# DECAY

decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$Pol=-0.42 {I11} (1978Eg02), -0.09 {I4} (1976Ro06) 
RI$I|g(263.8)/I|g(917.6)/I|g(3219.2)=15 {I1}/73 {I2}/12 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=negative, Pol=-0.28 (1976Pr15) 
M,MR$from 1976Bi15. +0.09 from 1976Pr15 
RI$ REVERSE BRANCHING IN 1980Ke01 SEEMS A MISPRINT (SEE BRANCHING IN 1976Br15 FROM THE SAME GROUP AS 76% 8 FOR 507G) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
I|g(1462)/I|g(1525)/I|g(1964)=48 {I3}/44 {I3}/7.5 {I20} (1976Be13) 
|d(Q/D)=-0.96 {I10} for J(4715)=4 (1976Be13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
|r=0.34 {I3} (1976Ul01). Other: 0.41 {I4} (1961Be19) 
TI$from 1976Ul01 
M$from the shape of the positron spectrum and the ratio I(e{+|+})/I(ce(K))=9.0 {I18} (1961Be19) 
I(CEK)=10, I(e{+|+})=90 18 (1961Be19) I(e{+|+})/IG(313G)=0.00205 17 (1976Ul01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
(3300p)(899|g)(|q): A{-2}=-0.04 {I4}, A{-4}=-0.12 {I8} 
(3300p)(1523|g)(|q): A{-2}=-0.02 {I6}, A{-4}=+0.03 {I9} 
(3300p)(2422|g)(|q): A{-2}=+0.05 {I9}, A{-4}=-0.10 {I11} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E3]
decay_uncertain: ?
decay_comment:
(3440p)(1523|g)(|q): A{-2}=+0.23 {I2}, A{-4}=-0.07 {I2} 
(3440p)(2422|g)(|q): A{-2}=+0.55 {I10}, A{-4}=-0.40 {I13} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$(4000p)(1523|g)(|q): A{-2}=+0.20 {I5}, A{-4}=+0.35 {I6} 
$(4000p)(899|g)(|q): A{-2}=+0.03 {I10}, A{-4}=+0.12 {I12} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 0.0070 {I12} (1985Da04), 0.0103 {I31} (1980Sa32), 0.0079 {I20} (1977In04). Others: 0.0022 {I17} (1978De08, same laboratory as 1985Da04), 1971Ke14 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
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$100 {I8} for {+208}Pb target, 100 {I10} for {+197}Au target (2018Ha10) 
$E2 matrix element=+0.205 eb {I6} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
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$6.9 {I3} for {+208}Pb target, 6.9 {I5} for {+197}Au target (2018Ha10) 
$E2 matrix element=+0.222 eb {I11} 


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:
$The 587|g was too weak to be seen in the experiment, yet by including this transition in GOSIA analysis of Coul. ex. data, 2016Ha23 could determine its E2 matrix element and B(E2)(W.u.) 
$Branching ratio for 587|g=0.36% {I+15-8}, deduced by compiler from level T{-1/2}=0.214 ps {I47} and B(E2)|_(587|g)=0.0135 {I+57-29} 
$E2 matrix element=+0.26 eb {I+5-3}. This can be compared with <1.0 in {+42}Ca Adopted dataset in the ENSDF database 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$0.99 {I10} for {+197}Au target (2018Ha10) 
$E2 matrix element=-0.237 eb {I+23-27} 
$M1 matrix element=+0.97 |m{-N} (2018Ha10) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$0.28 {I8} for {+208}Pb target, 0.39 {I19} for {+197}Au target (2018Ha10) 
$I|g(2424)/I|g(899)=0.35 {I7} was measured by the authors in {+12}C({+32}S,2p){+42}Ca reaction using the EAGLE Compton-suppressed HPGe detector array at the Heavy Ion laboratory of the University of Warsaw. Compiler's note: corresponding value is 0.43 {I3} in {+42}Ca Adopted dataset in the ENSDF database (May 2016 update) 
$E2 matrix element=-0.064 eb {I3} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$0.93 {I7} for {+208}Pb target, 1.29 {I13} for {+197}Au target (2018Ha10) 
$E2 matrix element=+0.243 eb {I12} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$0.28 {I8} for {+208}Pb target, 0.45 {I13} for {+197}Au target (2018Ha10) 
$|d(M3/E2)=+0.05 {I4} 
$E2 matrix element=+0.42 eb {I+3-4} 


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$0.192 {I11} was deduced by 1978En02 from B(E2)=8.7|*10{+-3} {I7} (1971HoYN) and T{-1/2}=48 ps {I4}. Using the same B(E2) and T{-1/2}=34 ps {I3}, evaluators get |d=0.161 {I14}. Sign from |g(|q, lin) in (|a,n|g). |d=-0.15 {I3} from ({+3}He,|a|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$unweighted average of 6.7 {I4} from |b{+-} decay, 15.1 {I5} from (|a,n|g) and 4.8 {I8} from (p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$from Adopted Gammas; sign(|d) from |g(|q,pol) 
A{-2}=+0.01 {I1}, A{-4}=-0.02 {I1}. Pol=-0.06 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.50 {I25} for J=5/2; +0.8 {I+4-10} for J=3/2 
A{-2}=-0.48 {I1}, A{-4}=+0.01 {I1}. Pol=+0.01 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.20 {I5} for J=5/2; >+11, or <-5.6 for J=3/2 
A{-2}=+0.11 {I2}, A{-4}=+0.01 {I2}. Pol=+0.35 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_comment:
MR$0.00 {I2} for 19/2+ to 15/2+; +0.7 {I1} for 15/2+ to 15/2+ 
A{-2}=+0.37 {I5}, A{-4}=-0.19 {I6}. Pol=+0.37 {I25} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
MR$-0.03 {I2}; +0.07 {I3}; -0.11 {I2} for different J|p values 
A{-2}=-0.28 {I3}, A{-4}=-0.01 {I4}. Pol=-0.33 {I18} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
MR$-0.02 {I3}; +0.06 {I3}; +0.09 {I3} for different J|p values 
A{-2}=-0.27 {I4}, A{-4}=-0.05 {I5}. Pol=-0.40 {I17} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
B(E2)=0.0071 {I3} (1971HoYN), deduced from known lifetime of 593 level and measured (but not quoted) branching ratio 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
|d(Q/D)=+0.10 {I7} for J=3/2, -0.62 {I10} for J=5/2. But adopted J|p(2877)=1/2- 
A{-2}=-0.21 {I8}, A{-4}=-0.12 {I14} 


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$weighted average of 1157.002 {I3} from {+44}K |b{+-} decay, 1157.022 {I15} from {+44}Sc |e decay (4.0420 h), 1157.002 {I15} from {+44}Sc |e decay (58.61 h), 1157 {I1} from ({+16}O,2p|g), 1157.0 {I2} from ({+18}O,2p2n|g), 1157.031 {I15} from ({+14}C,|a2n|g), 1156.89 {I15} from (n,|g) E=thermal, 1158 {I1} from (p,p'|g), and 1155.9 {I5} from (|m{+-},n|g) 
M$|DJ=2, Q |g from DCO in ({+18}O,2p2n|g); M2 rejected by RUL 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_uncertain: S
decay_comment:
TI$branching deduced by the evaluators from q{-|K}{+2}(E0/E2)=I{-K}(E0)/I{-K}(E2)=0.54 {I9} and assuming 80% K-shell conversion of E0 transition. 
$q{-|K}{+2}(E0/E2)=0.54 {I9}, X(E0/E2)=0.23 {I4}, |r{+2}(E0)=0.14 {I5} (2005Ki02 evaluation). 
$|G(pair formation)/|G=8.8|*10{+-4} {I14} from (p,p') (1976Ul01); |G(pair formation)=2.1|*10{+-8} eV {I3} from (e,e') (1978Gr02). 


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$weighted average of 1126.076 {I10} from {+44}K |b{+-} decay, 1126.084 {I20} from {+44}Sc |e decay (58.61 h), and 1126.092 {I40} from ({+14}C,|a2n|g). Others: 1126 {I1} from ({+16}O,2p|g), 1126.1 {I2} from ({+18}O,2p2n|g), 1126.03 {I15} from (n,|g) E=thermal, 1127 {I1} from (p,p'|g), and 1124.1 {I7} from (|m{+-},n|g) 
M,MR$|d(O/Q)=-0.05 {I+4-3} from p|g(|q) in (p,p'|g); M2, M3 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from {+44}Sc |e decay (4.0420 h). Others: 1499.45 {I4} from {+44}K |b{+-} decay, 1499.4 {I3} from ({+18}O,2p2n|g), 1499.30 {I18} from (n,|g) E=thermal, 1501 {I2} from (p,p'|g), and 1510 {I10} from (|m{+-},n|g) 
RI$from {+44}Sc |e decay (4.0420 h). Others: 100.0 {I37} from {+44}K |b{+-} decay and 100.0 {I25} from (p,p'|g) 
M,MR$|d(Q/D) is weighted average of -0.15 {I+4-9} (1970La09) and -0.14 {I7} (1966Ma31) in (p,p'|g), -0.137 {I17} (1968Wa21), and -0.07 {I3} (1971Ok03) in {+44}Sc |e decay (4.0420 h); E1+M2 ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 2656.41 {I3} from {+44}K |b{+-} decay, 2656.48 {I4} from {+44}Sc |e decay (4.0420 h), 2656.2 {I5} from (n,|g) E=thermal, and 2656 {I3} from (p,p'|g) 
RI$weighted average of 12.52 {I59} from {+44}K |b{+-} decay, 12.31 {I33} from {+44}Sc |e decay (4.0420 h), and 17.0 {I38} from (p,p'|g) 
M$Q from p|g(|q) in (p,p'|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 761.10 {I3} from {+44}K |b{+-} decay, 761.3 {I1} from ({+18}O,2p2n|g), and 761.19 {I10} from (n,|g) E=thermal. Others: 761.19 {I20} from ({+14}C,|a2n|g) and 764 {I1} from (p,p'|g) 
RI$from ({+14}C,|a2n|g). Others: 100 {I50} from {+44}K |b{+-} decay, 100.0 {I52} from ({+18}O,2p2n|g), and 100.0 {I79} from (p,p'|g) 
M,MR$|d(Q/D) from weighted average of -0.18 {I8} from ({+14}C,|a2n|g) and -0.25 {I+9-31} from (p,p'|g); E1+M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1887.21 {I28} from {+44}K |b{+-} decay, 1887.3 {I2} from ({+18}O,2p2n|g), 1887.45 {I20} from ({+14}C,|a2n|g), and 1887.3 {I3} from (n,|g) E=thermal. Other: 1890 {I2} from (p,p'|g) 
RI$weighted average of 100 {I50} from {+44}K |b{+-} decay, 93.1 {I69} from ({+18}O,2p2n|g), 85.4 {I42} from ({+14}C,|a2n|g), and 95.9 {I30} from (p,p'|g) 
M,MR$|d(O/Q)=-0.08 {I+3-6} from (p,p'|g); M2,M3 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1001.876 {I20} from {+44}Sc |e decay (58.61 h), 1001.9 {I1} from ({+18}O,2p2n|g), and 1001.850 {I31} from ({+14}C,|a2n|g). Others: 1001 {I1} from ({+16}O,2p|g) and 1001.85 {I15} from (n,|g) E=thermal 
M$Q, |DJ=2 from DCO in ({+18}O,2p2n|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E$weighted average of 2144.23 {I8} from {+44}K |b{+-} decay, 2144.33 {I10} from {+44}Sc |e decay (4.0420 h), 2144.5 {I5} from (n,|g) E=thermal, and 2144 {I2} from (p,p'|g) 
RI$others: 100 {I19} from {+44}Sc |e decay (4.0420 h) and 100.0 {I90} from (p,p'|g) 
$B(M1)(W.u.)=0.044 {I+40-16} if M1, B(E2)(W.u.)=27 {I+24-10} if E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 3301.21 {I14} from {+44}K |b{+-} decay, 3301.35 {I6} from {+44}Sc |e decay (4.0420 h), 3301.5 {I6} from (n,|g) E=thermal, and 3304 {I4} from (p,p'|g) 
RI$weighted average of 42.6 {I70} from {+44}K |b{+-} decay, 38 {I11} from {+44}Sc |e decay (4.0420 h), and 49.3 {I75} from (p,p'|g) 
M$Q from p|g(|q) in (p,p'|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$weighted average of 651.355 {I9} from {+44}K |b{+-} decay, 651.07 {I12} from (n,|g) E=thermal, and 652 {I1} from (p,p'|g) 
RI$weighted average of 13.30 {I51} from {+44}K |b{+-} decay and 6.8 {I41} from (p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$others: 1024.4 {I3} from ({+18}O,2p2n|g), 1024.66 {I20} from (n,|g) E=thermal, and 1026 {I1} from (p,p'|g). 
RI$other: 28.4 {I68} from (p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$weighted average of 2150.786 {I17} from {+44}K |b{+-} decay, 2150.840 {I22} from {+44}Sc |e decay (4.0420 h), 2150.5 {I2} from ({+18}O,2p2n|g), 2150.9 {I3} from (n,|g) E=thermal, and 2150 {I2} from (p,p'|g) 
RI$others: 100.0 {I74} from ({+18}O,2p2n|g) and 100.0 {I81} from (p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$unweighted average of 2423.3 {I6} from {+44}K |b{+-} decay and 2429 {I2} from (p,p'|g) 
M$(Q) from p|g(|q) in (p,p'|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$from (pol |g,|g'). Other: 1780 {I2} from (p,p'|g) 
M$D from p|g(|q) in (p,p'|g); |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$others: 3661.3 {I2} from (pol |g,|g') and 3659 {I4} from (p,p'|g) 
M$D from p|g(|q) in (p,p'|g); |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 368.207 {I14} from {+44}K |b{+-} decay, 368.8 {I3} from (n,|g) E=thermal, and 367 {I1} from (p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 1019.55 {I7} from {+44}K |b{+-} decay, 1017.8 {I7} from (n,|g) E=thermal, and 1015 {I1} from (p,p'|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:
E$weighted average of 403.86 {I20} from {+44}K |b{+-} decay, 404.4 {I3} from ({+18}O,2p2n|g), and 404.34 {I10} from (n,|g) E=thermal 
RI$from ({+18}O,2p2n|g). Other: 100 {I27} from {+44}K |b{+-} decay 
M$D, |DJ=1 from DCO in ({+18}O,2p2n|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
E$weighted average of 1428.7 {I4} from {+44}K |b{+-} decay, 1428.8 {I3} from ({+18}O,2p2n|g), and 1428.56 {I25} from (n,|g) E=thermal 
RI$from ({+18}O,2p2n|g). Other: 36 {I18} from {+44}K |b{+-} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=GT
decay_comment:
E$others: 2619.1 {I5} from (n,|g) E=thermal and 2617 {I4} from (p,p'|g) 
RI$from (p,p'|g). Other: 100 {I20} from {+44}K |b{+-} decay 
M$D+Q from (p,p'|g); |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E,RI$from ({+18}O,2p2n|g) require a T{-1/2}>44 ps. 
$B(M1)(W.u.)<0.041 if M1 
$B(E2)(W.u.)<2767 upper limit exceeds RUL=100 if E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
$B(M2)(W.u.)<1013 upper limit exceeds RUL=3 {I14}, RUL=3 would require a T{-1/2}>0.11 ns 
E$unweighted average of 628.9 {I1} from ({+18}O,2p2n|g), 628.53 {I9} from ({+14}C,|a2n|g), and 628.69 {I10} from (n,|g) E=thermal 
RI$weighted average of 92.1 {I32} from ({+18}O,2p2n|g) and 100 {I11} from ({+14}C,|a2n|g) 
M,MR$D+Q from |g(|q) in ({+14}C,|a2n|g); |D|p=yes from level scheme. |DJ=1 from DCO in ({+18}O,2p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
E$weighted average of 869.5 {I2} from ({+18}O,2p2n|g) and 869.45 {I15} from (n,|g) E=thermal 
RI$from ({+18}O,2p2n|g) 
M$D, |DJ=1 from DCO in ({+18}O,2p2n|g); |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 1809.1 {I4} from ({+18}O,2p2n|g) and 1808.9 {I5} from (n,|g) E=thermal 
RI$from ({+18}O,2p2n|g). Other: 48 from (n,|g) E=thermal 
M$from DCO in ({+18}O,2p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E$other: 3040 from (p,p'|g); not seen in (|g,|g') 
RI$from (p,p'|g) 
$B(M1)(W.u.)=0.0036 {I+9-11} if M1, B(E2)(W.u.)=1.09 {I+28-31} if E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from (|g,|g'), also seen in (p,p'|g). but this |g is not seen in (n,|g) E=thermal. It is likely a different level is populated in (n,|g) E=thermal 
RI$from (p,p'|g). 
M$Q from p|g(|q) in (p,p'|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 651.0 {I3} from ({+18}O,2p2n|g) 
RI$from (n,|g) E=thermal, where the 651.07|g is a doubly placed with intensity not divided. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Placement of this transition in (n,|g) E=thermal is considered unlikely by evaluators from the implied high mult=E5 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2982.47 {I15} from {+44}K |b{+-} decay and 2982.3 {I3} from (pol |g,|g') 
RI$other: 79 {I27} from (pol |g,|g') 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from ({+14}C,|a2n|g). Others: 1802 {I1} from ({+16}O,2p|g) and 1802.6 {I2} from ({+18}O,2p2n|g) 
M$Q, |DJ=2 from DCO in ({+18}O,2p2n|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$other: 3300.8 {I8} with I|g=4.6 {I9} unplaced in 1973In02; also a 3304.1 {I8} with I|g=3.8 {I8} placed from 3304 level in 1973In02 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$other: 682.2 {I6} with I|g=9.4 {I19} (1973In02) 
ASSIGNMENT FROM 4315 LEVEL (TABLE I IN 1976Co06) IS A MISPRINT 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1157.031 {I15} (1990Me15), 1157.015 {I15} (1983Gu11), 1156.92 {I15} (1974HeYW), 1156.9 {I6} (1973Si05), 1157.0 {I3} (1970Ei07), 1156.6 {I5} (1968Wa21). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1126.092 {I40} (1990Me15), 1126.079 {I20} (1983Gu11), 1126.18 {I15} (1974HeYW), 1127.2 {I6} (1970Ei07), 1125.7 {I5} (1968Wa21). 
$I|g(1126)/I|g(1157|g)=12.3 {I1}/100=0.0123 {I1} from the decay of g.s.+isomer mixture (1990Me15,1976Co06), 0.01254 {I22} (1983Gu11), 0.0108 {I20} (1974HeYW), 0.0120 {I7} (1968Wa21), <0.027 (1973Si05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1001.850 {I31} (1990Me15), 1001.888 {I20} (1983Gu11), 1001.86 {I15} (1974HeYW), 1001.5 {I10} (1970Ei07), 1001.8 {I5} (1968Wa21). 
$I|g(1002)/I|g(1157|g)=12.3 {I1}/100 from the decay of g.s.+isomer mixture (1990Me15,1976Co06), 0.01237 {I13} (1983Gu11), 0.0114 {I25} (1974HeYW), 0.0120 {I7} (1968Wa21), <0.027 (1973Si05) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$unresolved with a more intense transition from {+47}Sc (1986Wa19); quoted value is from level-energy difference 
RI$from <9.3 {I7} (1986Wa19) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_uncertain: S
decay_comment:
$1885.1 4, |s=0.00077 b 23 (2007ChZX), assignment of this |g in 2007ChZX is incorrect since 1883.5 is an E0 transition 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
E$other: 1159 {I3} from 2016Ca17 
M$from the Adopted Levels, Gammas dataset 
$B(E2)(W.u.)=9.7 {I9} (2003Sc21), from measured lifetime 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$rounded value from the Adopted Gammas. This |g with a branching of 90% was not seen by 2016Ca17, but an upper limit of 95 counts was stated by the authors from the detection sensitivity in their |g-ray spectrum 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1157.031 {I15} (1990Me15), 1157.015 {I15} (1983Gu11), 1156.92 {I15} (1974HeYW), 1156.9 {I6} (1973Si05), 1157.0 {I3} (1970Ei07), 1156.6 {I5} (1968Wa21). 
RI$from 1990Me15. Other: 1000 (1983Gu11), 1000 {I5} (1974HeYW), 1000 {I5} (1968Wa21) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1499.489 {I25} (1990Me15), 1499.436 {I15} (1983Gu11), 1499.20 {I20} (1974HeYW), 1499.4 {I3} (1973Si05), 1499.6 {I6} (1970Ei07), 1499.0 {I5} (1968Wa21). 
RI$weighted average of 9.0 {I2} (1990Me15), 9.22 {I37} (1983Gu11), 9.0 {I10} (1974HeYW), 9.1 {I4} (1973Si05), 9.2 {I5} (1968Wa21), 9.12 {I15} (1990Sc08). 
MR$values from this dataset: -0.137 {I17} (1968Wa21), -0.07 {I3} (1971Ok03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 2656.478 {I30} (1990Me15), 2656.435 {I50} (1983Gu11), 2657.14 {I20} (1974HeYW), 2656.4 {I5} (1973Si05), 2656.6 {I6} (1970Ei07), 2655.9 {I8} (1968Wa21). 
RI$weighted average of 1.11 {I4} (1990Me15), 1.11 {I3} (1983Gu11), 1.4 {I5} (1974HeYW), 1.3 {I1} (1973Si05), 0.9 {I1} (1968Wa21), 1.15 {I6} 1990Sc08. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2144.3 {I1} (1990Me15), 2144.43 {I20} (1983Gu11), 2144.8 {I8} (1973Si05) 
RI$weighted average of 0.02 {I2} (1990Me15), 0.039 {I7} (1973Si05). Other: 0.035 (1983Gu11). Accurate value is lacking due to large corrections to this peak from single escape of 2656.5|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 3301.3 {I1} (1990Me15), 3301.361 {I55} (1983Gu11), 3301.6 {I15} (1973Si05) 
RI$unweighted average of 0.0064 {I8} (1990Me15), 0.016 {I2} (1983Gu11), 0.018 {I3} (1973Si05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$from {+44}K decay (1976Co06,1990Me15) 
RI$|g ray reported by 1976Co06 (1990Me15) only. Its existence and assignment is considered (evaluator) uncertain due to lack of confirmation in other studies of {+44}Sc decay 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR$from |g(|q) 
$|G(E2)=0.0038 eV (1986Be30) which corresponds to B(E2)|_=0.00042 e{+2}b{+2} {I8} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M D+Q from |g|g(|q). Ne E1+M2 from |d's and comparison to RUL 
MR -0.26 {I8} or -2.0 {I4} from |g|g(|q) in (n,|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI weighted ave. (ext.) from (n,|g) E=thermal and |b{+-} decay branching ratios in Table IV of 1980Hu10 
M D+Q from |g(|q) in (n,|g). M1+E2 from |D|p=no 
MR -0.01 {I4} or +4.0 {I7} from (pol n,|g) and (n,|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI weighted ave. (int.) from (n,|g) E=thermal and |b{+-} decay branching ratios in Table IV of 1980Hu10 
M D+Q from |g|g(|q). Ne E1+M2 from |d and comparison to RUL 
MR weighted av from (pol n,|g), (n,|g) and (d,p|g). Others: weighted av of +8 {I3} from (n,|g) and (d,p|g) ruled out by CP(pol n,|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI weighted ave. (ext.) from (n,|g) E=thermal and |b{+-} decay branching ratios in Table IV of 1980Hu10 


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:
M D,Q from comparison to RUL. E1,M2 from |D|p=yes. Probably not E1 since B(E1)|_(W.u.)=3.2|*10{+-9} {I10} is |?1 order of magnitude less than values previously compiled ({ICf.} Fig. 1 of 1979En04) 


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:
M D,Q,E3 from comparison to RUL. E1,M2 from |DJ|p|<2,yes. Probably not E1 since B(E1)|_(W.u.)=6.7|*10{+-10} {I17} is |?1 order of magnitude less than values previously compiled ({ICf.} Fig. 1 of 1979En04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI unresolved contaminant with I|g|?300. I|g from |g|g spectra 
A{-2}=+68 {I9}, A{-4}=-11 {I12} for composite peak 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from {+46}K |b{+-} decay: data set #2; 2285 {I3} from {+46}K |b{+-} decay: data set #1 is inconsistent with 2268 separation of adopted levels. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M$(1229|g)(1858|g)(|q): A{-2}=-0.124 {I23}, A{-4}=-0.038 {I34} 
MR$-0.03 {I2} for J(4432)=3 and 1.00 {I6} for J(4432)=4 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M$(4189|g)(1346|g)(|q): A{-2}=-0.044 {I10}, A{-4}=-0.004 {I16} 
MR$0.38 {I2} for J(5535)=2 or 0.03 {I1} for J(5535)=3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M$(4366|g)(1346|g)(|q): A{-2}=0.200 {I19}, A{-4}=-0.011 {I28} 
MR$0.06 {I2} for J(5712)=2 or 0.45 {I5} or 1.47 {I5} for J(5715)=3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M$(4765|g)(1346|g)(|q): A{-2}=-0.216 {I27}, A{-4}=0.056 {I40} 
MR$0.70 {I3} for J(6111)=2 or -0.17 {I5} for J(6111)=3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
1984Al18 warn that this assignment is speculative. Another possible placement is from the {+50}Ti 5186-keV state in {+50}Sc 0.35-sec |b{+-} decay 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$ from Adopted dataset of {+47}Ca in ENSDF database, based on data in 1984Al18 (reference 57 in 2012Mo11). Uncertainty of 18.4 listed in table I of 2012Mo11 is in error 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M2
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
RI$ from Adopted dataset of {+47}Ca in ENSDF database, based on data in 1984Al18 (reference 57 in 2012Mo11). Uncertainty of 13.1 listed in table I of 2012Mo11 is in error 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$ from Adopted dataset of {+47}Ca in ENSDF database, based on data in 1984Al18 (reference 57 in 2012Mo11). Uncertainty=2.4 listed in table I of 2012Mo11 
$ |g(|q) is isotropic consistent with 1/2+ assignment for 2599.7 level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_BE_unit: e^2 x (fm)^6
decay_BE_info: ;TYPE=BE3;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE3W
decay_comment:
E$ doublet-peak structure in |g spectrum 
RI$ from Adopted dataset of {+47}Ca in ENSDF database, taken from 1984Al18. 2012Mo11 list <2 with source reference 1984Al18, but this value if from an earlier paper 1970Wa29 (same group as 1984Al18). According to an e-mail reply of April 14, 2012 from S. Leoni (corresponding author of 2012Mo11), value of <2 is preferred, since branching ratio of 1.29 {I9} gives too high a B(E3)(W.u.) value 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
$Branching ratios=99 {I1} 
$1373.1|g-564.9|g(|q): A{-2}=-0.05 {I3} 
MR$0.36 {I+7-6} or 10 {I+17-4} for J=3/2, -0.03 {I7} or 5 {I+3-1} for J=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:
E$weighted average of 3831.3 {I2} from (|g,|g') and 3832.2 {I5} from (n,n'|g). 
M$Q from p|g(|q) in (p,p'|g) and M2 ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from (n,n'|g). Other: 451.9 {I5} from (p,p'|g). 
RI$from (p,p'|g). Other: 100 {I13} from {+49}K |b{+-}n decay. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_uncertain: S
decay_comment:
M$from observation of E0 e+/e- pair emission to g.s. 
$q{-K}{+2}(E0/E2)=0.95 {I4}; X(E0/E2)=0.0503 {I19}; |r{+2}(E0)=0.0145 {I9} (2005Ki02,1970Be39). 
$|w(E0)=4.817|*10{+10}; |w(E0)(K)=1.342|*10{+8}; |w(E0)(ipf)=4.817|*10{+10}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$unweighted average of 671.4 {I1} from (n,n'|g) and 672.1 {I2} from (p,p'|g). 
M$Q from |g(|q) in (n,n'|g); M2 ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from (n,n'|g). Other: 675.0 {I1} from (p,p'|g). 
RI$from (p,p'|g). Others: 100 {I4} from {+48}K |b{+-} decay and 100 {I8} from (n,n'|g). 
M,MR$D(+Q) and |d from p|g(|q) in (p,p'|g); |D|p=yes from level scheme. 


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:
RI$unweighted average of 22 {I6} from {+48}K |b{+-} decay, 25.0 {I28} from (n,n'|g), and 37.0 {I28} from (p,p'|g). 
RI$I|g(4507|g)/I|g(675|g)=0.37 {I3} from (p,p'|g) discrepant, 0.22 {I6} from |b{+-} decay consistent. 
M$O from p|g(|q) in (p,p'|g); M3 ruled out by RUL. 


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$weighted average of 780.1 {I1} from (n,n'|g) and 780.4 {I2} from (p,p'|g). 
M$D from |g|g(|q) in (p,p'|g) and |g(|q) in (n,n'|g); |D|p=(no) from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$other: I(648|g)/I(754|g)=100 {I20}/41 {I20} from (p,p'|g) is discrepant. 
M$D from |g(|q) in (n,n'|g); |D|p=(yes) from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$other: 753.9 from ({+48}Ca,{+48}Ca'|g). 
M$D from |g(|q) in (n,n'|g); |D|p=(no) from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI$other: 6.3 {I4} from {+48}K |b{+-} decay is discrepant. 
M$D from |g(|q) in (n,n'|g); |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_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 29 {I4} from {+48}K |b{+-} decay and 30 {I4} from (n,n'|g). Other: 67 {I17} from (p,p'|g) is discrepant. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$level-energy difference=866.16 
RI$weighted average of 23 {I4} from {+48}K |b{+-} decay and 28.6 {I32} from (n,n'|g). 
M$D from |g(|q) in (n,n'|g); |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_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$from {+48}K |b{+-} decay. Others: 100 {I9} from (n,n'|g) and 100 {I17} from (p,p'|g). 
M$D from |g(|q) in (n,n'|g); |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$level-energy difference=2073.35 
RI$weighted average of 15 {I4} from {+48}K |b{+-} decay and 26 {I9} from (n,n'|g). 
M$D from comparison to RUL; |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
RI$from {+48}K |b{+-} decay. Other: 35 {I8} from (n,n'|g). 
M$D from |g(|q) in (n,n'|g); |D|p=(no) from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
RI$from {+48}K |b{+-} decay. Other: 100 {I14} from (n,n'|g). 
M$D from |g(|q) in (n,n'|g); |D|p=(no) from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from (|g,|g'). Other: 7300.9 from {+48}K |b{+-} decay. 
RI$from {+48}K |b{+-} decay. 
M$from |g(|q) and |g asymmetry in (|g,|g'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$other: 9300 from (|a,|a'|g) and {+48}K |b{+-} decay. 
M$from |g(|q) and |g asymmetry in (|g,|g') and |a|g(|q) in (|a,|a'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1,E2)
decay_comment:
RI I|g(2249|g)/I|g(4272|g)=27 {I6}/31 {I8} (1978De17). Note discrepancy with I|g(2250|g)/I|g(4272|g)=43 {I9}/100 {I20} in (d,p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E weighted av (int) of 3123.0 {I10} (calculated by evaluator from recoil-corrected values given by 1969ArZT) and 3123.4 {I3} (2003ChZS) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$from A{-2}=+0.47 {I7}, which supports a |DJ=2 character. The measured linear polarization asymmetry of +0.05 {I8} is consistent with an electric transition 


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{-2}=+0.072 {I5}, which supports a dipole character. The measured linear polarization asymmetry with a positive value is consistent with an electric transition 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
M$3358|g(|q) consistent with |DJ=2, quadrupole transition; E2 from |D|p and polarization data from 2012Mo11 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$this |g is indicated as questionable in level-scheme Fig. 4 of 2016Ga07; also its presence is not evident in authors' spectral Fig. 1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
M$660|g(|q) consistent with |DJ=1, dipole transition; E1 from |D|p and polarization data from 2012Mo11 


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$weighted average of 1027.0 {I5} from {+50}K |b{+-} decay (472 ms), 1026.2 {I3} from ({+238}U,X|g), and 1026.7 {I1} from ({+48}Ca,X|g). Others: 1027 {I1} from {+51}K |b{+-}n decay (365 ms), 1027 {I1} from {+52}K |b{+-}2n decay (110 ms), and 1028 {I2} from ({+50}Ca,p'|g) 
M$|g(|q) and linear polarization in {+208}Pb({+48}Ca,X|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E$from |b{+-} decay. Other: 1976 {I1} from |b{+-}n decay; 1978.2 {I6} in {+48}Ca({+238}U,X|g) is discrepant, possibly due to Doppler-shift effects. It is possible that 1978,2|g defined a level separate from 3002, (2+), but there is no strong evidence for its existence 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2504.9 {I5} from {+50}K |b{+-} decay (472 ms) and 2503 {I1} from {+51}K |b{+-}n decay (365 ms) 
RI$from {+50}K |b{+-} decay . Other: 100 {I17} from |b{+-}n decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3531.8 {I5} from {+50}K |b{+-} decay (472 ms) and 3530 {I2} from {+51}K |b{+-}n decay (365 ms) 
RI$from {+50}K |b{+-} decay . Other: 133 {I17} from |b{+-}n decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 2964 {I8} from ({+50}Ca,p'|g), 2971.4 {I6} from ({+238}U,X|g), and 2970.2 {I2} from ({+48}Ca,X|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 3008.9 {I5} from {+50}K |b{+-} decay and 3008 {I2} from {+51}K |b{+-}n decay 
RI$from {+50}K |b{+-} decay. Others: 60 {I20} from {+51}K |b{+-}n decay and 75 {I25} from ({+50}Ca,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 4035.6 {I5} from {+50}K |b{+-} decay and 4035 {I2} from {+51}K |b{+-}n decay. Other: 4030 {I18} from ({+50}Ca,p'|g) 
RI$from {+50}K |b{+-} decay. Others: 100 {I20} from {+51}K |b{+-}n decay, and 100 {I25} from ({+50}Ca,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 603 {I11} from ({+50}Ca,p'|g), 595.5 {I3} from ({+238}U,X|g), and 594.8 {I1} from ({+48}Ca,X|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(3009)/I|g(4030)=44 {I12}/56 {I15}; note that this ratio is reversed in table I of 2014Ri04, which is probably a misprint 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$from {+238}U({+48}Ca,X|g) 
E$Others: 2379.0 {I13} in {+48}Ca({+238}U,X|g), 2377 {I1} in {+51}K |b{+-}n decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$from {+238}U({+48}Ca,x|g) 
E$Others: 3437 {I6} in {+48}Ca({+238}U,X|g), 3460 {I2} in {+51}K |b{+-}n decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$intensity/100 decays of {+51}K (2006Pe16) 
E$From 2006Pe16. Other: 3460, |DE and I|g are not given (1983RaZR) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1738 {I17} in {+1}H({+54}Ca,pn|g) and 1753 {I15} in {+9}Be({+55}Sc,{+53}Ca|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
$|G{-|g}=0.048 
E$from 1977Ko10. 
M$from A{-2}=+0.52 {I3}, A{-4}=-0.06 {I5}, POL=+0.12 {I3} (1977Ko10). 
MR$from 1977Ko10. Other: 0.04 {I+12-4} (1968Yo04). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$|G{-|g}=0.044 
MR,TI$for 5/2; |d=0.035 {I+17-35} and |G{-|g}=0.026 eV for J=9/2 (1968Yo04). 
M,MR$from A{-2}=-0.395 {I17}, A{-4}=+0.02 {I3} (1968Yo04) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
$|G{-|g}=0.070 
M,MR$from A{-2}=+0.44 {I4}, A{-4}=-0.10 {I4} (1987Zi02). Other: A{-2}=+0.54 {I3}, A{-4}=-0.01 {I5}, |d=0.07 {I+71-7} (1968Yo04) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$|G{-|g}=0.025 
M,MR$from A{-2}=+0.46 {I4}, A{-4}=-0.27 {I4} (1987Zi02). Other: A{-2}=+0.45 {I4}, A{-4}=-0.02 {I5}, |d=0.05 {I+120-5} (1968Yo04) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M,MR$from A{-2}=+0.36 {I7}, A{-4}=-0.21 {I9} (1987Zi02). Other: |d=-1.8 {I3} is alternative solution to |g(|q) (1987Zi02). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
$|G{-|g}=0.051 
M,MR$from A{-2}=-0.10 {I4}, A{-4}=+0.01 {I5} (1987Zi02). Other: +0.035 {I+110-35} (1968Yo04) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: D+Q
decay_comment:
$|G{-|g}=0.083 
M$from A{-2}=-0.394 {I24}, A{-4}=+0.013 {I23} (1968Yo04) 
MR,TI$|d=0.16 {I+5-4} and |G{-|g} = 0.083 eV for J=5/2 and |d=0.035 {I+18-35} and |G{-|g}=0.050 eV for J=9/2 (1968Yo04) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: D+Q
decay_comment:
$|G{-|g}=0.093 
M,MR$from A{-2}=-0.408 {I23}, A{-4}=+0.03 {I3} (1968Yo04) 
MR,TI$for J=5/2; |d=0.035 {I+9-35} and I(|g+ce)=0.056 eV for J=9/2 (1968Yo04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$|G{-|g}=0.33 
M,MR$from A{-2}=-0.28 {I4}, A{-4}=-0.03 {I4} (1977Ko10). 
MR$from 1977Ko10. Other:+0.035 {I+260-35} (1968Yo04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 611.5 {I5} from 1969Ni03 and 611.2 {I2} from 1973Ha10 
M$dipole from |g(|q) (1969Ni03) and |g|g(|q) (2007Sc26); |D|p requires M1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average from 1971Ro30, 1973Ha10 and 1969Ni03 
M$from |g(|q) (1969Ni03) and RUL 
MR$|d(O/Q)=-0.01 {I3} (2007Sc26), -0.07 {I24} (1970Ba26), +0.39 {I7} or +0.25 {I7} (1969Ni03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2(+M3))
decay_comment:
M$ |g|g(|q) (2007Sc26) and RUL 
MR$or -0.16 {I12} 
E$weighted average from 1971Ro30, 1973Ha10 and 1969Ni03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average from 1971Ro30, 1973Ha10 and 1969Ni03 
$975.4 4 from 1971Ro30, 975.1 4 from 1973Ha10, 975.0 5 1969Ni03 
M,MR$from 1970Ba26. Other: |d=0.000 {I21} (2007Sc26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$others: 611.6 {I5} (1980HoZO) and 610.7 {I5} (1969Ga27) 
RI$other: I|g(611|g)/I|b(total)=0.56 {I14} (1969Al12) 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
$I|g(Mg+Mg)=100 {I4} 
$I|g(Si+Ne)=100 {I4} 
M$ 2007Ch40 assign E1 
$The A{-2} and A{-4} values assume that the decay occurs at the target position. Fitting skewed distributions gives A{-2}=-0.32 {I3}, A{-4}=-0.01 {I4} 


decay_energy_unit: KEV
decay_multipolarity: (Q)
decay_comment:
$I|g(Mg+Mg)=89 {I3} 
$I|g(Si+Ne)=90 {I3} 
M$ 2007Ch40 assign E2 
$The A{-2} and A{-4} values assume that the decay occurs at the target position. Fitting skewed distributions gives A{-2}=+0.27 {I3}, A{-4}=-0.03 {I4} 


decay_energy_unit: KEV
decay_multipolarity: (O)
decay_comment:
$I|g(Mg+Mg)=18.5 {I10} 
$I|g(Si+Ne)=19.9 {I9} 
M$ 2007Ch40 assign E3 
$The A{-2} and A{-4} values assume that the decay occurs at the target position. Fitting skewed distributions gives A{-2}=+0.59 {I5}, A{-4}=+0.13 {I7} 


decay_energy_unit: KEV
decay_multipolarity: (D)
decay_comment:
$I|g(Mg+Mg)=13.2 {I5} 
$I|g(Si+Ne)=10.5 {I4} 
M$ |DJ=(0), dipole transition 
M$ 2007Ch40 assign (E1) 


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:
M$ from |a(expt)=0.041 {I4} (1972Bi13) in {+43}Ca(p,n|g); |a(K)(expt)=0.031 {I2}, K/L(expt)=9.0 {I7} (1966WaZW) in {+40}Ca(|a,p|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ NOTE THAT IN 1998En08 AND 1978En02, BRANCHING OF 44% (TAKEN FROM 1977Di17) IS SHOWN FROM 2114 LEVEL TO 880 LEVEL, BUT IN 1977Di17 THIS BRANCHING CORRESPONDS TO DECAY TO 1158 LEVEL, INSTEAD 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$|g not seen in {+24}Mg({+24}Mg,|ap|g) and {+28}Si({+20}Ne,|ap|g) (2007Ch40) due to this transition feeding 470-ns isomer 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$average of +0.09 {I2} (1987Fr09), +0.12 {I3} (1970Ba51). Other: 0.13 (1967Ph01) 
A{-2}=-0.30 {I3} (1967Ph01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from 1970Ba51. Others: -1.18 {I7} (1987Fr09), 0.16 (1967Ph01) 
A{-2}=-0.703 {I14}, -0.44 {I3} (1967Ph01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from 1970Ba51. Others: -0.51 {I5} or -4.5 {I+12-25} (1987Fr09), 0.85 or 2.2 (1967Ph01) 
A{-2}=-0.51 {I6} (1967Ph01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
I|g(457)/I|g(1185)=23/64 (1987Fr09) 
MR$from 1970Fo06. Others: -0.28 {I10} or -1.20 {I18} (1970Ba51) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
I|g(1337)/I|g(1185)=13/64 (1987Fr09) 
MR$from 1970Ba51. Others: -0.03 {I7} (1987Fr09), +1.8 {I+7-5} (1970Ba51) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.19 {I2} for 9/2 to 7/2, +0.42 {I3} or +4.1 {I5} for 5/2 to 7/2 (1970Ba51); -0.22 {I3} or -1.37 {I6} for 9/2 to 7/2 (1987Fr09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
I|g(595)/I|g(1051)=25/75 (1987Fr09) 
MR$weighted average of -0.14 {I6} (1970Ba51), -0.24 {I4} (1970Fo06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
MR$+0.12 {I3} for 5/2 to 7/2 (1987Fr09), +0.03 {I3} or -6.9 {I+21-14} for 5/2 to 7/2 and +0.07 {I2} or >+6 or <-29 for 9/2 to 7/2 (1970Ba51) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
MR$+0.15 {I15} for 7/2 to 7/2, +0.49 {I7} for 9/2 to 7/2 (1987Fr09); -0.42 {I14} or -1.5 {I+5-7} for 5/2 to 7/2, -0.15 {I9} or +2.0 {I+5-4} for 7/2 to 5/2 and +0.36 {I7} for 9/2 to 7/2 (1970Ba51) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
MR$+0.30 {I3} for 9/2 to 7/2 (1987Fr09); +0.16 {I3} for 9/2 to 7/2 and -0.09 {I5} or -3.8 {I5} for 5/2 to 7/2 (1970Ba51) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$weak |g in 1970Ba51, but the most intense |g from this level in 1987Fr09. I|g(2833)/I|g(2104)=9 {I4}/34 {I5} (1970Ba51) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
MR$+0.01 {I5} for 15/2 to 11/2 and +0.74 {I+17-14} for 11/2 to 11/2 (1987Fr09), +0.04 {I+110-21} for 11/2 to 11/2 (1970Ba51) 
E$from 1970Sa24 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
MR$-0.48 {I12} or -1.4 {I4} for 7/2 to 9/2; -0.08 {I10} or +1.27 {I23} for 9/2 to 9/2 and +0.41 {I7} for 11/2 to 9/2 (1970Ba51). But the adopted J|p for the 3140 level is 13/2+ 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ NOTE THAT IN 1998En08 AND 1978En02, BRANCHING OF 44% (TAKEN FROM 1977Di17) IS SHOWN FROM 2114 LEVEL TO 880 LEVEL, BUT IN 1977Di17 THIS BRANCHING CORRESPONDS TO DECAY TO 1158 LEVEL 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$from Fig. 1 of 1977Di17 
RI$ NOTE THAT BRANCHING RATIOS QUOTED ON PAGE 452 OF 1977Di17 ARE INCONSISTENT WITH THOSE GIVEN IN AUTHORS' FIG. 1. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
From intensity balance, this |g-ray accounts for 80% of the total intensity, other 20% intensity is unaccounted for 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
From intensity balance, this |g-ray accounts for 25% of the total intensity, other 75% intensity is unaccounted for 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
From intensity balance, this |g-ray accounts for 60% of the total intensity, other 40% intensity is unaccounted for 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
From intensity balance, this |g-ray accounts for 70% of the total intensity, other 30% intensity is unaccounted for 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
From intensity balance, this |g-ray accounts for 50% of the total intensity, other 50% intensity is unaccounted for 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
From intensity balance, this |g-ray accounts for 40% of the total intensity, other 60% intensity is unaccounted for 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
|d(Q/D)=0.00 {I6} or +3.7 {I+8-15} for J|p(res)=3/2 and J|p(3290)=3/2; -0.81 {I20} for J|p(3290)=5/2 (1970Ma13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
|d(Q/D)=+0.11 {I12} or +2.7 {I+5-13} for J|p(res)=3/2 and J|p(2987)=3/2; -0.78 {I40} for J|p(2987)=5/2 (1970Ma13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
|d(Q/D)=-0.18 {I16} or -5.7 {I+20-60} for J|p(res)=7/2 and J|p(1885)=9/2; +0.22 {I16} for J|p(1885)=5/2 (1970Ma13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
A{-2}=-0.22 {I12}, A{-4}=+0.04 {I13} (1977Di17) 
|d(Q/D)=+0.05 {I8} for 9/2 to 7/2; -0.70 {I22} for 9/2 to 9/2; and +0.02 {I11} for 9/2 to 11/2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
A{-2}=+0.38 {I4}, A{-4}=-0.14 {I4} (1977Di17) 
|d(Q/D)=+0.90 {I14} or -0.20 {I7} for 9/2 to 9/2 transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$11.1 (1976Po03) 
M$|g(lin pol) result disagrees with expected mult=E2 (1976Po03) 
$POL=-0.21 {I21}. ADO=1.33 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$other: 167 {I1} from ({+19}F,2pn|g) 
RI$from (|a,n|g). Other: 45 {I3} from (p,n|g) 
M,MR$or |d(Q/D)=+2.5 {I2} from |g(|q) in (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LT
decay_comment:
E$weighted average of 234.85 {I25} from ({+19}F,2pn|g) and 234.6 {I5} from (|a,n|g) 
RI$from (|a,n|g). Others: 100 {I15} from ({+19}F,2pn|g) and 100.0 {I30} from (p,n|g) 
M,MR$|d(Q/D) from |g(|q) in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E4
decay_BE_unit: e^2 x (fm)^8
decay_BE_info: ;TYPE=BE4;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE4W
decay_comment:
E$from {+44}Sc IT decay. Others: 271.16 {I15} from ({+19}F,2pn|g) and 270.6 {I5} from (|a,n|g) 
RI,M$from IT decay with mult from ce data. 


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$from ({+19}F,2pn|g). Other: 349.5 {I5} from (|a,n|g) 
M$from |g(|q,pol) in ({+19}F,2pn|g) with |DJ=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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 190.0 {I8} from ({+19}F,2pn|g) and 189.8 {I5} from (|a,n|g) 
RI$from (|a,n|g). Other: 45 {I4} from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 356.94 {I12} from ({+19}F,2pn|g) and 356.5 {I5} from (|a,n|g) 
RI$from (|a,n|g). Other: 100 {I4} from (p,n|g) 
M$Q with |DJ=2 from |g(|q) in (p,n|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LT
decay_comment:
E$from ({+19}F,2pn|g). Other: 424.5 {I5} from (|a,n|g) 
RI$from (|a,n|g). Others: 1.0E2 {I5} from ({+19}F,2pn|g) and 28 {I4} from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
$B(M2)(W.u.)<9.7 upper limit exceeds RUL=3, which would require T{-1/2}>41 ps for |d(M2/E1)=-0.04 {I3} 
E$weighted average of 530.95 {I15} from ({+19}F,2pn|g) and 531.7 {I5} from (|a,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 206.4 {I5} from ({+19}F,2pn|g) and 206.1 {I5} from (|a,n|g) 
M$(D) from |g(|q) in ({+19}F,2pn|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from ({+19}F,2pn|g). Other: 281.0 {I5} from (|a,n|g) 
RI$from (|a,n|g). Others: 100 {I15} from ({+19}F,2pn|g) and 100 {I4} from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E$other: 581.7 from ({+18}O,p3n|g) 
$B(M1)(W.u.)>7.9|*10{+-7} if pure M1, B(E2)(W.u.)>0.0065 if pure 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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=GT
decay_comment:
E$from ({+19}F,2pn|g). Other: 926.0 {I10} from (|a,n|g) 
M$D from |g(|q) in ({+19}F,2pn|g); |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E4)
decay_comment:
E$from 1990Me15. Other: 271.260 {I18} (1983Gu11), 271.15 {I20} (1974HeYW) 
RI$deduced from I(|g+ce)=100 and calculated |a=0.139 from BrIcc 
M$from |a(exp)=0.139 {I3} (1955Bl23). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$I(rel)=7.3 
E$1973Ar14 also place this |g from 1197 level, but this placement is not adopted in their final level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$I(rel)=18.3 
E$seen in coincidence with 745|g in 1973Dr08, which excludes another placement of this |g from 1507 level deexcited by 745|g in 1973Ar14 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$I(rel)=1.6 
E$report only in 1973Ar14; this |g is not seen in 1973Dr08 and other studies which only report a single 986|g from this level. Besides, with I|g(915) in 1973Ar14 and T{-1/2} in 1973Ar14, it would require a B(M2)(W.u.)=750 for this transition that is greatly larger than RUL=3. Therefore, this transition is considered questionable and not included in the Adopted dataset by the evaluators. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$1973Dr08 report that 1052|g is probably in coincidence with 235|g, 281|g, 350|g and 396|g, which make this placement of 1052|g to g.s. by 1973Ar14 questionable. Note that a 1052.3|g is placed from the 1683 level by 2005La19 in ({+18}O,p3n|g) 
$I(rel)=5.7 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
$I(rel)=5.3 for probable doublet 
E$placed by 1973Ar14; not confirmed in other studies. This |g is also placed from 667 level by 1973Ar14. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$I(rel)=2.5 
E$1973Ar14 also place this |g from a 745 level, which however is excluded by observed coincidence of this |g with the 762|g to g.s. in 1973Dr08. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
E$others: 67.875 {I5} (1988Al27), 67.85 {I4} (1967Ri06), 67.85 {I7} (1963Kl06) 
RI$weighted average (LWM) of 94.2 {I15} (1967Ri06), 98.1 {I15}(1988Al27), and 96.0 {I15} (1990Sc08). Original uncertainty of 0.5 (1967Ri06) seemed unrealistically low. Evaluators increased it to 1.5. 
M$from |a(K)exp=0.123 {I23} (1967Ri06); |a(exp)=0.10 {I5} (1963Kl06). |a(exp)=0.069 {I11}, deduced by evaluator from decay scheme by using %I|g(67.9)=93.5% {I15} (1990Sc08), and neglecting the very weak 146-keV transition. |a(exp)=0.069 {I11} disagrees with a theoretical value of 0.0845 {I25} (1976Ba63). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$others: 78.337 {I3} (1988Al27), 78.38 {I4} (1967Ri06), 78.44 {I7} (1963Kl06) 
RI$weighted average (LWM) of 100.0 {I11} (1967Ri06), 100.0 {I11} (1988Al27), and 100.0 {I13} (1990Sc08). Original uncertainty of 0.5 (1967Ri06) seemed unrealistically low. Evaluators increased it to 1.1. 
M$from |a(K)exp=0.031 {I5} (1967Ri06); |a(exp)=0.017 {I8} (1963Kl06). |a(exp)=0.019 {I14}, deduced by evaluator from decay scheme by using %I|g(78.4)=97.4% {I13} (1990Sc08), I|e(to 67.9 level)=0.7% {I3} (1988Al27), and neglecting the very weak 146-keV transition. |a(exp)=0.019 {I14} disagrees with a theoretical value of 0.0302 {I9} (1976Ba63) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_comment:
E$from level energy difference. Other: 147 {I15} (1967Ri06) 
RI$weighted average (LWM) of 0.10 {I3} (1967Ri06), 0.093 {I6} (1988Al27), and 0.095 {I3} (1990Sc08). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
M$it seems that authors' assignment of (E1) is inconsistent with the measured and predicted pol values with the same sign which would indicate M1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E,RI$authors of 1974Ko22 also place this |g from 1146.9 level but that placement is not confirmed in other studies. The intensity is probably mostly for the transition placed here. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$the placement of this transition is not seen in other studies and considered as questionable by the evaluators. See the placement from 968.2 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
M$it seems that authors' assignment of M1 is inconsistent with the measured and predicted pol values with the same sign which would indicate E1. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$from |g spectra gating on 408.2|g in Fig.2 of 2005La19; not placed by the authors. It is placed here by the evaluators based on |g|g-coin and exact match to the level-energy difference. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E,RI$unobserved transition; branching estimated as less than 10% of |g-intensity depopulating the level (2005La19). E|g from level-energy difference 


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$from level energy (B. Singh, May 01, 2021). Other: 12.4 from |e decay, with |DE=+0.1-0.2 keV in 2008Bu01 evaluation. Comment modified by B. Singh, May 01, 2021. 
RI$from |e decay 
$|a(K)exp=428 {I37} 
$|a(K)exp value deduced by B. Singh, May 01, 2021, weighted average of 429 {I117} from |e decay, 413 {I37} from (p,p'|g), and 580 {I120} from Coul. ex. 
M$D,Q from comparison to RUL. |DJ|p=2,yes from level scheme 
CC$from BrIcc for M2. Other: 501 {I43} from |a(K)exp=428 {I37}, and |a=1.17(|a(K)exp), the ratio of total |a/|a(K) (theory) from BrIcc. 2008Bu01 evaluation used K/L+=3. Comment added by B. Singh, May 01, 2021 
$B(M2)(W.u.) deduced by B. Singh, May 01, 2021 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2 x (fm)^4
decay_BM_info: ;TYPE=BM3;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM3W
decay_comment:
RI weighted ave of I|g(377|g)/I|g(364|g)=0.087 {I13} from (p,|g), 0.094 {I7} from (|a,p|g), 0.088 {I5} from (p,p'|g), and 0.0958 {I21} from Coul. ex. 
M from |g(|q) in (|a,p|g) and comparison to RUL 
BE2W FROM BE2UP IN COUL. ex. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_mixing_ratio_info: ;ERR=LT
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI unweighted ave of I|g(543|g)/(531|g)=0.719 {I16} from (p,|g), 0.684 {I19} from (p,p'|g), and 0.710 {I10} from Coul. ex. 
M from |g(|q) in (|a,p|g) and Coul. ex. 
MR from comparison to RUL. |d(543|g)=-0.04 {I6} from |g(|q) in (|A,p|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_mixing_ratio_info: ;ERR=LT
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
RI other I|g(708|g)/I|g(720|g)=0.007 {I3} from Coul. ex. 
M D+Q from |g(|q) in Coul. ex. |D|p=yes from level scheme 
MR from comparison to RUL. |d(708|g)=+1.2 {I+14-5} from |g(|q) in Coul. ex. 


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 |g(|q) in (|a,p|g) and Coul. ex. 
MR unweighted av of +0.09 {I6} from (|a,p|g) and +0.18 {I3} from Coul. ex.; |g(|q) 
BM1W,BE2W From gW(125|')|G{-0}{+2}/|G in (|g,|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_mixing_ratio_info: ;ERR=LT
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
MR from comparison to RUL. |d(974)=+0.09 {I+17-12} from |g(|q) in (|a,p|g) and -0.32 {I+6-11} from |g(|q) in Coul. ex. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI from Coulomb excitation 
M from |g(|q) in Coul. ex. and Coul. ex. 
MR from |g(|q) in Coul. ex. |d=+0.05 {I+13-9} if J=7/2 or -0.9 {I4} if J=5/2 in (|a,p|g) discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M D+Q from |g(|q) in (|a,p|g); |DJ=1 d+Q or |DJ=2 Q from DCO in ({+18}O,p2n|g). Ne E1+M2 from |d and comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_mixing_ratio_info: ;ERR=LT
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI unweighted ave of I|g(1056|g)/I|g(597|g)=0.56 {I10} from {+28}Si({+19}F,2p|g), {+30}Si({+18}O,p2n|g),..., 1.54 {I24} from (|a,p|g), and 0.8 {I5} from (p,p'|g). Other: 1.07 from {+30}Si({+18}O,p2n|g) 
MR from comparison to RUL. |d(1057|g)=+0.03 {I3} from |g(|q) in (|a,p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M,MR from |g(|q) in (|a,p|g) and comparison to RUL. Other possibilities excluded by level scheme. |DJ=1 d+Q or |DJ=2 Q from DCO in ({+18}O,p2n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M Q from |g(|q) in ({+7}Li,p2n|g); |DJ=0 d or |DJ=2 Q from DCO in ({+18}O,p2n|g). Ne M2 from comparison to RUL 


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 |DJ=0 d or |DJ=2 Q from DCO in ({+18}O,p2n|g). Ne M2 from comparison to RUL. |D|p=2 from level scheme 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M |DJ=1 d+Q or |DJ=2 Q from DCO in ({+18}O,p2n|g). Ne M2 from comparison to RUL. |DJ=2 from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2)
decay_comment:
E$from level energy. Other: 12.47 {I+14-30} from E(K-electron)=7.97 keV {I+14-30}. Comment added B. Singh, May 01, 2021. 
RI$from I(|g+ce) and |a. I|g value modified and comment added by B. Singh, May 01, 2021 
CC$from BrIcc for M2. Other: 501 {I43} from |a(K)exp=428 {I37}, and |a=1.17(|a(K)exp), the ratio of total |a/|a(K) (theory) from BrIcc. 2008Bu01 evaluation used K/L+=3. Comment added by B. Singh, May 01, 2021 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2)
decay_comment:
E$from level energy. Comment added B. Singh, May 01, 2021. 
RI$from I(|g+ce) and |a. I|g value modified and comment modified by B. Singh, May 01, 2021 
CC$from BrIcc for M2. Other: 501 {I43} from |a(K)exp=428 {I37}, and |a=1.17(|a(K)exp), the ratio of total |a/|a(K) (theory) from BrIcc. 2008Bu01 evaluation used K/L+=3. Comment added by B. Singh, May 01, 2021 
$%ce(K)=1.2|*10{+-2} {I3} 
TI$1966Po04 gave I(|g+ce)=12 {I3} based on ce(K) value only. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
A{-2}=17% {I3}, A{-4}=0% {I3}. Experimental linear polarization=-8% {I18}, predicted=27% {I7} (1975Ol01). Note that adopted |DJ|p=2,no does not seem to be consistent with linear polarization data (evaluator) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from |g(|q) and linear polarization (evaluator) 
A{-2}=22% {I7}, A{-4}=-6% {I7}. Experimental linear polarization=26% {I18}, predicted=33% {I16} (1975Ol01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M |DJ=1 D+Q or |DJ=2 Q from DCO. |=Q from comparison to RUL; |=E1+M2 from large DCO and small |d from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_comment:
$|a(exp)=5.09|*10{+-4} 
M,CC from the adopted |g's. Assumed by the evaluator to normalize |a. 1970Bl02 used |a=0.00045 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M from |a(K)exp and Coul. ex. (1970Ea02). 
MR 0|<|d|<1.0 or -0.1|<|d|<0.0 from |a(K)exp and Coul. ex. (1970Ea02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI other authors give I|g(760|g)/I|g(1290|g)|?1. 1983Ra17 did not consider the 1290|g in their DSAM measurements 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
2139|g assigned to 2151 state by 1983Ra17; however, T{-1/2} (1983Ra17) is inconsistent with T{-1/2}(2151) in (p,|g) but is consistent with T{-1/2} (1985Av04) for the 2138 state 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
Originally assigned to the 2352 state based on coincidence with an |?1260|g and previously known state at 2351. 1985Av04 also assigned a 1049|g to the 2352 state along with a 1055|g to the 2290 state. Evaluator believes that there is only one |g and it should be assigned to the 2290 state. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1,Q
decay_comment:
M from upper limit on B(E3)|^ (1967Bl17). |=E1 from |a(K)exp. 
MR |d>1.60 if M1+E2; |d=8.8|*10{+-3} {I41} if M2+E3 from |a(K)exp. 
EKC From I(K x-ray)/I(12.4|g)=27.3 {I28} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2)
decay_comment:
E$from level energy. Comment added B. Singh, May 01, 2021. 
RI$from I(|g+ce) and |a. I|g value modified and comment modified by B. Singh, May 01, 2021 
CC$from BrIcc for M2. Other: 501 {I43} from |a(K)exp=428 {I37}, and |a=1.17(|a(K)exp), the ratio of total |a/|a(K) (theory) from BrIcc. 2008Bu01 evaluation used K/L+=3. Comment added by B. Singh, May 01, 2021 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$absolute intensity determined by 2015Ku16 from a comparison of relative photon intensities of the 720.22|g and the 511-annihilation radiation, and the absolute intensity of the latter measured separately. This value can be compared with 0.154 {I12} in the {+45}Ti decay dataset in the ENSDF database, where the value was taken from 1971Zu01. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Absolute I|g=0.0118 {I13} in the ENSDF database and 1971Zu01 
$I|g=13.7 {I43} (2015Ku16), relative to 100 for 720.22|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Absolute I|g=0.085 {I9} in the ENSDF database and 1971Zu01 
$I|g=59.4 {I64} (2015Ku16), relative to 100 for 720.22|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Note that in the text on page 408, 2015Ku16 quote I|g=0.00299, which is a misprint. 
$Absolute I|g=0.0407 {I43} in the ENSDF database and 1971Zu01 
$I|g=25.5 {I36} (2015Ku16), relative to 100 for 720.22|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
E$from {+45}Sc(n,|g). 
M$from adopted |g's. 
|a(K)exp/|a(L)exp=10 {I3} (1952Bu25); |a|?1 (1948Go16). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E3
decay_comment:
RI corrected for internal conversion. 
M based on |a and T{-1/2}. 
CC determined from |g intensity balance (1982Ti02). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$B(GT)=0.009 {i5}(exp) {i3}(tensor). The "exp" uncertainty is the sum of statistical and experimental systematic contributions. The "tensor" uncertainty is from estimation of uncertainties during tensor calculations. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M D(+Q) from |g(|q) in (|a,p|g). |D|p=yes from level scheme 
MR 0.00 {I18} from |g(|q) in (|a,p|g). Comparison to RUL and |DJ|p limits |d to <0.03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 130.6 {I2} from (p,n|g) and 130.94 {I4} from (|m{+-},|g). 
M,MR$from |a(exp) in (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
E$weighted average of 121.2 {I2} from (p,n|g) and 121.41 {I4} from (|m{+-},|g). 
M$D(+Q) from |g(|q) in (p,n|g); |D|p=no from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
E$weighted average of 370.2 {I2} from (p,n|g) and 370.29 {I5} from (|m{+-},|g). 
M$D(+Q) from |g(|q) in (p,n|g); |D|p=no from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 519.9 {I2} from (p,n|g) and 520.3 {I2} from (|m{+-},|g). 
M,MR$from |g(|q,pol) and |a(exp) in (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
RI$from (p,n|g). Other: 4.2 {I13} from (|m{+-},|g). 
M,MR$D+Q and |d from |g(|q) in (p,n|g); |D|p=yes from level scheme. 
MR$other: -1.8 {I3} also from (p,n|g) is ruled out by RUL since it would require an isomeric T{-1/2}>60 ns for 1402 level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
E$weighted average of 779.0 {I2} from (p,n|g) and 780.1 {I8} from (|m{+-},|g). 
RI$from (p,n|g). Other: 100 {I24} from (|m{+-},|g). 
M,MR$from |g(|q,pol) and |a(exp) in (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
RI$weighted average of 13.7 {I20} from (p,n|g) and 12.5 {I25} from (|m{+-},|g). 
M$D+Q from |g(|q) in (p,n|g); |D|p=yes from level scheme. 
MR$+0.02 {I11} or +3.7 {I+28-16}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
M$D+Q from |g(|q) in (p,n|g); |D|p=yes from level scheme. 
MR$0.00 {I4} or +8 {I2} if J=3 or +0.74 {I10} or -6.0 {I20} if J=4. The smaller |d values are favored but the larger ones can't be completely ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
M,MR$D+Q with |d=+0.04 {I12} or -2.5 {I1} from |g(|q) in (p,n|g); |D|p=yes from level scheme. The smaller |d is favored but the larger one can't be completely ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_comment:
M,MR$D+Q with |d=-0.03 {I6} or +7 {I+4-2} from |g(|q) in (p,n|g); |D|p=yes from level scheme. The smaller |d is favored but the larger one can't be completely ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$+0.38 {I5} or +1.7 {I2} if J=2 or +0.20 {I4} if J=3 from |g(|q) and linear polarization in (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$-0.0 {I2} or -1.6 {I6} if J=3 or +0.06 {I2} or -4 {I+1-2} if J=4. Others: +0.03 {I7} or -1.35 {I+40-30} if J=3, or -0.36 {I50} or -5.4 {I+9-11} if J=4 (1971Ro27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$+0.36 {I2} or -14 {I3} if J|p=2-, -0.05<|d<+0.2 if J|p=1-, or -0.27|<|d<+|@ if J|p=1+. Other: +0.75 {I+44-33} if J=1 or +0.29 {I3} if J=2 (1971Ro27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.50 {I10} or -5.5 {I+20-30} if J|p=1- or +14 {I2} if J|p=2-. Other: +0.40 {I3} if J=2 (1971Ro27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$-0.45 {I10} if J=1, +0.47 {I2} or -15 {I5} if J=2, or -0.09 {I1} if J=3. Others: +0.78 {I+70-46} if J=1, +0.25 {I4} or -6.0 {I+15-35} if J=2, -0.14 {I8} if J=3 (1971Ro27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$+0.04 {I12} or -2.5 {I1} if J=2 or -0.36 {I8} or -10 {I+4-10} if J=3. Others: -0.18 {I6} or -1.39 {I17} if J=2, -0.52 {I4} or -4.0 {I+11-16} if J=3 (1971Ro27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$-0.03 {I6} or +7 {I+4-2} if J=2 or +0.6 {I1} if J=3. Others: -0.01 {I6} or <-9.5, or 6.3 {I+31-16} if J=2, +0.55 {I7} or >10 or <-10 if J=3 (1971Ro27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$others: -0.18 {I2} or <-6 for J=3 (1971Ro27) 
MR$-0.63 {I3}, <-20, or >+100 if J=2 or -0.17 {I2} if J=3. Others: -1.00 {I5} o r-3.60 {I4} if J=2, -0.18 {I2} or <-6 if J=3 (1971Ro27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$+0.34 {I8} or +1.5 {I3} if J=1, +0.27 {I3} if J=2, -0.21 {I3} if J=3. Others: +1.0 {I+19-6} if J=1, +0.29 {I4} if J=2, -0.17 {I2} if J=3 (1971Ro27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$+0.15 {I+2-1} or +2 {I1} if J=1 or +0.30 {I5} if J=2. Others: +0.21 {I5} or -4.10 {I8} if J=2 (1971Ro27) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M$from |a(exp) deduced from intensity balance consideration and |g|g(|q) in |b{+-} decay (2017Ga25) 
MR$from |g|g(|q) in |b{+-} decay (2017Ga25). Other: <0.5 from |a(exp) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M3)
decay_comment:
E$264.0755 {I8} (1979He19) from decay of {+182}Ta used as reference, supplemented by lines from decays of {+133}Ba and {+152}Eu (1984Al18); 256.94 {I10} (1970Wa29); 257 {I1} (1968Ch11) 
RI$weighted average of 100 {I2} (2017Ga25) and 98 {I3} (deduced from I(|g+ce)=102 {I3} and |a(257|g,M3)=0.0366 in 1984Al18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$72.8042 {I8} (1967Be65) from K|a{-2} x ray of Pb was used as reference (1984Al18); 71.54 {I20} (1970Wa29); 72 {I1} (1968Ch11) 
RI$weighted average of 58.4 {I60} (2017Ga25) and 52 {I5} (deduced from I(|g+ce)=54 {I5} and |a(71|g,M1)=0.0396 in 1984Al18) 
MR$from (1519|g)(71|g)(|q) (2017Ga25). Other: <0.5 from |a(exp)=0.13 {I+13-11} deduced by evaluators from intensity balance 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1519.44 {I30} (1970Wa29); 1519 {I1} (1968Ch11) 
RI$weighted average of 59.6 {I17} (2017Ga25) and 62.1 {I6} (1984Al18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$1591.00 {I30} (1970Wa29); 1591 {I1} (1968Ch11) 
RI$weighted average of 36.3 {I10} (2017Ga25) and 37.9 {I6} (1984Al18) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$From |g(|q) and |g(lin pol) in {+208}Pb({+48}Ca,X|g) 
E,RI from {+48}Ca({+238}U,X|g). 
E$Others: 1065 in {+48}Ca({+48}Ca,x|g), {+208}Pb({+48}Ca,X|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
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 {+54}Sc IT decay. 
M$from 1998Gr14 ({+54}Sc IT decay), based on the comparison of the half-life of the isomer with Weisskopf estimates for given transition energy. 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
E from weighted average of 110.5 {I3} (1998Gr14) and 110.7 {I5} (2012Ka36). 
M from 1998Gr14 based on the comparison of the half-life of the isomer with Weisskopf estimates for given transition energy. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E From weighted average values of 246.9 {I4} (2008Ma01) and 247.3 {I3} (2010Cr02). 
RI absolute intensity: 65 {I9} (2010Cr02). Other: 97 {I32} (2008Ma01), 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$authors' weighted average of 692 {I6} in {+9}Be({+56}Ti,{+55}Sc|g) and 700 {I8} in {+9}Be({+55}Sc,{+55}Sc'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$authors' weighted average of 572 {I5} from {+9}Be({+56}Ti,{+55}Sc|g) and 573 {I7} in {+9}Be({+55}Sc,{+55}Sc'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$authors' weighted average of 1535 {I14} in {+9}Be({+56}Ti,{+55}Sc|g) and 1542 {I14} in {+9}Be({+55}Sc,{+55}Sc'|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=AP;ERR=?
decay_uncertain: S
decay_comment:
E$existence of this transition suggested by 2017St22, but due to detector threshold setting, this |g was not detected. This transition is not included in the Adopted dataset. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$weighted average of values from 2010Cr02 and 2020Mi13 
$E|g=587.2 {I3}, I|g=100 {I12} (2010Cr02) 
$E|g=587.5 {I4}, I|g=100 {I18} (2020Mi13) 
$E|g=587 {I2}, I|g=2.2% {I6} (2004Li75); relative I|g=100 {I27} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_comment:
E$weighted average of values from 2010Cr02 and 2020Mi13 
RI$unweighted average of values from 2010Cr02 and 2020Mi13 
$E|g=140.5 {I3}, I|g=61 {I7} (2010Cr02) 
$E|g=140.6 {I4}, I|g=37 {I8} (2020Mi13) 
$E|g=140.6 {I5} (2012Ka36). E|g=140 {I2}, I|g=1.4% {I1} (2004Li75), relative I|g=64 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E,RI$weighted average of values from 2010Cr02 and 2020Mi13 
$E|g=727.1 {I3}, I|g=32 {I5} (2010Cr02) 
$E|g=728.0 {I6}, I|g=24 {I7} (2020Mi13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E,RI$from 2010Cr02 only 
M$assigned by evaluator based on transition intensity balance at 727.3 level. Note that |a(theory)(E2)=5.59 for 47.7-keV transition, does not permit a significant E2 admixture 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of values from 2010Cr02 and 2020Mi13 
RI$unweighted average of values from 2010Cr02 and 2020Mi13 
$E|g=187.8 {I3}, I|g=61 {I8} (2010Cr02) 
$E|g=187.9 {I5}, I|g=36 {I7} (2020Mi13) 
$E|g=188.2 {I5} (2012Ka36). E|g=188 {I2}, I|g=1.8% {I3} (2004Li75), relative I|g=82 {I14} 
M$from Weisskopf estimates (2010Cr02) 


decay_energy_unit: KEV
decay_comment:
$Some evidence in 2021Wi05 for the observation of a weak 167|g, with its intensity less than that of 412.5 gamma. 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
E$The evaluators consider this transition uncertain due to the very low count rate as seen in Fig.20 of 2007Do17. However authors have reported I|g= 35 {I19} in Table 10. 
$No proton coincidence was observed with this |g due to limited statistics (2007Do17) 


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$from {+44}V |b{++} decay (111 ms) 
M$from |g(|q,pol) in ({+19}F,2np|g) and |g(|q) in (|a,|g) E=res 


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$weighted average of 1371.22 {I8} from {+44}V |b{++} decay (150 ms), 1370.0 {I5} from {+45}Cr |ep decay, 1371.21 {I15} from ({+19}F,2np|g), and 1371.4 {I5} from ({+14}N,pn|g) 
M$Q with |DJ=2 from |g(|q) in ({+28}Si,2|a|g) and (|a,|g) E=res and M2 ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 1447.88 {I13} from {+44}V |b{++} decay (111 ms) and 1447.68 {I12} from (|a,|g) E=res 
RI$from {+44}V |b{++} decay (111 ms) 


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$from {+44}V |b{++} decay (111 ms) 
RI$weighted average of 42 {I7} from {+44}V |b{++} decay (111 ms) and 35 {I7} from (|a,|g) E=res 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$weighted average of 2093.2 {I8} from ({+19}F,2np|g), 2092.9 {I8} from ({+14}N,pn|g), and 2092.9 {I8} from (|a,|g) E=res 
MR$from |g|g(|q) data in {+40}Ca(|a,|g) (1981Di09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
E$weighted average of 469.86 {I10} from ({+19}F,2np|g) and 469.6 {I1} from ({+14}N,pn|g) 
M,MR$D+Q from |g(|q) in {+40}Ca(|a,|g) E=res (1981Di09); |d=-4.2 {I8} for J(8963)=3 or -5.7 {I14} for J(8963)=4. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1561.00 {I8} from {+44}V |b{++} decay (150 ms), 1560.90 {I15} from ({+19}F,2np|g), and 1560.7 {I4} from ({+14}N,pn|g) 
M$Q with |DJ=2 from |g(|q) in ({+19}F,2np|g) and |g asymmetry in (|a,|g) E=res; M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$unweighted average of 886.4 {I5} from ({+19}F,2np|g) and 884.7 {I3} from ({+14}N,pn|g) 
M,MR$-2<|d(Q/D)<2 for J|p= 3-, 0 for J|p=5- from |g(|q) with Q preferred in (|a,|g) E=res (1977Di07); (Q) from |g(|q) in ({+19}F,2np|g); (M2) ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$weighted average of 1607.2 {I5} from ({+19}F,2np|g) and 1607.0 {I5} from ({+14}N,pn|g) 
MR$|d(Q/D)=+0.15 {I10} for J|p= 3-, -0.1<|d<0.1 for J|p=5- in (|a,|g) E=res (1977Di07); (D) from |g(|q) in ({+19}F,2np|g); (E1) from |D|p=(yes). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E$|g reported in (|a,|g) only; not in {+44}V |e decay 
$B(M1)(W.u.)<0.022 if pure M1, B(E2)(W.u.)<40 if pure E2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E$|g reported in (|a,|g) only; not in {+44}V |e decay 
$If M1, B(M1)(W.u.)=0.010 {I+8-4}. If E2, B(E2)(W.u.)=11 {I+9-4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E$from {+44}V |b{++} decay (111 ms) 
$If M1, B(M1)(W.u.)=0.0031 {I+24-10}. If E2, B(E2)(W.u.)=1.0 {I+7-3} 


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=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
E$from ({+19}F,2np|g). Other: 2492.6 {I14} from ({+14}N,pn|g) 
M$Q with |DJ=2 from |g(|q) in ({+19}F,2np|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1162.49 {I15} from ({+19}F,2np|g) and 1162.8 {I3} from ({+14}N,pn|g) 
M$Q with |DJ=2 from |g(|q) in ({+19}F,2np|g) and ({+14}N,pn|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 368.80 {I10} from ({+19}F,2np|g) and 368.9 {I1} from ({+14}N,pn|g) 
M$Q with |DJ=2 from |g(|q) in ({+19}F,2np|g) and ({+14}N,pn|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$-0.32 {I+10-5} when J=2 for 3415 level, -0.09 {I7} when J=3 for 3415 level (1971Si13); +0.01 {I4} for J(3415)=3 (1980Di14). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$from ({+28}Si,2|a|g). 
$Mult=M3 implied by |DJ|p makes this transition unlikely in view of competing 1815 (implied mult=E2) transition (evaluators) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$Mult=M3 implied by |DJ|p makes this transition unlikely in view of competing 1815 (implied mult=E2) transition (evaluators) 
$I|g(25|')/I|g(75|')=1.69 {I21} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
M,MR$|d(O/Q) from |g(|q) for J(2454)=4 (1971Si13); M2(+E3) ruled out by RUL. Other: |d(Q/D)=+0.42 {I+12-9} for J(2454)=3 
$B(E2)(W.u.)=30 {I6} for pure E2 (1973Di04) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|DJ=2 from |g(|q) in 1971Si13; M2 ruled out by RUL 
$B(E2)(W.u.)=23 (1971Si13), 24 {I6} (1973Di04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
M,MR$|d(D+Q) with |DJ=0 from |g(|q) in 1971Si13; E1+M2 ruled out by RUL 
$B(E2)(W.u.)=6.5 (1971Si13), 7.0 {I13} (1973Di04). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$|DJ=2 from |g(|q) in 1971Si13; M2 ruled out by RUL 
$B(E2)(W.u.)=0.14 (1971Si13), 0.15 {I+50-20} (1973Di04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_comment:
M,MR$D(+Q) from |g(|q) in 1981Di09; |d=+0.15 {I10} in authors' previous 1977Di07 work. |D|p=(yes) from level scheme. Other |d=-4.3 {I7} or -3.6 {I10} (1981Di09) implying large M2 admixtures are unlikely from RUL. 1981Di09 give |d values of -1.3 and -1.0 for other spin sequences which have been rejected. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$|d=+2.3 {I+40-12} for J(3415)=2 and |||d||>11 for J(3415)=3 (1977Di07); revised values of their previous results in 1971Si13, with |d=+1.6 {I+12-6} for J(3415)=2, and >+6 or +0.4 {I+10-9} for J(3415)=3; second result for J=3 ruled out in 1977Di07 
$|g(|q) consistent with J(3415)=2 or 3 (1971Si13,1977Di07) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2+M1)
decay_comment:
M,MR$D+Q from |g(|q) in 1981Di09; |d=-4.2 {I8} for J(8960)=3; -5.7 {I14} for J(8960)=4. Other: -4.4 for J(3646)=4, -3.8 for J(3646)=3 in earlier 1977Di07 paper. |D|p=(no) from level scheme. 1981Di09 give |d values of -3.1 {I20}, -3.8 {I4}, and -4.6 {I10} for other spin sequences which have been rejected. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
MR$|||d||<2.0 for J(4061)=3; 0 for J(4061)=5 or 4 (1977Di07). 
$B(E2)(W.u.)<40 for J|p=3- or 5- (1977Di07). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
$|g(|q) from 1977Di07 is consistent with J(4061)=3,4,5 
MR$+0.15 {I10} for J(4061)=3, |||d||>0.5 for J(4061)=4, |||d||<0.1 for J(4061)=5 (1977Di07). 
$B(E1)(W.u.)<5|*10{+-5}, B(M2)(W.u.)<5 for J|p=3- or B(M2)(W.u.)<1 for J|p=5- (1977Di07). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$|g(|q) consistent with J(8954)=1 and J(1905)=2 or 0 (1971Si13). |d(Q/D)=+0.5 to +4.5 (1971Si13) for J(1905)=2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$-0.475 {I52} or -0.091 {I23} (1981Di09) 
MR$1981Di09 give -0.091 {I22} for J(8960)=2 and J(3646)=4; +0.169 {I16} (not isoscalar M2/E1) for J(8960)=3 and J(3646)=2; +0.153 {I16} (not isoscalar M2/E1) for J(8960)=4 and J(3646)=3; +0.200 {I15} (not isoscalar M2/E1) for J(8960)=2 and J(3646)=1; -0.324 {I23} (marginal M2/E1) for J(8960)=2 and J(3646)=2; -0.416 {I35} (marginal M2/E1) for J(8960)=2 and J(3646)=2; -0.475 {I54} (marginal M2/E1) for J(8960)=4 and J(3646)=4; -0.084 {I24} for J(8960)=2 and J(3646)=3; -0.091 {I22} for J(8960)=3 and J(3646)=4; -0.095 {I22} for J(8960)=4 and J(3646)=5. Other: |d(Q/O)=+0.153 {I25} for J(8960)=2 and J(3646)=4 (1981Di09) is inconsistent with M2 and M3 strengths deduced by authors which disfavors J=2 for 8960 level, thus rejected by 1981Di09. For recommended J|p=(3-,4+) for 8960 level and 4(-) for the 3646 level, two values of |d(Q/D) are: -0.475 {I52} and -0.091 {I23}. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$1981Di09 give |d=-0.76 {I40} (not isoscalar M2/E1) for J(8960)=2 and J(3176)=3; +0.041 {I57} for J(8960)=3 and J(3176)=3; +0.44 {I5} (not isoscalar M2/E1) for J(8960)=4 and J(3176)=3; +0.027 {I37} for J(8960)=2 and J(3176)=2; +0.43 {I5} (not isoscalar M2/E1) for J(8960)=3 and J(3176)=2; d=-0.61 {I11} (not isoscalar M2/E1) for J(8960)=3 and J(3176)=4; +0.056 {I80} for J(8960)=4 and J(3176)=4; |d=+0.44 {I6} (not isoscalar M2/E1) for J(8960)=2 and J(3176)=1. For recommended J|p=(3-,4+) for 8960 level and 3(-) for the 3176 level, values of |d(Q/D) are: +0.041 {I57} and +0.44 {I5}. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$-0.29 {I11} or +4.0 {I+30-4} (1971Si13). 
$|g(|q) consistent with J(8987)=2 and J(2531)=2 (1971Si13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M,MR$from |g(|q) in 1971Si13 for J(2454)=4; |d=+0.09 {I5} for J(2454)=3. Others: |d(O/Q)=+0.20 {I7} for J(8992)=2 and J(2454)=4, -0.06 {I6} for J(8992)=2 and J(2454)=3 
$|g(|q) consistent with J(8992)=4 and J(2454)=4 or 3 (1971Si13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q(+O)
decay_comment:
MR$from |g(|q) in 1971Si13. Other: |d(Q/D)=+1.9 {I+4-3} if J(8992)=2 
$|g(|q) consistent with J(8992)=2 or 4 and J(1083)=2 (1971Si13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$-0.09 {I17} for J(3415)=3 (1980Di14). 
RI$weighted average of 49 {I5} (1980Di14) and 62 {I6} (2013Sc16) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$-0.3 {I2} or +3.7 {I13} (1980Di14). 
RI$weighted average of 27 {I5} (1980Di14) and 28 {I5} (2013Sc16) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$-0.84 {I25} or -11 {I7} (1980Di14). 
RI$unweighted average of 39 {I5} (1980Di14) and 59 {I7} (2013Sc16) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$+0.01 {I4} for J(3415)=3 (1980Di14); previous results in 1971Si13: -0.32 {I+5-10} for J(3415)=2, -0.09 {I7} for J(3415)=3 
RI$weighted average of 51 {I5} (1980Di14) and 51.1 {I13} (2013Sc16) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$weighted average of 18 {I5} (1980Di14) and 16.8 {I7} (2013Sc16) 
MR$0<|d<+1 (1980Di14). 
$|g(|q) consistent with J(9227)=2 and J(2886)=2 (1971Si13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$from 1980Di14. Other: +0.02 {I4} (1971Si13). 
$|g(|q) consistent with J(9227)=2 and J(2531)=2 or 3 (1971Si13) 
RI$from 2013Sc16. Other: 100 {I5} (1980Di14) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$weighted average of 51 {I5} (1980Di14) and 46.7 {I11} (2013Sc16) 
MR$from 1980Di14 for J(9227)=2. Other: +0.02 {I7} (1971Si13) 
$|g(|q) consistent with J(9227)=2 or 3 (1971Si13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$weighted average of 1.3 {I5} (1980Di14) and 1.53 {I18} (2013Sc16) 
$|g(|q) consistent with J(9227)=2 or 3 (1971Si13) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$weighted average of 89 {I7} (1980Di14) and 82 {I4} (2013Sc16) 
M,MR$-0.11 {I7} from |g(|q) for J(3415)=3 (1980Di14). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
$B(M1)(W.u.)=0.27 {I7} from |G{-|g}=0.051 eV {I12} (1978Di11). 
$Measured |w{-|g}=|G{-|a}|G{-|g}/|G=0.046 eV {I11} (1978Di11) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$B(E2)(W.u.)=1.9 {I7} from |G{-|g}=0.073 eV {I25}(1978Di11). 
$B(M1)(W.u.)=0.021 {I7} if J(3756)=1 (1978Di11). 
$Measured |w{-|g}=|G{-|a}|G{-|g}/|G=0.066 eV {I22} (1978Di11) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
$B(M1)(W.u.)=3.8 {I10} from |G{-|g}=0.75 eV {I20} (1978Di11). 
$Measured |w{-|g}=|G{-|a}|G{-|g}/|G=0.24 eV {I5} (1978Di11) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$B(E2)(W.u.)=0.5 {I2} from |G{-|g}=0.019 eV {I7} (1978Di11). 
$B(M1)(W.u.)=0.005 {I2} if J(3756)=1 (1978Di11). 
$Measured |w{-|g}=|G{-|a}|G{-|g}/|G=0.006 eV {I2} (1978Di11) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$2011Mi02 give B(E3)(W.u.)|?=3 from their measured lifetime and the branching 2.0% {I3} for 3176|g quoted from 2000UrZX. However, the lifetime=21.8 ps read off from Fig.2 of 2011Mi02 and the same branching give a B(E3)(W.u.)=4.3. It is likely that 2011Mi02 could have used the lifetime value as half-life in calculating their B(E3), since a T{-1/2}=21.8 ps would give B(E3)(W.u.)=3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M from |g(|q) and n|g(|q) in (|a,n|g) and |a(exp) in (HI,xn|g) 
MR from |g(|q) and n|g(|q) in (|a,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LT
decay_comment:
E weighted av of 1185.8 {I2} from ({+24}Mg,2pn|g), 1188.61 {I20} from (HI,xn|g), 1187 {I1} from (p,n|g), and 1187.9 {I3} from (|a,n|g). 1188.03 {I35} is the mean of 1188.13 {I35} (LWM) and 1187.92 {I26} (RT) with |DE(|g) from RT 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$the calculated transition strength for this |g gives B(E2)(W.u.)=4.|*10{+3} {I3}, which well exceeds the RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$value of -2.6 {I3} results in E2 transition strength which greatly exceeds the RUL, with B(M1)(W.u.)=0.023 {I8}; B(E2)(W.u.)=3.2|*10{+3} {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$value of -2.3 {I1} results in E2 transition strength which greatly exceeds the RUL, with B(M1)(W.u.)=0.0170 {I22}; B(E2)(W.u.)=710 {I80} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
Unresolved from {+45}Sc, 691|g, in singles. I|g obtained by studying the yield dependence of the 691-keV peak in the n|g coincidence spectrum on the pulse shape discrimination method and subtracting the contribution of the {+45}Sc 691|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$2<|a(exp)<20, from I|g(37|g) and I|g(292|g) measured just above the production threshold for the 330-keV state (1968Je03) 


decay_energy_unit: KEV
decay_multipolarity: D+Q
decay_comment:
$355<I{-|g}(rel)<618 
RI,M,MR limits deduced after subtraction of {+48}V, 586|g. The small contamination of this line did not seem to alter the results from |g(|q) 


decay_energy_unit: KEV
decay_multipolarity: (Q)
decay_comment:
M I|g(15|')/I|g(90|')>1? linear polarization (1975Ol01) consistent with L|<2 
Degenerate with a 984|g from {+48}Ti. Placement at top of cascade based only on |g|g-coin (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E4]
decay_BE_unit: e^2 x (fm)^8
decay_BE_info: ;TYPE=BE4;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE4W
decay_comment:
E$assumed from {+46}Sc |b{+-} decay scheme and photoneutrons from Be. 
RI$from {+46}Sc |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
E$weighted average of values from ({+28}Si,2|a2p|g), ({+16}O,2p|g), ({+9}Be,2pn|g), and (p,p'|g). 
RI,M,MR$from (p,p'|g) 
Large B(M2)(W.u.) suggests that |d is too large. 


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 values from ({+28}Si,2|a2p|g), ({+16}O,2p|g), ({+9}Be,3n|g), ({+9}Be,2pn|g) and ({+12}C,|a2p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of values from ({+28}Si,2|a2p|g), ({+9}Be,2pn|g), (|a,n|g), and (p,p'|g). 
RI$weighted average of values from ({+16}O,2p|g), (|a,n|g), and (p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of values from ({+28}Si,2|a2p|g), ({+9}Be,3n|g), ({+9}Be,2pn|g) and ({+12}C,|a2p|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 values from ({+28}Si,2|a2p|g), ({+9}Be,3n|g) and ({+9}Be,2pn|g). Separated by 0.8 {I8} from |g in decay of 6242 level according to ({+9}Be,2pn|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$weighted average of values from ({+28}Si,2|a2p|g), ({+9}Be,3n|g) and ({+9}Be,2pn|g). 
RI$from ({+28}Si,2|a2p|g) and ({+12}C,|a2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of values from ({+28}Si,2|a2p|g), ({+9}Be,3n|g) and ({+9}Be,2pn|g). 
RI$from ({+28}Si,2|a2p|g) and ({+12}C,|a2p|g) 
$B(E2)(W.u.)=8.2 {I9} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$Assigned as the transition between 3950 and 2010 (1968Er04), evaluator (scw) Re-assigned the |g-ray to 3940 to 2010 transition; 
$Unplaced in 1987Mo17 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$Assigned as the transition between 3950 and 2010 (1968Er04), evaluator (SCW) re-assigned the |g-ray to 3940 to 2010 transition; 
$Unplaced in 1987Mo17 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$weighted average of -1.1 {I1} (1976ReZP), -3.1 {I9} (1971Ga08), -1.54 {I15} (1968Le04), -1.07 {I15} (1967Ch22). 


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:
RI$ uncertainty of 0.1 quoted in table I of 2011Me11 seems a misprint 
$B(M1)=0.033 {I3} for |d(E2/M1)=0 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E weighted av of 159.381 {I15} from |b{+-} decay, 159.369 {I20} from from ({+12}C,3n|g) and 159.27 {I4} from (n,|g). Arithmetic mean of 159.370 {I12} (NRM) and 159.375 {I12} (RT) adopted. 
CC from |a(K)exp=0.00406 {I21} and K/L+|?10 in |b{+-} decay. |a(K)exp anomalous with theory: |a(K)=0.00560 {I12} 
$|a(K)exp=0.00406 {I21} |a(L)exp|?0.000406 {I21} 
ELC FROM EKC AND K/L+. LC=0.000512 11 (THEORY) 
$|a(M)exp|?5.19|*10{+-5} {I31} |a(N)exp|?2.78|*10{+-6} {I17} 
EMC,ENC$FROM ELC AND L/M=7.82 23 AND L/N=146.0 43 (THEORY) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M,MR D+Q, -0.30 {I6} or -14 {I10} from |g|g(|q) in (n,|g). Ne E1+M2 from comparison to RUL and |d. |d Ne -14 {I10} from comparison to RUL 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W
decay_comment:
M D+Q from |g(|q) in ({+3}He,|a|g). |D|p=yes from level scheme 
MR -0.219 {I37} if J{-i}=3/2 or -0.274 {I23} if J{-i}=5/2 from |g(|q) in ({+3}He,|a|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M,MR D+Q from |s(96|')/|s(126|') in (|g,|g'). |D|p=no from level scheme see table in 1976Ra03 for |d's 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_mixing_ratio_info: ;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
M D(+Q) from |s(96|')/|s(126|') in (|g,|g'). |D|p=no from level scheme 
MR from |s(96|')/|s(126|') in (|g,|g') 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M D(+Q) from |g(|q) in ({+14}C,3n|g). |D|p=yes from level scheme 
$-0.028|<|d|<0.02 from -0.18 {I20} |g(|q) in ({+14}C,3n|g); |<0.028 {I6} from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2(+M3))
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M,MR$D(+Q), +0.3 {I4}, or E2(+M3), -0.0 {I3}, from |g(|q) in ({+14}C,3n|g) and comparison to RUL. J|)J or J|)J-2 from angular anisotropy in ({+40}Ca,3p|g). Ne D(+Q) from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
EKC Anomalous with theory: |a(K)=0.00560 {I12} 
K/L+ Visual inspection of photographic spectrometer. 1986Re12 also obtained K/L+|?10. K/L+=9.6 {I10} (theory) 
ELC From |a(K)exp and K/L+. |a(L)=0.000512 {I11} (theory) 
EMC,ENC$FROM ELC AND L/M=7.82 23 AND L/N=146.0 43 (THEORY) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2(+M3))
decay_comment:
M,MR D(+Q), +0.3 {I4}, or E2(+M3), -0.00 {I30} (1986Wa19). J|)J or J|)J-2 from angular anisotropy (1994Ca04). |=M2 from comparison to RUL (evaluator). |=D(+Q) from level scheme 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR other: -0.027 {I7} (1972We18); note that this is discrepant with other results. See discussion in Adopted Gammas 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI other: I|g(1093)=88% {I6}, I|g(1252)=12% {I6} from |g(|q) (1972We18). See discussion in Adopted Gammas 
M predicted linear pol=-0.18 to -0.06; exp=-0.3 to 0 
MR other: -0.15 {I6} (1972We18) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
M predicted linear pol=+0.43 to +0.56; exp=+0.2 to +0.7 (1973Sa12) 
MR other: -0.01 {I2} (1973Sa12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$|s{-|g}{+Z}(b)=0.0076 {I7} 
RI from I|g(1556|g)=8.7 (1972Kn07) and I|g(1556|g)/I|g(1396|g)=1/1.75 (1969Te01) (evaluator). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$|s{-|g}{+Z}(b)=0.0017 {I4} 
RI from I|g(doublet)=3.0 and adopted I|g(244|g)/I|g(1794|g)=0.491 {I23} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (M1,E2)
decay_comment:
$|G{-|g}/|G=0.77 {I3} 
M D,Q from |s(96|')/|s(126|'). |d{+2}<0.001 from RUL(M2) not consistent with |s(96|')/|s(126|') 
MR see table in 1976Ra03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E,RI from 1956Te26 
MR from adopted T{-1/2}=210 ps {I6}, E|g=159.381, J{-i}, J{-f}, and B(E2)|^. See discussion in Adopted Gammas 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
RI assuming no contamination from 1.44 to 0.16 MeV transition. Discrepant with other results. See discussion in Adopted Gammas. 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
$B(M1)=0.0445 |m{+2}{-n} {I10} (2024Ut02) 
$calculated by 2024Ut02 using |d=0.098 {I9} determined by combining data from a Coulomb excitation measurement in the literature. 


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$weighted average of 983.526 {I12} from {+48}Sc |b{+-} decay, 983.525 {I4} from {+48}V |e decay, and 983.517 {I4} from (n,|g) E=thermal. Others: 983.4 {I3} from ({+14}C,2n|g), 983.7 {I5} from ({+7}Li,p2n|g), 983.1 {I3} from (|a,p|g), 983.50 {I15} from (p,p'|g), and 983.1 {I15} from Coulomb excitation. 
M$from ce data in |e and |b{+-} decay, |g(|q,pol) in (p,p'|g), and |g|g(|q) in (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1312.120 {I12} from {+48}Sc |b{+-} decay, 1312.105 {I6} from {+48}V |e decay, and 1312.096 {I7} from (n,|g) E=thermal. Others: 1312.1 {I6} from ({+14}C,2n|g), 1312.5 {I7} from ({+7}Li,p2n|g), 1311.7 {I3} from (|a,p|g), and 1312.20 {I10} from (p,p'|g). 
M$from ce data in |e and |b{+-} decay, |g(|q) in (p,p'|g), and |g|g(|q) in (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 1437.521 {I21} from {+48}V |e decay and 1437.487 {I10} from (n,|g) E=thermal. Others: 1436.9 {I5} from (|a,p|g) and 1436.80 {I10} from (p,p'|g). 
RI$from (p,p'|g). Others: 100.0 {I25} from {+48}V |e decay, 100 {I6} from (n,|g) E=thermal, 100 {I5} from (n,n'|g), and 100.0 {I2} from (|a,p|g). 
M$D+Q from |g|g(|q) in (p,p'|g) and (n,|g) E=thermal, and |g(|q) in (n,n'|g); E1+M2 ruled out by RUL. 
MR$weighted average of +0.18 {I3} in (n,n'|g), +0.10 {I4} in (n,|g) E=thermal, and +0.18 {I9} from (p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 2420.94 {I5} from {+48}V |e decay, 2420.90 {I4} from (n,|g) E=thermal, and 2420.70 {I20} from (p,p'|g). 
RI$weighted average of 5.58 {I25} from {+48}V |e decay, 5.42 {I36} from (n,|g) E=thermal, 5.0 {I12} from (n,n'|g), and 3.5 {I10} from (p,p'|g). Other: 1.0 {I2} from (|a,p|g) is discrepant. 
M$Q from p|g(|q) and |g(|q) in (p,p'|g); M2 ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 2013.66 {I16} from (n,|g) E=thermal and 2014.00 {I20} from (p,p'|g). 
M$isotropic p|g(|q) in (p,p'|g); M2 ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 803.05 {I25} from {+48}V |e decay, 802.87 {I6} from (n,|g) E=thermal, and 804.0 {I12} from (p,p'|g). 
RI$weighted average of 5.83 {I52} from {+48}V |e decay, 5.5 {I14} from (|a,p|g), 4.55 {I33} from (n,|g) E=thermal, and 5.1 {I11} from (p,p'|g). Other: 9.0 {I50} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$unweighted average of 928.326 {I6} from {+48}V |e decay and 928.290 {I10} from (n,|g) E=thermal. Others: 928.4 {I6} from (p,p'|g); 927.4 {I7} from (|a,p|g) is discrepant. 
RI$from {+48}V |e decay. Others: 31.5 {I41} from (|a,p|g), 31.8 {I17} from (n,|g) E=thermal, 35.0 {I60} from (n,n'|g), and 33.8 {I24} from (p,p'|g). 
M,MR$D(+Q) from |g(|q) in (p,p'|g); |D|p=no from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 2240.396 {I10} from {+48}V |e decay and 2240.375 {I19} from (n,|g) E=thermal. Others: 2240.2 {I7} from (|a,p|g) and 2240.0 {I3} from (p,p'|g). 
RI$from {+48}V |e decay. Others: 100 {I6} from (|a,p|g), 100 {I6} from (n,|g) E=thermal, 100 {I15} from (n,n'|g), and 100 {I3} from (p,p'|g). 
M$D+Q from |g(|q) in (n,n'|g) and p|g(|q) in (p,p'|g); E1+M2 ruled out by RUL. 
MR$from |g(|q) in (n,n'|g). Other: +0.26 {I5} from p|g(|q) in (p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$unweighted average of 944.129 {I6} from {+48}V |e decay and 944.104 {I7} from (n,|g) E=thermal. Others: 943.6 {I5} from (|a,p|g) and 945.1 {I5} from (p,p'|g) are discrepant. 
M$D+Q from |g(|q) in (n,n'|g); E1+M2 ruled out by RUL. 
MR$from |g(|q) in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1037.522 {I12} from {+48}Sc |b{+-} decay, 1037.0 {I5} from ({+14}C,2n|g), 1037.9 {I5} from ({+7}Li,p2n|g), 1037.1 {I4} from (|a,p|g), and 1037.599 {I25} from (n,|g) E=thermal. 
M$Q from p|g(|q) in (|a,p|g); M2 ruled out by RUL. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from (n,n'|g) and (|a,p|g). 
RI$from (|a,p|g). Other: 8 {I3} from (n,n'|g) is discrepant. Note that this transition is not seen in |e decay, (p,p'|g) and (n,|g) E=thermal, indicating a weak intensity. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$unweighted average of 1063.9 {I1} from {+48}V |e decay, 1063.19 {I5} from (n,|g) E=thermal, and 1064.0 {I10} from (p,p'|g). 
RI$unweighted average of 8.2 {I17} from (|a,p|g), 10.3 {I8} from (n,|g) E=thermal, 23 {I8} from (n,n'|g), and 17.4 {I8} from (p,p'|g). Other: 57 {I12} from {+48}V |e decay is strongly discrepant with other values. 


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=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LT
decay_comment:
E$weighted average of 2375.20 {I4} from {+48}V |e decay and 2375.211 {I19} from (n,|g) E=thermal. Others: 2374.7 {I4} from (|a,p|g) and 2374.8 {I8} from (p,p'|g). 
RI$from (p,p'|g). Others: 100.0 {I35} from {+48}V |e decay, 100.0 {I22} from (|a,p|g), 100 {I6} from (n,|g) E=thermal, and 100 {I23} from (n,n'|g). 
M,MR$D(+Q) from |g(|q) in (n,n'|g) with |d=0.00 {I3} and p|g(|q) in (p,p'|g) with |d=0.00 {I4}; |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from (n,|g) E=thermal. Others: 2387.6 {I5} from (|a,p|g) and 2387.3 {I3} from (p,p'|g). 
RI$from (p,p'|g). Others: 100.0 {I34} from (|a,p|g), 100 {I6} from (n,|g) E=thermal, and 100 {I15} from (n,n'|g). 
M$D+Q from |g|g(|q) in (n,|g) E=thermal, |g(|q) in (|g,|g') and p|g(|q) in (p,p'|g); |D|p=no from level scheme. 
MR$from combination of -0.2 {I1} or 4 {I1} from (p,p'|g), <0.5 from (n,|g) E=thermal, and 0.1<|d<0.8 from (|g,|g'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from (n,|g) E=thermal. Others: 3369.6 {I14} from (|a,p|g) and 3371.5 {I12} from (p,p'|g). 
RI$weighted average of 12.4 {I34} from (|a,p|g), 19.0 {I15} from (n,|g) E=thermal, 20 {I5} from (n,n'|g), and 15.6 {I11} from (p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from {+48}Sc |b{+-} decay. Others: 175.3 {I3} from ({+14}C,2n|g) and 175.9 {I5} from ({+7}Li,p2n|g). 
RI$from {+48}Sc |b{+-} decay. Others: 100 {I11} from ({+24}Mg,3p|g), 100 {I4} from (|a,p|g), and 100 {I5} from ({+3}He,3n|g). 
M$assumed based on comparions with RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from {+48}Sc |b{+-} decay. Others: 1212.4 {I10} from ({+7}Li,p2n|g) and 1212.3 {I6} from (|a,p|g). 
RI$weighted average of 31.86 {I54} from {+48}Sc |b{+-} decay, 29.9 {I39} from (|a,p|g), and 27 {I10} from ({+3}He,3n|g). Others: 20.1 {I30} from ({+24}Mg,3p|g) is discrepant. 
M$Q from p|g(|q) in (|a,p|g); M2 ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from (n,|g) E=thermal. 
RI$weighted average of 10.2 {I23} from (|a,p|g) and 7.96 {I54} 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$from (n,|g) E=thermal. Other: 2632.5 {I8} from (|a,p|g). 
RI$from (|a,p|g). Other: 100 {I7} from (n,|g) E=thermal. 
M$D+Q from |g|g(|q) in (n,|g) E=thermal and p|g(|q) in (p,p'|g); E1+M2 ruled out by RUL. 
MR$weighted average of -0.10 {I5} from |g|g(|q) in (n,|g) E=thermal and -0.18 {I4} from p|g(|q) in (p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from (n,|g) E=thermal. 
RI$unweighted average of 3.4 {I11} from (|a,p|g) and 1.08 {I43} from (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$from (n,|g) E=thermal. Other: 2716 {I1} from (|g,|g), 2714.9 from (p,p'|g). 
RI$from (p,p'|g). Others: 100 {I13} from (|a,p|g), 100 {I8} from (n,|g) E=thermal, 100 {I6} from (|g,|g), and 100 {I15} from (n,n'|g). 
M$from |g(|q) and azimuthal asymmetries in (|g,|g'). Other: M1+E2 with |d=+0.9 {I+14-5} from p|g(|q) and comparison to RUL in (p,p'|g) is discrepant. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from (n,|g) E=thermal. Other: 3700 {I1} from (|g,|g), 3698.3 from (p,p'|g). 
RI$weighted average of 61 {I13} from (|a,p|g), 67 {I5} from (n,|g) E=thermal, 54 {I8} from (n,n'|g), and 53.8 {I31} from (p,p'|g). Other: 92 {I6} from (|g,|g') is discrepant. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$from (|a,p|g) only. 1993Ko57 in (n,n'|g) suggest that this |g is the same as the 2726|g from the 5146 state in their work. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 2756.5 {I7} from (n,|g) E=thermal and 2755 {I1} from (|g,|g). Other: 2757.2 from (p,p'|g). 
RI$weighted average of 63 {I15} from (n,|g) E=thermal, 42 {I10} from (n,n'|g), and 42 {I8} from (p,p'|g). Other: I(2756|g)/3738|g)=257 {I22}/100 {I22} is discrepant. 
M,MR$D(+Q) and |d from p|g(|q) in (p,p'|g) and (M1) from azimuthal asymmetries in (|g,|g'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from (n,|g) E=thermal. Others: 3737.8 {I13} from (|a,p|g), 3739 {I1} from (|g,|g), 3740.5 from (p,p'|g). 
RI$from (p,p'|g). Others: 100 {I12} from (n,|g) E=thermal, 100 {I16} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 423.2 {I4} from (|a,p|g) and 423.629 {I9} from (n,|g) E=thermal. 
RI$from (n,|g) E=thermal. Other: 100 {I6} from (|a,p|g); I(424|g)/I(1487|g)=|?50/100 {I25} in (n,n'|g) and 23 {I5}/100 {I5} in (p,p'|g) are discrepant. 
M,MR$D+Q, -0.24 {I14} or <-3.7, if J=4 from |g|g(|q) in (n,|g) E=thermal. Pure E2 ruled out by RUL 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from (n,n'|g). 
RI$from (|a,p|g). Other: I(559|g)/I(1487|g)=50 {I15}/100 {I25} in (n,n'|g) is discrepant. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from (n,|g) E=thermal. Other: 1486.8 {I17} from (|a,p|g). 
RI$weighted average of 33 {I6} from (|a,p|g) and 41.5 {I24} from (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$from (n,|g) E=thermal. Other: 1556.6 in (n,n'|g), 1556.3 in (p,p'|g). 
RI$weighted average of 26.7 {I40} from (|a,p|g), 24.0 {I15} from (n,|g) E=thermal, and 37.0 {I69} from (p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LT
decay_comment:
E$weighted average of 2866.7 {I13} from (|a,p|g) and 2868.59 {I4} from (n,|g) E=thermal. 
RI$from (|a,p|g). Others: 100 {I6} from (n,|g) E=thermal and 100 {I7} from (p,p'|g). 
M,MR$D(+Q) and |d from p|g(|q) in (p,p'|g); |D|p=yes from level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from (n,|g) E=thermal. Other: 811 {I3} from (n,n'|g). 
RI$weighted average of 56.3 {I94} from (|a,p|g), 44.2 {I25} from (n,|g) E=thermal, and 41.0 {I90} from (n,n'|g). 
M$pure E2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from (n,|g) E=thermal. Others: 1614.3 {I13} from (|a,p|g), 1614 {I4} from (n,n'|g), and 1615.1 {I11} from (p,p'|g). 
RI$from (n,|g) E=thermal. Others: 100 {I10} from (|a,p|g) and 100 {I15} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E,RI$from (|a,p|g). 
M,MR$D(+Q) and |d from p|g(|q) in (|a,p|g); |D|p=(yes) from level scheme. Other: |d(4|)4)=-0.32 {I+16-25} in (|a,p|g) excluded by comparison to RUL assuming |D|p=yes. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$from (n,|g) E=thermal. Other: 834.0 {I8} from (|a,p|g). 
RI$weighted average of 73.1 {I96} from (|a,p|g) and 68.2 {I39} from (n,|g) E=thermal. 
$B(E2)(W.u.)=1.3|*10{+3} {I+6-3} exceeds RUL=300. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from (n,|g) E=thermal. Others: 3090.1 {I11} from (|a,p|g) and 3088 {I7} from (n,n'|g). 
RI$from (n,|g) E=thermal. Other: 100 {I12} from (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from (n,|g) E=thermal. 
RI$weighted average of 22 {I5} from (|a,p|g) and 27 {I5} from (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$other: 3332 {I8} from (n,n'|g). 
RI$weighted average of 53 {I10} from (|a,p|g) and 45 {I22} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from (|g,|g). Other: 4314 {I9} from (n,n'|g), 4312 from (|a,p|g). 
RI$from (|a,p|g). Other: 100 {I22} from (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from (n,|g) E=thermal. Other: 2094 from (|a,p|g); not seen in (n,n'|g). 
RI$from (n,|g) E=thermal. Other: 20 {I4} from (|a,p|g) is discrepant. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from (n,|g) E=thermal. Other: 3401 {I8} from (n,n'|g), 3406 from (|a,p|g). 
RI$from (n,|g) E=thermal. Other: 100 {I13} from (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$weighted average of 50 {I10} from (|a,p|g) and 56 {I5} from (n,|g) E=thermal. 
M$D+Q from |g|g(|q) in (n,|g) E=thermal; |D|p=no from level scheme. 
MR$from -0.13|<|d<-0.10 from 3473.9|g-983.5|g(|q) and +0.10|<|d<+0.13 from 7168.7|g-3473.9|g(|q) in (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_comment:
E$weighted average of 1231.4 {I6} from ({+14}C,2n|g) and 1231.8 {I5} from ({+7}Li,p2n|g). 
RI$from (|a,p|g). Others: 100 {I20} from ({+24}Mg,3p|g) and 100 {I8} from ({+7}Li,p2n|g). 
M$Q from p|g(|q) in (|a,p|g). |DJ|p=2,no from the level scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from (n,|g) E=thermal. Other: 3600 {I8} from (n,n'|g). 
RI$from (n,|g) E=thermal. Other: 100 {I19} from (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$from (n,|g) E=thermal. Other: 3963 {I9} from (n,n'|g). 
RI$from (n,|g) E=thermal. Other: 100 {I18} from (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from ({+7}Li,p2n|g). 
RI$from (|a,p|g). 
M$D(+Q) from p|g(|q) in (|a,p|g); |D|p=no from level scheme . 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1,E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M,MR$E2 if J=7, M1+E2, |d=-1.25 {I25} if J=5, or M1+E2, |d=-1.7 {I+9-12} if J=6, from p|g(|q) in (|a,p|g) and comparison to RUL. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M,MR$D+Q, |d=-0.02 {I+7-3} if J=7, or |d=-0.07 {I+7-9} if J=5, or M1+E2, |d=+1.5 {I3} if J=6, from p|g(|q) in (|a,p|g) and comparison to RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from (n,|g) E=thermal. 
RI$from (|a,p|g). Other: I(2396|g)/I(3198|g)=100 {I8}/97 {I3} from (n,|g) E=thermal is discrepant. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$from (n,|g) E=thermal. Other: 5640 {I2} from (|g,|g). 
RI$from 82 {I+103-82} in (n,|g) E=thermal. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$D(+Q) from p|g(|q) in (|a,p|g); E1(+M2) ruled out by RUL. 
MR$|d(9|)8)=0.00 {I5} or |d(7|)8)=-0.09 {I9} from p|g(|q) in (|a,p|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$D+Q from p|g(|q) in (|a,p|g); E1+M2 ruled out by RUL. 
MR$|d(9|)8)=0.10 {I5} or |d(7|)8)=-0.14 {I8} from p|g(|q) in (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+7}Li,p2n|g). Other: 1538 from (|a,p|g). 
M,MR$Q if J=10 or D+Q, -0.78 {I7}, if J=8 from p|g(|q) in (|a,p|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$D+Q from p|g(|q) in (|a,p|g); E1+M2 ruled out by RUL. 
MR$|d(8|)7)=+0.07 {I+7-5} or |d(6|)7)=-0.10 {I5} from p|g(|q) in (|a,p|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M,MR$|d(10|)9)=-0.03 {I4}, |d(8|)9)=-0.02 {I4}, |d(8|)7)=-0.05+5-2, or |d(6|)7)=-0.19 {I+13-3} from p|g(|q) in (|a,p|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M,MR$|d(11|)10)=0.00 {I6}, |d(9|)10)=-0.05 {I7}, |d(9|)8)=0.00 {I7}, or |d(7|)8)=-0.07 {I9} from p|g(|q) in (|a,p|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR,M$|d(12|)11)=+0.02 {I6}, |d(10|)11)=-0.05 {I6}, |d(10|)9)=+0.02 {I6}, |d(8|)9)=-0.05 {I6}, |d(8|)7)=+0.02 {I6}, or |d(6|)7)=-0.07 {I6} from p|g(|q) in (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$others: 983.5 {I2} (1970Ei07), 987.0 {I10} (1968KeZZ), 983.3 {I4} (1967Ko01), 986 {I3} (1957Va08) 
RI$others: 1000 (1970Ei07,1967Ko01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$others: 1312.1 {I3} (1970Ei07), 1311.2 {I5} (1968KeZZ), 1311.4 {I6} (1967Ko01), 1314 {I4} (1957Va08), 1311.85 {I20} (1974HeYW) 
RI$others: 1000 (1970Ei07), 1000 {I3} (1967Ko01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$others: 1037.6 {I2} (1970Ei07), 1039.9 {I10} (1968KeZZ), 1037.1 {I5} (1967Ko01), 1040 {I3} (1957Va08) 
RI$others: 980 {I20} (1970Ei07), 980 {I30} (1967Ko01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$others: 175.0 {I4} (1970Ei07), 175 {I1} (1968KeZZ), 175.3 {I5} (1967Ko01) 
RI$others: 60 {I10} (1970Ei07), 94 {I5} (1967Ko01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$others: 1212.6 {I3} (1970Ei07), 1212.5 {I10} (1968KeZZ), 1212.3 {I7} (1967Ko01) 
RI$others: 22 {I5} (1970Ei07), 25 {I2} (1967Ko01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 983.521 {I7} (1979Gr01), 983.526 {I5} (1990Me15), 983.526 {I5} (2005TrZZ). Others: 983.497 {I25} (1974HeYW), 983.20 {I15} (1973Ba02), 983.3 {I4} (1967Ko01), 986 {I3} (1957Va08) 
RI$from 2005TrZZ. Others: 1000 {I2} (1990Me15), 1000 (1975Al23, 1967Ko01,1957Va08), 1000 {I5} (1974HeYW) 
M$|a(exp)=1.23|*10{+-4} {I6} (1967Ko01), 1.26|*10{+-4} {I4} (1957Va08); K/L1=11.2 {I1}, L1/M1=7.2 {I1} (1984Bu34) 
$I(ce)/I|b{++}=2.54|*10{+-4} {I12} (1967Ko01), 2.28|*10{+-4} {I7} (1957Va08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1312.096 {I6} (1979Gr01), 1312.090 {I12} (1990Me15), 1312.115 {I5} (2005TrZZ), 1312.038 {I31} (1974HeYW), 1312.10 {I10} (1973Ba02), 1312.0 {I5} (1969Ar03), 1311.4 {I6} (1967Ko01), 1311.1 {I6} (1963Ri01). Other: 1314 {I4} (1957Va08) 
RI$others: 975 {I8} (1990Me15), 970 {I10} (1975Al23), 999 {I50} (1974HeYW), 990 {I40} (1967Ko01), 980 {I30} (1963Ri01), 980 {I30} (1957Va08) 
M$|a(exp)=5.9|*10{+-5} {I3} (1967Ko01), 6.3|*10{+-5} {I2} (1957Va08) 
$I(ce)/I|b{++}=1.17|*10{+-4} {I6} (1967Ko01), 1.14|*10{+-4} {I4} (1957Va08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1437.35 {I7} (1990Me15), 1437.529 {I15} (2005TrZZ), 1437.9 {I20} (1969Ar03), and 1438 {I2} (1967Ko01) 
RI$others: 1.2 {I2} (1990Me15), 1.1 {I4} (1969Ar03), 1.3 {I6} (1967Ko01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 2421.8 {I5} (1990Me15), 2420.93 {I4} (2005TrZZ), 2421.7 {I25} (1969Ar03) 
RI$others: 0.10 {I5} (1990Me15), 0.05 {I3} (1969Ar03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 803.25 {I8} (1990Me15) and 802.85 {I3} (2005TrZZ). Other: 801.5 {I10} (1973Ba02) 
RI$others: 1.5 {I2} (1990Me15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
E$weighted average of 928.326 {I6} (1979Gr01), 928.327 {I9} (1990Me15), 928.34 {I6} (2005TrZZ), and 928.280 {I36} (1974HeYW). Others: 928.0 {I5} (1973Ba02), 928.9 {I7} (1967Ko01) 
RI$others: 7.7 {I5} (1990Me15), 7.62 {I9} (1974HeYW); 10 {I1} (1975Al23) and 12 {I2} (1967Ko01) are discrepant 
$I(ce)/I(|b{++})=5.0|*10{+-6} {I25} (1967Ko01) 
M$|a(exp)=2.0|*10{+-4} {I10} (1967Ko01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 2240.394 {I11} (1979Gr01), 2240.398 {I10} (1990Me15), 2240.396 {I16} (2005TrZZ), and 2240.35 {I6} (1974HeYW). Others: 2240.2 {I2} (1973Ba02), 2240.1 {I5} (1969Ar03), 2240.1 {I7} (1967Ko01), 2240.6 {I10} (1963Ri01) 
$1957Va08 placed a E|g=2253 {I15} from a 3240 level and assigned J|p=4+ from their |g|g(|q) and ce data, however, 1957Va08 didn't see the strong 944|g. So the 2253|g from 1957Va08 should correspond to the 2240|g seen in other studies, considering large |DE|g=15 keV 
RI$others: 24.1 {I4} (1990Me15), 18 {I5} (1975Al23), 23.9 {I15} (1974HeYW), 24 {I3} (1969Ar03), 25 {I3} (1967Ko01), 29 {I2} (1963Ri01), 26 {I2} (1957Va08) 
M$|a(exp)=1.51|*10{+-5} {I17} (1957Va08) 
MR$+0.21 {I5} from |g|g(|q) for J(3224)=3 (1957Va08) 
$I(ce)/I|b{++}=7.06|*10{+-7} {I35} (1957Va08) 
$2240|g-984|g(|q): A{-2}=+0.104 {I8}, A{-4}=+0.003 {I12} (1957Va08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 944.132 {I6} (1979Gr01), 944.125 {I7} (1990Me15), 944.135 {I12} (2005TrZZ), 944.117 {I25} (1974HeYW). Others: 943.9 {I3} (1973Ba02), 944.3 {I5} (1967Ko01) 
RI$others: 77.6 {I9} (1990Me15), 79 {I3} (1975Al23), 77.5 {I50} (1974HeYW), 80 {I5} (1967Ko01) 
M$|a(exp)=1.25|*10{+-4} {I11} (1967Ko01) 
$I(ce)/I(|b{++})=2.07|*10{+-5} {I12} (1967Ko01) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_uncertain: S
decay_comment:
E$from Adopted Gammas, not seen in decay studies. 
RI$from I(938|g)/I(2375|g) in Adopted Gammas and I(2375|g) in this dataset 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_comment:
E$weighted average of 2375.1 {I5} (1990Me15) and 2375.20 {I4} (2005TrZZ). Other: 2375.6 {I25} (1969Ar03) 
RI$other: 0.10 {I3} (1969Ar03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$9204.7|g-983.53|g(|q): A{-2}=+0.011 {I43} (1969Te06) 
$10641.9|g-983.53|g(|q): A{-2}=+0.133 {I43} (1969Te06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$other: +0.19|<|d|<+0.23, or -0.38|<|d|<-0.30, or -0.12|<|d|<-0.06 from 1437.5|g-983.5|g(|q), -0.23|<|d|<-0.19 for J(2421)=1 or +0.30|<|d|<+0.38 for J=2 or +0.06|<|d|<+0.12 for J=3 from 9204.7|g-1437.5|g(|q) (1969Te06) 
$1437.5|g-983.5|g(|q): A{-2}=-0.006 {I27}, A{-4}=-0.004 {I40} (1969Te06) 
$9204.7|g-1437.5|g(|q): A{-2}=-0.022 {I25} (1969Te06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 2644 quoted in 1969Te06 
MR$others: -0.25|<|d|<-0.22 or -0.31|<|d|<-0.28 from 2633.3|g-983.5|g(|q), +0.28|<|d|<+0.31 for J(3617)=2 or Mult=Q for J(3617)=2 from 8009.1|g-2633.3|g(|q) (1969Te06) 
$2633.3|g-983.5|g(|q): A{-2}=+0.056 {I28}, A{-4}=-0.002 {I41} (1969Te06) 
$8009.1|g-2633.3|g(|q): A{-2}=-0.114 {I50} (1969Te06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 3485 quoted in 1969Te06 
MR$-0.13|<|d<-0.10 from 3473.9|g-983.5|g(|q), +0.28|<|d|<0.31 for J(4457)=2 or +0.10|<|d<+0.13 for J=3 from 7168.7|g-3473.9|g(|q) in 1969Te06 
$3473.9|g-983.5|g(|q): A{-2}=+0.018 {I7}, A{-4}=+0.010 {I16} (1969Te06) 
$7168.7|g-3473.9|g(|q): A{-2}=-0.033 {I21} (1969Te06) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M$if J=6, E1+M2 excluded from |d and comparison to RUL. 
MR$-0.02 {I+7-3} if J=7, -0.07 {I+7-9} if J=5, or +1.5 {I3} if J=6. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$|d(12|)11)=+0.02 {I6}, |d(10|)11)=-0.05 {I6}, |d(10|)9)=+0.02 {I6}, |d(8|)9)=-0.05 {I6}, |d(8|)7)=+0.02 {I6}, or |d(6|)7)=-0.07 {I6}. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)=100 {I6} (1993Ko57). 
$d|s/d|W=70 {I7} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=75 {I7} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=72 {I7} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$A{-2}=+0.32 {I4}, A{-2}=-0.06 {I7} (1993Ko57). 
$I|g(rel)=8.7 {I5} (1993Ko57). 
$d|s/d|W=15.6 {I23} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=22 {I4} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=18 {I3} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g(rel)=8.1 {I4} (1993Ko57). 
$d|s/d|W=10.0 {I15} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=10.9 {I16} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=10.0 {I15} (E=5.4 MeV, |q=55|'). 
$A{-2}=+0.25 {I4}, A{-2}=-0.03 {I5} (1993Ko57). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)=0.4 {I1} (1993Ko57). 
$d|s/d|W=0.41 {I16} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=0.7 {I2} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=0.5 {I2} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)=0.9 {I2} (1993Ko57). 
$d|s/d|W=2.8 {I4} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=1.45 {I25} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=2.3 {I4} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)=0.4 {I1} (1993Ko57). 
$d|s/d|W=1.43 {I25} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=1.8 {I3} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=1.6 {I3} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g(rel)=1.1 {I3} (1993Ko57). 
$d|s/d|W=4.2 {I7} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=5.2 {I8} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=4.6 {I7} (E=5.4 MeV, |q=55|'). 
$A{-2}=+0.08 {I5}, A{-2}=-0.013 {I50} (1993Ko57). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$I|g(rel)=2.3 {I1} (1993Ko57). 
$d|s/d|W=3.7 {I6} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=5.9 {I9} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=5.4 {I8} (E=5.4 MeV, |q=55|'). 
$A{-2}=+0.18 {I4}, A{-2}=+0.02 {I5} (1993Ko57). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)~0.4 (1993Ko57). 
$d|s/d|W=0.74 {I17} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=1.8 {I3} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=1.4 {I4} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$I|g(rel)=1.3 {I3} (1993Ko57). 
$d|s/d|W=5.7 {I9} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=7.2 {I11} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=6.8 {I10} (E=5.4 MeV, |q=55|'). 
$A{-2}=-0.18 {I6}, A{-2}=+0.001 {I30} (1993Ko57). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)=1.2 {I2} (1993Ko57). 
$d|s/d|W=4.0 {I6} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=3.5 {I6} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=4.2 {I7} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$d|s/d|W=0.95 {I18} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=0.5 {I3} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=0.76 {I25} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
RI$intensity not reported in 1993Ko57 
$d|s/d|W=3.3 {I5} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=3.4 {I5} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=3.5 {I5} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)=0.8 {I2} (1993Ko57). 
$d|s/d|W=2.4 {I10} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=2.6 {I4} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=2.3 {I5} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)|?0.1 (1993Ko57). 
$d|s/d|W=1.3 {I2} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=1.6 {I4} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=1.15 {I25} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)|?0.5 (1993Ko57). 
$d|s/d|W=0.94 {I18} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=0.6 {I2} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=0.77 {I17} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)|?0.3 (1993Ko57). 
$d|s/d|W=1.9 {I3} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=2.0 {I4} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=1.6 {I4} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$from I|g(rel)|?0.1 (1993Ko57). Note that 1974Di08 report this transition as the strongest one from 3783 level. 
$d|s/d|W=1.5 {I5} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=1.00 {I25} (E=5.9 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$from I|g(rel)=0.10 {I3} (1993Ko57). 
$d|s/d|W=0.33 {I13} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=0.5 {I2} (E=5.9 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$unplaced by 1974Di08. 
RI$from I|g(rel)=0.20 {I5} (1993Ko57). 
$d|s/d|W=0.8 {I3} (E=5.9 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$I|g(rel)|?0.4 (1993Ko57). 
$d|s/d|W=1.8 {I5} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=2.8 {I5} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=2.0 {I4} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$unplaced in 1974Di08; placement suggested by evaluator based on energy and branching ratio agreement with (n,|g). 
$d|s/d|W=0.7 {I3} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=0.72 {I17} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=1.0 {I3} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$d|s/d|W=1.8 {I3} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=1.9 {I3} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=2.0 {I3} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$d|s/d|W=1.36 {I25} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=1.8 {I4} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=2.0 {I4} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$d|s/d|W=0.68 {I22} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=1.23 {I23} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=0.75 {I15} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$d|s/d|W=0.5 {I2} (E=4.9 MeV, |q=125|'). 
$d|s/d|W<0.5 (E=5.9 MeV, |q=55|'). 
$d|s/d|W=0.7 {I3} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$d|s/d|W=0.30 {I15} (E=4.9 MeV, |q=125|'). 
$d|s/d|W<0.5 (E=5.9 MeV, |q=55|'). 
$d|s/d|W=0.4 {I2} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
$d|s/d|W=0.67 {I15} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=0.60 {I22} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=0.8 {I3} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_comment:
$d|s/d|W=0.4 {I2} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=0.8 {I3} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=0.5 {I2} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
RI$I(2162|g)/I(3600|g) from E(beam)=5.9 and 5.4 Mev in 1974Di08 don't agree 
$d|s/d|W=1.20 {I25} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=0.55 {I11} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
$d|s/d|W=0.25 {I11} (E=4.9 MeV, |q=125|'). 
$d|s/d|W=0.8 {I3} (E=5.9 MeV, |q=55|'). 
$d|s/d|W=0.95 {I22} (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$it is probably the same transition as 2285|g from 4581 level in (n,|g) E=thermal 
$d|s/d|W=0.3 {I1} (E=5.9 MeV, |q=55|'). 
$d|s/d|W<0.2 (E=5.4 MeV, |q=55|'). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$placement by 1993Ko57 based on agreement with (|a,p|g) data of 1979Gl07 and small I|g. 
$I|g(rel)|?0.1 (1993Ko57). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$from |g(|q,pol) in 1976Mo26 
$A{-2}=+0.55 {I7}, A{-4}=-0.43 {I10} 
$A{-2}=+0.26 {I1}, A{-4}=-0.15 {I1}, POL=-0.39 {I1} (1976Mo26). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$Q from p|g(|q) (1969Mo09); M2 ruled out by RUL 
$A{-2}=+0.60 {I6}, A{-4}=-0.32 {I8} 
$A{-2}=+0.33 {I3}, A{-4}=-0.11 {I3} (1974Ba05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$others: 93 {I2} (1969Mo09), 97 {I1} (1969Ka10), and 94 {I2} (1978DeYT). 
M,MR$D+Q from |g|g(|q) (1966Ma31); E1+M2 ruled out by RUL. Other: +0.11 {I+13-11} from p|g(|q) (1969Mo09). 
$A{-2}=+0.55 {I3}, A{-4}=+0.02 {I4} 
$A{-2}=+0.35 {I3}, A{-4}=-0.03 {I2} (1974Ba05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$others: 7 {I2} (1969Mo09), 3.4 {I10} (1969Ka10), and 6 {I2} (1978DeYT). 
M$Q from p|g(|q) in 1969Mo09 and |g(|q) in 1974Ba05; M2 ruled out by RUL 
$A{-2}=+0.61 {I9}, A{-4}=-0.40 {I11} 
$A{-2}=+0.38 {I3}, A{-4}=-0.15 {I3} (1974Ba05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$others: 20 {I3} (1969Ka10) and 29 {I3} (1978DeYT). 
$A{-2}=-0.08 {I14}, A{-4}=+0.02 {I16} (1974Ba05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$others: 65 {I3} (1969Ka10) and 71 {I3} (1978DeYT). 
M$D+Q from p|g(|q) (1969Mo09); E1+M2 ruled out by RUL 
MR$from 1973Ba02, reanalysis of p|g(|q) in 1969Mo09; original |d=+3.5 {I+6-4} from p|g(|q) in 1969Mo09. Other: +0.27 {I4} or >60 from statistical model analysis (1974Ba05) 
$A{-2}=+0.16 {I3}, A{-4}=+0.14 {I4} 
$A{-2}=+0.11 {I4}, A{-4}=-0.01 {I4} (1974Ba05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI$other: 83 {I2} (1978DeYT). 
MR$-0.2 {I1} or 4 {I1} (1974Ba05). 
$A{-2}=+0.07 {I6}, A{-4}=-0.01 {I5} (1974Ba05) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$other: 2648 from 1969Mo09. Note that 2650|g placed from a 3633 level in 1969Mo09 is suggested to be the same as the 2644|g from the 4940 state in (|a,p|g) (1979Gl07) and (n,|g) E=thermal (1984Ru06). 
M,MR$D+Q from p|g(|q) (1969Mo09), E1+M2 ruled out by RUL 
$A{-2}=+0.21 {I3}, A{-4}=-0.02 {I4} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI$others: 57 {I6} (1968Mo20) and 71 {I6} (1969Ka10). 
M,MR$D+Q from p|g(|q) (1968Mo20); E1+M2 ruled out by RUL. However, it is discrepant with adopted multipolarity. 
$A{-2}=+0.14 {I4}, A{-4}=-0.04 {I6} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$other: 2883 (1969Mo09). 
RI$weighted average of 75 {I5} (1969Mo09) and 71 {I5} (1978DeYT). 
$A{-2}=-0.31 {I3}, A{-4}=+0.06 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 2938.0 {I7} from ({+46}Ar,5n|g), 2936.4 {I16} from (|a,2n|g), and 2935.5 {I20} from ({+9}Be,3n|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 230.39 {I30} from ({+46}Ar,5n|g), 229.6 {I7} from (|a,2n|g), and 229.3 {I3} from ({+9}Be,3n|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$unweighted average of 803.4 {I4} from ({+46}Ar,5n|g), 801.3 {I6} from (|a,2n|g), and 801.5 {I6} from ({+9}Be,3n|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$unweighted average of 1223.7 {I11} from ({+46}Ar,5n|g), 1219.8 {I10} from (|a,2n|g), and 1219.9 {I10} from ({+9}Be,3n|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$E|g=1562.302 {I5} (1979He19) from the decay of {+110m}Ag was used as reference (1984Al18); 1553.71 {I20} (1970Wa29); 1554 {I1} (1969Wa24) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$E|g=1115.546 {I4} (1979He19) from the decay of {+65}Zn was used as reference (1984Al18); 1121.03 {I10} (1970Wa29); 1122 {I1} (1969Wa24) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$E|g=529.653 {I11} (1979He19) from the decay of {+83}Rb was used as reference (1984Al18); 523.50 {I10} (1970Wa29); 524 {I1} (1969Wa24) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$Rounded value from the Adopted Gammas. Existence of the 1554|g from {+50}Sc decay (0.35 s) searched, but not observed by 1984Al18 and 1963Ka16 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$ weak |g shown in level scheme figure 3 of 2002Ja16, where prompt |g rays of 1554 and 1121 keV in {+50}Ti were seen in {+208}Pb({+48}Ca,X|g) reaction. 2002Ja16 do not give any source reference for 3340|g. No such |g is given by 2009Ni17 and 2005Id03, thus not listed in Adopted Levels, gammas dataset 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
$Interference from 1228|g in {+42}Ca. 
$POL=-0.27 {I29} (1979St13) 
MR$from 1978Ha17, but no |g(|q) coefficients are listed 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: S
decay_comment:
E,RI$|g not observed. E|g from {+50}Ti Adopted dataset in the ENSDF database. I|g estimated by 2021Bo21 from a background line near 2314 keV as 5% of the I|g for 2756|g from 4310 level (2021Bo21) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: [E0]
decay_uncertain: ?
decay_comment:
$Estimated intensity of possible E0 transition as 10{+-6} of the intensity of the unobserved 2314-keV transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$uncertainty of 0.089 in Table I of 2021Bo21 seems a misprint, as implied by the uncertainty for the branching ratio. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: S
decay_comment:
E$previously reported |g transition not observed by 2021Bo21. Authors mention that this |g ray could be masked by a Compton edge of strong higher energy |g ray, such as 3132 transition from 5807 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(292|g)(1576|g)(|q): I|g(28|')/I|g(85|')=0.95 {I2} 
$(292|g)(630|g)(|q): I|g(28|')/I|g(85|')=1.10 {I2} 
$(292|g)(1237|g)(|q): I|g(28|')/I|g(85|')=1.21 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(258|g)(1576|g)(|q): I|g(28|')/I|g(85|')=0.81 {I2} 
$(258|g)(292|g)(|q): I|g(28|')/I|g(85|')=1.43 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(387|g)(1576|g)(|q): I|g(28|')/I|g(85|')=0.68 {I2} 
$(387|g)(292|g)(|q): I|g(28|')/I|g(85|')=1.54 {I4} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$|g from 2010Cr02: Phys Rev C 82, 014311 (2010); not seen in 2017Ri09 but included in the fit to extract the upper limit for I|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$591 {I1} with I|g(absolute)=40% {I20} (2004Li75). This |g was also reported in 2002Sh43 and 2008Ma01 


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:
E$weighted average of 1128.2 {I4} ({+56}Sc |b{+-} decay (26 ms+75 ms), 2004Li75); 1128.7 {I3} ({+56}Sc |b{+-} decay (26 ms),2010Cr02); 1128.8 {I5} (({+48}Ca,X|g),2004Fo09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 751.5 {I5} ({+56}Sc |b{+-} decay (26 ms+75 ms), 2004Li75); 750.9 {I4} ({+56}Sc |b{+-} decay (26 ms),2010Cr02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1160.0 {I5} ({+56}Sc |b{+-} decay (26 ms+75 ms), 2004Li75); 1160.6 {I3} ({+56}Sc |b{+-} decay (75 ms),2010Cr02); 1161.0 {I5} (({+48}Ca,X|g),2004Fo09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 690.2 {I4} ({+56}Sc |b{+-} decay (26 ms+75 ms), 2004Li75); 689.6 {I3} ({+56}Sc |b{+-} decay (75 ms),2010Cr02); 690.0 {I5} (({+48}Ca,X|g),2004Fo09) 


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:
E$Unweighted average of 117 keV {I2} (2005Ga01 - ({+76}Ga,X|g)), 114 keV {I2} (2002MaZN - ({+86}Kr,X|g)), and 109.0 keV {I6} (2012Ka36 - ({+238}U,X|g)). 
M$Proposed in 2012Ka36 considering similar E2 isomers such as {+54m}Sc and {+56m}Sc. Higher multipolarities excluded, based on RUL. 


decay_energy_unit: KEV
decay_multipolarity: [E2]
decay_comment:
E$Uncertainty estimated by the evaluator based on the note in 2012Ka36 that systematic uncertainty of |g-ray energy was 0.5 keV and statistical uncertainty was much smaller, evaluator assume 0.3 keV. 
M$Proposed in 2012Ka36 considering similar E2 isomers such as {+54m}Sc and {+56m}Sc. Higher multipolarities excluded, based on RUL. 


decay_energy_unit: KEV
decay_multipolarity: [M2]
decay_comment:
E$Could not perform |g-|g coincidence for placement. Not adopted by evaluator. Not mentioned/discussed in primary publication (2011Da08) of 2002MaZN work. 


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:
E$this value can be compared to 113.3 keV {I23} in {+59}Ti Adopted dataset in the ENSDF database (April 2018 update), and 109.0 keV in 2012Ka36 (Phys. Rev. C 86, 054319). 


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:
$The 125.0|g may be the same as 126 keV {I2} reported by 2002MaZN from its coincidence with heavy ions. 


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:
$This |g may be the same as 126 keV {I2} reported by 2002MaZN from its coincidence with heavy ions. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$|g not seen, only an upper limit is given. This is in contrast to 235-keV transition in {+44}Sc from an analog level at 235 keV, where branching ratio of parity-conserving (166|g) to parity non-conserving transition (235|g) is 1:2 


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:
BE2$B(E2) deduced in 2011Ho02 assuming a 45% branching ratio for 57-keV transition as discussed in 1980Gr04. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$ from figure 1 of 2001Br29. E|g=777.4 from level-energy difference. E|g=772.2 in table II of 2001Br29 is a misprint 


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,RI from |b{++} decay 
M from |a(K)exp in (p,n|g), |g(|q) in (p,|g), and comparison to RUL 
MR value from |a(K)exp in (p,n|g); sign from |g(|q) in (p,|g). Note that 1978Kr19 recommended +0.10 {I6} from |g(|q) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_mixing_ratio_info: ;ERR=LE
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M$J|)J or J|)J-2 from angular anisotropy in ({+40}Ca,n2p|g). Ne M2 from comparison to RUL. |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
M from |g(|q) in (p,n|g). |D|p=no from level scheme 
MR -0.2 {I+1-2} or -2.4 {I+7-11} from |g(|q) in (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E weighted average from (p,n|g), {+28}Si({+28}Si,2|ap|g) E=125 MeV, {+10}B({+40}Ca,n2p|g),{+24}Mg({+32}S,2|ap|g),..., and {+28}Si({+28}Si,2|ap|g) E=110, 115 MeV 
M$approximately stretched Q in ({+32}S,2|ap|g). J|)J or J|)J-2 from angular anisotropy in ({+40}Ca,n2p|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M Q(+O) from |g(|q) in (p,|g). |D|p=no from level scheme 
MR -0.01 {I8} from |g(|q) in (p,|g). |<0.00091 {I19} from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$approximately stretched Q in ({+32}S,2|ap|g); J|)J or J|)J-2 from angular anisotropy in ({+40}Ca,n2p|g). Ne M2 from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$J|)J or J|)J-2 from angular anisotropy in ({+40}Ca,n2p|g). Ne M2 from from comparison to RUL; Ne J|)J from existence of cascade 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:
M$J|)J or J|)J-2 from AD. Ne M2 from comparison to RUL. Ne J|)J from existence of cascade 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:
M$J|)J or J|)J-2 from AD and DCO in {+28}Si({+28}Si,2|ap|g) E=125 MeV and from angular anisotropy in ({+40}Ca,n2p|g). Ne J|)J from existence of cascade transition; Ne M2 from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$J|)J-2 Q from DCO in {+28}Si({+28}Si,2|ap|g) E=125 MeV. Ne M2 from comparison to RUL. |DJ=2 from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
RI$branching ratios in {+28}Si({+28}Si,2|ap|g) E=125 MeV and {+28}Si({+28}Si,2|ap|g) E=110, 115 MeV are discrepant 
M$J|)J-1 d from AD in {+28}Si({+28}Si,2|ap|g) E=125 MeV. Ne E1 from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI$branching ratios in {+28}Si({+28}Si,2|ap|g) E=125 MeV and {+28}Si({+28}Si,2|ap|g) E=110, 115 MeV are discrepant 
M$J|)J-1 d from AD in {+28}Si({+28}Si,2|ap|g) E=125 MeV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
E,RI$from {+28}Si({+28}Si,2|ap|g) E=125 MeV 
M$J|)J-2 Q from AD in {+28}Si({+28}Si,2|ap|g) E=125 MeV. Ne M2 from comparison to RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI only the unshifted peak was analyzed by 1976To02 due to the presence of another strong line near the shifted peak 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$J|)J or J|)J-2 from AD. |=M2 from comparison to RUL. |= J|)J from existence of cascade transition? 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
M$J|)J or J|)J-2 from AD and DCO. |=M2 from comparison to RUL. |= J|)J from existence of cascade transition? 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR -0.29 {I7} or <-0.6 given by 1986De13 for 3793|g assumed to belong to this transition since 3793|g was not observed (evaluator) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|a(exp)=0.0411 {I28} 
M,MR from |a(K)exp and K/L+ (evaluator) 
CC |S|a(exp)'s 
EKC,ELC+,K/L+$from 1967Me18 (E=5.8 MeV; s) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 308.24 {I6} from {+48}Cr |e decay (21.56 h), 308.9 {I5} from ({+40}Ca,2p|g), 308.3 {I1} from ({+24}Mg,n3p|g), 308.2 {I2} from ({+16}O,pn|g), 308.5 {I8} from (p,|g), and 308.3 {I1} from (p,n|g) 
M$from ce data and |g|g(|q,pol) in {+48}Cr |e decay (1979PrZU,1968We01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 112.31 {I8} from {+48}Cr |e decay (21.56 h), 112.4 {I1} from ({+24}Mg,n3p|g), 112.4 {I2} from ({+16}O,pn|g), and 112.5 {I1} from (p,n|g). Other: 112.2 {I5} from ({+40}Ca,2p|g) 
RI$from {+48}Cr |e decay. 
M$from ce data and |g|g(|q,pol) in {+48}Cr |e decay (1979PrZU,1968We01) 
MR$from |g|g(|q) in {+48}Cr |e decay (1968We01). Other: -0.14<|d<-0.02 from |g(|q) in (p,n|g) (1973SaZF) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from (p,n|g). Others: 428.2 {I5} from ({+40}Ca,2p|g), 427.8 {I4} from ({+24}Mg,n3p|g), 427.9 {I2} from ({+16}O,pn|g), and 428.0 {I12} from (p,|g) 
M$from |g(|q,pol) and |g(|q) in (p,n|g) (1976Ri01,1973SaZF). 
MR$from |g(|q) in (p,n|g) (1973SaZF). Other: 0.13 {I8} from |g(|q,pol) in (p,n|g) (1976Ri01), -0.13 {I3} from |g(|q) in ({+16}O,pn|g) (1974Ta15) 


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$weighted average of 97.7 {I1} from ({+24}Mg,n3p|g), 98.0 {I2} from ({+16}O,pn|g), and 98.0 {I1} from (p,n|g). Other: 99.0 {I10} from ({+40}Ca,2p|g) 
RI$unweighted average of 50 {I13} from ({+40}Ca,2p|g), 52 {I11} from ({+24}Mg,n3p|g), 40.8 {I28} from ({+16}O,pn|g), and 61.3 {I32} from (p,n|g) 
M,MR$D(+Q) with |d=+0.15 {I23} from |g(|q) in (p,n|g); |D|p=yes from level scheme; M2 is less likely based on RUL. Other: |d(Q/D)=0.0 {I2} from ({+16}O,pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1+M2)
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
$B(M2)(W.u.)=2.2 {I+46-18} exceeds RUL=1.0 
E$weighted average of 210.8 {I5} from ({+40}Ca,2p|g), 210.3 {I1} from ({+24}Mg,n3p|g), 210.4 {I2} from ({+16}O,pn|g), 210.7 {I8} from (p,|g), and 210.4 {I1} from (p,n|g) 
RI$from ({+16}O,pn|g). Others: 100 {I13} from ({+40}Ca,2p|g), 100 {I11} from ({+24}Mg,n3p|g), and 100.0 {I32} from (p,n|g) 
M$D+Q from |g(|q) in (p,n|g); |D|p=yes from level scheme 
MR$from |g(|q) in (p,n|g). Other: +0.03 {I5} from ({+16}O,pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from ({+24}Mg,n3p|g) and (p,n|g). Others: 185.5 {I5} from ({+16}O,pn|g) 
RI$from ({+24}Mg,n3p|g) and (p,n|g). Others: 12.4 {I34} from ({+16}O,pn|g) 
M,MR$D(+Q) from |g(|q) in (p,n|g); |D|p=no from level scheme. Other: |d(Q/D)=+0.01 {I9} from |g(|q) in ({+16}O,pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from ({+24}Mg,n3p|g) and (p,n|g). Others: 613.5 {I2} from ({+16}O,pn|g); 616.1 {I15} from (p,|g) is discrepant 
RI$from ({+24}Mg,n3p|g) and (p,n|g). Others: 100.0 {I34} from ({+16}O,pn|g) 
M$from |g(|q) and |g(pol) in (p,n|g) and |g(|q) in ({+16}O,pn|g). 
MR$unweighted average of -0.44 {I10} (1974Ta15) from ({+16}O,pn|g) (1974Ta15), -0.19 {I2} (1973SaZF) and -0.28 {I5} (1976Ri01) from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from ({+24}Mg,n3p|g), ({+16}O,pn|g), and (p,n|g). Other: 199.6 {I5} from ({+40}Ca,2p|g), 
RI$unweighted average of 44.0 {I10} from ({+40}Ca,2p|g), 75 {I9} from ({+24}Mg,n3p|g), 82 {I15} from ({+16}O,pn|g), and 59 {I8} from (p,n|g) 
M$from |g(|q,pol) in ({+16}O,pn|g) (1976Ri01) 
MR$from |g(|q) in ({+16}O,pn|g) (1974Ta15). Others: -0.11 {I9} from |g(|q,pol) in ({+16}O,pn|g) (1976Ri01), -0.23<|d<+0.03 from (p,n|g) (1973SaZF) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from (p,n|g). Others: 627.7 {I5} from ({+40}Ca,2p|g), 627.2 {I3} from ({+24}Mg,n3p|g), and 627.2 {I4} from ({+16}O,pn|g) 
RI$from (p,n|g). Others: 100 {I10} from ({+40}Ca,2p|g), 100 {I9} from ({+24}Mg,n3p|g), and 100 {I15} from ({+16}O,pn|g) 
M$Q from |g(|q) in (p,n|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from ({+24}Mg,n3p|g). Others: 226.4 {I5} from ({+40}Ca,2p|g), 226.3 {I2} from ({+16}O,pn|g), 227.2 {I8} from (p,|g), and 226.3 {I1} from (p,n|g) 
RI$from (p,n|g). Others: 100.0 {I22} from ({+24}Mg,n3p|g) and 100.0 {I22} from ({+16}O,pn|g) 
M$M1+E2 with |d(E2/M1)=-0.14 {I12} or E1+M2 with |d(M2/E1)=-2.7 {I6} from |g(|q,pol) in (p,n|g) (1976Ri01), with the latter ruled out by RUL 
MR$from |g(|q) in (p,n|g) (1973SaZF). Other: -0.14 {I12} from |g(|q,pol) in (p,n|g) (1976Ri01), -0.02 {I4} from |g(|q) in ({+16}O,pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$from ({+24}Mg,n3p|g). Others: 324.2 {I5} from ({+16}O,pn|g) and 324.2 {I1} from (p,n|g) 
RI$from (p,n|g). Others: 3.4 {I9} from ({+24}Mg,n3p|g) and 3.3 {I11} from ({+16}O,pn|g) 
M,MR$D(+Q) from |g(|q) in (p,n|g) (1973SaZF); |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
E$weighted average of 436.6 {I1} from ({+24}Mg,n3p|g) and 436.8 {I1} from (p,n|g). Other: 436.7 {I5} from ({+16}O,pn|g) 
RI$from (p,n|g). Others: 5.3 {I10} from ({+24}Mg,n3p|g) and 5.4 {I22} from ({+16}O,pn|g) 
M,MR$D(+Q) from |g(|q) in (p,n|g) (1973SaZF); |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from ({+24}Mg,n3p|g) and (p,n|g). Other: 457.2 {I15} from (p,|g) 
RI$from (p,n|g). Other: 100 {I20} from (p,|g) 
M$M1(+E2) with |d=0.00 {I5} or E1+M2 with |d=-3.4 {I10} for J(765)=3 from |g(|q,pol) in (p,n|g) (1976Ri01), with the latter ruled out by RUL. 
MR$from |g(|q) in (p,n|g) (1973SaZF). Other: 0.00 {I5} from |g(|q,pol) in (p,n|g) (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_comment:
E$from ({+24}Mg,n3p|g) and (p,n|g). Other: 767.4 {I15} from (p,|g) is discrepant 
RI$from (p,n|g) 
M,MR$D(+Q) from |g(|q) in (p,n|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 775.8 {I5} from ({+40}Ca,2p|g) and 776.2 {I10} from ({+16}O,pn|g) 
M$strong stretched dipole from |g anisotropy in ({+16}O,pn|g) (1974Ta15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from (p,n|g) and ({+24}Mg,n3p|g). Other: 310.8 {I2} from ({+16}O,pn|g) 
RI$from (p,n|g) and ({+16}O,pn|g). Other: 100.0 {I34} from ({+24}Mg,n3p|g) 
M$from |g(|q,pol) and |g(|q) in (p,n|g) (1976Ri01,1973SaZF) 
MR$from |g(|q) in ({+16}O,pn|g) (1974Ta15). Other: 0.05 {I9} from |g(|q,pol) in (p,n|g) (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from ({+24}Mg,n3p|g). Others: 537.2 {I10} from ({+16}O,pn|g), 537.0 {I15} from (p,|g), and 537.2 {I2} from (p,n|g) 
RI$weighted average of 5.6 {I11} from ({+24}Mg,n3p|g), 9.9 {I33} from ({+16}O,pn|g), and 8.7 {I33} from (p,n|g). 
M,MR$Q(+O) from |g(|q) in ({+16}O,pn|g) (1974Ta15); M2(+E3) ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_mixing_ratio_info: ;ERR=LE
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LT
decay_comment:
E$weighted average of 1100.0 {I10} from ({+40}Ca,2p|g), 1099.2 {I4} from ({+24}Mg,n3p|g), 1099.2 {I2} from ({+16}O,pn|g), and 1099.3 {I2} from (p,n|g). Other: 1102.5 {I25} from (p,|g) 
M$from |a(K)exp and |g(|q,pol) in (p,n|g) 
MR$from |a(K)exp=4.0|*10{+-5} {I6} in (p,n|g) (1977Sa03). Other: -0.015 {I155} from |g(|q,pol) in (p,n|g) (1976Mo26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LE;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LE
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 627.7 {I5} from ({+40}Ca,2p|g), 627.4 {I4} from ({+24}Mg,n3p|g), and 627.7 {I8} from ({+16}O,pn|g) 
M,MR$D(+Q) from |g(|q) in ({+16}O,pn|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from ({+24}Mg,n3p|g) and (p,n|g). Other: 651.9 {I10} from ({+16}O,pn|g) 
RI$from (p,n|g). Other: 100 {I6} from ({+24}Mg,n3p|g) 
M$M1+E2 with |d=-0.32 {I14} or E1+M2 with |d=-4 {I2} for J(1265)=5 from |g(|q,pol) in (p,n|g) (1976Ri01), with the latter ruled out by RUL 
MR$weighted average of -0.32 {I14} (1976Ri01) and -0.15 {I12} (1973SaZF) in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 501.7 {I1} from ({+24}Mg,n3p|g), 501.9 {I2} from ({+16}O,pn|g), and 501.8 {I1} from (p,n|g) 
RI$from ({+24}Mg,n3p|g). Others: 100 {I10} from ({+16}O,pn|g) and 100 {I5} from (p,n|g) 
M$M1+E2 with |d=-0.23 {I17} or E1+M2 with |d=-1.8 {I5} for J(1558)=4 from |g(|q,pol) in (p,n|g) (1976Ri01), with the latter ruled out by RUL 
MR$weighted average of -0.09 {I3} from |g(|q) in (p,n|g) (1973SaZF) and -0.12 {I4} from |g(|q) in ({+16}O,pn|g) (1974Ta15). Other: -0.23 {I17} from |g(|q,pol) in (p,n|g) (1976Ri01) 


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$from ({+24}Mg,n3p|g). Others: 812.7 {I10} from ({+16}O,pn|g) and 812.2 {I3} from (p,n|g) 
RI$weighted average of 18 {I4} from ({+24}Mg,n3p|g), 41 {I10} from ({+16}O,pn|g), and 28 {I5} from (p,n|g) 
M$Q from |g(|q) in (p,n|g) and (Q) from |g anisotropy in ({+16}O,pn|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 586.5 {I4} from ({+24}Mg,n3p|g), 586.4 {I5} from ({+16}O,pn|g), and 586.3 {I2} from (p,n|g) 
M,MR$D(+Q) from |g(|q) in ({+16}O,pn|g); |D|p=(no) from level scheme. Other: stretched dipole D from |g anisotropy in ({+40}Ca,2p|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=LE;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=LE
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 504.7 {I3} from ({+24}Mg,n3p|g) and 504.9 {I2} from ({+16}O,pn|g) 
RI$from ({+24}Mg,n3p|g). Others: 100 {I10} from ({+16}O,pn|g) and 100 {I10} from (|a,pn|g) 
M,MR$D(+Q) from |g(|q) in ({+16}O,pn|g); |D|p=(no) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$from ({+24}Mg,n3p|g). Other: 1006.3 {I10} from ({+16}O,pn|g), 1007.0 from (|a,pn|g) 
RI$weighted average of 54 {I8} from ({+24}Mg,n3p|g), 43 {I10} from ({+16}O,pn|g), and 45 {I10} from (|a,pn|g) 
M$(Q) from |g anisotropy in ({+16}O,pn|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 976.6 {I4} from ({+24}Mg,n3p|g) and 977.3 {I2} from ({+16}O,pn|g) 
M,MR$D+Q with |d=-0.34 {I4} from |g(|q) in ({+16}O,pn|g); E1+M2 with this |d value is ruled out by RUL; stretched dipole (|DJ=1) from anisotropy in ({+40}Ca,2p|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$weighted average of 1604.2 {I4} from ({+24}Mg,n3p|g) and 1603.4 {I15} from ({+16}O,pn|g) 
RI$other: I(1604|g)/I(977|g)=100/75 from ({+40}Ca,2p|g) 
M$stretched (|DJ=2) quadrupole or |DJ=0 dipole from angular anisotropy in ({+40}Ca,2p|g); M2 ruled out by RUL; |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$other: 712.7 {I10} from ({+16}O,pn|g) 
M$stretched dipole (|DJ=1) from |g anisotropy in ({+40}Ca,2p|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from ({+16}O,pn|g). Other: 394.9 {I4} from ({+24}Mg,n3p|g) 
RI$from ({+24}Mg,n3p|g). Other: 49 from ({+40}Ca,2p|g) 
M,MR$D+Q from |g(|q) in ({+16}O,pn|g); E1+M2 with the given |d is ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1371.4 {I4} from ({+24}Mg,n3p|g) and 1371.9 {I3} from ({+16}O,pn|g) 
RI$from ({+24}Mg,n3p|g). 
M,MR$Q(+O) from |g(|q) in ({+16}O,pn|g); M2(+E3) ruled out by RUL. Other: |g anisotropy from ({+40}Ca,2p|g) consistent with |DJ=0 or |DJ=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:
E,RI$other: 716.9 {I10} with I|g=100 {I15} from ({+16}O,pn|g) 
M$(D), |DJ=(1) from |g anisotropy in ({+16}O,pn|g); |D|p=(no) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$other: 1221.8 {I15} from ({+16}O,pn|g) 
RI$weighted average of 39 {I7} from ({+24}Mg,n3p|g) and 45 {I15} from ({+16}O,pn|g) 
M$(Q), |DJ=(2) from |g anisotropy in ({+16}O,pn|g); (M2) ruled out by RUL 


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$weighted average of 775.7 {I4} from ({+24}Mg,n3p|g) and 774 {I1} from ({+16}O,pn|g) 
M$stretched D from |g anisotropy in ({+40}Ca,2p|g); (M1) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E,RI$from ({+24}Mg,n3p|g). Other: 806.6 {I10} from ({+16}O,pn|g) 
M$stretched dipole from |g anisotropy in ({+40}Ca,2p|g) and ({+16}O,pn|g); |D|p=(no) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E,RI$other: 1588 with I|g=50 from ({+40}Ca,2p|g) 
M$stretched (|DJ=2) quadrupole or |DJ=0 dipole from angular anisotropy in ({+40}ca,2p|g); M2 ruled out by RUL; |D|p=(no) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$other: 1523.5 {I16} from ({+16}O,pn|g) 
M$(Q) from |g anisotropy in ({+16}O,pn|g) for 1523.5|g, placed from a 3586, (7-) level which is only tentatively proposed by 1974Ta15. But the level scheme here gives |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1680.3 {I4} from ({+24}Mg,n3p|g) and 1680.5 {I6} from ({+16}O,pn|g) 
M$|DJ=0 or stretched quadrupole (|DJ=2) from |g anisotropy in ({+40}Ca,2p|g) and |g(|q) in ({+27}Al,3n3p|g); M2 ruled out by RUL; |D|p=(no) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$|DJ=0 or stretched quadrupole (|DJ=2) from |g anisotropy in ({+40}Ca,2p|g) and |g(|q) in ({+27}Al,3n3p|g); M2 ruled out by RUL; |D|p=(no) from level scheme 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D,Q
decay_uncertain: ?
decay_comment:
E$from ({+40}Ca,2p|g) only 
M$|DJ=0 dipole or |DJ=2 stretched quadrupole from |g anisotropy in ({+40}Ca,2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$from ce data in 1979PrZU and |g|g(|q,pol) in 1968We01. 
$A{-2}=-0.057 {I15}, A{-4}=-0.055 {I22} (1969PaZT), for 112|g-308|g(|q) 
$A{-2}=-0.060 {I6}, A{-4}=+0.002 {I4} (1967Au02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI$other: 55 (1994Ca04) 
M$|g(|q) shows strong stretched dipole pattern (1973Hu08) 
$A{-2}=-0.40 {I2}, A{-4}=+0.02 {I2} 
$Anisotropy=0.82 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$other: 100 from 1994Ca04, and the original value=55 is normalized to 100 for the sum of all decays to the ground state 
$A{-2}=0.00 {I2}, A{-4}=-0.01 {I2} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI$other: 5.5 (1994Ca04) 
M$|g(|q) consistent with stretched dipole (1973Hu08) 
$A{-2}=-0.11 {I4}, A{-4}=+0.03 {I5} 
$Anisotropy=0.89 {I7} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_uncertain: ?
decay_comment:
E$this energy is inconsistent with level-energy difference=1581 and values in other studies. It is more likely in error 
$Anisotropy=1.7 {I4} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_uncertain: ?
decay_comment:
$placed from the 4675 level by 1991Ca30 in {+27}Al({+27}Al,3n3p|g) and 2002Br42 in {+24}Mg({+28}Si,n3p|g), which is adopted by the evaluator. 
$Anisotropy=1.4 {I1} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_uncertain: ?
decay_comment:
$placed from the 4969 level by 1991Ca30 in {+27}Al({+27}Al,3n3p|g) and 2002Br42 in {+24}Mg({+28}Si,n3p|g), which is adopted by the evaluator. 
$Anisotropy=0.8 {I2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$placement from the level scheme in FIG.3 of 1991Ca30; this |g is placed from the 2627 level in TABLE II, which should be incorrect 
$A{-2}=-0.81 {I15}, A{-4}=+0.17 {I14} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$placement from the level scheme in FIG.3 of 1991Ca30; this |g is placed from a 1655 level in TABLE II, which should be incorrect 
$A{-2}=-1.3 {I2}, A{-4}=+0.5 {I1} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E$1704 in FIG.3 of 1991Ca30 is a typo since level-energy difference gives 1764 from the level scheme in FIG.3 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
$tentatively placed by 1991Ca30; this placement is confirmed by 2002Br42 for a 2046|g in {+24}Mg({+28}Si,n3p|g). A 2045|g placed from a 8290 level by 1994Ca04 (same authors as 1991Ca30) in {+10}B({+40}Ca,2p|g) should be the same transition. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
$tentatively placed by 1991Ca30; this placement is confirmed by 2002Br42 for a 2343|g in {+24}Mg({+28}Si,n3p|g). A 2344|g placed from a 8589 level by 1994Ca04 (same authors as 1991Ca30) in {+10}B({+40}Ca,2p|g) should be the same transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$I{-rel}=1.5 
E$uncertainty of 5 keV quoted by 2002Br42 seems unusually large and could be a typo, which could be 0.5 keV. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$I{-rel}=11 listed in Table III of 2002Br42 could be in error since it is inconsistent with the branching ratio 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from |g(|q,pol) in 1976Ri01 and |g(|q) in 1974Ta15 
MR$others: -0.11 {I9} for J(627)=6+, +0.19 {I10} for J=4+ (1976Ri01) 
$A{-2}=-0.57 {I2}, A{-4}=+0.08 {I2} 
$A{-2}=-0.46 {I3}, A{-4}=+0.03 {3}, POL=-0.08 {I10} (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$other: 586 {I1} (1976Mo26) 
$A{-2}=-0.34 {I3} from 1974Ta15, 1976Mo26 found that the same line is almost degenerate with a transition in {+45}Ti 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
E$this |g is unassigned by 1974Ta15; a similar |g is found to de-excite the 1686 levels by 2002Br42 


decay_energy_unit: KEV
decay_multipolarity: D+Q
decay_comment:
E$1974Ta15 assigned this |g to the 2626 state but this |g is found to deexcite the 2232 level in other studies (1991Ca30, 1994Ca04, 2002Br42) 
$I(977.3|g)/I(1371.9|g)=26 {I5}/74 {I5} (1974Ta15) 
$A{-2}=-0.93 {I10}, A{-4}=+0.15 {I12} 


decay_energy_unit: KEV
decay_comment:
E$unassigned by 1974Ta15; placement from 1976Mo26. Other: 712 {I1} (1976Mo26) 
$A{-2}=-1.0 {I5} (1976Mo26) 


decay_energy_unit: KEV
decay_multipolarity: D+Q
decay_comment:
E$1974Ta15 assigned this |g to a 1650, 8(+) state but this |g is found to deexcite the 2626 level in other studies by 1991Ca30, 1994Ca04, and 2002Br42 
$A{-2}=-0.41 {I2} 


decay_energy_unit: KEV
decay_multipolarity: (D)
decay_comment:
E$the placement from a 3586 level by 1974Ta15 is tentative with no supporting |g|g-coin. A transition with the similar energy is found to de-excite the 3982 level based on |g|g-coin, by 1976Mo26 in {+27}Al({+24}Mg,2pn|g) and by 1977Sa03 in (|a,pn|g), and is confirmed by 1991Ca30 in {+27}Al({+27}Al,3p3n|g) and {+40}Ca({+14}N,2n4p|g). Other: 805 {I1} (1976Mo26) 
$I(1523.5|g)/I(806.6|g)=32 {I15}/68 {I15} (1974Ta15) 
$A{-2}=-0.18 {I11} (1976Mo26) 
$W(0|')/W(90|')=0.42 {I23} (1974Ha33) 


decay_energy_unit: KEV
decay_multipolarity: (Q)
decay_comment:
E$the placement from a 3586 level by 1974Ta15 is tentative with no supporting |g|g-coin and also this transition is masked by 1524.2|g of {+42}Ca as noted in 1974Ta15. The same transition is suggested by 1977Sa03 in (|a,pn|g) to deexcite the 4150 level, which is adopted in Adopted Levels 
$I(1523.5|g)/I(806.6|g)=32 {I15}/68 {I15} (1974Ta15) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$1977Sa03 suggest that this |g may be the same as the 1523.5|g placed as deexciting the 3586 state by 1974Ha33 in {+34}S({+16}O, pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$D+Q from |g(|q) in 1973SaZF; E1+M2 is ruled out by RUL for measured |d(Q/D) in 1973SaZF 
MR$from -0.14<|d<-0.02 in 1973SaZF 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from -0.15<|d<-0.12 in 1973SaZF. Others: -0.13 {I8} for J|p(428)=5+, +0.31 {I15} or +7 {I5} for 3+, <-1.2 for 4+ (1976Ri01) 
$A{-2}=-0.46 {I2}, A{-4}=-0.06 {3}, POL=-0.20 {I10} (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$from -0.21<|d<-0.17 in 1973SaZF. Others: -0.28 {I5} for J|p(613)=4+, -0.21 {I6} or -2.5 {I10} for 3-, , +0.27 {I5} for 5- (1976Ri01) 
$A{-2}=+0.16 {I2}, A{-4}=+0.01 {2}, POL=+0.56 {I6} (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$from -0.08<|d<-0.06 in 1973SaZF. Others: |d(E2/M1)=-0.14 {I12} or |d(M2/E1)=-2.1 {I6} from |g(|q,pol) in 1976Ri01 
$A{-2}=-0.27 {I2}, A{-4}=+0.01 {3}, POL=-0.18 {I4} (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$from -0.03<|d<-0.01 in 1973SaZF. Others: 0.00 {I5} for 3+, -3.4 {I10} for 3-, <-0.58 for 2- (1976Ri01) 
$A{-2}=-0.29 {I1}, A{-4}=-0.01 {2}, POL=-0.25 {I5} (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
M$M1+E2 for J(1056)=3- or E1+M2 for 2+ from |g(|q,pol) in 1976Ri01, with the former consistent with |g(|q) in 1973SaZF 
MR$from 1976Ri01. Other: |d(M2/E1)<-0.58 for J(1056)=2+ (1976Ri01) 
$A{-2}=-0.22 {I2}, A{-4}=+0.03 {2}, POL=-0.60 {I10} (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_mixing_ratio_info: ;ERR=LE
decay_comment:
M,MR$from |a(K)exp=4.0|*10{+-5} {I6} (1977Sa03). Others: |d(M2/E1)=-0.015 {I155} from |g(|q,pol) in 1976Mo26; -0.1 {I3} for J|p(1099)=4-, +0.33 {I13} for 5+, -2.0 to -0.3 for 3+ from |g(|q,pol) in 1976Ri01 
$A{-2}=+0.40 {I2}, A{-4}=-0.01 {I2}, POL=-0.32 {I18} (1976Mo26) 
$A{-2}=+0.39 {I6}, A{-4}=+0.02 {9}, POL=+0.69 {I10} (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$from -0.26<|d<-0.03 in 1973SaZF. Others: -0.32 {I14} for J|p(1265)=5+, -0.05 {I5} or 3 to 12 for 3+, >0.7 for 4-, -4 {I2} for 5- (1976Ri01) 
$A{-2}=-0.53 {I9}, A{-4}=+0.15 {9}, POL=-0.24 {I9} (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR$from -0.11<|d<-0.06 in 1973SaZF. Others: -0.23 {I17} for J|p(1558)=4-, -1.8 {I5} for 4+, 0.3 to 1.7 for 2+ (1976Ri01) 
$A{-2}=-0.71 {I5}, A{-4}=+0.15 {6}, POL=-0.18 {I16} (1976Ri01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M from |a(exp) in (p,n|g) and comparison to RUL. |D|p=1 d |g from recoil-|g(|q) in (40C,3p|g) 
MR see discussion in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI weighted av of I|g(62|g)/I|g(153|g)=72.4 {I35}/100.0 {I52} from (|a,p|g) and 68.9 {I32}/100.0 {I32} from (p,n|g). I|g(62|g)/I|g(153|g)=54.0 {I7}/100.0 {I4} from B=decay and 100/92 from (p,|g) discrepant 
M D from comparison to RUL. |D|p=no from the level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M Q(+O) from p|g(|q) in (|a,p|g). Ne M2(+E3) from comparison to RUL. |DJ=2 Q or |DJ=0 d |g from recoil-|g(|q) in ({+40}Ca,3p|g) 
MR -0.03 {I3} from p|g(|q)in (|a,p|g). <0.00033 {I3} from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
M from |a(exp) and |g(|q) in (p,n|g) 
$0.05<|d<0.5 from |g(|q) in (p,|g). Other: +0.18 {I5} from (p,n|g) not adopted from comparison to RUL. |d<0.054 {I14} from comparison to 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:
M D,E2 from |a(exp) in (p,n|g). |D|p=yes from level scheme 
MR 0.6 {I5} from |a(exp) in (p,n|g), <0.06 from comparison to RUL if E1+M2 


decay_energy_unit: KEV
decay_multipolarity: D,Q
decay_uncertain: ?
decay_comment:
$$ 7.3|<I{-|g}|<250 from I|g(1023|g)/I|g(1157|g)=5/11 and I|g(1023|g)/I|g(2178|g)=5/2 in ({+40}Ca,3p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M from |a(exp) in (p,n|g) and comparison to RUL. |DJ=2 Q or |DJ=0 d from recoil-|g(|q) in ({+40}Ca,3p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=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:
$-0.04<|d<0.10 
M D(+Q) from p|g(|q) in (|a,p|g). Ne E1 from comparison to RUL. |DJ=2 Q or |DJ=0 d |g from recoil-|g(|q) in ({+40}Ca,3p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M D,E2 from comparison to RUL. |DJ=2 Q or |DJ=0 d from recoil-|g(|q) in ({+40}Ca,3p|g). |DJ|p=2,no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2,E2
decay_comment:
M D+Q,Q from p|g(|q) in (|a,p|g). |d(9/2) and comparison to RUL exclude E1+M2; Ne M2 from comparison to RUL 


decay_energy_unit: KEV
decay_multipolarity: (M1(+E2))
decay_mixing_ratio_info: ;ERR=LT
decay_uncertain: ?
decay_comment:
$0.26 W.u.|<B(M1)|<1.7 W.u. 
M D from comparison to RUL. |D|p=no from the level scheme 
$0.4|<I{-|g}|<2.5 from I|g(134|g)/I|g(599|g)=0.0125 and I|g(134|g)/I|g(1707|g)=0.025 in ({+40}Ca,3p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2 x (fm)^4
decay_BM_info: ;TYPE=BM3;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM3W
decay_comment:
M Q+O from p|g(|q) in (|a,p|g). Ne M2+E3 from comparison to RUL. |DJ=2 Q or |DJ=0 d from recoil-|g(|q) in ({+40}Ca,3p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_comment:
M,MR other: D+Q, -0.85 {I+6-4} (J{-i}=11/2); Q+O, +0.01 {I2} (J{-i}=15/2) (1973Sa12). |D(11/2) not consistent with |a(exp) in (p,n|g) (evaluator). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR -0.18 {I8}; -11 {I6}; <-31 (J{-i}=3/2). Other J{-i} considered but results not presented by 1975Ha12 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR -0.02 {I20}; <+11.4; >+2.3; -|@ (J{-i}=3/2). J{-i}=5/2 also considered by 1975Ha12 but results not presented. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
MR -0.10<|d<+1.00 (J{-i}=J{-f}=9/2); -0.10<|d<+0.90 (J{-i}=J{-f}=11/2); -0.10<|d<+0.80 (J{-i}=J{-f}=13/2). It is not clear if 1975Ha12 considered and rejected J{-i}=7/2 (evaluator) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Evaluator's Note: possible contaminant since I|g(1268|g)/I|g(1254|g)|?1 and 1254|g was observed in (|a,p|g) while 1268|g was not. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
$|a(exp)=0.0346 {I22} 
MR note that 1967Me18 adopt |d|?-0.5 from their |g(|q) data. This is discrepant both with their ce data and with comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2+M3)
decay_comment:
MR$from DCO value; agrees with the theoretical value 0.03 obtained from |g-ray transition probabilities using the ANTOINE computer code. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 226.2 {I6} from (|a,p|g), 226.2 {I5} from (|a,np|g), and 226.3 {I3} from (p,n). Other: 225 {I3} from Coulomb excitation 
M$D(+Q) from |g(|q) in (|a,np|g). M1 is suggested from RUL, however E2 component is required from Coulomb excitation. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 94.0 {I5} from (|a,np|g) and 94.3 {I3} from (p,n) 
M$D(+Q) with |d=+0.08 {I+28-8} from |g(|q) in (|a,np|g), D from RUL; magnetic character from |D|p=no 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 320.6 {I8} from (|a,p|g) and 320.2 {I3} from (p,n). Other: 320 {I3} from Coulomb excitation 
RI$other: 7.7 {I19} in (|a,np|g) discrepant. 
M$D,E2 from comparison to RUL; E2 component from Coulomb excitation. |DJ,|D|p=2,no from the decay scheme. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 909.9 {I5} from (|a,np|g) and 909 {I1} from (p,n|g) 
M,MR$D+Q from |g(|q) in (|a,np|g) and M2 ruled out by RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 684.0 {I5} from (|a,np|g) and 683.8 {I3} from (p,n|g) 
M$D+Q from |g(|q) in (|a,pn|g) and M1(+E2) from |g(|q) and linear polarization in (p,n|g) 
MR$from (|a,pn|g). Other: +0.01 {I9} from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M$from |g(|q,pol) in (p,n|g) with |d=+0.01 {I16} or -7.1 {I+20-40} (1974Ri13); -1.37 to -0.32 (1974To10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$1481, 1509 |g rays placed with 2816 state in ({+3}He,p|g) and 1493, 1499 |gs placed with 1725 and 1811 states, respectively, in (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$1481, 1509 |gs placed from 2816 state in ({+3}He,p|g) and 1493, 1499 |gs placed from 1725 and 1811 states, respectively, in (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 516.0 {I4} (1974Ri13) and 517 {I1} (1975Gu22) 
RI$other: 49 (1974Ri13) 
MR$|d(3+)=+5.7 excluded by comparison to RUL (1974Ri13). 
$POL=-0.49 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 684.0 {I3} (1974Ri13), 684.4 {I5} (1974Ri02), 683.4 {I3} (1975Gu22) 
MR$others: -0.44 to +0.17 or -11.2 to -1.7 (1974To10) 
$POL=-0.12 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 912.9 {I3} (1974Ri13), 912.7 {I5} (1974Ri02), 912 {I1} (1975Gu22) 
RI$unweighted average of 72 {I6} (1974To10) and 69 {I5} (1975Gu22). Other: 61 (1974Ri13) 
$POL=+0.34 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E$unweighted average of 946 {I1} (1974Ri13) and 943 {I1} (1975Gu22) 
M,MR$from |g(|q) (1974To10). 
RI$unweighted average of 28 {I4} (1974To10) and 31 {I5} (1975Gu22). Other: 39 (1974Ri13) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 943.1 {I4} (1974Ri13), 943.4 {I5} (1974Ri02), and 945 {I1} (1975Gu22) 
$POL=-0.02 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
$POL=-0.47 {I6} 
E$weighted average of 1013.5 {I3} (1974Ri13), 1013.1 {I5} (1974Ri02), and 1013 {I2} (1975Gu22) 
RI$88 {I5} in 1974To10 seems too high as compared to 58 in 1975Gu22 and 67 in 1974Ri02 
MR$other: +0.08 {I3} (1974To10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1046.3 {I5} (1974Ri13), 1044.9 {I5} (1974Ri02), and 1045 {I1} (1975Gu22) 
RI$other: 23 (1974Ri13, 1974Ri02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1082.1 {I5} (1974Ri13), 1080 {I1} (1974Ri02), and 1081 {I1} (1975Gu22) 
RI$others: 10 (1974Ri13, 1974Ri02), 12 {I3} (1974To10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1106.9 {I3} (1974Ri13), 1106.2 {I5} (1974Ri02), and 1106 {I1} (1975Gu22) 
MR$from |g(|q) (1974To10). 
$POL=-0.02 {I4} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$POL=+0.36 {I9} 
E$weighted average of 1130.1 {I3} (1974Ri13), 1129.6 {I5} (1974Ri02), and 1128 {I1} (1975Gu22) 
RI$unweighted average of 82 {I2} (1974Ri13), 83 {I5} (1974To10), and 85 {I5} (1975Gu22). Other: 84 (1974Ri02) 
MR$other: -0.12 to +0.05 or +1.2 {I2} (1974To10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 1162.9 {I3} (1974Ri13), 1162.2 {I5} (1974Ri02), and 1161 {I1} (1975Gu22) 
RI$unweighted average of 18 {I3} (1974Ri13), 17 {I3} (1974To10), and 14 {I5} (1975Gu22) 
MR$-0.017 to +0.36 or |<-1.7 (1974To10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E$weighted average of 1173.1 {I3} (1974Ri13), 1173.6 {I5} (1974Ri02), and 1173 {I1} (1975Gu22) 
RI$average of 49 {I2} (1974Ri13), 55 {I3} (1974To10), and 43 {I6} (1975Gu22). Other: 50 (1974Ri02) 
MR$other: -0.36 to +2.2 (1974To10) 
$POL=+0.59 {I10} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$weighted average of 1206.5 {I3} (1974Ri13), 1206.6 {I5} (1974Ri02), and 1205 {I1} (1975Gu22) 
RI$average of 51 {I2} (1974Ri13), 45 {I3} (1974To10), and 57 {I6} (1975Gu22). Other: 50 (1974Ri02) 
MR$+0.01 {I16} or -7.1 {I+20-40} (1974Ri13); -1.37 to -0.32 (1974To10) 
$POL=-0.36 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 277 {I1} (1974Ri13), 275 {I1} (1974Ri02), and 275.0 {I5} (1975Gu22) 
RI$other: 11 (1974Ri02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 375.7 {I4} (1974Ri13), 375.1 {I5} (1974Ri02), and 375.7 {I5} (1975Gu22) 
RI$other: 54 (1974Ri13, 1974Ri02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1289 {I1} (1974Ri13), 1288.7 {I5} (1974Ri02), and 1288 {I1} (1975Gu22) 
RI$other: 15 (1974Ri13, 1974Ri02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1321.7 {I3} (1974Ri13), 1322.0 {I5} (1974Ri02), and 1320 {I1} (1975Gu22) 
RI$other: 20 (1974Ri13, 1974Ri02) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$B(M1)=0.87 {I+41-22}, B(E2)=0.037 {I+64-34} (2024Be12) 
$B(M1)=0.88 {I+42-22}, B(E2)=0.038 {I+66-35} (compiler) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$from weighted av of +0.43 {I3} in {+51}V(|g,|g), +0.52 {I7} from pulsed beam in Coul. ex., and 0.49 {I3} from B(E2)=0.0132 {I14} in Coul. ex. and adopted T{-1/2}=184 ps {I6}. Other: 0.3 {I+6-3} from (|a,p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$From {+51}Ti |b{+-} decay 
MR$From weighted average value. Weighted av. is +6.8 {I8} or -0.16 {I2} based on +6.5 {I7} or -0.14 {I2} (1969Ha46); -0.18 {I2} or +9 {I2} (1963Ro15), assuming |d(320|g)=+0.45 {I3} in {+51}Ti |b{+-} decay. Other: <-4.7 in {+51}V(p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$From {+51}Ti |b{+-} decay 
M,MR$mult=E2(+M3) and |d(M3,E2)=-0.03 {I9} in {+48}Ti(|a,p|g); |d<4|*10{+-4} from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI$from weighted av of 31 {I6} (n,|g) and 33.3 {I20} (|a,p|g). 
M,MR$mult=E2(+M3) and |d(M3,E2)=-0.05 {I18} in {+48}Ti(|a,p|g). From RUL=1 one expects |d<0.001 (evaluator). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI$from (p,|g). 
MR$|d>3.3 or |d=+0.36 {I15} in {+48}Ti(|a,p|g); small value favored; B(E2)(W.u.)>44 if |d>3.3. 


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$from weighted av of 31 {I5} in (p,p'|g), 28 {I3} in (p,|g), and 23 {I4} in (|a,p|g). 
MR$|d(M3,E2)=0.0 {I+4-8} in {+48}Ti(|a,p|g); |d<9|*10{+-4} if upper limit of RUL is 1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$2334|g is assigned by 1980Ka40 in (n,n'|g) to the 3264 level only (it is not reported by 1970PoZZ or 1982Ab06). Based on (n,|g), at least part of this transition should be placed with 3943 level. 
RI$I|g(2338|g)/I|g(2946|g)=0.69 {I+28-21} in (p,p'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$might include a contribution from the 3386 level seen in (n,n'|g) and (n,|g), which decays mainly to the 1609 level. If so, then the branching given for the 1775|g would be too large. The (p,p'|g) work would not be able to resolve two closely spaced 3383 levels. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from weighted av of (p,p'|g) and (n,|g). 
E$1782.2|g entirely to the 3396 level by 1970PoZZ in (n,n'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
$B(E2)(W.u.)=10 {I3} 
E$the 3133|g is unassigned in (n,|g) E=thermal, and the 3453|g is placed from the 6830 level. The energies and branching are reasonably consistent with the values of 1980Ka40 in (n,n'|g) so it is possible that the 3454 level is being populated in (n,|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$from (p,|g). The value (I(3256|g)/I(3577|g)=1.5) from (n,n'|g) may be a misprint. In (p,p'|g) only the 3576|g is reported. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$the 2696|g is reported only in (p,|g) and the 3626|g is only in (n,n'|g) by 1970PoZZ. There is an unlabelled peak at 2696 in the spectrum of 1970PoZZ. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.09 {I1} or +5.9 {I5} in {+50}Ti(p,|g) 
$B(M1)(W.u.)=0.047 {I9}, B(E2)(W.u.)=0.043 {I13} if |d=-0.09 {I1}; B(M1)(W.u.)=0.0013 {I4}, B(E2)(W.u.)=5.2 {I10} if |d=+5.9 {I5} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.01 {I3} or -5.0 {I10} in {+50}Ti(p,|g) 
$B(M1)(W.u.)=0.021 {I4}, B(E2)(W.u.)=0.0002 {I+14-2} if |d=+0.01 {I3}; B(M1)(W.u.)=0.0008 {I4}, B(E2)(W.u.)=2.1 {I4} if |d=-5.0 {I10} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: M1+E2
decay_comment:
MR$+0.26 {I10} or >15 in {+50}Ti(p,|g) 
$B(M1)(W.u.)=0.022 {I5}, B(E2)(W.u.)=0.13 {I10} if |d=+2.6 {I10}; B(M1)(W.u.)<0.00012, B(E2)(W.u.)>1.6 if |d>15 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$+0.00 {I2} or -4.7 {I4} in {+50}Ti(p,|g) 
$B(M1)(W.u.)=0.0098 {I19} if |d=+0.00 {I2}; B(M1)(W.u.)=0.00042 {I11}, B(E2)(W.u.)=0.54 {I10} if |d=-4.7 {I4} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E1(+M2)
decay_comment:
MR$+0.014 {I17} or -1.79 {I8} from {+50}Ti(p,|g) 
$B(E1)(W.u.)=0.00019 {I4}, B(M2)(W.u.)=0004 {I+9-4} if |d=+0.014 {I17} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.25 {I3} or >23 in {+50}Ti(p,|g) 
$B(M1)(W.u.)=0.0034 {I7}, B(E2)(W.u.)=0.010 {I3} if |d=-0.25 {I3}; B(M1)(W.u.)<8.1|*10{+-6}, B(E2)(W.u.)>0.14 if |d>23 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.077 {I6} or +5.5 {I2} in {+50}Ti(p,|g) 
$B(M1)(W.u.)=0.00049 {I10}, B(E2)(W.u.)=0.47 {I9} if |d=+5.5 {I2}; B(M1)(W.u.)=0.015 {I3}, B(E2)(W.u.)=0.0029 {I7} if |d=-0.077 {I6} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR$-0.080 {I4} or -3.32 {I5} in {+50}Ti(p,|g) 
$B(M1)(W.u.)=0.028 {I6}, B(E2)(W.u.)=0.0050 {I11} if |d=-0.080 {I4}; B(M1)(W.u.)=0.0024 {I5}, B(E2)(W.u.)=0.72 {I14} if |d=-3.32 {I5} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$may be misplaced. 3611 level deduced by 7996|g transition from this level is different from that seen in other reactions. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$|g(|q): A{-2}=0.075 {I24}, A{-4}=-0.029 {I28} (1969Ha46); A{-2}=0.013 {I30}, A{-4}=-0.03 {I5} (1963Ro15) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
CC$other: |a(K)exp=0.00153 {I3}, |a(exp)=0.00169 {I5} (1984HaZS). See also 1973Wi10, 1970Ri11, 1970Ca17, 1969Dr01, 1968Ri17, and 1969WiZW. 
E$others: 320.082 {I6} (1975Bo07, original value was 320.0761 {I55} relative to E|g=411.794 for the Au standard) 
RI$from weighted average of 9.8 {I6} (1955Bu01), 9.72 {I15} (1963MeZZ), 10.20 {I63} (1965Dh01), 9.75 {I20} (average of 2 values, 1965Le24), 10.2 {I10} (1970Ri11), 9.85 {I9} (1980Sc07), 10.30 {I19} (1984Fi10), 9.86 {I8} (1991Ba11), 9.96 {I9} (1994Ko34), 9.91 {I1} (2005Ya01), 9.87 {I3} (2010Mo01). Others: |? 2 (1940Wa02), 3 (1945Br02), 8 (1952Ly17), 21 (1952Ma49), 9.8 (1955Bi29), 9 {I1} (omitted as outlier, 1955Co56), 10.1 {I3} (1980Sc07). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI I|g might include a contribution from the 3386 level seen in (n,n'|g) and (n,|g), which decays mainly to the 1609 level. If so, the branching given for the 1775|g would be too large. The (p,p'|g) work would not be able to resolve two closely spaced 3383 levels. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR from |g(|q) (1962Ri09). From B(E2)(320 level)=0.0132 and adopted T{-1/2}=184 ps {I6} one gets |d=0.49 {I3}. 


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:
$ce(K)=5.4 {I23}; ce(L)=0.51 {I22}; ce(M)=0.06 {I3}; ce(N)=0.0029 {I14} 
$|a(exp)=4.6 {I18} (1972Bo59) 
MR,M Mult from |a(K)exp in (n,|g). |d=0.066 {I+34-66} from |a(exp) in (n,|g). From RUL one expects |d<0.0064 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_comment:
M from 1998Gr14 based on the comparison of the half-life of the isomer with Weisskopf estimates for given transition energy. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 349.3 {I6} in {+55}Ti |b{+-} decay and 347.9 {I3} in {+9}Be({+48}Ca,pn|g) 
RI$from {+55}Ti |b{+-} decay. Other: 12 {I9} in {+9}Be({+48}Ca,pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D,Q)
decay_comment:
$R{-ang}=1.2 {I1} 
M$|g(|q) suggests |DJ=1, dipole, |DJ=2, quadrupole also possible from |DJ|p assigned by 2011De20 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: S
decay_comment:
E$ existence of transition deduced from observed coincidence between the 113 and 175 |g rays. Such a transition is below the detection threshold. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$ A 114 {I2} |g seen in {+58}Ti decay is either a member of |g-cascade from high-lying excited state in {+58}V or corresponds to direct decay of a 114 level to the g.s. Since no other transition was observed, the latter possibility seems more likely. Other: 116 {I2} (2002MaZN) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$ this |g is either a member of |g-cascade from high-lying excited state in {+58}V or corresponds to direct decay of a 114 level to the g.s. Since no other transition was observed, the latter possibility seems more likely. Other: 116 {I2} (2002MaZN) 
RI$80% {I10} of {+58}Ti |b- decay occurs through the 114 transition. This value is an upper limit for direct feeding of a possible 114 level in {+58}V and gives I|b{+-}(g.s.)|<20% {I10} giving log {Ift}>4.5, consistent with J{+|p}({+58}V g.s.)|=0 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 81.0 {I7} from ({+76}Ge,X|g) (2014Su11) and 82.0 {I3} from ({+238}U,F|g) (2021Wi05) 
M$E2 multipolarity is assigned by 2021Wi05, based on Weisskopf estimates for transition probabilities of various multipolarities. Authors mention that M1 admixture is not ruled out. But it is not clear how E1 or E1 with small M2 admixture is ruled out 


decay_energy_unit: KEV
decay_comment:
E$observed as a delayed transition within a 10-|ms time window; the |g rays were detected at least 300 ns after the ion implantation. 
$It is assumed that 81-keV transition feeds the ground state, there does not seem any experimental evidence provided by 2014Su11 


decay_energy_unit: KEV
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$E2 multipolarity is assigned by 2021Wi05, based on Weisskopf estimates for transition probabilities of various multipolarities. Authors mention that M1 admixture is not ruled out. But it is not clear how E1 or E1 with small M2 admixture is ruled out 


decay_energy_unit: KEV
decay_multipolarity: (M2)
decay_BM_unit: mu^2 x (fm)^2
decay_BM_info: ;TYPE=BM2;ERR=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LT
decay_comment:
$ For a 3/2+ state at 12.4 keV in mirror nucleus {+45}Sc, B(M2)(W.u.)=0.042 {+10-6}. If 3/2- is assigned to 107-keV level, then B(E2)(W.u.)<0.05 compared to B(E2)(W.u.)=15 {I1} for a 377, 3/2- level in {+45}Sc 


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 752.1 {I2} from {+48}Mn |b{++} decay, 752.2 {I2} from {+49}Fe |b{++}p decay, 752.0 {I2} from ({+10}B,pn|g), 752.2 {I3} from ({+28}Si,2|a|g), 752.3 {I2} from ({+16}O,2n|g), 752.13 {I13} from ({+14}N,np|g), and 752.4 {I5} from ({+3}He,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1106.1 {I2} from {+48}Mn |b{++} decay, 1105.2 {I6} from {+49}Fe |b{++}p decay, 1106.3 {I2} from ({+10}B,pn|g), 1106.4 {I3} from ({+28}Si,2|a|g), 1106.5 {I2} from ({+16}O,2n|g), 1106.4 {I3} from ({+14}N,np|g), and 1106.4 {I5} from ({+3}He,n|g) 
M$Q from |g(|q) data, M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$others: 1586.4 {I6} in ({+10}B,pn|g); 1589.2 {I10} from ({+14}N,np|g) (1979Ek03) is discrepant, which is a quite broad peak as mentioned in 1979Ek03. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M2]
decay_uncertain: ?
decay_comment:
E$from ({+40}Ca,pn|g) (1994Ca04) 
RI$from I(87|g)/I(1675|g)=0.6/6 in ({+40}Ca,pn|g) (1994Ca04) 
$B(M2)(W.u.)=9.2|*10{+3} {I+38-31} exceeds RUL=1. 


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=LT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM2W;ERR=LT
decay_comment:
E$weighted average of 1675.0 {I4} from {+48}Mn |b{++} decay, 1675.3 {I4} from ({+10}B,pn|g), 1674.9 {I6} from ({+16}O,2n|g), 1675.3 {I3} from ({+14}N,np|g), and 1675.3 {I10} from ({+3}He,n|g) 
RI$from {+48}Mn |b{++} decay. Other: 100 {I20} from ({+10}B,pn|g) 
M,MR$D(+Q) from |g|g(|q) in ({+3}He,n|g); |D|p=(yes) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 530.8 {I3} from ({+10}B,pn|g), 531.0 {I3} from ({+28}Si,2|a|g), 530.6 {I2} from ({+16}O,2n|g), and 530.77 {I17} from ({+14}N,np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from ({+14}N,np|g). Others: 531.0 {I5} from {+48}Mn |b{++} decay, 530.8 {I3} from ({+10}B,pn|g), 531.0 {I3} from ({+28}Si,2|a|g), and 530.6 {I2} from ({+16}O,2n|g) 
M,MR$D+Q from |g(|q) in ({+10}B,pn|g), with |d(Q/D) deduced by the evaluator from 5.5% {I15-10} E2 component in 1979Ha45; M2 ruled out by RUL. Others: |d(Q/D)=-0.36 {I+28-61} from |g(|q) in ({+16}O,2n|g) (1975Ha04), +0.01 {I5} or >7 from |g|g(|q) in ({+3}He,n|g) (2003Je06), >20 for J|p=6- from |g(|q) in ({+14}N,np|g) (1979Ek03) 


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$weighted average of 1742.5 {I10} from ({+10}B,pn|g), 1743.4 {I3} from ({+28}Si,2|a|g), and 1744.0 {I5} from ({+14}N,np|g) 
M$from |g(|q,pol) in ({+14}N,np|g) (1979Ek03), and |g anisotropy (|DJ=0 or 2) in ({+40}Ca,pn|g) (1994Ca04) 


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$weighted average of 1876 {I2} from ({+10}B,pn|g), 1875.4 {I3} from ({+28}Si,2|a|g), and 1878.2 {I12} from ({+14}N,np|g) 
M$stretched (|DJ=2) quadrupole or |DJ=0 dipole from angular anisotropy in ({+40}Ca,pn|g) (1994Ca04); |DJ=0 ruled out by |g excitation function from level scheme; M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M$stretched (|DJ=2) quadrupole or |DJ=0 dipole from angular anisotropy in ({+40}Ca,pn|g) (1994Ca04); |DJ=0 ruled out by |g|g(DCO) in ({+28}Si,2|a|g) (1996Ca38); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$weighted average of 752.0 {I2} (1979Ha45) and 752.4 {I5} (1973Ku10). other: 752 (1994Ca04) 
$A{-2}=+0.27 {I4}, A{-4}=-0.06 {I5} (1973Ku10) 
$A{-2}=+0.19 {I6}, A{-4}=-0.04 {I6} (1979Ha45) 
$anisotropy=1.21 {I7} (1994Ca04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E$from 1979Ha45. Others: 1106.3 {I5} (1973Ku10), 1106 (1994Ca04) 
RI$weighted average of 61 {I10} (1979Ha45) and 71 {I12} (1973Ku10). Other: 97 (1994Ca04) 
$A{-2}=+0.32 {I12}, A{-4}=-0.05 {I13} (1973Ku10) 
$A{-2}=+0.25 {I6}, A{-4}=-0.03 {I4} (1979Ha45) 
$anisotropy=1.3 {I1} (1994Ca04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E,RI$1979Ha45. Other: 1586, I|g=97 (1994Ca04). It could be a doublet with the transition deexciting the 5648 level seen in 1998Br34 
$A{-2}>0 (1979Ha45) 
$anisotropy=1.4 {I1} (1994Ca04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1675.4 {I3} (1979Ha45) and 1674.0 {I10} (1973Ku10). Other: 1673 (1994Ca04) 
RI$weighted average of 24 {I5} (1979Ha45) and 31 {I11} (1973Ku10). Other: 6 (1994Ca04). 
$A{-2}=+0.10 {I16}, A{-4}=+0.04 {I19} (1973Ku10) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 530.7 {I2} (1979Ha45) and 531.6 {I5} (1973Ku10). Other: 531 (1994Ca04) 
RI$weighted average of 18 {I4} (1979Ha45) and 14 {I3} (1973Ku10). Other: 5 (1994Ca04). 
MR$deduced from 5.5% {I15-10} E2 component from |g(|q), as given in 1979Ha45 
$A{-2}=+0.05 {I10}, A{-4}=-0.01 {I100} (1973Ku10) 
$A{-2}=+0.09 {I4}, A{-4}=+0.02 {I4} (1979Ha45) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: S
decay_comment:
E,RI$from 1973Ku10 only; not observed. A 2205|g is placed from the 4064,J=3 level by 2003Je06 in ({+3}He,n|g), different from this 5(-) level, which is also proposed in 2003Je06 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$from 1994Ca04 only. This transition is not seen in any other study and is considered questionable by the evaluator. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E,RI$from 1979Ha45. Other: 1744 with I|g=65, placed from a 7062 level in 1994Ca04 
M$D,Q from anisotropy=1.4 {I2} (1994Ca04); Q favored by level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
E,RI$from 1979Ha45. Other: 1874 with I|g=80, placed from a 5318 level in 1994Ca04 
M$D,Q from anisotropy=1.4 {I2} (1994Ca04); Q favored by level scheme 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$placement from Adopted Gammas. It is placed from a 10431, (13+) to the 8409 level by 1994Ca04 
RI$from 1994Ca04 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E,RI$from 1994Ca04; placement from Adopted Gammas. It is placed from a 10610, (14+) to the 8409 level by 1994Ca04 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
MR$|d(M2/E1)>6 from 1979Ek03 for J|p=5- 
$A{-2}=+0.006 {I15}, A{-4}=+0.072 {I16}, POL=-0.03 {I9} (1979Ek03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
MR$|d(E2/M1)>20 from 1979Ek03 for J|p=6- 
$A{-2}=-0.017 {I12}, A{-4}=+0.120 {I14}, POL=+0.10 {I14} (1979Ek03) 


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 D,Q from recoil-|g(|q) in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),...; Ne M2 from comparison to RUL. |DJ|p=2,no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M from |g(|q) and |g|g(|q). |D|p=no from level scheme 
MR >+0.070 from |g(|q) and |g|g(|q) in (|a,n|g); <0.106 {I18} from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1(+M2))
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_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 av (int.) of 2431.5 {I6} from (|a,n|g) and 2431 {I1} from {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),... 
M,MR from |g(|q) in (|a,n|g). |d<0.30 {I6} from comparison to RUL. |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M,MR Q+O, -0.13 {I11}, from |g|g(|q) and |g(linear pol) in (|a,n|g). Ne M2, |d(E2+M3)<0.00088 {I14} from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M |DJ=0 d or |DJ=2 Q |g from AD in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),... Ne M2 from comparison to RUL. |DJ|p=2,no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
RI weighted av (int.) from {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C, n2p|g),... and (|a,n|g) 
M |DJ=0 d or |DJ=2 Q |g from AD in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),... Ne M2 from comparison to 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=LT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W;ERR=LT
decay_comment:
M |DJ=0 d or |DJ=2 Q |g from AD in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),... E1 consistent with AD ratios for 364 and 702 |g's in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),... (1999Br40). 


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 J|)J D or J|)J-2 Q |g from AD and DCO in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),..; large Q component from |g(|q) in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),.. Ne M2 from comparison to 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:
M |DJ=0 d or |DJ=2 Q |g from AD in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),... Ne M2 from comparison to RUL. |D|p=yes from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M,MR D+Q from AD in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g), \... Ne E1+M2 from |d and comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M |DJ=2 Q from AD in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C, \n2p|g),...; Ne M2 from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M |DJ=2 Q transition from AD in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),... Ne M2 from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M D,E2 from comparison to RUL. Recoil-|g(|q) in {+12}C({+40}Ca,n2p|g),{+40}Ca({+12}C,n2p|g),... Consistent with pure Q 


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 |DJ=1 from AD and DCO in {+12}C({+40}Ca,n2p|g), {+40}Ca({+12}C,n2p|g),... M1 from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted av (int.) of 271.9 keV {I6} (1978Me19), 272 keV {I1} (1990Ca06), 272 keV {I1} (1998Ca26), and 271.8 keV {I4} (2001Br32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted av (int.) of 812.3 keV {I6} (1978Me19), 812 keV {I1} (1990Ca06), 812 keV {I1} (1998Ca26), and 812.6 keV {I4} (2001Br32) 
RI mean of 53 (1991Ca23) and 56 (2001Br32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted av (int.) of 478.2 {I6} keV (1978Me19), 479 {I1} keV (1990Ca06), 479 {I1} (1998Ca26), and 478.4 {I4} (2001Br32) 
RI mean of 39 (1991Ca23) and 46 (2001Br32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted av (int.) of 1290.8 {I6} keV (1978Me19), 1291 keV {I1} (1990Ca06), 1291 keV {I1} (1998Ca26), and 1290.8 keV {I4} (2001Br32) 
RI mean of 49 (1991Ca23) and 39 (2001Br32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted av (int.) of 937 keV {I1} (1990Ca06), 938 keV {I1} (1998Ca26), and 938.3 keV {I4} (2001Br32) 
RI mean of 43 (1991Ca23) and 53 (2001Br32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
E$weighted av (int.) of 690.6 keV {I6} (1978Me19), 691 keV {I1} (1990Ca06), 690 keV {I1} (1998Ca26), and 690.1 keV {I4} (2001Br32) 
RI mean of 40 (1991Ca23) and 45.5 (2001Br32) 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
RI 78% {I3} (1999Br40) 
M D from comparison to RUL; |=E1 since B(E1)(W.u.)=2|*10{+-3} is about 10 times faster than any other E1 in this nuclear region (1999Br40). 


decay_energy_unit: KEV
decay_multipolarity: D
decay_comment:
RI 4.0% {I5} (1999Br40) 
M J|)J-1 |g from AD (1998Ca26, 1999Br40) 
[I|g(35|')+I|g(145|')]/2I|g(90|')=0.83 {I5} (1999Br40) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
RI mean of 1.6 (1991Ca23) and 1.9 (1998Ca26) 
M |DJ=0 D or |DJ=2 Q |g from AD (1999Br40). |=Q from comparison to RUL (evaluator). E1 consistent with AD ratios for 364 and 702 |g's (1999Br40). Large Q admixture from recoil-|g(|q) (1991Ca23) discrepant 
[I|g(35|')+I|g(145|')]/2I|g(90|')=1.28 {I9} (1999Br40) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted av (ext.) of 704 keV {I1} (1991Ca23), 701.9 keV {I4} (1999Br40), and 702 keV {I1} (2001Br32) 
M stretched (|DJ=1) D |g (1991Ca23, 1998Ca26, 1999Br40). 
[I|g(35|')+I|g(145|')]/2I|g(90|')=0.90 {I7} (1999Br40) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted av (ext.) of 2332 keV {I1} (1991Ca23), 2330.0 keV {I4} (1999Br40), and 2330 keV {I2} (2001Br32) 
RI mean of 10 (1991Ca23) and 13 (1998Ca26) 
M stretched (|DJ=1) D |g (1991Ca23); J|)J-1 |g from AD (1998Ca26, 1999Br40)). 
[I|g(35|')+I|g(145|')]/2I|g(90|')=0.79 {I7} (1999Br40) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI mean of 8 (1991Ca23) and 10.5 (2001Br32) 
M stretched (|DJ=1) D |g (1991Ca23); J|)J-1 |g from AD and DCO (1998Ca26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
RI mean of 3 (1991Ca23) and 4.1 (2001Br32) 
M stretched (|DJ=2) Q or |DJ=0 D |g (1991Ca23); J|)J D or J|)J-2 Q |g from AD (1998Ca26). |=M2 from comparison to RUL (evaluator) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI mean of 3 (1991Ca23) and 7.5 (2001Br32) 
M stretched (|DJ=1) D |g (1991Ca23); J|)J-1 |g from AD and DCO (1998Ca26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI mean of 52 (1991Ca23) and 55.5 (2001Br32) 
M |DJ=2 Q or |DJ=0 D |g (1991Ca23); J|)J D or J|)J-2 Q |g from AD and DCO (1998Ca26); large Q component (1973BlZW). |=M2 from comparison to RUL (evaluator) 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
RI 79% {I4} (1999Br40) 
M,MR from AD (1999Br40) 
[I|g(35|')+I|g(145|')]/2I|g(90|')=0.60 {I6} (1999Br40) 


decay_energy_unit: KEV
decay_multipolarity: M1+E2
decay_comment:
RI 72% {I3} (1999Br40) 
M,MR D+Q from AD (1999Br40). |=E1+M2 from |d and comparison to RUL (evaluator) 
[I|g(35|')+I|g(145|')]/2I|g(90|')=0.45 {I5} (1999Br40) 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
RI 28% {I3} (1999Br40) 
M |DJ=0 D or |DJ=2 Q from AD (1999Br40); pure Q (1998Ca26). |=M2 from comparison to RUL (evaluator) 
[I|g(35|')+I|g(145|')]/2I|g(90|')=1.30 {I11} (1999Br40) 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
RI 65% {I5} (1999Br40) 
M |DJ=0 D or |DJ=2 Q transition from AD (1999Br40); pure Q (1998Ca26). |=M2 from comparison to RUL (evaluator) 
[I|g(35|')+I|g(145|')]/2I|g(90|')=1.25 {I14} (1999Br40) 


decay_energy_unit: KEV
decay_multipolarity: E2
decay_comment:
RI 80% {I6} (1999Br40) 
M D,E2 from comparison to RUL (evaluator). Recoil-|g(|q) consistent with pure Q 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted av (int.) of 20045 keV {I1} (1991Ca23), 2044 keV {I2} (1999Br40), and 2043.8 {I10} (2001Br32) 
RI$mean of 21 (1991Ca23), 56 (1999Br40), and 26 (2001Br32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$mean of 3.2 (1998Ca26) and 1.7 (2001Br32) 
M |DJ=1 from AD and DCO (1998Ca26). M1 from comparison to RUL (evaluator) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted av (ext.) of 2216 keV {I1} (1991Ca23) and 2214.2 keV {I10} (2001Br32) 
RI$mean of 4 (1991Ca23) and 3.3 (2001Br32) 
M stretched (|DJ=1) D |g (1991Ca23); J|)J-1 |g from AD (1998Ca26) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$unweighted av of 478 keV {I1} (1991Ca23), 481 keV {I1} (1998Ca26), and 476.3 keV {I4} (2001Br32) 
M stretched (|DJ=1) D |g (1991Ca23); J|)J-1 |g from AD (1998Ca26). M1 from comparison to RUL (evaluator) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
E$weighted av (ext.) of 2216 keV {I1} (1991Ca23), 2213 keV {I2} (1998Ca26), and 2691.1 keV {I10} (2001Br32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M from |g(|q), |g|g(|q), and |g(linear pol) 
MR 0.00 {I4} (1973Sa12). <3.5|*10{+-4} {I6} from comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M Q(+O) from |g(|q) and |g|g(|q). Comparison to RUL excludes M2 
MR +0.02 {I16}. <1.2|*10{+-3} {I4} from comparison to RUL 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR |d's from 1971Bl09 are based on |d(1300|g)=+0.11 which is inconsistent with RUL(M3) using adopted T{-1/2} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
These three transitions account for most of the decay of the 5.57-MeV state, but the decay is complex and a complete decay scheme could not be constructed 


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$weighted average of 783.3 {I1} from {+50}Mn |e decay (1.75 min), 783.6 {I3} from ({+32}S,|a2p|g), 783.3 {I3} from ({+28}Si,|a2p|g), 783.3 {I5} from (|g,|g'), 783.4 {I2} from (p,p'|g), and 783.3 {I2} from (|a,|a'|g). Others: 778 {I2} from (p,n|g) and 783 {I1} from (n,n'|g) 
M$from |g(|q,pol) in ({+16}O,|a2p|g), |g|g(DCO) in ({+32}S,|a2p|g), and RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1098.0 {I2} from {+50}Mn |e decay (1.75 min), 1097.9 {I3} from ({+32}S,|a2p|g), 1098.2 {I3} from ({+28}Si,|a2p|g), 1097.9 {I5} from ({+16}O,|a2p|g), 1098.2 {I3} from (p,p'|g), and 1098.1 {I2} from (|a,|a'|g). Other: 1107 {I3} from (p,n|g) 
M$from |g(|q,pol) in ({+16}O,|a2p|g), |g|g(DCO) in ({+32}S,|a2p|g), and RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$others: 2138 {I1} from (n,n'|g), 2140 {I5} from (p,n|g) 
M$D(+Q) from |g(|q) in (p,p'|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1282.4 {I3} from {+50}Mn |e decay (1.75 min), 1282.3 {I3} from ({+32}S,|a2p|g), 1282.1 {I3} from ({+28}Si,|a2p|g), 1282.6 {I5} from ({+16}O,|a2p|g), 1282.7 {I7} from (p,p'|g), and 1282.7 {I2} from (|a,|a'|g) 
M$from |g(|q,pol) in ({+16}O,|a2p|g), |g|g(DCO) in ({+32}S,|a2p|g), and RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 1443.3 {I2} from {+50}Mn |e decay (1.75 min), 1443.3 {I3} from ({+28}Si,|a2p|g), 1443.1 {I5} from ({+16}O,|a2p|g), and 1442.7 {I7} from (p,p'|g) 
M$D(+Q) from |g(|q) in (p,p'|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1]
decay_comment:
E$weighted average of 2845.0 {I5} from (|g,|g') and 2846.1 {I6} from (p,p'|g) 
RI$from (|g,|g'). Others: 50 {I5} from {+50}Mn |e decay, 50 {I22} from (p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E$weighted average of 3628.0 {I5} from (|g,|g') and 3629.3 {I5} from (p,p'|g) 
M$from |g(|q) and polarization asymmetry in (|g,|g') 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E$weighted average of 467.9 {I5} from ({+16}O,|a2p|g) and 467.7 {I8} from (p,p'|g) 
RI$from (p,p'|g) (1968Mo07). Others: 100 {I16} from ({+16}O,|a2p|g), 100 {I11} from 1972Ra14 in (p,p'|g) 
M$from |g(|q) in (p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
E$weighted average of 1910.9 {I9} from ({+16}O,|a2p|g) and 1910.7 {I8} from (p,p'|g) 
RI$weighted average of 79 {I9} from (p,p'|g) (1968Mo07) and 79 {I16} from ({+16}O,|a2p|g). Other: 133 {I23} from 1972Ra14 in (p,p'|g) is in disagreement 
M,MR$D+Q from p|g(|q) in (p,p'|g); RUL forbids M2. But |g(|q) data in ({+28}Si,|a2p|g), suggesting pure dipole, is in disagreement with results from (p,p'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 661.5 {I3} from {+50}Mn |e decay (1.75 min), 661.5 {I3} from ({+28}Si,|a2p|g), 661.7 {I5} from ({+16}O,|a2p|g), and 661.9 {I6} from (|a,|a'|g). Other: 662 {I2} from (p,p'|g) 
RI$from {+50}Mn |b{++} decay (1.75 min). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1944.5 {I5} from {+50}Mn |e decay (1.75 min) and 1944.4 {I3} from ({+28}Si,|a2p|g) 
RI$from {+50}Mn |b{++} decay (1.75 min). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
M,MR$|d(J=1)=-0.09 {i29}, |d(J=2)=+0.34 {i13} from p|g(|q) in (p,p'|g) which suggests D(+Q), but |DJ|p requires E2 if the parent level is the same one as the 0+,3895 level in (p,t) 


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$weighted average of 1580.5 {I3} from ({+32}S,|a2p|g), 1580.9 {I3} from ({+28}Si,|a2p|g), 1581.1 {I5} from ({+16}O,|a2p|g), and 1581.2 {I5} from (|a,|a'|g) 
M$from |g(|q,pol) in ({+16}O,|a2p|g), |g|g(DCO) and |g|g(ADO) in ({+32}S,|a2p|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$weighted average of 1595.2 {I3} from ({+32}S,|a2p|g), 1595.9 {I3} from ({+28}Si,|a2p|g), 1595.7 {I5} from ({+16}O,|a2p|g), and 1596.5 {I5} from (|a,|a'|g) 
M$from |g(|q,pol) in ({+16}O,|a2p|g), |g|g(DCO) and |g|g(ADO) in ({+32}S,|a2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$unweighted average of 414.5 {I3} from ({+32}S,|a2p|g) and 413.6 {I3} from ({+28}Si,|a2p|g) 
RI$weighted average of 18 {I6} from ({+32}S,|a2p|g) and 15.2 {I14} from ({+28}Si,|a2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 2009.3 {I3} from ({+32}S,|a2p|g) and 2009.8 {I3} from ({+28}Si,|a2p|g) 
RI$from ({+28}Si,|a2p|g). Other: 100 {I12} from ({+32}S,|a2p|g) 
M$Q from |g|g(DCO) and |g|g(ADO) in ({+32}S,|a2p|g), |g|g(ADO) in ({+28}Si,|a2p|g); M2 ruled out by RUL 


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$weighted average of 196.3 {I3} from ({+32}S,|a2p|g) and 195.6 {I3} from ({+28}Si,|a2p|g) 
RI$weighted average of 3.4 {I11} from ({+32}S,|a2p|g) and 3.0 {I3} from ({+28}Si,|a2p|g) 
M$D from |g|g(DCO) and |g|g(ADO) in ({+32}S,|a2p|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 610.3 {I3} from ({+32}S,|a2p|g), 610.1 {I3} from ({+28}Si,|a2p|g), and 609.9 {I5} from ({+16}O,|a2p|g) 
RI$from ({+28}Si,|a2p|g). Others: 100 {I11} from ({+16}O,|a2p|g), 100 {I10} from ({+32}S,|a2p|g) 
M$from |g(|q,pol) in ({+16}O,|a2p|g), |g|g(DCO) and |g|g(ADO) in ({+32}S,|a2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 662.4 {I3} from ({+32}S,|a2p|g), 662.2 {I3} from ({+28}Si,|a2p|g), and 661.8 {I5} from ({+16}O,|a2p|g) 
RI$other: 100 {I10} from ({+32}S,|a2p|g) and ({+16}O,|a2p|g) 
M$from |g(|q,pol) in ({+16}O,|a2p|g), |g|g(DCO) and |g|g(ADO) from ({+32}S,|a2p|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$weighted average of 1272 {I1} from ({+32}S,|a2p|g) and 1272.2 {I3} from ({+28}Si,|a2p|g) 
RI$weighted average of 4.3 {I15} from ({+32}S,|a2p|g) and 2.8 {I3} from ({+28}Si,|a2p|g). Other: <4.9 from ({+16}O,|a2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$unweighted average of 2028.1 {I3} from ({+32}S,|a2p|g) and 2029.7 {I3} from ({+28}Si,|a2p|g) 
M$from |g|g(DCO) and |g|g(ADO) in ({+32}S,|a2p|g) and ({+28}Si,|a2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$weighted average of 273.3 {I3} from ({+32}S,|a2p|g) and 272.9 {I3} from ({+28}Si,|a2p|g) 
RI$other: 44 {I4} from {+24}Mg({+32}S,|a2p|g) is in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 2300.9 {I3} from ({+32}S,|a2p|g) and 2303.2 {I3} from ({+28}Si,|a2p|g) 
RI$also from ({+32}S,|a2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$unweighted average of 3303.3 {I3} from ({+32}S,|a2p|g) and 3306.3 {I3} from ({+28}Si,|a2p|g) 
RI$from ({+32}S,|a2p|g) 
M$from |g(DCO) in ({+32}S,|a2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 3577.1 {I10} from ({+32}S,|a2p|g) and 3580.3 {I10} from ({+28}Si,|a2p|g) 
M$Q from |g|g(ADO) in ({+28}Si,|a2p|g); M2 ruled out by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1815.5 {I3} from ({+32}S,|a2p|g) and 1816.2 {I3} from ({+28}Si,|a2p|g) 
RI$weighted average of 29 {I5} from ({+32}S,|a2p|g) and 33 {I7} from ({+28}Si,|a2p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$unweighted average of 5119.1 {I10} from ({+32}S,|a2p|g) and 5123.4 {I10} from ({+28}Si,|a2p|g) 
M$Q from |g|g(ADO) in ({+32}S,|a2p|g) and M2 ruled out by RUL 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$from 1994Ha43. A 3045|g was also assigned to {+50m}Mn |b{++} decay; from comparison of pure {+50m}Mn and mixed {+50}Mn and {+50m}Mn samples 1994Ha43 concluded that this is a doublet and up to 60% of the peak area in the mixed sample spectra may be attributed to a nonanalog decay branch in {+50}Mn. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E$(6)+ to 2+ transition is highly unlikely, |g not included in Adopted Levels, Gammas dataset. This |g may correspond to 3045|g assigned to {+50}Mn decay by 1994Ha43, and placed from a 3827,(0+) level 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
E$Rounded value from the Adopted Gammas. 
$Observation of this |g was claimed only by 1989Si07 in a complex |g-ray spectrum shown in their Fig. 2. This |g was not seen by 2019La09, 2011Do08 or 1984Al10. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 783.4 {I5} (1973De09) and 782.9 {I5} (1974Ku11) 
$A{-2}=+0.22 {I3}, A{-4}=-0.03 {I3}, pol=+0.35 {I5} (1974Ku11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1098.2 {I5} (1973De09) and 1097.5 {I5} (1974Ku11) 
RI$other: 81 {I4} (1973De09) 
$A{-2}=+0.25 {I4}, A{-4}=-0.05 {I4}, pol=+0.39 {I7} (1974Ku11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E$weighted average of 1283.1 {I5} (1973De09) and 1282.0 {I5} (1974Ku11) 
RI$other: 32 {I3} (1973De09) seems in disagreement 
$A{-2}=+0.30 {I5}, A{-4}=+0.05 {I7}, pol=+0.48 {I10} (1974Ku11) 


decay_energy_unit: KEV
decay_comment:
E$deduced by evaluators from averaged energy differences of E|g values for the decay of 3628, 4997, 7948 and 8528 levels 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$other: |G(2845|g)/|G=0.38 {I13} (1998En05) consistent with value from 2016Pa04, but much less precise 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
RI$other: |G{-0}/|G=0.90 {I8} (1970Mo26,1973MoYZ) consistent with 100% branch for 8884.8|g as in 2016Pa04 
$I|g(90|')/I|g(130|')=0.82 {I8}. POL=+0.68 {I13}. Also mult=dipole (1970Mo26,1973MoYZ,from |g(|q)) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
$A{-2}=+0.36 {I3}, A{-4}=-0.05 {I3}; A{-2}=+0.37 {I1}, A{-4}=-0.01 {I1} for 2142|g (1968Mo07) 
$A{-2}=+0.29 {I7}, A{-4}=+0.12 {I9}; A{-2}=+0.20 {I5}, A{-4}=-0.04 {I9} for 783|g (1968Mo07) 
$A{-2}=+0.06 {I2}, A{-4}=+0.05 {I3}; A{-2}'=+0.29 {I5}, A{-4}'=-0.20 {I4} for 2142|g (1972As01) 
E$unweighted average of 2141.1 {I3} (1972Ra14) and 2141.8 {I1} (1972As01) 
$%branching=97 {I1} (1968Mo07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=+0.13 {I7}, A{-4}=-0.06 {I8}; A{-2}=+0.09 {I4}, A{-4}=+0.05 {I6} for 2378|g (1968Mo07) 
$A{-2}=+0.34 {I4}, A{-4}=+0.29 {I6}; A{-2}=+0.14 {I10}, A{-4}=+0.08 {I15} for 783|g (1968Mo07) 
$A{-2}=+0.04 {I2}, A{-4}=+0.02 {I1}; A{-2}'=-0.58 {I10}, A{-4}'=+0.65 {I12} for 2378|g (1972As01) 
E$unweighted average of 2377.8 {I3} (1972Ra14) and 2378.8 {I4} (1972As01) 
$%branching=91 {I2} (1968Mo07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
$A{-2}=+0.42 {I8}, A{-4}=+0.07 {I9}; A{-2}=+0.37 {I5}, A{-4}=+0.09 {I6} for 1443|g (1968Mo07) 
$A{-2}=+0.37 {I11}, A{-4}=+0.11 {I15}; A{-2}=+0.24 {I8}, A{-4}=0 for 1098|g (1968Mo07) 
$A{-2}=+0.29 {I11}, A{-4}=-0.10 {I15}; A{-2}=+0.34 {I6}, A{-4}=0 for 783|g (1968Mo07) 
$A{-2}=(+0.1 {I14}), A{-4}=+0.3 {I4}; A{-2}'=-0.43 {I12}, A{-4}'=+0.09 {I7} for 1443|g (1972As01) 
E$unweighted average of 1443.3 {I2} (1972Ra14) and 1442.1 {I4} (1972As01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=(+1.6 {I13}), A{-4}=+0.4 {I3}; A{-2}'=-0.7 {I2}, A{-4}'=+0.02 {I3} for 2811|g (1972As01) 
E$weighted average of 2811.2 {I3} (1972Ra14) and 2812.1 {I8} (1972As01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=0.0 {I7}, A{-4}=0.0 {I1}; A{-2}'=0.0 {I6}, A{-4}'=0.0 {I3} for 1730|g (1972As01) 
E$weighted average of 1730.0 {I3} (1972Ra14) and 1729 {I1} (1972As01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 2846.3 {I8} (1972Ra14) and 2846.0 {I6} (1972As01) 
$%branching=20 {I10} (1968Mo07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$A{-2}=-0.48 {I7}, A{-4}=+0.08 {I8} for 3629|g (1968Mo07) 
$A{-2}=+0.04 {I6}, A{-4}=+0.02 {I1}; A{-2}'=+0.14 {I32}, A{-4}'=-0.10 {I16} for 3629|g (1972As01) 
E$from 1972As01. Other: 3629 {I2} (1972Ra14) 
$%branching=80 {I10} (1968Mo07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$A{-2}=-0.24 {I7}, A{-4}=+0.08 {I11} for 2915|g (1968Mo07) 
$A{-2}=+0.24 {I7}, A{-4}=+0.22 {I9} for 783|g (1968Mo07) 
$A{-2}=-0.01 {I6}, A{-4}=+0.05 {I1}; A{-2}'=+0.06 {I13}, A{-4}'=-0.07 {I7} for 2915|g (1972As01) 
E$weighted average of 2914.3 {I6} (1972Ra14) and 2915.1 {I5} (1972As01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$A{-2}=+0.50 {I8}, A{-4}=+0.03 {I9} for 1911|g (1968Mo07) 
$A{-2}=+0.24 {I11}, A{-4}=0 for 1443|g (1968Mo07) 
$A{-2}=+0.28 {I8}, A{-4}=-0.14 {I10} for 1098|g (1968Mo07) 
$A{-2}=+0.43 {I12}, A{-4}=0 for 783|g (1968Mo07) 
E$weighted average of 1911.1 {I8} (1972Ra14) and 1910 {I1} (1972As01) 
$%branching=44 {I5} (1968Mo07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=-0.2 {I2}, A{-4}=+0.01 {I7}; A{-2}'=(0.0), A{-4}'=(0.0) for 1963|g (1972As01) 
E$weighted average of 1962.9 {I4} (1972Ra14) and 1963.6 {I4} (1972As01) 
$%branching=65 {I15} (1968Mo07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D+Q)
decay_comment:
$A{-2}=+0.04 {I3}, A{-4}=-0.08 {I4} for 3112|g (1968Mo07) 
$A{-2}=+0.14 {I5}, A{-4}=0 for 783|g (1968Mo07) 
E$weighted average of 3111.9 {I15} (1972Ra14) and 3112 {I1} (1972As01) 
MR$ -0.09 {i29} for J=1 or +0.34 {i13} for J=2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=-0.03 {I2}, A{-4}=+0.01 {I1}; A{-2}'=(0.0 {I15}), A{-4}'=+0.1 {I4} for 2056|g (1972As01) 
E$weighted average of 2055.2 {I10} (1972Ra14) and 2055.5 {I4} (1972As01) 
$%branching=55 {I10} (1968Mo07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=+0.08 {I5}, A{-4}=0 for 3267|g (1968Mo07) 
$A{-2}=+0.12 {I5}, A{-4}=0 for 783|g (1968Mo07) 
$A{-2}=0.0 {I8}, A{-4}=+0.02 {I12}; A{-2}'=(0.0 {I29}), A{-4}'=(+0.4 {I9}) for 3267|g (1972As01) 
E$unweighted average of 3268.8 {I8} (1972Ra14) and 3266 {I1} (1972As01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=+0.01 {I3}, A{-4}=0.00 {I1}; A{-2}'=(0.0 {I31}), A{-4}'=0.00 {I13} for 3285|g (1972As01) 
E$unweighted average of 3287 {I2} (1972Ra14) and 3282.6 {I11} (1972As01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$A{-2}=(0.0 {I19}), A{-4}=0.0 {I7}; A{-2}'=-0.45 {I51}, A{-4}'=0.00 {I34} for 1205|g (1972As01) 
E$weighted average of 1205.2 {I4} (1972Ra14) and 1205.5 {I7} (1972As01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from E(level) difference. 
M from {+51}V(p,n|g). Comparison to RUL gives |d{+2}<7.8|*10{+-4}. 
MR |d{+2}<0.017 in {+51}V(p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from weighted average of 603.3 {I4} in (n,|g) and 603.8 {I5} in |e decay. Other:603.4 {I9} in (p,n|g) 
other |d:+0.07 {I4} in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from a weighted average of 1353.5 {I9} in (n,|g) and 1353.9 {I8} in |e decay. other: 1352.8 {I3} in (|a,n|g) 
other |d:+0.19 {I3} from (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E from (p,n|g) 
M D(+Q) from |g(|q) in (|a,n|g); polarity from no parity change based on L({+3}He,|a)=3 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
E seen only by 1980Sa07, value is from E(level) difference. 
M from an intensity balance, 1980Sa07 determine |a(exp)=1.3 {I4}. This is consistent with E1 or with M1+E2 with |d<0.12. From RUL one expects |d<0.026, and from adopted levels one has |D|p=no. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
|g(|q): A{-2}=-0.503 {I6}, A{-4}=-0.001 {I9}, |g(Pol)=-0.4 to -0.1 (1973Sa12) 
MR from 1973Sa12. Other: -0.19 {I+4-2} (1980Ka10). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
MR |d(M3,E2)=0.00 {I2} (1973Sa12), -0.02 {I2} (1980Ka10). 
|g(|q): A{-2}=+0.341 {I20}, A{-4}=-0.098 {I18}, |g(Pol)=+0.3 to 1.0 (1973Sa12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
MR |d(M3,E2)=0.00 {I3} (1978Ka32), |d(M3,E2)=0.00 {I5} (1973Sa12). 
|g(|q): A{-2}=+0.281 {I21}, A{-4}=-0.067 {I22} (1973Sa12) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
E 1193|g is seen by 1980Ka10 in coincidence with both the 775 and 905|g's, and the coincidence intensities cannot be accounted for by introducing a 2385-2255 transition since such a transition would have B(M1)(W.u.) and/or B(E2)(W.u.) greatly exceeding RUL. 
|g(|q): A{-2}=-0.174 {I21}, A{-4}=-0.073 {I27} (1973Sa12) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E seen only by 1980Sa07, value is from E(level) difference 
M from an intensity balance, 1980Sa07 determine |a(exp)=1.3 {I4}. This is consistent with E1 or with M1+E2 with |d<0.12. From RUL one expects |d<0.026, and from the known J|p's one has |D|p=no. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E not observed. Value deduced from E(level) difference. 
RI 1970Sa15 report an upper limit on the branching with I|g<0.3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
|g(|q): A{-2}=+0.09 {I2}; A{-4}=+0.02 {I2} (1985Av04) 
|d(M3,E2): -0.04 {I5} (1971Iy03), -0.04 {I3} (1985Av04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR other value -4.3 {I8} (1985Av04) is ruled out by RUL. 
|g(|q): A{-2}=-0.13 {I7}; A{-4}=-0.10 {I8} (1985Av04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
RI from branching in (|a,n|g) one expects I|g=44 
Other |d: -0.49 {I11} or -1.7 {I5} (1972Eg01). 
|g(|q): A{-2}=-0.04 {I2}; A{-4}=+0.01 {I2} (1985Av04) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$ if 8179.2 level energy is correct, then E|g should be 6744.8, not 6740.8 as listed in table I of 2013Pa38 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: ?
decay_comment:
1976Ar13 reported this |g with a relative intensity of 0.22 {I5}. There is no evidence for a 1213-keV |g in the Compton suppressed Ge(Li) spectra of 1977Ya08. This, and the apparent absence of a 766-keV |g, claimed by 1976Ar13 to feed a level at 2647 keV, lead evaluators to doubt that the 2647-keV level is detectably populated. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI authors give I|g=0.088 in their table iv and I|g=0.008 in their drawing. From adopted branching from 2768 level, one expects I|g=0.010 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
1976Ar13 claim to have observed the 766|g with an intensity |?1.3 times that of the 647.5. The Compton suppressed Ge(Li) spectra of 1977Ya08 demonstrate this is in error. 1978Be32 consider no evidence for 766|g in these spectra, and estimate I|g(766)/I|g(647) can not be greater than 0.05. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
DCO=0.96 {I4} (2000ApZX), DCO=1.10 {I2}, gate on 936 quadrupole transition (2007Ku19), pol=+0.09 {I3} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
DCO=1.13 {I5} (2000ApZX), DCO=1.06 {I8}, gate on 1434 quadrupole transition (2007ku19), pol=+0.10 {I2} (2007ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
DCO=0.87 {I9} (2000ApZX), DCO=1.07 {I4}, gate on 1434 quadrupole transition (2007Ku19), pol=+0.13 {I4} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
DCO=1.08 {I4} (2000ApZX), DCO=1.10 {I3}, gate on 1434 quadrupole transition (2007Ku19), pol=+0.15 {I3} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
DCO=1.27 {I15} (2000ApZX), DCO=1.20 {I7}, gate on 1434 quadrupole transition (2007Ku19), pol=+0.17 {I4} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
DCO=1.30 {I4}, gate on 1434 quadrupole transition (2007Ku19). 
RI based on I|g(398|g) and I|g for the sum. 
M$ DCO=1.30 {I4} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
DCO=0.58 {I11} (2000ApZX), DCO=0.73 {I8}, gate on 1434 quadrupole transition (2007Ku19), pol=-0.20 {I5} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M From 2007Ku19. DCO=0.57 {I10} (2000ApZX), DCO=0.72 {I6}, gate on 1434 quadrupole transition (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
DCO=1.02 {I7} (2000ApZX), DCO=1.20 {I3}, gate on 1434 quadrupole transition (2007Ku19), pol=+0.16 {I4} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
DCO=1.02 {I17} (dipole gated) (2000ApZX), DCO=0.750 {I16}, gate on 1434 quadrupole transition (2007Ku19), pol=-0.08 {I4} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR from 1977Be22 
DCO=0.77 {I8} (2000ApZX), DCO=0.72 {I3}, gate on 1434 quadrupole transition (2007Ku19), pol=-0.11 {I3} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
DCO=0.63 {I6} (2000ApZX), DCO=0.800 {I22}, gate on 1434 quadrupole transition (2007Ku19), pol=-0.12 {I4} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$from 2007Ku19. 
DCO=0.78 {I7} (dipole gated) (2000ApZX), DCO=0.650 {I18}, gate on 1434 quadrupole trasition (2007Ku19), pol=-0.04 {I4} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
DCO=0.61 {I6} (2000ApZX), DCO=0.78 {I4}, gate on 1434 quadrupole trasition (2007Ku19), pol=-0.15 {I5} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI from |g|g-coin spectra. 
DCO=0.57 {I3}, gate on 1434 quadrupole transition (2007Ku19), pol=-0.14 {I5}, (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
DCO=0.54 {I6} (2000ApZX), DCO=0.70 {I7}, gate on 1434 quadrupole transition (2007Ku19), pol=-0.04 {I5} (2007Ku19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
DCO=1.10 {I27} (2000ApZX), DCO=1.26 {I8}, gate on 1434 quadrupole transition (2007Ku19), pol=+0.14 {I5} (2007Ku19). 


decay_energy_unit: KEV
decay_multipolarity: E1
decay_comment:
E$compiler assumes E|g=7252.3 and E(level)=7252.9 instead of reverse values in Table II of 2018Wi07 
$|g(asymmetry)=-1.00 {I66} 


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 weighted average of values of {+50}Ti(|a,n|g), {+52}Cr(n,|g) thermal, and {+52}Cr(n,|g). 
MR$from (n,|g). Other: +0.11 {I7} from (|a,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from weighted average of values of {+50}Ti(|a,n|g), (HI,xn|g), and {+53}Cr(n,n'|g). 
MR Other: -0.17 {I+14-10} (|a,pn|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI 64 for I|g(1289.8)=100 (1973Gu04). 
MR other: -0.34 {I4} (1972Ca11). 
M A2=+0.128 8, A4=+0.002 8 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI 7.2 for I|g(1289.8)=100 (1973Gu04). 
M A2=-0.224 13, A4=-0.007 18 
MR 0.000 +24-21 (1973Gu04), 0.00 5 (1972Ca11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI 13 for I|g(1289.8)=100 (1973Gu04). 
MR other: +0.08 {I9} (1972Ca11). 
M A2=+0.279 2, A4=-0.001 1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI 30 for I|g(1289.8)=100 (1973Gu04). 
MR other: -0.03 {I2} (1972Ca11). 
M A2=-0.298 13, A4=-0.019 17 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E other: 1537.3 {I8} (1973Gu04) 
M A2=+0.327 22, A4=-0.065 18 
MR +0.03 3 (1973Gu04). 
RI 5 for I|g(1289.8)=100 (1973Gu04). (1972Ca11) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M A2=+0.31 3, A4=+0.07 3 
MR alternate solution of +4.7 {I+25-12} (1972Ca11) ruled out by comparison of B(E2) and T{-1/2} in Coul. ex. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 50 for I|g(1289.8)=100 (1973Gu04). 
MR -0.01 {I2} (1973Gu04), 0.00 {I2} (1982By01), -0.002 {I8} (1972Ca11). 
M A2=+0.323 8, A4=-0.095 7 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI 30 for I|g(1289.8)=100 (1973Gu04). 
MR other: -0.10 to -0.34 (1982By01). 
M A2=-0.462 9, A4=+0.009 11 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 16 for I|g(1289.8)=100 (1973Gu04). 
MR 0.00 {I4} (1982By01), (1973Gu04). 
M A2=+0.292 25, A4=-0.067 22 


decay_energy_unit: KEV
decay_multipolarity: M1(+E2)
decay_comment:
RI 5 for I|g(1289.8)=100 (1973Gu04). 
MR other: -0.16 to -0.28 (1982By01). 
M A2=-0.501 10, A4=+0.015 14 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
From 1978Wa09. It was not observed. E|g was calculated from level energies separation by the authors 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M from T{-1/2} determined by DSAM, it is sufficient to assure that these transitions are predominantly dipole, see 1978Na06. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M1+E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$taken by 2021Kl03 from the average of |d=0.080 and 0.025, which are deduced by the authors from A{-2}/A{-0} in 2011De20 and 2003Ap01, respectively. 


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.)=8.7 {I30} measured from Coulomb excitation cross section (2005Bu29), which gives level T{-1/2}=5.0 ps {I+26-13} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$from ({+48}Ca,X|g) (2006Zh42). Other: 450.1 {I7} in ({+11}B,2np|g) (2003Ap01). Values of E|g in the two studies differ significantly, however, it appears less likely that there are two closely-spaced J=3 levels. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q,Q
decay_comment:
M$from |g(|q) in (t,p|g) 
$|d(Q/D)=+1.0 {I11} for J(3166)=2, |d=+2.1 {I16} for J(3166)=3. |d(O/Q)=+0.18 {I18} for J(3166)=4 in (t,p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from ({+48}Ca,X|g). Ordering of the 588|g - 609|g cascade in ({+11}B,2np|g) (2003Ap01) reversed in ({+48}Ca,X|g) (2006Zh42). E|g=608.8 {I6} in ({+11}B,2np|g) 
RI$unweighted average of 32.4 {I11} in ({+48}Ca,X|g) and 41.5 {I15} in ({+11}B,2np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$from ({+48}Ca,X|g). Other: E|g=848.6 {I6} in ({+11}B,2np|g) 
RI$unweighted average of 29.6 {I12} in ({+48}Ca,X|g) and 41.7 {I15} in ({+11}B,2np|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$E|g=1069.8 {I5} (2003Ap01). E|g=1069.97 {I18}, I|g=60.7 (1977Na12) 
$Sign of A{-4} is inconsistent with |DJ=2 transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
$E|g=1501.3 {I7} (2003Ap01). E|g=1498.96 {I45}, I|g=8.4 (1977Na12, unplaced |g). Unweighted average of the two E|g values taken. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$|d(O/Q)|>+1.73 or +0.35 {I35} for J(2687)=4. |d(Q/D)|>+0.27 for J(2687)=3, -0.3 {I14} for J(2687)=2, and |>+0.36 or -0.78 {I42} for J(2687)=1 


decay_energy_unit: KEV
decay_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 the Adopted Gammas 
$Measured B(E2)(W.u.) in 2005Bu29 given relative to known corresponding value for the first 2+ state in {+54}Cr, taken from literature. Authors made systematic comparison of measured B(E2)(W.u.) values for the first 2+ states in {+48},{+50},{+52},{+54},{+56},{+58}Cr isotopes, and showed that the collectivity of the first 2+ state in {+56}Cr was much lower than that of neighbouring even-even Cr isotopes, appearing similar to that for {+52}Cr with the N=28 subshell closure. Small B(E2)(W.u.) and high excitation energy of this level indicated closure of N=32 subshell in {+56}Cr. 


decay_energy_unit: KEV
decay_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 'adopted gammas' 
$ B(E2) from 2005Bu29 given relative to known corresponding value for {+54}Cr in the literature. 


decay_energy_unit: KEV
decay_comment:
E$ placement by the evaluators based on work by 2006Zh42. 2006Ma11 placed this |g from a 4588, (8+) level, but the yrast 8+ member is most likely at 4680 keV as in 2006Zh42 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Weighted average of 207.8 {i4} ({+59}V |b{+-} decay), 208 {i1} ({+59}Cr it decay (96 |ms)), and 207.1 {i3} ({+48}Ca,2p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$Weighted average of 102.0 {i4} ({+59}V |b{+-} decay), 102 {i1} ({+59}Cr it decay (96 |ms)), and 102.7 {i2} ({+48}Ca,2p|g). 


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:
M RUL eliminates E3, M3 and higher multipolarities; M2 favored by analogy with isomeric states in neighboring nuclides. 
1999So20 conclude that the 193|g is the isomeric transition rather than the 208|g (suggested in 1998Gr14) because the 208|g and 102|g are present in {+59}V |b{+-} decay but the 193|g is not. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,M1+E2
decay_comment:
M$from Weisskopf estimates, and observation of no time delay between the 127- and 98-keV |g rays within the experimental detection limit of |?150 ns (2014Su07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$from Weisskopf estimates and non-observation of a long lifetime for 71-keV level 
$E|g=71 {I2} (2005Ga01) is unplaced 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D,M1+E2
decay_comment:
$E|g=97 {I2} (2005Ga01) 
M$from Weisskopf estimates, and observation of no time delay between the 127- and 98-keV |g rays within the experimental detection limit of |?150 ns 


decay_energy_unit: KEV
decay_comment:
E$weighted average of 446 {I1} ({+62}V decay), 449 {I4} ({+1}H({+62}Cr,{+62}Cr'|g)), 440 {I7} ({+9}Be({+62}Cr,{+62}Cr'|g)) 


decay_energy_unit: KEV
decay_comment:
E$from summed |g-ray spectrum from all the three reactions. Others: 1010 {I7} in ({+65}Mn,{+62}Cr) reaction, and 1012 {I7} in ({+66}Fe,{+62}Cr)+({+68}Co,{+62}Cr) 
$The 1012|g was observed in coincidence with the 439|g not with 726|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 430 {I2} from {+64}V |b{+-} decay, 420 {I7} from ({+64}Cr,{+64}Cr'|g), 423 {I6} from ({+65}Mn,{+64}Cr) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from summed |g-ray spectrum from all the three reactions. Others: 962 {I7} in ({+65}Mn,{+64}Cr) reaction, and 964 {I8} in ({+66}Fe,{+64}Cr)+({+68}Co,{+64}Cr) (2021Ga02) 


decay_energy_unit: KEV
decay_comment:
E$from 423 {I6} in ({+65}Mn,{+64}Cr) reaction, and 420 {I7} in ({+66}Fe,{+64}Cr)+({+68}Co,{+64}Cr). More precise energy is 430 {I2} from {+64}V |b{+-} decay (2014Su11) 


decay_energy_unit: KEV
decay_comment:
E$from summed |g-ray spectrum from all the three reactions. Others: 962 {I7} in ({+65}Mn,{+64}Cr) reaction, and 964 {I8} in ({+66}Fe,{+64}Cr)+({+68}Co,{+64}Cr) 


decay_energy_unit: KEV
decay_multipolarity: M1
decay_comment:
$B(M1)=0.043 |m{+2}{-n} {I3} (2024Ut02) 
$M1/E2 mixing ratio is unknown, by varying possible E2 component by a factor of 100, 2024Ut02 determine transition is dominant M1, uncertainty covers the range of physical E2 strengths. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$from 2007Do17. Other: 313 {I1} (2016Or03) 
RI$weighted average of 65 {I13} (2016Or03) and 63 {I6} (2007Do17) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$from 2007Do17. Other: 90 {I1} (2016Or03) 
RI$from 2016Or03 
M$possible assignment deduced from |g-intensity balance at 313-keV level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$from 2007Do17. This line was observed only partially due to some problems with the data acquisition system in 2016Or03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E$weighted average of 149.0 {I1} from {+50}Fe |e decay (152.0 ms), 149.2 {I1} from ({+12}C,pn|g), and 149.2 {I1} from (p,n|g) 
M$|DJ=1, dipole from DCO in ({+32}S,|apn|g); |DJ|p requires M1. |d(Q/D)=+0.02 {I3} from |g|g(|q) in (p,n|g) 
RI$from {+50}Fe |e decay. Others: 100 {I30} from ({+28}Si,|apn|g), 100 {I2} from 2000Sc35 and 100 from (1971Ki17) in (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 799.6 {I2} from {+50}Fe |e decay (152.0 ms) and 800.0 {I1} from (p,n|g) 
RI$from {+50}Fe |e decay. Others: 60 {I30} from ({+28}Si,|apn|g), 56 {I2} from 1971Ki17 in (p,n|g), but 156 {I3} from 2000Sc35 in (p,n|g) is in disagreement 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$weighted average of 805.4 {I1} from ({+12}C,pn|g) and 805.1 {I5} from (p,n|g) 
RI$from ({+12}C,pn|g). Other: 100.0 {I24} from ({+28}Si,|apn|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
M$(M1) listed in 1998Sv02, but with revised 5+ for 1917 level as in 2002Ol01, this transition should be E2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
$I|g(149|g)/I|g(800|g)=1.77 {I6} (1971Ki17) is in disagreement with 0.64 {I2} from 2000Sc35, but in a good agreement with the ratio in {+50}Fe |e decay. See Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$ M1+E2, |d=+2.55 {I27} for J|p=4+ for 1917 level in 2000Sc35, but for revised J|p=5+, the transition should be pure E2. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2+M3
decay_comment:
MR +0.41 {I14} or +1.4 {I4} (1972Fo25) 
|g(|q): A{-2}=-0.09 {I3}, A{-4}=0 (1972Fo25); A{-2}=+0.004 {I8}, A{-4}=-0.005 {I9} (1974Sc17) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|g(|q): A{-2}=-0.11 {I6}, A{-4}=+0.05 {I8} (1977No01); A{-2}=-0.01 {I3}, A{-4}=0.01 {I3}, |d=0.17 {I5} (1978Fo09) 
E,RI$Other: E|g=238.0 {I5}, I|g=137 {I7} (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|g(|q): A{-2}=+0.17 {I11}, A{-4}=-0.11 {I15} (1977No01); A{-2}=0.06 {I6}, A{-4}=0.10 {I8} (1978Fo09) 
E,RI$Other: E|g=901.5 {I5}, I|g=79 {I6} (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
|g(|q): A{-2}=+0.60 {I29}, A{-4}=+0.10 {I41} (1977No01). 
E,RI$Other: E|g=1139.3 {I5}, I|g=16 {I5} (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|g(|q): A{-2}=-0.29 {I5}, A{-4}=-0.04 {I8} (1977No01); A{-2}=-0.07 {I4}, A{-4}=-0.11 {I4}, |d=0.00 {I8} (1978Fo09) 
E,RI$Other: E|g=349.0 {I5}, I|g=85 {I7} (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
|g(|q): A{-2}=+0.23 {I13}, A{-4}=-0.30 {I18} (1977No01); A{-2}=0.21 {I7}, A{-4}=0.01 {I9} (1978Fo09) 
E,RI$Other: E|g=1249.9 {I5}, I|g=106 {I8} (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|g(|q): A{-2}=+0.47 {I17}, A{-4}=-0.12 {I25} (1977No01); A{-2}=0.20 {I8}, A{-4}=0.08 {I10} (1978Fo09) 
E,RI$Other: E|g=1467.8 {I5}, I|g=95 {I8} (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
|g(|q): A{-2}=+0.23 {I26}, A{-4}=-0.22 {I38} (1977No01); A{-2}=0.23 {I11}, A{-4}=-0.16 {I13} (1978Fo09) 
E,RI$Other: E|g=1817.7 {I5}, I|g=62 {I5} (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
|g(|q): A{-2}=+0.45 {I15}, A{-4}=-0.10 {I22} (1977No01); A{-2}=0.30 {I12}, A{-4}=-0.10 {I15} (1978Fo09) 
E,RI$Other: E|g=1762.3 {I5}, I|g=53 {I5} (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
|g(|q): A{-2}=-0.41 {I5}, A{-4}=0.0 {I8} (1977No01); 
E,RI$Other: E|g=429.0 {I5}, I|g<103 (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
|g(|q): A{-2}=+0.38 {I6}, A{-4}=-0.07 {I9} (1977No01); A{-2}=0.36 {I5}, A{-4}=-0.10 {I6} (1978Fo09) 
E,RI$Other: E|g=722.2 {I5}, I|g=82 {I6} (1978Fo09) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|g(|q): A{-2}=-0.23 {I10}, A{-4}=+0.02 {I14} (1977No01); A{-2}=0.29 {I4}, A{-4}=-0.10 {I4}, |d=-0.05 {I5} (1978Fo09) 
E,RI$Other: E|g=458.5 {I5}, I|g=100 (1978Fo09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E,RI$From 1978Fo09. Other: E|g=1500 (1978NoZW) 
|g(|q): A{-2}=-0.61 {I12}, A{-4}=-0.07 {I14}, |d=-0.23 {I6} (1978Fo09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E,RI$From 1978Fo09. Other: E|g=830 (1978NoZW) 
|g(|q): A{-2}=-0.47 {I10}, A{-4}=-0.00 {I12}, |d=-0.12 {I4} (1978Fo09) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
E,RI$From 1978Fo09. Other: E|g=705 (1978NoZW) 
|g(|q): A{-2}=0.47 {I8}, A{-4}=-0.11 {I10} (1978Fo09) 
M from Adopted Gammas 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
|d=-0.038 {I10} from E(p)=6.85 MeV data, |d=-0.005 {I10} from E(p)=6.50 MeV data, if J(826)=3 (1976Ta14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
E$Weighted average values of 869.3 keV 5 (1976St19), 869.4 keV 5 (1976Av06), 869.2 keV 6 (1978Me19), and 870.1 keV 5 (1979Me03). 
$POL=-0.0580 {I43}, A{-2}=-0.41 {I3}, A{-4}=+0.06 {I6} (2007Ax01). Other: |d=-0.10 {I5} (1976Av06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$POL=-0.0155 {I57}, A{-2}=-0.53 {I2}, A{-4}=+0.02 {I1} (2007Ax01). Other: |d=-0.30 {I10} (1976Av06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$POL=-0.0623 {I61}, A{-2}=-0.37 {I2}, A{-4}=+0.00 {I5} (2007Ax01). Other: |d=-0.08 {I7} (1976Av06). 


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 weighted average of values in {+53}Fe |e decay and (|a,p|g). 
MR others: +0.49 {I3} (|a,p|g), +0.6 {I3} (p,n|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M predicted linear pol=+70 to +0.91, exp=+1.0 {I4} (1973Sa10) 
M A2=+0.436 19, A4=-0.084 17; LINEAR POLARIZATION 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M A2=-0.13 1, A4=+0.02 1 (1973Ch25); A2=-0.12 1, A4=-0.01 1 (1974Ke11) 
MR from 1970Mc14. Other: +0.47 {I11} (1966Go21) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M A2=+0.26 1, A4=-0.02 2 (1973Ch25); A2=+0.22 1 (1971Wi21). 
MR 0 (1970Mc14), -0.03 {I7} (1971Wi21). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M A2=+0.27 2, A4=+0.09 2 (1973Ch25) 
MR from 1970Mc14. Others: +3.2 -15+5 or +0.6 -1+2 (1973Ch25); +3.7 -5+14 (1971Wi21). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
M A2=-0.28 7, A4=+0.01 7 (1973Ch25); A2=-0.18 2 (1971Wi21) 
MR -0.09 {I1} or -3.4 {I13} (1971Wi21). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
M A2=-0.33 3, A4=+0.05 3 (1973Ch25); A2=-0.42 3 (1971Wi21) 
MR -0.3 -28+2 or -1.6 {I15} (1973Ch25); -1.5 {I15} (1971Wi21). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D,E2
decay_comment:
M A2=+0.17 1, A4=-0.02 1 (1973Ch25); A2=+0.060 15 (1971Wi21) 
MR +1.3 -3+5 or -0.14 {I12} (1973Ch25); +2.1 -4+8 or -0.32 {I11} (1971Wi21). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
M A2=+0.59 8 , A4=-0.02 8 (1973Ch25); A2=+0.52 1, A4=+0.16 2 (1971Wi21). 
MR from 1973Ch25. Other: +1.6 {I8} (1971Wi21) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.97 {I4}, R{-DCO}(150|'-97|')=0.95 {I4}, R{-DCO}(127|'-97|')=0.95 {I4}, DCO gate=A 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.84 {I5}, R{-DCO}(150|'-97|')=0.59 {I3}, R{-DCO}(127|'-97|')=0.76 {I4}, DCO gate=B 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.02 {I5}, R{-DCO}(150|'-97|')=1.00 {I4}, R{-DCO}(127|'-97|')=1.03 {I4}, DCO gate=A 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.95 {I20}, R{-DCO}(150|'-97|')=0.30 {I5}, R{-DCO}(127|'-97|')=0.60 {I10}, DCO gate=C 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$R{-DCO}(150|'-127|')=1.08 {I5}, R{-DCO}(150|'-97|')=1.03 {I4}, R{-DCO}(127|'-97|')=1.27 {I5}, DCO gate=D 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.55 {I4}, R{-DCO}(150|'-97|')=0.32 {I2}, R{-DCO}(127|'-97|')=0.62 {I4}, DCO gate=B 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.94 {I12}, R{-DCO}(150|'-97|')=1.03 {I11}, R{-DCO}(127|'-97|')=1.12 {I14}, DCO gate=B 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$R{-DCO}(150|'-127|')=0.91 {I13}, R{-DCO}(150|'-97|')=1.13 {I13}, R{-DCO}(127|'-97|')=1.30 {I17}, DCO gate=A 
$|DJ=0 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.56 {I3}, R{-DCO}(150|'-97|')=0.31 {I1}, R{-DCO}(127|'-97|')=0.59 {I3}, DCO gate=D 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.46 {I3}, R{-DCO}(150|'-97|')=0.23 {I2}, R{-DCO}(127|'-97|')=0.51 {I2}, DCO gate=D 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.98 {I7}, R{-DCO}(150|'-97|')=1.07 {I7}, R{-DCO}(127|'-97|')=1.10 {I7}, DCO gate=D 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$R{-DCO}(150|'-127|')=1.01 {I14}, R{-DCO}(150|'-97|')=0.99 {I12}, R{-DCO}(127|'-97|')=1.14 {I14}, DCO gate=D 
$|DJ=0 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.38 {I13}, R{-DCO}(150|'-97|')=0.28 {I5}, R{-DCO}(127|'-97|')=0.58 {I6}, DCO gate=A 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.62 {I3}, R{-DCO}(150|'-97|')=0.39 {I2}, R{-DCO}(127|'-97|')=0.64 {I3}, DCO gate=F 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.06 {I8}, R{-DCO}(150|'-97|')=1.19 {I8}, R{-DCO}(127|'-97|')=1.08 {I7}, DCO gate=A 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.98 {I16}, R{-DCO}(150|'-97|')=1.25 {I19}, R{-DCO}(127|'-97|')=1.02 {I17}, DCO gate=D 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.52 {I3}, R{-DCO}(150|'-97|')=0.31 {I2}, R{-DCO}(127|'-97|')=0.56 {I3}, DCO gate=B 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.98 {I5}, R{-DCO}(150|'-97|')=1.09 {I5}, R{-DCO}(127|'-97|')=1.07 {I5}, DCO gate=F 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.77 {I3}, R{-DCO}(150|'-97|')=0.51 {I2}, R{-DCO}(127|'-97|')=0.77 {I3}, DCO gate=D 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.02 {I7}, R{-DCO}(150|'-97|')=1.10 {I7}, R{-DCO}(127|'-97|')=1.03 {I6}, DCO gate=D 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.84 {I4}, R{-DCO}(150|'-97|')=0.63 {I3}, R{-DCO}(127|'-97|')=0.79 {I3}, DCO gate=D 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.10 {I10}, R{-DCO}(150|'-97|')=1.10 {I9}, R{-DCO}(127|'-97|')=0.96 {I8}, DCO gate=D 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$R{-DCO}(150|'-127|')=1.07 {I19}, R{-DCO}(150|'-97|')=1.46 {I26}, R{-DCO}(127|'-97|')=1.22 {I25}, DCO gate=D 
$|DJ=0 


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:
K/L+M=7.1 {I10} (1969Ba25). 
M$M1+E2 from |d=+0.10 {I+11-4} (|a,n|g) (1972Og04). But M1 is given by comparison to RUL, so Mult=M1. 


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:
Linear polarization p=-0.33 2 from (A,PNG) by 1979To05. 
M$M1(+E2) from |d=+0.038 {I+30-20} (|a,n|g) (1972Og04). But d is given by comparison to RUL, 211|g to 4+, so Mult=M1. 
MR others: +0.04 ({+7}Li,3np|g), -0.00 {I2} (|a,pn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M$M1(+E2) from |d=+0.023 {I+30-10} (|a,n|g) (1972Og04). But d is given by comparison to RUL, 251|g to 4+, so Mult=M1. 
$|a(K)exp=0.0030 {I11} 


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$M1(+E2) from |d=0.06 {I+9-8} (|a,n|g) (1972Og04). But d is given by comparison to RUL, 407|g to 3+, so Mult=M1. 
$|a(K)exp=0.0009 {I4} 


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$M1(+E2) from |d=-0.045 {I70} (|a,n|g) (1972Og04). But d is given by comparison to RUL, 470.5|g to 5+, so Mult=M1. 


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$M1+E2 from |d=+0.18 {I10} (|a,n|g) (1972Og04). But d is given by comparison to RUL, 967|g to 3+, so Mult=M1. 


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$M1+E2 from |d=+0.002 {I20} (|a,n|g) (1972Og04). But d is given by comparison to RUL, 1375|g to (2)+, so Mult=M1. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
P(|g)=-0.11 {I2} from 1973Za07. 1970Og04 give |d=-0.30, here -0.030 corrected by evaluator. 
MR others: 0.00 {I7} (1972Hi05); 0.28 {I8} (1972Mi12); 0.25 {I5} (1973Za07) 
K/L+M>7, |a(K)exp=0.016 {I8}. 
A{-2}=-0.21 {I1}, A{-4}=-0.04 {I2} (p,n|g) (1974Ke11). 
A{-2}=-0.07 {I3}, A{-4}=-0.06 {I4} (|a,n|g) (1974Ke11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
A{-2}=-0.20 {I3}, A{-4}=-0.00 {I4} (p,n|g) (1972Og04). 
A{-2}=-0.07 {I2}, A{-4}=-0.03 {I3} (|a,n|g) (1974Ke11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR others: 0.088 {I35} (1972Hi05), -0.11 {I4} or <-8 (1972Mi12). 
A{-2}=-0.13 {I2}, A{-4}=-0.02 {I2} (p,n|g) (1974Ke11). 
A{-2}=0.01 {I1}, A{-4}=-0.03 {I3} (|a,n|g) (1974Ke11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR other: -0.25 {I+9-15} (1972Mi12). 
A{-2}=0.23 {I4}, A{-4}=-0.05 {I5} (p,n|g) (1972Og04). 
A{-2}=0.02 {I2}, A{-4}=-0.02 {I3} (|a,n|g) (1974Ke11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR or -8 {I+3-9} but eliminated since E2 strength would be 2080 W.u. 
A{-2}=-0.07 {I7}, A{-4}=-0.04 {I11} (p,n|g) (1974Ke11). 
A{-2}=0.02 {I2}, A{-4}=-0.03 {I3} (|a,n|g) (1974Ke11). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$transitions in {+54}Mn and {+56}Mn are too close to distinguish (2006Me08) 
RI$|>70% of |g-ray yield in {+54}Mn due to known cascading from 1073 level (2006Me08) 


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 calculated from T{-1/2} and B(E2). Others: +0.07 {I1} (HI,xn|g) and (|a,p|g), +0.049 {I9} (Coul. ex.). 
EKC 0.014 {I3} (Coul. ex.). 


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 |d=+0.6 {I+5-10} or +1.6 {I+8-30} in (|a,p|g). 
BM1W,BE2W B(M1)(W.u.)=0.004 {I3} or 0.002 {I2}; B(E2)(W.u.)=0.6 {I+11-5} or 1.5 {I8} (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR |d=+0.2 {I+6-1} or +2.6 {I+80-13} (|a,p|g). 
BM1W,BE2W B(M1)(W.u.)=0.05 {I3} or 0.007 {I+20-7}; B(E2)(W.u.)<12 or =17 {I+13-8} (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
RI (|a,p|g). 
MR |d=-0.02 {I8}, or 1/|d=0.04 {I8} in (|a,p|g). 
B(M1)(W.u.),B(E2)(W.u.): B(M1)(W.u.)=0.05 {I2} or 0; B(E2)(W.u.)=0 or 40 {I20} (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E transition observed only in coincidence spectra. 
RI based on I|g for 1402|g and 2241|g and adopted decay scheme. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: (D+Q)
decay_comment:
M value assumes negative parity for 2311.5 level. 
MR from 1972Sa38; values from 1973Hi07 are -0.15 {I+20-30} for J|p=13/2-, and +0.25 {I+5-25} for J|p=9/2-. The negative parity is assumed only for purpose of the calculation. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
MR from 1973Hi07 is +0.2 {I3} (M3/E2 mixing ratio). 
M value assumes negative parity for 2727 level. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
RI 10 {I2} for {+55}Mn(K{+-},xpyn|g); 1.9 {I8} for {+59}Co(K{+-},xpyn|g); 2.7 {I8} for Fe(K{+-},xpyn|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
E value was calculated by evaluator from the energy difference between the initial level and the final level. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR other: +0.21 {I3} (1974Po14). 
A2=0.17 2; A4=-0.02 2 (1977Na12). A2=0.06 2; A4=-0.07 2 (1974Po14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
MR other: +0.22 {I4} (1974Po14). 
A2=-0.07 1; A4=-0.02 2 (1977Na12). A2=0.05 3; A4=-0.08 3 (1974Po14). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M from |a deduced from intensity balances in {+55}Mn(n,|g) and {+56}Cr |b{+-} decay, and RUL, which give |d(26|g)<0.05 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M from |a deduced from intensity balances in {+55}Mn(n,|g) and {+56}Cr |b{+-} decay, and RUL, which give |d(84|g)<0.5. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M E2 or M1+E2 depending on whether J(215)=1+ or 2+ 
MR |d(E2/M1): +0.03 {I5} or -5 {I1} if J(215)=2 in {+55}Mn(n,|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from 1971Va01. 
CC |a(exp)=2.0 {I2} from |g|g-coin and intensity balance (1961Es02); |a(exp)=1.4 {I7} from intensity balance (1971Va01). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$Percent=1.7 {I3} 
E$transitions in {+54}Mn and {+56}Mn are too close to distinguish (2006Me08) 
RI$|<30% of |g-ray yield in {+56}Mn due to known cascading from 1073 keV level in {+54}Mn (2006Me08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
E weighted av from |b{+-} decay and ({+13}C,3np|g) and ({+15}n,2n|a|g) 
M d from |a=0.05; M1 from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M1)
decay_comment:
MR |>+0.2 if J=3/2; |>+1 if J=5/2 from adopted gammas 
E NOTE APPARENT MISPRINT IN TABLE I OF 1978Da04 GIVING EG=105.8 (EVALUATORS) 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
$|s{-|g}=19.5 {I65} 
Observed definitely between E(n)=6.09 and 13.2 MeV and possibly between E(n)=5.05 and 6.09 MeV. The threshold of |?5 to 6 MeV is consistent with a 2742-1061 transition in {+57}Mn. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$ 377.4 3 (2000Ap02), 376.45 10 (1978Na06) 
DCO=1.41 {I9} (gate: 144|g) 
A{-2}=-0.45 {I3}. Other: A{-2}=-0.69 {I2} (1978Na06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$ |g placed from 1880 level in 2010St01 
E$ 280.0 3 (2000Ap02), 279.83 12 (1978Na06) 
DCO=1.02 {I4} (gate: 144|g) 
A{-2}=-0.10 {I3}. Other: A{-2}=-0.39 {I2} (1978Na06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E$ |g placed from 1601 level in 2010St01 
E$ 144.1 3 (2000Ap02), 144.13 15, UNPLACED TRANSITION IN 1978Na06 
DCO=0.67 {I5} (gate: 377|g) 
A{-2}|?0 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$ |g placed from 1601 level in 2010St01 
E$ 1154.8 4 (2000Ap02), 1153.54 20 (1978Na06) 
DCO=1.05 {I5} (gate: 582|g) 
A{-2}=-0.3 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E$ |g placed from 3042 level in 2010St01 
E$ 581.9 7 (2000Ap02), 581.43 20 (1978Na06) 
DCO=0.99 {I4} (gate: 582|g) 
A{-2}=-0.22 {I5} 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: (Q)
decay_comment:
E$ from level-energy difference. E|g=1268 {I2} (|g from 2000Ap02 only) fits poorly in the level scheme 
DCO=0.82 {I6} (gate: 582|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$Placement from {+59}Cr |b{+-} decay. A comparable 1126.3 keV 3 |g is placed from 3767 keV level in ({+48}Ca,pn|g). However, 1238 keV level is not reported in ({+48}Ca,pn|g) 2010St01 and did not observe 1238|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$Weighted average of 252.5 {I1} ({+48}Ca,pn|g) and 251.6 {I3} ({+70}Zn,X|g). 
M$From ({+48}Ca,pn|g) and RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$unweighted average of 157.2 {I5} (|b{+-} data), 157.3 {I2} (({+64}Ni,X|g) data), 156.7 {I1} (({+70}Zn,X|g) data). Weighted average is 156.8 {I2} but with reduced |h{+2}=3.9 
CC$value overlaps M1 and E2 
$B(E2)(W.u.) is obtained by 2009Va16 with constrained B(M1)=0.008 based on T{-1/2}(157 level)<1.7 ns (minimum flight time between the secondary target and the particle detector) since mixing ratio of the 157-keV transition could not be obtained from their |g(|q) data. 


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:
$B(E2)(W.u.) is obtained by 2009Va16 with constrained B(M1)=0.008 based on T{-1/2}(157 level)<1.7 ns (minimum flight time between the secondary target and the particle detector) since mixing ratio of the 157-keV transition could not be obtained from their |g(|q) data. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$relative to I|g=1520 {I40} and 2300 {I60} for 311|g and 415|g from {+109}Ag target excitation, respectively. 8.1% uncertainty due to the background subtraction and uncertainty due to the relative efficiency correction were taken into account. The uncertainty due to the normalization to the {+109}Ag target excitation is included in the quoted uncertainty. 
E$no |g-rays were observed in coincidence with this transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$|?11 if no other |g transitions from the 186.4 and 1148.7 levels. Other: E|g=189 {I1}, I|g=17% of the |b strength (2002MaZN) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E1)
decay_comment:
E$from 2011Li50. 2005GaZR cite a priv. comm. from an experiment by J.M. Daugas (2004) at GANIL facility where observation of a 40-keV transition was reported 
RI$63 {I+20-13} deduced from I(|g+ce) and |a. 
M$from |a(exp) and no observable half-life (2011Li50) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M2)
decay_comment:
E$from 2011Li50. Others: 135.3 {I5} (2012Ka36), 135 {I10} (2005GaZR, ce spectrum) 
RI$90 {I+3-2} deduced from I(|g+ce) and |a 
M$based on Weisskopf estimates and hindrance factor of 9 (2011Li50). Also M2-E1 cascade is consistent with expected intensity of 135.3|g in |g(ce) coin spectrum (2005GaZR) 


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 764.8 {I3} from {+50}Co |e decay (38.8 ms) and 765.3 {I6} from {+51}Ni |ep decay (23.8 ms). Other: 767 {I7} from ({+50}Fe,{+50}Fe'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_mixing_ratio_info: ;ERR=GT
decay_comment:
M D+Q from R{-141-97}=I{-|g}(141|')/I{-|g}(97|')=0.4 {I2} (2004Ek03); D+Q is assumed to be M1+E2 due to considerable mixing ratio being observed in 2004Ek03. Level scheme requires (M1+E2). 
MR From 2004Ek03 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E1]
decay_comment:
RI$Intensity of transition has been corrected for the angular distribution by 1998Ur05, as specified in literature. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E4
decay_BE_unit: e^2 x (fm)^8
decay_BE_info: ;TYPE=BE4;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE4W
decay_comment:
CC E4 CC(THEORY)'S MULT. BY 0.975 5 (Cf. 1990Ne01) 
M$From experimental E4 systematics for f7/2-shell nuclei see {+28}Si({+28}Si,2p2n|g) (2005Ga20). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI possibly overestimated; source may contain an expected but yet unobserved 2+ isomer of {+52}Co (1997Ha04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M Angular distribution analysis could not be performed for the 2735and 2753 transitions in 1998Ur05 since their broadened line shapes were overlapping. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
E Uncertainty assigned to transition by evaluators. 
M |DJ=1 transition (implied by spin assignment made in 1998Ur05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
RI Intensity of transition has been corrected for the angular distribution by 1998Ur05. 
M Angular distribution analysis could not be performed for the 2735 and 2753 transitions in 1998Ur05 since their broadened lineshapes were overlapping; the authors assume this |g-ray to be of |DJ=1 character. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E4
decay_comment:
CC E4 CC(THEORY)'S MULT. BY 0.975 5 (Cf. 1990Ne01) 
M$From experimental E4 systematics for f7/2-shell nuclei (2005Ga20). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=CONV
decay_comment:
$B(E2) in e{+2}b{+2} units. Other: B(E2)=0.0163 {I20}, using mean lifetime |t=11.3 ps {I14} (2004Yu07). Note that the two values differ by 4-5 standard deviations 


decay_energy_unit: KEV
decay_comment:
$I|g(2488)/I|g(1288)=4.4 {I10} in {+52}Fe Adopted dataset in the ENSDF database (July 2015 update). 


decay_energy_unit: KEV
decay_comment:
$I|g(2755)/I|g(1556)=10 {I5} in {+52}Fe Adopted dataset in the ENSDF database (July 2015 update). There is also a 740.6|g to a 4400 level with an intensity of about 50% that of the 2755|g 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E$from literature, not seen in the present experiment 
$I|g(2759)/I|g(1910)=3.1 {I11} in {+52}Fe adopted Levels in the ENSDF database (July 2015 update) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_mixing_ratio_info: ;ERR=AP
decay_comment:
$R{-150-97}=1.70 {I7} 
MR Angular distribution for transition requires considerable |DJ=2 admixture. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI from branching ratio of |g rays 647 and 682 in 1978Ka32 and I|g of |g ray 682 in 1973Sa10. 
MR |d=-0.05 {I+8-11} (1978Ka32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M$predicted linear pol=+0.41 to +0.67; exp=+0.2 to 1.6 (1973Sa10) 
M A2=+0.306 26, A4=-0.011 24; LINEAR POLARIZATION 
MR MR=+0.00 5 (1978Ka32) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI$uncertainty for relative intensity is not given by 2023Pa08. See comment for 1328 level for intensity-imbalance issue at this level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$See comment for 2339 level for intensity-imbalance issue at this level 
M$M1+E2 in Fig. 1 and Table I is a misprint, perhaps a carry over of (incorrect) M1+E2 assignment in the Adopted Levels, Gammas dataset in the ENSDF database for {+53}Fe (March 31, 2007 update) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E4
decay_BE_unit: e^2 x (fm)^8
decay_BE_info: ;TYPE=BE4;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE4W
decay_comment:
$B(E4)=6.46|*10{+-6} e{+2}b{+4} {I5} (2023Pa08); deduced E4 reduced matrix element=0.01137 eb{+2} {I5} (2023Pa08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M5
decay_BM_unit: mu^2 x (fm)^8
decay_BM_info: ;TYPE=BM5;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM5W
decay_comment:
$B(M5)=3.31|*10{+-3} |m{-N}{+2}b{+4} {I16} (2023Pa08); deduced M5 reduced matrix element=0.257 |m{-N}b{+2} {I6} (2023Pa08) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E6
decay_BE_unit: e^2 x (fm)^12
decay_BE_info: ;TYPE=BE6;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE6W
decay_comment:
$Conversion coefficients for 3040.6, E6 transition obtained via e-mail communication from Dr. Tibor Kibedi (ANU), April 02, 2023. 
$B(E6)=2.61|*10{+-7} e{+2}b{+6} {I81} (2023Pa08); deduced E6 reduced matrix element=0.00229 |m{-N}b{+3} {I35} (2023Pa08) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_multipolarity: E0
decay_comment:
E from (p,p'|g). 
B(E0)(2561|g):B(E2)(1153|g)=0.49 {I8} in (p,p'|g). 
TI from electron-pair measurement (1972Wa28). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E4
decay_BE_unit: e^2 x (fm)^8
decay_BE_info: ;TYPE=BE4;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE4W
decay_comment:
M from {+40}Ca({+16}O,2p|g), based on a pulsed-beam search revealed a weak 10+ to 6+ E4 cross-over transition, see 1978NoZY. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E4
decay_comment:
RI from I|g(146|g):I|g(3578|g)=98.0 {I2}:2.0 {I2} (1978NoZY). 
M measured B(E4) is consistent with the negative polarization charge. From RUL, |g to 6+ cannot be M4. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.96 {I5}, R{-DCO}(150|'-97|')=0.99 {I5}, R{-DCO}(127|'-97|')=0.94 {I5}, DCO gate=B, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.99 {I5}, R{-DCO}(150|'-97|')=1.03 {I5}, R{-DCO}(127|'-97|')=0.94 {I5}, DCO gate=B, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.02 {I5}, R{-DCO}(150|'-97|')=0.96 {I4}, R{-DCO}(127|'-97|')=1.05 {I4}, DCO gate=A, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$R{-DCO}(150|'-127|')=0.95 {I8}, R{-DCO}(150|'-97|')=0.91 {I6}, R{-DCO}(127|'-97|')=0.96 {I7}, DCO gate=A, |DJ=2 
$|DJ=0 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.57 {I9}, R{-DCO}(150|'-97|')=0.40 {I5}, R{-DCO}(127|'-97|')=0.85 {I9}, DCO gate=A, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.84 {I17}, R{-DCO}(150|'-97|')=0.74 {I12}, R{-DCO}(127|'-97|')=0.85 {I14}, DCO gate=A, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.64 {I21}, R{-DCO}(150|'-97|')=0.50 {I11}, R{-DCO}(127|'-97|')=0.49 {I13}, DCO gate=A, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$R{-DCO}(150|'-127|')=1.13 {I15}, R{-DCO}(150|'-97|')=1.43 {I13}, R{-DCO}(127|'-97|')=1.24 {I14}, DCO gate=C, |DJ=2 
$|DJ=0 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.96 {I30}, R{-DCO}(150|'-97|')=1.00 {I20}, R{-DCO}(127|'-97|')=0.98 {I22}, DCO gate=A, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.79 {I10}, R{-DCO}(150|'-97|')=0.71 {I7}, R{-DCO}(127|'-97|')=0.70 {I8}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.29 {I11}, R{-DCO}(150|'-97|')=1.53 {I11}, R{-DCO}(127|'-97|')=1.17 {I9}, DCO gate=A, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.31 {I25}, R{-DCO}(150|'-97|')=1.71 {I25}, R{-DCO}(127|'-97|')=1.07 {I16}, DCO gate=B, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.94 {I6}, R{-DCO}(150|'-97|')=1.13 {I7}, R{-DCO}(127|'-97|')=1.05 {I6}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.21 {I32}, R{-DCO}(150|'-97|')=1.70 {I36}, R{-DCO}(127|'-97|')=0.75 {I21}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.89 {I5}, R{-DCO}(150|'-97|')=0.80 {I4}, R{-DCO}(127|'-97|')=1.14 {I6}, DCO gate=E, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.95 {I8}, R{-DCO}(150|'-97|')=1.19 {I9}, R{-DCO}(127|'-97|')=1.12 {I8}, DCO gate=C, |DJ=2 
$R{-DCO}(150|'-127|')=1.06 {I13}, R{-DCO}(150|'-97|')=1.57 {I16}, R{-DCO}(127|'-97|')=1.25 {I12}, DCO gate=E, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.75 {I7}, R{-DCO}(150|'-97|')=0.71 {I5}, R{-DCO}(127|'-97|')=0.85 {I6}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.09 {I13}, R{-DCO}(150|'-97|')=1.16 {I12}, R{-DCO}(127|'-97|')=1.02 {I11}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$R{-DCO}(150|'-127|')=0.91 {I20}, R{-DCO}(150|'-97|')=1.02 {I19}, R{-DCO}(127|'-97|')=0.89 {I23}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.08 {I27}, R{-DCO}(150|'-97|')=1.00 {I30}, R{-DCO}(127|'-97|')=1.13 {I34}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.72 {I5}, R{-DCO}(150|'-97|')=0.64 {I4}, R{-DCO}(127|'-97|')=0.85 {I5}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.70 {I13}, R{-DCO}(150|'-97|')=0.55 {I7}, R{-DCO}(127|'-97|')=0.84 {I10}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.09 {I16}, R{-DCO}(150|'-97|')=1.23 {I14}, R{-DCO}(127|'-97|')=1.08 {I15}, DCO gate=B, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.86 {I9}, R{-DCO}(150|'-97|')=0.60 {I6}, R{-DCO}(127|'-97|')=0.87 {I8}, DCO gate=F, |DJ=2 
$R{-DCO}(150|'-127|')=0.94 {I7}, R{-DCO}(150|'-97|')=0.98 {I6}, R{-DCO}(127|'-97|')=1.00 {I6}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.04 {I17}, R{-DCO}(150|'-97|')=0.92 {I10}, R{-DCO}(127|'-97|')=0.91 {I10}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.95 {I35}, R{-DCO}(150|'-97|')=0.94 {I26}, R{-DCO}(127|'-97|')=0.92 {I23}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.89 {I5}, R{-DCO}(150|'-97|')=0.94 {I5}, R{-DCO}(127|'-97|')=0.97 {I5}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.50 {I10}, R{-DCO}(150|'-97|')=0.55 {I8}, R{-DCO}(127|'-97|')=0.75 {I10}, DCO gate=B, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.00 {I20}, R{-DCO}(150|'-97|')=0.90 {I17}, R{-DCO}(127|'-97|')=0.96 {I17}, DCO gate=D, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.85 {I21}, R{-DCO}(150|'-97|')=1.06 {I27}, R{-DCO}(127|'-97|')=1.39 {I33}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.79 {I12}, R{-DCO}(150|'-97|')=0.99 {I12}, R{-DCO}(127|'-97|')=0.94 {I11}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.00 {I7}, R{-DCO}(150|'-97|')=1.19 {I8}, R{-DCO}(127|'-97|')=1.07 {I6}, DCO gate=E, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.14 {I15}, R{-DCO}(150|'-97|')=1.25 {I13}, R{-DCO}(127|'-97|')=1.06 {I12}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.57 {I8}, R{-DCO}(150|'-97|')=0.44 {I6}, R{-DCO}(127|'-97|')=0.78 {I8}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.92 {I10}, R{-DCO}(150|'-97|')=0.79 {I7}, R{-DCO}(127|'-97|')=0.79 {I7}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.90 {I5}, R{-DCO}(150|'-97|')=0.92 {I5}, R{-DCO}(127|'-97|')=0.96 {I5}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.08 {I8}, R{-DCO}(150|'-97|')=1.28 {I9}, R{-DCO}(127|'-97|')=1.25 {I8}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.93 {I11}, R{-DCO}(150|'-97|')=1.29 {I13}, R{-DCO}(127|'-97|')=1.29 {I13}, DCO gate=L, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.53 {I10}, R{-DCO}(150|'-97|')=0.53 {I8}, R{-DCO}(127|'-97|')=0.63 {I8}, DCO gate=C, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$R{-DCO}(150|'-127|')=1.22 {I11}, R{-DCO}(150|'-97|')=1.74 {I13}, R{-DCO}(127|'-97|')=1.41 {I11}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$R{-DCO}(150|'-127|')=0.96 {I12}, R{-DCO}(150|'-97|')=0.91 {I10}, R{-DCO}(127|'-97|')=0.92 {I10}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$R{-DCO}(150|'-127|')=1.07 {I17}, R{-DCO}(150|'-97|')=1.69 {I24}, R{-DCO}(127|'-97|')=1.28 {I17}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$R{-DCO}(150|'-127|')=1.04 {I14}, R{-DCO}(150|'-97|')=0.88 {I9}, R{-DCO}(127|'-97|')=0.82 {I8}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1+M2
decay_comment:
$R{-DCO}(150|'-127|')=0.81 {I9}, R{-DCO}(150|'-97|')=0.78 {I6}, R{-DCO}(127|'-97|')=0.85 {I6}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.92 {I9}, R{-DCO}(150|'-97|')=0.72 {I5}, R{-DCO}(127|'-97|')=0.84 {I6}, DCO gate=I, |DJ=1 
$R{-DCO}(150|'-127|')=0.99 {I6}, R{-DCO}(150|'-97|')=1.04 {I5}, R{-DCO}(127|'-97|')=1.04 {I6}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.20 {I18}, R{-DCO}(150|'-97|')=1.57 {I19}, R{-DCO}(127|'-97|')=1.35 {I18}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.90 {I6}, R{-DCO}(150|'-97|')=0.91 {I5}, R{-DCO}(127|'-97|')=0.98 {I6}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$R{-DCO}(150|'-127|')=0.92 {I11}, R{-DCO}(150|'-97|')=1.03 {I10}, R{-DCO}(127|'-97|')=0.96 {I9}, DCO gate=E, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.77 {I11}, R{-DCO}(150|'-97|')=0.54 {I7}, R{-DCO}(127|'-97|')=0.83 {I8}, DCO gate=C, |DJ=2 
$R{-DCO}(150|'-127|')=0.72 {I20}, R{-DCO}(150|'-97|')=0.54 {I11}, R{-DCO}(127|'-97|')=0.61 {I14}, DCO gate=J, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.27 {I38}, R{-DCO}(150|'-97|')=0.92 {I20}, R{-DCO}(127|'-97|')=1.18 {I32}, DCO gate=J, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.01 {I6}, R{-DCO}(150|'-97|')=1.12 {I6}, R{-DCO}(127|'-97|')=1.01 {I6}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$R{-DCO}(150|'-127|')=1.08 {I18}, R{-DCO}(150|'-97|')=1.08 {I14}, R{-DCO}(127|'-97|')=0.94 {I12}, DCO gate=L, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.98 {I10}, R{-DCO}(150|'-97|')=0.63 {I6}, R{-DCO}(127|'-97|')=0.81 {I7}, DCO gate=G, |DJ=2 
$R{-DCO}(150|'-127|')=0.98 {I6}, R{-DCO}(150|'-97|')=0.93 {I5}, R{-DCO}(127|'-97|')=0.95 {I5}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.74 {I15}, R{-DCO}(150|'-97|')=0.57 {I9}, R{-DCO}(127|'-97|')=0.79 {I14}, DCO gate=G, |DJ=2 
$R{-DCO}(150|'-127|')=1.01 {I10}, R{-DCO}(150|'-97|')=0.92 {I7}, R{-DCO}(127|'-97|')=0.98 {I8}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.21 {I38}, R{-DCO}(150|'-97|')=1.48 {I26}, R{-DCO}(127|'-97|')=1.69 {I31}, DCO gate=I, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.02 {I7}, R{-DCO}(150|'-97|')=1.17 {I7}, R{-DCO}(127|'-97|')=1.13 {I7}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.80 {I18}, R{-DCO}(150|'-97|')=0.81 {I12}, R{-DCO}(127|'-97|')=0.83 {I16}, DCO gate=N, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.22 {I19}, R{-DCO}(150|'-97|')=2.01 {I28}, R{-DCO}(127|'-97|')=1.08 {I14}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.30 {I30}, R{-DCO}(150|'-97|')=1.92 {I33}, R{-DCO}(127|'-97|')=1.72 {I33}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$R{-DCO}(150|'-127|')=0.94 {I37}, R{-DCO}(150|'-97|')=0.99 {I27}, R{-DCO}(127|'-97|')=0.85 {I24}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.23 {I55}, R{-DCO}(150|'-97|')=1.27 {I25}, R{-DCO}(127|'-97|')=1.39 {I30}, DCO gate=M, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.89 {I21}, R{-DCO}(150|'-97|')=0.79 {I14}, R{-DCO}(127|'-97|')=0.77 {I16}, DCO gate=G, |DJ=2 
$R{-DCO}(150|'-127|')=1.00 {I7}, R{-DCO}(150|'-97|')=1.15 {I7}, R{-DCO}(127|'-97|')=1.04 {I6}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.95 {I7}, R{-DCO}(150|'-97|')=1.02 {I7}, R{-DCO}(127|'-97|')=1.01 {I7}, DCO gate=N, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$R{-DCO}(150|'-127|')=0.87 {I14}, R{-DCO}(150|'-97|')=0.88 {I9}, R{-DCO}(127|'-97|')=0.84 {I9}, DCO gate=N, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=1.08 {I16}, R{-DCO}(150|'-97|')=1.84 {I22}, R{-DCO}(127|'-97|')=1.36 {I18}, DCO gate=H, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$R{-DCO}(150|'-127|')=0.99 {I19}, R{-DCO}(150|'-97|')=1.02 {I18}, R{-DCO}(127|'-97|')=1.10 {I23}, DCO gate=J, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.90 {I9}, R{-DCO}(150|'-97|')=1.09 {I9}, R{-DCO}(127|'-97|')=1.07 {I10}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.94 {I7}, R{-DCO}(150|'-97|')=1.12 {I7}, R{-DCO}(127|'-97|')=1.19 {I7}, DCO gate=H, |DJ=1 
$R{-DCO}(150|'-127|')=0.93 {I10}, R{-DCO}(150|'-97|')=0.74 {I7}, R{-DCO}(127|'-97|')=0.85 {I8}, DCO gate=G, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$R{-DCO}(150|'-127|')=1.15 {I37}, R{-DCO}(150|'-97|')=1.80 {I52}, R{-DCO}(127|'-97|')=1.67 {I47}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.04 {I10}, R{-DCO}(150|'-97|')=1.08 {I8}, R{-DCO}(127|'-97|')=1.03 {I8}, DCO gate=N, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E1
decay_comment:
$R{-DCO}(150|'-127|')=0.78 {I22}, R{-DCO}(150|'-97|')=0.66 {I15}, R{-DCO}(127|'-97|')=0.78 {I19}, DCO gate=J, |DJ=2 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
$R{-DCO}(150|'-127|')=1.43 {I45}, R{-DCO}(150|'-97|')=1.80 {I52}, R{-DCO}(127|'-97|')=1.29 {I35}, DCO gate=K, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=0.93 {I16}, R{-DCO}(150|'-97|')=1.22 {I17}, R{-DCO}(127|'-97|')=0.99 {I12}, DCO gate=N, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
$R{-DCO}(150|'-127|')=1.04 {I13}, R{-DCO}(150|'-97|')=1.19 {I13}, R{-DCO}(127|'-97|')=1.19 {I14}, DCO gate=N, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$R{-DCO}(150|'-127|')=1.10 {I32}, R{-DCO}(150|'-97|')=0.99 {I18}, R{-DCO}(127|'-97|')=0.93 {I14}, DCO gate=N, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
$R{-DCO}(150|'-127|')=0.93 {I20}, R{-DCO}(150|'-97|')=1.03 {I16}, R{-DCO}(127|'-97|')=0.97 {I15}, DCO gate=N, |DJ=1 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E weighted average of values from {+55}Co |e decay, (p,n|g), and (n,2n|g). 
M from |DJ|p, recommended upper limits, and |a(K)exp 
MR from |a(K)exp 
$|a(K)exp=0.0013 {I4} (1966Fi06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E weighted average of values from {+55}Co decay, (|a,n|g), (p,n|g), (n,2n|g), and (HI,xn|g). 
MR weighted average of +0.32 {I2} (|a,n|g) and +0.40 {I3} ({+55}Co decay). Other: |+0.4 {I2} (HI,xn|g). 
$|a(K)exp=0.000164 {I18} (1966Fi06) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
$|a(K)exp=0.000073 {I5} (1966Fi06) 
M based on the study of 1408|g distribution following decay from polarized and aligned {+55}Co. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
$|a(K)exp=0.00022 {I4} (1966Fi06) 
MR other: -0.21 {I+28-20} or -2.15 {I+75-85} (p,n|g), -0.13 {I8} (HI,xn|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E in (HI,xn|g), 1981Fr08 indicate that the 847|g, which is known as the transition to g.s. in {+56}Fe, could not be attributed to their coincidence spectra. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E in (HI,xn|g), 1981Fr08 indicate that 847|g, which is known as the transition to g.s. in {+56}Fe, could not be attributed to their coincidence spectra. Same as 847|g above. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
ce(L)+ce(M)=0.0000008 {I4} 
1966Fi06 pointed out 520|g's |a(K)exp was roughly by estimated value (the 520|g was not resolved from the 511|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
ce(L)+ce(M)=0.0000137 {I10} 
MR weighted average from +0.37 {I4} (1961Ch12) and +0.42 {I4} (1968Sa15). Other: +0.36 {I11} (1960Ba20). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
ce(L)+ce(M)=0.0000156 {I8} 
M 1966Fi06 estimated M1+(9-33%)E2. 
MR -0.04 {I1} or -4.1 {I2} (1973Ca06). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M predicted linear polarization=+0.45 to +0.75 exp=+0.54 {I12}(1972Sa38). 
A2=+0.330 6, A4=-0.063 6 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from 1975Ro28 based on branching ratio of 92, 477, and 1408. 
E the uncertainty is estimated by evaluator. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M predicted linear polarization=+0.40 to +0.75 exp=+0.53 {I15}(1972Sa38). 
A2=+0.355 3, A4=-0.093 3 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
RI value is 10 for sum of two 917.4 transitions. 
A2=-0.197 28, A4=-0.035 41. A2 VALUE APPLIES TO BOTH 917.4 TRANSITIONS. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR from 1985Av04. Others: -0.21 {I+28-20} or -2.15 {I+90-85} (1971Ro01); -0.19 or -2.75 (1970Pi04). 
A2=-0.54 5, A4=0.04 6 (1970Pi04 EP=3.40 MEV); A2=-0.30 5, A4=0.00 5 (1970Pi04 EP=3.50 MEV). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
A2=0.39 5, A4=0.03 6 (1970Pi04 EP=3.50); A2=0.22 2, A4=-0.01 2 (1971Ro01 EP=4.10 MEV); A2=0.19 3, A4=-0.02 3 (1971Ro01 EP=4.35 MEV). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR 0.00 {I16} or |d<-11 (1971Ro01). 
A2=0.30 3, A4=-0.09 4 (1971Ro01 EP=4.10 MEV); A2=0.06 5, A4=0.02 6 (1971Ro01 EP=4.35 MEV). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR 0.00 {I19} or |d<-3.7 if J=11/2; +5.65>|d>+0.36 if J=9/2 (1971Ro01). 
A2=0.38 6, A4=-0.18 8 (1971Ro01 EP=4.35 MEV). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI %Branching=5.4 {I21} from B(E2)=0.0037 {I10} (e,e') and adopted T{-1/2}; %Branching=5 {I3} in {+56}Fe(p,p'|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1(+E2)
decay_comment:
MR from 1038-1238 cascade (1980Sh28). Others: 0.00 {I4} from 1038-(1238)-847 cascade (1980Sh28), -0.02 {I2} (1974Ho25), +0.01 {I4} (1971Ag04), +0.02 {I2} (1971Ta18), -0.003 {I10} (1986Br01). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR others: -0.12 {I5} (1980Sh28), -0.136 {I13} (1974Ho25), -0.11 {I2} (1971Ta18), -0.11 {I2} (1971Ag04), -0.116 {I+13-12} (1984Oh03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR others: -0.27 {I+5-4} (1980Sh28), -0.266 {I16} (1974Ho25), -0.28 {I3} (1971Ta18), -0.278 {I11} (1971Ag04). -0.27 {I+9-12} (1984Oh03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR others: 0.00 {I3} (1980Sh28), 0.00 {I2} (1980Sh28), -0.01 {I1} (1974Ho25), -0.02 {I1} (1971Ta18), -0.023 {I8} (1971Ag04), -0.022 {I+5-6} (1984Oh03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR others: +0.23 {I7} or +8.6 {I+10-31} (1984Oh03), +0.163 {I54} (74h025), +0.22 {I7} (1980Sh28), +0.19 {I6} (1971Ag04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR others: +0.43 {I6} (1974Ho25), +0.51 {I6} (1971Ag04), +0.46 {I9} (1980Sh28), +0.524 {I+20-19} (1984Oh03). 


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 others: +1.17 {I42} or -0.09 {I18} (1971Ag04), +0.12 {I1} (1980Sh28), +0.15 {I11} (1974Ho25). +0.077 {I+81-64} (1984Oh03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR others: 0.37 {I6} or 1.56 {I20} (1974Ho25), +0.41 {I6} or +1.63 {I20} (1971Ag04), +0.430 {I21} (1984Oh03). 


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 others: +0.41 {I+7-8} or -0.33 {I9} (1980Sh28), -1,70 {I+26-33} (74h025), +1.6 {I3} or -0.25 {I10} (1971Ag04). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E weighted average of values of 1988Wa26 and 1979He19. 
MR others: -2.0 {I+6-10} 0R 0.30 {I+19-15} (74h025), +2.6 {I+20-10} or -0.5 {I2} (1971Ag04), -2.8 {I+13-11} (1984Oh03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR others: -0.18 {I14} or >6.7 (74h025), -0.26 {I20} or <-3.7 (1971Ag04), -0.228 {I+46-42} (1984Oh03). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
R=0.90 {i2} (2000Ap03) 
A{-2}=+0.15 {I2}, A{-4}=-0.06 {I4} (1974Po15). 
A{-2}=+0.30 {I3}, A{-4}=-0.06 {I4} (1977Be27). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
R=1.17 {I2} (2000Ap03) 
A{-2}=+0.20 {I2}, A{-4}=-0.06 {I2} (1974Po15). 
A{-2}=+0.32 {I3}, A{-4}=-0.03 {I3} (1977Be27). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=LT
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
A{-2}=+0.23 {I3}, A{-4}=-0.08 {I3} (1974Po15) 
A{-2}=+0.32 {I3}, A{-4}=-0.06 {I3} (1977Be27) 
R=1.12 {I2} (2000Ap03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
A{-2}=-0.14 {I6}, A{-4}=-0.01 {I6} (1974Po15). 
A{-2}=0.32 {I3}, A{-4}=-0.02 {I3} (1977Be27). 
R=1.09 {I10} (2000Ap03) 


decay_energy_unit: KEV
decay_comment:
RI$The authors indicated that transitions in {+56}Fe and {+27}Al are too close to deduce |g-ray yield 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$847|g(|q) results quoted from D.L. Smith, Report ANL/NDM-20, Argonne National Laboratory (1976): 
$A{-2}=+0.521 {I30}, A{-4}=-0.511 {I33} at E(n)=0.93 MeV; deduced W(125|')=1.193 {I13} 
$A{-2}=+0.539 {I13}, A{-4}=-0.302 {I14} at E(n)=0.98 MeV; deduced W(125|')=1.113 {I5} 
$A{-2}=+0.435 {I17}, A{-4}=-0.144 {I19} at E(n)=1.08 MeV; deduced W(125|')=1.053 {I7} 
$A{-2}=+0.398 {I39}, A{-4}=-0.331 {I44} at E(n)=1.18 MeV; deduced W(125|')=1.125 {I17} 
$A{-2}=+0.312 {I31}, A{-4}=+0.020 {I4} at E(n)=1.28 MeV; deduced W(125|')=0.990 {I2} 
$A{-2}=+0.396 {I18}, A{-4}=+0.039 {I20} at E(n)=1.38 MeV; deduced W(125|')=0.982 {I8} 
$A{-2}=+0.319 {I22}, A{-4}=-0.167 {I25} at E(n)=1.59 MeV; deduced W(125|')=1.062 {I10} 
$A{-2}=+0.226 {I12}, A{-4}=-0.155 {I15} at E(n)=1.68 MeV; deduced W(125|')=1.058 {I6} 
$A{-2}=+0.216 {I10}, A{-4}=-0.082 {I13} at E(n)=1.79 MeV; deduced W(125|')=1.030 {I5} 
$A{-2}=+0.245 {I31}, A{-4}=-0.089 {I36} at E(n)=1.85 MeV; deduced W(125|')=1.033 {I14} 
$A{-2}=+0.190 {I18}, A{-4}=-0.023 {I21} at E(n)=2.03 MeV; deduced W(125|')=1.008 {I8} 


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 
M from |G and adopted J|p. See also 1984Pl05. 
MR from T{-1/2}, B(E2)|^, E|g, and |a 
KC FROM EKC IN EC DECAY. 
LC,MC+ FROM EKC AND K:L:M+ IN EC DECAY. CONSISTENT WITH VALUES OBTAINED FROM CC AND K:L:M+. 
BE2W from adopted B(E2)|^ and J 


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:
KC,LC,MC+ KC FROM EKC; LC,MC+ FROM CC, K/L+, AND L/M+ (10% UNCERTAINTY ASSUMED IN L/M+ BY EVALUATORS) IN EC DECAY 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M D+Q from |g(|q) in Coul. ex. and |e decay; and |DJ|p 
MR weighted average of |g(|q) in Coul. ex. and |e. Other |d's excluded by comparison to RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2(+M3)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
RI intensity ratios for these three gammas from (n,n'|g) do not agree with results from (|a,pn|g) indicating that a different level is being populated in (n,n'|g) compared to other reactions. 
MR from (n,n'|g) 
M Q(+O) from |g(|q) in (n,n'|g); E2(+M3) from RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_uncertain: S
decay_comment:
K/T,L/T,M+/T$FROM EC DECAY 
E from |e decay 
RI from deduced I(|g+ce) and |a from adopted gammas; uncertainty given from I(|g+ce) and |a only; does not include uncertainty in I|g normalization. 
TI deduced from decay scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI 1974Ti01 noted that their measurement of I|g(122|g)/I|g(136|g)=7.23 {i29} agreed with the branching ratio from |e decay (1971Ko19), but differed from that of 1969Wa12, where I|g(122|g)/I|g(136|g)=8.70 {i8}. The branching ratio in the adopted gammas agrees with 1969Wa12. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
KC,LC,MC+ KC FROM EKC; LC,MC+ FROM CC, K/L+, AND L/M+ (10% UNCERTAINTY ASSUMED IN L/M+ BY EVALUATORS) 
$K:L:M+=100:9.0:1.5 (1955Co31) 
See summary in comments above 
M,MR 1996Me11 claim that E|g=122 keV is mostly E2 with a negligible M1 component based on their Ice data; this conclusion is not supported by other data. Their data are: K/L=9.04 {i19}; L1/L2=13.1 {i3}; L1/L3=8.7 {i5}; L1/M=9.7 {i10}; |a(L1)exp=2.04|*10{+-2} {i6}; |a(L2)exp=1.56|*10{+-3} {i9}; |a(L3)exp=2.34|*10{+-3} {i21} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
KC,LC+ KC FROM EKC; LC+, UNWEIGHTED AV FROM LC+(K/LC++1)=CC AND (KC+L+)/K=K+/K 
$|a/K=1.118 {I5} (1967Ha06) 
See summary in comments above 
M,MR 1996Me11 claim that the relative weight of the E2 component for the E|g=136 keV is: 83% {I+8-12}; this conclusion is not supported by other data. Their data are: K/L=8.68 {i27}; L1/L2=12.2 {i16}; L1/L3=9.0 {i18}; L1/M=7.9 {i22}; |a(L1)exp=1.2|*10{+-2} {i3}; |a(L2)exp=1.0|*10{+-3} {i4}; |a(L3)exp=1.4|*10{+-3} {i6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
Not observed by 1965Ma38 or clearly seen by 1965Sp06 
MR -0.186<|d<-0.072 or -6.99<|d<-2.38 (1975Co22) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR -25|<|d|<-9 or -0.4|<|d|<-0.3 (1975Ta09). Shell model favors smaller value (see footnote on 1627 level) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
MR -10|<|d|<-5.5 or +0.35|<|d|<+0.45 (1975Ta09). CP (1978Ve06) show that |d=+0.40 {i5} is preferred 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E from the energy difference of initial and final levels; E|g=1351.8 {i10} (1980Ve05) which the evaluator feels must be a typographical error 


decay_energy_unit: KEV
decay_comment:
(M2+M3)/M1,N1/M1$from 1979Sa32 ({+57}Fe in Au; iron-free spectrometer). See also 1976Sh30, 1973Sh01, and 1972Fu08; these measurements show chemical effects on the outer-shell ratios and spectral shapes 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
M,MR from |g|g(|q,h) (1963De04, NaI). |d=-2.580 {i24} less likely since it would give too large an E2 transition probability. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
Not observed due to experimental limitations. 1971Ba10 suggest that I|g would be weak since |S(isotope formation)=72.2% {i57}. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$Deduced |s(352|g)=0.2848 b {I15} from average of 0.2844 b {I19} with reference to |s(2223|g)=0.3325 b {I7} in {+1}H(n,|g), and 0.2858 b {I26} with reference to |s(841|g)=0.353 b {I2} in {+32}S(n,|g) (2017Fi03) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$this |g has interference from intense 4462 gamma. Energy is not listed in Table II of 2017Fi03, value given here is from level-energy difference 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$level-energy difference=5920.73 
E,RI$5920.20 and 5922.7 form a doublet, intensity divided on the basis of the intensity balance. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$from unweighted average of branching ratio at all measured energies. Other: 12.29 {I21} from weighted average. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$from unweighted average of branching ratio at all measured energies. Other: 14.3 {I2} from weighted average. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M,MR D+Q from |g|g(|q), |g(|q), RUL 
MR from {+58}Co |e decay. Others: -0.57 {I6} (n,|g), -0.50 {I5} (n,n'|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M from |g(|q) in (n,n'|g) and RUL 
MR from (n,n'|g). Other: +6.3 in (|a,p|g); mult=Q in ({+13}C,3n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
$I|g(2876)/I|g(1674)=0.07 {I9} in (|m{+-}n|g) is in severe disagreement with adopted ratio of 1.5 {I6} 
MR from (n,|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
$B(E2)(W.u.)=1000 {I+107-330} is larger than RUL by a factor of 2 to 4. This suggests that either the reported T{-1/2} is too small or branching is too large. Note that this |g is not reported in (|a,p|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
Observation of the 1446|g would lead one to expect 2855|g and 4531|g populating 1675 and g.s., respectively 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
Calibration energy. See 1974Ti01. Note that from {+58}Co decay, this energy is 810.7593 {I29} (2000He14 evaluation) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
M |a(K)exp=3.0|*10{+-4} {I1}, K/(L+M)=8 {I1}, |a=3.4|*10{+-4} {I1} (1962Fr13). Other: K/L=11.8 (1962Ma33) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI from weighted average of 0.77 {I4} (Hill, report BNWL-S(|a)-315, 1965), 0.81 {I3} (1968Ri03), 0.70 {I2} (1972DyZY), 0.645 {I15} (1973Ba67), 0.69 {I2} (Denecke as quoted in 1973Ba67), 0.69 {I2} [Legrand et al., Atomic Energy Review 11 (1973) 524], 0.74 {I4} (1974HeYW), and 0.682 {I17} (1982Gr10). The internal uncertainty is 0.008, the reduced-|h{+2} is 4.4, and the external uncertainty 0.016. 
M |a(K)exp=0.00024 {I4} (1962Ma33) 
MR from |g|g(|q) and |g(|q,t) (1972Fo05) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI from weighted average of 0.68 {I5} (Hill, report BNWL-S(|a)-315, 1965), 0.57 {I3} (1968Ri03), 0.49 {I3} (1972DyZY), 0.506 {I15} (1973Ba67), 0.527 {I15} (Denecke as quoted in 1973Ba67), 0.525 {I13} [Legrand et al., Atomic Energy Review 11, 524 (1973)], 0.54 {I4} (1974HeYW), and 0.511 {I15} (1982Gr10). The internal uncertainty is 0.007, the reduced |h{+2} is 2.2, and the external uncertainty 0.01. 
$ 1969DyZX SUPERSEDED BY 1972DyZY 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
RI$from 1978Na06. Other: 1.5 {I2} (2000ApZW), probably used as a gating transition for obtaining intensities of other |g rays. 
A{-2}=+0.19 {I2}, A{-4}=-0.06 {I2}. DCO=1.01 {i5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_mixing_ratio_info: ;ERR=?
decay_comment:
$DCO=1.0 {I3}, 0.40 {I20}; the latter with gate on |DJ=1 |g 
E$authors' |DE|g=0.04 seems a misprint 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR -0.37 {I+5-7} (1989Co01) 
$(864|g)(810|g)(|q): A{-2}=+0.479 {I9}, A{-4}=+0.081 {I13} 
$(864|g)(810|g)(|q): B{-2}=-0.75 {I3}, B{-4}=-0.08 {I2} (1989Co01) 
E$ tentative placement by 1969Fa05 from 5414 to 4550 level is not adopted by the evaluators 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$ intensity divided by the evaluators based on branching ratio in adopted gammas. Total I|g=17.6 {I12} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M from |g|g(|q) (1989Co01) 
$(1446|g)(810|g)(|q): A{-2}=+0.351 {I18}, A{-4}=+1.17 {I4} 
$(1446|g)(810|g)(|q): B{-2}=-0.58 {I12}, B{-4}=-1.08 {I10} (1989Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$(1107|g)[864|g](810|g)(|q): A{-2}=+0.02 {I3}, A{-4}=+0.01 {I4} 
$(1107|g)(1674|g)(|q): A{-2}=-0.04 {I4}, A{-4}=+0.02 {I5} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR -0.16 {I+4-5} (1989Co01) 
$(1971|g)(810|g)(|q): A{-2}=-0.05 {I5}, A{-4}=-0.05 {I6} 
$(1971|g)(810|g)(|q): B{-2}=+0.10 {I8}, B{-4}=+0.09 {I7} (1989Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR -0.22 {I+10-13} (1989Co01) 
$(2066|g)(810|g)(|q): A{-2}=+0.44 {I4}, A{-4}=-0.04 {I5} 
$(2066|g)(810|g)(|q): B{-2}=+0.65 {I9}, B{-4}=+0.15 {I7} (1989Co01) 
E$ tentative placement also suggested by 1969Fa05 from 4322 level but not adopted by the evaluators 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+(Q)
decay_comment:
$(2273|g)(810|g)(|q): A{-2}=+0.287 {I11}, A{-4}=-0.002 {I18} 
$(2273|g)(810|g)(|q): B{-2}=-0.44 {I8}, B{-4}=+0.01 {I5} (1989Co01) 
MR -0.02 {I7} (1989Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(2433|g)(810|g)(|q): A{-2}=+0.43 {I7}, A{-4}=+0.9 {I3} consistent with 0->2->0 cascade with mult=Q for each transition 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR -0.42 {I7} (1989Co01) 
$(2726|g)(810|g)(|q): A{-2}=+0.35 {I5}, A{-4}=-0.16 {I5} 
$(2726|g)(810|g)(|q): B{-2}=-0.35 {I11}, B{-4}=+0.02 {I8} (1989Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR +0.04 {I14} (1989Co01) 
$(1674|g)(2066|g)(|q): A{-2}=-0.06 {I3}, A{-4}=-0.01 {I4} 
$(1674|g)[2066|g](810|g)(|q): A{-2}=-0.16 {I4}, A{-4}=-0.02 {I5} 
$(1674G)[2066G](810G)(THETA): A2=-0.19 4, A4=+0.02 5 
$(1674|g)[2066|g](810|g)(|q): B{-2}=+0.49 {I24}, B{-4}=-0.16 {I21} (1989Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
MR -0.19 +24 -27 (1989Co01) 
$(2876|g)[864|g](810|g)(|q): A{-2}=+0.02 {I4}, A{-4}=+0.01 {I5} 
$(2876|g)(1674|g)(|q): A{-2}=+0.10 {I5}, A{-4}=-0.06 {I6} 
$(2876|g)[864](810|g)(|q): B{-2}=+0.05 {I46}, B{-4}=-0.11 {I24} (1989Co01) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+(Q)
decay_comment:
$(3326|g)(864|g)(810|g)(|q): A{-2}=-0.03 {I5}, A{-4}=+0.01 {I6} 
$(3326|g)(1674|g)(|q): A{-2}=-0.22 {I5}, A{-4}=-0.05 {I6} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(6506|g)(1862|g)(|q): A{-2}=-0.16 {I3}, A{-4}=+0.02 {I5} 
$(6506|g)(2726|g)(|q): A{-2}=-0.16 {I3}, A{-4}=0.00 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(7262|g)[1107|g](1674|g)(|q): A{-2}=-0.155 {I25}, A{-4}=-0.01 {I5} 
$(7262|g)(1107|g)(|q): A{-2}=-0.048 {I24}, A{-4}=+0.02 {I5} 
$(7262|g)(1971|g)(|q): A{-2}=-0.03 {I3}, A{-4}=-0.01 {I3} 
$(7262|g)(2782|g)(|q): A{-2}=+0.32 {I10}, A{-4}=+0.01 {I8} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$(8370|g)(1674|g)(|q): A{-2}=-0.241 {I16}, A{-4}=-0.006 {I20} 
$(8370|g)[864|g](810|g)(|q): A{-2}=-0.072 {I19}, A{-4}=+0.005 {I6} 
$(8370|g)(864|g)(|q): A{-2}=+0.056 {I23}, A{-4}=+0.002 {I12} 
$(8370|g)(864|g+810|g)(|q): A{-2}=+0.002 {I7}, A{-4}=-0.001 {I14} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$R{-180|'/90|'}=1.44 {I2} 
$DCO{+(d)}=1.70 {I3} 
$ DCO{+(d)}=1.83 {I8} with gate at 498|g, 1.74 {i4} for gate at 623|g 1.76 {I6} for gate at 761|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
$R{-180|'/90|'}=0.81 {I2} Y 
$ DCO{+(d)}=0.96 {I5} with gate at 498|g, 0.88 {i3} for gate at 623|g 0.88 {I3} for gate at 761|g 
M$ Compilers note: sign of A{-4} is inconsistent with |DJ=1 assignment 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_comment:
$The 811-keV |g is dominantly contributed by the decay of the the ground state of {+58}Cu, thus its intensity from isomer decay could not be extracted. The intensity of 811|g from the isomer decay should be the same as that for the 1266|g 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E Weighted average of data from |b{+-} decay, ({+15}N,3np|g), ({+18}O,3n|a|g) and ({+48}Ca,2n|g). 
|d(D,Q)=-0.02 {I4} or -3.8 {I6} in ({+18}O,3n|a|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
E$Other value 1425.5 {i6} - ({+15}N,3np|g), ({+18}O,3n|a|g). 
M$Other: (D) in ({+15}N,3np|g), ({+18}O,3n|a|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
RI from weighted average of 12.9 {I10} (1977Pa18) and 11.0 {I14} (2001Oi02). Uncertainty lowest input value. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from weighted average of 4.5 {I13} (1977Pa18) and 3.7 {I6} (2001Oi02). Uncertainty lowest input value. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI from weighted average of 6.7 {I8} (1977Pa18) and 6.9 {I10} (2001Oi02). Uncertainty lowest input value. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E,RI$From 2017FiZZ. I|g scaled with respect to I|g(287.03|g)=59 of this dataset. The 568.52- and 570.84-keV doublet has been resolved. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$Transition is indicative of a quadrupole nature. However, |g-ray must facilitate |DJ=1, an argument supported by A{-2} coefficient approaches the upper limit of that of a highly mixed 11/2 to 9/2 transition. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$Weighted average of 16.4 {I8} (2010Ho13) and 13.9 {I13} (1978No03). 
$(1291|g)(824|g)(|q): A{-2}=+0.17 {I7}, A{-4}=+0.05 {I9} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1
decay_comment:
RI$Weighted average of 13.8 {I7} (2010Ho13) and 14.6 {I14} (1978No03). 
$(1476|g)(824|g)(|q): A{-2}=-0.18 {I7}, A{-4}=+0.4 {I1} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$Weighted average of 17.4 {I12} (2010Ho13) and 17.6 {I20} (1978No03). 
M$E2 from |DJ|p not consistent with |b{+-} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_comment:
RI$Weighted average of 67.2 {I34} (2010Ho13) and 71.1 {I36} (1978No03). 
$(1969|g)(824|g)(|q): A{-2}=-0.22 {I4}, A{-4}=-0.02 {I5} 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
$(654.8|g)(207.0|g)(|q): A{-2}=-0.03 {i4}, A{-4}=+0.07 {i5} consistent with quadrupole-dipole cascade 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
$(788.5|g)(654.8|g)(|q): A{-2}=+0.18 {i4}, A{-4}=+0.05 {i6} consistent with quadrupole-quadrupole cascade 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
$(1342.3|g)(788.5|g)(|q): A{-2}=+0.12 {i11}, A{-4}=0.00 {i16} consistent with quadrupole-quadrupole cascade 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
M$|g|g(|q) consistent with 4 -> 2 -> 0, Q(|b{+-})Q cascade; E2 in 2010Ho13 
$E|g=1299.0 {I4}, I|g=28 {I9} (1983Ru06) 
$(1299|g)(877|g)(|q): A{-2}=+0.06 {I7}, A{-4}=+0.10 {I10} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D
decay_comment:
M$|g|g(|q) consistent with 3 -> 2 -> 0, D-Q cascade; M1 in 2010Ho13 
$(1814|g)(877|g)(|q): A{-2}=-0.38 {I9}, A{-4}=-0.14 {I12} 
$E|g=1815.0 {I6}, I|g=23 {I8} (1983Ru06) placed from 3634 to 1820 level; latter level is no longer included in the present level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
M$|g|g|g(|q) consistent with 4 -> 3 -> 2 -> 0, D-D-Q cascade; M1 in 2010Ho13 
$(942|g)[1814|g](877|g)(|q): A{-2}=+0.23 {I7}, A{-4}=0.00 {I11} 
M$(M1) in 2010Ho13 
$E|g=942.1 {I4}, I|g=29 {I8} (1983Ru06) placed from 1820 to 877 level; former level is no longer included in the present level scheme 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI$relative to I|g=1520 {I40} and 2300 {I60} for the 311|g and 415|g in {+109}Ag target excitation, respectively. 8.1% uncertainty due to the background subtraction and additional uncertainty due to the relative efficiency correction were included in the given result. 
M$from Coulomb excitation 
$B(E2): 2015Ga38 give 14.0 W.u. {I+13-11} obtained from minimization of the 2D |h{+2} surface constrained by the T{-1/2} measurements in 2011Ro02 (Phys. Rev. Lett. 106, 022502) and 2010Lj01 (Phys. Rev. C 81, 061301) and 13 W.u. {I+4-3}, projecting the |h{+2} surface at Q=0. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 746.4 {I1} in |b{+-}n decay, 746.4 {I1} and 746.0 {I2} in {+238}U({+64}Ni,X|g) 
M$|DJ=2, Q from |g|g(|q) in {+238}U({+64}Ni,X|g); RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=GT;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W;ERR=GT
decay_comment:
E$weighted average of 1017.4 {I3} in |b{+-}n decay, 1016.7 {I1} and 1016.7 {I3} in {+238}U({+64}Ni,X|g) 
M$|DJ=2, Q from |g|g(|q) in {+238}U({+64}Ni,X|g); RUL 


decay_energy_unit: KEV
decay_multipolarity: Q
decay_comment:
$E|g=746.4 {I1}, I|g not given (2006Ho20) 
$E|g=746.0 {I2}, I|g=100 {I8} (2007Lu13) 
$(746|g)(1017|g gate)(|q): A{-2}=+0.14 {I3}, A{-4}=+0.01 {I4} (2006Ho20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$E|g=1016.7 {I1}, I|g=100 (2006Ho20) 
$E|g=1016.7 {I3}, I|g=79 {I9} (2007Lu13) 
$(1017|g)(746|g gate)(|q): A{-2}=+0.14 {I3}, A{-4}=-0.09 {I3} (2006Ho20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
$E|g=1077.8 {I2}, I|g=12 {I3} (2006Ho20) 
$(1078|g)(1017|g gate)(|q): A{-2}=-0.13 {I6}, A{-4}=+0.22 {I8} (2006Ho20) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$E|g=1078.9 {I3}, I|g=50 {I7} (2006Ho20) 
$E|g=1077.5 {I4}, I|g=54 {I7} (2007Lu13); note that 1078|g is a doublet in 2006Ho20, but only one line is listed in 2007Lu13 
$(1079|g)(1017|g gate)(|q): A{-2}=+0.31 {I5}, A{-4}=-0.11 {I7} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: Q
decay_comment:
$E|g=781.0 {I1}, I|g=30 {I2} (2006Ho20) 
$E|g=781.3 {I4}, I|g=16 {I3} (2007Lu13) 
$(781|g)(1017|g+1079|g gate)(|q): A{-2}=+0.11 {I3}, A{-4}=-0.06 {I5} (2006Ho20) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_multipolarity: [M4]
decay_uncertain: ?
decay_comment:
E,RI$ 393.7|g with implied M4 multipolarity is not seen, upper limit of intensity established by 2013Ol06 as <0.15 relative to 100 for 363.7|g 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
E,RI$ 397.6|g with implied M2 multipolarity is not seen, upper limit of intensity established by 2013Ol06 as <0.15 relative to 100 for 363.7|g 


decay_energy_unit: KEV
decay_comment:
E$Weighted average of 574.7 keV 10 (2007Lu13), 571 keV 6 (2008Ad04), and 567 keV 6 (2008Ad04). Other value: 573 keV (1999Ha05). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$ assignment based on |g-ray peak observed in prompt |b-|g spectrum (2011Da08) 
RI$ absolute intensity>10 {I5} (2011Da08) 


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:
$For T{-1/2}(573 level)=33 ps {I23}, B(E2)(W.u.)=15 {I11} (2017Ol08). Compiler obtains B(E2)(W.u.)=15 {I+35-6} using upper and lower limits for level half-life 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI$uncertainty of 0.1 in Table 1 of 2017Ol08 is probably a misprint as it seems too low to be realistic in view of uncertainties for other |g-ray intensities. Compiler assigns 1.0 
$If E2, B(E2)(W.u.)>0.13 (2017Ol08) 
$If M1, B(M1)(W.u.)>1.9|*10{+-4} (2017Ol08) 


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:
$Compiler obtains B(M1)(W.u.)=1.8|*10{+-5} {I+20-6} using upper and lower limits for level half-life 


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:
$Compiler obtains B(M1)(W.u.)=2.8|*10{+-5} {I+32-10} using upper and lower limits for level half-life 


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:
$Compiler obtains B(M1)(W.u.)=3.8|*10{+-5} {I+42-13} using upper and lower limits for level half-life 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3
decay_BM_unit: mu^2 x (fm)^4
decay_BM_info: ;TYPE=BM3;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM3W
decay_comment:
E from {+58}Co IT decay 
$|d(E4/M3)<0.009 from |d{+2}=2.7|*10{+-5} {I55} (deduced in 2006Ra03 evaluation from measured subshell ratios). See IT decay dataset 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR$-0.33 {I6} or -2.3 {I4} from |g(|q) data in (d,n|g). However, comparison of experimental and theoretical cross sections and isomer ratios from {+58}Ni(n,p) and {+59}Co(n,2n) reactions over incident neutron energy range of 0.97 to 20.35 MeV (1999Av04, 2004Se01, and 2015HoZZ) support |d(E2/M1)=2.3 over 0.33 


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 weighted average of I|g(28)/I|g(53)=0.40 {I3} (|a,n|g), 0.62 {I12} (d,n|g), and 0.56 {I8} (p,|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1(+E2))
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
MR other: -0.04 {I2} (1972Ha61) in (p,n|g) 
RI I|g(112)/I|g(58)=1.59 {I14} which is a weighted average of 1.72 {I21} (|a,n|g) and 1.50 {I18} (p,n|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
RI branching from 1971Xe01 in (|a,n|g). 1971Ro08 in (|a,n|g) report 25.2 {I17}: 9.2 {I9}: 100 {I3} at 8 MeV and 29 {I6}: 27.8 {I9}: 100 {I3} at 10 MeV 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E4]
decay_uncertain: ?
decay_comment:
E$this transition to 373.9, 5+ level is seen only in (|a,n|g) and not in (p,|g) or ({+3}He,p|g). Its placement from this level is highly questionable in view of E4 required. Either the placement is wrong or it defines another level. Also the existence of another level could explain the different branching ratios in (|a,n|g) compared to (p,|g) or ({+3}He,p|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M3]
decay_uncertain: ?
decay_comment:
$In view of high and unlikely multipolarity of M3 implied for this transition, evaluators consider this placement, proposed only in (p,|g), uncertain 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3
decay_comment:
RI from I(|g+ce) and |a 
M L1/(L2+L3)=1.070 {I15}, M1/(M2+M3)=1.19 {I6}, L/M=6.62 {I13}, N1/M1=0.034 {I10} (1971Pl02); K/LM+=2.25 {I15} (1968Wi10), 2.0 {I+11-6} (1967St23), 1.9 {I2} (1950St22); |a(K)exp=1860 {I100} (based on average K| x ray/I(25|g)=722 {I26} (680 {I88} (1968Wi10), 710 {I50} (1967St23), 733 {I33} (1970Ca19)) and fluorescence yield 0.389 {I14}) 
$|d(E4/M3)<0.014 from |d{+2}<2|*10{+-4} (1971Pl02); <0.009 from |d{+2}=2.7|*10{+-5} {I55} (deduced in 2006Ra03 evaluation from measured subshell ratios listed above) 
E from 1971Pl02. Others: 24.87 {I4} (1970Ca19), 1954Ca18, 1950St22. See also 1967St23 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E4]
decay_uncertain: ?
decay_comment:
E$this transition to 373.9, 5+ seen only in (|a,n|g) is highly improbable, it is either a wrong placement or defines a separate level near this energy 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$|g assigned to {+55}Mn(|a,p|g){+58}Fe in 1971Ro08, by 1971Xe01 observed it in coincidence with neutrons 


decay_energy_unit: KEV
decay_uncertain: ?
decay_comment:
E$unassigned in 1975Er03, placed from 2478 level in 1970Er03 in the decay of 8396 level with 6% {I1} branching 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$ 5885 IN 1970Er03 IS A MISPRINT 
RI$ UNCERTAINTY INCREASED FROM 1 TO 2 (MINIMUM 5% AS SUGGESTED IN 2005Er07) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2+M1
decay_comment:
MR$-0.33 {I6} or -2.3 {I4} (1970Be33). However, comparison of experimental and theoretical cross sections and isomer ratios from {+58}Ni(n,p) and {+59}Co(n,2n) reactions over incident neutron energy range of 0.97 to 20.35 MeV (1999Av04, 2004Se01, and 2015HoZZ) support |d(E2/M1)=2.3 over 0.33 
CC$from Adopted Gammas for adopted E|g=28.30 {I15} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3(+E4)
decay_mixing_ratio_info: ;ERR=LT
decay_BM_unit: mu^2 x (fm)^4
decay_BM_info: ;TYPE=BM3;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM3W
decay_comment:
E$from {+58}Co Adopted Levels, Gammas dataset in the ENSDF database (October 2015 update). 
RI$measured absolute photon intensity (2019Mo11). This value can be compared with 0.0397 {I6} in evaluation by 2010Ne01: Nucl. Data Sheets 111, 897, where no E4 component was assumed. 
M,MR$M3 is known previously from measured subshell ratios. From measured absolute photon intensity of 24.9|g, 2019Mo11 deduced %E4<0.00063% or |d(E4/M3)<0.0251. Compiler obtains |d(E4/M3)=0.020 {I+14-20} or <0.034, using measured I|g=0.0387 {I16} by 2019Mo11, I(|g+ce)=100, and theoretical total conversion coefficients for M3 and E4 from BrIcc code. 
$Compiler's note: for RUL<100 for B(E4)(W.u.), compiler obtains %E4<4.4|*10{-6} or |d(E4/M3)<0.0021, i.e. the upper limit for |d should be about a factor of 10 smaller, or upper limit for %E4 a factor of 140 smaller. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E from |b{+-} decay; 1098.50 {I5} in (p,|g), 1099.4 {I2} in (|a,p|g). 
M from |a(exp) in {+59}Fe |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M D+Q from (|a,p|g); not E1+M2 from RUL. 
MR$From (|a,p|g). Others: 0.16 {I9} from (|g,|g), 0.0 {I6} 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 from |b{+-} decay. 
M From D+Q from |g|g(|q) and |a(exp) in {+59}Fe |b{+-} decay. 
MR From {+59}Fe |b{+-} decay 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
M,MR from |g|g(|q) in {+59}Fe |b{+-} decay; RUL disallows large solutions (+1.7 to +2.1). Other: -0.06 {I3} ({+59}Fe |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:
E Other: 334.56 {I7} in (p,|g) 
M D(+Q) from |g|g(|q) in {+59}Fe |b{+-} decay; Adopted |D|p=no. 
MR or -0.05 {I+3-7} from {+59}Fe |b{+-} decay. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E weighted average from ({+15}N,4n|g) and (|a,p|g). Other E|g: 1459.00 {I21} in (p,|g). 
M pure Q from (|a,p|g); not M2 from RUL. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_mixing_ratio_info: ;ERR=LT
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=GT;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W;ERR=GT
decay_comment:
E Weighted average from |b{+-} decay and (|a,p|g). Other E|g: 382.25 {I7} in (p,|g). 
M D+Q from (|a,p|g); adopted |D|p=no. 
MR from RUL; however, |d(D,Q)=-4 {I2} from (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E weighted average from |b{+-} decay and (|a,p|g). Other E|g: 1481.03 {I5} in (p,|g). 
M D+Q from (|a,p|g); adopted |D|p=no. 
MR from B(E2) in Coulomb excitation and adopted T{-1/2} and branching; sign from (|g,|g). Others: >-0.4 and <+0.1 from (|g,|g); -5 {I+2-5} from (|a,p|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E from (|a,p|g). Other E|g: 553.88 {I5} in (p,|g). 
M D(+Q) from (|a,p|g) with larger uncertainty in |d=+0.01 {I4}; adopted |D|p=no. 


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 (|a,p|g). Other E|g: 1743.85 {I7} in (p,|g). 
M D+Q from (|a,p|g); not E1+M2 from RUL. 
MR From (|a,p|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:
Other E|g: 795.43 {I6} in (p,|g). 
M D(+Q) from (|a,p|g) with larger uncertainty in |d=+0.04 {I9}, Adopted |D|p=(no). 
MR from (|a,p|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:
MR from (|a,p|g), if J(2087 level)=5/2. 
M D(+Q) from (|a,p|g) with larger uncertainty in |d=-0.07 {I14}; adopted |D|p=(no). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D(+Q)
decay_comment:
E weighted average from ({+15}N,4n|g) and (|a,p|g). 
MR -0.05 {I8} if J(2153 level)=9/2, +0.11 {I6} if J=13/2. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 56.5 {I15} (1973Pa16), 55.5 {I17} (1970Le03) 
I(1099|g)=56.5% {I9} assuming adopted normalization. 
M |a(exp)=1.36|*10{+-4} {I10} (1964Co34), 1.84|*10{+-4} {I27} (1953Hi02), |a(K)exp=1.61|*10{+-4} (1952Me53). 
M internal pair formation coefficient consistent with E2 theory (1970Sc19) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI 3.08 {I10} (1973Pa16), 2.95 {I8} (1970Le03) 
MR$From 192|g-1099|g(|q) assuming |d(Q,O)=0 for 1099|g (1973Pa16) in good agreement with +0.21 {I2} (1971Ar07). Other: -0.07 to +0.02 (1953Sc23). 
M |a(exp)=0.007 {I3} (1952Me53). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_comment:
RI 43.2 {I11} (1973Pa16), 44.1 {I12} (1970Le03) 
I(1292|g)=43.2% {I9} assuming adopted normalization. 
M |a(exp)=1.07|*10{+-4} {I8} (1964Co34), 1.06|*10{+-4} {I16} (1953Hi02), |a(K)exp=1.19|*10{+-4} 6 (1952Me53). Internal pair formation coefficient consistent with E2 theory (1970Sc19). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M1+E2
decay_comment:
RI 1.02 {I4} (1973Pa16), 0.98 {I4} (1970Le03) 
M$From |g|g(|q) (See data above with ref) and RUL in Adopted Gammas. 
MR (or +1.78 {I+15-20}) from 1971Ar07 (sign reversed by evaluator). Large solutions disallowed by RUL. Other values listed in previous evaluator (2002Ba42) by c.m. Baglin - current evaluator could not track source reference: -0.06 {I3} or +1.97 +16-15 from 142|g-192|g(|q) for adopted |d(192|g); -0.009 {I+8-16} or +1.77 +7-3 from 142|g-1292|g if |d(Q,O)=0 for 1292|g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1+E2)
decay_comment:
RI 0.27 {I1} (1973Pa16), 0.24 {I4} (1970Le03) 
M$From |g|g(|q) (See data above with ref) and RUL in Adopted Gammas. 
MR (or -0.05 {I+3-7}) from 1971Ar07 (sign reversed by evaluator). previous evaluator C. Baglin (2002Ba42) list -0.03 {I7} or +1.9 {I3} from 335|g-1099|g(|q) if |d(Q,O)=0 for 1099|g - source reference unknown. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: D+Q
decay_comment:
E |g forms doublet with {+59}Ni |g in 1974Mo02. 
MR weighted average of +0.25 {I5} (1970Co21) and +0.16 {I5} (1980Ha17). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
Placement shown as tentative because |g absent in other (n,n'|g) studies. E|g=891.8 from level energy difference. Not adopted - transition for |DJ=4 in Adopted Levels. 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI others: 82 (1982Ka29), 47 (1980Ab06), 123 {I9} (1979Ka34); inconsistent branching may indicate a complex |g. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_uncertain: ?
decay_comment:
|g placed by 1979Ka34; not confirmed in 1982Ka29, but |g with similar energy is reported from this level in (p,p'|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E 1680.82 {I7} (1982KaZL), 1681.07 {I14} (1979Ka34). 
RI from 1980Ab06; 133 in 1982Ka29. Could plausibly form a doublet with |g from 3141 level known from (p,|g). 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
E$|g-ray not adopted by the evaluator for spin-parity assignments in Adopted Levels, which yields a |DJ of 3 or more from 1/2+ to 2153.62 keV level with conflicting spin-parity assignments. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3+(E4)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
$%I|g=2.07 {I3}, %I(|g+ce)=99.75 {I3} 
RI$I|g is given at equilibrium of {+60m}Co(10.467 min) with {+60}Fe(2.62|*10{+6} y). 
E(|g),Mult.,|d,|a,I(|g+ce) from Adopted Levels, Gammas. 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: M3+(E4)
decay_mixing_ratio_info: ;ERR=LT
decay_comment:
%I|g=2.07 {I3} 
|a(K)=39.3, |a(L)=6.80, |a(M+..)=1.0 
|a(K)exp=39.0 {I19} (1989Mu15), 43.1 {I18} (1970Ca19). 
|a(K)exp/|a(L)exp=5.78 {I15}, |a(L)exp/|a(M)exp=7.53 {I18}, |a(L1)exp/|a(L23)exp=2.26 {I8} (1971Pl02). 
E from 1962Ha46, cryst. 
M,MR from |a(L1)exp/|a(L23)exp=2.26 {I8} (1971Pl02). 
$I(|g+ce)=99.75 {I3} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1285.7 {I3} in |b{+-} decay, 1284.5 {I6} in ({+48}Ca,p2n|g) and 1286.4 {I9} in ({+70}Zn,X|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
RI$deduced from p-|g-|g coin data 
$A{-2}=-0.16 {I12} for the unresolved doublet: 708.5 and 710.0 keV 
$I|g(135|')/I|g(90|')=0.89 {I8} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
$A{-2}=-0.16 {I12} for the unresolved doublet: 708.5 and 710.0 keV 
$I|g(135|')/I|g(90|')=0.89 {I8} 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 994.8 {I2} from {+63}Fe |b{+-} decay, 995.0 {I5} from ({+48}Ca,p2n|g), and 994.5 {I1} from (d,{+3}He|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (D)
decay_comment:
E$weighted average of 1382.6 {I10} from ({+48}Ca,p2n|g), 1381.9 {I8} from (d,{+3}He|g), and 1383.0 {I4} from ({+70}Zn,X|g) 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 499.6 {I3} from {+63}Fe |b{+-} decay and 499.4 {I2} from (d,{+3}He|g) 
RI$other: 45 {I5} from (d,{+3}He|g) is discrepant 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
E$weighted average of 1494.6 {I3} from {+63}Fe |b{+-} decay and 1495.2 {I2} from (d,{+3}He|g) 
RI$other: 100 {I5} from (d,{+3}He|g). 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from ({+48}Ca,p2n|g). Other: 290.3 {I5} from ({+70}Zn,X|g) 
RI$weighted average of 15 {I6} from ({+48}Ca,p2n|g) and 9.0 {I20} from ({+70}Zn,X|g) 
M$(D), |DJ=(1) from |g(|q) in ({+48}Ca,p2n|g); |D|p=no from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: E2
decay_BE_unit: e^2 x (fm)^4
decay_BE_info: ;TYPE=BE2;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE2W
decay_comment:
E$weighted average of 1673.2 {I10} from ({+48}Ca,p2n|g), 1671.5 {I10} from (d,{+3}He|g), and 1673.9 {I4} from ({+70}Zn,X|g) 
RI$from ({+70}Zn,X|g). Other: 100 {I12} from ({+48}Ca,p2n|g) 
M$Q, |DJ=2 from |g(|q) in ({+48}Ca,p2n|g) and ({+70}Zn,X|g); M2 ruled by RUL 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [E2]
decay_comment:
E$weighted average of 461.3 {I5} from {+63}Fe |b{+-} decay and 460.3 {I4} from (d,{+3}He|g) 
RI$other: 118 {I13} from (d,{+3}He|g) is discrepant 
$B(E2)(W.u.)<3593 upper limit exceeds RUL=300 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: [M1,E2]
decay_comment:
E$weighted average of 893.8 {I5} from {+63}Fe |b{+-} decay and 893.0 {I3} from (d,{+3}He|g) 
RI$other: 100 {I13} from (d,{+3}He|g) 
$B(M1)(W.u.)<0.097 if M1, B(E2)(W.u.)<210 if E2 


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$weighted average of 355.7 {I4} from ({+48}Ca,p2n|g) and 356.2 {I3} from ({+70}Zn,X|g) 
M$D, |DJ=1 from |g(|q) in ({+48}Ca,p2n|g); |D|p=(no) from level scheme in band assignment 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$from ({+70}Zn,X|g). Other: 407.0 {I5} from ({+48}Ca,p2n|g) 
M$(D) from |g(|q) in ({+48}Ca,p2n|g); |D|p=(no) from level scheme 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M1)
decay_BM_unit: mu^2
decay_BM_info: ;TYPE=BM1;ERR=CONV
decay_BMW_unit: Weisskopf
decay_BMW_info: ;TYPE=BM1W
decay_comment:
E$weighted average of 585.8 {I10} from ({+48}Ca,p2n|g) and 587.2 {I4} from ({+70}Zn,X|g) 
M$(D), |DJ=1 from |g(|q) in ({+70}Zn,X|g); |D|p=(no) from level scheme based on band assignment 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (E2)
decay_comment:
E$weighted average of 673.0 {I3} ({+76}Ge,X|g) and 672.3 {I4} in ({+70}Zn,X|g) 
RI$weighted average of 63 {I14} ({+76}Ge,X|g) and 67 {I6} in ({+70}Zn,X|g) 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
RI$using I|g(310.8|g)/I|g(1346|g from {+64}Co |b{+-}) and |b{+-} time spectrum 1985Ru05 deduce 5% intensity for 310.8|g and 95% |b{+-} feeding to the g.s. 2000HaZL assign 93% feeding to g.s. and 2% to 1561 level 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_comment:
M$anisotropy suggests |DJ=2, E2, which is consistent with only the 3+ assignment by 2000As05, not 2+. However, no data for anisotropy measurements are available 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_relative_intensity_unit: %
decay_comment:
$ B(E2)=0.0022 {I15}, B(E2)(W.u.)=1.4 {I10}, assuming |d{+2}(E2/M1)(1190|g)=0.0877 from shell-model calculations. For pure E2, B(E2)=0.0150 {I20}. Compiler obtains B(E2)=0.028 {+55-11} and B(E2)(W.u.)=18 {I+36-7} for pure E2 


decay_energy_unit: KEV
decay_energy_info: ;ERR=?
decay_uncertain: S
decay_comment:
E$from 1998Gr14. 2012Re11 see the 175.3 and 252.8 |g rays, but not the 214|g, thus they suggest placement of 214|g from the long-lived isomer, and that of 252.8 gamma from a non-isomeric level, reversing the ordering of 252-214 |g cascade proposed by 1998Gr14 


decay_energy_unit: KEV
decay_relative_intensity_unit: %
decay_multipolarity: (M3)
decay_comment:
$ This |g seen in laser-enhanced singles |g spectrum (2008Pa33) 
M$ proposed by 2008Pa33 from comparison of Weisskopf estimates for E3, M3 and E4 transitions. 


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:
$In deducing B(E1)(W.u.), 100% branch is assumed for 192|g 
M$proposed by 2015So23 as E1 based on comparison of the measured half-life with expected half-lives for different mutipolarities of 192 and 446 |g rays: M1, E2, E3 for intraband transitions with assumed 1 W.u. transition probability; E1, M2, E3 for interband transitions with theoretical transition probabilities from shell-model calculations. 


decay_energy_unit: KEV
decay_multipolarity: [E1]
decay_BE_unit: e^2 x (fm)^2
decay_BE_info: ;TYPE=BE1;ERR=CONV
decay_BEW_unit: Weisskopf
decay_BEW_info: ;TYPE=BE1W
decay_comment:
$In deducing B(E1)(W.u.), 100% branch is assumed for 192|g 
$Multipolarity of 192|g is proposed (by 2015So23) as E1 based on comparison of the measured half-life with expected half-lives for different mutipolarities of 192 and 446 |g rays: M1, E2, E3 for intraband transitions with assumed 1 W.u. transition probability; E1, M2, E3 for interband transitions with theoretical transition probabilities from shell-model calculations. 


decay_energy_unit: KEV
decay_comment:
E$From the energy difference between prompt 972|g and 1292|g transitions. Other: 320.5 {I2} from minimization of |h{+2} fitting of both E|g and T{-1/2} 


