cm,{+252}Cf SF decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 631.84 {I8} from {+100}Y |b{+-} decay (732 ms) and 631.6 {I2} from {+100}Y |b{+-} decay (0.94 s) 
RI$weighted average of 22.0 {I20} from {+100}Y |b{+-} decay (732 ms) and 19 {I4} from {+100}Y |b{+-} decay (0.94 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 865.05 {I8} from {+100}Y |b{+-} decay (732 ms) and 865.0 {I2} from {+100}Y |b{+-} decay (0.94 s) 
RI$weighted average of 64 {I4} from {+100}Y |b{+-} decay (732 ms) and 71 {I12} from {+100}Y |b{+-} decay (0.94 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 983.59 {I8} from {+100}Y |b{+-} decay (732 ms) and 983.2 {I3} from {+100}Y |b{+-} decay (0.94 s) 
RI$weighted average of 34 {I4} from {+100}Y |b{+-} decay (732 ms) and 35 {I6} from {+100}Y |b{+-} decay (0.94 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1196.08 {I7} from {+100}Y |b{+-} decay (732 ms) and 1196.2 {I2} from {+100}Y |b{+-} decay (0.94 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 833.5 {I3} in {+100}Y |b{+-} decay (0.94 s); and 833.4 {I2} in {+248}Cm,{+252}Cf SF decay. 
RI$weighted average of 16 {I6} in {+100}Y |b{+-} decay (0.94 s); and 24 {I6} in {+248}Cm,{+252}Cf SF decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1185.4 {I3} in {+100}Y |b{+-} decay (0.94 s); and 1185.6 {I1} in {+248}Cm,{+252}Cf SF decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR$from |g|g(|q) in {+248}Cm,{+252}Cf SF decay (2019Ur01). Other: +1.4 {I+4-2} from |g|g(|q) in {+252}Cf SF decay (2008GoZL) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1110.5 {I3} from {+100}Y |b{+-} decay (732 ms) and 1110.1 {I3} from {+100}Y |b{+-} decay (0.94 s) 
RI$weighted average of 48 {I14} in {+100}Y |b{+-} decay (735 ms) and 88 {I16} in {+100}Y |b{+-} decay (0.94 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1441.2 {I3} from {+100}Y |b{+-} decay (732 ms) and 1441.4 {I2} from {+100}Y |b{+-} decay (0.94 s) 
RI$from {+100}Y |b{+-} decay (735 ms). Other: 73 {I12} from {+100}Y |b{+-} decay (0.94 s) 
$Branching ratios from the decays of two {+100}Y activities are in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR$from |g|g(|q) in {+248}Cm,{+256}Cf SF decay for J=6 for 1961 level. 
M$large D+Q mixing ratio favors M1+E2 over E1+M2 


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:
E$average of 404.0 in {+252}Cf SF decay and 403.4 in (|a,F|g) 
RI$from {+252}Cf SF decay. Uncertainty of 20% assumed for B(E2)(W.u.) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$1.7 {I3} per 100 fissions of {+252}Cf (1971Ch44) 
M$from |g(|q) and RUL 
$A{-2}=+0.46 {I9}, A{-4}=+0.56 {I19}, or A{-2}=+0.33 {I18} with A{-4}=0 in (fragment)|g(|q) (1972Wi15); A{-2}=+0.192 {I29} with A{-4}=0 (2010SmZZ); A{-2}=+0.26 {I4}, A{-4}=+0.02 {I5} (1976Wo04) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$1.26 {I19} per 100 fissions of {+252}Cf (1971Ch44) 
$A{-2}=+0.085 {I6}, A{-4}=+0.010 {I10} from 352|g-213|g-correlation (2008GoZL) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ I|g(497)/I|g(352)=0.47 (2005Ja12) 
RI$0.57 {I14} per 100 fissions of {+252}Cf (1971Ch44) 
$A{-2}=+0.095 {I8}, A{-4}=+0.013 {I13} from 497|g-352|g-correlation (2008GoZL) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M,MR$2008GoZL report |d(E2/M1)=+1.4 {I+4-2} from 850|g-352|g-correlation with A{-2}=-0.156 {I22}, A{-4}=+0.082 {I34}. Large mixing ratio and in-band transition favors M1+E2 over E1+M2. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$This |g is not confirmed in {+248}Cm,{+252}Cf SF decay (2019Ur02), also not reported in {+100}Y |b{+-} decay (0.94 s); thus omitted in the Adopted dataset. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$from Level-scheme Fig. 1 in Erratum, not listed in Table I of Erratum. (E|g confirmed with author of Erratum, Dec 12, 2022) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$from Table 1 in Erratum, 638.2 in Fig. 1 of Erratum. (E|g confirmed with author of Erratum, Dec 12, 2022) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$A{-2}=+0.25 {I12}, A{-4}=+1.09 {I16} for (119|g)(213|g)(|q) (1978Se03) is typical of a 0-2-0 cascade. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
E$from level energy. Transition seen in |bce data 
TI$from Branching(118|g)=0.68 {I6} (1986Wo01), deduced from weighted average of values from singles mode (|bce data) and in |g|g coincidence mode with 2439|g and 2480|g (1986Wo01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR$from (666|g)(213|g)(|q) (1986Wo01). Sign(|d) reassigned by the evaluators from the angular distribution pattern shown by the authors for the 666-213 cascade 
M$large |d(Q/D) favors M1+E2 over E1+M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$(351.99|g)(212.67|g)(|q): A{-2}=+0.100 {I7}, A{-4}=+0.010 {I9} (2019Ur01), consistent with 4 |) 2 |) 0 spin sequence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$(497.36|g)(351.99|g)(|q): A{-2}=+0.107 {I7}, A{-4}=+0.010 {I10} (2019Ur01), consistent with 6 |) 4 |) 2 spin sequence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(850.24|g)(351.99|g+212.67|g)(|q): A{-2}=-0.109 {I9}, A{-4}=+0.080 {I14} (2019Ur01), consistent with 4 |) 4 |) 2 spin sequence, with no solution for |d for 5 |) 4 |) 2 and 6 |) 4 |) 2 spin sequences 
MR$from |g|g(|q) (2019Ur01) for J(1415 level)=4, no |d solution for J(1415 level)=5 or 6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$(625.55|g)(497.36|g)(|q): A{-2}=+0.111 {I11}, A{-4}=+0.009 {I16} (2019Ur01), consistent with 8 |) 6 |) 4 spin sequence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(1291.6|g)(351.99|g+212.67|g)(|q): A{-2}=+0.018 {I33}, A{-4}=+0.186 {I46} (2019Ur02) consistent with 4 |) 4 |) 2 spin sequence 
MR$for J(1856 level)=4, no |d solution obtained for J(1856 level)=3 or 5 (2019Ur02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(900.00|g)(497.36|g+351.99|g+212.67|g)(|q): A{-2}=-0.017 {I15}, A{-4}=+0.026 {I21} (2019Ur01), consistent with 6 |) 6 |) 4 and 7 |) 6 |) 4 spin sequences, with no |d solution for 8 |) 6 |) 4 
MR$+0.74 {I7} for J(1962 level)=6 and +0.09 {I3} for J(1962 level)=7 from |g|g(|q) (2019Ur01), no |d solution for J(1962 level)=8 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(1566.05|g)(351.99|g+212.67|g)(|q): A{-2}=-0.076 {I59}, A{-4}=+0.005 {I87} (2019Ur01), consistent with 4 |) 4 |) 2 and 5 |) 4 |) 2 spin sequences, with no |d solution for 6 |) 4 |) 2 
MR$+1.0 {I4} for J(2131 level)=4 and +0.01 {I9} or +25 {I18} for J(2131 level)=5 from |g|g(|q) (2019Ur01), no |d solution for J(2131 level)=6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$(1643.8|g)(351.99|g)(|q): A{-2}=+0.077 {I49}, A{-4}=+0.003 {I69} (2019Ur02) consistent with 4 |) 4 |) 2, 5 |) 4 |) 2, and possibly also with 6 |) 4 |) 2 spin sequences 
MR$+0.24 {I9} or +3 {I1} for J(2208 level)=5; +0.32 {I13} for J(2208 level)=4 (2019Ur02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(1680.0|g)(351.99|g+212.67|g)(|q): A{-2}=+0.064 {I32}, A{-4}=+0.094 {I46} from {+252}Cf SF decay; and A{-2}=+0.111 {I35}, A{-4}=+0.107 {I56} from {+248}Cm SF decay (2019Ur02), both consistent with 4 |) 4 |) 2 spin sequence 
MR$for J(2245 level)=4, weighted average of |d(Q/D)=-1.6 {I3} from {+248}Cm SF decay and -2.0 {I4} from {+252}Cf SF decay, with no |d solution obtained for J(2245 level)=5 or 6 (2019Ur02) in both the studies. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$(739.0|g)(497.36|g)(|q): A{-2}=+0.107 {I17}, A{-4}=+0.003 {I25} (2019Ur01), consistent with 10 |) 8 |) 6 spin sequence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
MR$+0.92 {I12} for J(2526 level)=6 and +0.02 {I3} for J(2526 level)=7 from |g|g(|q) (2019Ur01), no |d solution for J(2526 level)=8 from {+252}Cf SF decay; +0.84 {I10} for J(2526 level)=6 and +0.05 {I3} for J(2526 level)=7 from |g|g(|q) (2019Ur01), no |d solution for J(2526 level)=8 from {+248}Cm SF decay 
$(1464.25|g)(497.36|g+351.99|g+212.67|g)(|q): A{-2}=-0.057 {I19}, A{-4}=+0.014 {I30} (2019Ur01), consistent with 6 |) 6 |) 4 and 7 |) 6 |) 4 spin sequences, with no |d solution for 8 |) 6 |) 4 
$(1464.25|g)(497.36|g+351.99|g+212.67|g)(|q): A{-2}=-0.037 {I17}, A{-4}=+0.040 {I30} (2019Ur01), consistent with 6 |) 6 |) 4 and 7 |) 6 |) 4 spin sequences, with |d solution for 8 |) 6 |) 4 from the measurement using {+248}Cm SF decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
$(1332.15|g)(625.55|g+497.36|g+351.99|g+212.67|g)(|q): A{-2}=-0.086 {I31}, A{-4}=-0.023 {I47} (2019Ur01), consistent with 9 |) 8 |) 6, with no |d solution for 8 |) 8 |) 6 and 10 |) 8 |) 6 
MR$from |g|g(|q) (2019Ur01) for J(3020 level)=9, no |d solution for J(3020 level)=8 or 10. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$other: I(212|g)/I(352|g)=37(13)/56(28) (1973Kh05) 
M$suggested by K/L ratio of measured conversion electrons in 1973Kh05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(1291.6|g)(summed |g)(|q): A{-2}=+0.018 {I33}, A{-4}=+0.186 {I46}; summed |g corresponds to 351.99|g and 212.67|g in the g.s. band. 
MR$for J(1856)=4, no |d solution obtained for J(1856)=3 or 5 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(1643.8|g)(351.99|g)(|q): A{-2}=+0.077 {I49}, A{-4}=+0.003 {I69} 
MR$+0.24 {I9} or +3 {I1} for J(2208)=5; +0.32 {I13} for J(2208)=4 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(1680.0|g)(summed |g)(|q): A{-2}=+0.064 {I32}, A{-4}=+0.094 {I46}, giving |d(1680.0|g)=-2.0 {I4} from {+252}Cf SF decay; and A{-2}=+0.111 {I35}, A{-4}=+0.107 {I56}, giving |d(1680.0|g)=-1.6 {I3} from {+248}Cm SF decay. Summed |g corresponds to 351.99|g and 212.67|g in the g.s. band. 
MR$for J(2245)=4 from {+248}Cm SF decay, no |d solution obtained for J(2245)=5 or 6. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$ (g{-K}-g{-R})/Q{-0}=-0.28 {I5} 
$(177|g)[134|g](98|g)(|q): A{-2}=+0.335 {I15}, A{-4}=+0.033 {I22} 
$(177|g)(134|g)(|q): A{-2}=+0.255 {I14}, A{-4}=+0.022 {I20} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$ (g{-K}-g{-R})/Q{-0}=-0.144 {I13} 
$(147|g)(104|g)(|q): A{-2}=+0.309 {I13}, A{-4}=-0.024 {I18} 
$(147|g)(223|g)(|q): A{-2}=+0.139 {I19}, A{-4}=-0.028 {I28} 


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 the intensity ratio I(K|a| x ray)/I|g(98) averaged over the gates on the 134,223,310,661,688,575 and 1300 transitions 


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$from the ratio I(K|a| x ray)/I|g(104) in the 217 gate 
E$|g not reported by 1987Oh01, but could be obscured by contamination. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$378.6|g-133.6 cascade is quadrupole (|DJ=2)-dipole (|DJ=1) 
$(378.6|g)(133.6|g)(|q): A{-2}=-0.20 {I1}, A{-4}=+0.07 {I2} 
$(378.6|g)(231.7|g)(|q): a{-2}=+0.10 {i1}, a{-4}=-0.08 {i2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$(298.7|g)(104.3|g)(|q): A{-2}=-0.07 {I1}, A{-4}=+0.04 {I2} 
$(298.7|g)(222.8|g)(|q): A{-2}=-0.05 {I2}, A{-4}=0.00 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$450.5 in figure 4 of 2004Ur06 
$(450.0|g)(176.4|g)(|q): A{-2}=-0.13 {I2}, A{-4}=+0.01 {I2} 
$(450.0|g)(310.0|g)(|q): A{-2}=+0.10 {I1}, A{-4}=+0.02 {I2}; A{-2}=+0.06 {I1}, A{-4}=+0.03 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$(401.8|g)(251.0|g)(|q): A{-2}=+0.04 {I2}, A{-2}=+0.02 {I4} 
$(401.8|g)(146.6|g)(|q): A{-2}=-0.10 {I1}, A{-4}=+0.04 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$|DJ=1,0 from |g|g(|q) 
$710.0|g-133.6 cascade is dipole (|DJ=1)-dipole (|DJ=1) 
$(710.0|g)(231.7|g)(|q): A{-2}=-0.15 {I4}, A{-4}=-0.02 {I5} 
$(710.0|g)(133.6|g)(|q): A{-2}==0.33 {I4}, A{-4}=-0.03 {I5} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$843.7|g-98.0 cascade is quadrupole (|DJ=2)-dipole (|DJ=1) 
$(843.7|g)(98.1|g)(|q): A{-2}=-0.08 {I5}, A{-4}=+0.12 {I7} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$(428.0|g)(152.1|g)(|q): A{-2}=-0.11 {I2}, A{-4}=+0.05 {I2} 
$(428.0|g)(298.7|g)(|q): A{-2}=+0.11 {I2}, A{-4}=+0.06 {I2}; A{-2}=+0.09 {I1}, A{-4}=-0.03 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(510.5|g)(202.3|g)(|q): A{-2}=-0.01 {I2}, A{-4}=-0.07 {I2} 
$(510.5|g)(378.6|g)(|q): A{-2}=+0.06 {I1}, A{-4}=+0.01 {I1} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
MR$ from average of -0.16 {I9} and -0.13 {I10} (2009Go18). 
$ |d(E2/M1)=-0.16 {I9} or -2.1 {I4} from (310.0|g)(98.2|g)(|q), assuming pure E2 for 310.0|g. This |d value is in agreement with theoretical value of -0.13 for 3/2[411] orbital. For 3/2[422] and 3/2[402] orbitals, theoretical |d=+0.44 and +0.22, respectively 
$ |d(E2/M1)=-0.13 {I10} or -2.2 {I6} from (222.9|g)(98.2|g)(|q), assuming pure E1 for 222.9|g 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$(222.9|g)(98.2|g)(|q): A{-2}=+0.08 {I2}, A{-4}=+0.02 {I3}. Correlation is attenuated due to 0.6 ns half-life of 98.2-keV level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$(310.0|g)(98.2|g)(|q): A{-2}=-0.12 {I2}, A{-4}=0.00 {I4}. Correlation is attenuated due to 0.6 ns half-life of 98.2-keV level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$ A{-2}=-0.073 {I27}, A{-4}=+0.149 {I40} for 908.0-326.5 |g|g cascade consistent with 4->4->2 cascade with mult=Q for 4 -> 4 transition 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ A{-2}=-0.139 {I30}, A{-4}=-0.065 {I44} for 1090.4-151.8 |g|g cascade consistent with 3->2->0 cascade with mult=Q for 3 -> 2 transition. Coefficients have been corrected by the authors for perturbed angular correlations. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ A{-2}=-0.118 {I27}, A{-4}=-0.007 {I39} for 697.0-486.6 |g|g cascade consistent with 5->6>4 cascade with mult=D for 5 -> 6 transition 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ A{-2}=-0.016 {I11}, A{-4}=-0.034 {I16} for 578.6-1090.4 |g|g cascade consistent with 4->3->2 cascade with mult=Q for 3 -> 2 transition and mult=D for 4 -> 3 transition 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ A{-2}=+0.125 {I38}, A{-4}=+0.03 {I6} for 967.4-486.6 |g|g cascade consistent with 8->6->4 cascade with mult=Q for both transition 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ A{-2}=-0.07 {I6}, A{-4}=-0.10 {I9} for 1961.5-326.5 |g|g cascade consistent with 7->6->4 cascade with mult=D for 7 -> 6 transition 


decay_energy_unit: KEV
decay_uncertain: S
decay_comment:
E$From level energy differences. Not observed directly, but required by the coincidence relationship 
RI$6 {I1} from intensity balance and Mult=E1 (|a=4.5 {I8}). Other: I|g=4 {I1} from intensity balance and Mult=M1 (|a=8.4 {I17}) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(884.3|g)(151.90)(|q): A{-2}=-0.028 {I22}, A{-4}=+0.047 {I32} 
MR$+0.37 {I4} or -5 {I1} for J(1036)=2, no |d solution obtained for J(1036)=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(763.80|g)(326.50)(|q): A{-2}=-0.061 {I38}, A{-4}=-0.221 {I57} 
MR$for J(1242)=3, no |d solution obtained for J(1242)=2 or 4 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$(1090.20|g)(151.90)(|q): A{-2}=-0.066 {I11}, A{-4}=-0.008 {I15} 
MR$for J(1242)=3, no |d solution obtained for J(1242)=2 or 4 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(891.1|g)(summed |g)(|q): A{-2}=-0.34 {I7}, A{-4}=+0.07 {I9} from {+248}Cm SF decay; summed |g corresponds to 326.50|g and 151.90|g in the g.s. band. 
MR$for J(1369)=3, no |d solution obtained for J(1369)=4 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(908.10|g)(326.50)(|q): A{-2}=-0.051 {I24}, A{-4}=+0.113 {I36}. Note: 326.50|g is from 4 |) 2, not 2 |) 0 as in Table II of 2019Ur02 
MR$+0.8 {I1} or -5 {I2} for J(1386)=4, no |d solution obtained for J(1386)=3, 5 or 6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(1059.70|g)(summed |g)(|q): A{-2}=-0.010 {I23}, A{-4}=+0.038 {I35}; summed |g corresponds to 326.50|g and 151.90|g in the g.s. band. 
MR$+0.60 {I8} for J(1539)=4, -0.14 {I3} for J(1539)=3, +0.08 {I3} for J(1539)=5, and no solution for J(1539)=6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(630.50|g)(486.45)(|q): A{-2}=+0.089 {I14}, A{-4}=+0.023 {I19} consistent with 8 |) 6 |) 4 cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(1174.40|g)(summed |g)(|q): A{-2}=-0.049 {I31}, A{-4}=-0.068 {I46}; summed |g corresponds to 326.50|g and 151.90|g in the g.s. band. 
MR$+0.03 {I5} or +9 {I3} for J(1653)=5; no solution for J(1653)=4 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$(697.05|g)(summed |g)(|q): A{-2}=-0.082 {I18}, A{-4}=-0.022 {I27}; summed |g corresponds to 486.45|g, 326.50|g and 151.90|g in the g.s. band. 
MR$for J(1662)=5, no |d solution obtained for J(1662)=4 or 6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E,RI$from {+248}Cm SF decay 
$(966.90|g)(summed |g)(|q): A{-2}=+0.242 {I35}, A{-4}=-0.031 {I56}; summed |g corresponds to 486.45|g, 326.50|g and 151.90|g in the g.s. band. 
MR$-0.26 {I3} for J(1932)=6, -0.60 {I12} for J(1932)=5, and +0.97 {I5} for J(1932)=7 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$(498.10|g)(summed |g)(|q): A{-2}=-0.030 {I16}, A{-4}=+0.011 {I23}; summed |g corresponds to 630.50|g, 486.45|g, 326.50|g and 151.90|g in the g.s. band. 
MR$for J(2093)=7, no |d solution obtained for J(2093)=6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(756.45|g)(630.50)(|q): A{-2}=+0.096 {I24}, A{-4}=-0.031 {I35} consistent with 10 |) 8 |) 6 cascade 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
I|g estimated from intensity balance of 109 keV level assuming no direct |b feeding of 109 keV level. Observation hindered by the presence of a 247.6 keV |g in {+103}Nb. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$uncertainty of 0.12 in 1999Jo01 seems too small, the evaluators assign the same energy as for the other placement from 3522 level 
RI$1 {I2} (1999Jo01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$45 {I+35-27} (1991Gr16) 
Placement from ({+32}S,3pn|g) (1997Ta10). 1991Gr16 placed this |g from a 274.5+x to 248+x 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
Placement from ({+32}S,3pn|g) (1997Ta10). 1991Gr16 placed this |g from a 248+x level. The 248+x level in 1991Gr16 is omitted here. 
DCO=0.47 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI$From branching ratios from {+40}Ca({+50}Cr,3p) in 1991Ju05 
M$deduced from angular distribution (1991Mi15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$Angular distribution A{-2}=-0.17 {i1}, A{-4}=+0.04 {i1}, 1991Ju05 
M$established in 1991Mi15 fixing |D' |p 


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:
$Other: R(DCO)=1.18 {i13} 1997We04 
$Angular distribution A{-2}=+0.15 {i1}, A{-4}=-0.01 {i2}, 1991Ju05 


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:
$Other: R(DCO)=1.09 {i2} from 1997We04 
$Angular distribution A{-2}=+0.13 {i1}, A{-4}=-0.09 {i1}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
Appears to be the 992 keV |g seen in 1991Ju05, and assigned to the 1954 keV level, except the 1063 keV |g should not be in coincidence as in 1993Pa05. However, the |g energy is taken from 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI$Deduced from branching ratios in 1991Ju05 
$Angular distribution A{-2}=-0.40 {i9}, A{-4}=+0.13 {i11}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$Other: R(DCO)=1.15 {i14} (1997We04) 
$Angular distribution A{-2}=+0.26 {i2}, A{-4}=-0.09 {i3}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$Angular distribution A{-2}=+0.32 {i1}, A{-4}=-0.08 {i2}, 1991Ju05 
$other: R(DCO)=1.24 {i14} (1997We04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$other: R(DCO)=1.08 {i1} (1991Ju05) and 0.90 {i5} (1997We04). 
$Angular distribution A{-2}=+0.24 {i1}, A{-4}=-0.06 {i2}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$other: R(DCO)=1.18 {i13} (1991Ju05). 
$Angular distribution A{-2}=0.28 {i3}, A{-4}=-0.10 {i3}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$other: R(DCO)=1.09 {i3} (1995Ju05). 
$Angular distribution A{-2}=+0.27 {i1}, A{-4}=-0.07 {i1}, 1991Ju05 
E$Branching comparing 1991Ju05 with 2003Pa09 suggests multiple placement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$likely the 297.9 |g seen in 1991Ju05 depopulating the earlier proposed 1349 keV level as several coincidences match 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$other: R(DCO)=1.06 {i1} (1995Ju05) and 0.97 {i4} (1997We04). 
$Angular distribution A{-2}=0.30 {i1}, A{-4}=-0.10 {i3}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Since this appears to be the 169 |g assigned to the 2905 {I19}/2{-} in 1991Ju05, this |g energy is used 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$other: R(DCO)=1.04 {i4} (1991Ju05) and 0.97 {i12} (1997We04). 
$Angular distribution A{-2}=+0.61 {i7}, A{-4}=-0.21 {i7}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$Other: R(DCO)=1.10 {i13} (1997We04). 
$Angular distribution A{-2}=+0.34 {i1}, A{-4}=-0.11 {i2}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$Other: R(DCO)=1.08 {i1} (1995Ju05) and 1.19 {i13} (1997We04). 
$Angular distribution A{-2}=0.23 {i1}, A{-4}=-0.05 {i4}, 1991Ju05 
M$supported by DCO and angular distribution 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$uncertainty of +0.01 for the DCO ratio quoted by 2003Pa09 seems to be a misprint. Evaluator increased this to +0.10. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$Other: R(DCO)=1.04 {i3} (1995Ju05) and 0.95 {i11} (1997We04). 
$Angular distribution A{-2}=+0.24 {i1}, A{-4}=-0.07 {i2}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$Possibly the 293.9 depopulating a 2988 keV level shown in 1991Ju05. Comparing branching ratios from intensities for the 291|g and 1145|g transitions obtained from ({+50}Cr,3p|g), the result is comparable to ({+32}s,3p|g), although for the same reaction 1991Ju05 is about half of that in 2003Pa09. 
$Angular distribution A{-2}=-0.58 {i4}, A{-4}=+0.15 {i5}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$Other:R(DCO)=1.14 {i3} (1995Ju05) and 0.90 (11) (1997We04). 
$Angular distribution A{-2}=0.33 {i2}, A{-4}=-0.08 {i2}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
E$Assigned to 2905 keV level in 1991Ju05. The 493|g and 997|g branching agrees with 2003Pa09 for placement from the 4776.8 keV level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$Other: R(DCO)=1.06 {i3} (1991Ju05). 
$Angular distribution A{-2}=+0.30 {i1}, A{-4}=-0.011 {i2}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$from R(DCO) 
$Other: R(DCO)=1.10 {I3} (1991Ju05). 
$Angular distribution A{-2}=+0.25 {i2}, A{-4}=-0.09 {i2}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$Used value from 2003Pa09 as 1991Ju05 has no uncertainties here either 
$Angular distribution A{-2}=-0.11 {i2}, A{-4}=-0.00 {i3}, 1991Ju05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$R(DCO)=0.60 {I1} 
M$E1 proposed in 1995Sc37 based on a stretched D from R(DCO) and decay of similar level in {+90}Tc 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$in table III (1993Bo33), I|g values of 244|g and 965|g are reversed: I|g(244|g)=26 {I7}, I|g(965|g)=10 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1983OxZZ. Other: 658.5 {I5} (1985Be12) 
RI$I|g=100 in 1983OxZZ normalized to 2.78 as in 1985Be12 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1983OxZZ. Others: 1154.0 (1985Be12), 1155.1 (1981Ga05). 
RI$others: 0.97 {I3} (1983OxZZ), 0.81 (1981Ga05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 1983OxZZ. Others: 1272.6 (1985Be12), 1272.0 (1981Ga05) 
RI$from 1983OxZZ. Others: 1.80 {I16} (1985Be12), 1.31 (1981Ga05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$most of the intensity must be contributed by an impurity. It is observed very weakly in (HI,xn|g) with I|g(949|g)/I|g(991|g)=0.014 (1993Bo33) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
A{-2}=+0.35 {I4}, A{-4}=+0.08 {I4}. R(DCO)=0.86 {I8} (1993Bo33) 
A{-2}=+0.28 {I3}, A{-4}=-0.05 {I1}. R(DCO)=0.69 {I2} (1993Si14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
A{-2}=-0.27 {I2}, A{-4}=+0.05 {I2}. R(DCO)=0.57 {I7} 
A2=-0.31 3, A4=-0.07 1. ^R(DCO)=1.29 2 (1993Si14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
A{-2}=+0.28 {I2}, A{-4}=-0.02 {I2}. R(DCO)=1.10 {I11} 
A2=-0.06 4, A4=-0.14 2. ^R(DCO)=0.87 1 (1993Si14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=-0.46 {I3}, A{-4}=+0.08 {I3}. R(DCO)=0.57 {I7} 
A2=-0.41 3, A4=-0.02 1. ^R(DCO)=1.62 2 (1993Si14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.39 {I3}, A{-4}=+0.01 {I3} (1993Bo33). 
A{-2}=-0.14 {I2}, A{-4}=+0.08 {I1}. R(DCO)=1.44 {I2} (1993Si14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
A{-2}=+0.30 {I2}, A{-4}=+0.01 {I7}. R(DCO)=1.05 {I12} 
A2=+0.14 3, A4=-0.02 1. ^R(DCO)=0.98 2 (1993Si14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=-0.44 {I3}, A{-4}=+0.05 {I4}. R(DCO)=0.51 {I8} 
A2=-0.53 3, A4=+0.07 1. ^R(DCO)=1.33 1 (1993Si14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=-0.39 {I2}, A{-4}=+0.02 {I2}. R(DCO)=0.52 {I9} 
A2=-0.31 3, A4=+0.06 1. ^R(DCO)=1.78 3 (1993Si14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
A{-2}=+0.30 {I2}, A{-4}=-0.03 {I2}. R(DCO)=0.98 {I20} (1993Bo33). 
A{-2}=-0.02 {I2}, A{-4}=-0.02 {I2}. R(DCO)=0.93 {I2} (1993Si14) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$from |g|g(|q) and |g(lin pol) in {+63}Cu({+31}p,3pn|g). Inconsistent with ce measurements in {+90}Mo |e decay which give M1+E2 with |d<0.36 


decay_energy_unit: KEV
decay_multipolarity: [M2+E3]
decay_uncertain: S
decay_comment:
E$From level-energy differences. For an attempt to measure the conversion electron energy see 1988GeZV. 
TI$From intensity balance of 124.7 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_uncertain: ?
decay_comment:
$DCO=1.2 {I6} (gate: 1774|g, |DJ=2, quadrupole) 
$POL=-0.08 {I4} 
M$Pol is inconsistent with E2 assignment. 


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 (|a,2n|g). Other I|g: 52 {I5} in ({+6}Li,3n|g), 67 in (|a,2np|g), 96 {I6} in (p,n|g) based on 55|' |g intensity. 
M Q from |g(|q) in ({+6}Li,3n|g). Other: Q+O, |d=-0.15 {I5} in (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2+E3)
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 Q+O from |g(|q) in ({+6}Li,3n|g) and (p,n|g); |D|p=yes from level scheme. 
MR weighted average of -0.11 {I6} in ({+6}Li,3n|g) and -0.15 {I5} in (p,n|g). 
Other E|g: 1982.5 {I6} in (p,|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 ({+6}Li,3n|g). 
M from |a(K)exp (deduced from the delayed components) and |a(exp) in (|a,2n|g). Not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average from (p,|g) and (p,n|g). Other E|g: 328.6 in (|a,2n|g). 
|d(D,Q)=-0.25|<|d|<+0.2 or <-3 or >+10 in (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:
M Q from |g(|q) in ({+6}Li,3n|g) and (|a,2n|g); not M2 from RUL. 
|d(Q,O)=-0.03 {I7} from (p,n|g); |d(E2,M3)<0.0023 from RUL. 
Other E|g: 2292.0 {I3} in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=AP;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=AP
decay_comment:
E weighted average from (|a,2n|g), (p,|g) and (p,n|g). 
M,MR from |g(|q) in (p,n|g); mult=E1+M2 disallowed by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average from {+91}Mo |e decay (64.6 s), (p,|g), (p,n|g). 
RI 73 {I3} in Mo |e decay (64.6 s), 96 {I4} in (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 from ({+6}Li,3n|g), (|a,2n|g) and (p,n|g). 
RI from (p,n|g). Other I|g: 57 from (|a,2n|g), 90 {I9} from ({+6}Li,3n|g). 
M from |g(|q) in (p,n|g) and RUL. 
MR weighted average of -0.42 {I5} from ({+6}Li,3n|g) and -0.49 {I+5-6} in (|a,2n|g). Other: -0.27 to -0.14, -4.8 to -3 in (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI weighted average from (|a,2n|g) and (p,n|g). 
M,MR D(+Q) from |g(|q) in (p,n|g); |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_uncertain: ?
decay_comment:
Placed on the basis of excitation function in (p,n|g) (1977Sc28) but B(E2)(W.u.) is unexpectedly large compared with other B(E2)(W.u.) values. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
E weighted average from ({+6}Li,3n|g) and (|a,2n|g). 
M D(+Q) from ({+6}Li,3n|g). 
MR average of -0.02 {I5} from ({+6}Li,3n|g), -0.04 {I5} from (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average from {+91}Mo |e decay (15.49 min), (|a,2n|g), (p,n|g). 
Other I|g: 122 in (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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
E weighted average from ({+6}Li,3n|g) and (|a,2n|g). 
Other I|g: 16 from (|a,2n|g). 
M D from (|a,2n|g); |D|p=yes 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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
E weighted average from ({+6}Li,3n|g), (|a,2n|g) and (|a,2np|g). 
RI from (|a,2n|g). 
M Q from |g(|q) in ({+6}Li,3n|g); not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E weighted average from ({+6}Li,3n|g), (|a,2n|g) and (|a,2np|g). 
M Q from |g(|q) in ({+6}Li,3n|g); not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E unweighted average of 2062.1 {I5} from ({+6}Li,3n|g), 2063.0 {I2} from (|a,2n|g) and 2062.5 {I3} from ({+19}F,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
CC=0.0190 2 IF MULT=M1(+E2). 
E weighted average of 254.5 {I5} from ({+6}Li,3n|g), 254.3 {I1} from (|a,2n|g), 254.4 {I3} from ({+19}F,4n|g). 
RI from (|a,2n|g). Other I|g: 163 {I16} from ({+6}Li,3n|g), 70 {I15} from ({+19}F,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E weighted average of 884.5 {I3} from ({+19}F,4n|g), 884.6 {I5} from ({+6}Li,3n|g), 884.5 {I2} from (|a,2n|g). 
RI uncertainty from (|a,2n|g) (0.5) seems unrealistically low; evaluator suspects a typographical error and adopts an order of magnitude higher uncertainty. 
M D from ({+19}F,4n|g), (D+Q) from (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
Other E|g: 497.9 from ({+6}Li,3n|g). 
M from ({+19}F,4n|g); not stretched Q, from |g(|q) for 497|g doublet 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:
Presumably the E|g=185.0 {I5}, d(+Q), |d=-0.05 {I5} transition placed from a 5455 level in (|a,2n|g) and ({+6}Li,3n|g) based on a different order for the 421|g-186|g-497|g cascade. 
M D(+Q) intraband |g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M D from DCO in {+76}Ge({+19}F,4n|g) but level scheme from that reaction requires a |DJ=2 transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E,M,MR from (|a,2n|g); however, |g was placed in that study from a 5270 level established assuming a different order for 422|g-186|g-497|g cascade. 
RI from ({+19}F,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
E from 1986Wa34. Other measurements: 104.5 keV {I1} (1951Ov01), 104.5 keV {I1} (1970He03). 
|a(K)exp: weighted average of 115 {I5} (1987La18) and 118 {I4} (1993Hi09). Other data: |a(K)exp=52 {I6} (1986Wa34); |a(exp) of the order of 50 (1951Ov01). 
|a(K)exp/|a(L+...)exp: from 1951Ov01. Others: 2.1 (1951Pr20), 2.0 {I1} (1954On06), 2.96 {I24} (1986Wa34). Note that authors quote K/L (1951Ov01) or K/(L+M) (1986Wa34), but L peaks presumably include M and higher shell lines also in these studies. 
M from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q+O
decay_comment:
A{-2}=+0.12 {I2}, A{-4}=-0.06 {I2}, A6=0.00 {I3}; (1976Br14); A{-2}=+0.18 {I4} (1977Ha49). 
MR -0.110 {I5} or >15 (1977Ha49); -0.11 {I6} or -10 {I4} (1976Br14). Larger solutions excluded by data from other reactions; datum of 1976Br14 preferred to that of 1977Ha49 because high precision of latter suggests a typographical error in reported uncertainty. 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
A{-2}=-0.38 {I6}, A{-4}=+0.03 {I5} (1976Ba50). Other: 1974Be36. 
M D+Q from |g(|q), not E1+M2 from RUL. 


decay_energy_unit: KEV
decay_multipolarity: (M1+E2)
decay_comment:
A{-2}=-0.10 {I6}, A{-4}=-0.06 {I6} (1976Ba50). Other: 1974Be36. 
M (D+Q) from |g(|q), not E1+M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
Other E|g: 1790.3 {I1} (1973BeYD). 
A{-2}=+0.28 {I2}, A{-4}=+0.02 {I3} (1976Ba50). Others: 1974Be36, 1979Fi06. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
A{-2}=+0.19 {I2}, A{-4}=0.00 {I1} (1979Fi06). Other: 1976Ba50. 
M (Q) from |g(|q), not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2)
decay_comment:
A{-2}=+0.15 {I4}, A{-4}=-0.03 {I3} (1979Fi06). Others: 1974Be36, 1976Ba50. 
M Q from |g(|q), |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_multipolarity: (E2)
decay_comment:
EKC From measured I(K| x ray) and I|g (1974Be36). 
ECC From intensity balance of the delayed components (1974Be36). 
E given as 50.1 in fig. 3 of 1979Fi06; it is unclear whether this is a measured value. E|g=50 (uncertainty unstated) in 1976Ba50. 
M from |a(K)exp and |a(exp). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
A{-2}=+0.29 {I4}, A{-4}=-0.03 {I2} (1979Fi06). Others: 1974Be36, 1976Ba50. 
M Q from |g(|q), not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=+0.42 {I7}, A{-4}=+0.08 {I6} (1974Be36); A{-2}=+0.34 {I3}, A{-4}=+0.01 {I3} (1976Ba50). 
M D+Q from |g(|q), not E1+M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI calculated from I(429|g):I(2414|g)=15.0 {I15}:26.0 {I26} (1974Be36) and I(429|g). Other I(429|g):I(2414|g)=11:15 (1976Ba50). 
M from |g(|q) in 1976Ba50. 
A{-2}=-0.18 {I5}, A{-4}=-0.04 {I6} (1976Ba50). Other: 1974Be36. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
MR -0.09<|d<0 from 1979Fi06. |d=+0.12 {I+4-3} from 1974Be36 is inconsistent with datum from 1979Fi06 and with result from ({+6}Li,3n|g). 
A{-2}=-0.22 {I4}, A{-4}=+0.06 {I4} (1979Fi06); A{-2}=-0.01 {I7}, A{-4}=+0.12 {I7} (1974Be36); A{-2}=-0.06 {I3}, A{-4}=-0.02 {I3} (1976Ba50). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
A{-2}=-0.34 {I8}, A{-4}=+0.07 {I8} (1976Ba50). 
RI I(450|g):I(819|g)=6.0 {I6}:61 {I6} in 1974Be36, 7:77.2 in 1976Ba50. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
A{-2}=+0.34 {I3}, A{-4}=+0.13 {I3} (1979Fi06); A{-2}=+0.47 {I8}, A{-4}=-0.05 {I6} (1974Be36); A{-2}=+0.30 {I3}, A{-4}=-0.06 {I4} (1976Ba50). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
A{-2}=+0.32 {I3}, A{-4}=-0.08 {I1} (1979Fi06). Others: 1974Be36, 1976Ba50. 
M Q from |g(|q), not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
A{-2}=-0.35 {I4}, A{-4}=+0.01 {I2} (1979Fi06). Others: 1974Be36, 1976Ba50. 
RI I(254|g):I(885|g)=7.0 {I7}:7.0 {I7} in 1974Be36, 15:10 in 1976Ba50. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
A{-2}=+0.29 {I7}, A{-4}=-0.03 {I5} (1979Fi06). Other: 1976Ba50. 
RI uncertainty much lower than that for strongest lines; evaluator suspects that it may be an order of magnitude too low. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
I|g=21.0 {I10}, A{-2}=-0.45 {I5}, A{-4}=-0.02 {I2} for doublet (1979Fi06); inconsistent with mult=stretched Q for either component. 
E for doublet; E|g=497.9 in fig. 3 of 1979Fi06. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=-0.56 {I9}, A{-4}=+0.17 {I7} (1979Fi06). Other: 1976Ba50. 
RI uncertainty much lower than that for strongest lines; evaluator suspects that it may be an order of magnitude too low. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
I|g=21.0 {I10}, A{-2}=-0.45 {I5}, A{-4}=-0.02 {I2} for doublet (1979Fi06). Inconsistent with mult=stretched Q for either component. 
E for doublet; E|g=497.2 in fig. 3 of 1979Fi06. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
MR -0.15 {I15} or +1.10 {I4}; larger solution improbable since level scheme implies |D|p=yes. 
A{-2}=+0.12 {I4}; A{-4}=-0.02 {I4} (1977Sc28). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR -0.27|<|d|<-0.14 or -4.8|<|d|<-3; E1+M2 excluded by RUL, even for the smallest of these |d values. 
A{-2}=+0.09 {I5}; A{-4}=-0.02 {I4} (1977Sc28). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M DCO=1.4 {I6}. E2 shown in the authors' email reply, but their level scheme indicates a |DJ=1 transition, making M1+E2 more likely. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M D from DCO=0.56 {I18}. M1 given in the authors' email reply, but E1 is implied by authors' level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M E1 shown in the authors' email reply, but a |DJ=0, |D|p=no transition is implied by authors' level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M DCO=1.8 {I9}. E2 indicated in the authors' email reply, but |DJ=1 in their proposed level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M D from DCO=0.40 {I15}. M1 shown in the authors' email reply, but E1 required by authors' level scheme. However, DCO seems far too low for a D, |DJ=0 transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q+D)
decay_comment:
M DCO=1.3 {I3}. E2 shown in the authors' email reply, but M1+E2 seems more likely based on authors' level scheme (where |DJ=1, |D|p=no). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M D from DCO=0.58 {I24}. Authors propose M1, but their level level scheme requires a |DJ=2 transition, inconsistent with DCO. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M E2 listed in the authors' email reply, but |DJ=1 from authors' level scheme, so M1+E2 seems more likely. DCO=1.2 {I6} is too imprecise to enable a definitive assignment. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M D from DCO=0.43 {I20}. However, M1 is shown in the authors' email reply and E2 is required by authors' level scheme. 
Coincident with 356|g, 422|g and 884|g, but not with 919|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 90.50 {I14} (p,n|g), 90.2 {I2} ({+7}Li,3n|g) and 90.4 {I2} (1978Ba18) (|g,n). 
M from |a(K)exp, |a(L+...)exp in (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:
M from |a(K)exp and |g(|q) in (p,n|g); |g(|q) in (|a,xn|g). 
|d(Q,O)=-0.012 {I21} from |g(|q), <0.0003 from RUL. |a(K)exp, |a(L+...)exp consistent with |d=0. 


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,MR from |a(K)exp, |a(L+...)exp and |g(|q) in (p,n|g), and |g(|q) in (|a,xn|g) and ({+3}He,p2n|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 122.5 {I2} in ({+7}Li,3n|g) and 123.07 {I17} in (p,n|g). 
RI weighted average of 32 {I5} in (p,n|g) and 30 {I5} in (d,t|g). 
M,MR from |a(K)exp, |a(L+...)exp, |g(|q) in (p,n|g); |g(|q) in ({+3}He,p2n|g), |g|g(|q) in (|a,xn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI weighted average from (p,n|g) and (d,t|g). 
M from |a(K)exp, |a(L+...)exp, |g(|q) in (p,n|g); |g(|q) in (|a,xn|g); |g|g(|q) in (|a,xn|g). 
MR +0.01 {I2} from |g(|q), |g|g(|q) in (p,n|g), (|a,xn|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=GE;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GE
decay_comment:
E from ({+7}Li,3n|g). 
M stretched D from |g(|q) in ({+7}Li,3n|g) and ({+3}He,p2n|g); |D|p=(yes) from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2+E3
decay_comment:
A{-2}=+0.083 {I15}, A{-4}=-0.128 {I16}; A{-6}=+0.111 {I19}. 
M Q+O from from |g(|q); RUL eliminates E2+M3 for prompt |g. 
I|g=95.8% {I11}. 


decay_energy_unit: KEV
decay_multipolarity: M1(+E2)
decay_comment:
|a(K)exp=0.064 {I6} (implying |d|<0.16) 
A{-2}=-0.33 {I2}, A{-4}=+0.01 {I2} (E(p)=3340); A{-2}=-0.25 {I1}, A{-4}=+0.02 {I2} (E(p)=4000); A{-2}=-0.16 {I1}, A{-4}=+0.02 {I1} (|a,xn|g). 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
A{-2}=+0.15 {I5}, A{-4}=-0.07 {I6} (E(p)=3340); A{-2}=+0.17 {I1}, A{-4}=-0.04 {I2} (E(p)=4000); A{-2}=+0.13 {I1}, A{-4}=0.00 {I1} (|a,xn|g). 
M,MR |a(K)exp=0.0119 {I11}, |a(L+...)exp=0.0013 {I2} (implying |d|?0); |d(Q,O)=-0.012 {I21} from |g(|q); <0.0003 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|a(K)exp=0.053 {I5}, |a(L+...)exp=0.0070 {I6} require |d=0.11 {I+13-11} and |<0.11, respectively. 
A{-2}=-0.38 {I2}, A{-4}=+0.03 {I2} (E(p)=3340); A{-2}=-0.28 {I1}, A{-4}=-0.02 {I1} (E(p)=4000); A{-2}=-0.19 {I1}, A{-4}=0.00 {I1} (|a,xn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
|a(K)exp=0.0116 {I16}, |a(L+...)exp=0.0023 {I8}. 
A{-2}=-0.16 {I27} A{-4}=+0.05 {I8} (E(p)=4000); A{-2}=-0.17 {I2}, A{-4}=0.00 {I2} (|a,xn|g). 
MR unweighted average of +0.06 {I9}, 0.25 {I5} and 0.30 {I+17-9} from |g(|q), |a(K)exp, |a(L+...)exp, respectively. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
|a(K)exp=0.109 {I11}, |a(L+...)exp=0.016 {I5} require |d|<0.15. 
A{-2}=-0.11 {I5}, A{-4}=+0.06 {I6} (E(p)=4000); A{-2}=-0.14 {I2}, A{-4}=-0.02 {I3} (E(p)=4500); A{-2}=-0.12 {I1}, A{-4}=+0.03 {I1} (|a,xn|g). 
123|g-358|g(|q): A{-2}=+0.02 {I3}, A{-4}=+0.04 {I3} and A{-2}=+0.17 {I4}, A{-4}=+0.07 {I4} (|a,xn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
|a(K)exp=0.0344 {I30}, |a(L+...)exp=0.0039 {I4} [giving |d=0.2 {I+1-2}, cf. |d=+0.009 {I+17-18} from |g|g(|q), |g(|q)]. 
A{-2}=-0.26 {I2}, A{-4}=+0.01 {I2} (E(p)=4000); A{-2}=-0.22 {I1}, A{-4}=0.00 {I2} (E(p)=4500); A{-2}=-0.14 {I2}, A{-4}=+0.02 {I2} (|a,xn|g). 
195|g-150|g(|q): A{-2}=-0.23 {I2}, A{-4}=+0.06 {I2} and A{-2}=-0.23 {I2}, A{-4}=0.00 {I2} (|a,xn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
A{-2}=-0.01 {I2}, A{-4}=+0.01 {I2} (E(p)=4000); A{-2}=-0.02 {I1}, A{-4}=0.00 {I2} (E(p)=4500); A{-2}=+0.05 {I3}, A{-4}=-0.02 {I4} (|a,xn|g). 
804|g-150|g(|q): A{-2}=+0.34 {I5}, A{-4}=-0.08 {I6} and A{-2}=+0.15 {I6}, A{-4}=+0.02 {I7} (E(p)=4500). Incorrectly identified as 954|g-150|g(|q) in table II of 1977Da01. 
M assumed to be pure Q. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
A{-2}=-0.04 {I1}, A{-4}=0.00 {I1} (E(p)=4000); A{-2}=-0.03 {I1}, A{-4}=0.00 {I1} (E(p)=4500); A{-2}=-0.04 {I1}, A{-4}=+0.01 {I1} (|a,xn|g). 
MR |<-3 or -0.34 {I+27-33}. Since adopted |D|p=yes, the first solution is unlikely. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=-0.05 {I3}, A{-4}=-0.01 {I3} (E(p)=4000); A{-2}=-0.09 {I1}, A{-4}=0.00 {I2} (E(p)=4500); A{-2}=-0.12 {I2}, A{-4}=+0.02 {I2} (|a,xn|g). 
MR |<-0.8 or -0.7 {I+6-16}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E from 1977Da01; not reported by other authors. 
A{-2}=+0.06 {I6}, A{-4}=-0.06 {I6} (E(p)=4500); A{-2}=+0.01 {I1}, A{-4}=-0.02 {I1} (|a,xn|g). 
921|g-164|g(|q): A{-2}=+0.20 {I11}, A{-4}=+0.12 {I13} (E(p)=4500); A{-2}=+0.14 {I11}, A{-4}=+0.11 {I12} (|a,xn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
A{-2}=-0.21 {I2}, A{-4}=+0.01 {I2} (E(p)=4500); A{-2}=-0.30 {I3}, A{-4}=+0.02 {I4} (|a,xn|g). 
1060|g-150|g(|q): A{-2}=-0.13 {I6}, A{-4}=-0.09 {I7} and A{-2}=-0.33 {I6}, A{-4}=+0.09 {I6} (E(p)=4500). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E from 1977Da01; not reported by other authors. 
A{-2}=-0.04 {I1}, A{-4}=-0.01 {I1} (E(p)=4500); A{-2}=-0.04 {I1}, A{-4}=+0.01 {I2} (|a,xn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
934|g-195|g(|q): A{-2}=+0.02 {I9}, A{-4}=-0.20 {I12} or A{-2}=-0.07 {I12}, A{-4}=-0.17 {I14} (E(p)=4500); A{-2}=-0.01 {I11}, A{-4}=+0.12 {I11} (|a,xn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.12 {I3}, A{-4}=-0.01 {I4} (E(p)=4500). 
1129|g-150|g(|q): A{-2}=+0.13 {I12}, A{-4}=-0.03 {I15} (E(p)=4500). 


decay_energy_unit: KEV
decay_multipolarity: D+Q
decay_comment:
A{-2}=-1.00 {I6}, A{-4}=+0.19 {I6} (E(p)=4500). 
1033|g-164|g(|q): A{-2}=-1.2 {I3}, A{-4}=+0.2 {I3} (E(p)=4500). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=-0.08 {I2}, A{-4}=+0.02 {I2} (E(p)=4500); A{-2}=+0.06 {I2}, A{-4}=-0.07 {I3} (|a,xn|g). 
1164|g-164|g(|q): A{-2}=+0.33 {I21} A{-4}=-0.30 {I27} (E(p)=4500); A{-2}=-0.02 {I14}, A{-4}=-0.02 {I14} (|a,xn|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
A{-2}=-0.10 {I3}, A{-4}=-0.06 {I4}; very different from |g(|q) from ({+7}Li,3n|g) which leads to the adopted Q+O assignment. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
A{-2}=-0.02 {I7}, A{-4}=+0.05 {I9}; very different from |g(|q) from ({+7}Li,3n|g) which implies a Q transition. 


decay_energy_unit: KEV
decay_multipolarity: E1
decay_comment:
E from 1978Ba18. Other: 88 {I5} (1958Du80). 
M from |a(K)exp=0.14 {I1} (1978Ba18) based on I(90|g)/I(K| x ray)=10.3. 


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:
B(E2)(W.u.)=8.74 {I25} from measured B(E2)|^=0.0175 {I5} in Coulomb excitation. 
E weighted average of 743.82 {I17} from (n,n'|g), 743.92 {I16} from from Coulomb excitation and 744.2 {I1} from (p,2n|g). 
M from |g(|q) in Coulomb excitation and RUL. 
MR abs(|d) from Coul. ex.; sign from |d=+0.25 {I+9-6} from (|a,p|g), +0.25 {I+13-11} from (n,n'|g), +0.30 {I+10-8} and +0.21 {I4} from |g(|q) in Coulomb excitation, +0.26 {I8} from (p,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 65.0 {I2} from (p,2n|g) and 64.6 {I3} from Coulomb excitation. 
RI from Coulomb excitation. Other: <1.0 from (p,2n|g). 
M D from RUL; |D|p=no 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:
B(E2)(W.u.) from measured B(E2)|^=0.0157 {I5}. 
E weighted average of 808.42 {I22} from (n,n'|g) and 808.58 {I15} from Coulomb excitation. 
RI from Coulomb excitation. 
M Q from ({+16}O,p2n|g); not M2 from RUL. 
|d(Q,O)=-0.03 {I+6-8} from (|a,p|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:
B(E2)(W.u.) from measured B(E2)|^=0.0241 {I8}. 
E from |e decay (6.85 h). 
M Q from ({+16}O,p2n|g); not M2 from RUL. 
|d(Q,O)=-0.18 {I18} from (|a,p|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:
B(E2)(W.u.) from measured B(E2)|^=0.0179 {I6}. 
E weighted average of 978.83 {I22} from (n,n'|g) and 979.01 {I18} from Coulomb excitation. Other E|g: 979.3 {I1} from (p,2n|g). 
M D+Q from |g(|q) in Coulomb excitation; not E1+M2 from RUL. 
MR from T{-1/2} and B(E2), sign from |g(|q) in Coulomb excitation and |g|g(|q) in (p,2n|g). Other |d: -0.40 {I+18-47} from (n,n'|g); -0.251 {I11}, abs(|d)<0.5 and |d=-0.4 {I3} or +2.1 {I3} from |g(|q) in Coulomb excitation; -0.27 {I+9-13} from (|a,p|g); -0.13 {I7} from |g|g(|q) in (p,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 103.7 {I2} from (p,2n|g), 103.94 {I15} from (n,n'|g) and 103.5 {I3} from Coulomb excitation. 
RI unweighted average of 10.9 {I9} from Coulomb excitation, 3 {I2} from (p,2n|g) and 14.4 {I24} from (n,n'|g). The weighted average from (n,n'|g) and Coulomb excitation is 10.1 {I22}. 


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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
E weighted average of 338.67 {I17} from (n,n'|g), 338.77 {I9} from Coulomb excitation and 338.6 {I2} from (p,2n|g). 
RI weighted average from (p,2n|g) and Coulomb excitation. 
M D+Q from (p,2n|g); |D|p=no from level scheme. 
MR from (p,2n|g). Other |d: -0.12 {I+7-9} from (|a,p|g), 0.00 {I16} from (n,n'|g), -0.14 {I7} and +0.13 {I11} from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=GT
decay_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=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
B(E2)(W.u.) from measured B(E2)|^=0.00257 {I23}. 
E weighted average of 1082.3 {I3} from (n,n'|g), 1082.6 {I3} from Coulomb excitation and 1082.6 {I2} from (p,2n|g). 
RI unweighted average of 29 {I4}, 30.9 {I15} and 40.0 {I23} from Coulomb excitation, 38 {I2} from (p,2n|g). Others: 51.5 {I15}, 37, 33, and 18 {I6} from (n,n'|g). The weighted average of all data is 39 {I4}. 
M D(+Q) from (n,n'|g); not E1+M2 from RUL. 
MR >1.8 from B(E2)|^=0.00257 {I23} in Coulomb excitation and adopted |g properties if T{-1/2}>2.8 ps. Other |d: -0.4 to +1.8 from (n,n'|g); -2.47 from |g(|q) in Coulomb excitation (2002Ka05), but uncertainty is unstated and the sign is inconsistent with |d from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E from (p,2n|g). 318.27 {I17} from (n,n'|g) for triplet, 318.16 {I20} from Coulomb excitation for doublet. 
M,MR from (p,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 from (p,2n|g). 318.27 {I17} from (n,n'|g) for triplet, 318.16 {I20} from Coulomb excitation for doublet. 
RI unweighted average of 32.1 {I19} and 61 {I3} from Coulomb excitation, 53 {I2} from (n,n'|g), 31 {I5} from (p,2n|g). The weighted average is 44 {I7}. 
M D(+Q) from (n,n'|g) and Coulomb excitation; adopted |D|p=no. 
|d(D,Q)=-0.04 {I9} or -10 {I+5-80} from (n,n'|g), >+0.07 from Coulomb excitation. 


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 553.07 {I25} from (n,n'|g), 553.3 {I4} from Coulomb excitation and 553.1 {I1} from (p,2n|g). 
RI weighted average of 49 {I4} and 57 {I6} from Coulomb excitation, 51 {I2} from (n,n'|g), 61 {I5} from (p,2n|g). 
M D(+Q) from (n,n'|g); adopted |D|p=no. 
MR from |g|g(|q) in (p,2n|g). Other |d: -0.3 {I+3-7} from (n,n'|g), -0.03 {I5} from (p,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:
B(E2)(W.u.) from measured B(E2)|^=0.00381 {I24}. 
E weighted average of 1297.2 {I4} from (n,n'|g), 1297.3 {I3} from Coulomb excitation and 1297.4 {I1} from (p,2n|g). 
RI weighted average of 100 {I6} and 100 {I6} from Coulomb excitation, 100 {I4} from (n,n'|g), 100 {I5} from (p,2n|g). 
M D+Q from (p,2n|g); not E1+M2 from RUL. 
MR 0.355 {I25} from B(E2)|^=0.00381 {I24} in Coulomb excitation and adopted branching and T{-1/2}; sign from |d=+0.31 {I9} from |g|g(|q) in (p,2n|g). Other: 0.33 {I+17-6} from Coulomb excitation. 


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,MR from (p,2n|g). Other |d: +0.10 {I+18-15} from |g(|q) in (n,n'|g) if J(1315)=5/2. 
M D+Q from (p,2n|g); |D|p=(no) 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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
E weighted average of 385.22 {I2}, 385.38 {I9} from |e decay (6.85 h), 385.07 {I17} from (n,n'|g) and 385.1 {I2} from (p,2n|g). 
M Q from ({+16}O,p2n|g); not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
Other E|g: 585.1 {I2} from (p,2n|g). 
RI from (p,2n|g). 
M D+Q from |g(|q) in (n,n'|g) and |g|g(|q) in (p,2n|g). 
MR from |g|g(|q) in (p,2n|g). Other |d: -0.55 {I+17-25} from |g(|q) in (n,n'|g), but that assumes J(1395 level)=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from (p,2n|g). 
RI weighted average of 23.5 {I12} from (n,n'|g) and 27 {I2} from (p,2n|g). 
M,MR D+Q from |g|g(|q) in (p,2n|g), |D|p=(no) 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 1482.8 {I4} from (n,n'|g) and 1483.5 {I1} from (p,2n|g). Other: 1483.8 {I2} from 2010Or01 in (p,2n|g). 
RI weighted average from (n,n'|g) and (p,2n|g). 
M,MR D+Q from |g|g(|q) in (p,2n|g), |D|p=(no) from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E from |e decay (6.85 h). 
RI average of 22.3 {I20} from |e decay (6.85 h), 30.2 {I21} from {+82}Se({+16}O,p4n|g) and 14 {I2} from (p,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=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,RI from |e decay (6.85 h). 
M D+Q from (p,2n|g); M1 from {+82}Se({+16}O,p4n|g). 
MR weighted average of -0.09 {I3} from (n,n'|g) and -0.11 {I2} from (p,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,RI from (p,2n|g). E|g=689.1 {I5} for doubly-placed |g and I|g=11 from suitably divided intensity in (n,n'|g). 
M not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=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,MR from (p,2n|g). Other E|g: 626.1 {I6} from (n,n'|g). 
RI weighted average of 33.3 {I18} from (n,n'|g) and 32 {I3} from (p,2n|g). 
M from |g|g(|q) in (p,2n|g); |D|p=(no) 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 from (p,2n|g). 
RI unweighted average of 29.8 {I18} from (n,n'|g) and 22 {I3} from (p,2n|g). 
M not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M D+Q from (p,2n|g) and (n,n'|g); |D|p=no from RUL. 
MR other |d: -0.40 {I5} or -1.60 {I15} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 1679.7 {I2} from (p,2n|g) and 1679.1 {I4} from (n,n'|g). 
RI weighted average of 38 {I2} from 1973Va09 in (n,n'|g) and 36 {I3} from (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,MR from (p,2n|g). 
RI weighted average from (n,n'|g) and (p,2n|g). 
M D+Q from |g|g(|q) in (p,2n|g); not E1+M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=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,MR from (p,2n|g). Other E|g: 1682.1 {I6} from (n,n'|g). 
RI weighted average of 58.3 {I21} (1973Va09) in (n,n'|g) and 54 {I4} from (p,2n|g). 
M D+Q from (p,2n|g); |D|p=no 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:
Other E|g: 1685.3 {I5} from (n,n'|g). 
Other I(737|g):I(1686|g): 100 {I5}:63.4 {I24} (1973Va09), 100:69 (1992De08) and 100:88 (1982Av05) in (n,n'|g). 
M not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI for multiplet; branching is from suitably divided I|g in (n,n'|g). This branch is not reported in (p,2n|g), so placement is indicated as tentative here. See comment on 646|g also. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement from (p,2n|g); note, however, that a 646.2|g deexcites the 1454 level (fed by 318|g from 1773 level in (n,n'|g) but not in (p,2n|g)), so assumed order of 318|g and 646|g may differ in the two reaction studies. 
M M2 and higher-order multipolarity excluded by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
B(M1)(W.u.)=0.043 {I9}, B(E2)(W.u.)=4.4 {I10} or B(M1)(W.u.)=0.046 {I10}, B(E2)(W.u.)=1.3 {I12} 
M D+Q from (p,2n|g); |D|p=(no) from level scheme. 
MR +0.32 {I6} or +0.17 {I8} from |g|g(|q) in (p,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
B(M1)(W.u.)=0.164 {I+11-12}, B(E2)(W.u.)=2.5 {I14} or B(M1)(W.u.)=0.157 {I12}, B(E2)(W.u.)=8 {I4}. 
M D+Q from |g|g(|q) in (p,2n|g); not E1+M2 from RUL for either possible value of |d. 
MR +0.14 {I4} or +0.26 {I6} from |g|g(|q) in (p,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:
RI note that branching from (n,n'|g) varies widely (34 {I6} (1973Va09), 127 (1992De08), 48 (1983Av05)). 
M D+Q from |g|g(|q) in (p,2n|g); not E1+M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=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,MR from (p,2n|g). 
RI weighted average of 28 {I3} from (n,n'|g) and 38 {I5} from (p,2n|g). 
M D+Q from |g|g(|q) in (p,2n|g); not E1+M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
M D+Q from |g(|q) in (n,n'|g); large |d favors |D|p=no. 
Other |d: +0.40 {I+4-8} or +4.5 {I5} from (n,n'|g) if J=15/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M D+Q from |g|g(|q) in (p,2n|g); not E1+M2 from RUL. 
MR from 2010Or01; supersedes |d=-0.14 {I5} (2005Mc13) in (p,2n|g), reported prior to correction of a data analysis problem in that study. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E,RI from {+93}Mo |e decay (6.85 h). Doubly placed in (n,n'|g) and differently placed in (p,2n|g), but the much stronger 1500|g accompanying the 689|g in those alternative placements is absent in {+93}Mo |e decay (6.85 h). 
M from ({+16}O,p4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI from {+93}Mo |e decay (6.85 h). Other: 133 from {+82}Se({+16}O,p4n|g); |g not reported in (n,n'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E 318|g in (n,n'|g) is multiplet deexciting both 1126 and 1297 levels; however, the relatively stronger 553|g and 1297|g, which also deexcite the 1297 level in (n,n'|g), were not observed by 1973Ta10. 
A{-2}=+0.07 {I16}, A{-4}=+0.07 {I23}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=+0.07 {I2} (1982Av05). 
MR +8 {I+62-4} also possible (1982Av05), but inconsistent with |d from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
A{-2}=-0.08 {I2} (1982Av05). 
|d=-1.7 {I+8-10} also possible (1982Av05) but inconsistent with adopted value. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
Branching=100.0 {I15} (1973Va09). Others: 100 (1992De08), 100 {I19} (1970Go46). 
A{-2}=+0.02 {I2} (1982Av05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
Branching=51.5 {I15} (1973Va09). Others: 37 (1992De08), 33 (1982Av05), 18 {I6} (1970Go46). 
A{-2}=-0.04 {I3} (1982Av05). 
MR from -0.38<|d<+1.8 (1982Av05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
A{-2}=+0.015 {I22} (1982Av05). 
|d(D,Q)=-0.04 {I9} or -10 {I+5-80} (1982Av05). 
Branching=53.1 {I20} (1973Va09). Other: 24 (1992De08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
Branching=51.0 {I20} (1973Va09). Others: 73 (1992De08), 40 (1982Av05), 64 {I15} (1970Go46). 
A{-2}=+0.04 {I3} (1982Av05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
Branching=100.0 {I25} (1973Va09). Other: 100 (1992De08). 
M,MR A{-2}=+0.03 {I3} (1982Av05); |d=+0.10 {I+18-15} if J(1315)=5/2 (1982Av05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
Branching=100 (1992De08 and 1982Av05). 
A{-2}=+0.02 {I2} (1982Av05). 
MR -0.55 {I+17-25} if 5/2 to 5/2 transition (1982Av05), but adopted J(1395)=(7/2-). 


decay_energy_unit: KEV
decay_comment:
E for doubly-placed |g. 1992De08 report 689|g-779|g coin. 
Branching=11 (1992De08; doublet I|g suitably divided). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
If the 704|g, instead, deexcited the (9/2+) member of the 1682 doublet proposed in 1992De08, its branching would be 50 {I2} (1973Va09) (other value: 72 (1982Av05)). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
A{-2}=+0.10 {I3} (1982Av05). 
|d from -0.25<|d(D,Q)<+1.0 if J=13/2 (1982Av05). 
Branching=100 {I5} (1973Va09). Other: 100 (1992De08,1982Av05). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E 744 or 950; order of coincident 744|g and 950|g not established because levels exist at both 744 and 950. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
If 1950|g deexcited the (9/2+) member of proposed 1950 doublet, its branching would be 109 {I6} (1973Va09). Others: 43 (1982Av05), 65 {I20} (1970Go46). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Placed by 1982Av05 and 1973Va09; absent in 1992De08, so shown as tentative. E|g from 1973Va09. 
Branching=24 from I(600|g)/I(2203|g) in 1982Av05 and branching(2203|g) in 1992De08. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Other E|g: 744.7 {I3} (1972Kr02). 
M pure E2 inconsistent with measured T{-1/2}. 
MR abs(|d) from B(E2) and T{-1/2} of the 744 level. From |g(|q), |d=+0.14 {I12} (2002Ka05), +0.30 {I+10-8} (1981Yo07), +0.21 {I4} (1972St23). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Magnitude from T{-1/2} and B(E2); sign from 2002Ka05. Other: abs(|d)|<0.5 from |g(|q) (1981Yo07); |d=-0.4 {I3} or +2.1 {I3} from |g(|q) (2002Ka05). 
Other E|g: 979.0 {I10} (1972Kr02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
Other E|g: 339.3 {I10} (1972Kr02). 
Branching=100.0 {I25} (2002Ka05), 100 {I6} (1981Yo07), 100 {I3} (1972St23). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
Other E|g: 1084.0 {I10} (1972Kr02). 
RI average of 29 {I4} (2002Ka05), 30.9 {I15} (1981Yo07), 40.0 {I23} (1972St23). 
MR >1.8 from B(E2), T{-1/2}>2.8 ps, and adopted |g properties. Other |d: -0.21 or -2.47 (uncertainty unstated) from |g(|q) (2002Ka05), but first solution untenable if T{-1/2}>2.8 ps. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_mixing_ratio_info: ;ERR=GE
decay_comment:
Unweighted average of Branching=61 {I3} (1981Yo07), 32.1 {I19} (1972St23). Possibly the 318|g is a multiplet as is observed in some other reaction studies. 
MR if J=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
Branching=100 {I6} (1981Yo07), 100 {I6} (1972St23). 
M D+Q transition; not E1+M2 from RUL. 
MR from B(E2), T{-1/2} and adopted branching. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
Other |a(K)exp: 1.7|*10{+4} {I3} from I(31|g)/I(K| x ray)=8.0|*10{+-5} {I10} (1977Mo07), assuming |w{-K}=0.75 {I3}; 2.4|*10{+4} {I9} (1999ZhZY). 
Other sub-shell ratios: K/(L+M)=0.18 {I2} (1964Ho08), 0.12 {I2} (1972FlZM); K/(L+M+...)=0.19 {I2} (1982Re09); L/(M+N+...)=3.8 {I4} (1982Re09). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M A{-2}=-0.32 {I23}, DCO=0.48 {I9}, P=+0.08 {I7} (2007Wa45). Note that sign of A{-2} is negative (2009Ho07); omission of sign by 2007Wa45 is a typographical error. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E|g from level energy difference. There is no evidence that 2010Or01 detected this |g, so the M4 multipolarity they indicate for it is presumed to have been taken from the literature. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M D,E2 from RUL and adopted level T{-1/2}. However, 2010Or01 indicate E2 multipolarity and propose an inconsistent (1/2+) to 7/2+ placement. If placement is correct, the authors' J|p assignment for the 1773 or 1127 level must be incorrect. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR +0.32 {I6} or +0.17 {I8} (2006Or09). 
Uncertainty in E|g is from 2010Or01. All other data are taken from 2006Or09; these supersede data from 2005Mc13 for which an analysis error resulted in different branching (49 {I4}) and |d (-0.23 {I7}) values. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR +0.14 {I4} or +0.26 {I6} (2006Or09). 
Uncertainty in E|g is from 2010Or01. All other data are taken from 2006Or09; these supersede data from 2005Mc13 for which an analysis error resulted in a different |d value (-0.13 {I6}). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M authors' attribution of E2 multipolarity to this |g appears to be erroneous; they place it connecting 11/2+ and 9/2- levels. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M from 2005Mc13. 
MR from 2010Or01. |d=-0.14 {I5} from (1326|g)(656|g)(|q) (2005Mc13); however this is presumably erroneous due to the data analysis problem reported in the authors' erratum. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR -1.9 {I8} reported by 2010Or01 is inconsistent with authors' stated B(E2)(W.u.); evaluator presumes it to be a typographical error and adopts the value (=-0.19 {I8}) given by 2007Or01. 


decay_energy_unit: KEV
decay_multipolarity: M4
decay_comment:
$|a(K)exp=2.56|*10{+4} {I9} from ratio of K xrays and 30.76|g (2020Ho10). Measurement is |a(K)|w(K)=1.92|*10{+4} {I7} and 2020Ho10 uses |w(K)=0.751 {I4} to deduce |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3
decay_comment:
EKC$Others: 800 {i50} (1961Ci07), 570 {i100} (1962Ki08), 1600 {i350} (1962Yi01), 780 {i70} (1969SaZP, unpublished), 970 {i150} (1971Ge11). All values are from measurements of I(K| x ray)/I|g(40.9|g) corrected by 1985Mu05 for |w(K)=0.747 (1979Kr13). 
$|a(K)exp/|a(L+...)exp from 1962Ki08. Other: |a(K)exp:|a(L)exp:|a(M)exp=31:100:36 (1950Ca10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
EKC$value corrected for the contribution of the L+M line of a lower-energy transition using the theoretical coefficient for the L+M conversion and the associated K-line intensity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
EKC,ELC+$From isomeric-delayed radiation using the pulsed beam. |a(K)exp=0.109 {i10} from in-beam measurement. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
EKC$value corrected for the contribution of the L+M line of a lower-energy transition using the theoretical coefficient for the L+M conversion and the associated K-line intensity. 
MR$-0.3<|d<+0.7 from n-|g(|q) angular correlations (1979Fe10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.04 {i12} or +3.7 {i11} from n-|g(|q) angular correlations (1979Fe10) if mult.=M1+E2, J=4 in conflict to the adopted value. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$0.53<|d<1.32 from n-|g(|q) angular correlations (1979Fe10) if mult.=E1+M2, J=3 in conflict to the adopted value. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$4765.5 quoted in Table 2 of 2020Kn01 could be a typo, since 4765.5+58.0 add up to 4824, about 10 keV away from its parent level at around 4814 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Placement shown as (33/2+) to (29/2+) in table I of 2005Bu08 but (29/2+) to (25/2+) in authors' figure 5. Note that ordering of the 1069.1-872.6 cascade is not established 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Placement shown as (29/2+) to (25/2+) in table I of 2005Bu08 but (33/2+) to (29/2+) in authors' figure 5. Note that ordering of the 1069.1-872.6 cascade is not established 
$R(ADO)=1.26 {i15} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
RI$I{-|g}(235)/I{-|g}(756)=0.49 {i6} from Limitation of Relative Statistical Weight, LRSW, analysis (1985ZiZY,1992Ra09) of the six values 0.34 {i13} (1969Br29), 0.6 {i2} (1969Fo01), 0.4 {i1} (1972Er08), 0.67 {i7} (h. H. Hansen et al., 1973, as quoted in 1975De17), 0.54 {i3} (1975De17), and 0.43 {i2} (1976Ho04). This analysis increases the uncertainty of the value of 1976Ho04 from 0.02 to 0.026 to reduce its relative weight from 63% to 50%. The resulting internal uncertainty is 0.019, the reduced-|h{+2} is 3.2, the external uncertainty is 0.03, and the lrsw analysis expands the final uncertainty to 0.06 to include the most precise value of 0.43. Other values are 4 (1966Ts01), <0.4 (1967Br21), and 4.5 {i19} (1968BoZX). Since the six values used are discrepant, one can also deal with this discrepancy by use of the RAJEVAL method (1992Ra08) which increases three of the uncertainties and gives 0.438 {i19} or by the Normalized Residual method (1992Ja06) which increases two of the uncertainties and gives 0.447 {i31}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$I{-|g}(724)/I{-|g}(756)=0.814 {i4} from weighted average of the following 11 values: 0.781 {i24} (1965Br37), 0.81 {i6} (1966Ts01), 0.776 {i13} (1967Br21), 0.825 {i11} (1968BoZX), 0.810 {i10} (1969Br29), 0.825 {i16} (1969Fo01), 0.788 {i16} (1969GuZV), 0.770 {i20} (1972Er08), 0.829 {i5} [h. H. Hansen et al., report eur-5038e (1973)], 0.811 {i3} (average of 2 values in 1975De17, and in the analysis the uncertainty was increased to 0.0037 to reduce its relative weight to 50%), and 0.789 {i14} (1976Ho04). The reduced-|h{+2}=2.88 and the fit is dominated by the Hansen et al. and 1975De17 values. 
MR$weighted av of -0.12 {i2} (1976Kr01) and -0.09 {i4} (1965Co18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from 100.0=I{-|g+ce}(756) + I{-|g+ce}(724) + I{-|b-}(235) + I{-|b-}(0) with I{-|b-}(235)=1.08 {i7}, I{-|b-}(0)=0.0010 {i3}, I{-|g}(724)/I{-|g}(756)=0.814 {i4}, |a(724)=0.00157 {i4}, and |a(756)=0.00142 {i3}. 
MR$weighted av of +0.16 {i6} (1976Kr01) and +0.08 {i9} (1965Co18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
E$from 1976Ho04 
M$from |a(K)exp and K/LMN 
CC$|a(M4, theory)|*0.975 {i5} as suggested by 1990Ne01 
EKC$Weighted av of 2.36 {i22} and 2.37 {i23} from ce(K)(236|g)/ce(K)({+152}Sm 122|g)=3.45 {i30} and ce(K)(236|g)/ce(K)({+152}Gd 344|g)=76.5 {i68} (1969Fo01) and |a(K)({+152}Sm 122|g)=0.685 and |a(K)({+152}Gd 344|g)=0.031 (1989Pe11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Placement shown as (33/2+) to (29/2+) in table I of 2005Bu08 but (29/2+) to (25/2+) in authors' figure 5. Note that ordering of the 1069.1-872.6 cascade is not established. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|a(K)(E2)=0.0351, |a(K)(M1)=0.0164 
M$from |a(K)exp=0.039 {I6} (1971Mu13); from |a(K)exp<0.02 from |gce/|g|b{+-} (1970Mi02) 
MR$-0.04 {I3} or +3.9 {I+5-4} (1978Kr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|a(K)(E2)=0.0113, |a(K)(M1)=0.00707 
M$from |a(K)exp=0.014 {I2} (1971Mu13); |a(K)exp=0.0050 {I25} from |gce/|g|b{+-} (1970Mi02) 
MR$-0.04 {I3} or +4.0 {I5} (1978Kr03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$poor fit in the level scheme. Level-energy difference=557.44. This |g-ray energy was not used in the fitting procedure 


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$From |g-ray intensity balance at 930.88 level |a(28.4|g)|<5.9, and a comparison with theoretical |a(E2)=1084 and |a(M1)=8.50. 
BM1W>0.59 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
%I|g=0.22 {I6} 
M from intensity balance at 930.88 level |a(28.4|g)|<5.9, and a comparison with |a(E2)=1084 and |a(M1)=8.63 


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:
M$proposed by 1999Ge01 from ce spectrum and also based on the 28|g(E2)-185|g(M1)-173|g(M1) cascade from 735,(8-) level. But M1 from |a(K)exp=4.7 {I5} in 1986LhZX 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average (NRM) of 400.48 {I4} (1979Bo26, curved-crystal), 400.81 {I8} (2007Ri01,2007RiZZ) and 400.5 {I1} (1982VoZP). Uncertainty in 2007RiZZ was doubled in the NRM procedure. 
RI$weighted average of 20.5 {I25} (2007RiZZ) and 19.2 {I8} (1982VoZP). 
TI$20 (2007Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 498.08 {I25} (2007Ri01,2007RiZZ) and 498.0 {I3} (1982VoZP) 
RI$weighted average of 0.80 {I15} (2007RiZZ) and 0.72 {I8} (1982VoZP) 
TI$0.80 (2007Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
E$weighted average of 103.73 {I10} (2007Ri01,2007RiZZ) and 103.7 {I1} (1982VoZP) 
RI$unweighted average of 0.91 {I8} (2007RiZZ) and 0.67 {I6} (1982VoZP) 
TI$1.10 (2007Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 504.25 {I4} (1979Bo26, curved-crystal data) and 504.37 {I8} (2007Ri01,2007RiZZ) 
RI$from 2007RiZZ. Others: 31 {I4} (1982VoZP,1981DeYV), 19 {I2} (1989WaZV) 
TI$30.3 (2007Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 253.3 {I5} (2007Ri01,2007RiZZ) and 253.4 {I1} (1982VoZP) 
RI$weighted average of 0.12 {I6} (2007RiZZ) and 0.21 {I3} (1982VoZP) 
TI$0.12 (2007Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 303.8 {I8} (2007Ri01,2007RiZZ) and 303.2 {I1} (1982VoZP) 
RI$weighted average of 0.16 {I6} (2007RiZZ) and 0.22 {I3} (1982VoZP) 
TI$0.16 (2007Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 704.1 {I3} (2007Ri01,2007RiZZ) and 703.3 {I2} (1982VoZP) 
RI$weighted average of 0.58 {I14} (2007RiZZ) and 0.36 {I5} (1982VoZP) 
TI$0.58 (2007Ri01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
RI$deduced from I(|g+ce)(173.3|g)+I|g(358.6|g)=189 and |a(34|g)=2.55. Other: |?640 (1980MoZJ) 
M$proposed by 1999Ge01 from ce spectrum and also based on the 28|g(E2)-185|g(M1)-173|g(M1) cascade from 735,(8-) level. But M1 from |a(K)exp=4.7 {I5} in 1986LhZX 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$deduced from |S(I(|g+ce) of |g rays from 707)=252 and |a(28|g)=110.5 
M$|a(K)exp=57 {I18} (1986LhZX). Also ce data (L-conversion line) from 1999Ge01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E$weighted av from |b{+-} decay, {+252}Cf SF decay, {+248}Cm SF decay 
If E1 B(E1)(W.u.)=1.5|*10{+-5} {I2} 


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
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$|d{+2}(E2/M1)=0.010 {I7} (deduced by 2017Ha12 from |g-ray branching ratios) 
$Uncertainty of 0.02 in B(E2) value in Table III of 2017Ha12 seems a misprint. Compiler obtains a factor of 10 larger uncertainty. Either the uncertainty is a misprint in 2017Ha12 or the authors did not take into account large uncertainty in the value of |d(E2/M1) 


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:
RI$I|g(435)/I|g(217)=0.52 {I8} (measured by 2017Ha12). Other: 18 in {+103}Nb Adopted dataset in the ENSDF database (Mar 2009 update) 


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:
$Note that B(M2)(W.u.) exceeds RUL(M2)=1 by almost a factor of 4. Allowing for |d(E3/M2)=1 does not remove this inconsistency, since B(E3)(W.u.) is also much larger than RUL(E3)=100. It is possible that the problem lies in an incomplete decay scheme of the isomer since two |g rays of 63.5 and 147.5 are still unplaced 


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:
$Note that B(M2)(W.u.) exceeds RUL(M2)=1 by almost a factor of 4. Allowing for |d(E3/M2)=1 does not remove this inconsistency, since B(E3)(W.u.) is also much larger than RUL(E3)=100. It is possible that the problem lies in an incomplete decay scheme of the isomer since two |g rays of 63.5 and 147.5 are still unplaced 
$E|g=204.6 (1999Ge01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$Others: I|g(196|g)/I|g(312|g)=132 {I24} in 2012Ka36 in contradiction with 2011Wa03. The authors in 2012Ka36 stated that the 196.2|g is contaminated in their work by a 197.1 keV |g ray, produced in the {+19}F(n,n') reaction, and that a correction to I|g(196.2|g) was applied 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$From I|g(117|g)/I|g(312|g)=76 {I28} and I|g(312|g)=62 {I20} (2011Wa03). Note that I|g(117|g)/I|g(312|g)=126 {I20} in 2012Ka36 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$I|g(196|g)/I|g(312|g)=61 {I24} in 2011Wa03, but 132 {I24} in 2012Ka36. The authors in 2012Ka36 stated that the 196.2|g is contaminated in their work by a 197.1 keV |g ray, produced in the {+19}F(n,n') reaction, and that a correction to I|g(196.2|g) was applied 


decay_energy_unit: KEV
decay_comment:
M$ possibly stretched quadrupole from observation of relative intensity of 444|g at 40|'-163|' geometry (1991Ge01) 


decay_energy_unit: KEV
decay_comment:
M$ quadrupole (E2) from observation of 58% {I8} counts at 40|'-163|' angles and comparison to 59-61% counts for a known first 2+ to 0+ |g ray in {+84}Zr (1991Ge01). But the assignment is not firm 
E$ 443.8 {I3} (1991Ge01), 443.8 (1997Bu17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
CC$Symmetrized from |a(exp)=11.5 {I+69-31} from intensity balance in {+58}Ni({+32}S,2pn) 
M,MR$From |a(exp) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
CC$Symmetrized from |a; |a(exp)=11.5 {I+69-31} from intensity balance in {+58}Ni({+32}S,2pn) 
M,MR$From |a(exp) 
RI uncertainty given as +120-90. 
M,MR from |a(exp) of 11.5 {I +69-31} calculated from intensity balance in {+58}Ni({+32}S,2pn). A small mixture of E2, |d=0.05 {I+12-4}, is allowed. 


decay_energy_unit: KEV
decay_comment:
E level energy difference is 908.45 {I11}. E The significant deviation of the energy level E and contribution to a large chi-square fit to the E level energies suggest a larger uncertainty than given 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E level energy difference is 1105.28 {I11}. E The significant deviation of the energy level E and contribution to a large chi-square fit to the E level energies suggest a larger uncertainty than given 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$In Table 1 of 1991Wi15, this |g transition was shown depopulating a level at 3842 keV and feeding a 17/2+ level. However, this would feed the 2743 keV level at 21/2+. On the other hand, their level scheme shows this transition to come from the 2963 keV level, and this is in agreement with the level scheme shown in 1993IdZY. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$0.0 {I4} or -5.2 {I+9-13} 
M$D+Q from R(DCO) in {+58}Ni({+36}Ar,|a2p|g), |D|p=no from assumed band structure 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.02 {I6} or -5.6 {I+13-24} 
M$D(+Q) from R(DCO) in {+58}Ni({+36}Ar,|a2p|g), |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
MR$-0.01 {I4} or -4.8 {I+8-11}, the latter is excluded by comparison to RUL. 
M$D(+Q) from R(DCO) in {+58}Ni({+36}Ar,|a2p|g), |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+1.0 {I+5-3} or -0.7 {I3} 
M$D(+Q) from R(DCO) in {+58}Ni({+36}Ar,|a2p|g), |D|p=no from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR$-0.21 {I+11-14} or -2.4 {I+7-9} 
M$D(+Q) from R(DCO) in {+58}Ni({+36}Ar,|a2p|g), |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.02 {I5} or -4.6 {I+9-13} 
M$D(+Q) from R(DCO) in {+58}Ni({+36}Ar,|a2p|g), |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R(DCO)=1.09 {I3} (1992We02), 1.12 {I3}, POL=+0.07 {I1} (2007An21), A{-2}=+0.22 {I2}, A{-4}=-0.15 {I3}, POL=+0.068 {I7} (2013Zh10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R(DCO)=1.04 {I2} (1992We02), 1.04 {I1}, POL=+0.10 {I2} (2007An21), A{-2}=+0.27 {I2}, A{-4}=-0.08 {I3}, POL=+0.11 {I3} (2013Zh10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$R(DCO)=0.51 {I3} (1992We02,1994Ka20) 
MR$-0.05 {I3} or -4.0 {I4} (1994Ka20), the latter is excluded by comparison to RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
$R(DCO)=0.55 {I5} (1992We02,1994Ka20) 
MR$-0.01 {I4} or -4.8 {I+8-11} (1994Ka20), the latter is excluded by comparison to RUL. 


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$average of values from (HI,xn|g) and {+89}Mo IT decay 
M$|a(K)exp=0.28 {I6} (1991He04) in {+89}Tc |e decay (12.9 s) gives |d(M4/E3)=0.39 {I12}, but this admxiture of M4 gives unrealistically large B(M4)(W.u.). RUL=10 for B(M4)(W.u.) suggests negligible |d(M4/E3). Value of |a(K)exp=0.28 {I6} (1991He04) agrees better with M3. Multipolarity assignment here is essentially from systematics supporting 1/2- for the isomer and dominant E3 multipolarity to 7/2+ level, and only marginally supported by large value of |a(K)exp 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (E3)
decay_comment:
E$268.8 {I3} (1983OxZZ) 
$I|g(269|g)/I|g(119|g)=115 {I30}/100 (1983OxZZ) for the composite activity 
M$|a(K)exp=0.28 {I6} (1991He04) in {+89}Tc |e decay (12.9 s) gives |d(M4/E3)=0.39 {I12}, but this admxiture of M4 gives unrealistically large B(M4)(W.u.). RUL=10 for B(M4)(W.u.) suggests negligible |d(M4/E3). Value of |a(K)exp=0.28 {I6} (1991He04) agrees better with M3. Multipolarity assignment here is essentially from systematics supporting 1/2- for the isomer and dominant E3 multipolarity to 7/2+ level, and only marginally supported by large value of |a(K)exp 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$spans minimum and maximum limits of |d=-2.4 {I7} (from |g(|q)) and -3.7 {I+17-13} (from R(DCO)) (1993Ka24) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$D from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), |D|p=yes from level scheme 
RI$weighted average of 3.8 {I12} from {+90}Tc |e decay (50.7 s), 5.0 {I3} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), 12.5 {I5} from {+66}Zn({+28}Si,2p2n|g), 8.9 {I16} ({+40}Ca,|a4p|g), and 4.6 {I4} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from ({+3}He,3n|g). Other 80 {I50} in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), 14.2 {I22} in {+90}Tc |e decay (50.7 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 481.7 {I3} ({+90}Tc |e Decay (50.7 s)), 482.40 {I15} ({+58}Ni({+3}Ar,4p|g),({+35}Cl,3p|g)), 482.4 {I10} ({+90}Zr({+3}He,3n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$other: 15.5 {i19} in ({+3}He,3n|g) 
M$D from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), |D|p=yes 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:
M$Q from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), M2 excluded by comparison to RUL. 
RI$weighted average of 54 {I8} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), 64.3 {I11} from {+66}Zn({+28}Si,2p2n|g), 53.6 {I9} ({+40}Ca,|a4p|g). Other: 7.0 {I7} from ({+3}He,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$weighted average of 63.9 {i22} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), 34.3 {i19} ({+40}Ca,|a4p|g), and 46 {i6} from ({+3}He,3n|g) 
M$D from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), |D|p=yes 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:
M$Q from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), M2 excluded by comparison to RUL. 
RI$from ({+40}Ca,|a4p|g). Other: 95 {I14} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|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:
RI$weighted average of 54 {i8} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), 52 {i4} from ({+28}Si,2p2n|g) and 57 {i3} from ({+40}Ca,|a4p|g). 
M$D from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), |D|p=yes 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:
M$D+Q from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), E1+M2 excluded by comparison to RUL 
RI$weighted average of 44 {I3} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g) and 64 {I2} from ({+40}Ca,|a4p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$weighted average of 100 {I15} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g) and 100 {I2} from ({+40}Ca,|a4p|g). Other: 39 {I3} from ({+28}Si,2p2n|g) 
M$(D+Q) from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), E1+M2 excluded by comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$weighted average of 39 {I5} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g) and 37 {I2} from ({+40}Ca,|a4p|g). 
M$D+Q from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), |D|p=no from level scheme 


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$D from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), |D|p=yes from level scheme 
RI$weighted average of 42 {I6} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), 41 {I4} from ({+28}Si,2p2n|g) and 72 {I3} from ({+40}Ca,|a4p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$D(+Q) from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), |D|p=no from level scheme 
RI$from ({+40}Ca,|a4p|g). Other: 15 {I4} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|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$D from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), |D|p=yes from level scheme 
RI$weighted average of 33.1 {I23} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), 38 {I3} from ({+28}Si,2p2n|g) and 36.8 {I15} from ({+40}Ca,|a4p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 24 {I3} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g) and 49 {I5} from ({+40}Ca,|a4p|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$Q from R(DCO) in {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g), M2 excluded by comparison to RUL 
RI$other: 48 {I4} from ({+40}Ca,|a4p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Anisotropy=0.80 {I10} 
$See Adopted Levels, Gammas for adopted placement from 12016 level (1992Ka27). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Anisotropy=0.84 {I9} 
$See Adopted Levels, Gammas for adopted placement from 11136 level (1992Ka27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Anisotropy=1.52 {I31} 
$See Adopted Levels, Gammas for adopted placement from 12383.5 level (1992Ka27). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Anisotropy=1.67 {I32} 
$See Adopted Levels, Gammas for adopted placement from 12383.5 level (1992Ka27). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$from 2009Be49. Other: 951.2 {I10} (1982De34). Evaluators adopt value from 2009Be49, as they also observe ground state transition which supports a level at 1897 keV, rather than at 1899.5-keV as proposed by 1982De34. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$observed only by 2009Be49 
RI$calculated from I|g(1896.6|g)/I|g(948.5|g)=0.059 {I9} from 2009Be49 and I|g(948.5|g)<50 from 1982De34. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$observed only by 2009Be49 
RI$calculated from I|g(536.6|g)/I|g(1484.7|g)=0.57 {I8} from 2009Be49 and I|g(536.1|g)=21 {I2} from 1982De34. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$transition not observed in 2009Be49, upper limit on intensity of I|g(2534|g)/I|g(1586.2|g) < 0.056 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E weighted average from {+91}Tc |e decay, ({+28}Si,2pn|g), (|a,3n|g). 
M Q from |g(|q), |D|p=no from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M Q from |g(|q); not M2 from RUL, assuming T{-1/2}<10 ns based on prompt coincidence component in 654|g in (|a,3n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M not M2 or higher from RUL. |g(|q) in (|a,3n|g) consistent with Q (|DJ=2) or D+Q (|DJ=1) or D(+Q) (|DJ=0); the level scheme implies the latter. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
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 265.1 {I3} in ({+28}Si,2pn|g), 265.0 in ({+31}P,n2p|g). 
RI weighted average of 12.0 {I8} from ({+28}Si,2pn|g) and 12.8 {I13} from (|a,3n|g). Other: 20.0 {I7} from ({+31}P,n2p|g). 
M Q (|DJ=2) or D (|DJ=0) from anisotropy and |g(|q) in ({+28}Si,2pn|g); magnetic D from ({+31}P,n2p|g); |DJ=0 favored by level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
ECC 0.055 {I15} from Ice and I|g assuming |a(exp)=0.11 for 662|g({+137}Cs) (1956Sm96); revised by evaluator assuming |a(exp)({+137}Cs)=0.104. 
RI from 1976De37, relative to I(1508|g, {+91}Nb)=50.4 {I15}. Other value: 107 {I9} (1970He03, renormalized so I(1508|g, {+91}Nb)=50.4) 
M from |a(exp). 


decay_energy_unit: KEV
decay_multipolarity: M4
decay_comment:
TI intensity imbalance=44 {I4} assuming negligible |e branch to 653 level. 
RI 28 {I3} in equilibrium deduced from the decay scheme. 


decay_energy_unit: KEV
decay_multipolarity: M4
decay_comment:
RI 1367 {I60} in equilibrium. I|g(653)=918 {I40} for (3.3 min) decay, after correction by authors for 65 s T{-1/2}(652 level) (1976De37). 
M from Adopted Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M anisotropy ratio=0.83 {I1}, A{-2}=+0.26 {I5}, A{-4}=+0.01 {I2} (1993Si14). Interpreted by authors as a |DJ=0, D transition. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M R{-int}|?1.52 {I20}; R{-asym}|?0.52 {I4}; Pol{-asym}|?+0.16 {I11}. A D assignment, inconsistent with level scheme. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI 20.25 {I10} is listed by 2004Ra12 but that uncertainty seems unrealistically low and is presumed here to be an order of magnitude larger. 
M R{-int}|?2.17 {I21}; R{-asym}|?1.40 {I3}; Pol{-asym}|?-0.06 {I5} favors M1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E other E|g: 1509.58 {I13} in (|a,2n|g), 1509.47 {I3} in (p,p'|g), 1509.68 {I15} in ({+32}S,2p2n|g). 
M from Coulomb excitation; Q from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E weighted average of 773.09 {I3} in (n,n'|g), 773.05 {I12} in (|a,2n|g), 773.10 {I8} in (p,p'|g), 772.97 {I15} in ({+32}S,2p2n|g). 
|d(Q,O)=-0.12 {I+22-14} from (p,p'|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=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
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 unweighted average of 244.30 {I5} in (n,n'|g) and 244.47 {I7} in (p,p'|g). Others: 244.5 {I2} in (|a,2n|g), 243.6 {I3} in ({+37}Cl,2p2n|g), 243.7 {I6} in |e decay. 
M D(+Q) from (n,n'|g); |D|p=yes from level scheme. 


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 85.25 {I20} in (n,n'|g), 85.5 {I2} in (|a,2n|g). Others: 84.3 {I3} in ({+37}Cl,2p2n|g), 85.0 {I5} in |e decay, 84.6 from ({+16}O,6n|g). 
RI unweighted average of 11.9 {I3} in (|a,2n|g), 15.1 {I10} in |e decay. 
M E1 or M1 from RUL; adopted |D|p=yes. 


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 329.83 {I5} in (n,n'|g), 329.76 {I12} in (|a,2n|g). Others: 329.1 {I3} in ({+37}Cl,2p2n|g), 329.3 {I3} in |e decay, 330.9 {I4} in (p,p'|g). 
RI from (|a,2n|g). 
M Q from (|a,2n|g); not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
Other E|g: 148.0 {I2} in (|a,2n|g), 147.3 {I3} in ({+37}Cl,2p2n|g). 
M stretched Q from |g(|q) in ({+37}Cl,2p2n|g); not M2 from |a(exp)=0.24 {I10} in (|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:
Other |d: -0.09 {I+5-21} from |g(|q) in (p,p'|g); |d|<0.04 from RUL. 
M D+Q from |g(|q) in (p,p'|g) and (n,n'|g); adopted |D|p=yes. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E weighted average of 479.95 {I11} from (n,n'|g), 480.12 {I14} from (p,p'|g) and 480.0 {I2} from (|a,2n|g). 
MR D+Q from |g(|q) in (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:
RI unweighted average of 19.7 {I11} in (n,n'|g) and 23.5 {I25} in (p,p'|g). 
M,MR D+Q from |g(|q) in (p,p'|g); adopted |D|p=no. 
Other |d: +2.5 {I+6-4} or possibly -0.04 {I+7-6} from |g(|q) in (n,n'|g), neither of which is consistent with the (p,p'|g) result. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
IF MR=-0.73 10, CC=0.023 4, BE1W<0.00094, BM2W<2.6E+4. 
Other E|g: 304.8 {I2} in (p,p'|g). 
M,MR D+Q from |g(|q) in (n,n'|g). Adopted |D|p=yes; however, if |d=-0.73 {I10} as reported in (n,n'|g), B(M2)(W.u.) will exceed RUL, unless T{-1/2}(3369) exceeds ~80 ns. Alternatively, 305|g may be complex in (n,n'|g), possibly making |d unreliable; the 305|g branch is relatively stronger in (n,n'|g) than in (p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
Other E|g (I|g): 362.3 {I2} (49 {I6}) in (p,p'|g). 
M D+Q from |g(|q) in (n,n'|g); adopted |D|p=no. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI from (p,p'|g). Placement is considered to be tentative since no evidence for this |g could be found from excit or |g|g coin in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
Other E|g (I|g): 1086.4 {I2} (32 {I5}) in (p,p'|g). 
M D+Q from |g(|q) in (p,p'|g) and (n,n'|g); adopted |D|p=no. 
MR +0.27 {I+51-24} from (p,p'|g) but -0.6 {I2} or possibly +4 {I+4-2} from |g(|q) in (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:
M D+Q from |g(|q) in (n,n'|g); |D|p=no from RUL. 
MR other |d: -0.80 {I7} or possibly -3.7 {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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
Other E|g: 1053.4 {I2} from (p,p'|g). 
M Q from |g(|q) in (p,p'|g); adopted |D|p=no. 
|d(Q,O)=-0.12 {I+19-32} from (p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
Other E|g: 1297.6 {I2} from (p,p'|g). 
M,MR D, |d(D,Q)=0.00 {I6} from |g(|q) in (n,n'|g); |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
Other E|g: 1097.7 {I2} in (|a,2n|g), 1098 {I1} in ({+32}S,2p2n|g), 1096.8 {I3} in ({+37}Cl,2p2n|g). 
M yrast cascade |g, mult=Q to 5-, from (|a,2n|g), ({+32}S,2n2p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
Other E|g: 2178.48 {I13} from (p,p'|g). 
MR -0.02 {I6} or +2.5 {I5} if J(3689)=2; +0.35 {I4} if J(3689)=3 (2010Go15) in (n,n'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E tentative placement from (p,p'|g). E|g=807.7 {I3}, branching=36.1 {I12} from (n,n'|g) if correctly placed. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
Other I|g: 82 {I5} in (p,p'|g); 119 {I18} (2000Ga30) in (n,n'|g). 
M,MR |d(D,Q)=0.00 {I12} or -6 {I+2-15} if J(3815)=2; from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
Other E|g: 2304.3 {I3} in (p,p'|g). 
M,MR |d(D,Q)=-0.01 {I+15-11} or +2.3 {I+9-7} if J(3815)=2; from |g(|q) in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
Other E|g: 2416.9 {I5} in (|g,|g'), 2415.5 {I5} in (p,p'|g). Other I|g: 49 {I24} in (|g,|g') for uncertain |g, 54 {I8} from (p,p'|g). 
M,MR from |g(|q) in (n,n'|g); |d=+0.30 {I+17-10} or +1.15 {I26}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
Other E|g: 3943.96 {I17} in (p,p'|g), 3944.1 {I3} in (|g,|g'). 
RI % photon branching=78 {I28} from (|g,|g'). However, no other |g is known to deexcite this level. 
M from (|g,|g') and (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other E|g: 628.25 {I11} from 2000Ga30 in (n,n'|g), but this |g was not confirmed by 2010Go15 in that reaction. 
M Q yrast decay |g ray to 7-, from (|a,2n|g), ({+32}S,2n2p|g). Electric from positive IPDCO in ({+28}Si,2|a2n|g). 


decay_energy_unit: KEV
decay_comment:
Reported in (n,n'|g) by 2000Ga30, but not by 2010Go15 (possibly unresolved from strong 1340|g there). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M |g(|q) in (n,n'|g) excludes pure Q or pure D, |DJ=0. 
Other E|g: 2195.54 {I14} from 2000Ga30 in (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 from (|g,|g'). E|g=3121.07 {I19} from (n,n'|g) is too low for this placement, suggesting the presence of a second level near 4630 keV (as adopted here). 
RI from (|g,|g'). 
M (D) from (|g,|g'); |D|p=(yes) from 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_uncertain: ?
decay_comment:
E weighted average of 3494.1 {I4} in (|g,|g') and 3493.6 {I3} in (n,n'|g). 
RI from (|g,|g'). 
M (D) in (|g,|g'); |D|p=no 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 from (|a,2n|g). 
RI from ({+16}O,6n|g). 
M stretched Q from |g(|q) in ({+37}Cl,2p2n|g); not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
Other E|g: 110.4 from ({+16}O,6n|g), 110.7 from ({+28}Si,2|a2n|g). 
RI from ({+28}Si,2|a2n|g). 
M D from |g(|q) and anisotropy in ({+37}Cl,2p2n|g); authors assume |DJ=1 transitions are M1(+E2). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
A{-2}=-0.05 {I3}, A{-4}=+0.08 {I4} (1971Le19); A{-2}=+0.05 {I2} (1971Na16), +0.099 {I10} (1971Co08), +0.082 {I15} (1974Ba11). 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
E from 2006Ru06. 
M from relative intensities at 96|' and 126|' (1977Me01) and I|g(90|')/I|g(127|')=1.9 {I5} (2006Ru06). 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
Unplaced inelastic transition from 2000DeZY, tentatively placed by evaluator as in Adopted Levels, Gammas. |G{+2}{-|g0}/|G=0.0075 {I9} eV for J=2 (2000DeZY) if analyzed as an elastic |g. 


decay_energy_unit: KEV
decay_multipolarity: D
decay_uncertain: ?
decay_comment:
M |D|p=(yes) (2000DeZY) is inconsistent with placement. 
|G{+2}{-|g0}/|G=0.011 {I2} eV (2000DeZY) if analyzed as an elastic |g. 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
$|G{-|g0}/|G=0.78 {I28} 
E weighted average of 3944.1 {I3} (2000DeZY) and 3943.9 {I2} (2006Ru06). 
RI %I|g(3944)=78 {I28} from |G{-|g0} (1977Me01) and averaged |G{+2}{-|g0}/|G. 
I|g(90|')/I|g(127|')=1.0 {I2} (2006Ru06). 


decay_energy_unit: KEV
decay_multipolarity: (D)
decay_uncertain: ?
decay_comment:
|g placed by evaluator, consistent with Adopted Levels, Gammas 
|G{+2}{-|g0}/|G=0.0066 {I12} eV (2000DeZY) if analyzed as an elastic |g, assuming J=2. 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
$|G{-|g0}/|G=0.90 {I8} 
E from 2006Ru06. 
M I|g(90|')/I|g(127|')=0.72 {I7} (2006Ru06). |D|p=(yes). 
|G{-|g0}=0.145 {I40} from self absorption (1977Me01). 
Other |G{-|g0}; |G: 0.59 {I17} from |G{-|g0} of 1977Me01 and averaged |G{+2}{-|g0}/|G. 


decay_energy_unit: KEV
decay_multipolarity: (D)
decay_uncertain: ?
decay_comment:
|g placed by evaluator, consistent with Adopted Levels, Gammas 
|G{+2}{-|g0}/|G=0.0091 {I26} eV for J=1 (2000DeZY) if analyzed as an elastic |g. 


decay_energy_unit: KEV
decay_multipolarity: (D)
decay_uncertain: ?
decay_comment:
Placed by evaluator, based on E|g and Adopted Levels, Gammas. 
|G{+2}{-|g0}/|G=0.012 {I4} eV for J=1 (2000DeZY) if analyzed as an elastic |g. 


decay_energy_unit: KEV
decay_multipolarity: (D)
decay_uncertain: ?
decay_comment:
Placed by evaluator, based on E|g. 
|G{+2}{-|g0}/|G=0.016 {I6} eV (2000DeZY) if analyzed as an elastic |g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
May include E|g=1340.8 {I4} placed by 2000Ga30 from 3943 level. 
M A{-2}=-0.235 {I10}, A{-4}=-0.008 {I16} (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Absent in 2010Go15. I|g from I(480|g)=3.4 {I2} from 2010Go15 and I(157|g):I(480|g)=1.0 {I5}:99.0 {I5} (2000Ga30), allowing an additional 15% uncertainty in I|g data from 2000Ga30. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
Other E|g: 480.54 {I2} (2010Go15); this fits placement poorly. 
M A{-2}=-0.01 {I4}, A{-4}=0.00 {I6} (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 214.3 {I3} (2010Go15). 
I(214|g):I(537|g)=5 {I1}:95 {I1} (2000Ga30). 
M A{-2}=-0.2 {I3}, A{-4}=+0.2 {I3} (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
I(1582|g):I(3091|g)=21 {I3}:79 {I3} (2000Ga30). 
M A{-2}=+0.14 {I5}, A{-4}=-0.11 {I7} (2010Go15). 
MR +2.5 {I+6-4} or possibly -0.04 {I+7-6} (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI I(1086|g):I(305|g)=15 {I1}:67 {I1} (2000Ga30). 
M A{-2}=-0.04 {I7}, A{-4}=-0.01 {I11} (2010Go15). 
MR -0.6 {I2} or possibly +4 {I+4-2} (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M A{-2}=-0.187 {I16}, A{-4}=+0.015 {I26} (2010Go15). 
MR -0.80 {I7} or possibly -3.7 {I7} (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
RI I(1297|g):I(1053|g)=39 {I1}:47 {I2} (2000Ga30). 
M A{-2}=-0.08 {I5}, A{-4}=0.00 {I8} (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
M A{-2}=+0.19 {I3}, A{-4}=-0.01 {I4} (2010Go15). 
MR -0.02 {I6} or +2.5 {I5} if J(3689)=2; +0.35 {I4} if J(3689)=3 (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
M A{-2}=-0.08 {I8}, A{-4}=-0.05 {I12} (2010Go15). 
MR 0.00 {I12} or -6 {I+2-15} if J(3815)=2 (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
RI I(2305|g):I(965|g)=36 {I1}:43 {I1} (2000Ga30). 
M A{-2}=+0.22 {I6}, A{-4}=+0.01 {I8} (2010Go15). 
MR -0.01 {I+15-11} or +2.3 {I+9-7} if J(3815)=2 (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from I(2639|g)=0.168 {I17} in 2010Go15 and I(1865|g):I(2639|g)=46 {I1}:54 {I1} (2000Ga30) at 90|', allowing additional 15% uncertainty in data from 2000Ga30. I|g consistent with I|g=0.126 {I17} from 2010Go15 for unplaced E|g=1863.8 {I5} line, but energy match is poor. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M A{-2}=-0.10 {I8}, A{-4}=0.00 {I12} (2010Go15). 
|g not reported by 2000Ga30 but E|g probably exceeds E cutoff for that study. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement from 2010Go15; 2000Ga30 placed |g from 4308 level instead. 
RI I(1301|g):I(2798)=22 {I1}:43 {I1} (2000Ga30) cf. 28 {I6}:100 {I12} here. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI I(1623|g):I(1868)=20 {I1}:80 {I1} (2000Ga30). 
M A{-2}=+0.45 {I22}, A{-4}=-0.04 {I28} (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E 2000Ga30 report E|g=1123.24 {I15} for line with much stronger branch than this |g which 2010Go15 did not place. 
RI I(1123|g):I(1905)=47 {I1}:53 {I1} (2000Ga30). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
RI I(1457|g):I(2798)=35 {I1}:43 {I1} (2000Ga30). 
M A{-2}=-0.09 {I6}, A{-4}=-0.08 {I8} (2010Go15). 
MR -0.02 {I+9-11} or -5 {I+2-5} if J(4308)=2; +0.14 {I5} if J(4308)=4 (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
M A{-2}=+0.27 {I9}, A{-4}=+0.02 {I10} (2010Go15). 
MR +0.1 {I+4-2} or +1.7 {I+11-9} if J(4308)=2 (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average of 1703.47 {I28} (2000Ga30) and 1702.3 {I6} (2010Go15). Unweighted average is 1702.9 {I6}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
RI I(1579|g):I(2147)=36 {I1}:45 {I1} (2000Ga30). 
M A{-2}=+0.41 {I19}, A{-4}=-0.02 {I25} (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI absent in 2010Go15. I|g from I(2147) here and I(2920|g):I(2147)=19 {I1}:45 {I1} (2000Ga30), allowing additional 15% uncertainty in I|g data from 2000Ga30. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI I(1429|g):I(2154)=42 {I1}:45 {I1} (2000Ga30). 
M A{-2}=+0.08 {I15}, A{-4}=+0.09 {I23} (2010Go15). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR from table 4 (summary of observed electromagnetic transition rates) of 1975Pa19; |d misprinted in table 3 (summary of |g(|q) analyses). 
A{-2}=-0.35 {I2}, A{-4}=-0.03 {I3} (1975Pa19); A{-2}=-0.28 {I5} (1968Li10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=-0.44 {I10}, A{-4}=-0.08 {I11} (1975Pa19). |d is |>1.2 if J=5; +0.5 to +2.8 if J=3; +0.25 {I+25-11} or +5 {I+14-3} if J=4. 


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:
Other E|g: 943.81 {I12} from (n,|g) E=thermal, 943.7 {I5} from |e decay (43.5 min), 941.8 {I7} from ({+13}C,{+12}C|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 1362.94 {I7} in |e decay (2.75 h) and 1363.02 {I3} and 1363.01 {I3} in IT decay. Other E|g: 1363.16 {I7} in (p,n|g), 1964.1 {I10} in ({+13}C,{+12}C|g). 
M,MR from |a(K)exp=0.0036 {I7} in {+93}Mo IT decay, and |g(|q,H,t) in {+93}Tc |e decay (2.75 h). Other |d: +0.5 {I+9-7} from (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 unweighted average of 114.024 {I9} and 114.065 {I5} from IT decay, 114.20 {I5} from |e decay (2.75 h) and 114.27 {I12} from (p,n|g). The weighted average is 114.057 {I13}. 
RI unweighted average of 0.69 {I2} from IT decay, 0.84 {I15} from |e decay (2.75 h) and 0.906 {I15} from (p,n|g). The weighted average is 0.83 {I7}. 
M from |a(K)exp=0.30 {I15} in {+93}Mo IT decay and |g(|q) in (n,|g). 
MR from |g(|q) in (p,n|g). Abs(|d)<1.3 from |a(K)exp in {+93}Mo IT decay, <0.11 if B(E2)(W.u.)<300. 


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 1477.113 {I20} and 1477.138 {I2} from IT decay, 1477.14 {I8} from |e decay (2.75 h) and 1477.33 {I7} from (p,n|g). The weighted average is 1477.138 {I4}. Other: 1480.7 {I16} in ({+13}C,{+12}C|g). 
RI weighted average from IT decay, |e decay (2.75 h) and (p,n|g). 
M from |a(K)exp=0.0026 {I4} in {+93}Mo IT decay; Q from |g(|q) in (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 1520.28 {I9} from |e decay (2.75 h) and 1520.39 {I7} from (p,n|g). 
M,MR from |a(K)exp=0.0029 {I6} and |g(|q,H,t) in {+93}Tc |e decay (2.75 h). Other |d: -1.2 {I+3-5} from |g(|q) in (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 IT decay. 684.66 {I7} from (p,n|g). 
M from |a(K)exp=0.00153 {I24}, K/L=8 {I1} in {+93}Mo IT decay and |g(|q) in (p,n|g). 
|d(Q,O)=+0.12 {I2} from |g(|q) in (p,n|g), but <0.07 from |a(K)exp and <4|*10{+-5} if B(M3)(W.u.)<10 (based on RUL). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
M D+Q from (p,n|g); adopted |D|p=yes. 
MR abs(|d)<0.01 from B(M2)(W.u.)<1; however, |d=+0.27 {I+13-10} in (p,n|g). 
B(E1)(W.u.)=1.25|*10{+-5} if |d=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 2409.05 {I19} from |e decay (2.75 h) and 2409.20 {I12} from (p,n|g). 
M Q from (p,n|g); |D|p=no from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_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 (p,n|g). 
M,MR D+Q from |g(|q) in (p,n|g). |d implies |D|p=no from RUL, but this contradicts |p(2540 level)=- implied by log| {Ift} in |e decay (43.5 min). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E possibly the same as the 3161.2|g seen in (p,n|g) and placed from a separate level, so placement is shown as uncertain here. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E weighted average of 1363.01 {I3} (2009Ho07) and 1363.02 {I3} (1977Me03). 
|a(K)exp: weighted average of 0.00039 {I10} (1974Ch12) and 0.00032 {I10} (1974An24). K/(L+M)=7.4 {I14} (1974An24). 
M,MR from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+(E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E unweighted average of 114.065 {I5} (2009Ho07) and 114.024 {I9} (1977Me03). 
M,MR from |a(K)exp (1974Ch12). 
%I|g=99.074 {I23} assuming adopted decay scheme normalization. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E weighted average of 1477.138 {I2} (2009Ho07) and 1477.113 {I20} (1977Me03). 
M from |a(K)exp=0.00025 {I4}, the weighted average of 0.00034 {I10} (1974Ch12) and 0.00023 {I5} (1953Fo12, renormalized so |a(K)(263)=0.517). 
%I|g=99.074 {I23}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E unweighted average of 684.714 {I1} (2009Ho07) and 684.672 {I9} (1977Me03). 
M from |a(K)exp=0.00153 {I24}, the weighted average of 0.0017 {I4} (1974Ch12) and 0.00144 {I29} (1953Fo12, renormalized so |a(K)(263)=0.517). Supported by K/L=8.0 {I10} (1953Fo12). 
|d(Q,O)<0.07 from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E4
decay_comment:
E unweighted average of 263.036 {I1} (2009Ho07) and 263.062 {I5} (1977Me03). 
M from |a(exp)=0.687 {I17} (1989ViZY). Other |a(exp): 0.71 {I4}, weighted average of 0.72 {I5} (1963Bo29) and 0.70 {I5} (1985Su04; based on intensity balance at the 2162 level, assuming E2-theory value for |a(685 transition)). Supported by K/L=3.5 {I2} (1965Gr29); other K/L: 3.09 {I6} (1953Fo12), 2.79 {I15} (1953Al02), 2.9 {I2} (1951Ru24). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|a(K)exp: weighted average of 0.00039 {I10} (1974Ch12) and 0.00032 {I10} (1974An24). K/(L+M)=7.4 {I14} (1974An24). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
%I|g=24.3 {I6} based on recommended decay scheme normalization. 
|a(K)exp: weighted average of 0.00027 {I10} (1974Ch12) and 0.00030 {I8} (1974An24). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
%I|g=14.3 {I5} assuming recommended decay scheme normalization. 
E weighted average of 2644.5 {I3} from 1974Ch12 and 2644.8 {I5} from 1977Po13. 
RI weighted average of 25 {I3} (1977Po13), 23.5 {I13} (1974An24), and 26.0 {I15} (1974Ch12). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E from 2007ChZX. Other E|g: 7126.18 {I7} (1991Is05) does not fit placement well. 
RI from 1991Is05. Other: I|g=28 {I5} (2007ChZX). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
Very weak, otherwise unknown |g, for which the level scheme indicates mult=M3 (with B(M3)(W.u.) grossly exceeding RUL); not adopted. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI 190 in 1972Ma16. Value from 1972Du13 is preferred because, in (p,n|g) and {+93}Tc |e decay (43.5 min), only the 2182|g deexcites the 2182 level, so that |g is expected to be the strongest branch here. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
|DJ=4 required for this transition; absent in 1972Du13. Not adopted. Possibly deexcites a nearby level (see Adopted Levels, Gammas (2440.4 level)); but, if so, E|g is somewhat low here. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=AP;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E 1513 (1972Du13); increased by evaluator for consistency with E|g scale in 1972Ma16. Otherwise unknown |g, so shown as uncertain. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=AP;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E 1792 (1972Du13); increased by evaluator for consistency with E|g scale in 1972Ma16. Otherwise unknown |g, so shown as uncertain. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E placed by 1972Ma16 but, from Adopted Levels, this placement requires mult |>E3 for transition; not adopted. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI from 1976Ru03; shown as uncertain because |g should have been observed by other authors, but was not. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI weighted average of 8.3 {I9} (1976Ru03), 7.4 {I8} (1983Mi13), 11.0 {I11} (1999Ka60). 
M A{-2}=+0.05 {I20}, A{-4}=+0.04 {I2} (1999Ka60). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q+O
decay_comment:
M A{-2}=-0.32 {I1}, A{-4}=+0.05 {I1} (1999Ka60). 
MR weighted average of +0.11 {I+1-3} (1976Ru03) and +0.15 {I+2-4} (1999Ka60). Both values violate RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M A{-2}=-0.34 {I3}, A{-4}=+0.08 {I4} (1999Ka60). 
MR weighted average of +0.15 {I+5-3} (1976Ru03, if J=11/2), +0.10 {I+3-2} (1999Ka60). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M,MR A{-2}=-0.02 {I3}, A{-4}=0.0 {I3} (1999Ka60). 
MR weighted average of +0.36 {I+19-15} (1976Ru03) and +0.20 {I+17-12} (1999Ka60); violates RUL if mult=E1+M2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI weighted average from 1976Ru03 and 1999Ka60. 
M,MR A{-2}=+0.06 {I3}, A{-4}=+0.01 {I3} (1999Ka60). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI unweighted average of 6.9 {I9} (1983Mi13), 9.0 {I6} (1999Ka60), 10.2 {I10} (1976Ru03). 
M,MR A{-2}=+0.02 {I2}, A{-4}=+0.01 {I2} (1999Ka60). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI weighted average of 79 {I5} from 1983Mi13 and 79 {I4} (1999Ka60). Other I|g: 57.3 {I17} (1976Ru03). 
M,MR A{-2}=+0.08 {I4}, A{-4}=+0.01 {I4} (1999Ka60). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from |a(K)exp. A{-2}=+0.19 {I1}, A{-4}=0.00 {I1} (1999Ka60). 
|d(Q,O)=+0.02 {I5} (1976Ru03) from |g(|q). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
M,MR A{-2}=-0.04 {I1}, A{-4}=+0.01 {I1} (1999Ka60). |d=+0.03 {I1} or -1.2 {I1}; second solution would violate RUL if |D|p=yes. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M,MR A{-2}=-0.06 {I1}, A{-4}=0.00 {I2} (1999Ka60). However, |d is far too large for a |D|p=yes transition; adopted |D|p=no. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI weighted average from 1983Mi13 and 1976Ru03. Other: 4.29 {I21} (1976Ru03; however, spectra suggest a much larger value). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
RI weighted average from 1983Mi13 and 1999Ka60. 
M,MR A{-2}=-0.02 {I1}, A{-4}=+0.01 {I1} (1999Ka60). |d=+10.70 {I12} or -0.05 {I11}; first solution far too large for a |D|p=yes transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
E not observed; E from level energy difference. 
RI from B(M1)(W.u.)=0.7 (1983Mi13) and T{-1/2}=0.76 ns {I4}, I(|g+ce)(9.7)=70.6%. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
M,MR A{-2}=+0.02 {I2}, A{-4}=+0.02 {I2} (1999Ka60). |d=+0.04 {I4} or -0.98 {I11}. 
RI weighted average from 1983Mi13 and 1999Ka60. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E,RI from 1999Ka60. |g not reported by 1983Mi13 or 1976Ru03. 
M,MR A{-2}=+0.24 {I3}, A{-4}=+0.01 {I4} (1999Ka60). Note that 1999Ka60 indicate a 3/2- to 3/2+ transition but their |d=-1.28 {I+14-15} implies a B(M2)(W.u.) value which would grossly exceed RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M from |a(K)exp; see also the general comment on |a(K)exp data of 1975Gu04. 
|a(K)exp: based on I(123|g) from 1975Gu04; |a(K)exp=0.097 {I29}, consistent with M1 theory, based on I(411|g) from 1975Gu04 and adopted I(411|g)/I(123|g)=0.289 {I13} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted average from 1983Mi13 and 1999Ka60. 
RI from 1999Ka60. Other I|g: 3.4 {I5} from 1983Mi13. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M from |a(K)exp; see general comment on |a(K)exp data of 1975Gu04 also. |a(K)exp: relative to |a(K)exp(203)=0.010 {I3}. A{-2}=+0.04 {I1}, A{-4}=+0.03 {I1} from |g(|q) (1999Ka60). 
|d(D,Q)=0.00 {I5} from |g(|q) (1976Ru03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M A{-2}=-0.21 {I4}, A{-4}=+0.05 {I5} (1999Ka60). 
|d(D,Q)=+0.02 {I5} (1976Ru03), -0.05 {I7} (1999Ka60). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from 1983Mi13. Other I|g: 18.9 {I18} in 1976Ru03 (table I) but |g omitted from level diagram; spectrum shows impurity nearby. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Placed by 1976Ru03 from 3024 level in table I but not in fig. 5, and attributed to (p,|g) in fig. 1; not adopted. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Placed by 1976Ru03 from 3069 level in table I but not in fig. 5, and |g absent in spectra of figs. 1 and 2; not adopted. 


decay_energy_unit: KEV
decay_multipolarity: E4
decay_comment:
M$K/L=3.60 {I72} from beam-off singles spectrum (2016Zh61). Other: K/L=3.48 {I61} from beam-on singles spectrum (2016Zh61). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$D+Q from |g|g(|q) in |b{++} decay (52.0 min); M1+E2 from RUL. 
MR$-0.87 {I+9-17} or -3.2 {I+7-9} from |g(|q) in (p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$|d=-0.10 {i12} (1979Ka22) for the M1 component of this |g is consistent with |DJ=2 for this transition 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$coincides with a transition of similar energy, intensity of contaminant transition was subtracted 


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$from L1/L23 in 61-d |e decay 
MR$value from the evaluation of 1981HaZY (based on L1/L23 in 61-d |e decay); sign from linear pol in Coul. ex. Other: 0.624 {i23} from T{-1/2} and B(E2)|^=0.0369 {i19} 


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$weighted average of 765.789 {I9} ({+95}Tc |e decay (20.0 h)), 765.9 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 765.95 {I14} (Coulomb excitation), 766.1 {I4} ({+65}Cu({+36}S,|apn|g)), 765.9 {I1} ({+82}Se({+18}O,5n|g)) 
M$D+Q from |g(|q) in (|g,|g). M1+E2 from observation in Coul. ex. 
MR$from |g(|q) in (|g,|g). Other: 0.079 {i12} from T{-1/2} and B(E2)|^=0.0004 {i1} 


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 582.082 {I3} ({+95}Tc |e decay (61 d)), 582.2 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 582.38 {I23} (Coulomb excitation) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 786.198 {I4} ({+95}Tc |e decay (61 d)), 786.2 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 786.31 {I20} (Coulomb excitation) 


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 616.49 {I2} ({+95}Tc |e decay (61 d)), 616.5 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 617.4 {I5} (Coulomb excitation) 


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$weighted average of 820.624 {I5} ({+95}Tc |e decay (61 d)), 820.8 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 820.8 {I2} (Coulomb excitation) 
MR$sign from |g(|q) in (|a,n|g) or (|a,3n|g). Value from T{-1/2} and B(E2)|^=0.00060 {i15}. Other: -0.15 {i17} from Coul. ex. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
E$weighted average of 181.88 {I5} ({+95}Tc |e decay (20.0 h)), 181.5 {I5} (Coulomb excitation); not observed in {+65}Cu({+36}S,|apn|g) 
M$D,E2 from comparison to RUL. |D|p=no from level scheme 


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 947.67 {I2} ({+95}Tc |e decay (20.0 h)), 947.9 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 947.72 {I9} (Coulomb excitation), 947.3 {I4} ({+65}Cu({+36}S,|apn|g)), 947.8 {I1} ({+82}Se({+18}O,5n|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 253.068 {I4} ({+95}Tc |e decay (61 d)), 252.6 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 252.8 {I1} (Coulomb excitation) 


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 835.149 {I5} ({+95}Tc |e decay (61 d)), 835.3 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 834.97 {I17} (Coulomb excitation) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1039.264 {I6} ({+95}Tc |e decay (61 d)), 1039.0 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 1039.40 {I10} (Coulomb excitation) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 852.60 {I2} ({+95}Tc |e decay (61 d)), 852.8 {I1} (Coulomb excitation) 
M$D+Q from |g(|q) in Coul. ex. |D|p=no from the level scheme 
MR$-0.02 {i8} or -3.6 {I+11-21} 


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 1056.70 {I25} ({+95}Tc |e decay (20.0 h)), 1056.79 {I2} ({+95}Tc |e decay (61 d)), 1057.0 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 1057.0 {I1} (Coulomb excitation) 


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$weighted average of 125.8 {I3} ({+95}Tc |e decay (20.0 h)), 125.8 {I3} (Coulomb excitation) 
M$d from comparison to RUL. |D|p=no from level scheme 
RI$from Coulomb Excitation 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
E$weighted average of 307.93 {I2} ({+95}Tc |e decay (20.0 h)), 307.8 {I3} (Coulomb excitation) 
M$d,E2 from comparison to RUL. |D|p=no 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 1073.71 {I2} ({+95}Tc |e decay (20.0 h)), 1073.9 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 1074.0 {I1} (Coulomb excitation) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1369.75 {I15} ({+95}Tc |e decay (61 d)), 1369.8 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$observed only in ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)) 
RI$from intensity ratio at |q=80|' and E|a=14 MeV w.r.t. to 1222 keV |g-ray in (|a,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_comment:
E$weighted average of 1221.90 {I15} ({+95}Tc |e decay (20.0 h)), 1222.00 {I3} ({+95}Tc |e decay (61 d)), 1222.1 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)) 
M$from comparison to RUL and |a(K)exp in 61-d |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 593.16 {I6} ({+95}Tc |e decay (20.0 h)), 593.3 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 593.2 {I4} ({+65}Cu({+36}S,|apn|g)), 593.1 {I1} ({+82}Se({+18}O,5n|g)), 593.2 {I5} ({+16}O({+82}Se,3n|g)) 
RI$from {+92}Zr(|a,n|g), {+94}Zr(|a,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 774.99 {I1} ({+95}Tc |e decay (20.0 h)), 775.2 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 774.4 {I4} ({+65}Cu({+36}S,|apn|g)), 774.9 {I1} ({+82}Se({+18}O,5n|g)), 774.4 {I5} ({+16}O({+82}Se,3n|g)) 
RI$from {+92}Zr(|a,n|g), {+94}Zr(|a,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LE;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LE
decay_comment:
E$weighted average of 604.04 {I2} ({+95}Tc |e decay (20.0 h)), 604.0 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 603.5 {I1} ({+82}Se({+18}O,5n|g)), 604.0 {I5} ({+16}O({+82}Se,3n|g):xundl-6)) 
RI$weighted average of 100 {I3} ({+95}Tc |e decay (20.0 h)), 100 {I10} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 100 {I6} ({+82}Se({+18}O,5n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 785.93 {I2} ({+95}Tc |e decay (20.0 h)), 785.9 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 785.6 {I4} ({+82}Se({+18}O,5n|g)), 785.9 {I5} ({+16}O({+82}Se,3n|g)) 
RI$weighted average of 48 {I3} ({+95}Tc |e decay (20.0 h)), 46 {I5} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)) 
M,MR$from |g(|q) in 20-h |e decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_uncertain: ?
decay_comment:
E$weighted average of 385.9 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 385.8 {I1} ({+82}Se({+18}O,5n|g)), 386.0 {I5} ({+16}O({+82}Se,3n|g)) 
RI$from {+92}Zr(|a,n|g), {+94}Zr(|a,3n|g) 
$alternative placement of 385.2 keV |g-ray from 1937.4 keV, suggested in {+65}Cu({+36}S,|apn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_comment:
E$weighted average of 396.6 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 396.4 {I2} ({+82}Se({+18}O,5n|g) 
RI$from {+92}Zr(|a,n|g), {+94}Zr(|a,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
E$weighted average of 990.7 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 990.1 {I3} ({+82}Se({+18}O,5n|g)) 
RI$from {+92}Zr(|a,n|g), {+94}Zr(|a,3n|g) 
M$(D+Q) from |g(|q) in (|a,n|g) or (|a,3n|g). |D|p=yes from the level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1111.2 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 1110.7 {I1} ({+82}Se({+18}O,5n|g)), 1110.8 {I5} ({+16}O({+82}Se,3n|g)) 
RI$from ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 173.5 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 173.8 {I1} ({+82}Se({+18}O,5n|g)), 174.0 {I5} ({+16}O({+82}Se,3n|g):xundl-6) 
RI$weighted average of 7.9 {I8} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 7.79 {I23} ({+82}Se({+18}O,5n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 691.7 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 691.7 {I4} ({+65}Cu({+36}S,|apn|g)), 691.4 {I1} ({+82}Se({+18}O,5n|g)), 691.5 {I5} ({+16}O({+82}Se,3n|g)) 
RI$weighted average of 100 {I11} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 100 {I3} ({+82}Se({+18}O,5n|g)) 
M$stretched Q 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 347.8 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 347.8 {I4} ({+65}Cu({+36}S,|apn|g)), 347.9 {I1} ({+82}Se({+18}O,5n|g)), 348.0 {I5} ({+16}O({+82}Se,3n|g):xundl-6) 
RI$weighted average of 100 {I11} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 100.0 {I4} ({+82}Se({+18}O,5n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 521.8 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 521.4 {I2} ({+82}Se({+18}O,5n|g)), 522.0 {I5} ({+16}O({+82}Se,3n|g)) 
RI$weighted average of 3.2 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 7.9 {I8} ({+82}Se({+18}O,5n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_comment:
E$weighted average of 552.6 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 552.3 {I2} ({+82}Se({+18}O,5n|g)), 553.0 {I5} ({+16}O({+82}Se,3n|g)) 
RI$weighted average of 28 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 15.8 {I23} ({+82}Se({+18}O,5n|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 674.1 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 673.7 {I3} ({+82}Se({+18}O,5n|g)), 673.8 {I5} ({+16}O({+82}Se,3n|g)) 
RI$weighted average of 100 {I10} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 100 {I5} ({+82}Se({+18}O,5n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$observed only in ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)) 
RI$from ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$suggested but not observed in {+82}Se({+18}O,5n|g) 
RI$estimated on the basis of relative intensity data of 2004Ch18 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+(E2)
decay_comment:
E$weighted average of 151.4 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 153.1 {I4} ({+65}Cu({+36}S,|apn|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 151.9 {I5} ({+82}Se({+18}O,5n|g)), 151.7 {I5} ({+16}O({+82}Se,3n|g):xundl-6) 
M$from DCO in {+82}Se({+18}O,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 902.7 {I3} ({+92}Zr(|a,n|g), {+94}Zr(|a,3n|g)), 904.8 {I4} ({+65}Cu({+36}S,|apn|g)),902.5 {I1} ({+82}Se({+18}O,5n|g)), 902.5 {I5} ({+16}O({+82}Se,3n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$weighted average of 1444.9 {I2} ({+82}Se({+18}O,5n|g)), 1445.1 {I5} ({+16}O({+82}Se,3n|g):xundl-6) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$|g not observed in this decay, but is seen in {+95}Tc |e decay. I{-|g} computed from ce{-K}(204)/ce{-K}(765)=0.010 {i3} (1974An22), |a{-K}(204)=0.046, and |a{-K}(765)=0.00128. See comment on I{-|b-}(204). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$the 204 and 561 |g energies are not consistent with the 765 |g energy; E{-|g}(204)+E{-|g}(561)-E{-|g}(765)=0.19 keV {i2}. The 765 and 204 values imply E{-|g}(561)=561.69. 
RI$from directly measured values of 0.015 {i1} (1976Ho04) and 0.015 {i6} (1977Me12); other: 0.011 {i3} deduced from ce{-K}(561)/ce{-K}(765)=0.00025 {i5} (1974An22), |a{-K}(561)=0.0029, and |a{-K}(765)=0.00128. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted av of 765.79 {i1} (1977Me12) and 765.786 {i19} (1971He20) 
EKC$Other: 0.00128 {i9} (1977Me12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$other: 616.45 {i5} (1974An05) 
EKC$Weighted av of 0.00236 {i11} (1974An05) and 0.00231 {i12} (1977Me12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
MR$29% E2 admixture (1977Me12) would require |a(K)=0.023 in disagreement with |a(K)exp=0.0120 {i4} (1977Me12) 
EKC$Unweighted av of 0.0179 {i10} (1974An05) and 0.0120 {i4} (1977Me12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$From relative intensity, 770.7 kev |g ray is placed above 666.0 keV |g ray by {+16}O({+82}Se,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 778.224 {I15} ({+96}Nb |b{+-} decay), 778.22 {I4} ({+96}Tc |e decay (4.28 d)), 778.3 {I2} ({+94}Zr(|a,2n|g)), 778.26 {I10} ({+95}Mo(n,|g) E=thermal), 778.28 {I10} ({+96}Mo(n,n'|g)), 778.1 {I1} ({+82}Se({+18}O,4n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 719.562 {I17} ({+96}Nb |b{+-} decay), 719.5 {I2} ({+96}Tc |e decay (4.28 d)), 719.55 {I5} ({+96}Tc |e decay (51.5 min)), 719.9 {I5} ({+94}Zr(|a,2n|g)), 719.53 {I11} ({+95}Mo(n,|g) E=thermal), 719.55 {I10} ({+96}Mo(n,n'|g)), 719.4 {I4} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 100.0 {I13} ({+96}Nb |b{+-} decay), 100.0 {I6} ({+96}Mo(n,n'|g)) 
MR$from {+95}Mo(n,|g) E=thermal 


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$weighted average of 1497.807 {I15} ({+96}Nb |b{+-} decay), 1497.72 {I10} ({+96}Tc |e decay (4.28 d)), 1497.65 {I9} ({+96}Tc |e decay (51.5 min)), 1497.84 {I11} ({+95}Mo(n,|g) E=thermal), 1497.76 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 47.9 {I10} ({+96}Nb |b{+-} decay), 47 {I4} ({+96}Tc |e decay (4.28 d)), 40.5 {I19} ({+96}Tc |e decay (51.5 min)), 42.2 {I22} ({+95}Mo(n,|g) E=thermal), 40.4 {I6} ({+96}Mo(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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
E$weighted average of 847.69 {I2} ({+96}Nb |b{+-} decay), 847.7 {I1} ({+96}Tc |e decay (4.28 d)), 847.6 {I3} ({+96}Tc |e decay (51.5 min)), 847.67 {I11} ({+95}Mo(n,|g) E=thermal), 849.7 {I1} ({+82}Se({+18}O,4n|g)) 
MR$from {+95}Mo(n,|g) E=thermal 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 1625.90 {I5} ({+96}Nb |b{+-} decay), 1625.7 {I1} ({+96}Tc |e decay (4.28 d)), 1625.8 {I4} ({+96}Tc |e decay (51.5 min)), 1625.7 {I3} ({+95}Mo(n,|g) E=thermal), 1625.88 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 13.6 {I8} ({+96}Nb |b{+-} decay), 10.6 {I11} ({+96}Tc |e decay (51.5 min)), 9.2 {I5} ({+95}Mo(n,|g) E=thermal), 9.05 {I22} ({+96}Mo(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 849.929 {I13} ({+96}Nb |b{+-} decay), 849.86 {I4} ({+96}Tc |e decay (4.28 d)), 849.85 {I10} ({+96}Tc |e decay (51.5 min)), 849.8 {I2} ({+94}Zr(|a,2n|g)), 849.95 {I11} ({+95}Mo(n,|g) E=thermal), 849.97 {I10} ({+96}Mo(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$weighted average of 241.377 {I15} ({+96}Nb |b{+-} decay), 241.6 {I2} ({+96}Tc |e decay (4.28 d)), 241.4 {I2} ({+96}Tc |e decay (51.5 min)), 241.6 {I5} ({+94}Zr(|a,2n|g)), 241.2 {I2} ({+95}Mo(n,|g) E=thermal), 241.36 {I10} ({+96}Mo(n,n'|g)), 242.0 {I1} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 7.2 {I8} ({+96}Nb |b{+-} decay), 12.6 {I19} ({+96}Tc |e decay (51.5 min)), 8.5 {I22} ({+94}Zr(|a,2n|g)), 8.8 {I5} ({+95}Mo(n,|g) E=thermal), 8.23 {I22} ({+96}Mo(n,n'|g)), 17.5 {I16} ({+82}Se({+18}O,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$weighted average of 371.807 {I15} ({+96}Nb |b{+-} decay), 371.8 {I2} ({+96}Tc |e decay (4.28 d)), 371.5 {I2} ({+96}Tc |e decay (51.5 min)), 371.63 {I13} ({+95}Mo(n,|g) E=thermal), 372.0 {I1} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 5.41 {I18} ({+96}Nb |b{+-} decay), 6.4 {I18} ({+96}Tc |e decay (4.28 d)), 4.4 {I9} ({+96}Tc |e decay (51.5 min)), 4.8 {I3} ({+95}Mo(n,|g) E=thermal), 25 {I3} ({+82}Se({+18}O,4n|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:
E$weighted average of 1091.349 {I12} ({+96}Nb |b{+-} decay), 1091.30 {I4} ({+96}Tc |e decay (4.28 d)), 1091.30 {I8} ({+96}Tc |e decay (51.5 min)), 1091.2 {I5} ({+94}Zr(|a,2n|g)), 1091.30 {I11} ({+95}Mo(n,|g) E=thermal), 1091.38 {I10} ({+96}Mo(n,n'|g)), 1091.4 {I6} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 100 {I3} ({+96}Nb |b{+-} decay), 100 {I7} ({+96}Tc |e decay (4.28 d)), 100 {I8} ({+96}Tc |e decay (51.5 min)), 100 {I10} ({+94}Zr(|a,2n|g)), 100 {I6} ({+95}Mo(n,|g) E=thermal), 100.00 {I22} ({+96}Mo(n,n'|g)), 100 {I10} ({+82}Se({+18}O,4n|g)) 
MR$from {+96}Tc |e decay (4.28 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 108.95 {I11} ({+96}Nb |b{+-} decay), 108.8 {I5} ({+82}Se({+18}O,4n|g)) 
RI$from {+96}Nb |b{+-} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 350.053 {I19} ({+96}Nb |b{+-} decay), 350.1 {I5} ({+96}Tc |e decay (4.28 d)), 350.32 {I15} ({+96}Tc |e decay (51.5 min)), 349.7 {I2} ({+95}Mo(n,|g) E=thermal), 350.05 {I10} ({+96}Mo(n,n'|g)), 350.6 {I2} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 5.3 {I4} ({+96}Nb |b{+-} decay), 5.3 {I3} ({+96}Tc |e decay (51.5 min)), 5.2 {I6} ({+95}Mo(n,|g) E=thermal), 13.6 {I3} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 352.56 {I3} ({+96}Nb |b{+-} decay), 352.5 {I3} ({+96}Tc |e decay (4.28 d)), 352.50 {I15} ({+96}Tc |e decay (51.5 min)), 352.3 {I2} ({+95}Mo(n,|g) E=thermal), 352.61 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 4.15 {I19} ({+96}Nb |b{+-} decay), 5.2 {I3} ({+96}Tc |e decay (51.5 min)), 5.5 {I6} ({+95}Mo(n,|g) E=thermal), 4.97 {I16} ({+96}Mo(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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
E$weighted average of 480.705 {I17} ({+96}Nb |b{+-} decay), 481.0 {I5} ({+96}Tc |e decay (4.28 d)), 480.70 {I5} ({+96}Tc |e decay (51.5 min)), 480.5 {I2} ({+95}Mo(n,|g) E=thermal), 480.42 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 29.23 {I24} ({+96}Nb |b{+-} decay), 22 {I8} ({+96}Tc |e decay (4.28 d)), 28.9 {I14} ({+96}Tc |e decay (51.5 min)), 25 {I4} ({+95}Mo(n,|g) E=thermal), 42.1 {I8} ({+96}Mo(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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
E$weighted average of 1200.231 {I13} ({+96}Nb |b{+-} decay), 1200.17 {I8} ({+96}Tc |e decay (4.28 d)), 1200.15 {I8} ({+96}Tc |e decay (51.5 min)), 1200.1 {I5} ({+94}Zr(|a,2n|g)), 1200.1 {I4} ({+95}Mo(n,|g) E=thermal), 1200.20 {I10} ({+96}Mo(n,n'|g)), 1200.1 {I3} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 100.0 {I5} ({+96}Nb |b{+-} decay), 100 {I8} ({+96}Tc |e decay (4.28 d)), 100 {I5} ({+96}Tc |e decay (51.5 min)), 100 {I9} ({+95}Mo(n,|g) E=thermal), 100.0 {I10} ({+96}Mo(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$weighted average of 1317.4 {I4} ({+96}Tc |e decay (51.5 min)), 1317.33 {I12} ({+95}Mo(n,|g) E=thermal), 1317.50 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+96}Mo(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
E$weighted average of 350.053 {I19} ({+96}Nb |b{+-} decay), 349.9 {I2} ({+96}Tc |e decay (4.28 d)), 349.7 {I2} ({+95}Mo(n,|g) E=thermal) 
RI$weighted average of 47 {I9} ({+96}Nb |b{+-} decay), 58 {I17} ({+96}Tc |e decay (4.28 d)), 78 {I8} ({+95}Mo(n,|g) E=thermal) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
E$weighted average of 591.24 {I5} ({+96}Nb |b{+-} decay), 591.3 {I6} ({+96}Tc |e decay (4.28 d)), 591.19 {I13} ({+95}Mo(n,|g) E=thermal) 
RI$weighted average of 92 {I8} ({+96}Nb |b{+-} decay), 90 {I50} ({+96}Tc |e decay (4.28 d)), 100 {I6} ({+95}Mo(n,|g) E=thermal) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 593.25 {I14} ({+96}Nb |b{+-} decay), 593.2 {I2} ({+95}Mo(n,|g) E=thermal) 
RI$weighted average of 30 {I8} ({+96}Nb |b{+-} decay), 47 {I6} ({+95}Mo(n,|g) E=thermal) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 721.629 {I19} ({+96}Nb |b{+-} decay), 721.5 {I3} ({+96}Tc |e decay (4.28 d)), 721.57 {I15} ({+95}Mo(n,|g) E=thermal), 721.77 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100 {I6} ({+96}Nb |b{+-} decay), 100 {I40} ({+96}Tc |e decay (4.28 d)), 99 {I10} ({+95}Mo(n,|g) E=thermal), 100.0 {I9} ({+96}Mo(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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 1441.129 {I24} ({+96}Nb |b{+-} decay), 1441.14 {I10} ({+96}Tc |e decay (4.28 d)), 1440.9 {I2} ({+95}Mo(n,|g) E=thermal), 1441.05 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 43.4 {I19} ({+96}Nb |b{+-} decay), 45 {I5} ({+96}Tc |e decay (4.28 d)), 55 {I6} ({+95}Mo(n,|g) E=thermal), 28.0 {I9} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
E$weighted average of 364.90 {I13} ({+95}Mo(n,|g) E=thermal), 365.13 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 9.4 {I8} ({+95}Mo(n,|g) E=thermal), 9.3 {I4} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
E$weighted average of 608.67 {I11} ({+95}Mo(n,|g) E=thermal), 608.70 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100 {I6} ({+95}Mo(n,|g) E=thermal), 100.0 {I13} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
E$weighted average of 736.86 {I11} ({+95}Mo(n,|g) E=thermal), 736.89 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 97 {I6} ({+95}Mo(n,|g) E=thermal), 97.0 {I13} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
E$weighted average of 1456.2 {I3} ({+95}Mo(n,|g) E=thermal), 1456.26 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 9 {I3} ({+95}Mo(n,|g) E=thermal), 9.72 {I22} ({+96}Mo(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$weighted average of 800.36 {I13} ({+95}Mo(n,|g) E=thermal), 800.22 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 59 {I5} ({+95}Mo(n,|g) E=thermal), 67.4 {I9} ({+96}Mo(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$weighted average of 928.4 {I5} ({+95}Mo(n,|g) E=thermal), 928.24 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 11 {I5} ({+95}Mo(n,|g) E=thermal), 7.34 {I19} ({+96}Mo(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$weighted average of 1647.6 {I3} ({+95}Mo(n,|g) E=thermal), 1647.82 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100 {I9} ({+95}Mo(n,|g) E=thermal), 100.0 {I9} ({+96}Mo(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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
E$weighted average of 219.081 {I18} ({+96}Nb |b{+-} decay), 219.4 {I4} ({+96}Tc |e decay (4.28 d)), 218.98 {I13} ({+95}Mo(n,|g) E=thermal) 
RI$weighted average of 5.12 {I8} ({+96}Nb |b{+-} decay), 4.3 {I11} ({+96}Tc |e decay (4.28 d)), 20 {I13} ({+96}Tc |e decay (51.5 min)), 6.6 {I7} ({+95}Mo(n,|g) E=thermal) 
MR$from {+96}Nb |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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 460.040 {I12} ({+96}Nb |b{+-} decay), 460.04 {I7} ({+96}Tc |e decay (4.28 d)), 460.0 {I3} ({+96}Tc |e decay (51.5 min)), 460.5 {I5} ({+94}Zr(|a,2n|g)), 459.88 {I12} ({+95}Mo(n,|g) E=thermal), 459.98 {I10} ({+96}Mo(n,n'|g)), 459.5 {I1} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 45.9 {I3} ({+96}Nb |b{+-} decay), 47 {I4} ({+96}Tc |e decay (4.28 d)), 100 {I30} ({+96}Tc |e decay (51.5 min)), 55 {I13} ({+94}Zr(|a,2n|g)), 49 {I3} ({+95}Mo(n,|g) E=thermal), 49.0 {I14} ({+96}Mo(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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
E$weighted average of 568.871 {I12} ({+96}Nb |b{+-} decay), 568.88 {I7} ({+96}Tc |e decay (4.28 d)), 568.8 {I2} ({+96}Tc |e decay (51.5 min)), 569.1 {I5} ({+94}Zr(|a,2n|g)), 568.80 {I12} ({+95}Mo(n,|g) E=thermal), 568.79 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100.0 {I5} ({+96}Nb |b{+-} decay), 100 {I7} ({+96}Tc |e decay (4.28 d)), 90 {I30} ({+96}Tc |e decay (51.5 min)), 100 {I25} ({+94}Zr(|a,2n|g)), 100 {I7} ({+95}Mo(n,|g) E=thermal), 100.0 {I16} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 810.330 {I15} ({+96}Nb |b{+-} decay), 810.3 {I4} ({+96}Tc |e decay (51.5 min)), 810.8 {I2} ({+95}Mo(n,|g) E=thermal), 810.49 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 19.13 {I17} ({+96}Nb |b{+-} decay), 70 {I30} ({+96}Tc |e decay (51.5 min)), 30 {I7} ({+95}Mo(n,|g) E=thermal), 23.4 {I10} ({+96}Mo(n,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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 812.581 {I15} ({+96}Nb |b{+-} decay), 812.54 {I4} ({+96}Tc |e decay (4.28 d)), 812.6 {I2} ({+94}Zr(|a,2n|g)), 812.48 {I13} ({+95}Mo(n,|g) E=thermal), 812.19 {I10} ({+96}Mo(n,n'|g)), 812.4 {I1} ({+82}Se({+18}O,4n|g)) 
MR$from {+96}Tc |e decay (4.28 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
E$weighted average of 853.0 {I10} ({+96}Tc |e decay (51.5 min)), 853.03 {I15} ({+95}Mo(n,|g) E=thermal), 852.86 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100 {I40} ({+96}Tc |e decay (51.5 min)), 100 {I8} ({+95}Mo(n,|g) E=thermal), 100.0 {I8} ({+96}Mo(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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 1702.5 {I5} ({+96}Tc |e decay (51.5 min)), 1702.8 {I3} ({+95}Mo(n,|g) E=thermal), 1702.79 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 40 {I8} ({+96}Tc |e decay (51.5 min)), 47 {I4} ({+95}Mo(n,|g) E=thermal), 33.3 {I8} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1003.6 {I7} ({+95}Mo(n,|g) E=thermal), 1003.69 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+96}Mo(n,n'|g). Other: 29 {I18} ({+95}Mo(n,|g) E=thermal). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1352.9 {I3} ({+95}Mo(n,|g) E=thermal), 1353.35 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+96}Mo(n,n'|g). Other: 100 {I30} ({+95}Mo(n,|g) E=thermal). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 914.6 {I3} ({+95}Mo(n,|g) E=thermal), 914.52 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 20 {I5} ({+95}Mo(n,|g) E=thermal), 11.4 {I3} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1042.7 {I2} ({+95}Mo(n,|g) E=thermal), 1042.60 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 41 {I5} ({+95}Mo(n,|g) E=thermal), 27.9 {I6} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1761.8 {I3} ({+95}Mo(n,|g) E=thermal), 1762.09 {I10} ({+96}Mo(n,n'|g)) 
$from {+96}Mo(n,n'|g). Other: 100 {I14} ({+95}Mo(n,|g) E=thermal). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 615.90 {I7} ({+96}Tc |e decay (51.5 min)), 615.8 {I2} ({+95}Mo(n,|g) E=thermal), 615.35 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+96}Mo(n,n'|g). Other: 83 {I6} ({+96}Tc |e decay (51.5 min)), 25 {I3} ({+95}Mo(n,|g) E=thermal). 


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$weighted average of 966.4 {I2} ({+96}Tc |e decay (51.5 min)), 966.3 {I2} ({+95}Mo(n,|g) E=thermal), 966.29 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+96}Mo(n,n'|g). Other: 56 {I4} ({+96}Tc |e decay (51.5 min)), 29 {I5} ({+95}Mo(n,|g) E=thermal) 


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$weighted average of 968.5 {I2} ({+96}Tc |e decay (51.5 min)), 968.21 {I12} ({+95}Mo(n,|g) E=thermal), 968.54 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+96}Mo(n,n'|g). Other: 100 {I7} ({+96}Tc |e decay (51.5 min)), 100 {I5} ({+95}Mo(n,|g). 


decay_energy_unit: KEV
decay_comment:
E$weighted average of 1096.58 {I8} ({+96}Tc |e decay (51.5 min)), 1096.7 {I5} ({+95}Mo(n,|g) E=thermal) 
RI$Not given in (n,n'|g), Other: 89 {I6} ({+96}Tc |e decay (51.5 min)), 25 {I10} ({+95}Mo(n,|g) E=thermal) 


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$weighted average of 1815.6 {I5} ({+96}Tc |e decay (51.5 min)), 1815.4 {I4} ({+95}Mo(n,|g) E=thermal), 1816.14 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+96}Mo(n,n'|g). Other: 49 {I4} ({+96}Tc |e decay (51.5 min)), 19 {I5} ({+95}Mo(n,|g) E=thermal). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 405.1 {I3} ({+95}Mo(n,|g) E=thermal), 405.95 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 6.1 {I15} ({+95}Mo(n,|g) E=thermal), 19.0 {I8} ({+96}Mo(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$weighted average of 1846.2 {I8} ({+96}Tc |e decay (51.5 min)), 1846.3 {I3} ({+95}Mo(n,|g) E=thermal), 1846.98 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100 {I12} ({+95}Mo(n,|g) E=thermal), 100.0 {I8} ({+96}Mo(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$weighted average of 1202.1 {I2} ({+95}Mo(n,|g) E=thermal), 1202.43 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100 {I11} ({+95}Mo(n,|g) E=thermal), 100.0 {I15} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 864.82 {I12} ({+95}Mo(n,|g) E=thermal), 865.00 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 54 {I3} ({+95}Mo(n,|g) E=thermal), 56.5 {I22} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1105.8 {I5} ({+94}Zr(|a,2n|g)), 1106.44 {I13} ({+95}Mo(n,|g) E=thermal), 1106.47 {I10} ({+96}Mo(n,n'|g)), 1106.2 {I5} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 100 {I5} ({+95}Mo(n,|g) E=thermal), 100.0 {I22} ({+96}Mo(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$weighted average of 1237.8 {I2} ({+96}Tc |e decay (51.5 min)), 1238.17 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+96}Mo(n,n'|g). Other: 100 {I10} ({+96}Tc |e decay (51.5 min)). 


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$weighted average of 1957.1 {I5} ({+96}Tc |e decay (51.5 min)), 1957.78 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+96}Mo(n,n'|g). Other: 74 {I6} ({+96}Tc |e decay (51.5 min)). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
E$weighted average of 314.34 {I7} ({+96}Nb |b{+-} decay), 314.27 {I5} ({+96}Tc |e decay (4.28 d)), 314.3 {I2} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 18 {I3} ({+96}Nb |b{+-} decay), 16.1 {I16} ({+96}Tc |e decay (4.28 d)) 
MR$from {+96}Tc |e decay (4.28 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
E$weighted average of 316.27 {I9} ({+96}Nb |b{+-} decay), 316.50 {I6} ({+96}Tc |e decay (4.28 d)), 316.4 {I2} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 14.3 {I20} ({+96}Nb |b{+-} decay), 9.2 {I13} ({+96}Tc |e decay (4.28 d)) 
MR$from {+96}Tc |e decay (4.28 d) 


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$weighted average of 1126.965 {I21} ({+96}Nb |b{+-} decay), 1126.85 {I6} ({+96}Tc |e decay (4.28 d)), 1125.6 {I5} ({+94}Zr(|a,2n|g)), 1126.3 {I2} ({+95}Mo(n,|g) E=thermal), 1126.91 {I10} ({+96}Mo(n,n'|g)), 1126.8 {I6} ({+82}Se({+18}O,4n|g)) 
RI$weighted average of 100 {I5} ({+96}Nb |b{+-} decay), 100 {I8} ({+96}Tc |e decay (4.28 d)), 100 {I16} ({+82}Se({+18}O,4n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 2008.5 {I3} ({+95}Mo(n,|g) E=thermal), 2008 {I3} ({+95}Mo(n,|g) E=2 keV), 2008.82 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100 {I15} ({+95}Mo(n,|g) E=thermal), 100.0 {I7} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 555.5 {I2} ({+95}Mo(n,|g) E=thermal), 555.48 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 18 {I4} ({+95}Mo(n,|g) E=thermal), 11.5 {I9} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1164.50 {I14} ({+95}Mo(n,|g) E=thermal), 1164.4 {I3} ({+96}Mo(n,n'|g)) 
RI$weighted average of 84 {I9} ({+95}Mo(n,|g) E=thermal), 59.7 {I12} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2011.8 {I3} ({+95}Mo(n,|g) E=thermal), 2011.98 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100 {I14} ({+95}Mo(n,|g) E=thermal), 100.0 {I14} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 120.3 {I4} ({+96}Nb |b{+-} decay), 120.3 {I5} ({+96}Tc |e decay (4.28 d)) 
RI$weighted average of 6 {I3} ({+96}Nb |b{+-} decay), 5.3 {I13} ({+96}Tc |e decay (4.28 d)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$weighted average of 100 {I8} ({+96}Nb |b{+-} decay), 100 {I7} ({+96}Tc |e decay (4.28 d)) 
MR$from {+96}Tc |e decay (4.28 d) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$weighted average of 740.7 {I2} ({+95}Mo(n,|g) E=thermal), 740.59 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+95}Mo(n,|g) thermal 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1346.9 {I3} ({+96}Nb |b{+-} decay), 1346.8 {I2} ({+95}Mo(n,|g) E=thermal), 1347.26 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+95}Mo(n,|g) thermal 


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$weighted average of 891.5 {I2} ({+95}Mo(n,|g) E=thermal), 891.03 {I10} ({+96}Mo(n,n'|g)) 
RI$from (n,n'|g), other: 56 {I13} ({+95}Mo(n,|g) E=thermal) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1360.4 {I4} ({+95}Mo(n,|g) E=thermal), 1360.91 {I10} ({+96}Mo(n,n'|g)) 
RI$from (n,n'|g), other: 80 {I30} ({+95}Mo(n,|g) E=thermal) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 2208.6 {I7} ({+95}Mo(n,|g) E=thermal), 2208.55 {I10} ({+96}Mo(n,n'|g)) 
RI$from (n,n'|g), other: 100 {I60} ({+95}Mo(n,|g) E=thermal) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from (n,n'|g), other: 37 {I7} ({+95}Mo(n,|g) E=thermal) 
E$weighted average of 1046.2 {I2} ({+95}Mo(n,|g) E=thermal), 1045.80 {I10} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$from (n,n'|g), other: 44 {I12} ({+95}Mo(n,|g) E=thermal) 
E$weighted average of 1155.4 {I2} ({+95}Mo(n,|g) E=thermal), 1155.64 {I10} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$from (n,n'|g), other: 100 {I12} ({+95}Mo(n,|g) E=thermal) 
E$weighted average of 1396.3 {I2} ({+95}Mo(n,|g) E=thermal), 1396.26 {I10} ({+96}Mo(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:
RI$from (n,n'|g), other: 77 {I12} ({+95}Mo(n,|g) E=thermal) 
E$weighted average of 1398.4 {I3} ({+95}Mo(n,|g) E=thermal), 1398.36 {I10} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1425.1 {I2} ({+95}Mo(n,|g) E=thermal), 1424.99 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+95}Mo(n,|g) E=thermal 


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$weighted average of 991.7 {I4} ({+95}Mo(n,|g) E=thermal), 992.18 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 24 {I8} ({+95}Mo(n,|g) E=thermal), 48.4 {I23} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1459.0 {I5} ({+95}Mo(n,|g) E=thermal), 1459.36 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100 {I30} ({+95}Mo(n,|g) E=thermal), 100.0 {I23} ({+96}Mo(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$weighted average of 1461.1 {I8} ({+95}Mo(n,|g) E=thermal), 1461.64 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 60 {I30} ({+95}Mo(n,|g) E=thermal), 82.5 {I23} ({+96}Mo(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$weighted average of 1507.9 {I3} ({+95}Mo(n,|g) E=thermal), 1508.65 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+95}Mo(n,|g) E=thermal 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$from (n,n'|g) 
E$weighted average of 2401.9 {I10} ({+95}Mo(n,|g) E=thermal), 2400.54 {I10} ({+96}Mo(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:
RI$from (n,|g), E=th. 
E$weighted average of 2507.6 {I15} ({+95}Mo(n,|g) E=thermal), 2506.64 {I10} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1709.0 {I4} ({+95}Mo(n,|g) E=thermal), 1709.72 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+96}Mo(n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 929.3 {I2} ({+94}Zr(|a,2n|g)), 929.4 {I4} ({+82}Se({+18}O,4n|g)) 
RI$from {+82}Se({+18}O,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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 1320.9 {I5} ({+95}Mo(n,|g) E=thermal), 1320.77 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 45 {I25} ({+95}Mo(n,|g) E=thermal), 78 {I3} ({+96}Mo(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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 1918.6 {I5} ({+95}Mo(n,|g) E=thermal), 1919.36 {I10} ({+96}Mo(n,n'|g)) 
RI$weighted average of 100 {I40} ({+95}Mo(n,|g) E=thermal), 100 {I3} ({+96}Mo(n,n'|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 2663.8 {I15} ({+95}Mo(n,|g) E=thermal), 2663.71 {I10} ({+96}Mo(n,n'|g)) 
RI$from {+95}Mo(n,|g) E=thermal 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
E$weighted average of 738.7 {I5} ({+94}Zr(|a,2n|g)), 738.3 {I4} ({+82}Se({+18}O,4n|g)) 
RI$from {+82}Se({+18}O,4n|g), other: 80 {I30} {+94}Zr(|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 546.2 {I5} ({+94}Zr(|a,2n|g)), 545.6 {I1} ({+82}Se({+18}O,4n|g)) 
E,RI$from {+82}Se({+18}O,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$observed only in {+82}Se({+18}O,4n|g) 
E$from {+82}Se({+18}O,4n|g), otherL 879.3 {I5} ({+94}Zr(|a,2n|g)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from Adopted Gammas. Other: +1.6 {I3} (1986Ed01),: +1.6 {I+4-6} (1971Ba59), +1.7 {i2} (1986BeZK) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=0.0131 {i16}, |a(L1)exp/|a(L2)exp=20.9 {i30}, |a(L1)exp/|a(L3)exp=39 {i6}, |a(L2)exp/|a(L3)exp=1.9 {i5}, |a(L1)exp/(|a(L2)exp+|a(L3)exp)=13.7 {i20} 
M,MR$from 1999Ma54 
$Ratios of the |a(L)exp values were measured by 1969Ag05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp=0.0129 {i20}, |a(L1)exp/|a(L2)exp=25 {i4}, |a(L1)exp/|a(L3)exp>62, |a(L2)exp/|a(L3)exp>2, |a(L1)exp/(|a(L2)exp+|a(L3)exp)=22 {i7} 
M,MR$from 1999Ma54 
$Ratios of the |a(L)exp values were measured by 1969Ag05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.16 {i6} or +1.5 {i2} 
E$second placement of 241|g from a 2219 level proposed earlier is not supported in this experiment 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.04 {i3} or -6.1 {i9} 
RI$8.52 {i2} listed in 2007Le05. Since the quoted uncertainty seems unrealistic, we took I|g=8.5 


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;ERR=CONV
decay_comment:
MR$weighted average of +0.40 {I3} from OSIRIS data and +0.42 {I10} from YRAST Ball data at WNSL-Yale (2016Th01). (719|g)(778|g(|q) pattern shown in Figs. 3 and 4 of 2016Th01 does not agree with |d=+1.1 reported as one of the solutions in a previous work 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$B(E2)(W.u.)=0.2 given in Table 4 of 2016Th01 is B(E2) value, uncertainty is incorrect since |d(E2/M1) overlaps 0, implying B(E2)=0. Compiler obtains B(E2)(W.u.)=63 {I+171-63} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from (480.55|g)(719.55|g)(|q); pure E2 is also supported (480.55|g)(1497.97|g)(|q) data (2016Th01); |d=-0.12 {I4} reported earlier is not supported by the current |g|g(|q) data shown in Fig. A.2 of 2016Th01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from (1200.39|g)(778.23|g)(|q) (Fig. A.3 in 2016Th01); previous value of |d=0.89 {I10} is not supported by current data 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$from |g(|q) from polarized nuclei ({+97}Nb |b{+-} decay). Other: -0.06|<|d|<+0.01 (|a,n|g); -0.04 {I1} (Coul. ex.) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$DCO=0.73 {I6} 
M$M2 adopted by 2004Ch18 but based on their DCO |DJ=1, D+Q can not be excluded; no mult is adopted 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$DCO=0.43 {I2} 
M$M1+E2 with |d=-0.16 {I3} adopted by 2004Ch18 based on their DCO, which contradicts their adopted J|p for the parent level; no mult is adopted 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$DCO=1.45 {I7} 
M$M1+E2 with |d=+0.90 {I8} adopted by 2004Ch18 based on their DCO, which contradicts their adopted J|p for the parent level; no mult is adopted 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$-0.06|<|d|<+0.01; adopted value: -0.05 {I3} from |g(|q) from polarized nuclei ({+97}Nb |b{+-} decay) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from coin data |?40% of singles intensity of the doublet (I|g=42 {I3}) belongs to this transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$or |d=+4.4 {I4} (which would lead to T{-1/2}(level)=68 ps, in disagreement with the measured T{-1/2} of 1975BoYF). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$from {+97}Nb decay dataset in ENSDF database. In 2014Kr11, this |g ray could not be resolved from a strong line at 1148.1 keV from {+97}Zr decay. Placement is from {+97}Mo Adopted dataset in ENSDF database 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
E$deduced from level difference. ce line observed in (p,p'|g) and (t,p|g) studies 
M$from observation in ce data only 
$Branching ratio for two photon emission: |G{-|g|g}/|G<0.0001 at 95% confidence level (2014He12). Two methods were used, one based on direct population of 735, 0+ state, and the second based on population of 735, 0+ level through 1024|g from 1758,2+ level. 
$Strength parameter |r{+2}(E0)=0.0273 {I25} (1971AnZV,(p,p'|g)). 2005Ki02 evaluation gives |r{+2}(E0)=0.0273 {I11} 


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: S
decay_comment:
E$from level-energy difference. 
RI$from B(E2)(735,0+ to 787,2+) in Coul. ex. 
$B(E2)(W.u.) from B(E2)|^=0.130 {I+14-34} (2002Zi06). Other B(E2)(W.u.)=21.8 {I11} from B(E2)|^=0.293 {I14} (1978La17). 


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$weighted average of 787.363 {I20} from {+98}Nb |b{+-} decay (51.1 min) and 787.38 {I2} from (n,n'|g). Others: 787.4 {I3} from {+98}Nb |b{+-} decay (2.86 s), 787.26 {I15} from (|a,2n|g), 787.42 {I10} from (n,|g) E=th, 787.4 {I5} from ({+30}Si,X|g), and 787.5 {I3} from Coulomb excitation 
M$Q from |g|g(|q) in (|a,2n|g) and |g(|q) in (n,n'|g); M2 ruled out by RUL 


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$weighted average of 644.847 {I20} from {+98}Nb |b{+-} decay (51.1 min) and 644.81 {I2} from (n,n'|g). Others: 645.1 {I3} from {+98}Nb |b{+-} decay (2.86 s), 644.70 {I15} from (|a,2n|g), 644.89 {I11} from (n,|g) E=th, and 644.9 {I3} from Coulomb excitation 
MR$weighted average of +1.67 {I25} from |g|g(|q) in (|a,2n|g) and +1.70 {I16} from |g(|q) in (n,n'|g). Others: +0.58 {I5} from |g|g(|q) in (n,|g) E=thermal; +0.27 {I2} from matrix elements in Coul. ex. 


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$weighted average of 697.38 {I10} from {+98}Nb |b{+-} decay (51.1 min), 697.10 {I46} from (|a,2n|g), 697.6 {I2} from (n,|g) E=th, and 697.6 {I5} from Coulomb excitation 
RI$weighted average of 5.0 {I3} from {+98}Nb |b{+-} decay (51.1 min), 5.8 {I7} from (|a,2n|g), 5.9 {I17} from (n,|g) E=th, and 5.8 {I16} from Coulomb excitation 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1432.4 {I3} from {+98}Nb |b{+-} decay (2.86 s), 1432.175 {I20} from {+98}Nb |b{+-} decay (51.1 min), 1432.29 {I20} from (|a,2n|g), 1432.31 {I11} from (n,|g) E=th, 1432.30 {I3} from (n,n'|g), and 1432.2 {I3} from Coulomb excitation 
RI$unweighted average of 88.7 {I8} from {+98}Nb |b{+-} decay (51.1 min), 81.5 {I16} from (|a,2n|g), 84 {I7} from (n,|g) E=th, 84.9 {I10} from (n,n'|g), and 82 {I7} from Coulomb excitation 
M$Q from |g(|q) in (n,n'|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 722.626 {I20} from {+98}Nb |b{+-} decay (51.1 min) and 722.66 {I2} from (n,n'|g). Others: 722.48 {I15} from (|a,2n|g), 722.70 {I10} from (n,|g) E=th, 722.4 {I5} from ({+30}Si,X|g), and 722.8 {I3} from Coulomb excitation 
M$also supported by |g|g(|q) in (n,|g) E=thermal and |g(|q) in (n,n'|g). Deduced |d(O/Q)=-0.05 {I11} (n,n'|g); -0.04 {I3} (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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 326.7 {I6} from {+98}Nb |b{+-} decay (2.86 s), 326.43 {I13} from {+98}Nb |b{+-} decay (51.1 min), 326.05 {I25} from (|a,2n|g), and 326.21 {I12} from (n,|g) E=th 
RI$weighted average of 5.1 {I9} from {+98}Nb |b{+-} decay (2.86 s), 4.6 {I9} from {+98}Nb |b{+-} decay (51.1 min), 7.0 {I3} from (|a,2n|g), 6.3 {I6} from (n,|g) E=th, and 5.7 {I5} from Coulomb excitation 


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$weighted average of 971.7 {I3} from {+98}Nb |b{+-} decay (2.86 s), 970.86 {I10} from {+98}Nb |b{+-} decay (51.1 min), 971.03 {I16} from (|a,2n|g), 971.01 {I11} from (n,|g) E=th, 971.14 {I3} from (n,n'|g), and 971.3 {I5} from Coulomb excitation 
RI$unweighted average of 53 {I6} from {+98}Nb |b{+-} decay (2.86 s), 61 {I3} from {+98}Nb |b{+-} decay (51.1 min), 65.9 {I10} from (|a,2n|g), 60 {I6} from (n,|g) E=th, 72.9 {I10} from (n,n'|g), and 70 {I15} from Coulomb excitation 
MR$others: -1.6 {I+7-15} from |g(|q) in (n,n'|g), -2.15 {I15} from |g|g(|q) in (n,|g) E=thermal; +0.42 {I7} from matrix elements in Coul. ex. 


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$weighted average of 1024.3 {I3} from {+98}Nb |b{+-} decay (2.86 s), 1023.7 {I1} from {+98}Nb |b{+-} decay (51.1 min), 1023.61 {I16} from (|a,2n|g), 1023.60 {I11} from (n,|g) E=th, 1023.74 {I3} from (n,n'|g), and 1023.7 {I5} from Coulomb excitation 
RI$from (n,n'|g) 
M$also supported by |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$weighted average of 1758.4 {I6} from {+98}Nb |b{+-} decay (2.86 s), 1758.46 {I12} from {+98}Nb |b{+-} decay (51.1 min), 1758.64 {I14} from (|a,2n|g), 1758.9 {I5} from (n,|g) E=th, 1759.1 {I2} from (n,n'|g), and 1758.8 {I5} from Coulomb excitation 
RI$weighted average of 10.6 {I21} from {+98}Nb |b{+-} decay (2.86 s), 5.5 {I9} from {+98}Nb |b{+-} decay (51.1 min), 5.4 {I21} from (n,|g) E=th, and 6.7 {I8} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 530.61 {I30} from (|a,2n|g) and 531.3 {I3} from (n,n'|g) 
RI$weighted average of 39 {I3} from (|a,2n|g) and 42 {I6} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1175.57 {I20} from (|a,2n|g) and 1175.66 {I8} from (n,n'|g) 
RI$from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$weighted average of 259.00 {I10} from {+98}Nb |b{+-} decay (51.1 min), 258.96 {I26} from (|a,2n|g), 259.01 {I10} from (n,|g) E=th, 258.98 {I4} from (n,n'|g), and 258.9 {I5} from Coulomb excitation 
RI$weighted average of 26.3 {I7} from {+98}Nb |b{+-} decay (51.1 min), 22.0 {I19} from (|a,2n|g), 28 {I3} from (n,|g) E=th, 25.5 {I8} from (n,n'|g), and 27.0 {I20} from Coulomb excitation 
M$|d(Q/D)=+0.01 {I6} from (|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$from (|a,2n|g) and (n,|g) E=thermal. Other: 507.8 {I3} from {+98}Nb |b{+-} decay (51.1 min) 
RI$from (n,|g) E=thermal. Other: 3.9 {I20} from {+98}Nb |b{+-} decay (51.1 min) 


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$weighted average of 1230.15 {I5} from {+98}Nb |b{+-} decay (51.1 min), 1230.04 {I15} from (|a,2n|g), 1230.23 {I12} from (n,|g) E=th, 1230.17 {I4} from (n,n'|g), 1230.3 {I5} from ({+30}Si,X|g), and 1230.1 {I3} from Coulomb excitation 
M$|d(Q/D)=-0.04 {I7} (|g|g(|q) in (|a,2n|g); 0.00 {I2} (|g|g(|q) in (n,|g)); -0.04 {I1} (|g(|q) in (n,n'|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$weighted average of 2017.48 {I10} from {+98}Nb |b{+-} decay (51.1 min), 2018.01 {I53} from (|a,2n|g), 2017.4 {I2} from (n,|g) E=th, 2017.3 {I3} from (n,n'|g), 2017.3 {I5} from ({+30}Si,X|g), and 2017.4 {I5} from Coulomb excitation 
RI$weighted average of 21.1 {I13} from {+98}Nb |b{+-} decay (51.1 min), 16.2 {I17} from (|a,2n|g), 19.2 {I21} from (n,|g) E=th, 17.0 {I10} from (n,n'|g), and 23.0 {I20} from Coulomb excitation. Other: 58 {I14} from ({+30}Si,X|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1250.00 {I19} from (|a,2n|g) and 1250.14 {I6} from (n,n'|g). Other: 1250.2 {I6} from {+98}Nb |b{+-} decay (2.86 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 594.66 {I13} from {+98}Nb |b{+-} decay (51.1 min), 594.65 {I12} from (|a,2n|g), and 594.6 {I3} from (n,|g) E=th 
RI$weighted average of 8.2 {I24} from {+98}Nb |b{+-} decay (51.1 min) and 21 {I8} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 672.59 {I10} from {+98}Nb |b{+-} decay (51.1 min), 672.50 {I17} from (|a,2n|g), 672.63 {I11} from (n,|g) E=th, and 672.50 {I4} from (n,n'|g) 
RI$weighted average of 78 {I6} from {+98}Nb |b{+-} decay (51.1 min), 79 {I3} from (|a,2n|g), 83 {I8} from (n,|g) E=th, and 89 {I4} from (n,n'|g) 
M,MR$from |g(|q) in (n,n'|g); E1+M2 ruled out by RUL due to large quadrupole mixing. Other: |d=+6.7 {I+34-17} from |g|g(|q) (|a,2n|g) agrees well 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1317.33 {I10} from {+98}Nb |b{+-} decay (51.1 min), 1317.37 {I17} from (|a,2n|g), 1317.40 {I12} from (n,|g) E=th, and 1317.43 {I11} from (n,n'|g) 
M,MR$from |g(|q) in (n,n'|g); E1+M2 ruled out by RUL due to large quadrupole mixing. Other: |d=+2.9 {I+6-5} from |g|g(|q) in (|a,2n|g) agrees well 


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 1419.7 {I3} from {+98}Nb |b{+-} decay (2.86 s), 1419.07 {I10} from {+98}Nb |b{+-} decay (51.1 min), 1419.48 {I22} from (|a,2n|g), 1419.39 {I13} from (n,|g) E=th, and 1419.41 {I5} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 713.817 {I20} from {+98}Nb |b{+-} decay (51.1 min) and 713.87 {I5} from (n,n'|g). Others: 713.80 {I16} from (|a,2n|g) and 713.88 {I15} from (n,|g) E=th 
E$other: 100 {I5} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$others: 791.58 {I17} from (|a,2n|g), 791.5 {I2} from (n,|g) E=th, and 792.0 {I2} from (n,n'|g) 
RI$weighted average of 85.5 {I5} from {+98}Nb |b{+-} decay (51.1 min), 83 {I4} from (|a,2n|g), 78 {I9} from (n,|g) E=th. Other: 150 {I20} from (n,n'|g) 
M$|d(M3/E2)=+0.07 {I8} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1436.42 {I5} from {+98}Nb |b{+-} decay (51.1 min), 1436.68 {I25} from (|a,2n|g), 1436.6 {I3} from (n,|g) E=th, and 1437.0 {I3} from (n,n'|g) 
RI$weighted average of 27.6 {I4} from {+98}Nb |b{+-} decay (51.1 min), 23.4 {I19} from (|a,2n|g), 29 {I6} from (n,|g) E=th, and 23 {I4} from (n,n'|g) 
M$|d(M3/E2)=-0.03 {I7} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
E$weighted average of 900.85 {I21} from (|a,2n|g), 900.9 {I2} from (n,|g) E=th and 900.96 {I15} from (n,n'|g). Placement from (|a,2n|g); it is placed from the 2333.4, 4+ level in (n,|g) E=th and (n,n'|g) and replaced from the 2333.2, 2+ level by evaluators.. 
M,MR$|g|g(|q) in (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 575.06 {I10} from {+98}Nb |b{+-} decay (51.1 min), 575.06 {I10} from (|a,2n|g), 575.0 {I2} from (n,|g) E=th, and 574.4 {I3} from (n,n'|g) 
RI$weighted average of 6.2 {I7} from {+98}Nb |b{+-} decay (51.1 min) and 7.1 {I21} from (n,|g) E=th. Value of 26 {I5} in (n,n'|g) is discrepant, not used in averaging. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 823.39 {I5} from {+98}Nb |b{+-} decay (51.1 min), 823.33 {I16} from (|a,2n|g), 823.44 {I12} from (n,|g) E=th, and 823.35 {I7} from (n,n'|g) 
RI$unweighted average of 64.1 {I14} from {+98}Nb |b{+-} decay (51.1 min), 77 {I5} from (|a,2n|g), 45 {I4} from (n,|g) E=th, and 43.1 {I23} from (n,n'|g) 
MR$others: |d(Q/D)=-2.7 {I+11-21} or -0.24 {I20} from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1546.03 {I5} from {+98}Nb |b{+-} decay (51.1 min), 1546.30 {I22} from (|a,2n|g), 1545.95 {I12} from (n,|g) E=th, and 1546.06 {I8} from (n,n'|g) 
$|d(M3/E2)=-0.04 {I4} 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$weighted average of 833.556 {I20} from {+98}Nb |b{+-} decay (51.1 min), 833.61 {I13} from (n,|g) E=th, and 833.70 {I11} from (n,n'|g). Others: 833.52 {I15} from (|a,2n|g) and 833.6 {I5} from ({+30}Si,X|g) 
M$|d(M3/E2)=-0.01 {I7} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: ((M1+E2))
decay_comment:
E$weighted average of 986.34 {I27} from (|a,2n|g), 985.5 {I4} from (n,|g) E=th, and 985.8 {I2} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1631.26 {I50} from (|a,2n|g), 1631.4 {I2} from (n,|g) E=th, and 1631.03 {I10} from (n,n'|g) 
RI$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 315.0 {I2} from {+98}Nb |b{+-} decay (51.1 min), 314.9 {I2} from (|a,2n|g), and 314.6 {I3} from (n,|g) E=th 
RI$weighted average of 2.9 {I7} from {+98}Nb |b{+-} decay (51.1 min) and 2.8 {I19} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 401.99 {I10} from {+98}Nb |b{+-} decay (51.1 min), 402.33 {I39} from (|a,2n|g), and 402.2 {I2} from (n,|g) E=th 
RI$weighted average of 13.1 {I15} from {+98}Nb |b{+-} decay (51.1 min), 10.0 {I14} from (|a,2n|g), and 8 {I3} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 661.15 {I19} from {+98}Nb |b{+-} decay (51.1 min), 661.16 {I40} from (|a,2n|g), 661.5 {I5} from (n,|g) E=th, and 660.7 {I4} from (n,n'|g) 
RI$weighted average of 28 {I4} from {+98}Nb |b{+-} decay (51.1 min), 17.8 {I13} from (|a,2n|g), 19 {I9} from (n,|g) E=th, and 32 {I7} from (n,n'|g) 
$|d(M3/E2)=+0.09 {I10} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 909.67 {I5} from {+98}Nb |b{+-} decay (51.1 min), 909.52 {I17} from (|a,2n|g), 909.59 {I13} from (n,|g) E=th, and 909.54 {I8} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 987.47 {I10} from {+98}Nb |b{+-} decay (51.1 min), 987.48 {I10} from (|a,2n|g), 987.6 {I5} from (n,|g) E=th, and 987.6 {I8} from (n,n'|g) 
RI$weighted average of 32.8 {I22} from {+98}Nb |b{+-} decay (51.1 min), 20 {I9} from (n,|g) E=th, and 16 {I13} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 1632.17 {I10} from {+98}Nb |b{+-} decay (51.1 min), 1632.46 {I33} from (|a,2n|g), 1631.4 {I2} from (n,|g) E=th, and 1631.03 {I10} from (n,n'|g) 
RI$unweighted average of 59.9 {I22} from {+98}Nb |b{+-} decay (51.1 min), 40.5 {I16} from (|a,2n|g), 57 {I9} from (n,|g) E=th, and 60 {I8} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 151.8 {I2} from {+98}Nb |b{+-} decay (51.1 min) and 151.9 {I2} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 380.4 {I2} from {+98}Nb |b{+-} decay (51.1 min) and 380.05 {I43} from (|a,2n|g) 
RI$weighted average of 15 {I4} from {+98}Nb |b{+-} decay (51.1 min) and 21.8 {I17} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI$38 {I12} from {+98}Nb |b{+-} decay (51.1 min) but this |g is not confirmed in (|a,2n|g), only an upper limit is given. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 975.02 {I14} from {+98}Nb |b{+-} decay (51.1 min), 975.25 {I32} from (|a,2n|g), and 975.2 {I3} from (n,n'|g) 
RI$weighted average of 38 {I4} from {+98}Nb |b{+-} decay (51.1 min), 35.9 {I17} from (|a,2n|g), and 30 {I8} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1052.95 {I10} from {+98}Nb |b{+-} decay (51.1 min), 1053.04 {I26} from (|a,2n|g), and 1052.96 {I13} from (n,n'|g) 
RI$weighted average of 46 {I8} from {+98}Nb |b{+-} decay (51.1 min), 55 {I3} from (|a,2n|g). Other: 104 {I7} from (n,n'|g) is discrepant. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 86.65 {I10} from {+98}Nb |b{+-} decay (51.1 min) and 86.51 {I32} from (|a,2n|g) 
RI$other: 8 {I5} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
E$others: 172.89 {I16} from (|a,2n|g), 171.9 {I7} from (n,n'|g) 
RI$weighted average of 65 {I4} from {+98}Nb |b{+-} decay (51.1 min), 74 {I3} from (|a,2n|g). Other: 25 {I14} from (n,n'|g) is discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 996.30 {I5} from {+98}Nb |b{+-} decay (51.1 min), 996.33 {I16} from (|a,2n|g), and 996.44 {I13} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 544.52 {I39} from (|a,2n|g), 545.0 {I2} from (n,|g) E=th, and 544.2 {I4} from (n,n'|g) 
RI$weighted average of 7.4 {I9} from (|a,2n|g), 13 {I4} from (n,|g) E=th, and 17 {I7} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$unweighted average of 1775.37 {I23} from (|a,2n|g), 1774.7 {I2} from (n,|g) E=th, and 1774.31 {I11} from (n,n'|g) 
RI$from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 555.3 {I2} from {+98}Nb |b{+-} decay (51.1 min), 555.07 {I35} from (|a,2n|g), 555.4 {I2} from (n,|g) E=th, and 555.4 {I3} from (n,n'|g) 
RI$weighted average of 38 {I25} from {+98}Nb |b{+-} decay (51.1 min), 47 {I7} from (|a,2n|g), 59 {I7} from (n,|g) E=th. Other: 161 {I30} from (n,n'|g) is discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$weighted average of 814.8 {I3} from {+98}Nb |b{+-} decay (51.1 min), 814.46 {I26} from (|a,2n|g), 814.2 {I2} from (n,|g) E=th, and 814.1 {I2} from (n,n'|g) 
RI$weighted average of 50 {I25} from {+98}Nb |b{+-} decay (51.1 min), 50 {I3} from (|a,2n|g), 62 {I15} from (n,|g) E=th. Other: 94 {I8} from (n,n'|g) is discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1140.83 {I47} from (|a,2n|g) and 1140.8 {I4} from (n,|g) E=th 
RI$weighted average of 29 {I4} from (|a,2n|g) and 32 {I15} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$weighted average of 1785.66 {I14} from {+98}Nb |b{+-} decay (51.1 min), 1785.90 {I24} from (|a,2n|g), 1785.4 {I3} from (n,|g) E=th, and 1785.1 {I2} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
E$weighted average of 350.78 {I12} from {+98}Nb |b{+-} decay (51.1 min) and 350.81 {I18} from (|a,2n|g) 
RI$from (|a,2n|g). Other: I(350.8|g)/I(1063.7|g)=15 {I6}/100 {I6} from {+98}Nb |b{+-} decay (51.1 min), is discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 557.5 {I1} from {+98}Nb |b{+-} decay (51.1 min) and 557.08 {I39} from (|a,2n|g) 
RI$from (|a,2n|g). Other: I(557.5|g)/I(1063.7|g)=39 {I6}/100 {I6} from {+98}Nb |b{+-} decay (51.1 min) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$unweighted average of 1063.0 {I2} from {+98}Nb |b{+-} decay (51.1 min) and 1064.27 {I18} from (|a,2n|g) 
RI$from (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1187.1 {I5} from {+98}Nb |b{+-} decay (51.1 min), 1187.50 {I43} from (|a,2n|g), 1187.6 {I3} from (n,|g) E=th, and 1187.6 {I3} from (n,n'|g) 
RI$weighted average of 80 {I50} from {+98}Nb |b{+-} decay (51.1 min), 49 {I18} from (n,|g) E=th, and 49 {I9} from (n,n'|g). Others: 9.7 {I7} from (|a,2n|g) is discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1833.0 {I3} from {+98}Nb |b{+-} decay (51.1 min), 1832.93 {I33} from (|a,2n|g), 1833.0 {I3} from (n,|g) E=th, and 1832.4 {I2} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 603.28 {I10} from {+98}Nb |b{+-} decay (51.1 min), 603.25 {I17} from (|a,2n|g), 603.33 {I12} from (n,|g) E=th, 603.1 {I4} from (n,n'|g), and 603.1 {I5} from ({+30}Si,X|g) 
RI$weighted average of 66 {I4} from {+98}Nb |b{+-} decay (51.1 min), 63.3 {I12} from (|a,2n|g), 63 {I5} from (n,|g) E=th, 49 {I10} from (n,n'|g), and 55 {I11} from ({+30}Si,X|g) 
M$|d(M3/E2)=-0.08 {I11} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$weighted average of 1110.76 {I10} from {+98}Nb |b{+-} decay (51.1 min), 1110.75 {I16} from (|a,2n|g), 1110.81 {I14} from (n,|g) E=th, 1110.78 {I7} from (n,n'|g), and 1110.3 {I5} from ({+30}Si,X|g) 
M$|d(M2/E1)=-0.05 {I10} from (|a,2n|g); D also from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 172.44 {I10} from {+98}Nb |b{+-} decay (51.1 min) and 172.47 {I26} from (|a,2n|g) 
RI$weighted average of 4.6 {I5} from {+98}Nb |b{+-} decay (51.1 min) and 3.6 {I5} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
E$weighted average of 335.258 {I20} from {+98}Nb |b{+-} decay (51.1 min), 335.15 {I16} from (|a,2n|g), and 334.5 {I5} from ({+30}Si,X|g) 
RI$weighted average of 53.4 {I11} from {+98}Nb |b{+-} decay (51.1 min) and 52.8 {I8} from (|a,2n|g). Other: 180 {I70} from ({+30}Si,X|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1168.827 {I20} from {+98}Nb |b{+-} decay (51.1 min), 1168.81 {I16} from (|a,2n|g), and 1168.5 {I5} from ({+30}Si,X|g) 
$|d(M3/E2)=+0.01 {I4} from (|a,2n|g) 
RI$other: 100 {I21} from ({+30}Si,X|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
E$weighted average of 1913.4 {I4} from {+98}Nb |b{+-} decay (51.1 min), 1913.60 {I33} from (|a,2n|g), 1913.1 {I3} from (n,|g) E=th, and 1913.6 {I2} from (n,n'|g) 
RI$from (n,n'|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$unweighted average of 1980.17 {I5} from {+98}Nb |b{+-} decay (51.1 min), 1981.20 {I32} from (|a,2n|g), 1979.9 {I3} from (n,|g) E=th, and 1980.3 {I3} from (n,n'|g) 
$Only the 1980|g reported in (|a,2n|g), |d(M3/E2)=+0.01 {I11} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$weighted average of 1285.63 {I16} from (|a,2n|g), 1285.42 {I14} from (n,|g) E=th, and 1285.6 {I2} from (n,n'|g) 
M$|d(M2/E1)=-0.02 {I3} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 157.88 {I10} from {+98}Nb |b{+-} decay (51.1 min), 157.87 {I16} from (|a,2n|g), and 157.6 {I4} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 330.37 {I10} from {+98}Nb |b{+-} decay (51.1 min) and 330.18 {I23} from (|a,2n|g) 
RI$weighted average of 29.3 {I25} from {+98}Nb |b{+-} decay (51.1 min) and 23 {I6} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 493.18 {I10} from {+98}Nb |b{+-} decay (51.1 min) and 493.09 {I20} from (|a,2n|g) 
RI$weighted average of 29 {I7} from {+98}Nb |b{+-} decay (51.1 min) and 23 {I6} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 944.39 {I44} from (|a,2n|g) and 944.7 {I2} from (n,|g) E=th 
RI$from (|a,2n|g). Other: 118 {I30} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1452.69 {I42} from (|a,2n|g) and 1452.3 {I3} from (n,|g) E=th 
RI$from (|a,2n|g). Other: 100 {I30} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
E$weighted average of 1466.79 {I10} from {+98}Nb |b{+-} decay (51.1 min), 1466.96 {I24} from (|a,2n|g), and 1467.1 {I3} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
E$weighted average of 399.65 {I10} from {+98}Nb |b{+-} decay (51.1 min) and 399.43 {I18} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$weighted average of 676.87 {I10} from {+98}Nb |b{+-} decay (51.1 min) and 676.66 {I26} from (|a,2n|g) 
RI$weighted average of 34 {I6} from {+98}Nb |b{+-} decay (51.1 min) and 33.5 {I24} from (|a,2n|g) 
$|d(M2/E1)=-0.01 {I10} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1002.9 {I2} from {+98}Nb |b{+-} decay (51.1 min) and 1002.85 {I31} from (|a,2n|g) 
RI$weighted average of 31 {I13} from {+98}Nb |b{+-} decay (51.1 min) and 24.4 {I10} from (|a,2n|g) 
$|d(M3/E2)=+0.03 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1511.68 {I2} from {+98}Nb |b{+-} decay (51.1 min), 1511.65 {I34} from (|a,2n|g), and 1512.0 {I3} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
E$weighted average of 1540.92 {I5} from {+98}Nb |b{+-} decay (51.1 min), 1540.47 {I52} from (|a,2n|g), and 1541.6 {I3} from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 446.91 {I10} from {+98}Nb |b{+-} decay (51.1 min), 446.78 {I17} from (|a,2n|g), 446.99 {I13} from (n,|g) E=th, and 447.2 {I3} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$unweighted average of 476.35 {I10} from {+98}Nb |b{+-} decay (51.1 min), 475.23 {I17} from (|a,2n|g), and 475.3 {I5} from ({+30}Si,X|g) 
M$|d(M3/E2)=+0.01 {I3} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$unweighted average of 753.19 {I14} from {+98}Nb |b{+-} decay (51.1 min), 752.41 {I16} from (|a,2n|g), and 752.7 {I5} from ({+30}Si,X|g) 
RI$weighted average of 73 {I9} from {+98}Nb |b{+-} decay (51.1 min), and 81.2 {I16} from (|a,2n|g). Other: 42 {I5} from ({+30}Si,X|g) is discrepant 
M$|d(M2/E1)=-0.01 {I4} from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1599.50 {I33} from (|a,2n|g) and 1598.8 {I7} from (n,|g) E=th 
RI$from (|a,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1193.09 {I30} from (|a,2n|g), 1193.3 {I3} from (n,|g) E=th, and 1193.1 {I4} from (n,n'|g) 
RI$from (n,|g) E=th 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1701.503 {I20} from {+98}Nb |b{+-} decay (51.1 min), 1701.8 {I3} from (n,|g) E=th, and 1701.8 {I6} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1908.6 {I2} from {+98}Nb |b{+-} decay (51.1 min) and 1909.7 {I6} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1945.01 {I5} from {+98}Nb |b{+-} decay (51.1 min), 1945.1 {I4} from (n,|g) E=th, and 1945.7 {I3} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 560.7 {I5} from (|a,2n|g) and 560.2 {I5} from ({+30}Si,X|g) 
RI$from ({+30}Si,X|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1394.07 {I10} from {+98}Nb |b{+-} decay (51.1 min), 1394.2 {I2} from (n,|g) E=th, and 1394.7 {I3} from (n,n'|g) 
RI$other: 100 {I24} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from relative I|g of 408.4|g from 3809.6 level and that only a small fraction of the intensity of the 408.4|g doublet may belong here 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 878.1 {I5} from (|a,2n|g) and 877.6 {I5} from ({+30}Si,X|g) 
RI$from ({+30}Si,X|g) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
E$from level energy difference 
M$no corresponding |g ray seen in ce data 
TI$from I(|g+ce)(absolute)(735)=26 {I4} determined from ce(854 E0 in {+98}Zr)/ce(735 E0 in {+98}Mo)=0.56 {I6} (1983VaZJ) and absolute intensity I(|g+ce)=14.4 {I14} of 854 transition in {+98}Zr (see {+98}Y |b{+-} decay: 0.548 s). 1987Ma58 deduced a value of 26 {I6} using I(|g+ce)(854)=15 {I3}. Other %I(|g+ce) measurements: 5.5 {I11} (1976He10), 6 {I2} (1967Hu07) 
$ce(854)/ce(735)=0.40 in 1971Fo21 gives absolute I(|g+ce)|?30 (as deduced by 1976He10). Others: ce(854)/ce(735)=0.36 {I6}, 0.47 {I5} in two different reactions (1983VaZQ) is consistent with that from 1987Ma58 and 1971Fo21. See general comment on I|g for details of these measurements 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$absolute I|g=13 {I1} (1987Ma58). Others: 3.2 {I5} (1976He10), 4.0 {I20} (1969Hu07). See also general comment on I|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$E|g=644.6 {I5}, I|g=1.6 {I5} (1971Le19) 
MR$2016Th01 discussed their result with previous measurements and conclude that a larger mixing ratio (dominant E2 component) is favored by the analysis of their (645|g)(787|g)(|q) data (Fig. A.4 in 2016Th01), as well as |d(E2/M1)=+3.2 {I+46-14} deduced from OSIRIS data. Low values of +0.13 {I4}, +0.27 {I2} and 0.58 {I5} reported in previous experiments are inconsistent with the |g|g(|q) data in the present experiment, while a value of +1.70 {I16} reported in a previous (n,n'|g) experiment is in agreement with the present result 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$also from |g(|q) (1971Le19) 
$|d(M3/E2)=+0.02 {I3} (2016Th01) 
$E|g=722.8 {I2}, I|g=85 {I4} (1971Le19) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|d(M3/E2)=-0.01 {I7} (2016Th01) 
M$also from |g(|q) in 1971Le19 
$E|g=833.7 {I2}, I|g=57 {I2} (1971Le19) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$2016Th01 did not observe this |g in coincidence with the 1023|g as expected from previously reported data. Upper limit of intensity is given by 2016Th01 


decay_energy_unit: KEV
decay_multipolarity: [M3]
decay_uncertain: ?
decay_comment:
$Mult=M3 implied by |DJ|p makes this transition very unlikely, thus its placement is marked as questionable. 


decay_energy_unit: KEV
decay_comment:
$2016Th01 placed this transition feeding the 2333.02 level, however, the least-squares fit procedure (using GTOL code) reproduces the level energies of the 2333 doublet in 2016Th01 better if this |g were to feed the 2333.41 level, thus the evaluators place this |g from the 3021.83 level to 2333.41 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
$|d(M2/E1)=-0.01 {I4} (2016Th01) 
$E|g=752.8 {I5}, I|g=12 {I3} (1971Le19) 
RI$the intensity in the present experiment is consistent with results from a previous (|a,2n|g) experiment, but not with the previous |b-decay results. 2016Th01 point out that in previous |b decay study, if the intensities of the two gamma rays (753.0 and 753.19) near this energy were to be interchanged, then the results agree with the present data. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$poor fit. Level-energy difference=1630.4 
RI$total I|g=0.86 {I10}. Intensity division is based on adopted gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 6080.0 {I6} (1971He10) 
RI$weighted average of 0.17 {I2} (1971He10) and 0.20 {I5} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 6435.6 {I6} (1971He10) 
RI$weighted average of 0.37 {I3} (1971He10) and 0.34 {I4} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
$Other: 6624.6 {I6}, I|g=10.0 (1971He10) 
M$from radiation strength (1971He10) 
RI$absolute intensity=10.0 (1960Gr36) 
$(6625|g)(2017|g)(|q) gives J|p(2017)=3,4 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 6883.5 {I6} (1971He10) 
RI$weighted average of 0.25 {I2} (1971He10) and 0.17 {I3} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 7208.8 {I11} (1971He10) and 7210.7 {I4} (1991Is05) 
RI$other: 0.10 {I3} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 7854.6 {I6} (1971He10) and 7853.9 {I4} (1991Is05) 
RI$other: 0.11 {I5} (1991Is05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR$from |g(|q). |d=+0.13 {I4} is also possible but less likely from syst which suggest dominant E2 component for transitions from second 2+ to first 2+ states. 1970SwZZ give |d=2.3 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
$Branching ratio for two photon emission: |G{-|g|g}/|G<0.0001 at 95% confidence level (2014He12). Two methods were used, one based on direct population of 735, 0+ state, and the second based on population of 735, 0+ level through 1024|g from 1758,2+ level. 


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: S
decay_comment:
E$from the Adopted dataset. Transition expected from Coulomb excitation. 
TI$from B(E2)|^=0.130 {I+14-34} (2002Zi06). Other: 0.00191 {I9} from B(E2)|^=0.293 {I14} (1978La17). 
$B(E2)(W.u.) from B(E2)|^=0.130 {I+14-34} (2002Zi06). Other B(E2)(W.u.)=21.8 {I11} from B(E2)|^=0.293 {I14} (1978La17). 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
$(1024|g)(735ce) coin (1969Hu07) 
E$from level difference 
TI$from I(|g+ce)(697|g+1024|g+1282|g). No |b{+-} decay is expected to 735 state 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$based on branching ratios for 3097 level in (|a,2n|g), 2016Th01 proposed interchanging the placements of 753.0|g and 753.19|g, i.e. former from 2976 level, and the latter from 3097 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$I{-s}(eVb)=14.5 {I18} 
$|G{+2}{-0}/|G(meV)=10.0 {I13} (2008Ru04) 
$B(E1)(|_)=0.18|*10{+-5} {I4}, B(M1)(|_)=0.017 {I3} 
$I|g(90|')/I|g(127|')=0.71 {I19} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E From curved-crystal measurement (1979Bo26). 
M |a(K)exp suggests M1+E2, but placement in level scheme requires, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_uncertain: S
decay_comment:
E from the adopted gammas 
RI from the adopted branching ratios and I|g(451|g)=5.5 {I10} 
TRANSITION ADDED. 910115 TWB 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_uncertain: S
decay_comment:
E from the adopted gammas 
RI from the adopted branching ratios and I|g(264|g)=5.2 {I10} 
TRANSITION ADDED. 910115 TWB 


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$unweighted average 535.666 {I14} from {+100}Nb |b{+-} decay and 535.547 {I13} from (n,n'|g). Others: 535.3 {I5} in (t,p|g), 535.6 {I5} in ({+30}Si,X|g), 536 {I1} in ({+136}Xe,X|g). 
M$|DJ=2, 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$from (n,n'|g). Others: 159.5 {I1} in {+100}Nb |b{+-} decay, 159.1 {I5} in (t,p|g) 
RI$from Coulomb excitation. 
M$|DJ|p and T{-1/2}(level) are consistent with only E2, not M2. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
E$from level energy difference. Transition observed only in ce data 
TI$deduced from Ice(K)(695|g)/Ice(K)(159|g)=0.63 {I8} (unweighted average of 0.62 {I5} and 0.76 {I5} from (p,p'|g), and 0.50 {I3} from (t,p|g)) 
$q{-K}{+2}(E0/E2)=0.61 {I10}, X(E0/E2)=0.014 {I2}, |r{+2}(E0)=0.036 {I6} (2005Ki02, evaluation) 
$B(E0)(Wilkinson units)=0.17 {I2} 


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$weighted average of 368.6 {I5} from {+100}Nb |b{+-} decay (1.5 s) and 369.1 {I1} from (n,n'|g) 
RI$weighted average of 1.4 {I3} from {+100}Nb |b{+-} decay (1.5 s), 2.01 {I21} from (n,n'|g), and 1.70 {I20} from Coulomb excitation 


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_comment:
E$weighted average of 528.263 {I18} from {+100}Nb |b{+-} decay (1.5 s), 528.263 {I18} from {+100}Nb |b{+-} decay (2.99 s), 528.4 {I5} from (t,p), 528.21 {I2} from (n,n'|g), and 528.4 {I5} from ({+30}Si,X|g) 
RI$from (n,n'|g). Others: 100.0 {I20} from Coul. ex., 100.0 {I22} from {+100}Nb |b{+-} decay (1.5 s), 100 {I13} from {+100}Nb |b{+-} decay (2.99 s) 
M$from |g|g(|q) in {+100}Nb |b{+-} decay, |g(|q) in (n,n'|g); M2 ruled out by RUL 
MR$from |g|g(|q) in {+100}Nb |b{+-} decay (1.5 s). Other: +3.4 {I4} 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$weighted average of 1063.7 {I1} from {+100}Nb |b{+-} decay (1.5 s), 1063.7 {I2} from {+100}Nb |b{+-} decay (2.99 s), 1064.1 {I1} from (|g,|g'), 1063.76 {I3} from (n,n'|g), and 1064 {I1} from ({+30}Si,X|g) 
RI$weighted average of 36.3 {I22} from {+100}Nb |b{+-} decay (1.5 s), 42 {I9} from {+100}Nb |b{+-} decay (2.99 s), 38.1 {I4} from (n,n'|g), 58 {I25} from ({+30}Si,X|g), and 38.0 {I10} from Coulomb excitation 
M$Q from |g(|q) in (n,n'|g) and |g|g(|q) in {+100}Nb |b{+-} decay (1.5 s); 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$weighted average of 600.5 {I1} from {+100}Nb |b{+-} decay (1.5 s), 600.5 {I1} from {+100}Nb |b{+-} decay (2.99 s), and 600.39 {I2} from (n,n'|g). Others: 599.8 {I5} from (t,p), 601 {I1} from ({+136}Xe,X|g), and 600.3 {I5} from ({+30}Si,X|g) 
M$from T{-1/2}(level), |DJ|p and RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from (n,n'|g). Other: 400 {I1} from {+100}Nb |b{+-} decay (1.5 s) 
RI$weighted average of 5 {I3} from {+100}Nb |b{+-} decay (1.5 s), 4.9 {I7} from (n,n'|g), and 5.8 {I11} from Coulomb excitation 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 768.7 {I1} from {+100}Nb |b{+-} decay (1.5 s), 768.8 {I2} from {+100}Nb |b{+-} decay (2.99 s), and 768.77 {I3} from (n,n'|g) 
RI$from Coulomb excitation. Other: 100.0 {I13} from (n,n'|g), 100 {I9} from {+100}Nb |b{+-} decay (1.5 s) 
M$Q from |g(|q) in (n,n'|g) and |g|g(|q) in {+100}Nb |b{+-} decay (1.5 s); M2 ruled out by RUL 


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$weighted average of 928.3 {I1} from {+100}Nb |b{+-} decay (1.5 s), 928.4 {I2} from {+100}Nb |b{+-} decay (2.99 s), and 928.34 {I3} from (n,n'|g) 
RI$weighted average of 74 {I3} from {+100}Nb |b{+-} decay (1.5 s), 71 {I8} from {+100}Nb |b{+-} decay (2.99 s), 72.8 {I9} from (n,n'|g), and 73.0 {I10} from Coulomb excitation 
M,MR$from |g|g(|q) {+100}Nb |b{+-} decay (1.5 s) and RUL. Other: -0.36 {I7} from |g(|q) in (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 440.9 {I1} from {+100}Nb |b{+-} decay (1.5 s) and 440.83 {I5} from (n,n'|g) 
RI$unweighted average of 41.2 {I19} from {+100}Nb |b{+-} decay (1.5 s) and 33.6 {I21} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 969.1 {I1} from {+100}Nb |b{+-} decay (1.5 s) and 969.06 {I7} from (n,n'|g) 
M$|g|g(|q) in {+100}Nb |b{+-} decay (1.5 s), |DJ|p and RUL (|b|g coin in {+100}Nb |b{+-} decay (1.5 s) suggests 1504.6 level has T{-1/2}<50 ns) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 471 {I1} from {+100}Nb |b{+-} decay (1.5 s), 471.2 {I3} from {+100}Nb |b{+-} decay (2.99 s), and 471.39 {I9} from (n,n'|g) 
RI$weighted average of 23 {I14} from {+100}Nb |b{+-} decay (1.5 s), 18 {I7} from {+100}Nb |b{+-} decay (2.99 s), and 16.8 {I20} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 543.4 {I2} from {+100}Nb |b{+-} decay (1.5 s), 543.2 {I2} from {+100}Nb |b{+-} decay (2.99 s), 543.62 {I6} from (n,n'|g), and 544.1 {I5} from ({+30}Si,X|g) 
RI$from {+100}Nb |b{+-} decay (1.5 s). Others: 100 {I8} from (n,n'|g), 100 {I15} from {+100}Nb |b{+-} decay (2.99 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1071.6 {I2} from {+100}Nb |b{+-} decay (1.5 s) and 1071.77 {I3} from (n,n'|g). Others: 1071.6 {I3} from {+100}Nb |b{+-} decay (2.99 s) and 1071.9 {I5} from ({+30}Si,X|g) 
RI$weighted average of 69 {I13} from {+100}Nb |b{+-} decay (2.99 s), 74.0 {I12} from (n,n'|g), and 52 {I16} from ({+30}Si,X|g); the transition mainly deexcites the 1607 level. Other: 116 {I19} from {+100}Nb |b{+-} decay (1.5 s) is in disagreement. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from (n,n'|g). Other: 635.4 {I3} from {+100}Nb |b{+-} decay (2.99 s) 
RI$weighted average of 53 {I8} from {+100}Nb |b{+-} decay (2.99 s), 55 {I3} from (n,n'|g), and 55 {I3} from Coulomb excitation 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 707.5 {I2} from {+100}Nb |b{+-} decay (2.99 s) and 707.68 {I3} from (n,n'|g) 
RI$from (n,n'|g) and Coulomb excitation. Other: 100 {I14} from {+100}Nb |b{+-} decay (2.99 s) 
M$from T{-1/2}(level), |DJ|p and 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$weighted average of 711.0 {I2} from {+100}Nb |b{+-} decay (2.99 s), 711.16 {I6} from (n,n'|g), 711 {I1} from ({+136}Xe,X|g), and 711.1 {I5} from ({+30}Si,X|g) 
M$from T{-1/2}, |DJ|p 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$from (n,n'|g). Other: 844.5 {I5} from ({+30}Si,X|g) 
RI$from Coulomb excitation. Others: 100 {I14} from ({+30}Si,X|g), |?100 in (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$unweighted average of 1372.73 {I4} from (n,n'|g) and 1371.4 {I5} from ({+30}Si,X|g) 
RI$from Coulomb excitation. Other: 20 {I6} in {+168}Er({+30}Si,X|g), 36.1 {I15} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 913.2 {I5} from {+100}Nb |b{+-} decay (1.5 s) and 913.72 {I9} from (n,n'|g) 
RI$from (n,n'|g). Other: 70 {I30} from {+100}Nb |b{+-} decay (1.5 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1441.5 {I2} from {+100}Nb |b{+-} decay (1.5 s) and 1441.69 {I7} from (n,n'|g) 
RI$from (n,n'|g). Other: 100 {I22} from {+100}Nb |b{+-} decay (1.5 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$unweighted average of 1501.9 {I1} from {+100}Nb |b{+-} decay (1.5 s) and 1502.4 {I2} from (n,n'|g) 
M$|g|g(|q) in {+100}Nb |b{+-} decay (1.5 s), |DJ|p and RUL (|b|g coin in {+100}Nb |b{+-} decay (1.5 s) suggests 1504.6 level has T{-1/2}<50 ns) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$|g|g(|q) in {+100}Nb |b{+-} decay (1.5 s), |DJ|p and RUL (|b|g coin in {+100}Nb |b{+-} decay (1.5 s) suggests 1504.6 level has T{-1/2}<50 ns) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 639.0 {I3} from {+100}Nb |b{+-} decay (2.99 s) and 639.2 {I2} from (n,n'|g) 
RI$weighted average of 22 {I3} from {+100}Nb |b{+-} decay (2.99 s) and 29 {I4} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 966.9 {I2} from {+100}Nb |b{+-} decay (2.99 s) and 967.1 {I1} from (n,n'|g) 
RI$from (n,n'|g). Other: 100 {I11} from {+100}Nb |b{+-} decay (2.99 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1567.4 {I3} from {+100}Nb |b{+-} decay (2.99 s) and 1567.8 {I2} from (n,n'|g) 
RI$unweighted average of 35 {I5} from {+100}Nb |b{+-} decay (2.99 s) and 70 {I4} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Placement uncertain since a transition of similar energy is assigned to the 3129 level in {+100}Nb |b{+-} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 681.8 {I4} from {+100}Nb |b{+-} decay (2.99 s) and 682.5 {I5} from ({+30}Si,X|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 1280.4 {I2} from {+100}Nb |b{+-} decay (2.99 s) and 1280.9 {I2} from (n,n'|g) 
RI$from {+100}Nb |b{+-} decay (2.99 s) 
M,MR$from |g|g(|q) in {+100}Nb |b{+-} decay (2.99 s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 461.2 {I2} from {+100}Nb |b{+-} decay (2.99 s) and 461.0 {I2} from (n,n'|g) 
RI$from {+100}Nb |b{+-} decay (2.99 s). Other: 100 {I21} from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1427.9 {I3} from {+100}Nb |b{+-} decay (2.99 s) and 1428.1 {I3} from (n,n'|g) 
RI$from {+100}Nb |b{+-} decay (2.99 s). Other: 120 {I20} 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$weighted average of 781 {I1} from ({+136}Xe,X|g) and 780.1 {I5} from ({+30}Si,X|g) 
M$from T{-1/2}, |DJ|p and RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$placement considered uncertain since a transition of similar energy is assigned to the 3062 level in {+100}Nb |b{+-} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$others: 535.4 {I2} (2001Su11), 535.7 {I1} (1987Me06) from Ge detector 
RI$100 {I5} (2012Ro01), 100.0 {I23} (1987Me06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$159.5 {I1} (1987Me06), 159.6 {I2} (2001Su11) 
RI$I(|g+ce)=6.7 {I11} (1987Me06). I|g=14.3 {I11} (2012Ro01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
E$others: 528.0 {I2} (2001Su11), 528.3 {I1} (1987Me06) from Ge detector 
RI$14.0 {I12} (2012Ro01), 9.0 {I17} (1987Me06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$1280.3 {I2} (2001Su11), 1280.6 {I2} (1987Me06) 
RI$11.2 {I12} (2012Ro01), 24.5 {I16} (1987Me06) 
M,MR$deduced by the evaluator from (1280|g)(600|g)(|q): A{-2}=+0.23 {I15}, A{-4}=-0.02 {I26} (1987Me06). J|p=3- for 2416 level was also suggested by L(|a,|a')=3 but 3- choice gives |d(M2/E1)<-0.3, which seems too high to be realistic 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
$ce(K)(E0)/I(|g+ce)(159+694)=0.071 {I4} (1987Es01). This ratio gives I(|g+ce)(694|g)/I(|g+ce)(159|g)=0.093 {I5} and I(ce(K)(695,E0))/I(ce(K)(159|g,E2))=0.50 {I3} 


decay_energy_unit: KEV
decay_multipolarity: (D)
decay_comment:
E$2901.2 {I1} (2006Ru06) 
$I|g(90|')/I|g(127|')=1.22 {I12} 
$I|g(90|')/I|g(127|')=0.73 {I20} (2006Ru06) 


decay_energy_unit: KEV
decay_multipolarity: (D)
decay_comment:
E$2906.3 {I1} (2006Ru06) 
$I|g(90|')/I|g(127|')=1.19 {I12} 
$I|g(90|')/I|g(127|')=0.95 {I19} (2006Ru06) 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
E$3242.5 {I1} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.91 {I12} 
$I|g(90|')/I|g(127|')=0.70 {I10} (2006Ru06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E$2595.2 {I1} (2006Ru06) 
$B(E1)(|_)=0.09|*10{+-5} {I3}, B(M1)(|_)=0.008 {I3} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.74 {I20} (2006Ru06) 
$I{-s}=20 eVb {I2}. |G{+2}{-0}/|G=11.4 meV {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E$2754.7 {I2} (2006Ru06) 
$Placement from 2006Ru06 
$|G{+2}{-0}/|G(meV)=3.3 {I9}. I{-s}(eVb)=4.9 {I14} 
$B(E1)(|_)=0.07|*10{+-5} {I3}, B(M1)(|_)=0.007 {I2} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.79 {I19} (2006Ru06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$3290.1 {I1} (2006Ru06) 
$B(E1)(|_)=0.20|*10{+-5} {I4}, B(M1)(|_)=0.018 {I4} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.72 {I7} (2006Ru06) 
$I|g(90|')/I|g(127|')=1.08 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$|g from 2006Ru06 only 
$B(E1)(|_)=0.34|*10{+-5} {I7}, B(M1)(|_)=0.031 {I6} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.62 {I12} (2006Ru06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$|g from 2006Ru06 only 
$B(E1)(|_)=0.21|*10{+-5} {I4}, B(M1)(|_)=0.018 {I3} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.72 {I13} (2006Ru06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E$3483.4 {I1} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.94 {I7} 
$B(E1)(|_)=1.02|*10{+-5} {I12}, B(M1)(|_)=0.091 {I10} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.68 {I7} (2006Ru06) 


decay_energy_unit: KEV
decay_multipolarity: (D)
decay_comment:
E$3570.3 {I1} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.96 {I10} 
$I|g(90|')/I|g(127|')=0.75 {I10} (2006Ru06) 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
E$3614.7 {I1} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.67 {I14} 
$I|g(90|')/I|g(127|')=0.64 {I15} (2006Ru06) 


decay_energy_unit: KEV
decay_multipolarity: (D)
decay_comment:
E$3627.8 {I1} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.36 {I12} 
$I|g(90|')/I|g(127|')=0.71 {I12} (2006Ru06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$2595.2 {I1} (2006Ru06) 
$I{-s}=20 eVb {I2}. |G{+2}{-0}/|G=11.4 meV {I12} 
$B(E1)(|_)=0.23|*10{+-5} {I9}, B(M1)(|_)=0.020 {I8} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.74 {I20} (2006Ru06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$3658.7 {I1} (2006Ru06) 
$B(E1)(|_)=0.41|*10{+-5} {I8}, B(M1)(|_)=0.036 {I7} (2006Ru06) 
$I|g(90|')/I|g(127|')=0.8 {I2} 
$I|g(90|')/I|g(127|')=0.65 {I14} (2006Ru06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR$from |g(|q). Alternate |d=-0.11 {I4} is inconsistent with that from |g|g(|q) data in {+100}Nb |b{+-} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR$from |g(|q). Alternate |d=+19.6 +|@-9.8 is inconsistent with that from |g|g(|q) in {+100}Nb |b{+-} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$unresolved from a background line near this energy. Using branching ratio from Coulomb excitation data, I|g=2.2 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
$Other |d(E2/M1)=+5.2 {I+33-15}, deduced by evaluators from E2 and M1 matrix elements in 2012Wr03, where |d=+4.4 {I15} was used as input in their GOSIA analysis 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$Other |d(E2/M1)=-0.27 {I+8-6}, deduced by evaluators from E2 and M1 matrix elements in 2012Wr03, where |d=-27 {I2} was used as input in their GOSIA analysis 


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:
$B(E2) deduced from ratio of yields of 780|g (8+ to 6+ transition) and 711|g (6+ to 4+ transition). Evaluators assume that the B(E2) value given by 1986Ho25 is B(E2)|_ 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$statistical uncertainty is 0.1 in 1982VoZP. Evaluators assign |?2% to include a crude estimate of systematic uncertainty. 
$Relative I|g=100 {I8} (2012Ro01) 
E$others: 535.7 {I1} (1987Me06), 535.5 {I1} (1982VoZP), 535.4 {I5} (1976Ah06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$same value in 1987Me06 and 1982VoZP 
RI$8.2 {I12} in 1982VoZP from I(|g+ce)=10.8 {I6} and |a=0.22 
$I|g(159.5)/I|g(535.7)=28.7 {I16}/100 {I8} (2012Ro01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
E,M$transition seen in ce measurements (1975Kh05). K/L=11.7 {I38} (1975Kh05) 
TI$using branching of 695 transition from the Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
E$528.2 {I1} (1982VoZP), 528.3 {I1} (1987Me06) 
$I|g(528.2)/I|g(535.7)=21.2 {I15}/100 {I8} (2012Ro01) 
M$from T{-1/2}(1064 level), |d(528|g) and RUL 
MR$from A{-2}=-0.22 {I3}, A{-4}=+0.31 {I3} for (528|g)(536|g)(|q) (1987Me06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$1063.7 {I1} (1982VoZP), 1063.9 {I2} (1987Me06) 
$I|g(1063.7)/I|g(535.7)=8.9 {I7}/100 {I8} (2012Ro01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$768.6 {I1} (1982VoZP), 768.9 {I2} (1987Me06) 
$I|g(768.7)/I|g(535.7)=8.1 {I6}/100 {I8} (2012Ro01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$928.2 {I1} (1982VoZP), 928.5 {I2} (1987Me06) 
$I|g(928.3)/I|g(535.7)=7.3 {I6}/100 {I8} (2012Ro01) 
MR$from A{-2}=+0.38 {I7}, A{-4}=0.00 {I12} for (928|g)(536|g)(|q) (1987Me06) 
M$from T{-1/2}(1464 level), |d(928|g) and RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$440.9 {I1} (1982VoZP), 440.7 {I2} (1987Me06) 
$I|g(440.9)/I|g(535.7)=1.9 {I2}/100 {I8} (2012Ro01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$969.1 {I1} (1982VoZP), 969.1 {I4} (1987Me06) 
$I|g(969.1)/I|g(535.7)=5.6 {I5}/100 {I8} (2012Ro01) 
$(969|g)(536|g)(|q): A{-2}=+0.30 {I12}, A{-4}=+1.43 {I24} (1987Me06) is typical of 0-2-0 cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$543.5 {I1} (1982VoZP), 543.0 {I2} (1987Me06) 
$No relative intensity given in 2012Ro01 from {+100}Nb g.s. decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1071.7 {I2} (1982VoZP), 1071.5 {I3} (1987Me06) 
$I|g(1071.6)/I|g(535.7)=0.9 {I1}/100 {I8} (2012Ro01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$1501.9 {I1} (1982VoZP), 1502.0 {I3} (1987Me06) 
$I|g(1501.9)/I|g(535.7)=12.7 {I11}/100 {I8} (2012Ro01) 
$(1502|g)(536|g)(|q): A{-2}=+0.36 {I8}, A{-4}=+1.05 {I14} (1987Me06) is typical of 0-2-0 cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$622.4 {I2} (1982VoZP), 622.6 {I2} (1987Me06) 
$I|g(622.5)/I|g(535.7)=3.7 {I4}/100 {I8} (2012Ro01) 
$(622|g)(769|g)(|q): A{-2}=+0.31 {I9}, A{-4}=+1.26 {I19} (1987Me06) is typical of 0-2-0 cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$1022.2 {I2} (1982VoZP), 1022.8 {I2} (1987Me06) 
$I|g(1022.5)/I|g(535.7)=12.3 {I11}/100 {I8} (2012Ro01) 
$(1022|g)(528|g)(|q): A{-2}=+0.08 {I5}, A{-4}=+0.27 {I7} (1987Me06) 
$(1022|g)(1064|g)(|q): A{-2}=+0.41 {I25}, A{-4}=+1.28 {I43} (1987Me06) is typical of 0-2-0 cascade 
$(1022|g)(536|g)(|q): A{-2}=-0.01 {I4}, A{-4}=+0.15 {I6} (1987Me06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1653.9 {I2} (1982VoZP), 1653.9 {I4} (1987Me06) 
$I|g(1653.9)/I|g(535.7)=3.0 {I4}/100 {I8} (2012Ro01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1256.5 {I4} (1982VoZP), 1257.8 {I5} (1987Me06) 
$I|g(1256.5)/I|g(535.7)=2.1 {I3}/100 {I8} (2012Ro01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=?
decay_comment:
MR from a{-22}=-0.43 and a{-44}=0.0. No uncertainty given by the authors (1988GiZX). M1+E2 is the most probable multipolarity 


decay_energy_unit: KEV
decay_comment:
No half-life could be determined for this |g-ray. The mass assignment is based on |g|g-coin measurements 


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$A{-2}=-0.12~{I1}; A{-4}=0.02~{I2} in {+252}Cf SF decay (2009Go18); p|g=0.04~{I19} in {+252}Cf SF decay (1996Ur04); Also, K/L=4.8 in 1970Wa05 is consistent with E2, but the 94.9-keV |g-ray was assigned to A=106 {I+-1} molybdenum isotope 
MR$Also: -0.12~{I3} or -2.9~{I5} from 283.2|g-94.9|g(|q) in {+252}Cf SF decay (2009Go18), and -0.5~{I3} in {+252}Cf SF decay (1996Ur04) 


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$A{-2}=-0.357~{I5}, A{-4}=+0.023~{I8} {+252}Cf SF decay (2006Or05); Also: A{-2}=-0.17~{I1}, A{-4}=-0.01~{I2} in {+252}Cf SF decay (2009Go18) 
MR$Also: -0.25~{I4} or -2.3~{I2} in {+252}Cf SF decay (2009Go18) 


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}=+0.324~{I6}, A{-4}=+0.012~{I9} in {+252}Cf SF decay (2006Or05); Also: A{-2}=-0.156~{I9}, A{-4}=+0.005~{I14} in {+252}Cf SF decay (2006Or05) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.12~{I1}; A{-4}=0.02~{I2} from {+252}Cf SF decay (2009Go18); p|g=0.04~{I19} from {+252}Cf SF decay (1996Ur04); Also, K/L=4.8 in 1970Wa05 is consistent with E2, but the 94.9-keV |g-ray was assigned to A=106 {I+-1} molybdenum isotope 
MR$Also: -0.12~{I3} or -2.9~{I5} from 283.2|g-94.9|g(|q) from {+252}Cf SF decay (2009Go18), and -0.5~{I3} in {+252}Cf SF decay (1996Ur04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.357~{I5}, A{-4}=+0.023~{I8} from {+252}Cf SF decay (2006Or05); Also: A{-2}=-0.17~{I1}, A{-4}=-0.01~{I2} in {+252}Cf SF decay (2009Go18) 
MR$Also: -0.25~{I4} or -2.3~{I2} from {+252}Cf SF decay (2009Go18) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=+0.324~{I6}, A{-4}=+0.012~{I9} from {+252}Cf SF decay (2006Or05); Also: A{-2}=-0.156~{I9}, A{-4}=+0.005~{I14} from {+252}Cf SF decay (2006Or05) 


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$consistent with (171.9|g)(|q) (1972Wi15) being Q; E2 from observed band structure. 
E$from curved crystal spectrometer (1979Bo26); others: 171.57 {I10} (1969WiZX), 171.7 (1970Ch11), 172.2 {i2} (1970Jo20), 171.6 {i2} (1974ClZX), 172.0 (1977YoZM) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp from ratio of intensities K|a| x ray line in Mo and 66|g in a gated spectrum 
$(66.0|g)(253.7|g)(|q): A{-2}=-0.03 {I2}, A{-4}=+0.04 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(exp) from intensity balance 
$(152.1|g)(414.5|g)(|q): A{-2}=-0.04 {I2}, A{-4}=-0.07 {I4} 
$(152.1|g)(306.4|g)(|q): A{-2}=+0.10 {I3}, A{-4}=-0.06 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from I|g(66)/I|g(99)=0.95 {I15} in a gated mode. Similar photon intensities for the two lines suggest same mult for 66|g and 99|g 
$(99.4|g)(326.3|g)(|q): A{-2}=-0.05 {I2}, A{-4}=+0.05 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(exp) from intensity balance; |a(K)exp from ratio of intensities K|a| x ray line in Mo and 110|g when gated with 123|g and 406|g 
$(110.2|g)(379.5|g)(|q): A{-2}=-0.06 {I2}, A{-4}=+0.04 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(exp) from intensity balance; |a(K)exp from ratio of intensities K|a| x ray line in Mo and 123|g in a gated spectrum 
$(123.4|g)(405.9|g)(|q): A{-2}=-0.07 {I2}, A{-4}=+0.02 {I3} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
$ -1.44<|d(E2/M1)<-0.44 from (306.4|g)(152.1|g)(|q), pure E1 assumed for 306.4|g. This |d value is in agreement with theoretical value of -0.20 for 5/2[402] orbital. For 5/2[413] orbital, theoretical |d is +0.79 
$ -1.76<|d(E2/M1)<-0.31 from (414.5|g)(152.1|g)(|q), pure E2 assumed for 414.5|g 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
$(110.2|g)(348.3|g)(|q): A{-2}=+0.14 {I3}, A{-4}=+0.06 {I4} 
$ |d=-0.18 {I9} or -0.0012 {I+570-1} from (110.2|g)(348.3|g)(|q), pure E1 assumed for 348.3|g. This |d value is in agreement with theoretical value of -0.16 for 7/2[523] orbital 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$from |a(exp) in 2006Ur01 using intensity balance considerations; A{-2}/A{-0}=+0.11 {I2}, A{-4}/A{-0}=-0.03 {I2} for (110.8|g)(222.2|g)(|q), gives |DJ=1 for 222.2|g (2006Ur01) 
E$Other: 222.5 keV in 1997Hw03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from |a(exp)=0.34 {i8}, deduced by the evaluators from the intensity balances and I|g in 2006Ur01; A{-2}/A{-0}=+0.11 {I2}, A{-4}/A{-0}=-0.03 {I2} for (110.8|g)(222.2|g)(|q), gives |DJ=1 for 110.8|g, in-band transition (2006Ur01) 
MR$calculated by evaluators from |a(exp) and the BrIccMixing program 
E$Other: 111.3 keV in 1997Hw03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-2}/A{-0}=+0.07 {I1}, A{-4}/A{-0}=-0.0 {I2} for (110.8|g)(138.9|g)(|q), gives |DJ=1 for 138.9|g. Also A{-2}/A{-0}=-0.09 {I2}, A{-4}/A{-0}=-0.0 {I2} (138.9|g)(413.7|g)(|q), gives |DJ=1 for 138.9|g; in-band transition (2006Ur01) 
E$Other: 139.3 keV in 1997Hw03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}/A{-0}=-0.09 {I2}, A{-4}/A{-0}=-0.0 {I2} (138.9|g)(413.7|g)(|q), gives |DJ=2 for 413.7|g, in-band transition (2006Ur01) 
E$Other: 413.2 keV in 1997Hw03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$139.3 keV in 1997Hw03 
RI$ 74.7 in 1997Hw03 
M$E1 from |a=0.04 {I3} in 1997Hw03, obtained by double gating on 111|g and 222|g. However, the uncertainty overlaps with M1 assignment within two standard deviations. The individual intensities were not given by the authors 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$from |a(exp) in 2006Ur01 using intensity balance considerations; A{-2}/A{-0}=+0.11 {I2}, A{-4}/A{-0}=-0.03 {I2} for (110.8|g)(222.2|g)(|q), gives |DJ=1 for 222.2|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from |a(exp)=0.34 {i8}, deduced by the evaluators from the intensity balances and I|g in 2006Ur01; A{-2}/A{-0}=+0.11 {I2}, A{-4}/A{-0}=-0.03 {I2} for (110.8|g)(222.2|g)(|q), gives |DJ=1 for 110.8|g 
MR$deduced by evaluators from |a(exp) using the BrIccMixing program 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-2}/A{-0}=+0.07 {I1}, A{-4}/A{-0}=-0.0 {I2} for (110.8|g)(138.9|g)(|q), gives |DJ=1 for 138.9 |g; A{-2}/A{-0}=-0.09 {I2}, A{-4}/A{-0}=-0.0 {I2} (138.9|g)(413.7|g)(|q), gives also |DJ=1 for 138.9|g (2006Ur01). 


decay_energy_unit: KEV
decay_comment:
E$From level energy difference. Reported in 2017Pa01, but the energy was tentatively given as around 300 keV. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (E2)
decay_comment:
$B(E2)(W.u.)=1.8 {I3}, assuming 100% branch for 81|g 
M$from |a(exp)=3.5 {I8} in {+9}Be({+107}Ag,X|g) (2008Ga04) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (E2)
decay_comment:
M$from |a(exp)=3.5 {I8} (deduced from intensity-balance arguments, 2008Ga04). Mult=E1+M2 is also possible if J|p=5- for 1524-keV isomer, with required |d=1.07 to match |a(exp)=3.5 {I8} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI,TI$2019Pa16 report total intensity assuming M1 multipolarity for the 146|g. I|g deduced by compiler from total intensity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$from {+58}Ni({+40}Ca,p2|a|g). Other: 797.7 {I17} in {+90}Rh |ep decay 
M$|DJ=2, Q from DCO, RUL(for E2 amd M2) gives E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
TI$per 100 decays from 2019Pa16 
RI$from I(|g+ce) and |a for assumed mult(179.2|g)=M1 
$Relative I|g=100 {I25} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$strong |g-ray identified in coincidence with Tc K|a| x ray but not placed in a decay scheme by 1994Zh26. 


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:
Other I|g: 128 {I5} at 65|' in ({+36}Ar,3p|g); 109 {I20} in ({+40}Ca,3p|g). 
M |D|p=no 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=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=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M DCO ratio consistent with Q (|DJ=2) or D (|DJ=0); 1994Ru01 assume the latter. 
Other I|g: 50 {I3} at 65|' in ({+36}Ar,3p|g); 61 {I9} in ({+40}Ca,3p|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
R: 1.02 {I5}; consistent with D multipolarity, but level scheme implies |DJ=2.. 
I(1048.6|g+1049.1|g)=4.3 {I2} (1993Ar01). 


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 213.8 {I2} from ({+3}He,2np|g), 213.81 {I12} from |e decay and 213.7 {I1} from (p,n|g). 
M D,E2 from RUL; adopted |DJ=(2). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
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:
E weighted average of 259.4 {I2} from ({+3}He,2np|g) and 259.27 {I15} from |e decay. 
M 259|g is D from ({+3}He,2np|g); adopted |D|p=(no). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
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:
E weighted average of 134.4 {I2} from ({+3}He,2np|g) and 134.60 {I9} from |e decay. 
M D from ({+3}He,2np|g); adopted |D|p=(no). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E,M |g unresolved from D 647.2|g in ({+40}Ca,5pn|g) where anisotropy of doublet is consistent with stretched Q; thus, mult=Q is favored for this component. 


