ADOPTED LEVELS, GAMMAS for 57Fe

Author: M. R. Bhat |  Citation: Nucl. Data Sheets 85, 415 (1998) |  Cutoff date: 24-Sep-1998 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-836.2 keV 5S(n)= 7646.08 keV 4S(p)= 10559.31 keV 21Q(α)= -7320.2 keV 4
Reference: 2012WA38

References:
  A  57Mn β- decay  B  57Co ε decay
  C  57Fe(γ,γ): MOSSBAUER  D  48Ca(13C,4nγ) E=25-65 MeV
  E  56Fe(n,n’γ)  F  54Cr(α,nγ), (pol α,nγ)
  G  55Mn(t,nγ), 56Fe(t,dγ):?  H  55Mn(α,pnγ) E=25,28.6 MeV
  I  56Fe(n,γ), (pol n,γ) E=THERMAL  J  56Fe(n,γ) E=1151.5 EV RES
  K  56Fe(d,p), 57Fe(p,p’),  L  56Fe(pol d,p) E=10 MeV
  M  56Fe(d,pγ) E=6 MeV  N  Coulomb Excitation
  O  58Fe(p,d), (d,t), (3He,α)  P  59Co(μ-,2nγ), (π-,xγ),
  Q  58Ni(14C,15O) E=72 MeV  R  60Ni(p,xγ), 62Ni(p,xγ)

General Comments:

Resonance parameters: see 1984Fi09, 1983Ma54, 1983Ka09, 1981MuZQ, and the (n,γ) and (γ,n) references cited below

Levels: Configuration: see discussion in (n,γ) E=thermal on the configurations of the g.s., 14.4, 1627.3 and 1725.4, and capture states

Levels: Note: Jπ arguments based on γ(θ) from (α,nγ) are considered tentative by the evaluator since a Gaussian distribution of the magnetic substates was assumed and this is model dependent (see (13C,4nγ))

Levels: B(E2): see Coulomb excitation

Gammas: See (13C,4nγ), (α,nγ), and (n,γ) for unplaced gammas

Gammas: B(M1)(W.u.),B(E1)(W.u.),B(E2)(W.u.): calculated by evaluators from adopted T1/2 and γ properties, except as noted

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










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
     0.0ABCDEFGHIJKLMNOPQR 1/2- STABLE      
    14.4129 6 ABCDEFGHIJKLMNOP R 3/2- 98.3 ns 3      14.4129 6 
  100
M1+E2
     0.0
1/2-
   136.4743 5 ABCDEFGHIJKLMNOPQR 5/2- 8.7 ns 3     122.0614 4 
   136.4743 5 
  100 10 
   12.0 12 
M1+E2
E2
    14.4129
     0.0
3/2-
1/2-
   366.759 7 AB DEFGHIJKLMNOPQR 3/2- 10.5 ps 14     230.29 2 
   352.36 1 
   366.75 1 
    9.2 11 
  100 11 
   17.7 20 
(M1+E2)
M1+E2
M1+E2
   136.4743
    14.4129
     0.0
5/2-
3/2-
1/2-
   706.416 16 AB DEFGHIJK MNOP R 5/2- 4.1 ps 11     339.54 18 
   569.92 4 
   692.03 2 
   706.4 2 
    1.7 3 
   11.0 13 
  100 11 
    5.7 24 
M1+E2
M1+E2
M1+E2
[E2]
   366.759
   136.4743
    14.4129
     0.0
3/2-
5/2-
3/2-
1/2-
  1007.13 4 A  DEF HI K M      7/2- 0.13 ps 7     640.20 14 
   870.68 5 
   992.68 8 
    4.7 32 
  100.0 16 
   51.6 16 
E2
M1+E2
E2
   366.759
   136.4743
    14.4129
3/2-
5/2-
3/2-
  1139.9 10 ?         J                
  1197.81 13    DEF HI K M      9/2- 2.9 ps 4    1061.60 17 
  100
E2
   136.4743
5/2-
  1265.52 13 A   E   IJKLM OPQR 1/2- 82 fs 19     898.4 20 
  1250.6 22 
  1265.0 22 
  100
    4.8 7 
    2.7 7 



   366.759
    14.4129
     0.0
3/2-
3/2-
1/2-
  1356.83 18    DEF HI KLM      7/2- 0.18 ps 7     650.4 19 
   990.1 21 
  1342.7 22 
  100
   43 7 
   40 5 
M1+E2
E2
E2
   706.416
   366.759
    14.4129
5/2-
3/2-
3/2-
  1627.256 24 A   E   IJKLM      3/2- 56 fs 8     920.85 2 
  1260.60 3 
  1612.78 2 
  1627.05 8 
   14.1 16 
   46 5 
  100 11 
    3.9 5 


M1+E2

   706.416
   366.759
    14.4129
     0.0
5/2-
3/2-
3/2-
1/2-
  1725.38 3 A   E   IJKLM      3/2- 31 fs 4     460.1 4 
  1019.02 4 
  1358.71 6 
  1710.2 3 
  1725.09 6 
    0.48 17 
   27.6 29 
   14.3 16 
    4.0 9 
  100 11 




M1+E2
  1265.52
   706.416
   366.759
    14.4129
     0.0
1/2-
5/2-
3/2-
3/2-
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  1976.63 20     E   I          (1/2-,3/2,5/2-)      251.1 3 
  1840.2
  1976.4 11 
   25
  100
   24



  1725.38
   136.4743
     0.0
3/2-
5/2-
1/2-
  1989.66 20    DEF H           9/2- 0.18 ps +17-6     791.6
   983.0 3 
  1282.85 27 
   66
   78
  100

M1+E2
E2(+M3)
  1197.81
  1007.13
   706.416
9/2-
7/2-
5/2-
  1991 5           K        1/2-,3/2-        
  2113.11 17         I          (1/2,3/2,5/2-)      849.5 5 
  2113.4 3 
   27 8 
  100 17 


  1265.52
     0.0
1/2-
1/2-
  2118.6 5     E     KLM      5/2- 46 fs 12    1111.6
  1412.1 5 
  2104.4 11 
   29
  100 15 
   69 13 

M1+E2

  1007.13
   706.416
    14.4129
7/2-
5/2-
3/2-
  2206.88 14     E   I KL  O    5/2- 10 fs 3     942.0 14 
  1199.9
  1841 3 ?
  2192.8 4 
  2206.8 6 
    8 4 
   42
 
  100 19 
   84 22 





  1265.52
  1007.13
   366.759
    14.4129
     0.0
1/2-
7/2-
3/2-
3/2-
1/2-
  2217.66 18         I K        (5/2+)     1851.3 4 
  2081.2 3 
  2202.7 8 
   46 10 
   77 17 
  100 32 



   366.759
   136.4743
    14.4129
3/2-
5/2-
3/2-
  2220.2    E         O    (7/2-) > 0.3 ps   1853.3
  2083.8
  2205.8
   10
   94
  100

(M1+E2)

   366.759
   136.4743
    14.4129
3/2-
5/2-
3/2-
  2330.41 16         IJ         (1/2,3/2,5/2+)      703.4 4 
  100

  1627.256
3/2-
  2355.96 5    DEF H           (11/2)- 0.06 ps 2    1158.37 18 
  1348.86 19 
   41 4 
  100 10 
M1+E2
(E2)
  1197.81
  1007.13
9/2-
7/2-
  2358 12           K        1/2-,3/2-        
  2455.55 15    DEF HI   M      9/2+ > 1.4 ps   1448.52 20 
  100
(E1+M2)
  1007.13
7/2-
  2456 5           KL       1/2+,7/2+,9/2+        
  2505.29 12     E   I KLM      5/2+ 78 fs 18     780.0
  1798.1 3 
  2138.63 18 
  2368.6 3 
  2490.8 13 
    5
   10 2 
  100 12 
   47 2 
   18 6 





  1725.38
   706.416
   366.759
   136.4743
    14.4129
3/2-
5/2-
3/2-
5/2-
3/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  2564.22 21         I KL       3/2-      837.9 3 
  2562.4 5 
  100 17 
   57 16 


  1725.38
     0.0
3/2-
1/2-
  2574.5 4     E     K M      (1/2,3/2,5/2-) 18 fs 4    2207.6 8 
  2574.4 4 
   38 15 
  100 13 


   366.759
     0.0
3/2-
1/2-
  2593.6 6     E              (3/2-,5/2-) 37 fs 10    1586.4
  1887.1
  2593.5
   82
  100
   18



  1007.13
   706.416
     0.0
7/2-
5/2-
1/2-
  2599.4 3         I K        (1/2,3/2,5/2+)     2462.1 7 
  2598.1 11 
  100 17 
   43 15 


   136.4743
     0.0
5/2-
1/2-
  2697.17 17     E   IJKLM   Q  1/2- 6 fs 2    1991.0 10 
  2330.6 5 
  2682.5 3 
  2696.6 3 
    7 2 
   15 2 
  100 5 
   65 3 




   706.416
   366.759
    14.4129
     0.0
5/2-
3/2-
3/2-
1/2-
  2758.30 11         I K            1492.4 4 
  2391.80 20 
   27 5 
  100 14 


  1265.52
   366.759
1/2-
3/2-
  2821.07 23     E   I K        (1/2,3/2,5/2+) 60 fs +20-10     603.54 19 
  1812.9 5 
  100 16 
   44 13 


  2217.66
  1007.13
(5/2+)
7/2-
  2835.89 7     E   IJK        3/2,5/2      723.0 20 
  1828.9 10 
  2129.48 9 
  2469.17 16 
  2821.5 6 
  2835.43 19 
    1.5 15 
    4.5 30 
  100 11 
   90 17 
   15 3 
   37 6 






  2113.11
  1007.13
   706.416
   366.759
    14.4129
     0.0
(1/2,3/2,5/2-)
7/2-
5/2-
3/2-
3/2-
1/2-
  2855.0 4         I K               
  2878.7 4    DEF H           (13/2)- < 0.14 ps   1680.58 21 
  100
(E2)
  1197.81
9/2-
  2904.28 24     E   I              2198.2 5 
  2537.1 5 
  100 26 
   47 13 


   706.416
   366.759
5/2-
3/2-
  2921.20 10         I KLM      1/2-,3/2- 33 fs 6    1655.37 19 
  2216.2 5 
  2554.3 5 
  2906.0 4 
  2920.5 4 
   42 3 
 
   31 3 
   45 4 
  100 9 





  1265.52
   706.416
   366.759
    14.4129
     0.0
1/2-
5/2-
3/2-
3/2-
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  2970.89 22         IJK        (1/2,3/2,5/2+)     2603.1 15 
  100

   366.759
3/2-
  2987.95 15         I K        (1/2,3/2,5/2+)      657.56 9 
  1722.40 13 
  2618.9 9 
   76 12 
  100 14 
   15 6 



  2330.41
  1265.52
   366.759
(1/2,3/2,5/2+)
1/2-
3/2-
  3059.1 3     E   I K        1/2+     2691.6 5 
  2922.5 10 
   50 16 
  100 10 


   366.759
   136.4743
3/2-
5/2-
  3098.95 15         I K            2091.85 16 
  100

  1007.13
7/2-
  3110 5           K               
  3122.76 21         I K            2755.90 21 
  100

   366.759
3/2-
  3134.8 4    D F H           (15/2)- 160 ps 7     256.03 11 
  100
M1+E2
  2878.7
(13/2)-
  3182.77 20         IJK        1/2-,3/2-      211.87 9 
   977.1 7 
  1457.4 5 
  1825.9 3 
  2815.0 6 
  3166.9 11 
   50 8 
   31 19 
   25 7 
   56 14 
   56 14 
  100 82 






  2970.89
  2206.88
  1725.38
  1356.83
   366.759
    14.4129
(1/2,3/2,5/2+)
5/2-
3/2-
7/2-
3/2-
3/2-
  3205.6 5         I K   O    5/2-,7/2-      988.2 5 
  100

  2217.66
(5/2+)
  3239.89 12         IJK M      1/2+      735.1 3 
  1022.0 3 
  1263.3 3 
  2873.7 3 
  3103.1 4 
  3225.3 4 
  3239.30 20 
    6.0 16 
    7.5 17 
   14.9 21 
   55 6 
  100 15 
   45 9 
   52 7 







  2505.29
  2217.66
  1976.63
   366.759
   136.4743
    14.4129
     0.0
5/2+
(5/2+)
(1/2-,3/2,5/2-)
3/2-
5/2-
3/2-
1/2-
  3269.26 13    D F H           (13/2)+ 0.37 ps +21-11     813.73 15 
   913.37 16 
   49 3 
  100 3 
(E2)
(E1+M2)
  2455.55
  2355.96
9/2+
(11/2)-
  3284 5           K               
  3301.77 10         I K        (5/2-,7/2-)     1674.62 13 
  2104.5 5 
  2935.8 8 
   57 15 
  100 24 
   36 15 



  1627.256
  1197.81
   366.759
3/2-
9/2-
3/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  3322.48 11         I K        1/2-,3/2-      564.19 6 
  1115.64 15 
  1345.2 5 
  1965.3 2 
   76 8 
   31 5 
   21 4 
  100 14 




  2758.30
  2206.88
  1976.63
  1356.83

5/2-
(1/2-,3/2,5/2-)
7/2-
  3336.59 25         I              2970.0 3 
  100

   366.759
3/2-
  3340.33 18         I               884.78 10 
  100

  2455.55
9/2+
  3345          K        7/2+,9/2+        
  3371.11 16         IJKL    Q  3/2-     1041.1 5 
  1646.0 3 
  3356.3 2 
    9 3 
   21 4 
  100 12 



  2330.41
  1725.38
    14.4129
(1/2,3/2,5/2+)
3/2-
3/2-
  3427.68 8         IJKLM   Q  3/2- 3.0 fs +6-29    2721.17 9 
  3060.90 17 
  3291.1 2 
  3414.3 13 
   85 9 
    9.3 16 
   19 4 
  100 11 




   706.416
   366.759
   136.4743
    14.4129
5/2-
3/2-
5/2-
3/2-
  3452 5           K               
  3473 5           K        5/2-,7/2-        
  3513.8 4    D               (17/2) < 0.14 ps    379.06 13 
  100

  3134.8
(15/2)-
  3535 5           K        7/2+,9/2+        
  3535.92 18         I              1810.51 17 
  100

  1725.38
3/2-
  3548 5           K        7/2+,9/2+        
  3561.34 12         I               803.09 8 
  1447.0 3 
  100 11 
   38 10 


  2758.30
  2113.11

(1/2,3/2,5/2-)
  3608 5           K        7/2+,9/2+        
  3608.51 21         I              1982.1 4 
  100

  1627.256
3/2-
  3661 5           K               
  3752 5           K        7/2+,9/2+        
  3784 10           K        7/2+,9/2+        
  3791.59 9         IJ         3/2+     1460.9 3 
  1584.6 3 
  2066.17 12 
  2164.69 18 
  2526.2 3 
  3776.6 2 
  3791.7 10 ?
   16.3 26 
   14.3 25 
  100 12 
   41 6 
   59 14 
   16 6 
   33







  2330.41
  2206.88
  1725.38
  1627.256
  1265.52
    14.4129
     0.0
(1/2,3/2,5/2+)
5/2-
3/2-
3/2-
1/2-
3/2-
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  3827 10           K        5/2-,7/2-        
  3862.42 19         I              1655.51 12 
  100

  2206.88
5/2-
  3881 10           K               
  3902 10           K        5/2-,7/2-        
  3926.0 20          J         (1/2,3/2,5/2-)        
  3936.1 7         I K        5/2-,7/2-     3921.5 7 
  100

    14.4129
3/2-
  3981.18 24         I KLM      3/2- 7 fs 12    1159.5 13 
  1284.0 5 
  1381.7 2 
  3615.3 11 
  3981.7 4 
   15 8 
   77 39 
  100 13 
 
   77 17 





  2821.07
  2697.17
  2599.4
   366.759
     0.0
(1/2,3/2,5/2+)
1/2-
(1/2,3/2,5/2+)
3/2-
1/2-
  4042.60 24         I K        5/2-,7/2-     2415.1 3 
  100

  1627.256
3/2-
  4081 10           K               
  4093 10           K               
  4136.62 10         I          (1/2,3/2,5/2+)      575.09 19 
   834.91 8 
  1077.3 3 
  1215.38 5 
  1282.3 6 
  1300.9 4 
  1931.8 7 
   90 48 
  100 11 
   19 5 
   48 11 
   43 20 
   43 10 
   29 10 







  3561.34
  3301.77
  3059.1
  2921.20
  2855.0
  2835.89
  2206.88

(5/2-,7/2-)
1/2+
1/2-,3/2-

3/2,5/2
5/2-
  4138.57 18           KLM      5/2+ 15 fs 8    1632.94 16 
  2783.8 5 
  3774.0 8 
  4002.4 9 
  100 6 
   81 15 
   22 5 
   17 4 




  2505.29
  1356.83
   366.759
   136.4743
5/2+
7/2-
3/2-
5/2-
  4144.3 5         I          (1/2,3/2,5/2+)     2517.0 5 
  100

  1627.256
3/2-
  4209.59 12         I K        (3/2)-      601.3 2 
  1026.4 3 
  1110.9 3 
  1305.3 3 
  1705.0 8 
  2097 2 
  2582.0 3 
  2943.4 5 
  3842.4 3 
  4073.3 3 
  4194.8 4 
  4210.2 10 
   48 8 
   17 4 
   17 4 
   24 7 
   38 8 
   17 10 
   31 8 
   28 7 
  100 12 
   72 10 
   45 11 
   24 7 












  3608.51
  3182.77
  3098.95
  2904.28
  2505.29
  2113.11
  1627.256
  1265.52
   366.759
   136.4743
    14.4129
     0.0

1/2-,3/2-


5/2+
(1/2,3/2,5/2-)
3/2-
1/2-
3/2-
5/2-
3/2-
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  4239 10           K        3/2+,5/2+        
  4316 10           K        7/2+,9/2+        
  4363 10           K        5/2-,7/2-        
  4378.68 21         I          (1/2,3/2,5/2-)      335.9 3 
  1006.9 5 
  1255.5 8 
  2654.3 4 
  4378.3 4 
   25 7 
   19 7 
   13 7 
   31 13 
  100 16 





  4042.60
  3371.11
  3122.76
  1725.38
     0.0
5/2-,7/2-
3/2-

3/2-
1/2-
  4379.44 19          JKLM      (1/2,3/2,5/2-) 3 fs 4    1458.09 21 
  1681.3 5 
  4013.6 4 
   22 3 
   12 4 
  100 9 



  2921.20
  2697.17
   366.759
1/2-,3/2-
1/2-
3/2-
  4432.4 8    D F             < 0.14 ps   1297.8 5 
  100

  3134.8
(15/2)-
  4459.70 14         I K     Q  5/2-,7/2-     1119.8 6 
  1351.8 10 
  1700.8 3 
  2348.9 9 
  2734.2 3 
  2832.46 18 
    3.8 19 
    9.4 39 
   21 4 
   11 6 
   28 5 
  100 13 






  3340.33
  3110
  2758.30
  2113.11
  1725.38
  1627.256



(1/2,3/2,5/2-)
3/2-
3/2-
  4492          KL       5/2+        
  4525          K        7/2+,9/2+        
  4525.54 23    D F H           (17/2+) 0.29 ps 9    1256.27 19 
  100
(E2)
  3269.26
(13/2)+
  4544 10           K        1/2+        
  4572.8 5         I K        1/2+     1973.4 4 
  100

  2599.4
(1/2,3/2,5/2+)
  4597.4 3         I KLM      5/2+ 5 fs 8    2033.2 2 
  2870.8 11 
  100
 


  2564.22
  1725.38
3/2-
3/2-
  4652 10           K        5/2-,7/2-        
  4680 10           K               
  4691.75 15         I K        (5/2+)     1355.6 4 
  1369.1 2 
  1487.2 9 
  1836.4 4 
  1855.9 4 
  2186.4 4 
  2486.0 6 
  4555.3 3 
  100 25 
  100 18 
   23 8 
   46 9 
   46 9 
   31 8 
   62 17 
   69 17 








  3336.59
  3322.48
  3205.6
  2855.0
  2835.89
  2505.29
  2206.88
   136.4743

1/2-,3/2-
5/2-,7/2-

3/2,5/2
5/2+
5/2-
5/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  4719 10           K               
  4753 10           K        5/2-,7/2-        
  4771 10           K        3/2+,5/2+        
  4823.9 5           KLM      < 10 fs   1584.0 4 
  100

  3239.89
1/2+
  4902 10           K               
  4922.9 7           KLM      5/2+ 7 fs 10    2418.3 10 
  3565.4 8 
  100 13 
   70 9 


  2505.29
  1356.83
5/2+
7/2-
  4970 20               O    (5/2-,7/2-)        
  4976 10           K        3/2+,5/2+        
  5019 10           K        5/2-,7/2-        
  5064 10           KL       (1/2+)&(7/2-)        
  5085 10           K               
  5099          K               
  5115 10           K        1/2+        
  5140.25 20         I KL       (1/2,3/2,5/2+)     1899.5 5 
  2574.3 3 
  3027.55 15 
   55 20 
  100 21 
  100 14 



  3239.89
  2564.22
  2113.11
1/2+
3/2-
(1/2,3/2,5/2-)
  5178.44 25         I K        1/2+     1197.27 7 
  2480.2 6 
  5042.1 8 
  100 11 
   17 6 
   50 15 



  3981.18
  2697.17
   136.4743
3/2-
1/2-
5/2-
  5195          K               
  5221.6 3         I K        (1/2-,3/2,5/2+)     2385.3 4 
  3014.7 3 
  4856.6 13 
   75 18 
  100 19 
   83 34 



  2835.89
  2206.88
   366.759
3/2,5/2
5/2-
3/2-
  5238.7 4         I K        (1/2,3/2,5/2+)        
  5250          K        1/2+        
  5271 10           K        1/2+        
  5289          KL  O    5/2+        
  5334          K        7/2+,9/2+        
  5362.1 9           KLM      5/2+ 6 fs +15-6    2856.7 9 
  100

  2505.29
5/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  5404 10           K               
  5422 10           K        3/2+,5/2+        
  5445 10           K        7/2+,9/2+        
  5472 10           K        3/2+,5/2+        
  5500 10           K        1/2+        
  5512 10           K               
  5525 10           K        1/2+        
  5545          K               
  5564 10           K        3/2+,5/2+        
  5590 10           K               
  5623 10           K               
  5641 10           K               
  5675 10           K               
  5688 10           K               
  5721 10           K        1/2+&(7/2+,9/2+)        
  5737 10           K        1/2+        
  5769 10           K               
  5802 10           K        3/2+,5/2+        
  5825          K        3/2+,5/2+        
  5844          K        1/2+        
  5864          K        3/2+,5/2+        
  5900          K               
  5918          K               
  5936          K               
  5956          K        3/2+,5/2+        
  5983          K        3/2+ TO (9/2+)        
  6025          K        3/2+,5/2+        
  6044          K        3/2+,5/2+        
  6083          K               
  6103          K        7/2+,9/2+        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  6130          K        1/2+        
  6148          K               
  6171          K        3/2+,5/2+        
  6187.1 3    D   H           (21/2+) 0.11 ps 4    1661.54 20 
  100 10 
(E2)
  4525.54
(17/2+)
  6194          K        7/2+,9/2+        
  6212          K        1/2+        
  6230          K        3/2+,5/2+        
  6252          K        7/2+,9/2+        
  6270          K        7/2+,9/2+        
  6305          K               
  6323          K               
  6340          K               
  6370          K        3/2+,5/2+        
  6408          K        3/2+,5/2+        
  6427          K        3/2+,5/2+        
  6496          K               
  6512          K        3/2+,5/2+        
  6542          K        1/2+        
  6571          K        3/2+,5/2+        
  6589          K        3/2+,5/2+        
  6640          K        3/2+,5/2+        
  6672          K        3/2+,5/2+        
  6703          K        3/2+,5/2+        
  6725          K               
  7646.7 7          J         1/2-     3267.0 20 ?
  3721.3 20 ?
  3854.3 35 
  4217.9 25 
  4276.5 30 
  4408.0 30 
  4463.5 20 
  4810.0 30 ?
  4950.1 20 
  5920.8 30 
  6017.8 30 
  6381.8 20 
  6507.0 10 ?
  7279.6 30 
  7508.8 20 
  7631.7 20 
  7645.5 20 
    1.9 10 
    1.9 12 
    1.9 11 
    1.2 8 
    1.7 8 
    1.3 8 
    5.5 10 
    1.5 10 
    5.0 14 
    5.6 13 
    1.1 5 
   35 5 
   <1.0
    1.9 7 
    5.2 8 
  100 4 
   41 4 


E1
M1,E2
M1,E2
E1
M1,E2

M1
M1,E2
M1,E2
M1

M1,E2
E2
M1,E2
M1
  4379.44
  3926.0
  3791.59
  3427.68
  3371.11
  3239.89
  3182.77
  2835.89
  2697.17
  1725.38
  1627.256
  1265.52
  1139.9
   366.759
   136.4743
    14.4129
     0.0
(1/2,3/2,5/2-)
(1/2,3/2,5/2-)
3/2+
3/2-
3/2-
1/2+
1/2-,3/2-
3/2,5/2
1/2-
3/2-
3/2-
1/2-

3/2-
5/2-
3/2-
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  8323.0 5    D   H           (25/2+) < 0.14 ps   2135.9 3 
  100 17 
(E2)
  6187.1
(21/2+)
    10.45E+3 5 ?              O    (7/2-)        

E(level): For states connected by gammas, calculated using least-square adjustment procedures with the energy of the s- and p-wave capture states held fixed and uncertain gammas not included in the calculation. Uncertainty in 198Au reference scale (|+1.1 eV) for 122γ and 136γ added in quadrature after adjustment. Other energies from 56Fe(d,p),57Fe(p,p’),59Co(d,α), except as noted

Jπ(level): From angular momentum transfer in (d,p), except as noted

T1/2(level): From DSAM or RDM in (13C,4nγ), except as noted

I(γ): Relative-photon branching from each level

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Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - ΔJ=2 POSITIVE-PARITY band.
  3269.26 13  (13/2)+ 0.37 ps +21-11       
  4525.54 23  (17/2+) 0.29 ps 9    1256.27 19 
  100
(E2)
  3269.26
(13/2)+
  6187.1 3  (21/2+) 0.11 ps 4    1661.54 20 
  100 10 
(E2)
  4525.54
(17/2+)
  8323.0 5  (25/2+) < 0.14 ps   2135.9 3 
  100 17 
(E2)
  6187.1
(21/2+)

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Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
    14.4129 3/2- 98.3 ns 3      14.4129 6 M1+E20.00223 188.56B(E2)(W.u.)=0.37 7, B(M1)(W.u.)=0.0078 3, α=8.56 26, α(K)=7.35 19, α(L)=0.779 42
   136.4743 5/2- 8.7 ns 3     122.0614 4 M1+E2+0.120 10.0240B(E2)(W.u.)=2.3 4, B(M1)(W.u.)=0.00118 17, α=0.0240 14, α(K)=0.0214 12, α(L)=0.00224 20
5/2- 8.7 ns 3     136.4743 5 E2 0.137B(E2)(W.u.)=10.9 16, α=0.137 15, α(K)=0.134, α(L)=0.0139
   366.759 3/2- 10.5 ps 14     230.29 2 (M1+E2)+0.02 8B(E2)(W.u.)=0.2 +15-2, B(M1)(W.u.)=0.0124 25
3/2- 10.5 ps 14     352.36 1 M1+E2+0.025 9B(E2)(W.u.)=0.4 3, B(M1)(W.u.)=0.038 8
3/2- 10.5 ps 14     366.75 1 M1+E2-0.45 5B(E2)(W.u.)=15 4, B(M1)(W.u.)=0.0049 10
   706.416 5/2- 4.1 ps 11     339.54 18 M1+E2+0.083 5B(E2)(W.u.)=0.23 9, B(M1)(W.u.)=0.0020 7
5/2- 4.1 ps 11     569.92 4 M1+E2+0.097 8B(E2)(W.u.)=0.15 6, B(M1)(W.u.)=0.0027 9
5/2- 4.1 ps 11     692.03 2 M1+E2-0.465 8B(E2)(W.u.)=10 3, B(M1)(W.u.)=0.011 4
5/2- 4.1 ps 11     706.4 2 [E2] B(E2)(W.u.)=2.9 15
  1007.13 7/2- 0.13 ps 7     640.20 14 E2 B(E2)(W.u.)=9.×101 9
7/2- 0.13 ps 7     870.68 5 M1+E2-0.6 +2-5B(E2)(W.u.)=1.1×102 9, B(M1)(W.u.)=0.12 7
7/2- 0.13 ps 7     992.68 8 E2 B(E2)(W.u.)=1.1×102 7
  1197.81 9/2- 2.9 ps 4    1061.60 17 E2 B(E2)(W.u.)=11.1 16
  1356.83 7/2- 0.18 ps 7     650.4 19 M1+E2+1.1 +6-3B(E2)(W.u.)=6.×102 4, B(M1)(W.u.)=0.11 8
7/2- 0.18 ps 7     990.1 21 E2 B(E2)(W.u.)=6.×101 3
7/2- 0.18 ps 7    1342.7 22 E2 B(E2)(W.u.)=12 5
  1627.256 3/2- 56 fs 8    1612.78 2 M1+E2-0.35 5B(E2)(W.u.)=4.7 16, B(M1)(W.u.)=0.051 10
  1725.38 3/2- 31 fs 4    1725.09 6 M1+E2+0.04 5B(E2)(W.u.)=0.1 +3-10, B(M1)(W.u.)=0.094 18
  1989.66 9/2- 0.18 ps +17-6     983.0 3 M1+E2-4.5 5B(E2)(W.u.)=8.×101 8, B(M1)(W.u.)=0.0019 19
9/2- 0.18 ps +17-6    1282.85 27 E2(+M3)0.00 2B(E2)(W.u.)=(3.×101 3)
  2118.6 5/2- 46 fs 12    1412.1 5 M1+E2-0.08 5B(E2)(W.u.)=0.5 7, B(M1)(W.u.)=0.09 3
  2355.96 (11/2)- 0.06 ps 2    1158.37 18 M1+E2-0.45 5B(E2)(W.u.)=17 7, B(M1)(W.u.)=0.057 21
(11/2)- 0.06 ps 2    1348.86 19 (E2) B(E2)(W.u.)=1.1×102 4
  2455.55 9/2+ > 1.4 ps   1448.52 20 (E1+M2)0.00 4B(E1)(W.u.)<0.00011
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
  2878.7 (13/2)- < 0.14 ps   1680.58 21 (E2) B(E2)(W.u.)>23
  3134.8 (15/2)- 160 ps 7     256.03 11 M1+E2-0.07 2B(E2)(W.u.)=1.2 7, B(M1)(W.u.)=0.0082 4
  3269.26 (13/2)+ 0.37 ps +21-11     813.73 15 (E2) B(E2)(W.u.)=1.1×102 7
(13/2)+ 0.37 ps +21-11     913.37 16 (E1+M2)0.00 3B(E1)(W.u.)=0.0011 7
  4525.54 (17/2+) 0.29 ps 9    1256.27 19 (E2) B(E2)(W.u.)=48 15
  6187.1 (21/2+) 0.11 ps 4    1661.54 20 (E2) B(E2)(W.u.)=31 12
  8323.0 (25/2+) < 0.14 ps   2135.9 3 (E2) B(E2)(W.u.)>7.0

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0.01/2- STABLE μ=+0.09044 7 (1989Ra17), T=5/2
Small spectroscopic factor in (d,p) implies that 57Fe g.s. is deformed (1973De23).
  1007.137/2- 0.13 ps 7  T1/2(level): From DSAM in (α,pnγ).
  1139.9   Based on existence of primary γ in res (n,γ).
  1265.521/2- 82 fs 19  Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
  1356.837/2- 0.18 ps 7  T1/2(level): From DSAM in (α,pnγ).
  1627.2563/2- 56 fs 8  Jπ(level): L(n)=1 in (d,p). J|=1/2 from γγ(θ) in (n,γ) E=thermal and CP in (pol n,γ) E=thermal.
  1725.383/2- 31 fs 4  Jπ(level): L(n)=1 in (d,p). J|=1/2 from γγ(θ) in (n,γ) E=thermal and CP in (pol n,γ) E=thermal.
  1989.669/2- 0.18 ps +17-6  T1/2(level): From DSAM in (n,n’γ).
  2118.65/2- 46 fs 12  Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
T1/2(level): From DSAM in (n,n’γ).
  2206.885/2- 10 fs 3  T1/2(level): From DSAM in (n,n’γ).
  2220.2(7/2-) > 0.3 ps T1/2(level): From DSAM in (n,n’γ).
  2355.96(11/2)- 0.06 ps 2  T1/2(level): From DSAM in (α,pnγ).
  2455.559/2+ > 1.4 ps T1/2(level): From DSAM in (α,pnγ).
  2505.295/2+ 78 fs 18  Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
  2564.223/2-   E(level): From (α,nγ).
Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
  2593.6(3/2-,5/2-) 37 fs 10  T1/2(level): From DSAM in (n,n’γ).
  2697.171/2- 6 fs 2  E(level): From 57Mn β- decay.
Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
T1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
  2821.07(1/2,3/2,5/2+) 60 fs +20-10  T1/2(level): From DSAM in (n,n’γ).
  2921.201/2-,3/2- 33 fs 6  E(level): From 57Mn β- decay.
T1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
  3098.95   L(n)=2+4 doublet in (d,p).
E(level): L(n)=2+4 doublet in (d,p).
  3269.26(13/2)+ 0.37 ps +21-11  E(level): ΔJ=2 POSITIVE-PARITY band.
T1/2(level): From DSAM in (α,pnγ).
  3371.113/2-   E(level): From (α,nγ).
Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
  3427.683/2- 3.0 fs +6-29  E(level): From (α,nγ).
Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
  35357/2+,9/2+   L(n)=4 in (d,p) inconsistent with 1811γ to 3/2- state. Therefore, state observed in (n,γ) is probably different.
  3535.92   See comment on preceding state.
E(level)Jπ(level)T1/2(level)Comments
  3981.183/2- 7 fs 12  E(level): From 57Mn β- decay. From (α,nγ).
Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
T1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
  4138.575/2+ 15 fs 8  E(level): From 57Mn β- decay.
Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
T1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
  4379.44(1/2,3/2,5/2-) 3 fs 4  E(level): From 57Mn β- decay.
T1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
  44925/2+   Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
  4525.54(17/2+) 0.29 ps 9  E(level): ΔJ=2 POSITIVE-PARITY band.
  4597.45/2+ 5 fs 8  E(level): From 57Mn β- decay.
Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
T1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
  4823.9 < 10 fs Jπ=(1/2+) & (3/2+) from analyzing power(θ) and σ(θ) in (pol d,p) based on empirical curves. Data clearly show this level to be a doublet.
E(level): Jπ=(1/2+) & (3/2+) from analyzing power(θ) and σ(θ) in (pol d,p) based on empirical curves. Data clearly show this level to be a doublet. From 57Mn β- decay.
T1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
  4922.95/2+ 7 fs 10  E(level): From 57Mn β- decay.
Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
T1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
  4970(5/2-,7/2-)   E(level): From ε decay.
Jπ(level): From angular momentum transfer in (p,d) and (d,p) and Coulomb excitation.
  52895/2+   Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
  5362.15/2+ 6 fs +15-6  E(level): From 57Mn β- decay.
Jπ(level): From angular momentum transfer and analyzing power in (d,p) and (pol d,p).
T1/2(level): From centroid shift of γ-rays in coincidence with p in (d,pγ).
  6187.1(21/2+) 0.11 ps 4  E(level): ΔJ=2 POSITIVE-PARITY band.
T1/2(level): From DSAM in (α,pnγ).
  7646.71/2-   γΓnΓγ/Γ=68.7 meV 15; σ0Γγ=161 b×eV 4 from 1983Ma13; not consistent with 1981MuZQ.
E(level): γΓnΓγ/Γ=68.7 meV 15; σ0Γγ=161 b×eV 4 from 1983Ma13; not consistent with 1981MuZQ.
  8323.0(25/2+) < 0.14 ps E(level): ΔJ=2 POSITIVE-PARITY band.
    10.45E+3(7/2-)   IAS?(57Mn) from 58Fe(p,d).
E(level): IAS?(57Mn) from 58Fe(p,d).

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Additional Gamma Comments:

E(level)E(gamma)Comments
    14.4129    14.4129E(γ): from ε decay. From ε decay
I(γ): From ε decay
M(γ): from Γ and adopted Jπ. See also 1984Pl05.
   136.4743   122.0614E(γ): Recommended γ-ray calibration energy from ε decay.
   136.4743E(γ): Recommended γ-ray calibration energy from ε decay.
M(γ): Q from γ(θ,H,t) in ε decay and Coulomb excitation; E2 from RUL
   366.759   230.29M(γ): D+Q from γ(θ) in Coul. ex. and ε decay; and ΔJπ
  1007.13   640.20E(γ): From (13C,4nγ)
I(γ): From (13C,4nγ)
M(γ): From comparison to RUL and ΔJπ
   870.68E(γ): From 57Mn β- decay
I(γ): From (13C,4nγ)
   992.68E(γ): From 57Mn β- decay
I(γ): From (13C,4nγ)
M(γ): From comparison to RUL and ΔJπ
  1197.81  1061.60E(γ): From (13C,4nγ)
I(γ): From (13C,4nγ)
M(γ): From comparison to RUL and ΔJπ
  1265.52   898.4E(γ): From γ-inelastic scattering
I(γ): From γ-inelastic scattering
  1250.6E(γ): From γ-inelastic scattering
I(γ): From γ-inelastic scattering
  1265.0E(γ): From γ-inelastic scattering
I(γ): From γ-inelastic scattering
  1356.83   650.4E(γ): From γ-inelastic scattering
I(γ): From γ-inelastic scattering
   990.1E(γ): From γ-inelastic scattering
I(γ): From γ-inelastic scattering
M(γ): From comparison to RUL and ΔJπ
  1342.7E(γ): From γ-inelastic scattering
I(γ): From γ-inelastic scattering
M(γ): From comparison to RUL and ΔJπ
  1976.63   251.1I(γ): From (n,n’γ)
  1840.2E(γ): From (n,n’γ)
I(γ): From (n,n’γ)
  1976.4I(γ): From (n,n’γ)
  1989.66   791.6E(γ): From (α,pnγ)
I(γ): From (n,n’γ)
   983.0E(γ): From (13C,4nγ)
I(γ): From (n,n’γ)
M(γ): D+Q from γ(θ) in (n,n’γ); M1+E2 from RUL. From γ(θ) in (α,nγ) and (pol α,nγ) and final Jπ
  1282.85E(γ): From (13C,4nγ)
I(γ): intensity ratios for these three gammas from (n,n’γ) do not agree with results from (α,pnγ) indicating that a different level is being populated in (n,n’γ) compared to other reactions.. From (n,n’γ)
M(γ): Q(+O) from γ(θ) in (n,n’γ); E2(+M3) from RUL
  2118.6  1111.6E(γ): from (n,n’γ); added 0.75 to conform to (d,pγ) energy scale
I(γ): From (n,n’γ)
  1412.1E(γ): From (d,pγ)
I(γ): From (d,pγ)
M(γ): D+Q from γ(θ) in (n,n’γ); M1+E2 from RUL
  2104.4E(γ): From (d,pγ)
I(γ): From (d,pγ)
  2206.88  1199.9E(γ): From (n,n’γ)
I(γ): From (n,n’γ)
  1841E(γ): From γ-inelastic scattering
E(level)E(gamma)Comments
  2220.2  2083.8M(γ): from γ(θ) in (n,n’γ) and ΔJπ.
  2355.96  1158.37E(γ): From (13C,4nγ)
I(γ): consistent with Iγ=43 in (α,nγ), but not with Iγ=92 in (13C,4nγ) or Iγ=67 in (n,n’γ). From (α,pnγ)
  1348.86E(γ): From (13C,4nγ)
I(γ): From (α,pnγ)
M(γ): From comparison to RUL and ΔJπ
  2455.55  1448.52E(γ): From (13C,4nγ)
I(γ): From (13C,4nγ)
M(γ): M1+E2 (1978Kr19); disagrees with the adopted decay scheme
  2505.29   780.0E(γ): From (n,n’γ)
I(γ): From (n,n’γ)
  1798.1E(γ): From (d,pγ)
I(γ): From (d,pγ)
  2368.6E(γ): From (d,pγ)
I(γ): From (d,pγ)
  2574.5  2207.6E(γ): From (d,pγ)
I(γ): From (d,pγ)
  2574.4E(γ): From (d,pγ)
I(γ): From (d,pγ)
  2593.6  1586.4E(γ): From (n,n’γ)
I(γ): From (n,n’γ)
  1887.1E(γ): From (n,n’γ)
I(γ): From (n,n’γ)
  2593.5E(γ): From (n,n’γ)
I(γ): From (n,n’γ)
  2697.17  2330.6E(γ): From (d,pγ)
I(γ): From (d,pγ)
  2696.6I(γ): From (d,pγ)
  2878.7  1680.58E(γ): From (α,nγ)
I(γ): From (α,nγ)
M(γ): from comparison to RUL and γ(θ) in (13C,4nγ)
  2921.20  1655.37E(γ): From (d,pγ)
I(γ): From (d,pγ)
  2554.3E(γ): From (d,pγ)
I(γ): From (d,pγ)
  2906.0E(γ): From (d,pγ)
I(γ): From (d,pγ)
  2920.5E(γ): From (d,pγ)
I(γ): From (d,pγ)
  3134.8   256.03E(γ): From (13C,4nγ)
M(γ): D+Q from γ(θ) in (α,nγ); M1+E2 from RUL
  3269.26   813.73E(γ): From (13C,4nγ)
I(γ): From (13C,4nγ)
M(γ): Q from γ(θ) in (13C,4nγ); E2 from RUL
   913.37E(γ): From (13C,4nγ)
I(γ): From (13C,4nγ)
M(γ): M1+E2 (1978Kr19); disagrees with the adopted decay scheme. From γ(θ) in (α,nγ) and (pol α,nγ) and final Jπ
  3513.8   379.06E(γ): From (13C,4nγ)
I(γ): From (13C,4nγ)
  3981.18  3615.3E(γ): From (d,pγ)
  4138.57  1632.94E(γ): From (d,pγ)
I(γ): From (d,pγ)
  2783.8E(γ): From (d,pγ)
I(γ): From (d,pγ)
  3774.0E(γ): From (d,pγ)
I(γ): From (d,pγ)
  4002.4E(γ): From (d,pγ)
I(γ): From (d,pγ)
E(level)E(gamma)Comments
  4379.44  1458.09E(γ): From (d,pγ)
I(γ): From (d,pγ)
  1681.3E(γ): From (d,pγ)
I(γ): From (d,pγ)
  4013.6E(γ): From (d,pγ)
I(γ): From (d,pγ)
  4432.4  1297.8E(γ): From (13C,4nγ)
I(γ): From (13C,4nγ)
  4525.54  1256.27E(γ): From (13C,4nγ)
I(γ): From (13C,4nγ)
M(γ): Stretched-quadrupole radiation pattern in (13C,4nγ)
  4597.4  2870.8E(γ): From (d,pγ)
  4823.9  1584.0E(γ): From (d,pγ)
  4922.9  2418.3E(γ): From (d,pγ)
I(γ): From (d,pγ)
  3565.4E(γ): From (d,pγ)
I(γ): From (d,pγ)
  5362.1  2856.7E(γ): From (d,pγ)
I(γ): From (d,pγ)
  6187.1  1661.54E(γ): From (13C,4nγ)
I(γ): From (α,pnγ)
M(γ): Stretched-quadrupole radiation pattern in (13C,4nγ)
  7646.7  3854.3M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  4217.9M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  4276.5M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  4408.0M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  4463.5M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  4950.1M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  5920.8M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  6017.8M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  6381.8M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  7279.6M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  7508.8M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  7631.7M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  7645.5M(γ): From ΔJπ and systematics of primary gammas. 1978We09 and 1970Ch10 note that the 7509γ is one of the very rare primary E2 transitions and that most of the other transitions appear to be magnetic dipoles in contrast to s-wave capture where most transitions appear to be electric dipoles
  8323.0  2135.9E(γ): From (13C,4nγ)
I(γ): From (α,pnγ)
M(γ): Stretched-quadrupole radiation pattern in (13C,4nγ)

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