# LEVEL

level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)(from 540 level)=0.089 {I13}, weighted average of 0.088 {I13} (1980La01), 0.091 {I16} (1968Mc08), and 0.09 {I3} (1961St02) 
$B(E2)(from g.s.)=0.0190 {I23}, weighted average of 0.0203 {I23} (1980La01), 0.0185 {I25} (1968Mc08), 0.015 {I5} (1961St02) 
$|b{-22}=0.144 (1980La01), |b{-02}=0.044 (1980La01) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$Adopted B(E3) is from B(E3)=0.043 {I7} (1980La01, with only 1626|g from 2166 level) and Branching(1626|g)=0.81 (from the Adopted Gammas) 
T$from B(E3)=0.053 {I9} and the Adopted |g-ray branching ratio 
$|b{-3}=0.115 or 0.152 (1980La01). B(E3)=0.053 gives |b{-3}=0.128 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$2840 in 1972SeZR 
$ d|s/d|W=0.035 mb/sr {I1} at 6|', 0.0165 mb/sr {I4} at 15|'. |s(6|')/|s(15|')>2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_uncertain: ?
level_comment:
$Partial T{-1/2}(2|n+0|n,|b|b to 539,2+ level)>25|*10{+20} y (2014Ar08) 
$Partial T{-1/2}(2|n,|b|b to 539.5,2+ level)>11|*10{+20} y (2007Ar02) (90% confidence limit); >16|*10{+20} y (1995Ba29); >5|*10{+20} y (1992Bl06) 
$Partial T{-1/2}(0|n,|b|b to 539.5,2+ level)>1.6|*10{+23} y (2007Ar02) (90% confidence limit); >1.1|*10{+21} y (1995Da37) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
$Population of this level in {+100}Mo |b|b decay is confirmed by the observation of 22 |g|g coin events between 539.5|g and 590.8|g (2006Ho17,2009Ki04,2001De17) 
$Partial T{-1/2}(2|n,|b|b to 1130,0+ level)=7.5|*10{+20} y {I6}(stat) {I6}(syst) (2014Ar08) 
$Partial T{-1/2}(2|n+0|n,|b|b to 1130,0+ level)=6.9|*10{+20} y {I+10-8}(stat) {I7}(syst) (2010Be34). 
$Partial T{-1/2}(0|n+2|n)=6.0|*10{+20} y {I+20-13} (2009Ki04,2006Ho17) for decay to the 1130, 0+ state. The statistical uncertainty of +1.9-1.1 and systematic uncertainty of 0.6 have been combined in quadrature. 
$Partial T{-1/2}(2|n,|b|b to 1130,0+ level)=5.7|*10{+20} y {I+15-12} (2007Ar02) (90% confidence limit); 6.1|*10{+20} y {I+18-11} (1995Ba29); >12|*10{+20} y (1992Bl06) 
$Partial T{-1/2}(0|n+2|n)=5.9|*10{+20} y {I+17-11}(stat) {I6}(syst) (2001De17) 
$Partial T{-1/2}(0|n,|b|b to 1130,0+ level)>8.9|*10{+22} y (2007Ar02) (90% confidence limit); >1.7|*10{+21} y (1995Da37) 
$Others for partial T{-1/2} for decay to 1130 level: 2002De18, 2000De41, 1999Bb19 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_uncertain: ?
level_comment:
$Partial T{-1/2}(2|n+0|n,|b|b to 1362,2+ level)>108|*10{+20} y (2014Ar08) 
$Partial T{-1/2}(|b|b)>44|*10{+20} y at 90% confidence level for decay to 1362.2 keV 2+ level (2009Ki04,2006Ho17). 
$Partial T{-1/2}(2|n+0|n,|b|b to 1362,2+ level)>13|*10{+20} y (1995Ba29); >6|*10{+20} y (1992Bl06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_uncertain: ?
level_comment:
$Partial T{-1/2}(2|n+0|n,|b|b to 1741,0+ level)>40|*10{+20} y (2014Ar08) 
$Partial T{-1/2}(|b|b)>48|*10{+20} y at 90% confidence level for decay to 1741.0 keV 0+ level (2009Ki04,2006Ho17). 
$Partial T{-1/2}(2|n,|b|b to 1741,0+ level)>13|*10{+20} y (1995Ba29) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_uncertain: ?
level_comment:
$Partial T{-1/2}(2|n+0|n,|b|b to 2051,0+ level)>43|*10{+20} y (2014Ar08) 
$Partial T{-1/2}(|b|b)>38|*10{+20} y at 90% confidence level for decay to 2051.7 keV 0+ level (2009Ki04,2006Ho17). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_uncertain: ?
level_comment:
$Partial T{-1/2}(|b|b)>40|*10{+20} y at 90% confidence level for decay to 2387.2 keV 0+ level (2009Ki04,2006Ho17). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
MOMM1$other: -0.236 {i12} (1984Al11) 
E$analogous 3/2+ state in {+99}Ru at 89 keV with |m=-0.284 {i6} 
J$M1 |g to 5/2+, log| {If{+1u}t}=8.2 from 1/2- 
T$from 1986Sc15. Others: 0.55 ns {i3} (1966Ch13), 0.56 ns {i3} (1973Be72), 0.58 ns {i2} (1970La16) via |g|g(t) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T$0.20 ns {i4} (K| x ray)(198|g)(t) 1970La16; 0.14 ns {i3} from B(E2)=0.006 {i1} 
J$based on L=0 (d,p) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
T$from 1978Ba18 (221|g,307|g)(t) pulsed beam. Others: 17.5 |ms {i15} (1961Kr01,1964Br27), 22.5 |ms {i4} (1970Uy01,1971Uy01) 
J$L=5 (p,d), M2 |g decay to 7/2+ state; HF(M2) correspond with regional h11/2 to g7/2 transitions 
$%IT decay=100 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$L(d,p)=3, J=3/2 or 5/2 excit in (|a,n|g). 7/2- in (d,p) is preferred on model arguments and J=3/2 in (|a,n|g) is preferred from |g(|t) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
T$17.5 |ms {i4} (1978Ba18) (221|g,307|g)(t) pulsed beam; 17.5 |ms {i15} (1961Kr01,1964Br27); 22.5 |ms {i4} (1970Uy01,1971Uy01) 
%IT=100 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T (198|g)(127|g)(t) av: 0.55 ns {i3} (1966Ch13), 0.58 ns {i2} (1970La16) 0.56 ns {i3} (1973Be72). Others: 1966CoZX, 1971Bo13 
g-factor=-0.207 {i17} (1966Au06) (198|g)(127|g)(|q,H,t) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T$from 1970La16 (K| x ray)(198|g)(t), scin 
Branching: I|g(325|g)/I|g(198|g)=0.19 {i2} (1971Si16), 0.21 (1966Wo06), 0.21 (1966Ar05), 0.15 {i4} (1965Ev06) 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2
level_comment:
E different from the 720 level seen in (|a,3n|g) with J|p(9/2+), because of primary |g from level with J|p=1/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$from adopted levels 
BE2$from |eB(E2)=0.0306 {I24}, weighted av. of 0.028 {I4} (1969Ri09) and 0.032 {I3} (1967Ki02). Others: 0.030 {i5} (1962Ri09) at E({+20}Ne)=14.36 MeV, 0.036 {I5} (1962Ri09) at E({+20}Ne)=15.38 MeV, 0.046 {I5} (1987Ar17) 
1971Po02 studied isomer shift of 127|g Mossbauer spectrum 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
T from 1974Er04, DSA method. Others: 1973Be72, 1970Va33 (upper limit) 
BE2$other: 0.127 {i12} (1987Ar17) 


level_energy_unit: KEV
level_comment:
E$From the author's spectrum, a comparison with the adjacent peaks at 1440 and 1555 suggest that the energy should be 1490 in agreement with the +13 keV deviation. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$measured by 2015Ki14 using fast-timing |g|g-coin technique, with gates on 184, 127, and 234 |g rays. Note that more precise value of 0.655 ns {I4} is recommended in the {+101}Ru Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
T$from {+101}Ru Adopted Levels in the ENSDF database. In 2015Ki14, time spectra for this state were obtained with gates on 222 and 306 |g rays, and by using the literature half-life of this level, prompt response function and walk for the constant fraction discriminator (CFD) were analyzed at low |g-ray energies. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0151 {I10} (at 6|'), 0.0177 {I13} (at 18|'), 0.0062 {I5} (at 31|'), 0.0048 {I5} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.065 {I6} (at 6|'), 0.470 {I26} (at 18|'), 0.150 {I13} (at 31|'), 0.150 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=3.10 {I16} (at 6|'), 0.295 {I15} (at 18|'), 0.547 {I28} (at 31|'), 0.215 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.034 {I2} (at 6|'), 0.0330 {I26} (at 18|'), 0.0530 {I33} (at 31|'), 0.0330 {I19} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|s(mb/sr)=0.0370 {I21} (at 6|'), 0.0610 {I32} (at 18|'), 0.0630 {I33} (at 31|'), 0.0335 {I19} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0217 {I14} (at 6|'), 0.0500 {I27} (at 18|'), 0.0160 {I11} (at 31|'), 0.0177 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.0670 {I35} (at 6|'), 0.0520 {I33} (at 18|'), 0.103 {I6} (at 31|'), 0.114 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0060 {I11} (at 6|'), 0.0100 {I11} (at 18|'), 0.0270 {I17} (at 31|'), 0.0167 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.034 {I2} (at 6|'), 0.0260 {I17} (at 18|'), 0.0140 {I12} (at 31|'), 0.0070 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.0100 {I11} (at 6|'), 0.0080 {I11} (at 18|'), 0.0230 {I15} (at 31|'), 0.0220 {I15} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0070 {I11} (at 6|'), 0.0060 {I11} (at 18|'), 0.0080 {I11} (at 31|'), 0.004 {I1} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0060 {I11} (at 6|'), 0.0070 {I11} (at 18|'), 0.0080 {I11} (at 31|'), 0.0080 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.086 {I5} (at 6|'), 0.219 {I11} (at 18|'), 0.0460 {I25} (at 31|'), 0.0580 {I31} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0372 {I21} (at 6|'), 0.165 {I9} (at 18|'), 0.0337 {I18} (at 31|'), 0.0426 {I23} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0266 {I16} (at 6|'), 0.0040 {I4} (at 18|'), 0.0053 {I4} (at 31|'), 0.00170 {I31} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.157 {I8} (at 6|'), 0.0205 {I12} (at 18|'), 0.0328 {I18} (at 31|'), 0.0093 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.00350 {I35} (at 6|'), 0.0047 {I4} (at 18|'), 0.0124 {I7} (at 31|'), 0.0079 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0121 {I8} (at 6|'), 0.0364 {I20} (at 18|'), 0.0113 {I7} (at 31|'), 0.0106 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0149 {I9} (at 6|'), 0.0118 {I8} (at 18|'), 0.0238 {I13} (at 31|'), 0.0252 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0065 {I5} (at 6|'), 0.0152 {I9} (at 18|'), 0.00300 {I25} (at 31|'), 0.0057 {I4} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0080 {I11} (at 6|'), 0.0054 {I5} (at 18|'), 0.0116 {I7} (at 31|'), 0.0126 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0210 {I15} (at 6|'), 0.0330 {I19} (at 18|'), 0.0430 {I24} (at 31|'), 0.0470 {I26} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0540 {I34} (at 6|'), 0.231 {I12} (at 18|'), 0.0540 {I29} (at 31|'), 0.0670 {I35} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0270 {I17} (at 6|'), 0.063 {I4} (at 18|'), 0.0178 {I10} (at 31|'), 0.0223 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0550 {I34} (at 6|'), 0.103 {I6} (at 18|'), 0.0242 {I14} (at 31|'), 0.0317 {I18} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0051 {I6} (at 6|'), 0.0111 {I8} (at 18|'), 0.00340 {I35} (at 31|'), 0.0042 {I5} (at 40|') 


level_energy_unit: KEV
level_comment:
E$unresolved doublet (2017Fr08) 
J$3/2+,5/2+&9/2-,11/2- 
$|s(mb/sr)=0.0270 {I17} (at 6|'), 0.083 {I5} (at 18|'), 0.0454 {I25} (at 31|'), 0.0510 {I28} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.235 {I12} (at 6|'), 0.0201 {I14} (at 18|'), 0.0395 {I21} (at 31|'), 0.0102 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.178 {I10} (at 6|'), 0.0236 {I14} (at 18|'), 0.0338 {I19} (at 31|'), 0.0074 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0240 {I16} (at 6|'), 0.076 {I4} (at 18|'), 0.0213 {I12} (at 31|'), 0.0214 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0144 {I12} (at 6|'), 0.035 {I2} (at 18|'), 0.0113 {I8} (at 31|'), 0.0109 {I10} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.012 {I1} (at 6|'), 0.0176 {I12} (at 18|'), 0.0051 {I4} (at 31|'), 0.005 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0158 {I12} (at 6|'), 0.0067 {I6} (at 18|'), 0.0094 {I7} (at 31|'), 0.0039 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0104 {I9} (at 6|'), 0.0092 {I8} (at 18|'), 0.0041 {I5} (at 31|'), 0.0052 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0070 {I11} (at 6|'), 0.0070 {I11} (at 18|'), 0.0060 {I11} (at 31|'), 0.004 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0290 {I18} (at 6|'), 0.0580 {I31} (at 18|'), 0.0219 {I13} (at 31|'), 0.0246 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0210 {I15} (at 6|'), 0.0240 {I16} (at 18|'), 0.0070 {I11} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0550 {I34} (at 6|'), 0.0061 {I4} (at 18|'), 0.0129 {I8} (at 31|'), 0.0076 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0157 {I11} (at 6|'), 0.0218 {I12} (at 18|'), 0.0074 {I6} (at 31|'), 0.0058 {I5} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0290 {I18} (at 6|'), 0.0276 {I15} (at 18|'), 0.00480 {I31} (at 31|'), 0.0057 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0051 {I5} (at 6|'), 0.0150 {I9} (at 18|'), 0.0039 {I4} (at 31|'), 0.0040 {I5} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.262 {I14} (at 6|'), 0.092 {I5} (at 18|'), 0.0668 {I34} (at 31|'), 0.0301 {I17} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0080 {I8} (at 6|'), 0.0220 {I13} (at 18|'), 0.0053 {I4} (at 31|'), 0.0073 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0185 {I12} (at 6|'), 0.0193 {I11} (at 18|'), 0.0053 {I6} (at 31|'), 0.0086 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0327 {I19} (at 6|'), 0.0307 {I17} (at 18|'), 0.0059 {I4} (at 31|'), 0.0053 {I4} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0094 {I9} (at 6|'), 0.0091 {I8} (at 18|'), 0.0203 {I12} (at 31|'), 0.0165 {I10} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0047 {I7} (at 6|'), 0.0039 {I4} (at 18|'), 0.0106 {I7} (at 31|'), 0.0071 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0153 {I12} (at 6|'), 0.0135 {I9} (at 18|'), 0.0071 {I6} (at 31|'), 0.0051 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0300 {I18} (at 6|'), 0.0323 {I18} (at 18|'), 0.073 {I4} (at 31|'), 0.06 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0300 {I18} (at 6|'), 0.0500 {I27} (at 18|'), 0.0070 {I8} (at 31|'), 0.0100 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.045 {I3} (at 6|'), 0.0460 {I25} (at 18|'), 0.0080 {I11} (at 31|'), 0.0110 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.035 {I2} (at 6|'), 0.0330 {I26} (at 18|'), 0.0121 {I10} (at 31|'), 0.0089 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0085 {I7} (at 6|'), 0.0136 {I9} (at 18|'), 0.0047 {I6} (at 31|'), 0.0039 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0550 {I34} (at 6|'), 0.075 {I4} (at 18|'), 0.0159 {I11} (at 31|'), 0.0225 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.035 {I2} (at 6|'), 0.0550 {I29} (at 18|'), 0.0191 {I13} (at 31|'), 0.0210 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.185 {I10} (at 6|'), 0.226 {I12} (at 18|'), 0.0430 {I24} (at 31|'), 0.0630 {I33} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0120 {I12} (at 6|'), 0.0095 {I9} (at 18|'), 0.0220 {I15} (at 31|'), 0.0230 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0500 {I32} (at 6|'), 0.0630 {I33} (at 18|'), 0.0120 {I12} (at 31|'), 0.0150 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0210 {I15} (at 6|'), 0.0310 {I19} (at 18|'), 0.0130 {I12} (at 31|'), 0.0080 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0053 {I9} (at 6|'), 0.0068 {I8} (at 18|'), 0.0106 {I11} (at 31|'), 0.0100 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0380 {I28} (at 6|'), 0.0460 {I25} (at 18|'), 0.0060 {I11} (at 31|'), 0.0060 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.141 {I8} (at 6|'), 0.159 {I8} (at 18|'), 0.0343 {I19} (at 31|'), 0.0450 {I25} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.063 {I4} (at 6|'), 0.080 {I4} (at 18|'), 0.0220 {I15} (at 31|'), 0.0250 {I24} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.094 {I5} (at 6|'), 0.075 {I4} (at 18|'), 0.0266 {I16} (at 31|'), 0.0230 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0120 {I12} (at 6|'), 0.0125 {I10} (at 18|'), 0.0059 {I6} (at 31|'), 0.0053 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0330 {I26} (at 6|'), 0.0262 {I16} (at 18|'), 0.0129 {I10} (at 31|'), 0.0120 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0077 {I10} (at 6|'), 0.0107 {I8} (at 18|'), 0.0015 {I7} (at 31|'), 0.0030 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.034 {I2} (at 6|'), 0.0344 {I20} (at 18|'), 0.0180 {I14} (at 31|'), 0.0113 {I10} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0530 {I33} (at 6|'), 0.0620 {I33} (at 18|'), 0.0200 {I22} (at 31|'), 0.0190 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0123 {I9} (at 6|'), 0.0181 {I11} (at 18|'), 0.0040 {I7} (at 31|'), 0.0060 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.109 {I6} (at 6|'), 0.129 {I7} (at 18|'), 0.0302 {I18} (at 31|'), 0.0390 {I22} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0160 {I13} (at 6|'), 0.020 {I7} (at 18|'), 0.0047 {I6} (at 31|'), 0.005 {I2} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0140 {I12} (at 6|'), 0.0139 {I10} (at 18|'), 0.0042 {I6} (at 31|'), 0.004 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0047 {I7} (at 6|'), 0.0077 {I7} (at 18|'), 0.0029 {I4} (at 31|'), 0.002 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.063 {I4} (at 6|'), 0.084 {I4} (at 18|'), 0.0207 {I13} (at 31|'), 0.0250 {I16} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0110 {I11} (at 6|'), 0.0096 {I8} (at 18|'), 0.00240 {I32} (at 31|'), 0.0033 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0170 {I13} (at 6|'), 0.0279 {I17} (at 18|'), 0.0100 {I11} (at 31|'), 0.0130 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0170 {I13} (at 6|'), 0.0195 {I13} (at 18|'), 0.0070 {I11} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0060 {I11} (at 6|'), 0.0083 {I8} (at 18|'), 0.0060 {I11} (at 31|'), 0.005 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0100 {I11} (at 6|'), 0.0134 {I11} (at 18|'), 0.0090 {I21} (at 31|'), 0.0100 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.510 {I27} (at 6|'), 0.465 {I24} (at 18|'), 0.357 {I18} (at 31|'), 0.220 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.037 {I4} (at 6|'), 0.0180 {I14} (at 18|'), 0.0190 {I14} (at 31|'), 0.0160 {I22} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0290 {I18} (at 6|'), 0.0263 {I16} (at 18|'), 0.0183 {I11} (at 31|'), 0.0161 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|s(mb/sr)=0.052 {I9} (at 6|'), 0.0210 {I23} (at 18|'), 0.0150 {I13} (at 31|'), 0.0130 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.090 {I21} (at 6|'), 0.077 {I4} (at 18|'), 0.0600 {I32} (at 31|'), 0.0360 {I27} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0260 {I17} (at 6|'), 0.0214 {I13} (at 18|'), 0.0095 {I9} (at 31|'), 0.0068 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.150 {I8} (at 6|'), 0.094 {I5} (at 18|'), 0.0500 {I27} (at 31|'), 0.0430 {I24} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.028 {I6} (at 6|'), 0.0280 {I33} (at 18|'), 0.0230 {I23} (at 31|'), 0.0130 {I31} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.103 {I8} (at 6|'), 0.061 {I4} (at 18|'), 0.0320 {I26} (at 31|'), 0.0220 {I23} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0500 {I32} (at 6|'), 0.0442 {I24} (at 18|'), 0.0305 {I17} (at 31|'), 0.0223 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0420 {I29} (at 6|'), 0.0235 {I13} (at 18|'), 0.0158 {I10} (at 31|'), 0.0107 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0530 {I33} (at 6|'), 0.0354 {I20} (at 18|'), 0.0198 {I12} (at 31|'), 0.0150 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0230 {I15} (at 6|'), 0.0164 {I11} (at 18|'), 0.0084 {I6} (at 31|'), 0.0076 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.114 {I6} (at 6|'), 0.078 {I4} (at 18|'), 0.0456 {I24} (at 31|'), 0.0311 {I18} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.078 {I4} (at 6|'), 0.0630 {I33} (at 18|'), 0.0391 {I21} (at 31|'), 0.0287 {I17} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.034 {I2} (at 6|'), 0.0277 {I16} (at 18|'), 0.017 {I1} (at 31|'), 0.0116 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0600 {I32} (at 6|'), 0.0458 {I25} (at 18|'), 0.0253 {I15} (at 31|'), 0.0184 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.493 {I25} (at 6|'), 0.341 {I17} (at 18|'), 0.181 {I9} (at 31|'), 0.109 {I6} (at 40|') 
E$there are potentially small contributions from a weak, but unresolved L=2 transition (2017Fr08). 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0120 {I12} (at 6|'), 0.0090 {I11} (at 18|'), 0.005 {I1} (at 31|') 
E$not seen in (p,d) in 2017Fr08 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0430 {I24} (at 6|'), 0.035 {I2} (at 18|'), 0.0210 {I15} (at 31|'), 0.0170 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0450 {I25} (at 6|'), 0.0300 {I18} (at 18|'), 0.0150 {I13} (at 31|'), 0.0100 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0170 {I13} (at 6|'), 0.0110 {I12} (at 18|'), 0.0060 {I11} (at 31|'), 0.005 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0480 {I31} (at 6|'), 0.0250 {I16} (at 18|'), 0.0160 {I13} (at 31|'), 0.0110 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.060 {I4} (at 6|'), 0.0380 {I22} (at 18|'), 0.0260 {I17} (at 31|'), 0.0150 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0530 {I33} (at 6|'), 0.0450 {I25} (at 18|'), 0.0330 {I19} (at 31|'), 0.0250 {I24} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0200 {I22} (at 6|'), 0.0160 {I13} (at 18|'), 0.0070 {I11} (at 31|'), 0.0060 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0520 {I33} (at 6|'), 0.0370 {I21} (at 18|'), 0.0210 {I15} (at 31|'), 0.0140 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.102 {I6} (at 6|'), 0.062 {I4} (at 18|'), 0.0320 {I26} (at 31|'), 0.0230 {I23} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.093 {I6} (at 6|'), 0.0530 {I33} (at 18|'), 0.0250 {I16} (at 31|'), 0.0190 {I22} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.685 {I35} (at 6|'), 0.448 {I23} (at 18|'), 0.241 {I12} (at 31|'), 0.166 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.113 {I7} (at 6|'), 0.065 {I4} (at 18|'), 0.0380 {I28} (at 31|'), 0.0250 {I24} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.052 {I4} (at 6|'), 0.0500 {I32} (at 18|'), 0.0340 {I26} (at 31|'), 0.0240 {I23} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0210 {I32} (at 6|'), 0.0220 {I23} (at 18|'), 0.0170 {I22} (at 31|'), 0.0110 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.039 {I5} (at 6|'), 0.0240 {I32} (at 18|'), 0.0120 {I21} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0350 {I35} (at 6|'), 0.0280 {I25} (at 18|'), 0.0170 {I13} (at 31|'), 0.0110 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.055 {I7} (at 6|'), 0.0270 {I17} (at 18|'), 0.0240 {I16} (at 31|'), 0.0120 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.034 {I4} (at 6|'), 0.0220 {I23} (at 18|'), 0.0130 {I21} (at 31|'), 0.013 {I5} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0270 {I24} (at 6|'), 0.0210 {I15} (at 18|'), 0.0155 {I12} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0180 {I22} (at 6|'), 0.0180 {I14} (at 18|'), 0.0140 {I12} (at 31|'), 0.0079 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.044 {I4} (at 6|'), 0.0310 {I25} (at 18|'), 0.0200 {I14} (at 31|'), 0.0130 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.047 {I4} (at 6|'), 0.0330 {I26} (at 18|'), 0.0210 {I15} (at 31|'), 0.0170 {I22} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.048 {I4} (at 6|'), 0.0390 {I28} (at 18|'), 0.0270 {I17} (at 31|'), 0.0190 {I22} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.055 {I4} (at 6|'), 0.046 {I4} (at 18|'), 0.0230 {I23} (at 31|'), 0.0160 {I22} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0310 {I34} (at 6|'), 0.0210 {I23} (at 18|'), 0.0120 {I21} (at 31|'), 0.0130 {I21} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0200 {I22} (at 6|'), 0.0230 {I23} (at 18|'), 0.0120 {I12} (at 31|'), 0.0110 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=1.12 {I6} (at 8|'), 3.93 {I20} (at 18|'), 2.79 {I14} (at 27|'), 1.16 {I6} (at 33|'), 1.11 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0350 {I27} (at 8|'), 0.086 {I5} (at 18|'), 0.0534 {I28} (at 27|'), 0.0239 {I13} (at 33|'), 0.0227 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.187 {I10} (at 8|'), 0.263 {I13} (at 18|'), 0.318 {I16} (at 27|'), 0.488 {I25} (at 33|'), 0.396 {I20} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=7.7 {I4} (at 8|'), 0.73 {I4} (at 18|'), 2.52 {I13} (at 27|'), 2.38 {I12} (at 33|'), 1.04 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.070 {I5} (at 8|'), 0.209 {I11} (at 18|'), 0.139 {I7} (at 27|'), 0.0631 {I33} (at 33|'), 0.0653 {I34} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$|s(mb/sr)=0.073 {I6} (at 8|'), 0.134 {I7} (at 18|'), 0.205 {I11} (at 27|'), 0.277 {I14} (at 33|'), 0.317 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.415 {I22} (at 8|'), 1.17 {I6} (at 18|'), 0.683 {I34} (at 27|'), 0.328 {I17} (at 33|'), 0.371 {I19} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|s(mb/sr)=0.231 {I12} (at 8|'), 0.336 {I17} (at 18|'), 0.425 {I21} (at 27|'), 0.328 {I17} (at 33|'), 0.186 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.342 {I18} (at 8|'), 0.0478 {I25} (at 18|'), 0.136 {I7} (at 27|'), 0.114 {I6} (at 33|'), 0.0533 {I28} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.133 {I7} (at 8|'), 0.316 {I16} (at 18|'), 0.178 {I9} (at 27|'), 0.070 {I4} (at 33|'), 0.091 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.0190 {I14} (at 8|'), 0.020 {I8} (at 18|'), 0.0169 {I10} (at 27|'), 0.0232 {I13} (at 33|'), 0.0309 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.145 {I9} (at 8|'), 0.532 {I27} (at 18|'), 0.477 {I24} (at 27|'), 0.240 {I12} (at 33|'), 0.178 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.211 {I11} (at 8|'), 0.197 {I10} (at 18|'), 0.103 {I5} (at 27|'), 0.098 {I5} (at 33|'), 0.0545 {I28} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0154 {I9} (at 8|'), 0.0209 {I13} (at 18|'), 0.0209 {I13} (at 27|'), 0.0184 {I11} (at 33|'), 0.0158 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.393 {I21} (at 8|'), 1.11 {I6} (at 18|'), 0.74 {I4} (at 27|'), 0.347 {I18} (at 33|'), 0.321 {I16} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0360 {I27} (at 8|'), 0.0081 {I6} (at 18|'), 0.0154 {I9} (at 27|'), 0.0179 {I10} (at 33|'), 0.0162 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.178 {I10} (at 8|'), 0.0255 {I13} (at 18|'), 0.0546 {I28} (at 27|'), 0.0560 {I29} (at 33|'), 0.0281 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=1.05 {I5} (at 8|'), 0.111 {I6} (at 18|'), 0.351 {I18} (at 27|'), 0.365 {I18} (at 33|'), 0.168 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0160 {I13} (at 8|'), 0.0053 {I5} (at 18|'), 0.0049 {I6} (at 27|'), 0.0006 {I3} (at 33|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.005 {I1} (at 8|'), 0.0056 {I7} (at 18|'), 0.0062 {I5} (at 27|'), 0.0059 {I4} (at 33|'), 0.0076 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.0039 {I7} (at 8|'), 0.0069 {I5} (at 18|'), 0.0090 {I6} (at 27|'), 0.0068 {I5} (at 33|'), 0.00260 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0134 {I11} (at 8|'), 0.0307 {I16} (at 18|'), 0.0176 {I9} (at 27|'), 0.0095 {I6} (at 33|'), 0.0098 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0047 {I8} (at 8|'), 0.00200 {I22} (at 18|'), 0.00230 {I23} (at 27|'), 0.00220 {I23} (at 33|'), 0.00130 {I21} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0024 {I8} (at 8|'), 0.00240 {I23} (at 18|'), 0.00490 {I32} (at 33|'), 0.0045 {I3} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.005 {I1} (at 8|'), 0.00420 {I29} (at 18|'), 0.0057 {I4} (at 27|'), 0.0085 {I5} (at 33|'), 0.0096 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0280 {I25} (at 8|'), 0.0103 {I7} (at 18|'), 0.0069 {I5} (at 27|'), 0.0088 {I5} (at 33|'), 0.0098 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0080 {I8} (at 8|'), 0.0127 {I8} (at 18|'), 0.0153 {I8} (at 27|'), 0.0169 {I9} (at 33|'), 0.0134 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0140 {I11} (at 8|'), 0.0230 {I12} (at 18|'), 0.0109 {I6} (at 27|'), 0.0067 {I4} (at 33|'), 0.0066 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0450 {I25} (at 8|'), 0.0264 {I15} (at 18|'), 0.0260 {I33} (at 27|'), 0.0220 {I12} (at 33|'), 0.0124 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.391 {I21} (at 8|'), 0.93 {I5} (at 18|'), 0.556 {I28} (at 27|'), 0.360 {I27} (at 33|'), 0.313 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0082 {I9} (at 8|'), 0.0082 {I7} (at 18|'), 0.0103 {I7} (at 27|'), 0.0131 {I8} (at 33|'), 0.0106 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0170 {I13} (at 8|'), 0.0152 {I9} (at 18|'), 0.0191 {I11} (at 27|'), 0.0204 {I11} (at 33|'), 0.0143 {I8} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.086 {I5} (at 8|'), 0.116 {I6} (at 18|'), 0.160 {I8} (at 27|'), 0.200 {I14} (at 33|'), 0.202 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0430 {I29} (at 8|'), 0.0102 {I7} (at 18|'), 0.015 {I1} (at 27|'), 0.0140 {I12} (at 33|'), 0.0060 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0180 {I14} (at 8|'), 0.0017 {I4} (at 18|'), 0.0059 {I5} (at 27|'), 0.0071 {I5} (at 33|'), 0.00230 {I32} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0530 {I33} (at 8|'), 0.131 {I7} (at 18|'), 0.081 {I4} (at 27|'), 0.0470 {I25} (at 33|'), 0.0388 {I20} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.058 {I4} (at 8|'), 0.085 {I4} (at 18|'), 0.089 {I5} (at 27|'), 0.071 {I4} (at 33|'), 0.0408 {I21} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0430 {I29} (at 8|'), 0.130 {I7} (at 18|'), 0.107 {I6} (at 27|'), 0.071 {I4} (at 33|'), 0.0495 {I26} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0200 {I14} (at 8|'), 0.0568 {I30} (at 18|'), 0.0462 {I25} (at 27|'), 0.0301 {I16} (at 33|'), 0.0282 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.389 {I20} (at 8|'), 0.0432 {I23} (at 18|'), 0.117 {I6} (at 27|'), 0.145 {I7} (at 33|'), 0.077 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.248 {I13} (at 8|'), 0.441 {I22} (at 18|'), 0.290 {I15} (at 27|'), 0.197 {I10} (at 33|'), 0.138 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0410 {I29} (at 8|'), 0.112 {I6} (at 18|'), 0.080 {I4} (at 27|'), 0.0525 {I28} (at 33|'), 0.0396 {I21} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.207 {I11} (at 8|'), 0.0568 {I30} (at 18|'), 0.128 {I7} (at 27|'), 0.159 {I8} (at 33|'), 0.088 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.423 {I22} (at 8|'), 0.0270 {I33} (at 18|'), 0.129 {I7} (at 27|'), 0.163 {I8} (at 33|'), 0.087 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.049 {I4} (at 8|'), 0.045 {I3} (at 27|'), 0.0420 {I23} (at 33|'), 0.0198 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.081 {I5} (at 8|'), 0.0430 {I24} (at 27|'), 0.0400 {I22} (at 33|'), 0.0290 {I18} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0190 {I22} (at 8|'), 0.0210 {I15} (at 18|'), 0.0270 {I17} (at 33|'), 0.017 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0230 {I23} (at 8|'), 0.0360 {I21} (at 18|'), 0.0240 {I16} (at 33|'), 0.0134 {I8} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.090 {I5} (at 8|'), 0.0385 {I20} (at 18|'), 0.0162 {I10} (at 27|'), 0.0377 {I20} (at 33|'), 0.0202 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.091 {I5} (at 8|'), 0.188 {I10} (at 18|'), 0.128 {I10} (at 27|'), 0.091 {I5} (at 33|'), 0.072 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.136 {I8} (at 8|'), 0.287 {I14} (at 18|'), 0.167 {I9} (at 27|'), 0.108 {I6} (at 33|'), 0.087 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0520 {I33} (at 8|'), 0.075 {I4} (at 18|'), 0.0508 {I26} (at 33|'), 0.0295 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0160 {I22} (at 8|'), 0.0196 {I12} (at 18|'), 0.0111 {I8} (at 33|'), 0.0058 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.083 {I5} (at 8|'), 0.0446 {I23} (at 18|'), 0.0528 {I27} (at 33|'), 0.0429 {I22} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0250 {I24} (at 8|'), 0.0022 {I7} (at 18|'), 0.0042 {I6} (at 33|'), 0.0033 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.081 {I5} (at 8|'), 0.181 {I9} (at 18|'), 0.0550 {I34} (at 27|'), 0.077 {I4} (at 33|'), 0.0601 {I31} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.113 {I7} (at 8|'), 0.291 {I15} (at 18|'), 0.095 {I5} (at 27|'), 0.083 {I5} (at 33|'), 0.085 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.097 {I6} (at 8|'), 0.166 {I8} (at 18|'), 0.135 {I7} (at 27|'), 0.112 {I6} (at 33|'), 0.0602 {I31} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0320 {I26} (at 8|'), 0.0531 {I28} (at 18|'), 0.0190 {I22} (at 27|'), 0.0190 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0540 {I34} (at 8|'), 0.125 {I6} (at 18|'), 0.087 {I5} (at 27|'), 0.064 {I6} (at 33|'), 0.0459 {I24} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.086 {I6} (at 8|'), 0.080 {I4} (at 18|'), 0.0650 {I34} (at 27|'), 0.0180 {I31} (at 33|'), 0.0343 {I18} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.089 {I6} (at 8|'), 0.095 {I5} (at 18|'), 0.0660 {I35} (at 27|'), 0.0440 {I24} (at 33|'), 0.0421 {I22} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.072 {I5} (at 8|'), 0.0379 {I21} (at 18|'), 0.0250 {I16} (at 27|'), 0.0220 {I15} (at 33|'), 0.0265 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.080 {I7} (at 8|'), 0.160 {I9} (at 18|'), 0.075 {I4} (at 27|'), 0.081 {I5} (at 33|'), 0.0578 {I30} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.069 {I6} (at 8|'), 0.107 {I6} (at 18|'), 0.079 {I5} (at 27|'), 0.0650 {I34} (at 33|'), 0.0332 {I19} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.174 {I11} (at 8|'), 0.198 {I10} (at 18|'), 0.134 {I7} (at 27|'), 0.118 {I6} (at 33|'), 0.045 {I3} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.031 {I4} (at 8|'), 0.072 {I4} (at 18|'), 0.0610 {I32} (at 27|'), 0.0552 {I29} (at 33|'), 0.032 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.140 {I21} (at 8|'), 0.0426 {I23} (at 18|'), 0.035 {I2} (at 27|'), 0.0441 {I24} (at 33|'), 0.0280 {I33} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.046 {I7} (at 8|'), 0.0140 {I21} (at 18|'), 0.0220 {I15} (at 27|'), 0.029 {I5} (at 33|'), 0.021 {I4} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.085 {I6} (at 8|'), 0.0460 {I31} (at 18|'), 0.0400 {I22} (at 27|'), 0.0510 {I28} (at 33|'), 0.0330 {I26} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0200 {I32} (at 8|'), 0.0170 {I22} (at 18|'), 0.0291 {I17} (at 27|'), 0.0201 {I12} (at 33|'), 0.0140 {I21} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.046 {I5} (at 8|'), 0.0230 {I23} (at 18|'), 0.0208 {I14} (at 27|'), 0.0244 {I14} (at 33|'), 0.0180 {I22} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.127 {I8} (at 8|'), 0.0240 {I16} (at 18|'), 0.0330 {I26} (at 27|'), 0.0480 {I26} (at 33|'), 0.0150 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.026 {I4} (at 8|'), 0.0520 {I28} (at 18|'), 0.0260 {I17} (at 33|'), 0.0100 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.033 {I4} (at 8|'), 0.0540 {I29} (at 18|'), 0.0550 {I29} (at 33|'), 0.038 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.121 {I8} (at 8|'), 0.0270 {I16} (at 18|'), 0.0260 {I24} (at 27|'), 0.0290 {I18} (at 33|'), 0.0344 {I19} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.043 {I4} (at 8|'), 0.0650 {I34} (at 18|'), 0.0400 {I22} (at 27|'), 0.0330 {I26} (at 33|'), 0.0213 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$From Budapest data for (n,|g) 
MOME2$From coulomb excitation, other value: -0.33 {I4} (1998Hi01) Others: 1980La01, 1979Bo28 
MOMM1 From IPAC (1989Ra17), recalculated for T{-1/2} 
J E2 |g to 0+ (|a,2n|g) 
T$From B(E2) evaluation (2001Ra27) (207-d {+102}Rh |e decay) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
$ q{-K}{+2}(E0/E2)=0.175 {I15}, X(E0/E2)=0.0142 {I12}, |r{+2}(E0)=0.014 {I3} (2005Ki02, evaluation) 
J E0 |g to 0+ ({+102}Rh |e decay (207 d)) 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J E2+M1 |g to 4+; |g|g(|q) in {+102}Rh |e decay (2.9 y) consistent with J=3 or 5; log| {Ift} rules out J=3 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J |g|g(|q) results from {+102}Rh |e decay (207 d) consistent with J=2, not with J=1 or J=3; strong population of this level from the 3+ 42-eV resonance in {+101}Ru(n,|g) 
J parity from E1 to |p=+ states 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J (1106)(475)(|q) is consistent with J(d,Q)2(Q)0 for J(1581 level)=2 or 3. Not consistent with J=1 (1970Si13) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J (1562)(475)(|q) is consistent with J(d,Q)2(Q)0 for J(8037 level)=2 and |d(1562|g)=-1.9 {i4}. Not consistent with J=1 or 3 for any |d (1970Si13) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J (1152)(1103)(|q) is consistent with J(d,Q)2(Q)0 for J(2261 level)=2 and |d(1158|g)=-0.25 {i5}. Not consistent with J=1 or 3. For additional |g|g(|q) data, see 1970Si13 
J the parity is obtained from |a(K)exp measurements of 1993Fa11 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J (628)(475)(|q) is consistent with J(D+Q)2(Q)0 for J(1103 level)=2 and |d(628|g)=60 {i20}. Not consistent with J=0,1,3,4 for any |d (1970Si13) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J (1049)(475)(|q) is consistent with J(D+Q)2(Q)0 for J(1521 level)=3 and |d(1047|g)=-7.0 {i6}. Not consistent with J=1 or 2 for any |d. (419)(1103)(|q) is consistent with J(D+Q)2(Q)0 J(1521 level)=3 and |d(419|g)=-7.2 {i1}. Not consistent with J=1 or 2 for any |d (1970Si13) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
J J|p=1 suggested by 1982Co15 not consistent with angular-correlation data of {+102}Rh (207 d) decay 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J|p=6+ is suggested by 1982Co15 from population ratio measurements. In contradiction with J|p=(5-) from (|a,2n|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$Weighted average of 0.640 {I6} (1980La01), 0.66 {i6} (1968Mc08), 0.617 {i5} (1979Bo28) 
MOME2$Weighted average of -0.68 {I8} (1979Bo28), -0.57 {I7} (1980La01) and -0.64 {I5} (1998Hi01). Values obtained from the angular correlation measurement for the 1103.2-keV |g-ray, the sign of the interference term in the Coulomb excitation was determined to be negative (1976Fa02) 
T From B(E2) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T calculated using |g(1103.5)-branching=0.359 {i13} (see adopted |g's) 
BE2 From 0.0165 {i19} (1968Mc08) and 0.0130 {i22} (1979Bo28). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$B(E2)(2+ to 4+)=0.33 {i5} 
T$From B(E2)(2+ to 4+)=0.33 {i5} which is a weighted average of 0.36 {i7} (1968Mc08) and 0.30 {i6} (1979Bo28) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$ average of two measured values of +0.43 {I2} and +0.43 {I1} with statistical uncertainty only. The statistical uncertainty on the average value is 0.01, whereas the uncertainty including that in the absolute value is 0.03, arising mainly from the calibration value 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
$< 3{+-} ||E2|| 0{++} > =0.381 {I8} (exp1), fit is performed assuming 0+ to 3- excitation only. Value is 0.28 {I+6-8} for exp1 + exp3 and fit for the 2+/3- doublet 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: D
level_comment:
T$From the review of (2004Wo02). Others: 39.260 d {I20} (1981Va11), 39.214 d {I13} (1981Mi10); 39.254 d {I8} (1980Ho17), 39.296 d {I9} (1976WaZH). 39.35 d {I5} (1971De11), 39.5 d {I5} (1965Fl02), 39.4 d {I4} (1959Ca12), 1957Wr37, 1952Ko27, 1951Su90, 1948Mo33 
J$L=2 in (d,p). |m agrees with values for other J=3/2 states in this region. 
MOMM1$others: 0.225 {I60} (1981Ha11), 0.18 {I2} (1981Mu18) all using the low temperature nuclear orientation technique. 0.2071 {I31} (1990Hi02) NMR on oriented {+103}Ru in Fe. Other references: 1979KrZV, 1976Ba39. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E implied from several |g-ray doublets of |DE=2.8 keV including a g.s. transition in {+103}Tc |b{+-} decay, (n,|g) and (|a,n|g) 
J$L=2 in (p,d),(d,t). 210.8|g from 213 is |DJ=1 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$L=4 (d,p),(d,t). log| {Ift}=6.2 from 5/2+ excludes 9/2+. 
T from prompt component (210.7|g)(t) (1975Kl04) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
T from |g(t): unweighted av of 1.56 ms {I5} (1970Uy01), 1.67 ms {I10} (1975Kl04), 1.85 ms {I6} (1975Ba60). Others: 1964Br27, 1967Iv03, 1968Io01 
J$from L=5 (d,p),(p,d),(d,t), B(M2)(W.u.)(24.6|g,M2) syst and E(11/2-) regional trend. If J|p were 9/2-,the transition to 213 level could be an E1 and B(E1)(W.u.)|<1.5|*10{+-9}. This would be too slow (1981En06) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J L=2 in (d,p),(p,d),(d,t). 5/2+ suggested by 1982Be19 from (d,p)/(p,d) spectroscopic strength and |g(|q) in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J probable member of complex unresolved multiplet observed in (d,p),(p,d) and (d,t). No unambiguous L assignment. |g to 5/2+, |g(|q) in (|a,n|g) suggest 1/2. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J probable member of complex unresolved multiplet observed in (d,p),(p,d) and (d,t). No unambiguous L assignment. Preferential |g decay of the 554-keV level to g.s. and the presence of a L=0 component in the unresolved multiplet in (p,d) suggest (1/2+) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J probable member of complex unresolved multiplet observed in (d,p),(p,d) and (d,t). No unambiguous L assignment. Excit of 344|g suggest 7/2,9/2 in (|a,n|g). 344|g(|q) favors 9/2. 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J probable member of complex unresolved multiplet observed in (d,p),(p,d) and (d,t). No unambiguous L assignment. Population and depopulation of 562-keV level suggest 1/2+,3/2,5/2+; log| {Ift}=5.32 in {+103}Tc |b{+-} decay excludes 1/2+,3/2- 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J L=(2) in (d,p),(p,d). 5/2+ suggested from (d,p)/(p,d) spectroscopic strength (1982Be19). Excit, n|g(|q) for 324.7|g in (|a,n|g) suggest 3/2, although 5/2 cannot be ruled out. In disagreement with J|>9/2 from {+102}Ru(n,|g) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
E 735.2 and 736.89 keV levels separately observed in (|a,n|g) 
J$D+Q |g to (7/2)+, |g(|q) suggest J=5/2 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J L=0 (d,p),(p,d),(d,t). J|p assignment consistent with strong level population in (n,|g) and preferential |g decay to 1/2+ states. 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_comment:
J$stretched Q from excit and angular distribution in (|a,n|g). Member of |DJ=2 band based on 7/2+ at 213 keV. 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J suggested from population in (n,|g) and |g decay pattern. Consistent with observation of unresolved multiplet at 773.8 keV in (d,p) with L=0 and L=2 components and a possible multiplet at 777.0 keV in (p,d) with a predominant L=2 component. 1/2+ ruled out from log| {Ift} 


level_energy_unit: KEV
level_spin_parity: (LE 5/2+)
level_comment:
J may be a member of a possible unresolved multiplet observed in (d,p),(p,d),(d,t) with L=2. |g decay pattern suggest J|<5/2 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
Probably member of a possible unresolved multiplet observed in (d,p),(p,d),(d,t) with L=2 as main component 
J from allowed |b-transition with log| {Ift}=5.8 from 5/2+. J|p=3/2+,5/2+,7/2+ possible; 7/2+ ruled out from L=2 


level_energy_unit: KEV
level_spin_parity: (LE 5/2+)
level_comment:
May be member of a possible unresolved multiplet observed in (d,p),(p,d),(d,t) with L=2. |g decay pattern suggest J|<5/2 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_comment:
J$|g to (1/2+). |g excitation function of 383 keV |g in (|a,n|g) suggests 5/2 or 3/2 while its isotropic angular distribution favors 3/2 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
E$might be identical with 1171.3 level seen in (|a,n|g) 
J population and depopulation in (n,|g) permits J=1/2,3/2,5/2. (625.8|g-250.5|g)(|q) and (625.8|g-(250.5|g)-294.4|g)(|q) suggests 3/2 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
From |g(t): T{-1/2}=1.85 ms {I6} (1975Ba60) and 1.56 ms {I5} (1970Uy01) 
%IT=100 
E$From Adopted levels 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
J suggested by 1982Be19 from (d,p)/(p,d) spectroscopic strength ratio. g.s. not observed by 1998Ba89 


level_energy_unit: KEV
level_comment:
E may correspond to (404-406) doublet observed in {+103}Tc |b{+-} decay and (n,|g) 
S C{+2}S'=0.82 if J=5/2 and C{+2}S'=0.92 if J|p=3/2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E unresolved doublet. L=2 and J=(5/2) suggested by 1982Be19 for one component from (d,p)/(p,d) spectroscopic strength ratio with C{+2}S'=0.032. L=(1) and J=(3/2) suggested by 1998Ba89 for other component with C{+2}S'=(0.018) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E may correspond to the 541-keV level observed with L=2 and (2J+1)C{+2}S=0.14 by 1971Fo01. Not observed by 1998Ba89 


level_energy_unit: KEV
level_comment:
Unresolved multiplet of states with excitation energy from 548 to 563 keV with L=2 (J=5/2 and C{+2}S'=0.074) and L=0 (J=1/2 and C{+2}S'=0.046) as major components and L=(1) (J=3/2 with C{+2}S'=0.018) as a small admixture. May partially correspond to the 551-keV state reported with L=0 by 1971Fo01 


level_energy_unit: KEV
level_comment:
J|p=5/2+ suggested by 1982Be19 from (d,t)/(d,p) spectroscopic strength ratio 
S other: 0.22 (1982Be19) 


level_energy_unit: KEV
level_comment:
J|p=(5/2)+ suggested by 1982Be19 from (d,t)/(d,p) spectroscopic strength ratio 
S other: 0.04 (1982Be19) 


level_energy_unit: KEV
level_comment:
J (3/2)+ suggested by 1982Be19 from (d,t)/(d,p) spectroscopic strength ratio 
S other: 0.18 (1982Be19) 


level_energy_unit: KEV
level_comment:
Unresolved multiplet. A mixture of L=0 ((2J+1)C{+2}S=0.10) and L=2 ((2J+1)C{+2}S=0.03) necessary to fit the experimental data. Not observed by 1998Ba89 


level_energy_unit: KEV
level_comment:
C{+2}S'=0.47 for J|p=5/2 and =0.51 for J|p=3/2 
E may be associated with 902.96+905.50+907.58 states excited in (n,|g), so might be an unresolved multiplet 


level_energy_unit: KEV
level_comment:
L C{+2}S=0.35 if J=5/2, C{+2}S=0.44 if J=3/2 
E may correspond to (404-406) doublet observed in {+103}Tc |b{+-} decay and (n,|g) 


level_energy_unit: KEV
level_comment:
E possible unresolved multiplet with predominant L=2 component 
L C{+2}S=0.11 if J=5/2, C{+2}S=0.13 if J=3/2 


level_energy_unit: KEV
level_comment:
E from (p,d). May be associated with 902.96+905.50+907.58 states excited in (n,|g). 
S calculated for J|p=3/2+ 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: D
level_comment:
T$ measured at room temperature (293K to 298K) (2009Go29). Half-life measured at 19K is 39.219 d {I35} (2009Go29); difference of 0.009 d {I30} indicates no change in T{-1/2} with temperature 
J$ from adopted dataset for {+103}Ru in ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
T$measured by 2015Ki14 using fast-timing |g|g-coin technique, with gates on 211, 560 and 669 |g rays. The half-life is considered as tentative since the constant fraction discriminator (CFD) walk correction for the 211 |g ray was based on data for the 7/2+ state in {+101}Ru 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: NS
level_comment:
T$measured by 2016Ki20 using fast-timing |g|g-coin technique, with gates on 294 and 271 |g rays. 
$This level is interpreted by 2016Ki20 as a triaxial state, based on comparison with triaxial rotor plus particle model calculations. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=1.06 {I6} (at 8|'), 4.43 {I22} (at 18|'), 2.36 {I12} (at 27|'), 1.10 {I6} (at 33|'), 0.99 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0060 {I11} (at 8|'), 0.0236 {I13} (at 18|'), 0.0131 {I8} (at 27|'), 0.0092 {I6} (at 33|'), 0.0085 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=7.7 {I4} (at 8|'), 0.98 {I5} (at 18|'), 2.54 {I13} (at 27|'), 2.47 {I12} (at 33|'), 1.09 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.098 {I6} (at 8|'), 0.172 {I9} (at 18|'), 0.262 {I13} (at 27|'), 0.338 {I17} (at 33|'), 0.246 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$|s(mb/sr)=0.087 {I5} (at 8|'), 0.228 {I12} (at 18|'), 0.278 {I14} (at 27|'), 0.363 {I18} (at 33|'), 0.430 {I22} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$|s(mb/sr)=0.292 {I16} (at 8|'), 0.568 {I29} (at 18|'), 0.536 {I27} (at 27|'), 0.419 {I21} (at 33|'), 0.237 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0460 {I31} (at 8|'), 0.165 {I9} (at 18|'), 0.088 {I5} (at 27|'), 0.0483 {I25} (at 33|'), 0.0441 {I23} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.85 {I4} (at 8|'), 2.69 {I14} (at 18|'), 1.27 {I6} (at 27|'), 0.646 {I33} (at 33|'), 0.668 {I34} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.257 {I14} (at 8|'), 0.0400 {I22} (at 18|'), 0.098 {I5} (at 27|'), 0.094 {I5} (at 33|'), 0.0386 {I20} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0130 {I12} (at 8|'), 0.00220 {I32} (at 18|'), 0.0049 {I4} (at 27|'), 0.00430 {I29} (at 33|'), 0.00190 {I22} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0180 {I14} (at 8|'), 0.075 {I4} (at 18|'), 0.0445 {I24} (at 27|'), 0.0255 {I14} (at 33|'), 0.018 {I1} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.127 {I10} (at 8|'), 0.177 {I9} (at 18|'), 0.070 {I5} (at 27|'), 0.081 {I5} (at 33|'), 0.0470 {I26} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.341 {I19} (at 8|'), 0.0510 {I33} (at 18|'), 0.121 {I6} (at 27|'), 0.114 {I6} (at 33|'), 0.0600 {I32} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.088 {I8} (at 8|'), 0.205 {I11} (at 18|'), 0.114 {I6} (at 27|'), 0.0580 {I31} (at 33|'), 0.056 {I3} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.186 {I10} (at 8|'), 0.81 {I4} (at 18|'), 0.485 {I25} (at 27|'), 0.263 {I13} (at 33|'), 0.204 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.18 {I1} (at 8|'), 0.557 {I28} (at 18|'), 0.308 {I16} (at 27|'), 0.180 {I9} (at 33|'), 0.151 {I8} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0400 {I28} (at 8|'), 0.0630 {I33} (at 18|'), 0.090 {I5} (at 27|'), 0.120 {I6} (at 33|'), 0.079 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.382 {I20} (at 8|'), 0.073 {I4} (at 18|'), 0.145 {I7} (at 27|'), 0.159 {I8} (at 33|'), 0.089 {I5} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0150 {I21} (at 8|'), 0.0256 {I15} (at 18|'), 0.0302 {I17} (at 27|'), 0.0393 {I21} (at 33|'), 0.0386 {I20} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.003 {I1} (at 8|'), 0.0078 {I6} (at 18|'), 0.0039 {I4} (at 27|'), 0.00430 {I29} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.553 {I29} (at 8|'), 1.55 {I8} (at 18|'), 0.74 {I4} (at 27|'), 0.415 {I21} (at 33|'), 0.373 {I19} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|s(mb/sr)=0.076 {I5} (at 8|'), 0.075 {I6} (at 18|'), 0.031 {I5} (at 27|'), 0.0344 {I19} (at 33|'), 0.025 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0420 {I29} (at 8|'), 0.142 {I7} (at 18|'), 0.080 {I4} (at 27|'), 0.0424 {I23} (at 33|'), 0.0301 {I16} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.003 {I1} (at 8|'), 0.0088 {I6} (at 18|'), 0.0087 {I6} (at 27|'), 0.0106 {I6} (at 33|'), 0.0070 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0016 {I8} (at 8|'), 0.0089 {I6} (at 18|'), 0.00350 {I35} (at 27|'), 0.00250 {I33} (at 33|'), 0.00140 {I21} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0090 {I11} (at 8|'), 0.0164 {I10} (at 18|'), 0.0121 {I8} (at 27|'), 0.0168 {I10} (at 33|'), 0.0208 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.569 {I29} (at 8|'), 0.082 {I4} (at 18|'), 0.202 {I10} (at 27|'), 0.218 {I11} (at 33|'), 0.103 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0090 {I11} (at 8|'), 0.0084 {I6} (at 18|'), 0.00260 {I33} (at 27|'), 0.00330 {I26} (at 33|'), 0.00190 {I22} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0300 {I25} (at 8|'), 0.101 {I5} (at 18|'), 0.0571 {I30} (at 27|'), 0.0289 {I16} (at 33|'), 0.0228 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0360 {I21} (at 8|'), 0.091 {I5} (at 18|'), 0.0578 {I30} (at 27|'), 0.0337 {I17} (at 33|'), 0.0273 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0210 {I15} (at 8|'), 0.0385 {I21} (at 18|'), 0.0195 {I11} (at 27|'), 0.0074 {I6} (at 33|'), 0.0096 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.186 {I10} (at 8|'), 0.497 {I25} (at 18|'), 0.278 {I14} (at 27|'), 0.147 {I8} (at 33|'), 0.139 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0310 {I19} (at 8|'), 0.109 {I6} (at 18|'), 0.069 {I4} (at 27|'), 0.0360 {I19} (at 33|'), 0.0271 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0070 {I11} (at 8|'), 0.0048 {I5} (at 18|'), 0.0046 {I5} (at 27|'), 0.00330 {I26} (at 33|'), 0.00140 {I21} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0039 {I8} (at 8|'), 0.0055 {I5} (at 18|'), 0.0038 {I4} (at 27|'), 0.00410 {I29} (at 33|'), 0.00310 {I25} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0130 {I12} (at 8|'), 0.0175 {I10} (at 18|'), 0.0230 {I13} (at 27|'), 0.0259 {I14} (at 33|'), 0.0157 {I9} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0370 {I27} (at 8|'), 0.083 {I4} (at 18|'), 0.093 {I5} (at 27|'), 0.114 {I6} (at 33|'), 0.122 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0100 {I11} (at 8|'), 0.0344 {I18} (at 18|'), 0.0236 {I13} (at 27|'), 0.0137 {I8} (at 33|'), 0.0094 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0140 {I12} (at 8|'), 0.0226 {I12} (at 18|'), 0.0341 {I18} (at 27|'), 0.0416 {I22} (at 33|'), 0.0362 {I19} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.0330 {I19} (at 8|'), 0.052 {I4} (at 18|'), 0.0587 {I30} (at 27|'), 0.0401 {I21} (at 33|'), 0.0284 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.079 {I5} (at 8|'), 0.0494 {I26} (at 27|'), 0.0491 {I26} (at 33|'), 0.0224 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.0230 {I23} (at 8|'), 0.0392 {I21} (at 27|'), 0.0548 {I29} (at 33|'), 0.0610 {I31} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.080 {I5} (at 8|'), 0.0193 {I11} (at 18|'), 0.034 {I2} (at 27|'), 0.0396 {I21} (at 33|'), 0.0219 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0260 {I24} (at 8|'), 0.0529 {I28} (at 18|'), 0.0233 {I13} (at 33|'), 0.0169 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.044 {I3} (at 8|'), 0.099 {I5} (at 18|'), 0.071 {I7} (at 27|'), 0.0394 {I21} (at 33|'), 0.0375 {I20} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.160 {I9} (at 8|'), 0.155 {I8} (at 18|'), 0.078 {I10} (at 27|'), 0.087 {I5} (at 33|'), 0.0588 {I30} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0420 {I29} (at 8|'), 0.0120 {I8} (at 18|'), 0.0230 {I13} (at 33|'), 0.0144 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0420 {I29} (at 8|'), 0.109 {I6} (at 18|'), 0.075 {I9} (at 27|'), 0.0497 {I26} (at 33|'), 0.0387 {I20} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0330 {I34} (at 8|'), 0.0440 {I24} (at 18|'), 0.0540 {I29} (at 27|'), 0.0519 {I27} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0180 {I22} (at 8|'), 0.0376 {I21} (at 18|'), 0.0336 {I19} (at 27|'), 0.0148 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.369 {I20} (at 8|'), 0.81 {I4} (at 18|'), 0.554 {I28} (at 27|'), 0.306 {I16} (at 33|'), 0.263 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.067 {I6} (at 8|'), 0.0650 {I34} (at 18|'), 0.0375 {I21} (at 27|'), 0.0278 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.042 {I6} (at 8|'), 0.0609 {I32} (at 18|'), 0.0500 {I27} (at 27|'), 0.0223 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.050 {I4} (at 8|'), 0.0230 {I13} (at 18|'), 0.0226 {I13} (at 27|'), 0.0091 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.064 {I4} (at 8|'), 0.079 {I4} (at 18|'), 0.086 {I5} (at 27|'), 0.076 {I4} (at 33|'), 0.0297 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.106 {I7} (at 8|'), 0.214 {I11} (at 18|'), 0.140 {I7} (at 27|'), 0.091 {I5} (at 33|'), 0.0640 {I33} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0360 {I35} (at 8|'), 0.072 {I4} (at 18|'), 0.0470 {I26} (at 27|'), 0.0375 {I20} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.047 {I4} (at 8|'), 0.0660 {I35} (at 18|'), 0.0400 {I22} (at 27|'), 0.0372 {I21} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0110 {I21} (at 8|'), 0.0290 {I18} (at 18|'), 0.0230 {I15} (at 27|'), 0.0136 {I11} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0330 {I34} (at 8|'), 0.0415 {I23} (at 18|'), 0.0320 {I19} (at 27|'), 0.0234 {I14} (at 33|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.063 {I5} (at 8|'), 0.0460 {I31} (at 18|'), 0.071 {I4} (at 27|'), 0.072 {I4} (at 33|'), 0.045 {I3} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.076 {I5} (at 8|'), 0.090 {I6} (at 18|'), 0.099 {I5} (at 27|'), 0.068 {I4} (at 33|'), 0.0400 {I28} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.078 {I6} (at 8|'), 0.080 {I21} (at 18|'), 0.128 {I7} (at 27|'), 0.091 {I5} (at 33|'), 0.063 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.032 {I4} (at 8|'), 0.0600 {I32} (at 18|'), 0.0280 {I25} (at 27|'), 0.0193 {I11} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.035 {I4} (at 8|'), 0.0490 {I27} (at 18|'), 0.0190 {I22} (at 27|'), 0.0280 {I17} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.0120 {I21} (at 8|'), 0.0292 {I17} (at 18|'), 0.045 {I3} (at 27|'), 0.0205 {I13} (at 33|'), 0.0140 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.007 {I2} (at 8|'), 0.0231 {I14} (at 18|'), 0.0420 {I29} (at 27|'), 0.0131 {I9} (at 33|'), 0.0097 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0310 {I25} (at 8|'), 0.0184 {I11} (at 18|'), 0.0230 {I23} (at 27|'), 0.0166 {I10} (at 33|'), 0.0084 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.091 {I6} (at 8|'), 0.150 {I8} (at 18|'), 0.131 {I7} (at 27|'), 0.101 {I5} (at 33|'), 0.0622 {I32} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.038 {I4} (at 8|'), 0.0630 {I33} (at 18|'), 0.0480 {I31} (at 27|'), 0.0338 {I19} (at 33|'), 0.0220 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0150 {I21} (at 8|'), 0.0430 {I24} (at 18|'), 0.0146 {I11} (at 33|'), 0.0205 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0280 {I25} (at 8|'), 0.0610 {I32} (at 18|'), 0.0320 {I19} (at 33|'), 0.020 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.196 {I10} (at 8|'), 0.077 {I4} (at 18|'), 0.095 {I5} (at 27|'), 0.123 {I6} (at 33|'), 0.076 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.185 {I10} (at 8|'), 0.177 {I9} (at 18|'), 0.101 {I6} (at 27|'), 0.092 {I5} (at 33|'), 0.069 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0380 {I28} (at 8|'), 0.060 {I9} (at 18|'), 0.0448 {I24} (at 27|'), 0.0278 {I16} (at 33|'), 0.0236 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.083 {I5} (at 8|'), 0.135 {I7} (at 18|'), 0.095 {I5} (at 27|'), 0.0524 {I27} (at 33|'), 0.0492 {I25} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.173 {I10} (at 8|'), 0.126 {I6} (at 18|'), 0.110 {I6} (at 27|'), 0.093 {I5} (at 33|'), 0.0665 {I35} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.023 {I4} (at 8|'), 0.084 {I4} (at 18|'), 0.0670 {I35} (at 27|'), 0.0370 {I21} (at 33|'), 0.0299 {I18} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.120 {I8} (at 8|'), 0.128 {I7} (at 18|'), 0.097 {I5} (at 27|'), 0.090 {I5} (at 33|'), 0.0460 {I25} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.168 {I10} (at 8|'), 0.173 {I9} (at 18|'), 0.150 {I8} (at 27|'), 0.129 {I7} (at 33|'), 0.073 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.069 {I5} (at 8|'), 0.0520 {I33} (at 18|'), 0.0390 {I22} (at 27|'), 0.0400 {I22} (at 33|'), 0.0270 {I17} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.053 {I8} (at 8|'), 0.0310 {I19} (at 27|'), 0.0273 {I14} (at 33|'), 0.0154 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.040 {I4} (at 8|'), 0.050 {I4} (at 18|'), 0.073 {I4} (at 27|'), 0.0480 {I26} (at 33|'), 0.0370 {I21} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.079 {I8} (at 8|'), 0.0300 {I25} (at 18|'), 0.0410 {I23} (at 27|'), 0.0246 {I15} (at 33|'), 0.0240 {I16} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.081 {I9} (at 8|'), 0.034 {I2} (at 18|'), 0.0600 {I32} (at 27|'), 0.0270 {I16} (at 33|'), 0.0280 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.0280 {I33} (at 8|'), 0.069 {I4} (at 18|'), 0.083 {I5} (at 27|'), 0.0500 {I27} (at 33|'), 0.0294 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.0130 {I21} (at 8|'), 0.0210 {I15} (at 18|'), 0.0370 {I21} (at 27|'), 0.0246 {I15} (at 33|'), 0.0131 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.039 {I6} (at 8|'), 0.059 {I4} (at 18|'), 0.073 {I4} (at 27|'), 0.0470 {I26} (at 33|'), 0.0273 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.132 {I8} (at 8|'), 0.119 {I6} (at 18|'), 0.081 {I5} (at 27|'), 0.070 {I4} (at 33|'), 0.0410 {I23} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.083 {I6} (at 8|'), 0.068 {I4} (at 18|'), 0.0410 {I29} (at 27|'), 0.0390 {I22} (at 33|'), 0.0255 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.143 {I8} (at 8|'), 0.102 {I6} (at 18|'), 0.079 {I5} (at 27|'), 0.075 {I4} (at 33|'), 0.0490 {I27} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.086 {I6} (at 8|'), 0.091 {I5} (at 18|'), 0.080 {I5} (at 27|'), 0.0610 {I32} (at 33|'), 0.0354 {I20} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.076 {I6} (at 8|'), 0.0480 {I31} (at 18|'), 0.035 {I2} (at 27|'), 0.034 {I2} (at 33|'), 0.0161 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.173 {I10} (at 8|'), 0.172 {I9} (at 18|'), 0.144 {I8} (at 27|'), 0.120 {I6} (at 33|'), 0.070 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0260 {I33} (at 8|'), 0.066 {I4} (at 18|'), 0.045 {I3} (at 27|'), 0.0360 {I27} (at 33|'), 0.0240 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.119 {I7} (at 8|'), 0.086 {I5} (at 18|'), 0.066 {I4} (at 27|'), 0.075 {I4} (at 33|'), 0.0446 {I24} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.041 {I4} (at 8|'), 0.088 {I5} (at 18|'), 0.0590 {I31} (at 27|'), 0.0540 {I29} (at 33|'), 0.0394 {I22} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.086 {I6} (at 8|'), 0.0310 {I25} (at 18|'), 0.0300 {I18} (at 27|'), 0.057 {I3} (at 33|'), 0.0369 {I21} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.064 {I4} (at 8|'), 0.0500 {I32} (at 18|'), 0.0330 {I19} (at 27|'), 0.0480 {I26} (at 33|'), 0.0274 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.092 {I6} (at 8|'), 0.0480 {I31} (at 18|'), 0.0280 {I17} (at 27|'), 0.0510 {I28} (at 33|'), 0.0318 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.049 {I4} (at 8|'), 0.0650 {I34} (at 18|'), 0.0490 {I27} (at 27|'), 0.0460 {I25} (at 33|'), 0.0318 {I18} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOME2$from Coul. ex. 
MOMM1$from IMPAC (1989Ra17) 
J$Coul. excited, L in (d,d') 
T$from B(E2)=0.841 {I16} (1987Ra01) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$others: 0.834 {I44} (1980La01), 1.04 (1956Te26), 0.928 {I7} (1958St32), 0.81 (1968Mc08) 
MOME2 from 1980La01. Others: -0.84 {I21} (1973No04), -0.66 {I5} (1977Ma41); Q estimated under the assumption of a positive interference term 
T$from B(E2)(|_)=0.168 {I9} (2006Sr01) 
$Diagonal E2 matrix element=-0.71 {I11} (2006Sr01) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$6.0 ps 3 from B(E2)(|_)=0.226 {I11} (2006Sr01) 
$Diagonal E2 matrix element=-0.79 {I15} (2006Sr01). B(E2)=0.431 {I47} (1980La01); 0.390 {I69} (1968Mc08) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$other: 0.0276 {I30} (1968Mc08) 
T$7.6 ps 10 from average of B(E2)(|_)=0.0049 {I3} and B(E2)(|_)=0.113 {I11} (2006Sr01). The |g-ray branching ratios were taken from adopted levels. 
$Diagonal E2 matrix element=+0.62 {I8} (2006Sr01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(|_)=0.139 {I11} and |g-ray branching from adopted gammas in ENSDF for {+104}Ru 
$Diagonal E2 matrix element=-0.58 {I18} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from average of two values obtained from B(E2)(|_)=0.101 {I13} and B(E2)(|_)=0.028 {I6}. The |g-ray branching ratio were taken from adopted gammas 
$Diagonal E2 matrix element=-0.08 {I+11-25} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$ average of two measured values of +0.40 {I1} and +0.39 {I1} with statistical uncertainty only. The statistical uncertainty on the average value is 0.01, whereas the uncertainty including that in the absolute value is 0.03, arising mainly from the calibration value 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: H
level_comment:
J$5909.9|g from 1/2+ in {+104}Ru(n,|g) E=th:primary; L(d,p)=2; systematics of the 3/2+ states in Ru isotopic chain 
T$weighted average of: 4.45 h {I2} (1955Wi59), 4.44 h {I2} (1960Ri03), 4.43 h {I2} (1962Br15), 4.39 h {I10} (1965Pi01); Others: 1974Ca26, 1950Sl06, 1950Su07, 1946Bo28 
MOMM1$From oriented {+105}Ru decay 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
J$L(d,p)=2; 20.559|g M1+E2 to 3/2+ ; 5/2+ is supported by the single-particle spectroscopic strength; 
CONF$|nd{-5/2} 
T$from 20.559|g(t) in {+105}Tc |b{+-} decay (1975Su02) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: NS
level_comment:
J$L(d,p)=2; 143.26|g M1+E2 to 5/2+; 
T$from 143.26|g(t) in 1978Ho06. Not corrected for side feeding. Perhaps associated with T{-1/2} of 208.8-keV level 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$208.89|g to 5/2+, 229.51|g to 3/2+; L(d,p)=4; single-particle spectroscopic strength supports 7/2+ 
CONF$|ng{-7/2} 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2+)
level_comment:
J$244.35|g to 3/2+, 223.79|g to 5/2+; no primary transition from 1/2+ in {+104}Ru(n,|g) E=th:primary 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J$138.446|g M1+E2 to 5/2+, 246.29|g to 3/2+; However, L(d,p)=4,3 suggests 5/2-,7/2 or 9/2+ assignment 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$113.34|g to 1/2+, 252.07|g M1(+E2) to 5/2+, 272.65|g M1+E2 to 3/2+; 5637.1|g from 1/2+ in {+104}Ru(n,|g) E=th:primary; systematics of the 3/2+ states in Ru isotopic chain 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$L(d,p)=1; 162.25|g to 1/2+, 213.66|g E1 to 5/2+; 5588.4|g from 1/2+ in {+104}Ru(n,|g) E=th:primary 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J$L(d,p)=2; 169.18|g M1+E2 to 3/2+, 282.67|g to (1/2+), 333.90|g M1+E2 to 5/2+; no primary |g-ray from 1/2+ n-capture state supports 5/2+ 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$L(d,p)=2; 306.76|g M1+E2 to 1/2+, 357.94|g M1+E2 to 5/2+, 5444.0|g from 1/2+ in {+104}Ru(n,|g) E=th:primary 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$L(d,p)=2; 565.02|g to 3/2-, 640.34|g M1+E2 to (3/2+,5/2+); 5023.4|g from 1/2+ {+104}Ru(n,|g) E=th:primary 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
J$1008.4|g to 3/2+, 1201.6|g to 1/2+, 1510.6|g to 3/2-; 4076.7|g from 1/2+ in {+104}Ru(n,|g) E=th:primary 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
E$Could be unresolved multiplet given two close lying levels are observed at 244 and 246~keV in (n,|g) 
L$The adopted J|p supports L=4 
S$for L=4, |n1g{-7/2} in 1976Ma49; Otherwise: 0.04~{I1} for L=3, |n1f{-5/2} or 0.03~{I1} for L=3, |n1f{-7/2} in 1976Ma49 
CONF$|n1g{-7/2}, |n1f{-5/2}, |n1f{-7/2} 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
S$for L=2, |n2d{-3/2} in 1976Ma49; Also: 0.31~{I2} for L=2, |n2d{-5/2} in 1976Ma49 
CONF$|n2d{-3/2} or 2|nd{-5/2} 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_comment:
S$for L=3, |n1f{-5/2} in 1976Ma49; Also: 0.18 {I5} for L=3 |n1f{-7/2} or 0.030 {I15} for L=1, |n2p{-1/2} or L=1, |n2p{-3/2} in 1976Ma49 
CONF$|n1f{-5/2}, |n1f{-7/2}, |n2p{-1/2}, |n2p{-3/2} 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
S$for L=3, |n1f{-5/2} in 1976Ma49; Also: 0.15~{I3} for L=3, |n1f{-7/2} in 1976Ma49 
CONF$|n1f{-7/2}, |n1f{-7/2} 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
S$for L=2, 2d{-3/2} in 1976Ma49; Also: 0.12~{I3} for L=2, 2d{-5/2} in 1976Ma49 
CONF$|n2d{-3/2}, |n2d{-5/2} 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2+)
level_comment:
L$the adopted J|p supports L=4 
S$for L=4, |n1g{-7/2} in 1976Ma49; Otherwise: 1.1~{I4} for L=5, |n1h{-11/2} in 1976Ma49 
CONF$|n1g{-7/2}, |n1h{-11/2} 


level_energy_unit: KEV
level_spin_parity: (3/2:9/2)
level_comment:
S$for L=4, |ng{-7/2} in 1976Ma49; Otherwise: 0.9~{I4} for L=5 |nh{-11/2} in 1976Ma49 
CONF$|n1g{-7/2}, |n1h{-11/2} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: D
level_comment:
T From the evaluation of 2004Wo02. Others: 373.59 d (1980Ho17) {i15}, 371.63 d {i17} (1977DeYO), 371.7 d {I15} (1983Wa26), 366.5 d {I8} (1956Sc87), 372 d {I4} (1957Me47), 365.8 d {I17} (1960Ea02), 371 d 1 (1961Wy01), 368.0 d {I18} (1965Fl02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J L=2 (t,p) 
T$From time-integral perturbed angular correlations with Gammasphere in connection with a {+252}Cf SF source (2004Sm04,2005Sm08). T{-1/2} calculated assuming the same transition quadrupole moment as {+108}Ru. Other: 0.26 ns {I7} (1995Sc24) 
G$From {+252}Cf SF decay (2004Sm04,2005Sm08) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J suggested by 1980Su01 from similar decay properties of this level compared to the 3+ levels in neighboring nuclei: {+102}Ru, {+104}Ru, {+108}Ru. Consistent with (821|g)(270|g)(|q) data 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
E$From adopted levels 
T$From time-integral perturbed angular correlations with Gammasphere in connection with a {+252}Cf SF source (2004Sm04,2005Sm08). T{-1/2} calculated assuming the same transition quadrupole moment as {+108}Ru. Other: 0.26 ns {I7} (1995Sc24) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: MIN
level_comment:
J$(5/2)+ is consistent with log| {Ift}=5.77 {I9} to 7/2+, {+107}Rh g.s. with negligible branching to 9/2+ first excited state; 1979St24 suggest 3/2+ from systematics with {+103}Ru, {+105}Ru g.s. 
T$from (194|g,374|g,406|g,848|g) decay curves (1978Fr16) semi. Others: 3.6 min {I1} (194|g,406|g)-decay curves (1969WiZX), 4.2 min {I3} (1962Pi02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$from 1978Fr16 (165|g decay curve). Others: 4.5 min {i2} (1962Pi02), 4.4 min {i2} (1969WiZX), 4.6 min {i1} (1976KaYO) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$weighted average of 0.345 ns 30 in SF decay and 0.41 ns 7 in |b{+-} decay. Other: 0.41 {i7} (1995Sc24) |b|g(t) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from 1986Ma22. Recoil-distance Doppler shift measurements. The value is an average for the 4+ states in {+108}Ru and {+110}Ru since E|g(4+ to 2+)=423 in both nuclides, and these transitions were not resolved. Other: <0.08 ns (1995Sc24) |b|g(t) 
J$|g to 2+. Probable member of g.s. rotational band 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$|g|g(|q) in {+108}Tc |b{+-} decay on the 732.6 and 733.9 doublet consistent only with J(975)=0 if J(974)=3 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$from 1974JaZN. Other: 0.22 ns {i4} (1970Ch11) from recoil-distance Doppler shift, this value is an average of {+108}Ru and {+110}Ru because the 423|g is common to both nuclides and was not resolved. 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$ From transition multipolarities deduced using |g|g(|q) data, but values of angular correlation coefficients were not provided in 2009Lu01 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
J$direct feeding in {+109}Tc |b{+-} decay (J|p=(5/2+)); systematics of odd-N Ru isotopes; configuration assignment 
T$Weighted average of 34.5 s {i10} (using 206, 226|g(t) in 1978Fr16), 33 s {i3} (using 206,358|g(t) in 1976MaYL), 34.5 s {i2} (using 68,206,226, 890|g(t) in 1987Ka29,1986KaZS) 32.2 s {i10} (using 116.4,206,226, and 358|g(t) in 1969WiZX), 34.5 s {i24} (1967Fr16,1967Gr25, using chemical separation), and 35 s {i2} (using 206|g(t) in 1976Tr02). Other: 35 s (1971Ri02); 1987Ka29 found no evidence for a 12.6 s activity reported by 1978Fr16, 1969WiZx. 
CONF$probably a mixture of |n5/2[413] or |n5/2[402] Nilsson configurations. The assignment is consistent with the observed g{-K}-g{-R}|?0.4 from the in-band cascade-to-crossover branching ratios, compared to 0.7 and 0.05 expected from deformed Woods-Saxon model for the |n5/2[402] and |n5/2[413] orbitals, respectively 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: US
level_comment:
J$68.8|g E2 to (5/2+); probable |n1/2[411] Nilsson configuration 
T$using 68.8|g(t) in {+109}Tc |b{+-} decay (1992PeZX) 
CONF$probable K|p=1/2+, |n1/2[411] Nilsson configuration 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: US
level_comment:
J$96.2|g E1 to (5/2+); band assignment; possible configuration=|n5/2[532] 
T$from 96|g(t), weighted average of 0.68 |ms {i3} (1999Ge01), 0.75 |ms {i15} (1976ChZD), 0.54 |ms {i15} (1974ClZX), and 0.54 |ms {i17} (1992PeZX). Other: 0.55 |ms from 96|g(t) in 1970Jo20 
MOMM1$from g=-0.22 {I1} using TDPAD (1976ChZD). 
CONF$|n5/2[532] Nilsson orbital. From the experimental g factor, one can deduce a g{-K}=-0.20, assuming g{-R}=0.28, which is consistent with g{-K}(|n5/2[532])=-0.38 and g{-K}(|n5/2[402])=-0.42, but not with g{-K}(|n5/2[413])=+0.33 and g{-K}(|n1/2[411])=+1.75. The larger energy staggering supports |n5/2[532], compared to |n5/2[402]. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: NS
level_comment:
J$35.7|g M1 to (5/2-), 131.8|g (E1) to (5/2+); band assignment 
T$from {+254}Cf SF decay (1981SeZW) using time-of-flight method. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: NS
level_comment:
J$137.9|g E1+M2 to (5/2+), 69.1|g to (1/2+) 
T$from |b-137.9|g(t) in {+109}Tc |b{+-} decay (1995Sc24). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)+
level_lifetime_unit: NS
level_comment:
J$195.0|g M1 to (5/2+), 98.9|g (E1) to (5/2-) 
T$from |b-195|g(t) in {+109}Tc |b{+-} decay (1995Sc24). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_comment:
J$98.2|g (M1) to (7/2-), 134.2|g to (5/2-); band assignment 
T$from {+254}Cf SF decay (1981SeZW) using time-of-flight method. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: NS
level_comment:
J$172.3 (E2) to (7/2-); band assignment 
T$from {+254}Cf SF decay (1981SeZW) using time-of-flight method. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$332.5|g to (5/2+); band assignment 
CONF$possible |n7/2[404] Nilsson state (2009Di12 in {+252}Cf SF decay). The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_lifetime_unit: NS
level_comment:
J$514.5|g to (5/2+), 445.8|g to (1/2+), 376.7|g to (3/2-); direct feeding from (5/2+) in {+109}Tc |b{+-} decay 
T$from |b-445.8|g(t) in {+109}Tc |b{+-} decay (1995Sc24). 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
J$374.7|g (E2) to (11/2-); band assignment 
T$from {+254}Cf SF decay (1981SeZW) using time-of-flight method. 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: PS
level_comment:
J$691.0|g (E2) to (19/2-); band assignment 
T$using the Doppler Profile Method in {+248}Cm SF decay (2012Sm02). statistical uncertainty=0.16 ps, systematic uncertainty=0.15 ps 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: PS
level_comment:
J$822.0|g to (23/2-); band assignment 
T$using the Doppler Profile Method in {+248}Cm SF decay (2012Sm02). statistical uncertainty=0.062 ps, systematic uncertainty=0.055 ps 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: US
level_comment:
T$From |g(t) in 1999Ge01. Other: 0.75 |ms {i15} (1976ChZD), 0.54 |ms {I17} (1992PeZX, using 96.1|g(t)) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$Unweighted average of 11.6 s {I6} (using |b-112|g(t) in 1991Jo11), 12.2 s {I1} (using 96|g(t) in 1986KaZS), 11.98 s {I4} (using 112|g(t) in 1986KaZS), 11.8 s {I2} (using 374|g(t) in 1986KaZS) and 12.6 s {I5} (using 374|g(t) in 1978Fr16). Others: 17.0 s {I1} (using 374|g(t) in 1975Fe12), 14.7 s {I13} (using 112|g(t) in 1976MaYL) and 15.9 s {I5} (using 374|g(t) in 1969WiZX) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J$240.7|g E2 to 0+ 
T$Unweighted average of 0.34 ns 4 from {+252}Cf decay (1974JaYY) and 0.30 ns {I2} from {+254}Cf decay (1980ChZM). Others: 0.50 ns {I8} in 1995Sc24, 0.23 ns in 1972Wi15 and 1970Ch11, and <0.5 ns in 1970Wa05 
MOMM1$+0.88 {i14}, from g-factor=+0.44 {i7} measured using time-integral perturbed angular correlation technique in 2005Sm08 and in 2004Sm04 (T{-1/2}=0.30 ns 2 was used) 
MOME2$-0.74 {i9} from lifetime measurements using Doppler-profile method in 1999SmZX 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: NS
level_comment:
J$372.1|g M1+E2 to 2+ and 612.9|g to 0+. Branching ratio favors 2+ 
T$From 372.1|g(t) (centroid-shift) in 1995Sc24. Others: 0.01 ns {I16} from 612.9|g(t) (centroid-shift) in 1995Sc24 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$422.6|g E2 to 2+; member of the g.s. band 
T$From 2001Kr13, using differential recoil distance method. Others: 13.4 ps 10 (1986Ma22). However, this is a combined value for {+108}Ru and {+110}Ru since the 4+ to 2+ transitions in those isotopes can not be resolved 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$896.7|g to 2+. No transition to the ground state nor feeding to or from the levels with J>2 were observed 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$575.7|g E2 to 4+; member of the g.s. band 
T$From 2001Kr13, using differential recoil distance method 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$2082.8|g to (3+); nonobservation of |g to 2+ and 0+; direct population in {+110}Tc |b- decay (J|p=2,3+) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: NS
level_comment:
T$From 372.1|g(t) in 1995Sc24 using the centroid shift. Others: 0.01 ns {I16} for 613.0|g(t) in 1995Sc24 using the centroid shift 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$From 1974JaYY, deduced by varying the distance between source and one of the fragment detectors with a micrometer screw. Others: 0.23 ns from 1972Wi15 and 1970Ch11 and <0.5 ns from 1970Wa05 
MOMM1$+0.88 {I14}, from g-factor=+0.44 {I7} measured using time-integral perturbed angular correlation technique (T{-1/2}=0.30 ns 2 from 1980ChZM, {+254}Cf decay) in 2005Sm08 and 2004Sm04 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$From 2001Kr13, using differential recoil distance method. Others: 13.4 ps 10 (1986Ma22). However, this is a combined value for {+108}Ru and {+110}Ru since the 4+ to 2+ transitions for both isotopes can not be resolved 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$From 1980ChZM, by varying the distance between the source and the fission fragments detector using a micrometer screw 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
$Quadrupole moment in eb units 
T$mean lifetime |t=0.46 ns {I3}, deduced by 2017Do01 from their B(E2)|_ value for 240.7|g. Compiler obtains T{-1/2}=0.317 ns {I+25-22} from listed B(E2)|_ value. In the ENSDF database, value is 0.32 ns {I2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced by compiler from B(E2)|_=0.023 {I1} for 612.9|g. Value is 12 ps {I+8-3} from B(E2)|_=0.35 {I13} for 372.1|g, assumed as E2. In the ENSDF database, adopted value is 0.16 ns {I8} from 372|g(t), and a second value listed as 0.01 ns {I16} from 612.9|g(t), both from 1995Sc24 (Z. Phys. A352, 237), where the authors listed an average value of 0.09 ns {I7} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$deduced by compiler from B(E2)|_=0.0293 {I+31-21} for 422.6|g. Value in the ENSDF database is 15.4 ps {I17} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
T$deduced by compiler from B(E2)|_=0.015 {I2} for 619.2|g assumed as E2. Other: 35 ps {I+86-14} from B(E2)|_=0.31 {I+21-22} for 247.1|g assumed as E2. No value is available from the previous literature 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$deduced by compiler from B(E2)|_=0.38 {I+9-4} for 575.7|g. Value in the ENSDF database is 2.4 ps {I10} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=445 ps {I34} (2019Ga29) from the three samples approach. Other: 335 ps {I26} from measured mean lifetime |t=483 ps {I38} (2019Ga29) from interpolation approach. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_comment:
T$from 1988Pe13 after mass separation. Others: 3 s {I1} (1978Fr16) growth-decay curve of 275|g. 1.5 s {I3} (1975Fe12) timed-separation method; Ru activity from thermal {+235}U(n,F) chem; 23-min {+111}Pd |b{+-} counted. 2.1 s {I6} (1976MaYL) {+252}Cf SF, timed gas-separation method, 275|g-decay curve. 
E$g.s. assignment was confirmed by 1988Pe13 using on-line isotope separator facility IGISOL. 
J$strong beta feeding to (7/2+) {+111}Rh g.s. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 327.0|g(t), following {+112}Ru |b{+-}-decay using a mass separated source (1991Jo11,1988Pe13,1988AyZZ). Others: 2.6 s 1, deduced from the growth and decay of 348|g in {+112}Pd (1987GiZW), 4.65 s 14 (1970WiZN), 4.1 s 3 (1976MaYL), and 3.6 s 5 (1978Fr16), but some of these activities probably belong to {+112}Rh. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J$236.8|g E2 to the g.s. 
T$from recoil-distance Doppler-shift method (1974JaZN,1974JaYY). Other: 0.16 ns {I4} (1970Ch11) 
MOMM1$+0.88 {I18}, deduced from g=+0.44 {I9} (2004Sm04, 2005Sm08) using the time-integral correlation technique. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$650.0|g (E2) to 6+; band assignment 
T$Other: 1.7 ps {I+13-5} in {+252}Cf SF decay (2013Sn01) using DSAM 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: PS
level_comment:
J$270.8|g to 6+; 605.7|g (E2) to 5+; band assignment 
T$Other: 2.2 ps {I+7-14} in {+252}Cf SF decay (2013Sn01) using DSAM 


level_energy_unit: KEV
level_spin_parity: 9+
level_lifetime_unit: PS
level_comment:
J$694.4|g (E2) to 7+; band assignment 
T$Other: 1.3 ps {I+7-6} in {+252}Cf SF decay (2013Sn01) using DSAM 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J$723.3|g (E2) to 8+; band assignment 
T$Other: 1.4 ps {I3} in {+252}Cf SF decay (2013Sn01) using DSAM 


level_energy_unit: KEV
level_spin_parity: 11+
level_lifetime_unit: PS
level_comment:
J$756.3|g (E2) to 9+; band assignment 
T$Other: 0.9 ps {I5} in {+252}Cf SF decay (2013Sn01) using DSAM 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
J$763.2|g (E2) to 10+; band assignment 
T$weighted average of 0.80 ps {I12} in {+248}Cm SF decay (2012Sm02) (Doppler-broadened lineshape technique) and 1.12 ps {I+15-14} in {+252}Cf SF decay (2013Sn01) (DSAM) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$from recoil-distance Doppler-shift method (1974JaZN,1974JaYY). Other: 0.16 ns {I4} (1970Ch11) 
MOMM1$+0.88 {I18}, deduced from g=+0.44 {I9} (2004Sm04, 2005Sm08), using the time-integral correlation technique. 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: PS
level_comment:
T$using DSAM for 605.7|g in 2013Sn01, but the branching intensities for the 270.8|g and 605.7|g were not taken into account 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
T$from decay of 263.5|g assigned to {+113}Ru after mass separation (1998Ku17). This value confirms previous values of the same group: 0.80 s {I10} (1988Pe13) and 0.80 s {I6} (1992PeZX). Others: 2.69 s {I10} (1969WiZX) 3.2 s {I3} (1976MaYL), 3.0 s {I7} (1978Fr16). These early assignments seem close to the new assignment {+113}Rh half-life. 
J$from 2007Ku23 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
T$from 1998Ku17 
E$x ~ 130 {I18} (2003Au03) because above the 99 keV level and below. 160 keV. 2007Ku23 propose about 120 keV in agreement with 2003Au03 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_comment:
E$from 2003Zh14. There is no connection between this band head given by 2003Zh14 and the level scheme from 2007Ku23. More work is needed to clarify the level scheme 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
E$in the Erratum energy changed from g.s. to 0.0+x, based on results in 2007Ku23: Eur. Phys. Jour. A33, 307 (2007) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$Measured mass excess=-71774.2 keV {I17} (2023Hu25) 
E$from 2023Hu25, difference of measured mass excesses of the g.s. and the isomer. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MS
level_comment:
J$From systematics of neighboring nuclides (2010Ku25) 
T$from 2010Ku25. Others: 400 ms {I100} (1991AyZY), 740 ms {I80} (1992Ay02) 
%B-$the error in Q does not allow to be sure for a branching in %|b{+-}n 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MS
level_comment:
J$ from 2011Ri07. 2010Ku25 had proposed (1/2+) 
T$ from decay curves for 292|g (from decay of {+115}Ru to {+115}Rh) (2010Ku25). Weighted average of 318 ms {I29} and 343 ms {I28} measured in this work and 270 ms {I38} in authors' previous work 2010Ku01. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2+)
level_comment:
J$ from 2011Ri07. 2010Ku25 had proposed (3/2+) 
$ Possible member of |n3/2[431] oblate configuration 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (9/2-)
level_lifetime_unit: MS
level_comment:
J$ from 2011Ri07. 2010Ku25 had proposed (7/2-) 
E$ x |? 20 keV (2010Ku25) 
T$ from the decay curve for 61.7|g (2010Ku25) 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_comment:
$Measured mass excess=-65925.6 keV {I58} (2023Hu25) 
E$from 2023Hu25, from difference of measured mass excesses of the g.s. and the isomer. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=0.11 (1997Mo25) 
T$from (ion)|b correlated curve (2015Lo04). Other: 204 ms {I+32-29} (2006Mo07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. 
T$measured by 2021Ha19 from the decay curve of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 204 ms {I6} (2015Lo04: Phys. Rev. Lett. 114, 192501); 204 ms {I+32-29} (2006Mo07: Phys. Rev. C 73, 035801). Weighted average of the three values is 203 ms {I6}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
J$1/2+ with configuration=|n1/2[400] proposed in 2012LaZT. 3/2+ from systematic trends (2012Au07); 1/2+ also in theoretical calculations (1997Mo25) 
$Theoretical T{-1/2}=163.5 ms, %|b{+-}n=0.42 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+117}Ru 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Other: 142 ms {I+18-17} (2006Mo07, from ion-|b correlated curves). See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$reverse ordering of the 82.5-102.9 |g cascade is also possible, which will give a level at 82.5 keV instead of that at 102.7 keV 


level_energy_unit: KEV
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$1/2- with configuration=|n1/2[541] proposed in 2012LaZT 
T$from |g(t) method (2012Ka36). Other: 2.0 |ms {I3} (2012LaZT). Isomer was also reported in 2007To23 but without any half-life information 


level_energy_unit: KEV
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$1/2- with configuration=|n1/2[541] proposed in 2012LaZT 
$Number of implanted fragments=3.1|*10{+5} 
T$from |g(t) method (2012Ka36). Others: 2.0 |ms {I3} (2012LaZT), 1.4 |ms {I6} (2006ToZW) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. 
E$it is assumed that the observed activity corresponds to the g.s. of {+117}Ru 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 151 ms {I3} (2015Lo04: Phys. Rev. Lett. 114, 192501); 142 ms {I+18-17} (2006Mo07: Phys. Rev. C 73, 035801). Weighted average of the three values is 152 ms {I3}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=173.9 ms, %|b{+-}n=2 (2019Mo01) 
$Theoretical T{-1/2}=130 ms; %|b{+-}n=2.25, 2.63 (2021Mi17, %|b{+-}n for four different fission barriers) 
T$weighted average of 98 ms {I10} (2021Ha19) and 99 ms {I3} (2015Lo04); both from (implanted ions)|b-correlated decay curves at RIBF-RIKEN. Other: 123 ms {I+48-35} (2006Mo07, from (ion)|b decay curve) 
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)|bn-correlated events. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=165.6 ms, %|b{+-}n=2.9, %|b{+-}2n=0.0 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+119}Ru 
J$5/2- in theoretical calculations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$reverse ordering of the 90.8-136.3 |g cascade is also possible, which will give a level at 90.8 keV, instead of 136.3 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. No events for |b{+-}2n decay mode were detected by 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+119}Ru 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 69.5 ms {I20} (2015Lo04: Phys. Rev. Lett. 114, 192501). Weighted average of the two values is 69.2 ms {I20}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=107.9 ms, %|b{+-}n=3.4 (2003Mo09) 
$Theoretical T{-1/2}=71 ms, %|b{+-}n=0.9 (2016Ma12) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 45 ms {I2} (2015Lo04: Phys. Rev. Lett. 114, 192501). Weighted average of the two values is 45 ms {I2}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=88.3 ms, %|b{+-}n=7.1, %|b{+-}2n=0.0 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+121}Ru 
$Measured |s=143 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+121}Ru isotope<0.001% (2010Oh02) 
J$3/2- in theoretical calculations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. No events for |b{+-}2n decay mode were detected by 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+121}Ru 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 29 ms {I2} (2015Lo04: Phys. Rev. Lett. 114, 192501). Weighted average of the two values is 30 ms {I3}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=68.6 ms, %|b{+-}n=8.5, %|b{+-}2n=0.0 (2003Mo09) 
$Measured |s=13 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+122}Ru isotope<0.001% (2010Oh02) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$measured half-life is assumed to correspond to the ground state of {+123}Ru 
J$3/2+ from systematics (2021Ko07: NUBASE2020) and 1/2- in theoretical calculations (2019Mo01) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 
$Theoretical T{-1/2}=52.1 ms (2019Mo01), 33.4 ms (2016Ma12) 
$Theoretical %|b{+-}n=15, %|b{+-}2n=0.0 (2019Mo01); %|b{+-}n=2.5, %|b{+-}2n=0.3 (2016Ma12) 
$Measured |s=2 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+123}Ru isotope<0.001% (2010Oh02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=45.0 ms, %|b{+-}n=15.8, %|b{+-}2n=0.0 (2003Mo09) 
$Measured |s=0.6 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+124}Ru isotope<0.001% (2010Oh02) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay, thus 100% |b{+-} decay is assigned by inference 
$Theoretical T{-1/2}=33.0 ms, %|b{+-}n=18, %|b{+-}2n=0 (2019Mo01) 
$Theoretical T{-1/2}=20.6 ms, %|b{+-}n=6.8, %|b{+-}2n=1.0 (2016Ma12) 
$A total of seven counts were assigned to {+125}Ru, one event with the spectrometer setting on Rh, and six events for setting on Pd. Misidentification of this isotope is not likely since no events were observed for neighboring hydrogen-like peaks (2018Sh11) 
$Production |s=0.06 pb for Rh setting, and 0.05 pb for Pd setting, with 30% systematic uncertainty for |s 
E$it is assumed that the observed events correspond to ground-state activity. 
J$11/2- from |W{-|n}=11/2- orbital proposed in 2019Mo01 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 33.0 ms (2019Mo01) and 20.6 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+125}Ru is expected to be <25 ms, based on measured half-lives of 25 ms for {+122}Ru, 19 ms for {+123}Ru, and 15 ms for {+124}Ru, available in literature. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
E$the {+89}Rh fragments claimed to have been observed by 1995Ry03 may be from the g.s. or an isomer of {+89}Rh. However no events due to {+89}Rh were either observed in the GSI experiment (2007WeZX, 2000WeZZ, E. Wefers et al., 2000 GSI annual report 2001-1, p10); or in the RIBF-RIKEN study by 2016Ce02, where an upper limit of one event was assigned to {+89}Rh, thus the laboratory identification of this nuclide remains unconfirmed 
J$9/2+ proposed from systematics (2021Ko07); 3/2+ (2019Mo01, theoretical calculations); 7/2+ in 1995Ry03, 
T$from 2016Ce02, based on upper limit of one event assigned to {+89}Rh, with the assumption that the ratio of number of identified events associated with nuclei of the same T{-z} is the same as that for the neighboring T{-z} nuclei. One event assigned to {+89}Rh was assumed for ground-state activity, although, the authors mentioned that the proton decay could occur from either the ground state or from an isomeric activity. Other: |?1.5 |ms (1995Ry03) from time-of-flight. 
T$Theoretical proton decay T{-1/2}=7 |ms (2007Me28), using Q value of 708 keV; 201 ns (for l=0), 214 ns (for l=2) and 4 |ms (for l=5) (2015Sh03), using Q value of 700 keV 
T$theoretical |b decay T{-1/2}=90 ms (2019Mo01) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: MS
level_comment:
T$from implant-|b(t) in 2019Pa16. Other: 12 ms {I+9-4} from implant-|b(t) (2001Ki13, 2002Fa13). 
%ECP$from the number of |bp decays relative to the total number decays (2019Pa16). 
J$from log {Ift}=3.6 to 0+ ground state of {+90}Ru. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (6,7,8)
level_lifetime_unit: S
level_comment:
T$weighted average of 0.55 s {I3} from implant-|b(t) and 0.58 s {I4} from implant-|b-p(t), both from 2019Pa16. Other: 1.0 s {I+3-2} from implant-|b(t) (2001Ki13, 2002Fa13). 
%ECP$from the number of |bp decays relative to the total number decays (2019Pa16). 
J$no |b feeding to yrast 4+ in {+90}Ru; population of (13/2+) and (9/2+) levels in |bp decay to {+89}Tc; shell model calculations in 2019Pa16 predict J|p=7+ 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: S
level_comment:
T$weighted average of 0.55 s {I3} from implant-|b(t) and 0.58 s {I4} from implant-|bp(t); both analyses used multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
J 9/2+ favored from systematics (2004De40). However, 2012Au07 propose 7/2+, also attributed to systematics. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J level possibly analogous to |b-decaying 1/2- isomeric states in the {+89}Tc and {+87}Nb isotones. 
T from 2004De40. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E order of 500|g-619|g cascade not established so an alternative value of E=683 is possible. 
J band assignment. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T listed by 2012Lo08 as weighted average of 1.47 s {I22} (2004De40) and 1.7 s {I2} (2001Ki13). 
J from Adopted Levels. From systematics, 2012Au07 suggest 7/2+. 
%B+P measured by 2012Lo08 assuming the half-life value 1.60 s {I15} and based on observation of 12 |bp coincidence events. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$weighted average of 1.60 s {I2} from implant-|b(t) and 1.12 s {I33} from implant-|bp(t); both analyses used multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16). Value is combined result for the ground state and the isomer. 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). Value is combined result for the ground state and the isomer. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: S
level_comment:
T$weighted average of 1.60 s {I2} from implant-|b(t) and 1.12 s {I33} from implant-|bp(t); both analyses used multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16). Value is combined result for the ground state and the isomer. 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). Value is combined result for the ground state and the isomer. 
E$from the Adopted Levels for {+91}Rh in the ENSDF database (2013 update). 


level_energy_unit: KEV
level_spin_parity: (GE6+)
level_lifetime_unit: S
level_comment:
J |e decay to {+92}Ru(6+) is probably allowed and feeding of {+92}Ru(8+) is evident; existence of a low-lying J=5 state is not supported by shell-model calculations or Rh g.s. J|p systematics. However, see comment on J(0+x) level which may, in reality, Be the g.s. 
T from time behavior of 163|g, 340|g, 818|g and 919|g in {+92}Ru following {+92}Rh |e decay (2004De40). Others: 3.0 s {I8} (2001Xu05, 2005Xu04; from 893|g({+91}Tc)(t) following |ep decay); 5.6 s {I5} (2001Ki13); 5.6 s {I3} (2002Ku21; from time-to digital converter spectrum gated by 817|g, 865|g and 990|g); 2.9 s {I+15-8}, preliminary datum from 2000WeZZ for level(s) produced in {+112}Sn bombardment of Be. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J possible |e decay branches observed to 0+ and 2+ levels in {+92}Ru; shell-model calculations predict a very low energy 2+ level which may in fact be the g.s., but no 1+ state. However, the decay scheme is very tentative and the branch to {+92}Ru(0+ g.s.) may be overestimated. 
T from two-component fit to time spectrum of 866|g({+92}Ru) following |e decay from a {+92}Rh source containing both {+92}Rh isomers (2004De40). 


level_energy_unit: KEV
level_spin_parity: (15-)
level_comment:
E the order of the 1034|g-936|g cascade is not established, so E=3878, J|p=(14-) is a possible alternative. 


level_energy_unit: KEV
level_spin_parity: (19-)
level_comment:
E the order of the 1420|g-632|g cascade is not established, so E=7173, J|p=(20-) is a possible alternative. 


level_energy_unit: KEV
level_spin_parity: (20-)
level_comment:
E the order of the 1114|g-306|g cascade is not established, so E=7499 is also possible. Alternatively, E=6059 or 6867 and J|p=(20-) if order of 1419|g and 632|g is reversed. 


level_energy_unit: KEV
level_spin_parity: 15(-)
level_comment:
E the order of the 1034|g-936|g cascade is not established, so E=3878, J|p=14(-) is a possible alternative. 


level_energy_unit: KEV
level_spin_parity: 19(-)
level_comment:
E the order of the 1420|g-632|g cascade is not established, so E=7173, J|p=(20-) would be a possible alternative. 


level_energy_unit: KEV
level_spin_parity: 20(-)
level_comment:
E the order of the 1114|g-306|g cascade is not established, so E=7499 is also possible. Alternatively, E=6059 or 6867 and J|p=(20-) if order of 1420|g and 632|g is reversed. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$weighted average of 5.60 s {I9} from implant-|b(t) and 5.67 s {I26} from implant-|bp(t); both analyses used multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: S
level_comment:
T$weighted average of 3.18 s {I22} from implant-|b(t) and 2.6 s {I+14-7} from implant-|bp(t); both analyses used multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T weighted average of 11.9 s {I7} (2004De40; from fit to growth and decay time behavior of the 7 lines attributed to {+93}Rh decay) and 13.9 s {I16} (2001Ki13). Other datum: 5.7 s {I+13-9} (preliminary result from 2000WeZZ; probably superseded by 2001Ki13). 


level_energy_unit: KEV
level_spin_parity: (35/2+)
level_comment:
E an alternative value of 5171.6 is possible because the order of the 451|g-463|g cascade could not Be established in ({+40}Ca,3p2n|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J 13/2+ suggested by 2000Sc31 was based on the supposition that the 864.1|g seen in {+93}Pd |e decay is the same as the 865.9|g previously reported in the {+58}Ni({+40}Ca,3p2n|g) reaction by 1995Ro06. In {+94}Ag |ep decay, the latter line has E|g=866.0 {I1} and deexcites a (17/2+) 1719 level. The evaluator concludes that the 864.1|g from |e decay must be a different transition. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$recommended value obtained from the analysis of the shape of the peaks in the revolution time spectrum using exponentially modified Gaussian (EMG) function in 2023Xi01. 
J$based on the systematics of the J|p of the observed isomers in the neighboring isotopes and the isotones in 2023Xi01. The authors of 2023Xi01 states that the isomeric state is a proton-hole state. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: S
level_comment:
T$from 1980Ox01 
J$log| {Ift}=6.7 compared with calculated 6.39 from decay to (4+) in {+94}Ru (1996Jo06). However decay to (2+) in {+94}Ru log| {Ift}=6.7 is not predicted 


level_energy_unit: KEV
level_energy_info: ;OFF=X+0.0
level_spin_parity: (8+)
level_lifetime_unit: S
level_comment:
T$from 1980Ox01, other: 25 s {I2} (1980No06). 
J$log| {Ift}=5.3 to (8+); log| {Ift}=6.7 to (7-). No feeding to (6+). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_uncertain: ?
level_comment:
E$this level was proposed by 2012Na23 based on 798|g-1766|g-coincidence but the ordering of transitions in this cascade is tentative from shell-model calculations (2012Na23). Reverse ordering will give a level at 1821 keV 
J$shell-model predictions (2012Na23) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
J$from log| {Ift}=5.3 to 7/2(+), no direct feeding to 5/2+ ground state and log| {Ift}=5.8 to 9/2+, supported by comparison with the neighboring N=50 nuclei and Shell model calculations. 
T$from |g{-942}(t) of {+95}Ru (1975We03) 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$1/2-,3/2- from log| {Ift}=6.0 {I+6-4} to 1/2+ and log| {Ift}=4.8 {I+4-3} to (3/2-). 1/2 from shell model. 
%EC+%B+,%IT$from comparison of I|g(543|g) with intensities of |g's following |e decay of 543 state assuming mult(543|g)=M4. Other: %IT=85 from %I|g(543|g)=77 (1981Gr20) and |a(543|g)=0.102 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$by comparison of neighboring {+93}Tc (N=50) level scheme. Also, from the non observation of this non-yrast state in fusion evaporation reaction and in the |b{++} decay of the (21/2+) isomer in {+95}Pd Shell model predicts 7/2+ at 650 keV (2003Ba39). 


level_energy_unit: KEV
level_spin_parity: (15/2+,17/2+)
level_comment:
J$from 2003Ba39, possible L=0 proton emission to this state from the (8+) state in {+96}Ag 
E$according to 2003Ba39, this level could be identical to the 2067 keV level, though the assignment is not unique. 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_lifetime_unit: PS
level_comment:
T$from 1998Ju05; Other: 31 ps {i6} (RDDS 1980No06). Probably not corrected for side feeding. 
G$weighted average of two measurements, done with Fe- (1.28 {I19}) and Ni-hosts (0.69 {I14}) (1999Ju04) 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: PS
level_comment:
G$Weighted average of two measurements, done with Fe- (0.80 {I30}) and Ni-hosts (0.04 {I59}) (1999Ju04) 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
$I{-|e+|b+}|?20% from the intensity balance. However, this value is much larger than the systematic values for |DJ=4 and no parity change (4th forbidden non-unique). Such transitions typically have log| {Ift}>20 (1973Ra10) which translates into I{-|e+|b+}<1|*10{+-13}. The reason for this is a large number of unplaced gamma rays. 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_comment:
$I{-|e+|b+}=5.7% {i7} from the intensity balance. However, this value is much larger than systematic values for |DJ=2 and no parity change (2nd forbidden non-unique). Such transitions typically have log| {Ift}> 11 (1973Ra10) which translates into I{-|e+|b+}<1|*10{+-4}. The reason for this is a large number of unplaced gamma rays. 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_lifetime_unit: PS
level_comment:
G$weighted average of two measurements, done with Fe- (1.28 {I19}) and Ni-hosts (0.69 {I14}) (1999Ju04) 


level_energy_unit: KEV
level_spin_parity: (35/2+)
level_lifetime_unit: PS
level_comment:
G$Weighted average of two measurements, done with Fe- (0.33 {I15}) and Ni-hosts (0.67 {I27}) (1999Ju04) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: MIN
level_comment:
J$log| {Ift}=5.4 to 6+ and 5+ levels in {+96}Ru, M3 |g from 3+. 
T$from 1975Gu01. Others: 9.5 min {i3} (1971Do08), 9.25 min {i10} (1970As08) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$log| {Ift}=5.5 to 4+ and 5.6 to 2+ levels in {+96}Ru. 
T$from 1975Gu01 in IT decay. Other values: 1.45 min {i20} (1971Do08), 1.55 min {i15} (1970As08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$the relative order of |g's in the cascade 131.1|g-647.9|g is not established. If the 131.1|g is the lowest in this cascade, E(level)=256.7 instead of 773.5 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 30.3 min {I9} (1975Pl05), 31.1 min {I8} (1974Oh07), 30 min {I2} (1971Lo12) and 32 min {I2} (1962Ba28). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T$weighted average of 47.9 min {I6} (1975Pl05), 44.3 min {I8} (1974Oh07) and 40 min {I2} (1971Lo12). 
%EC+%B+$from {+97}Rh IT decay 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2)
level_comment:
J$log| {Ift}=5.76 {I19} (log| {If{+1u}t}=7.3) from (5/2+) {+97}Pd; |g to (7/2+) but not to 1/2- level; 5/2+ from ({+40}Ca,3p|g), (({+3}He,pn|g),(d,n|g)) 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_comment:
J$(17/2) from D(+Q) |g to (15/2)+ level; |p=(-) based on non observance of E2 |g from (21/2), 3056, to (17/2+), 1553 (1986Pi04, ({+40}Ca,3p|g)) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: MIN
level_comment:
J$log| {Ift}=5.4 to 2+ in {+98}Ru ({+98}Rh |e decay (8.72 min)), 112|g M1 from 1+ and analogy with 2+ isomer in {+96}Rh. J=1 is not ruled out 
T$weighted average of 8.7 min {I1} (1956Ka25), 9.05 min {I30} (1970As08), 8.3 min {I2} (1972Ba37), 8.90 min {I15} (2001SeZY) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E$2014Ku04 in {+75}As({+28}Si,2p3n|g) point out that this (5+) level, most likely, is not the same as the 3.6-min isomer with J|p=(5+), however, evaluators assume here that the two levels are the same. This level is consistent with isomer energy E|<100 keV if mult(|g to g.s.)=M3. This isomer does not seem related to a 6-keV level quoted by 1974Si18 from an unpublished {+96}Ru(|a,pn|g) study, the details of which are not available and whose existence has not been confirmed in any of the later in-beam |g-ray studies. 2017Au03 suggest 60 keV {I50} from systematic trend. 
J$in analogy with (5+) isomers in {+96}Rh and {+100}Rh. J|p=5+ is consistent with evidence of |b{++},|e feeding (log| {Ift}|?5.6 in {+98}Rh |e decay (3.6 min)) to 4+ state in {+98}Ru 
T$weighted average of 3.6 min {I2} (1978Ki17), 3.5 min {I3} (1974Si18). Other: 3 min {I1} (1966At02). 
$%IT from 1978Ki17, deduced from intensities of |g lines in {+98}Ru associated with the decays of the 3.6-min isomer and the 8.72-min ground state. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
$Note that there is a large intensity imbalance at this level in data from {+75}As({+28}Si,2p3n|g) reaction, on the basis of which 2014Ku04 suggest that this level is likely to be different from the one populated in {+98}Pd |e decay, where no intensity imbalance is found. 
J$M1 |g to (2)+ gives (1,2,3)+; no |b feeding from 0+ parent and absence of transitions from 1+ states favors 3+ 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$since ordering of 206-146 |g cascade is not established in 2014Ku04, this level is either at 194.0 or 254.9 keV 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$since ordering of 139-223 |g cascade is not established, this level is either at 271.9 or 187.5 keV 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
J$note that 227.1|g D (|DJ=1) to (5+) is inconsistent with the 117.0|g Q (|DJ=2) from (5+), which could indicate the placements of those related |g rays by 2014Ku04 in {+75}As({+28}Si,2p3n|g) are problematic, assuming the multipolarities are correct. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J$515.6|g D (|DJ=1) from (6-), assumed to be (E1) in 2014Ku04; 594.9|g D (|DJ=1) from (6+), assumed to be (M1) 


level_energy_unit: KEV
level_spin_parity: (7+)
level_comment:
J$841.6|g E2 to (5+) 
$Based on the detailed level scheme from their high-spin study, 2014Ku04 in {+75}As({+28}Si,2p3n|g) deduce that the 841|g feeds a level at E=56 keV with J|p=(5+) rather than the (2)+ ground state as proposed by 1983Be63 via (|a,pn|g) and (d,3n|g) and adopted in other high-spin studies, which results in a level at 841 with J|p=(4+). Note that the argument for the placement in 1983Be63 does not take into account that the 3.6-min isomer decays mostly to the g.s. by %IT=89. The evaluators have adopted the placement by 2014Ku04. 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
E$the ground state would not be seen as the 841|g proceeds to the isomer at 56 keV, according to the level scheme given in the Adopted dataset 
J$from Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (7-)
level_comment:
J$(11+) in Adopted Levels. 1998Ch04 assigned (7-) based on the argument that the estimated partial lifetime (about 2 ps) for 1407 transition was found to be two orders of magnitude higher than the Weisskopf estimate for M1 transition and therefore was too large to be for M1 but possible for E1 transition. However, the assignment of Mult=E1 but not M1 cannot be justified by this argument in evaluators' point of view. 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$Hauser-Feshbach analysis suggests J=3+ (1970As08), but this is inconsistent with M1 |g from 1+ (112 level) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
$Level proposed by 1994SiZZ, but none of the |g rays given by 1993ViZZ fits this level. This level is not included in the Adopted dataset. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
E,J$2014Ku04 state that the 3.6-min isomer with J|p=(5+) but unknown excitation energy is not populated in their study and therefore point out that this 5+ level at E=56 keV seen in their study, most likely, is not the same as the 3.6-min isomer. However, evaluators assume in Adopted Levels that the two levels are the same. See comments for this level in Adopted Levels. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$since ordering of 206-146 |g cascade is not established, this level is either at 194.0 or 254.9 keV 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
E$this level is based on the placement of 841|g to the 56, 5+ level proposed in 2014Ku04, while the 841|g has been placed to the (2)+ ground state in previous |g-spectroscopy studies, resulting in a different level scheme from that proposed by 2014Ku04, with the latter adopted by the evaluators in Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_comment:
J from syst. log| {Ift}=7.1 to 1/2+. No |g from 9/2+ 
T from 1974An23. Other: 16.1 d (1959To25), 16 d {I1} (1956Hi32), 15.0 d {I2} (1955Fa12). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
%IT Deduced from B(M4)(W.u.)<30 (RUL). 
MOMM1 From NMR on oriented nuclei. {+99}Rh implanted in iron (1985Ed06); Other values: 5.62 {i6} from NMR on oriented nuclei (2005St24,1995Se20); 5.666 {I14} from NMR on oriented nuclei (1986Ni02) 
J J measured by atomic beam magnetic resonance method (1975Ru06,1978Ru04,2013Ma15). log| {Ift}=5.2 to |p=+ 
T from 1956Ka25. 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J log| {Ift}=5.6 from (5/2)+; M1,E2 |g to 9/2+. 7/2 slightly favored by excitation functions in (p,n|g). 


level_energy_unit: KEV
level_comment:
E$9686 listed in table 1 and figure 1 of 2014Ku20 is a misprint if E|g=1256 keV from this level is correct 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: H
level_comment:
J$spin from atomic-beam method (1975Ru06,1978Ru04) and parity from M1(84.02|g)-E1(74.78|g) cascade from 1+, 158 level 
$Proposed configuration=|p(g{-9/2}{+4},p{-1/2}){-1/2-} ~# |n(d{-5/2},s{-1/2}){-1/2+ or 3/2+} (1965Ev05) 
T$unweighted average of 20.2 h {I1} from 1995KeZZ and 20.8 h {I1} from 1953Ma64. Others: 18 h {I1} (1964An13), 21 h (1950Su29), 19.4 h 1(1948Li03) 
T$note that 1995KeZZ give 20.20 h {I5} in Table 5.2 but 20.2 h {I1} in both their abstract and the conclusion. The evaluators have therefore adopted 20.2 h {I}. 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: NS
level_comment:
J$E1 126.1|g from 1+; M1+E2 32.68|g to 1-. Probable E3 |g from (5+) (see comment for 107.6 isomer). Absence of |e feeding from 0+ suggests J>1 
$Proposed configuration=|p(g{-9/2}{+4},p{-1/2}){-1/2-} ~# |n(d{-5/2},s{-1/2}){-3/2+ or 5/2+} (1965Ev05) 
T$from |g|g(t) in {+100}Pd |e decay (1979En03). Other: 25.3 ns {I31} from |g(t) in (p,n|g) (1983Bi04) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
J$M1 84.0|g from 1+. (84.0|g)(74.8|g)(|q) in {+100}Pd |e decay rules out J=0 and favors J=2 over J=1. 
$Proposed configuration=|p(g{-9/2}{+5}){-9/2+} ~# |n(d{-5/2},s{-1/2}){-5/2+} and/or |p(g{-9/2}{+5}){-7/2+} ~# |n(d{-5/2},s{-1/2}){-3/2+} (1965Ev05). From measured magnetic moment, 1965Ma34 support the second configuration 
T$weighted average of 217 ns {I5} from |g(t) (1983Bi04) in (p,n|g), 213.6 ns {I20} (1979En03) and 214.5 ns {I20} (1971Re06) from |g(t) in {+100}Pd |e decay. Others (discrepant): 235 ns {I3} (1965Ma34) and 180 ns {I20} (1965Ev05) in {+100}Pd |e decay. 1983Bi04 use |g(t) in (p,n|g), all other references use |g|g(t) in {+100}Pd |e decay 
MOMM1$from g factor measurement using |g|g(|q,H,t) in {+100}Pd |e decay with a Knight-shift correction (1966Ma54; value is 4.26 {I6} in 1965Ma34). 2014StZZ compilation quotes +4.324 {I8}. Other: 4.304 {I30} (1971Re06) 
MOME2$perturbed angular correlation (cited as 0.153 in theory paper by 1996Bl15 from their paper to appear, yet no further publication seems to have appeared). 2008Py02 use the same value of 0.153. Uncertainty of 0.018 seems to be assigned by 2016St14. Other: Q=0.076 {I20} (1979Vi12), estimated value from a comparison of quadrupole interaction frequencies in {+100}Rh and {+99}Ru, using Q=0.23 {I5} for a 99-keV level in {+99}Ru 


level_energy_unit: KEV
level_spin_parity: (1,2)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$53.7|g (2)- and 86.3|g to 1- are not E2 (from RUL); log| {Ift}>7.8 from 0+ suggests J>1. Negative parity proposed by 1983Bi04 based on lifetime estimates 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M2
level_comment:
E$from the 74.9|g-32.7|g cascade in {+100}Rh IT decay, although, the decay scheme of the isomer does not seem as well established. However, proposed 74.9-32.7 and 32.7-74.9 cascades as the main decay modes are consistent with mult=E3 and M3 for one of the components of 74.9|g and 32.7|g, respectively. Mult=E1 and M1+E2 for the second component of 74.9|g and 32.7|g, respectively are known from {+100}Pd |e decay 
J$probable E3-M1 cascade to 1-, systematics of odd-odd nuclei in this mass region. 
$Possible configuration=|p(g{-9/2}{+5}){-7/2+} ~# |n(d{-5/2},s{-1/2}){-3/2+}, based on similar configurations for other low-lying states proposed by 1965Ev05 
T$weighted average of 4.7 min {I3} (1974Si18), 4.8 min {I5} (1978Ki07), 4.5 min {I3} (1982MaZP), as also listed in {+100}Rh IT decay 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$log| {Ift}=4.4 from 0+ 
$Proposed configuration=|p(g{-9/2}{+5}){-7/2+} ~# |n(d{-5/2},s{-1/2}){-5/2+} (1965Ev05) 
T$other: <0.5 ns in |e decay (1979En03) 


level_energy_unit: KEV
level_spin_parity: (7+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M3
level_comment:
J$|DJ=2, E2 112.0|g to (5+) 
T$unweighted average of 120 ns {I5} (1984Ma30) in ({+6}Li,4n|g), 140 ns {I5} (1986Du04) in ({+7}Li,3n|g) and 135 ns {I20} (1984Ma30) in (|a,2np|g). Different charge states of this isomer were produced from the breakup of {+112}Sn nucleus in heavy-ion collisions (1995Gr14). Lifetime of the isomer in fully-ionized charge state is calculated to be 250 ns (1995Gr14) 
MOMM1$from g factor=+0.67 {I2} (1990Bi03) by PAD method using T{-1/2}=140 ns {I5} (1986Du04) in ({+7}Li,3n|g). Other: g factor=+0.69 {I6} with T{-1/2}=165 ns (1986RaZU) in ({+7}Li,3n|g) 
$Configuration=|pg{-9/2}~#|nd{-5/2} (1990Bi03) from comparison of measured g factor with model predicted values. Some admixture of Configuration=|pg{-9/2}~#|ng{-7/2} cannot be ruled out (1990Bi03) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=0, E1 383.2|g to (8+) and |DJ=1, E1 1050.9|g to (7+) 
T$from Doppler broadening of 1050|g peak (1984Ma30) in ({+6}Li,4n|g) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$Proposed configuration=|p(g{-9/2}{+4},p{-1/2}){-1/2-} ~# |n(d{-5/2},s{-1/2}){-1/2+ or 3/2+} (1965Ev05) 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: NS
level_comment:
T$|g|g(t) (1979En03) 
$Proposed configuration=|p(g{-9/2}{+4},p{-1/2}){-1/2-} ~# |n(d{-5/2},s{-1/2}){-3/2+ or 5/2+} (1965Ev05) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$values from this dataset: 213.6 ns {I20} (1979En03), 214.5 ns {I20} (1971Re06), 235 ns {I3} (1965Ma34), 180 ns {I20} (1965Ev05) 
J$(84|g)(75|g)(|q) rules out J=0 and favors J=2 over J=1 
$g factor: from |g|g(|q,H,t). Other: 2.152 {I15} (1971Re06) 
$Q=0.076 {I20} (1979Vi12), an estimated value from a comparison of quadrupole interaction frequencies in {+100}Rh and {+99}Ru, using Q=0.23 {I5} for a 99-keV level in {+99}Ru 
$Proposed configuration=|p(g{-9/2}{+5}){-9/2+} ~# |n(d{-5/2},s{-1/2}){-5/2+} and/or |p(g{-9/2}{+5}){-7/2+} ~# |n(d{-5/2},s{-1/2}){-3/2+} (1965Ev05) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$other: <0.5 ns from |g|g(t) (1979En03) 
$Proposed configuration=|p(g{-9/2}{+5}){-7/2+} ~# |n(d{-5/2},s{-1/2}){-5/2+} (1965Ev05) 


level_energy_unit: KEV
level_spin_parity: (7+)
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) (1986Du04). Other: 165 ns (1986RaZU). 
$g factor from TDPAD method in 1990Bi03 using T{-1/2}=140 ns {I5} from 1986Du04. Other: +0.69 {I6}, with T{-1/2}=165 ns in 1986RaZU 
$Configuration=|pg{-9/2}~#|nd{-5/2} (1990Bi03) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: Y
level_comment:
T$from 1965Ev06 monoisotopic source. Others: 3.0 y {i4} (1965Hi07) mixed {+101}Rh+{+102}Rh source, 5 y {i1} (1955Fa12), 10 y {i3} (1960Pe05) 
J$L=0 (p,t) gives J=1/2- for {+103}Rh target 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
J$from atomic beam (1975Ru06), |p from M4 |g to 1/2- 
MOMM1$others: +5.472 {i14} (1986Ni02), +5.49 {i9} (1973Ka28), +5.475 {i12} (1985Ed06) 
T$from 1966Ar05. Others: 4.39 d {i8} (1968Li08), 4.43 d {i6} (1965Ev04), 4.7 d {i2} (1956Ka25). Others: 1948Li03, 1949Eg04, 1952Sc11, 1955Fa12 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
T$from 1970Va33 (ce)(ce)(t). Other: 1.77 ns {i5} (1974BeZJ) |g|g(t) 
J$M1 |g to 9/2+, log| {Ift}=5.5 from 5/2+ 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: PS
level_comment:
T$from 1970Va33 (ce)(ce)(t). Other: 66 ps {i10} (1974BeZJ) |g|g(t) 
J$M1+E2 |g to 7/2+. Excit function in (p,n|g) is consistent with J=5/2 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
T$from 1974BeZJ (K| x ray)(590|g)(t) 
J$M1 |g to 9/2+. log| {Ift}=5.6 from 5/2+, excit in (p,n|g) rule out J=5/2 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$Probably different from the 978 level. |s/|s(g.s.) is similar to that for the |s(1130,0+)/|s(g.s.,0+)in {+102}Ru (p,t), suggesting that is the 1/2- state expected from coupling with the excited 0+ in the core (1975De19) 


level_energy_unit: KEV
level_spin_parity: 5/2+,7/2+
level_comment:
E$1813 keV in (p,t) may correspond 
J$from |g decays to 5/2+ and 9/2+ states, log| {Ift}=5.8 from 5/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
T 4.34 d {i1} (1966Ar05), 4.39 d {i8} (1968Li08), 4.43 d {i6} (1965Ev04). Others: 1948Li03, 1952Sc11, 1956Ka25 
g-factor=+1.22 {i2} (1973Ka28); fits empirical g-factor syst of regional g9/2 proton states 


level_energy_unit: KEV
level_comment:
$d|s/d|W=3.4 
E$author's value of 966 in Table I is a misprint, see Fig.1 
J$|s(1058)/|s(996) suggests J(996)=3/2, J(1058)=5/2 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: Y
level_comment:
T$Determined relative to T{-1/2}=3.742 y {I10} of {+102m}Rh. |g-ray net peak area ratios of 127-, 198-, and 325-keV from {+101}Rh{+g} over 696-keV from {+102}Rh{+m} were used to obtain effective "growth rates" of {+101g}Rh activity. Finally using the combined growth rate of 0.014928 y {I2033} from three ratio vs. time data fits and {+102}Rh{+m} half-life, {+101}Rh{+g} half-life was determined. Reported uncertainty includes statistical and systematic contributions. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$|s(mb/sr)=1.77 {I9} (at 6|'), 1.33 {I7} (at 10|'), 0.459 {I23} (at 14|'), 0.648 {I33} (at 18|'), 0.533 {I27} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.187 {I10} (at 6|'), 0.374 {I19} (at 10|'), 0.651 {I33} (at 14|'), 0.90 {I5} (at 18|'), 0.670 {I34} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|s(mb/sr)=0.655 {I33} (at 6|'), 0.497 {I25} (at 10|'), 0.159 {I8} (at 14|'), 0.197 {I10} (at 18|'), 0.177 {I9} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|s(mb/sr)=0.0128 {I11} (at 6|'), 0.0260 {I17} (at 10|'), 0.0277 {I17} (at 14|'), 0.0170 {I13} (at 18|'), 0.0177 {I13} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.70 {I4} (at 6|'), 0.94 {I5} (at 10|'), 0.583 {I29} (at 14|'), 0.296 {I15} (at 18|'), 0.353 {I18} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|s(mb/sr)=0.78 {I4} (at 6|'), 0.687 {I35} (at 10|'), 0.231 {I12} (at 14|'), 0.306 {I16} (at 18|'), 0.267 {I14} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|s(mb/sr)=0.038 {I5} (at 6|'), 0.082 {I5} (at 10|'), 0.098 {I5} (at 14|'), 0.089 {I5} (at 18|'), 0.0420 {I23} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0130 {I12} (at 6|'), 0.0200 {I14} (at 10|'), 0.0290 {I18} (at 14|'), 0.034 {I2} (at 18|'), 0.0232 {I15} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.434 {I22} (at 6|'), 0.559 {I29} (at 10|'), 0.334 {I17} (at 14|'), 0.170 {I9} (at 18|'), 0.188 {I10} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.642 {I32} (at 6|'), 0.431 {I22} (at 10|'), 0.609 {I31} (at 14|'), 0.295 {I15} (at 18|'), 0.217 {I11} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.116 {I6} (at 6|'), 0.105 {I6} (at 10|'), 0.071 {I4} (at 14|'), 0.087 {I5} (at 18|'), 0.076 {I4} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0270 {I24} (at 6|'), 0.0370 {I27} (at 10|'), 0.0200 {I14} (at 14|'), 0.0200 {I14} (at 18|'), 0.0185 {I13} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.588 {I30} (at 6|'), 0.77 {I4} (at 10|'), 0.455 {I23} (at 14|'), 0.252 {I13} (at 18|'), 0.275 {I14} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0540 {I29} (at 6|'), 0.0390 {I28} (at 10|'), 0.0148 {I11} (at 14|'), 0.0206 {I14} (at 18|'), 0.0185 {I12} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.268 {I14} (at 6|'), 0.183 {I10} (at 10|'), 0.274 {I14} (at 14|'), 0.152 {I8} (at 18|'), 0.115 {I6} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=1.32 {I7} (at 6|'), 1.75 {I9} (at 10|'), 1.03 {I5} (at 14|'), 0.558 {I28} (at 18|'), 0.628 {I32} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.586 {I30} (at 6|'), 0.78 {I4} (at 10|'), 0.406 {I21} (at 14|'), 0.239 {I12} (at 18|'), 0.262 {I14} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.311 {I16} (at 6|'), 0.168 {I10} (at 10|'), 0.295 {I15} (at 14|'), 0.147 {I8} (at 18|'), 0.099 {I6} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.262 {I14} (at 6|'), 0.320 {I17} (at 10|'), 0.161 {I8} (at 14|'), 0.103 {I6} (at 18|'), 0.110 {I6} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.107 {I6} (at 6|'), 0.118 {I7} (at 10|'), 0.0660 {I35} (at 14|'), 0.0330 {I19} (at 18|'), 0.035 {I2} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.149 {I9} (at 6|'), 0.199 {I11} (at 10|'), 0.124 {I7} (at 14|'), 0.095 {I6} (at 18|'), 0.092 {I5} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.057 {I4} (at 6|'), 0.082 {I7} (at 10|'), 0.0430 {I29} (at 14|'), 0.0290 {I25} (at 18|'), 0.0310 {I25} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.060 {I4} (at 6|'), 0.105 {I8} (at 10|'), 0.070 {I4} (at 14|'), 0.053 {I4} (at 18|'), 0.0400 {I28} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0330 {I26} (at 6|'), 0.058 {I7} (at 10|'), 0.0240 {I23} (at 14|'), 0.0170 {I22} (at 18|'), 0.0170 {I22} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.099 {I5} (at 6|'), 0.106 {I7} (at 10|'), 0.077 {I4} (at 14|'), 0.044 {I3} (at 18|'), 0.0382 {I21} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.103 {I6} (at 6|'), 0.071 {I5} (at 10|'), 0.142 {I7} (at 14|'), 0.089 {I5} (at 18|'), 0.0550 {I29} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.230 {I12} (at 6|'), 0.284 {I15} (at 10|'), 0.195 {I10} (at 14|'), 0.116 {I7} (at 18|'), 0.114 {I6} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.128 {I8} (at 6|'), 0.146 {I8} (at 10|'), 0.093 {I5} (at 14|'), 0.0530 {I33} (at 18|'), 0.0530 {I33} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.087 {I5} (at 6|'), 0.084 {I5} (at 10|'), 0.091 {I5} (at 14|'), 0.060 {I4} (at 18|'), 0.0460 {I25} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.082 {I5} (at 6|'), 0.099 {I6} (at 10|'), 0.101 {I6} (at 14|'), 0.080 {I5} (at 18|'), 0.0620 {I33} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.094 {I5} (at 6|'), 0.111 {I6} (at 10|'), 0.078 {I4} (at 14|'), 0.0460 {I25} (at 18|'), 0.0450 {I25} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.158 {I8} (at 6|'), 0.195 {I10} (at 10|'), 0.117 {I6} (at 14|'), 0.061 {I4} (at 18|'), 0.073 {I4} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0320 {I26} (at 6|'), 0.044 {I3} (at 10|'), 0.0310 {I19} (at 14|'), 0.0130 {I12} (at 18|'), 0.0190 {I14} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0400 {I28} (at 6|'), 0.0470 {I31} (at 10|'), 0.0250 {I16} (at 14|'), 0.0060 {I11} (at 18|'), 0.0160 {I13} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0270 {I17} (at 6|'), 0.0340 {I26} (at 10|'), 0.0270 {I17} (at 14|'), 0.0120 {I21} (at 18|'), 0.0160 {I13} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0540 {I34} (at 6|'), 0.074 {I5} (at 10|'), 0.0420 {I23} (at 14|'), 0.0260 {I24} (at 18|'), 0.0300 {I18} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0360 {I27} (at 6|'), 0.042 {I4} (at 10|'), 0.0270 {I17} (at 14|'), 0.0180 {I22} (at 18|'), 0.0170 {I13} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0380 {I28} (at 6|'), 0.0470 {I31} (at 10|'), 0.0290 {I18} (at 14|'), 0.0180 {I14} (at 18|'), 0.0200 {I14} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0500 {I32} (at 6|'), 0.068 {I5} (at 10|'), 0.0420 {I29} (at 14|'), 0.0220 {I15} (at 18|'), 0.0260 {I17} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.129 {I7} (at 6|'), 0.162 {I9} (at 10|'), 0.110 {I6} (at 14|'), 0.061 {I4} (at 18|'), 0.0610 {I32} (at 22|') 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_lifetime_unit: D
level_comment:
MOMM1 From nuclear orientation (1989Ra17) 
T From |g decay following |b decay (1998Sh21). Others: 210 d {i6} (1941Mi02), 206 d {i3} (1961Hi06), 205 d {i10} (1961Mc10) 
J |g(|q,H,t) in {+102}Rh |e decay (207 d) and shell model suggest J|p=2- 


level_energy_unit: KEV
level_spin_parity: 6(+)
level_lifetime_unit: Y
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1 From 1989Ra17 
%IT from 1991Bi01 
T from 1998Sh21. Others 2.9 y 1963Bo17,1965Hi07 
J$J=6 from low-temperature nuclear orientation and NMR (1989Hi12). |p=+ is expected from shell model and Rh systematics 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$<r{+2}>{+1/2}=4.4942 fm {i23} (2004An14, evaluation) 
J=1/2 (optical spectroscopy) (1976Fu06) 
|p: - from |m (exp vs theory) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted av: 56.12 min {I1} (1973Gu06), 56.114 min {I20} (1981Va11); others: 1944Fl01, 1945Wi03, 1947Fl03, 1950Me26, 1957Jo19, 1967VuZZ, 1969KoZW, 1972Pa10, 1974Sa15, 1978La21 
J E3 transition to g.s. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
T$From {+103}Rh |b{+-} decay.Weighted av: 1.06 ns {I5} (1973Ba52), 1.13 ns {I3} (1972Ja01) and 1.13 ns {I7} (1972Ja01) 
J M1 decay to 7/2+ state, and |m (exp vs calc) (1973Ba52) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$From B(E2) in Coul. ex. 
MOME2$other: -0.32 {I20} (1989Ra17) 
MOMM1$other: +0.69 {I12} (1988Be45) 
J M1+E2 |g decay to g.s. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$From B(E2) in Coul. ex. 
MOME2$Other -0.41 {I18} (1989Ra17) 
MOMM1$others: +1.08 {I8}, +0.93 {I20} (1989Ra17,1988Be45) 
J from 357|g(|q); |g decays: E2 to 1/2-, M1 to 3/2- 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T from centroid-shift analysis of (225|b)(497|g)(t) calibrated with {+60}Co,{+198}Au sources (1968Ra06); others: 1953En06, 1969Be81, 1970Be10 
J$E1 |g to 3/2-, M1+E2 |g to 7/2+ 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_comment:
J from 564|g excit and |g(|q) in {+100}Mo({+6}Li,3n|g) and 564|g(|q) and linear pol measurements in {+100}Mo({+7}Li,4n|g) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
T from {+103}Rh(|g,|g') if J=1/2 and adopted branching (1981Ca10) 
J$J=1/2 from |g(|q) |g to 5/2- gives |p=- 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
J from |g excit and |g(|q) in {+100}Mo({+6}Li,3n|g) and |g(|q) and pol measurements in {+100}Mo({+7}Li,4n|g). |DJ=1 transition to 11/2+ and E2 to 9/2+ states 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J based on |g(|q), excit, |g decay to 3/2- and 5/2- states 
T from 1972SiZO (DSA method). Other: 1.7 ps (1972SiZO) via (B(E2); 3/2- to 7/2-)=0.29, I(553|g) branching=22% 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
BE2 Others: 0.0117 {I15} (1972SiZO), 0.0133 (1969Bl04) 
T via B(E2)=0.0131 (1972Sa03) and I|g(880)-branching=9% 
J based on 585|g(|q) Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
$B(E2)(From (9/2- to 5/2-)=0.178 {I9} 
T$From B(E2)(9/2- to 5/2-) in Coul. ex. 
J$based on 562|g(|q) Coul. ex., and excit, band member 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$ From B(E2)=0.0132 {I12} in Coul. ex. Other: 0.60 ps 10 from {+103}Rh(|g,|g') (1981Ca10). 
J from M1+E2 to 1/2- 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_comment:
J from 717|g(|q) in {+100}Mo({+6}Li,3n) and {+100}Mo({+7}Li,4n). E2 transition to 9/2- state and band structure 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_comment:
J from 895|g(|q) in {+100}Mo({+6}Li,3n|g) and {+100}Mo({+7}Li,4n|g). E2 transition to 13/2+ level and band structure 


level_energy_unit: KEV
level_spin_parity: 23/2-
level_comment:
J$ 260|g is D from 260|g(|q) in {+94}Zr({+12}C,p2n|g). M1 from observed |DJ=1 band structure transition to 21/2- state 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_comment:
J$from |g(|q) and band member 
$Interpreted in {+100}Mo({+6}Li,3n|g), ({+7}Li,4n|g) as member of a band based on the 21/2+ state with |DI=1 


level_energy_unit: KEV
level_spin_parity: 25/2-
level_comment:
J$from |g(|q) and band member 
J$D from 315|g(|q) in {+94}Zr({+12}C,p2n|g). M1 from observed |DJ=1 band structure to (23/2)- 


level_energy_unit: KEV
level_spin_parity: 29/2+
level_comment:
J$from |g(|q) and band member. 
$ Based on {+100}Mo({+6}Li,3n|g), ({+7}Li,4n|g) results evaluator interpret this level as being member of the |pg{-9/2}, |a=+1/2 band 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
T weighted average: 1.06 ns {I5} (1973Ba52) via (557|g)(53|g)(t), 1.13 ns {I3} (1972Ja01) via (553|g+444|g)(53|g)(t), 1.13 ns {I7} (1972Ja01) via (70-150|b)(ce(K) 53|g)(t) 
T others: 1958Fl40, 1969Zo02, 1970Be10, 1978BeYS 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T from |g(t) (1981Va11) 
T see also 1944Fl01, 1945Wi03, 1947Fl03, 1950Me26, 1957Jo19, 1967VuZZ, 1969KoZW, 1972Pa10, 1973Gu06, 1974Sa15, 1978La21 
%IT=100 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
E$From Adopted levels 
T$From 1981Ca10, if J|p=3/2 is assumed 
|G{-0}=1.30 {I13} 
$Based on |G{-0}/|G = 0.75 from Table of Isotopes: R.B.Firestone and V.S. Shirley (Wiley, New York, 1996) Vol.1. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$From B(E2)=216 {I6} 
BE2$weighted av: 0.228 {I14} (1970GrYS), 0.245 {I18} (1972Sa03). 0.22 {I1} (1988Ta23), 0.209 {I15} (1958Mc02,1969Bl04) 0.198 {I11} (1970GrYR) and 0.213 {I16} (1972SiZO) 
G$others: g=0.68 {I17} (1971SpZT), 0.70 {I21} (1973MiZC) if T{-1/2}=6.7 ps. Others: 1971BhZV, 1972Sz03, 1974HeYO 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$From B(E2) 
BE2$Weighted average of 0.358 {i14} (1970GrYS), 0.326 {I29} (1974Mi02) 0.343 {I13} (1989Lo08), 0.334 {I35} (1970GrYR) 
G$others: g=0.42 {I6} (1974HeYO), 0.4 {I1} {I14} (1973MiZC), 0.44 {I2} (1972Sz03), 0.39 {I7} (1971BhZV), 0.47 {I10} (1971SpZT); T{-1/2}=73 ps assumed 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
T from 1972SiZO (DSA method). Other: 1.7 ps (1972SiZO) via B(E2) (3/2- to 7/2-)=0.29, I(553|g)-branching=22% 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T via B(E2) (1972Sa03) 
J$J=5/2 from |g(|q) (1972Sa03) 
BE2$others: 0.0117 {I15} (1972SiZO), 0.0133 (1969Bl04), 0.0132 {I16} (1988Ta23) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
T$From B(E2)(9/2- to 5/2-) 
$B(E2)(From (9/2- to 5/2-)=0.178 {I9} B(E2) is weighted average of 0.178 {I15} (1989Lo08); 0.181 {I15} (1972Sa03) 0.175 {I2} (1972SiZO); Other: 0.144 {I16} (1972SiZO) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J$J=5/2 from |g(|q) (1988Ta23) 
BE2$From 1972Sa03 for adopted branching %I|g(749|g)=52 {I5}. Others: B(E2)=0.0032 {I4} (1988Ta23), 0.8 (1971GrXO) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T from B(E2)=0.0132 {I12} (1972Sa03) and |d(1277|g)=-0.62 {I30} 
BE2$for adopted branching %I|g (1277|g)=75.2 {I23}. Other: B(E2)=0.040 {I6} (1988Ta23) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$|s(mb/sr)=1.79 {I9} (at 6|'), 1.27 {I6} (at 10|'), 0.434 {I22} (at 14|'), 0.611 {I31} (at 18|'), 0.470 {I24} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.121 {I6} (at 6|'), 0.265 {I14} (at 10|'), 0.499 {I25} (at 14|'), 0.669 {I34} (at 18|'), 0.475 {I24} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|s(mb/sr)=0.84 {I4} (at 6|'), 0.630 {I32} (at 10|'), 0.210 {I11} (at 14|'), 0.274 {I14} (at 18|'), 0.232 {I12} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|s(mb/sr)=0.0090 {I21} (at 6|'), 0.0300 {I18} (at 10|'), 0.0387 {I21} (at 14|'), 0.0367 {I21} (at 18|'), 0.0199 {I12} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.595 {I30} (at 6|'), 0.83 {I4} (at 10|'), 0.519 {I26} (at 14|'), 0.245 {I13} (at 18|'), 0.299 {I15} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$|s(mb/sr)=0.79 {I4} (at 6|'), 0.586 {I30} (at 10|'), 0.206 {I11} (at 14|'), 0.264 {I13} (at 18|'), 0.224 {I11} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$|s(mb/sr)=0.0300 {I18} (at 6|'), 0.0250 {I16} (at 10|'), 0.0150 {I13} (at 14|'), 0.0170 {I13} (at 18|'), 0.0140 {I12} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|s(mb/sr)=0.0440 {I24} (at 6|'), 0.073 {I4} (at 10|'), 0.097 {I5} (at 14|'), 0.079 {I4} (at 18|'), 0.0410 {I23} (at 22|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.004 {I1} (at 6|'), 0.0060 {I11} (at 10|'), 0.003 {I1} (at 14|'), 0.003 {I1} (at 18|'), 0.002 {I1} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=1.73 {I9} (at 6|'), 1.51 {I8} (at 10|'), 1.43 {I7} (at 14|'), 0.643 {I33} (at 18|'), 0.632 {I32} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.597 {I30} (at 6|'), 0.72 {I4} (at 10|'), 0.424 {I21} (at 14|'), 0.225 {I12} (at 18|'), 0.247 {I13} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.441 {I23} (at 6|'), 0.561 {I29} (at 10|'), 0.343 {I17} (at 14|'), 0.185 {I10} (at 18|'), 0.194 {I10} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.092 {I5} (at 6|'), 0.079 {I5} (at 10|'), 0.083 {I5} (at 14|'), 0.0390 {I22} (at 18|'), 0.0400 {I28} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0220 {I15} (at 6|'), 0.0230 {I23} (at 10|'), 0.0570 {I35} (at 14|'), 0.081 {I5} (at 18|'), 0.0560 {I35} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0460 {I25} (at 6|'), 0.0370 {I27} (at 10|'), 0.0160 {I22} (at 14|'), 0.0190 {I22} (at 18|'), 0.0150 {I21} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.213 {I11} (at 6|'), 0.255 {I13} (at 10|'), 0.151 {I8} (at 14|'), 0.081 {I4} (at 18|'), 0.084 {I4} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.398 {I20} (at 6|'), 0.511 {I26} (at 10|'), 0.300 {I25} (at 14|'), 0.162 {I8} (at 18|'), 0.181 {I9} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.125 {I7} (at 6|'), 0.078 {I4} (at 10|'), 0.081 {I4} (at 14|'), 0.0490 {I27} (at 18|'), 0.0380 {I22} (at 22|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0090 {I21} (at 6|'), 0.0150 {I21} (at 10|'), 0.0260 {I24} (at 14|'), 0.0200 {I22} (at 18|'), 0.0200 {I14} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|s(mb/sr)=0.07 {I2} (at 6|'), 0.125 {I8} (at 10|'), 0.177 {I9} (at 14|'), 0.167 {I9} (at 18|'), 0.103 {I6} (at 22|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.007 {I2} (at 6|'), 0.0090 {I11} (at 10|'), 0.0160 {I13} (at 14|'), 0.0130 {I31} (at 18|'), 0.0090 {I21} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0360 {I21} (at 6|'), 0.0300 {I18} (at 10|'), 0.0100 {I11} (at 14|'), 0.0170 {I13} (at 18|'), 0.0140 {I12} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.056 {I3} (at 6|'), 0.071 {I4} (at 10|'), 0.0610 {I32} (at 14|'), 0.0540 {I29} (at 18|'), 0.0530 {I28} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0120 {I12} (at 6|'), 0.0070 {I11} (at 10|'), 0.0100 {I11} (at 14|'), 0.0080 {I11} (at 18|'), 0.005 {I1} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.087 {I5} (at 6|'), 0.127 {I7} (at 10|'), 0.086 {I5} (at 14|'), 0.0370 {I21} (at 18|'), 0.0420 {I23} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0270 {I24} (at 6|'), 0.0360 {I21} (at 10|'), 0.0224 {I14} (at 14|'), 0.0122 {I10} (at 18|'), 0.0148 {I11} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.142 {I7} (at 6|'), 0.175 {I9} (at 10|'), 0.118 {I6} (at 14|'), 0.0600 {I32} (at 18|'), 0.0650 {I34} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0250 {I16} (at 6|'), 0.0140 {I12} (at 10|'), 0.0318 {I18} (at 14|'), 0.0273 {I16} (at 18|'), 0.0273 {I16} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.177 {I9} (at 6|'), 0.227 {I12} (at 10|'), 0.146 {I8} (at 14|'), 0.076 {I4} (at 18|'), 0.085 {I4} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0420 {I29} (at 6|'), 0.0570 {I35} (at 10|'), 0.0380 {I22} (at 14|'), 0.0190 {I14} (at 18|'), 0.0190 {I14} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0550 {I34} (at 6|'), 0.066 {I4} (at 10|'), 0.0440 {I24} (at 14|'), 0.0330 {I19} (at 18|'), 0.0270 {I17} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0330 {I26} (at 6|'), 0.0370 {I27} (at 10|'), 0.0280 {I17} (at 14|'), 0.0120 {I12} (at 18|'), 0.0120 {I12} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0210 {I23} (at 6|'), 0.0240 {I23} (at 10|'), 0.0100 {I11} (at 14|'), 0.0066 {I10} (at 18|'), 0.006 {I1} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.459 {I23} (at 6|'), 0.396 {I20} (at 10|'), 0.414 {I21} (at 14|'), 0.184 {I10} (at 18|'), 0.169 {I9} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0350 {I27} (at 6|'), 0.0360 {I35} (at 10|'), 0.0330 {I34} (at 14|'), 0.0080 {I11} (at 18|'), 0.0110 {I21} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.058 {I4} (at 6|'), 0.071 {I5} (at 10|'), 0.0410 {I29} (at 14|'), 0.0310 {I34} (at 18|'), 0.0330 {I34} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.066 {I4} (at 6|'), 0.065 {I4} (at 10|'), 0.0630 {I33} (at 14|'), 0.034 {I2} (at 18|'), 0.0320 {I19} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.078 {I5} (at 6|'), 0.091 {I6} (at 10|'), 0.067 {I4} (at 14|'), 0.035 {I2} (at 18|'), 0.0390 {I22} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0380 {I28} (at 6|'), 0.0320 {I26} (at 10|'), 0.034 {I2} (at 14|'), 0.0190 {I14} (at 18|'), 0.0151 {I12} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.107 {I6} (at 6|'), 0.137 {I8} (at 10|'), 0.103 {I6} (at 14|'), 0.056 {I3} (at 18|'), 0.0590 {I31} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.066 {I4} (at 6|'), 0.077 {I4} (at 10|'), 0.0580 {I31} (at 14|'), 0.0370 {I21} (at 18|'), 0.0400 {I22} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0530 {I33} (at 6|'), 0.0350 {I27} (at 10|'), 0.070 {I4} (at 14|'), 0.0460 {I25} (at 18|'), 0.034 {I2} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0250 {I33} (at 6|'), 0.0290 {I25} (at 10|'), 0.0260 {I17} (at 14|'), 0.0260 {I17} (at 18|'), 0.0190 {I14} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0340 {I26} (at 6|'), 0.045 {I3} (at 10|'), 0.0320 {I19} (at 14|'), 0.0200 {I14} (at 18|'), 0.0210 {I15} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.084 {I5} (at 6|'), 0.100 {I31} (at 10|'), 0.0650 {I34} (at 14|'), 0.034 {I2} (at 18|'), 0.0370 {I21} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.075 {I4} (at 6|'), 0.082 {I5} (at 10|'), 0.0610 {I32} (at 14|'), 0.0290 {I18} (at 18|'), 0.0320 {I19} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0240 {I23} (at 6|'), 0.0300 {I25} (at 10|'), 0.0190 {I14} (at 14|'), 0.0160 {I22} (at 18|'), 0.0135 {I11} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.078 {I4} (at 6|'), 0.102 {I6} (at 10|'), 0.0580 {I31} (at 14|'), 0.0370 {I27} (at 18|'), 0.0390 {I22} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0520 {I33} (at 6|'), 0.0570 {I35} (at 10|'), 0.0400 {I22} (at 14|'), 0.0250 {I16} (at 18|'), 0.0150 {I11} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.071 {I5} (at 6|'), 0.108 {I7} (at 10|'), 0.0630 {I33} (at 14|'), 0.044 {I3} (at 18|'), 0.0410 {I29} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.051 {I6} (at 6|'), 0.044 {I5} (at 10|'), 0.0540 {I29} (at 14|'), 0.0300 {I25} (at 18|'), 0.0210 {I23} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.051 {I5} (at 6|'), 0.064 {I5} (at 10|'), 0.0420 {I23} (at 14|'), 0.0230 {I23} (at 18|'), 0.0290 {I25} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.093 {I5} (at 6|'), 0.087 {I5} (at 10|'), 0.074 {I4} (at 14|'), 0.0390 {I22} (at 18|'), 0.0380 {I22} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.224 {I12} (at 6|'), 0.266 {I14} (at 10|'), 0.174 {I9} (at 14|'), 0.088 {I5} (at 18|'), 0.093 {I5} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.089 {I5} (at 6|'), 0.109 {I6} (at 10|'), 0.068 {I4} (at 14|'), 0.0350 {I27} (at 18|'), 0.034 {I2} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.077 {I6} (at 6|'), 0.090 {I11} (at 10|'), 0.049 {I8} (at 14|'), 0.0240 {I32} (at 18|'), 0.0250 {I33} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.068 {I5} (at 6|'), 0.110 {I8} (at 10|'), 0.096 {I6} (at 14|'), 0.050 {I4} (at 18|'), 0.039 {I5} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.055 {I4} (at 6|'), 0.083 {I7} (at 10|'), 0.064 {I4} (at 14|'), 0.050 {I4} (at 18|'), 0.053 {I6} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.051 {I4} (at 6|'), 0.071 {I5} (at 10|'), 0.053 {I4} (at 14|'), 0.0360 {I35} (at 18|'), 0.025 {I4} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
T$weighted average of: 41.8 s {I7} (1939Cr03), 42.8 s {I5} (1963Cs01), 41.7 s {I7} (1966Wa11) 
J from log| {Ift}=4.55 to 0+ 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) in {+103}Rh(n,|g) (1961Du05) 
J$E3-E1 and M3=M1 cascades from the 128 level to the 1+ g.s. along with T{-1/2} (128 level) uniquely yield J|p(128 level)=5+, J|p(97 level)=2+, and J|p(51 level)=2- 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
J$see 51 level 
T$weighted average of: 4.37 min {I5} (1939Cr03), 4.41 min {I2} (1959El41), 4.29 min {I5} (1963Cs01), 4.28 min {I3} (1966Wa11) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: NS
level_comment:
T$from 1990Bi03. Other: 34.6 ns {I6} (1986KoZT) 
MOMM1$1.98 {I6} (1990Bi03) from TDPAD method 
J$E1 |g to 6+ with |D' J=0 and E1 |g to 5+ with |D' I=1. Configuration=((|p g{-9/2})(|n h{-11/2})) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: H
level_comment:
J$129.782|g E3 from 1/2-; {+106}Pd(t,|a)=4; systematics 
T$weighted average of 35.357 h {I37} and 35.319 h {I24} measured, at room temperature and 19 K in 2009Go29, 35.4 h {I1} in 1965Pi01, and 35.47 h {I8} in 1967Ko05; Other: 35.88 h {I2} in 1962Br15 
MOMM1$from NMR on oriented {+105}Rh in Fe and Ni (1985Ed06/1981Ha19); Others: 4.428~{I18} (1974WeYR), 4.61~{I16} (1976Ba39), 4.34~{I12} (1977Wi10) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$149.115|g M1+E2 to 7/2+; L({+3}He,d)=4, L(t,|a)=4 
T$|g-|g(t) in {+105}Ru |b{+-} decay (1972Ja01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$286.65|g to 5/2+, 316.496|g M1+E2 to 3/2+, 393.378|g E1 to 3/2-; L({+3}He,d) =0 
T$from |b-|g(t) in {+105}Ru |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$350.211|g E1 to 5/2-, 413.538|g E1 to 3/2-, 676.355|g E1 to 1//2-; L({+3}He,d)=2 
T$from |b-|g(t) in {+105}Ru |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$851.927|g 3/2+, 1172.37|g to 9/2+; 7/2+ ruled out by log| {Ift}=6.965~{I9} in {+105}Ru |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$700.98|g to 1/2+, 987.40|g to 5/2+, 1017.470|g (M1+E2) to 3/2+; L({+3}He,d)=2. However L({+3}He,d)=(3) can not be excluded 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2)
level_comment:
J$1228.73|g to 3/2+, 1698.167|g to 7/2+; log| {Ift}=6.276~{I20} in {+105}Ru |b{+-} decay rules out 7/2+ 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2)
level_comment:
J$1238.2|g to to 3/2+, 1708.7|g to 7/2+; log| {Ift}=7.38~{I5} in {+105}Ru |b{+-} decay rules out 7/2+ 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$1251.907|g to 3/2+, 1571|g to 9/2+; log| {Ift}=6.259~{I22} in {+105}Ru |b{+-} decay rules out 7/2+ 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_comment:
J$133.0|g M1 to 17/2-, 168.6|g M1(+E2) to 17/2-, 335.0|g M1 to 17/2-, 475.5|g to 15/2-; band member 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
T$from (1110|b)(676.4|g)(t) (1970Be79). 
J$J=3/2 as (350|g)(326|g)(|q) is consistent with 3/2(D)5/2(Q)1/2 and (413|g)(263|g)(|q) is consistent with 3/2(D)3/2(D,Q)1/2 (1979Sa23). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$If this level is identical with 1829-keV level observed in {+105}Ru |b{+-} decay with adopted J|p=(5/2,3/2+) then L=4 is excluded 


level_energy_unit: KEV
level_comment:
$Second component of assumed doublet to which L=(1) is assigned is considered as very doubtful by the evaluators 


level_energy_unit: KEV
level_comment:
L$if level is the same as 866-keV level observed in (t,|a) L assignment is in disagreement with adopted J|p 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
T From critical review of (2004Wo02). Others: 29.80 s (1969KoZW), 30.36 s {i15} (1966Mi10), 30 s (1950Gl05); see also 1946Se30, 1970RuZQ 
J log| {Ift}=4.31 from 0+ via 371.6-d {+106}Ru decay 
MOMM1 From NMR on oriented nuclei (1990Oh01). Others: from temperature dependence of nuclear orientation: 2.52 {I5} (1990Oh01), 3.07 {I9} (1977Ru08) 


level_energy_unit: KEV
level_spin_parity: (6)+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
For E|g=140, |a(M5)|?800, one gets B(M5)(W.u.)|?1.50|*10{+9}|*branching(IT). Branching(IT)|<7|*10{+-7} if B(M5)(W.u.)|<10 
E deduced from Q(|b{+-})(130-min {+106}Rh isomer)=3677 {I10} (1966De11) minus Q(|b{+-})(29.8-s {+106}Rh g.s.)=3541 {I6} (2003Au03) mass adjustment 
T weighted average of 130 min {I2} (1958Ma39) scin |g-decay curves, chem separated sources and 133 min {I4} (1960Se07). Others: 1955Ba20, 1955Ne03 
J from log| {Ift}=5.21 to 5+ and feeding of 6+ but not 4+ states in {+106}Pd 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: MIN
level_comment:
T$av: 23.0 min {I5} (1955Ba19), 21.7 min {I4} (1962Pi02), 20.5 min {I5} (1969WiZX) 303|g-decay curve. Others: 1943Bo03, 1955Ne03, 1969WiZX 
J|p: L(d,{+3}He)=4, J|p=9/2+ ruled out from analyzing power in (pol t,|a) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J$J|p=7/2+,9/2+ from L=4 in (d,{+3}He) and J|p=7/2+ ruled out by analyzing power data in (pol t,|a) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT
level_comment:
T$from |g|g(t) in {+107}Ru |b{+-} decay (1986Ka43) 
J J|p=1/2-,3/2- from L=1 in (d,{+3}He) and J|p=3/2- ruled out by analyzing power data in (pol t,|a) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) in {+107}Ru |b{+-} decay (1986Ka43) 
J$in (d,{+3}He) state at 386 keV is weakly excited with L=(1,2). Not observed in (pol t,|a). log| {Ift}>7.5; strong |g transition (E2) to J|p=7/2+ ground state and weak |g transition (E1) to 1/2- level together with an intense 10-keV (M1) |g feeding this level suggest J|p=(3/2+). This could be a possible candidate for the theoretically predicted J|p=3/2+ intruder state. This state should only be excited very weakly, if at all, in proton pickup reactions. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$in (d,{+3}He) a state at 386 keV is weakly excited with L=(1,2). Not observed in (t,|a). Strong 10.54-keV (E2) |g transition to (3/2+) points to similar character of both states. Could be the theoretically predicted J|p=1/2+ intruder state. The absence of a measurable |b branch to this level is in agreement with the J|p=(1/2+) assignment. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$|g transitions to 7/2+ and 1/2- states suggest 3/2+ or 5/2-. J|p=5/2- is less probable because this would imply that the 31.5 and 405.8 |g rays are both E1 transitions which are known to be strongly hindered in this mass region. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$J|p=3/2+,5/2+ from L=2 in (d,{+3}He) and L=(2) in (pol t,|a). J|p=3/2+ ruled out by analyzing power data in (pol t,|a) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$J|p=1/2- and 3/2- from L=1 in (d,{+3}He) and L=(1) in (pol t,|a). J|p=1/2- ruled out by analyzing power data in (pol t,|a) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$L=(1+3) from (d,{+3}He). Not observed in (pol t,|a). log| {Ift}=8.1 for the corresponding |b transition points to a first-forbidden transition. J|p=3/2-,5/2- are the most probable J|p values suggested from |g decay pattern. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$from L=1 in (d,{+3}He) and L=1 in (pol t,|a). J|p=1/2- ruled out by analyzing power data in (pol t,|a) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J$from L=3 in (d,{+3}He) and L=3 in (pol t,|a). J|p=7/2- ruled out by analyzing power data in (pol t,|a) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-,7/2-)
level_comment:
J from the log| {Ift}=8.2 value a negative parity for this level seems to be favored. |g decay to negative parity levels. 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
J$level must be different from those observed in {+108}Pd at 1006 keV and at 1001 keV with L=4 in {+108}Pd(d,{+3}He) |g's to 3/2- and 5/2- and forbidden log| {Ift} 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2+)
level_comment:
J from log| {Ift}=5.9 the corresponding |b transition seems to be allowed which implies J|p=3/2+,5/2+,7/2+ for this level. J|p=3/2+ is excluded but J|p=5/2+ is not 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2+)
level_comment:
J the relatively low value for the log| {Ift} value, namely 6.1, suggests an allowed |b transition. A |g to the 9/2+ state again excludes 3/2+. 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2+)
level_comment:
J$the relatively low value for the log| {Ift} value, namely 6.2, suggests an allowed |b transition. A |g to the 9/2+ state excludes 3/2+. Level at 1871 keV observed in (d,{+3}He) with L=(3) and level at 1865 keV in (pol t,|a) with L=1, are very probably not the same level as observed in |b decay. 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+,7/2+)
level_comment:
J the relatively low value for the log| {Ift} value, namely 6.0, suggests an allowed |b transition. From the |g decay pattern 3/2+ cannot be excluded. 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)+
level_comment:
J from the log| {Ift} value, namely 5.9, an allowed |b transition is most likely. A |g to the 9/2+ state again excludes 3/2+. 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+,7/2+)
level_comment:
J the relatively low value for the log| {Ift} value, namely 6.0, suggests an allowed |b transition. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
J$log| {Ift}=5.5 to 0+. 
T$from 1962Pi02. Others: 17 s {i1} (1976KaYO), 17 s {i1} (1978Fr16) 17.5 s (1958Ba02), 18 s {i1} (1955Ba19) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (5+)
level_lifetime_unit: MIN
level_comment:
E$1995Au04 give -60 {i110}; %|b{+-}: no it Decay branch observed 
J$log| {Ift}=6.6 to 6+ and log| {Ift}=6.6 to 1335 level. |p is from shell model 
T$from 1969Pi08. Other: 5.9 min {i2} (1984Bh02) 
E$x=115 {I18} (2012Au07) from mass measurement 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8-)
level_comment:
E$245-455 (2003Fo09) from systematics of 8- states in {+100}Rh, {+102}Rh and {+104}Rh; if 63|g taken from literature is non-existent 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_comment:
J$L(pol t,|a)=4 and L-1/2 from analyzing power fits 
T$weighted average of 80 s {i2} (using |b(t), 326.8|g(t), 426.1|g(t) in 1978Ka10), 79.8 s {i10} (using 178.0|g(t), 291.4|g(t), 326.7|g(t), 426.1|g(t) in 1978Fr16 1976KaYO), 82 s {i1} (using strong |g(t) in 1977Ba57), 81.2 s {i29} (using 326|g(t) in 1969WiZX); Other: 114 s (using 326|g(t) in 1975Fe12) 
CONF$K|p=7/2+, |p7/2[413] Nilsson orbital 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(pol t,|a)=4 and L+1/2 transfer from analyzing power fits; 206.29|g M1 to 7/2+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay); Other: < 0.5 ns using |b-206|g(t) in 1998Lh02 ({+109}Ru |b{+-} decay, centroid shift method) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: US
level_comment:
J$225.98|g E2 to 7/2+, 148.12|g from 1/2- 
T$from (116|g)(226|g)(t) in 1987Ka29 ({+109}Ru |b{+-} decay, slope method) 
CONF$K|p=1/2+, |p1/2[431] Nilsson orbital 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: NS
level_comment:
J$31.80|g M1+E2 to 3/2+, 220.64|g M1+E2 from 5/2+ 
T$from (221|g)(32|g)(t) in 1987Ka29 ({+109}Ru |b{+-} decay, slope method) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$358.79|g E2 to 7/2+, 101.1|g to 1/2+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay); Other: < 0.5 ns from |b-359|g(t) in 1998Lh02 ({+109}Ru |b{+-} decay, centroid shift method). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_comment:
J$L(pol t,|a)=1 and L-1/2 transfer from analyzing power fits 
T$weighted average of 33 ns {I2} from (194|g)(116|g)(t) in 1987Ka29 ({+109}Ru |b{+-} decay, slope method) and 34 ns {i2} from |b-374|g(t) in 1998Lh02 ({+109}Ru |b{+-} decay, slope method) 
CONF$K|p=1/2-, |p1/2[301] Nilsson orbital 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J$183.85|g E2 to 3/2+, 203.6|g to 9/2+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay); Other: 0.43 ns 23 from |b-183.85|g(t) in 1998Lh02 ({+109}Ru |b{+-} decay, centroid shift method) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,{+3}He)=2, L(pol t,|a)=(2) and L+1/2 transfer from analyzing power fits; 68.07|g M1 to 3/2+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay); Others: <0.5 ns 427|g(t) in 1998Lh02 ({+109}Ru |b{+-} decay, centroid shift) and 8 ns 1 in 1987Ka29 ({+109}Ru |b{+-} decay, close to timing resolution of Ge(Li) detectors). 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: PS
level_comment:
J$252.45|g to 3/2+ and 272.1|g to 9/2+, 220.64|g M1+E2 to (3/2)+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay); Other: <0.6 ns from |b-221|g(t) in 1998Lh02 ({+109}Ru |b{+-} decay, centroid shift method) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$L(pol t,|a)=(1) and L+1/2 transfer from analyzing power fit, L(d,{+3}He)=1; band assignment 
T$< 0.83 ps from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay), but B(M1)(W.u.)>3.4 exceeds RUL(IV)=3 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$55.01|g to 3/2-, 249.2|g to 1/2-; systematics and analogy of decay patterns with {+103,105,107}Rh. L=(1+3) in (d,{+3}He), but authors suggested that L=1 component is probably due to the tail of strong 540 peak; band assignment 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$245.09|g (E2) to 5/2+, 465.65|g to 9/2+; direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)). Note, that if 245.09|g is E1+M2, then J{+|p}=7/2- could be also consistent 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(pol t,|a)=L(d,{+3}He)=1 and L+1/2 transfer from analyzing power fits; 117.67|g to 5/2- and 366.81|g to 1/2- 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(pol t,|a)=(d,{+3}He)=3 and L-1/2 transfer from analyzing power fits, 482.0|g to 1/2-. 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$382.8|g to (5/2)+, 451.2|g to 7/2+, 860.09|g to 7/2+. Not populated in |b{+-} decay (J{+|p}=(5/2+)) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L(pol t,|a)=(3) and L-1/2 transfer from analyzing power fits, L(d,{+3}He)=3 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (1/2)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$239.90|g to 3/2-, 606.7|g to 1/2-, 621.9|g to 3/2+, no |g to J=5/2, 7/2 and 9/2 levels 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$L(d,{+3}He)=2 could correspond to both 1011 and 1026 level, 584.8|g to 5/2+, 1011.7|g to 7/2+, no |g to 9/2+ 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,{+3}He)=2 could correspond to both 1011 and 1026 level, 820.20|g to 9/2+, 800.5|g to 3/2+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2-)
level_lifetime_unit: PS
level_comment:
J$310.39|g to 3/2-, 677.2|g to 1/2-, 692.5|g to 3/2+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
J$L(pol t,|a)=L(d,{+3}He)=4 and L+1/2 transfer from analyzing power fits; 454.6|g to (11/2+), 1096.30|g to 7/2+; Not populated in |b{+-} decay (J{+|p}=(5/2+)) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2,7/2+
level_comment:
J$750.2|g to 5/2+, 818.3|g to 3/2+, 1177.0|g to 7/2+, direct feeding from (5/2+) in {+109}Ru |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: PS
level_comment:
J$638.9|g to (7/2)+, 952.00|g to 3/2+, no |g to 9/2+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$985.8|g to 5/2+, 1054.0|g to 3/2+, no |g's to J=7/2 and 9/2; Not populated in |b{+-} decay (J{+|p}=(5/2+)) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$499.94|g to (3/2)+, 869.5|g to (11/2+); strong direct feeding in {+109}Ru |b{+-} decay (J{+|p}=from (5/2+)) 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: 5/2+,7/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$265.61|g to (3/2+), 480.1|g to 9/2+; direct feeding in {+109}Ru |b{+-} decay (J{+|p}=from (5/2+)) 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$strong direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)); 1570.4|g to 3/2+, 1287.0|g to (11/2+) 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$strong direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)); 652.5|g to (3/2+), 1757.1|g to 9/2+; no |g's to 11/2+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)); 960.5 to (3/2)+, 1765.7|g to 9/2+; no |g's to 11/2+ 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
J$1641.5|g to 1/2-, 1588.7|g to 5/2+, no |g to 9/2+; direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$strong direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)); 1720.0|g to 1/2-, 2094.3|g to 7/2+, no |g's to 9/2+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay); 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$2117.3|g to 7/2+, 1891.4|g to 3/2+, no |g's to 9/2+ direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)); 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2)
level_comment:
J$direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)); 1616.5|g to 3/2-, 2184.7|g to 7/2+, no |g's to 1/2 and 9/2+ levels 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)); 1816.5|g to 1/2-, 1763|g to 5/2+ 
T$from |b|g|g(t) in 2011BuZZ ({+109}Ru |b{+-} decay); 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2)
level_comment:
J$direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)); 1767.0|g to 5/2+, 2193.8|g to 7/2+, no |g's to 1/2 and 9/2+ levels 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2)
level_comment:
J$1537.5|g to (7/2)+, 1850.8|g to 3/2+, no |g's to 1/2 and 9/2+ levels direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2)
level_comment:
J$1879.3|g to 3/2+, 1811.4|g to 5/2+; no |g's to 1/2 and 9/2+ levels direct feeding in {+109}Ru |b{+-} decay (J{+|p}=(5/2+)) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_comment:
T$weighted average of 33 ns {I2} from (194|g)(116|g)(t) in 1987Ka29 (slope method) and 34 ns {i2} from |b-374|g(t) in 1998Lh02 (slope method) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$Others: <0.5 ns 427|g(t) in 1998Lh02 (centroid shift) and 8 ns 1 in 1987Ka29 (close to timing resolution of Ge(Li) detectors) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
J$from 2018Bu16. In {+109}Rh Adopted Levels, the assignment is (3/2)+, which is refuted by 2018Bu16. 
$Compilers' note: going through all the experimental arguments for assignment of spin of this level as detailed in the ENSDF database, and additional arguments about absence of |g transitions to 7/2+ g.s. and from higher 5/2- and 7/2+ levels, long half-life of the level, and experimental large B(E2)(W.u.) values for transitions between the 225.9, 3/2+; 257.7; 409.7, 7/2+ and 478.3, 5/2+ levels consistent with interpretation of a collective structure based on a K|p=1/2+ intruder level at 257.7 keV. E-mail communication of Jan 25, 2023 between Dr. Jun Chen (one of the evaluators of A=109 in the ENSDF database) and B. Singh discussed the J|p assignment and concluded that (1/2)+ is the preferred choice for 257.7 level 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J$Direct population of 0+ and 2+ states in {+110}Pd following {+110}Rh |b{+-} (3.35 s) decay 
T$Weighted average of 3.0 s 2 (from |b(t) in 1970Pi01), 3.1 s 2 (from 374|g(t) in 1970Pi01), 3.3 s {I3} (from 374|g(t) in 1978Fr16) and 3.5 s {I1} (from 374|g(t) in 1986KaZS). Other: 5.0 s 8 (from 374|g(t) in 1963Ka21) 
CONF$Probable |p7/2+[413](g{-9/2})~#|n5/2+[413](g{-7/2}) (for prolate deformation) based on the systematics of the neighboring odd-Ru and odd-Pd nuclei. The Gallagher-Moszkowski rule favors the J|p=1+ assignment 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (6+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$Direct population of (5+) state of {+110}Pd in {+110}Rh |b{+-} (28.0 s) decay 
T$Weighted average of 28.5 s {I15} (from 374|g(t) in coincidence with 500<E|b<2005 keV) and 26 s {I3} (from 374|g(t)) in 1970Pi01. Other: 34 s {I4} (from |g(t)) in 1970Wa28 
CONF$Probable |p7/2+[413](g{-9/2})~#|n5/2+[413](g{-7/2}) (for prolate deformation) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (7-)
level_comment:
J$65.8|g M1+E2 to (6-) 
T$Note that 16 ns {I4} from 65.8|g(t) in 2004Lu03. However, if this level is a band-member, then the lifetime should originate from another state. The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7-)
level_lifetime_unit: NS
level_comment:
T$From 65.8|g(t) in 2004Lu03. However, this level is assigned as a collective, band-member in the adopted levels, and hence, the lifetime should originate from another state 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: S
level_comment:
$Measured mass excess=-82664.3 keV {I18} (2023Hu01), with reference to mass of {+133}Cs. 
E$from 2023Hu01, difference of measured mass excesses of the g.s. and the isomer. 
T$2023Hu01 list 28.5 s {I13} from 2021Ko07 (NUBASE2020). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
T$11 s {I1} (1978Fr16) 275 |g-decay curve; 13.5 s {I15} (1976MaYL) {+252}Cf SF, timed gas-separation method, 275 |g-decay curve 
J$allowed (log| {Ift}=4.7) |b- from (5/2+), Systematics in odd-A Rh supports the (7/2+) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_comment:
J$based on assumption that this level is the lowest member of intruder band. 
T$from |g|g(t) (1990Ro13) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_comment:
J$Direct |b{+-} decay feeding to the 0+ and 2+ states in {+112}Pd; systematics of known J|p and configurations in neighbouring nuclei 
T$weighted average of 3.5 s {I4} (1999Lh01) and 3.8 s {I6} (1988Ay02); Others: 2.1 s {I3} (1991Jo11), 1.2 s 6 (1987GiZW), 0.8 s {I1} (1976MaYL), 5.17 s {I7} (1969WiZX), <1.5 s (1978Fr16), 0.7 s {I3} (1985Bu05) 
CONF$|p7/2+[413]~#|n5/2+[413] and prolate deformation from systematics of known orbitals in neighbouring nuclei (|p7/2+[413] in even-Z {+111}Ru and {+113}Pd nuclei and |n5/2+[413] in even-n {+107-111}Rh nuclei); the assignment is supported by the Gallagher-Moszkowski rule 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
J$327.0|g M1+E2 to (1+), 244.8|g M1(+E2) to (1+,2+); possible direct feeding in {+112}Ru (J|p=0+) |b{+-} decay 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (6+)
level_lifetime_unit: S
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$direct |b{+-} feeding to 5+ and 6+ states in {+112}Pd; systematics of known J|p and configurations in neighbouring nuclei 
T$weighted average of 6.73 s {I15} (1999Lh01) and 6.8 s {I2} (1988Ay02) 
CONF$|p7/2+[413]~#|n5/2+[413] and prolate deformation from systematics of known orbitals in neighbouring nuclei (|p7/2+[413] in even-Z {+111}Ru and {+113}Pd nuclei and |n5/2+[413] in even-n {+107-111}Rh nuclei); the assignment is supported by the Gallagher-Moszkowski rule 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_comment:
T$From 1991Jo11 using a two component fit to 777.5|g-|b(t) ({+112}Pd), one associated with decay from {+112}Ru (1.75 s {I7}) and the other with a direct population of {+112}Rh in fission. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y+60.58
level_spin_parity: (7-)
level_comment:
T$24 ns {I6} for 60.3|g originating from a nuclide with A=112 {I1} in 1970Jo20; 45 ns {I3} for 60.6|g in 1974ClZX, assigned to {+111}Rh by the authors 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_comment:
$Measured mass excess=-79603.7 keV {I17} (2023Hu01), with reference to mass of {+85}Rb. 
T$others: 3.6 s {I3} in {+112}Rh Adopted Levels in the ENSDF database, and 3.4 s {I4} in 2021Ko07 (NUBASE2020) are in severe disagreement with value measured by 2023Hu01. See 2023Hu01 for a critique of the evaluated T{-1/2} in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: S
level_comment:
$Measured mass excess=-79565.2 keV {I17} (2023Hu01), with reference to mass of {+133}Cs and {+112}Rh g.s.; weighted average of the two values. 
E$from 2023Hu01, difference of measured mass excesses of the g.s. and the isomer, authors' weighted average of 38.5 keV {I26} and 38.3 keV {I26}from two independent mass measurements 
T$others: 6.76 s {I12} in {+112}Rh Adopted Levels in the ENSDF database, and 6.73 s {I15} in 2021Ko07 (NUBASE2020) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
J$log| {Ift}=4.1 from 0+ 
E$Assumed to be g.s. on basis of mass syst (1997Au04) 
T$from 1988Ay02. Others 1.68 s {I7} (1970WiZN),1.86 s {I5} (2003Lh01) 2003Lh01 say that the half-life of the low spin could be shorter. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$log| {Ift}=4.8 {I+3-2} from 0+ for Q=4800 {I200} and I|b=14%; however, the large Q and probable incomplete level scheme suggests that this branch may be an upper limit. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$From 1988Ay02 for a level with J=(4,5),1.86 s {I5}(2003Lh01) It is the same group. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$From {+114}Rh Adopted Levels in the ENSDF database (Jan 2012 update). The half-life, taken from 1988Ay02 (Nucl. Phys. A480, 104), is the same as for the 1+ g.s. 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: S
level_comment:
$Measured mass excess=-75551.8 keV {I41} (2023Hu01), with reference to mass of {+114}Rh g.s. 
E$from 2023Hu01, difference of measured mass excesses of the g.s. and the isomer. 


level_energy_unit: KEV
level_energy_info: ;ERR=SY;ERR=?
level_spin_parity: (6-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$An excitation energy of 150 keV derived from systematics (1997Au04) 
T$from 2001Wa04, supersedes 1988Ay02 (same group) 
J$log| {Ift}=5.8 to (6+) no feeding to levels with J|<4 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$from {+116}Rh Adopted Levels in the ENSDF database (Dec 2009 update). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
$Measured mass excess=-70729 keV {I2} (2023Hu01), with reference to mass of {+133}Cs. 
T$2023Hu01 cite value of 685 ms {I39} from 2021Ko07 (NUBASE2020) 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: S
level_comment:
$Measured mass excess=-70608.3 keV {I28} (2023Hu01), with reference to mass of {+116}Rh g.s. 
E$from 2023Hu01, difference of measured mass excesses of the g.s. and the isomer. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
T$from 1991Pe10. Other: 394 ms +47-43 (2007Mo07) Report by 1970WeZX gives T{-1/2}=1.7 s {i3} (not adopted) 
J$from syst of odd Rh nuclei. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n adopted from 2021Ha19, where (implants)|b|n-coin method used. Other: 3.1 {I4} (2006Mo07). Weighted average of the two values is 2.9 {I4}, and unweighted average is 2.6 {I5} 
$Theoretical T{-1/2}=90.2 ms, %|b{+-}n=2 (2019Mo01) 
$Theoretical T{-1/2}=391.7 ms; %|b{+-}n=2.11, 1.98 (2021Mi17, %|b{+-}n for four different fission barriers) 
E$the observed activity is assumed to correspond to the ground state, although, from systematics of odd-odd Rh isotopes, two activities are expected, a low-spin g.s. and a high-spin isomer. Thus, it is possible that the observed activity is a mixture of the two activities, the other may correspond to 0+x, (7-) level 
J$expected to be low spin, possible 1+ from systematics of odd-odd Rh nuclides 
T$weighted average of 294 ms {I17} (2021Ha19, (implants)|b-correlated decay curve); 285 ms {I10} (2015Lo04, (implants)|b decay); 266 ms {I+22-21} (2006Mo07, (implants)|b-decay curve); 310 ms {I30} (2000Jo18, 574.6|g decay curve, authors also quote 300 ms {I60} in the abstract). This half-life may correspond to a mixture of two activities 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7-)
level_comment:
E,J$possible high-spin (J=4-10) isomer from systematics and from {+118}Rh decay to {+118}Pd (2006Wa10) which populates both low- and high-spin levels. See comments for the g.s. 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: MS
level_comment:
$Measured mass excess=-64994 keV {I5} (2023Hu01), with reference to mass of {+133}Cs. 
J$from systematics, cited by 2023Hu01 from 2021Ko07 (NUBASE2020) 
T$from {+118}Rh Adopted Levels in the ENSDF database (January 2022 update), which included measurement from 2021Ha19 (Phys. Lett. B816, 136266). 2023Hu01 cite value of 282 ms {I9} from 2021Ko07 (NUBASE2020) 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: MS
level_comment:
$Measured mass excess=-64804.9 keV {I78} (2023Hu01), with reference to mass of {+118}Rh g.s. 
E$from 2023Hu01, difference of measured mass excesses of the g.s. and the isomer. 
J$from systematics, cited by 2023Hu01 from 2021Ko07 (NUBASE2020). 
T$cited by 2023Hu01 from 2021Ko07 (NUBASE2020) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MS
level_comment:
T$from |b(t) in (2006Mo07). Other: 190 {I10} ms from (2006ToZW) 
J$from systematics of odd Rh nuclei. 
%B-N$from |b-n coincidence in (2006Mo07) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MS
level_comment:
J,%B-N$from Adopted Levels of {+119}Rh in ENSDF database; J|p from systematics 
$Theoretical T{-1/2}{-1/2}=107.6 ms, %|b{+-}n=3.77 (2003Mo09) 
E$the measured half-life is assumed to correspond to the ground state of {+119}Rh 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 171 ms {I18} (Adopted Levels of {+119}Rh in ENSDF database, value taken from 2006Mo07: Phys. Rev. C73, 035801) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Earlier value: 6.4 {I16} (2006Mo07: Phys. Rev. C 73, 035801). Weighted average of the two values is 4.1 {I13} (compiler's note) 
E$the observed activity is assigned to the g.s. of {+119}Rh, but there is the possibility of two activities, based on systematics odd-A Rh nuclei. 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 190 ms {I6} (2015Lo04: Phys. Rev. Lett. 114, 192501); 171 ms {I18} (2006Mo07, also 190 ms {I10} in 2006ToZW (thesis from Michigan State Univ.). Weighted average of the three values is 189 ms {I6}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=82.7 ms, %|b{+-}n=4.0, %|b{+-}2n=0.0 (2003Mo09) 
$Theoretical T{-1/2}=180 ms, %|b{+-}n=1.3, %|b{+-}2n=0.2 (2016Ma12) 
T$from weighted average of 131 ms {I5} (2015Lo04, implanted ions-|b correlated curves and maximum likelihood method), and 136 ms {I+14-13} (2006Mo07, timing of |b spectrum; earlier value from the same group was 120 ms {I10} reported in 2004Wa26) 
E$assumed as the g.s. 
J$1- to 4- based on |W{-p}=3/2+ and |W{-n}=5/2- from theoretical considerations (1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Previous value: <5.4 (2006Mo07: Phys. Rev. C 73, 035801). No events for |b{+-}2n decay mode were detected by 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+120}Rh 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 131 ms {I5} (2015Lo04: Phys. Rev. Lett. 114, 192501); 136 ms {I+14-13} (2006Mo07, earlier value from the same group: 120 ms {I10} in 2004Wa26). Weighted average of the three values is 133 ms {I5}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from timing of |b spectrum (2006Mo07). 
E$assumed as the g.s.(evaluator) 
J$systematics: J|p=7/2+ for {+105,107,109}Rh 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}{-1/2}=62.3 ms, %|b{+-}n=8.6 (2003Mo09) 
E$the measured half-life is assumed to correspond to the ground state of {+121}Rh 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 151 ms {I+67-58} (Adopted Levels of {+121}Rh in ENSDF database, value taken from 2006Mo07: Phys. Rev. C73, 035801) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. 
E$the observed activity is assumed to correspond to the g.s. of {+121}Rh 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 76 ms {I5} (2015Lo04: Phys. Rev. Lett. 114, 192501); 151 ms {I+67-58} (2006Mo07, Phys. Rev. C 73, 035801). Weighted average of the three values is 73.5 ms {I20} (compiler's note) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
E$assumed as the g.s. 
T$ lower limit from estimated time-of-flight in 1997Be70. Actual half-life is expected to be much longer as suggested by the systematics value of 80 ms (2012Au07) and theoretical value of 58.5 ms (1997Mo25) 
$Theoretical %|b{+-}n=8.7, %|b{+-}2n=0.01 (1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$ Number of implanted fragments=8.6|*10{+3} 
E$ in 2012Au07, this isomer was incorrectly assigned to {+122}Ru 
T$ from |g(t) method (2012Ka36) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. No events for |b{+-}2n decay mode were detected by 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+122}Rh 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier value: 51 ms {I6} (2015Lo04: Phys. Rev. Lett. 114, 192501). Weighted average of the two values is 52.3 ms {I15}, as it is heavily weighted by the value in 2021Ha19 (compiler's note) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}{-1/2}=53.5 ms, %|b{+-}n=9.2, %|b{+-}2n=0.01 (2003Mo09) 
E$the measured half-life is assumed to correspond to the ground state of {+122}Rh 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$measured half-life is assumed to correspond to the ground state of {+123}Rh 
J$7/2+ from systematic trends (2021Ko07); 1/2- predicted in calculations of 2019Mo01 
T$weighted average of 42.2 ms {I18} (2021Ha19, |b-delayed neutron counting) and 42 ms {I4} (2015Lo04, (implanted ions)|b correlated curves) 
$%|b{+-}n: from |b-delayed neutron counting (2021Ha19) 
$Theoretical T{-1/2}=162.3 ms (2019Mo01), 70.7 ms (2016Ma12) 
$Theoretical %|b{+-}n=70, %|b{+-}2n=0.0 (2019Mo01); %|b{+-}n=23.5 %|b{+-}2n=0.1 (2016Ma12) 
$Measured |s=1470 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+123}Rh isotope<0.001% (2010Oh02) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=31.0 ms, %|b{+-}n=16.8, %|b{+-}2n=0.40 (2003Mo09) 
$Measured |s=110 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+124}Rh isotope<0.001% (2010Oh02) 
E$measured half-life is assumed to correspond to the ground state of {+124}Rh 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. No events for |b{+-}2n decay mode were detected by 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+124}Rh 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier value: 30 ms {I2} (2015Lo04: Phys. Rev. Lett. 114, 192501). Weighted average of the two values is 31.5 ms {I23} (compiler's note) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=25.3 ms, %|b{+-}n=23.4, %|b{+-}2n=0.04 (2003Mo09) 
$Measured |s=11 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+125}Rh isotope<0.001% (2010Oh02) 
E$measured half-life is assumed to correspond to the ground state of {+125}Rh 
J$7/2+ from systematic trends (2012Au07); 5/2+ predicted in calculations of 1997Mo25 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=23.0, %|b{+-}2n=0.43 (2003Mo09) 
$Measured |s=0.7 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+126}Rh isotope=0.46% (2010Oh02) 
E$measured half-life is assumed to correspond to the ground state of {+126}Rh 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical ones. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=31.26, %|b{+-}2n=0.19 (1997Mo25) 
E$measured half-life is assumed to correspond to the ground state of {+127}Rh 
J$5/2+ from theoretical considerations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay 
$Theoretical T{-1/2}=20.4 ms, %|b{+-}n=26.0, %|b{+-}2n=0.26, %|b{+-}3n=0.0 (2003Mo09: Phys. Rev. C67, 055802) 
$Theoretical T{-1/2}=24.4 ms, %|b{+-}n=84.6, %|b{+-}2n=0.9, %|b{+-}3n=0.1 (2016Ma12: Phys. Rev. C93, 025805) 
$A total of 22 counts were assigned to {+127}Rh, 10 events with the spectrometer setting on Pd, and 12 events for setting on Sn. Probability of misidentification of this isotope is <0.01% (2018Sh11). 
$Production |s=0.097 pb for Pd setting, and 0.098 pb for Sn setting, with 30% systematic uncertainty for all |s. 
E$it is assumed that the observed events correspond to ground-state activity. 
T$measured by 2015Lo04 at RIBF-RIKEN. 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay, thus 100% |b{+-} decay is assigned by inference 
$Theoretical T{-1/2}=8.4 ms, %|b{+-}n=47, %|b{+-}2n=6 (2019Mo01) 
$Theoretical T{-1/2}=20.3 ms, %|b{+-}n=76.1, %|b{+-}2n=5.7 (2016Ma12) 
$Only one count was assigned to {+128}Rh with the spectrometer setting on Sn. Probability of misidentification of this isotope is 0.83% (2018Sh11) 
$Production |s=0.007 pb for Sn setting, with 30% systematic uncertainty for |s 
E$it is assumed that the observed event corresponds to ground-state activity. 
J$1- or 6- from |W{-|p}=5/2+, |W{-|n}=7/2- orbitals proposed in 2019Mo01 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 8.4 ms (2019Mo01) and 20.3 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+128}Rh is expected to be <25 ms, based on measured half-lives of 26.5 ms for {+125}Rh, 19 ms for {+126}Rh, and 20 ms for {+127}Rh, available in literature. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
%EC+%B+$expected decay modes assigned by the evaluators. Systematic values suggest {+90}Pd is bound to 1 proton emission (S(p)=1140 syst {I540}) but potentially unbound (S(2p)=-50 {I500}) to 2p emission (2017Wa10). 
$A total of two events were assigned by 2016Ce02 to {+90}Pd 
T$> 760 ns from time-of-flight (2016Ce02) through the BigRIPS fragment separator and ZDS spectrometer (2016Ce02). Theoretical calculations predict a T{-1/2} of 73 ms (2019Mo01). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$|e decay considered as negligible by 2018Pa20 
%B+P$from number of single-pixel events with |DE>1500 keV (2018Pa20). 
T$measured by 2018Pa20, using maximum likelihood method (MLH) for (implant)(positron)-correlated decay curve, where the fit function contained the parent, |b-daughter, and |bp-daughter decay components with half-lives and %|bp branching ratios, and a constant background for random correlations. Two generations of isotopes were considered in the Bateman equation. Decay constants for {+91}Rh and {+90}Ru daughters were taken from literature. The measured half-life compared with theoretical value 44.5 ms from shell-model calculations by 1997He24: Nucl. Phys. A627, 35. 
$Measured Q(|e)({+91}Pd)=11.8 MeV {I22} (2018Pa20) from (implants)|b correlated energy curve, by taking into account contribution from {+91}Rh daughter activity, and assuming that the observed endpoint energy corresponds to g.s. to g.s. |b{++} transition. Other: 12.64 MeV {I50} (syst, 2017Wa10: AME-2016) 
$390 implantation counts were assigned to {+91}Pd by 2018Pa20. 
$|b-decay correlation fraction=70% {I4} (2018Pa20) 
$As no beta-delayed |g rays were observed, 2018Pa20 assumed 100-(%|b{++}p)=97.0% {I+9-11} |b{++} feeding to the g.s. of {+91}Rh, implying log| {Ift}=3.4 {I5} for this transition. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$weighted average of 1.06 s {I3} from implant-|b(t) and 0.91 s {I29} from implant-|bp(t); both analyses used multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
J 7/2+ or 9/2+ based on shell-model calculations in (1g{-9/2}, 2p{-1/2}) model space (2000Sc31) and on systematics of J|p(g.s.) in neighboring odd-N nuclides. 2001Xu05 favor 9/2+ based on statistical model calculation of proton branching to different final states in the {+92}Ru |ep decay daughter as a function of assumed J|p({+93}Pd). Shell-model calculations by 2004Ru02 also favor a 9/2+ g.s. 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
E a different value (1096) was proposed in ({+58}Ni,|an|g); there, I(984|g) and I(1096|g) were too similar to define the cascade order and the 205|g and 887|g, now known from ({+40}Ca,|an|g), were unobserved. 


level_energy_unit: KEV
level_spin_parity: (25/2-,27/2-)
level_uncertain: ?
level_comment:
J (D) 515|g to (25/2+) 2871; probably feeds level of equal or lower J; member of sequence analogous to |p=- yrast sequences in the {+89}Mo and {+91}Ru N=47 isotones. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T$ measured by 2012Lo08 from decay curves of time correlations between implantations and decay radiation. Decay curves were fitted with Poisson distribution using log-likelihood function by consideration of decay of parent, daughter and grand-daughter 
J$ from {+93}Pd Adopted Levels in ENSDF database 
%B+P$ measured by 2012Lo08 based on observation of 1548 |bp coincidence events. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$weighted average of 1.18 s {I2} from implant-|b(t) and 1.16 s {I2} from implant-|bp(t); both analyses used multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 14+
level_lifetime_unit: NS
level_comment:
T$ from time distribution of |g rays below the 14+ isomer (2011Br01) using ROOT implementation of MINUIT computer code and one exponential fit.. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (19-)
level_lifetime_unit: NS
level_comment:
J$tentative assignment based on Weisskopf estimates 
T$ from time distribution of 1651|g using ROOT implementation of MINUIT computer code (2011Br01). 
$Dominant configuration=|p[(p{-1/2}{+-1}g{-9/2}{+-3})]{-11}~# |n[g{-9/2}{+-2}]{-8} 


level_energy_unit: KEV
level_spin_parity: (14+)
level_lifetime_unit: NS
level_comment:
E$Isomeric ratio R=30 % {I1} (2017Pa35) 
T$From |g(t) in 2017Pa35, but the gating |g-ray transitions were not given by the authors 


level_energy_unit: KEV
level_spin_parity: (19-)
level_lifetime_unit: NS
level_comment:
E$Isomeric ratio R=6.8 % {I29} (2017Pa35) 
J$From 2011Br11 
T$From |g(t) in 2017Pa35, but the gating |g-ray transitions were not given by the authors 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from implant-|b(t) using multiparameter fit to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T$average of the limit of 1.7s|<T{-1/2}|<7.5s from |b|g(t) (1997Sc30). 
J$from the systematics of N=49 nuclei and the fact that the neighboring even-even nuclei are spherical (close to N=50) and the odd neutron (or neutron hole) occupies the g9/2 orbital. 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$from the analysis of decay-curves for the strongest {+95}Rh |g's (1982Ku15). Others: 14.2 s {i24} from |bp(t) (1982No06) 
J$strong feeding of the (21/2+) state in {+95}Rh with a log| {Ift}|?5.5 
$%IT from I(524)=10.6 {I3}, and I(1351)=100 {I3} in 1982Ku15. The intensity of the 1351 |g's has a 10.6x1.0393=11.0 {I3} component due to the {+95}Pd |g, and the I(1351) in {+95}Rh following |e+|b{++} decay is equal to 89 {I3}. 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: S
level_comment:
$%IT from I(524)=10.6 {I3}, and I(1351)=100 {I3} in 1982Ku15. The intensity of the 1351 |g's has a 10.6x1.0393=11.0 {I3} component due to the {+95}Pd |g, and the I(1351) in {+95}Rh following |e+|b{++} decay is equal to 89 {I3}.. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T$ measured by 2012Lo08 from decay curves of time correlations between implantations and decay radiation. Decay curves were fitted with Poisson distribution using log-likelihood function by consideration of decay of parent, daughter and grand-daughter. Weighted average of half-lives deduced from |b|g- and |bp-decay data. T{-1/2}=8.0 s {I6} from decay curve analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (21/2+)
level_lifetime_unit: S
level_comment:
$ No evidence was found by 2012Lo08 for %|b{++}p decay mode of this isomer which might be populated by the |b decay of {+95}Ag. In ENSDF database for {+95}Pd Adopted Levels, %|b{++}p=0.93 {I15}; %|b{++}p=0.90 {I16} is quoted in {+95}Pd |b{++}P decay dataset in ENSDF; 2012Lo08 quote %|b{++}p=0.74 {I19} from literature 
T$ from {+95}Pd Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (21/2+)
level_lifetime_unit: S
level_lifetime_info: ;ERR=?
level_comment:
E,T$from the Adopted Levels of {+95}Pd (2010 update) in the ENSDF database. Energy is rounded value 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (21/2+)
level_lifetime_unit: S
level_comment:
T$from implant-|b(t) using multiparameter fit to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 
E,J$from the Adopted Levels of {+95}Pd in the ENSDF database (October 2010 udpate) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: NS
level_comment:
T$from 1989Al05. Others: 11.7 ns {i28} (1983Pi05), 4.6 ns {i14} (1983Gr01) 
J$from systematics of even-even N=50 nuclei, E2 |g from (8+) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: US
level_comment:
T$weighted average of 2.0 |ms {I3} (2007My02) and 2.2 |ms {I3} (1983Gr01) 
J$from systematics of even-even N=50 {I8}+ isomers 


level_energy_unit: KEV
level_spin_parity: (15+)
level_lifetime_unit: NS
level_comment:
T$from 1989Al05. Other: 58 ns 5 (1983Pi05) 
J$systematics of 15+ states in even-even N=50 nuclei 
MOMM1$from TDPAD. 


level_energy_unit: KEV
level_spin_parity: (15,16,17)-
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
T$ measured by 2012Pa19 from 2154|g(t) and 1713|g(t) with T{-1/2}= 37.9 ns {I10} and 35.6 ns {I22}, respectively; weighted average taken 
E$ it is also possible that isomer is above the 8385 level fed by a low-energy (unobserved) transition. Estimated energy of such a transition is <100 keV from experimental conditions. 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: US
level_comment:
E$Isomeric ratio R=76 % {I1} (2017Pa35) 
T$From |g(t) in 2017Pa35, but the gating |g-ray transitions were not given by the authors 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MIN
level_comment:
J$from shell model and analogy with other N=51 nuclei. configuration=2d5/2 
T$weighted average of 3.1 min {I1} (1980Go11), 3.0 min {I2} (1980Za11), and 3.3 min {I3} (1969At01). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$log| {Ift}=5.85 from (9/2+) {+97}Ag; 686.4|g to g.s. is (M1+E2) (|g(|q) data of 1990Pi01). From shell model probable configuration=1g7/2 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 17.7 min {I4} (1972Ga21), 18.0 min {I5} (1972Ba37), 18 min {I1} (1969An32), 17.5 min {I5} (1956Ka25). Others: 17 min {I3} (1955At34), 15 min {I3} (1953At27) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$from |g|g(|q) in {+92}Mo({+10}B,3np|g) (2009FrZZ), but no details available 
T$from DSAM in {+92}Mo({+10}B,3np|g) (2009FrZZ) 
$Possible fragment of one-phonon mixed symmetry state (2009FrZZ), based on large M1 transition strength for |g to first 2+ state 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$possible |g to 0+, but 3,4+ are not ruled out 
T$from DSAM in {+92}Mo({+10}B,3np|g) (2009FrZZ) 
$Possible fragment of one-phonon mixed symmetry state (2009FrZZ), based on large M1 transition strength for |g to first 2+ state 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J$proposed by 1984Pi11 in ({+32}S,2p2n|g) based on |g(|q) and systematics; |b feeding from (6+) parent 
$Possible configuration=|pg{-9/2}{+-1}~#|pp{-1/2}{+-1} (1997Ce08) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J$proposed by 1997Ce08 in ({+58}Ni,2p2|a|g) based on the 454|g-434|g-979|g cascade from (11-) to 8+ with mult=stretched dipole for 454|g and 434|g 


level_energy_unit: KEV
level_spin_parity: (7+)
level_comment:
J$1559.2|g to 8+ and 579.4|g to (9+); |b feeding from (6+). But (7+) is inconsistent with 2043.1|g to (4+) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$mean lifetime |t<16.3 ps (from B(E2)(W.u.)>3.9 in the 2009FrZZ conference paper); |t<15 ps {I1} (B(E2)(W.u.)>4.2 {I3}) listed in 2009FrZZ presentation. Due to contamination in the intensity of 862.9|g, only an upper limit of lifetime could be determined by 2009FrZZ 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=16.9 ps {I30} (RDDS method, 2009FrZZ), value is preliminary and listed in the presentation 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$(2+) from |g|g(|q) (2009FrZZ), but no details available 
T$effective mean lifetime |t=179 fs {I30} from DSAM (2009FrZZ) 
$Possible fragment of one-phonon mixed symmetry state (2009FrZZ), based on large M1 transition strength for |g to first 2+ state 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=27.8 ps {I20} (RDDS method, 2009FrZZ), value is preliminary and listed in the presentation 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$(2+) proposed, but 3,4+ are not ruled out in 2009FrZZ 
T$effective mean lifetime |t=100 fs {I30} from DSAM (2009FrZZ) 
$Possible fragment of one-phonon mixed symmetry state (2009FrZZ), based on large M1 transition strength for |g to first 2+ state 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=95.6 ps {I20} (RDDS method, 2009FrZZ), value is preliminary and listed in the presentation 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+108,98}=-1.231 fm{+2} {I4} (stat) {I4} (syst volt) {I13} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: MIN
level_comment:
J log| {Ift}=5.2 to 200.4 level which decays by M1 to 9/2+. log| {Ift}=5.8 to 1527.4 level which decays to (1/2-). Syst 
T from |g(t) (1969Ph01) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
J |g to (5/2)+ is |DJ=2, E2; |g to (7/2)+ is |DJ=1, M1. Inconsistent with 1275.8|g to (3/2+) in |b{++} decay 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J |g to (7/2+) is |DJ=1, D; |g to (9/2) is |DJ=0, D+Q Inconsistent with 1233.1|g, 1476.3|g to (3/2+) in |b{++} decay 


level_energy_unit: KEV
level_spin_parity: (31/2+)
level_comment:
$ Possible configuration=|pg{-9/2}{+-2}~#|ng{-7/2}~#|nd{-5/2}{+2} or |pg{-9/2}{+-4}~#|ng{-7/2}; maximum aligned state 


level_energy_unit: KEV
level_comment:
$|d<r{+2}>{+108,99}=-1.121 fm{+2} {I6} (stat) {I3} (syst volt) {I15} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2)+
level_lifetime_unit: PS
level_comment:
T$weighted average of 168 ps {I6} and 157 ps {I4} from centroid shift and deconvolution method, respectively (2022Iv01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 665.5|g to 0+ 
T$other: 9.2 ps {I6} (RDDS in {+24}Mg({+80}Se,4n|g); 2012An17,2011An04,2011AnZZ) 
MOMM1$g factor=+0.30 {I14} from transient magnetic field technique in inverse kinematics (2011To09) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 750.6|g to 2+; band assignment 
T$other: 1.66 ps {I12} (RDDS in {+24}Mg({+80}Se,4n|g); 2011AnZZ) 
MOMM1$g factor=+0.45 {I14} from transient magnetic field technique in inverse kinematics (2011To09) 


level_energy_unit: KEV
level_spin_parity: 3(+)
level_comment:
J$from |g|g(|q) and possible 3-phonon state in ({+3}He,2n|g) (2009Ra06). Possible direct |e feeding from (5)+ (|DJ=0 or 1) produces conflicting J|p=(4,5,6), probably due to incomplete knowledge of the decay scheme. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 773.2|g to 4+; band assignment 
T$other: 1.66 ps {I8} (RDDS in {+24}Mg({+80}Se,4n|g); 2011AnZZ) 
MOMM1$g factor=+1.47 {I87} from transient magnetic field technique in inverse kinematics (2011To09). This value is not listed in 2014StZZ. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$tentative assignment from |g|g(|q) and one-phonon mixed-symmetry state in ({+3}He,2n|g) (2009Ra06); possible allowed |e feeding from (2)+ 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$|DJ=(2) 1115.8|g to 4+ gives J=(2+ or 6+). |b{++} feeding from (5)+ and (2)+ isomers produce conflicting J|p assignments probably due to incomplete knowledge of the decay schemes. However, a stronger |b{++} feeding from (2)+ isomer suggests a preference for J|p=2+ 


level_energy_unit: KEV
level_spin_parity: (1-:4+)
level_comment:
J$1956.0|g to 2+; 614.1|g from (3-) 
E$level not confirmed in other studies other than |e decay studies 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 798.6|g to 6+; band assignment 
T$other: 1.75 ps {I7} (RDDS in {+24}Mg({+80}Se,4n|g); 2011AnZZ) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_comment:
J$|DJ=2, E2 988.9|g to 6+; |DJ=0, M1 190.3|g to 8+ 
T$from |g|g(t), centroid-shift method (1982An17) 


level_energy_unit: KEV
level_spin_parity: (2+,3+)
level_comment:
J$1819.6|g to 4+ gives J=2 to 6. Fairly strong and possibly allowed |e feeding from (2)+ parent suggests a preference for 2+,3+. Possible weak |e feeding from (5)+ parent produces a conflicting J|p assignment of J=(4,5,6), probably due to incomplete knowledge of the decay scheme 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 881.1|g to 8+; band assignment 
T$other: 0.51 ps {I6} (RDDS in {+24}Mg({+80}Se,4n|g); 2011AnZZ) 


level_energy_unit: KEV
level_spin_parity: 9-
level_comment:
E$corresponding to 8715 level in ({+12}C,3n|g) deexcited by the 875.9|g 
J$|DJ=1, E1 875.9|g to 8+; |DJ=2, Q 822.8|g to 7-; band assignment 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 892.3|g to 10+; band assignment 
T$other: 1.81 ps {I14} (RDDS in {+24}Mg({+80}Se,4n|g); 2011AnZZ) 


level_energy_unit: KEV
level_spin_parity: 11-
level_comment:
E$corresponding to 4792 level in ({+12}C,3n|g) deexcited by the 809.4|g 
J$|DJ=2, E2 809.4|g to 9-; 994.3|g to 10+; band assignment 


level_energy_unit: KEV
level_spin_parity: (12-)
level_comment:
E$corresponding to 6691 level in ({+58}Ni,4p|g) deexcited by the 626.2|g 
J$|DJ=(2), (Q) 939.0|g to (10-); 626.2|g to (11-); band assignment 


level_energy_unit: KEV
level_spin_parity: 13-
level_comment:
E$corresponding to 3982 level in ({+12}C,3n|g) deexcited by the 805.7|g 
J$|DJ=2, E2 805.7|g to 11-; |DJ=1, D 908.1|g to 12+; band assignment 


level_energy_unit: KEV
level_spin_parity: 15-
level_lifetime_unit: PS
level_comment:
E$corresponding to 6768 level in ({+12}C,3n|g) deexcited by the 1035.4|g 
J$|DJ=2, E2 1035.4|g to 13-; 786.0|g to 14+; band assignment 
T$from DSAM for 1035|g (2020Si20). Listed in {+72}Ge({+35}Cl,|apn|g) dataset 


level_energy_unit: KEV
level_spin_parity: (16)+
level_comment:
E$corresponding to 6168 level in ({+12}C,3n|g) deexcited by the 479.4|g 
J$|DJ=2, E2 1231.8|g to 14+; band assignment 


level_energy_unit: KEV
level_spin_parity: (17)-
level_lifetime_unit: PS
level_comment:
E$corresponding to 5732 level in ({+12}C,3n|g) deexcited by the 940.2|g 
J$|DJ=2, E2 940.2|g to 15-; 706.4|g to (16)+ 
T$from DSAM for 940|g (2020Si20). Listed in {+72}Ge({+35}Cl,|apn|g) dataset 


level_energy_unit: KEV
level_spin_parity: (18+)
level_comment:
J$|DJ=2, Q 1032.0|g to (16)+; band assignment. 2001Zh26 proposed (17+) based on |DJ=1 band assignment, but |g(|q) and |g(DCO) for 1032|g in ({+58}Ni,4p|g) (2000ApZY) are inconsistent with a |DJ=1 transition 


level_energy_unit: KEV
level_spin_parity: (19)-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 1071.2|g to (17)-; band assignment 
T$from DSAM for 1071|g (2020Si20). Listed in {+72}Ge({+35}Cl,|apn|g) dataset 


level_energy_unit: KEV
level_spin_parity: (20+)
level_comment:
J$1419.0|g to (18+); band assignment. 2001Zh26 proposed (18+) based on (17+) for 7970 level and |DJ=1 band assignment. 


level_energy_unit: KEV
level_spin_parity: (21)-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=2, E2 1388.0|g to (19)-; band assignment 
T$effective half-life=0.15 ps from DSAM for 1388|g (2020Si20), assuming 100% side feeding. Listed in {+72}Ge({+35}Cl,|apn|g) dataset 


level_energy_unit: KEV
level_spin_parity: (20)+
level_comment:
E$corresponding to 13165 level in ({+58}Ni,4p|g) and 13159 level in ({+37}Cl,p2n|g), deexcited by the 1736.4|g 
J$|DJ=1, E1 1736.4|g to (19)-; possible band head 


level_energy_unit: KEV
level_spin_parity: (22-)
level_comment:
E$corresponding to 11816 level in ({+35}Cl,|ap2n|g) deexcited by the 1107.1|g 
J$|DJ=1, D 1107.1|g to (21)- 


level_energy_unit: KEV
level_spin_parity: (22+)
level_comment:
E$corresponding to 9913 level in ({+58}Ni,4p|g) and ({+37}Cl,p2n|g) deexcited by the 1200.3|g 
J$|DJ=2,Q 1200.3|g to (20)+; band assignment 


level_energy_unit: KEV
level_spin_parity: (23-)
level_comment:
E$corresponding to 10709 level in ({+35}Cl,|ap2n|g) and 13200 level in ({+37}Cl,p2n|g), deexcited by the 609.9|g 
J$|DJ=2, Q 1717.2|g to (21)-; |DJ=1, Q 609.9|g to (22-); band assignment 


level_energy_unit: KEV
level_spin_parity: (23+)
level_comment:
E$corresponding to 14559 level in ({+58}Ni,4p|g) and 14451 level in ({+35}Cl,|ap2n|g), deexcited by the 1293.4|g 
J$1293.4|g to (22+); band assignment 


level_energy_unit: KEV
level_spin_parity: (25-)
level_comment:
E$corresponding to 12591 level in ({+37}Cl,p2n|g), deexcited by the 1384.0|g 
J$|DJ=2, Q 1384.0|g to (23-); band assignment 


level_energy_unit: KEV
level_spin_parity: (24+)
level_comment:
E$corresponding to 15009 level in ({+35}Cl,|ap2n|g) and 15016 level in ({+58}Ni,4p|g), deexcited by the 558.1|g and 1851.4|g 
J$558.1|g to (23+), 1851.4|g to (22+); band assignment 


level_energy_unit: KEV
level_spin_parity: (25+)
level_comment:
E$corresponding to 13158 level in ({+35}Cl,|ap2n|g), 10227 level in ({+58}Ni,4p|g), and 11423 level in ({+37}Cl,p2n|g), deexcited by the 1510.0|g 
J$|DJ=1, D 1510.0|g to (24+); band assignment 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_comment:
J$from the Adopted Levels, based on |g(|q) and |g(lin pol) measurements of 2001Pe05. 1981Pi02 proposed 8- based on M2 from for 988.6|g(lin pol) 
T$|g|g(t) (1982An17) 


level_energy_unit: KEV
level_spin_parity: 14-
level_uncertain: ?
level_comment:
E$reverse ordering of 1036-940 cascade in the Adopted Levels, Gammas gives a different level energy. 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
$Identified as one-phonon mixed-symmetry state 
J$tentative assignment from |g|g(|q) data (2009Ra06) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+108,100}=-0.929 fm{+2} {I1} (stat) {I9} (syst volt) {I8} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
MOMM1$from 1986Ni02 
T$1972Ny01 from ce(K)(296|g,590|g) decay curves (s) for ten half-lives. Others: 8.5 h {i5} (1970Bo22), 8.27 h {i9} (1968Pa24), 8.4 h {i3} (1965Ev04), 8.5 h {i3} (1956Ka25) 
J$L(d,t)=2, log| {Ift}=5.9 to 7/2+ 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: NS
level_comment:
T tentative assignment (1978Ha11) 80|g(t) 
J$80|g is M1+E2; syst with first-excited states of {+103}Pd,{+105}Pd 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_comment:
J$from L({+3}He,|a|g)=4,5 and L(d,t)=(4,5). |g to 15/2-. 1985Sa24 in suggest that the decay only to 15/2- implies a J|p higher than that allowed by the L value (via one step process) and that the excitation might proceed by two-step processes; however, if the (d,t) peak corresponds to this level, the agreement in the L values is correct. 


level_energy_unit: KEV
level_comment:
$|d<r{+2}>{+108,101}=-0.827 fm{+2} {I2} (stat) {I7} (syst volt) {I8} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
J E0 |g to 0+ 
T weighted average of 14.3 ns {i5} (p,2n|g), 14.6 ns {i7} (p,p'|g) and 17 ns {i2} (7.7-min {+102}Ag |e decay). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T deduced from B(E2)(J=second 2+ to third 0+)=0.008 {i2} 
J from |g|g(|q) in {+102}Ag |e decay (7.7 min) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T deduced by the evaluator from B(E2)(J=0 to fourth 2+)=0.0010 {i3} 
J E2+M1 |g to 2+; p'|g(|q) in (p,p'|g) consistent with J=2 only 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
E the existence of a close-lying doublet was established by comparing the I|g(835)/I|g(1555) ratio in different reactions. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T deduced by the evaluator from B(E2)(J=2 to 4')=0.017 {i4} 
J E2 |g to 2+; log| {Ift} in {+102}Ag |e decay (12.9 min) 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: NS
level_comment:
J from |g(|q) in |g(linear pol) in (HI,xn|g), (5+) is proposed by 1981Pi02. J=(4-), proposed by 1976Gr12 from the same reaction, is in contradiction to |g(linear pol) results of 1981Pi02. However, 1981Pi02 take into account the possibility of a very close-lying doublet. This possibility is ruled out by 1986An03. From systematics J=4- most probable 
T from (a,|g(t)) in {+100}Ru(|a,2n) (1986An03) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J from p'|g(|q) in (p,p'|g). J|p=(3-) from B(E3) and level systematics in Coul. ex. 
$B(E3)=0.060 {I6} (2002Ki06, evaluation) 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
J J=(3,4) from p'|g(|q) in (p,p'|g); from log| {Ift} in {+102}Ag |e decay (12.0 min) J=3, and negative parity can be excluded. 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
J E2 to 6+, |DJ=2 for 1228|g (from |g|g(|q) from oriented nuclei in (HI,xn|g), 1976Gr12). Consistent with |g(|q) results of 1981Pi02 in (HI,xn|g) 


level_energy_unit: KEV
level_comment:
E the 1461.1-keV |g-ray attributed to a tentative level at 2018 keV (1971Hn05), was assigned to the 2737-keV level from p|g-coincidence results (1977La16). 


level_energy_unit: KEV
level_comment:
E recalculated by the evaluator. There was an obvious typing error (4742) in the level energy given by 1996Je02 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2): from 1977La16. Used as normalization for all other B(E2)'s obtained by 1986Lu06 
|b{-2}: weighted average of 0.17 {i2} (1979An23,DWBA) and 0.15 {i2} (1980Fo15,CCBA), both from (p,p') at E(p)=6 MeV 
G From dynamic field technique (1980Br01) 
T deduced by the evaluators from B(E2) value. 
Q=-0.2 {i2}, estimated by 1977La16 under the assumption of a positive interference term. For {+102}Ru, however, this interference term was found to be negative (1976Fa02). 
Q=-0.21 {i7} (1977Ma41); value based on the sum intensity for the unresolved 556-keV |g-rays of {+102}Pd and {+104}Pd and determined relative to Q=-0.72 for {+110}Pd. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)(J=first 2+ to second 2+)=0.045 {i3} 
T deduced by the evaluator from B(E2) value and I|g(977)/I|g(1534+977)=0.49 {i4} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
T from |g(t) In(p,p'|g) 
B(E2)(J=second 2+ to second 0+)=5.4|*10{+-2} {i22} 
B(E2)(J=first 2+ to second 0+)<2.4|*10{+-5} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$deduced by the evaluator from B(E2)(J=second 2+ to third 0+)=0.008 {i2} 
B(E2)(J=first 2+ to third 0+)=0.008 {i2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced by the evaluator from B(E2)(J=0 to third 2+)=0.0010 {i3} 
B(E2)(J=0 to third 2+)=0.0010 {i3} 
B(E2)(J=first 2+ to third 2+)=0.0038 {i12} 
B(E2)(J=second 0+ to third 2+)=0.25 {i16} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T deduced by the evaluator from B(E2)(J=2 to 4')=0.017 {i4} 
B(E2)(J=second 2+ to second 4+)=0.023 {i5} 
B(E2)(J=first 2+ to second 4+)=0.017 {i4} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J a large spin, probably 6+, is suggested by the large intensity reduction of the 832-keV K line in the bombardment with 12-MeV protons, compared to 14 MeV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from the weighted average of 12.1 ps {I1}, 12.6 ps {I1}, 12.4 ps {I3}, 12.2 ps {I3}, 11.9 ps {I3}, 12.5 ps {I3}, 11.9 ps {I6}, 11.2 ps {I6}, and 12.0 ps {I5} obtained by direct and indirect gates. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from the weighted average of 2.3 ps {I1}, 2.5 ps {I1}, 2.6 ps {I1}, 2.6 ps {I1} and 2.8 ps {I1} obtained from indirect gates. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$from the weighted average of 1.36 ps {I10}, 1.25 ps {I14}, 1.40 ps {I12}, 1.45 ps {I15}, and 1.25 ps {I13} obtained from indirect gates 2016Ko04 obtain T{-1/2}=1.35 ps {I4}. Final value of half-life includes a correction for slowing down in the target and stopper foil. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$from the weighted average of 1.32 ps {I8}, 1.16 ps {I7}, 1.31 ps {I8} and 1.15 ps {I14} obtained by direct and indirect gates 2016Ko04 obtain T{-1/2}=1.25 ps {I10}. Final value of half-life includes a correction for slowing down in the target and stopper foil. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8-
level_lifetime_unit: PS
level_comment:
T$from the weighted average of 8.2 ps {I4}, 8.5 ps {I5}, 7.8 ps {I4} and 8.5 ps {I5} obtained from direct gates. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9-
level_lifetime_unit: PS
level_comment:
T$from the weighted average of 18.8 ps {I11}, 18.1 ps {I11}, 18.6 ps {I11}, and 19.5 ps {I11} obtained from direct gates 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 10-
level_lifetime_unit: PS
level_comment:
T$from the weighted average of 4.2 ps {I3}, 4.7 ps {I3}, 5.0 ps {I3} and 4.2 ps {I3} obtained by direct gates. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$from 2016Le16 for the 2|e decay of {+102}Pd to the first 2+ state of {+102}Ru at 475.1 keV with 90% confidence level. Limits of T{-1/2} for decays to excited states are (at 90% confidence level): >8.8|*10{+18} y for decay to 943.7,0+ level; >1.4|*10{+19} y for decay to 1103.1,2+. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+108,102}=-0.6782 fm{+2} {I2} (stat) {I66} (syst volt) {I59} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
T$from 1981Va11. Others: 16.961 d {I16} (1975Cz03), 16.9 d {I1} (1968Pa24) 18.4 d {I5} (1969Gr13), 17.5 d {I5} (1954Ri09), 17.0 d {I4} (1953Me24) 
J 3/2+,5/2+ from L(d,p),(d,t)=2; allowed |e transition in 7/2+ {+103}Ag decay with log| {Ift}=5.9 excludes 3/2+. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T from (148|g)(119|g)(t) (1969Ha03). Others: 0.63 ns {I6} T{-1/2} (1972Bf01), 1.9 ns {I4} (1969Ba02) 
J 3/2+,5/2+ from L(d,p)=2; 5/2+ eliminated by 119|g(|q) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$consistent with I|g(M1)-branching mainly to 3/2+ state and negligible |e branching; could be member of a possibly unresolved doublet observed at 500 keV with L(d,t)=(0,2) and L(d,p)=0 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
Could be member of the probably unresolved doublet observed at 499 keV with L(d,t)=(0,2) and L(d,p)=0 
J consistent with M1 |g-decays to 3/2+ and 5/2+ states and negligible |e branching 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
L=2,(0) excitation at 1067 keV in (d,t)(1973RiZL); however not observed by 1980Sc23 in similar (d,t) experiments 
J$(M1,E2) to 5/2+ 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J 5/2+,7/2+,9/2+ from allowed |e transition from 7/2+ {+103}Ag decay with log| {Ift}=5.7; 7/2+,9/2+ excluded if J|p=1/2+ for 499- and 727-keV states 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: FS
level_comment:
J$D+Q |g to 5/2+, log| {Ift}=4.8 from 7/2+ parent. L(d,t)=2 to 1271 keV level may correspond. 1987Ja01 assign 7/2+, not compatible with L=2 
T$from 1987Ja01 in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
J rel |g excit favors 9/2,11/2; M1,E2 decay to 5/2+ state excludes 11/2; if J=9/2 decays to 5/2+ states M1 is ruled out 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
J probably identical with L(d,t)=4 excitation at 2480 keV. If so, consistent with log| {Ift}=5.9 in {+103}Ag |e decay from 7/2+ 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (53/2)
level_comment:
J for a detailed discussion on J|p assignments for the different band members see 1999Ny01. No convincing evidence given by 1993Je02 and 1999Ny01 that this band is a superdeformed band. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
T from |g(t) (1981Va11). Others: 16.96 d {I2} (1975Cz05), 18.4 d {I5} (1969Gr13), 16.9 d {I1} (1968Pa24), 17.0 d {I4} (1953Me24), 17.5 d {I5} (1954Ri09) 


level_energy_unit: KEV
level_comment:
E may be unresolved doublet corresponding to 499-504 keV doublet observed in {+103}Ag |e decay and {+103}Rh(p,n|g) 


level_energy_unit: KEV
level_comment:
If identical to 532-keV level observed in {+103}Ag |e/|b{++} decay, {+94}Zr({+12}C,3n|g) and {+103}Rh(p,n|g) and 533-keV level in (d,t), L assignment is in disagreement with adopted J|p=7/2+ value for this level 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
E observed only by 1975Di09 
T 25 ns {I2} (1975Di09) 67|g(t) pulsed beam 
J$from adopted levels. 
G$from |g(|q,H,t) via {+103}Rh(d,2n|g) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
Branching: I|g(900|g)/I|g(656|g)/I|g(633|g)/I|g(368|g)=100/43 \ {I10}/46 {I11}/26 {I6} (p,n|g), 100/46 {I13}/19 {I8}/31 {I9} ({+103}Ag decay) (1975Di09). Experimental branching ratios via (|a,n|g),({+12}C,3n|g) do not correspond; see 1974Gr07 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$ Following 2008Ro13 this level is clearly a doublet. C{+2}S=0.16 if L=0 and J|p=1/2+ (2008Ro13), C{+2}S=0.29 if L=2 and J|p=3/2+ (2008Ro13) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E other: 610 {I15} (1980Sc23). C{+2}S=0.36 if L=2 and J|p=3/2+ (2008Ro13), C{+2}S=0.29 if L=2 and J|p=5/2+ (2008Ro13) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_uncertain: ?
level_comment:
E other: 800 {I15} (1980Sc23) 
E$Not observed by 2008Ro13 although the energy resolution was much better 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
L$From 2008Ro13. C{+2}S=0.052 if L=2 and J|p=3/2+ (2008Ro13), C{+2}S=0.042 if L=2 and J|p=5/2+ (2008Ro13) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$Considered as tentative by the evaluator. Observed only by 1973RiZL. Cannot be identical with 11/2+ state seen in (HI,xn) and (p,n|g). Also not observed by 2008Ro13 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E other: 1030 {I15} (1980Sc23). C{+2}S=0.15 if L=2 and J|p=3/2+ (2008Ro13), C{+2}S=0.12 if L=2 and J|p=5/2+ (2008Ro13) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
L L=(0) is ruled out if excitation corresponds with 1069-keV level in {+103}Ag |e +|b{++} decay and (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
L=(0) is ruled out if excit corresponds with 1274-keV level observed in {+103}Ag |e +|b{++} decay and {+103}Rh(p,n|g) 


level_energy_unit: KEV
level_comment:
E may be identical with 1943-keV excitation observed by 1973RiZL could be an unresolved doublet as in {+103}Ag |e decay two states at 1953 and 1964 keV, respectively, are observed 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
Not observed by 1999Ny01 
Branching: I|g(267|g)/I|g(148|g)=0.77 {I10} ({+12}C,3n|g) disagrees with 0.47 {I2} ({+103}Ag decay), 0.49 {I4} (p,n|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
J$from Adopted Levels of {+103}Pd in ENSDF database (2009 update) 
T$from 357.45|g(t) in 2021Ri01. Other: 16.991 d {I19} from Adopted Levels of {+103}Pd in ENSDF database (2009 update) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
T$derived from eight measurements using the 4 depopulating transitions and the centroid shift method and deconvolution method (2022Iv01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOME2$other: -0.45 {I10}. Method: Coul. ex. reorientation precession technique. 
MOMM1$IMPAC. Other: see 1989Ra17. 
J$L(p,t)=2 
T$from B(E2)(0-2)=0.535 {I35} (1987Ra01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$from B(E2) in Coul. ex. 
J$log| {Ift}=6.1 from 2+. 1794|g to 0+ g.s., M2 |g would not be likely, M1 |g to 2+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$others: 0.46 {I7} (1956Te26), 0.55 {I4} (1958St32), 0.61 {I9} (1962Er05), 0.55 {I5} (1968MiZZ), 0.51 {I5} (1970Ch01) 
Q=-0.25 {I12} or +0.05 {I11} (1970Ch01) 
T$from B(E2) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$ uncertainty in g factor is relative to that of {+106}Pd (2011Ch23). Recommended g=+0.446 {I30} (2011Ch33), from present result and and previous measurement 
T$ from Adopted Levels for {+104}Pd in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+108,104}=-0.4464 fm{+2} {I2} (stat) {I45} (syst volt) {I38} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$L=2 in {+106}Pd(p,d) (1975An06); Also: L=2 in {+106}Pd(d,t) 1980Sc23 
$<r{+2}>=4.5128 fm{+2} {I25} (2004An14) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$L=2 in {+106}Pd(p,d) (1975An06); 280.54|g M1+E2 to 5/2+; 64.072|g M1(+E2) from 1/2+ 
T$weighted average of 45 ps {I5} from B(E2)|^(280.54|g)=0.0095~{I5} in Coulomb excitation with |a(280.54|g)=0.0238~{I4}, and 67 ps {I17} from |g|g(t) in {+105}Ag |e decay (41.29~d) (1974Be71) 
MOMM1$from IPAC in 1981Al19 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$L=4 in {+106}Pd(p,d) (1975An06); 306.30|g M1+E2 to 5/2+ 
T$from B(E2)|^(306.30|g)=0.00117~{I11} in Coulomb excitation, and |a(306.30|g)=0.0188~{I3} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$L=2 in {+106}Pd(p,d) (1975An06); 38.77|g M1(+E2) to 3/2+, and 319.24|g M1+E2 to 5/2+ 
T$weighted average of 38 ps {I2} in 1962Me07, 48 ps {I7} in 1971Sh21, 40 ps {I10} from |b-|g(t) in {+105}Rh |b{+-} decay (1974Be71), 20 ps {I3} from B(E2)|^(319.24|g)=0.0082~{I4} in Coulomb excitation 
MOMM1$from IPAC in 1981Al19 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
J$L=0 in {+106}Pd(p,d) (1975An06); 344.61|g E2 to 5/2+ 
T$weighted average of 1.01 ns {I5} from 618-344|g(t) and 22X-344|g(t) in {+105}Ag |e decay (41.29~d) (1970Sc10), 0.88 ns {I5} from |g|g(t) in {+105}Ag |e decay (41.29~d) (1974Be71), 801 ps {I64} in {+105}Ag |e decay (41.29~d) (1969Ka02) and 1.07 ns {I24} from B(E2)|^(344.61|g)=0.0022~{I5} in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_lifetime_unit: PS
level_comment:
J$L=2 in {+106}Pd(p,d) (1975An06); 442.25|g M1+E2 to 5/2+ 
T$from B(E2)|^(442.25|g)=0.185~{I7} in Coulomb excitation, and |a(442.25|g)=0.00756~{I11}; Others: 3.71 ps {I9} from DSAM in 1972SiZP; 3.8 ps {I10} from DSAM in 1971SiYG, and 3.81 ps {I14} from RDDS in 1971SiYQ 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$L=5 in {+106}Pd(p,d) (1975An06); 182.92|g M2 to 7/2+ 
T$weighted average of 36.1 |ms {I4} from 155.39|g-182.85|g(t) in 1970BlZT, 34.2 |ms {I6} in 1965Mc03, 33 |ms {I6} in 1956Ve03, and 36 |ms {I3} in 1958Du80 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$L=(2) in {+104}Pd(d,p) (1963Cu02); 560.79|g M1+E2 to 5/2+; 6534.0|g from the (1/2+) resonance 
T$from DSA (1974Er05); Others:<35~ps from B(E2)|^(560.79|g)=0.0095~{I9} in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$155.38|g E2 to 11/2-, 325.43|g E1 to 5/2+, and 644.63|g E1+M2 to 5/2+ 
T$from |g|g(t) in {+105}Ag |e decay (41.29 d) 
MOMM1$from IPAC in 1981Al19 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L=2 in (p,d) (1975An06); 331.58|g M1+E2 to 5/2+, and 370.28|g M1+E2 to 3/2+ 
T$from B(E2)|^(650.78)=0.0078~{I6} in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
J$L=0 in (p,d) (1975An06); 392.73|g M1+E2 to 3/2+, and 673.24|g E2 to 5/2+ 
T$from B(E2)(673.24|g)=0.0082~{I9} in Coulomb excitation; Others:>2~ps from DSA (1974Er05) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L=2 in {+106}Pd(p,d) (1975An06); 421.03|g M1(+E2) to 7/2+, and 446.8|g M1+E2 to 3/2+ 
T$from B(E2)|^(727.28)=0.0057~{I25} in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J$L=4 in {+106}Pd(p,d) (1975An06); 781.3|g E2 to 5/2+, 339.4|g M1(+E2) to (7/2)+; band member 
T$weighted average of 1.7 ps {I4} from DSAM in 1971SiYG, 1.11 ps {I28} in 1974Er05, 1.80 ps {I28} from RDDS in 1971SiYQ, 1.4 ps {I1} in 1970GeZY, and 1.94 ps {I13} from B(E2)|^(781.3)=0.101~{I7} in Coulomb excitation; Other: 2.9 ps {I3} from DSAM in 1972SiZX 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L=0 in {+106}Pd(p,d) (1975An06); 401.75|g to 3/2+, 962.45|g to 5/2+ 
T$from B(E2)|^(962.45|g)=0.008~{I5} in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$L=(0) in {+104}Pd(d,p) (1963Cu02); 360.72|g E1 to 5/2+, 414.85|g (E1) to 1/2+, 807.57|g E1(+M2) to 3/2+ 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
J$L=5 in {+106}Pd(d,t) (1980Sc23); 140.0|g to (11/2)+, 399.9|g to (11/2+), 628.1|g to 9/2+; assumed near-yrast level 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T$from 618|g-344|g(t) and 22X-344|g(t) in 1970Sc10; Others: 0.88 ns {I5} in 1974Be71, 0.801 ns {I64} in 1969Ka02 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
T$443-645|g(t) with cooled NaI detectors (1981Al19) 
$g=-0.427~{I25} from IPAC in 1981Al19 
CONF$2{++}~#|nh{-11/2} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
BE2$0.0095~{I5} 
BE2$weighted average of 0.0085~{I7} (1985Ta19), 0.0073~{I16} (1981Ch42), 0.0110~{I10} (1971Bo08); 0.0097~{I16} (1970GeZQ); Other: 0.002~{I1} (1968Ga22), |<0.013 (1962Va20) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
BE2$0.00117~{I11} 
BE2$weighted average of 0.0012~{I1} (1985Ta19), 0.0012~{I2} (1971Bo08), 0.0011~{I1} (1970GeZQ), 0.004~{I1} (1968Ga22); Other: 0.0011~{I2} (1970GeZQ) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
BE2$0.0082~{I4} 
BE2$weighted average of 0.0073~{I8} (1985Ta19), 0.0095~{I20} (1981Ch42), 0.0081~{I10} (1971Bo08), 0.0088~{I7} (1970GeZQ), 0.008~{I2} (1968Ga22) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
BE2$0.0022~{I5} 
BE2$weighted average 0.0023~{I3} (1985Ta19), 0.0015~{I3} (1971Bo08), 0.0027~{I3} (1970GeZQ), 0.020~{I4} (1968Ga22) Other: 0.0028~{I3} (1970GeZQ),|<0.026 (1962Va20) 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
T$3.8 ps {I10} from DSAM in 1971SiYG, 3.81 ps {I14} from RDDS in 1971SiYQ 
BE2$0.185~{I7} 
BE2$weighted average of 0.190~{I16} (1985Ta19), 0.162~{I27} (1981Ch42), 0.165~{I13} (1971Bo08), 0.197~{I10} (1970GeZQ); Others: 0.18~{I4} (1968Ga22), 0.19~{I1} (1970GeZY) , 0.21 (1962Va20) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
T$1.9 ps {I5} (1974Er05) 
BE2$0.0095~{I9} 
BE2$weighted average of 0.0092~{I14} (1985Ta19), 0.0111~{I38} (1981Ch42), 0.0075~{I10} (1971Bo08), 0.0110~{I7} (1970GeZQ), 0.006~{I2} (1968Ga22) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
BE2$0.0078~{I6} 
BE2$weighted average of 0.0086~{I17} (1985Ta19), 0.0066~{I13} (1971Bo08), 0.0079~{I7} (1970GeZQ), 0.017~{I5} (1968Ga22) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
T$>2~ps (1974Er05) 
BE2$0.0082~{I9} 
BE2$weighted average of 0.0089~{I16} (1985Ta19), 0.0057~{I11} (1971Bo08), 0.0092~{I7} (1970GeZQ), 0.005~{I3} (1968Ga22) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
BE2$0.0057~{I25} 
BE2$weighted average of 0.0043~{I9} (1985Ta19), 0.0024~{I6} (1971Bo08), 0.0123~{I8} (1970GeZQ), 0.010~{I3} (1968Ga22). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
T$1.7 ps {I4} from DSAM in 1971SiYG, 1.80 ps {I28} from RDDS in 1971SiYQ, 1.11 ps {I28} (1974Er05) 
BE2$0.101~{I7} 
BE2$weighted average of 0.0966~{I80} (1985Ta19), 0.119~{I30} (1981Ch42), 0.0827~{I83} (1971Bo08); 0.113~{I6} (1970GeZQ); Other: 0.059 (1962Va20) 


level_energy_unit: KEV
level_comment:
$|d<r{+2}>{+108,105}=-0.3769 fm{+2} {I3} (stat) {I35} (syst volt) {I90} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2)=0.670 {I19} in Coul. ex. Others: 13.6 ps {I44} via (|g,|g') (1977Ga06) 14.3 ps 4 from (e,|e') (1991We15) 
MOMM1$Other: +0.80 {I4} (1989Ra17) 
J L(p,t)=2 
MOME2 Deduced from (e,e') E=183,250 MeV (1973Ho05). Others: -0.56 {I8} or -0.41 and -0.51 {I7} (1989Ra17) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2)=0.0175 {I13} in Coul. ex. with branching (1128|g)=35.2% {I6}. 
J from E2 to g.s. 
MOMM1$Other: +0.60 {I12} (1989Ra17) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J from E0 to g.s. 
B(E2)[2+(511 keV) to 0+(1133 keV)]=0.021 {I4}: weighted average of 0.018{I4} (1969Ro05) and 0.026 {I5}(1995Sv01) in Coul. ex. 
T from B(E2)[2+(511 keV) to 0+(1133 keV)]=0.021 {I4} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T from B(E2)[2+ (511 keV) to 4+(1229 keV)]=0.38 {I3} 
$ B(E2)[2+ (511 keV) to 4+(1229 keV)]=0.38 {I3} weighted average of B(E2)[2+ (511 keV) to 4+(1229 keV)]=0.39 {I5} (1969Ro05) and 0.38 {I4} (1995Sv01). Other: 0.51 {I9} (1962Ec03) 
J L(p,t)=4 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J L(p,t)=0 
T$From measured B(E2)(W.u.)=2.4 +0.4-0.3 and adopted branching for 1196|g in Coul. ex. (1995Sv01) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J L(p,p')=4 
T$From measured B(E2)(W.u.)=35 {I+5-4} and adopted branching for 804|g in Coul. ex. (1995Sv01) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J E2 to 4+. J=6 from strong E2 in cascade to g.s. 
T$From measured B(E2)(W.u.)=89 {I+10-13} and adopted branching for 848|g in Coul. ex. (1995Sv01) via ({+13}C,3n|g) and (847|g)(|q) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T from B(E3)=0.128 {I19} (1969Ro05) and adopted gamma branching 
J E1 to 2+. J=3 from (1572|g)(512|g)(|q), 1572|g(|q), J=2-,3- from av res n capture 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: NS
level_comment:
T from |a|g(t) in {+104}Ru(|a,2n|g) 
J E1 to 4+, M1+E2 to 3-. J=4 from (748|g)(1046|g)(|q); 222|g(|q). 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J L(p,p')=5. {I1},4- from av res. |g to 4+ eliminates J=1. In contradiction with L(d,p)=0+2 for unresolved doublet at 2578 keV. L(p,p') eliminates also J|p=4- 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J J=0 from (1062|g)(1050|g)(|q), (2113|g)(512|g)(|q) |p=+ from log| {Ift}=5.76 from {+106}Rh (J|p=1+) |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_comment:
J L=2 (d,p). J=(2,3)+ from av res 
Discrepancies exist for branching ratios of the 2626 and 3054 keV levels in (n,|g) and (n,n'|g) reactions due to unresolved doublet of 1498|g deexciting both levels 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J L(p,p')=(4) could be unresolved doublet with 2713.6 level L=2+0 for may be unresolved doublet in (d,p) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T from (K| x ray)(|g)(t) in {+106}Ag |e decay (8.28 d) 
J E2 to 3+. J=5 from (1199|g)(1046|g)(|q), (1528|g)(717|g)(|q), (linear pol 1199|g)(1046|g)(|q) and |g-deexcitation pattern 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T from (K x-ray)(|g)(t) (1968We16) in {+106}Ag |e decay (8.28 d) 
J E1 to 4-. J=5 from (linear pol 1394|g)(1046|g)(|q) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J E2 to 6+. J=8 from strong E2 in cascade to g.s. in {+96}Zr({+13}C,3n|g) 
T$From measured B(E2)(W.u.)=107 {I+13-26} and adopted branching for 886|g in Coul. ex. (1995Sv01) in ({+13}C,3n|g) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T from |a|g(t) in {+104}Ru(|a,2n|g) 
J suggested from (205,299|g)(|q), 299|g linear pol data and |g-decay pattern 


level_energy_unit: KEV
level_spin_parity: 9(-)
level_lifetime_unit: NS
level_comment:
T from |a|g(t) in {+104}Ru(|a,2n|g) 
J J=9 from |DJ(285|g,D+Q) to(8-)=-1 and |DJ(463|g,D+Q)=-1 to (8-) in ({+13}C,3n|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
G$ From |g|g(|q,H). Weighted average of 0.384 {I33} (1968Jo17), 0.349 {I27} (1968Bo15), 0.369 {I29} (1970Si20), 0.382 {I28} (1972Jo06) Others: 1965Ko12, 1966Au06, 1967Mu09 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
From (873|g)(1128|g)(|q,H): g-factor is weighted average of 0.307 {I92} (1970Si20), 0.285 {I54} (1968Bo15); 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
J if level is identical with adopted 3161.0 level then J=0 for that level proposed from (2651|g)(512|g)(|q) in {+106}Rh |b{+-} decay is in conflict with adopted J|p=(1,2+) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
Several types of 2|b g.s. decay of {+106}Cd have been investigated to this level with the following corresponding T{-1/2}: T{-1/2}(2|n)>4.8|*10{+19} y (90% c.l.) (2006St11); Process: 2|e T{-1/2}(2|n)|>5.0|*10{+18} y (90% c.l.) (2003Da24); Process: |b{++}|b{++} T{-1/2}(0|n)|>1.4|*10{+19} y (90% c.l.) (2003Da24); Process: |b{++}|b{++} T{-1/2}(2|n)|>5.8|*10{+17} y (90% c.l.) (2003Da24); Process: 2|e T{-1/2}(2|n)>5.8|*10{+17} y (90% c.l.) (1995Ge14); Process: 2|e T{-1/2}(2|n)|>1.2|*10{+18} y (90% c.l.) (2003Da24); Process: |e |b{++} T{-1/2}(0|n)|>7.0|*10{+19} y (90% c.l.) (2003Da24); Process: |e |b{++} T{-1/2}(0|n)|>8.0|*10{+18} y (90% c.l.) (2003Da24); Process: 2|e T{-1/2}(0|n)>1.5|*10{+17} y (90% c.l.) (1984No09); Process: 2|e T{-1/2}(0|n+2|n))>2.4|*10{+20} y (90% c.l.) (1999Be81); Process: |b{++}|b{++} T{-1/2}(2|n)|>4.1|*10{+20} y (90% c.l.) (1999Be81); Process: (|e |b{++}) T{-1/2}(0|n)|>3.7|*10{+20} y (90% c.l.) (1999Be81); Process: (|e|b{++}) T{-1/2}(0|n+2|n))>6.6|*10{+18} (1996Ba46) Process:|b{++}|e T{-1/2}(0|n+2|n))>10|*10{+18} (1996Ba46) Process:|b{++}|b{++} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
Several types of 2|b{++} {+106}Cd g.s. decay of have been investigated to this level with the following corresponding T{-1/2}: T{-1/2}(2|n)>3.9|*10{+19} y (2006St11); Process: 2|e T{-1/2}(0|n)|>6.0|*10{+18} y (90% c.l.); (2003Da24); Process: |b{++}|b{++} T{-1/2}(0|n)|>3.1|*10{+19} y (90% c.l.); (2003Da24); Process: |e |b{++} T{-1/2}(2|n)>3.0|*10{+19} y (90% c.l.); (2006St11); Process: 2|e T{-1/2}(0|n+2|n))>1.6|*10{+20} y (90% c.l.) (1999Be81); Process: |b{++}|b{++} T{-1/2}(0|n+2|n))>2.6|*10{+20} y (90% c.l.) (1999Be81); Process: |e |b{++} T{-1/2}(0|n+2|n))>3.5|*10{+18} y (90% c.l.) (1996Ba46); Process: 2|e T{-1/2}(0|n+2|n))>7.3|*10{+18} y (90% c.l.) (1996Ba46); Process: |b{++}|e T{-1/2}(0|n+2|n))>10|*10{+18} y (90% c.l.) (1996Ba46); Process: |b{++}|b{++} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
Several types of 2|b{++} {+106}Cd g.s. decay have been investigated to this level with the following corresponding T{-1/2}: T{-1/2}(0|n)|>1.4|*10{+19} y (90% c.l.); (2003Da24); Process: |e |b{++} T{-1/2}(2|n)>4.9|*10{+19} y (90% c.l.); (1999Be81); Process: 2|e T{-1/2}(0|n+2|n))>1.4|*10{+20} y (90% c.l.) (1999Be81); Process: |e|b{++} T{-1/2}(0|n+2|n))>5.1|*10{+18} y (90% c.l.) (1996Ba46); Process: 2|e T{-1/2}(0|n+2|n))>7.8|*10{+18} y (90% c.l.) (1996Ba46); Process: |b{++}|e 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
$T{-1/2}(2|n)>5.8|*10{+19} y (90% c.l.)(2006St11); Process: 2|e T{-1/2}(0|n)|>1.4+19 y (90% c.l.) (2003Da24); Process: |e |b{++} T{-1/2}(2|n)>7.3|*10{+19} y (90% c.l.)(1999Be81); Process: 2|e T{-1/2}(0|n+2|n))>1.1|*10{+20} y (90% c.l.) (1999Be81); Process: |e|b{++} T{-1/2}(0|n+2|n))>6.2|*10{+20} y (90% c.l.) (1996Ba46); Process: 2|e T{-1/2}(0|n+2|n)) 8.1|*10{+18} y (90% c.l.) (1996Ba46); Process:|b{++}|e 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
B(E0; 1706 to g.s.)/B(E2; 1706 to 511)<0.038 
B(E0; 1706 to g.s.)/B(E2; 1706 to 1128)<0.003 
B(E0; 1706 to 1133)/B(E2; 1706 to 511)<2.0 
B(E0; 1706 to 1133)/B(E2; 1706 to 1128)<0.13 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
B(E0; 2001 to g.s.)/B(E2; 2001 to 511)=12 {I3} 
B(E0; 2001 to g.s.)/B(E2; 2001 to 1128)=0.020 {I4} 
B(E0; 2001 to 1133)/B(E2; 2001 to 511)<37 
B(E0; 2001 to 1133)/B(E2; 2001 to 1128)<0.28 
B(E0; 2001 to 1706)/B(E2; 2001 to 511)<220 
B(E0; 2001 to 1706)/B(E2; 2001 to 1128)<1.7 


level_energy_unit: KEV
level_spin_parity: 2+,3+
level_uncertain: S
level_comment:
E deduced S(n)=9562.8 {I11} where E|g is corrected for recoil-energy loss and res E(n)|=0 (1970Bo29) 
1971Co19 obtained av reduced widths (I|g/E|g{+3}) of E1 and M1 branchings from J=2 and/or 3 res 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J if level corresponds to adopted 3069.9 level, then J|p=(2-,3-) from (n,|g) in conflict with adopted value 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2)=0.670 {I19} 
BE2 Weighted average of 0.650 {I40} (1989Lo08) 0.689 {I37} (1971Bo08), 0.61 {I6} (1970Ch01), 0.71 {I4} (1969Ro05), 0.646 {I45} (1958St32), 0.626 {I60} (1995Sv01). Others: 0.61 {I9} (1962Er05), 0.59 {I9} (1956Te26) 
Deduced Q: -0.56 {I8} or -0.41 {I8} (1972Lu08) via ({+32}S,{+32}S'|g) E=56 MeV; 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2)=0.0175 {I13} and adopted gamma branching 
BE2 From weighted average of 0.0180 {I15} (1969Ro05), 0.0166 {I37} (1961St02), 0.0167 {I34} (1962Ga10) and 0.0165 {I30} (1995Sv01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
B(E2)[2+(511 keV) to 0+(1133 keV)]=0.021 {I4}: weighted average of 0.018{I4} (1969Ro05) and 0.026 {I5}(1995Sv01) 
T from B(E2)[2+(511 keV) to 0+(1133 keV)]=0.021 {I4} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T from B(E2)[2+ (511 keV) to 4+(1229 keV)]=0.38 {I3} 
$ B(E2)[2+ (511 keV) to 4+(1229 keV)]=0.38 {I3} weighted average of B(E2)[2+ (511 keV) to 4+(1229 keV)]=0.39 {I5} (1969Ro05) and 0.38 {I4} (1995Sv01). Other: 0.51 {I9} (1962Ec03) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T from B(E3). Other 0.5 ps {I2} from Doppler-broadened 1572|g lineshape (1969Ro05) 
BE3$B(E3)=0.128 {I19} (1969Ro05) 
BE3 Calculated for I|g(1572|g) branching=91.9% {I12} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Value is near the limit of DSAM and exhibits large uncertainty. T{-1/2}=1.39 ps {I21} from B(E2)(W.u.)=0.14 {I12} in Coulomb Excitation from 1995Sv01: Nucl.Phys. A584, 547 (1995) was used in the calculation for |r{+2}(E0) by authors (2016Pe06) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$From |t=460 fs {I+190-110} (Different from their earlier value in 2016Pe06 (Eur.Phys.J. A 52, 96)). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+108,106}=-0.2277 fm{+2} {I2} (stat) {I21} (syst volt) {I24} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=17 ps {I8} (2017Al45) from (621.9|g)(511.9|g)(t). This value can be compared with T{-1/2}=12.2 ps {I4} in {+106}Pd Adopted Levels in the ENSDF database; and mean lifetime |t=17.50 ps {I+48-45} in 2016Pr01 (At. Data Nucl. Data Tables 107, 1) evaluation. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: Y
level_comment:
T 6.5|*10{+6} y {I3} specific activity (1969Fl04) fission product chem, ms. Other: |?7|*10{+6} y (1949Pa17) 
J L=2 (d,p),(d,t), S(d,t)/S(d,p); 5/2+ characteristic of odd-mass {+101}Pd-{+111}Pd g.s. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: US
level_comment:
T from (452|g)(116|g)(t) 1969Gr18. Other: 1978Ho06 
J L=0 (d,p),(d,t) 
For empirical systematics of regional E2 isomerism between s1/2 and d5/2 states, see 1978Ho06 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$from 1957St87. Others: 23 s {I2} (1952Fl10), 23 s (1958Sc03) 
E$low-lying 11/2- isomerism: 25-ns {+103}Pd at 785, 36-|ms {+105}Pd at 489, 4.7-min {+109}Pd at 189, 5.5-h {+111}Pd at 172 
J$L=5 (d,p),(d,t), E3(214|g) to g.s., T{-1/2}, configuration=h11/2 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$L(d,p)=1. |g to 5/2+. If (d,p) and |b{+-} decay are populating different levels, then J|p=1/2-,3/2- for E=1473 {I7} and J|p=1/2+ to 9/2+ for E=1472.3. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2 
T$from B(E2) in Coulomb excitation 
MOMM1$from 1980Br01, 1989Ra17. Other: +0.64 {i6} (1985ThZY) 
MOME2$from 1989Ra17. Other: -0.70 {i27} (1981Ko06) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$|a,|g(|q) in Coulomb excitation 
T$weighted average of 6.8 ps 11 from B(E2) in Coulomb excitation, and 6.1 ps 4 from B(E2) in (e,e'). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
E$transition not observed. Energy is from E(level) difference. 
J$L(t,p)=0 
T$from B(E2) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$|g's to 2+. Not fed in decay of 2.382-min {+108}Ag, J|p=1+, or 438-y {+108}Ag, J|p=6+. Not seen in Coulomb excitation, (t,p), (p,p') or (d,d'). Analogy to {+104}Pd, {+106}Pd in (n,n'|g) (1975Go11) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
T$from B(E2) in Coulomb excitation 
J$multiple Coulomb excitation. Comparison with boson expansion model. |g to 2+. Excited in (d,d'), (p,p'), (p,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(p,p')=3 
T$from Doppler broadening in Coulomb excitation 
BE3$from in Coulomb excitation for I(1612|g)=100% 
B3$from (p,p') 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
Charge distribution parameters: half-density radius=5.227 fm {i19}, surface thickness=2.545 fm {i29}, rms radius=4.585 fm {i9} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 deduced from anharmonic model fit to form factor 
MOME2 deduced from matrix elements extracted from an anharmonic analysis of form factor 
T from B(E2) and |a=0.0089 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$B(E2)(931-434)/B(E2)(434-g.s.)=1.37 {i7} 
T$from B(E2)(931-434)/B(E2)(434-g.s.), with B(E2)(434-g.s.) of 1978Ar07 and %I|g(497|g)=80.2 {I2}, |d(497|g)=-3.1 {i4} 
BE2$deduced from anharmonic model fit. Authors point out that the 2+ form factor is not defined over a wide enough momentum transfer range to reliably extract B(E2) (B(E2)=0.0170 {i14} from Coulomb excitation) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
S others: 0.24 {i2} (1979An23), 0.24 (1975Ko12) from DWBA; 0.25 {i1} (1966Ro04), 0.26 (1975Ko12) from coupled-channel calculation 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2). 
BE2$weighted average of values of 1969Ro05 (0.76 {i5}), 1971Bo08 (0.79 {i5}), 1971Ha08 (0.70 {i7}). 1962Ec01 (0.78 {i6}), 1958St32 (0.74 {i5}), 1962Er05 (0.82 {i12}), 1956Te26 (0.78 {i12}), and 0.76 {I+11-7} (1995Sv01) 
G from 1980Br01, |g(|q,h), recoil through thin magnetized Fe layer on Cu backing. Dynamic field calibrated using g-factor=0.398 {i21} for 2+ level in {+106}Pd (1989Ra17). Others: 0.37 {i4} (1974Hu01), |g(|q,h), IMPAC. Transient field calculated in framework of Lindhard-Winther model with inclusion of decays-in-flight corrections; 0.40 {i6} (1969He11), IMPAC. Authors' value (0.30 {i4}) recalculated by 1974Hu01 to correct for effect of static- and transient-field angular shifts. Note, |g({+106}Pd)=0.32 {i6} (1974Hu01), 0.37 {i7} (1969He11 as corrected by 1974Hu01); 0.42 {i5} (1979LaZL) 
MOME2 weighted average of values of 1971Ha08 (-0.58 {i13}), 1972Lu08 (-0.51 {i6}) using reorientation effect, and 1976Ha21 (-0.66 {i18}) using the reorientation precession technique. 1976Ha21 determined that excitation via the second 2+ level interferes constructively with the direct excitation. The above authors also give Q values for the case of destructive interference. Others: 1971WaZT determined Q=Q({+110}Pd 2+)+0.11 {i4} and 1977Ma41 determined Q({+110}Pd 2+)+0.24 {i5} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J x,931|g(|q) consistent only with J=2 (1969Ro05) 
T$from B(E2) and %I|g(931|g)=19.4 {I12} 
BE2$weighted av: 0.0096 {I10} (1995Sv01), 0.0170 {I14} (1969Ro05), 0.0095 {i15} (1961St02), 0.0112 {i26} (1962Ga10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2$B(E2)(614|g 2+ to 4+) weighted av: 0.20 {I4} (1995Sv01), 0.50 {I7} (1969Ro05) 
T$from B(E2) and I|g(614|g)=100% 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
BE2$B(E2)(619|g 2+ to 0+)=0.031 {I3}. weighted av: 0.032 {I3} (1995Sv01), 0.027 {I6} (1969Ro05) 
T$from B(E2) and I|g(618|g)=100% 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
BE2$B(E2)(880|g 2+ to 0+)<0.00072; B(E2)(383|g 2+ to 0+)<0.0115 
T$from B(E2)(880|g) with I|g (880|g)=82.7% {i17} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$B(E2)(389|g 2+ to 0+)=0.90 {I+10-9}; B(E2)(393|g 4+ to 2+)=0.077 {I+19-13}; B(E2)(510|g 2+ to 2+)=0.035 {I+13-16}; B(E2)(1007|g 2+ to 2+)=0.0051 {I+29-6}; B(E2)(1441|g 0+ to 2+)=0.00144 {I+16-21} 
T$from B(E2)(1441|g) with I|g (1441|g)=15.6% {i27} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2$B(E2)(184|g 2+ to 4+)=0.020 {I+15-6}; B(E2)(576|g 4+ to 4+)=0.092 {I+17-14} B(E2)(694|g 2+ to 4+)=0.303 {I+35-30}; B(E2)(1191|g 2+ to 4+)|<0.0016 
T$from B(E2)(694|g) with I|g (694|g)=80% {i4} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2$B(E2)(331|g 4+ to 4+)=0.006 {I+15-6}; B(E2)(908|g 4+ to 4+)<0.0054; B(E2)(1025|g 2+ to 4+)=0.016 {I+6-4} 
T$from B(E2)(1025|g) with I|g (694|g)>68%. Value chosen is the midpoint of values for branching of 68% and 100% 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$from Doppler-broadening of 1612|g in coin spectrum (1969Ro05) 
BE3$from yield of 1612|g and assumption that %I|g(1612|g)=100 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
J the 1048 {i4}+ level could not be resolved from the 1053 level; however, the 4+ level is not expected to be excited since the {+109}Ag g.s. configuration=((|p 2p{-1/2}){+-1}(|p 1g{-9/2}){+-2})+((|p2p{-3/2}{+-1})(|p 1g{-9/2}{+-2})) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$ uncertainty in g factor is relative to that of {+106}Pd (2011Ch23). Recommended g=+0.342 {I22} (2011Ch33), from present result and and previous measurement 
T$ from Adopted Levels for {+108}Pd in ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
J$L(d,p)=L(d,t)=2 and direct |b-feeding to J|p=7/2+ in {+109}Ag 
T$using the Limitation of Relative Statistical Weight method and 13.45 h 1 (2015Kr07), 13.7012 h 24 (1990Ab06), 13.404 h 8 (1988Ba60), 13.85 h 17 (1983Ch42), 13.427 h 14 (1977Gi11), 13.67 h 7 (1970Bo22), 13.47 h {i1} (1962Br15), 13.45 h {i1} (1959St28). Others: 13.99 h {i16} (1958Gu09), and 14.1 h {i3} (1948Mo33). 
CONF$a mixture between |n5/2+[413] and |n5/2+[402] Nilsson configurations. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
J$L(d,p)=L(d,t)=0. {I113}.4|g E2 to 5/2+ 
T$from (178.0|g)(113.4|g)(t) measurements by 1978Ka10 in {+109}Rh |b{+-} decay 
CONF$K|p=1/2+, |n1/2[411] Nilsson configuration. Assignment is tentative 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
J$L(d,p)=L(d,t)=5, 188.990|g E3 to 5/2+ 
T$using the Limitation of Relative Statistical Weight method and 4.694 m 2 (2015Kr07), 4.696 m 3 (1990Ab06), 4.750 min {I4} (1992An19), 4.663 min {i11} (1992KaZM), 4.6 min {i4} (1970Bo22), 4.7 min {i1} (1967Na18), 4.69 min {i1} (1959St28), and 4.75 min {i5} (1957St87) 
CONF$Most likely the K|p=3/2-, |n3/2-[541] (h{-11/2}) Nilsson configuration 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
J$direct feeding in {+109}Rh |b{+-} decay (J|p=7/2+) ; L(d,t)=2, L(d,p)=0+2; average res rules out 7/2+ and 9/2+; 35.34|g M1 to 3/2+, 81.78|g E1(+M2) to (7/2)- 
T$Other: 0.57 ns {I15} from 1998Lh02 using the centroid-shift method of delayed-coincidence. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$373.80|g E2 to 0+; L(t,p), L(|a,|a')=2 
T$Weighted average of 45.5 ps {I17} (from recoil-distance technique in 1989Ko40), 43.6 ps {I8} (from adopted B(E2)|^=0.876 {I16}) and 46 ps {I6} (from recoil distance Doppler-shift technique in 2008De30) 
MOMM1$using dynamical field technique in 1980Br01. Others: +0.6 {I4} using time integral perturbed angular correlations in 2005Sm08 and 2004Sm04 (T{-1/2}=46.6 ps {I14} was used), +0.70 {I6} using transient field technique in 1985ThZX, 0.74 {I6} using recoil into gas in 1979LaZL, 0.68 {I8} (in Fe host) and 0.72 {I8} (in alloy host) using transient field implantation perturbed-angular-correlation technique in 1974Hu01 
MOME2$using reorientation precession technique in 1976Ha21 (-0.60 {i14} for destructive interference). Others: -0.47 {i3} from (e,e') in 1991We15, -0.28 {i3} from (e,e') in 1973PeYX, -0.55 {i8} or -0.35 {i8} from Coulomb excitation in 1972Lu08, -0.72 {i8} or -0.45 {i8} from Coulomb excitation in 1971Ha08, -0.48 {i5} or -0.23 {i5} from Coulomb excitation in 1970Be45 
BE2$Weighted average of 0.87 {I3} (1991We15), 0.80 {I7} (1976Li19) in {+110}Pd(e,e'), 0.82 {I5} (symmetrized from 0.85 {I+2-7} in 1989SvZZ), 0.88 {I6} (1971Bo08), 0.82 {I8} (1971Ha08), 0.91 {I6} (1969Ro05), 0.91 {I3} (weighted average of 0.92 {I6}, 0.90 {I6}, 0.91 {I6} and 0.91 {I6} in 1962Ec01), 0.94 {I8} (1962Ga10) and 0.86 {I6} (1958St32). Others: 0.78 in 1962Er05 and 0.91 in 1962Ri09 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$439.76|g E2+M1 to 2+ and 813.7|g to 0+; L(t,p)=2 
T$From 1989Ko40 using the recoil-distance technique. Others: 18.6 {I+5-9} (1989SvZZ) and 14.0 {i18} from 1969Ro05 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$547.04|g E2 to 2+; member of the g.s. band; L(t,p)=4 
T$From 1989Ko40 using the recoil-distance technique. Others: 4.5 ps {I+3-1} (1989SvZZ) and 3.8 ps {i6} (1969Ro05) 
$B(E4)=91|*10{+-4} {I14} from (e,e') in 1991We15 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=0; 572.89|g to 2+; non-observation of |g-ray transition to g.s (J|p=0+); assignment in {+110}Pd(p,p'),(d,d'),(pol d,d') 
T$From 1989Ko40 using the recoil-distance technique. Others: 10.6 ps {I+4-8} (1989SvZZ) and 8.0 ps {i14} (1969Ro05) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$L(t,p)=0; 796.83|g to 2+; non-observation of |g-ray transition to g.s (J|p=0+); assignment in {+110}Pd(p,p'),(d,d'),(pol d,d') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=(2); 267.4|g to 0+, 840.9|g to 2+; band member 
T$From recoil-distance technique in 1989Ko40. Others: 12.1 ps {I+10-17} (1989SvZZ) and <16 ps (1969Ro05), both from Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$477.8|g to 4+, 584.6|g to 2+; band member 
T$From recoil-distance technique in 1989Ko40. Other: 5.4 ps {I+5-4} from Coulomb excitation in 1989SvZZ 
$B(E4)|?0.001 from (e,e') in 1991We15 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$653.1|g to 4+; member of the g.s. band 
T$From 1989Ko40 using the recoil-distance technique. Other: 1.46 ps {I+14-7} in Coulomb excitation (1989SvZZ) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$905.2|g to 2+; 144|g to 6+; band member; assignment in {+110}Pd(p,p'),(d,d'),(pol d,d'); 
T$From 1989Ko40 using recoil-distance technique. Other: 1.9 ps {I4} in Coulomb excitation (1989SvZZ) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$L(t,p)=(4); 463.9|g to 2+, 1014|g to 4+; band member 
$B(E4)=56|*10{+-4} {I13} from {+110}Pd(e,e') (1991We15) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$L(t,p), L(|a,|a')=3; assignment in {+110}Pd(p,p'),(d,d'),(pol d,d') 
$|e B(E3)|^=0.086 {I12} in 1969Ro05, weighted average of 0.083 {I15} and 0.093 {I21}. |b{-3}=0.140 {I11}, deduced from B(E3), assuming |e=1 (3- state decays entirely to first 2+ state) 


level_energy_unit: KEV
level_spin_parity: (5,6+)
level_comment:
J$487|g to 6+, 1140|g to 4+. Note, that this level was assigned as the 6+ member of the g.s. band in Coulomb excitation, but this was contradicted in {+176}Yb({+31}P,X|g) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$1048.3|g to 4+, 2094|g to 2+ and 2452|g to 0+. Note, that assignment in {+110}Pd(p,p'),(d,d'),(pol d,d') favors 4+ 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$2474.4|g to 0+, 1076.7|g to 4+. Note that J|p=1- in {+110}Pd(p,p'),(d,d') (1990Pi14 and 1992Pi08), but J|p=(3-,4+) in {+110}Pd(pol d,d') (1993He13) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$1216.5|g to 6+, 1392.1|g to 4+; 890.5|g to (2+). Note, that significant feeding in {+110}Rh |b{+-} decay (28.0 s) (J|p=(6+)) would suggest J|p=5+ 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$817.6|g to 6+, 1593.6|g to (3+); 904.5|g to (2+). Note, that significant feeding in {+110}Rh |b{+-} decay (28.0 s) (J|p=(6+)) would suggest J|p=5+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$B(E2)|^=0.87 {I3} in 1991We15 and 0.80 {I7} in 1976Li19 
MOME2$-0.47 {i3} (1976Li19). Other:-0.28 {i3} (1973PeYX) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Others: 46 ps {i6} from recoil distance Doppler shift technique in 2008De30 
BE2$0.85 {I+2-7} from E2 matrix element of 0.919 {I+12-35} in 1989SvZZ, 0.88 {i6} in 1971Bo08, 0.82 {i8} in 1971Ha08, 0.91 {i6} in 1969Ro05, 0.91 {i3} in 1962Ec01 (the weighted average of 0.92 {i6}, 0.90 {i6}, 0.91 {i6} and 0.91 {i6}), 0.78 in 1962Er05, 0.94 {I8} in 1962Ga10, 0.91 in 1962Ri09 and 0.86 {i6} in 1958St32 
MOMM1$+0.62 {I6} (using dynamic field technique in 1980Br01). Others: +0.62 {I6} (1974Hu01), +0.70 {I6} (1985ThZX), 0.74 {I6} (1979LaZL), 1980Ka34, and 1969He11 
MOME2$-0.72 {I14} or -0.60 {I14} (using reorientation precession technique in 1976Ha21). Others: -0.55 {I7} (1972Lu08), -0.72 {I12} or -0.45 {I12} (1971Ha08) and -0.48 {I5} or -0.27 {I5} (1970Be45) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Others: 18.6 ps {I+5-9} from 1989SvZZ and 14.0 ps {I18} in 1969Ro05 
$B(E2)|^=0.0128 {I11} in 1969Ro05, 0.094 {I4} in 1961St02. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
E$From 1969Ro05 
$|e B(E3)|^=0.086 {i12}, from weighted average of 0.083 {i15} and 0.093 {i21} in 1969Ro05. |b{-3}=0.140 {i11}, deduced from |eBE3 by assuming that the 3- state decays 100% to the first 2+ state (|e=1) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$from 2016Le16 for the 2|b{+-} decay of {+110}Pd to the first 2+ state of {+110}Cd at 657.76 keV with 90% confidence level. Limits of T{-1/2} for decays to excited states are (at 90% confidence level): >4.0|*10{+20} y for decay to 1473.1,0+ level; >3.0|*10{+20} y for decay to 1475.8,2+. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+108,110}=0.2052 fm{+2} {I3} (stat) {I21} (syst volt) {I22} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
T$23.4 min {I2} (1977Kr14) |g-decay curves. Others: 1952Mc34, 1957Dz14 
J$allowed |b transition (log| {Ift}=5.85) to 7/2+, 59.8 level of {+111}Ag. |g from 1/2+,7/2+ level 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
J$L(d,p)=0+2 for the 191.3+195.1 levels, 1984KaZW suggest J|p=(7/2-) not adopted by evaluators 
E$multiplet (|DE|<3 keV); L(n)=0+2 fits angular distribution 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
T$from 5.5 h {I1} (1952Mc34). Other: 5.5 h {I2} (1957Dz14) 
E$Branching: I|g(172|g,{+111}Pd)/I|g(391|g,{+111}Ag)=6.3 {I6} unweighted av of 6.5 {I8} (1977Kr14), 6.1 {I2} (1969Be11). Other: 8.7 {I6} (1969Sc12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$doublet deduced from DWBA fits to angular distribution. No broadening was observed, so the energies of the individual components are the same to |<3 keV 
J$3/2+ assigned to L=2 component in analogy with levels in {+109}Pd (at 291) and {+107}Pd (at 380) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$7/2+,9/2+ from L(d,p)=4 in Adopted Levels for {+111}Pd in ENSDF database, rotational like structure favors 7/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
T$from 547|g(t) and 580|g(t) (2019Kr05). 
J$from the Adopted Levels of {+111}Pd in the ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
E$from the Adopted Levels of {+111}Pd in the ENSDF database 
T$from 172|g(t) at 95% confidence level (2014Li17) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T$Weighted average of 21.045 h +29-65 (1977Gi11), 21.12 h 8 (1974Ro18), 20.12 h 6 (1971Ba28), 21.0 h 5 (1959Gi66) and 21.02 h 2 (1957Me49) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L=2 in {+110}Pd(t,p) (1972Ca10); 348.7|g to 0+ 
T$from recoil-distance Doppler-shift method in {+252}Cf SF decay (1986Ma22) Other: <1 ns from {+252}Cf SF decay (1970Ch11); Also: T{-1/2} might be overestimated according to B(E2) systematics in 2011Ki17 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$388.0|g E2(+M1) to 2+ and 736.7|g (E2) to 0+; systematics of the second 2+ states; Other: (4+) from L(t,p)=(4) in {+110}Pd(t,p) (1972Ca10) 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_comment:
J$978.2|g to 2+ and 831.9|g to 4+; near-yrast state populated in {+252}Cf SF decay (1999Bu32); not observed in {+112}Rh |b{+-} decay (3.6 s), (1+) (1999Lh01) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J$662.7|g to 3+, 876.0|g to 4+; no observation |g rays to 2+ states; observation in {+112}Rh |b{+-} decay (3.76 s), J|p=(6+); band member 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$464.7|g to 2+, 791.1|g M1+E2 to 3+, a tentative 1004.7|g to 4+; observation in {+112}Rh |b{+-} decay (3.76 s), J|p=(6+); band member 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_comment:
J$1069.2|g to 4+ and 1214.8|g to 2+; not observed in {+112}Rh |b{+-} decay (3.6 s), (1+) (1999Lh01) 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
J$1758.7|g to 2+, a tentative 2106.6|g to 0+; direct feeding in {+112}Rh |b{+-} decay (3.6 s), J|p=(1+) 


level_energy_unit: KEV
level_spin_parity: (4,5+)
level_comment:
J$159.9|g to (4)-, 1471.5|g to 4+, 1258.2|g to 3+. No transitions to 2+; observation in {+112}Rh |b{+-} decay (3.76 s), J|p=(6+) 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J$1204.3|g M1+E2 to 6+,1658.5|g to 3+; direct feeding in {+112}Rh |b{+-} decay (3.76 s), J|p=(6+); Others: J=4 in {+252}Cf SF decay (1999Bu32) and {+208}Pb({+18}O,X|g) (2001Kr08) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$2+ in the adopted levels 
L$20|' data contains impurities, which leads to an ambiguous L-value; d|s/d|W analysis in 1972Ca10 favors rather L=4 than L=0 or 2 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+108,112}=0.361 fm{+2} {I4} (stat) {I4} (syst volt) {I3} (syst wave meter) {I11} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
E$tentative g.s. assignment based on T{-1/2} syst. 
T$weighted av of 84 s {i6} (1958Al90), 91 s {i12} (1970Ar19), { 100 s {i5}} (1975BrYM), 90 s (1981Me17), 90 s {i3} (1974Gr29) 
J$from syst and log| {Ift}=5.5 to 7/2+ 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$M2 |g to (5/2+). Syst gives 11/2- The evaluator has accepted the arguments of 2005Fo09: The isomeric transition to the ground state has a half-life of 0.3 s. The previous assignment of 11/2 would make the transition an E3. The Weisskopf estimate of the half-life for such a transition is greater than 1 s. Assigning a J of 9/2. allows this transition to be an M2/E3, with a corresponding half-life estimate of less than 1 s. The structure of 113Pd now appears consistent with the discovery of the new 81.0-keV transition. 
T$from 1993Pe11 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
T$35.1|g depopulating the level observed in singles |g spectrum, but was absent in |b gated |g spectrum, which supports the proposed half-life of this level >1|ms in 1993Pe11 (Nucl. Phys. A561, 416). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
E$ 2014Ku28 confirmed 11/2- yrast excitation position at 98.9 keV as originally proposed in 1999Ho25: Eur. Phy. J. A{-6}, 43; thereby refuting its location at 166 keV proposed in 2005Fo09: Phys. Rev. C 72, 014315. In the Adopted Levels of {+113}Pd in ENSDF database, location of the 11/2- level was adopted at 166 keV following 2005Fo09. This should be reconsidered and re-evaluated. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 2.4 min {i1} (1958Al90), 2.45 min {i10} (1975BrYN), 2.42 min {i15} (1988Ay02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to g.s. 
T$from RDDS method (2008De30). The older value 0.20 ns {I6}(1974JaYY) from |g|g(t) in {+252}Cf SF decay seems too high 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$ from RDDS method (2008De30). Note that this value is a factor of |?2 smaller than the adopted value in ENSDF database. 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
$This level may also be a bandhead of band #7 in Fig. 4 of 2013Lu18 
E$2013Lu18 show two separate levels in Fig. 4 at 2520.9 keV both with J|p=(6-) belonging to two different bands; one decaying by 336.4 and 1019.8 transitions, and the other by 455.1 and 889.6 transitions, but in authors' Table 2, all four gamma rays from 2520.9 levels are shown in both places. The compilers assume that there is only one level at this energy, as also in Adopted dataset for {+114}Pd in ENSDF database 


level_energy_unit: KEV
level_spin_parity: (15+)
level_comment:
E$5011.9 in Table 2 and Fig. 4 of 2013Lu18 is incorrect, as stated in the Erratum to 2013Lu18 published in Nucl. Phys. A983, 321 (2019). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=103 ps {I10} (2019Ga29), from HPGe start gates on 644|g (10+|)8+), 715|g (8+|)6+), 648|g (6+|)4+) and 1332|g (5-|)4+); and LaBr{-3}(Ce) stop gates on 520|g (4+|)2+) and 333|g (2+|)0+). Authors compared their result with |t=118 ps {I20} from 2008De30 (Phys. Rev. C 78, 051302(R)); and 116 ps {I6} (H. Mach et al., JYFL annual report (University of Jyvaskyla, 2003). 2019Ga29 recommend mean lifetime |t=113 ps {I5}, from weighted average of the three independent measurements. Compiler notes that in Table II, 2019Ga29 list 115 ps {I5}, which is a misprint. 
$Transition quadrupole moment Q{-0}=2.96 eb {I6}; deformation parameter |b{-2}=0.231 {I5} (2019Ga29); both are magnitudes 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=22 ps {I13} (2019Ga29), from HPGe start gates on 644|g (10+|)8+), 715|g (8+|)6+), and 333|g (2+|)0+); and LaBr{-3}(Ce) stop gates on 648|g (6+|)4+) and 520|g (4+|)2+). An indirect measurement gave |t=20 ps {I22}, from summed lifetime |t=123 ps {I19} for the first 2+ and 4+ states from HPGe start gates on 644|g (10+|)8+) and 715|g (8+|)6+); and LaBr{-3}(Ce) stop gates on 648|g (6+|)4+) and 333|g (2+|)0+), and subtracting measured lifetime |t=103 ps {I10} for the first 2+ state. Weighted averaged lifetime |t=21 ps {I11}, recommended value as confirmed by the corresponding author of 2019Ga29 in e-mail reply of March 19, 2020 
$Transition quadrupole moment Q{-0}=2.22 eb {I58}; deformation parameter |b{-2}=0.177 {I44} (2019Ga29); both are magnitudes 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
T$measured mean lifetime |t=2 ps {I8} or |<10 ps (2019Ga29) from HPGe gates on 520|g (4+|)2+) and 333|g (2+|)0+). 
$Transition quadrupole moment Q{-0}|>1.51 eb; deformation parameter |b{-2}|>0.123 (2019Ga29); both are magnitudes 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+108,114}=0.487 fm{+2} {I5} (stat) {I4} (syst volt) {I3} (syst wave meter) {I24} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_lifetime_unit: S
level_comment:
J$see 2005Fo09 for the discussion about the new assignment of 1/2+ to the g.s. and all positive parity 
T$from 1987FoZY, 1990Fo07. Previous T{-1/2} measurements report mixture of the two isomers: 45 s {I3} (1958Al90), 41 s {I4} (1966We07) 36 s {I3} (1968Kj01), 37.4 s {I4} (1968RoZZ), 30 s {I2} (1970Ar19), 41 s {I2} (1973BrXC), 47 s {I2} (1981Me17) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$weighted average of 13.6 s {I12} (1970Ar19), 12.5 s {I6} (1975BrYN), 11.1 s {I8} (1986RoZN), 11.5 s {I4} (1990Fo07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+108,116}=0.574 fm{+2} {I5} (stat) {I4} (syst volt) {I3} (syst wave meter) {I44} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
T$from 1991Pe04. Others: 4.4 s {i2} (1990RoZX), 5.0 s {I+5-7} (1968We11), 4.8 s {i3} (1970WeZX). 
J$log| {Ift}=4.8 from (7/2+) suggests (5/2+,7/2+,9/2+), No |g from 11/2- isomer, hence J|p is unlikely to be 7/2+ or 9/2+ 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: MS
level_comment:
T$from 1991Pe10, other: 18 ms {i2} (1990Pe10), same authors. 
J$analogy to {+119}Ag, {+121}Sn. T{-1/2}. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$by comparing fission yields, authors suggest |?70% |b feeding to the g.s. which gives: log| {Ift}|?4.8. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
J$(5/2+) in {+117}Pd Adopted Levels in the ENSDF database (March 2009 update); (3/2+) in 2013Lu18 (Nucl. Phys. A919, 67) 
T$from {+117}Pd Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$(7/2+) in {+117}Pd Adopted Levels in the ENSDF database; (5/2+) in 2013Lu18 (Nucl. Phys. A919, 67) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
$T{-1/2} and decay mode from {+117}Pd Adopted Levels in the ENSDF database 
J$(11/2-) in {+117}Pd Adopted Levels in the ENSDF database; (9/2-) in 2013Lu18 (Nucl. Phys. A919, 67) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 1989Ko22 (|g-multiscaling; also 1988Pe13 from the same group who reported measured T{-1/2}=2.24 s {I17}). Other: 3.1 s {I3} (1969We11, from fission studies). 


level_energy_unit: KEV
level_comment:
E$ordering of the 539.3|g-411.2|g cascade is not uniquely determined in 2007St19, but it is established in 2013Lu18 from observed higher (by 18%) intensity of the 539.3|g as compared to that of the 411.2|g, which is given here. Ordering was shown as reversed in 2007St19 


level_energy_unit: KEV
level_comment:
E$corresponds to 3775.3, level in the Adopted dataset, with the ordering of the |g cascade from {+252}Cf SF decay (2013Lu18) 


level_energy_unit: KEV
level_spin_parity: 10+
level_comment:
E$corresponds to 4143.1, (12+) level in the Adopted dataset, with the ordering of the |g cascade from {+252}Cf SF decay (2013Lu18) 


level_energy_unit: KEV
level_spin_parity: 12+
level_comment:
E$corresponds to 3286.7, (10+) level in the Adopted dataset, with the ordering of the |g cascade from {+252}Cf SF decay (2013Lu18) 


level_energy_unit: KEV
level_comment:
J$2006Wa10 suggest this level as possible 5+ member of |g band, but according to 2006StZW and 2003WuZZ, the 5+ member is most likely the 1856 level decaying by a 672.9|g. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+108,118}=0.648 fm{+2} {I5} (stat) {I6} (syst volt) {I3} (syst wave meter) {I65} (syst atomic factors) (2022Ge04). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=2.26 s, %|b{+-}n=0.0 (2003Mo09) 
$Theoretical T{-1/2}=584 ms, %|b{+-}n=0.3 (2016Ma12) 
T$from |b decay curve (2006Mo07). Other: 0.5 s {I1} (from multiscaling of |b-gated K|a| x ray, 1993Ja03) is in agreement but less precise than in 2006Mo07 
$Theoretical half-life calculation: 2012Ch48, 1997Bo24 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$The evidence of the isomer is reported by 2007To23, however no information is given on the half-life. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_lifetime_unit: US
level_comment:
$ Number of implanted fragments=2.8|*10{+4} 
T$ deduced by assuming two cascading-decay components and constant background for time spectrum of 135.5-keV |g ray (2012Ka36) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from Adopted Levels of {+121}Pd in ENSDF database 
$Theoretical T{-1/2}{-1/2}=1.27 s, %|b{+-}n=0.0 (2003Mo09) 
E$the measured half-life is assumed to correspond to the ground state of {+121}Pd 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 285 ms {I24} (Adopted Levels of {+121}Pd in ENSDF database; value taken from 2006Mo07: Phys. Rev. C 73, 035801) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Earlier measurement: <0.8 (2006Mo07: Phys. Rev. C 73, 035801) 
E$it is assumed that the observed activity corresponds to the g.s. of {+121}Pd 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 291 ms {I1} (2015Lo04: Phys. Rev. Lett. 114, 192501); 285 ms {I24} (2006Mo07) Weighted average of the three values is 291 ms {I1}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n from |bn coincidence (2006Mo07). Theoretical %|b{+-}n=0.03 (1997Mo25) 
T$from |b decay curve (2006Mo07) 
$ Theoetical half-life calculations: 2012Ch48, 1997Bo24 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Earlier measurement: |<2.5 (2006Mo07: Phys. Rev. C 73, 035801) 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 195 ms {I5} (2015Lo04: Phys. Rev. Lett. 114, 192501); 175 ms {I16} (2006Mo07) Weighted average of the three values is 195 ms {I5}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-N$from Adopted Levels of {+122}Pd in ENSDF database 
$Theoretical T{-1/2}{-1/2}=951 ms, %|b{+-}n=0.06 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 175 ms {I16} (Adopted Levels of {+122}Pd in ENSDF database; value taken from 2006Mo07: Phys. Rev. C 73, 035801) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n: from |b-delayed neutron counting (2021Ha19). Other: 10 {I6} measured by 2014SmZZ 
E$measured half-life is assumed to correspond to the ground state of {+123}Pd 
J$3/2+ from systematics (2021Ko07: NUBASE2020), 3/2- from theoretical considerations (2019Mo01) 
T$weighted average of 114 ms {I2} (2021Ha19, |b-delayed neutron counting), 108 ms {I1} (2015Lo04, implanted ion-|b correlation), 174 ms {I+38-34} (2006Mo07, ion-|b correlation), and 170 ms {I+45-38}(stat){I18}(syst) (2014SmZZ, implant ion-|b correlation). 
$Measured mass-excess: -60430 {I316}, with systematic uncertainty=315, statistical uncertainty=29 from 10 counts events (2016Kn03) 
$Theoretical T{-1/2}=392.8 ms, %|b{+-}n=1 (2019Mo01); T{-1/2}=172 ms, %|b{+-}n=0.5 (2016Ma12) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_uncertain: ?
level_comment:
E,J$a level with J|p=(11/2-) is shown in the decay scheme in Fig.4 of 2019Ch24, with no further explanation and discussion. This level is proposed by 2019Ch24 probably as the parent level to feed the high-spin levels in {+123}Ag from {+123}Pd |b{+-} decay. No observation of this level has been made in any studies. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT;ISO=M
level_comment:
$%IT decay mode assumed to be 100% in view of only |g-decay observation 
E$energy of 62.2 keV for the isomer stated in 2012Au07 seems too low in view of first 2+ state in {+124}Pd at 590 keV. Absolute energy of this isomer was not measured in 2012Ka36 
T$from |g(t) method; estimated because |g-ray events were equally distributed in the 20-|ms range of the time spectrum (2012Ka36) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT
level_comment:
$Number of implanted fragments=3.8|*10{+4} 
E$energy of 62.2 keV for the isomer stated in 2012Au07 seems too low in view of first 2+ state in {+124}Pd at 590 keV. Absolute energy of this isomer was not measured in 2012Ka36 
T$from |g(t) method; estimated because |g-ray events were equally distributed in the 20-|ms range of the time spectrum (2012Ka36) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Other measurement: 17 {I5} (2014SmZZ: thesis, Univ. of Notre Dame, work at GSI); P{-n} values measured for {+123},{+124},{+125},{+126}Pd and {+125},{+126},{+127},{+128}Ag in this work are systematically much larger as compared to corresponding values in 2021Ha19 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 88 ms {I15} (2015Lo04: Phys. Rev. Lett. 114, 192501). Others: 38 ms {I+38-19} (2006Mo07); 144 ms {I+25-24} (2014SmZZ). Weighted average of the values from 2021Ha19 and 2015Lo04 is 94 ms {I3}, heavily weighted by the value in 2021Ha19 (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}{-1/2}=288.7 ms, %|b{+-}n=0.77 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 38 ms {I+38-19} (Adopted Levels of {+124}Pd in ENSDF database; value taken from 2006Mo07: Phys. Rev. C 73, 035801) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=265 ms, %|b{+-}n=2.9 (2003Mo09) 
$Measured |s=7 nb (2008Oh06), 94 pb {I27} (2008Be33) 
E$the reported half-life is assumed to correspond to the g.s. of {+125}Pd 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 
J$3/2+ from systematic trend (2012Au07), 9/2- in theoretical calculations (1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Other measurement: 12 {I4} (2014SmZZ: thesis, Univ. of Notre Dame, work at GSI); P{-n} values measured for {+123},{+124},{+125},{+126}Pd and {+125},{+126},{+127},{+128}Ag in this work are systematically much larger as compared to corresponding values in 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+125}Pd 
J$(11/2-) proposed for the g.s. in 2019Wa14: Phys. Lett. B792, 263 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 57 ms {I10} (2015Lo04: Phys. Rev. Lett. 114, 192501); 61 ms {I+8-7} (2014SmZZ). Weighted average of the three values is 64.1 ms {I17}; weighted heavily by the value in 2021Ha19 (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}-n: other measurement: 22 {I9} (2014SmZZ) 
$Measured |s=0.7 nb (2008Oh06) 
T$weighted average of 51 ms {I3} (2021Ha19), 48.6 ms {I8} (2015Lo04) and the values obtained by 2014Wa26 from decay curves of several |g rays in {+126}Ag: 54 ms {I3} for 254.3|g, 56 ms {I4} for 263.2|g, 48 ms {I2} for 287.0|g, 48 ms {I3} for 365.0|g, 46 ms {I5} for 583.5|g, 46 ms {I3} for 661.9|g, 48 ms {I2} for 842.6|g, 46 ms {I4} for 914.7|g, 52 ms {I4} for 1133.2|g, and 41 ms {I3} for 1502.0|g. Other: 56 ms {I+11-9} (2014SmZZ). 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M3
level_comment:
T$weighted average of the values obtained by 2014Wa26 from decay curves of |g rays in {+126}Pd (20 ms {I3} for 296.7|g, 20 ms {I3} for 542.4|g, 21 ms {I2} for 693.3|g, 18 ms {I4} for 787.7|g, 23 ms {I5} for 1330.2|g) and |g rays in {+126}Ag (25 ms {I2} for 193.7|g, 27 ms {I2} for 203.7|g, 27 ms {I10} for 227.9|g, 17 ms {I4} for 359.5|g, 26 ms {I3} for 598.1|g, and 23 ms {I2} for 741.8|g). 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
T$from time difference between the 86-keV transition and the |g rays below the 2023 keV level (2013Wa24) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=210 ms, %|b{+-}n=8.2, %|b{+-}2n=0.0 (2003Mo09) 
$Measured |s=80 pb (2010Oh02), systematic uncertainty |?40%. Probability of misidentification of {+127}Pd isotope<0.001% 
E$measured half-life is assumed to correspond to g.s. of {+127}Pd 
J$3/2+ from systematic trend (2012Au07), 11/2- in theoretical predictions of 1997Mo25 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Other measurement: <19 (2014SmZZ: thesis, Univ. of Notre Dame, work at GSI). No events for |b{+-}2n decay mode were detected by 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+127}Pd 
J$(11/2-) proposed for the g.s. in 2019Wa14: Phys. Lett. B792, 263 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier value: 38 ms {I2} (2015Lo04: Phys. Rev. Lett. 114, 192501). Other: 73 ms {I+24-23} (2014SmZZ). Weighted average of the two values is 38 ms {I2}; weighted heavily by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=74.2 ms, %|b{+-}n=6.7 (2003Mo09) 
$Measured |s=12 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+128}Pd isotope<0.001% (2010Oh02) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Other measurement: 20 {I5} (2014SmZZ: thesis, Univ. of Notre Dame, work at GSI); P{-n} values measured for {+123},{+124},{+125},{+126}Pd and {+125},{+126},{+127},{+128}Ag in this work are systematically much larger as compared to corresponding values in 2021Ha19. No events for |b{+-}2n decay mode were detected by 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+128}Ag 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier value: 59 ms {I5} (2015Lo04: Phys. Rev. Lett. 114, 192501). Others: 73 ms {I+10-9} (2014SmZZ); 58 ms {I5} (1996WoZZ: Conf. Proc. NWE'96, Amsterdam, p107). Weighted average of values from 2021Ha19 and 2015Lo04 is 66.6 ms {I24} (compiler's note). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. No events for |b{+-}2n decay mode were detected by 2021Ha19 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier value: 35 ms {I3} (2015Lo04: Phys. Rev. Lett. 114, 192501). Other: <26.2 ms (2014SmZZ, thesis, Univ. of Notre Dame, GSI work). Weighted average of the two values is 36 ms {I5} (compiler's note). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=97.19, %|b{+-}2n=2.29 (1997Mo25) 
E$measured half-life is assumed to correspond to the ground state of {+129}Pd 
J$7/2- from theoretical considerations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay 
$Theoretical T{-1/2}=60.8 ms, %|b{+-}n=75.8, %|b{+-}2n=2.4 (2003Mo09: Phys. Rev. C67, 055802) 
$Theoretical T{-1/2}=31.1 ms, %|b{+-}n=74.6, %|b{+-}2n=0.9 (2016Ma12: Phys. Rev. C93, 025805) 
$A total of 52 counts were assigned to {+129}Pd, 16 events with the spectrometer setting on Pd, and 36 events for setting on Sn. Probability of misidentification of this isotope is <0.01% (2018Sh11). 
$Production |s=0.21 pb for Pd setting, and 0.39 pb for Sn setting, with 30% systematic uncertainty for all |s. 
E$it is assumed that the observed events correspond to ground-state activity. 
T$measured by 2015Lo04 at RIBF-RIKEN. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay, thus 100% |b{+-} decay is assigned by inference 
$Theoretical T{-1/2}=68.5 ms, %|b{+-}n=84, %|b{+-}2n=3 (2019Mo01) 
$Theoretical T{-1/2}=25.2 ms, %|b{+-}n=72.9, %|b{+-}2n=1.2 (2016Ma12) 
$A total of five events were assigned by 2018Sh11 to {+130}Pd. As no events were observed for neighboring hydrogen-like peaks, misidentification of {+130}Pd nuclide is unlikely. 
$Production |s=0.040 pb for Sn setting, with 30% systematic uncertainty for |s 
T$experimental half-life is not known. From time-of-flight of about 550 ns for the fragments through the transport system, as given in a companion paper 2018Fu08, half-life is expected to be >550 ns. From a general decreasing trend of |b-decay half-lives with increasing neutron number, half-life is expected to be <40 ms, based on known half-lives of 31 ms {I7} for {+129}Pd, 35 ms {I3} for {+128}Pd, 38 ms {I2} for {+127}Pd, and 48.6 ms {I12} for {+126}Pd, as available in literature 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay, thus 100% |b{+-} decay is assigned by inference 
$Theoretical T{-1/2}=54.7 ms, %|b{+-}n=23, %|b{+-}2n=66, %|b{+-}3n=0 (2019Mo01) 
$Theoretical T{-1/2}=20.1 ms, %|b{+-}n=21.6, %|b{+-}2n=61.9, %|b{+-}3n=0.8 (2016Ma12) 
$Only one count was assigned to {+131}Pd with the spectrometer setting on Sn. Misidentification of this isotope is unlikely since no events were observed for neighboring hydrogen-like peaks (2018Sh11) 
$Production |s=0.007 pb, with 30% systematic uncertainty for |s 
E$it is assumed that the observed event corresponds to ground-state activity. 
J$3/2- from |W{-|n}=3/2- orbital proposed in 2019Mo01 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 57.0 ms (2019Mo01) and 20.1 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+131}Pd is expected to be <35 ms, based on measured half-lives of 38 ms for {+127}Pd, 35 ms for {+128}Pd, and 31 ms for {+129}Pd, available in literature. 


level_energy_unit: KEV
level_comment:
$Proton decay mode assigned as {+92}Ag is expected to be proton-unbound nucleus from theoretical S(p)=-0.67 MeV (1997Mo25) 
$Measured production |s=0.03 pb {I+2-1} (2016Ce02) 
$A total of eight events assigned to {+92}Ag in 2016Ce02, which are assumed by the evaluator to correspond to the g.s. activity of {+92}Ag 
$Theoretical |b-decay half-life=20.5 ms (1997Mo25) 
J$1-6 from proton in 7/2 and neutron in 5/2 orbital (1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_comment:
$A total of 31 events were assigned to {+93}Ag by 2016Ce02, which are assumed to correspond to the g.s. activity of {+93}Ag. 
$Dominant proton decay mode of {+93}Ag is expected from S(p)=-1510 keV {I710} (syst, 2012Wa38). Significant drop in number of observed counts for {+93}Ag with respect to neighboring isotopes with the same T{-z} value shows with 10|s confidence level that {+93}Ag is proton emitter with T{-1/2} lower than or comparable to time-of-flight through the separator (2016Ce02). 
$Measured production |s=3.3 pb {I2} (2016Ce02) 
J$9/2+ proposed from systematics (2012Au07), 7/2+ in 1997Mo25 theoretical calculations 
T$from 2016Ce02, based on assignment of 31 events to {+93}Ag and measured time-of-flight, with the assumption that ratio of number of identified events associated with nuclei of the same T{-z} is the same as that for the neighboring T{-z} nuclei. For half-life of {+93}Ag, N({+95}Cd)/N({+93}Ag)=N({+96}Cd)/N({+94}Ag) was used, with T{-z}=-1/2 for {+93}Ag and {+95}Cd and T{-z}=0 for {+94}Ag and {+96}Cd. Other: |?1.5 |ms (1995Ry03) 
T$theoretical |b-decay T{-1/2}=94 ms (1997Mo25). Systematic |b-decay T{-1/2}=5 ms (2012Au07) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 0.61 s 2 (2004Mu30), 0.59 s 2 (2004Pl01), 0.36 s 3 (2002La18), 0.42 s 5 (1994Sc35). Other: 0.45 s +20-13 (2002StZZ) 
J$level feeds (6+) and (8+) levels in {+94}Pd in |e+|b{++} decay. Assignment supported by shell-model calculations (2004Pl01) 
E$x |?700 keV from shell-model calculations (2002La18) 


level_energy_unit: KEV
level_energy_info: ;ERR=SY;ERR=?
level_spin_parity: (21+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
T$weighted average of 0.47 s 8 (2004Pl01), 0.39 s 4 (2004Mu30), 0.3 s 2 (2002La18) 
J$level feeds (20+) level in {+94}Pd in |e+|b{++} decay. Assignment supported by shell-model calculations (2004Pl01) 
E$This level undergoes |b-delayed proton emission as well as direct emission of 1 and 2 protons. In the single proton emission, 2 levels in {+93}Pd are fed, one at 4994 keV with a proton energy of 790 30 keV, and another at 4751 keV with a proton energy of 1010 {I30} keV. Combining these numbers, a Q{-p}=5.78 MeV 30 is quoted by 2005Mu15 for this level. From 2003Au03, one obtains a proton separation energy of 890 keV with a systematic error of 643 keV for {+94}Ag. Therefore, the level energy is 6670 keV with a uncertainty of 709 kev from systematics. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7+)
level_lifetime_unit: S
level_comment:
T$weighted average of 0.48 s {I2} from implant-|b(t) and 0.47 s {I2} from implant-|bp(t); both analyses used multiparameter fit to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 
E,J$from the Adopted Levels of {+95}Pd in the ENSDF database (October 2010 udpate) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T$weighted average of 1.74 s {I13} (from |b|g(t) in 1997Sc30). and 1.85 s 34 (from |g(t) in 2003Do09); Other result: 2.0 s {I1} (1994Sc35) is superseded by 1997Sc30. 
$With a Q(|ep)=5518 keV 401 (2003Au03, Systematic uncertainty), this level is expected to decay by |ep, yet the branching ratio is unknown. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T$ measured by 2012Lo08 from decay curves of time correlations between implantations and decay radiation. Decay curves were fitted with Poisson distribution using log-likelihood function by consideration of decay of parent, daughter and grand-daughter. Note that in text of 2012Lo08 paper T{-1/2}=1.80 s {I8} from |bp-energy spectrum and |bp-decay; and T{-1/2}=1.81 s {I13} from decay curve analysis. 
J$ from {+95}Ag Adopted Levels in ENSDF database 
%B+P$ measured by 2012Lo08 based on observation of 1705 |bp coincidence events. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8)+
level_lifetime_unit: S
level_comment:
E$from calculations (1997Sc30) which predict g.s. is 8+ 
J$log| {Ift}|?5.3 to (8+), no significant I|e to (6+) nor to (10+), |p from coupling a neutron and a proton in g9/2 orbits. 
T$from |g(t) in {+60}Ni({+40}Ca,p3n) (2003Ba39) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (2+)
level_lifetime_unit: S
level_comment:
J$log| {Ift}|?5.9 to 2+, no significant I|e to 0+ nor to 4+ 
T$from |g(t) in {+60}Ni({+40}Ca,p3n) (2003Ba39) 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: (15+,13-)
level_lifetime_unit: US
level_comment:
J$possible values from Shell model calculation (1997Gr02) 
T$from |g(t) in Ni({+112}Sn,X) (1997Gr02) 
E$Z>1138=470+668. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8)+
level_lifetime_unit: S
level_comment:
E$from calculations(1997Sc30) which predict g.s. is 8+ 
J$log| {Ift}|?5.3 to 8+, no significant I|e to 6+ nor to 10+ 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: (15+,13-)
level_lifetime_unit: US
level_comment:
J$possible values from shell model calculation (1997Gr02) 
T$from |g(t) (1997Gr02) 
E$Z>1138=470+668. 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
E$ assumed as the g.s. based on shell-model predictions. However, predicted 2+ is very close in energy, thus absolute energy of the 8+ is not known 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (15+)
level_comment:
E$ y<50 (from 2011Bo23: Phys Rev C 84, 044311 (2011)) 
$ configuration=|p|n(p{-1/2}{+2}|p(g{-9/2}{+7})|n(g{-9/2}{+9}); |p(g{-9/2}{+-3}|n(g{-9/2}{+-1} holes coupled to maximum spin of 15+ 


level_energy_unit: KEV
level_spin_parity: (17+,15+,16+)
level_comment:
E$ group of expected G-T resonance states at 9.5 MeV,17+; 10.2 MeV,15+ and 10.6 MeV, 16+ with a combined |b{++} feeding of 32%. These states are expected to decay 67% by |g decay to 15+ state in {+96}Ag by M1/E2 transitions and 33% by delayed-proton decay to {+95}Pd 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (15+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
$ Isomeric ratio=10.9% {I6} (2011Bo23) 
E$ yrast trap isomer, x<50 from experimental considerations 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (19+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M3
level_comment:
$ Isomeric ratio=2.0% {I12} (2011Bo23) 
T$ from summed time distribution of 4167|g, and 4265|g and maximum likelihood fitting method (2011Bo23). In figure 4b of 2011Bo23, the uncertainty is quoted as 0.04 |ms 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (13-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
T$ from decay curve obtained from gating on 743|g, fitted with a single exponential and a time-dependent background. The low intensity of the 743|g and short (12 |ms) collection time gives an imprecise half-life. 2011Be34 state that the 743|g corresponds to the decay of an additional longer-lived isomer. Note that in 2011Bo23 (Phys Rev C 84, 044311 (2011)), the half-life of this isomer is measured as 100 |ms. 
$ Isomeric ratio=0.59% {I9} (2011Be34) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (15+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$ from decay curve obtained from gating on 257|g, 630|g, 667|g and 1506|g, fitted with a single exponential and constant background. 
$ Isomeric ratio=10.8% {I12} (2011Be34) 
E$ y-x estimated as 77 keV from theoretical B(E2) and measured isomer half-life 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: S
level_comment:
%B+P$ Measured by 2012Lo08 based on observation of 43540 |bp coincidence events. 
$ (8+) state populated 22% {I10} of the time 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (2+)
level_lifetime_unit: S
level_comment:
%B+P$ Measured by 2012Lo08 based on observation of 46858 |bp coincidence events. 
$ (2+) state populated 78% {I10} of the time 


level_energy_unit: KEV
level_spin_parity: (15+)
level_lifetime_unit: US
level_comment:
E$Isomeric ratio R=18.7 % {I4} (2017Pa35) 
T$From |g(t) in 2017Pa35 (Table I), but the gating |g-ray transitions were not given by the authors. Also, 1.66 |ms {I31} from 43.7|g(t) in Fig. 6, but 1.48 |ms {I27} from 43.7|g(t) in the text (2017Pa35); 1.55 |ms {I3} was also reported in 2017Pa35 using 630|g(t) and 667|g(t) 


level_energy_unit: KEV
level_spin_parity: (19+)
level_lifetime_unit: US
level_comment:
E$Isomeric ratio R=1.4 % {I8} (2017Pa35) 
T$From |g(t) in 2017Pa35, but the gating |g-ray transitions were not given by the authors 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (2+)
level_comment:
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 
E,J$From the Adopted Levels of {+96}Ag in the ENSDF database (October 2008 update) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
E$given by 2019Pa16 as the g.s. based on shell-model calcualtions. However, the predicted 2+ is close in energy. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
J$J|p based on shell model calculations (2005Li58,1990Al07) and analogy with odd-A N=50 isotopes ({+91}Nb to {+95}Rh) 
T$weighted average (external unc.) of 25.9 s {I4} (1999Hu10) and 25.3 s {I3} (1997Sc30) 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: NS
level_comment:
T$ centroid-shift method from the time differences of any combination of 1290 and 763 transitions with 2572 and 1306 transitions (2005Li58) 


level_energy_unit: KEV
level_spin_parity: (9/2)
level_comment:
$RMS charge radius: |d<r{+2}>({+97}Ag,{+109}Ag)= 1.29 fm{+2} {I20}(stat) {I9}(syst) (2014Fe01) 
$Isotope shift: |d|n({+97}Ag,{+109}Ag)= -4.67 GHz {I66}(stat) {I8}(syst) (2014Fe01) 
J$(9/2+) in Adopted Levels of {+97}Ag in ENSDF database. J=9/2 tentatively assigned from present experiment and comparison with theoretical predictions 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: S
level_comment:
$%|ep=0.0011 {I+5-4} (1996He25,1997Ra22) 
J$hyperfine structure measurements (2014Fe01) permit J=6 and 5; shell-model predictions with possible configuration=|pg{-9/2}{+-1}~#|nd{-5/2} favor 6+ (1995Sc50, 1998Ce03, 2004Co15, J=J{-max}-1 favored); possible |e feeding to (8+) at E=2773 in {+98}Pd also favors 6+. But J|p=5+ from systematics of neighboring Ag isotopes is not completely ruled out. 
T$weighted average of 47.7 s {I3} (2000Hu17) and 47.1 s {I5} (1982Ku15). Other: 44.5 s {I12} (1978Hu11), this value seems discrepant. Weighted average of all the three values is 47.4 s {I5} with a reduced |h{+2}=3.6 
MOMM1$value for J=6; for J=5, |m=4.57 {I7}, hyperfine structure using in-gas-cell laser ionization spectroscopy (2014Fe01) 
$RMS charge radius: |d<r{+2}>({+98}Ag,{+109}Ag)=1.01 fm{+2} {I16}(stat){I7}(syst) for J=6, 0.95 fm{+2} {I16}(stat), {I7}(syst) for J=5 (2014Fe01) 
$Isotope shift: |d|n({+98}Ag,{+109}Ag)=-3.58 GHz {I47}(stat){I8}(syst) for J=6, -3.34 GHz {I47}(stat){I8}(syst) for J=5 (2014Fe01) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
E$ordering of the 107- and 61-keV |g rays in a cascade is from 2017Pa35 in {+9}Be({+124}Xe,X|g) on the premise that no delayed component of 61-keV |g ray was seen. 2017Pa35 also point out that their ordering of this cascade is consistent with that proposed in previous studies by M. Vencelj et al. (2000) and N. Braun (2012); see citations below in comment for half-life. 1992Pl01, in their study of the |e decay had proposed a reversed ordering based on decay pattern and |g intensities from |g|g-coin spectra accumulated for 26 hours. 
J$107|g E2 to (6+). Possible member of the |pg{-9/2}{+-1}~#|nd{-5/2} multiplet (2004Co15, shell model calculations) 
T$from 107|g(t) (2017Pa35) in {+9}Be({+124}Xe,X|g). Other measurements: 0.14 |ms {I4} (2019Ha26, |g(t) at RIBF-RIKEN); 2017Pa35 quote 160 ns {I10} from M. Vencelj et al., Balk. Phys. Lett. Special issue, p298 (2000); 142 ns {I13} and 158 ns {I26} from N. Braun, Ph.D. thesis, Cologne (2012). 2017Au03 quote 220 ns {I20} from R. Grzywacz, ENAM conference Proc. p430 (1998, Bellaire, Michigan). Note that previous values were all for 168 level because of the earlier placement of 107|g from 168 level. Weighted average of all the measurements also gives 161 ns {I7} with reduced |h{+2}=2.2 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$61|g M1 to (4+), 1997|g and 2376|g from 1+. Possible member of |pg{-9/2}{+-1}~#|nd{-5/2} multiplet (2004Co15, shell model calculations) 


level_energy_unit: KEV
level_spin_parity: (2+,3+)
level_comment:
J$1176|g, 1346|g, 1650|g, 2030|g from 1+, 347|g to (3+), no |e feeding from 0+. J{+|p}=2+ predicted by shell model calculations (2004Co15) for member of |pg{-9/2}{+-1}~#|nd{-5/2} multiplet 


level_energy_unit: KEV
level_spin_parity: (2,3+)
level_comment:
J$625|g, 795|g and 1098|g from 1+, 899|g to (3+), no |e feeding from 0+. J{+|p}=2+ predicted by shell model calculations (2004Co15) for member of |pg{-9/2}{+-1}~#|ng{-7/2} multiplet 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
J$assignment by 2017Pa35, based on E2 transition to (6+) 
T$from 107|g(t) in 2017Pa35, as listed in authors' Table I and Fig. 2. Value of 160 ns {I7} also quoted in authors' text and Fig. 7. 2019Ha26 measured T{-1/2}=0.14 |ms {I4} from 107|g(t) 
$Measured isomeric ratio R=18% {I4} (2019Ha26), 4.2% {I10} (2017Pa35) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: S
level_comment:
J log| {Ift}=5.6 to (7/2)+. Systematics of light Ag nuclei. 
T from 1981Hu03. Other: 1.8 min {I2} (1967Do06); 3.0 min {I5} (1967Ba26) 
$RMS charge radius: |d<r{+2}>({+99}Ag,{+109}Ag)= 0.91 fm{+2} {I12}(stat) {I7}(syst) (2014Fe01) 
$Isotope shift: |d|n({+99}Ag,{+109}Ag)= -3.21 GHz {I25}(stat) {I11}(syst) (2014Fe01) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$RMS charge radius: |d<r{+2}>({+99m}Ag,{+109}Ag)= 1.10 fm{+2} {I25}(stat) {I8}(syst) (2014Fe01) 
$Isotope shift: |d|n({+99m}Ag,{+109}Ag)= -4.00 GHz {I94}(stat) {I11}(syst) (2014Fe01) 
J from systematics of light Ag nuclei. 
T from IT decay (1982Ku15). Other: 15 s {I2} (1978Hu11). 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
$RMS charge radius: |d<r{+2}>({+99}Ag,{+109}Ag)= 0.91 fm{+2} {I12}(stat) {I7}(syst) (2014Fe01) 
$Isotope shift: |d|n({+99}Ag,{+109}Ag)= -3.21 GHz {I25}(stat) {I11}(syst) (2014Fe01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$RMS charge radius: |d<r{+2}>({+99m}Ag,{+109}Ag)= 1.10 fm{+2} {I25}(stat) {I8}(syst) (2014Fe01) 
$Isotope shift: |d|n({+99m}Ag,{+109}Ag)= -4.00 GHz {I94}(stat) {I11}(syst) (2014Fe01) 


level_energy_unit: KEV
level_spin_parity: (5)+
level_lifetime_unit: MIN
level_comment:
J$log| {Ift}=6.1 to 6+, log| {Ift}=6.5 to levels that deexcite to 2+ and systematics (J|p({+102}Ag g.s.,{+104}Ag g.s.)=5+) give J=(5). Parity from M1(+E2)-M1(+E2) cascade from (3)+. See also J|p comments for 236.1 or 303.6 level 
$Proposed configuration=|p(g{-9/2}{+-3}){-9/2+}~#|nd{-5/2}, consistent with measured magnetic moment (2014Fe01) 
T$weighted average of 2.00 min {I10} (1980Ha20) and 2.06 min {I25} (1983Ra10). 1983Ra10 cannot distinguish the g.s. and the isomer on the basis of half-life. Others: 2.00 min {I3} (total |g absorption, 1995Ba25). 2.3 min {I1} (|g(t), 1970Hn03), 1.9 min {I3} (|g(t), 1971In03). 7.5 min {I1} from 1967Do06, 8 min {I1} from 1967Ba26 and 9 min from 1966Bu05 can not be confirmed in later studies. 
$rms charge radius: |d<r{+2}>({+100}Ag,{+109}Ag)=0.83 fm{+2} {I10}(stat) {I6}(syst) (2014Fe01) 
$Isotope shift: |d|n({+100}Ag,{+109}Ag)=-2.95 GHz {I22}(stat) {I11}(syst) (2014Fe01) 
$|m, rms charge radius and isotope shifts: measured by hyperfine structure study (2014Fe01) using in-gas-cell laser ionization spectroscopy at LISOL facility of cyclotron center in Leuven. 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$936.6|g from 1+; M1,E2(368.7|g)-M1,E2(567.9|g) cascade from 1+; and systematics (J|p=2+ for 9-keV isomer in {+102}Ag and 6-keV isomer in {+104}Ag) 
$Configuration=|p(g{-9/2}{+-3}){-9/2+}~#|n(d{-5/2},g{-7/2}){-5/2+} and/or |p(g{-9/2}{+-3}){-7/2+}~#|n(d{-5/2},g{-7/2}){-5/2+}, as proposed for {+102}Ag by 2010Go08. 
T$weighted average of 2.30 min {I15} (1980Ha20) and 2.06 min {I25} (1983Ra10). 1983Ra10 cannot distinguish the g.s. and the isomer on the basis of half-life 
$RUL=10 for B(M3)(W.u.) gives %IT=100, however from a maximum of B(M3)(W.u.) value of 2.9 in A=80-100 mass range (data for about ten M3 transitions available in Nudat 2), %IT probably does not exceed |?30% 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J$69.8|g |DJ=1, D to (5)+; parity change would require E2 or E1 for 69.8|g and hence isomeric lifetimes, which is less likely. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
J$M1(+E2) 220.7|g to (2)+ gives (1,2,3)+; M1(+E2)(111.4|g)-M1(+E2)(124.7|g) cascade to g.s. J=(5) gives (3)+ for 236.1 level, (4)+ for 124.7 level and positive parity for g.s. 


level_energy_unit: KEV
level_spin_parity: (7+)
level_comment:
J$195.3|g D, |DJ=1 to (6+); parity change would require E2 or E1 for 195.3|g and hence isomeric lifetimes, which is less likely. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
J$M1(+E2) 288.1|g to (2)+ gives (1,2,3)+; M1(+E2)(179.0|g)-M1(+E2)(124.7|g) cascade to g.s. J=(5) gives (3)+ for 303.6 level, (4)+ for 124.7 level and positive parity for g.s. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_comment:
J$1369.4|g D,|DJ=1 to (7+); negative parity is proposed by 1996Al16 based on the fact that there is no competitive E2 or low-energy M1 connecting |g-ray branches to positive-parity states. 


level_energy_unit: KEV
level_spin_parity: (10-)
level_comment:
J$614.2|g D,|DJ=1 from (11-); Doppler-broadening of 614.2|g indicates M1 transition 
$Intensity imbalance suggests that in addition to the 195.2|g, other low-energy |g rays might deexcite the 2242 level (1996Al16) 


level_energy_unit: KEV
level_spin_parity: (9-)
level_comment:
J$228.9|g (M1),|DJ=1 from (10-) 
$Intensity imbalance suggests that in addition to the 128.9|g, a cascade of at least two low-energy |g rays might deexcite the 2250 level (1996Al16) 


level_energy_unit: KEV
level_spin_parity: (16+)
level_uncertain: ?
level_comment:
J$890.6|g to (15+) 
E$ordering of 961-891 cascade is uncertain. Reverse ordering gives E(level)=4701 


level_energy_unit: KEV
level_spin_parity: (18-)
level_uncertain: ?
level_comment:
J$1152.0|g (Q),|DJ=2 to (16-) 
E$ordering of 1297-1152 cascade is uncertain. Reverse ordering gives E(level)=6471 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
MOMM1$other: 5.74 {i41} (1983Va09,2005St24) 
J$J=9/2 (1970Wa35) atomic beam; mass number inferred from 9 min {i2} decay rate of silver isotope formed by 80 to 100 MeV on palladium target with chem. Measured |m establishes positive parity 
T$unweighted av of 11.4 min {i3} (1978Ha11), 10.8 min {i2} (1967Do05), 11.2 min {i1} (1966Pa14). Others: 1966Bu05, 1967Ba26 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$unweighted av: 3.08 s {i8} (1978Ha11), 3.12 s {i12} (1975Ca01) 
J$1/2- isomerism occurs in {+103}Ag at 134 keV and in {+105}Ag for g.s. 


level_energy_unit: KEV
level_spin_parity: 9/2
level_comment:
$RMS charge radius: |d<r{+2}>({+101}Ag,{+109}Ag)= 0.70 fm{+2} {I10}(stat) {I6}(syst) (2014Fe01) 
$Isotope shift: |d|n({+101}Ag,{+109}Ag)= -2.48 GHz {I26}(stat) {I11}(syst) (2014Fe01) 
J$9/2+ in Adopted Levels of {+101}Ag in ENSDF database. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$RMS charge radius: |d<r{+2}>({+101m}Ag,{+109}Ag)= 0.68 fm{+2} {I9}(stat) {I5}(syst) (2014Fe01) 
$Isotope shift: |d|n({+101m}Ag,{+109}Ag)= -2.40 GHz {I21}(stat) {I11}(syst) (2014Fe01) 
E,T$ from Adopted Levels of {+101}Ag in ENSDF database 
J$(1/2)- in Adopted Levels of {+101}Ag in ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 5(+)
level_lifetime_unit: MIN
level_comment:
J from 1970Wa35, atomic beam, |p suggested from |m and syst 
T Weighted average of 13.0 min {i4} (1967Ch05), 12.8 min {i5} (1970Hn03). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1 From 1989Ra17. 
%IT %IT-branching was established by following the decay of the 556.7|g in {+102}Pd (see 1971Hn05) 
J from 1968Gr01, atomic beam, |p from M1,E2 from 1+ 
T from 1967Ch05. Other: 1970Hn03. 


level_energy_unit: KEV
level_spin_parity: 4(+)
level_comment:
J cascade in {+102}Cd |e decay of 213|g(M1) 58.9|g(M1) and 97.4|g(M1), connecting 2+ to 5+ levels, gives apart from gs J|p=5+,J|p(156.3 level)=3+, and J|p(97.4 level)=4+, 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9-,10-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J J|p=9- favored from DCO, 10- from systematics 
T from time correlation spectrum in {+92}Mo({+12}C,pn) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (12-)
level_lifetime_unit: PS
level_comment:
Data of different (HI,xn|g) reactions for branching of this level are in mutual disagreement (see 1983Tr01 and 1995Ra13) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (13-)
level_lifetime_unit: PS
level_comment:
T the evaluators have correlated the T{-1/2}(274.5|g)=1.50 ps {i33} with the 3194.5-keV level (1995Ra13) and not with a 3661.9-keV level 1 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (14-)
level_comment:
J J|p=14- suggested from DCO and corresponding states in {+106}Ag 
Branching is not reliable because 554.8 is a member of a complex 102 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
E the position of this level was deduced from |g-ray energy differences of |g-rays ordered according to |g|g-coincidence results (1991Ke08). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 12-
level_lifetime_unit: PS
level_comment:
T calculated as a weighted average of T{-1/2}(466|g)=0.49 ps {i11} and T{-1/2}(816|g)=0.46 ps {i9} (1989Vo13) by the evaluators as both |g's deexcite the same level. 
Data of different (HI,xn|g) reactions for branching of this level are in mutual disagreement (see 1981Tr01 and 1995Ra13) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 13-
level_lifetime_unit: PS
level_comment:
T the evaluators have correlated the T{-1/2}(274.5|g)=1.50 ps {i33} with the 3194.5-keV level and not with a 3661.9-keV level as suggested by 1992Le10 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: MIN
level_comment:
$<r{+2}>{+1/2}=4.4976 fm {i70} (2004An14, evaluation) 
J$J=7/2 via atomic beam (1976Fu06). log| {Ift}=5.85 from (5/2)+ to |p=+ 
1970Wa35 determined hyperfine structure anomaly (atomic beam) 
T from ce decay curves (1975Di09); others: 67.2 min {I24} (1966Ja12), 66.3 min {I20} (1962Pa05), 69 min {I6} (1960Pr14), 60 min {I6} (1955Jo25) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
J based on M1 |g decay to 7/2+ g.s. and no feeding from 134-keV, 1/2- isomeric state but 5/2+ and 7/2+ cannot be excluded 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J |p=+ from M1,E2 |g decay to 7/2+, 11/2+ states. If J|p=5/2+ for {+103}Cd g.s., 9/2+ and 11/2+ eliminated from log| {Ift}=6.0 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$|p=+ from M1,E2 to 7/2+. J=3/2,5/2,7/2 from log| {Ift}=5.22 from (5/2)+, |g to 9/2+. No |g decay to 11/2+ favors 5/2 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
E consistent with (1449|g)(27|g) coin relation, I(|g+ce)(27|g,M1) for level intensity balance, and |g-ray pairs of |DE=27 keV including a g.s. transition 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)+
level_comment:
1980Ka05 propose an almost completely different decay pattern for this level; We adopted the decay pattern of 1978Lh01 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_lifetime_unit: PS
level_comment:
E$ Table with the measured lifetimes of 2008Ra06 gives this level as 5300.9, this is likely an error 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$rounded-off energy from adopted levels, gammas 


level_energy_unit: KEV
level_spin_parity: 19/2+
level_comment:
J$listed as 19/2+ in partial decay scheme of 2003Da07. Also compatible with DCO=0.64 {I11}. 19/2- is given in Table with |g energies, so probably typo. 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: MIN
level_comment:
J$from atomic beam (1969Fu11), log| {Ift}=5.48 to 4+ level in {+104}Pd 
T$from 1971Mu22. Others: 70 min {I3} (1959Gi63), 69 min {I3} (1960Am02), 66 min {I1} (1960Nu02), 73 min (1939En02) 
MOMM1$others: +3.917 {I8} (1985Va06), |D<r{+2}>=0.416 {I83} (1989Di12) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
J$from atomic beam (1969Fu11), M1 |g from 90.6, 1+ level 
T$from |b{++} decay 1971Mu22. Others: 27 min {I1} (1959Gi63), 29.8 min {I5} (1960Nu02) 
%IT$from 1990Gu24. This value is very different from the old value (33% {I5}) from 1971Mu22. 
MOMM1$from |b-, and |g-NMR/ON. Others: 3.7 {I1} (2010Go08) from resonant laser ionization source technique, +3.7 {I2} (1961Am02), 4.1 {I3} (cited by 1989Ra17 from a conference report) 
$MOMM1 from 2010Go08 added by B. Singh, Jan 15, 2016 


level_energy_unit: KEV
level_spin_parity: (14)-
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.29 ps {I5} (1989Vo13) and 0.21 ps {I4} (2004Da14). (B. Singh, Jan 15, 2016) 
J$M1 |g to 13- 


level_energy_unit: KEV
level_spin_parity: (15-)
level_lifetime_unit: PS
level_comment:
J$member of a well-developed |D' J=1 sequence 
T$weighted average of 0.20 ps {I4} (1989Vo13) and 0.22 ps {I4} (2004Da14). (B. Singh, Jan 15, 2016) 


level_energy_unit: KEV
level_spin_parity: (16-)
level_lifetime_unit: PS
level_comment:
J$member of a well-developed |D' J=1 sequence 
T$weighted average of 0.25 ps {I5} (1989Vo13) and 0.24 ps {I4} (2004Da14). (B. Singh, Jan 15, 2016) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MIN
level_comment:
MOMM1$ from |b-, and |g-NMR/ON. Other: 3.7 {I1} (2010Go08) from resonant laser ionization source technique. From structure calculations, the measured magnetic moment is consistent with completely mixed configurations: |pg{-9/2}{+-3}{-7/2+}~#|n(d{-5/2},g{-7/2}){-5/2+} and |pg{-9/2}{+-3}{-9/2+}~#|n(d{-5/2},g{-7/2}){-5/2+} 
$ Most intense |g rays in {+104}Pd from decay of {+104}Ag used for |g-NMR/ON method: 555.8 (first 2+ to 0+), 767.6 (first 4+ to 2+), and 941.6 (2265.4, 4+ to first 4+). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (14)-
level_lifetime_unit: FS
level_comment:
T$this value can be compared to 208 fs {I42} (2004Da14: Phys. Rev. C69, 044317); 0.24 ps {I4} in {+104}Ag Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (15-)
level_lifetime_unit: FS
level_comment:
T$this value can be compared to 222 fs {I42} (2004Da14: Phys. Rev. C69, 044317); 0.21 ps {I4} in {+104}Ag Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_comment:
J$L({+3}He,d)=1; L(p,t)=0 
T$from {+105}Ag |e decay (1974Ro18). Others: 41.2~d {I3} (1967Pi03), 40.0~d {I7} (1950Gu54) 
$<r{+2}>=4.5237 fm{+2} {I49} (2004An14) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
J$27.67|g (M1+E2) to 7/2+; systematics in 2013La11; L({+3}He,d)=4 
T$from |g-27.67ce(t) coinc. in 1979Fr03; Other: 1.8 ns {I2} from X-27.67ce(t) coinc. in 1976Sv04 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: NS
level_comment:
J$816.5|g M1+E2 to 13/2+, 1064.9|g E2 to 11/2+ 
T$unweighted average of 5.1 ns {I4} from 1980Le05 by |a|g(t) and 6.0 ns {I2} from 1979Ka05. 
MOMM1 Calculated for J|p=15/2+ from g=+0.497 {I19} obtained by 1980Le05 from DPAD. Other: g=0.58 {I6} (1979Ka05, DPAD) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (27/2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ X |? 4600 (1994Je12). Probably band head of a superdeformed band 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
E$Possible ns isomer just above that level. Suggestion based on 248.6, 615.5, 643.0, and 864.1 |g(t) in 1979Ka05. 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: NS
level_comment:
T$unweighted average of 5.12 ns {I4} in 1980Le05 from |a-|g(t) and 6.0 ns {I2} from 816|g-579|g(t) in 1979Ka05; 6.0 ns {I2} from |g-R.F. in 1985Ke09 
G$+0.508~{I25} from TDPAD in 1985Ke09, +0.497~{I19} from DPAD in 1980Le05, 0.58~{I6} from DPAD in 1979Ka05. 
CONF$|pg{-9/2}{+-1}|nd{-5/2}{+2} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
T from |g-decay (1965Eb01). Others: 24.0 min {I2} (1953Be42), 24.0 min 10 (1973ArZI); see also: 1938Du01, 1938Po03, 1939En02, 1948Mo33, 1961Ra06, 1967St10 
J J=1 from atomic beam (1958Re10,1959Ew89). |p=+ from log| {Ift}=4.9 to 0+ 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
For B(M5)(W.u.)|<10 and |a(90|g)|?1200 one gets branching(IT)|<4.2|*10{+-6}%. %|b{+-} will be completely negligible since the only allowable branch has |DJ=6 
T from |b{++} counting (1988Ry01). Others: 8.46 d {I10} from |g decay (1961Sm04); 8.4 d {I2} (1960Ro12), 8.2 d {I2} (1938Po03) 
J J=6 from atomic beam (1959Ew89). |p=+ from log| {Ift}=5.09 to 5+ 
E based on E|g from J=4+, 503- and 712-keV states via (|a,n|g) 1980Sa05; other: 87.95 (1975An07) 
MOME2 Weighted average of +1.11 {I11} (1989Ra17) and +1.06 {I16} (1989Di12) from collinear LASER spectroscopy 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J |p=+ from L=4 ({+3}He,d); J=2 suggested from |g transition to ground state. Member of probable band built on the g.s. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
J$|p=+ from L=4 ({+3}He,d); J=(3) from strong feeding to (2)+, weak feeding to 1+ and absence of feeding to 6+ 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J |p=+ from L({+3}He,d)=4. 1980Sa05 note that spectroscopic strength of 330-keV excitation in ({+3}He,d) of 1975An07 suggests a doublet, J|p=5+,7+. J=5 from |DJ(239|g,M1+E2)=1. J=5 preferred above J=7 because excitation energy is lower than for 332-keV level 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
J |p=+ from L({+3}He,d)=4. 1980Sa05 note that spectroscopic strength of 330-keV excitation in ({+3}He,d) of 1975An07 suggests a doublet, J|p=5+,7+. J=7 from |DJ(242|g,M1+E2)=1 in {+96}Zr({+14}N,4n|g) preferred above J=5 because excitation energy is higher than 328-keV level 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
J |p=+ from L=4 ({+3}He,d); deexcitation to (3)+ state only. Member of probable band built on the g.s. 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
J |p=+ from M1+E2 to 6+. J=7 from |DJ(536|g,M1+E2)=1 in {+96}Zr({+14}N,4n|g) to J|p=6+ 89 keV level. J=7 preferred over J=5 because excitation energy is much higher than J=6 level. 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
J |DJ(393|g,Q)=2 from |g(|q) in {+96}Zr({+14}N,4n) to J|p=5+ 329 keV level. J=7 preferred above J=3 due to its position in the level scheme. |p=+ because 393|g is very unlikely to be M2 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
J from |DJ(436|g,E1)=1 in {+96}Zr({+14}N,4n). E1 |g to 6+, |g's to 5+ and 7+ 
Levels at 765.14 and 765.62 seen in (|a,n|g) are considered as one level by the evaluators 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: PS
level_comment:
J from |DJ(541|g,E1+M2)=-1 to 332 keV (J|p=7+) level in {+96}Zr({+14}N,4n) 
T from DSA in {+96}Zr({+14}N,4n|g) (1990VoZW) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J (6+)suggested from deexcitation to (5)+, (7)+ states in (|a,n|g). In disagreement with adopted J|p=8- from (HI,xn|g) 


level_energy_unit: KEV
level_comment:
Levels at 1003.4 and 1003.98 observed by 1980Sa05 are considered as the same level by the evaluators, a possibility suggested by the authors 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: PS
level_comment:
J from |DJ(169|g,D+Q)=1 to 843 keV level (J|p=8-) in {+96}Zr({+14}N,4n) 
T from DSA in {+96}Zr({+14}N,4n|g) (1990VoZW) 


level_energy_unit: KEV
level_spin_parity: (3-,4-)
level_comment:
E$should be different from 1106-keV level because this level decays only to (4)- level 
J$suggested by 1980Sa05 in {+103}Rh(|a,n|g) 


level_energy_unit: KEV
level_spin_parity: (2-,3-,4-)
level_comment:
J$suggested by 1980Sa05 in {+103}Rh(|a,n|g) 
J L({+3}He,d)=1 for 1133.83 and/or 1135.66, |g to (3,4)- 


level_energy_unit: KEV
level_spin_parity: 10-
level_lifetime_unit: PS
level_comment:
J from |DJ(376|g,D+Q)=-1 to 9(-) in {+96}Zr({+14}N,4n) 
T from DSA in {+96}Zr({+14}N,4n|g) (1990VoZW) 


level_energy_unit: KEV
level_spin_parity: 11-
level_lifetime_unit: PS
level_comment:
T from DSA in {+96}Zr({+14}N,4n|g) (1990VoZW) 
J from |DJ(720|g,Q)=-2 to 9(-) in {+96}Zr({+14}N,4n) 


level_energy_unit: KEV
level_spin_parity: 13-
level_lifetime_unit: PS
level_comment:
T from DSA in {+96}Zr({+14}N,4n|g) (1990VoZW) 
J from |DJ(981|g,Q)=-2 to 11(-) in {+96}Zr({+14}N,4n) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
E deduced from E|g's originating from 4+ states, at 503 and 712 keV, in cascade to isomer and g.s. 
%|e=100; no evidence of IT decay (1975An07) 


level_energy_unit: KEV
level_spin_parity: (12)
level_comment:
J$ 12+ in table with gamma rays assigned to decay of positive parity states in {+106}Ag (1994Je11), (12) in authors' level scheme 


level_energy_unit: KEV
level_spin_parity: (14)
level_comment:
J$ 14+ in table with gamma rays assigned to decay of positive parity states in {+106}Ag (1994Je11), (14) in authors' level scheme 


level_energy_unit: KEV
level_spin_parity: 18+
level_lifetime_unit: PS
level_comment:
T$effective half-life 
T$effective half-life. Effective half-life is obtained assuming 100% side-feeding into the top of the band via a cascade of 5 transitions with the same moment of inertia as the in-band transitions The highest |g ray for which a line shape was observed was then fitted and the extracted life time is called effective lifetime. This lifetime was used as input parameter to extract the lifetimes of the states lower in the cascade (see also 2005Si23) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J,T$ from adopted dataset for {+106}Ag in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$from Adopted Levels {+106}Ag in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 14-
level_comment:
T$according to 2014LiZZ communication, lifetime of this level is being analyzed 
$B(M1)(J -> J-1)/B(E2)(J -> J-2)=13.0 {I37} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
$Level not populated in the present study 
$Configuration=|pg{-9/2}{+-1}~#|ng{-7/2} 
T$from Adopted Levels {+106}Ag in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$Energy, T{-1/2} and decay modes from {+106}Ag Adopted Levels in the ENSDF database (May 2007 update) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOMM1$other: -0.11367965 {I15} (1974Sa25). |D<r{+2}>=0.148 {I31} (1989Di12) 
J$1/2 (1976Fu06) optical, L=0 (p,t), L=1 ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T$from 1947Br05. Agrees with the last result: 44.5 s {I8} (2000Yo07); Others: 40 s {I2} (1940Al01),44 s {I1} (1951Wo15),43.8 s {I6} (1963Ve13), 44.2 s {I3} (1967Ab07) 
J$E3 transition to 1/2- g.s. 
MOMM1,MOME2$|m using radiation detection of NMR method, Q: level mixing resonance on oriented nuclei. 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: NS
level_comment:
E$follows regional trend of low-lying 9/2+ states: {+101}Ag at g.s., {+103}Ag at 27 keV, {+105}Ag at 53 keV, {+109}Ag at 133 keV, {+111}Ag at 130 keV 
T$from 1972Ja01 (796|g)(32|g)(t), scin. Others: 1962La10, 1969Be75 
B(E2)(9/2+ to 7/2+)=0.24 {I9} exp, 0.185 theory (1974Ku09) 
J$L=4 ({+3}He,d), M1+E2(32|g) to 7/2+ state and syst. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
MOMM1$others: +1.05 {I14} (1984Ba72), +0.92 {I18} (1986Ba14) 
T$5.0 ps {I9} (1974Mi02) recoil-distance Doppler shift 
J$L=2 (p,t), L=1 ({+3}He,d), Coul. ex., M1+E2(325|g) to 1/2- g.s. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
MOMM1$others: +1.13 {I15} (1984Ba72), +1.03 {I18} (1986Ba14), +0.93 {I15} (1984Wo08) 
T$30 ps {I2} (1974Mi02) recoil-distance Doppler shift, 35 ps {I2} (1989Lo08) 
J$L=2 (p,t), J=5/2 from |g(|q) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$0.27 ps {I8} (1970Ro14) DSA. Other: 0.21 ps {I7} (1974Er05) DSA 
J$L=2 (p,t), L=1 ({+3}He,d), Coul. ex., D+Q(786|g) to 1/2- g.s. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
T$from (K| x ray)(829|g)(t) (1969Be75) 
J$L=2 ({+3}He,d), E1(597|g) to 3/2- state, M1(829|g) to 7/2+ state 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.0203 {I22}, I|g(950|g)-branching=12.6% {I10}. Others: 1970Ro14, 1974Er05 (DSA) 
J$L=2 (p,t), M1+E2 |g decays to 3/2-,5/2- states, E2(950|g) to 1/2- g.s., T{-1/2} from B(E2) and DSA methods agree 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$from I|g(1465|g) branching and B(E2) limits (1970Ro14) 
J$L=2 (p,t). M1+E2 |g to 3/2-, not to 5/2- 


level_energy_unit: KEV
level_spin_parity: (15/2)+
level_comment:
Unobserved |g feeding in prompt |g(804|g)-coin spectra suggests 1577-keV isomer (T{-1/2}=?) 
J$|g's to (13/2)+, (11/2)+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T 44.3 s {I2} (1947Br05). Others: 40 s {I2} (1940Al01), 44 s {I1} (1951Wo15), 43.8 s {I6} (1963Ve13), 44.2 s {I3} (1967Ab07), 40 s {I6} (1973Co10) 
E 7/2+ isomerism systematics: 65.7-min {+103}Ag g.s., 7.2-min {+105}Ag at 25 keV, 40-s {+109}Ag at 88 keV, 65-s {+111}Ag at 60 keV 
For model interpretations of anomalously low-lying 7/2+ states in odd-A silver isotopes, see 1972Pa17, 1974Ku09 
%IT=100 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
Branching: I|g(98|g)/I|g(423|g)=0.10 {I2} (1967Bl08), <0.11 (1974Pa15), 0.09 {I3} (1979Sc30) via ({+6}Li,3n|g); see Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
Branching: I|g(786|g)/I|g(462|g)/I|g(364|g)=100/40 {I7}/<15 (1974Pa15), 100/44 {I9}/12 {I6} (1970Ro14, Coul. ex.) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
T from 1969Be75 (K| x ray)(829|g)(t) 
Branching: I|g(829|g)/I|g(797|g)/I|g(597|g)=100/40 {I1}/4.6 {I3} (1974Pa15), 100/40 {I4}/5.3 {I6} (1974HeYW), 100/38 {I14}/4.6 {I8} (1962La10) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
Branching: I|g(950|g)/I|g(856|g)/I|g(625|g)/I|g(526|g)=29 {I3}/2.0 {I4}/78 {I7}/100 (1974Pa15), 24 {I2}/1.8 {I8}/78 {I5}/100 (1970Ro14, Coul. ex.) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
$Branching: I|g(1130|g)/I|g(1097|g)/I|g(898|g)/I|g(800|g)/ I|g(437|g)/I|g(301|g)= 74 {I4}/20 {I2}/100/20 {I2}/2.7 {I4}/27 {I2} (1974Pa15), 72 {I11}/20 {I3}/100/30 {I5}/--/30 {I4} (1974HeYW) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (15/2)+
level_comment:
Isomeric state (T{-1/2}=?) suggested by unobserved |g feeding in prompt |g(804|g)-coin spectra 
Branching: I|g(586|g)/I|g(804|g)=0.51 {I19} (1979Sc30), 0.43 {I3} (1979Po13) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (15/2)+
level_comment:
Branching: I|g(1026|g)/I|g(809|g)=0.35 {I10} (1979Sc30), 0.17 {I6} (1979Po13) 
Assigned to g9/2 band on basis of intraband I|g(cascade)/I|g(crossover) systematics; see 1979Ka05,1979Po13 


level_energy_unit: KEV
level_comment:
E$unresolved doublet. Based on previously known energies of 325 and 423, the authors obtain a 423:325 strength ratio of 3:2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T 5.0 ps {I9} (1974Mi02) recoil-distance Doppler shift. Others: 6.1 ps {I7} from B(E2)=0.212 {I12} and |d(325|g)=-0.207 (adopted value) 
B(E2)=0.202 {I18} (1973Co10,1970Ro14), 0.219 {I15} (1958Mc02) 
g-factor=0.41 {I14} (1973MiZC), 0.59 {I18} (1971SpZT), 0.58 {I20} (1970RoZS), recalculated for T{-1/2} dependence. Core-excitation model predicts g=0.53 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$J=5/2 established by |g(|q) (1958Mc02) 
T 30 ps {I2} (1974Mi02) recoil-distance Doppler shift. Others: 38 ps {I2} from B(E2)=0.308 {I14} and I|g(423|g) branching=93.5% {I6} 
B(E2)=0.334 {I23} (1958Mc02), 0.287 {I24} (1970Ro14), 0.303 {I24} (1973Co10) 
g-factor=0.36 {I13} (1973MiZC), 0.4 {I1} (1971SpZT), 0.71 {I31} (1970RoZS), recalculated for T{-1/2} dependence. Core-excitation model predicts g=0.27 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T from DSA (1970Ro14). Others: 0.21 ps {I7} (1974Er05) DSA; 0.28 ps {I12} from B(E2)=0.0028 {I5}, branching=0.64 {I5} and |d=-0.057 {I10} 
B(E2): from 1970Ro14. Other: 0.0032 (1967Bl08) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.0203 {I22}, branching=12.6% {I10}. Other: 0.84 ps {I27} DSA (1970Ro14). 
B(E2): from 1970Ro14. Other: 0.025 (1967Bl08) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
J$atomic beam (1976Fu06). |p: E1 |g from 2- 
T$from wt avg (Lweight program) of 2.353 min {i9} (1992KaZM), 2.37 min {i1} (1974Ry01), 2.38 min {i3} (1971Jo07), 2.41 min {i2} (1965Eb01), 2.42 min {i2} (1960Wa10), 2.43 min {i5} (1958Gu09). Earlier measurements: 1962Th12, 1957Se19, 1948Pe03, 1948Mo33 
MOMM1$from radiative detection of NMR (1989Ra17) 
E$probable configuration=((|p 1g{-9/2}){+-3}{-7/2+}(|n 2d{-5/2}))1+ 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
J$E1 |g to 1+. M4 |g from 6+. |p from L(d,p)=2 
T$from |g|g(t) in (n,|g). T{-1/2}<1 ns from ce|g(t) in {+108}Ag it decay 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: Y
level_lifetime_info: ;ISO=M
level_comment:
J$optical hyperfine structure pattern (1975Fi07). |p from M4 |g to 2- 
T$from 2004Sc04. 2004Sc04 has followed the decay by using a ionization chamber for about 20 years.Others: 310 y {i132} (1969Vo11), 127 y {i21}(1970Ha32), 418 y {i15} (1992Sc25) 
MOMM1$: from optical interference spectroscopy of hyperfine structure (1989Ra17) 
MOME2$from 1984Be53. 
$J|p:|D<r{+2}>({+108}Ag-{+107}Ag)=0.022 {i3} fm{+2}, ({+110}Ag-{+108}Ag)=0.152 {i10} fm{+2} (1975Fi07) where the {+110}Ag level referred to is the isomer 
E$probable configuration=((|p 1g{-9/2}){+-3}{-7/2+}(|n 2d{-5/2}))6+ 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
J$E1 |g to 2-. |g(|q) and excitation function in (p,n|g) 
T$from p,|g(t) in (p,n|g). Other: 50 ns {i3} (n,|g) 
MOMM1$from |g(|q,H,t) in (p,n|g). 


level_energy_unit: KEV
level_spin_parity: 4-,3-
level_comment:
J$M1-E1-M1 cascade to 6+ via 485 and 156 levels, and |g to 2- establisher J|p(598)=3-,4-, J|p=(156)=5+,6+, and J|p(485)=4-,5- 


level_energy_unit: KEV
level_spin_parity: 2+,3+
level_comment:
E$av res (n,|g) data give J|p=0-,2-, which suggests probable presence of a |p=- level at this energy. No evidence for such a level is seen in the secondary (n,|g) data 
J$M1 |g to 2+, M1 |g to 3+ 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J$M1 |g to 2-. |g to (4)-. Av res (n,|g) suggests J|p=1-,2-,3- for 705.7 + 708.8. Mult(121|g)=M1(+E2) is in conflict with |DJ=2 placement. 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
J$|g's to 1+,3+ and 3-,4- from the 1051.844 level suggests J|p=(2,3+). Decay from the 1051.566 allows J|p=0+,1,2,3+. Av res (n,|g) suggests a doublet with one member having J|p=1+ and the other having |p=-. Feeding from a 0- resonance suggests J=1 for at least one member of the doublet. L(d,p)=(2) for E=1048 {i4}. These data are consistent with J|p(1051.566)=(1+) and J|p(1051.844)=(2-). 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
J$|g's to 1+, 1-, 3+, and 3-. Av res (n,|g) establishes J|p=0- or 2- for either or both 1079.2 and 1079.8. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
J |g(|q) and excitation function are consistent with J=3, not with 1 or 2 
T other: 55 ns {i5} (1974Be47) 
G weighted average of 1.294 {i6} (1974Be47) from d,|g(|q,H,t) and 1.301 {i11} (1976Ha57) from p,|g(|q,H,t). Data are relative to g-factor=+1.443 {i3} (1969Bl18) for the 5/2+, 197 level in {+19}F. All values have been corrected for diamagnetic shielding (1989Ra17). Knight shift corrections have been applied, 0.522% {i3} (1954So05) for the silver in silver value of 1974Be47 and -0.5% {i3} (1974Be47) for silver in palladium value of 1976Ha57. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E deexciting 286.7|g is probably the same transition as the 286.89|g from the 803.7 level or the 287.16|g from the 611.7 level in (n,|g) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J |g(|q) consistent with J=3, |d=+0.017 {i18} or with J=2, |d large. The large |d is not consistent with |a(K)exp data in (n,|g) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$deexciting 113.6|g is probably the same transition as the 113.595|g from the 598.67 level or the 113.800|g from the 408.36 level in (n,|g) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E the deexciting 427.4|g is probably the same transition as the 427.051|g from the 765.47 level in (n,|g) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E the deexciting 212.2|g is probably the same transition as the 212.314|g from the 799.69 level in (n,|g). The unplaced 201.3|g could also deexcite this level 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: Y
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$from Adopted Levels for {+108}Ag in ENSDF database. 
$ Configuration=|pg{-9/2}{+-3}~#|nd{-5/2} 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: Y
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$from Adopted Levels for {+108}Ag in ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: Y
level_comment:
T$Determined relative to T{-1/2}=10.551 y {I11} of {+133}Ba using net peak area ratios of 356-keV from {+133}Ba over 434-keV from {+108}Ag{+m}. One hundred fifty |g-ray spectra, each about 1-week long, were collected over a period of approximately three years. Reported uncertainty includes statistical and systematic contributions. The result supersedes their preliminary half-life value of 440 y {I84} determined from one year data (Norman, E., 2005. Proc. Inter. Conf. Nucl. Data Sci. Technol. St. Fe, NM, AIP Conf. Proc. 769, p14-18). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$from atomic beam (1937Ja01,1950Cr26); |p=+ from L({+3}He,d)=L(d,{+3}He)=L(p,|a)=1, L(t,p)=0 and |m 
MOMM1$by means of the NMR method. Other: -0.13056 {I2} (1954So05) 
CONF$|p(p{-1/2}){+-1} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J$88.0336|g E3 to 1/2-; atomic beam (1965St18) 
T$weighted average of 40 s 2 (1940Al01), 40.4 s 2 (1945Wi11), 39.2 s 2 (1947Br05), 40 s 1 (1951Wo15), 39.80 s {i10} (1967Mi11), 39.3 s {i3} (1967Ab07) and 38.0 s 12 (2000Yo07). Other: 35 s {i5} (1973Co10) 
MOMM1$by means of the NMR method 
MOME2$by means of the Level Mixing Resonance on Oriented Nuclei method 
CONF$|p(g{-9/2}){+-1} 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
J$L({+3}He,d)=(d,{+3}He)=L(p,|a)=4; 44.77|g M1+E2 to 7/2+; 602.5|g E2 from 5/2+ 
T$from |g|g(t) in {+109}Pd |b{+-} decay (1972Ja01). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=(d,{+3}He)=L(p,|a)=1; 311.36|g M1+E2 to 1/2-; 103.9|g M1+E2 from 5/2- 
BE2$weighted average of 0.222 {i19} (1970Ro14), 0.210 {i18} (1973Co10) and 0.249 {i17} (1958Mc02) in Coulomb Excitation 
T$weighted average of 5.9 ps 7, using Recoil Distance Method in Coulomb Excitation (1974Mi02) and 5.9 ps 5 from B(E2)=0.228 {I12} and |d(311.3|g)=0.192 {i7} in Coulomb Excitation. Others: 6.9 ps {i7} by RDM (1970MiZS) and 6.3 ps {i18} (1970Ro14). 
MOME2$-0.54 {I10}, -0.64 {I10}, -0.81 {I10} or -0.91 {I10}, depending on the relative sign of the matrix elements (1972Th16) 
MOMM1$from g=+0.73 {I6} 
$g-factor (transition field method): +0.73 {I6}, weighted average of 0.79 {I12} (1984Ba72), +0.77 {I10} (1984Wo08) and 0.66 {I10} (1986Ba14). Other: 0.58 {I24} (1970RoZS). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2, L(p,|a)=3; 415.17|g E2 to 1/2- 
BE2$weighted average of 0.320 {i26} (1970Ro14) and 0.315 {I24} (1973Co10). Other: 0.377 {i26} (1958Mc02) 
T$weighted average of 32.6 ps {i16} (1989Lo08) and 34.7 ps {i21} (1974Mi02), using the RDM method. Others: 35 ps {i4} (1970MiZS,RDM), 40 ps {i3} (1970Ro14), 40.2 ps {i23} from B(E2)=0.317 {i18} and |d(103.5|g)=-0.039 {i17}. 
MOMM1$from g=+0.34 {I3} 
$g-factor (transition field method): +0.34 {I3}, weighted average of 0.36 {I6} (1984Ba72), +0.36 {I5} (1984Wo08) and 0.29 {I6} (1986Ba14) 
MOME2$-0.16, -0.26, -0.33, or -0.43, depending on the relative sign of the matrix elements (1972Th16) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(d,{+3}He)=L(p,|a)=1; 701.85|g M1+E2 to 1/2- 
T$weighted average of 0.24 ps {i7} (1974Er05) and 0.5 ps {i2} (1970Ro14), using the DSAM method. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J$413.02|g E1+M2 to 3/2-, 636.29|g E2 to 7/2+. |g|g(|q) for 413.02|g in {+109}Pd |b{+-} decay (1977Bo04) is also consistent with J=3/2 
T$from delayed coincidence in {+109}Pd |b{+-} decay (1982Br19) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2; L(p,|a)=3; 862.82|g E2 to 1/2-; 551.4|g(|q) and 862.82|g(|q) in Coulomb excitation (1970Ro14) are only consistent with J=5/2 
T$weighted average of 1.42 ps 21 from B(E2)=0.0173 {I17} (1970Ro14) and 1.3 ps 4 from DSAM (1970Ro14). Other: 1.3 ps {I+8-4} (1974Er05,DSAM) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J$L(p,p')=4; |g(|q) in Coulomb excitation is consistent with J=9/2 (1989Lo08); 675.5|g E2 to 5/2- 
T$from RDM in Coulomb excitation (1989Lo08) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2; 1012.9|g(|q) in Coulomb excitation is consistent with J=3/2 or, with smaller probability, J=5/2 (1970Ro14). 1970Ro14 suggest J=3/2 based on spin of analogous level in {+107}Ag. 
T$from DSAM in Coulomb excitation (1970Ro14) 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2)-
level_comment:
E$Possible multiplet in (p,|a) (1977SmZM) 
J$L(t,p)=4. J=(9/2+) based on DWBA analysis in (p,|a) is inconsistent. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
$1973Co10 observed 327|g (5/2- to 7/2+) and 282 (5/2- to 9/2+) gammas through Coulomb excitation measurements. These gammas have branching ratios of 0.37% {i9} and 0.05% {i3}, respectively. See {+109}Ag Coulomb excitation. The 327|g is also seen by 1983Ch42. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 0.222 {i19} (1970Ro14), 0.210 {i18} (1973Co10) and 0.249 {i17} (1958Mc02). 
T$weighted average of 5.9 ps 7, using Recoil Distance Method in Coulomb Excitation (1974Mi02) and 5.9 ps 5 from B(E2)=0.228 {I12} and |d(311.3|g)=0.192 {i7} in Coulomb Excitation. Others: 6.9 ps {i7} by RDM (1970MiZS) and 6.3 ps {i18} (1970Ro14). 
$Q=-0.54 {I10}, -0.64 {I10}, -0.81 {I10} or -0.91 {I10}, depending on the relative sign of matrix elements (1972Th16) 
$g-factor: +0.73 {I6}, weighted average of 0.79 {I12} (1984Ba72), +0.77 {I10} (1984Wo08) and 0.66 {I10} (1986Ba14). Other: 0.58 {I24} (1970RoZS). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 0.320 {i26} (1970Ro14) and 0.315 {I24} (1973Co10). Other: 0.377 {i26} (1958Mc02). 
T$weighted average of 32.6 ps {i16} (1989Lo08) and 34.7 ps {i21} (1974Mi02), using the RDM method. Others: 35 ps {i4} (1970MiZS,RDM), 40 ps {i3} (1970Ro14), 40.2 ps {i23} from B(E2)=0.317 {i18} and |d(103.5|g)=-0.039 {i17}. 
$g-factor: +0.34 {I3}, weighted average of 0.36 {I6} (1984Ba72), +0.36 {I5} (1984Wo08) and 0.29 {I6} (1986Ba14) 
$Q=-0.16, -0.26, -0.33, or -0.43, depending on the relative sign of matrix elements (1972Th16) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 1.42 ps 21 from B(E2)=0.0173 {I17} (1970Ro14) and 1.3 ps 4 from DSAM (1970Ro14). Other: 1.3 ps {I+8-4} (1974Er05,DSAM) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$from 1970Ro14 by DSAM 
J$1012.9|g(|q) results are consistent with J=3/2 or, with smaller probability, J=5/2 (1970Ro14). 1970Ro14 suggest J=3/2 based on spin of analogous level in {+107}Ag. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
%EC$From 1965Fr01 
J$J=1 from atomic beam magnetic resonance technique (1969Cu09); |p=+ from {+110}Ag |b{+-} Decay (1962Ka07) and |m 
T$Weighted average of 24.7 s {I7} (1970Va08), 24.93 s {I22} (1967Yu01), 24.42 s {I14} (1962Ma38), 24.2 s {I12} (1957Se19), 24 s {I2} (1954Bo39) and 24.5 s {I3} (1946Hi06). Others: 22 s (2010Sc10), 24 s (1944Fl01), 23 s (1938Re04), 22 s (1938Po03) and 22 s (1935Am01) 
MOMM1$2.7111 {I10} (using NMR in 1976Wi03). Other:2.84 {I5} (using atomic beam magnetic resonance technique in 1969Cu09) 
MOME2$0.24 {I12}, determined by measuring the spin-lattice relaxation time (1981Do17) 
CONF$|p7/2[413]~#|n5/2[413] (for prolate deformation), the Gallagher-Moszkowski rule favors J|p=1+ assignment 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$From a least-squares fit to E|g pairs that populate this level and g.s. in {+109}Ag(n,|g) E=thermal. |DE|g are from 1975Cl03, but estimated by the evaluators if not reported reported in 1975Cl03. Others: 1.28 keV {I10} (1970Ka05), 1.113 keV (1979Bo41) and 3.18 keV (1968El03) 
J$From L(d,p)=2; 1.112|g E1 to 1+ 
T$From ce-inner shell vacancy delayed coincidences (1975Cl03) 
CONF$|p1/2[301]~#|n5/2[402] (for prolate deformation) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
%IT$From I(|g+ce)(116|g)=100 - I(|g+ce)(658|g+1476|g+1783|g) 
J$From atomic-beam technique (1958Ew84); 116.48|g M4 to 2- 
T$Weighted average of 249.950 d {I24} (2002Un02), 249.790 d {I16} (1983Wa26) 249.74 d {I5} (1980Ho17), 249 d {I3} (1962Ni01) and 252.5 d {I15} (1957Ge07). Others: 270 d (1950Gu54) and 225 d {I20} (1938Li07) 
MOMM1$Weighted average of +3.589 {I4} (NMR on brute force oriented nuclei in 1992Hu09) and +3.587 {I4} (from atomic-beam magnetic resonance technique in 1967Sc04) 
MOME2$+1.44 {I10} (1984Be53) 
CONF$|p7/2[413]~#|n5/2[413] (for prolate deformation) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
J$117.607|g E1(+M2) to 2-; J=3 from |g(|q) and |g-ray excitation function (1976Ha57); |p=+ from comparison of experimental and calculated g-factors (1974Be47) 
T$Weighted average of 36.7 ns {I7} (from 117.607|g(t) pulsed-beam delayed coincidence method in 1976Ha57), 37 ns {I5} (using pulsed-beam delayed coincidence method in 1974Be47), 36.5 ns {I20}, 37 ns {I4}, 37 ns {I2} (using delayed coincidence technique in 1971Gu05, 1967Es03 and 1963Be51, respectively) and 33 ns {I3} (1967WiZZ as quoted in 2000De11) 
MOMM1$Weighted average of 3.87 {I5} (1974Be47) (reevaluated value using adopted lifetime. |m=3.83 {I5} using T{-1/2}=37 ns {I5} in 1974Be47) and 3.74 {I4} (1976Ha57), (reevaluated value using adopted lifetime. |m=3.73 {I4} using T{-1/2}=36.7 ns {I7} in 1976Ha57) (both |m, deduced from pulsed-beam time-differential perturbed angular correlation technique) 


level_energy_unit: KEV
level_spin_parity: (1,2,3+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$424.71|g to 1+; 423.60|g to 2-. In {+110}Pd(p,n|g), {+109}Ag(d,p|g) a 231.7|g is observed, so that this level can be a close-lying doublet 


level_energy_unit: KEV
level_spin_parity: 0-,1-
level_comment:
E$From neutron separation energy (2003Au03). Other: 6810 keV {i1} (1967Bo06) 
J$From s-wave capture by {+109}Ag g.s (J|p=1/2-) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$Deduced by the evaluators using E|g pairs that populate this level and g.s.. |DE|g were estimated from 1975Cl03. Others: 1.28 keV 10 (1970Ka05), 1.113 (1979Bo41) and 3.18 (1968El03) 


level_energy_unit: KEV
level_comment:
E$possible unresolved doublet 
L$DWBA fit was generated assuming an admixture of 15% L=0 and 85% L=2 transfers. For L=2 transfer, S=0.875 (for d3/2 |n-orbital) or S=0.725 (for d5/2 |n-orbital). For L=0 transfer, S=0.035 (for s1/2 |n-orbital) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
T$From adopted levels 
MOMM1$+3.726 {I36} in 1976Ha57 (g=1.242 {I12}) and 3.831 {I45} in 1974Be47 (g=1.277 {I15}, average of g=1.264 {I20} from {+110}Pd(p,n|g) and g=1.289 {I18} from {+109}Ag(d,p|g)). Both 1976Ha57 and 1974Be47 determined the g-factor using the pulsed-beam differential perturbed angular distribution (DPAD) method 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$Level energy, half-life, J|p and decay modes are from {+110}Ag Adopted Levels in the ENSDF database (August 2011 update) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_comment:
J$from atomic beam (1976Fu06), L(d,{+3}He)=1 
T$from 7.45 d {i1} (1960Ba49), 7.450 d {i17} (1974Ro18). Others: 7.48 d {i1} (1968RoZZ), 7.5 d {i1} (1950Jo53) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T$64.8 s {i8} (1974Gr29) 4|p|b, on-line ms. Other: 74 s {i3} (1957Sc22) 
J$based on E3 |g decay to g.s. Isomeric 7/2+ analogs: 39.6-s {+109}Ag at 88 keV and 44.3-s {+107}Ag at 93 keV 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
T$from |b(ce(K) 70|g)(t) (1976Sv04). Other: 0.92 ns {i4} (1972Ja01) (415|g,575|g,694|g)(70|g)(t) 
J$L=4 ({+3}He,d),(d,{+3}He), M1+E2 |g to 7/2+, no feeding from J|p=5/2+. Analogs: 2.6-ns {+109}Ag at 133 keV, 2.8-ns {+107}Ag at 126 keV 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J$consistent with (1282|g)(575|g)(|q) (1976Be34). Excit in ({+3}He,pn|g) 
E$a 166|g is placed deexciting this level in {+111}Pd decay, but in ({+3}He,pn|g) this transition is from a 876-keV level 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$%|b{+-} feeding assumed negligible for 1U-transition %|b{+-}=0.7 {i2} from 23.4-min {+111}Pd decay data 


level_energy_unit: KEV
level_comment:
$In ({+3}He,pn|g) a 1905.2|g deexcites a 1965.8 level. It is possible that the 1905|g assigned here to the 1964.4 level actually deexcite the higher-energy member of the 1965 doublet 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$associated with 1180-keV state in 23-min {+111}Pd decay |DE=5 given by authors, |DE=10 by evaluators to agree with adopted 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$From half-life measurements, 2015Kr07 provide evidence of population of this level in the decay of the 23.4-min activity, whereas in corresponding dataset in the ENSDF database, this level is absent 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2
level_uncertain: ?
level_comment:
$Level population proposed by 2015Kr07 based on comparison with ({+3}He,pn|g) results from 1987Ze04 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
T$from (96.8|g+245.4|g+342.1|g)(t) (2016Co01) measured over 3 half-lives. 
J$from the Adopted Levels of {+111}Ag in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 2(-)
level_lifetime_unit: H
level_comment:
J$J=2 from atomic beam (1964Ch06); similarities to {+110}Ag. Given the known proton and neutron orbitals near the Fermi surface, no intrinsic state with |p=+ and J=2 can be expected at low energy 
$|m=0.0547 {I5} (1964Ch06), using atomic-beam magnetic-resonance method 
T$Weighted average of 3.14 h 2 (1972Wa03), 3.12 h 1 (1968RoZZ), 3.14 h 5 (1962In01) and 3.16 h 2 (1969Sa09) 
CONF$|pp{-1/2}~#|n(d{-5/2}/g{-7/2}) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
J$direct feeding in {+112}Pd |b{+-} decay (J|p=0+); similarities to {+110}Ag. 
CONF$|pg{-9/2}~#|ng{-7/2} 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (6+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$X|?137 keV, using E(6{++})=118 keV for the same configuration in {+110}Ag. Probably a long-lived isomeric state 
J$97.5|g from (6-); similarities to {+110}Ag 
T$possibly a long-lived isomeric state 
CONF$|pg{-9/2}~#|ng{-7/2} 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_comment:
J$atomic beam (1976Fu06), negative parity from |m. 
T from 1970Tr02. Other: 5.25 h {I4} (1968RoZZ). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%IT$from 1990Fo07 
J$allowed |b{+-} decay to 5/2+ level. E3 |g to 1/2-. 
T$weighted av of 67.8 s {I21} (1974Gr29) and 70.0 s {I25} (1975BrYM). Others: 72 s {I9} (1958Al90), 66 s {I12} (1970Ma47). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Energy, T{-1/2} and decay modes from {+113}Ag Adopted Levels in the ENSDF database (May 2009 update) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
E$from difference in measured masses of ground state and isomer 
MOMM1,MOME2$from hyperfine structure measurements (2024De01) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
T$weighted average of 4.5 s {i3} (1971Fo22), 5.1 s {i3} (1971Ro19), 4.52 s {i7} (1972Wa06), and 5.0 s {i2} (1975BrYN) 
J$log| {Ift}=4.2 from 0+ parent 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (LE 6+)
level_lifetime_unit: MS
level_comment:
T$from 1990Pe10 
E$the relative position of the four transitions in the cascade is not known (34.5, 43.9, 47.4, 73.1) 
J$From sum of multiples of cascading transitions 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
T$from 1964Ba36. Others: 20 min (1969WiZX,1970OsZZ), 21.1 min {I5} (1958Al90), 20.4 min {I17} (1990Fo07) 
J$from log| {Ift}=6.7 to 1/2+, 1U transition to 5/2+, 360.5 level 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T$from 1974Gr29 4|p|b, on-line ms. Others: 20 s {I10} (1958Al90), 49 s {I6} (1968Kj01), 17 s {I5} (1970OsZZ), 55 s {I2} (1970We08), 19 s {I2} (1973BrXC) 
E$E3 transition observed by 1990Fo07 
J$E3 |g to g.s. Isomerism identified in {+111}Ag (T{-1/2}=65 s) at 60 keV, and in {+109}Ag (T{-1/2}=40 s) at 88 keV 
%IT$from 1990Fo07 


level_energy_unit: KEV
level_spin_parity: (0-)
level_lifetime_unit: S
level_comment:
J$Before 2005Ba94 J|p was (2)- but now E3 |g from 3+ gives 0+ 
T$From2009BA52. Other: 237 s {I5} (2005Ba94). Previous measurements were lower: 2.5 min {I1} (1958Al90), 2.68 min {I1} (1970OsZZ), 2.58 min {I8} (1974Gr29), 2.65 min {I6} (1974Bj01), 2.70 min {I8} (1990Fo07). These data were contaminated by the 20 s isomer 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
$%IT: from 2005Ba94, %IT=6.0 (1990Fo07) 
J$E3 |g to (3+), 
T$weighted av: 9.8 s {I1} (2005Ba94),10.4 s {I8} (1971Fo22), 10.5 s {I5} (1974Bj01), 8.5 s {I2}(1974Gr29), 8.7 s {I2} (1970OsZZ), 8.2 s {I2} (1990Fo07) 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: S
level_comment:
J log| {Ift}=6.0-7.0 to 0+ and 2+; (E1) 379|g-(M1) 49.8|g- M1 45.8|g cascade relation from the 1+ level allows |p=- 
T from 1979HiZR. Others: |?5 s (1967Fr16), 5.3 s {I9} (1968We10), 5.6 s {I2} (1969We11), 3.7 s {I2} (1971Fo22), 4.00 s {I4} (1974Gr29) 


level_energy_unit: KEV
level_spin_parity: 4(+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%IT From {+118}Ag IT decay (2.0 s) 
J E3 |g to 1(-) 
T from 1979HiZR. Others: 1.9 s {I2} (1989Ko22), 2.8 s {I3} (1971Fo22) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Energy, T{-1/2} and decay modes from {+118}Ag Adopted Levels in the ENSDF database (Feb 1993 update). Note that J|p=4(+) in ENSDF dataset 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J$from syst of spins and parities for low-lying levels in lighter odd-Ag isotopes, no |b-feeding to the g.s. of {+119}Cd. 
T$from |g(t) (1975Ka09) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
J$from syst of spins and parities for low-lying levels in lighter odd-Ag isotopes 
T$from |b(t) (1970OsZZ) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$2017Ki08 mention this level as the ground state. In {+119}Ag Adopted Levels in the ENSDF database (Dec 2008 update), two long-lived activities of 2.1-s, (7/2+) and 6.0-s, (1/2-) are listed without any information about their relative spacing. In 2017Au03 (NUBASE-16), (7/2+) state is treated as an isomer at an energy of 20 keV {I20} from systematic trend. 
$T{-1/2} and decay mode from {+119}Ag Adopted Levels in the ENSDF database. 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 


level_energy_unit: KEV
level_spin_parity: 3(+)
level_lifetime_unit: S
level_comment:
J log| {Ift} values to 2+ and 4+ allow J=3, syst of spin and parity for g.s. in even-Ag isotopes 
T$weighted average of 1.17 s {I5} (1971Fo22) and 1.25 s {I3} (1983Re05) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
$Energy, T{-1/2} and decay modes from 2017Au03 (NUBASE-16), where J|p=7(-), where original data are from mainly from 2012Ba58 (Phys. Rev. C86, 064311). For half-life, data from 2003Wa13 (Phys. Rev. C67, 064303) and 1971Fo22 (Phys. Lett. B36, 334) were also used. Note that J|p=6(-) in {+120}Ag Adopted Levels in the ENSDF database (Dec 2001 update) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
%B-N$The %|b{+-}n is an average, given by the authors, of 0.093 {I2} deduced using their value of T{-1/2}=0.91 s {I6} from delayed-n counting, and 0.067 {I2} deduced using their value of T{-1/2}=0.78 s {I1} from |b-ray counting. The authors' uncertainty was chosen to overlap the two values. 
T$weighted average of 0.78 s {I1} (|b-ray counting: 1983Re05), 0.72 s {I10} (|b-ray counting: 1982Fo10), 0.91 s {I6} (delayed n-counting: 1983Re05), 1.04 s {I8} (|b-ray counting: 1995Fe12), 0.8 s {I1} (|g-ray counting: 1974Gr29), 0.661 s {I+75-72} (delayed n-counting: 2006Mo07) 
J$from systematics, J|p is expected to be 1/2- or 7/2+. |b feeding of the 508, 879, and 1341 levels, which have J|p=(7/2-) or higher, ruled out the 1/2- alternative. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
$Level half-life and decay mode from {+121}Ag Adopted Levels in the ENSDF database (Jan 2009 update) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 1/2-
level_comment:
E$only single state was observed in Penning Trap measurement due to low statistics and short half-life of the isomer 
MOMM1$from hyperfine structure measurements (2024De01) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: S
level_comment:
%|b{+-}n from neutron counting (1983Re05). other: %|b{+-}n|<1.3 from |bn coincidence (2006Mo07) 
E Assumed as g.s. 
J log {Ift}|?5.4 to 2+ and 5.9 to (4+) suggest (3+) 
T $weighted average of 0.520 s {I14} (1995Fe12) and 0.57 s {I3} (1983Re05); others: 0.48 s {i8} from |g multiscaling (1978Sh03); 0.357 s {I24} for a mixed source of gs and msec isomers, from |b decay curve (2006Mo07) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J $from hyperfine splitting (2000Kr18) 
T $from beta-delayed neutron decay curve as a function of laser frequency (2000Kr18); other: 0.357 s {I24} for a mixed source of gs and msec isomers (2006Mo07). 


level_energy_unit: KEV
level_spin_parity: (9-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
E$Q{-|b} systematics: E(high spin)-E(gs)=80 {I50} in NUBASE (2003Au02) 
J $from hyperfine splitting (2000Kr18) 
T $from beta-delayed neutron decay curve as a function of laser frequency (2000Kr18); other: 0.357 s {I24} for a mixed source of gs and msec isomers (2006Mo07). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
J$from systematics of lower mass odd-Ag isotopes J|p=1/2- or 7/2+, but 1/2- is disfavored by the observed |b feeding of three levels which feed an 11/2(-) isomer 
T$weighted average of 0.272 s {I24} (2006Mo07, implant-|b correlations); 0.293 s {I7} (1995Fe12, |b and neutron counting using a laser-ionized source at ISOLDE-CERN facility); 0.35 s {I4} (1989Hu10, |g-counting); 0.30 s {I2} (1986Ma42, |g counting); 0.30 s {I1} (1983Re05; neutron counting); 0.350 s {I20} from neutron and |g-decay curves (2021Te02). Others: 0.396 s {I15} (2014TeZY) from neutron and |g-decay curves; 0.39 s {I3} (1976Lu02, neutron counting) 
$%|b{+-}n: weighted average of 0.55 {I9} (1983Re05, uncertainty of 3.6% statistical and 15% systematic given in 1983Re05 combined in quadrature by the evaluator), 0.60 {I25} (2014TeZY, neutron-|b measurement), 1.0 {I5} (2006Mo07, from implant-|b decay curve analysis), and 1.01 {I24} (2021Te02, neutron counting) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
E$the position of the 1/2- isomer is identified by 2019Ch24 in {+123}Pd |b{+-} decay based on |g|g-coin; 0+x in 2013La11. 
J$from shell-model predictions (2019Ch24) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
E$this isomer feeds the 1426.4 level directly or indirectly (2013La11), but the feeding transition has not been observed. 
T$from |g(t) (2013La11) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
E$this isomer feeds the 1426.1 level directly or indirectly (2013La11), but the feeding transition has not been observed. 
T$from |g(t) of 382|g+592|g+390|g (2013La11) 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
T$from |g(t), weighted average of 393 ns {I16} (2013La11) and 396 ns {I37} (2009St28). Other: 0.32 |ms {I3} (2006ToZW) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
T$fitted from neutron activity with respect to the implant and decay time at the tape station. 
$%|b{+-}n: from weighted average of extracted P{-1n} for individual I|b values with respect to the |g transitions using values in 1989Hu10. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3+)
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=111 ms, %|b{+-}n=1.26 (2003Mo09) 
$On the basis of half-life of low-spin activity, %|b{+-}n measured in 2006M007 is assumed for this level rather than the 144-ms high-spin activity 
T$from |g-decay curves (2014Ba18). Others: 180 ms {I3} (2015Lo04, ion-|b correlated curve), 187 ms +15-14 (2006Mo07), 172 ms {I5} (1995Fe12, delayed-neutron decay curve), 0.17 s {I3} from |g multiscaling (1984Hi03) and 0.54 s {I8} from delayed-neutron multiscaling (1983Re05). It is possible that half-life values in 2015Lo04, 2006Mo07, 1995Fe12 and 1984Hi03 are for mixed activities proposed by 2014Ba18 
J$from 2013La11 based on systemmatics. However, shell-model calculations by 2013La11 suggest 1- ground state and 3+ at 64 keV. 2012Au07 suggest 3+ from systematics. Others: (2-) (2014Ba18) from decay pattern to levels in {+124}Cd and shell-model configuration, |>2 (2005Ka45) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (8-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
$Measured %|b{+-}n=1.3 {I9} (2006Mo07) is assumed for the low-spin activity, however, it is possible that the high-spin isomer also decays by delayed-neutron emissions 
J,T$from 2014Ba18, half-life from |g-decay curves. Other: J|>7 (2005Ka45) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_uncertain: ?
level_comment:
E$reverse ordering of the 75.5-155.6 |g cascade is also possible, which will give a level at 75.5 keV instead of 155.6 keV 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M3
level_comment:
T$weighted average of 1.46 |ms {I20} (2013La11), 1.62 |ms {I+29-24} (2012Ka36), 1.3 |ms {I3} (2005WaZY) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3+)
level_comment:
J$from 2013La11 based on systemmatics. However, shell-model calculations by 2013La11 suggest 1- ground state and 3+ at 64 keV. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M3
level_comment:
J$from systematics and observed decay pattern (2013La11). However, shell-model calculations by 2013La11 suggest 1- ground state and 3+ at 64 keV. 
T$weighted average of 1.46 |ms {I20} (2013La11), 1.62 |ms {I+29-24} (2012Ka36), 1.3 |ms {I3} (2005WaZY) 
$Number of implanted fragments=5.7|*10{+4} (2012Ka36) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Other measurement: 1.3 {I9} (2006Mo07: Phys. Rev. C 73, 035801); <9 (2014SmZZ: thesis, Univ. of Notre Dame, work at GSI) 
E$according to 2014Ba18 (Phys. Rev. C 89, 054321), it is assumed that the 205-ms activity corresponds to the g.s. of {+124}Ag. 2014Ba18 proposed a high-spin isomeric activity with T{-1/2}=144 ms {I20} 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 180 ms {I3} (2015Lo04: Phys. Rev. Lett. 114, 192501, could be for mixed activity); 191 ms {I28} (2014Ba18, assigned by authors to the decay of the g.s.); 187 ms {I+15-14} (2006Mo07, could be for mixed activity). Others: 256 ms {I78} (2014TeZY, thesis IPNO-T-13-07); 230 ms {I+28-25} (2014SmZZ); three other values from 1983-1995. Weighted average of values from 2021Ha19 (assuming the half-life for g.s. decay only) and 2014Ba18 is 201 ms {I15} (compiler's note) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=111 ms, %|b{+-}n=4.1 (2003Mo09) 
J$others: 7/2+ from systematics (2012Au07), 9/2+ in theoretical calculations (1997Mo25) 
T$weighted average of 166 ms {I7} (1995Fe12, delayed neutron decay curve) and 150 ms {I8} (2015Lo04, ion-|b correlated decay curve) 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$from |g(t); weighted average of 0.474 |ms {I35} (2013La11), 0.498 |ms {I+21-20} (2012Ka36), and 0.47 |ms {I11} (2009St28, earlier value: 0.44 |ms {I9} in 2006ToZW and 2007To23). Other: 240 ns {I50} (2005WaZY, many authors are same as for 2009St28) 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$weighted average of 0.474 |ms {I35} (2013La11), 0.498 |ms {I+21-20} (2012Ka36), and 0.47 |ms {I11} (2009St28, earlier value: 0.44 |ms {I9} in 2006ToZW and 2007To23). Other: 240 ns {I50} (2005WaZY, many authors are same as for 2009St28) 
$Number of implanted fragments=2.4|*10{+5} (2012Ka36) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Other measurement: 11.8 {I10} (2014SmZZ: thesis, Univ. of Notre Dame, work at GSI); P{-n} values measured for {+123},{+124},{+125},{+126}Pd and {+125},{+126},{+127},{+128}Ag in this work are systematically much larger as compared to corresponding values in 2021Ha19 
E,J$the 146-ms activity is assumed to correspond to the decay of the g.s. of {+125}Ag, proposed as (9/2+) in 2013La01 ( Phys. Rev. C 87, 034308). Note that 2019Ch24 (Phys. Rev. Lett. 122, 212502) proposed 1/2- isomer in {+125}Ag 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier value: 150 ms {I8} (2015Lo04: Phys. Rev. Lett. 114, 192501). Others: 267 ms {I10} (2014TeZY, thesis IPNO-T-13-07); 163 ms {I+11-9} (2014SmZZ); 166 ms {I7} (1995Fe12: Z. Phys. A353, 9). Weighted average of values from 2021Ha19 and 2015Lo04 is 149 ms {I8} (compiler's note) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
$%|b{+-}n deduced by 2021Ba34 from decay scheme 
J$from the decay pattern of {+125}Pd, and shell-model calculations performed by 2019Ch43 (Phys. Rev. Lett. 123, 142501) using the KSHELL code with 
T$measured by 2021Ba34, with a weighted average of 176.1 {I49} s, 176.4 {I50} s, 173.5 {I80} s, and 174 {I15} s from decay curves for 50.5, 384.1, 643.8, and 606.6-keV |g rays, respectively 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_comment:
$%|b{+-}n deduced by 2021Ba34 from decay scheme 
E,J$From 2019Ch43 
T$measured by 2021Ba34 from decay curve of 352.6-keV |g ray 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
$Measured %|b{+-}n: 3.8 {I2} (2021Ha19), 13.7 {I11} (2014SmZZ). These values probably include 0+x and 0+y levels 
J$as proposed in 2013La11 based on systematics of odd-odd Ag isotopes as well as the N=79 isotone {+128}In. 2021Ko07 also suggested 3+ from systematics. Other: J|<4 (2014Ba18) from decay pattern to levels in {+126}Cd. 
T$from background-subtracted sum of the transitions de-exciting the 1579-, 1944-, 2469- and 2662-keV levels in {+126}Cd (2014Ba18). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (GE 8)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
$Measured %|b{+-}n: 3.8 {I2} (2021Ha19), 13.7 {I11} (2014SmZZ). These values probably include 0+x and 0+y levels 
E$2021Ko07 suggested 100 {I100} from systematics 
J$from decay pattern to levels in {+126}Cd (2014Ba18). 2021Ko07 proposed 9- from systematics 
T$from background-subtracted sum of the transitions de-exciting the 2120-, 2584-, 2666- and 2758-keV levels in {+126}Cd (2014Ba18). Other measured T{-1/2} values: 103.2 ms {I14} (2021Ha19), 98 ms {I5} (2015Lo04), 114 ms {I3} (2014SmZZ), 95 ms (2000Ka48), 107 ms {I12} (1995Fe12). Only one activity in {+126}Ag is reported by 2021Ha19, 2015Lo04, 2000Ka48 and 1995Fe12, whose half-life agrees with that of the high-spin isomer in 2014Ba18. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M3
level_comment:
J$based on systematics and observed decay pattern (2013La11). 
T$from |g(t) (2013La11). Other: >20 |ms (2012Ka36) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3+)
level_comment:
J$as proposed in 2013La11 based on systematics of odd-odd Ag isotopes as well as N=79 isotone {+128}In. However, shell-model calculations by 2013La11 suggest 1- ground state and 3+ at 231 keV. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$Number of implanted fragments=1.3|*10{+5} (2012Ka36) 
J$based on systematics and observed decay pattern. However, shell-model calculations by 2013La11 suggest 1- ground state and 3+ at 231 keV. 
T$from |g(t) (2013La11). Other: >20 |ms (2012Ka36, |g(t), estimated value because |g-ray events were equally distributed in the 20-|ms range of the time spectrum) 


