ADOPTED LEVELS, GAMMAS for 89Y

Author: Balraj Singh |  Citation: Nucl. Data Sheets 114, 1 (2013) |  Cutoff date: 20-Oct-2012 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-2833 keV 3S(n)= 11482 keV 3S(p)= 7076.8 keV 24Q(α)= -7966.7 keV 23
Reference: 2012WA38

References:
  A  89Sr β- decay (50.563 d)  B  89Y IT decay (15.663 S)
  C  89Zr ε decay (4.161 M)  D  89Zr ε decay (78.41 H)
  E  74Ge(18O,2npγ),76Ge(18O,4NPG)  F  87Rb(α,2nγ)
  G  88Sr(p,γ)  H  88Sr(p,p’),(pol p,p) IAR
  I  88Sr(d,n)  J  88Sr(3He,d)
  K  88Sr(16O,15N)  L  89Y(γ,γ’)
  M  89Y(E,E’)  N  89Y(n,n’)
  O  89Y(n,n’γ)  P  89Y(p,p’),(pol p,p’)
  Q  89Y(p,p’γ)  R  89Y(d,d’)
  S  89Y(3He,3He’)  T  89Y(α,α’)
  U  90Zr(E,E’p)  V  90Zr(n,d)
  W  90Zr(d,3He),(pol d,3He)  X  92Zr(p,α),(pol p,α)
  Y  88Sr(p,γ) IAR  Z  88Sr(p,n) IAR
  a  89Y(γ,p) IAR  b  89Y(γ,p),(γ,XN):GDR
  c  89Y(E,E’p) IAR  d  89Y(E,p): GIANT RES
  e  89Y(π++’),(π--’)  f  89Y(π+,K+):HYPERNUCLEUS
  g  89Y(HI,HI)  h  90Zr(pol t,α),(t,α)
  i  90Zr(α,α’p)  j  90Zr(6Li,7Be)
  k  90Zr(12C,13N),(13C,14N)  l  91Zr(d,α)
  m  93Nb(3He,7Be) 

General Comments:

Other reactions:

89Y(e,γ) E=50-100 keV: 1987Am01

89Y(K-,K-) (analysis): 1983Ba71

89Y(γ,γ) E=35.86, 39.36 keV: 1996Ra30, 1996Ra29

89Y(π+,K+) E=1060 MeV/c: 1996Ha05, 1996Ha47, 1995Aj01, 1991Pi07, 1989Pi11, 1989Ch32, 1988Ch48. Measured |L hypernuclei spectra.

89Y(K--) E=720 MeV/c: 1981Be17 (also 1981Bo09)

90Zr(p,2p): 1967Ar11 (E=156 MeV), 1971La16 (E=600 MeV)

90Zr(π+,pπ+), (π-,pπ-) E=500 MeV: 1998Mo09

93Nb(γ,α) E=16-25 MeV: 1991An07, 1991An22

NMR studies (recent): 1997Se12, 1997Au07, 1996Oh03, 1996Wi28, 1996St23, 1995So19, 1995Go39, 1994Ma25, 1993Al02

Hyperfine structure measurements (selected): 2010Ba31, 2006Ca38, 1994Ri10, 1992Vi04, 1988Go04

Structure calculations (selected references only): 2011Ro08, 1997He24, 1996Ri01, 1995Re08, 1995Gu09, 1992Si14, 1990Va13. C. Sharma et al., Eur. Phys. J. A48, 138 (2012) analyzed structures of positive-parity bands by projected shell-model calculations

89Y isotope identified using mass spectrometry technique by F.W. Aston, Nature 112, 449 (1923)

Levels: Levels marked with XREF=Y in the level table refer to the following reactions and levels populated therein:

Levels: 88Sr(p,γ) IAR: 12076, 13070, 14060, 14492, 15837

Levels: 88Sr(p,n) IAR: 12076, 13070, 13991, 14060, 14492, 14781

Levels: 89Y(γ,p),(γ,xn):GDR: 16790, 21800

Levels: 89Y(γ,p) IAR: 14060, 15800, 16800, 17000 (GDR), 17400, 21000 (GDR)

Levels: 89Y(e,e’p) IAR: 13000, 14500, 14900, 15800, 16700, 17700, 18900, 20300, 21700

Levels: 89Y(e,p): giant res: 16800, 27000

Levels: 89Y(π++’),(π--’): 0

Levels: 89Y(π+,K+):hypernucleus: 0, 6010, 7380, 12790, 14420, 19980, 21680, 27000

Levels: 89Y(HI,HI): 0

Levels: 90Zr(pol t,α),(t,α): 0, 909, 1507, 1745

Levels: 90Zr(α,α’p): 0, 910, 1600

Levels: 90Zr(6Li,7Be): 0, 909, 1507, 1745

Levels: 90Zr(12C,13N),(13C,14N): 0, 910, 1510, 1740, 2220

Levels: 91Zr(d,α): 0, 910, 1510, 1740, 4310

Levels: 93Nb(3He,7Be): 0, 910

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

Q-value: S(2n)=20833.9 28, S(2p)=17689.8 25 (2011AuZZ)

Q-value: Values in 2003Au03: Q(β-)=-2832.9 28, S(n)=11474 3, S(p)=7069.0 26, Q(α)=-7959.3 26, S(2n)=20825.7 28, S(2p)=17681.9 26










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
      0.0ABCDEFG IJKLMNOPQRSTUVWX      efghijklm 1/2- STABLE      
    908.97 3 AB DEFG IJKLMNOPQ STU WX         hijklm 9/2+ 15.663 s 5 
% IT = 100
    908.960 25 
   100
M4+E5
      0.0
1/2-
   1507.41 9   C  FG IJKLMNOPQRSTUVWX         hijkl  3/2- 23.9 fs +25-21     1507.42 10 
   100
M1+E2
      0.0
1/2-
   1744.74 18    D FG IJKLMNOPQRSTU WX         hijkl  5/2- 0.64 ps 6     1744.7 2 
   100
E2
      0.0
1/2-
   2222.43 18      FG IJK MNOPQRST   X            k   5/2+ 0.97 ps 28      715.2 3 
   1313.2 3 
    46.0 9 
   100.0 9 
[E1]
[E2]
   1507.41
    908.97
3/2-
9/2+
   2529.80 20    D FG     MNOPQRST   X                7/2+ 0.08 ps 4     1620.8 2 
   100

    908.97
9/2+
   2566.55 15    DEFG      NOP                        11/2+ 0.35 ps 7     1657.5 2 
   100
M1+E2
    908.97
9/2+
   2622.1 3    D FG  JK  NOPQ     WX                9/2+ 0.21 ps 10     1713.1 3 
   100
(M1+E2)
    908.97
9/2+
   2687?      G                                        
   2871.7 4       G IJ  MNOPQRST V X                (7/2)+ < 0.2 ps    1962.8 4 
   100

    908.97
9/2+
   2881.53 10       G IJKL NOP R  UV X                (3/2)- 19.9 fs +21-19     2881.48 10 
   100

      0.0
1/2-
   2892.98 15     EF        OP                        13/2+ 0.18 ps 3      326.5 5 
   1984.1 2 
    ≈1.4
   100 3 

E2
   2566.55
    908.97
11/2+
9/2+
   3067.76 10       G IJKL NOP                        3/2- 45.0 fs +15-11     1559.8 5 
   3067.7 1 
    10.6 8 
   100.0 8 

(M1+E2)
   1507.41
      0.0
3/2-
1/2-
   3107.26 24      FG I  LMNOP RST  WX                (5/2)- 0.034 ps 3     1361.8 9 
   1599.8 4 
   3107.3 3 
    11.0 9 
    10.2 10 
   100.0 13 
(M1+E2)
(M1+E2)
[E2]
   1744.74
   1507.41
      0.0
5/2-
3/2-
1/2-
   3138.9 3       G    L NOP R   V X                (5/2)- 0.11 ps +7-3      916.1 5 
   1631.6 4 
   3139.1 5 
    12.1 10 
    16.3 8 
   100.0 12 
[E1]

[E2]
   2222.43
   1507.41
      0.0
5/2+
3/2-
1/2-
   3247.6 5       G       OP                        (3/2,5/2)      1740.2 5 
   3247.5 9 
   100.0 19 
     7.4 19 
D+Q

   1507.41
      0.0
3/2-
1/2-
   3343.44 15     EF        O                         13/2- 0.42 ps 14      450.5 1 
    776.89 6 
     6.2 6 
   100 3 
E1
E1
   2892.98
   2566.55
13/2+
11/2+
   3360                       X                       
   3410.7 4       G       OP                        (5/2+)      2501.4 5 
   100

    908.97
9/2+
   3451.3 6       G       OP                        (7/2+)      2542.3 6 
   100
D+Q
    908.97
9/2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   3503.6 4       G       OP                        (7/2-)       364.7 5 
   1996.2 5 
     6.3 10 
   100.0 10 


   3138.9
   1507.41
(5/2)-
3/2-
   3515.9 3       G IJKL  OP     V                  (3/2)-      1770.0 10 ?
   3515.9 3 
 
   100

(M1+E2)
   1744.74
      0.0
5/2-
1/2-
   3557.4 5       G       OP     V                  (7/2-)      1812.5 9 
   2050.1 8 
   2648.3 6 
    25 4 
   100 3 
    76 3 


D+Q
   1744.74
   1507.41
    908.97
5/2-
3/2-
9/2+
   3560                       X                (1/2)        
   3621.1 6       G       O         Y         ij l  (11/2)      2712.1 6 
   100
D+Q
    908.97
9/2+
   3630.3 6               OP                        (11/2)+      2721.3 6 
   100
(M1+E2)
    908.97
9/2+
   3715.3 4       G IJK M OP RST    YZ    e      lm 5/2+       843.6 5 
   1492.7 4 
   2806.7 8 
    31.1 23 
    80 4 
   100 5 

(M1+E2)

   2871.7
   2222.43
    908.97
(7/2)+
5/2+
9/2+
   3747.7 8               OP                        (9/2)+      2838.7 8 
   100
(M1+E2)
    908.97
9/2+
   3752.9 4               O                         (5/2+)       341.9 5 
   2008.3 6 
   2844.2 8 
    12.0 12 
   100 3 
    35 3 



   3410.7
   1744.74
    908.97
(5/2+)
5/2-
9/2+
   3790                       X                       
   3810                       X                       
   3848.3 4       G       OP                        (3/2-,5/2-)      2103.5 5 
   2340.8 6 
   100.0 14 
    17.8 14 
(M1+E2)
(M1+E2)
   1744.74
   1507.41
5/2-
3/2-
   3862.4 5       G       OP                        (3/2,5/2)-      2355.1 5 
   3861.8 9 
   100.0 24 
    31.1 24 


   1507.41
      0.0
3/2-
1/2-
   3924 5                P                               
   3976.8 6               OP                        (11/2)+      1447.0 5 
   100

   2529.80
7/2+
   3992.2 1       G I  LM OP  STU                   3/2- 9.3 fs +11-10     3992.1 1 
   100
(M1+E2)
      0.0
1/2-
   4015.3 7       G IJ    OP                        1/2+      1792.8 7 
   4015.4 15 
    75 7 
   100 7 


   2222.43
      0.0
5/2+
1/2-
   4022.96 23         I     OP R                      (3/2)-       955.0 3 
   1800.8 4 
   2278.6 7 
   2515.3 6 
   4022.9 15 
    57 3 
    73 4 
    77 4 
   100 4 
    40 4 
(M1+E2)
(M1+E2)

(M1+E2)

   3067.76
   2222.43
   1744.74
   1507.41
      0.0
3/2-
5/2+
5/2-
3/2-
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   4060                       X                       
   4104.9 5               OP                        (7/2+)      1574.9 7 
   1882.5 8 
   3196.3 12 
   100 6 
    78 6 
    61 5 

(M1+E2)
(M1+E2)
   2529.80
   2222.43
    908.97
7/2+
5/2+
9/2+
   4132.22 16     EF                                  15/2- 1.59 ps 28      788.6 1 
   1239.28 7 
    49 3 
   100 3 
M1+E2
E1
   3343.44
   2892.98
13/2-
13/2+
   4171.3 1       G    LM OP  ST          e   i   m 3/2-,5/2- 10.1 fs +15-11     4171.2 1 
   100

      0.0
1/2-
   4188.1 6         IJK   OP R                      5/2+      2680.9 7 
   3278.7 9 
   100.0 22 
    19.2 22 


   1507.41
    908.97
3/2-
9/2+
   4230.4 12               OP R                      (7/2)      3321.4 12 
   100

    908.97
9/2+
   4251 5            L   P                               
   4254.40 23      F                                  (15/2+) 1.4 ps 7     1361.2 2 
   100

   2892.98
13/2+
   4309.3 6               OP   T          e   i  l  (7/2)-      2086.7 7 
   3400.5 9 
   100.0 14 
    13.1 14 


   2222.43
    908.97
5/2+
9/2+
   4334.1 12               OP RS                          3425.1 12 
   100

    908.97
9/2+
   4354.7 10               OP RS                          3445.7 10 
   100

    908.97
9/2+
   4383 5                P                               
   4408.4 8               OP                        1/2,3/2,5/2-      2901.0 10 
   4408.2 13 
    67 8 
   100 8 


   1507.41
      0.0
3/2-
1/2-
   4449.75 16     EF                                  17/2- 4.5 ps 10      317.5 1 
   1106.5 1 
    50.0 20 
   100.0 10 
M1
E2
   4132.22
   3343.44
15/2-
13/2-
   4457.6 7         I     OP   T                    7/2-,9/2-      1927.8 6 
   100

   2529.80
7/2+
   4460 20         IJ         T                    (1/2+)        
   4476.3 13         IJ    OP RST                    (5/2+)      2253.8 12 
   100

   2222.43
5/2+
   4489 5                P RST                           
   4508 5                P R                             
   4529.3 16               OP       X      e g       5/2+,7/2+      3620.3 16 
   100

    908.97
9/2+
   4537.5 20               OP                        3/2-,5/2-      4537.4 20 
   100

      0.0
1/2-
   4555 5                P   T                    7/2-,9/2-        
   4588 5         IJK    P   T                    5/2+        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   4603 5                P   T                    7/2-,9/2-        
   4616.8 5            L                            1/2,3/2,5/2-      4616.7 5 
 

      0.0
1/2-
   4625.8 5            L                            1/2,3/2,5/2-      4625.7 5 
 

      0.0
1/2-
   4636 5                P                               
   4654 5                P                               
   4682 5                P                               
   4737 5                P                        3/2-,5/2-        
   4770 5                P RS                            
   4785 5                P R                             
   4817 5                P R                             
   4825.38 17     EF                                  17/2+ ≥ 3.5 ps     570.5 3 
    693.2 2 
   1931.9 3 
    11 6 
   100 7 
    14 4 

E1
(E2)
   4254.40
   4132.22
   2892.98
(15/2+)
15/2-
13/2+
   4831 5          J     P              e       m 3/2+,5/2+        
   4838.59 17      F                                  19/2- 21 ps 8      388.9 1 
    706.3 1 
   100 1 
    51 9 
M1+E2
E2
   4449.75
   4132.22
17/2-
15/2-
   4849 5         I      P                        3/2-,5/2-        
   4862 5         I      P       X                       
   4888 5                P       X                       
   4907 5                P       X                       
   4920.46 17     EF                                  (19/2+) 6.2 ps 21       95.07 3 
    470.72 5 
    38 3 
   100 5 
(M1+E2)
E1
   4825.38
   4449.75
17/2+
17/2-
   4927 5          JK    P                               
   4954 5          JK    P                               
   4973 5                P                               
   4992 1            L                            1/2,3/2,5/2-      4991 1 
 

      0.0
1/2-
   5006 8                P    U W         g       (5/2)-        
   5026 8                P    U                          
   5046 8                P    U                          
   5075 8         IJK    P                g i   m (1/2+)        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   5085.4 6            L   P           b    g     m 1/2,3/2,5/2-      5085.3 6 
 

      0.0
1/2-
   5099 8                P       X                       
   5115 8                P  S    X                       
   5125 8                P  S    X                       
   5152.1 8            L   P              e g i   m 1/2,3/2,5/2-      5151.9 8 
 

      0.0
1/2-
   5167.7 3            L   P         Z      g i     1/2,3/2,5/2-      3660.6 10 
   5167.5 3 
     4 2 
   100 2 


   1507.41
      0.0
3/2-
1/2-
   5183 8          J     P           b    g i     3/2+,5/2+        
   5211 8                P       X        g  j    (3/2-)        
   5257 8                P                               
   5263.88 20     EF                                  (21/2+) 1.46 ps 28      343.37 12 
    425.6 3 
   100.0 18 
     1.55 24 
M1
[E1]
   4920.46
   4838.59
(19/2+)
19/2-
   5275 8          J     P         Z      g  j    (1/2+)        
   5289 8                P                        3/2-,5/2-        
   5303 8                P                               
   5309.83 20      F                                  (21/2-) 4.5 ps 9      471.1 2 
    860.1 1 
   100 10 
     5.3 6 
(M1)
(E2)
   4838.59
   4449.75
19/2-
17/2-
   5321 8                P                               
   5343 8         IJ     P              e g    l  (1/2+)        
   5362 8         I      P                               
   5382 8                P       X        g    lm (1/2)        
   5412.1 4      F                                  (19/2-) 1.25 ps 28      962.3 3 
   100

   4449.75
17/2-
   5419.4 5            L   P              e g ij    1/2,3/2,5/2-      5419.2 5 
 

      0.0
1/2-
   5430 8          J     P                        (3/2+,5/2+)        
   5455 8                P                               
   5476 8                P                               
   5506 8                P                               
   5542 8                P                               
   5562 8                P                               
   5582 8                P                               
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   5592 8                P       X                       
   5614.4 15            L                            1/2,3/2,5/2-      5614.2 15 
 

      0.0
1/2-
   5625.8 2         IJ L   P       XY       g  j    1/2,3/2,5/2-      4117.4 5 
   5625.6 2 
     9 2 
   100 2 


   1507.41
      0.0
3/2-
1/2-
   5631 8         IJ     P       X                       
   5647 8         I      P                               
   5653.9 15            L                            1/2,3/2,5/2-      5653.7 15 
 

      0.0
1/2-
   5668 8                P       X                       
   5694 8                P  S    X                       
   5725 8          J     P                               
   5739 8          J     P                               
   5753 8                P                               
   5774 8                P                               
   5789.4 8            L   P         Z b    g    l  1/2,3/2,5/2-      5789.2 8 
 

      0.0
1/2-
   5796.4 8            L                            1/2,3/2,5/2-      5796.2 8 
 

      0.0
1/2-
   5801 8                P                               
   5820 8                P                               
   5843 8                P                               
   5853 8                P                               
   5879.4 4      F                                  (19/2+) 0.14 ps 10      615.5 3 
   100
(M1)
   5263.88
(21/2+)
   5888 8         IJK    P         Z      g     m 3/2+,5/2+        
   5910.7 2            L   P           b    g i     1/2,3/2,5/2-      3028 2 
   5910.5 2 
     4 3 
   100 3 


   2881.53
      0.0
(3/2)-
1/2-
   5923.4 9            L                            1/2,3/2,5/2-      5923.2 9 
 

      0.0
1/2-
   5950 8                P                               
   5981 8                P                               
   6004 8                P                               
      6.01E3 13                                f               
   6100 20         IJ                              3/2+,5/2+        
   6122.9 2            L                            1/2,3/2,5/2-      6122.7 2 
 

      0.0
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   6158.9 4 ?     F                                        895.0 3 ?
 

   5263.88
(21/2+)
   6198.90 21     EF                                  (23/2+) 0.19 ps 4      935.01 5 
   1360.3 3 ?
   100
 
M1+E2

   5263.88
   4838.59
(21/2+)
19/2-
   6200 20         IJ                              7/2+,9/2+        
   6201.9 8         I  L                            1/2,3/2,5/2-      6201.7 8 
 

      0.0
1/2-
   6206.3 3         I  L                            1/2,3/2,5/2-      6206.1 3 
 

      0.0
1/2-
   6275.6 2          JKL                            1/2,3/2,5/2-      6275.4 2 
 

      0.0
1/2-
   6297.6 3          JKL                            1/2,3/2,5/2-      6297.4 3 
 

      0.0
1/2-
   6300 20         I                               1/2+        
   6331.6 2            L                            1/2,3/2,5/2-      6331.4 2 
 

      0.0
1/2-
   6359.1 2            L                            1/2,3/2,5/2-      6358.9 2 
 

      0.0
1/2-
   6398.2 2            L                            1/2,3/2,5/2-      6398.0 2 
 

      0.0
1/2-
   6441.5 2            L                            1/2,3/2,5/2-      2925 3 
   6441.2 2 
    10 8 
   100 8 


   3515.9
      0.0
(3/2)-
1/2-
   6472.3 18         IJ L                            1/2,3/2,5/2-      6472.0 18 
 

      0.0
1/2-
   6479 3            L                            1/2,3/2,5/2-      6479 3 
 

      0.0
1/2-
   6493.5 8         IJ L                            1/2,3/2,5/2-      6493.5 8 
 

      0.0
1/2-
      6.5E3 3                     U                   (7/2-)        
   6532.3 3            L                            1/2,3/2,5/2-      6532.0 3 
 

      0.0
1/2-
   6592.2 3          J L                            1/2,3/2,5/2-      6591.9 3 
 

      0.0
1/2-
   6608.9 5          J L                            1/2,3/2,5/2-      6608.6 5 
 

      0.0
1/2-
   6651.6 8            L                            1/2,3/2,5/2-      6651.3 8 
 

      0.0
1/2-
   6666.8 8            L                            1/2,3/2,5/2-      6666.5 8 
 

      0.0
1/2-
   6674.4 3      F                                  (23/2+) ≤ 0.7 ps    1410.5 2 
   100

   5263.88
(21/2+)
   6680 20          J                                     
   6728 2            L                            1/2,3/2,5/2-      6728 2 
 

      0.0
1/2-
   6750            M                           1.0 MeV 2       
   6751.1 12            L                            1/2,3/2,5/2-      6750.8 12 
 

      0.0
1/2-
   6772.0 14            L                            1/2,3/2,5/2-      6771.7 14 
 

      0.0
1/2-
   6780 20          JK           W Y             m 7/2-        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   6782.9 6            L                            1/2,3/2,5/2-      6782.6 6 
 

      0.0
1/2-
   6798.2 5            L                            1/2,3/2,5/2-      6797.9 5 
 

      0.0
1/2-
   6852.4 8            L                            1/2,3/2,5/2-      6852.1 8 
 

      0.0
1/2-
   6866 2            L                            1/2,3/2,5/2-      6866 2 
 

      0.0
1/2-
   6880                  S                            
   6921 2            L                            1/2,3/2,5/2-      6921 2 
 

      0.0
1/2-
   6934.7 11            L                            1/2,3/2,5/2-      6934.4 11 
 

      0.0
1/2-
   6944.5 12            L                            1/2,3/2,5/2-      6944.2 12 
 

      0.0
1/2-
   6959.6 14            L                            1/2,3/2,5/2-      6959.3 14 
 

      0.0
1/2-
   6987.4 15            L                            1/2,3/2,5/2-      6987.1 15 
 

      0.0
1/2-
   7003.8 3            L                            1/2,3/2,5/2-      7003.5 3 
 

      0.0
1/2-
   7066.8 15            L                            1/2,3/2,5/2-      7066.5 15 
 

      0.0
1/2-
   7077.7 3            L                            1/2,3/2,5/2-      7077.4 3 
 

      0.0
1/2-
      7.1E3                   T                           
   7106 3            L                            1/2,3/2,5/2-      7106 3 
 

      0.0
1/2-
   7118.2 6            L                            1/2,3/2,5/2-      7117.9 6 
 

      0.0
1/2-
   7147.1 6            L                            1/2,3/2,5/2-      7146.8 6 
 

      0.0
1/2-
   7178.6 3            L                            1/2,3/2,5/2-      7178.3 3 
 

      0.0
1/2-
   7183.7 3      F                                  (25/2+) 0.21 ps 7      985 1 ?
   1920.2 3 
   ≈36
   100 22 

[E2]
   6198.90
   5263.88
(23/2+)
(21/2+)
   7190?         J                                     
   7193.8 4      F                                  (23/2+) 0.35 ps 14      994.5 5 
   1930 1 
   100 22 
   ≈89


   6198.90
   5263.88
(23/2+)
(21/2+)
   7198 2            L                            1/2,3/2,5/2-      7198 2 
 

      0.0
1/2-
   7225.3 8            L                            1/2,3/2,5/2-      7225.0 8 
 

      0.0
1/2-
   7240 3            L                            1/2,3/2,5/2-      7240 3 
 

      0.0
1/2-
   7255 3            L                            1/2,3/2,5/2-      7255 3 
 

      0.0
1/2-
   7259.5 3      F                                  (23/2+)      1995.6 4 
   100

   5263.88
(21/2+)
      7.3E3 40                       W                        
   7304.4 5            L                            1/2,3/2,5/2-      7304.1 5 
 

      0.0
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   7325.4 9            L                            1/2,3/2,5/2-      7325.1 9 
 

      0.0
1/2-
      7.38E3 21                                f               
   7383.7 5            L                            1/2,3/2,5/2-      7383.4 5 
 

      0.0
1/2-
   7420.4 8            L                            1/2,3/2,5/2-      7420.1 8 
 

      0.0
1/2-
   7431.6 3     EF                                  (25/2+) 0.49 ps 14      172.1 1 
    757.1 2 
   1232.6 2 
    34 4 
   ≈42
   100 8 
(M1)
(M1)
(M1)
   7259.5
   6674.4
   6198.90
(23/2+)
(23/2+)
(23/2+)
   7452.1 8            L                            1/2,3/2,5/2-      7451.8 8 
 

      0.0
1/2-
   7475.2 15            L                            1/2,3/2,5/2-      7474.9 15 
 

      0.0
1/2-
   7484.1 11            L                            1/2,3/2,5/2-      7483.8 11 
 

      0.0
1/2-
   7527.9 14            L                            1/2,3/2,5/2-      7527.6 14 
 

      0.0
1/2-
   7536 3            L                            1/2,3/2,5/2-      7536 3 
 

      0.0
1/2-
   7548 5            L                            1/2,3/2,5/2-      7548 5 
 

      0.0
1/2-
   7556 4            L                            1/2,3/2,5/2-      7556 4 
 

      0.0
1/2-
   7566 3            L                            1/2,3/2,5/2-      7566 3 
 

      0.0
1/2-
   7588.1 18            L                            1/2,3/2,5/2-      7587.8 18 
 

      0.0
1/2-
   7590.0 3      F                                  (25/2+) 0.35 ps 14      396.1 2 
   100
(M1)
   7193.8
(23/2+)
   7618.4 9            L                            1/2,3/2,5/2-      7618.1 9 
 

      0.0
1/2-
   7640.8 11            L                            1/2,3/2,5/2-      7640.4 11 
 

      0.0
1/2-
   7652.3 20            L                            1/2,3/2,5/2-      7651.9 20 
 

      0.0
1/2-
   7666.1 6            L                            1/2,3/2,5/2-      7665.7 6 
 

      0.0
1/2-
   7692.2 8            L                            1/2,3/2,5/2-      7691.8 8 
 

      0.0
1/2-
   7703.3 15            L                            1/2,3/2,5/2-      7702.9 15 
 

      0.0
1/2-
   7714.0 14            L                            1/2,3/2,5/2-      7713.6 14 
 

      0.0
1/2-
   7722.2 9          JKL             Z        ij    (1/2+)      7721.8 9 
 

      0.0
1/2-
   7750.5 5            L                            1/2,3/2,5/2-      7750.1 5 
 

      0.0
1/2-
   7774.4 5            L                            1/2,3/2,5/2-      7774.0 5 
 

      0.0
1/2-
   7787.5 3            L                            1/2,3/2,5/2-      7787.1 3 
 

      0.0
1/2-
   7799.2 8            L                            1/2,3/2,5/2-      7798.8 8 
 

      0.0
1/2-
   7811.8 17            L                            1/2,3/2,5/2-      7811.4 17 
 

      0.0
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   7830.2 6            L                            1/2,3/2,5/2-      7829.8 6 
 

      0.0
1/2-
   7834.6 3     EF                                  (27/2+) 1.25 ps 28      244.6 1 
    402.9 2 
    650.9 1 
    58 8 
  ≈226
   100 13 
(M1)
M1
(M1)
   7590.0
   7431.6
   7183.7
(25/2+)
(25/2+)
(25/2+)
   7838.7 8            L                            1/2,3/2,5/2-      7838.3 8 
 

      0.0
1/2-
   7866.8 17            L                            1/2,3/2,5/2-      7866.4 17 
 

      0.0
1/2-
   7902.5 5            L                            1/2,3/2,5/2-      7902.1 5 
 

      0.0
1/2-
   7920.5 3            L                            1/2,3/2,5/2-      7920.1 3 
 

      0.0
1/2-
   7922.7 2            L                            1/2,3/2,5/2-      7922.3 2 
 

      0.0
1/2-
   7937.8 9            L                            1/2,3/2,5/2-      7937.4 9 
 

      0.0
1/2-
   7961.7 11            L                            1/2,3/2,5/2-      7961.3 11 
 

      0.0
1/2-
   7968.8 9            L                            1/2,3/2,5/2-      7968.4 9 
 

      0.0
1/2-
   7986.0 8            L                            1/2,3/2,5/2-      7985.6 8 
 

      0.0
1/2-
   7996.1 5            L                            1/2,3/2,5/2-      7995.7 5 
 

      0.0
1/2-
   8018 2            L                            1/2,3/2,5/2-      8018 2 
 

      0.0
1/2-
   8027.7 8            L                            1/2,3/2,5/2-      8027.3 8 
 

      0.0
1/2-
   8050            M                           1.2 MeV 2       
   8067.3 5            L                            1/2,3/2,5/2-      8066.9 5 
 

      0.0
1/2-
   8099.0 14            L                            1/2,3/2,5/2-      8098.6 14 
 

      0.0
1/2-
   8129.3 3            L                            1/2,3/2,5/2-      8128.9 3 
 

      0.0
1/2-
   8142.1 12            L                            1/2,3/2,5/2-      8141.7 12 
 

      0.0
1/2-
   8150.8 17            L                            1/2,3/2,5/2-      8150.4 17 
 

      0.0
1/2-
   8159.7 9            L                            1/2,3/2,5/2-      8159.3 9 
 

      0.0
1/2-
   8175.6 9            L                            1/2,3/2,5/2-      8175.2 9 
 

      0.0
1/2-
   8198.9 5            L                            1/2,3/2,5/2-      8198.5 5 
 

      0.0
1/2-
   8210.9 8            L                            1/2,3/2,5/2-      8210.5 8 
 

      0.0
1/2-
   8221.2 3            L                            1/2,3/2,5/2-      8220.8 3 
 

      0.0
1/2-
   8264.2 3     EF                                  (29/2+) 0.97 ps 21      429.6 1 
    832.9?
   100 16 
   <15
M1+E2
[E2]
   7834.6
   7431.6
(27/2+)
(25/2+)
   8270.7 6            L                            1/2,3/2,5/2-      8270.3 6 
 

      0.0
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8285.4 17            L                            1/2,3/2,5/2-      8285.0 17 
 

      0.0
1/2-
   8311.0 5            L                            1/2,3/2,5/2-      8310.6 5 
 

      0.0
1/2-
   8320.1 6            L                            1/2,3/2,5/2-      8319.7 6 
 

      0.0
1/2-
   8330.4 14            L                            1/2,3/2,5/2-      8330.0 14 
 

      0.0
1/2-
   8338.1 8            L                            1/2,3/2,5/2-      8337.7 8 
 

      0.0
1/2-
   8369 2          J L                            1/2,3/2,5/2-      8369 2 
 

      0.0
1/2-
   8380.0 9            L                            1/2,3/2,5/2-      8379.6 9 
 

      0.0
1/2-
   8403.1 9            L                            1/2,3/2,5/2-      8402.7 9 
 

      0.0
1/2-
   8438.0 8            L                            1/2,3/2,5/2-      8437.6 8 
 

      0.0
1/2-
   8455 4            L                            1/2,3/2,5/2-      8455 4 
 

      0.0
1/2-
   8466.9 8            L                            1/2,3/2,5/2-      8466.5 8 
 

      0.0
1/2-
   8483.2 9            L                            1/2,3/2,5/2-      8482.8 9 
 

      0.0
1/2-
   8495.2 8            L                            1/2,3/2,5/2-      8494.8 8 
 

      0.0
1/2-
   8513.5 5            L                            1/2,3/2,5/2-      8513.1 5 
 

      0.0
1/2-
   8530.6 8            L                            1/2,3/2,5/2-      8530.2 8 
 

      0.0
1/2-
   8548.3 12            L                            1/2,3/2,5/2-      8547.9 12 
 

      0.0
1/2-
   8556.0 9            L                            1/2,3/2,5/2-      8555.6 9 
 

      0.0
1/2-
   8568.0 6            L                            1/2,3/2,5/2-      8567.6 6 
 

      0.0
1/2-
   8586.9 6            L                            1/2,3/2,5/2-      8586.5 6 
 

      0.0
1/2-
   8603 3            L                            1/2,3/2,5/2-      8603 3 
 

      0.0
1/2-
   8610.8 12            L                            1/2,3/2,5/2-      8610.4 12 
 

      0.0
1/2-
   8642.1 8            L                            1/2,3/2,5/2-      8641.6 8 
 

      0.0
1/2-
   8668.0 5            L                            1/2,3/2,5/2-      8667.5 5 
 

      0.0
1/2-
   8720.4 4     EF                                  (31/2+) 0.48 ps 14      456.2 2 
    885.9?
   100 16 
   <23
(M1)
[E2]
   8264.2
   7834.6
(29/2+)
(27/2+)
   8764.2 3            L                            1/2,3/2,5/2-      8763.7 3 
 

      0.0
1/2-
   8779.3 11            L                            1/2,3/2,5/2-      8778.8 11 
 

      0.0
1/2-
   8843.4 5            L                            1/2,3/2,5/2-      8842.9 5 
 

      0.0
1/2-
   8864 4            L                            1/2,3/2,5/2-      8864 4 
 

      0.0
1/2-
   8877.3 5            L                            1/2,3/2,5/2-      8876.8 5 
 

      0.0
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8899.3 6            L                            1/2,3/2,5/2-      8898.8 6 
 

      0.0
1/2-
   8926.3 14            L                            1/2,3/2,5/2-      8925.8 14 
 

      0.0
1/2-
   8981 3            L                            1/2,3/2,5/2-      8981 3 
 

      0.0
1/2-
   8994.5 17            L                            1/2,3/2,5/2-      8994.0 17 
 

      0.0
1/2-
   9002.8 15            L                            1/2,3/2,5/2-      9002.3 15 
 

      0.0
1/2-
   9024.2 9            L                            1/2,3/2,5/2-      9023.7 9 
 

      0.0
1/2-
   9043.4 6            L                            1/2,3/2,5/2-      9042.9 6 
 

      0.0
1/2-
   9057.8 15            L                            1/2,3/2,5/2-      9057.3 15 
 

      0.0
1/2-
   9069.0 11            L                            1/2,3/2,5/2-      9068.5 11 
 

      0.0
1/2-
   9082 2            L                            1/2,3/2,5/2-      9082 2 
 

      0.0
1/2-
   9093.4 8            L                            1/2,3/2,5/2-      9092.9 8 
 

      0.0
1/2-
   9112.7 19            L                            1/2,3/2,5/2-      9112.2 19 
 

      0.0
1/2-
   9121.4 8            L                            1/2,3/2,5/2-      9120.9 8 
 

      0.0
1/2-
   9147.0 9            L                            1/2,3/2,5/2-      9146.5 9 
 

      0.0
1/2-
   9161.2 14            L                            1/2,3/2,5/2-      9160.7 14 
 

      0.0
1/2-
   9175.7 9            L                            1/2,3/2,5/2-      9175.2 9 
 

      0.0
1/2-
   9191.2 8            L                            1/2,3/2,5/2-      9190.7 8 
 

      0.0
1/2-
   9204.5 5            L                            1/2,3/2,5/2-      9204.0 5 
 

      0.0
1/2-
   9240.0 6            L                            1/2,3/2,5/2-      9239.5 6 
 

      0.0
1/2-
   9256.1 6            L                            1/2,3/2,5/2-      9255.6 6 
 

      0.0
1/2-
   9280.2 15            L                            1/2,3/2,5/2-      9279.7 15 
 

      0.0
1/2-
   9290.8 15            L                            1/2,3/2,5/2-      9290.3 15 
 

      0.0
1/2-
   9301.1 12            L                            1/2,3/2,5/2-      9300.6 12 
 

      0.0
1/2-
   9308.4 14            L                            1/2,3/2,5/2-      9307.9 14 
 

      0.0
1/2-
   9320 2            L                            1/2,3/2,5/2-      9319 2 
 

      0.0
1/2-
   9326.7 11            L                            1/2,3/2,5/2-      9326.2 11 
 

      0.0
1/2-
   9351.2 8            L                            1/2,3/2,5/2-      9350.7 8 
 

      0.0
1/2-
   9374.7 8            L                            1/2,3/2,5/2-      9374.2 8 
 

      0.0
1/2-
   9401.8 18            L                            1/2,3/2,5/2-      9401.3 18 
 

      0.0
1/2-
   9410.0 17            L                            1/2,3/2,5/2-      9409.5 17 
 

      0.0
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   9449.6 9            L                            1/2,3/2,5/2-      9449.1 9 
 

      0.0
1/2-
   9471 3            L                            1/2,3/2,5/2-      9470 3 
 

      0.0
1/2-
   9482.0 15            L                            1/2,3/2,5/2-      9481.5 15 
 

      0.0
1/2-
   9503 3            L                            1/2,3/2,5/2-      9502 3 
 

      0.0
1/2-
   9532 4            L                            1/2,3/2,5/2-      9531 4 
 

      0.0
1/2-
   9541 3            L                            1/2,3/2,5/2-      9540 3 
 

      0.0
1/2-
   9575.6 18            L                            1/2,3/2,5/2-      9575.0 18 
 

      0.0
1/2-
   9593.6 15            L                            1/2,3/2,5/2-      9593.0 15 
 

      0.0
1/2-
   9623.7 11            L                            1/2,3/2,5/2-      9623.1 11 
 

      0.0
1/2-
   9660.9 8            L                            1/2,3/2,5/2-      9660.3 8 
 

      0.0
1/2-
   9679.4 2            L                            1/2,3/2,5/2-      9678.8 2 
 

      0.0
1/2-
   9901.0 8            L                            1/2,3/2,5/2-      9900.4 8 
 

      0.0
1/2-
   9912.0 8            L                            1/2,3/2,5/2-      9911.4 8 
 

      0.0
1/2-
   9964.2 9            L                            1/2,3/2,5/2-      9963.6 9 
 

      0.0
1/2-
   9973.2 6            L                            1/2,3/2,5/2-      9972.6 6 
 

      0.0
1/2-
   9990.3 12            L                            1/2,3/2,5/2-      9989.7 12 
 

      0.0
1/2-
  10005.8 15            L                            1/2,3/2,5/2-     10005.2 15 
 

      0.0
1/2-
  10017.6 18            L                            1/2,3/2,5/2-     10017.0 18 
 

      0.0
1/2-
  10037.4 15            L                            1/2,3/2,5/2-     10036.8 15 
 

      0.0
1/2-
  10049 2            L                            1/2,3/2,5/2-     10048 2 
 

      0.0
1/2-
  10065 4            L                            1/2,3/2,5/2-     10064 4 
 

      0.0
1/2-
  10073.9 19            L                            1/2,3/2,5/2-     10073.3 19 
 

      0.0
1/2-
  10091.3 14            L                            1/2,3/2,5/2-     10090.7 14 
 

      0.0
1/2-
  10108.2 14            L                            1/2,3/2,5/2-     10107.6 14 
 

      0.0
1/2-
  10141.3 12            L                            1/2,3/2,5/2-     10140.7 12 
 

      0.0
1/2-
  10173.0 11            L                            1/2,3/2,5/2-     10172.4 11 
 

      0.0
1/2-
  10194.5 24            L                            1/2,3/2,5/2-     10193.9 24 
 

      0.0
1/2-
  10276.2 19            L                            1/2,3/2,5/2-     10275.6 19 
 

      0.0
1/2-
  10286.9 19            L                            1/2,3/2,5/2-     10286.3 19 
 

      0.0
1/2-
  10307.1 11            L                            1/2,3/2,5/2-     10306.5 11 
 

      0.0
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  10324.5 12            L                            1/2,3/2,5/2-     10323.9 12 
 

      0.0
1/2-
  10340.5 15            L                            1/2,3/2,5/2-     10339.9 15 
 

      0.0
1/2-
  10379.3 9            L                            1/2,3/2,5/2-     10378.7 9 
 

      0.0
1/2-
  10395.0 12            L                            1/2,3/2,5/2-     10394.3 12 
 

      0.0
1/2-
  10412.7 7            L                            1/2,3/2,5/2-     10412.0 7 
 

      0.0
1/2-
  10424.8 9            L                            1/2,3/2,5/2-     10424.1 9 
 

      0.0
1/2-
  10460.9 18            L                            1/2,3/2,5/2-     10460.2 18 
 

      0.0
1/2-
  10469 6            L                            1/2,3/2,5/2-     10468 6 
 

      0.0
1/2-
  10504 5            L                            1/2,3/2,5/2-     10503 5 
 

      0.0
1/2-
  10513.8 15            L                            1/2,3/2,5/2-     10513.1 15 
 

      0.0
1/2-
  10538.1 19            L                            1/2,3/2,5/2-     10537.4 19 
 

      0.0
1/2-
  10641.6 11            L                            1/2,3/2,5/2-     10640.9 11 
 

      0.0
1/2-
  10659.7 18            L                            1/2,3/2,5/2-     10659.0 18 
 

      0.0
1/2-
  10668.2 11            L                            1/2,3/2,5/2-     10667.5 11 
 

      0.0
1/2-
  10697.4 8            L                            1/2,3/2,5/2-     10696.7 8 
 

      0.0
1/2-
  10736.8 14            L                            1/2,3/2,5/2-     10736.1 14 
 

      0.0
1/2-
  10744.5 18            L                            1/2,3/2,5/2-     10743.8 18 
 

      0.0
1/2-
  10753 3            L                            1/2,3/2,5/2-     10752 3 
 

      0.0
1/2-
  10937 3       G                                 (5/2+)      9193 6 
   9431 6 
  10025 6 
  10937 6 
    34 9 
    47 12 
    11 3 
   100 25 




   1744.74
   1507.41
    908.97
      0.0
5/2-
3/2-
9/2+
1/2-
  10967.5 11            L                            1/2,3/2,5/2-     10966.8 11 
 

      0.0
1/2-
  11058.9 15            L                            1/2,3/2,5/2-     11058.2 15 
 

      0.0
1/2-
  11069 2            L                            1/2,3/2,5/2-     11068 2 
 

      0.0
1/2-
  11081.8 9            L                            1/2,3/2,5/2-     11081.1 9 
 

      0.0
1/2-
  11106.9 18            L                            1/2,3/2,5/2-     11106.2 18 
 

      0.0
1/2-
  11192.5 19            L                            1/2,3/2,5/2-     11191.7 19 
 

      0.0
1/2-
  11200 2            L                            1/2,3/2,5/2-     11199 2 
 

      0.0
1/2-
  11419.3 14            L                            1/2,3/2,5/2-     11418.5 14 
 

      0.0
1/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  11463.0 18            L                            1/2,3/2,5/2-     11462.2 18 
 

      0.0
1/2-
  11474 3            L                            1/2,3/2,5/2-     11473 3 
 

      0.0
1/2-
  11498 3            L                            1/2,3/2,5/2-     11497 3 
 

      0.0
1/2-
  11517 2            L                            1/2,3/2,5/2-     11516 2 
 

      0.0
1/2-
  11535.9 5            L                            1/2,3/2,5/2-     11535.1 5 
 

      0.0
1/2-
  11560.7 6            L                            1/2,3/2,5/2-     11559.9 6 
 

      0.0
1/2-
  11571.2 8            L                            1/2,3/2,5/2-     11570.4 8 
 

      0.0
1/2-
  11601.8 17            L                            1/2,3/2,5/2-     11601.0 17 
 

      0.0
1/2-
  11611 2            L                            1/2,3/2,5/2-     11610 2 
 

      0.0
1/2-
  11623 3            L                            1/2,3/2,5/2-     11622 3 
 

      0.0
1/2-
  11646.0 19            L                            1/2,3/2,5/2-     11645.2 19 
 

      0.0
1/2-
  11660.4 14            L                            1/2,3/2,5/2-     11659.6 14 
 

      0.0
1/2-
  11669.3 18            L                            1/2,3/2,5/2-     11668.5 18 
 

      0.0
1/2-
  11691.4 18            L                            1/2,3/2,5/2-     11690.6 18 
 

      0.0
1/2-
  11739.8 12            L                            1/2,3/2,5/2-     11739.0 12 
 

      0.0
1/2-
  11770.0 12            L                            1/2,3/2,5/2-     11769.2 12 
 

      0.0
1/2-
  11802 2            L                            1/2,3/2,5/2-     11801 2 
 

      0.0
1/2-
  11817 3            L                            1/2,3/2,5/2-     11816 3 
 

      0.0
1/2-
  11832.1 15            L                            1/2,3/2,5/2-     11831.3 15 
 

      0.0
1/2-
  11843 2            L                            1/2,3/2,5/2-     11842 2 
 

      0.0
1/2-
  11854 2            L                            1/2,3/2,5/2-     11853 2 
 

      0.0
1/2-
  11873.5 19            L                            1/2,3/2,5/2-     11872.7 19 
 

      0.0
1/2-
  11913.2 14            L                            1/2,3/2,5/2-     11912.3 14 
 

      0.0
1/2-
  11946.9 18            L                            1/2,3/2,5/2-     11946.0 18 
 

      0.0
1/2-
  11962.3 14            L                            1/2,3/2,5/2-     11961.4 14 
 

      0.0
1/2-
  11984 2            L                            1/2,3/2,5/2-     11983 2 
 

      0.0
1/2-
  11991 2            L                            1/2,3/2,5/2-     11990 2 
 

      0.0
1/2-
     12E3 2                     U                   (1/2+,3/2+)        
  12076 15        H                YZ              5/2+ 16 keV 2       
     12.79E3 12                                f               
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  13070 15        H                YZ  c           (1/2+) 70 keV      
     13.8E3 2             M  P                        1.2 MeV 2       
  13991 15        H                 Z              5/2+ 50 keV      
     14.0E3 2             M                           4.5 MeV 4       
  14060 15        H                YZa             3/2+ 50 keV      
  14369 15        H                                (1/2-)        
     14.42E3 16                                f               
  14492 15        H                YZ  c           3/2+ 65 keV 7       
  14655 15        H                                (3/2-) 30 keV      
     14.7E3 3                  R T                    4.4 MeV 4       
  14781 15        H                 Z              7/2+ 20 keV      
  14833 15        H                                25 keV      
  14912 15        H                                (7/2-) 30 keV      
     15E3 2                       W                        
  15006 15        H                    c           (3/2+,5/2+) 25 keV      
  15176 15        H                                3/2+ 55 keV 21       
  15293 15        H                                5/2+ 45 keV 7       
  15323 15        H                                       
  15478 15        H                                40 keV      
  15787 15        H                                (7/2-) 55 keV      
  15837 15        H                Y a c           (1/2+) 78 keV 15       
  16127 15        H                                (1/2+) 80 keV 15       
  16247 15        H                                       
  16317 15        H                                       
     16.4E3           L                            3.95 MeV      
  16527 15        H                                50 keV 15       
  16607 15        H                                50 keV 15       
  16647 15        H                                50 keV 15       
  16717 15        H                                (5/2-) 65 keV 15       
  16729 15                           a c           (1/2+)        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  16767 15        H                                50 keV 15       
  16790 40            LM             ab d          3.9 MeV 2       
  16917 15        H                                (7/2-) 40 keV 15       
     17E3 2                     U                   (3/2+,5/2+)        
  17127 15        H                                50 keV 15       
  17427 15        H                  a c           (1/2+) 65 keV 15       
  17507 15        H                                       
     18.9E3                            c                  
     19.98E3 12                                f               
     20.3E3?                            c                  
     21.5E3 2            L              a             4.0 MeV 3       
     21.68E3 12                                f               
     21.8E3 3                            bc                  
     27E3 1                                f               
     28.0E3 5             M            Z   d     j    8 MeV      

E(level): From least-squares fit to Eγ data for levels populated in γ-ray studies. Others are generally from individual reactions

T1/2(level): From ΔS(a) in (α,2nγ), unless otherwise stated. For IAR and giant resonances, values given are widths

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Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
    908.97 9/2+ 15.663 s 5 
% IT = 100
    908.960 25 M4+E50.00041 40.00851B(E5)(W.u.)=0.147 15, B(M4)(W.u.)=3.995 2, α=0.00851
   1507.41 3/2- 23.9 fs +25-21     1507.42 10 M1+E2-0.13 2B(E2)(W.u.)=2.1 2, B(M1)(W.u.)=0.26 3
   1744.74 5/2- 0.64 ps 6     1744.7 2 E2 B(E2)(W.u.)=2.3 2
   2222.43 5/2+ 0.97 ps 28      715.2 3 [E1] B(E1)(W.u.)=0.00030 9
5/2+ 0.97 ps 28     1313.2 3 [E2] B(E2)(W.u.)=4.3 13
   2566.55 11/2+ 0.35 ps 7     1657.5 2 M1+E2-15 8B(E2)(W.u.)=5.5 11, B(M1)(W.u.)=6.E-5 5
   2622.1 9/2+ 0.21 ps 10     1713.1 3 (M1+E2) B(E2)(W.u.)=(3.9), B(M1)(W.u.)=(0.010)
   2892.98 13/2+ 0.18 ps 3     1984.1 2 E2 B(E2)(W.u.)=4.3 8
   3067.76 3/2- 45.0 fs +15-11     3067.7 1 (M1+E2)+0.05 B(E2)(W.u.)=(0.89), B(M1)(W.u.)=(0.0077)
   3107.26 (5/2)- 0.034 ps 3     1361.8 9 (M1+E2)+0.6 B(E2)(W.u.)=(6.8), B(M1)(W.u.)=(0.0116)
(5/2)- 0.034 ps 3     1599.8 4 (M1+E2)-0.25 B(E2)(W.u.)=(2.8), B(M1)(W.u.)=(0.0067)
(5/2)- 0.034 ps 3     3107.3 3 [E2] B(E2)(W.u.)=2.0 2
   3138.9 (5/2)- 0.11 ps +7-3      916.1 5 [E1] B(E1)(W.u.)=0.00038 25
(5/2)- 0.11 ps +7-3     3139.1 5 [E2] B(E2)(W.u.)=0.6 4
   3247.6 (3/2,5/2)      1740.2 5 D+Q-0.24  
   3343.44 13/2- 0.42 ps 14      450.5 1 E1 B(E1)(W.u.)=0.00052 18
13/2- 0.42 ps 14      776.89 6 E1 B(E1)(W.u.)=0.0016 6
   3451.3 (7/2+)      2542.3 6 D+Q-0.03  
   3515.9 (3/2)-      3515.9 3 (M1+E2)-0.65 +15-30 
   3557.4 (7/2-)      2648.3 6 D+Q-0.08  
   3621.1 (11/2)      2712.1 6 D+Q+0.10  
   3630.3 (11/2)+      2721.3 6 (M1+E2)+0.19  
   3715.3 5/2+      1492.7 4 (M1+E2)-0.15  
   3747.7 (9/2)+      2838.7 8 (M1+E2)+0.40  
   3848.3 (3/2-,5/2-)      2103.5 5 (M1+E2)+1.8  
(3/2-,5/2-)      2340.8 6 (M1+E2)-0.50  
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
   3992.2 3/2- 9.3 fs +11-10     3992.1 1 (M1+E2)-0.90 B(E2)(W.u.)=(1.27), B(M1)(W.u.)=(0.0186)
   4022.96 (3/2)-       955.0 3 (M1+E2)-0.10  
(3/2)-      1800.8 4 (M1+E2)-1.25  
(3/2)-      2515.3 6 (M1+E2)-0.80  
   4104.9 (7/2+)      1882.5 8 (M1+E2)+0.28  
(7/2+)      3196.3 12 (M1+E2)-0.15  
   4132.22 15/2- 1.59 ps 28      788.6 1 M1+E2+0.08 4B(E2)(W.u.)=0.10 9, B(M1)(W.u.)=0.0092 18
15/2- 1.59 ps 28     1239.28 7 E1 B(E1)(W.u.)=7.5E-5 14
   4449.75 17/2- 4.5 ps 10      317.5 1 M1 0.00867B(M1)(W.u.)=0.051 12, α=0.00867
17/2- 4.5 ps 10     1106.5 1 E2 B(E2)(W.u.)=2.1 5
   4825.38 17/2+ ≥ 3.5 ps     693.2 2 E1 B(E1)(W.u.)<0.00023
17/2+ ≥ 3.5 ps    1931.9 3 (E2) B(E2)(W.u.)<0.029
   4838.59 19/2- 21 ps 8      388.9 1 M1+E2+0.20 50.00540B(E2)(W.u.)=3.3 21, B(M1)(W.u.)=0.011 5, α=0.00540 11
19/2- 21 ps 8      706.3 1 E2 B(E2)(W.u.)=2.2 10
   4920.46 (19/2+) 6.2 ps 21       95.07 3 (M1+E2)-0.05 30.212B(M1)(W.u.)>1.1 4, α=0.212
(19/2+) 6.2 ps 21      470.72 5 E1 B(E1)(W.u.)>0.00036 13
   5263.88 (21/2+) 1.46 ps 28      343.37 12 M1 0.00714B(M1)(W.u.)=0.36 7, α=0.00714
(21/2+) 1.46 ps 28      425.6 3 [E1] B(E1)(W.u.)=4.6E-5 12
   5309.83 (21/2-) 4.5 ps 9      471.1 2 (M1) B(M1)(W.u.)=0.044 11
(21/2-) 4.5 ps 9      860.1 1 (E2) B(E2)(W.u.)=0.57 15
   5879.4 (19/2+) 0.14 ps 10      615.5 3 (M1) B(M1)(W.u.)=0.7 5
   6198.90 (23/2+) 0.19 ps 4      935.01 5 M1+E2-0.12 4B(E2)(W.u.)=2.5 18, B(M1)(W.u.)=0.14 3
   7183.7 (25/2+) 0.21 ps 7     1920.2 3 [E2] B(E2)(W.u.)=4.4 18
   7431.6 (25/2+) 0.49 ps 14      172.1 1 (M1) 0.0417B(M1)(W.u.)=3.0 10, α=0.0417
(25/2+) 0.49 ps 14     1232.6 2 (M1) B(M1)(W.u.)=0.024 8
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
   7590.0 (25/2+) 0.35 ps 14      396.1 2 (M1) B(M1)(W.u.)=1.0 4
   7834.6 (27/2+) 1.25 ps 28      244.6 1 (M1) 0.0167B(M1)(W.u.)=0.70 19, α=0.0167
(27/2+) 1.25 ps 28      650.9 1 (M1) B(M1)(W.u.)=0.064 17
   8264.2 (29/2+) 0.97 ps 21      429.6 1 M1+E2-0.07 4B(E2)(W.u.)=8 7, B(M1)(W.u.)=0.27 9
(29/2+) 0.97 ps 21      832.9[E2] B(E2)(W.u.)<8
   8720.4 (31/2+) 0.48 ps 14      456.2 2 (M1) B(M1)(W.u.)=0.43 17
(31/2+) 0.48 ps 14      885.9[E2] B(E2)(W.u.)<19

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
      0.01/2- STABLE μ=-0.1374154 3 (1977Ha12,1989Ra17,2011StZZ)
Configuration=πp1/2.
    908.979/2+ 15.663 s 5 
% IT = 100
μ=+6.37 4 (2007Ch07,2011StZZ), Q=-0.43 6 (2007Ch07,2011StZZ)
BE5|^=0.00056 5 (e,e’); β5=0.055 (p,p’).
   1507.413/2- 23.9 fs +25-21  B(E2)|^=0.0097 11 (e,e’); β2=0.079 13 (n,n’); 0.060 (p,p’).
   1744.745/2- 0.64 ps 6  B(E2)|^=0.0164 15 (e,e’). β2=0.079 10 (n,n’); 0.072 (p,p’).
   2222.435/2+ 0.97 ps 28  B(E3)|^=0.0258 23 (e,e’). β3=0.160 17 (n,n’); 0.156 (p,p’).
   2529.807/2+ 0.08 ps 4  B(E3)|^=0.037 3 (e,e’). β3=0.14 3 (n,n’); 0.146 (p,p’).
   2566.5511/2+ 0.35 ps 7  β5=0.027 (p,p’).
   2622.19/2+ 0.21 ps 10  β5=0.047 (p,p’).
   2871.7(7/2)+ < 0.2 ps β3=0.079 13 (n,n’); 0.111 (p,p’).
   2881.53(3/2)- 19.9 fs +21-19  β2=0.087 16 (n,n’); 0.066 (p,p’).
   3107.26(5/2)- 0.034 ps 3  β2=0.065 8 (n,n’); 0.046 (p,p’).
   3621.1(11/2)   XREF: γ(3612).
   3715.35/2+   XREF: R(3740)S(3680).
   4171.33/2-,5/2- 10.1 fs +15-11  XREF: S(4180).
   4251   XREF: L(?).
   4309.3(7/2)-   XREF: l(4310).
   4408.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   4529.35/2+,7/2+   XREF: X(4550).
   4616.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   4625.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   48313/2+,5/2+   XREF: J(4840).
   49921/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   5006(5/2)-   XREF: W(5000).
   5075(1/2+)   XREF: I(5100)J(5080).
   5085.41/2,3/2,5/2-   XREF: p(5089).
Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
   5152.11/2,3/2,5/2-   XREF: p(5148).
Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   5167.71/2,3/2,5/2-   XREF: p(5170).
Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   51833/2+,5/2+   XREF: J(5190).
   5211(3/2-)   XREF: X(5220).
   5275(1/2+)   XREF: J(5270).
   5343(1/2+)   XREF: J(5340).
   5382(1/2)   XREF: X(5380).
   5419.41/2,3/2,5/2-   XREF: p(5421).
Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   5614.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   5625.81/2,3/2,5/2-   XREF: p(5622).
Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   5653.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   5789.41/2,3/2,5/2-   XREF: p(5793).
Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   5796.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   58883/2+,5/2+   XREF: K(5870).
   5910.71/2,3/2,5/2-   XREF: p(5915).
Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   5923.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
      6.01E3   E(level): Hypernuclear state.
   6122.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6201.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6206.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6275.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6297.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6331.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6359.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6398.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
   6441.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6472.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   64791/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6493.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
      6.5E3(7/2-)   E(level): Wide structure due to deep hole states.
   6532.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6592.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6608.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6651.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6666.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   67281/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6750 1.0 MeV 2  E(level): Giant resonance.
   6751.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6772.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   67807/2-   XREF: W(6800).
   6782.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6798.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6852.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   68661/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   69211/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6934.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6944.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6959.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   6987.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7003.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
   7066.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7077.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
      7.1E3   E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
   71061/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7118.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7147.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7178.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   71981/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7225.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   72401/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   72551/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
      7.3E3   E(level): Wide structure due to deep hole states.
   7304.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7325.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
      7.38E3   E(level): Hypernuclear state.
   7383.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7420.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7452.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7475.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7484.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7527.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   75361/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   75481/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   75561/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   75661/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
   7588.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7618.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7640.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7652.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7666.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7692.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7703.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7714.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7722.2(1/2+)   XREF: J(7720)K(7710).
Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7750.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7774.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7787.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7799.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7811.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7830.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7838.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7866.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7902.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7920.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7922.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7937.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7961.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7968.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7986.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   7996.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
   80181/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8027.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8050 1.2 MeV 2  E(level): Giant resonance.
   8067.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8099.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8129.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8142.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8150.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8159.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8175.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8198.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8210.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8221.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8270.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8285.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8311.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8320.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8330.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8338.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   83691/2,3/2,5/2-   XREF: J(?).
Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8380.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8403.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8438.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   84551/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8466.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
   8483.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8495.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8513.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8530.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8548.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8556.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8568.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8586.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   86031/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8610.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8642.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8668.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8764.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8779.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8843.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   88641/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8877.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8899.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8926.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   89811/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   8994.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9002.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9024.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9043.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9057.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
   9069.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   90821/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9093.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9112.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9121.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9147.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9161.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9175.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9191.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9204.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9240.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9256.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9280.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9290.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9301.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9308.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   93201/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9326.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9351.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9374.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9401.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9410.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9449.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   94711/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9482.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
   95031/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   95321/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   95411/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9575.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9593.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9623.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9660.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9679.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9901.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9912.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9964.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9973.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
   9990.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10005.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10017.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10037.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  100491/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  100651/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10073.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10091.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10108.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10141.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10173.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10194.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10276.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
  10286.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10307.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10324.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10340.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10379.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10395.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10412.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10424.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10460.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  104691/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  105041/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10513.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10538.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10641.61/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10659.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10668.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10697.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10736.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10744.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  107531/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  10967.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11058.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  110691/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11081.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11106.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
  11192.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  112001/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11419.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11463.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  114741/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  114981/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  115171/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11535.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11560.71/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11571.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11601.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  116111/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  116231/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11646.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11660.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11669.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11691.41/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11739.81/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11770.01/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  118021/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  118171/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11832.11/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  118431/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  118541/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11873.51/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
E(level)Jπ(level)T1/2(level)Comments
  11913.21/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11946.91/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  11962.31/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  119841/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
  119911/2,3/2,5/2-   Jπ(level): Population in (γ,γ’) from 1/2- ground state by dipole or quadrupole excitation. Above 7 MeV, 5/2- is less likely due to predominance of dipole excitation.
     12E3(1/2+,3/2+)   E(level): Wide structure due to deep hole states.
  120765/2+ 16 keV 2  Γγ0=7 2, Γp=5.5 5
E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
     12.79E3   E(level): Hypernuclear state.
  13070(1/2+) 70 keV Γγ0=16 3, Γp=46 KEV
E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
     13.8E3 1.2 MeV 2  E(level): Giant resonance.
  139915/2+ 50 keV Γp=8 4
E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
     14.0E3 4.5 MeV 4  E(level): Giant resonance.
  140603/2+ 50 keV Γγ0=7 3, Γp=26 4
E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
  14369(1/2-)   E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
     14.42E3   E(level): Hypernuclear state.
  144923/2+ 65 keV 7  Γγ0=11.3 19, Γp=20 3
E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
  14655(3/2-) 30 keV E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
     14.7E3 4.4 MeV 4  E(level): Giant resonance.
  147817/2+ 20 keV Γp=4 KEV
E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
  14912(7/2-) 30 keV E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
     15E3   E(level): Wide structure due to deep hole states.
  15006(3/2+,5/2+) 25 keV E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
  151763/2+ 55 keV 21  Γp=6.3 10
E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
  152935/2+ 45 keV 7  Γp=4 3
E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
  15837(1/2+) 78 keV 15  Γγ0=40 8
E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
E(level)Jπ(level)T1/2(level)Comments
  16127(1/2+) 80 keV 15  E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
     16.4E3 3.95 MeV E(level): Giant resonance.
  16729(1/2+)   E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
  16790 3.9 MeV 2  E(level): Giant resonance.
     17E3(3/2+,5/2+)   E(level): Wide structure due to deep hole states.
  17427(1/2+) 65 keV 15  E(level): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p).
     19.98E3   E(level): Hypernuclear state.
     21.5E3 4.0 MeV 3  E(level): Giant resonance.
     21.68E3   E(level): Hypernuclear state.
     21.8E3   XREF: c(?).
     27E3   E(level): Hypernuclear state.
     28.0E3 8 MeV XREF: d(27000).
E(level): Giant resonance.

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Additional Gamma Comments:

E(level)E(gamma)Comments
    908.97    908.960M(γ): α(exp) in 89Y IT decay. E5 admixture is suggested by L=5 in (e,e’), (p,p’), (n,n’) and (α,α’) from 1/2-
   1744.74   1744.7M(γ): ΔJ=2 γ to 1/2- and RUL
   2222.43    715.2I(γ): from (n,n’γ). Iγ=22 4 in (α,2nγ), 43 in (p,p’γ)
   2622.1   1713.1M(γ): ce data in 89Zr ε decay
   4449.75    317.5E(γ): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p)
M(γ): From (18O,2npγ), (18O,4npγ)
   4920.46    470.72E(γ): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p)
M(γ): From (18O,2npγ), (18O,4npγ)
   5263.88    343.37E(γ): IAR of 89Sr, confirmed by comparison of Γp with S-factors in 88Sr(d,p)
M(γ): From (18O,2npγ), (18O,4npγ)

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