# DECAY

decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|a(K)exp=0.0029 {I3} (1989Ri03). 
RI corrected for expected small contribution from an unresolved transition; see comment on 1036|g from 1755.8 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|a(K)exp=0.017 {I4} (1989Ri03). 
Other: E|g=633.9 {I3}, I|g=6.0 {I10} (2007ChZX; Budapest data). Evaluator suspects |g may be complex in 2007ChZX. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other: E|g=697.68 {I20}, I|g=3.9 {I10} (2007ChZX; Budapest data). Evaluator suspects |g may be complex in 2007ChZX. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
|a(K)exp=0.013 {I5} (1989Ri03). 
M |a(K)exp lies between |a(K)(E1) and |a(K)(E2); |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|a(K)exp=0.0127 {I9} (1989Ri03). 
Other: E|g=588.91 {I17}, I|g=8.7 {I15} (2007ChZX; Budapest data). Evaluator suspects |g may be complex in 2007ChZX. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E0)
decay_comment:
|a(K)exp=0.017 {I3} (1989Ri03). 
Other: E|g=738.7 {I3}, I|g=4.4 {I15} (2007ChZX; Budapest data). Evaluator suspects |g may be complex in 2007ChZX. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI see comment on 1245|g from 1763 level. 
|a(K)exp=0.0021 {I5} (1989Ri03); mult=E2 for possible doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other: E|g=851.8 {I3}, I|g=6.8 {I15} (2007ChZX; Budapest data). Evaluator suspects |g may be complex in 2007ChZX. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E|g=1054.25 {I3} (from 1755.3 level in 1989Ri03) fits this placement. I(1054|g):I(1197|g)=12.2:11.6 (1988Bo44); however, see comment on 1054|g from 1755.3 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E 1095.77 {I8} (from 1614 level in 1989Ri03) does not fit this placement; placement from 1573 level not adopted. I(1095|g):I(1197|g)=9.3:11.6 (1988Bo44). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI see comment on 1197|g from 1811 level. 
|a(K)exp=0.0086 {I13} (1989Ri03) and mult=M1+E0 for doublet. However, mult=E0 component is inconsistent with both placements in level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
|a(K)exp=0.0037 {I19} (1989Ri03). 
Other: E|g=1238.6 {I6}, I|g=6.3 {I15} (2007ChZX; Budapest data). Evaluator suspects |g may be complex in 2007ChZX. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E0)
decay_comment:
|a(K)exp=0.0081 {I13} (1989Ri03). 
Other: E|g=1007.85 {I11}, I|g=18 {I3} (2007ChZX; Budapest data). Evaluator suspects |g may be complex in 2007ChZX. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|a(K)exp=0.0050 {I7} (1989Ri03). 
Other: E|g=984.69 {I20}, I|g=13.1 {I24} (2007ChZX; Budapest data). Evaluator suspects |g may be complex in 2007ChZX. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement from 1988Bo44, where I(1025|g):I(985|g)=8.9:31.0 is almost consistent with I|g apportionment of presumed doublet in 1989Ri03 as deduced from 1726 level branching. E|g, however, is 0.3 keV low for this placement. E|g=1024.3 {I3} from 2007ChZX (Budapest data) is even further from expected value. 
RI,M see comments on 1025|g from 1726 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
|a(K)exp=0.0089 {I19} (1989Ri03). I(938|g):I(1112|g)=17.4:68.3 (1988Bo44), consistent with I|g data from 1989Ri03. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
|a(K)exp=0.0071 {I11} (1989Ri03). I(1005|g):I(1112|g)=28.4:68.3 (1988Bo44). 
Evaluator rejects alternative placement (1991Bo51) of |g from an otherwise unsupported 1481.6 level because that two-photon cascade measurement could not differentiate between a 1005.2|g-476.3|g cascade from a 1481.6 level and the 478.4|g-1003.7|g cascade from the established 1482.0 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
|a(K)exp=0.0051 {I12} (1989Ri03), mult=M1+E2, |d=0.9 {I+12-5} for probable doublet. 
RI 2.99 {I21} for doublet and I(1025|g):I(1112|g)=21.4:68.3 (1988Bo44) and I(1112|g)=4.8 {I7} (1989Ri03) imply I(1025|g from 1726 level)=1.5, leaving I|g=1.5 for 1025|g from 1706 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
|a(K)exp=0.0049 {I6} (1989Ri03) and mult=M1+E2 for doublet. I(1046|g):I(1112|g)=17.1:68.3 (1988Bo44). From I|g(1046 doublet)=3.90 {I20} and I|g(1112)=4.8 {I7} in 1989Ri03, one expects I|g(1046 from 1726 level)=1.2, leaving I|g(1046)=2.7 from 1169 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
|a(K)exp=0.0099 {I16} (1989Ri03). 
M |a(K)exp>|a(K)(M1) but an E0 component is inconsistent with placement. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
EG=1305.45 13 FROM 1989Ri03 IMPLIES E(LEVEL)=1726.35 13. 
No E|g from 1989Ri03 fits this placement; not adopted. I(1305|g):I(1112|g)=12.0:68.3 (1988Bo44). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g=5.0 {I4}, |a(K)exp=0.0020 {I4}, mult=E2(+M1) (1989Ri03). I|g I(1351|g):I(1112|g)=31.2:68.3 (1988Bo44) is inconsistent with branching from 1989Ri03; 1351|g is probably a multiplet in 1989Ri03 with I|g=2.3 deexciting the 1726 level, leaving I|g=2.7 to deexcite the 2053 and/or 2071 levels. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
|a(K)exp=0.06 {I4} (1989Ri03). Other: 0.4 {I2} (1976Be23). 
M E2 or possibly E1 from |a(K)exp of 1989Ri03. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
|a(K)exp=0.0108 {I16} (1989Ri03). 
M M1+E0 from |a(K)exp, but E0 component inconsistent with placement; the ce spectrum could conceivably contain an undetected impurity. 
Other I|g: 7.8 {I24} (2007ChZX; Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
|a(K)exp=0.0050 {I10} (1989Ri03). I(1356|g):I(1117|g)=34.7:47.6 (1988Bo44). 
M |a(K)exp does not rule out an E0 component, but |DJ=1 from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|a(K)exp=0.0059 {I3} (1989Ri03); corresponds to |d=0.38 {I+18-16}. 
E|g also consistent with placement from 1573 level. For 1755 level, I(1141|g)/I(1054|g) in 1988Bo44 and I(1141|g) in 1989Ri03 imply that all I(1054|g) of 1989Ri03 belongs here; leaving essentially no I|g for placement from the 1573 level. 
Other: E|g=1054.44 {I9}, I|g=17.5 {I15} (2007ChZX; Budapest data). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
I(1036|g):I(1279|g)=15.5:54.1 (1988Bo44). The 1035.197 {I15} |g (I|g=16.2 {I10}), placed from 1250 level by 1989Ri03, could plausibly be a doublet which includes this transition. From branching in 1988Bo44 and I(1279|g)=3.6 {I3} (1989Ri03), I|g=1.0, 15.2 for |?1035|g from 1755.8, 1250 levels, respectively. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
The 1076.7|g (I|g=2.8 {I3}), placed from 1199 level by 1989Ri03, is a doublet which presumably includes this transition. From I(1077|g):I(1279|g)=20.8:54.1 (1988Bo44) and I(1279|g)=3.6 {I3} (1989Ri03), I(1077|g from 1755 level)=1.4 leaving I|g=1.4 for 1077|g from 1199 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement from 1991Bo51. I(1237|g):I(1279|g)=34.0:54.1 (1988Bo44), combined with I(1279|g)=3.6 {I3} (1989Ri03), suggests that 1238|g (I|g=6.8 {I3}) in 1989Ri03 is a doublet having I|g=2.3 at this placement and I|g=4.5 unplaced. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
|a(K)exp=0.0038 {I11} (1989Ri03). I(1381|g):I(1279|g)=44.0:54.1 (1988Bo44), consistent with I|g in 1989Ri03. Placement is from 1991Bo51 (E|g misprinted as 1387.84 {I6} in 1991Bo51). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement from 1991Bo51. I(969|g):I(1544|g)=19.3:13.9 (1988Bo44). I(969|g)/I(1543|g)=1.4 in 1988Bo44 cf. 0.82 {I19} in 1989Ri03. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
|a(K)exp=0.0040 {I4} (1989Ri03), mult=M1+E2 for possible doublet. 
RI I(1061|g):I(1388|g)=25.0:63.9 (1988Bo44). Placement from 1988Bo44 and (n,|g) E=7.78 eV res; however, I|g=9.2 {I7} in 1989Ri03 suggests 1062|g is a doublet in 1989Ri03 with I|g=3.5 from 1763 level and the remaining I|g=5.7 unplaced. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
|a(K)exp=0.0021 {I5}, mult=E2 for doublet. 
Placement from 1988Bo44; placed from 1459 level by 1989Ri03. 
RI I(1245|g):I(1388|g)=23.7:63.9 (1988Bo44) and I|g=5.86 {I23} in 1989Ri03 imply I|g=3.3 from 1763 level, leaving I|g=2.6 from 1459 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M see comment on 1197|g from 1573 level. 
RI based on I(1197|g)/I(1110|g) from 1988Bo44, I(1197|g) from 1811 level in 1989Ri03 should be 8.5; this leaves no I|g for the alternative placement of the 1197|g from the 1573 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from I(1293|g):I(1110|g)=5.4:17.9 (1988Bo44), I(1293|g) from 1811 level in 1989Ri03 should be 1.8, leaving I|g=0.9 for placement from the 1668 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI E|g=1120.83 {I2} (I|g=12.1 {I4}), placed elsewhere by 1989Ri03, may include this transition. From I(1119|g):I(1446|g)=5.2:19.5 (1988Bo44) and I(1446|g)=5.8 {I7} in 1989Ri03, I(1121|g from 1821 level)=1.5, leaving I|g=10.6 for 1121|g from 1121 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
1988Bo44 place |g of similar energy from 2228 level; since E|g from 1989Ri03 is low for placement from 1929 level, evaluator shows this placement as tentative. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
I(1267|g):I(1332|g)=12.0:15.6 (1988Bo44). 
E|g close to unplaced E|g=1266.04 {I5} (I|g=6.6 {I6}) of 1989Ri03, but E|g from 1989Ri03 implies E(level)=1945.56 {I6} which is 5|s low. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E|g=1350.75 {I9}, placed from 1725 level by 1989Ri03, may be a multiplet including this transition. 
I(1352|g):I(1332|g)=6.3:9.3 (1988Bo44). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E|g=1350.75 {I9}, placed from 1726 level by 1989Ri03, may be a multiplet including this transition. 
I(1350|g):I(1650|g)=11.0:12.5 (1988Bo44). Other: 8.3 {I19}:28.2 {I19} (2007ChZX, Budapest data). 
Other data: E|g=1350.4 {I3}, I|g=8.3 {I19} (2007ChZX, Budapest data), but |g may have more than one placement. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2070.1 3. 
May be same as unplaced E|g=1456.0 {I3} in 1989Ri03. 
I(1457|g):I(1650|g)=10.7:12.5 (1988Bo44). 
Absent in 2007ChZX (Budapest data). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
Other data: E|g=1649.78 {I10}, I|g=28.2 {I19} (2007ChZX, Budapest data); |g appears to be too strong relative to 1350|g so it may be complex. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2082.3 3. 
May be same as E|g=1381.2 {I3} in 1989Ri03, now placed from 1755 level; if so, I|g=3.5 {I8} in 1989Ri03 will be for a doublet. 
I(1382|g):I(1606|g)=6.0:25.7 (1988Bo44). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2081.80 25 IF IT FEEDS 681 LEVEL. 
May be same as unplaced E|g=1400.77 {I25} in 1989Ri03; if so, I|g (4.7 {I6}) in 1989Ri03 implies a doublet. 
I(1403|g):I(1606|g)=8.1:25.7 (1988Bo44). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2081.4 4. 
May be same as unplaced E|g=1605.1 {I4}, I|g=2.3 {I7} in 1989Ri03. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2088.47 14. 
May be same as unplaced E|g=1407.44 {I14} in 1989Ri03. 
I(1409|g):I(1713|g)=7.4:17.1 (1988Bo44). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2147.21 7. 
May be same as E|g=1446.16 {I7}, unplaced in 1989Ri03. 
I(1445|g):I(1532|g)=5.6:9.9 (1988Bo44) but 5.8:2.0 in 1989Ri03. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2147.06 19. 
May be same as E|g=1530.31 {I19}, unplaced in 1989Ri03. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2183.36 9. 
May be same as unplaced E|g=1502.33 {I9} in 1989Ri03; however, I(1502.33|g) is higher than expected, and this may indicate a doublet. 
I(1503|g):I(1462|g)=4.9:6.9 (1988Bo44). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement from 1988Bo44; placed from 1929 level by 1989Ri03, but E|g slightly low for that placement. 
I(1508|g):I(1807|g)=16.9:21.6 (1988Bo44). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement from 1988Bo44; placed from 1763 level by 1989Ri03. 
I(1549|g):I(1508|g)=7.3:16.9 (1988Bo44); from I(1549|g)=3.8 {I3} in 1989Ri03, one expects I|g=0.70 from 2228 level, leaving I|g=3.1 from 1763 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2250.42 9. 
May be same as unplaced E|g=1462.24 {I9} in 1989Ri03; however, I(1462.24|g) is higher than expected, and this may indicate a doublet. 
I(1461|g):I(2035|g)=11.5:27.9 (1988Bo44). 
Absent in 2007ChZX (Budapest data). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2250.92 19. 
May be same as unplaced E|g=1530.31 {I19} in 1989Ri03. 
I(1529|g):I(2035|g)=10.1:27.9 (1988Bo44). 
Absent in 2007ChZX (Budapest data). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2309.0 5. 
May be same as unplaced E|g=1588.4 {I5} in 1989Ri03. 
I(1588|g):I(1888|g)=9.5:10.4 (1988Bo44). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
EG FROM 1989Ri03 GIVES E(LEVEL)=2393.3 4. 
May be same as unplaced E|g=1605.1 {I4} in 1989Ri03. 
I(1606|g):I(1973|g)=8.9:41.7 (1988Bo44). 
Absent in 2007ChZX (Budapest data). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
I(1715|g):I(1973|g)=7.9:41.7 (1988Bo44). 
Other: E|g=1714.7 {I3}, I|g=6.8 {I15} in 2007ChZX (Budapest data), but stronger branches from same level are not reported there. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
Other: E|g=2462.5 {I3}, I|g=10.2 {I19} (2007ChZX; Budapest data). Evaluator suspects |g may be complex in 2007ChZX. 
I(2463|g):I(2559|g)=7.7:18.4 (1988Bo44). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from table 1 of 1989Ri03; 1.4 {I7} (based on table 3) is presumed by the evaluator to be a misprint. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placed elsewhere in (n,|g) E=thermal. Associated with upper member of doublet and with a 1250 level in Adopted Levels, Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g in (n,|g) E=thermal does not allow this placement. Associated with upper member of doublet in Adopted Levels, Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Placed elsewhere in (n,|g) E=thermal. Associated with upper member of doublet in Adopted Levels, Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI I|g|<0.54 may be from {+116}In |b{+-} decay. 
|g placed elsewhere in (n,|g) E=thermal. Not adopted. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1958Ch36. 
|a(K)exp=1.69 {I5} (1966As02); K/L=4.5 {I6} (1960Bl10). 
M from |a(K)exp and K/L. 
MR from |g(|q) (1966As02), value adopted by 1976Kr21. Other values: 0.309 {I15}, from B(E2)=1.76 {I10} (1961Ha21) and T{-1/2}=37 ps {I3} (1960Bl10); 0.44 {I6}, from |a(K)exp; 0.44 {I9} from K/L=4.5 {I6} (1960Bl10 deduce 0.29 {I3}). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from |a(K)exp=1.11 {I5} (1966As02). 
MR from |g(|q) (1966As02). Others: 0.26 {I+12-26} from |a(K)exp (1966As02); -0.34 {I+32-15} from |g(|q) (1959De29); 1956Go47. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M2
decay_comment:
RI$from intensity balance at 1085 level (2019Kr06) 
E$from the Adopted Gammas of {+179}Hf in the ENSDF database (2009 update) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from {+180}Hf IT decay (5.53 h) 
M$from ce data in {+180}Hf IT decay (5.53 h) and {+179}Hf(n,|g), E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
CC$experimental value from {+180}Hf IT decay (5.53 h) (1986BeZE). 
E,RI$from {+180}Hf IT decay (5.53 h) 
M$K forbidden E1 transition. Multipolarity from ce data in {+180}Hf IT decay (5.53 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2+E3
decay_BE_unit: e^2 x (fm)^6
decay_BE_info: ;TYPE=BE3;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE3W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
E,RI$from {+180}Hf IT decay (5.53 h) 
M$from ce data in {+180}Hf IT decay (5.53 h) 
MR$from |g|g(|q) in {+180}Hf IT decay (5.53 h) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$weighted average of 98 {I4} in {+180}Lu |b{+-} decay and 90 {I4} in {+179}Hf(n,|g), E=thermal. 
M,MR$from Coulomb excitation (1974Va09). 
MR$Others: -0.45 {I25} or <-10 (1983Gr30) and 2.2 {I13} (1991Gr19); both from |g(|q) in {+180}Hf(n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$others: -0.4 {I1} or >25 (1983Gr30) and +0.09 {I3} or -15 {I+10-5} (1991Gr19) both from |g(|q) in {+180}Hf(n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$an unplaced M1 130.26|g observed in {+179}Hf(n,|g), E=thermal could correspond to this placement. 


decay_energy_unit: KEV
decay_multipolarity: (D+Q)
decay_comment:
M$stretched Q or unstretched D+Q from R(DCO) in {+180}Hf({+136}Xe,{+136}Xe'|g). (D+Q) from assumed band assignment. 


decay_energy_unit: KEV
decay_comment:
M,MR$M1+E2 with |d=1.2 {I+16-6} from ce data in {+180}Hf(n,n'|g) is inconsistent with |DJ=2 from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=1.05 {I5}, |a(L1+L2)exp=1.26 {I7}, |a(L3)exp=1.20 {I7}, |a(M)exp=0.62 {I6}, |a(N+O)exp=0.184 {I16} (1986RoZM). 
$ce(L):ce(M):ce(N) exp=<2300:<730:<100 (1967Pr08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.113 {I9}, |a(L1+L2)exp=0.0481 {I9}, |a(L3)exp=0.0246 {I9}, |a(M)exp=0.0171 {I12}, |a(N+O)exp=0.0039 {I4} (1986RoZM) 
$ce(K):ce(L2):ce(L3):ce(M):ce(N)exp=<650:170:60:60:15 (1967Pr08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.042 {I3}, |a(L)exp=0.0131 {I14}, |a(M)exp=0.0051 {I6} (1986RoZM). 
$ce(K)/ce(L2) exp=3.0 (1967Pr08). 


decay_energy_unit: KEV
decay_comment:
RI$I|g=82 % {I2}, relative intensity de-exciting the 5.5-h {+180}Hf isomer measured following reactor shut down (1974Bu22). 


decay_energy_unit: KEV
decay_comment:
RI$I|g=18% {I2}, relative intensity de-exciting the 5.5-h {+180}Hf isomer, measured following reactor shut down (1974Bu22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(L1)exp=0.33 {I4}, |a(M)exp=0.21 {I2} (1986RoZM). 
$ce(K):ce(L1):ce(L2):ce(L3):ce(M) exp=|<30:20:20:|<20:20 (1967Pr08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$peak exhibits triplet structure 
E$unplaced by 1974Bu22. Placement by evaluator on basis of (n,n'|g) data. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.032 {I5} (1986RoZM). 
RI$may include weak {+178}Hf line. 
E$1990Bo52 place a 408.5|g from a level at 2017.8 keV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp=0.271 {I24}, |a(L)exp=0.039 {I4}, |a(M)exp=0.0092 {I4} (1986RoZM). 
$ce(K):ce(L2):ce(M) exp=100:20:7 (1967Pr08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$|a(L)exp=0.068 {I9} (1986RoZM). |a(L1+L2)exp=0.48 {I4} must be a misprint in 1986RoZM and could correspond to |a(K)exp. 
$ce(K)/ce(L12) exp=5.4 (1967Pr08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$placement from 1991Gr19. 1983Gr30 place the |g as a single depopulating transition from a 2+ level at 1260.7 keV. 1991Gr19 argue that such a decay pattern would be unusual for a low-lying state in a deformed nucleus. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2)
decay_comment:
$|a(exp)=9 {I6} from intensity balance (1999Da09). 
M$M2 or E3 from |a(exp). M2 proposed by 1999Da09 assuming lowest multipole dominates. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
MR$from |g(|q) in 1974Va09. Other: 0.7 {I2} is not favored when considering systematics of similar transitions in this region. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 93.33 {I2} (1961Ed01), 93.332 {I6} (1970Re08), 93.263 {I15} (1971Gu02), and 93.328 {I15} (1972GeZG). 
RI$weighted average of 17.6 {I4} (1961Ed01), 18.0 {I5} (1970Re08), 19.5 {I17} (1971Gu02), and 15.5 {I8} (1972GeZG). 
$|a(exp)=4.77 {I6} (1986BeZE), 4.91 {I23} (1967Ne07), 5.14 {I24} (1961Ed01). ce(K)/ce(L1)+ce(L2)/ce(L3)/ce(M)+ce(N)+ce(O) exp: 205 {I12}/343 {I17}/239 {I13}/169 {I12} s (1961Ed01). Others: 1967Sc19, 1968Gv01, 1968El02, 1970Gv01, 1972Dr02. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 215.25 {I13} (1961Ed01), 215.251 {I13} (1970Re08), 215.241 {I15} (1971Gu02), and 215.243 {I15} (1972GeZG). 
RI$weighted average of 88.2 {I25} (1961Ed01), 86.5 {I20} (1970Re08), 85.9 {I25} (1971Gu02), and 86.2 {I25} (1972GeZG). 
$|a(K)exp=0.123 {I9} (1961Ed01); ce(L1)/ce(L3) exp: 0.73 {I5}, ce(L2)/ce(L3) exp: 1.52 {I10} (1968Gv01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 332.5 {I3} (1961Ed01), 332.307 {I36} (1970Re08), 332.272 {I15} (1971Gu02), and 332.269 {I18} (1972GeZG). 
RI$weighted average of 100 {I4} (1961Ed01), 100.0 {I25} (1970Re08), 100 {I4} (1971Gu02), and 100.0 {I25} (1972GeZG). 
$|a(K)exp=0.038 {I3} (1961Ed01). ce(L1)/ce(L3) exp: 1.8 {I1}, ce(L2)/ce(L3) exp: 1.6 {I1} (1968Gv01,1975Gr18). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 443.8 {I6} (1961Ed01), 443.181 {I55} (1970Re08), 443.168 {I15} (1971Gu02), and 443.149 {I20} (1972GeZG). 
RI$weighted average of 86.6 {I46} (1961Ed01), 90.4 {I30} (1970Re08), 84.8 {I25} (1971Gu02), and 86.4 {I25} (1972GeZG). 
$|a(K)exp=0.0189 {I17} (1961Ed01). ce(L1)/ce(L3) exp: 3.0, ce(L2)/ce(L3) exp: 1.9 s (1968Gv01,1975Gr18). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$weighted average of 57.54 {I1} (1961Ed01), 57.549 {I5} (1970Re08), 57.442 {I15} (1971Gu02), and 57.44 {I5} (1972GeZG). 
RI$weighted average of 51.3 {I12} (1961Ed01), 51.3 {I20} (1970Re08), and 47.5 {I34} (1971Gu02). 
$|a=0.75 {I3} from intensity balance at 1084 level. 
CC$experimental value (1986BeZE). 
M$K-forbidden E1 transition. Multipolarity from ce(L1)/ce(L2) exp=4.02 {I18}, ce(L1)/ce(L3) exp=4.49 {I9}, ce(L2)/ce(L3) exp=1.16 {I3}, ce(M1)/ce(M2) exp=3.79 {I15}, ce(M2)/ce(M3) exp=1.28 {I6}, ce(N1)/ce(N2) exp=4.1 {I5}, ce(N1)/ce(N3) exp=6.7 {I13}, ce(N2)/ce(N3) exp=1.6 {I4}, weighted averages from 1967Gi11, 1967Sc19, 1970Gv01, 1972Dr02, and 1981Fr05. Penetration parameters are |l(1)=7.0 {I7} and |l(2)=0, from ce(L1)/ce(L3) exp: 4.49 {I20}, ce(L2)/ce(L3) exp: 1.16 {I5}, and |a(L3)exp=0.061 {I4} (1981Fr05). |d(M2/E1)=-0.009 {I+65-85}, |d(E3/E1)=0.013 {I20} (1972Kr06), |g(|q,H,t). Other: 1961Ed01. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2+E3
decay_comment:
E$weighted average of 500.714 {I66} (1970Re08), 500.702 {I15} (1971Gu02), and 500.680 {I25} (1972GeZG). 
RI$weighted average of 13.6 {I12} (1970Re08), 15.7 {I14} (1971Gu02), 15.1 {I8} (1972GeZG), and 15.2 {I4} (1971Ja21). Value from 1971Ja21 is deduced by the evaluator using their measured ratio I|g(443|g)/I|g(501|g)=5.70 {I15} and I|g(443|g)=86.8 {I25}. 
$|a(K)exp=0.0383 {I12}, |a(L)exp=0.0168 {I11} (1967Gi11). ce(L1)/ce(L3) exp: 3.0 {I3}, ce(L2)/ce(L3) exp: 3.0 {I3} (1968Gv01). Others: 1961Ed01, 1967Sc19, 1990Mi25. 
MR$-5.3 {I4} from |g|g(|q) in 1961Bo25 and -5.3 {I3} from |g anisotropy in 1971Kr18. Also 1962Ko15. Penetration parameter |l=-40 {I8} from ce(K)/ce(L1)/ce(L2)/ce(L3) exp: 0.043 {I3}/0.0072 {I5}/0.0072 {I5}/0.0023 {I2} consistent with |d=5.4 (1977Se10). Penetration parameter |l=-44 {I6} from |a(K)exp=0.0463 {I12}, ce(K)/ce(L) exp=2.65 {I10}, ce(L1)/ce(L2) exp=1.00 {I4}, ce(L1)/ce(L3) exp=3.0 {I2}, and |d=-5.5 {I2} (1990Mi25,1990MiZP). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
M$M1 from {+180}Hf({+238}U,{+237}U|g) 2001Sh36, in disagreement with the 13/2+ to (13/2-) transition. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
M$E2 from {+180}Hf({+238}U,{+237}U|g) 2001Sh36, in disagreement with the (15/2+) to (13/2-) transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=2321.9 {I4}; I|g=0.05 {I2} (doublet in |g-transition table from single spectrum of 2002Bo41). Most likely corresponds to 2320.7+2323.4 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=2368.5 {I5}; I|g=0.06 {I3} (doublet in |g-transition table from single spectrum of 2002Bo41). Most likely corresponds to 2366.3+2370.7 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from |g-transition table from single spectrum of 2002Bo41; not listed in the table of decay of high lying levels 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
Other E|g: 107.3 {I3} (1989Ry04). 
RI The authors' value of I|g=120 {I30} includes the contribution from {+184}Hf isomer also present in the source. 
Coincident with Hf(K| x ray) and E|b|>450 keV (1989Ry04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
RI from I(|g+ce)=2.29 {I20} and authors' assumed |a of 2.724 (1995Kr04), I|g=0.62 {I5}; however, this includes contribution from {+184}Lu |b decay, so evaluator deduces I|g(IT decay) assuming I(|g+ce)(107|g)=I(|g+ce)(243|g)=I(|g+ce)(368|g). Then I|g(from |b{+-} decay)=0.35 {I6}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
RI from I(|g+ce)=1.18 {I7} and authors' assumed |a of 0.155 (1995Kr04), I|g=1.02 {I6}; however, this includes contribution from {+184}Lu |b decay, so evaluator deduces I|g(IT decay) assuming I(|g+ce)(243|g)=I(|g+ce)(368|g). Then I|g(from |b{+-} decay)=0.15 {I9}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
E reported only by 1995Kr04. 
RI from I(|g+ce)=0.5 {I1} and authors' assumed |a of 0.820 (1995Kr04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_comment:
E reported only by 1995Kr04. 
RI from I(|g+ce)=0.4 {I1} and authors' assumed |a of 0.108 (1995Kr04). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$E2 multipolarity favoured for this transition, based upon single-particle Weiskopff estimates. Assignment further supported by intensity balance arguments 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$R{-ang}=0.85 {I13} 
M$E2 multipolarity favoured for this transition, based upon single-particle Weiskopff estimates. Assignment further supported by intensity balance arguments 


decay_energy_unit: KEV
decay_multipolarity: (M1)
decay_comment:
E,M$from {+158}Ta IT decay (2016Ca15). The 66|g was seen in coincidence with 6037|a (2016Ca15, Fig. 2c). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
M$E1 or M1 restricted by |a-|g prompt coinc (higher mult would imply too long T{-1/2}'s); M1 from intensity balance 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E value from the level scheme of 2011La01, but not listed in their table of measured |g properties (their Table 1). 


decay_energy_unit: KEV
decay_comment:
E from the level scheme drawing of 2011La01. In their table of measured |g properties (their Table 1), they list only one 793.5 |g, which they place from the 3261.2+x, (31/2-), level. 


decay_energy_unit: KEV
decay_comment:
E$average of 111.8 in {+168}Re |a decay and 111.2 in {+164}W |e decay 
$ A 99.9|g may also deexcite 111 level with I|g about 18% of that for 111|g (see {+164}W |e decay) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Coin with 372|g and 402|g and not with 111|g 
M$E1 from |a(exp)=0.39 {I44}, estimated from |g and |g(K| x ray) coin spectra 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$ stretched E2 expected from systematics. DCO and POL values are in disagreement 
$ POL=-0.03 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
CC(E1)=0.576, CC(M1)=7.21, CC(E2)=118. 
M if placement of 46|g is correct, E2 is ruled out because it would imply negative |e+|b{++} feeding of the 350 level; M1 would imply no |e+|b{++} branch to 350 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
CC(E1)=0.390, CC(M1)=4.66, CC(E2)=4.07. 
E 97.7 from fig. 3 of 1989Hi04, consistent with E(level) difference. E|g=97.1 from table 4 appears to be a misprint. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$presumed to be the same as the E|g=159.7 {I4} transition reported in |e decay. 
M$|D|p from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(total) from simultaneous observation of 110|g in singles and the number of 94 keV |g rays in coincidence with 110|g (1989Me02) 


decay_energy_unit: KEV
decay_comment:
RI$not determined; contaminant present. I|g<17 expected based on intensity balance at the 392 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E|g=121.2 {I10} in {+142}Nd({+30}Si,p3n|g), but order of 121|g and 104|g is reversed in that study. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
Other E|g: 284.8 {I10} from ({+30}Si,p3n|g); member of poorly resolved multiplet there. Possibly a 268|g placed in a separate band in that study is also a multiplet. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E from figs. 6 and 7 of 1992Th02, but not listed in table 2. Existence unconfirmed in a later {+145}Nd({+27}Al,4n|g) study; |g not adopted. 
RI I(225|g)/I(121|g)=0.30 {I15} (1992Th02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=AP;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=AP
decay_comment:
CC(E1)=0.0930; BE1W=1.4E-6 4. 
M D (|DJ=0) or Q (|DJ=2) to (1/2+) 11 level from ({+51}V,6n|g); not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI from ({+19}F,5n|g). I(225|g):I(458|g)=64 {I4}:100 {I3} in ({+51}V,6n|g). 
M from |g(|q) for intraband |g in ({+19}F,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
Other I|g: I(274|g):I(534|g)=48 {I3}:100 {I5} in ({+19}F,5n|g). 
M from |g(|q) for intraband |g in ({+19}F,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
Other I|g: I(210|g):I(439|g)=110 {I10}:100 {I4} in ({+19}F,5n|g). 
M (D) from |g(|q) for intraband |g in ({+19}F,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
Other I|g: I(243|g):I(452|g)=115 {I7}:100 {I14} in ({+19}F,5n|g). 
M D from |g(|q) for intraband |g in ({+19}F,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
Other E|g: 437.7 in ({+19}F,5n|g). 
Other I|g: I(437|g):I(230|g)=130 {I8}:100 {I12} in ({+19}F,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI from ({+19}F,5n|g). 65 {I10} in ({+51}V,6n|g). 
M (Q) from |g(|q) for intraband |g in ({+19}F,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Other E|g: 405.2 in ({+19}F,5n|g). 
Other I|g: I(404|g):I(765|g)=222 {I24}:100 {I42} in ({+19}F,5n|g). 


decay_energy_unit: KEV
decay_multipolarity: [E2]
decay_uncertain: S
decay_comment:
E from level energy difference; transition not observed. 
TI lower limit required to avoid negative |e feeding to 11 level 


decay_energy_unit: KEV
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
E from level energy difference; transition not observed. 
TI lower limit required to avoid negative |e feeding to 27 level 


decay_energy_unit: KEV
decay_multipolarity: [E1]
decay_uncertain: S
decay_comment:
E from level energy difference; transition not observed. 
TI at least 33 {I12} and no more than 267 {I30} to avoid negative |e feeding to 192 and 180 levels, respectively. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
Placed by evaluator, consistent with Adopted Levels, Gammas and with reported coincidences with 170|g, 153|g and possibly 165|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
RI 100 for doubly-placed |g; intensity divided based on adopted branching from 180.1 level. 
Coincident with 109|g, 153|g, 165|g, 170|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
R{-|g|g(|q)}=0.88 {I6}; too high for |DJ=1, |D|p=yes transition implied by placement in level scheme. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
M A{-2}=+0.04 {I13}; A{-4}=-0.08 {I22}. 
E |g omitted from Adopted Gammas. It is reported by 1993Li15 only and evaluator considers it likely that |g does not belong to {+169}Ta. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
M A{-2}=+0.33 {I10}; A{-4}=+0.20 {I9}. Level scheme implies E2, but A{-4} is not consistent with a Q transition. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M A{-2}=+0.48 {I10}; A{-4}=-0.10 {I13} for doublet to which this transition contributes 67% of the total intensity. A{-2}'=+0.27 {I6}. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E from figs. 1 (gated spectra) and 2 (level scheme) of 1993Li15; E|g=543.3 in table 1 (measured transition properties) is presumed to be a typographical error. 
M A{-2}=+0.23 {I5}; A{-4}=-0.05 {I7} for multiplet. A{-2}'=+0.28 {I7} for doublet. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
Order of 513|g and 524|g taken from 2003So08; 1993Li15 give the reverse order for these transitions. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
M A{-2}=+0.15 {I15}; A{-4}=-0.13 {I26} for doublet to which this |g contributes 67% of total I|g. A{-2}'=+0.17 {I8}. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
Unconfirmed in ({+51}V,6n|g) study by 2006Ha46; not included in Adopted Gammas. 
M A{-2}=+0.08 {I6}; A{-4}=-0.17 {I8} for doublet. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
Unconfirmed in ({+51}V,6n|g) study by 2006Ha46; not included in Adopted Gammas. 
M A{-2}=+0.08 {I6} for doublet. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E placed from J=65/2 band member in Adopted Levels, Gammas (a 1030|g deexcites the 73/2- 1/2[541] band member there). 


decay_energy_unit: KEV
decay_comment:
M apparent D character from |g(|q) ratio in {+124}Sn({+51}V,5n|g) is inconsistent with |DJ=2 placement and has not been adopted. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M apparent D character from |g(|q) ratio in {+124}Sn({+51}V,5n|g) is inconsistent with placement and has not been adopted. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g=647.0 {I3} in 1999Zh27 is replaced by a 637|g in 2001DeZX. The former is consistent with E|g from the ({+51}V,5n|g) study (647.7 {I2}) but not with the placement of the 319 |g-rays, so the 319|g placement is indicated as doubtful here and is not adopted. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I(619|g)/I(294|g)=1.45 in coin spectrum (1999Zh27). 
I|g=8.85 in table 1 appears to be a typographical error; possibly I|g=8.5. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$other: 253.1 {I3} from ({+16}O,4n|g). 
RI$other: 27 from ({+16}O,4n|g). 
M$intraband Q |g from ({+16}O,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$other: 301.0 {I3} from ({+16}O,4n|g). 
RI$other: 35 from ({+16}O,4n|g). 
M$intraband Q |g from ({+16}O,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$other: 173.8 {I3} from ({+16}O,4n|g). 
RI$other: 49 from ({+16}O,4n|g). 
M$intraband D+Q |g from ({+16}O,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$other: 291.7 {I3} from ({+16}O,4n|g). 
RI$other: 36 from ({+16}O,4n|g). 
M$intraband Q |g from ({+16}O,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$other: 200.6 {I3} from ({+16}O,4n|g). 
RI$other: 62 from ({+16}O,4n|g). 
M,MR$intraband D+Q |g from ({+16}O,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$other: 229.0 {I3} from ({+16}O,4n|g). 
RI$other: 85 from ({+16}O,4n|g). 
M,MR$intraband D+Q |g from ({+16}O,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$other: 238.5 {I3} from ({+16}O,4n|g). 
RI$other: 70 from ({+16}O,4n|g). 
M,MR$intraband D+Q |g from ({+16}O,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$other: 240.9 {I3} from ({+16}O,4n|g). 
RI$other: 35 from ({+16}O,4n|g). 
M$intraband D+Q |g from ({+16}O,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$other: 246.1 {I3} from ({+16}O,4n|g). 
RI$other: 156 from ({+16}O,4n|g). 
M,MR$intraband D+Q |g from ({+16}O,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$other: 252.0 {I3} from ({+16}O,4n|g). 
RI$other: 71 from ({+16}O,4n|g). 
M$intraband D |g from ({+51}V,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$other: 271.6 {I3} from ({+16}O,4n|g). 
RI$other: 32 from ({+16}O,4n|g). 
M$intraband D |g from ({+51}V,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$other: 237.2 {I3} from ({+16}O,4n|g). 
RI$other: 24 from ({+16}O,4n|g). 
M$intraband D+Q |g from ({+51}V,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
$I|g(52.1|g), as observed within the |?1 |ms coincidence time resolution, is only 15% as intense as expected from intensity balance considerations (1990Me12). This suggests either that T{-1/2}(52.1 level)> 1 |ms for this possible |DK=3 deexcitation or that there are alternative unobserved decay modes for the level, such as proceeding via the 31.2-keV (5/2-) level known from (HI,xn|g) studies. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
I|g/298.1|g=0.330 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.65 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.0 {I6} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.688 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.76 {I3} (2005Ha71). I|g(30|')/I|g(90|')=0.70 {I2} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.300 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.86 {I4} (2005Ha71); low for |DJ=2 transition. I|g(30|')/I|g(90|')=0.75 {I6} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.065 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.60 {I7} (2005Ha71); very low for |DJ=2 transition required by level scheme. I|g(30|')/I|g(90|')=0.83 {I6} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.345 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.75 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.03 {I7} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.154 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.74 {I4} (2005Ha71). I|g(30|')/I|g(90|')=0.92 {I8} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.373 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.84 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.08 {I6} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.623 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.77 {I2} for unresolved doublet (2005Ha71). I|g(30|')/I|g(90|')=0.64 {I2} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.077 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.88 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.11 {I10} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
I|g/298.1|g=0.366 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.63 {I5} (2005Ha71). I|g(30|')/I|g(90|')=0.40 {I2} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.188 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.71 {I5} (2005Ha71); very low for |DJ=2 transition required by level scheme. I|g(30|')/I|g(90|')=0.95 {I6} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.455 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.88 {I5} (2005Ha71). I|g(30|')/I|g(90|')=1.07 {I9} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
I|g/298.1|g=0.410 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.73 {I3} (2005Ha71). I|g(30|')/I|g(90|')=0.64 {I2} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.909 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.92 {I2} (2005Ha71). I|g(30|')/I|g(90|') normalized to 1.00. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
I|g/298.1|g=0.226 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.65 {I4} (2005Ha71). I|g(30|')/I|g(90|')=0.64 {I7} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.265 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.89 {I5} (2005Ha71). I|g(30|')/I|g(90|')=1.38 {I20} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
I|g/298.1|g=0.363 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.90 {I4} (2005Ha71). I|g(30|')/I|g(90|')=0.95 {I5} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.261 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.95 {I3} (2005Ha71). I|g(30|')/I|g(90|')=1.19 {I7} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.275 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.88 {I6} (2005Ha71). I|g(30|')/I|g(90|')=0.98 {I21} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.580 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.95 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.02 {I4} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.418 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.91 {I4} (2005Ha71). I|g(30|')/I|g(90|')=0.96 {I19} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.800 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.99 {I2} (2005Ha71). I|g(30|')/I|g(90|')=1.03 {I6} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.310 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.85 {I5} (2005Ha71). I|g(30|')/I|g(90|')=1.2 {I3} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.413 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.97 {I4} (2005Ha71). I|g(30|')/I|g(90|')=0.92 {I5} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.356 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.74 {I4}. I|g(30|')/I|g(90|')=0.71 {I6} (1985Ba48). 
I|g/298.1|g=0.328 (1985Ba48 at E=230 MeV). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.398 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.06 {I7} (2005Ha71). I|g(30|')/I|g(90|')=1.04 {I4} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.382 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.96 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.27 {I8} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.727 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.69 {I3} for 264.8|g+265.4|g+265.5|g (2005Ha71). I|g(30|')/I|g(90|')=0.76 {I4} for 264.6|g+265.8|g (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.429 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.86 {I6} (2005Ha71). I|g(30|')/I|g(90|')=0.50 {I2} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.461 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.91 {I4} (2005Ha71). I|g(30|')/I|g(90|')=0.96 {I5} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.727 (1985Ba48 at E=230 MeV) for doublet. 
M R{-ang}=0.69 {I3} for 264.8|g+265.4|g+265.5|g (2005Ha71). I|g(30|')/I|g(90|')=0.76 {I4} for 264.6|g+265.8|g (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.390 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.02 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.15 {I5} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
I|g/298.1|g=0.275 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.72 {I7} (2005Ha71). I|g(30|')/I|g(90|')=0.58 {I4} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.281 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.11 {I7} (2005Ha71). I|g(30|')/I|g(90|')=0.98 {I9} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.222 (1985Ba48 at E=230 MeV) for 237.2|g+238.5|g doublet. 
M R{-ang}=0.76 {I9} (2005Ha71). I|g(30|')/I|g(90|')=0.68 {I2} for 237.2|g+238.5|g (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.480 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.88 {I3} (2005Ha71). I|g(30|')/I|g(90|')=0.89 {I6} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.288 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.01 {I2} (2005Ha71). I|g(30|')/I|g(90|')=1.05 {I4} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.234 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.72 {I7} (2005Ha71). I|g(30|')/I|g(90|')=0.63 {I3} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.229 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.00 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.06 {I6} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
I|g/298.1|g=0.102 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.88 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.20 {I7} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
I|g/298.1|g=0.277 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.76 {I5} (2005Ha71). I|g(30|')/I|g(90|')=0.76 {I10} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.213 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.01 {I2} (2005Ha71). I|g(30|')/I|g(90|')=1.00 {I5} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.126 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.05 {I4} for 538.5|g+538.9|g (2005Ha71). I|g(30|')/I|g(90|')=0.89 {I10} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.342 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.05 {I3} (2005Ha71). I|g(30|')/I|g(90|')=1.04 {I10} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g/298.1|g=0.154 (1985Ba48 at E=230 MeV); for doublet. 
M I|g(30|')/I|g(90|')=0.53 {I9} for 627.2|g+628.8|g (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.561 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.02 {I3} (2005Ha71). I|g(30|')/I|g(90|')=1.47 {I10} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.230 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.04 {I3} (2005Ha71). I|g(30|')/I|g(90|')=0.94 {I6} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.118 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.01 {I7} (2005Ha71). I|g(30|')/I|g(90|')=1.40 {I15}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.405 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.02 {I3} (2005Ha71). I|g(30|')/I|g(90|')=1.06 {I7} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.184 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.08 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.3 {I4} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.337 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.07 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.20 {I10} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.161 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.11 {I5} (2005Ha71). I|g(30|')/I|g(90|')=0.90 {I12} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.256 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.08 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.08 {I7} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.138 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.18 {I7} (2005Ha71). I|g(30|')/I|g(90|')=0.82 {I13} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.152 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.18 {I4} (2005Ha71). I|g(30|')/I|g(90|')=0.92 {I7} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.147 (1985Ba48 at E=230 MeV). 
M R{-ang}=0.95 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.22 {I24} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/298.1|g=0.117 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.08 {I4} (2005Ha71). I|g(30|')/I|g(90|')=1.00 {I20} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
I|g/398|g=0.097 {I9}.7 (1985Ba48 at E=230 MeV). 
M R{-ang}=1.08 {I5} (2005Ha71). I|g(30|')/I|g(90|')=1.0 {I6} (1985Ba48). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI given as 41.2 and 41.6 in table 2 of 1985Ba48. 
M A{-2}=+0.36 {I5}, A{-4}=+0.05 {I6} for doublet; consistent with |d(D,Q)=0.50 {I10}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$35 {I3} for E|g=39.6 {I3} (1974CaZR) 
M$|a(L)exp=2.2 {I2}, |a(M)exp=0.09 {I5} (1974CaZR) suggest E1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$16 {I2} for E|g=90.1 {I8} (1974CaZR) 
M$|a(K)exp=9.9 {I13}, |a(L)exp=6.9 {I11} (1974CaZR). K/L ratio suggests M1+E2 (|d=1.0 {I2}), but |a(K)exp and |a(L)exp are larger than |a(K)(M1,E2) and |a(L)(M1,E2). For E1+M2, |a(K)exp and |a(L)exp give |d=0.60 {I5} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=0.92 {I16} 
I|g(159.6|g):I|g(293.0|g)=1.00:0.75. Branching ratio=1.00:0.35(7) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=1.12 {I21} 
I|g(194.5|g):I|g(372.4|g)=1.00:2.31. Branching ratio=1.00:2.90(32) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=0.93 {I12} 
I|g(216.8|g):I|g(410.5|g)=1.00:0.37. Branching ratio=1.00:0.54(8) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=0.91 {I14} 
I|g(216.1|g):I|g(411.1|g)=1.0:7.2. Branching ratio=1.0:3.5(3) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=0.89 {I17} 
I|g(242.3|g):I|g(468.4|g)=1.0:5.1. Branching ratio=1.0:3.1(3) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=1.06 {I15} 
I|g(260.0|g):I|g(505.0|g)=1.0:5.0. Branching ratio=1.0:2.0(3) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=0.99 {I19} 
I|g(248.5|g):I|g(490.8|g)=1.0:4.7. Branching ratio=1.0:2.4(3) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=0.98 {I13} 
I|g(271.6|g):I|g(528.6|g)=1.00:5.83. Branching ratio=1.00:1.60(24) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=0.98 {I11} 
I|g(260.5|g):I|g(509.0|g)=1.00:8.50. Branching ratio=1.00:2.20(25) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=1.25 {I14} 
I|g(288.1|g):I|g(560.0|g)=1.00:4.00. Branching ratio=1.00:2.41(6) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=1.04 {I15} 
I|g(266.1|g):I|g(526.6|g)=1.00:10.00. Branching ratio=1.00:3.20(24) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=0.96 {I14} 
I|g(297.3|g):I|g(586.0|g)=1.0:5.0. Branching ratio=1.0:2.0(4) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$DCO=1.19 {I14} 
I|g(277.7|g):I|g(543.8|g)=1.0:14.0. Branching ratio=1.0:3.1(3) for the same |g's deduced from measured |l data in 1996We07. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Total Ice=370 
RI I|g=430 and I(|g+ce)=800 deduced by authors are incorrect for an assumed E2 multipolarity. 
M$from ce(L2):ce(L3):ce(M2):ce(M3) exp=118:160:33:41. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from |a(K)exp=0.009 {I1}. B(E2)(W.u.)=3.1|*10{+-5} is consistent with E2 |DK=2 forbidden transition (1978Bu16). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M From |a=0.11 {I12} based on the intensity balance at 1666+W keV level and assuming M1 multipolarity for the 328.2 keV transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$|a(K)exp=8.1 {I4}, |a(L)exp=3.8 {I6} and |a(M)exp=0.94 {I21}; (ce(L1):ce(L2):ce(L3))exp=1.00:1.29:1.17 (1972Ad12); (ce(L1):ce(L2):ce(L3))exp=84.7 {I9}: 107.2 {I10}:100 and (ce(M1):ce(M2):ce(M3))exp=74.5 {I21}:106.2 {I29}: 100 (1988La19); A{-2}=-0.05 {I20} (1970Sk04). 
MR$From 1988La19; penetration parameter |l=0.6 {I3}. Others: 0.56 {I3} using the briccmixing program and conversion electron data in 1972Ad12; -0.10 {I4} or -4.2 {I8} from |g|g(|q) and 0.0 {I2} or 2.4 {I10} from PPDAC analysis in 1976Ao02; -0.096 {I37} from PPDAC analysis in 1974Ao01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$|a(K)exp=3.0 {I9} and |a(L1)exp=0.38 {I11} (1972Ad12); A{-2}=0.10 {I17} (2000Da09); A{-2}=-0.06 {I7} (1970Sk04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$(ce(K)/ce(L))exp=5.8 {I17}, (ce(L1):ce(L2):ce(L3))exp=1.00:0.27:0.29 (1972Ad12), |a(K)exp (115|g doublet)=0.29 {I9} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$ce(K)/ce(L)exp=6.2 {I10}, (ce(L1+L2)/ce(L3))exp=10 (1972Ad12); |a(K)exp (186|g doublet)=0.35 {I7} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$A{-2}=0.03 {I5} (1970Sk04). Other: |d=0.16 {I1} (2000Da09) and 0.26 {I4} (1995Ar18), assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M,MR$|a(K)exp=0.63 {I13}, |a(L)exp=0.17 {I6}, (ce(L1):ce(L2):ce(L3))exp=1.0:0.5:0.3 (1972Ad12); |a(K)exp=0.50 {I15} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
M,MR$|a(K)exp|?0.57, |a(L)exp|?0.093; (ce(L1)+ce(L2)):ce(L3)exp=1.1. (1972Ad12); |a(K)exp (186|g doublet)=0.35 {I7} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$A{-2}=0.11 {I5} (1970Sk04). Other: A{-2}=-0.01 {I5} (2000Da09), |d=0.26 {I2} (2000Da09) and 0.25 {I3} (1995Ar18), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$A{-2}=0.08 {I7} (1970Sk04). Other: |d=0.17 {I2} (2000Da09) and 0.17 {I2} (1995Ar18), assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$A{-2}=0.45 {I10} (1970Sk04). Other: |d=0.43 {I3} (2000Da09) and 0.49 {I3} (1995Ar18), assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$|a(K)exp=0.0235 was used for normalizing of the ce intensities in 1972Ad12. See 1972Ad12 for details. |a(L1)exp <0.002 (1972Ad12). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$|a(K)exp=0.071 {I8}, |a(L)exp=0.0110 {I13}, |a(M)exp=0.00183 {I8} (1972Ad12); |a(K)exp=0.071 {I10} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.03 {I7} and |a(K)exp=0.39 {I9} (2000Da09). Approximately 84% 195.3|g and 16% {I199}.9|g; A{-2}=0.14 {I7} (1970Sk04). 
MR$From A{-2}=0.14 {I7} (1970Sk04). Other: 0.21 {I2} (2000Da09) and 0.20 {I1} (1995Ar18), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$A{-2}=-0.02 {I14} (1970Sk04). Other: A{-2}=0.01 {I13} (2000Da09), |d=0.12 {I1} (2000Da09) and 0.16 {I1} (1995Ar18), assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=0.13 {I18}, but he value overlaps with that for the 204.7|g (2000Da09). 
MR$0.37 {I3} (2000Da09) and 0.43 {I3} (1995Ar18), assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.02 {I4}, |a(K)exp=0.48 {I7} and |a(L)exp=0.091 {I24} (2000Da09); A{-2}=0.15 {I8} (1970Sk04) 
MR$From |g(|q) in 1970Sk04. Other: 0.18 {I1} (2000Da09) and 0.21 {I1} (1995Ar18), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.08 {I39} (2000Da09) and A{-2}=-0.04 {I12} (1970Sk04) 
MR$0.12 {I1} (2000Da09) and 0.13 {I1} (1995Ar18), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-2}=0.17 {I9} (2000Da09), consistent with J to J transition. The value overlaps with that for the 678.6|g. |a(K)exp<0.006 (2000Da09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.42 {I24} (2000Da09). The value overlaps with that for the 226.2|g and 226.9|g. A{-2}=0.55 {I21} (1970Sk04). 
MR$From |g(|q) in 1970Sk04. Others: 0.37 {I3} (2000Da09), 0.39 {I3} (1995Ar18), 0.29 {I2} (1970Sk04) and 0.56 {I12} (1970Ba46) assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.20 {I4} and |a(K)exp=0.028 {I3} (2000Da09); A{-2}=0.38 {I10}, A{-4}=-0.08 {I14} (1970Sk04); A{-2}=0.303 {I12}, A{-4}=-0.068 {I20} (1982Ao02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$A{-2}=0.10 {I5} (1970Sk04). Other: A{-2}=-0.06 {I6} (2000Da09), |d=0.18 {I1} (2000Da09) and 0.20 {I1} (1995Ar18), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|a(K)exp=0.0074 {I8} and |a(L)exp=0.0016 {I3} (1972Ad12). Other: |a(K)exp=0.0048 {I6} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.02 {I7} (2000Da09) and A{-2}=-0.1 {I5} (1970Sk04). 
MR$0.17 {I1} (2000Da09) and 0.18 {I1} (1995Ar18), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$|a(K)exp=0.17 {I2} and |a(L)exp=0.030 {I9} (2000Da09). A{-2}=0.16 {I4}, A{-4}=-0.20 {I6} (1970Sk04); A{-2}=0.03 {I6}, A{-4}=0.08 {I8} (1975Ba13). A{-2}=0.048 {I7}, A{-4}=-0.006 {I11} (1982Ao02,1982Ao04). |a(exp)=0.37 {I18} (1970Sk04) and |a(exp)=0.32 {I15} (1971Hu14). |a(K)exp=0.169 {I28} and |a(L)exp=0.0203 {I41} (1982Ao04) 
MR$From |g(|q) in 1982Ao02 and 1982Ao04. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$|a(K)exp=0.0088 {I20} and |a(L)exp=0.0044 {I8} (1972Ad12). Other: |a(K)exp=0.013 {I4} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.3 {I4} (1970Sk04) and A{-2}=-0.07 {I5} (2000Da09). 
MR$0.16 {I1} (2000Da09) and 0.16 {I1} (1995Ar18), assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=+0.08 {I4} and |a(K)exp=0.25 {I6} (2000Da09). Others: A{-2}=0.52 {I13} (1970Sk04); A{-2}=0.15 {I10}, A{-4}=0.028 {I12} (1975Ba13). A{-2}=0.196 {I13}, A{-4}=0.037 {I19} (1982Ao04) 
MR$From 1982Ao04. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
M$A{-2}=-0.25 {I4} and |a(K)exp=0.016 {I6} (2000Da09); A{-2}=-0.22 {I10}, A{-4}=-0.03 {I10} (1975Ba13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.10 {I11} (2000Da09) 
MR$0.28 {I3} (2000Da09) and 0.34 {I2} (1995Ar18), using J=23/2, assuming K=17/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.22 {I17} (1975Ba13); A{-2}=0.27 {I5}, A{-4}=-0.08 {I6} (1982Ao04) 
MR$From |g(|q) in 1982Ao04. Other: |d=0.35 {I9} (2000Da09), assuming K=21/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.14 {I9} and |a(K)exp=0.41 {I8} (2000Da09); A{-2}=-0.07 {I19} (1975Ba13). 
MR$0.33 {I6} (2000Da09), assuming K=23/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.09 {I15} (2000Da09). The value overlaps with that for the 196.8|g. |a(K)exp=0.39 {I9} (2000Da09). Approximately 84% {I195}.3|g and 16% {I196}.9|g. 
MR$0.30 {I6} (2000Da09) and 0.38 {I1} (1995Ar18), using J=25/2, assuming K=17/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.14 {I7} and |a(K)exp=0.18 {I3} (2000Da09). Approximately 69% 232.5|g and 31% {I234}.1|g. Other: A{-2}=0.10 {I10} (1975Ba13). 
MR$0.33 {I5} (2000Da09), assuming K=23/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.42 {I24} (2000Da09). 
MR$0.27 {I4} (2000Da09) and 0.29 {I1} (1995Ar18), using J=27/2, assuming K=17/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.10 {I11} (2000Da09). The value overlaps with that for the 245.4|g and 245.6|g. 
MR$0.26 {I4} (2000Da09) and 0.34 {I1} (1995Ar18), using J=29/2, assuming K=17/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.10 {I11} (2000Da09). The value overlaps with that for the 245.4|g and 245.6|g. 
MR$1.0 {I4} (2000Da09), assuming K=25/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.20 {I12}, |a(exp)=0.45 {I4} and |a(K)exp=0.18 {I3} (2000Da09). Approximately 69% {I232}.5|g and 31% {I234}.1|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.22 {I5} (2000Da09). The value overlaps with that for the 363.4|g. |a(K)exp=0.08 {I2} (2000Da09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
M$Note that A{-2}=0.20 {I19} in 2000Da09, but this value is in disagreement with that expected for a pure E1 transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.05 {I21}, |a(K)exp=0.18 {I3} and |a(L)exp=0.031 {I8} (2000Da09) 
MR$0.24 {I4} (2000Da09), assuming K=35/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$A{-2}=0.16 {I6} (2000Da09). The value overlaps with that for the 461.9|g. |a(K)exp=0.051 {I7} and |a(L)exp=0.007 {I2} (2000Da09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
M$A{-2}=0.01 {I10} (2000Da09). The value overlaps with that for the 240.9|g. |a(exp)=0.043 {I4} and |a(K)exp=0.059 {I21} (2000Da09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$|a(K)exp=8.1 {i4}, |a(L)exp=3.8 {i6} and |a(M)exp=0.94 {i21}; (ce(L1):ce(L2):ce(L3))exp=1.00:1.29:1.17 (1972Ad12). (ce(L1):ce(L2):ce(L3))exp=84.7 {i9}: 107.2 {i10}:100 and (ce(M1):ce(M2):ce(M3))exp=74.5 {i21}:106.2 {i29}: 100 (1988La19). 
MR$From 1988La19; penetration parameter |l=0.6 {i3}. Others: 0.56 {i3} using the briccmixing program and conversion electron data in 1972Ad12; -0.10 {i4} or -4.2 {i8} from |g|g(|w) and 0.0 {i2} or 2.4 {i10} from ppdac analysis in 1976Ao02; -0.096 {i37} from ppdac analysis in 1974Ao01 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_uncertain: S
decay_comment:
E$From level energy differences. 
RI$From transition |g-ray intensity balance at the 172.2-keV level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_uncertain: S
decay_comment:
E$From level energy differences. Transition placed by the evaluator, based on the observed in 1972Ad12 73.15|g associated with the decay of the I|p=9/2-, |p9/2[514] bandhead at 73.15 keV. 
RI$From |g-ray intensity balance at the 73.15-keV level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$(ce(K)/ce(L))exp=5.8 {i17}, (ce(L1):ce(L2):ce(L3))exp=1.00:0.27:0.29 (1972Ad12). Other: |a(K)exp (115|g doublet)=0.29 {i9} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$Uncertainty assigned by the evaluator 
M$ce(K)/ce(L)exp=6.2 {i10}, (ce(L1+L2)/ce(L3))exp=10 (1972Ad12). Other: |a(K)exp (186|g doublet)=0.35 {i7} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI$From |g-ray intensity balance at 186.2 keV level, by assuming that there is no direct |e feeding to this level 
M$(ce(L)exp/ce(M+N+))exp=2.3 {i6},(ce(L2)/ce(L3))exp=0.77 (1972Ad12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$|a(K)exp=0.63 {i13}, |a(L)exp=0.17 {i6}, (ce(L1):ce(L2):ce(L3))exp=1.0:0.5:0.3 (1972Ad12). Others: |a(K)exp=0.50 {i15} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
M,MR$|a(K)exp|?0.57, |a(L)exp|?0.093; (ce(L1)+ce(L2)):ce(L3)exp=1.1. (1972Ad12). Other: |a(K)exp (186|g doublet)=0.35 {i7} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp=0.0235 was used for normalizing of the ce intensities. See 1972Ad12 for details. |a(L1)exp<0.002 (1972Ad12). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
E$From level energy differences. 
RI$From total |g-ray intensity balances at the 487-keV and 497-keV levels and the Alaga rule in |b decay to the 1/2+ and 3/2+ levels, where {Ift}(1/2- to 3/2+)/{Ift}(1/2- to 1/2+)=2.0. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|a(K)exp=0.071 {i8}, |a(L)exp=0.0110 {i13}, |a(M)exp=0.00183 {i8} (1972Ad12). Other: |a(K)exp=0.071 {i10} (1967Hu02). 


decay_energy_unit: KEV
decay_multipolarity: [E1]
decay_comment:
E,RI$The |g-ray was been observed. The energy determined from the conversion electron measurement (1972Ad12). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$|DE|g estimated by the evaluator. 0.1 keV reported in 1972Ad12, but the transition is 4|s from that calculated from the level differences 
M$|a(K)exp=0.0096 {i20} (1972Ad12). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|a(K)exp=0.0074 {i8} and |a(L)exp=0.0016 {i3} (1972Ad12). Other: |a(K)exp=0.0048 {i6} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$Assignment made by 1993Br06. 
M$|a(K)exp=0.0088 {i20} and |a(L)exp=0.0044 {i8} (1972Ad12). Other: |a(K)exp=0.013 {i4} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Assignment made by 1993Br06. 
M$|a(K)exp=0.0082 {i8} and |a(L)exp|?0.0014 (1972Ad12). Other: |a(K)exp=0.0079 {i24} (1967Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
E$Assignment made by 1993Br06. It was placed by 1972Ad12 and 1973Be66 to depopulate 1476.2 keV level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1
decay_comment:
E$Assignment made by 1993Br06. 
CC$|a(K)exp. 
M$|a(K)exp=0.13 {i6} and |a(L)exp=0.033 {i20} (1972Ad12). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=0.18 {I5}. The value overlaps with that for the 156.6|g. 
MR$0.45 {I8} (2000Da09) and 0.68 {I8} (1995Ar18), assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.03 {I7}. |a(K)exp=0.39 {I9} (2000Da09). Approximately 84% {I195}.3|g and 16% {I196}.9|g. 
MR$0.21 {I2} (2000Da09) and 0.20 {I1} (1995Ar18), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=0.13 {I18}. The value overlaps with that for the 204.7|g. 
MR$0.37 {I3} (2000Da09) and 0.43 {I3} (1995Ar18), assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.02 {I4}; |a(K)exp=0.48 {I7} and |a(L)exp=0.091 {I24} (2000Da09) 
MR$0.18 {I1} (2000Da09) and 0.21 {I1} (1995Ar18), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=0.42 {I24}. The value overlaps with that for the 226.2|g and 226.9|g. 
MR$0.37 {I3} (2000Da09) and 0.39 {I3} (1995Ar18), assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=0.10 {I11}. The value overlaps with that for the 245.6|g and 245.8|g. 
MR$0.34 {I3} (2000Da09) and 0.32 {I1} (1995Ar18), assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=0.01 {I10}. The value overlaps with that for the 240.8|g. 
MR$0.12 {I2} (2000Da09) and 0.13 {I1} (1995Ar18), assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=-0.02 {I7}. The value overlaps with that for the 258.8|g. 
MR$0.17 {I1} (2000Da09) and 0.18 {I1} (1995Ar18), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$|a(K)exp<0.002 (2000Da09), |a(K)(M1)=0.021, |a(K)(E2)=0.009 and |a(K)(E1)=0.003. 
E,RI$Others: E|g=718.8, I|g=13 {I1} is reported by 1995Ar18. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=-0.24 {I25}. |a(K)exp<0.002 (2000Da09), |a(K)(M1)=0.01, |a(K)(E2)=0.005 and |a(K)(E1)=0.002. 
E,RI$Others: E|g=937.0, I|g=20 {I2} is reported by 1995Ar18. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=-0.07 {I5}. The value overlaps with that for the 274.8|g. 
MR$0.16 {I1} (2000Da09) and 0.16 {I1} (1995Ar18), assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=-0.07 {I5}. The value overlaps with that for the 274.9|g. 
MR$0.11 {I2} (2000Da09) and 0.10 {I1} (1995Ar18), assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.10 {I11}. 
MR$0.28 {I3} (2000Da09) and 0.34 {I2} (1995Ar18), using J=23/2, assuming K=17/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=-0.09 {I15}. The value overlaps with that for the 196.8|g. |a(K)exp=0.39 {I9} (2000Da09). Approximately 84% {I195}.3|g and 16% {I196}.9|g. 
MR$0.30 {I6} (2000Da09) and 0.38 {I1} (1995Ar18), using J=25/2, assuming K=17/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=0.13 {I18}. The value overlaps with that for the 204.9|g. 
MR$1.1 {I5} (2000Da09), assuming K=19/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.14 {I7}. |a(K)exp=0.18 {I3} (2000Da09). Approximately 69% {I232}.5|g and 31% {I234}.1|g. 
MR$0.33 {I5} (2000Da09), assuming K=23/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=0.42 {I24}. The value overlaps with that for the 226.0|g and 226.2|g. 
MR$1.4 {I8} (2000Da09), assuming K=19/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=-0.02 {I7}. The value overlaps with that for the 258.7|g. 
MR$0.38 {I4} (2000Da09), assuming K=23/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=0.10 {I11}. The value overlaps with that for the 245.4|g and 245.6|g. 
MR$0.26 {I4} (2000Da09) and 0.34 {I1} (1995Ar18), using J=29/2, assuming K=17/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.10 {I11}. The value overlaps with that for the 245.4|g and 245.8|g. 
MR$1.0 {I4} (2000Da09), assuming K=25/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$A{-2}=0.32 {I16}. |a(K)exp=0.024 {I14} (2000Da09). The |a(K)exp value is in disagreement with the placement of the transition in the level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
RI$From the branching ratios given in 1995Ar18 and I|g=11 {I4} for the 630.8|g, |DJ=2 in-band transition from 2000Da09. 
MR$0.09 {I1} (1995Ar18), assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
RI$The intensity includes a possible contamination. Using the branching ratios from 1995Ar18, one may expect I|g|?23 for the 647.9|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.20 {I12}. |a(exp)=0.45 {I4}, |a(K)exp=0.18 {I3} (2000Da09). Approximately 69% {I232}.5|g and 31% {I234}.1|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
M$A{-2}=0.20 {I19}. This value is in disagreement with what would be expected for a pure E1 transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.05 {I21}. |a(K)exp=0.18 {I3} and |a(L)exp=0.031 {I8} (2000Da09) 
MR$0.24 {I4} (2000Da09), assuming K=35/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$A{-2}=0.16 {I6}. The value overlaps with that for the 461.9|g. |a(K)exp=0.051 {I7} and |a(L)exp=0.007 {I2} (2000Da09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$A{-2}=0.01 {I10}. The value overlaps with that for the 240.9|g. |a(exp)=0.043 {I4} and |a(K)exp=0.059 {I21} (2000Da09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.03 {I5} (1970Sk04). 
MR$Others: |d=0.18 {I1} (1970Sk04) and 0.12 {I2} (1970Ba46), assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.11 {I5} (1970Sk04). 
MR$Others: |d=0.18 {I2} (1970Sk04), 0.16 {I2} (1970Ba46) and 0.21 {I2} (1971Hu14), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.08 {I7} (1970Sk04). 
MR$Others: |d=0.15 {I1} (1970Sk04) and 0.16 {I2} (1970Ba46), assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.45 {I10} (1970Sk04). 
MR$Others: |d=0.45 {I10} (1970Sk04) and 0.54 {I8} (1970Ba46), assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.14 {I7} (1970Sk04). 
MR$Others: |d=0.17 {I2} (1970Sk04), 0.18 {I3} (1970Ba46) and 0.20 {I2} (1971Hu14), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.02 {I14} (1970Sk04). 
MR$Others: |d=0.21 {I2} (1970Sk04) and 0.19 {I1} (1970Ba46), assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.15 {I8} (1970Sk04). 
MR$Others: |d=0.16 {I2} (1970Sk04), 0.17 {I1} (1970Ba46) and 0.17 {I1} (1971Hu14), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.04 {I12} (1970Sk04). 
MR$|d=0.10 {I1} (1970Sk04) and 0.10 {I2} (1970Ba46), assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.55 {I21} (1970Sk04). 
MR$|d=0.29 {I2} (1970Sk04) and 0.56 {I12} (1970Ba46), assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$A{-2}=0.38 {I10}, A{-4}=-0.08 {I14} (1970Sk04); A{-2}=0.303 {I12}, A{-4}=-0.068 {I20} (1982Ao02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.10 {I5} (1970Sk04). 
MR$Others: |d=0.16 {I2} (1970Sk04), 0.16 {I1} (1970Ba46) and 0.17 {I1} (1971Hu14), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=-0.1 {I5} (1970Sk04). 
MR$Others: |d=0.17 {I1} (1970Sk04) and 0.18 {I3} (1970Ba46), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$Relative branching |g-ray intensity 
M$A{-2}=0.16 {I4}, A{-4}=-0.20 {I6} (1970Sk04); A{-2}=0.03 {I6}, A{-4}=0.08 {I8} (1975Ba13). A{-2}=0.048 {I7}, A{-4}=-0.006 {I11} (1982Ao02,1982Ao04). |a(exp)=0.37 {I18} (1970Sk04) and |a(exp)=0.32 {I15} (1971Hu14). |a(K)exp=0.169 {I28} and |a(L)exp=0.0203 {I41} (1982Ao04) 
MR$From |g(|q) in 1982Ao02 and 1982Ao04. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$Relative to I|g(311|g)=100. Weighted average of 15.2 {I40} (1971Hu14), 17.2 {I5} (1982Ao04), 11.4 {I25} (1970Ba46) and 10.3 {I34} (1975Ba13). Other: 10 {I1} (1973Sc20). 
M$A{-2}=0.190 {I41}, A{-4}=-0.071 {I49} (1982Ao02,1982Ao04). |a(K)exp=0.0127 {I16} (1982Ao04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$A{-2}=-0.3 {I4} (1970Sk04). 
MR$Others: |d=0.18 {I1} (1970Sk04) and 0.15 {I3} (1970Ba46), assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$A{-2}=0.52 {I13} (1970Sk04); A{-2}=0.15 {I10}, A{-4}=0.028 {I12} (1975Ba13). A{-2}=0.196 {I13}, A{-4}=0.037 {I19} (1982Ao04) 
MR$From 1982Ao04. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$From 1975Ba13. Not adopted, since it was not confirmed in {+170}Er({+11}B,4n|g) (2000Da09) or any other dataset. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$Contaminated with |g from Coulomb excitation of {+175}Lu 
M$A{-2}=-0.22 {I10}, A{-4}=-0.03 {I10} (1975Ba13). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
E$From 1975Ba13. 
M$A{-2}=0.22 {I17} (1975Ba13). A{-2}=0.27 {I5}, A{-4}=-0.08 {I6} (1982Ao04) 
MR$From 1982Ao04. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$Not adopted, since it was not confirmed in {+170}Er({+11}B,4n|g) (2000Da09) or any other dataset. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$out-of-beam intensity=324 {I5} 
A{-2}=+0.22 {I6} 
M$from |a(K)exp=0.029 {I1}, |a(L)exp=0.0076 {I5}, |a(M)exp=0.0020 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$out-of-beam intensity=577 {I11} 
A{-2}=+0.21 {I5} 
M$from |a(L)exp=0.073 {I9}, |a(M)exp=0.020 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$out-of-beam intensity=566 {I10} 
M$from |a(K)exp=0.149 {I11}, |a(L)exp=0.037 {I1}, |a(M)exp=0.013 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$out-of-beam intensity=435 {I13} 
A{-2}=+0.14 {I4} 
M$from |a(K)exp=0.0162 {I7}, |a(L)exp=0.0040 {I3}, |a(M)exp=0.0011 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$out-of-beam intensity=1000 {I27} 
M$from |a{-T}(exp)=0.21 {I6}, |a(L)exp=0.051 {I2}, |a(M)exp=0.019 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$out-of-beam intensity=22 {I2} 
A{-2}=+0.50 {I5} 
M$from |a(K)exp=0.084 {I5}, |a(L)exp=0.018 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$out-of-beam intensity=23 {I3} 
A{-2}=+0.38 {I8} 
M$from |a(K)exp=0.076 {I5}, |a(L)exp=0.011 {I1} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_uncertain: S
decay_comment:
The existence of this unobserved transition is established from coincidence relations in 1998Ko09. 
RI$ From I|g(431.1)|?4 and I|g(34)/I|g(431)|?0.013. 
M From |a{-T}>11 (1996Ko13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M from transition intensity balance at the 1242.9 level, deduced from the delayed spectrum. E1 multipolarity is also possible. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E from {+179}W |e decay (37.05 min). The mean of 6 determinations by 1963Va28 is 30.69 {I4}, but authors do not indicate systematic uncertainty. Other E|g: 30.7 {I3} in (d,2n|g), 30.5 {I5} in |e decay (37.05 min), 30.7 {I8} in ({+7}Li,4n|g) E=45 MeV. 
M anomalous E1 transition, from {+179}W |e decay (37.05 min). |a(E1 theory)=1.73 {I3}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M D+Q transition from |g(|q) in ({+7}Li,4n|g) E=38 MeV; M1,E2 from ce data in {+179}W |e decay (6.40 min) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other I|g: 33 {I10} in ({+7}Li,4n|g) E=38 MeV, 50 {I15} in (d,2n|g), 60 {I18} in (p,2n|g) relative to I(161|g)=100 {I30}. 


decay_energy_unit: KEV
decay_uncertain: S
decay_comment:
E from level energy difference; transition not observed. 
I(|g+ce)(7.3):I(|g+ce)(289)=63 {I31}:15 {I3} from {+179}W |e decay (6.40 min). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M D+Q from |g(|q) in ({+7}Li,4n|g) E=38 MeV; |D|p=yes from level scheme. 
Other I|g: 77 {I23} in ({+7}Li,4n|g) E=38 MeV, 41 {I12} in (d,2n|g), 61 {I18} in (p,2n|g) relative to I(101|g)=100 {I30}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
Other I|g: 100 {I30} in (d,2n|g) and (p,n|g); 112 {I34} in ({+7}Li,4n|g) E=38 MeV relative to I(101|g)=100 {I30}. 


decay_energy_unit: KEV
decay_multipolarity: [E2]
decay_uncertain: S
decay_comment:
E from level energy difference in (|a,t); |g unobserved. E|g consistent with an estimate of E=45 {I10}, based on transition energy systematics (28 keV in {+181}Ta, 60 keV in {+177}Ta, 72 keV in {+175}Ta, 83 keV in {+173}Ta). |g will Be very highly converted and may Be obscured by strong Ta K|a| x ray at 57 keV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other I(422|g):I(222|g)=31 {I6}:100 {I17}, weighted average from ({+7}Li,4n|g) E=38 MeV, (d,2n|g) and (p,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E weighted average from (d,2n|g) and ({+7}Li,4n|g) E=45 MeV. 
M |g(|q) in ({+7}Li,4n|g) E=38 MeV consistent with Q for doublet dominated by this intraband transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E weighted average from (d,2n|g) and ({+7}Li,4n|g) E=45 MeV. 
Other I(475|g):I(232|g)=100 {I30}:83 {I25} in (d,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M from |a(L)exp in ({+7}Li,4n|g). Other mult: not E1 from |a(exp) in ({+7}Li,4n|g) E=45 MeV. 
MR from ({+7}Li,4n|g) E=38 MeV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
B(M1)(W.u.) given here assumes negligible branching for 262|g, 595|g. 
M from |a(exp) in ({+7}Li,4n|g) E=45 MeV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
In ({+7}Li,4n|g) E=38 MeV, this transition was placed from the 31/2 member of the 9/2[514] band because the 307|g from that level was not resolved from the 305|g immediately below it in the band's |DJ=1 |g cascade. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_uncertain: ?
decay_comment:
E presumed to Be the same transition as the E|g=639.0 {I3} line reported in ({+7}Li,4n|g) E=38 MeV, but placed feeding the 29/2 (rather than the 31/2) member of the 9/2[514] band. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E 728.6 {I3} in ({+7}Li,4n|g) E=38 MeV for line which was partly associated with the 1/2[541] band; see comment on 2610+x level in that dataset. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M from intensity balance in ({+7}Li,4n|g) E=45 MeV if order of 353.3|g and 208.6|g shown here is correct. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
%I|g=18 {I3} assuming recommended normalization. 
E mean of 6 determinations by 1963Va28 is 30.69 {I4}, but authors do not state systematic uncertainty. Other E|g: 30.67 (1969Ko18), 30.67 (1968Ha39), 30.5 {I5} (1969Bi10). 
M from |a(L3)exp=0.57 {I11}, based on measured |a(L3)exp/|a(K)exp(E1 100.20|g in {+176}Ta)=1.9 {I4} (1963Va28). This is an anomalous E1 transition, based on ce(L1):ce(L2):ce(L3) exp in 1963Va28 and 1968Ha39. |a(E1)=1.73 {I3}. 
CC from |a(L3)exp, ce(L1):ce(L2):ce(L3):ce(M1):ce(M2):ce(n) exp= 168:250:100:73:113:40 (1963Va28) and ce(M1):ce(M2):ce(M3):(ce(M4)+ce(M5)) exp=170:235:100:30 (1968Ha39). Other ce(L1):ce(L2):ce(L3) exp=150:220:100 (1968Ha39). From theory, one expects |a=1.73. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
%I|g=0.228 {I22} based on adopted normalization. 
M from Adopted Gammas. M1,E2 from |a(L)exp=0.11 {I5} (1969Ko18). 


decay_energy_unit: KEV
decay_uncertain: S
decay_comment:
E from level energy difference; |g not observed, but existence is implied by |g|g coin data. 
I(|g+ce)>52 {I18}, <82 {I11} from intensity balance at 528, 520 levels, respectively. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI from I(146|g)/I(153|g)=0.34 in (d,2n|g), I(153|g)=2.4 is expected from 673 level, leaving I|g=10.2 deexciting the 781+x level (I|g=12.6 for doublet). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
RI see comment on 153|g from 673 level. 
A{-2}=+0.26 {I8} for doublet, ~81% of which deexcites this level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI based on I(443.6|g)=11.0 and adopted branching for the 925 level, only I|g(232.6)=3.2 is attributable to this transition, leaving I|g=70.9 to be placed from the 1253 level (I|g=74.1 for doublet). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.19 {I9} for possible doublet. 
RI includes an unplaced component which precedes the 1253 level. From I(252|g)=2.3 and adopted I(252|g)/I(486|g from 1177 level)=0.20, one expects I|g=11.5 from 1177 level in ({+7}Li,4n|g) E=38 MeV, cf. I(486|g doublet)=11.2; therefore, the evaluator shows the entire I|g deexciting the 1177 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M from |a(exp)=0.36 {I10}, which the evaluator presumes to be for this delayed component of the 233|g. 
A{-2}=-0.07 {I5} for multiplet dominated by this transition. 
RI see comment on 232.6|g from 925 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.20 {I8} for triplet. 
In Adopted Levels, this |g feeds the 31/2 member of the 9/2[514] band (not the 29/2 member). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.39 {I21}. 
In Adopted Levels, this |g feeds the 31/2 member of the 9/2[514] band (not the 29/2 member). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other I|g: I(295|g)/I(161|g)=0.67 {I15} (1997Ko13). 
M A{-2}=+0.42 {I8} for 294.7|g+293.7|g doublet dominated by 293.7|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other I|g: I(238|g)/I(133|g)=0.17 {I4} (1997Ko13). 
M A{-2}=-0.04 {I4} for 238.3|g+238.4|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
Other I|g: I(375|g)/I(199|g)=0.24 {I2} (1997Ko13). 
I|g(out-of-beam): 15 {I3} (1997Ko13). 
M A{-2}=+0.20 {I5}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other I|g: I(343|g)/I(184|g)=0.52 {I4} (1997Ko13). 
M A{-2}=+0.03 {I9} for 343.4|g+343.4|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
Other I|g: I(465|g)/I(242|g)=0.52 {I2} (1997Ko13). 
I|g(out-of-beam): 32 {I1} (1997Ko13). 
M A{-2}=+0.24 {I4}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
I|g(out-of-beam): 84 {I8} (1997Ko13). 
M |a(exp)=0.40 {I17} from delayed intensity balance at 1019 level (1997Ko13). 


decay_energy_unit: KEV
decay_uncertain: S
decay_comment:
E from Adopted Gammas. Highly-converted transition not seen in this study; possibly obscured by K|b{-1} x ray from Ta. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Mult: Not E1 
M |a(exp)|>5.2 from intensity balance at the 1327 level rules out E1; consistent with adopted mult=M1(+E2) (1997Ko13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI approximate. I|g(out-of-beam): 32 {I3} (1997Ko13). 
M A{-2}=+0.22 {I4} for 273.8|g+274.3|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other I|g: I(553|g)/I(283|g)=1.1 {I3} (1997Ko13). 
M A{-2}=+0.20 {I13} for 553.2|g+552.4|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other I|g: I(566|g)/I(290|g)=0.70 {I16} (1997Ko13). 
M A{-2}=+0.47 {I9} for 566.1|g+565.9|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g(out-of-beam): 20 {I3} (1997Ko13). 
M A{-2}=+0.42 {I8} for 293.7|g+294.7|g dominated by this |g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other I|g: I(606|g)/I(314|g)=0.70 {I17} (1997Ko13). 
I|g(out-of-beam): 6 {I1} (1997Ko13). 
E from 2004Ko58. Other E|g: 606.4 {I2} (1997Ko13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
Other I|g: I(646|g)/I(333|g)=1.02 {I25} (1997Ko13). 
I|g(out-of-beam): 19 {I1} (1997Ko13). 
M A{-2}=+0.35 {I7}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
I|g(out-of-beam): 11 {I1} (1997Ko13). 
M |a(exp)=2.7 {I4} from delayed intensity balance (1997Ko13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M M1(+E2) from |a(exp)=1.7 {I7} from intensity balance at the 2792 level (1997Ko13); D+Q from A{-2}=-0.63 {I14}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M M1,E2 from |a(exp)=0.26 {I14} from intensity balance at the 2727 level. D+Q from A{-2}=+0.05 {I15} (1997Ko13). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$|a(exp)=2.5 {I3} gives E1+M2 with |d=0.242 {I18}. However, |d value is inconsistent with RUL for M2 transitions 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$D+Q from R(DCO) in {+176}Yb({+11}B,|a3n|g),({+7}Li,3n|g), |D|p=no from level scheme 
MR$from R(DCO) in {+176}Yb({+11}B,|a3n|g),({+7}Li,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
MR$<0.3 from |a(K)exp in {+176}Yb({+11}B,|a3n|g)({+7}Li,3n|g). Other: 0.65 {I19} from |a(exp) also in {+176}Yb({+11}B,|a3n|g)({+7}Li,3n|g) gives M2 strength inconsistent with RUL. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (E2)
decay_comment:
$|a(exp)=0.09 {I8} from intensity balance. 
M$E2 or E3 from |a(exp); E3 excluded by comparison to RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$I|g=160 {I12} 
$|a(exp)=0.03 {I3} (1999Sa59) from intensity balance 
M$from |a(exp) 
$A{-2}=-0.01 {I3} (1998Dr07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$I|g=130 {I12} 
$|a(exp)=2.5 {I3} (1999Sa59) from intensity balance 
M$|a(exp) gives E1+M2 with |d=0.242 {I18}. However, |d value is inconsistent with RUL for M2 transition. 
$A{-2}=-0.06 {I5} (1998Dr07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$I|g=16.4 {I12} 
$|a(exp)=0.96 {I10} (1999Sa59) from intensity balance 
M$from |a(exp) 
$A{-2}=-0.14 {I3} (1998Dr07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g=26.2 {I18} 
$R(DCO)=1.4 {I2} (1334|g gated) (1999Sa59). 
$|d(E2/M1) given as 3.6 to 5.8 in 1999Sa59 based on R(DCO) 
$A{-2}=+0.02 {I7} (1998Dr07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$I|g=16.3 {I22} 
$|a(exp)=0.30 {I11} (1999Sa59) from intensity balance, |a(K)exp|<0.08 (2000Dr11) 
M,MR$from |a(K)exp. Other: 0.65 {I19} from |a(exp) gives M2 strength inconsistent with RUL. 
$A{-2}=-0.13 {I4} (1998Dr07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_mixing_ratio_info: ;ERR=?
decay_comment:
$I|g=142 {I9} 
$R(DCO)=1.1 {I1} (1092|g E2 gated) (1999Sa59). 
MR$from R(DCO) analysis 
$A{-2}=+0.17 {I9} (1998Dr07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$I|g=37 {I3} 
$R(DCO)=1.1 {I4} (1092|g E2 gated) (1999Sa59). 
$A{-2}=+0.33 {I10} (1998Dr07). 
RI$I|g(428|g)/I|g(225|g)=0.29 {I2} (1998Dr07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g=19.2 {I15} 
$|a(K)exp=0.094 {I9} (2000Dr11). 
M,MR$from |a(K)exp. 
$R(DCO)=1.1 {I3} (441|g E2 gated) (1999Sa59). 
$A{-2}=+0.35 {I5} (1998Dr07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$I|g=45 {I12} 
$|a(K)exp=0.082 {I7}, |a(L)exp|<0.021, |a(M)exp|?0.004 (2000Dr11). 
M$from |a(K)exp 
$A{-2}=-0.16 {I5} (1998Dr07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$I|g=15.0 {I13} 
$|a(K)exp=0.020 {I3} (2000Dr11). 
M$from |a(K)exp 
$A{-2}=+0.24 {I7} (1998Dr07). 
RI$I|g(418|g)/I|g(221|g)=2.3 {I4} (1998Dr07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3(+E4)
decay_BM_unit: mu^2 x (fm)^4
decay_BM_info: ;TYPE=BM3;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM3W
decay_comment:
MR$0.7 {I3} from |b{+-} decay doubtful because B(E4)(W.u.)=320. RUL requires B(E4)(W.u.)<10 for A>150. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$calculated by the evaluator from the intensity balance. Other values: 0.0125 {I28} from I(6.2|g)/L{-|a} x ray=0.0175 {I38} and I(482|g)/L{-|a} x ray=13.99 {I4} from 1976Ca11 
M$from {+181}W |e decay 
CC anomalous E1 with penetration parameter |l=-9 {I1} from 1969Bl12. The uncertainty in |a is from the penetration parameter only. Note that this value for |a is consistent with the intensity of the 476-keV |g feeding the 6-keV level. ce(M1):ce(M2):ce(M45):ce(M3)=1.9(2):3.3(3):1.7(2):1 ce(N1):ce(N2):ce(N3):ce(N45)=1.6(4):2.3(4):7.0(35):1 (1969Bl12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from adopted gammas. |d=+0.41 {I3} from |a and sign from (136|g)(346|g)(|q); A{-2}=+0.224 {I27}, A{-4}=-0.014 {I7} averaged from 1971Av02, 1969Kl11, 1972BeYN, and 1970WiZO. 
RI$from ce(K)(136)/ce(K)(133)=0.3713 {I10}, ce(L1)(136)/ce(L3)(133)=0.1084 {I7} (1988Bu13); and |a(K)exp(133)=0.497, I|g(136|g+137|g)=8.34. I|g=7.23 {I31} from the ce(K) ratios and I|g=7.33 {I35} from the ce(L) ratios. Others: from I|g(136):I|g(137)=4.7 {I2}:0.67 {I12} (1971Av02) and I|g(136+137)=8.34, I|g=7.3 {I13}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$Q from 133|g-(346|g)-136|g and 133|g-346|g angular correlations (1971Av02); B(M2)(W.u.) <1 from RUL rules out M2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2+E3
decay_comment:
RI$from 1990He02. Other values: 0.758 {I22} (1977Fr10), 0.5 {I1} (1971Av02), 0.92 {I5} (1976Ca11), and 1.45 {I20} (1974HeYW). The large, statistically significant, intensity variations reported for this transition may indicate the existence of a previously unreported |b-decaying isomer in {+181}Hf. See also the comments on possible |b feeding to the ground state. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from L1/L2=2.85 {I3}, L2/L3=2.17 {I3} (1983Bu18). Others: 6.2 {I7} from (133|g)(482|g)(|q), A{-2}=-0.289 {I11}, A{-4}=-0.074 {I4}, averaged from 1971Av02, 1971Sc05, 1977Fr10, and 1969Va22. 
CC$anomalous transition with penetration parameter |l=150 {I1} (1988Bu13). |l=176 {I15} (from 1971Av02, recalculated by the evaluator). |a(K)exp weighted average of 0.026 {I2}, 0.024 {I1}, 0.023 {I2}, and 0.021 {I2} compiled by 1966Ha50 and 0.0234 {I15} (1971Av02). 
M$a small parity-violating E1 admixture to this transition has been investigated by many authors. A precise value for p(|g)=-6.1|*10{+-6} {I7} was measured by 1971Lo09. For additional values see 1967Lo04, 1967Va29, 1969Cr02, 1970Bo50, 1970Va20, 1971Bo03, 1971De01, 1972Li11, 1972Ku23, and 1974Sc21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$L1/L2=0.184 {I2}, L2/L3=1.20 {I1} (1983Bu18), L1/L23=0.1004 {I12} (1989Ki23). Penetration parameters |l(1)=22 {I4}, |l(2)=-11 {I4} (1989Ki23). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3(+E4)
decay_comment:
MR$|d=0.7 {I3} from |a(K)exp=0.132 {I20} and K:L:M+=11.9 {I5}:2.4 {I1}:0.32 {I6} (1971Av02). See comment in adopted gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$from bent crystal spectrometer measurement (1956Bo67). 
RI$from I|g(136+137)=8.34 and I|g(136)=7.27 {I23} (see comment on 136|g). 
M,MR$L1:L2:L3=1.0:0.095:<0.01 and %E2=1 {I4} from 1966Al05; |a(K)exp=2.2 {I6} from 1971Av02. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$total intensity 57 from 1957Dr13, divided by the evaluator, according to the relative total intensity of 346 and 482 transitions. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
CC$anomalous transition, |a from {+181}Hf |b{+-} decay. 
M$M1:M2:M3:M45=186 {I19}:333 {I33}:100:167 {I17}, N1:N2:N3:N45=22 {I11}:33 {I16}:100: 14 {I7}, from 1969Bl12. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$|a(K)exp=0.97 {I9} from I|g(136)/I|g(153)=0.38 {I1} and ce(K)(153)/ce(K)(136)=1.83 {I2} assuming |a(K)(136)=1.39. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
MR$sign: from |g(|q) (1966As02); value: weighted average of: +0.360 {I15} from |a{-K}(exp)=1.41 {I4} and angular correlation (1966As02); 0.45 {I4} from angular distribution (1956De44); 0.435 {I22} from |a (1960Be16), 0.45 {I4} from T{-1/2} and B(E2) (1960Bl10) and 0.35 {I8} from angular distribution (1976In07). 
$A{-2}=-0.028 {I11}, A{-4}=0.007 {I17} (1976In07) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$sign: from |g(|q) (1966As02); value: weighted average of values: +0.357 {I13} from |a{-K}(exp)=0.80 {I4} and angular correlation (1966As02); 0.37 {I5} from angular distribution (1958Ma36, 1959De29); 0.37 {I15} from |a (1960Be16) and 0.53 {I+47-20} from angular distribution (1976In07). 
$A{-2}=0.026 {I12}, A{-4}=0.025 {I19} (1976In07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2)
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_uncertain: S
decay_comment:
E$ deduced from level-scheme fitting procedure (evaluators). This E|g is adopted in all the other datasets. Apparently, there is no direct measurement of this energy. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$From 1971He13. In 2004Ah10, it could not be determined because it overlaps the 156.3865 peak from {+182}Ta decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$doublet, the other component is from {+182}Hf IT decay (61.5 min). Total intensity resolved by 1974Wa14 by intensity matching of 97.8|g and 224.4|g in {+182}Hf 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2)
decay_comment:
M$ M2 consistent with L x-ray subshell ratios, but E1, E2, or E3 cannot be ruled out. 
E$from Adopted Gammas. Other: |?15 (1968Cl06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$63.2 {I3} (1986Se14) 
M$from |a(K)exp=1.22 {I16}, K/L=5.0 {I6} (1966Bi10) 
|DI|g(absolute)=0.8 per 100 decays. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$24.1 {I3} (1986Se14) 
M$from |a(K)exp=0.053 {I10} and K/L=2.1 {I5} (1966Bi10). |d>2.3 from |a(K)exp but K/L agrees with pure E2 
|DI|g(absolute)=0.6 per 100 decays. 


decay_energy_unit: KEV
decay_multipolarity: (M2)
decay_uncertain: S
decay_comment:
TI$from intensity balance at 16.273 level. This should be considered as lower limit since there may be additional |g rays feeding this level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|a(K)exp agrees with M1 with |d<0.5, K/L1 is lower than for pure M1; |a(L1)exp exceeds value for pure M1 
$ce(L2) mixed with ce(K)(154.0); ce(N) mixed with ce(M)(99.8|g) 
$ I(CEK)=48, I(CEL1)=9.5, I(CEL2)=3.2, I(CEM)=2.3, I(CEN)=2.2. CEL2 CONTAINS CONTRIBUTION FROM CEK(154.0G); CEN CONTAINS CONTRIBUTION CEM(99.8G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$Conversion coefficients are for 114.31+114.38, but the contribution from the 114.38|g is expected to be small. ce(L2) mixed with ce(L1)(114.6|g); ce(N) mixed with ce(L1)(125.0|g+125.1|g) and ce(K)(180.9|g) 
$ I(CEK)=75, I(CEL1)=9.0, I(CEL2)=3.0, I(CEM)=3.5, I(CEN)=2.6. CEL2 MIXED WITH CEL1(114.6G); CEN MIXED WITH CEL1(125.0G+125.1G) AND CEK(180.9G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M,MR$|a(K)exp and |a(L1)exp consistent with M1 with |d(E2/M1)<0.5 
$Conversion coefficients are for 132.55+132.69+133.88. ce(L2) mixed with ce(K)(190.3|g); ce(M) mixed with ce(L1)(142.2|g) and ce(N) mixed with ce(L3)(143.1|g) 
$ I(CEK)=77, I(CEL1)=10, I(CEL2)=2.4, I(CEM)=3.3, I(CEN)=1.1. CEL2 MIXED WITH CEK(190.3G); CEM MIXED WITH CEL1(142.2G) AND CEN MIXED WITH CEL3(143.1G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
$ce(K) mixed with KLM Auger electrons; ce(L1) mixed with ce(L1)(122.61+ 122.67|g)+ce(K)(178.6|g) 
$ I(CEK)=5, I(CEL1)=1.5. CEK MIXED WITH ^KLM AUGER ELECTRONS; CEL1 MIXED WITH CEL1(122.61+122.67G)+CEK(178.6G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|a(K)exp agrees with M1 with |d<0.45, K/L1 is lower than for pure M1; |a(L1)exp exceeds value for pure M1 
$ce(L2) mixed with ce(L1)(100.5|g) and ce(K)(156.0|g). ce(M) mixed with ce(N)(97.8|g) 
$ I(CEK)=45, I(CEL1)=9.5, I(CEL2)=(3.1), I(CEM)=2.2, I(CEN)=1.4. CEL2 MIXED WITH CEL1(100.5G) AND CEK(156.0G). CEM MIXED WITH CEN(97.8G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$ce(K) mixed with ce(L2)(99.8|g) and ce(L1)(100.5|g) 
$ I(CEK)=3.1, I(CEL2)=3.0, I(CEL3)=2.0, I(CEM)=1.0. CEK MIXED WITH CEL2(99.8G) AND CEL1(100.5G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
MR$from ce data 
RI$ 1979Va10 state that intensity per 100 neutron captures is |?15 for this |g ray. 
$ I(CEK)=8.0, I(CEL1+L2)=1.9, I(CEL3)=1.0, I(CEM)=0.8 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$|a(K)exp mixed with ce(L1)(122.61|g+122.67|g+122.9|g) 
$ I(CEK)=1.5, EKC MIXED WITH CEL1(122.61G+122.67G+122.9G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$ce(K) mixed with ce(L1)(139.4|g), ce(L1) mixed with ce(K)(250.9|g) 
$ I(CEK)=3.4, I(CEL1)=0.9. CEK MIXED WITH CEL1(139.4G), CEL1 MIXED WITH CEK(250.9G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
E$ level-energy difference=143.166 
$ce(K) mixed with impurity line from {+183}Ta. ce(L3) is mixed with ce(N)(133.8|g) 
$ I(CEK)=3.0, I(CEL2)=1.1. CEK MIXED WITH IMPURITY LINE FROM 183TA. ce(L3) is mixed with ce(N)(133.8|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$|a(K)exp for 250.97+251.32+251.77; mixed with ce(L1)(195.1|g) 
$ I(CEK)=(0.9); MIXED WITH CEL1(195.1G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$ce(L1) mixed with ce(L2)(114.31|g+114.37|g) 
$ I(CEK)=20, I(CEL1)=3.0. CEL1 MIXED WITH CEL2(114.31G+114.37G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$from L2/L3 ratio. 1979Va10 give E2,M1. ce(K) mixed with ce(L2)(133.8|g) 
$ I(CEK)=2.4, I(CEL2)=1.4, I(CEL3)=0.9. CEK MIXED WITH CEL2(133.8G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
M$quoted |a(L1)exp is consistent with M1, but no assignment was made by 1979Va10 since the assignment of L1 ce line is questionable. 
$ I(CEL1)=15 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$ce(L1) mixed with ce(L2)(99.8) and ce(K)(156.0|g) 
$ I(CEL1)=3.1. CEL1 MIXED WITH CEL2(99.8) AND CEK(156.0G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$|a(K)exp and |a(L1)exp for 122.61+122.67. ce(K) mixed with KLM Auger electrons, ce(L1) mixed with ce(L1)(122.9|g) and ce(K)(178.6|g) 
$ I(CEK)=30, I(CEL1)=(1.5). CEK MIXED WITH ^KLM AUGER ELECTRONS, CEL1 MIXED WITH CEL1(122.9G) AND CEK(178.6G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
M$from |a(K)exp, 1979Va10 suggest (M1) 
$ce(K) mixed with ce(L2)(97.8|g) 
$ I(CEK)=3.2, I(CEL1)=(1.0). CEK MIXED WITH CEL2(97.8G) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
$|a(K)exp and |a(L1)exp for 125.02+125.13. ce(L1) mixed with ce(N)(114.31|g+114.37|g) and ce(K)(180.9|g) 
$ I(CEK)=10, I(CEL1)=2.6. CEL1 MIXED WITH ce(N)(114.31|g+114.37|g) and ce(K)(180.9|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
%I|g=35 {I3} assuming adopted decay scheme normalization. 
M from |a(K)exp=0.65 {I6} (1969Mc08) based on I(K| x ray) (assuming all observed I(K| x ray) is attributable to conversion of the 73|g). Other |a(K)exp: ~0.5 (1967Mo13); |<1 if I(|g+ce)(73)|<100%. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M in the absence of |b{+-} feeding to the 48 level, I(|g+ce)(48|g)=I(|g+ce)(41|g) and this implies multipolarities of E2 and M1, respectively, for the 48|g and 41|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR from |a(K)exp=0.65 {I12}, calculated from I(K vacancies)=33 {I6} with the assumption that the 181|g and 345|g are E1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M |a(exp)|>7.9 from I(|g+ce)(44|g)|>(I(|g+ce)(181|g)+I(|g+ce)(3 44|g)) rules out E1 for 44|g; |a(exp)|<16.4 from I(|g+ce)(44|g)|<I(|g+ce)(139|g) rules out pure E2. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
The ordering of the 175 transition and the isomeric transition from the 1258+x level has not been determined in {+186}W({+238}U,{+239}Np|g) work. 
M$(E1) from |a(exp)=0.12 {I18} (1999Wh03) deduced from intensity balance. E2 assignment, however, is not ruled out. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (E1)
decay_uncertain: ?
decay_comment:
The ordering of the 175 transition and the isomeric transition from the 1258+x level has not been determined in this work 
M$(E1) from |a(exp)=0.12 {I18} (1999Wh03) deduced from intensity balance. E2 assignment, however, is not ruled out. 


decay_energy_unit: KEV
decay_comment:
$ Calculated |d(E2/M1)=0.75 using g{-K}=0.63, g{-R}=0.35 {I5} and Q{-0}=6.5 in the rotational-model expression (equation 1 in 2009La17) 


decay_energy_unit: KEV
decay_multipolarity: (M1+E2)
decay_comment:
$I|g(186.8|g/161.1|g)=12.8 {I28} (2021Wa39) 
M$The |g-ray total intensity balance at this level agrees for a pure M1 or E2 of 186.8|g within two standard deviations. Authors of 2021Wa39 note 186.8|g may be considered as a mixed M1/E2 transition and E3 161.1|g gives |a=0.49 {I11} for the 186.8|g based on their measured intensity ratio. 


decay_energy_unit: KEV
decay_multipolarity: (E3)
decay_comment:
M$Based on the ratio of (1+|a{-K(1e)})/(1+|a{-tot})=0.20 (2021Wa39), where |a{-K(1e)} and |a{-tot} are conversion coefficients for hydrogen like atom and for neutral atoms. Also from comparison of T{-1/2} of neutral atom to that of hydrogen-like atom (2021Wa39). 


decay_energy_unit: KEV
decay_multipolarity: (E2)
decay_comment:
M$tentative assignment (2020Wa29) based on measured |a(exp)=0.57 {I24}, consistent with Mult=M1 or E2, and considering that M1 assignment would indicate a competing E2 transition to 1287 level, which is not observed 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$From 2005Ca02. Others: 291.9 keV 5 (2011St21) and 292 keV (2009Al30,2012Al05) 
M$The authors in 2005Ca02 ruled out a M2 assignment due to the lack of tantalum x rays in the observed |g-ray spectrum (high conversion coefficient of a M2 transition would lead to an x-ray peak with approximately 70% of the counts observed in a |g-ray peak). However, M1 or E2 assignments cannot be unambiguously excluded. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$From 2005Ca02. Others: 291.9 keV 5 (2011St21) and 292 keV (2009Al30,2012Al05) 
RI$Evaluators assume 100% branch from this level, as no other |g rays were observed. 
M$The authors in 2005Ca02 ruled out a M2 assignment due to the lack of tantalum x rays in the observed |g-ray spectrum (high conversion coefficient of a M2 transition would lead to an x-ray peak with approximately 70% of the counts observed in a |g-ray peak). However, M1 or E2 assignments cannot be unambiguously excluded. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$stretched D |g from asymmetry ratio, (E1) based on theoretical arguments implying unique parity orbitals |ni{-13/2} and |ph{-11/2} and systematics of even-even nuclei in this mass region having a similar decay pattern: 11- level at about 3 MeV exitation energy decaying to 10+ level of the g.s. band by E1 transition. For example for {+156}Er, {+158}Er, {+158}Yb, {+158}Hf, {+160}Hf, {+162}W and {+164}W nuclei having this pattern no 11+ level was found, except for {+156}Er where this level is placed at more than 600 keV above 11- level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
R=0.88 {I7} 
M$stretched D |g from asymmetry ratio, (E1) based on theoretical arguments implying unique parity orbitals |ni{-13/2} and |ph{-11/2} and systematics of even-even nuclei in this mass region having a similar decay pattern: 11- level at about 3 MeV exitation energy decaying to 10+ level of the g.s. band by E1 transition. For example for {+156}Er, {+158}Er, {+158}Yb, {+158}Hf, {+160}Hf, {+162}W and {+164}W nuclei having this pattern no 11+ level was found, except for {+156}Er where this level is placed at more than 600 keV above 11- level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(13-) --> (11-) listed in Table III of 2016Jo01 seems a misprint in view of placement and J|p values shown in authors' Figure 5 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(8+) --> (6+) listed in Table III of 2016Jo01 seems a misprint in view of placement and J|p values shown in authors' Figure 5 


decay_energy_unit: KEV
decay_multipolarity: E1
decay_comment:
M$ from intensity balance at 441 level and RUL 
$ I|g(38.4|g)/I|g(441.7|g)=52 {I7}/100 {I14} (2010Sc02) 


decay_energy_unit: KEV
decay_multipolarity: M2
decay_comment:
$|a(K)exp/(|a(L+...)exp|a(M)exp)=3.7 {I7} (2010Sc02) 
$ I|g(378.3|g)/I|g(441.7|g)=30 {I4}/100 {I14} (2010Sc02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)(W.u.)=150 {I100} (2017Do06), but the evaluators obtain B(E2)(W.u.)=138 {I+276-55} using upper and lower bounds of half-life 
M$from DCO and RUL 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (M1)
decay_comment:
M$From 1995Hi02, based on K x-ray intensity and non-observation of 72|g. Note, however, that in table II (listing E|a, I|a, |a|g coin information) of 1995Hi02, 72|g is shown to be in coin with 5508|a group. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Weighted average of 251.7 {I2} in ({+28}Si,4n|g) and 252.3 {I2} in |e decay. 
M Q from |g(|q), not M2 from intensity balance in ({+28}Si,4n|g). 


decay_energy_unit: KEV
decay_multipolarity: (E2)
decay_comment:
Other E|g: 406.2 in ({+63}Cu,p2n|g). 
Placement is from ({+63}Cu,p2n|g); order of 405|g and 409|g was reversed in ({+28}Si,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$other: 79 (1995Hi02) 
M$from |a(K)exp=9.0 {I11} (2023Zh03, from I|g and I(K x-rays)). Other: |a(K)exp|?10 from |a|g-coin (1995Hi02) 
TI$from I|a for 5168|a 
RI$based on I(|g+ce)=I|a and |a. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
M DCO=0.8 {I3} (1992Th06). A{-2}=-0.29 {I7}, A{-4}=+0.04 {I7} (1983Dr08). 
RI undivided; see comment with 974.6|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M DCO=0.97 {I5} (1992Th06). A{-2}=+0.337 {I20}, A{-4}=-0.120 {I23} (1983Dr08). 
RI combined value for 558.4|g, 558.8|g, and 560.6|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M DCO=0.90 {I5} (1992Th06). A{-2}=+0.314 {I12}, A{-4}=-0.082 {I15} (1983Dr08) for unresolved doublet. 
RI combined value for 601.9|g, 602.5|g, and 603.8|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M DCO=0.88 {I4} (1992Th06). A{-2}=+0.34 {I3}, A{-4}=-0.05 {I4} (1983Dr08) for unresolved doublet. 
RI combined value for 378.0|g and 379.3|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E from {+169}Re |e decay. 
See {+154}Gd({+20}Ne,5n|g) for comment regarding order of 145.3|g and 181.7|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M from Adopted Gammas. 
Placed in accord with adopted placement of a 145|g from the ({+20}Ne,5n|g) study by 1985Re06. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
M A{-2}=-0.14 {I9}. 
Table 2 (measured {+169}W transition properties) and Figure 5 ({+169}W level drawing) in 1985Re06 show interchanged order for 145.3|g and 181.7|g; evaluator assumes Figure 5 to be correct. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E 428.4 3 (A), 428.4 2 (B) 
RI from ({+20}Ne,4n|g). Other: I(428|g)/I(916|g)=0.76 in ({+52}Cr,4n|g), 2.5 {I9} in |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 156.0 {I4} (1975St02), 156.9 {I2} (1992Me10), 156.6 {I2} (2001Ki10). 
I|g=54.1% {I7} assuming adopted decay scheme normalization. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$other: 88 {I5} (1992Me10). 
A{-2}=+0.13 {I4}, A{-4}=+0.02 {I4} (2001Ki10). 
E$other: 412.5 {I4} (1975St02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
M,MR from A{-2}=-0.13 {I23}, A{-4}=-0.04 {I24}, |d(D,Q)=+10 {I+5-|@} (2001Ki10); |D|p=(no) from level scheme. Pure D or pure Q not ruled out. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E0+E2(+M1)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
E$other: 15.6 {I12} (1992Me10). 
M,MR from |a(K)exp=0.046 {I11}, A{-2}=-0.01 {I13}, A{-4}=+0.23 {I24}, |d(D,Q)=-3.3 {I+1.6-|@}, q{+2}(E0/E2)=6.1 {I18}, X(E0/E2)=0.16 {I5} (2001Ki10). 
CC based on |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E0+E2+M1
decay_comment:
E weighted average of 702.4 {I2} (1992Me10), 702.8 {I2} (2001Ki10). 
RI$other: 14.2 {I10} (1992Me10). 
M,MR from |a(K)exp=0.067 {I15}, A{-2}=+0.04 {I6}, A{-4}=+0.12 {I7}, q{+2}(E0/E2)=10 {I3}, X(E0/E2)=0.23 {I7} (2001Ki10). 
CC based on |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 100 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.20 {I1}; A{-4}=-0.05 {I2} (1985Re06). I(25|')/I(90|')=1.21 {I3} (1983Re03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 80 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.32 {I2}; A{-4}=-0.09 {I3} (1985Re06). I(25|')/I(90|')=1.36 {I3} (1983Re03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI 4.6 in ({+52}Cr,4n|g) (1994Mc06). 
M A{-2}=-0.23 {I3}; A{-4}=+0.02 {I5}; 90|' polarization +0.39 {I19} (1985Re06). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 70 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.32 {I2}; A{-4}=-0.07 {I3} (1985Re06). I(25|')/I(90|')=1.39 {I3} (1983Re03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI 4.5 in ({+52}Cr,4n|g) (1994Mc06). 
M A{-2}=-0.29 {I4}; A{-4}=+0.06 {I5}; 90|' polarization +0.26 {I19} (1985Re06). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 51 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.35 {I2}; A{-4}=-0.11 {I3} (1985Re06). I(25|')/I(90|')=1.59 {I4} (1983Re03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 47 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.34 {I2}; A{-4}=-0.06 {I3} (1985Re06). I(25|')/I(90|')=1.36 {I4} (1983Re03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 38 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.33 {I2}; A{-4}=-0.03 {I3} (1985Re06). I(25|')/I(90|')=1.52 {I4} (1983Re03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 38 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.35 {I2}; A{-4}=-0.10 {I3} (1985Re06). I(25|')/I(90|')=1.46 {I5} (1983Re03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI 19 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.46 {I4}; A{-4}=-0.13 {I5} (1985Re06) for doublet dominated by this |g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 32 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.26 {I4}; A{-4}=-0.13 {I7} (1985Re06) for multiplet dominated by this |g. I|g from coin spectrum. I(25|')/I(90|')=1.71 {I6} (1983Re03). 


decay_energy_unit: KEV
decay_comment:
E from coincidence spectra (1985Re06). 
I(590|g+592|g)=23 in ({+52}Cr,4n|g) (1994Mc06). 
I|g=20.8 {I21}, A{-2}=+0.36 {I5}, A{-4}=-0.03 {I6} (1985Re06) for 590|g+592|g (from coincidence spectra). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 23 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.35 {I3}; A{-4}=-0.02 {I4} (1985Re06). I(25|')/I(90|')=1.37 {I7} (1983Re03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 17 in ({+52}Cr,4n|g) (1994Mc06). 
A{-2}=+0.36 {I5}; A{-4}=-0.04 {I6} (1985Re06). I(25|')/I(90|')=1.51 {I9} (1983Re03). 


decay_energy_unit: KEV
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
E from energy difference between 348.42|g and 343.88|g. 
Existence of transition established by |g|g coin in ({+30}Si,5n|g). 


decay_energy_unit: KEV
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
E from energy difference between 458.19|g and 450.60|g in ({+30}Si,5n|g). 
I(|g+ce)(7.6):I|g(457.8|g+458.2|g)=1.1 {I9}:100.0 {I22}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E 208.00 in Fig. 1(b) of 1994Es01. 
DCO=1.17 {I15} for multiply-placed |g; 1994Es01 suggest that an unresolved contribution from the expected |DJ=1, 207.73|g may account for a ratio that is a little higher than expected for a |DJ=2 transition 


decay_energy_unit: KEV
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
E from energy difference between 348.42|g and 343.88|g (see fig. 1(b) and table 3 of 1994Es01). 
Existence of transition established by absence of 212|g from 208|g-|g coin spectrum. 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
RI$reported by 1978Dr04 only as a mixed ({+172}W+contaminant) line. But it is considered suspect (evaluator) in {+172}W since its I|g from I|g(615|g)/I|g(1034|g)=3.2 (1978Dr04) is large enough to be detected in other reactions 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
A{-2}=0.18 {I4}, A{-4}=0.00 {I5} 
The intensity of this |g-ray as reported by 1978Dr04 is too large to be missed by 1994Es01. Moreover, sign of A{-2} reported by 1978Dr04 is inconsistent with a |DJ=1 (dipole) transition expected from |DJ|p. These considerations make this transition suspect 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
I|g(902|g)/I|g(414|g)=0.49 (1991Mc04) is in disagreement 
DCO=1.4 {I3}. A{-2}=-0.14 {I4}, A{-4}=-0.01 {I6} 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
TI$1.25(Ice(K)=1.0 {I3}) 
$ q{+2}(E0/E2)=3.6 {I11}; X(E0/E2)=0.060 {I18} 
$ AS PER E-MAIL REPLY (MAY 18, 2001) FROM THE LEAD AUTHOR, ICEK(761.6) IS ON THE SAME RELATIVE SCALE AS GAMMA-RAY INTENSITIES. In determining q{+2}, E2 transition corresponds to 0+ to 2+ transition of 638.4 KEV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$R{-ado}=1.42 {I9} 
RI$ other: I|g(419.1|g)/I|g(216.8|g)=4.93 {I34}; uncertainty of 3.34 quoted in table II is a misprint according to e-mail reply of Oct 18, 2012 from the authors. It should be 0.34 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E weighted average of 111.9 {I4} (1975St02), 112.1 {I2} (1977Ha24), and 112.9 {I2} (1977Be72). 
I|g=19.8% {I12} (absolute measurement of 1985Sz03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E weighted average of 243.0 {I4} (1975St02), 244.2 {I1} (1977Ha24), and 243.2 {I1} (1977Be72). 
I|g=37.4% {I21} (absolute measurement of 1985Sz03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E weighted average of 349.0 {I4} (1975St02) and 349.3 {I5} (1977Be72). 
I|g=4.7% {I3} (absolute measurement of 1985Sz03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
M from |g(|q) if J{-1}=J{-2}=6 and assuming small |d. Other possible allowed spins are J{-1}=5, J{-2}=6; and J{-1}=7, J{-2}=6. DCO ratios are not consistent with stretched quadrupole. 
MR from |a(K)exp|<0.0042 (1978Dr04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M from |a(K)exp=0.0023 {I5} (1978Dr04). |g(|q) (if J{-1}=J{-2}-1) and DCO ratios are consistent with stretched E1 (1978Dr04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M from |a(K)exp|<0.0047 (consistent with E1 or M1), |g(|q) (if J{-1}=J{-2}+1), and DCO ratios (1978Dr04). 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
TI$1.25(Ice(K)=0.4 {I1}) 
$q{+2}(E0/E2)=2.1 {I4}; X(E0/E2)=0.041 {I2} 
$ AS PER E-MAIL REPLY (MAY 18, 2001) FROM THE LEAD AUTHOR, ICEK(792) IS ON THE SAME RELATIVE SCALE AS GAMMA-RAY INTENSITIES. In determining q{+2}, E2 transition corresponds to 0+ to 2+ transition of 679.2 KEV 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$Compiler obtains B(E2)(W.u.)=167.8 {I23}. Per email reply from first author to XUNDL compiler on April 5, 2016, the 1.4% implied uncertainty in theoretical conversion coefficients taken from BrIcc code was not included in their B(E2) uncertainty. 
CC$Theoretical value from BrIcc code 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR -0.38 {I9} or -1.7 {I2} from angular distribution and deduced from relative intensities and conversion coefficients. 
A{-2}=-0.71 {I4}; A{-4}=0.13 {I4}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
MR -0.34 {I15} or -1.9 {I8} from angular distribution and deduced from relative intensities and conversion coefficients. 
A{-2}=-0.68 {I9}; A{-4}=+0.04 {I10}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A{-2}=-0.080 {I15}; A{-4}=+0.020 {I16} for triplet with 439.76|g of {+175}W and 440.80|g of {+176}W. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E0+E2+M1
decay_mixing_ratio_info: ;ERR=?
decay_comment:
M$from |a(K)exp=0.066 {I7}, |a(L)exp=0.0122 {I16}, |a(M)exp=0.0033 {I8} in {+176}Re |e decay. M1 is 21%. 
MR$uncertainty +0.6 -1.2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
M 1071|g E2 assignment from |a(K)exp=0.0032 {I7} in {+176}Re |e decay is not consistent with the J|p assignment of the depopulating level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E0+E2+M1
decay_mixing_ratio_info: ;ERR=?
decay_comment:
M from |a(K)exp=0.056 {I4}, and |a(L)exp=0.0034 {I4}. M1 is 13.7%. 
MR uncertainty +0.4 -0.5 
A{-22}=+0.21 {I8}, and A{-44}=+0.2 {I9} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E0+E2+M1
decay_mixing_ratio_info: ;ERR=?
decay_comment:
M from |a(K)exp=0.0083 {I16}. M1 is 11.1%. 
MR uncertainty +1.0 -0.7 
A{-22}=-0.22 {I14} and A{-44}=+0.24 {I16} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E0+E2+M1
decay_mixing_ratio_info: ;ERR=?
decay_comment:
M$from |a(K)exp=0.066 {I7}, |a(L)exp=0.0122 {I16}, |a(M)exp=0.0033 {I8}. M1 is 21%. 
MR uncertainty +0.6 -1.2 
A{-22}=+0.05 {I7}, A{-44}=+0.23 {I8} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
M 1071|g E2 assignment from |a(K)exp=0.0032 {I7} in 2001Ki10 is not consistent with the J|p assignment of the depopulating level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$From ce(L1+L2)exp:ce(L3)exp=520 {I40}/360 {I80} (2000Ro41). Others: ce(L1)exp:ce(L2)exp:ce(L3)exp=|?24:100:96 (1975El07) and DCO=0.83 {I11} (1997Sh36). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From ce(K)exp:ce(L2)exp:ce(L3)exp=53:100:83 (1975El07) in {+177}Re |e decay. The uncertainty in the Ice values is 20 %; DCO=1.1 {I1}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_uncertain: S
decay_comment:
E$From level energy differences. Not observed, but required by the coincidence relationships. 
RI$From I(|g+ce) intensity ratio in {+164}Dy({+18}O,5n|g) (1997Sh36) and the assumed Mult. and |a. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$From ce(L1)exp:ce(L2)exp:ce(L3)exp=100:|?18:|?13 (1975El07) in {+177}Re |e decay. The uncertainty in the Ice values is 20 %. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$From ce(K)exp:ce(L1+L2)exp:ce(L3)exp=100:50:29 (1975El07) in {+177}Re |e decay. The uncertainty in the Ice values is 20 %. DCO=0.93 {I8}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$DCO=0.86 {I7}. The value overlaps with that for the 484.5 and 485.1 keV |g rays. See 1997Sh36 in {+164}Dy({+18}O,5n|g)) for details. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
MR$-1.1<|d<-0.79 from the DCO ratios of the 404.9|g deduced when gated on the 144.3|g (1997Sh36) in {+164}Dy({+18}O,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.54 {I5}. The value overlaps with that for the 273.1 keV |g-ray. See 1997Sh36 in {+164}Dy({+18}O,5n|g) for details. 
MR$0.31 {I1}, assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$DCO=0.86 {I7}. The value overlaps with that for the 485.1 and 485.4 keV |g-rays. See 1997Sh36 for details. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.54 {I5}. The value overlaps with that for the 273.9 keV |g-ray. See 1997Sh36 for details. 
MR$0.28 {I1}, assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$DCO=0.86 {I7}. The value overlaps with that for the 484.5 and 485.4 keV |g-rays. See 1997Sh36 for details. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
MR$0.4<|d<1.0 or 1.0<|d<2.7 from the DCO ratios of the 377.3|g deduced when gated on the 143.7|g (1997Sh36). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Others: E|g=79.8 keV {I5} (1970Go20). 
M,MR$From ce(L1+L2)exp:ce(L3)exp=520 {I40}/360 {I80} (2000Ro41). Other: ce(L1)exp:ce(L2)exp:ce(L3)exp=|?24:100:96 (1975El07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$Others: E|g=95.6 keV {I5} (1970Go20). 
M$From ce(K)exp:ce(L2)exp:ce(L3)exp=53:100:83 (1975El07). The uncertainty of the Ice values is 20 %. 


decay_energy_unit: KEV
decay_comment:
E$Unresolved from 101.4|g, 7/2- to 5/2- transition within the |n5/2[512] band. Obscured by the 106.1|g and 103.6|g, the 2+ to 0+ transition in {+178}W and {+180}W, respectively. 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
E$Placed by the evaluator to depopulate the 135.2 keV level in accordance with adopted gammas 
M$From ce(L1)exp:ce(L2)exp:ce(L3)exp=100:|?18:|?13 (1975El07). The uncertainty of the Ice values is 20 %. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Placed by the evaluator to depopulate the 186.0 keV level in accordance with the adopted level scheme. 
RI$From the branching ratios in the adopted gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$Others: E|g=84.2 keV {I5} (1970Go20). Placed by the evaluator to depopulate the 186.0 keV level in accordance with the level scheme. 
M$from |a(K)exp|?0.40 {I11} (1975El07). 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
E,M$From adopted gammas. Other: 104.4 {I2} in 1975Ha32 and 1975El07. Unresolved from 101.2|g, 5/2- to 1/2- transition. Obscured by the 106.1|g and 103.6|g, the 2+ to 0+ transition in {+178}W and {+180}W, respectively. 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
E,M$From adopted gammas. Other: 116.9 {I3} in 1975Ha32 and 1975El07. Obscured by 116.65|g of {+177}Ta. Placed by the evaluator to depopulate the 252.4 keV level in accordance with the adopted level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$From adopted gammas. Other: 181.6 {I3} (1975Ha32 and 1975El07). Obscured by 181.1|g of {+178}W. 
RI$From the branching ratios in the adopted gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$From adopted gammas. Others: 196.85 {I20} (1975Ha32 and 1975El07) and 196.9 keV {I5} (1970Go20). 
M$From ce(K)exp:ce(L1+L2)exp:ce(L3)exp=100:50:29 (1975El07). The uncertainty of the Ice values is 20 %. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$From adopted gammas. Other: 209.9 {I5} (1975Ha32 and 1975El07) 
M$From |a(K)exp=0.14 {I4} (1975El07). 


decay_energy_unit: KEV
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
E$From level energy differences. Not observed directly, but required by the coincidence relationships. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$DCO=0.86 {I7}. The value overlaps with that for the 484.5 and 485.1 keV |g-rays. See 1997Sh36 for details. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.54 {I5}. The value overlaps with that for the 273.1 keV |g-ray. See 1997Sh36 for details. 
MR$0.31 {I1}, assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$|a(exp)=1.8 {I3} from intensity balance consideration (1997Sh36). |a(E1)=0.17, |a(E2)=1.18, |a(M1)=1.98. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$|a(exp)=0.4 {I4} from intensity balance consideration (1997Sh36). |a(E1)=0.06, |a(E2)=0.27, |a(M1)=0.62 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
The intensity of this transition has been used by the evaluators for normalization of the 2001Ki10 I|g values to those of 1970Go20. 
M$A{-2}=+0.08 {I2}, A{-4}=+0.02 {I2} (2001Ki10). |a(K)exp=0.12 (1968Be53); |a(K)theo=0.1064. The theoretical |a(K,E2) value for this transition was adopted by 1970Go20 as normalization for their experimental CC data (value updated to current BRICC value of 1.064 by evaluators - 12-jul-2008). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$|a(K)exp=0.0056 {I19} (1970Go20). |a(K)exp=0.00152 {I11}, |a(L)exp=0.00016 {I4}, A{-2}=+0.17 {I3} (2001Ki10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1+E2
decay_comment:
M$|a(K)exp=0.024 {i6} (1970Go20). A{-2}=0.00 {i6}, a{-4}=+0.22 {i7}. |a(K)exp=0.0076 {i5}, |a(L)exp=0.00110 {i14}, |a(M)exp=0.00035 {i5}; 
$q{+2}(E0/E2)=0.94 {I13}; X(E0/E2)=0.045 {I6} (2001Ki10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1+E2
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
M$|a(K)exp=0.0090 {I8}, |a(L)exp=0.0010 {I2}. 
$q{+2}(E0/E2)=1.5 {I3}; X(E0/E2)=0.076 {I+14-13} (2001Ki10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
M$|a(K)exp<0.0055 (1970Go20); a(K)exp=0.0068 {I15}, A{-2}=-0.15 {I6}, A{-4}=-0.3 {I6}. 
MR$Inconsistency between |d and |a(K) experimental values. An |a(K) value of 0.0024 is obtained from the experimental |d value 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1+E2
decay_comment:
M$|a(K)exp=0.061 {I10} (1970Go20). |a(K)exp=0.0176 {I11}, |a(L)exp=0.0027 {I2}, |a(M)exp=0.0014 {I2}, A{-2}=-0.07 {I5}, A{-4}=+0.14 {I6}. 
$q{+2}(E0/E2)=3.2 {I3}; X(E0/E2)=0.140 {I13} (2001Ki10) 


decay_energy_unit: KEV
decay_multipolarity: E0
decay_comment:
TI I(|g+ce)=0.024 {I2}, deduced by evaluators from experimental values |a{-K}/|a{-L}=5.6 {I8} and Ice(K)=0.044 {I3} (2001Ki10). 
$q{+2}(E0/E2)=26 {I2} and X(E0/E2)=1.73 {I12} (2001Ki10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1+E2
decay_comment:
M$|a(K)exp=0.0051 {I5}, |a(L)exp=0.00063 {I12}; A{-2}=+0.14 {I10}, A{-4}=+0.35 {I11} 
$q{+2}(E0/E2)=0.7 {I5}; X(E0/E2)=0.014 {I18} (2001Ki10) 
MR$Inconsistency between |d and |a(K) experimental values (evaluators) An |a(K) value of 0.0093 is obtained from the experimental |d value 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1+E2
decay_comment:
M$|a(K)exp=0.0149 {I13}, |a(L)exp=0.00255 {I28}, |a(M)exp=0.00092 {I12} 
$q{+2}(E0/E2)=6.9 {I+7-17}; X(E0/E2)=0.61 {I+7-15} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E0+M1+E2
decay_comment:
M$|a(K)exp=0.0101 {I8}, |a(M)exp=0.00059 {I7} 
$q{+2}(E0/E2)=3.7 {I+4-9}; X(E0/E2)=0.30 {I+3-7} (2001Ki10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$A{-2}=+0.01 {I7}, DCO=0.87 {I2} 
RI$The value reported by 1999Cu02 is very different from that of 1998Pu01, but is inconsistent with the intensity balance in their own level scheme, as shown in the former paper. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$ suggested by 1979Do02 based on weak anisotropies observed in their |g(|q) distribution (coefficients not reported). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$ suggested by 1979Do02 based on weak anisotropies observed in their |g(|q) distribution (A{-2}=-0.06 {I2}). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M from |a exp |<1.0 (determined from transition intensity balance in delayed spectrum); A{-2}=-0.37 {I2}, A{-4}=-0.02 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3
decay_BM_unit: mu^2 x (fm)^4
decay_BM_info: ;TYPE=BM3;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM3W
decay_comment:
E weighted average from |e decay, IT decay, (|a,3n|g) and ({+13}C,4n|g). 
RI,M from {+179}W IT decay (6.40 min). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E weighted average from |e decay, (|a,3n|g) and ({+13}C,4n|g). 
M E2(+M1) from |e decay; D+Q from ({+13}C,4n|g) and (|a,3n|g). 
Other I|g: 10.0 {I14} from |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E weighted average from |e decay, (p,3n|g), (|a,3n|g) and ({+13}C,4n|g). 
M from ce data in {+181}Ta(p,3n|g), {+177}Hf(|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
E weighted average from |e decay, (p,3n|g), (|a,3n|g) and ({+13}C,4n|g). 
M,MR D+Q from |g(|q) in (|a,3n|g); E2(+M1) (|d>1.9) from |a(L)exp, subshell ratios consistent with E2 in |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E weighted average from (p,3n|g), (|a,3n|g) and ({+13}C,4n|g). 
M D from ({+13}C,4n|g); E1 from |a(L)exp in (p,3n|g), (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
I|g is from |e decay; E|g is weighted average from |e decay and (p,3n|g). 
M,MR from |a(K)exp in {+181}Ta(p,3n|g), {+177}Hf(|a,2n|g). Other |d: 0.9 {I3} from |a(K)exp in |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
RI from ({+13}C,4n|g). Other I|g: 45.7 {I22} in ({+13}C,4n|g) relative to I(96|g)=100 {I30}; 21 in (p,3n|g); 38 in (|a,3n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E weighted average from |e decay, (p,3n|g), (|a,3n|g) and ({+13}C,4n|g). 
RI from |e decay. 
M from |a(K)exp in {+181}Ta(p,3n|g), {+177}Hf(|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other I|g: 87 in (|a,3n|g), 175 in (p,3n|g). 
M from ce data in {+181}Ta(p,3n|g), {+177}Hf(|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E from {+181}Ta(p,3n|g), {+177}Hf(|a,2n|g). 
RI from delayed |g's in ({+13}C,4n|g). 
M D+Q intraband |g in ({+13}C,4n|g) and (|a,3n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
RI weighted average of 29.8 {I16} (prompt |g's) and 34.8 {I23} (delayed |g's) in ({+13}C,4n|g). 
M from |a(K)exp in {+181}Ta(p,3n|g), {+177}Hf(|a,2n|g); D+Q from |g(|q) in ({+13}C,4n|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E,RI from (p,3n|g), (|a,2n|g). 
M evaluator presumes E1, suggested in (p,3n|g), (|a,2n|g), is erroneous. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI from (p,3n|g), (|a,2n|g) 
M mult=E2 suggested in (p,3n|g), (|a,2n|g) for line with E2 contaminant. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from |a(K)exp, |a(L)exp in {+181}Ta(p,3n|g), {+177}Hf(|a,2n|g); (Q) from |g(|q) in ({+13}C,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=?
decay_comment:
M from |a(K)exp=1.07 {I15} (relative to |a(K)exp(221.5|g)=|a(K)(M3 theory)=6.45) and K:L:M=237 {I30}:166 {I17}:120 {I60} (1969Ko18). Other data: ce(K):ce(L1):ce(L2):ce(L3):ce(M) exp=305:65:250:225:134 (1968Ha39). 
MR from sub-shell ratios (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E4]
decay_comment:
RI from intensity balance at 120.1 level. Transition observed in ce spectrum only. 
M L:M=4.1 {I5}:1.03 {I17} (1969Ko18). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3
decay_comment:
%I|g=8.81 {I24} assuming adopted normalization. 
M K:L:M=3.8 {I4}:1.61 {I16}:0.52 {I5} (1969Ko18). Other data: 1968Ha39. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=?
decay_comment:
M from |a(K)exp=0.59 {I23}, |a(L)exp=1.0 {I4} (1975Me20). K:L1:L2:L3:M=305:65:250:225:134 (1968Ha39). 
Other |d: |>2.8 from |a(K)exp. 


decay_energy_unit: KEV
decay_multipolarity: M3
decay_comment:
M from Adopted Gammas and K:L1:L2:L3:M=2000:720:|?100:360:270 (1968Ha39). 
I|g=17.0 {I10} in equilibrium with {+179}W IT decay (6.40 min). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
M,MR from |a(L)exp=5.4 {I8} (1975Me20); L2:L3:M=586:576:344 (1968Ha39) (cf. 2.78 {I4}:2.64 {I4}:1.41 {I2} from E2 theory). Subshell ratios consistent with pure E2. |d(M1,E2)>1.9 from |a(L)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 21.40 {I10} in 1975Me20 is a misprint, based on spectrum and authors' deduced I(|g+ce). 1973Ar11 report 1.4 {I3}. 
M L2:L3:M=116:108:45 (1968Ha39) (cf. 1.37 {I2}:1.24 {I2}:0.686 {I10} from E2 theory). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
%I|g=28 {I4} assuming adopted normalization. 
M from |a(K)exp=0.051 {I8}, |a(L)exp=0.011 {I1} (1975Me20). 
MR from Adopted Gammas; |d=0.9 {I3} from |a(K)exp in 1975Me20. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from |a(K)exp=0.15 {I3}, |a(L)exp=0.030 {I8} (1975Me20). K:L1:M=200:30:8 (1968Ha39). 
MR from |a(K)exp in 1975Me20. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g(delayed)=167 {I45} 
$M,|a from delayed intensity balance at 309 level, |a(exp)=4.9 {I16} assuming E2 multipolarity for 159.5|g and adopted E1 multipolarity for 189|g and 309|g. This |a(exp) implies |d(M1,E2)=0.30 {I+13-19}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$I|g(delayed)=31 {I3} 
M from |a(exp)<0.15, based on I(|g+ce) balance at 1832 level (1994Wa05). A{-2}=-0.50 {I5}. 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
$I|g(delayed)=924 {I41} 
M from unenumerated ce data of 1983Pe13 (both in-beam and out-of-beam data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M from |a(exp)<0.10, based on I(|g+ce) balance at 3582 level (1994Wa05). Supported by A{-2}=-0.23 {I19}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
A possible alternative placement exists from the 477.8 level. 
M A{-2}=+0.27 {I11}, A{-4}=-0.10 {I13} for possible doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M A{-2}=+0.16 {I9}, A{-4}=-0.02 {I7} for |g which may be doublet. 
1973Li06 place this |g from the 748 level only; however, a |g with this energy is also expected from the tentative 2291 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E 309.05 (1975Me21). 
M |a(K)exp=0.018 {I2} (1975Me21) from decomposition of complex ce line; |a(K)exp<0.027 if other ce components are ignored, ruling out M1 and E2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E 312.73 (1975Me21). 
M |a(K)exp=0.051 {I4} (1975Me21). |a(L)exp=0.017 {I2} for 312.7|g+315.0|g doublet. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M |a(K)exp=0.0055 {I12}, |a(L)exp=0.0011 {I2} (1975Me21); uncertainty given in 1975Me21 for |a(L)exp (0.002) is presumed to be a typographical error. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M |a(L)exp=0.017 {I2} (1975Me21) for 312.7+315.0 doublet. Given that mult(312.7)=E2, |a(L)exp(315.0)=0.015 {I6}, consistent with mult=E2, but an M1 admixture cannot be ruled out. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E1 multipolarity indicated in 1975Me21 is not consistent with placement in level scheme (M1(+E2) required there). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI may contain contribution from {+180}W (8+ to 6+ transition). 
M |a(K)exp=0.021 {I5}, mult=E2 for transition which may include an E2 contaminant. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from Hf(|a,xn|g). Other: 25 {I3} from {+176}Yb({+9}Be,5n|g), 9.3 from {+181}Ta(p,2n|g). 
M$D+Q from |g(|q) in {+176}Yb({+9}Be,5n|g), |D|p=no from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 115 {I8} from Hf(|a,xn|g) and 86 {I23} from {+176}Yb({+9}Be,5n|g). Other: 73 from {+181}Ta(p,2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$weighted average of 89 {I5} from Hf(|a,xn|g) and 107 {I3} from {+176}Yb({+9}Be,5n|g). Others: 100 {I20} in {+136}Xe({+48}Ca,4n|g) and 220 in {+181}Ta(p,2n|g). 
M$D from |g(|q) in Hf(|a,xn|g), |D|p=no from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$D+Q from |g(|q) in {+176}Yb({+9}Be,5n|g), |D|p= no from assumed band structure. 
RI$from {+176}Yb({+9}Be,5n|g). Others: 145 {I10} from Hg(|a,xn|g) and 63 from {+181}Ta(p,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$weighted average of 79.7 {I24} from {+176}Yb({+9}Be,5n|g) and 60 {I4} from Hf(|a,xn|g). Other: 170 from {+181}Ta(p,2n|g). 
M$D from |g(|q) in Hf(|a,xn|g), |D|p=no from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$D from |g(|q) in Hf(|a,xn|g), |D|p=no from level scheme. 
RI$from {+176}Yb({+9}Be,5n|g). Others: 25 from {+181}Ta(p,2n|g), 104 {I14} from Hf(|a,xn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
$|a(K)exp=0.0040 {I6} (1967Go22). 
M,MR$from |a(K)exp and A{-2}=+0.47 {I7}, A{-4}=-0.10 {I15} for 902|g-103|g(|q), assuming a J=2-2-0 cascade 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
M$from |a(exp)=0.55 {I4} (1979FaZR) 
$|a(exp): from intensity balance in delayed |g spectrum (1979FaZR). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (E1)
decay_comment:
M$from |a(exp) determined from intensity balance in 1979FaZR; in spectrum gated on 340.3|g, intensity of 125.0|g is significantly larger than the 158.1|g suggesting E1 for the former and M1 for the latter. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$weighted average of 100 {I10} (1966Bu08) and 100 {I17} (1981Av04). 
$|a(K)exp=0.11 (1967Bo08), |a(K)/|a(L) exp=2.1 {I5} (1967Bo08), 2.1 {I3} (1966Bu08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$weighted average of 110 {I11} (1966Bu08) and 94 {I10} (1981Av04). 
$|a(K)exp=0.039 {I10} (1967Bo08), 0.036 (1966Bu08); |a(K)/|a(L) exp=3.6 {I10} (1967Bo08), 3.1 {I4} (1966Bu08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$weighted average of 117 {I12} (1966Bu08) and 118 {I8} (1981Av04). 
$|a(K)exp=0.018 {I3} (1967Bo08), 0.017 (1966Bu08); |a(K)/|a(L) exp=3.6 {I11} (1967Bo08), 4.8 {I11} (1966Bu08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$weighted average of 120 {I12} (1966Bu08) and 92 {I8} (1981Av04). 
$|a(K)exp=0.012 {I4} (1967Bo08), 0.0083 (1966Bu08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
M$from A{-2}=0.47 {I7}, A{-4}=-0.10 {I15} from |g(|q) in (p,2n|g), and |a(K)exp=0.0046 {I6} ({+180}Re |e decay). Additional E3 mixing with |d(E3/E1)=-0.64 {I17} is consistent with these data (1971Ko17). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$not directly indicated in 2022HaAA, assumed by compiler since population of 3- level is given by authors. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI measured intensity I|g=6.8 was increased by the evaluator to balance feeding through the 113-keV level. Stronger 252.2-keV E3 transition feeding level could also be in error. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI intensity calculated from the intensity balance through the 385-keV level, assuming no direct feeding by |e decay. 
M from 1960Ha18, using relative intensities of nearby L2-electron lines. The limit on the intensity of the L2-line associated with this transition precludes the possibility of a substantial M1 component. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
RI$the intensity reported by 1973Li17 (I|g=888) is too large compared to the total intensity deexciting 1310-keV level. Also, the B(M1) is an order of magnitude smaller (relative to 521-keV B(E2)) than for other transitions in this band. I|g=220 has been calculated by evaluator assuming B(E2)/B(M1)=1400 from the systematics of the other band members. 
RI$702 (|a,2n|g) 
$A{-2}=+0.15 {I4}, A{-4}=-0.05 {I7} for 250.1+251.2. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_uncertain: ?
decay_comment:
RI 933 (|a,2n|g) 
M$intensity balance through lower levels requires E1 assignment. 
$A{-2}=-0.03 {I8}, A{-4}=-0.10 {I20}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$optimum agreement between experimental data and statistical-model calculations is obtained assuming |d{-|g}=0.47. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1+E0
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$E0 component suggested by ce data in {+182}Ta |b{+-} (1990Ka35) and q{-K}(E0/E2)=0.19 {I6} (1975We22) 
MR$17 {I+4-3} (1990Ka35) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_uncertain: S
decay_comment:
E$ B(E2)(W.u.)=200 {I60} is considered as large and improbable by the evaluators in view of relatively small B(E2)(W.u.) for other transitions from the 1257 level. Thus the presence of this transition is treated as questionable 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1+E0
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from {+182}Re decay (64.0 h). In |b{+-} decay, 1157+1158 doublet is not well resolved; with average energy of the doublet at 1157.510 {I15}, it deviates from level-energy difference by 0.2 keV in |b{+-} decay dataset. 
RI$unweighted average of 48.6 {I23} (|b{+-} decay) and 35 {I4} in |e decay (64 h). Other: 72 {I5} in Coul. ex. is high by |?70%. Values from (|a,2n|g) and (n,n'|g) cannot be used as these studies did not account for 1157 being a doublet with the second component from 1487 level 
M$ E0 component is estimated as 0.5% {I1} by the evaluators from comparison of |g-ray intensities and K-shell electron conversion data in 1976He18 
CC$ based on 0.5% {I1} E0 component and |d(E2/M1)=-9 {I+3-6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$all branchings relative to 1189|g, since efficiency problems at low energies such as 67.7 keV can be problematic. Branching for 31.7|g is from |b{+-} decay. Other: 2.8 {I6} from |e decay is low by a factor of |?2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
$|d(M2/E1)=+0.48 {I3}; |d(E3/E1)=-0.67 {I5} 
MR$from weighted averages of |d(M2/E1)=+0.44 {I6}, |d(E3/E1)=-0.69 {I10} (1983Ri05); |d(M2/E1)=+0.49 {I3}, |d(E3/E1)=-0.64 {I5} (1972Kr05); |d(M2/E1)=0.49 {I3}, |d(E3/E1)=0.72 {I7} (1972He10) 
M,CC$59% {I4} E1, 14% {I1} M2 and 27% {I3} E3. Conversion coefficient deduced for this admixture from BrIcc code 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$weighted average of +0.32 {I3} (1983Ri05), +0.30 {I2} (1980Sp01), +0.31 {I5} (1975Qu01), +0.30 {I2} (1972Kr05), 0.352 {I3} (1972He10,ce data, uncertainty increased to 0.02 in averaging procedure), 0.40 {I7} (1971Ga37,ce data), 0.346 {I7} (1967Ni03, ce data, uncertainty increased to 0.02 in averaging procedure). Values with sign are from |g(|q) or |g|g(|q) data 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
MR$-0.22 {I11} (1992Ch26), -0.023 {I4} (1983Ri05), 0.035 {I53} (1980Sp01 in {+182}Re decay); +0.014 {I13} (1975Qu01); all from |g(|q) or |g|g(|q). Subshell ratios in ce data (1967Ni03) give pure E1 consistent with RUL(M2)=1 suggests |d<0.006, thus the evaluators assign pure E1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=AP;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=AP
decay_comment:
$|d(M2/E1)=+0.36 {I10}; |d(E3/E1)=-0.28 {I12} 
M,CC$81% {I5} E1, 12% {I4} M2 and 7% {I2} E3. Conversion coefficient deduced for this admixture from BrIcc code 
M,MR$from |g(|q) and lin pol data of 1983Ri05, agrees with ce data of 1992Ch26 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1(+E0)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M,MR$from ce data in {+182}Ta |b{+-}, 1990Ka35 suggest M1+E2(+E0) with |d(E2/M1)=20 {I13}. |d(E2/M1)=+1.1 {I2} from |g|g(|q) in {+182}Ta |b{+-} (1992Ch26). E0 component is suggested by 1975We22 with q{-K}(E0/E2)=0.41 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$93 {I7} in (|a,2n|g) is high by |?60% 
$|d(M3/E2)=-0.11 {I+4-20} from |g(|q) in {+182}Ta |b{+-} decay is inconsistent with RUL(M3)=10, which suggests that |d should be near zero. |a(K)exp in {+182}Re |e decay is consistent with |d(M3/E2)=0 assigned by the evaluators. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
$|d(M2/E1)=-0.053 {I4} (1983Ri05,|g(|q) and lin pol); -0.08 {I5} (1992Ch26, |g|g(|q)); +0.06 {I+3-6} (1981Ka22,|g|g(|q)). But RUL=1 for M2 implies |d<0.005, thus the evaluators assign E1 
|d(M2/E1)=-0.08 {I5} (|g|g(|q) and ce in {+182}Ta |b{+-}, 1992Ch26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
$|d(M3/E2)=+0.067 {I10} from |g(|q) in {+182}Ta |b{+-}, but RUL(M3)=10 suggests |d(M3/E2) should be near zero. The evaluators assign pure E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$weighted averages taken of data from |b{+-}, |e and (n,n'|g) for all three |g rays from the 1510 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$35.5 {I21} from |e decay is quite in agreement 
MR$unweighted average of +2.2 {I2} (1992Ch26), +2.1 {I+3-2} (1983Ri05), +1.3 {I5} (1980Sp01), +0.9 {I4} (1975Qu01), +0.92 {I+13-7} (1972Kr05), +0.90m +40-23 (1972He10), 0.7 {I1} (1967Ni03). Weighted average is 1.0 {I2} but with reduced |h{+2}=10. Except for 1967Ni03, all other methods are |g(|q) on oriented nuclei or |g|g(|q) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
MR$+0.007 {I5} (1972Kr05), +0.027 {I7} (1992Ch26), -0.12 {I18} (1975Qu01), pure E1 from subshell data (1967Ni01), as also suggested by RUL for M2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2(+E3)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
E$weighted average from |b{+-} and |e decay 
M,MR$from ce data of 1976He18 and |g|g(|q) data of of 1992Ch26 in {+182}Ta |b{+-}. E3 admixture cannot be ruled out 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$from {+182}Re decay only, poor fit; |g not used in the level-scheme fitting procedure. Level-energy difference=1856.1 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
E$from {+182}Re decay only. This |g is considered as suspect by the evaluators since its intensity of 116 {I7} relative to 100 for 295.7|g is much too high to have missed detection in in-beam |g-ray study 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
$From |g(|q) in {+182}Re |e decay, 1980Sp01 give |d(Q/D)=-17 {I+10-24} or +0.06 {I+9-4}; favoring the former value from |d based on ce data of 1971Ga37. But 1971Ga37 assigned tentative E2 from their ce data. |d(M2/E1)=-17 {I+10-24} is inconsistent with RUL(M2)=1 for T{-1/2}(1960.30 level)<1 ns or so. The evaluators assign tentative E1 
RI$52 {I4} in (|a,2n|g) is discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1+E0
decay_comment:
$EKC=0.0030 1, ELC=0.00054 2 (1992Ch26) 
$EKC=0.00303 10 (1975We22) 
$ ICE(K)=101 3 (INCLUDES SMALL CONTRIBUTION FROM ICE(K) FOR 1113G); ICE(L)=18.5 7 (INCLUDES SMALL CONTRIBUTION FROM ICE(K) FOR 1181G) (1992Ch26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$ ICE(K)=67 (INCLUDES SMALL CONTRIBUTION FROM ICE(K) FOR 1224G); ICE(L)=12.1 5 (INCLUDES SMALL CONTRIBUTIONS FROM ICE(L) FOR 1224G AND ICE(K) FOR 1274G); ICE(M+N)+(ICE(K) FOR 1289G AND ICE(L) FOR 1231G)=19.4 8 (1992Ch26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$EKC=0.00032 2 (1992Ch26), EMC+ENC=0.00012 2 (1992Ch26) 
$ ICE(K)+(ICE(M+N) FOR 1189G)=5.6 3; ICE(L)=0.48 3; ICE(M+N)=0.17 3 (1992Ch26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
|d(M2/E1)=+0.48 {I3}, |d(E3/E1)=-0.67 {I5} 
$EKC=0.0037 3, ELC=0.00061 3, EMC+ENC=0.00014 1 (1992Ch26)$ 
$EKC=0.00418 14 (1975We22) 
$ ICE(K)=64 3 (INCLUDES CONTRIBUTION FROM ICE(M+N) FOR 1121G); ICE(L)=9.4 3; ICE(M+N)+(ICE(K) FOR 1257G)=5.6 3 (1992Ch26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_comment:
$ELC=0.0019 2, EMC+ENC=0.00036 3 (1992Ch26) 
$ ICE(K)+(ICE(L) FOR 1231G AND ICE(M+N) FOR 1221G)=19.4 8; ICE(L)+(ICE(K) FOR 1343G)=2.48 13; ICE(M+N)=0.51 3 (1992Ch26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
$EKC=0.0034 2, ELC=0.00049 4, EMC+ENC=0.00026 3 (1992Ch26) 
$ ICE(K)=6.8 3; ICE(L)=0.98 7, ICE(M+N)=0.51 7 (1992Ch26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
$EKC=0.0023 1, EMC+ENC=0.000085 7 (1992Ch26) 
$ ICE(K)=25.9 3; ICE(L)+(ICE(K) FOR 1289G AND ICE(M+N) FOR 1221G)=19.4 8; ICE(M+N)=0.94 10 (1992Ch26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3(+M2)
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
MR$ from ce data of 1992Ch26, 1976He18 and 1966Ko12; used weighted averaged I(ceK)=0.167 {I16} and I|g=0.113 {I4}, both relative to 100 for 1221|g; deduced |a{-K}(expt)=0.0038 {I4} 
$ ICE(K)=0.12 {I2} (1992Ch26), 0.18 {I1} (1976He18), 0.16 {I3} (1966Ko12) relative to 100 for K-conversion line for 1221|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$|a(exp)<0.27 (1994Re03) from intensity balance at 4038 level, 0.45 {I35} from prompt intensities given here 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
DCO=1.0 {I2}, |DJ=1 gated 
$(g{-K}-g{-R})/Q{-0}=0.060 {I10} for I|g(622.7|g)/I|g(320.0|g)= 0.61 {I18} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$total for 1158 doublet; about 1 unit of intensity should be assigned from the decay of 1487 level (evaluators) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI$too high an intensity as compared to values in |b{+-} and |e decays; possibly an incorrect assignment; also 4- to 2+ is not expected to be strong; only 0.027 expected from adopted branching ratios. Placement questioned by the evaluators 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$uncertainty in E|g, I|g table 1 of 1977Je02 seems too low to be consistent with others in the table. Evaluators have increased this by a factor of 10. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
M$ |a(K)exp is consistent with M1, E1+M2 (50% admixture of both) or M2+E3 (25% M2+75% E3). The half-life of the 2230 level makes E3, M3 or higher multipolarities unlikely. M2 is also unlikely since the transition is expected to be highly K-forbidden and the forbiddenness factor of 10{+3} is much smaller than expected for M2 transition and |DK-L=6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(g{-K}-g{-R})/Q{-0}=0.11 {i3} or 0.12 {i4} for I|g(558.2)/I|g(290.4)=0.57 {i30} or 0.48 {i30}, respectively 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$for 1157 doublet, |?2 units of intensity should be assigned to the decay of the 1487 level (evaluators) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$for J(1959)=3, |d=+0.01 {I+3-2} or -9 {I+2-4}. Negative A{-2} is inconsistent with |DJ=2 transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|DI|g(absolute)=0.4 per 100 decays. 
RI$calculated from the intensity balance at the 100 level. Measured value is I|g=58 {I4}. 
$ W(0|')-1=-0.057 {I25} 
$|a(L1)exp=0.11, 0.091 {I19}; |a(L2)exp=1.17 {I35}, 1.08 {I13}; |a(L3)exp=1.05 {I32}, 1.04 {I13}. 
$L1/L2=0.078 {I8}, L1/L3=0.083 {I9}, L2/L3=1.07 {I6} (1970Ag07) 
$ EL1C=0.090 27 (1970Ag07), EKC |? 0.874 (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.117 {I30}, 0.124 {I16} 
$ W(0|')-1=-0.154 {I3} 
$L1/L2=0.55 {I13}, L1/L3=0.080 {I20}, L2/L3=1.5 {I3} (1970Ag07) 
$ EKC=0.123 27 (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$|a(K)exp=0.038 {I12}, 0.045 {I7}; |a(L1)exp=0.0050 {I5}; |a(L2)exp=0.0057 {I7}; |a(L3)exp=0.0028 {I7}, 0.0032 {I5} 
$L1/L2=0.99 {I11}, L1/L3=1.82 {I25}, L2/L3=1.85 {I25} (1970Ag07) 
$ W(0|')-1=-0.154 {I4} 
$ EKC=0.044 9 (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1(+E0)
decay_comment:
MR$+21 {I+92-9} (1980Sp01) 
$|a(K)exp=0.00302 {I14}, 0.0030 {I3}, 0.0032 {I5} 
$L1/L2=6.8 {I6}, L1/L3=11.8 {I12}, L2/L3=1.8 {I2} (1970Ag07) 
M$E0 admixture is measured and discussed in 1975We22 from ce and |g(ce)(|q) data with q(E0/E2)=0.16 {I9} 
$ W(0|')-1=+0.004 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$ W(0|')-1=-0.103 {I6} 
$L1/L2=6.7 {I7}, L1/L3=20 {I2}, L2/L3=3.1 {I5} (1970Ag07) 
$|a(K)exp=0.00248 {I25}, 0.0026 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
$|d(M2/E1)=+0.48 {I3}; |d(E3/E1)=-0.67 {I5} 
M,CC$59% {I4} E1, 14% {I1} M2 and 27% {I3} E3. Conversion coefficient deduced for this admixture 
$|a(K)exp=0.0043 {I5}, 0.0041 {I8}, 0.0047 {I9} 
$ W(0|')-1=-0.243 {I9} 
$L1/L2=6.1 {I8}, L1/L3=32 {I5}, L2/L3=5.3 {I12} (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
MR$>+22 or <-35 (1980Sp01) 
$|a(K)exp=0.0046 {I5}, 0.0046 {I6}, 0.0047 {I10} 
$ W(0|')-1=+0.102 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$ Other: +0.30 {I2} (1980Sp01) 
$|a(K)exp|?6.0 (1971Ga37), |a(L1)exp=1.15 {I35}; |a(L2)exp=0.46 {I14}; |a(L3)exp=0.34 {I10} 
$L1/L2=2.40 {I14}, L1/L3=3.2 {I3}, L2/L3=1.36 {I12}, M1/M2=2.3 {I4}, M1/M3=2.5 {I5} M2/M3=1.1 {I3} (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$|a(K)exp=0.116 {I35} 
$ W(0|')-1=-0.14 {I3} 
$L1/L2|?4.3, K/L2|?28 (1971Ga37) 
$ EKC=0.17 5 FOR 151.1G+152.4G+153.9G 
MR$+0.035 {I53} from |g(|q) data consistent with RUL(M2)=1 which suggests |d near zero 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
$|d(M2/E1)=+0.36 {I10}; |d(E3/E1)=-0.28 {I12} 
M,CC$81% {I5} E1, 12% {I4} M2 and 7% {I2} E3. Conversion coefficient deduced for this admixture from BrIcc code 
$|a(K)exp=0.0052 {I24} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1(+E0)
decay_comment:
MR$+4.7 {I+6-5} (1980Sp01) 
M$E0 admixture is measured and discussed in 1975We22 from ce and |g(ce)(|q) data with q(E0/E2)=0.41 {I9} 
$ W(0|')-1=+0.029 {I4} 
$|a(K)exp=0.0035 {I4}, 0.0036 {I7}. |a(K)exp=0.00359 {I13} (1975We22) 
$L1/L2=6.7 {I15}, L1/L3>16, L2/L3>2.3 (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.36 {I3} (1980Sp01) 
$ W(0|')-1=-0.122 {I15} 
$|a(K)exp=2.7 {I8} (1971Ga37), |a(L1)exp=0.32 {I5}; |a(L2)exp=0.078 {I25}; |a(L3)exp=0.075 {I19} 
$L1/L2=4.0 {I6}, L1/L3=9.9 {I13}, L2/L3=2.1 {I17}, M1/M2=3.2 {I5}, M1/M3=5.4 {I10} M2/M3=1.8 {I6} (1971Ga37) 
$ L1/L2=4.1 7, L1/L3 AP 6.7, L2/L3 AP 1.7 (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$ W(0|')-1=-0.182 {I12} 
$|a(K)exp=0.20 {I4} 
$L1/L3=0.66 {I34} (1970Ag07) 
$ EKC=0.132 26 (1970Ag07) 
MR$+0.067 {I10} from |g(|q) data, but RUL(M3)=10 suggests |d near zero 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$A{-2}=-1.35 {I24}. Contribution from another component was considered 
$ W(0|')-1=-0.12 {I3} for 1158.1+1157.3 
MR$-0.047 to +1.1 (1980Sp01) 
$|a(K)exp=0.0021 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.84 to +1.8 (1980Sp01) 
$ W(0|')-1=-0.299 {I12} 
$L1/L2=1.99 {I19}, L1/L3=3.0 {I3}, L2/L3=1.50 {I19} (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$ W(0|')-1=+0.122 {I3} for 221.6+222.1 
$|a(K)exp=0.050 {I10} for 221.6|g+222.1|g (1970Ag07) 
$L1/L2>4 (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$ W(0|')-1=-0.182 {I7} 
$|a(K)exp=0.076 {I16} (1970Ag07) 
$L1/L2=0.50 {I11}, M1/M2=0.8 {I4}, M1/M3=1.1 {I7}, M2/M3=1.5 {I8} (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$ W(0|')-1=-0.183 {I4} 
$|a(K)exp=0.088 {I22}, L1/L2=0.66 {I13}, L1/L3=1.04 {I23}, L2/L3=1.6 {I3} (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$ W(0|')-1=+0.54 {I8} 
$|a(K)exp=2.3 {I7} for 107.1|g+108.6|g (1971Ga37) 
$L1/L2=0.74 {I8}, L1/L3=1.09 {I16}, L2/L3=1.6 {I3} (1971Ga37) 
MR$-0.56 to -1.3 (1980Sp01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$ FROM 1980Sp01 
$ W(0|')-1=-0.079 {I9} 
$|a(K)exp=0.67 {I11} (1970Ag07) 
$L1/L2=7.1 {I8}, L1/L3=17 {I3}, L2/L3=2.4 {I6}, M1/M2=4.9 {I14} (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
MR$+0.014 {I25} (1980Sp01) 
$ W(0|')-1=+0.117 {I20} 
$|a(L2)exp=0.0038 {I15} (1971Ga37) 
$ EL2C AP 0.012 (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$ W(0|')-1=-0.193 {I4} 
$|a(K)exp=0.069 {I19} (1970Ag07) 
$L1/L2=0.77 {I15}, L1/L3=1.23 {I23}, L2/L3=1.6 {I3} (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$ W(0|')-1=-0.18 {I3} 
$|a(L2)exp=0.0090 {I25}, L1/L2=0.83 {I20}, L1/L3=2.2 {I8}, L2/L3=2.7 {I10} (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
MR$ from 1980Sp01 
$ W(0|')-1=-0.001 {I3} 
$|a(K)exp=0.0037 {I4}, 0.0036 {I4}, 0.0041 {I8}. |a(K)exp=0.00399 {I13}, |a(L)exp=0.00060 {I3} (1975We22) 
$L1/L2=7.8 {I9}, L1/L3=23 {I5}, L2/L3=3.1 {I9} (1970Ag07) 
M$no E0 admixture found in |g(ce)(|q) and ce work of 1975We22 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$ W(0|')-1=+0.55 {I15} 
$|a(K)exp=2.3 {I7} for 107.1|g+108.6|g, M1/M2=2.1 {I9} (1971Ga37) 
MR$-0.41 to -1.7 (1980Sp01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.56 to +2.6 (1980Sp01) 
$ W(0|')-1=-0.31 {I6} 
$|a(K)exp=0.96 {I30} for 147.6|g+148.8|g+149.4|g, L1/L2=1.6 {I4}, L1/L3=2.8 {I19}, L2/L3=1.8 {I8} (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$ W(0|')-1=-0.165 {I14} 
$|a(K)exp=0.059 {I10}; |a(L1)exp=0.0067 {I10}; |a(L3)exp=0.0058 {I10} 
$|a(L1)exp=0.007 {I2}, L1/L2=0.97 {I18}, L1/L3=1.6 {I5}, L2/L3=1.7 {I5} (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$ FROM 1980Sp01 
$ W(0|')-1=+0.051 {I5} 
$|a(K)exp=0.87 {I21}; |a(L1)exp=0.140 {I17} 
$L1/L2=10 {I4}, L1/L3>27, L2/L3>2.5, M1/M2=9.9 {I18}, M1/M3=38 {I21}, M2/M3=4.4 {I24} (1971Ga37). 
$ L-SUBSHELL RATIOS ALSO LISTED BY 1970Ag07 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$ W(0|')-1=-0.194 {I4} 
$|a(K)exp=0.078 {I24}, 0.073 {I6}; |a(L1)exp=0.0105 {I11}; |a(L2)exp=0.0127 {I11}; |a(L3)exp=0.0080 {I10} 
$L1/L2=0.74 {I6}, L1/L3=1.10 {I10}, L2/L3=1.49 {I13} (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$ W(0|')-1=+0.23 {I11} 
MR$ FROM 1980Sp01 
$|a(K)exp=0.96 {I30} for 147.6|g+148.8|g+149.4|g, K/L2=37 {I25} (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.017 {I17} (1980Sp01) 
$ W(0|')-1=+0.129 {I9} 
$|a(K)exp=0.66 {I15}; |a(L1)exp=0.098 {I30}, 0.077 {I8}; |a(L2)exp=0.0081 {I7}; EL3C|?0.002 
$ EKC=0.48 8 (1971Ga37), EL1C=0.081 17 (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
$ W(0|')-1=+0.07 {I6} 
MR$from |g(|q), 1980Sp01 give |d(Q/D)=-17 {I+10-24} or +0.06 {I+9-4}; favoring the former value from |d based on ce data of 1971Ga37. But 1971Ga37 (also 1972Ga15) assigned tentative E2 from |a(K)exp=0.15 {I3} (1971Ga37) and questioned the placement and mult assignment. |d(M2/E1)=-17 {I+10-24} is inconsistent with RUL(M2)=1 for T{-1/2}(1960.33 level)<1 ns or so. The evaluators assign tentative E1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$ W(0|')-1=-0.173 {I5} 
$|a(K)exp=0.058 {I20}, 0.038 {I8}; |a(L1)exp=0.0052 {I8}; |a(L2)exp=0.0069 {I10}; |a(L3)exp=0.0036 {I13}, 0.0033 {I6} 
$L1/L2=0.82 {I15}, L1/L3=1.6 {I3}, L2/L3=2.0 {I4} (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$EKC|?0.32 
$|a(K)exp=0.17 {I5} for 151.1|g+152.4|g+153.9|g, L1/L2=2.1 {I6}, L1/L3>9.8, L2/L3>5.0 (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$ from 1980Sp01 
$ W(0|')-1=-0.07 {I5} 
$|a(K)exp=0.44 {I13}, 0.42 {I8}; |a(L1)exp=0.065 {I19}, 0.064 {I9} 
$L1/L2=8.7 {I19} (1971Ga37) 
$ EL1C=0.063 10, L1/L2=7.7 21 (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$ +0.28 +8-6 (1980Sp01) 
$ W(0|')-1=-0.12 {I6} 
$|a(K)exp=0.96 {I30} for 147.6|g+148.8|g+149.4|g (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$ from 1980Sp01 
$ W(0|')-1=+0.39 {I10} 
$|a(K)exp=0.53 {I15}, 0.35 {I11}; |a(L1)exp=0.074 {I14} 
$L1/L3>3 (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
MR$+0.016 {I24} (1980Sp01) 
$ W(0|')-1=+0.122 {I3} for 221.6+222.1 
$EKC|?0.04, 0.060 {I20}; |a(L1)exp=0.0068 {I8} 
$|a(K)exp=0.050 {I10} for 221.6|g+222.1|g, L1/L2>4 (1970Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(K)exp=0.17 {I5} for 151.1|g+152.4|g+154.0|g (1971Ga37) 
$L1/L2=2.9 {I8}, L1/L3=3.3 {I10}, L2/L3=1.2 {I5} (1971Ga37) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$ from 1980Sp01 
$ W(0|')-1=-0.004 {I15} 
$|a(K)exp=0.50 {I15}, 0.41 {I6}; |a(L1)exp=0.059 {I18}, 0.058 {I5} 
$L1/L2=7.8 {I8}, L1/L3>24, L2/L3>3 (1971Ga37) 
$ EKC=0.40 10 (1970Ag07) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_uncertain: S
decay_comment:
E,RI,M$ based on values in Adopted Levels, Gammas dataset. This most intense but lowest-energy transition is not reported in this decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
$|d(M2/E1)=+0.48 {I3}; |d(E3/E1)=-0.67 {I5} 
M,CC$59% {I4} E1, 14% {I1} M2 and 27% {I3} E3. Conversion coefficient deduced for this admixture 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
$|d(M2/E1)=+0.36 {I10}; |d(E3/E1)=-0.28 {I12} 
M,CC$81% {I5} E1, 12% {I4} M2 and 7% {I2} E3. Conversion coefficient deduced for this admixture from BrIcc code 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from IT decay (5.30 s). 47.07 {I10} from level energy difference in ({+14}C,|a3n|g). 
B(E2)(W.u.): from measured B(E2). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
Other E|g: 52.596 {I1} from |e decay, 52.73 {I10} from (n,n'|g), 52.52 {I5} from (n,|g) E=thermal. 
RI weighted average of 78 {I8} from |b{+-} decay, 83.1 {I26} from IT decay (5.30 s) and 81.5 {I21} from |e decay. Other I|g: 100.0 {I8} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
B(E2)(W.u.): from measured B(E2). 
Other E|g: 98.90 {I5} from (n,|g) E=thermal. All other data are consistent with adopted value. 
RI weighted average of 100 {I7} from |b{+-} decay, 100.0 {I26} from IT decay (5.30 s) and 100.0 {I18} from |e decay. Other: 90.5 {I9} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E in excellent agreement with 107.933 {I2} from |e decay, 107.91 {I3} from (n,n'|g) and 107.8 {I1} from ({+14}C,|a3n|g). Other E|g: 107.86 {I2} from (n,|g) E=thermal, 107.8 {I7} from (n,|g) E=4.1 eV. 
RI weighted average of 100 {I7} from |b{+-} decay, 100.0 {I16} from IT decay (5.30 s), 100.0 {I19} from |e decay, 100.0 {I7} from (n,|g) E=thermal. 
MR from |e decay. Other |d: -0.09 {I2} from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other E|g: 160.532 {I4} from |e decay, 160.63 {I10} from (n,|g) E=thermal, 160.39 {I4} from (n,n'|g), 161.0 {I1} from ({+14}C,|a3n|g). 
RI weighted average of 27.5 {I25} from (n,n'|g), 26.6 {I7} from |b{+-} decay, 27.0 {I3} from |e decay, 27.1 {I5} from IT decay (5.30 s). Others: 60 {I12} from ({+14}C,|a3n|g), 41.3 {I18} from (n,|g) E=thermal, 25.6 {I11} from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=AP;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=AP
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=AP;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=AP
decay_comment:
E unweighted average of 109.8 {I4} from ({+14}C,|a3n|g), 109.81 {I3} from (n,n'|g), 109.66 {I4} from (n,|g) E=thermal, 109.726 {I3} from |b{+-} decay, 109.731 {I2} from |e decay. The weighted average is 109.730 {I3}. 
RI unweighted average of 12.3 {I9} from (n,n'|g), 10.81 {I19} from (n,|g) E=thermal, 12.2 {I7} from |b{+-} decay, 12.42 {I20} from |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=AP;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=AP
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=AP;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=AP
decay_comment:
E weighted average of 162.3211 {I27} from |b{+-} decay and 162.330 {I5} from |e decay. Other E|g: 162.27 {I3} from (n,n'|g), 162.27 {I2} from (n,|g) E=thermal. 162.0 {I1} from ({+14}C,|a3n|g). 
RI from |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=AP;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=AP
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=AP;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=AP
decay_comment:
E unweighted average of 208.72 {I3} from (n,n'|g), 208.80 {I2} from (n,|g) E=thermal, 208.810 {I7} from |b{+-} decay, 208.812 {I2} from |e decay. The weighted average is 208.811 {I3}. Other E|g: 209.4 {I7} from (n,|g) E=4.1 eV, 209.8 {I1} from ({+14}C,|a3n|g). 
RI unweighted average of 12.6 {I12} from (n,n'|g), 12.31 {I13} from (n,|g) E=thermal, 12.5 {I5} from |b{+-} decay, 12.74 {I5} from |e decay. The weighted average is 12.68 {I7}. Other I|g: 13 {I7} from from (n,|g) E=4.1 eV, 17 from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E agrees well with 83.0 {I2} from ({+14}C,|a3n|g), 82.80 {I17} from (n,n'|g) and 82.919 {I2} from |e decay. 
RI unweighted average of 11.4 {I12} from |b{+-} decay, 9.2 {I7} from |e decay and 12.5 {I13} from (n,|g) E=thermal (the weighted average is 10.3 {I10}). Other I|g: 26 {I9} from (n,n'|g), 48 {I10} from ({+14}C,|a3n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E|g agrees well with 84.1 {I6} from ({+14}C,|a3n|g) and 84.712 {I2} from |e decay. 
RI average of 35.3 {I16} from |b{+-} decay and 30.7 {I16} from |e decay. Others: 68 {I25} from (n,n'|g), 28 {I7} from ({+13}C,|a3n|g), 46 {I4} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E agrees well with 192.63 {I6} from (n,n'|g), 192.65 {I7} from (n,|g) E=thermal, 192.646 {I7} from |e decay, 192.9 {I7} from (n,|g) E=4.1 eV. 
RI unweighted average of 9.3 {I20} from (n,n'|g), 8.7 {I3} from (n,|g) E=thermal, 9.4 {I3} from |b{+-} decay, 8.28 {I20} from |e decay; weighted average is 8.65 {I26}. Other I|g: 11 {I5} from (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E weighted average of 245.2 {I5} from (n,|g) E=thermal, 245.235 {I6} from |b{+-} decay, 245.243 {I6} from |e decay. Other: 245.6 {I7} from (n,|g) E=4.1 eV for doublet; presumed doublet (E|g=245.1 {I1}) in ({+14}C,|a3n|g). 
RI weighted average of 9.3 {I22} from (n,|g) E=thermal, 9.7 {I10} from |b{+-} decay, 8.0 {I8} from |e decay. Other: 8.9 in Coulomb excitation, 68 {I35} in (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
B(E2)(W.u.): from measured B(E2). 
Other E|g: 291.61 {I3} from (n,n'|g), 291.71 {I2} from (n,|g) E=thermal, 291.723 {I7} from |e decay, 291.8 {I7} from (n,|g) E=4.1 eV. Absent in ({+14}C,|a3n|g). 
RI from |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI unweighted average of 7.1 {I3} from |b{+-} decay, 6.6 {I6} from |e decay, 8.6 {I8} and 6.2 {I6} from Coulomb excitation (the weighted average is 7.0 {I3}). Others: 21 {I4} from (n,|g) E=thermal, 6.2 from (n,n'|g). 
MR from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Unweighted average of 209.867 {I4} from |b decay and 209.890 {I7} from |e decay. Other E|g: 209.7 {I1} from ({+14}C,|a3n|g), 209.80 {I3} from (n,n'|g), 209.86 {I4} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
Other E|g: 120.05 {I21} from (n,|g) E=thermal. 
Other I|g: 0.74 {I13} from |e decay, 0.84 {I17} from (n,|g) E=thermal 
MR from |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E weighted average of 203.22 {I6} from (n,n'|g), 203.284 {I8} from |b{+-} decay, 203.269 {I12} from |e decay, 203.28 {I5} from (n,|g) E=thermal. Other E|g: 203.1 {I1} from ({+14}C,|a3n|g). 
RI unweighted average of 18.1 {I5} from |b{+-} decay, 9.6 {I13} from |e decay, 6.04 {I17} from (n,|g) E=thermal, 15.7 {I23} from (n,n'|g). The weighted average is 7.4 {I21}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E unweighted average of 205.02 {I3} from (n,n'|g), 205.085 {I7} from |b{+-} decay, 205.081 {I9} from |e decay, 205.05 {I2} from (n,|g) E=thermal. Other E|g: 205.1 {I7} from (n,|g) E=4.1 eV. 
RI unweighted average of 30 {I5} from |e decay, 41.8 {I15} from |b{+-} decay, 23 {I11} from (n,|g) E=4.1 eV, 36 {I3} from (n,n'|g) (the weighted average is 39.7 {I23}). Other I|g: 13.01 {I17} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E,RI from |e decay. Other E|g: 313.005 {I30} from |b{+-} decay. Doublet in (n,n'|g) and (n,|g) E=thermal, and possibly in (n,|g) E=4.1 eV also. 
MR from |e decay. Other |d: +0.23 {I3} from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E weighted average of 365.62 {I10} from (n,n'|g), 365.644 {I30} from |b{+-} decay, 365.614 {I9} from |e decay, 365.61 {I5} from (n,|g) E=thermal, 365.5 {I2} from (n,|g) E=4.1 eV. 
RI unweighted average of discrepant data: 19.3 {I17} from |e decay, 22.9 {I19} from |b{+-} decay, 15.7 {I34} from (n,n'|g), 7.99 {I17} from (n,|g) E=thermal, 8.3 {I17} from(n,|g) E=4.1 eV (the weighted average is 8.2 {I9}). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=AP;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=AP
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=AP;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=AP
decay_comment:
Other E|g: 143.8 {I1} from ({+14}C,|a3n|g), 144.12 {I8} from (n,n'|g), 144.10 {I15} from (n,|g) E=thermal, 144.135 {I4} from |e decay and 143.0 {I7} from (n,|g) E=4.1 eV. 
RI weighted average of 9.0 {I19} from (n,n'|g), 10.5 {I9} from (n,|g) E=thermal, 9.4 {I3} from |b{+-} decay, 9.7 {I6} from |e decay. Other I|g: 15.3 {I12} from ({+14}C,|a3n|g) and 29 {I14} from (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=AP;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=AP
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=AP;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=AP
decay_comment:
Other E|g: 161.0 {I1} from ({+14}C,|a3n|g), 161.17 {I5} from (n,n'|g), 161.342 {I14} from |e decay. 
RI unweighted average of 33.4 {I13} from |b{+-} decay, 27 {I4} from |e decay, 56 {I5} from ({+14}C,|a3n|g), 64 {I6} from (n,n'|g) (weighted average is 35 {I5}). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
Other E|g: 245.1 {I1} from ({+14}C,|a3n|g) for multiplet, 244.26 {I4} from (n,n'|g), 244.24 {I13} from (n,|g) E=thermal, 244.266 {I3} from |e decay; 245.6 {I7} from (n,|g) E=4.1 eV for doublet. 
RI weighted average of 34 {I2} from (n,n'|g), 32.2 {I18} from (n,|g) E=thermal, 32.2 {I9} from |b{+-} decay, 31.2 {I7} from |e decay. Probable doublet in ({+14}C,|a3n|g) and (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
Other E|g: 245.94 {I3} from (n,n'|g), 246.04 {I8} from (n,|g) E=thermal, 246.062 {I2} from |e decay. 245.6 {I7} from (n,|g) E=4.1 eV for doublet; 245.1 {I1} from ({+14}C,|a3n|g) for presumed doublet. 
RI from |e decay and |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
Other E|g: 353.8 {I1} from ({+14}C,|a3n|g), 353.94 {I3} from (n,n'|g), 354.00 {I2} from (n,|g) E=thermal, 353.998 {I5} from |e decay and 353.9 {I2} from (n,|g) E=4.1 eV. 
RI unweighted average of 39 {I1} from (n,n'|g), 39.0 {I4} from (n,|g) E=thermal, 42.6 {I11} from |b{+-} decay, 40.8 {I7} from |e decay; other I|g: 24 {I12} from (n,|g) E=4.1 eV. And 30.7 {I25} from ({+14}C,|a3n|g) (weighted average =39.7 {I7}). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E weighted average of 406.612 {I23} from |b{+-} decay, 406.593 {I16} from |e decay and 406.65 {I21} from (n,n'|g); other E|g: 408.8 {I1} from ({+14}C,|a3n|g), 406.37 {I10} from (n,|g) E=thermal, 406.4 {I2} from (n,|g) E=4.1 eV. 
RI data are discrepant: 1.90 {I8} from |b{+-} decay, 2.5 {I6} from |e decay, 6.8 {I20} from (n,n'|g), 9.9 {I4} from (n,|g) E=thermal and 3.8 {I8} from (n,|g) E=4.1 eV; the unweighted average of these data is 5.0 {I15} (cf. weighted average =2.2 {I8}). E|g=408.8 {I1}, I|g=14.0 {I14} from ({+14}C,|a3n|g) suggests that |g may be complex there. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
Other E|g (I|g): 166.28 {I3} (115 {I12}) from (n,n'|g), 166.4 (76.3 {I15}) from Coulomb excitation. 
M,MR from Coulomb excitation; D+Q intraband |g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
Other E|g: 268.18 {I3} from (n,n'|g), 268.5 from Coulomb excitation, 268.0 {I3} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
Other E|g (I|g): 259.51 {I13} (100 {I7}) from (n,|g) E=thermal, 259.4 (100) from Coulomb excitation 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E,RI from (n,|g) E=thermal. Other E|g (I|g): 344.16 {I5} (52 {I9}) from (n,n'|g), 344.1 (49 {I3} from angular correlation; 57 from thick target yield) in Coulomb excitation. 
M,MR from Coulomb excitation; D+Q |g, |D|p from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g (I|g): weighted average of 452.18 {I4} (57 {I4}) from (n,n'|g) and 452.09 {I20} (63 {I7}) from (n,|g) E=thermal. Other: 452.0 (54 thick target yield; 68 {I5} from angular correlation) in Coulomb excitation). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Other E|g: 142.22 {I3} from (n,n'|g), 142.25 {I9} from (n,|g) E=thermal, 142.0 {I1} from ({+14}C,|a3n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E from (n,|g) E=thermal. 
RI average of 3.3 {I17} from (n,|g) E=thermal and 3.1 {I16} from |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E average of 313.28 {I3} from |b{+-} decay and 313.09 {I3} from (n,n'|g). Other E|g: 314.7 {I1} from ({+14}C,|a3n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E weighted average of 321.86 {I21} from (n,n'|g) and 322.1 {I1} from ({+14}C,|a3n|g). Other: 322.2 from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E from ({+14}C,|a3n|g). Other E|g (I|g): 153.98 {I10} (124 {I35}) from (n,n'|g) for doubly-placed |g; 153.8 {I19} (|?67) from (n,|g) E=thermal. Placement from ({+14}C,|a3n|g) and (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g, I|g, placement from (n,n'|g). E|g=467.5 {I9} in (n,|g) E=thermal with |g placed feeding the 9/2- 309 level; |g unobserved in ({+14}C,|a3n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
Other E|g (I|g); 219.4 (27 {I3}) from Coulomb excitation. 
M,MR from Coulomb excitation; D+Q intraband |g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI from (n,|g) E=4.1 eV. Other E|g (I|g): 451, I(451|g):I(857|g)=1.0|?:17 {I3} from (n,|g) E=4.1 eV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 611.3 (70 {I18}) from (n,|g) E=thermal: |g|g coin, 611.98 {I18} (20 {I5}) from (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 694.2 (100 {I21}) from (n,|g) E=thermal: |g|g coin, 695.69 {I18} (100 {I20}) for doublet in (n,n'|g), 695.4 {I2} (100 {I21}) from (n,|g) E=4.1 eV; absent in Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
B(E2)(W.u.): from measured B(E2). 
Other E|g (I|g): 903.0 (605 {I33}) from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 888.1 {I2} (100 {I19}) from (n,|g) E=4.1 eV, 887.5 (100 {I8}) from (n,|g) E=thermal: |g|g coin, 888.18 {I11} (100 {I10}) from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E E|g (I|g): weighted average of 587.29 {I13} (47 {I4}) from (n,|g) E=thermal and 587.49 {I9} (42 {I8}) from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 817.4 {I2} (12.3 {I25}) from (n,|g) E=4.1 eV, 817.1 (22.2 {I16}) from (n,|g) E=thermal: |g|g coin, 818.0 {I5} (22 {I5}) from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 927.2 {I2} (15 {I3}) from (n,|g) E=4.1 eV, 926.8 (7.2 {I4}) from (n,|g) E=thermal: |g|g coin, 927.8 {I6} (13 {I7}) from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 979.9 {I2} (60 {I12}) from (n,|g) E=4.1 eV, 979.4 (54.9 {I19}) from (n,|g) E=thermal: |g|g coin, 979.82 {I15} (66 {I13}) from (n,n'|g), 979.8 (45) from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
B(E2)(W.u.): from measured B(E2). 
Other E|g: 1026.4 {I2} (100 {I20}) from (n,|g) E=4.1 eV, 1025.9 (100.0 {I20}) from (n,|g) E=thermal: |g|g coin, 1026.19 {I13} (100 {I11}) from (n,n'|g), 1026.3 (100) from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): |?640.2 (9.1 {I18}) from (n,|g) E=4.1 eV, 640.8 for sole branch reported in Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 953.6 {I2} (12.1 {I24}) from (n,|g) E=4.1 eV, 953.29 {I16}, I(953|g):I(1006|g)=100 {I25}:53 {I18} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 941.09 {I3} (66.9 {I8}) from (n,|g) E=thermal, 942.8 (27) from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1099.9 (100 {I15}) from (n,|g) E=thermal: |g|g coin; possibly the E|g=1100.4 {I2} transition placed by 1973Ca02 from the 2127 level in (n,|g) E=4.1 eV; 1100.11 {I13} (100 {I18}) from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E from (n,n'|g). 
RI from (n,|g) E=thermal: |g|g. Other I|g: 48 {I21} from (n,n'|g), 20 {I9} from (n,|g) E=thermal, 19 from Coulomb excitation, 48 {I21} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1437.52 {I23} (100 {I12}) in (n,|g) E=thermal, 1437.8 {I4} (100 {I32}) from (n,n'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
Measured B(E2)|^=0.0034 {I4}. 
The sole branch seen in Coulomb excitation and |g is absent in other reaction studies, so placement shown as uncertain here. 
M E2 excitation in Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1262.9 {I4} (64 {I27}) from (n,n'|g), 1261.8 (48 {I6}) from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1423.2? 3 (100 {I27}) from (n,n'|g), 1424.1 (100 {I6}) from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
Measured B(E2)|^=0.018 {I2} from Coulomb excitation. 
Possibly the 1485.49|g placed from 3098 level in (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1346.9 (40 {I13}) from (n,|g) E=thermal: |g|g coin; 1347.6 (20) from Coulomb excitation 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
Other E|g (I|g): 1510.7 {I5} (100 {I30}) from (n,n'|g), 1509.2 (100 {I13}) from (n,|g) E=thermal: |g|g coin. 
B(E2)(W.u.): from measured B(E2). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
B(E2)(W.u.): from measured B(E2). 
Other E|g (I|g): 1557.4 {I5} (60 {I30}) from (n,n'|g), 1555.7 (169 {I15}) from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1565.6 (33 {I14}) from (n,|g) E=thermal: |g|g coin, and 1565.9 {I2} (49 {I25}) from (n,|g) E=4.1 eV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1612.1 (100 {I14}) from (n,|g) E=thermal: |g|g coin, and 1612.0 {I2} (100 {I51}) from (n,|g) E=4.1 eV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1528.9 (7.4 {I10}) from (n,|g) E=thermal: |g|g coin, 1528.6 {I3} (87 {I43}) from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1581.5 (19.5 {I24}) from (n,|g) E=thermal: |g|g coin, 1580.6 {I6} (80 {I41}) from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1628.0 (100 {I5}) from (n,|g) E=thermal: |g|g coin, 1627.13 {I22} (100 {I30}) from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1573.4 (8.1 {I9}) from (n,|g) E=thermal: |g|g coin, 1573.2 {I3} (104 {I30}) from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1626.0 (100 {I5}) from (n,|g) E=thermal: |g|g coin, 1627.2 {I2} (100 {I18}) from (n,|g) E=4.1 eV, 1627.13 {I22} (100 {I30}) from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1672.5 (23.8 {I26}) from (n,|g) E=thermal: |g|g coin and 1673.1 {I2} (11.4 {I23}) from (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1602.6 (100 {I7}) in (n,|g) E=thermal: |g|g coin, 1602.5 {I2} (100 {I20}) from (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1764.9 (71 {I5}) in (n,|g) E=thermal: |g|g coin, 1764.7 {I2} (87 {I18}) from (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1614.7 (100 {I4}) in (n,|g) E=thermal: |g|g coin, 1614.3 {I4} (100 {I50}) in (n,n'|g), 1615.3 {I2} (100 {I20}) in (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1885.5 {I2} (61 {I12}) from (n,|g) E=4.1 eV; 1884.0 from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1652.2 (4.0 {I14}) from (n,|g) E=thermal: |g|g coin, 1653.0 {I2} (29 {I14}) from (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1735.1 (100 {I4}) from (n,|g) E=thermal: |g|g coin, 1735.9 {I2} (100 {I19}) from (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1897.4 (16.3 {I15}) from (n,|g) E=thermal: |g|g coin, 1898.3 {I2} (24 {I5}) from (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1943.9 (2.6 {I13}) from (n,|g) E=thermal: |g|g coin, 1945.6 {I2} (14 {I3}) from (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1889.9 {I2} (100 {I21}) from {+182}W(n,|g) E=4.1 eV. 1890.1 (97 {I38}) from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2099.1 {I2} (88 {I18}) from {+182}W(n,|g) E=4.1 eV. 2098.9 (100 {I31}) from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 1917.1 from (n,|g) E=thermal: |g|g coin. 
RI weighted average of 10 {I4} from (n,|g) E=thermal and 15 {I6} from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2026.8 (4.4 {I16}) from (n,|g) E=thermal: |g|g coin. 
RI from (n,|g) E=thermal: |g|g; |?4 from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2080.8 {I2} (100 {I20}) in {+182}W(n,|g) E=4.1 eV; 2079.4 (100 {I8}) in (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2126.5 {I2} (46 {I24}) in {+182}W(n,|g) E=4.1 eV; 2125.9 (21 {I4}) from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2057.9 (100 {I33}) in (n,|g) E=thermal: |g|g for sole branch from this level seen in that study. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2117.0 (100 {I8}) in (n,|g) E=thermal: |g|g, 2119.2 {I2} (100 {I20}) from (n,|g) E=4.1 eV. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
RI 44 {I14} for |g that may partially or totally deexcite the 2231 level in (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2136.2 (33 {I8}) in (n,|g) E=thermal: |g|g. E|g=2133.8 also reported in (n,|g) E=thermal; |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Possibly the 2081.5|g reported in (n,|g) E=thermal: |g|g coin deexciting a 2373 level, so placement shown as uncertain here. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2447.4 (55 {I32}) from (n,|g) E=thermal: |g|g coin may be a doublet deexciting both the 2493 and 2494 levels. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
This is the only branch reported in (n,|g) E=thermal: |g|g coin so placement is shown here as uncertain. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
From (n,|g) E=thermal: |g|g coin only. I|g from I(2700|g)=19 {I3} and I(2700|g):I(2653|g)=100 {I27}:64 {I24} in (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI for possible doublet in (n,|g) E=thermal; |g absent in (n,|g) E=thermal: |g|g coin, so placement shown as tentative here. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Other E|g: 2804.7? from (n,|g) E=thermal: |g|g; placement from 1989Bo30, |g absent in 2005Su29, so placement considered uncertain.. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 2766.0 for sole branch reported in (n,|g) E=thermal: |g|g coin. 
E|g fits placement poorly. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 3422.42 {I19} (1993Pr09) in (n,|g) E=thermal; 3421.1 from (n,|g) E=thermal: |g|g coin, possibly for doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 3475.03 {I13} (1993Pr09) also in (n,|g) E=thermal, and 3475.1 from (n,|g) E=thermal; |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E for complex line. Other E|g: 3535.04 {I27} (1993Pr09) in (n,|g) E=thermal. And 3534.8 from (n,|g) E=thermal; |g|g coin. 
RI after correction for escape-peak contamination. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E|g=3579.15 {I7}, I|g=1.75 {I5} for complex line that probably feeds both the 2611 and 2613 levels in (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
Other E|g: 6190.78 {I6} from (n,|g) E=thermal: |g|g coin; 6193 {I3} from (n,|g) E=4.1 eV. 
M from (pol n,|g); strength in (n,|g) E=thermal favors E1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M L1/L2=6.8 {I4}, L2/L3=15.6 {I11}, L2/L3=2.30 {I25}, M1/M2=6.5 {I6}, M1/M3=14.6 {I14}, M2/M3=2.2 {I3} (1970Ag06); L1:L2:L3:M:N=3000:490:220:950:280 (1962Ha24); L1:L2:M1:M2:M3:N:O=180 {I20}:26 {I3}:12 {I2}:42 {I4}:7.0 {I10}:3.5 {I5}:10 {I1}:2.0 {I3}, |a(L1)exp=5.1 {I6} (1980Ar22). 
%I|g=8.0 {I3} assuming adopted decay scheme normalization. 
MR 0.084 {I13} from subshell ratios from 1980Ar22; -0.05 {I8} from |g|g(|q) (1973Kr01). Other: |<0.45 from |a(L1)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M L1/L2=5.3 {I4}, L2/L3=8.6 {I7}, L2/L3=1.60 {I17} (1970Ag06); L1:L2:L3:M:N=870:155:100:260:65 (1962Ha24), L1:L2:L3:M1:M2:M3:N:O=36 {I3}:7.0 {I7}:4.2 {I4}:8.5 {I8}:2.5 {I4}:1.0 {I2}:2.1 {I2}, |a(L1)exp=3.6 {I3} (1980Ar22). 
MR 0.127 {I21} from subshell ratios from 1980Ar22; -0.16 {I9} from |g|g(|q) (1973Kr01); <0.36 from |a(L1)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M K:L1:L2:L3:M:N=175:18:270:240:120:30 (1962Ha24); K:L1:L2:L3=10.6 {I15}:1.1 {I1}:14.3 {I6}:13.4 {I5}, |a(L2)exp=1.19 {I7} (1980Ar22). 
|d(M1,E2)>3.5 from |a(L2)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M K:L1:M:N=470:70:19:|?6 (1962Ha24); |a(K)exp=3.0 {I3} (1980Ar22). 
Other |d: -0.22 {I10} (1973Kr01); <0.49 from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M K:L1:L2:M=530:80:10:20 (1962Ha24); |a(K)exp=3.0 {I3} (1980Ar22). 
Other |d: 0.09 {I+32-9} from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI from 1977Br22. 
M K:L1:L2:L3:M:N=1300:220:|?45:21:58:17 (1962Ha24); |a(K)exp=0.960 {I20} (1980Ar22). 
MR sign from 1973Kr01; 0.22 {I8} from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M K:L1:M:N=100:18:4.8:1.3 (1962Ha24); |a(K)exp=0.46 {I4} (1980Ar22). 
Other |d: -0.29 {I4} (1973Kr01); 0.32 {I+20-32} from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI unweighted average of 8.0 {I1} (1977Br22), 10.4 {I4} (1974TaZX), 9.3 {I6} (1972Br55). 
M K:L1:L2:M= >50:27:27: |?12 (1962Ha24); L1:L2=1.0 {I2}:0.75 {I14}, |a(L1)exp=0.76 {I16} (1980Ar22). 
RI unweighted average of 27.5 {I6} (1977Br22), 32 {I2} (1974TaZX), 9.3 {I6} (1972Br55). 
MR sign from |g|g(|q) 1973Kr01, magnitude from analysis of earlier ce data by 1973Kr01; 0.6 {I3} from |a(L1)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M K:L1:L2:L3:M:N=>250:<120:9:|?5:20:5 (1962Ha24); L1:L2=3.8 {I5}:0.5 {I1}, |a(L1)exp=0.87 {I12} (1980Ar22). 
Other |d: 0.25 {I+27-25} from |a(L1)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M K:L1:L2:L3:M=8:1.6:|?0.5:|?0.3:0.5 (1962Ha24); |a(K)exp=0.51 {I9} (1980Ar22). 
Other |d: 0.6 {I3} from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI weighted average from 1977Br22 and 1974TaZX. 
M K:L1=|?6: |?0.8 (1962Ha24); |a(K)exp=0.31 {I8} (1980Ar22). 
MR |<0.8 from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI weighted average from 1977Br22 and 1974TaZX. 
M K:L3=2.4:<1.4 (1962Ha24); |a(K)exp=0.146 {I26} (1980Ar22). 
|d(M1,E2)|>3.8. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI unweighted average of 3.5 {I1} (1977Br22), 5 {I1} (1974TaZX), 3.2 {I2} (1974TaZX). 
M K:L1=3.8<0.8, M weak (1962Ha24); |a(K)exp=0.51 {I6} (1980Ar22). 
MR 0.13 {I+34-13} from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI from 1977Br22. 
M L1:M1=0.98 {I25}:0.22 {I5}, |a(L1)exp=9 {I3} (1980Ar22). 
|d(M1,E2)|<0.6 from |a(L1)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI unweighted average of 3.66 {I7} (1977Br22), 4 {I1} (1974TaZX), 4.5 {I3} (1974TaZX). 
M K:L1=13:1.9, L2 weak (1962Ha24); |a(K)exp=1.44 {I19} (1980Ar22). 
MR from |g|g(|q) (1973Kr01). Other: |<0.40 from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
RI from 1977Br22. Other I|g: 22 {I3} from 1974TaZX. 
M K:L1=24:<9 (1962Ha24); |a(K)exp=0.66 {I19} (1980Ar22). 
MR 1.0 {I+8-4} from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI weighted average from 1977Br22 and 1974TaZX. 
M K:L1=29:<5.4 (1962Ha24); |a(K)exp=0.31 {I3} (1980Ar22). 
Other |d: |<0.42 from |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E from 2014Hu02. Transition used as gate in |g|g coin measurements by 1993Pr09, but E|g not stated there. 
TI |>(I(|g+ce) to 47 level)=22.3%. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
Other E|g (I|g): 99.09 {I1} (3754 {I198}) (1993Pr09); 98.94 {I9} (2007ChZX), 98.90 {I1} (1668 {I59}) (2014Hu02). Unweighted average E|g from 2014Hu02, 2011Bo09 and 1993Pr09 is 99.00 {I5}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
Other E|g (I|g): 160.67 {I2} (759 {I125}) for multiplet (1993Pr09); 160.39 {I11} (348 {I22}) (2007ChZX); 160.36 {I5} (485 {I30}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 109.74 {I1} (1154 {I73}) (1993Pr09); 109.63 {I12} (365 {I29}) (2007ChZX); 109.55 {I5} (552 {I29}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 162.32 {I1} (6864 {I728}; corrected for background |g contaminant) (1993Pr09); 162.21 {I9} (3409 {I91}) (2007ChZX); 162.11 {I5} (4795 {I132}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 208.81 {I1} (562 {I31}) (1993Pr09); 208.81 {I11} (397 {I44}) (2007ChZX); 208.64 {I5} (560 {I21}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 192.62 {I2} (104 {I10}) (1993Pr09); 192.79 {I25} (62 {I20}) (2007ChZX); 192.49 {I5} (102 {I5}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
Other E|g (I|g): 291.68 {I4} (1040 {I52}) (1993Pr09); 291.64 {I9} (848 {I35}) (2007ChZX); 291.57 {I5} (1224 {I45}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E from level energy difference. E|g=17.2 {I2} in 2014Hu02 probably deduced similarly because |g was not, in fact, observed. 
RI from 2014Hu02 for unobserved |g; existence proposed based on DICEBOX statistical model calculations alone. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
Other E|g (I|g): 209.88 {I1} (333 {I21}) (1993Pr09); 209.79 {I16} (204 {I42}) (2007ChZX); 209.69 {I5} (369 {I14}) (2014Hu02). 


decay_energy_unit: KEV
decay_comment:
E from Adopted Gammas; not resolved by 2014Hu02 from 102|g or from a 101.8|g arising from the {+186}W target impurity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement from 1997Pr02. 2011Bo09 report only E|g=102.2 {I3}, placed (as in (n,n'|g)) from 309 level. Implied branchings for both placements exceed adopted values so observed transitions may be complex. |g absent in 2007ChZX and a multiplet in 2014Hu02 (with component energies assumed from the literature) and I|g(doublet)=51 {I9}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Presumably deexcites 623 level also, as in Adopted Levels, Gammas. 
Other E|g (I|g): 313.06 {I5} (1290 {I62}) (1993Pr09); 313.14 {I9} (985 {I73}) (2007ChZX); 313.02 {I5} (1600 {I88}) for doublet in 2014Hu02. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 365.56 {I8} (99 {I6}) (1993Pr09); 365.44 {I11} (283 {I27}) (2007ChZX); 365.39 {I5} (138 {I8}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 244.26 {I2} (177 {I10}) (1993Pr09); 244.13 {I14} (193 {I18}) (2007ChZX); 244.25 {I5} (226 {I10}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 246.06 {I2} (562 {I31}) (1993Pr09); 245.92 {I10} (514 {I22}) (2007ChZX); 245.88 {I5} (521 {I26}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 406.55 {I27} (43 {I3}) for doublet (1993Pr09); 405.8 {I3} (78 {I26}) (2007ChZX); 406.23 {I7} (55 {I5}) (2014Hu02). 1997Pr02 estimate I|g=8 for this placement. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 268.29 {I10} (16 {I3}) (1993Pr09); 268.7 {I3} (57 {I22}) (2007ChZX); 267.92 {I18} (21 {I5}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 453.0 {I5} (20 {I3}) (1993Pr09); 451.62 {I14} (2007ChZX); 452.37 {I9} (25 {I3}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 142.24 {I2} (146 {I31}) (1993Pr09); 141.3 {I3} (137 {I27}) (2007ChZX); 142.11 {I5} (85 {I5}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI reported by 2014Hu02 for unobserved transition; E|g and branching taken by authors from the literature. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E 312.72 {I5} (1600 {I88}) for doublet (2014Hu02). 
Placement from 2014Hu02; see comment on 313|g from 412 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(695|g)=6 {I2}:100 {I3} (2011Bo09). 
Other E|g (I|g): 491.9 {I5} (11 {I3}) (1993Pr09; I|g corrected for background |g); 365.44 {I11} (283 {I27}) (2007ChZX). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI from I|g:I(888|g)|?1:100 {I2} in table 2 and I(888|g) in table 1 of 2011Bo09. 
E|g=726.2 {I4}, I|g=15 {I2} for complex line (2011Bo09). 
Other E|g (I|g): 725.78 {I22} (12 {I4}) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Other E|g (I|g): 707.74 {I7} (74 {I6}) (1993Pr09); 706.42 {I11} (839 {I55}) (2007ChZX; |g appears to be contaminated and/or misplaced). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g=817.49 {I4}, I|g=358 {I5} in table 1 for complex line dominated by this placement (2011Bo09). 
Other E|g (I|g): 817.59 {I5} (374 {I52}) (1993Pr09). 
RI from I|g:I(1026|g)=11.1 {I6}:100.0 {I8} in table 2 and I(1026|g) in table 1 of 2011Bo09. This leaves I|g=39 {I18} to be placed from 1229 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1026|g)=16.3 {I3}:100.0 {I8} (2011Bo09). 
Other E|g (I|g): 927.30 {I4} (447 {I21}) (1993Pr09); 927.04 {I9} (438 {I22}) (2007ChZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1026|g)=61.5 {I7}:100.0 {I8} (2011Bo09). 
Other E|g (I|g): 979.87 {I3} (1747 {I94}) (1993Pr09); 979.58 {I9} (1896 {I73}) (2007ChZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 640.83 {I10} (24 {I3}) (1993Pr09); 
E|g=641.3 {I6} from table 1 of 2011Bo09. 
I|g:I(846|g)=9 {I1}:100 {I1} (2011Bo09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(846|g)=15 {I3}:100 {I1} (2011Bo09). 
Other E|g (I|g): 953.9 {I5} (63 {I17}) (1993Pr09); 955.0 {I6} (109 {I73}) (2007ChZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(846|g)=14 {I2}:100 {I1} (2011Bo09). 
Placement taken from table 2 of 2011Bo09. 
Other E|g (I|g): 1007.3 {I15} (29 {I19}) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement taken from 1997Pr02 and table 2 of 2011Bo09. 
Other E|g (I|g): 657.14 {I14} (16 {I3}) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g=696.78 {I3}, I|g=478 {I5} in table 1 for complex line dominated by this placement (2011Bo09). 
RI see comment on 697|g from 1320 level. 
Other E|g (I|g): 696.71 {I7} (510 {I21}) (1993Pr09); 696.56 {I10} (552 {I44}) (2007ChZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(697|g)=34 {I6}:100 {I12} (2011Bo09). 
Other E|g (I|g): 1149.88 {I17} (85 {I12}) (1993Pr09); 1151.0 {I5} (108 {I46}) (2007ChZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 802.90 {I17} (21 {I3}) (1993Pr09). 
Placement tentative in 2011Bo09 but definite in 1997Pr02. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(776|g)=44 {I5}:100 {I5} (2011Bo09). 
E|g=817.49 {I4}, I|g=358 {I5} in table 1 of 2011Bo09 for complex line. 
RI see comment on 817|g from 1026 level. 


decay_energy_unit: KEV
decay_comment:
E|g=652.22 {I2}, I|g=406 {I3} in table 1 for complex line that primarily deexcites the 1275 level. The adopted E|g is presumably from coincidence data, although table 2 of 2011Bo09 does not indicate this. 
Other E|g (I|g): 652.11 {I6} (426 {I21}) (1993Pr09). Placed by 1997Pr02 from an otherwise unknown 1064 level. Coincident with 313|g (1993Pr09, 1997Pr02, 2011Bo09). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI from I|g:I(1101|g)=9 {I4}:100 {I8} in table 2 and I(1101|g) in table 1 of 2011Bo09. 
Other E|g (I|g): 406.55 {I27} (43 {I3}) for doublet (1993Pr09). 1997Pr02 estimate I|g=31 for this placement. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1101|g)=63 {I7}:100 {I8} (2011Bo09). 
Other E|g (I|g): 1018.07 {I15} (302 {I31}) (1993Pr09). Placed by 1997Pr02 from an otherwise unknown 1064 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1100.74 {I7} (530 {I31}) (1993Pr09); 1100.21 {I14} (438 {I91}) (2007ChZX). |g indicated as a multiplet by 1997Pr02 but not by 1993Pr09; no alternative placement(s) given. 1997Pr02 estimate I|g=129 for this placement. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1101|g)=19 {I6}:100 {I8} (2011Bo09). 
Other E|g (I|g): 1210.80 {I14} (90 {I16}) (1993Pr09); 1210.19 {I23} (140 {I36}) (2007ChZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g=1261.2 {I12}, I|g=52 {I23} in table 1 for complex line (2011Bo09) 
RI from I|g/I(1101|g)=20 {I8}:100 {I8} in table 2 and I|g(1101|g) of 2011Bo09 this leaves no I|g for placement elsewhere. 
Other E|g (I|g): 1262.55 {I7} (322 {I21}) for doublet (1993Pr09); 1997Pr02 estimate I|g=38 for this placement. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g=696.78 {I3}, I|g=478 {I5} in table 1 for complex line (2011Bo09). 
RI from I|g:I(867|g)=76 {I14}:100 {I3} in table 2 and I(867|g) of 2011Bo09. This leaves I|g=402 {I20} for placement from 1150 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1289|g)=11 {I2}:100 {I4} (2011Bo09). 
Other E|g (I|g): 400.86 {I25} (30 {I3}) (1993Pr09). Tentatively placed by 1997Pr02 from 1551 level but placement not adopted. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1289|g)=42 {I4}:100 {I4} (2011Bo09). 
Other E|g (I|g): 1235.53 {I15} (94 {I9}) (1993Pr09); may include 1233.7|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1163|g)=89 {I3}:100 {I4} (2011Bo09). 
Other E|g (I|g): 959.97 {I25} (125 {I21}) (1993Pr09); 959.8 {I3} (190 {I40}) (2007ChZX). 


decay_energy_unit: KEV
decay_comment:
I|g:I(1163|g)=9 {I3}:100 {I4} (2011Bo09). 
Other E|g (I|g): 1064.0 {I6} (50 {I18}) for doublet (1993Pr09). Placed instead by 1997Pr02 from an otherwise unknown 1064 level. 


decay_energy_unit: KEV
decay_comment:
I|g:I(781|g)=27 {I8}:100 {I9} (2011Bo09). 
E|g=753.4 {I9}, I|g=9 {I3} in table 1 of 2011Bo09. 
Other E|g (I|g): 753.15 {I22} (8 {I3}) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
E|g=781.3 {I3}, I|g=34 {I3} in table 1 of 2011Bo09. 
Other E|g (I|g): 781.00 {I8} (32 {I4}) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(781|g)=38 {I16}:100 {I9} (2011Bo09). 
E|g=1066.7 {I5}, I|g=52 {I7} in table 1 of 2011Bo09. 
Other E|g (I|g): 1066.8 {I7} (40 {I16}) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1438|g)=42 {I6}:100 {I12} (2011Bo09). 
Other E|g (I|g): 1338.2 {I3} (92 {I9}) (1993Pr09). |g indicated as a multiplet by 1997Pr02 but not by 1993Pr09; no alternative placement(s) given. 
Placement from table 2 of 2011Bo09. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1417|g)=80 {I10}:100 {I12} (2011Bo09). 
Other E|g (I|g): 1463.58 {I7} (374 {I21}) for doublet (1993Pr09). 1997Pr02 estimate I|g=156 for this placement. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 320.97 {I8} (77 {I5}) (1993Pr09); may include 320.0|g. 
I|g:I(1425|g)=18 {I2}:100 {I4} (2011Bo09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1425|g)=44 {I3}:100 {I4} (2011Bo09). 
Other E|g (I|g): 1262.55 {I7} (322 {I21}) for doublet (1993Pr09), I|g=164 estimated for this placement by 1997Pr02; 1262.37 {I18} (328 {I44}) (2007ChZX). May include 1262.1|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1424.26 {I5} (489 {I31}) (1993Pr09); 1423.97 {I14} (620 {I55}) (2007ChZX; possibly for 1422.5|g+1424.6|g doublet). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1425|g)=32 {I7}:100 {I4} (2011Bo09). 
Other E|g (I|g): 1470.93 {I11} (239 {I21}) (1993Pr09), 1471.1 {I4} (201 {I73}) (2007ChZX); possibly for 1470.8+1471.5|g doublet). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1343.5 {I4} (78 {I11}) (1993Pr09). Placement is shown in parentheses in table 1 of 2011Bo09, but shown as definite by 1997Pr02. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1510|g)=8 {I3}:100 {I6} (2011Bo09). 
Other E|g (I|g): 326.55 {I8} (23 {I4}; I|g corrected for background |g) (1993Pr09); 325.50 {I25} (71 {I31}) (2007ChZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1510|g)=21 {I4}:100 {I6} (2011Bo09). 
Other E|g (I|g): 1262.55 {I7} (322 {I21}) for doublet (1993Pr09; 1997Pr02 estimate I|g=120 for this placement. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1510|g)=19 {I4}:100 {I6} (2011Bo09). 
E|g=1348.1 {I5}, I|g=58 {I22} from table 1. 
Other E|g (I|g): 1347.6 {I3} (99 {I11}) (1993Pr09; possibly for 1347|g to 1348|g multiplet); 1347.19 {I25} (346 {I44}) (2007ChZX; apparently for contaminated |g). 


decay_energy_unit: KEV
decay_comment:
E|g=1510.35 {I12}, I|g=350 {I30} in table 1 for complex line (2011Bo09). 
Other E|g (I|g): 1510.17 {I6} (530 {I31}) (1993Pr09); 1510.17 {I25} (419 {I55}) (2007ChZX; possible contribution from 1509|g and/or 1513|g. Fits placement poorly. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1510|g)=94 {I6}:100 {I6} (2011Bo09). 
Other E|g (I|g): 1555.69 {I12} (322 {I31}) (1993Pr09); 1555.60 {I25} (255 {I55}) (2007ChZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g=1158.3 {I4}, I|g=17 {I3} in table 1 for complex line (2011Bo09). 
RI from I|g:I(1570|g)=6 {I3} in table 2 and I(1570|g). This leaves I|g=3 {I8} for placement elsewhere. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1570|g)=15 {I3}:100 {I5} (2011Bo09). 
Other E|g (I|g): 1363.0 {I5} (43 {I14}) (1993Pr09); possibly for 1361|g to 1364|g multiplet. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1587|g)=37 {I10}:100 {I23} (2011Bo09). 
Other E|g (I|g): 1294.37 {I9} (146 {I21}; I|g corrected for background-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI from I|g:I(1587|g)|?17:100 {I23} in table 2 and I(1587|g) in table 1 of 2011Bo09. 
E|g=1540.5 {I9}, I|g=40 {I20} in table 1 for complex line (2011Bo09). 
Other E|g (I|g): 1539.5 {I4} (30 {I8}; I|g corrected for escape-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1587.32 {I24} (229 {I21}) (1993Pr09); may include 1589.8|g. Placed by 1997Pr02 from 1633 level. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1612|g)|?1:100 {I5} (2011Bo09). 
Other E|g (I|g): 723.83 {I13} (9 {I4}; corrected for background contribution) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1612|g)=30 {I2}:100 {I5} (2011Bo09). 
Other E|g (I|g): 1529.28 {I13} (229 {I21}) (1993Pr09); presumably for 1529|g+1530|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1627.09 {I5} (1331 {I73}) for doublet (1993Pr09); presumably for 1626|g+1628|g doublet. 1997Pr02 estimate I|g=770 for this placement. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1661|g)=49 {I16}:100 {I16} (2011Bo09). 
Placement from table 2. E|g=1615.06 {I7} (I|g=669 {I36}) from table 1 primarily deexcites the 1824 level (2011Bo09). 
Other E|g (I|g): 1615.13 {I9} (905 {I52}) (1993Pr09); probably for 1615|g to 1617|g multiplet. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1618|g)=26 {I8}:100 {I15} (2011Bo09). 
E|g=1455.3 {I8}, I|g=69 {I22} in table 1 of 2011Bo09. 
Other E|g (I|g): 1455.81 {I15} (166 {I21})for multiplet (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(1626|g)=11 {I2}:100 {I3} (2011Bo09). 
Other E|g (I|g): 1463.58 {I7} (374 {I21}) for doublet (1993Pr09); presumably the 1464|g+1466|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1627.09 {I5} (1331 {I73}) for doublet (1993Pr09); presumably for 1626|g+1628|g doublet. 1997Pr02 estimate I|g=562 for this placement. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1726|g)=10 {I2}:100 {I4} (2011Bo09). 
E|g=575.7 {I4}, I|g=17 {I3} in table 1 of 2011Bo09. 
Other E|g (I|g): 575.42 {I10} (18 {I3}) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(1684|g)=16 {I5}:100 {I5} (2011Bo09). 
E|g=1439.10 {I24}, I|g=93 {I23} in table 1 of 2011Bo09. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1684|g)=53 {I6}:100 {I5} (2011Bo09). 
Other E|g (I|g): 1633.07 {I20} (291 {I31}) (1993Pr09); probably for 1632|g+1634|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1615|g)=5 {I1}:100 {I3} (2011Bo09). 
Other E|g (I|g): 1823.5 {I5} (59 {I4}) (1993Pr09); possibly for 1821|g+1824|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1625|g)=27 {I8}:100 {I21} (2011Bo09). 
Other E|g (I|g): 1830.8 {I5} (48 {I15}) (1993Pr09); possibly for 1830|g+1831|g+1834|g multiplet. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1629|g)=57 {I25}:100 {I25} (2011Bo09). 
E|g=1545.3 {I3}, I|g=55 {I7} in table 1 for complex line that primarily deexcites the 2482 level (2011Bo09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(1629|g)=72 {I27}:100 {I25} (2011Bo09). 
E|g=1837.32 {I15}, I|g=173 {I5} in table 1 of 2011Bo09 for complex line. 
Other E|g (I|g): 1837.35 {I10} (250 {I31}) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(1870|g)=5 {I3}:100 {I7} (2011Bo09). 
Other E|g (I|g): 559.91 {I6} (47 {I4}) (1993Pr09). Placed by 1997Pr02 from1463 level. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1595|g)=11 {I2}:100 {I3} (2011Bo09). 
E|g=1676.3 {I6}, I|g=25 {I6} in table 1 of 2011Bo09. 
Other E|g (I|g): 1677.5 {I3} (68 {I9}) (1993Pr09); probably for 1677|g+1678|g doublet. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1595|g)=18 {I2}:100 {I3} (2011Bo09). 
E|g=1884.8 {I3}, I|g=88 {I5} in table 1 of 2011Bo09. 
Other E|g (I|g): 1885.07 {I25} (146 {I21}) (1993Pr09) 


decay_energy_unit: KEV
decay_comment:
I|g:I(1692|g)=8 {I3}:100 {I12} (2011Bo09). 
E|g=995.62 {I8}, I|g=73 {I3} in table 1 for unplaced |g (2011Bo09). 
Other E|g (I|g): 995.9 {I8} (51 {I22}) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1691.44 {I5} (395 {I21}) (1993Pr09) |g indicated as a doublet by 1997Pr02 but not by 1993Pr09. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1692|g)=36 {I10}:100 {I12} (2011Bo09). 
Other E|g (I|g): 1853.7 {I4} (125 {I21}) (1993Pr09); possibly for 1853|g+1854|g doublet. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1692|g)=12 {I7}:100 {I12} (2011Bo09). 
E|g=1901.1 {I4}, I|g=35 {I6} in table 1 for complex line (2011Bo09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1736|g)=4 {I2}:100 {I2} (2011Bo09). 
Other E|g (I|g): 473.9 {I5} (22 {I3}) (1993Pr09); 474.60 {I8} (2007ChZX). Placed from 1069 level by 1997Pr02 and 2007ChZX. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1736|g)=5 {I1}:100 {I2} (2011Bo09). 
E|g=1652.33 {I8}, I|g=234 {I6} in table 1 for complex line (2011Bo09). 
Other E|g (I|g): 1652.59 {I8} (250 {I21}) (1993Pr09); may include 1654.9|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1735.63 {I4} (863 {I42}) (1993Pr09) for doublet. 1997Pr02 estimate I|g=686 for this placement. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1736|g)=8 {I2}:100 {I2} (2011Bo09). 
Other E|g (I|g): 1944.46 {I18} (146 {I31}) (1993Pr09) for doublet. 1997Pr02 estimate I|g=58 for this placement. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1918|g)=35 {I10}:100 {I8} (2011Bo09). 
Other E|g (I|g): 1962.5 {I4} (52 {I25}; I|g corrected for escape-peak contamination) (1993Pr09); apparently includes a contaminant. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1691|g)=15 {I5}:100 {I16} (2011Bo09). 
E|g=834.2 {I11}, I|g=31 {I20} in table 1 of 2011Bo09. 
Other E|g (I|g): 834.53 {I16} (36 {I8}) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1691|g)=38 {I5}:100 {I16} (2011Bo09). 
Other E|g (I|g): 1935.2 {I4} (73 {I22}) (1993Pr09); probably for 1933|g+1936|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1691|g)=90 {I16}:100 {I16} (2011Bo09). 
Other E|g (I|g): 1982.41 {I23} (208 {I21}; I|g corrected for escape-peak contamination) (1993Pr09); probably for 1982|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1699|g)=58 {I15}:100 {I15} (2011Bo09). 
Other E|g (I|g): 1782.68 {I24} (94 {I12}) (1993Pr09); may include 1784|g. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI from I|g:I(1699|g)|?13:100 {I15} in table 2 and I(1699|g) in table 1 of 2011Bo09. 
Other E|g (I|g): 1890.96 {I25} (146 {I21}) (1993Pr09) for doublet. 1997Pr02 estimate I|g=83 for this placement. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(1699|g)=54 {I13}:100 {I15} (2011Bo09). 
Other E|g (I|g): 1989.5 {I4} (76 {I18}: I|g corrected for escape-peak contaminant) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(2029|g)=46 {I7}:100 {I6} (2011Bo09). 
Other E|g (I|g): 1735.63 {I4} (863 {I52}) (1993Pr09) for doublet. 1997Pr02 estimate I|g=177 for this placement. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1851|g)=10 {I6}:100 {I7} (2011Bo09). 
E presumably from coincidence data, but not so indicated in table 2. E|g=1158.3 {I4}, I|g=17 {I3} in table 1 for complex line that primarily deexcites a 1570 level (2011Bo09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(1851|g)=50 {I6}:100 {I7} (2011Bo09). 
E|g=2059.0 {I7}, I|g=71 {I10} in table 1 for complex line (2011Bo09). 
Other E|g (I|g): 2058.6 {I5} (87 {I18}) (1993Pr09); possibly for 2057|g+2059|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from I|g:I(2092|g)=100 {I30}:60 {I30} in table 2 and I(2092|g) in table 1 of 2011Bo09. 
E|g=2045.04 {I18}, I|g=66 {I5} in table 1 of 2011Bo09. 
Other E|g (I|g): 2045.0 {I5} (59 {I17}) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(1891|g)=16 {I11}:100 {I15} (2011Bo09). 
Other E|g (I|g): 1164.28 {I9} (198 {I42}) for multiplet (1993Pr09); probably for 1163.4|g to 1165.4|g multiplet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1890.96 {I25} (146 {I21}) for doublet (1993Pr09). 1997Pr02 estimate I|g=6.2 for this placement. 


decay_energy_unit: KEV
decay_comment:
I|g:I(1891|g)=34 {I16}:100 {I15} (2011Bo09). 
Other E|g (I|g): 2099.8 {I7} (40 {I17}) (1993Pr09); probably for 2099|g+2101|g. 


decay_energy_unit: KEV
decay_comment:
E presumably from coincidence data, but not so indicated in table 2; E|g=1057.1 {I11}, I|g=24 {I5} from table 1 of 2011Bo09. 
I|g:I(2080|g)=10 {I3}:100 {I4} (2011Bo09). 
Other E|g (I|g): 1057.6 {I3} (34 {I7}) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
E presumably from coincidence data, but not so indicated in table 2. Possibly the unplaced E|g=1192.0 {I3}, I|g=83 {I20} line from table 1 of 2011Bo09. 
I|g:I(2080|g)=8 {I3}:100 {I4} (2011Bo09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(2080|g)=27 {I4}:100 {I4} (2011Bo09). 
Other E|g (I|g): 2124.7 {I3} (99 {I12}) (1993Pr09); possibly includes 2124|g. 


decay_energy_unit: KEV
decay_comment:
I|g:I(2118|g)=6 {I2}:100 {I3} (2011Bo09). 
E|g=1138.4 {I4}, I|g=13 {I4} in table 1 for complex line (2011Bo09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(2118|g)=30 {I3}:100 {I3} (2011Bo09). 
Other E|g (I|g): 1957.06 {I21} (125 {I31}) (1993Pr09). May include 1959|g. I|g corrected for escape-peak contamination. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI from I|g:I(895|g)|?10:100 {I13} in table 2 and I(895|g) in table 1 of (2011Bo09). 
Other E|g (I|g): 895.7 {I15} (19 {I10}) (1993Pr09). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI from I|g:I(895|g)=16 {I6}:100 {I13} in table 2 and I(895|g) in table 1 of (2011Bo09). 
Other E|g (I|g): 2072.40 {I21} (70 {I17}; I|g corrected for escape-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(2177|g)=3 {I1}:100 {I3} (2011Bo09). 
E|g=713.4 {I11}, I|g=18 {I7} in table 1 of 2011Bo09. 
Other E|g (I|g): 713.30 {I10} (23 {I3}) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(2177|g)=5 {I2}:100 {I3} (2011Bo09). 
Other E|g (I|g): 1885.07 {I25} (146 {I21}) (1993Pr09); probably for 1885|g+1888|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(2177|g)=14 {I2}:100 {I3} (2011Bo09). 
Other E|g (I|g): 1967.8 {I3} (135 {I31}) (1993Pr09); apparently includes a contaminant. 


decay_energy_unit: KEV
decay_comment:
I|g:I(2022|g)=27 {I10}:100 {I14} (2011Bo09). 
Other E|g (I|g): 2184.03 {I9} (239 {I21}) (1993Pr09). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI from I|g:I(901|g)=13 {I8}:16 {I6} in table 2 and I(901|g) in table 1 of 2011Bo09. 
Other E|g (I|g): 1944.46 {I18} (146 {I31}) for doublet (1993Pr09). 1997Pr02 estimate I|g=83 for this placement. 


decay_energy_unit: KEV
decay_comment:
I|g:I(2137|g)=83 {I10}:100 {I8} (2011Bo09). 
Other E|g (I|g): 2236.17 {I14} (260 {I21}) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(2202|g)=15 {I3}:100 {I5} (2011Bo09). 
E|g=2249.65 {I19}, I|g=56 {I8} in table 1 for complex line (2011Bo09). 
Other E|g (I|g): 2249.0 {I5} (69 {I14}) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(2266|g)=32 {I8}:100 {I14} (2011Bo09). 
2011Bo09 report that this |g deexcites a 2066 level, but E|g does not fit that placement; E(level) is presumably misprinted and should have been 2266 instead (consistent with table 2 of 2011Bo09). 
Other E|g (I|g): 1975.03 {I4} (73 {I42}) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
E|g=1993.2 {I5}, I|g=28 {I7} in table 1 for complex line (2011Bo09). 
I|g:I(1133|g)=9 {I3}:24 {I5} (2011Bo09). 
Other E|g (I|g): 1993.4 {I8} (46 {I14}) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(1133|g)=6 {I4}:24 {I5} (2011Bo09). 
E|g=2283.6 {I5}, I|g=44 {I16} in table 1 for complex line (2011Bo09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(2326|g)=18 {I11}:100 {I14} (2011Bo09). 
E|g=2033.4 {I3}, I|g=69 {I6} in table 1 of 2011Bo09. 
Other E|g (I|g): 2034.0 {I3} (98 {I15}) (1993Pr09); possibly for 2034|g+2036|g doublet. 


decay_energy_unit: KEV
decay_comment:
E|g=2325.17 {I14}, I|g=230 {I13} in table 1 for complex line which may be partly a primary |g (2011Bo09). 
Other E|g (I|g): 2325.54 {I12} (364 {I21}) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E|g=2077.8 {I6}, I|g=28 {I13} in table 1 of 2011Bo09 for doublet. 
I|g:I(2366|g)=32 {I9}: |?83 (2011Bo09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(2366|g)|?17: |?83 (2011Bo09). 
E|g=2160.7 {I6}, I|g=80 {I13} in table 1 for doublet (2011Bo09). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
I|g:I(2366|g)|?4: |?83 (2011Bo09). 
E|g=2319.8 {I6}, I|g=68 {I5} from table 1 of 2011Bo09 presumably includes this transition. 
Other E|g (I|g): 2320.78 {I25} (98 {I12}) (1993Pr09); presumably for 2320|g+2322|g doublet. 


decay_energy_unit: KEV
decay_comment:
I|g:I(2369|g)=22 {I11}:|?100 (2011Bo09). 
E|g=2077.8 {I6}, I|g=28 {I13} in table 1 of 2011Bo09 for doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(2369|g)=86 {I13}:|?100 (2011Bo09). 
E|g=2160.7 {I6}, I|g=80 {I13} in table 1 of 2011Bo09 for doublet. 


decay_energy_unit: KEV
decay_comment:
I|g:I(2369|g)=57 {I11}:|?100 (2011Bo09). 
E|g=2322.2 {I5}, I|g=40 {I5} in table 1 of 2011Bo09 for doublet. 
See comment on 2319|g. 


decay_energy_unit: KEV
decay_comment:
E|g=2369.9 {I6}, I|g=72 {I15} in table 1 for complex line (2011Bo09). 
Other E|g (I|g): 2369.03 {I17} (166 {I21}; I|g corrected for escape-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_comment:
I|g:I(2286|g)=41 {I9}:100 {I10} (2011Bo09). 
Other E|g (I|g): 1064.0 {I6} (50 {I18}) for doublet (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
I|g:I(2286|g)=56 {I8}:100 {I10} (2011Bo09). 
Other E|g (I|g): 1108.1 {I4} (40 {I8}) (1993Pr09); apparently for 1107.7|g+1109.4|g doublet. 


decay_energy_unit: KEV
decay_comment:
E presumably from coincidence data, but not so indicated in table 2 of 2011Bo09; E|g=2285.5 {I4}, I|g=92 {I16} in table 1 for complex line. 
Other E|g (I|g): 2285.41 {I17} (76 {I11}; I|g corrected for escape-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
I|g:I(2286|g)=87 {I26}:100 {I10} (2011Bo09). This is the only branch reported in (n,|g): |g|g coin. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2481.78 {I17} (114 {I10}; I|g corrected for escape-peak contamination) (1993Pr09); presumably for 2479|g+2482|g doublet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2458.65 {I25} (114 {I21}; I|g corrected for escape-peak contamination) (1993Pr09); possibly includes 2461|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2476.41 {I15} (208 {I21}; I|g corrected for escape-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Other E|g (I|g): 2617.11 {I25} (53 {I15}); I|g corrected for escape-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2574.10 {I14} (114 {I10}; I|g corrected for escape-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2807.7 {I5} (31 {I4}; I|g corrected for escape-peak contamination) (1993Pr09); may include 2810|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 3344.32 {I11} (135 {I31}; I|g corrected for escape-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 3357.06 {I15} (187 {I42}; I|g corrected for escape-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Probably feeds both the 2611 and 2613 levels. 
Other E|g (I|g): 3579.5 {I6} (229 {I31}) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 3867.87 {I25} (114 {I42}; I|g corrected for escape-peak contamination) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 4091.91 {I14} (177 {I21}; I|g corrected by authors for escape-peak contaminant) (1993Pr09). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
Other E|g (I|g): 6144.23 {I8} (3941 {I218}) (1993Pr09); 6144.21 {I18} (3391 {I219}) (2007ChZX); 6144.28 {I6} (4771 {I185}) (2014Hu02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement from table 2 and text of 1997Pr02. This |g also deexcites an otherwise unknown 1223 level, according to 1993Pr09. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placed feeding 11/2+ 309 in table 2 and text of 1997Pr02; unplaced by 1993Pr09 and unobserved in 'Budapest' data from 2007ChZX. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Placement from 1993Pr09; |g omitted from table 2 and fig. 9 by 1997Pr02, so placement is shown as uncertain here. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Placement from 1997Pr02 (table 2); this presumably supersedes 1993Pr09's placement of this |g from the 1475 level. 


decay_energy_unit: KEV
decay_comment:
E from 1957Ch39 (curved crystal spectrometer; E relative to E(K| x ray) for W. 
M E2 excitation of level (1966Th07) based on relative yields from {+6}Li and {+7}Li Coulomb excitation. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI I(344|g)/I(259|g)=0.49 {I3} (1992La02) implies I(344|g)=4.1. 
MR from table 6 of 1992La02; +0.37 {I8} in table 2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Relative E|g: 46.48384 {I16} (1975Bo05). Other E|g: 46.484 {I2} (1970Ne11). 
RI unweighted average of 21.5 {I15} (1964Da15), 16.8 {I10} (1965Ed01). 
M L1:L2:L3=100:12.8:4.8 (1972Bb21); L1:L2:L3=87:12.7:6.0 (1965Al08); L1:L2:L3=7.4:1.05:0.5, |a(M1)exp=1.5, |a(N1)exp=0.45 (1955Mu19). 
%I|g=5.9 {I4} assuming adopted decay scheme normalization. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Relative E|g: 52.59515 {I12} (1975Bo05). Other E|g: 52.599 {I3} (1970Ne11). 
RI unweighted average of 21.5 {I12} (1964Da15), 17.3 {I11} (1965Ed01). 
M L1:L2:L3=100:15.7:9.6 (1972Bb21); L1:L2:L3=60:10.7:6.9 (1965Al08); L1:L2:L3=3.8:0.9:0.55, |a(M1)exp=0.9, |a(N1)exp=0.25 (1955Mu19); L1:L2:L3=2.3:28:25 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Relative E|g: 99.07932 {I9} (1975Bo05). 
RI unweighted average of 26.6 {I15} (1964Da15), 23.1 {I14} (1965Ed01). 
M |a(K)exp=1.4, L2:L3=1.55:1.45, |a(M3)exp=0.7, |a(L23)exp=0.2 (1955Mu19); L1:L2:L3=8.2:100:89 (1972Bb21). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Relative E|g: 107.93096 {I11} (1975Bo05). 
RI unweighted average of 44.1 {I22} (1964Da15), 37.2 {I22} (1965Ed01). 
M L1:L2=100:20.1 (1972Bb21); |a(K)exp=3.8, K:L1=3.8:0.6, |a(M1)exp=0.15, |a(N1)exp=0.04 (1955Mu19); L1:L2:L3=16.3:3.4:1.2 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Relative E|g: 160.5260 {I5} (1975Bo05). 
RI weighted average of 11.1 {I4} (1964Da15), 10.7 {I5} (1965Ed01). 
M L1:L2:L3=20.2:100:74.2 (1972Bb21); |a(K)exp=0.4 (1955Mu19); L1:L2:L3=0.35:1.35:0.96 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1965Gr16. 
RI weighted average of 2.36 {I12} (1964Da15), 2.10 {I12} (1965Ed01). 
L1:L2=1.3:0.17 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Relative E|g: 162.32112 {I27} (1975Bo05). 
RI weighted average of 18.9 {I8} (1964Da15), 17.6 {I8} (1965Ed01). 
M L1:L2=100:20.2 (1972Bb21); |a(K)exp=1.10 (1955Mu19); L1:L2:L3=1.8:0.37:0.20 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1965Gr16. 
RI weighted average of 2.28 {I9} (1964Da15), 2.3 {I4} (1965Ed01). 
M |a(K)exp=0.7 (1955Mu19); L1:L2:L3=0.14:0.03:0.02 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1965Gr16. 
RI unweighted average of 1.44 {I8} (1964Da15), 1.78 {I13} (1965Ed01). 
M L1:L2=80:100 (1972Bb21); |a(L1)exp=1.4 (1955Mu19); L1:L2=0.94:1.1 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1965Gr16. 
RI weighted average of 5.1 {I4} (1964Da15), 4.9 {I3} (1965Ed01). 
M L1:L2:L3=100:21:15 (1972Bb21); |a(L1)exp=1.1, |a(M1)exp=0.2 (1955Mu19). L1:L2=4.1:0.75 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1965Gr16. 
RI weighted average of 1.35 {I4} (1964Da15), 1.25 {I8} (1965Ed01). 
M |a(K)exp=0.65 (1955Mu19); L1:L2:L3=0.06:0.02:0.01 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Relative E|g: 291.7236 {I7} (1975Bo05). 
RI weighted average of 14.1 {I4} (1964Da15), 14.5 {I9} (1965Ed01). 
M |a(K)exp=0.07, |a(L2)exp=0.023 (1955Mu19); L1:L2:L3=0.09:0.13:0.02 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1965Gr16. 
RI weighted average of 1.22 {I7} (1964Da15), 1.3 {I1} (1965Ed01), 1.12 {I9} (1965Gr16). 
M |a(K)exp=5.4, L2:L3=1.55:1.45 (1955Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Relative E|g: 209.8669 {I4} (1975Bo05). 
RI weighted average of 17.2 {I5} (1964Da15), 16.0 {I10} (1965Ed01). 
M |a(K)exp=0.22, K:L2:L3=0.22:0.065:0.03 (1955Mu19); L1:L2:L3=0.25:0.56:0.39 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_comment:
E from 1965Gr16. 
RI unweighted average of 0.51 {I3} (1964Da15), 0.71 {I8} (1965Ed01), 0.48 {I4} (1965Gr16). 
M K:L1:L3=13.0 {I2}:2.8 {I2}:0.6 {I1} (1972Bb21); |a(K)exp=35, K:L1=35:6.0 (1955Mu19); L1:L3=4.4:1.1 (1965Al08). 
|d(M2,E3)=0.000 {I18} from subshell ratios from 1972Bb21. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E from 1965Gr16. 
RI unweighted average of 0.35 {I2} (1964Da15), 1.02 {I11} (1965Ed01), 0.35 {I4} (1965Gr16). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
E from 1965Gr16. 
RI weighted average of 0.23 {I2} (1964Da15), 0.26 {I2} (1965Ed01). 
M,MR from |a(K)exp=2.1 (1955Mu19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E from 1965Gr16. 
RI weighted average of 1.47 {I5} (1964Da15), 1.40 {I9} (1965Ed01). 
M |a(K)exp=0.65 (1955Mu19); L1:L2=0.026:0.056 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1965Gr16. 
RI weighted average of 3.4 {I1} (1964Da15), 3.1 {I2} (1965Ed01). 
M |a(K)exp=0.6, K:L1=0.6:0.13 (1955Mu19); L1:L3=0.20:0.006 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1965Gr16. 
RI weighted average of 27.1 {I8} (1964Da15) and 27.4 {I17} (1965Ed01) for doublet is 27.2 {I7}. 
M |a(K)exp=0.22, |a(L1)exp=0.035 (1955Mu19); L1:L2:L3=0.58:0.05:0.006 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E from 1965Gr16. 
RI weighted average of 1.76 {I18} (1964Da15), 1.6 {I3} (1965Ed01). 
M L1:L3=11.5:0.8 (1955Mu19); L1:L3=10:0.32 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Relative E|g: 144.12172 {I28} (1975Bo05). 
RI weighted average of 9.5 {I4} (1964Da15), 9.3 {I6} (1965Ed01). 
M |a(K)exp=1.65, K:L1=1.65:0.30, |a(M1)exp=0.10 {I1} (1955Mu19). L1:L2=1.85:0.18 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
Relative E|g: 161.34391 {I7} (1975Bo05). 
RI weighted average of 34.6 {I14} (1964Da15), 32.0 {I15} (1965Ed01). 
M L1:L2=100:15.4 (1972Bb21); |a(K)exp=1.15 (1955Mu19); L1:L2=4.30:0.50 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI weighted average of 32.0 {I10} (1964Da15), 32.9 {I20} (1965Ed01). 
Relative E|g: 344.2630 {I5} (1975Bo05). 
M |a(K)exp=0.15 (1955Mu19); L1:L2=0.38:0.79 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Relative E|g: 246.05851 {I21} (1975Bo05). 
RI from 1964Da15; 100 from (1965Ed01). 
M |a(L1)exp=0.07 (14955mu19); L1:L2:L3=4.3:0.34:0.041 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Relative E|g: 353.9887 {I3} (1975Bo05). 
RI weighted average of 43.2 {I13} (1964Da15), 40.5 {I24} (1965Ed01). 
M |a(K)exp=0.14, |a(L1)exp=0.025 (1955Mu19). L1:L2:L3=0.59:0.05:<0.006 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1965Gr16. 
RI unweighted average of 1.40 {I6} (1964Da15), 1.03 {I6} (1965Ed01), 1.4 {I1} (1965Gr16). 
M |a(L1)exp=0.35 (1955Mu19); L1:L2=0.19:0.034 (1965Al08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E from 1965Gr16. 
RI the weighted average of 27.1 {I8} (1964Da15) and 27.4 {I17} (1965Ed01) for the doublet is 27.2 {I7}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Second placement of 245|g suggested by evaluator, consistent with Adopted Levels, Gammas; see comment on 245|g from 453 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E 245.35 {I14} expected from level energy difference. Note that, in Adopted Levels, two transitions of similar energy deexcite the 453 and 292 levels, so the 245|g here is probably a doublet, consistent with the inordinately large branching implied if all I|g is placed from this level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E 406.55 {I14} expected from level energy difference, much closer to values reported in decay and (n,|g) studies; also branching here is significantly larger than adopted value. Possibly this |g is contaminated in ({+14}C,|a3n|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
$I(|g{-1}|g{-2})=80 {I30} 
E,RI from 1989Bo30; E|g fits placement very poorly and branch is unconfirmed by 2005Su29, so placement is shown as questionable here. A weaker 2617|g branch has been reported in (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$I(|g{-1}|g{-2})=30 
RI reported uncertainty of 999 is presumed to be a typographical error; 9 would be more realistic. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$I(|g{-1}|g{-2})=79 {I15} 
Other E|g (I|g): 2565.7 {I15} (130 {I40}) (1989Bo30). Placed by 1989Bo30 from an otherwise unknown 2775 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
From 1989Bo30; |g absent in 2005Su29, so placement shown as uncertain here. I|g=60 {I30} (1989Bo30). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E WEIGHTED AVERAGE OF 111.218 10 IN (N,G) E=THERMAL, 111.207 7 IN EC DECAY AND 111.192 20 IN B- DECAY IS 111.209 6. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E from |e decay. 
RI weighted average of 0.80 {I4} in |e decay (169 d), 0.86 {I4} in |e decay (35.4 d), 0.77 {I10} in |b{+-} decay. Other I|g: 1.3 {I3} in (n,|g) E=thermal; 2.2 {I2} for possibly contaminated |g in Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from |e decay. 
RI weighted average of 98.9 {I22} in |e decay (169 d), 98.9 {I16} in |e decay (35.4 d), 97.1 {I24} in |b{+-} decay. 
Weighted average from |e decay. Other |d: -19 {I+6-21} and -18 {I+4-2} from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from |e decay (35.4 d). 
RI weighted average of 12.1 {I5} in (n,|g) E=thermal, 10.8 {I20} in (n,n'|g), 12.42 {I22} in |e decay (35.4 d), 12.4 {I26} in (n,|g) E=7.6 eV, 12.5 {I4} in |e decay (169 d). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E weighted average from |e decay and (n,|g) E=thermal. 
RI weighted average of 76 {I4} in (n,|g) E=thermal, 52 {I9} in (n,n'|g), 67 {I5} in |e decay (35.4 d), 66 {I14} in (n,|g) E=7.6 eV. 
BE2W See comment on T{-1/2}(1121 level). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_comment:
E weighted average from |e decay and (n,|g) E=thermal. 
|d(M1,E2)=+2.3 {I6}. 
|r{+2}(E0)=0.0026 {I5} (1999Wo07). 
CC estimate based on |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E weighted average from |e decay and (n,|g) E=thermal. 
RI weighted average of 38.8 {I28} in (n,|g) E=thermal, 22 {I9} in (n,n'|g), 38.5 {I28} in |e decay (35.4 d), 40 {I9} in (n,|g) E=7.6 eV. 
BE2W See comment on T{-1/2}(1121 level). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E weighted average of 124.071 {I15} in (n,|g) E=thermal and 124.060 {I20} in |e decay. 
RI weighted average of 9.7 {I10} in (n,|g) E=thermal, 10.1 {I5} in |e decay (169 d), 9.8 {I19} in |e decay (35.4 d), 7.6 {I5} in |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
E weighted average of 226.743 {I12} in (n,|g) E=thermal and 226.748 {I10} in |e decay. 
M |d(M2,E1)=0.0 {I4}, |d(E3,E1)=+0.10 {I3} from |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
RI weighted average of 4.9 {I5} in (n,|g) E=thermal, 6.4 {I7} in |e decay (169 d), 6.3 {I12} in |e decay (35.4 d), 5.7 {I5} in |b{+-} decay, 5.5 {I11} in (n,|g) E=7.6 eV. 
E weighted average of 1018.75 {I9} in |b{+-} decay, 1018.93 {I5} in |e decay and 1018.63 {I8} in (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E from |e decay (169 d). 
RI weighted average of 4.1 {I6} in |b{+-} decay and 4.15 {I20} in |e decay (169 d). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from |e decay (169 d). 
RI weighted average of 4.54 {I28} in |b{+-} decay, 4.42 {I20} in |e decay (169 d) and 3.3 {I5} in (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E from |e decay (169 d). 
RI weighted average of 52 {I4} in (n,|g) E=thermal, 48.3 {I14} in |e decay (169 d), 50 {I5} in |b{+-} decay, 59 {I24} in (n,|g) E=7.6 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E from |e decay (169 d). 
MR from |g(|q,H,t) in |e decay; however, note that |d<0.017 if B(M2)(W.u.)<1 as required by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E from |e decay (169 d). 
RI weighted average of 2.93 {I19} in |b{+-} decay and 2.82 {I8} in |e decay (169 d). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
E from |e decay (169 d). 
RI weighted average of 9.0 {I12} in (n,|g) E=thermal, 10.1 {I5} in |e decay (169 d), 9.8 {I3} in |b{+-} decay, 10.5 {I35} in (n,n'|g), 15 {I3} in (n,|g) E=7.6 eV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E3)
decay_BE_unit: e^2 x (fm)^6
decay_BE_info: ;TYPE=BE3;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE3W
decay_comment:
E from |e decay (169 d). 
RI weighted average of 0.41 {I6} in |b{+-} decay and 0.35 {I3} in |e decay (169 d). 
BE3 From measured B(E3)|^=0.082 {I6} in Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E from |e decay (169 d). 
RI weighted average of 0.50 {I9} in |b{+-} decay and 0.60 {I6} in |e decay (169 d). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E3]
decay_BE_unit: e^2 x (fm)^6
decay_BE_info: ;TYPE=BE3;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE3W
decay_comment:
E from |e decay (169 d). 
RI weighted average of 0.65 {I7} in |b{+-} decay and 0.77 {I10} in |e decay (169 d). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
E from |e decay (169 d). 
RI weighted average of 29 {I7} in (n,|g) E=thermal, 40.6 {I6} in |e decay (169 d), 39.9 {I14} in |b{+-} decay, 49 {I11} in (n,n'|g). 
MR |d(M2,E1)=+0.070 {I6}, |d(E3,E1)=-0.025 {I4}, |l=-2.1 {I2}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E3)
decay_BE_unit: e^2 x (fm)^6
decay_BE_info: ;TYPE=BE3;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE3W
decay_comment:
E from |e decay (169 d). 
RI weighted average of 14.9 {I8} in |e decay (169 d), 14.9 {I11} in |b{+-} decay, 15 {I4} in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 932.2 in Coulomb excitation, 930.00 {I25} in (n,|g) E=thermal, 930.9 {I5} in |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI weighted average of 13.9 {I28} in (n,|g) E=7.6 eV, 11.8 {I25} in Coulomb excitation, 15.4 {I28} in |e decay (35.4 d), 19.5 {I20} in (n,|g) E=thermal. 
M small E0 component suggested in |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=GE
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=LT
decay_comment:
MR,M |d(M1,E2):-0.42 {I4} or >18, <-50 from |g(|q,H,t) (1973Kr01), 1.2 {I+10-5} from |a(K)exp if no E0 in |e decay (35.4 d), but 1974Mc08 suggest the possible presence of an E0 component; |d=+6 {I+6-3} from |g(|q) in Coulomb excitation (1971Mi08), where this larger solution is considered the more likely. The evaluator adopts |d|>+3. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI weighted average of 83 {I17} in (n,|g) E=7.6 eV, 70 {I7} in (n,n'|g), 86 {I4} in |e decay (35.4 d), 80 {I4} in (n,|g) E=thermal. Other I|g: 84 in Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI weighted average of 13 {I3} in (n,|g) E=7.6 eV, 15 {I4} in |b{+-} decay, 11.9 {I23} in |e decay (35.4 d), 7 {I3} in (n,n'|g). Other: 36 {I4} in (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E from |e decay (35.4 d). 
RI weighted average of 57 {I11} in (n,|g) E=7.6 eV, 69 {I10} in |b{+-} decay, 51 {I4} in |e decay (35.4 d), 74 {I7} in (n,|g) E=thermal. Other I|g: <43 in (n,n'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E from Coulomb excitation. 
BE2W From measured B(E2)|^=0.065 {I3} in Coulomb excitation. 
M,MR from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI from (n,|g) E=7.6 eV. |g should have been seen in (n,|g) E=thermal also, but was not, rendering this placement questionable. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E from {+198}Pt({+136}Xe,X|g). 
BE2W From measured B(E2)|^=0.069 {I+5-16} in Coulomb excitation. 
M,MR from Coulomb excitation. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=AP;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E,RI from (n,|g) E=7.6 eV. Other I|g: 14 {I7} from (n,|g) E=thermal; 29 {I11} from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E from (n,|g) E=thermal: |g|g coin. 
RI from (|g,|g'). Other: 25 {I13} from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E from (n,|g) E=thermal: |g|g coin. 
RI from (|g,|g'). Other: 34 {I21} from (n,|g) E=thermal: |g|g coin. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E from (n,|g) E=thermal: |g|g coin. 
RI weighted average of 71 {I39} from (n,|g) E=thermal: |g|g coin, 91 {I41} from (|g,|g'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from {+198}Pt({+136}Xe,X|g). 
M |a(exp)=4.3 {I24} in ({+136}Xe,X|g) favors M1, but uncertainty is large and authors do not rule out E2 and E1 which are within 2|s of deduced |a(exp). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI authors' measured value is 1.07 {I11}. Value shown here is based on authors' I(87|g)/I(91|g) and I(91|g) as revised by the evaluator 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E from E(ce(K)) (1988BuZD). Others: 111.2172 {I11} (1988BuZD, from E(ce(L))); 111.207 {I7} (1974Mc08). 
%I|g=17.2 {I4} assuming adopted normalization. 
M from L1/L2=0.124 {I14}, L1/L3=0.132 {I12}, L2/L3=1.07 {I8}, M1/M2=0.110 {I15}, M1/M3=0.12 {I2}, M2/M3=1.1 {I1} (1970Ag06) and |a(K)exp=0.71 {I3} (1973Ag07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from L2:L3:M:N=280 {I28}:120 {I12}: |?70: |?14 (1968Ag01), |a(K)exp=0.086 {I10} (1973Ag07), |a(K)exp=0.085 {I8} (1974Mc08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |a(K)exp=0.0063 {I6}, L1/L2=3.6 {I3}, L1/L3=10.2 {I10}, L2/L3=2.8 {I3} (1970Ag06); |a(K)exp=0.0058 {I3} (1974Mc08); K:L:M:N=132:24:6.2: |?1.4 (1966Ag03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
%I|g=38.1 {I11} assuming adopted normalization. 
M from L1/L3=12.6 {I18} (1970Ag06), L1/L2=1.3 {I+9-5} (1973Ag03), K:L:M:N=100:18:4.2: |?0.8 (1966Ag03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from L1/L2=3.0 {I5}, L1/L3=8.8 {I18}, L2/L3=2.9 {I8} (1976Kl06), |a(K)exp=0.0087 {I13} (1973Ag07), |a(K)exp=0.0089 {I6} (1974Mc04). 
MR from |g(|q,H,T) (1973Kr01). Others: -6.7 {I+15-26} (1973Hu06), -8.3 {I+16-28} (1973Ca08; |g|g(|q)). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M L1/L2=4.5 {I4}, L1/L3=11.6 {I15}, L2/L3=2.6 {I4} (1970Ag06), |a(K)exp=0.0050 {I7} (1973Ag07), |a(K)exp=0.0046 {I2} (1974Mc08), K:L=47:7.0 (1966Ag03). 
MR from |g(|q,H,T) (1973Kr01). Others: -17.5 {I+8-10} (1973Hu06), -13 {I+4-12} (1973Ca08; |g|g(|q)). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_comment:
|d(D,Q)=+2.3 {I6} from |g(|q,H,T) (1973Kr01). 
M from |a(K)exp=0.0107 {I10}, weighted average of 0.0110 {I11} (1974Mc08) and 0.0093 {I22} (1973Ag07). 
CC from 1.3 |a(K)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M,MR |d(E2,M1)>1.1 from |a(K)exp=0.0035 {I10} (1973Ag07). Others: 1974Mc08 (|a(K)exp=0.0037 {I19}), 1974SvZY. Feeding to 0+ g.s. rules out mixed multipolarity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
M,MR |a(K)exp=0.0421 {I12} (1974Mc08), 0.0032 {I10} (1973Ag07). From |g(|q,H,T) (1973Kr01) and |a(K)exp, |d(M2,E1)=-0.02 {I3}, |d(E3,E1)=0.10 {I3}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
E from 1976Kl06. 
RI from I(ce(K))/I(903ce(K))<0.0047 {I19} (1976Kl06) if mult=E2. 
M,MR from L1/L2<0.3, L1/L3<0.3, L2/L3=1.2 {I6} (1976Kl06). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |a(K)exp=0.0065 {I6} (1974Mc08), |a(K)exp=0.0053 {I13} (1973Ag07). 
MR from |g(|q,H,T) (1973Kr01). Other: 1/|d=-0.01 {I6} (1973Hu06). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from 1976Kl06. 
RI from adopted I(|g)/I(1275|g)=0.039 {I10}. 
M,MR from |a(K)exp=0.055 {I21} based on I(ce(K))/I(903ce(K))=0.0015 {I4} (1976Kl06) and I|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |a(K)exp=0.039 {I19} (1973Ag07), but 1974SvZY report |a(K)exp=0.16 {I7}. The latter value, if correct, would imply an E0 component (|a(K)=0.0174, 0.0516 from E2,M1 theory, respectively). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=GE
decay_comment:
M |a(K)exp=0.0036 {I6} (1974Mc08), 0.0027 {I6} (1973Ag07). 
MR from Adopted Gammas. |d=-0.42 {I4} or >18, <-50 from |g(|q,H,T) (1973Kr01). |d=1.2 {I+10-5} from |a(K)exp=0.0032 {I5} (weighted average of data of 1973Ag07, 1974Mc08). 1974Mc08 suggest the possible presence of an E0 component. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M |a(K)exp=0.0021 {I2} (1973Ag07), 0.0020 {I8} (1974Mc08). Other: 1974SvZY. Feeding of 0+ g.s. rules out mixed multipolarity. 
|d(E2,M1)>2.2 from |a(K)exp (1973Ag07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E from E(ce(K)) (1988BuZD). Others: 111.2172 {I11} (1988BuZD, from E(ce(L))); 111.207 {I7} (1974Mc08). 
M from L1/L2=0.124 {I14}, L1/L3=0.132 {I12}, L2/L3=1.07 {I8}, M1/M2=0.110 {I15}, M1/M3=0.12 {I2}, M2/M3=1.1 {I1} (1970Ag06) and |a(K)exp=0.71 {I3} (1973Ag07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from L1/L3=12.6 {I18} (1970Ag06), L1/L2=1.3 {I+9-5} (1973Ag03), K:L:M:N=100:18:4.2: |?0.8 (1966Ag03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M from L1/L2=3.0 {I5}, L1/L3=8.8 {I18}, L2/L3=2.9 {I8} (1976Kl06), |a(K)exp=0.0087 {I13} (1973Ag07), |a(K)exp=0.0089 {I6} (1974Mc04). 
MR from |g(|q,H,t) (1973Kr01). Others: -6.7 {I+15-26} (1973Hu06), -8.3 {I+16-28} (1973Ca08; |g|g(|q)). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M L1/L2=4.5 {I4}, L1/L3=11.6 {I15}, L2/L3=2.6 {I4} (1970Ag06), |a(K)exp=0.0050 {I7} (1973Ag07), |a(K)exp=0.0046 {I2} (1974Mc08), K:L=47:7.0 (1966Ag03). 
MR from |g(|q,H,t) (1973Kr01). Others: -17.5 {I+8-10} (1973Hu06), -13 {I+4-12} (1973Ca08; |g|g(|q)). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
M,MR |a(K)exp=0.0421 {I12} (1974Mc08), 0.0032 {I10} (1973Ag07). From |g(|q,H,t) (1973Kr01) and |a(K)exp, |d(M2,E1)=-0.02 {I3}, |d(E3,E1)=0.10 {I3}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
E from 1976Kl06. 
RI from I(ce(L2)) of 1976Kl06 if mult=E2. 
M,MR from L1/L2<0.3, L1/L3<0.3, L2/L3=1.2 {I6} (1976Kl06). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |a(K)exp=0.0065 {I6} (1974Mc08), |a(K)exp=0.0053 {I13} (1973Ag07). 
MR from |g(|q,H,t) (1973Kr01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |a(K)exp=4.2 {I17}, L1/L2=1.4 {I4} (1973Ag07). L1/L2=1.03 {I11}, L2/L3=1.26 {I15} (1973Ca08). 
MR from |a(K)exp and L-subshell ratios. Others: 0.63 {I3} (1973Ca08), 1973Ag07. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
M from |a(K)exp=0.0183 {I21} (1974Mc08), 0.022 {I5} (1973Ag07). 
MR unweighted average of -0.01 {I3} (1973Hu06) and -0.029 {I8} (1973Kr01) from |g(|q,H,t); however, the latter |d implies B(M2)(W.u.)=2.7 {I16} which violates RUL (|d<0.017 needed for B(M2)(W.u.)<1) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M from |a(K)exp|?0.003 (1973Ag07). Note that the value given in 1973Ag07 is misprinted as |?0.0003. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E3)
decay_comment:
%I|g=0.0203 {I18} assuming adopted normalization. 
M from |a(K)exp=0.0045 {I16} (1973Ag03) and 0.0049 {I9} (1973Ag07), also consistent with M1 which is ruled out by the decay scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E from ce data (1988BuZD). Other: 63.715 {I15} (1974Mc08). 
M from L2/L3=1.0 {I1}, L1/L3<0.03, L1/L2<0.03 (1973Ag07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
M,MR from |g(|q,H,t) (1982Al05), |a(K)exp=0.00634 {I11} (1987Bu26), and L1/L2=8.0 {I16} (1987Bu26, reanalysis of data from 1977Ga21), 1987Bu26 obtain |d(M2,E1)=+0.070 {I6}, |d(E3,E1)=-0.025 {I4}, and |l=-2.1 {I2}. Other |a(K)exp: 0.0064 {I14} (1974Mc08), 0.10 {I7} (1976Kl06), 0.0059 {I4} (1977Ga21). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
M from |a(K)exp=0.00283 {I18} (1977Ga21),0.0028 {I3} (1974Mc08), 0.0021 {I4} (1973Ag07); L1/L2=6.6 {I11} (1977Ga21); K:L:M=9.2:1.1:0.39 (1966Ag03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E3)
decay_comment:
M from |a(K)exp=0.0048 {I9} (1973Ag07), 0.0063 {I10} (1974Mc08); also consistent with M1 (which is ruled out by the decay scheme). K:L:M=3.4:0.61:0.13 (1966Ag03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
%I|g=6.56 {I22} assuming recommended normalization. 
M |a(K)exp=0.85 {I15}, L1/L2=3.1 {I+9-7}, L1/L3=5.4 {I+19-12}, L2/L3=1.7 {I+8-5} (1973Ag07). 
MR from L-subshell ratios of 1973Ag07. Others: L1/L2=1.5 {I3}, L1/L3=3.4 {I8} (1973Ca08), implying |d=0.89 {I+6-7} and 0.70 {I+7-8}, respectively, in disagreement with |d=0.53 {I7} from 1973Ag07. |a(K)exp data of 1973Ag07 and 1974Mc08 are consistent with |d from 1973Ag07, but not 1973Ca08. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from ce data (1988BuZD). Other: 55.278 {I5} (1974Mc08). 
M,MR from L1/L2=9.1 {I8} (1973Ag07). Other: L1/L2=8.3 {I22}, L1/L3=10 {I3} implying |d=0.173 {I+14-15} (1973Ca08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other E|g (I|g): 111.194 {I7} (209 {I33}) (2004Lo22); 111.11 {I9} (225 {I6}) (2007ChZX, Budapest data). 
RI the discrepancy between data from different sources is troubling; I|g from 1974Gr11 was corrected for self absorption; it is unclear whether data from 2004Lo22 and 2007ChZX required or received similar corrections. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other E|g (I|g): 252.842 {I11} (139 {I8}) (2004Lo22); 252.93 {I9} (140 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Other E|g (I|g): 792.12 {I6} (1975Bu01); 792.079 {I14} (223 {I4}) (2004Lo22); 791.86 {I9} (157 {I8}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other E|g (I|g): 903.1 {I1} (192 {I4}) (1975Bu01); 903.289 {I16} (231 {I4}) (2004Lo22); 903.16 {I9} (157 {I6}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
Other E|g (I|g): 894.8 {I1} (106.9 {I20}) (1975Bu01); 894.769 {I17} (128 {I3}) (2004Lo22); 494.52 {I9} (108 {I6}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other E|g (I|g): 757.25 {I6} (37.6 {I20}) (1975Bu01); 757.38 {I3} (48 {I2}) (2004Lo22); 757.37 {I14} (43 {I6}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_comment:
Other E|g (I|g): 1010.4 {I1} (55.4 {I20}) (1975Bu01); 1010.30 {I3} (68 {I3}) (2004Lo22); 1009.64 {I17} (47 {I6}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other E|g (I|g): 1121.6 {I3} (20.0 {I20}) (1975Bu01); 1121.42 {I4} (10 {I1}) (2004Lo22); 1121.09 {I17} (23 {I3}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
Other E|g (I|g): 226.742 {I12} (128 {I4}) (2004Lo22); 226.98 {I13} (61 {I3}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
Other E|g (I|g): 215.32 {I2} (19 {I1}) (2004Lo22); 215.24 {I12} (14.3 {I18}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
Other E|g (I|g): 318.015 {I17} (39 {I2}) (2004Lo22); 318.01 {I10} (22.5 {I26}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 930.3 {I2} (3 {I1}) (2004Lo22); 929.93 {I12} (14.9 {I14}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
Other E|g (I|g): 418.87 {I4} (17 {I1}) (2004Lo22); 419.21 {I12} (24 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
Other E|g (I|g): 339.62 {I6} (8 {I1}) (2004Lo22); 339.5 {I3} (5.3 {I22}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=GE
decay_comment:
Other E|g (I|g): 1275.2 {I1} (40 {I2}) (1975Bu01); 1275.15 {I5} (58 {I3}) (2004Lo22). 1274.51 {I9} (181 {I7}) (2007ChZX, Budapest data), presumed to include impurity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other E|g (I|g): 1386.4 {I1} (27.7 {I20}) (1975Bu01); 1386.43 {I4} (49 {I3}) (2004Lo22); 1386.20 {I21} (32 {I6}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
Other E|g (I|g): 294.945 {I24} (20 {I1}) (2004Lo22); 294.72 {I12} (17.4 {I18}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other E|g (I|g): 1313.7 {I4} (9.9 {I20}) (1975Bu01); 1313.7 {I4} (9.9 {I20}) 1975Bu01), 1314.0 {I1} (18 {I1}) (2004Lo22); 1313.9 {I5} (10 {I3}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_comment:
Other E|g (I|g): 1319.8 {I2} (17.0 {I16}) (1975Bu01); 1319.93 {I7} (25 {I6}) (2004Lo22); 1319.5 {I3} (13 {I3}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Other E|g (I|g): 1431.5 {I3} (15.6 {I18}) (1975Bu01); 1431.09 {I8} (22 {I2}) (2004Lo22); 1430.7 {I4} (14 {I6}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1412.3 {I5} (11.5 {I16}) (1975Bu01); 1411.92 {I8} (16 {I1}) (2004Lo22). 1411.32 {I15} (26 {I3}) (2007ChZX, Budapest data) suggest presence of an impurity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1568.3 {I3} (5 {I1}) (2004Lo22); 1569.59 {I23} (18 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 607.4 {I2} (20 {I4}) (1975Bu01); 607.73 {I4} (22 {I1}) (2004Lo22); 607.63 {I21} (8.9 {I26}) (2007ChZX, Budapest data). 
Alternative placement from 2223 level suggested by 1975Bu01. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 710.1 {I3} (13.9 {I20}) (1975Bu01); 710.25 {I5} (19 {I1}) (2004Lo22); 709.11 {I24} (21 {I3}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 711.4 {I3} (7.9 {I20}) (1975Bu01); 711.76 {I5} (18 {I1}) (2004Lo22); 711.6 {I4} (13 {I3}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1503.7 {I3} (9.1 {I18}) (1975Bu01); 1504.4 {I2} (17 {I2}) or 1502.0 {I4} (9 {I2}) (2004Lo22); 1503.23 {I21} (32 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 724.4 {I1} (23.8 {I20}) (1975Bu01); 724.41 {I4} (35 {I2}) (2004Lo22); 724.3 {I3} (18 {I6}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 769.33 {I10} (23.8 {I20} for doublet) (1975Bu01); 769.60 {I6} (17 {I2}) (2004Lo22); 769.66 {I19} (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Other E|g (I|g): 1766.5 {I3} (5.7 {I10}) (1975Bu01); 1766.2 {I2} (11 {I2}) (2004Lo22); 1764.18 {I22} (15 {I3}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_uncertain: ?
decay_comment:
Other E|g (I|g): 1996.0 {I3} (8.5 {I14}) (1975Bu01); 1995.7 {I2} (17 {I2}) (2004Lo22); 1996.5 {I7} (13 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1902.8 {I5} (6.9 {I17}) (1974Gr11; possible escape peak); 1901.6 {I3} (9 {I2}) (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 1919.0 {I3} (26 {I6}) (2007ChZX, Budapest data); this I|g appears excessively large. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2036.0 {I3} (4.6 {I14}) (1975Bu01); 2037.0 {I6} (5 {I2}) (2004Lo22); 2035.89 {I22} (35 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
Other E|g (I|g): 1945.1 {I3} (7.5 {I16}) (1975Bu01); 1945.1 {I2} (14 {I2}) (2004Lo22); 1945.4 {I3} (28 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 995.7 {I3} (7.9 {I20}) (1975Bu01); 996.23 {I8} (11 {I1}) (2004Lo22); 995.6 {I3} (9 {I3}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2014.9 {I3} (9.1 {I14}) (1975Bu01); 2015.8 {I2} (20 {I2}) (2004Lo22); 2014.2 {I5} (13 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 742.8 {I3} (8.1 {I16}) (1975Bu01); 743.25 {I7} (11 {I2}) (2004Lo22); 743.5 {I3} (10.1 {I26}) (2007ChZX, Budapest data). 
Alternative placement from 2370 level suggested by 1975Bu01. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2134.8 {I6} (5.0 {I16}) (1975Bu01); 2135.2 {I2} (11 {I2}) (2004Lo22); 2136.7 {I5} (18 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2183.6 {I3} (7.7 {I16}) (1975Bu01); 2183.6 {I1} (18 {I5}) (2004Lo22); 2182.66 {I23} (31 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2370.9 {I4} (4.6 {I14}) (1975Bu01); 2369.4 {I3} (25 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Other E|g (I|g): 782.13 {I9} (199 {I8}) (2007ChZX, Budapest data); line is presumably heavily contaminated. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 2284.6 {I2} (8.5 {I12}) (1975Bu01); 2284.2 {I2} (22 {I2}) (2004Lo22); 2284.38 {I23} (26 {I4}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 3668.1 {I3} (26 {I7}) (2007ChZX, Budapest data); this I|g appears excessively large. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 3865.7 {I5} (15 {I4}) (2007ChZX, Budapest data); this I|g appears excessively large. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 4082.51 {I25} (35 {I4}) (2007ChZX, Budapest data); large I|g may indicate presence of an impurity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 4227.5 {I5} (18 {I2}) (2004Lo22); 4226.2 {I3} (10 {I3}) (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Other E|g (I|g): 4562.1 {I3} (39 {I7}) (2007ChZX, Budapest data). This I|g suggests presence of an impurity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 5015.9 {I5} (1974Gr11), 5016.1 {I8} (2007ChZX, Budapest data), 5015.9 {I3} (2004Lo22). 
Other I|g: 33.4 {I15} (1975Bu01), 24 {I6} (2007ChZX, Budapest data), 27 {I2} (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g (I|g): 5090.0 {I4} (19 {I3}) (2007ChZX, Budapest data); I|g suggests presence of an impurity. Absent in 1974Gr11 and 2004Lo22. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 5116.4 {I5} (1974Gr11), 5116.3 {I7} (2007ChZX, Budapest data). 
Other I|g: 16.1 {I6} (1975Bu01), 11 {I3} (2007ChZX, Budapest data). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI I(|g)=7.3 {I3}, due partly to {+182}W(n,|g). 1974Gr11 assign all the intensity of the 5164,8|g to this impurity reaction. |g not observed by 2004Lo22. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 5242.9 {I5} (1974Gr11), 5243.3 {I8} (2007ChZX, Budapest data), 5242.7 {I7} (2004Lo22). 
Other I|g: 10.2 {I5} (1975Bu01), 8 {I4} (2007ChZX, Budapest data), 13 {I2} (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 5284.6 {I5} (1974Gr11), 5284.3 {I5} (2007ChZX, Budapest data), 5285.6 {I2} (2004Lo22). 
Other I|g: 11.7 {I4} (1975Bu01), 18 {I4} (2007ChZX, Budapest data), 32 {I6} (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E not reported by 1975Bu01. Other E|g (I|g): 5298.3 {I8} (9 {I3}) (2007ChZX, Budapest data), 5297.3 {I7} (13 {I3}) (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI 1975Bu01 report that E|g=5533.6 {I10} arises primarily from {+182}W(n,|g), but they cannot rule out a contribution from {+183}W. Other E|g (I|g): 5533.5 {I3} (17 {I3}) (2007ChZX, Budapest data), 5533.0 {I5} (20 {I2}) (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Probably a doublet feeding the 1614 and 1615 levels. 
Other E|g: 5796.7 {I5} (1974Gr11), 5797.0 {I3} (2007ChZX, Budapest data), 5796.73 {I13} (2004Lo22). 
Other I|g: 15.0 {I6} (1975Bu01), 22 {I3} (2007ChZX, Budapest data), 29 {I4} (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 5979.9 {I5} (1974Gr11), 5979.5 {I7} (2004Lo22). 
Other I|g: 3.5 {I2} (1975Bu01), 9 {I2} (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 6024.5 {I5} (1974Gr11), 624.6 {I33} (2007ChZX, Budapest data), 6024.4 {I3} 3 (2004Lo22). 
Other I|g: 23.3 {I10} (1975Bu01), 47 {I6} (2007ChZX, Budapest data), 66 {I3} (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI from 1975Bu01; may include small contribution from {+182}W(n,|g) transition to g.s.. Not reported by 2004Lo22. I|g=7125 {I250} (2007ChZX, attributed by evaluator to {+182}W present in natural W target. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 6289.5 {I5} (1974Gr11), 6289.9 {I3} (2007ChZX, Budapest data), 6290.3 {I2} (2004Lo22). 
Other I|g: 43.4 {I20} (1975Bu01), 32 {I3} (2007ChZX, Budapest data), 46 {I2} (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 6408.5 {I5} (1974Gr11), 6408.86 {I21} (2007ChZX, Budapest data), 6408.7 {I1} (2004Lo22). 
Other I|g: 73 {I3} (1975Bu01), 53 {I4} (2007ChZX, Budapest data), 69 {I3} (2004Lo22). 
Circular polarization favors J=0 for level fed by this |g (1972St06). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 6507.7 {I5} (1974Gr11), 6507.2 {I3} (2007ChZX, Budapest data), 6508.6 {I3} (2004Lo22). 
Other I|g: 17.8 {I9} (1975Bu01), 14.4 {I18} (2007ChZX, Budapest data), 22 {I1} (2004Lo22). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 7300.0 {I6} (1974Gr11), 7299.7 {I3} (2007ChZX, Budapest data), 7300.2 {I3} (2004Lo22). 
Other I|g: 30.2 {I22} (1975Bu01), 26 {I3} (2007ChZX, Budapest data), 28 {I1} (2004Lo22). 
Other E|g: 7300.7 {I3} (1975Bu01), 7299.7 {I3} (2007ChZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Other E|g: 7411.2 {I6} (1974Gr11), 7411.28 {I12} (2004Lo22, authors' recoil correction removed), 7412.02 {I24} (2007ChZX, Budapest data). 
Circular polarization confirms J=0 for level fed by this |g (1972St06). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=AP;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$placement of this transition is doubtful because an M3 multipolarity would be unlikely and the energy is only poorly known. Not included in Adopted Levels, Gammas. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=AP;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$authors also place this transition from the 1628 level but this is rejected by the evaluator because that implies M3 multipolarity. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
RI I(540|g)/I(903|g)=0.022 {I2} (1971Mi08). Authors state peak is weak in spectrum and could be contaminated; the adopted ratio is 0.0083 {I3}. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI I(792|g)/I(903|g)=0.934 {I30} (1971Mi08). 
Other |d:-19 {I+6-21} from A{-2}(792|g)=-0.114 {I14} (1971Mi08); -18 {I+4-2} from <M(E2)>/<M(M1)>(1991Wu05). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
1977Mc11 observe a 1022|g but place it, instead, from the 1386 level, inconsistent with Adopted Levels, Gammas; they do not report the 1133 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (E3)
decay_uncertain: S
decay_comment:
E unobserved, but must be present because level is Coulomb excited directly. E|g from level energy difference. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI from I(|g+ce)(483|g)/I(|g+ce)(1386|g)=0.14 {I3} (1971Mi08, calculated from I|g assuming |a(483|g)=0.023 and |a(1386|g)=0). 
|d(M1,E2)|<10 (1971Mi08). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=GE
decay_comment:
RI I(1275|g)/I(1386|g)=1.19 {I9} (1971Mi08). 
|d(M1,E2)=+6 {I+6-3} (1971Mi08) from A{-2}(1275|g)=+0.05 {I6}; authors favor this solution over the smaller one. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (M1)
decay_comment:
M |a(exp) favors M1, but uncertainty is large and authors do not rule out E2 or E1 which are within 2|s of deduced |a(exp). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2+E0
decay_comment:
MR$value reported for |d{-|g}(M1,E2); |r{+2}(E0)=0.0026 {I5} from 1999Wo07. 
CC$estimate based on |a(K)exp reported in Adopted dataset for {+184}W in ENSDF database. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
MR$Adopted dataset for {+184}W in ENSDF database gives: |d{-|g}(E1,M2)=0.0(4); |d{-|g}(E1,E3)=+0.10(3) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
MR$Adopted dataset for {+184}W in ENSDF database gives: |d{-|g}(E1,M2)=+0.070(6); |d{-|g}(E1,E3)=-0.025(4) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2+E3
decay_comment:
MR$Adopted dataset for {+184}W in ENSDF database gives: |d{-|g}(E1,M2)=-0.14(4); |d{-|g}(E1,E3)=-0.19(3) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI I|g=0.4 {I2} from intensity balance at 23.6 level, and |a(exp)=92 {I20} deduced in {+185}W IT decay (1.67 min). 
MR from |a=92 {I20} deduced in {+185}W IT decay (1.67 min). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI from I|g(66.1|g)=15 {I3}, and I|g(42.5|g)/I|g(66.1|g)=0.013 {I3} measured in {+185}W IT decay (1.67 min). 
M from {+185}W IT decay (1.67 min). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR from |a(L)exp=10.3 {I16} (weighted average of 11.0 {I28} and 10 {I2}, from {+185}W IT decay (1.67 min) (1969Ku07)). |a(M)exp=3.5 {I17} (1969Ku07). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_uncertain: ?
decay_comment:
RI from I|g(188|g)=0.48 {I8}, and I|g(94.6|g)/I|g(188|g)=0.129 {I10} measured in {+185}W IT decay (1.67 min). Other value: <0.3 (1970Ma60). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
RI from I|g(188|g)=0.48 {I8}, and I|g(122|g)/I|g(188|g)=0.125 {I11} measured in {+185}W IT decay (1.67 min). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
CC$E|g=69.7 keV is very close to the K-binding energy (=69.525 keV). The value for |a(K) used here covers the range from E|g<69.5 keV (|a(K)=0), to E|g=70.0 keV (|a(K)=10.4 for |d=0.27). 
MR$deduced from |a(L)exp=2.9 {I13}, |a(M)exp=0.8 {I3} (1969Ku07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI from 1970Gu02. Other value: 2.2 {I6} (1969Ku07). 
RI$|g ray placed twice in level scheme. I|g for component from 197.4 level is negligible. 
M,MR from |a(exp)=92 {I20}, deduced from intensity balance at 23.5 level and I|g=3.9 {I6}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR from |a(L)exp=10.3 {I16} (weighted average of 10 {I2} and 11.0 {I28}, from {+185}Ta |b{+-} decay (1969Ku07)). |a(M)exp=3.5 {I15} (1969Ku07). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
RI$=3.5 {I6} in |b{+-} decay, but 830|g may include a sum |g contribution there. 
M D+Q from |g(|q) in (n,n'|g); |D|p from decay scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E Other: 292.97 multiply placed in (n,n'|g). 
RI Other: 10.9 {I9} for triplet in (n,n'|g). Other: <400 for doublet in {+186}Ta |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$A comparable and more precise 650.25 {I11} |g unplaced in (n,n'|g). If considered, yields significant difference of the |h{+2} compared to that of the |h{+2} critical in the least squares fit. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E Other: 546.3 {I5} in |b{+-} decay. 
RI Other: <24 in Coulomb excitation; |?200 for poorly established 546.3|g in {+186}Ta |b{+-} decay (if the total I(547|g) is placed from this level). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M from Coulomb excitation. 
MR +13 {I+70-6} in Coulomb excitation, -0.25 {I5} or +6 {I1} in (n,n'|g). 
Other I|g: 96 {I20} or 128 {I10} in Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
|g in (n,n'|g) with similar E|g (but inappropriate multipolarity for this placement) is placed from 1463.8 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E possibly the unplaced 708.67 {I8} transition of (n,n'|g); I(709|g):I(195|g)=0.25 {I8}:1.00 {I10} in (n,n'|g). 


decay_energy_unit: KEV
decay_comment:
E$Placed by 1973Gu02 from 1520 level. A comparable 486.93 {I4} |g in (n,n'|g) is placed from a 1532 level. 


decay_energy_unit: KEV
decay_comment:
E$Placement from 1973Gu02 ({+186}Ta |b- decay). A comparable and more precise 567.10 {I2} |g is unplaced in (n,n'|g). If considered, yields significant difference of the |h{+2} compared to that of the |h{+2} critical in the least squares fit. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$limit is 0.18~{I+13-10} based on I(635|g)/I(294|g triplet)=5.6~{I8} in (n,n'|g); I|g=1~{I3} in 1973Gu02, 1.6~{I2} in 1970Pa16. 
E$from table 2 of 1973Gu02. E|g=294.7 in fig. 1; probably a misprint since authors do not identify any impurity near this energy. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: S
decay_comment:
$|g expected but not reported in |b{+-} decay; obscured by a {+185}W line. E|g from adopted gammas, I|g from I(309|g) and adopted branching. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_uncertain: S
decay_comment:
$|g expected but not reported in |b{+-} decay; probably obscured by contaminant. E|g from adopted gammas, I|g from I(309|g) and adopted branching. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$I|g=6.9~{I10} (1973Gu02) is possibly overestimated (I|g=3.5~{I4} in 1970Pa16). Additionally, the 293|g is a multiplet in (n,n'|g) and, from adopted I(293 multiplet)/I(1175|g)=0.41~{I6}, one expects I(293|g)<0.24 from the 1298 level in |b{+-} decay, leaving I|g=6.7~{I10} unplaced. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_uncertain: S
decay_comment:
$E|g from adopted gammas; transition expected based on adopted 1298-level branching, but would have been obscured in |b{+-} decay study by 1973Gu02 by a {+184}Ta line. I|g|?0.26 from I(1175|g) and adopted branching. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_uncertain: S
decay_comment:
$|g not observed, but it is expected with I|g|?5.6 based on I(1124|g) and adopted branching; it would have been obscured by a {+183}Hf impurity in the decay study by 1973Gu02. E|g is from adopted gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$from |a(K)exp|<0.04, |a(L)exp|<0.04 (1969Mo16); E1 is implied also by intensity balance at 1463 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
MR$Deduced by evaluators from A{-2}=-0.011~{I14} (1971Mo26) for 6418(excitation |g)-6295(scattered |g)(|q); alternative solution (-2.47~{I+15-17}) disfavored by RUL. 
M$from 1971Mo26. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$From Adopted Gammas (rounded value). |g reported by 2000Ya22; possibly the same As the unplaced 539.09|g In 1988GoZC. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Placed by evaluator, consistent with observation of a 589|g from this level in ({+238}U,{+238}U'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$rounded-off value from adopted gammas; |g not evident in spectrum shown in 1989Ku04 (possibly masked by intense 274|g), but authors imply that it was observed. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI$from |g yield (relative to 308|g) in 1977Mc11. 
$Anisotropy=1.29~{I6} (1977Mc11); consistent with 0+(E3)3-(E1)3+ sequence. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI$|g not observed; I|g is from upper limit for |g yield in 1977Mc11 relative to 1286|g yield in 1971Mi08 (both for E|a=15~MeV). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E,MR$from 1971Mi08; A{-2}=-0.02~{I5}. 
RI$from 1971Mi08; I|g/I|g(1286)=0.96~{I20} and 1.28~{I10} in independent determinations (1971Mi08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$From adopted gammas. Other: E|g=122.61 (1972Se06). 
RI$Weighted average of 0.565% {I24} (2016Lu16), 0.600% {I13} (1991Co17), 0.603% {I6} (1994Sc39), 0.604% {I3} (2000Mi03), 0.597% {I8} (2000Wo02). Others: 0.606~{I9} (1991Go23, if I(137|g)=9.47), 0.606~{I19} (1972Se06, if I(137|g)=9.47). 
M$K:L2:L3:M=0.32~{I8}:0.267~{I27}:0.222~{I11}:0.100~{I15} (1969La11). Other: 1964Ma36. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$others: 24.6 {I40} in {+187}Ta |b{+-} decay (2022Mu10); 18.6 {I10} in (n,|g) (2014Hu02). Comment added by B. Singh, March 31, 2022. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$others: 14.4 {I8} in {+187}Ta |b{+-} decay (2022Mu10); 15.3 {I9} in (n,|g) (2014Hu02). Comment added by B. Singh, March 31, 2022. 
M From ({+18}O,{+17}O|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$others: 3.4 {I8} in {+187}Ta |b{+-} decay (2022Mu10); 1.64 {I19} in (n,|g) (2014Hu02). Comment added by B. Singh, March 31, 2022. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E,M From ({+82}Se,{+81}Se|g). Mult assignment from extracted |a(exp)=0.8 {I1} data, assuming both the 148.97|g and 273.14|g of M1 character. 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
$I|g%=122 {I30} 
E$From 1973PrYV 
TI$deduced by the evaluator from conversion electron intensities (1973PrYV) and the adopted multipolarity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Placement was from 9/2- state at 916.5-keV (1997Bo14) 
M$|a(K)exp=0.16 {I6} is consistent with M1+E2, decay scheme requires E2. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
RI$|?0.54, deduced from the estimated ratio of I(|g+ce)(287|g)/I(|g+ce)(14|g)= 0.038 {I26} (2005Sh26) and |a(assuming 14|g M1)=264 and |a(assuming 287|g E2)=0.097. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M Assignment from extracted |a(exp)=0.8 {I1} data, assuming both the 148.8|g and 272.7|g of the M1 character (2005Sh26). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$77.3 in Fig. 3 of 2022Mu10; 77.28 {I4} in Adopted Gammas 
$Conversion coefficients for E|g=77.28 {I4} in {+187}W Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$124.2 in Fig. 3 of 2022Mu10; 124.23 {I3} in the Adopted Gammas 
$Conversion coefficients for E|g=124.23 {I3} in the Adopted Gammas 
$I|g(123.9)/I|g(201.3)=0.246 {I41} as compared to 0.126 {I2} in {+187}W Adopted Gammas, and 0.186 {I10} in (n,|g) (2014Hu02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
E$149.0 in Fig. 3 of 2022Mu10; 148.96 {I4} in the Adopted Gammas 
$I|g(148.8)/I|g(273.0)=0.144 {I8} as compared to 0.114 {I3} in the Adopted Gammas, and 0.153 {I9} in (n,|g) (2014Hu02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$350.4 in Fig. 3 of 2022Mu10; 350.40 {I11} in the Adopted Gammas 
$I|g(350.5)/I|g(273.0)=0.034 {I8} as compared to 0.025 {I2} in the Adopted Gammas, and 0.0164 {I19} in (n,|g) (2014Hu02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
E,RI$transition not observed; |s{-|g} calculated assuming feeding to the isomer |s{-9/2+}=400 mb {I16}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$ Also seen in {+188}Ta |b- decay, but not placed in the level scheme 
RI$From {+186}W({+136}Xe,X|g) 
M$From |a{-T}(exp)=0.77 {I6} in 2010La16 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$ from the measured total conversion coefficient of 0.77 {I6} in 2010La16, which is closest to the calculated value of 0.85 for M1. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$M1 or E2 from |a(exp) deduced from |g-ray intensity balance in {+190}W IT decay (111 ns) (2010La16) 
$Reduced hindrance factor f{-|n}=5.5 {I3}, |n=7, from B(M1)(W.u.) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$others: 207.0 {I3} (2005Ca02), 206 (2010La16), 207 (2000Po26) 
RI$others: 81 {I10} (2011St21), 129 {I33} (renormalized from 27 {I7} in 2005Ca02), 105 {I24} (renormalized from 65 {I15} 2000Po26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$others: 357.4 {I3} (2005Ca02), 358 (2010La16), 357 (2000Po26) 
RI$others: 92 {I10} (2011St21), 114 {I33} (renormalized from 24 {I7} in 2005Ca02), 107 {I24} (renormalized from 67 {I15} 2000Po26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$others: 484.0 {I4} (2005Ca02), 484 (2010La16), 485 (2000Po26) 
RI$others: 100 {I11} (2011St21), (100 {I33} (renormalized from 21 {I7} in 2005Ca02), 100 {I32} (renormalized from 62 {I20} 2000Po26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$from 2005Ca02. Others: E|g=592 (2010La16), 591 (2000Po26). This |g was not seen by 2009Al30, and not reported by 2011St21, perhaps due to its weak population. 
RI$deduced by evaluators from intensity balance at 1642 level. Others: 43 {I27} (2000Po26), renormalized from 27 {I17}, 100 {I38}, renormalized from 21 {I8} in 2005Ca02. This |g is as strong as the 484.1|g with I|g=21 {I7} in Table 1 of 2005Ca02, but seen in the |g spectrum in Fig. 4 of 2005Ca02, much weaker than the 484.1|g peak. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$|g reported by 2010La16 only 
RI$from {+190}W IT decay (166 |ms), based on data in 2010La16. Other: 3.4 {I9}, deduced by evaluators from I|g(102)/I|g(694)=4.8 {I11}/100 {I2} (2010La16) and I|g(694)=71 {I10} in 2011St21. 
M$M1, E2 from |a(exp) deduced from |g-ray intensity balance (2010La16); M1 is assigned in 2010La16, as dominant M1 may be more likely for (8+) to (8+) transition 
$Reduced hindrance factor f{-|n}=5.4 {I2}, |n=7, from B(M1)(W.u.)=7|*10{+-6} {I2}, as given in 2010La16 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$others: 694 (2010La16), 694.0 {I7} (2005Ca02), 695 (2000Po26); in 2005Ca02 and 2000Po26, this |g was placed from a 2335, 10+ level, as member of g.s. band). The decay scheme was modified by 2009Al30 and 2009Fa06 to place 694|g from this level, and omitting the 594|g from 1640 level as the 594|g was absent in the delayed |g spectrum obtained by 2009Al30 
RI$from {+190}W IT decay (166 |ms), based on data in 2010La16. Others: 71 {I10} (2011St21), 76 {I33} (renormalized from 16 {I7} in 2005Ca02), 64 {I24} (renormalized from 62 {I20} 2000Po26) 
$Reduced hindrance factor f{-|n}=3.7 {I1}, |n=6, from B(E2)(W.u.)=3.9|*10{+-4} {I6}, as given in 2010La16 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$from 2005Ca02. Others: E|g=592 (2010La16), 591 (2000Po26). This |g was not seen by 2009Al30, and not reported by 2011St21, perhaps due to its weak population. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$|g reported by 2010La16 only 
RI$deduced based on I|g(102)/I|g(694)=4.8 {I11}/100 {I2} (2010La16) 
$Reduced hindrance factor f{-|n}=5.4 {I2}, |n=7, from B(M1)(W.u.)=7|*10{+-6} {I2}, as given in 2010La16 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$others: 694 (2010La16), 694.0 {I7} (2005Ca02), 695 (2000Po26); in 2005Ca02 and 2000Po26, this |g was placed from a 2335, 10+ level, as member of g.s. band. The decay scheme was modified by 2009Al30 and 2009Fa06 to place 694|g from this level, and omitting the 594|g from 1640 level as the 594|g was absent in the delayed |g spectrum obtained by 2009Al30 
RI$deduced based on I|g(102)/I|g(694)=4.8 {I11}/100 {I2} (2010La16) 
$Reduced hindrance factor f{-|n}=3.7 {I1}, |n=6, from B(E2)(W.u.)=3.9|*10{+-4} {I6}, as given in 2010La16 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_comment:
M$from |a(exp) deduced by 2010La16 from |g-ray intensity balance 
$Others: 46-keV, (E1), |g ray to 2335, (10+) level in 2000Po26, with I|g=60 {I30} relative to I|g=62 {I21} for 484|g from (6+) state; 58.5 keV {I5} with I|g=60 {I13} relative to I|g=21 {I7} for 484|g (2005Ca02). In later work 58.5-keV peak was assigned to x rays by 2009Fa06 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$from the prompt relationship between 38|g and 96|g and the intensity balance (2011Da01, IT decay) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|a(K)exp=1.2 {I4} deduced from I|g(K| x ray) and I|g(96|g) (|a(K)=0.891 {I18} theory) (2011Da01, IT decay) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$ Observation of x rays, 38-keV, and 96-keV transitions in coin with 837|g indicates that 837-keV transition populates isomeric state in {+160}Re at 184 keV reported in 2011Da01 ({+160}Re IT decay dataset) 


decay_energy_unit: KEV
decay_multipolarity: [E2]
decay_uncertain: ?
decay_comment:
E$although a |g ray of this energy is visible in the singles spectra (2011Da01, Fig. 2a), no evidence of it from |g|g coin. was presented by the authors 


decay_energy_unit: KEV
decay_multipolarity: (E2)
decay_comment:
M$|a(K)exp=1.2 {I4} deduced from I|g(K| x ray) and I|g(96|g) (|a(K)=0.891 {I18} theory) 
$B(E2)(W.u.)=0.082 {I6} (assuming I|g(96|g)=100) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
E,M |g expected to form a cascade with 110|g to 0+x level in {+170}Ir |a decay (811 ms); may Be a highly-converted transition because transition is not evident in relevant |a-|g coin spectrum, so 2007Ha45 suggest M1 multipolarity, consistent with level scheme. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E highly tentative; however, observation of 2007|a-75|g coin (2007Ha45) suggests the existence of a transition connecting the 122+x and 75+x levels and such a transition may Be too highly converted to Be seen in |a-|g coincidence spectrum. Level scheme implies |D|p=(yes), suggesting a multipolarity of M2 or higher. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [M1,E2]
decay_uncertain: ?
decay_comment:
This second placement of 53|g is suggested by energy difference between 175|g and 122|g that deexcite the same level. 
M assumed, based on level scheme; however, I(53|g)/I(122|g) in {+170}Ir |a decay (811 ms) is approximately the same in the spectra gated by 5951|a or by the 6007|a (2007Ha45). Authors favor M1 multipolarity for this component and E1 for the other. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [M1]
decay_uncertain: S
decay_comment:
M expected by 2007Ha45 to form a cascade with 110|g to 0+x level. |g is absent in 5951|a-|g spectrum; this may indicate significant conversion, and authors suggest M1 multipolarity, consistent with level scheme. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E,M highly tentative |g; however, observation of 6005|a-75|g coin (2007Ha45) suggests the existence of a transition connecting the 122+x and 75+x levels and such a transition may be too highly converted to be seen in the |a-|g coincidence spectrum. However, level scheme suggests |D|p=(yes) so multipolarity of M2 or higher may be implied. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [M1]
decay_comment:
E,M E|g coincides with energy of K|b| x ray(Re) but peak is too strong relative to K|a| x ray in 6007|a-|g coin spectrum to be attributed entirely to Re K|b| x ray. Authors tentatively suggest M1 multipolarity based on the level scheme. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [M1,E2]
decay_uncertain: ?
decay_comment:
M assumed, based on level scheme; however, I(53|g)/I(122|g) is approximately the same in the spectra gated by the 5951|a and by the 6007|a (2007Ha45). Authors favor M1 multipolarity for this component and E1 for the other. 
This second placement of 53|g is suggested by energy difference between 175|g and 122|g (2007Ha45). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1,E2)
decay_comment:
$2016Li13 deduce B(E1)(W.u.)=2.4|*10{+-6} {I+5-3}, B(M1)(W.u.)=2.0|*10{+-4} {I2}, and B(E2)(W.u.)=1.0 {I+2-1} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1,E2)
decay_comment:
$2016Li13 deduce B(E1)(W.u.)=1.3|*10{+-6} {I+3-2}, B(M1)(W.u.)=1.2|*10{+-4} {I1}, and B(E2)(W.u.)=0.4 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 2023Zh03 
TI$from I|a=85.5 {I12} 
RI$from I(|g+ce) and |a 
M$from |a(K)exp=5.1 {I4} (2023Zh03, from I|g and I(Re K x-rays)). Other: |d(E2/M1)<1.8 from |a(K)exp=10 {I8} (1992Sc16). 
$I(K| x ray, Re):I(92|g)=95 {I15}:9 {I5} (1992Sc16). 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
$R(|q)=0.59 {I1}, could be for both the 272 |g rays, but the |g from (13/2-) level is more intense than the one from (19/2-) level 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
$R(|q)=0.85 {I3}, could be for 703, 704 and 705 |g rays, but the 703|g from (19/2-) level is more intense than 705|g from (21/2-) level, and 704|g is very weak 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
$R(|q)=0.48 {I2}, could be for 182 and 181 |g rays, but the 182|g from (21/2-) level is more intense than 181|g from (31/2+) level 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
$R(|q)=0.51 {I2}, could be for 207 and 205 |g rays, but 207|g from (25/2-) level is more intense than 205|g from (29/2-) level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M E1 or E2(+M1) but not pure M1 based on observed I(Re K| x ray) from 1992Sc16; if E2, I(|g+ce)(90) is comparable to I(|g+ce)(123). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M probably E1 or E2 based on observed I(Re K| x ray) from 1992Sc16. However, in either case, I(|g+ce)(136|g) will be significantly lower than I(|g+ce)(123|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
Other E|g: 122.7 {I5} from 2004GoZZ. 
M I(Re K| x ray)=24 {I4} rules out M1 and favors E1 (1992Sc16); also, E1 is consistent with 2004GoZZ's non-observance of ce associated x-rays for this transition. 
Note that the order of the 90|g-123|g-136|g cascade has not been determined, so it is equally likely that the 90|g or the 136|g deexcites this level instead of the 123|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E a 162|g deexciting the level fed by the 5830|a is shown in fig. 6.4, it appears in coincidence with the 5830|a in fig. 6.12, and is mentioned in text (section 6.4.1) of 2004GoZZ. However, in table 5.1, the |g coincident with the 5830|a has E|g=136.3 {I5}; the evaluator assumes that the latter E|g entry is erroneous. 
M,MR from |a(K)exp=0.69 {I6}, as deduced from I|g and I(Re K| x ray) (1992Sc16). |d=1.08 {I16} was deduced by 1992Sc16 from both |a(K)exp and from the relative intensities of the 5828|a and the (5828|a+ce(L)(162)) sum peak. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
M consistent with D based on angular distribution ratio in ({+55}Mn,4n|g) but level scheme requires |DJ=2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
Other I|g: 126 {I37} from ({+28}Si,p2n|g). 
M D from ({+55}Mn,4n|g); however, DCO and anisotropy in ({+28}Si,p2n|g) are consistent with Q also. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
M DCO=1.08 {I20}, anisotropy=1.19 {I20} (2004Zh05) suggest stretched Q; however, this conflicts with D assigned in Adopted Gammas based on data from ({+55}Mn,4n|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M DCO=0.99 {I15}; anisotropy=1.19 {I10} (2004Zh05). 
I(664|g)/I(298|g)=2.21 {I4} (2004Zh05); uncertainty probably an order of magnitude too low since uncertainty in each I|g is at least 5%. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E placement not adopted; presumed to be the 287.5|g known from ({+55}Mn,4n|g) and placed differently in that study. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
Expected but unobserved, possibly due to large conversion associated with the expected M1 multipolarity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M intensity balance at 20 level in |a decay (5.01 s) requires mult(20|g)=E1 if mult(190|g)=E1, E2 or M1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M intensity balance at 20 level in |a decay (5.01 s) (assuming mult(20|g)=E1) implies mult(190|g)=E1, but E2 cannot be ruled out. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M |D|p=no from level scheme; E2 is consistent with I(K| x ray) in {+171}Ir |a decay (5.01 s), M1 is not. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
RI reported only in spectrum gated by 5478|a but |g present also in spectrum gated by 5316|a. 
M intensity balance at 20 level requires mult(20|g)=E1 if mult(190|g)=E1, E2 or M1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M intensity balance at 20 level (with mult(20|g)=E1) implies mult(190|g)=E1, but E2 cannot be ruled out. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
RI observed only in spectrum gated by 5316|a. However, if I(|g+ce)(159.8)=I(5316|a)=12 {I1}, one would expect I|g=5.7 {I13}; possibly this is not the only transition deexciting the 370 level (see comment on 122|g multipolarity). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$from ({+52}Cr,4n|g) 
RI$other: I(474|g):I(241|g)=100 {I57}:32 {I23} in ({+30}Si,p2n|g), but 474|g is a doublet in that reaction. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$others: 721.4 {I3} in ({+30}Si,p2n|g) and 725.3 {I10} in ({+52}Cr,4n|g) 
RI$others: 220 {I110} in ({+30}Si,p2n|g) and 300 in ({+52}Cr,4n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI I(408|g)/I(203|g)=1.23 {I3} (1993Ca02); precision is atypically high and evaluator suspects it may be overestimated. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Coincidence data used to divide I|g. 
$A{-2}=+0.31 {I3}, A{-4}=-0.13 {I4} for doublet (comparable strength |g's). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$deduced from I|g(430.6|g)=52 {I10} (1990Hi05) and relative photon branchings from same level in 1989Ba49. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$ 190.4|g is listed as (10+) to (9+) in figure 2 of 2012Gu14, which seems in error. It should either be J+3 to J+2 or (17-) to (16-) if bandhead is 14-, as explained by 2012Gu14 
$R{-ADO}=1.21 {I10} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.72 {I4} (1995Ba67); DCO=1.05 {I11} is obtained by gating on the dipole (E1, |DJ=1) 1086.4 keV |g ray (1995Ba67). A{-2}=0.08 {I1}, A{-4}=-0.01 {I2} (1986Wa32); A{-2}=0.097 {I26}, A{-4}=-0.025 {I27} (1972Le04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.63 {I4} (1995Ba67). A{-2}=0.01 {I3}, A{-4}=0.03 {I3} (1986Wa32); A{-2}=0.036 {I61}, A{-4}=-0.056 {I63} (1972Le04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|a(exp) deduced from intensity balance considerations is consistent with the proposed assignment (1995Ba67). A{-2}=0.27 {I2}, A{-4}=-0.07 {I2} (1986Wa32); A{-2}=0.352 {I24}, A{-4}=-0.115 {I26} (1972Le04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.69 {I4} (1995Ba67); A{-2}=0.10 {I2}, A{-4}=0.00 {I2} (1986Wa32); A{-2}=0.099 {I17}, A{-4}=-0.009 {I19} (1972Le04). 
MR$Other: +0.21 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$DCO=0.69 {I4} (1995Ba67). A{-2}=0.03 {I2}, A{-4}=0.03 {I2} (1986Wa32); A{-2}=0.031 {I29}, A{-4}=-0.005 {I29} (1972Le04). 
MR$Other: +0.18 {I1} assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.71 {I4} (1995Ba67). A{-2}=-0.06 {I3}, A{-4}=0.00 {I4} (1986Wa32); A{-2}=0.106 {I53}, A{-4}=-0.159 {I58} (1972Le04). 
MR$Other: 0.16 {I1} assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$DCO=1.04 {I4} (1995Ba67); A{-2}=0.29 {I4}, A{-4}=-0.08 {I4} (1986Wa32); A{-2}=0.367 {I29}, A{-4}=-0.124 {I34} (1972Le04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.67 {I4} (1995Ba67); A{-2}=0.038 {I40}, A{-4}=0.060 {I42} (1972Le04). 
MR$+0.21 {I1} assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$DCO=0.64 {I4} (1995Ba67). A{-2}=0.10 {I2}, A{-4}=0.00 {I4} (1986Wa32); A{-2}=0.099 {I17}, A{-4}=-0.009 {I19} (1972Le04). I|g contaminated with 192.5|g. 
MR$Other: +0.15 {I1}, assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.65 {I4} (1995Ba67); A{-2}=0.09 {I3}, A{-4}=0.01 {I1} (1986Wa32); A{-2}=0.052 {I41}, A{-4}=0.002 {I44} (1972Le04). 
MR$Other: +0.19 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.70 {I4} (1995Ba67). A{-2}=0.17 {I7}, A{-4}=-0.05 {I7} (1986Wa32). 
MR$Other: +0.15 {I1}, assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$DCO=0.74 {I4} (1995Ba67); A{-2}=0.41 {I5}, A{-4}=-0.02 {I6} (1986Wa32); 
MR$Other: +0.19 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$DCO=0.72 {I15} (1995Ba67). A{-2}=0.02 {I2}, A{-4}=0.04 {I2} (1986Wa32). 
MR$Other: +0.16 {I1}, assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.67 {I4} (1995Ba67); A{-2}=0.07 {I6}, A{-4}=0.03 {I6} (1986Wa32). 
MR$Other: +0.20 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.73 {I8} (1995Ba67). A{-2}=0.32 {I16}, A{-4}=0.02 {I18} (1986Wa32). 
MR$Other: +0.18 {I1}, assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.83 {I51} (1995Ba67); DCO=1.02 {I15} is obtained by gating on the dipole (E1, |DJ=1) 1086.4 keV |g ray (1995Ba67). |a(exp)=2.10 {I14} from intensity balance considerations (1995Ba67). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.56 {I6} (1995Ba67); A{-2}=-0.06 {I6}, A{-4}=0.15 {I5} (1986Wa32); 
MR$+0.17 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=1.02 {I19} is obtained by gating on the dipole (E1, |DJ=1) 1086.4 keV |g ray (1995Ba67). |a(exp) deduced from intensity balance considerations is consistent with the proposed assignment (1995Ba67). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=1.08 {I13} is obtained by gating on the dipole (E1, |DJ=1) 1086.4 keV |g ray (1995Ba67). |a(exp) deduced from intensity balance considerations is consistent with the proposed assignment (1995Ba67). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M$DCO=0.98 {I24} is obtained by gating on the dipole (E1, |DJ=1) 1086.4 keV |g ray (1995Ba67). |a(exp) deduced from intensity balance considerations is consistent with the proposed assignment (1995Ba67). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.73 {I6} (1995Ba67); A{-2}=0.04 {I6}, A{-4}=-0.01 {I7} (1986Wa32); 
MR$Other: +0.17 {I1}, assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M$DCO=0.8 {I5} is obtained by gating on the dipole (E1, |DJ=1) 1086.4 keV |g ray (1995Ba67). |a(exp) deduced from intensity balance considerations is consistent with the proposed assignment (1995Ba67). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$DCO=2.5 {I5} is obtained by gating on the dipole (E1, |DJ=1) 1086.4 keV |g ray (1995Ba67). |a(exp) deduced from intensity balance considerations is consistent with the proposed assignment (1995Ba67). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
M$DCO=1.13 {I5} (1995Ba67); A{-2}=0.19 {I2}, A{-4}=-0.09 {I7} (1986Wa32); A{-2}=0.353 {I59}, A{-4}=-0.039 {I63} (1972Le04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M$DCO=0.75 {I6} (1995Ba67); A{-2}=0.09 {I6}, A{-4}=-0.01 {I7} (1986Wa32). 
MR$Other: +0.16 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.76 {I8} (1995Ba67); A{-2}=0.02 {I7}, A{-4}=0.03 {I7} (1986Wa32). 
MR$Other: +0.17 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$|a(exp)>19 from intensity balance considerations, compared to |a(E1)=0.98, |a(M1)=14.4 and |a(E2)=322 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|a(exp)=23 {I7} from intensity balance considerations (1995Ba67), consistent with the proposed E2 multipolarity. 
E$The proposed before 77.5|g assignment (1986Wa32 and 1972Le04) is rejected by 1995Ba67. For details see 1995Ba67. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.69 {I4} (1995Ba67); A{-2}=0.10 {I2}, A{-4}=0.00 {I2} (1986Wa32); A{-2}=0.099 {I17}, A{-4}=-0.009 {I19} (1972Le04). I|g contaminated with 193.5|g. 
MR$+0.21 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.69 {I4} (1995Ba67). A{-2}=0.03 {I2}, A{-4}=0.03 {I2} (1986Wa32); A{-2}=0.031 {I29}, A{-4}=-0.005 {I29} (1972Le04). 
MR$+0.18 {I1} assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.71 {I4} (1995Ba67). A{-2}=-0.06 {I3}, A{-4}=0.00 {I4} (1986Wa32); A{-2}=0.106 {I53}, A{-4}=-0.159 {I58} (1972Le04). 
MR$0.16 {I1} assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.64 {I4} (1995Ba67). A{-2}=0.10 {I2}, A{-4}=0.00 {I4} (1986Wa32); A{-2}=0.099 {I17}, A{-4}=-0.009 {I19} (1972Le04). I|g contaminated with 192.5|g. 
MR$+0.15 {I1}, assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.65 {I4} (1995Ba67); A{-2}=0.09 {I3}, A{-4}=0.01 {I1} (1986Wa32); A{-2}=0.052 {I41}, A{-4}=0.002 {I44} (1972Le04). 
MR$+0.19 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.70 {I4} (1995Ba67). A{-2}=0.17 {I7}, A{-4}=-0.05 {I7} (1986Wa32). 
MR$+0.15 {I1}, assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.74 {I4} (1995Ba67); A{-2}=0.41 {I5}, A{-4}=-0.02 {I6} (1986Wa32); 
MR$+0.19 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.72 {I15} (1995Ba67). A{-2}=0.02 {I2}, A{-4}=0.04 {I2} (1986Wa32). 
MR$+0.16 {I1}, assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.67 {I4} (1995Ba67); A{-2}=0.07 {I6}, A{-4}=0.03 {I6} (1986Wa32). 
MR$+0.20 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.73 {I8} (1995Ba67). A{-2}=0.32 {I16}, A{-4}=0.02 {I18} (1986Wa32). 
MR$+0.18 {I1}, assuming K=5/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.83 {I51} (1995Ba67); DCO=1.02 {I15} is obtained by gating on the dipole (E1, |DJ=1) 1086.4 keV |g ray (1995Ba67). 
CC$|a(exp)=2.10 {I14} from intensity balance considerations (1995Ba67). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.73 {I6} (1995Ba67); A{-2}=0.04 {I6}, A{-4}=-0.01 {I7} (1986Wa32); 
MR$+0.17 {I1}, assuming K=7/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$DCO=0.95 {I10} (1995Ba67). A{-2}=0.21 {I4}, A{-4}=-0.08 {I4} (1986Wa32). I|g contaminated with 401.6|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.75 {I6} (1995Ba67); A{-2}=0.09 {I6}, A{-4}=-0.01 {I7} (1986Wa32). 
MR$+0.16 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$DCO=0.76 {I8} (1995Ba67); A{-2}=0.02 {I7}, A{-4}=0.03 {I7} (1986Wa32). 
MR$+0.17 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$DCO=1.18 {I20} (1995Ba67). A{-2}=0.24 {I2}, A{-4}=-0.045 {I20} (1986Wa32). I|g contaminated with 449.1|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=-0.09 {I5}, A{-4}=0.05 {I7} (1986Wa32); I|g contaminated with 294.8|g. 
MR$+0.16 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$DCO=1.01 {I6} (1995Ba67). A{-2}=0.25 {I3}, A{-4}=-0.12 {I3} (1986Wa32). I|g contaminated with 498.8|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M$A{-2}=-0.09 {I5}, A{-4}=0.05 {I7} (1986Wa32); I|g contaminated with 294.1|g. 
MR$+0.13 {I1}, assuming K=9/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$DCO=1.15 {I5} (1995Ba67); A{-2}=0.25 {I3}, A{-4}=-0.07 {I3} (1986Wa32). I|g contaminated with 655.8|g. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
Placed in level scheme by 1989Kr06. E|g=253.7 (1989Sa02). Contaminated with lines from {+179}Re |e decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E weighted average from ({+11}B,4n|g) and |e decay. 
M very tentative assignment from ({+11}B,4n|g) based on intensity balance arguments. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E|g=58 keV predicted by Coriolis calculation which includes the N=5 interacting Nilsson orbitals (1972Le04). 
M from |a(exp) in ({+11}B,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI from (|a,6n|g). Other I|g: 100 {I10} from ({+18}O,4n|g), 100 {I20} from ({+11}B,4n|g) and 100 {I6} from ({+11}B,5n|g). 
M D+Q intraband |g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI from (|a,6n|g). Other I|g: 42 {I9} from ({+18}O,4n|g), 34 {I6} from ({+11}B,4n|g) and 18 {I4} from ({+11}B,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI weighted average of 73 {I19} from ({+18}O,4n|g), 46 {I17} from ({+11}B,4n|g), 60 {I4} from (|a,6n|g) and 76 {I10} from ({+11}B,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI weighted average of 47 {I9} from ({+18}O,4n|g), 30 {I6} from ({+11}B,4n|g) and 49 {I7} from ({+11}B,5n|g). Unweighted average is 42 {I6}. Other I(459|g):I(241|g)=22.0 {I19}:100.0 {I17} from (|a,6n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E weighted average from ({+11}B,5n|g) and ({+18}O,4n|g). 
RI weighted average from ({+11}B,5n|g), ({+18}O,4n|g) and (|a,6n|g). Other I(237|g):I(448|g)=139 {I16}:100 {I16} in ({+11}B,4n|g). 


decay_energy_unit: KEV
decay_multipolarity: [E2]
decay_comment:
E weighted average from ({+18}O,4n|g) and ({+11}B,4n|g). Other E|g: 500.4 {I2} from ({+11}B,5n|g). 
RI I(258|g):I(499|g) is 100 {I10}:73 {I15} in ({+18}O,4n|g), 100 {I9}:100 {I18} in ({+11}B,4n|g), 100 {I9}:50 {I9} in ({+11}B,5n|g), 100 {I4}:23 {I5} in (|a,6n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI unweighted average of 68 {I19} from ({+18}O,4n|g), 80 {I26} from ({+11}B,4n|g), 66 {I4} from (|a,6n|g) and 92 {I13} from ({+11}B,5n|g); the weighted average is 68 {I4}. 


decay_energy_unit: KEV
decay_multipolarity: (Q)
decay_comment:
I(1045|g):I(851|g):(633|g)=100 {I30}:36 {I10}:30 {I11} in ({+18}O,4n|g) but 6 {I13}:13 {I9}:100 {I24} in ({+11}B,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
RI unweighted average of 48 {I14} from ({+18}O,4n|g), 69 {I15} from ({+11}B,4n|g), 33 {I7} from (|a,6n|g) and 66 {I7} from ({+11}B,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E weighted average from ({+18}O,4n|g) and ({+11}B,4n|g). 
RI weighted average of 82 {I28} from ({+18}O,4n|g), 57 {I16} from ({+11}B,4n|g) and 52 {I7} from (|a,6n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI unweighted average of 15 {I4} from ({+18}O,4n|g) and 47 {I8} from ({+11}B,5n|g). Weighted average is 21 {I13}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
M,MR from |a(K)exp and |a(L)exp in ({+11}B.5n|g). |d=0.17 {I+47-17} from |a(K)exp, |<0.31 from |a(L)exp. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR from |a(K)exp and |a(L)exp in ({+11}B,5n|g). |d=1.0 {I+15-6} from |a(K)exp, |<0.7 from |a(L)exp. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
I|g=63.3 {I17}, 4.03 {I12}, 0.0393 {I10} and |a=7.80, 138.2, 1.415E4, respectively, if mult=E1, M1, E2. 
B(E1)(W.u.)=6.7|*10{+-9} {I12} if E1, B(M1)(W.u.)=4.4|*10{+-8} {I8} if M1, B(E2)(W.u.)=5.6|*10{+-4} {I16} if E2, assuming I(|g+ce)(56)=I(|g+ce)(165.2) in ({+11}B,5n|g). Alternatively, B(E1)(W.u.)=6.3|*10{+-9} {I12} if E1, B(M1)(W.u.)=4.2|*10{+-8} {I8} if M1, B(E2)(W.u.)=5.3|*10{+-4} {I15} if E2, assuming I(|g+ce)(56)=I(|g+ce)(362|g+706|g) in ({+11}B,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
I|g=56 {I9} or 89 {I4}, 13.0 {I21} or 20.7 {I10}, 1.43 {I22} or 2.28 {I12} and |a=0.3525, 4.828, 52.1, respectively, if mult=E1, M1, E2 depending on whether I(|g+ce)(56) is deduced from I(|g+ce) deexciting the 5352 or 5186 level in ({+11}B,5n|g). 
B(E1)(W.u.)=2.0|*10{+-10} {I4} if E1, B(M1)(W.u.)=4.8|*10{+-9} {I9} if M1, B(E2)(W.u.)=7.0|*10{+-5} {I14} if E2, assuming I(|g+ce)(56)=I(|g+ce)(165.2) in ({+11}B,5n|g). Alternatively, B(E1)(W.u.)=2.98|*10{+-10} {I25} if E1, B(M1)(W.u.)=7.2|*10{+-9} {I7} if M1, B(E2)(W.u.)=1.05|*10{+-4} {I12} if E2, assuming I(|g+ce)(56)=I(|g+ce)(362|g+706|g) in ({+11}B,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
|a=0.0388, 0.4137, 0.1645, respectively, if mult=E1, M1, E2. 
B(E1)(W.u.)=4.2|*10{+-12} {I4} if E1, B(M1)(W.u.)=4.4|*10{+-10} {I5} if M1, B(E2)(W.u.)=3.1|*10{+-6} {I3} if E2, assuming I(|g+ce)(56)=I(|g+ce)(165.2) in ({+11}B,5n|g). Alternatively, B(E1)(W.u.)=4.1|*10{+-10} {I4} if E1, B(M1)(W.u.)=4.1|*10{+-10} {I4} if M1, B(E2)(W.u.)=2.9|*10{+-6} {I3} if E2, assuming I(|g+ce)(56)=I(|g+ce)(362|g+706|g) in ({+11}B,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M since relatively little direct feeding to levels at the bottom of a band would be expected in this reaction, I(|g+ce)(65.3|g) should be comparable to I(|g+ce)(169|g)=118 {I6}; if so, |a(exp)(65.3|g)|?0.5, compared with |a(E1)=0.23, |a(M1)=3.08 and |a(E2)=24.8, thus favoring mult=E1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E line contaminated by close-lying, unplaced 119|g. 
M |a(exp)=3.7 {I7} from intensity balance (2002Th12). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
M E1 from level scheme; however, I(|g+ce) balance at 3542 level implies |a(exp)(264.7|g)=0.55 {I15} consistent with mult=M1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
Coincident with transitions in K|p=33/2- band. 
M I(|g+ce) balance at 5186 level implies |a(exp)(165.2)=0.75 {I28}, mult=E2(+M1), but level scheme requires E1. Possibly I|g is unreliable due to proximity of transitions with similar E|g. 


decay_energy_unit: KEV
decay_uncertain: S
decay_comment:
E from level energy difference. 
RI based on I(|g+ce) deexciting the 5389 level, I(|g+ce)(18)=323 {I9}, so I|g=36.7 {I10} if E1 (|a=7.80), 2.32 {I7} if M1 (|a=138.2) or 0.0228 {I6} if E2 (|a=1.415E4). 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
Placement shown as uncertain due to inconsistent coincidences with transitions in band(s) below the 5408 level (2002Th12). 
RI based on I(|g+ce) deexciting the 5186 level, I(|g+ce)(56)=70 {I4}, so I|g=52 {I3} if E1 (|a=0.3525), 12.0 {I6} if M1 (|a=4.828) or 1.32 {I7} (|a=52.1) if E2. However, based on I(|g+ce) deexciting the 5351 level, I(|g+ce)(56)=44 {I7} if mult=E1 for 165.2|g, implying I|g(56|g)=33 {I5} if E1, 7.6 {I12} if M1, 0.83 {I15} if E2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$from {+170}Er({+14}N,4n|g), {+181}Ta(|a,5n|g). Other: 2.6 {I5} from {+176}Yb({+10}B,6n|g),{+174}Yb({+11}B,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g). Other: 10.7 {I16} in {+170}Er({+14}N,4n|g), {+181}Ta(|a,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from {+170}Er({+14}N,4n|g), {+181}Ta(|a,5n|g). Other: I|g(145|g)/I|g(301.5|g)=4.1 {I36} in {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from {+176}Yb({+10}B,6n|g),{+174}Yb({+11}B,5n|g). Other: 143 {I21} in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from {+176}Yb({+10}B,6n|g),{+174}Yb({+11}B,5n|g). 261.5|g is multiply placed with undivided intensity in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g). Other: 140 {I30} in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from {+176}Yb({+10}B,6n|g),{+174}Yb({+11}B,5n|g). 261|g is multiply placed with undivided intensity in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$from {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g). Other: 130 {I15} in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g). Other: 175 {I60} in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from |a(K)exp in {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g). Other: +0.6 {I3} from |g(|q) in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g). Other: 324.5 {I2} in {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g). Other: 626.1 {I2} in {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g). Other: 116 {I21} from {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$from {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g). Other: 22 {I18} from {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g). Other: 160 {I40} from {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from {+176}Yb({+10}B,6n|g),{+176}Yb({+11}B,5n|g). Other: 150 {I40} from {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
E$transition observed by 1968Ha39 but not placed. Placement by evaluator on the basis of multipolarity, closeness in energy to calculated value of 36 keV by 1974Si14, and apparent E2 enhancement, which is consistent with this |g being the lowest member of the decoupled rotational band 1/2[541]. 
RI calculated from ce(L23) and |a(L23) (1968Ha39) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$calculated from ce data of 1968Ha39 and |a. I|g=21 {I6} from 1971Ak03 is too large to be consistent with the intensity balance. Contamination from neighboring Re x rays is possible. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
RI$or 60.4 
I|g(delayed)=5.0 
DCO=1.5 {I1} for doublet 
A{-2}=-0.18 {I4} for 281.4|g + 281.9|g multiplet. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_uncertain: ?
decay_comment:
E$see {+181}Os |e decay (105 min) for discussion of placement of this transition. 
M$from {+181}Os |e decay (105 min) 
RI$estimated by evaluator from intensity balance at the 390.7 level and |a. 


decay_energy_unit: KEV
decay_multipolarity: (Q)
decay_comment:
RI$total=5.8 {I14} for E|g=576.1 and 576.3 
$Assignment disagrees with that in {+176}Yb({+11}B,6n|g). Not in adopted gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$L1:L2:L3:M1:M2:M3:N::39 {I4}: 3.90 {I20}: 0.82 {I9}: 8.9 {I3}: 1.07 {I4}: 0.241 {I14}: 2.8 {I6} (1973Sv01). Others: L1:L2:L3:M::18.1:2.34:0.61:5.45 (1968Ha39), L1:L2:L3:M1:M2:M3::50.0:4.8:1.3:7.2:0.72:0.24 (1970Ak02), L1=36 {I4} (1973Bu08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$ ICE(K)=3.73 20 (1973Sv01). OTHERS: 1.73 (1968Ha39), 4.4 (1970Ak02), 3.6 8 (1973Bu08). 
M$K:L1+L2:L3:M:N::3.73 {I20}:<0.9:<0.25:0.156 {I18}:0.057 {I14} (1973Sv01). Other: K:L1:L3:M::1.73:0.35:<0.14:0.14 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
$ ICE(K)=0.08 3 (1973Sv01). OTHERS: 0.09 (1968Ha39), AP 0.05 (1970Ak02) 
RI$other: <1.5 (1973Sv01); this |g also coincides with another decay (1973Sv01). 
M,MR$K:L1+L2:L3::0.08 {I3}:<0.043:<0.0021 (1973Sv01). Other: K/L1=0.09/0.024 (1968Ha39). E2 is not ruled out by conversion data, |DJ|p requires E1 or E1+M2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$other: 2.7 {I12} (1973Sv01) 
M$M1:M2:M3:N:O::9.0 {I15}: 0.97 {I20}: 0.15 {I6}: 2.3 {I3}: 0.35 {I7} (1973Sv01). Others: L1:L2:L3:M::13.0:1.82:0.43:4.24 (1968Ha39), L1=40 {I8} (1973Bu08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$1973Bu08 quote I|g<0.02 and consider this |g as suspect. 1968Ha39 report weak K and L1 conversion lines corresponding to a 208.1. Placement of this |g in 1968Ha39 from 554 to 346 levels is rejected here since there seems no evidence for the population of a 346 level. 
$Ice(K)=0.0040 {I12} (1973Sv01). 1968Ha39 report both the K and L1 ce lines as weak. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$ ICE(K)=0.34 4 (1973Bu08). OTHERS: 0.355 (1973Sv01,1968Ha39), 0.37 (1970Ak02), 
M,MR$K:L1:L2:L3:M::0.355:0.045 {I6}:<0.0075:<0.013:0.014 {I4} (1973Sv01). Others: K:L1:L2:L3:M::0.355:0.05:0.012:0.010:0.02 (1968Ha39), K/L1=0.37/0.041 (1970Ak02). 


decay_energy_unit: KEV
decay_multipolarity: (M1)
decay_comment:
E,M$from Ice(M1)|?1.4 and Ice(M2)|?0.9 (1973Bu08). From comparison (by the evaluators) of M1/M2 experimental ratio with the calculated value from theory (using either HSICC or BrIcc codes), mult=M1+E2, |d|?2.4 or E1+M2, |d|?0.2; but adopted |D|p requires M1+E2. 1973Bu08 assign M1 
TI$deduced from intensity balance (evaluators) assuming no net |e feeding to the 269 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$Placement from 1970Ak02 and 1973Bu08. 1973Sv01 place it from a tentative 620 level; 1968Ha39 place it from a 346 level 
$ ICE(K)=1.32 11 (1973Sv01). OTHERS: 0.76 (1968Ha39), AP 1.9 (1970Ak02,1973Bu08). 
RI$0.7 (1973Sv01) for 110.46+111.39 
M$K:L2:M::0.76:|?0.024:0.045 (1968Ha39). Other: K/M=1.32 {I11}/0.043 {I18} (1973Sv01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$ AVERAGE ICE(K)=3.0 11 FROM ICE(K)=1.9 (1968Ha39), AP 4.1 (1970Ak02). OTHER: ICE(K)<3.9 (1973Sv01). 
M$K:L1:L2:L3:M:N:O::<3.9:<1.0:<0.43:<0.02:0.147 {I13}:0.043 {I6}:0.009 {I6} (1973Sv01). Other: K:L1:L3:M::1.90:|?0.26:0.02:0.12 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
$ ICE(K)=0.13 (1968Ha39). OTHER: <0.23 (1973Sv01). 
M$K:L1:L2::<0.23:<0.09:0.005 {I4} (1973Sv01). Other: K/L1=0.13:0.06 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$ ICE(K)=0.019 4 (1973Sv01). OTHERS: 0.033 (1968Ha39), 0.02 (1970Ak02). 
M,MR$K/L1+L2=0.019 {I4}/<0.010 (1973Sv01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$ ICE(K) AP 0.6 (1970Ak02). OTHERS: <1.0 (1973Sv01), AP 0.24 (1968Ha39) 
M,MR$from L1/M ratio. K:L1:M::<1.0:0.055 {I14}:0.028 {I4} (1973Sv01) other: K:L1:M::|?0.24:0.045:|?0.02 (1968Ha39). 
$ PLACEMENT FROM 554 TO 379 BY 1968Ha39 IS REJECTED 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$ ICE(K)=0.075 (1970Ak02). OTHERS: <0.09 (1973Sv01), 0.023 (1968Ha39), 
M$K/L1=<0.09/0.010 {I3} (1973Sv01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$L1:L2:L3:M:N::0.116 {I13}:0.025 {I6}:0.032 {I7}:0.036 {I9}:0.009 {I5} (1973Sv01). Others: K:L1:L2:L3:M::<0.61:0.08:0.030:0.036:0.035 (1968Ha39), K:L1:L2:L3::|?0.9:0.12:0.028:0.036 (1970Ak02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
$Placement from 1970Ak02 and 1973Bu08. 1973Sv01 place it from a tentative 620 level 
$ ICE(K) AP 0.06 (1970Ak02). OTHERS: <0.25 (1973Sv01), <0.14 (1968Ha39) 
M,MR$K/L1=<0.14/0.019 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
$ ICE(K)=0.068 9 (1973Sv01). OTHERS: 0.07 (1968Ha39), 0.04 (1970Ak02) 
M,MR$K:L1:L2:L3::0.068 {I9}:<0.012:<0.003:<0.002 (1973Sv01). Other: K:L1:L3:M::0.07:0.02:|?0.004:0.008 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$ ICE(K)=0.081 6 (1973Sv01). OTHERS: 0.10 (1968Ha39), 0.075 (1970Ak02), 0.08 2 (1973Bu08) 
M,MR$K:L1:L2:L3:M::0.081 {I6}:0.012 {I3}:<0.006:0.0021 {I11}:0.004 {I2} (1973Sv01). Other: K:L1:L2:M::0.10:0.019:<0.012:0.009 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$|a(K)(M1)=0.0499 used as normalization for ce data for other |g rays 
$ ICE(K)=5.23 20 (1973Sv01). OTHERS: 4.5 (1968Ha39), 5.8 (1970Ak02), 5.4 5 (1973Bu08). 
M,MR$K:L1+L2:L3:M:N::5.23 {I20}:0.84 {I4}:<0.01:0.198 {I9}:0.058 {I5} (1973Sv01). Others: K:L1+L2:M:N::5.8:0.88:0.19:0.04 (1970Ak02), K/L1=4.50/0.76 (1969Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
RI$0.7 (1973Sv01) for 110.46+111.39 
$ ICE(K)=0.245 25 (1973Sv01), 0.12 (1968Ha39). 
M,MR$K:L1:L2:L3::0.12:0.16:|?0.03:0.26 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$ICE(K)=0.0214 13 (1973Sv01). OTHERS: 0.037 (1968Ha39), 0.03 (1970Ak02) 
M,MR$K:L1+L2:L3::0.0214 {I13}:0.0043 {I7}:<0.0005 (1973Sv01). Other: K/L1=0.037/|?0.009 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$ ICE(K)=0.025 3 (1973Sv01). OTHERS: AP 0.033 (1968Ha39), 0.025 (1970Ak02). 
M,MR$K:L1+L2:L3::0.025 {I3}:0.0042 {I5}:<0.0005 (1973Sv01). Other: K/L1=|?0.033/0.007 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$ ICE(K)=0.65 4 (1973Sv01). OTHERS: 0.48 (1968Ha39), 0.47 (1970Ak02), 0.59 20 (1973Bu08). 
M$K; L1:L2:L3:M:N::0.65 {I4}:0.103 {I14}:0.0088 {I20}:<0.0021:<0.046:0.0064 {I11} (1973Sv01). Others: K:L1:L3:M::0.48:0.11:0.010:0.038 (1968Ha39), K:L1:L2:M::0.47:0.10:0.005:0.010 (1970Ak02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E weighted average of 114.48 {I7} from (|a,2n|g), 114.43 {I5} from |e decay (13.0 h), 114.48 {I16} from IT decay (1.04 ms), 114.35 {I7} from |e decay (9.9 h) and 114.5 {I1} from ({+11}B,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E weighted average of 145.31 {I11} from (|a,2n|g), 145.39 {I2} from |e decay (13.0 h), 145.35 {I12} from IT decay (1.04 ms) and 145.3 {I1} from ({+11}B,4n|g). 
RI from ({+11}B,4n|g). 
Other |d: 0.12 {I+6-12} from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E weighted average of 259.92 {I5} from |e decay (13.0 h), 259.8 {I1} from ({+11}B,4n|g). Other E|g: 258.8 {I3} from (|a,2n|g). 
RI unweighted average of 17.6 {I8} from ({+11}B,4n|g), 33 {I9} from (|a,2n|g) and 12.6 {I6} from |e decay (13.0 h). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E weighted average of 175.38 {I9} from (|a,2n|g), 175.370 {I25} from |e decay (13.0 h), 175.3 {I2} from IT decay (1.04 ms) and 175.3 {I1} from ({+11}B,4n|g). 
Other mult.: D+Q intraband |g from (|a,2n|g). 
Other |d: 0.15 {I3} from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E weighted average of 320.92 {I17} from (|a,2n|g), 320.80 {I8} from |e decay (13.0 h), 321.1 {I3} from IT decay (1.04 ms) and 320.8 {I1} from ({+11}B,4n|g). 
RI unweighted average of 32.1 {I10} from ({+11}B,4n|g), 26.6 {I18} from (|a,2n|g), 28 {I4} from |e decay (13.0 h) and 26 {I6} from IT decay (1.04 ms). 
M Q intraband |g from (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E weighted average of 236.2 {I3} from (|a,2n|g), 236.41 {I5} from |e decay (13.0 h), 236.5 {I1} from ({+11}B,4n|g). 
RI from |e decay (13.0 h). Other I|g: 4.7 {I7} from ({+11}B,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E weighted average of 381.88 {I19} from (|a,2n|g), 381.74 {I5} from |e decay (13.0 h), 381.7 {I1} from ({+11}B,4n|g). 
RI from |e decay (13.0 h). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
E weighted average of 496.4 {I7} from (|a,2n|g), 496.37 {I5} from |e decay (13.0 h). 
RI from |e decay (13.0 h). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E weighted average of 484.59 {I24} from (|a,2n|g), 484.49 {I5} from |e decay (9.9 h), 484.3 {I1} from ({+11}B,4n|g). 
M from |e decay; D from (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E weighted average of 203.73 {I10} from (|a,2n|g), 203.84 {I10} from |e decay (13.0 h), 203.9 {I2} from IT decay (1.04 ms) and 203.7 {I1} from ({+11}B,4n|g). 
M D+Q from (|a,2n|g) for intraband |g. 
Other |d: 0.14 {I+3-4} from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E unweighted average of 380.0 {I4} from (|a,2n|g), 379.1 {I3} from IT decay (1.04 ms) and 379.2 {I1} from ({+11}B,4n|g). Other E|g: 379.18 {I20} from |e decay (13.0 h), presumably for contaminated line. 
RI unweighted average of 51 {I13} from IT decay (1.04 ms), 15.7 {I10} from (|a,2n|g), 35 {I10} from |e decay (13.0 h), 53.1 {I16} from ({+11}B,4n|g). (the weighted average is 26 {I10}.) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E weighted average of 167.90 {I11} from (|a,2n|g), 167.85 {I2} from |e decay (13.0 h), 167.8 {I1} from ({+11}B,4n|g). 
MR from |g(|q) in (|a,2n|g); other |d: 0.14 {I7} from |e decay (13.0 h). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
Other I(737|g):I(851|g)=68 {I20}:100 {I20} in (|a,2n|g) where 355|g and 592|g branches were not seen. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E weighted average of 197.05 {I15} from (|a,2n|g), 197.10 {I4} from |e decay (13.0 h), 197.0 {I1} from ({+11}B,4n|g). 
RI from (|a,xn|g). 
MR from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E weighted average of 365.20 {I25} from (|a,2n|g), 364.925 {I23} from |e decay (13.0 h), 364.8 {I1} from ({+11}B,4n|g). 
RI unweighted average of 8.8 {I21} from (|a,2n|g), 7.5 {I14} from |e decay (13.0 h) and 12.5 {I12} from ({+11}B,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
E weighted average of 231.29 {I11} from (|a,2n|g), 231.6 {I2} from IT decay (1.04 ms) and 231.5 {I1} from ({+11}B,4n|g). 
MR from |d=0.10 {I+4-10} from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E weighted average of 435.45 {I20} from (|a,2n|g), 435.5 {I3} from IT decay (1.04 ms) and 435.2 {I1} from ({+11}B,4n|g). 
RI from ({+11}B,4n|g). Other I|g: 75 {I3} from (|a,2n|g), 74 {I15} from IT decay (1.04 ms). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E weighted average of 223.6 {I1} from ({+11}B,4n|g) and 223.48 {I11} from (|a,2n|g). 
RI weighted average of 100 {I3} from ({+11}B,4n|g) and 100 {I3} from (|a,2n|g). 
Other |d: 0.12 {I+6-12} from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E weighted average of 420.7 {I1} from ({+11}B,4n|g) and 420.48 {I11} from (|a,2n|g). 
RI unweighted average of 33.9 {I24} from ({+11}B,4n|g) and 29.1 {I3} from (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
E unweighted average of 256.43 {I21} in (|a,2n|g), 256.9 {I1} in ({+11}B,4n|g) and 257.4 {I2} in IT decay (1.04 ms). 
RI weighted average from (|a,2n|g), IT decay (1.04 ms) and ({+11}B,4n|g). 
MR 0.14 {I+5-10} from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E unweighted average of 488.2 {I3} in (|a,2n|g), 488.4 {I1} in ({+11}B,4n|g) and 487.9 {I3} in IT decay (1.04 ms). 
RI unweighted average of 75 {I7} from (|a,2n|g), 90 {I19} from IT decay (1.04 ms) and 101.9 {I21} in ({+11}B,4n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
Other E|g (I|g): 180.78 {I25} (440 {I100}) in |e decay (13.0 h) suggests that |g may have been contaminated in that study. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
E weighted average of 250.09 {I14} from (|a,2n|g) and 250.3 {I1} from ({+11}B,4n|g). 
RI weighted average from (|a,2n|g) and ({+11}B,4n|g). 
MR 0.10 {I+4-10} from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E weighted average of 474.2 {I3} from (|a,2n|g) and 473.9 {I1} from ({+11}B,4n|g). 
RI unweighted average of 43 {I4} from ({+11}B,4n|g) and 24 {I4} from (|a,2n|g); the weighted average is 30 {I10}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
E weighted average of 282.3 {I1} from ({+11}B,4n|g), 282.20 {I18} from (|a,2n|g) and 202.3 {I3} from IT decay (1.04 ms). 
RI unweighted average of 87 {I5} from (|a,2n|g), 76 {I3} from ({+11}B,4n|g) and 63 {I19} from IT decay (1.04 ms). 
MR 0.39 {I+20-39} from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E unweighted average of 539.1 {I1} from ({+11}B,4n|g), 539.32 {I23} from (|a,2n|g) and 538.1 {I3} from IT decay (1.04 ms). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E,RI weighted average from (|a,2n|g) (E|g=273.35 {I18}) and from ({+11}B,4n|g) (E|g=273.2 {I1}). 
M D+Q intraband |g from (|a,2n|g). 
MR from |g(|q) in (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E unweighted average of 523.5 {I1} from ({+11}B,4n|g) and 524.5 {I4} from (|a,2n|g). 
RI unweighted average of 61 {I5} from ({+11}B,4n|g) and 75 {I7} from (|a,2n|g). 
M (Q) intraband |g from (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
Other E|g (I|g): 304.2 {I2} (55 {I11}) in IT decay (1.04 ms) and 304.45 {I15} (121 {I6}) from (|a,2n|g). 
M D+Q intraband |g from (|a,2n|g). 
MR from (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
Other E|g: 584.9 {I3} from IT decay (1.04 ms), 586.1 {I4} from (|a,2n|g). 
M (Q) intraband |g from (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=AP;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=AP
decay_comment:
E weighted average of 193.89 {I16} from (|a,2n|g) and 193.8 {I1} from ({+11}B,4n|g) and 193.9 {I2} from IT decay. 
M from |a(K)exp in {+183}Re IT decay (1.04 ms). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E weighted average of 630.7 {I4} from (|a,2n|g) and 630.2 {I1} from ({+11}B,4n|g). 
M (Q) intraband |g from (|a,2n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E from level-energy difference; |g not resolved by 1981Av04 and 1966Em02 do not state E|g. 
RI From I(145|g) in 1981Av04 and I(|g+ce)(145|g):I(|g+ce)(259|g) \=82:6 from 1966Em02. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
Other I(|g+ce)(257|g):I(|g+ce)(488|g)=47:42 (1966Em02). 
RI may include I(259|g)=7; see comment on 260|g from 260 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M |a(K)exp=0.20 {I7}; K/L reported to be consistent with E2, but actual value not stated (1966Em02). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |a(K)exp=2.5, K:L1:L2:L3=5.6:1:0.17:0.065 (1970Ak01). L1:L2:L3:M1:N1:O1=6.5:1.0:0.36:1.5:0.44:0.13 (1960Ne03). K:L1:L2:L3:M=6320:1135:190:74:370 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |a(K)exp=1.42 (1970Ak01). K:L1:L2:L3:M1=1.6:0.32:0.055:0.02:0.10 (1960Ne03). K:L1:L2:L3:M=360:62:9.5:3.5:22 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M |a(K)exp=0.12 (1970Ak01). K:L12:L3=0.020:0.006:0.006 (1960Ne03). K:L2:L3:M=4.8:|?2:1.3:1.3 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M K:L1=7:1 (1970Ak01). K:L1:L2:L3:M1:N1=1.00:0.12:0.02:0.018:0.032:0.014 (1960Ne03). K:L1:L2:L3:M=240:40:|?7:5.8:12 (1968Ha39). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |a(K)exp=0.89, K:L1:L2=5:1:0.13 (1970Ak01). K:L1:L2:M1:N1=5.9:1.3:0.17:1.00:0.47 (1960Ne03). K:L1:L2: =1000:215:|?25:<106 (1968Ha39). 


decay_energy_unit: KEV
decay_multipolarity: [M1]
decay_comment:
RI I|g=0.45 {I11} (1983Br24) is inconsistent with intensity balance through the 955-keV level. Authors indicate that this transition may include a component from {+183}Os(13 h) decay. The adopted I(|g+ce) is calculated from the intensity balance through the 955-keV level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
E from 1970Ak01; not reported by 1983Br24. 
M L1/L2=9 (1970Ak01); |a(L1)exp=2.9. L1:L2=65:7.5 (1968Ha39). 
From 1960Ne03, 1968Ha39, and 1970Ak01. |d calculated from L1/L2=65/7.5 (1968Ha39) and I|g from relative electron intensities (1968Ha39,1970Ak01) and adopted |a. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M A{-2}=-0.056 {I14}, A{-4}=+0.013 {I14} (1968Ne01); A{-2}=+0.01 {I5}, A{-4}=+0.18 {I4} (1974Si14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M A{-2}=+0.032 {I25}, A{-4}=-0.007 {I25} (1968Ne01); A{-2}=-0.15 {I10}, A{-4}=+0.05 {I5} (1974Si14). . 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
E from 1968Ne01. 
RI I(236|g):I(382|g)=4.1 {I6}:115 {I15} (1968Ne01). 
M A{-2}=-0.09 {I13}, A{-4}=-0.17 {I13} (1968Ne01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M A{-2}=-0.054 {I10}, A{-4}=-0.008 {I10} (1968Ne01); A{-2}=-0.07 {I2}, A{-4}=-0.05 {I3} (1974Si14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E weighted average from 1968Ne01 and 1974Si14. 
M A{-2}=-0.03 {I3}, A{-4}=+0.03 {I3} (1968Ne01); A{-2}=-0.03 {I2} (1974Si14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M A{-2}=-0.016 {I30}, A{-4}=-0.020 {I30} (1968Ne01); A{-2}=-0.05 {I5}, A{-4}=+0.09 {I8} (1974Si14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M A{-2}=-0.003 {I20}, A{-4}=+0.011 {I20} (1968Ne01); A{-2}=-0.05 {I2}, A{-4}=-0.03 {I5} (1974Si14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M A{-2}=+0.06 {I12}, A{-4}=-0.18 {I13} (1968Ne01); A{-2}=+0.11 {I10}, A{-4}=-0.05 {I10} (1974Si14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E weighted average from 1968Ne01 and 1974Si14. 
M A{-2}=+0.10 {I4}, A{-4}=-0.02 {I5} (1968Ne01); A{-2}=+0.03 {I8}, A{-4}=-0.03 {I5} (1974Si14). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$deduced by compiler from data in 2000Pu01. Value of 5 {I4} listed in Table 1 of 2017Gu23 seems a misprint 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E5)
decay_BE_unit: e^2 x (fm)^10
decay_BE_info: ;TYPE=BE5;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE5W
decay_comment:
E|g from level energy difference, I|g from IT decay. 
M from subshell ratios in IT decay, mult=E3,E4 or E5; level scheme requires mult=E5. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
M not E1 from |a(exp)=3.8 {I10} from ({+7}Li,3n|g), but |a(exp) is lower than expected from theory for M1 or E2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
%I|g=13.6 {I3} assuming recommended normalization. 
E from 1988BuZD. Other E|g: 104.729 {I7} (1973Ag07). 
RI from 1974Mc08. 
M L1/L3=14.7 {I+27-20}, |a(K)exp=4.1 {I8} (1973Ag07); K:L1:L3:M:N=24.0:3.2:0.29:1.8:0.28 (1968Ag01). 
MR from |g(|q,H,T) (1973Hu06). Others: +0.226 {I14} (1973Kr01), 0.190 {I17} (1973Ag07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M4
decay_comment:
E from 1988BuZD. Other E|g: 83.28 {I4} (1973Ag07). 
M from L-subshell ratios: L1:L2:L3=0.275 {I19}:0.053 {I10}:1.000 (1974Mc08); L1/L2=4.3 {I10}, L1/L3=0.24 {I3}, L2/L3=0.06 {I1} (1973Ag07); L1/L2=5.5 {I3}, L2/L3=0.044 {I4} (1974Ga35); (L1+L2)/L3=0.295 {I13} (1973Ca08). L1:L2:L3:M:N=7.2:2.4:20.0:>9.0:3.0 (1968Ag01). 
TI from I(|g+ce)(83|g)=I(|g+ce)(105|g) based on the decay scheme. 
RI from I(|g+ce) and |a. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E5)
decay_comment:
E from level energy difference. 
TI from I(|g+ce)(188|g)/I(|g+ce)(83|g)=0.00069 (1974Ga35); uncertainty not stated by authors. 
RI from I(|g+ce) and |a. 
M from L1/L2<0.2 and L2/L3=1.8 {I8} (1974Ga35), mult=E3,E4 or E5. From decay scheme, mult=E5. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E from {+185}Os |e decay (1977Br22). Other values from {+185}W |b{+-} decay: 125 keV |b|g coin scin (1958Ar04), 126 keV {I2} scin (1958Bi39), 125.22 keV {I4} Ge(Li) (1971BrXV). Others: 1957Du49, 1957Wi16. 
RI measured absolute intensities: %I|g=0.0192 {I7} (1992Ke02); %I|g=0.0186 {I38}, from %I(|g+ce)=0.070 {I14} (1970Sh09) and |a(125|g)=2.76. 
M from ce data in {+185}Os |e decay. 
MR value recommended by 1976Kr21, based on +0.176 {I17} (1966As02), +0.186 {I12} (1970St08), and +0.186 {I19} (1972Be41), measured in {+185}Os |e decay. |d=0.187 {I37} deduced by 1981El11 from measured A{-2} and A{-4} angular correlation coefficients of 1970St08 and 1972Be41. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR value recommended by 1976Kr21 and derived from +0.176 {I17} (1966As02), +0.186 {I12} (1970St08), and +0.186 {I19} (1972Be41). |d=0.187 {I37} derived by 1981El11 from measured A{-2} and A{-4} angular correlation coefficients of 1970St08 and 1972Be41 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
RI from 1971Be78. 
Transition was observed by 1968Ha39 in ce spectrum and by 1971Be78 in |g|g-coincidence spectrum. 1977Br22 identified the peak at 121.2 keV as due to x-ray summing. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
RI I|g<2 from 1969Co16. This transition was observed by 1968Ha39 in ce spectrum with Ice(K)(157.7|g)/Ice(K)(646.1|g)=0.0032. However, 1969Co16 did not observe it in their ce and |g spectra; upper limits were given: Ice(K)(157.7|g)/Ice(K)(646.1|g)<0.0004, I|g(157.7|g)<2. 1971Be78 measured I|g(157.7|g)=2|+1. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
RI I|g<2 from 1969Co16. Weak K line of this transition was observed by 1968Ha39. 1969Co16 did not observe any ce line nor photon belonging to a 229.1-keV transition. Upper limits were Ice(K)(229|g)/Ice(K)(646|g)<0.0004; I|g(229|g)/I|g(646|g)<0.0002. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$other values: 6.8 {I6} (1969Co16), 6.75 (1970Pl04), 6.7 {I3} (1970Sc06). I|g=6.17 {I13} (1977Br22) is possibly a typographical error. Evaluator used a value of 6.71 {I13} for averaging. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
MR from adopted gammas. Other value: +0.176 {I17} from {+185}Re(p,p'|g) (1966As02). 
E$from {+185}Os |e decay. E|g's measured in Coulomb excitation: 126 {I1} (1957Wo32), 128 {I2} (1958Mc02), 128 {I1} (1959De29). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from from {+185}Re(p,p'|g) (1966As02). Other values: +0.16 {I4} (1958Mc02), +0.188 {I6} (1959De29). 
E$from {+186}W(d,3n|g) reaction. E|g's measured in Coulomb excitation: 160 {I2} (1957Wo32), 159 {I2} (1958Mc02), 159 {I2} (1959De29). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$from {+186}W(d,3n|g) reaction. E|g's measured in Coulomb excitation: 286 {I3} (1957Wo32), 287 {I4} (1958Mc02), 287 {I4} (1959De29). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
E|g and multipolarity from {+185}Os |e decay. E|g=645 {I15} was measured by 1960Na13 in Coulomb excitation. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
The width of the strong 242.9-keV |g-ray was 0.15 keV larger than expected. This indicates the presence of another |g with about the same energy. From the expected energy of the 15/2- member of the 9/2[514] band, the weaker |g of this doublet was assigned by 1971Ev02 to deexcite a 15/2- level at 1000 keV. The method of obtaining its intensity was not explained by 1971Ev02. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E1(+M2)
decay_comment:
M,MR$From |a{-tot}=0.55 {I27} from intensity balance at the 2009 level. |a{-tot}=0.59 {I23} if both the 317|g and 599|g have mult=M1, and 0.50 {I22} if they are both mult=E1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR Average of 0.146 {I6} (from intensity balance through 59-keV level in IT decay (1972Se06) and 0.124 {I+33-45} from subshell ratios in (n,|g) E=thermal (1969La11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E5)
decay_comment:
$B(E5)(W.u.)=0.069 exceeds RUL=0 
E$Deduced according to energy-level difference from precision measurement of (8{++}) isomer in 2015Ma60. 
M$From {+186}Re IT decay (1972Se06). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$ce(L1) peak is complex and assigned M1 in 1969La11. Statistical-model calculations also suggest pure M1 (|d=0) transition based on level intensity balance in 2016Ma35. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$Multiply-placed |g; I|g estimated from statistical-model analysis (2016Ma35); see 691-keV level. 
RI$Other value also in (n,|g): 11.5 {I23} in 1969La11 (undivided I|g); <5.7 in 2020Kr05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$Multiply-paced |g with unresolved I|g (1969La11); not observed in 2016Ma35; see 463-keV level. Questionable placement of |g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E 40.29 from 1972Se06. 
MR adopted value; weighted average of 0.146 {I6} from intensity balance through 59-keV level (1972Se06) and 0.124 {I+33-45} in (n,|g) E=thermal (1969La11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I(|g+ce)=17.5 {I11} 
RI$Other: 13.0 {I13} (1969La11) 
M$Ice(L1):Ice(L2):Ice(L3):Ice(N)=38.5 {I58}:4.5 {I9}:0.60 {I18}:4.20 {I42} (1969La11); reported as pure M1 in 2015BeZX. Ice(M) obscured by Ice(K) (127.4 transition). 
MR$Average of the deduced upper and lower limits and corresponds to an an E2 admixture of 0.2%, consistent with M1+<0.8%E2 reported in Table 3. of 1969La11. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I(|g+ce)=2.2 {I5} 
RI$Other: 1.44 {I22} (1969La11) 
M$Ice(L1):Ice(L2):Ice(L3):Ice(M):Ice(N)=20 {I5}:4.0 {I14}:2.1 {I6}: 5.3 {I16}:1.0 {I7} (1969La11) 
MR$consistent with |d=0.146 {I6} from intensity balance through 59-keV level (1972Se06) using Ice(M) from 1969La11 even though Ice(K) (109.5 transition) is superimposed onto the region. |d reported as M1+(1+1.6, 1-0.6) percent E2 in 1969La11. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$I(|g+ce)=0.47 {I9} 
RI$Other: 0.51 {I8} (1969La11) 
M$Ice(L1):Ice(L2):Ice(L3)=0.16 {I10}:0.68 {I7}:0.51 {I8} (1969La11). Ice(K) is obscured by Ice(L1) (40.4 transition); corrected Ice(K) intensity is significantly smaller than statistical uncertainty (1969La11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
$I(|g+ce)=2.38 {I14} 
RI$Other: 2.0 {I2} (1969La11) 
MR$Consistent with |d=0; deduced upper limit corresponds to an E2 admixture of 1.9% consistent with M1(+ <4 perecent E2) reported in Table 3 of 1969La11. 
M$Ice(K):Ice(L1):Ice(L3):Ice(M)=9.7 {I34}:1.80 {I18}:<0.20:0.350 {I35} (1969La11); pure M1 in (2015BeZX). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I(|g+ce)=0.95 {I7} 
RI$Other: 1.50 {I15} (1969La11) 
M$Ice(L1):Ice(L2):Ice(L3):Ice(M)=1.40 {I10}:0.26 {I8}:0.20 {I7}:0.45 {I9} (1969La11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_uncertain: S
decay_comment:
$I(|g+ce)=7|*10{+-5} {ILE} 
RI$Deduced from statistical-model calculations in 2016Ma35. 
E$Reported as an expected transition deduced from energy-level differences in 2016Ma35; 3-keV uncertainty assumed by evaluators. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_uncertain: S
decay_comment:
$I(|g+ce)=5|*10{+-3} {ILE} 
RI$Deduced from statistical-model calculations in 2016Ma35. 
E$Reported as an expected transition deduced from energy-level differences in 2016Ma35; 3-keV uncertainty assumed by evaluators. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
$I(|g+ce)=1.28 {I18} 
RI$Other: 1.37 {I14} (1969La11) 
M$Ice(K):Ice(L1)=3.3 {I15}:0.81 {I8} (1969La11); Ice from higher-order subshells indistinguishable due to interference from several overlapping lines. 
MR$Consistent with |d=0. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I(|g+ce)=2.45 {I14} 
RI$Other: 2.80 {I28} (1969La11); 2.73 {I22} (2020Kr05). 
$|a(K)exp: from Ice(K)=1.62 {I36} of 1969La11 after correction by evaluators for contamination by Ice(L1)(92.1 transition)=0.48 {I17}. Typographical error: listed as "L2" in column 20 of Table 3 in 1969La11. 
$|a(L1)exp: from Ice(L1) |< 0.33 of 1969La11 after correction by evaluators for contamination by Ice(K)(210.7 transition)=1.60 {I16}. 
Ice(M) obscured by Ice(K)(219.8 transition) and Ice(K)(220.5 transition). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$I(|g+ce)=3.05 {I18} 
RI$Other: 3.30 {I33} (1969La11); 3.36 {I28} (2020Kr05). 
M$Ice(L1):Ice(M)=0.28 {I4}:0.076 {I15} (1969La11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I(|g+ce)=0.36 {I9} 
RI$Other: 0.30 {I5} (1969La11); 0.32 {I16} (2020Kr05) 
M$Ice(K)=0.11 {I4} (1969La11); reported as E2 in 1969La11. 
MR$Average of the deduced upper and lower limits. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I(|g+ce)=0.76 {I17} 
RI$Other: 0.69 {I10} (1969La11); 0.74 {I12} (2020Kr05) 
M$Ice(L1)=0.085 {I43} (1969La11); Ice(K) obscured by Ice(M) (59.0 transition). 


