ADOPTED LEVELS, GAMMAS for 58Cu

Authors: Caroline D. Nesaraja, Scott D. Geraedts and Balraj Singh |  Citation: Nucl. Data Sheets 111, 897 (2010) |  Cutoff date: 12-Jan-2010 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-9.37×103 keV 5S(n)= 12430.2 keV 7S(p)= 2872.9 keV 7Q(α)= -6082.7 keV 6
Reference: 2012WA38

References:
  A  58Zn ε decay (86 MS)  B  28Si(36Ar,APNG)
  C  58Ni(p,n)  D  58Ni(p,nγ)
  E  58Ni(3He,t),(3He,tγ)  F  58Ni(6Li,6He)

General Comments:

Structure calculations (levels, transition probabilities, etc.): 2008Na24, 2007BeZX (Gamow-Teller transitions) 2006Va21, 2004Ho08, 2004Va38, 1977Ko02, 1975Wa29, 1971Ru09

Levels: Isotopic spins t are from (p,nγ) and (3He,t)

Q-value: Note: Current evaluation has used the following Q record

Q-value: Q(εp)=393.2 15 (2009AuZZ,2003Au03)

Q-value: S(2n)=29200 140 (2009AuZZ,syst); S(2p)=10200.5 25 (2009AuZZ)










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
      0.0ABCDEF 1+ 3.204 s 7 
% ε = 100
     
    202.99 24 A CDE  0+      203.2 3 
  100
[M1]
      0.0
1+
    443.64 18  BCDEF 3+ 0.32 ns 6     443.5 2 
  100
E2(+M3)
      0.0
1+
   1051.5 3 A CDEF 1+ 78 fs +19-13     607
   848.6 2 
  1052
   <5
  100
   <9

[M1]

    443.64
    202.99
      0.0
3+
0+
1+
   1427.85 25   CDEF 2+ > 0.66 ps    376.6
   984.2
  1225.1
  1427.8 3 
    3.4 19 
    8.5 41 
    1.7 5 
  100

(M1+E2)
[E2]
[M1+E2]
   1051.5
    443.64
    202.99
      0.0
1+
3+
0+
1+
   1549.5 3  BCDEF (4+) > 0.34 ps   1105.8 3 
  100
(M1+E2)
    443.64
3+
   1647.41 18  B D F (3+) > 0.90 ps    220
   596
  1203.5
  1445
  1647.4 2 
   <4.3
   <5
   27 8 
  <19
  100 8 


(M1+E2)

(E2(+M3))
   1427.85
   1051.5
    443.64
    202.99
      0.0
2+
1+
3+
0+
1+
   1652.5 5   CDEF 2+ 35 fs 7     601.4
  1208.2
  1449.5
  1653
    5.9 2 
  100 3 
    5.3 18 
   <4.1
(M1(+E2))
(M1(+E2))
[E2]

   1051.5
    443.64
    202.99
      0.0
1+
3+
0+
1+
   2065.0 3  B D   (5+)      418 1 
   515.4 3 
  1621.2 4 
   13 2 
   43 2 
  100 3 

D
(E2+M3)
   1647.41
   1549.5
    443.64
(3+)
(4+)
3+
   2070 20     E         
   2170 20     E         
   2249.2 8    D        596.7
   821.3
  100 6 
   12 6 


   1652.5
   1427.85
2+
2+
   2270 20     E         
   2690 20     EF 4+        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   2750.2 6    D   (4+)     1103.1
  1200.6
  2306.4
   73 15 
  100 15 
    8.9 33 
(M1(+E2))
(M1(+E2))

   1647.41
   1549.5
    443.64
(3+)
(4+)
3+
   2780 20     E         
   2815.2 6    D       1162.7
  1387.2
  2371.5
  100 19 
   57 14 
   81 19 



   1652.5
   1427.85
    443.64
2+
2+
3+
   2840 20     E         
   2920.6 5  B D F (5+)      856
  1274
  1372
  2477.5
   <2.8
   <2.8
   <2.8
  100 4 



Q
   2065.0
   1647.41
   1549.5
    443.64
(5+)
(3+)
(4+)
3+
   2930.9 8    D F (0+:4+)     1278.3
  1503.0
  100 8 
   30 8 


   1652.5
   1427.85
2+
2+
   2949 10     E  (1)+        
   3230 20     E         
   3280.2 8    D   (0+:4+)     1627.7
  1852.2
  100 6 
   19 6 


   1652.5
   1427.85
2+
2+
   3310 20     E         
   3421.0 5  B D   (7+)      500.5 3 
  1355.6 4 
    8 1 
  100 3 
Q
Q
   2920.6
   2065.0
(5+)
(5+)
   3460.1 11     EF (1)+     3257
  100

    202.99
0+
   3512.6 7  B D        592.0 5 
  100

   2920.6
(5+)
   3570 20     E         
   3677.9 8     EF (1)+     3234
  3475
 
 


    443.64
    202.99
3+
0+
   3717 10   C EF (1)+        
   3820 20     E         
   3890 20     E         
   4010     F        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   4065.6 6  B     (7+)     1145.2 5 
  2000 1 
   60 7 
  100 7 

Q
   2920.6
   2065.0
(5+)
(5+)
   4210 20     E         
   4441.4 6  B     (8+)     1020.4 4 
  100
D
   3421.0
(7+)
   4720 10     EF (1)+        
   5065 20     E  (1)+        
   5160 20   C EF (1)+        
   5190.6 23  B     (7+)     3125 3 
  100

   2065.0
(5+)
   5348.0 8  B     (9+)      906 1 
  1927 1 
   24 3 
  100 6 
D
Q
   4441.4
   3421.0
(8+)
(7+)
   5451 20     EF (1)+        
   5574.9 8  B     (9+)     1509.3 5 
  100
Q
   4065.6
(7+)
   5645 20     EF (1)+        
   6038 20     E  (1)+        
   6086 20     E  (1)+        
   6387.2 10  B     (10+)     1039 1 
  1946 1 
   21 4 
  100 8 
D
Q
   5348.0
   4441.4
(9+)
(8+)
   6497 20   C E  (1)+        
   6794.1 12  B     (9)     1446 1 
  100

   5348.0
(9+)
   6844 20     E  (1)+        
   7105 20     E  (1)+        
   7143 20     E  (1)+        
   7392.6 11  B     (11+)     1818
  2044 2 
   16 5 
  100

Q
   5574.9
   5348.0
(9+)
(9+)
   7586 20     E  (1)+        
   7700 20     E  (1)+        
   7752 20     E  (1)+        
   7907 20     E  (1)+        
   7993 20     E  (1)+        
   8063 20     E  (1)+        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8127.3 13  B     (11)     1740 1 
  100
(D)
   6387.2
(10+)
   8159 20     E  (1)+        
   8199 20     E  (1)+        
   8228.2 13 ? B     (9+)     2654 2 
  3037 3 
  100 25 
   50 25 


   5574.9
   5190.6
(9+)
(7+)
   8282 20     E  (1)+        
   8370 10     E  (1)+        
   8421 10     E  (1)+        
   8487.3 16  B     (12+)     2100 2 
  100
(Q)
   6387.2
(10+)
   8520 10     E  (1)+        
   8566 10     E  (1)+        
   8614 10     E  (1)+        
   8725 10     E  (1)+        
   8837 10     E  (1)+        
   8881.6 13  B         1489 1 
  2087 2 
  100 20 
   80 20 


   7392.6
   6794.1
(11+)
(9)
   8900     F 2.8 MeV      
   8916.9 11  B     (9+) 0.22 ps 18 
% p = 96 4
     
   8959 10     E  (1)+        
   9000 10     E  (1)+        
   9129 20     E  (1)+        
   9172 10     E  (1)+        
   9209 10   C E  (1)+        
   9307 10     E  (1)+        
   9371 10     E  (1)+        
   9444 20     E  (1)+        
   9567 10     E  (1)+        
   9645 10     E  (1)+        
   9680.7 23  B         2288 2 
  100

   7392.6
(11+)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   9747.2 11  B     (11+) 0.38 ps 4     830.2 3 
  1519 1 
  4171 3 
  4399
  100 5 
   23 5 
   27 5 
    5 5 
E2
E2
E2

   8916.9
   8228.2
   5574.9
   5348.0
(9+)
(9+)
(9+)
(9+)
   9783 10     E  (1)+        
   9804.3 15  B     (12)     1317 1 
  1677 1 
   50 12 
  100 12 


   8487.3
   8127.3
(12+)
(11)
   9861 10     E  (1)+        
   9989 10     E  (1)+        
  10291 10     E  (1)+        
  10329 10     E  (1)+        
  10388 10     E  (1)+        
  10554 10     E  (1)+        
  10597 10     E  (1)+        
  10776.6 17  B         1895 1 
  100

   8881.6

  10825 10     E  (1)+        
  10944.5 12  B     (13+) 0.104 ps 14    1197.3 5 
  100
E2
   9747.2
(11+)
  11137 10   C E  (1)+        
  11358 10     E  (1)+        
  11553 4  B         3066 3 
  100

   8487.3
(12+)
  11562 20     E  (1)+        
  11815 20     E  (1)+        
  11842 3  B         2038 2 
  100

   9804.3
(12)
  11903 20     E  (1)+        
  12034 20     E  (1)+        
     12.45E3 15     E         
  12520.9 13  B     (15+) 0.035 ps 7    1576.4 4 
  100
E2
  10944.5
(13+)
  12880 20   C E  (1)+        
  13130 3  B         2353 2 
  100

  10776.6

  14475.9 16  B     (17+)     1955 1 
  100
Q
  12520.9
(15+)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  14881 4  B         3039 3 
  100

  11842

  16000     F 14 MeV      
  16818 3  B     (19+)     2342 2 
  100
Q
  14475.9
(17+)
  19566 4  B     (21+)     2748 2 
  100
Q
  16818
(19+)
  22747 5  B     (23+)     3181 3 
  100

  19566
(21+)
  24000     F 25 MeV      

E(level): From least-squares fit to Eγ’s for levels populated in γ-ray studies. Other values are mostly from (3He,t)

T1/2(level): From DSAM in (p,nγ), except where noted otherwise

M(γ): From γγ(θ) and γ(lin pol) in (p,nγ) and γγ(θ)(DCO) in (36Ar,αpnγ) and RUL (for E2 and M2 transitions)

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Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - ν41π41 INTRUDER (SD) band.
   8916.9 11  (9+) 0.22 ps 18 
% p = 96 4
     
   9747.2 11  (11+) 0.38 ps 4     830.2 3 
  1519 1 
  4171 3 
  4399
  100 5 
   23 5 
   27 5 
    5 5 
E2
E2
E2

   8916.9
   8228.2
   5574.9
   5348.0
(9+)
(9+)
(9+)
(9+)
  10944.5 12  (13+) 0.104 ps 14    1197.3 5 
  100
E2
   9747.2
(11+)
  12520.9 13  (15+) 0.035 ps 7    1576.4 4 
  100
E2
  10944.5
(13+)
  14475.9 16  (17+)     1955 1 
  100
Q
  12520.9
(15+)
  16818 3  (19+)     2342 2 
  100
Q
  14475.9
(17+)
  19566 4  (21+)     2748 2 
  100
Q
  16818
(19+)
  22747 5  (23+)     3181 3 
  100

  19566
(21+)

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Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
    202.99 0+      203.2 3 [M1] 0.00846α=0.00846
    443.64 3+ 0.32 ns 6     443.5 2 E2(+M3)-0.02 4B(E2)(W.u.)=7.7 15
   1051.5 1+ 78 fs +19-13     848.6 2 [M1] B(M1)(W.u.)=0.43 +8-11
   1427.85 2+ > 0.66 ps    984.2(M1+E2)-0.8 +2-15B(E2)(W.u.)<2.7, B(M1)(W.u.)<0.0019?
2+ > 0.66 ps   1225.1[E2] B(E2)(W.u.)<0.35
2+ > 0.66 ps   1427.8 3 [M1+E2] B(E2)(W.u.)<10, B(M1)(W.u.)<0.010
   1549.5 (4+) > 0.34 ps   1105.8 3 (M1+E2)-0.77 5B(E2)(W.u.)<30, B(M1)(W.u.)<0.032
   1647.41 (3+) > 0.90 ps   1203.5(M1+E2)+0.53 13B(E2)(W.u.)<1.1, B(M1)(W.u.)<0.0023
(3+) > 0.90 ps   1647.4 2 (E2(+M3))-0.06 +16-27B(E2)(W.u.)<2.8
   1652.5 2+ 35 fs 7     601.4(M1(+E2))+0.02 5B(M1)(W.u.)=0.15 4
2+ 35 fs 7    1208.2(M1(+E2))-0.02 2B(M1)(W.u.)=0.31 7
2+ 35 fs 7    1449.5[E2] B(E2)(W.u.)=9 4
   2065.0 (5+)     1621.2 4 (E2+M3)-0.12 4 
   2750.2 (4+)     1103.1(M1(+E2))-0.07 +5-12 
(4+)     1200.6(M1(+E2))0.00 5 
   9747.2 (11+) 0.38 ps 4     830.2 3 E2 B(E2)(W.u.)=183 25
(11+) 0.38 ps 4    1519 1 E2 B(E2)(W.u.)=2.0 6
(11+) 0.38 ps 4    4171 3 E2 B(E2)(W.u.)=0.015 4
  10944.5 (13+) 0.104 ps 14    1197.3 5 E2 B(E2)(W.u.)=166 23
  12520.9 (15+) 0.035 ps 7    1576.4 4 E2 B(E2)(W.u.)=125 25

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
      0.01+ 3.204 s 7 
% ε = 100
μ=+0.479 13 (2010Co01), T=0
From comparison of measured magnetic-dipole moment with calculated values from shell-model using GXPF1 interaction, proposed dominant configuration=πp3/2~#νp3/2 (2010Co01).
   1652.52+ 35 fs 7  XREF: C(1638).
   2949(1)+   Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   3421.0(7+)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   3460.1(1)+   Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   3677.9(1)+   Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   3717(1)+   Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   4065.6(7+)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   4441.4(8+)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   4720(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   5065(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   5160(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   5348.0(9+)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   5451(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   5574.9(9+)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   5645(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   6038(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   6086(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   6387.2(10+)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   6497(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   6844(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   7105(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   7143(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   7392.6(11+)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   7586(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
E(level)Jπ(level)T1/2(level)Comments
   7700(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   7752(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   7907(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   7993(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8063(1)+   t=(1).
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8127.3(11)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   8159(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8199(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8228.2(9+)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   8282(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8370(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8421(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8487.3(12+)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   8520(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8566(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8614(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8725(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8837(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   8916.9(9+) 0.22 ps 18 
% p = 96 4
α 2330γ from this level proposed earlier is not confirmed by 2002Ru09.
E(level): α 2330γ from this level proposed earlier is not confirmed by 2002Ru09. ν41π41 INTRUDER (SD) band.
Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   8959(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9000(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9129(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9172(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9209(1)+   T=1
XREF: C(9200).
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9307(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
E(level)Jπ(level)T1/2(level)Comments
   9371(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9444(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9567(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9645(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9747.2(11+) 0.38 ps 4  Q(transition)=2.75 +27-24 (2001Ru02).
E(level): ν41π41 INTRUDER (SD) band.
Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   9783(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9804.3(12)   Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
   9861(1)+   T=2
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
   9989(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  10291(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  10329(1)+   T=1
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  10388(1)+   T=2
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  10554(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  10597(1)+   T=2
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  10825(1)+   T=2
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  10944.5(13+) 0.104 ps 14  Q(transition)=2.55 +19-15 (2001Ru02).
E(level): ν41π41 INTRUDER (SD) band.
Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
  11137(1)+   T=2
XREF: C(11200).
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  11358(1)+   T=2
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  11562(1)+   T=(2)
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  11815(1)+   T=2
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  11903(1)+   T=0
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  12034(1)+   T=2
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  12520.9(15+) 0.035 ps 7  Q(transition)=2.21 +26-19 (2001Ru02).
E(level): ν41π41 INTRUDER (SD) band.
Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
  12880(1)+   T=2
XREF: C(13000).
Jπ(level): From L(3He,t)=0, interpreted as Gamow-Teller transition.
  14475.9(17+)   E(level): ν41π41 INTRUDER (SD) band.
Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
E(level)Jπ(level)T1/2(level)Comments
  16818(19+)   E(level): ν41π41 INTRUDER (SD) band.
Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
  19566(21+)   E(level): ν41π41 INTRUDER (SD) band.
Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.
  22747(23+)   E(level): ν41π41 INTRUDER (SD) band.
Jπ(level): As proposed by 1998Ru01 and 2001Ru02, based on γγ(θ)(DCO) data in 28Si(36Ar,αpnγ); ascending spins assumed with increasing excitation energy. Parentheses in some cases have been added by the evaluators.

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