ADOPTED LEVELS, GAMMAS for 49V

Author: T. W. Burrows |  Citation: Nucl. Data Sheets 109, 1879 (2008) |  Cutoff date: 14-Jul-2008 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-2628 keV 3S(n)= 11555.5 keV 13S(p)= 6758.2 keV 9Q(α)= -9314.7 keV 11
Reference: 2012WA38

References:
  A  49Cr β+ decay  B  12C(40Ca,3PG),24Mg(32S,3PAG),
  C  46Ti(α,pγ)  D  48Ti(p,γ) E=960-2488 KEV RES
  E  48Ti(3He,d),(3He,PD),(d,n)  F  48Ti(16O,15N)
  G  49Ti(p,n),(p,nγ)  H  50Cr(t,α) E=13 MeV
  I  51V(p,t) E=40.2 MeV  J  52Cr(p,α) E=35 MeV
  K  48Ti(p,γ),(3He,PD), 52Cr(p,α)  L  48Ti(p,p),(p,p’),(p,p’γ) RES

General Comments:

Levels: Resonances: see 1978Ha15 and the references cited below for additional resonance states and more information on the resonance parameters. Others: see 1995Bu23

Levels: Bound-state t’s: from 50Cr(3He,α) in 49Cr

Levels: Γp, Γγ: from (p,γ)

Levels: %p,%γ: from Γp and Γγ

Levels: Multidimensional nonmetric scaling analysis: see 47V adopted levels, gammas and 46Ti(p,γ) E=0.4-1.8 MeV res (1991Bu05) for a comparison of results from multidimensional nonmetric scaling analysis of the data from 1986De13 by 1993Ca12 to an average-spin method analysis by 1988Va08 and 1991Ki11 of the data and results using the Nuclear Data Sheets "Strong " arguments for spin and parity assignments.

Gammas: Γγ: from (p,γ)

Q-value: Note: Current evaluation has used the following Q record -2626.5 2611552.9 266758.2 8 -9084 3 2003Au03










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
      0.0ABCDEFGHIJ   7/2- 330 d 15 
% ε = 100
     
     90.6392 17 ABCDE GHIJ   5/2- 228 ps 13      90.639 2 
  100
M1
      0.0
7/2-
    152.9282 17 A CDEFGHIJ   3/2- 19.90 ns 24      62.289 2 
   152.928 2 
   70.5 24 
  100 3 
(M1)
E2
     90.6392
      0.0
5/2-
7/2-
    748.27 9 ABCDE GH J   3/2+ 5.3 ps 6     595.35 14 
   657.60 14 
  100.0 15 
   85.2 15 
(E1(+M2))
(E1(+M2))
    152.9282
     90.6392
3/2-
5/2-
   1021.62 11 ABCDEFGHIJ   11/2- 3.4 ps 6    1021.63 14 
  100
E2
      0.0
7/2-
   1140.53 11  BCDE G  J   5/2+ 1.3 ps 6     392.7 6 
   987.61 26 
  1049.79 17 
  1140.7 3 
   10.5 10 
   31.4 17 
   44.5 21 
  100 4 
M1+E2
(E1(+M2))
E1+M2
E1(+M2)
    748.27
    152.9282
     90.6392
      0.0
3/2+
3/2-
5/2-
7/2-
   1155.32 10 ABCDEFGHIJ   9/2- 1.1 ps 3     133.80 17 
  1064.63 17 
  1155.33 17 
    3.9 8 
   30.0 6 
  100.0 10 
(M1(+E2))
E2
M1+E2
   1021.62
     90.6392
      0.0
11/2-
5/2-
7/2-
   1183?       H            
   1514.54 7 A CD  GHIJ   5/2- 31 fs 12     766 1 ?
  1361.61 7 
  1423.6 3 
  1514.4 4 
   37 11 
  100.0 22 
   20.3 11 
   58 3 
(E1(+M2))
M1+E2
(M1(+E2))
D,E2
    748.27
    152.9282
     90.6392
      0.0
3/2+
3/2-
5/2-
7/2-
   1602.68 12  BCD  G  J   7/2+ 0.47 ps 22     447.4 3 
   462.2 2 
   854.5 3 
  1512.0 3 
  1602.6 2 
    1.6 8 
   13.5 17 
   15 4 
  100 8 
   49.3 20 
(E1)
M1(+E2)
(E2)
(E1)
(E1+M2)
   1155.32
   1140.53
    748.27
     90.6392
      0.0
9/2-
5/2+
3/2+
5/2-
7/2-
   1610?       H     (9/2-,11/2-)        
   1643.19 18   CD  G      (3/2-,5/2) 36 fs 11    1490.24 18 
  1553?
  100
   <2.4
D+Q

    152.9282
     90.6392
3/2-
5/2-
   1646.43 21   CD  GH J   (1/2+) 6.6 ps 10     898.06 26 
  1493.6 3 
   87 12 
  100 12 
D+Q
(E1(+M2))
    748.27
    152.9282
3/2+
3/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   1661.40 13 A CDEFG IJ   3/2- 16 fs 7     912.3 10 
  1508.37 18 
  1570.83 17 
  1661.4 10 
    9.6 20 
   65.4 20 
  100.0 20 
   17.3 20 
(E1(+M2))
D,E2
M1(+E2)
(E2(+M3))
    748.27
    152.9282
     90.6392
      0.0
3/2+
3/2-
5/2-
7/2-
   1994.7 4   CD  GH J   3/2(+) 0.49 ps 21     854.5 4 
  1246.8 10 
  1841.0 8 
  1903.4 8 
   85 21 
   46 5 
  100 5 
   62 5 
(M1+E2)
D,E2
(E1+M2)
(E1(+M2))
   1140.53
    748.27
    152.9282
     90.6392
5/2+
3/2+
3/2-
5/2-
   2178.3 4  BCD  GH J   9/2+ 0.56 ps +49-28     575.4 9 
  1023 1 ?
  1037.4 5 
  1157.0 7 
  2178.3 8 
   11.3 17 
 
   33.9 17 
   16.1 17 
  100 5 
D(+Q)
D,Q
E2
D
D(+Q)
   1602.68
   1155.32
   1140.53
   1021.62
      0.0
7/2+
9/2-
5/2+
11/2-
7/2-
   2182.0 4 A CDEFGHIJ   7/2- 33 fs 12    1026.8 7 
  2090.7 7 
  2181.6 11 
   32 3 
  100 9 
    8 5 
(M1(+E2))
(M1+E2)
D,Q
   1155.32
     90.6392
      0.0
9/2-
5/2-
7/2-
   2204?    EF       (5/2-,7/2-)        
   2234.0 7 A CD  GHIJ   5/2 12 fs 8     572.5 25 ?
  2081.1 20 ?
  2142.9 10 
  2234.4 15 
   21.9 16 
   26.6 16 
  100.0 16 
    7.8 16 
D,E2
D,E2
D(+Q)
D+Q
   1661.40
    152.9282
     90.6392
      0.0
3/2-
3/2-
5/2-
7/2-
   2263.30 21  BC   G IJ   15/2- 0.65 ps +38-19    1241.69 18 
  100
E2
   1021.62
11/2-
   2265.3 3   CD  GH J   5/2- 35 fs 9     621?
  2112.3 3 
    5.3
  100 15 
D
D+Q
   1643.19
    152.9282
(3/2-,5/2)
3/2-
   2279?    E        1/2-,3/2-        
   2309.4 6 A CDE GHIJ   3/2- 14 fs 7    1560?
  2155.7 12 
  2218.6 8 
  2310.6 14 
   19
   86 5 
  100 5 
   52 5 
(E1(+M2))
D+Q
D+Q
(E2)
    748.27
    152.9282
     90.6392
      0.0
3/2+
3/2-
5/2-
7/2-
   2353.4 4   C   GHIJ   9/2- 33 fs 12    1198.9 11 
  1331.7 7 
  2262.2 20 ?
  2353.2 7 
    8.9 18 
   57.1 18 
   10.7 18 
  100.0 18 
D,E2
(M1+E2)
(E2(+M3))
M1+E2
   1155.32
   1021.62
     90.6392
      0.0
9/2-
11/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   2388.0 5   CDE GH J   5/2+ 57 fs 20     393.6 15 ?
  1247.8 12 ?
  1639.3 6 
  2235.5 16 ?
  2298.6 15 
  2388.6 14 
   16.9 17 
   11.9 17 
  100 5 
   <8.5
   28.8 17 
   11.9 17 
(M1(+E2))
D,E2
M1+E2

(E1(+M2))
(E1(+M2))
   1994.7
   1140.53
    748.27
    152.9282
     90.6392
      0.0
3/2(+)
5/2+
3/2+
3/2-
5/2-
7/2-
   2408.3 4   CD  GHIJ   (7/2-) < 8 fs    229.2 20 ?
  1252.9 8 
  1268?
  1385.7 10 ?
  2316.4 20 ?
  2408.4 4 
   <6.3
   18.3 14 
   33
    7.0 14 
   15.5 14 
  100.0 14 

D,E2
D
D,E2
D,E2
D(+Q)
   2178.3
   1155.32
   1140.53
   1021.62
     90.6392
      0.0
9/2+
9/2-
5/2+
11/2-
5/2-
7/2-
   2671.0 3  BCD    IJ   (11/2)- < 11 fs   1517 1 
  1649.2 3 
   33
  100
D,E2
M1+E2
   1155.32
   1021.62
9/2-
11/2-
   2671.3 9 ?   D  G  J   7/2-,9/2,11/2+ < 33.3 ps   1649.3 10 ?
  2579.2 20 ?
  2672.8 20 ?
  100.0 12 
    4.4 12 
    6.7 12 
D,E2
D,Q,E3

   1021.62
     90.6392
      0.0
11/2-
5/2-
7/2-
   2680.0 15    D  GH J   (7/2,9/2)     1526 2 ?
  1657 2 ?
  100 12 
  100 12 


   1155.32
   1021.62
9/2-
11/2-
   2727.5 3  BC   GHIJ   15/2- 0.10 ps 4     464.2 3 
  1705.5 7 
  100
  100
M1(+E2)
(E2)
   2263.30
   1021.62
15/2-
11/2-
   2741.0 5  BC          11/2+ 0.39 ps +36-17     562.5 7 
  1138.9 9 
  1585.8 9 
  1719.0 15 ?
   27.1 21 
  100 5 
   81 5 
  <10
D,E2
(E2)
(E1(+M2))
(E1(+M2))
   2178.3
   1602.68
   1155.32
   1021.62
9/2+
7/2+
9/2-
11/2-
   2786.4 3   C E G IJ   (9/2)- < 11 fs   1184.3 10 ?
  1631.0 5 
  1764.5 4 
  2697.2 20 ?
  2786.4 5 
    6.7 23 
   53.3 23 
  100.0 23 
    8.9 23 
   53.3 23 
D,E2
D+Q
D+Q,E2
D,E2
M1+E2,E2
   1602.68
   1155.32
   1021.62
     90.6392
      0.0
7/2+
9/2-
11/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   2796.6 15 ?      G  J       1775.0 15 ?
  2796 4 ?
   61 10 
  100 10 


   1021.62
      0.0
11/2-
7/2-
   2808.3 7   C   GH     5/2+ 0.32 ps 6    1206.6 10 
  1666.7 10 
  2058?
  2655.7 20 
  2808.5 20 
   26 5 
   24 5 
   54 17 
   88 8 
  100 8 
D,E2
D,E2
D,E2
(E1(+M2))
(E1(+M2))
   1602.68
   1140.53
    748.27
    152.9282
      0.0
7/2+
5/2+
3/2+
3/2-
7/2-
   2810.9 5   CDE G IJ   5/2-,7/2- < 12 fs    628.4 10 
  1673 2 ?
  2720.3 19 
  2810.9 5 
   33 5 
   25 6 
  100 5 
   75 5 
M1
D,E2
D,E2
D,E2
   2182.0
   1140.53
     90.6392
      0.0
7/2-
5/2+
5/2-
7/2-
   2861.5 5  BC     I    13/2- 0.10 ps 6     134 1 ?
   598.3 7 
  1706 1 
  1840 1 ?
 
   28.2 13 
  100 6 
 
(M1(+E2))
(M1(+E2))
E2(+M3)
D,E2
   2727.5
   2263.30
   1155.32
   1021.62
15/2-
15/2-
9/2-
11/2-
   3017.3 7   C   G I    < 33.3 ps   1414.1 10 ?
  2865.0 16 
  2926.5 13 
  3017.6 14 
   22.5 25 
  100 5 
   92 5 
   35 5 
D,Q



   1602.68
    152.9282
     90.6392
      0.0
7/2+
3/2-
5/2-
7/2-
   3133.9 5   C E  HIJ   (9/2,11/2,13/2) 0.22 ps +8-4     462.9 3 
  100
D
   2671.0
(11/2)-
   3134.0 6   CDE GHIJ   7/2,9/2(+) < 33.3 ps   1979.5 15 
  2112.8 16 
  2385.7 20 ?
  3043.5 20 ?
  3133.4 10 
   39.0 25 
   34.1 25 
   17.1 25 
   53.7 25 
  100.0 25 
D,Q
D,Q
D,Q,E3

D+Q
   1155.32
   1021.62
    748.27
     90.6392
      0.0
9/2-
11/2-
3/2+
5/2-
7/2-
   3152.1 10 ?    E G          2012.0 15 ?
  2131.0 15 ?
  100 10 
   61 10 


   1140.53
   1021.62
5/2+
11/2-
   3224 1    D         (1/2,3/2,5/2-)     1566
  3074
  100
  100


   1661.40
    152.9282
3/2-
3/2-
   3239.5 9    D  G IJ   7/2- < 33.3 ps   1725.2 10 
  3148.9 20 
  3238.2 20 
   50.8 17 
  100.0 17 
   13.1 17 
D,Q

D,Q,E3
   1514.54
     90.6392
      0.0
5/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   3242 2    D         (3/2,5/2,7/2-)        
   3248    E  H     1/2+        
   3259.5 4   CD         (GE 9/2)      473.1 2 
  100

   2786.4
(9/2)-
   3303.2 9       G      3/2-,5/2,7/2,9/2 < 33.3 ps   1121.0 10 
  3213.5 20 
  3302.6 20 
   54 6 
   40 6 
  100 4 
D,E2
D,Q,E3

   2182.0
     90.6392
      0.0
7/2-
5/2-
7/2-
   3305 3         I    (13/2-)        
   3325 2    D         (1/2+ TO 7/2+)        
   3325.2 4  B      IJ   (17/2-)      464 1 
   597.1 5 
  1061.9 5 
   36.84
   21.05
  100
D,Q
D
D
   2861.5
   2727.5
   2263.30
13/2-
15/2-
15/2-
   3340.5 11       GHIJ   < 33.3 ps   1106.3 10 
  3341.2 20 
   37 5 
  100 3 
D,E2

   2234.0
      0.0
5/2
7/2-
   3341.8 7   C    HIJ   (13/2+)      601.0 8 
   670.5 8 
  1163.0 10 
   72.5 25 
   78 5 
  100 5 
D,E2
D,E2
D,Q
   2741.0
   2671.0
   2178.3
11/2+
(11/2)-
9/2+
   3342 2    D         (1/2+ TO 9/2+)        
   3388 1    D   H J   (3/2,5/2-)     1729
  1876
   67
  100


   1661.40
   1514.54
3/2-
5/2-
   3388.5 9       GH J   5/2,7/2 < 33.3 ps    602.3 10 
  1745 2 ?
  2233.7 20 
  2638.9 20 
  3296 2 ?
   30 7 
   11.1 24 
   39 4 
  100 4 
   29 13 
D,E2
D,Q
D,Q
D,Q

   2786.4
   1643.19
   1155.32
    748.27
     90.6392
(9/2)-
(3/2-,5/2)
9/2-
3/2+
5/2-
   3405   DE   IJ   (3/2)-        
   3462.9 17    DE GH     (3/2+ TO 9/2+) < 33.3 ps   1862.0 15 ?
  3462.8 17 
 
 


   1602.68
      0.0
7/2+
7/2-
   3479 3 ?        I    (7/2-)        
   3500.6 10       G  J   < 33.3 ps   1092.2 10 
  3500.9 20 
   82 15 
  100 8 
D,E2

   2408.3
      0.0
(7/2-)
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   3516 2    D         (3/2- TO 9/2)        
   3521 2    D         (LE 9/2)        
   3531 2 ?   D    IJ   (LE 7/2-)     1870?
  1887?
  3378?
   25
   42
  100



   1661.40
   1643.19
    152.9282
3/2-
(3/2-,5/2)
3/2-
   3531.1 6       G IJ   5/2-,7/2,9/2+ < 33.3 ps   1178.4 10 
  1348.4 10 
  2015.6 20 
  2375.7 20 
  3378.5 20 
  3531.0 20 
   74 3 
   41 3 
   38 3 
   15 3 
  100 3 
   26 3 
D,E2
D,E2
D,Q

D,Q,E3

   2353.4
   2182.0
   1514.54
   1155.32
    152.9282
      0.0
9/2-
7/2-
5/2-
9/2-
3/2-
7/2-
   3603 2    D                
   3609 3         I    (7/2-)        
   3612 6 ?        IJ   (GE 11/2-)        
   3623.9 20       G I    LE 9/2 < 33.3 ps   2483.3 20 
  100
D,Q
   1140.53
5/2+
   3639.8 8    D  G IJ   (7/2-) < 33.3 ps   1461.5 10 
  2123.8 20 
  2618.1 20 
  3640.8 20 
   13 4 
   50 6 
  100 6 
   22.2 19 
D,Q
D,Q
D,Q

   2178.3
   1514.54
   1021.62
      0.0
9/2+
5/2-
11/2-
7/2-
   3665.9 7       G      11/2 < 33.3 ps   1312.1 10 
  1402.7 10 
  3666.7 20 
   35 3 
   17 3 
  100 3 
D,E2
D,Q
D,Q,E3
   2353.4
   2263.30
      0.0
9/2-
15/2-
7/2-
   3671 2    D     J   (1/2+ TO 9/2+)        
   3678 2    DE   IJ   (7/2)-        
   3694 6     E  H J   3/2+,5/2+        
   3721 2    D    I    (LE 7/2)-        
   3741 2    DE        1/2-,3/2-     2230
  3591
  3653
   67
  100
  100



   1514.54
    152.9282
     90.6392
5/2-
3/2-
5/2-
   3742.4 6  B      IJ   (19/2-)      416.9 5 
  1479.1 9 
  100
   93
D+Q
D,Q
   3325.2
   2263.30
(17/2-)
15/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   3757 2    DE  H     5/2-,7/2-        
   3771 2    D         (1/2+ TO 9/2+)        
   3782 2    D         (GE 9/2)        
   3795 3         I    (-)        
   3816 2    D         (LE 7/2-)     3725
  100

     90.6392
5/2-
   3825 3         I    (-)        
   3841 2    D     J   1/2(+),3/2,5/2-     2180
  2197
  100
   67


   1661.40
   1643.19
3/2-
(3/2-,5/2)
   3885.2 27         IJ          
   3912 2    DE  HI    (3/2)-     1650
  2270
  3761
   50
   83
  100


D(+Q)
   2265.3
   1643.19
    152.9282
5/2-
(3/2-,5/2)
3/2-
   3927 2    D   H J   (1/2+ TO 9/2+)        
   3960 2    D     J   (3/2-,5/2,7/2-)        
   3975 3        HIJ   (-)        
   4002 2    DE  H J   (3/2)-     1693
  2358
   67
  100


   2309.4
   1643.19
3/2-
(3/2-,5/2)
   4035 2    D         (3/2- TO 9/2+)        
   4048 3        HI           
   4064 6          J          
   4088 2    D   H     3/2(-),5/2,7/2-     1855
  2576
  3937
  4090
   33
  100
   83
   67




   2234.0
   1514.54
    152.9282
      0.0
5/2
5/2-
3/2-
7/2-
   4098 2    D    I    (LE 7/2-)        
   4129 2    DE        (5/2)-     3380
  100

    748.27
3/2+
   4152 2    D   H J          
   4165 3 ?        I           
   4218 2    DE   I    (3/2)-        
   4253 2    DE   IJ   1/2-,3/2-     2589
  2606
  100
  100


   1661.40
   1646.43
3/2-
(1/2+)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   4259 2    D    I    (3/2,5/2,7/2)        
   4270 2    D    I           
   4289 2    D   HI    3/2+,5/2+        
   4316 11         IJ          
   4359 2    D                
   4373 2    DE    J   1/2-,3/2-     2064
  2138
  2712
   60
   60
  100



   2309.4
   2234.0
   1661.40
3/2-
5/2
3/2-
   4397 2    D   H J   5/2-,7/2-        
   4422 2    D                
   4436 6     E    J          
   4470 6          J          
   4498 2    D     J   5/2(-),7/2(-)     3343
  4345
   43
  100


   1155.32
    152.9282
9/2-
3/2-
   4502    E  H J   1/2-,3/2-        
   4540 2    D   H J          
   4590 2    DE    J       2355
  100

   2234.0
5/2
   4599    E               
   4635 2    DE  H J   (5/2)-     4548
  4639
  100
   60


     90.6392
      0.0
5/2-
7/2-
   4662 6        H J   3/2+,5/2+        
   4740 2    D   H J   3/2+,5/2+        
   4796 6          J   (GE 11/2)        
   4840 2    DE  H J   1/2-,3/2-        
   4863 6        H J          
   4885 6     E    J          
   4947 2    DE    J   1/2-,3/2-     4853
  100

     90.6392
5/2-
   4959       H J   1/2+        
   4988 6          J          
   5010 6     E  H J   5/2-,7/2-        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   5042 2    D                
   5057    E        1/2-,3/2-        
   5072       H     3/2+,5/2+        
   5134 6     E  H J          
   5212 2    DE    J   1/2-,3/2-     2903
  100

   2309.4
3/2-
   5230 2    D   H            
   5257    E        1/2-,3/2-        
   5292 6        H J   1/2+        
   5347 6        H J   (3/2+,5/2+)        
   5387 6     E  H J   1/2-,3/2-        
   5411 6     E    J   5/2-,7/2-        
   5522       H     1/2+        
   5529.7 7  B           (21/2-)     1787 1 
  2204 1 
  100
   43
D

   3742.4
   3325.2
(19/2-)
(17/2-)
   5554       H            
   5597    E  H     1/2-,3/2-        
   5631?       H     (3/2+,5/2+)        
   5676    E        1/2-,3/2-        
   5689.9 8  B           (23/2-)      160 1 
  1947 1 
    2.7
  100

D,Q
   5529.7
   3742.4
(21/2-)
(19/2-)
   5718    E        1/2-,3/2-        
   5826    E        5/2-,7/2-        
   5889    E  H     1/2-,3/2-        
   5931?       H     (3/2+,5/2+)        
   5947    E        5/2-,7/2-        
   5987    E  H     1/2-,3/2-        
   6045    E        1/2-,3/2-        
   6058?       H     (3/2+,5/2+)        
   6146    E        1/2-,3/2-        
   6184    E  H            
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   6220    E  H     1/2-,3/2-        
   6258    E               
   6286?       H            
   6333    E  H     1/2-,3/2-        
   6368    E  H            
   6392    E  H            
   6430    E  H J          
   6474    E  H J          
   6521    E  H            
   6555    E        1/2-,3/2-        
   6563?       H     (3/2+,5/2+)        
   6603    E        1/2-,3/2-        
   6661 30     E               
   6683 30     E               
   6711 30     E               
   6816 30     E               
   6844.9 8  B           (23/2-)     1155 1 
  1315 1 
  3102 1 
  100
    6.2
   12.5
D


   5689.9
   5529.7
   3742.4
(23/2-)
(21/2-)
(19/2-)
   6856 30     E               
   6892 30     E               
   6943 30     E               
   6978 30     E               
   7054 30     E               
   7099 30     E               
   7137 30     E               
   7240 30     E               
   7290 30     E               
   7365 30     E               
   7430 30     E               
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   7478 30     E               
   7554 30     E               
   7605 30     E               
   7645 30     E               
   7745.0   DE        3/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
  3111
  3249?
  3620
  3658
  3741
  3830
  3931?
  3999
  4355
  5363
  5443
  5486
  5516
  6089
  6104
  6995?
  7592
  7654
  7745
   22.2
    5.6
   27.8
   94.4
   11.1
   55.6
    5.6
   50
   11.1
    5.6
   16.7
    5.6
   11.1
   27.8
   38.9
    5.6
  100
   72.2
    5.6
D,E2
D,E2
D,E2
D(+Q)
D,E2
D(+Q)
D,E2
D(+Q)
D,E2
(E1(+M2))
D+Q
D,E2
D+Q
D+Q
D+Q
(E1(+M2))
(M1+E2)
(M1(+E2))
E2+M3
   4635
   4498
   4129
   4088
   4002
   3912
   3816
   3741
   3388
   2388.0
   2309.4
   2265.3
   2234.0
   1661.40
   1643.19
    748.27
    152.9282
     90.6392
      0.0
(5/2)-
5/2(-),7/2(-)
(5/2)-
3/2(-),5/2,7/2-
(3/2)-
(3/2)-
(LE 7/2-)
1/2-,3/2-
(3/2,5/2-)
5/2+
3/2-
5/2-
5/2
3/2-
(3/2-,5/2)
3/2+
3/2-
5/2-
7/2-
   7750   DE        3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  3116
  3627
  3664
  3746
  3836
  3993
  4005
  4343
  4360
  5448
  5491
  6095
  6111
  6235
  6611
  7001
  7596
  7660
  7752
    6.7
    6.7
   30
   33.3
   23.3
    6.7
   30
   10
    6.7
   16.7
    3.3
   10
   36.7
    3.3
    3.3
    3.3
    3.3
  100
    3.3
D,E2
D,E2
D(+Q)
(M1(+E2))
(M1(+E2))
D,E2
(M1(+E2))
D,E2
D,E2
(M1+E2)
D,E2
D+Q
(E1(+M2))
D+Q
(E1)
(E1(+M2))
D+Q
(M1+E2)
E2(+M3)
   4635
   4129
   4088
   4002
   3912
   3757
   3741
   3405
   3388
   2309.4
   2265.3
   1661.40
   1646.43
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(5/2)-
(5/2)-
3/2(-),5/2,7/2-
(3/2)-
(3/2)-
5/2-,7/2-
1/2-,3/2-
(3/2)-
(3/2,5/2-)
3/2-
5/2-
3/2-
(1/2+)
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   7801.4 8  B           (25/2-)      956 1 
  2111 1 
  2271 1 
   88.9
  100
    8.9
D
D

   6844.9
   5689.9
   5529.7
(23/2-)
(23/2-)
(21/2-)
   7838.7 21    DE        (1/2-)     4098
  4451
  5574
  6177
  6196
  7090
  7685
    9
   21
   12
   47
  100
   26
   19







   3741
   3388
   2265.3
   1661.40
   1643.19
    748.27
    152.9282
1/2-,3/2-
(3/2,5/2-)
5/2-
3/2-
(3/2-,5/2)
3/2+
3/2-
   7910.2 21    DE        (1/2-)     4522
  5600
  5645
  5915
  6248
  6264
  7161
  7756
   29
   62
   25
   46
   62
   29
   62
  100








   3388
   2309.4
   2265.3
   1994.7
   1661.40
   1646.43
    748.27
    152.9282
(3/2,5/2-)
3/2-
5/2-
3/2(+)
3/2-
(1/2+)
3/2+
3/2-
   7943.5 21    DE        (3/2-)     3690
  3725
  4031
  4127
  4265
  4412
  4555
  5132
  5633
  5678
  5708
  5948
  6281
  6802
  7194
  7789
  7851
  7942
    6
    6
    6
    6
   28
    6
   17
   17
   50
  100
   11
   28
   83
   22
   11
   72
   78
   11


















   4253
   4218
   3912
   3816
   3678
   3531
   3388
   2810.9
   2309.4
   2265.3
   2234.0
   1994.7
   1661.40
   1140.53
    748.27
    152.9282
     90.6392
      0.0
1/2-,3/2-
(3/2)-
(3/2)-
(LE 7/2-)
(7/2)-
(LE 7/2-)
(3/2,5/2-)
5/2-,7/2-
3/2-
5/2-
5/2
3/2(+)
3/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8013.0 21    DE        (3/2-)     4789
  5703
  6351
  6872
  7264
  7859
  7921
  8012
    2
    6
    6
    5
  100
   15
    5
   23








   3224
   2309.4
   1661.40
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(1/2,3/2,5/2-)
3/2-
3/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8058.1 21    DE        (3/2,5/2+)     4317
  4670
  4799
  4816
  4834
  5670
  5748
  5793
  5823
  6063
  6412
  6543
  6917
  7309
  7904
  7966
   35
    9
    4
   13
    4
    9
   17
   17
   43
    9
   26
   57
   43
   30
  100
   17
















   3741
   3388
   3259.5
   3242
   3224
   2388.0
   2309.4
   2265.3
   2234.0
   1994.7
   1646.43
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
1/2-,3/2-
(3/2,5/2-)
(GE 9/2)
(3/2,5/2,7/2-)
(1/2,3/2,5/2-)
5/2+
3/2-
5/2-
5/2
3/2(+)
(1/2+)
5/2-
5/2+
3/2+
3/2-
5/2-
   8071.8 21    DE        (5/2)     5806
  6428
  7322
  7917
  7979
  8070
   22
   37
    5
  100
   32
   49






   2265.3
   1643.19
    748.27
    152.9282
     90.6392
      0.0
5/2-
(3/2-,5/2)
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8092.6   DE        (1/2-) 53 eV 15 
% IT = 4.8 19
% p = 95.2 19
  3456
  3718
  4089
  4179
  4249
  4349
  4851
  4866
  6429
  6447
  7341
  7936
  7999
    3.1
    7.8
    4.7
    4.7
    6.2
    6.2
    1.6
    6.2
    1.6
    9.4
    1.6
  100
    1.6
(E2(+M3))
D,E2
D,E2
D,E2
D,E2
D,E2
D,E2
D,E2
D,E2
(E1)
(E1)
D,E2
(E2+(M3))
   4635
   4373
   4002
   3912
   3841
   3741
   3242
   3224
   1661.40
   1646.43
    748.27
    152.9282
     90.6392
(5/2)-
1/2-,3/2-
(3/2)-
(3/2)-
1/2(+),3/2,5/2-
1/2-,3/2-
(3/2,5/2,7/2-)
(1/2,3/2,5/2-)
3/2-
(1/2+)
3/2+
3/2-
5/2-
   8104.2   D         3/2(-),5/2     4263
  4716
  4880
  5716
  5796
  6443
  6460
  6589
  6963
  7355
  7950
  8012
  8103?
   24
   12
   16
   16
   28
   28
  100
   76
   16
   36
   16
    8
    4













   3841
   3388
   3224
   2388.0
   2309.4
   1661.40
   1643.19
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
1/2(+),3/2,5/2-
(3/2,5/2-)
(1/2,3/2,5/2-)
5/2+
3/2-
3/2-
(3/2-,5/2)
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8117.5   D         3/2     3743
  4114
  4728
  4892
  5730
  5808
  5853
  5884
  6121
  6456
  6473
  6601
  6978
  7370
  7966
  8027
  8118
   13.6
   18.2
   22.7
   13.6
   13.6
   13.6
   13.6
   13.6
   59.1
   22.7
   31.8
    9.1
   45.4
   36.4
  100
   18.2
    9.1
D,E2
D,E2
D,E2
D,E2
D,E2
D,E2
D,E2
D,E2
D+Q
D+Q
D+Q
D,E2
D+Q
D+Q
D+Q
D(+Q)
Q+O
   4373
   4002
   3388
   3224
   2388.0
   2309.4
   2265.3
   2234.0
   1994.7
   1661.40
   1643.19
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
1/2-,3/2-
(3/2)-
(3/2,5/2-)
(1/2,3/2,5/2-)
5/2+
3/2-
5/2-
5/2
3/2(+)
3/2-
(3/2-,5/2)
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8131.5 21    D         (3/2-)     4528
  4600
  4743
  4889
  5743
  6136
  6469
  6488
  6616
  6990
  7382
  7977
  8039
  8130
    8.4
   12
    8.4
    2.4
   11
   14
   20
   29
   24
  100
   14
   20
    6.0
    2.4














   3603
   3531
   3388
   3242
   2388.0
   1994.7
   1661.40
   1643.19
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0

(LE 7/2-)
(3/2,5/2-)
(3/2,5/2,7/2-)
5/2+
3/2(+)
3/2-
(3/2-,5/2)
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8192 30     E               
   8246 30     E               
   8290.3   DE        3/2(-)     4287
  4548
  5980
  6295
  6627
  6645
  6773
  7148
  7540
  8137
  8197
  8288
    5.1
    5.1
   12.8
    5.1
    5.1
   20.5
    2.6
   51.3
  100
   18
    7.7
   10.3



D+Q
D+Q
D+Q


D+Q
D+Q
D+Q
Q+O
   4002
   3741
   2309.4
   1994.7
   1661.40
   1646.43
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2)-
1/2-,3/2-
3/2-
3/2(+)
3/2-
(1/2+)
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8371 30     E               
   8405 30     E               
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8416.1 9  B           (27/2-)      613 1 
  5690 1 
  100
   45
D
(Q)
   7801.4
   2727.5
(25/2-)
15/2-
   8444 30     E               
   8525.3 21    DE        (5/2)     4566
  4923
  6118
  6531
  6863
  6922
  7010
  7385
  7777
  8372
  8434
  8525
   14
   14
    3
    5
   57
    3
    5
   24
   19
   24
  100
    3












   3960
   3603
   2408.3
   1994.7
   1661.40
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2-,5/2,7/2-)

(7/2-)
3/2(+)
3/2-
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8628.2 21    DE        (3/2-)     5817
  6363
  6633
  6965
  6981
  7487
  7879
  8474
  8536
  8627
   26
   15
   37
   22
   48
  100
  100
   15
    4
    4










   2810.9
   2265.3
   1994.7
   1661.40
   1646.43
   1140.53
    748.27
    152.9282
     90.6392
      0.0
5/2-,7/2-
5/2-
3/2(+)
3/2-
(1/2+)
5/2+
3/2+
3/2-
5/2-
7/2-
   8633.1 21    DE        (5/2)     4504
  4673
  5117
  5245
  6245
  6323
  6398
  6450
  6638
  6970
  6989
  7029
  7117
  7492
  7884
  8479
  8541
  8632
   17
   12
    8
    8
    8
   29
   12
   17
   12
   12
   17
   12
   42
   38
   29
  100
   38
    4


















   4129
   3960
   3516
   3388
   2388.0
   2309.4
   2234.0
   2182.0
   1994.7
   1661.40
   1643.19
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(5/2)-
(3/2-,5/2,7/2-)
(3/2- TO 9/2)
(3/2,5/2-)
5/2+
3/2-
5/2
7/2-
3/2(+)
3/2-
(3/2-,5/2)
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8640.9 21    DE        (3/2-)     4422
  4639
  4680
  4728
  4799
  4899
  4919
  5002
  5401
  5623
  5834
  6330
  6996
  7124
  7891
  8486
  8548
  8639
    3
    3
    3
    6
    3
    3
    9
    3
    6
    3
    3
    3
   17
   11
   66
  100
   43
    3


















   4218
   4002
   3960
   3912
   3841
   3741
   3721
   3639.8
   3239.5
   3017.3
   2808.3
   2309.4
   1643.19
   1514.54
    748.27
    152.9282
     90.6392
      0.0
(3/2)-
(3/2)-
(3/2-,5/2,7/2-)
(3/2)-
1/2(+),3/2,5/2-
1/2-,3/2-
(LE 7/2)-
(7/2-)
7/2-

5/2+
3/2-
(3/2-,5/2)
5/2-
3/2+
3/2-
5/2-
7/2-
   8642.9 21    DE        (3/2-,5/2)     4383
  4389
  4640
  4682
  5254
  5317
  5400
  5508
  5625
  5831
  6254
  6332
  6377
  6407
  6647
  6979
  6995
  7126
  7501
  7893
  8488
  8550
  8641
    6
    6
   11
    6
    6
    6
    6
    6
   22
    6
    6
    6
    6
   17
   17
   56
   39
   17
   50
  100
   44
  100
   11























   4259
   4253
   4002
   3960
   3388
   3325
   3242
   3134.0
   3017.3
   2810.9
   2388.0
   2309.4
   2265.3
   2234.0
   1994.7
   1661.40
   1646.43
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2,5/2,7/2)
1/2-,3/2-
(3/2)-
(3/2-,5/2,7/2-)
(3/2,5/2-)
(1/2+ TO 7/2+)
(3/2,5/2,7/2-)
7/2,9/2(+)

5/2-,7/2-
5/2+
3/2-
5/2-
5/2
3/2(+)
3/2-
(1/2+)
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8682.0 21    DE        (5/2)     5011
  5044
  5357
  5458
  6274
  6294
  6417
  6447
  6687
  7019
  7035
  7166
  7541
  7933
  8528
  8590
  8681
    2
    2
    5
    2
    2
    2
    5
    2
    5
    9
    7
   11
    2
    9
  100
    7
   50

















   3671
   3639.8
   3325
   3224
   2408.3
   2388.0
   2265.3
   2234.0
   1994.7
   1661.40
   1646.43
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(1/2+ TO 9/2+)
(7/2-)
(1/2+ TO 7/2+)
(1/2,3/2,5/2-)
(7/2-)
5/2+
5/2-
5/2
3/2(+)
3/2-
(1/2+)
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8784.9 21    D         (5/2)     6377
  6397
  6789
  7122
  7269
  7644
  8036
  8631
  8693
  8784
    6
    6
   16
   29
   16
   16
   26
   19
   71
  100










   2408.3
   2388.0
   1994.7
   1661.40
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(7/2-)
5/2+
3/2(+)
3/2-
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8788.8 21    D         (5/2-)     5401
  5547
  5565
  5772
  6109
  6381
  6401
  6479
  6606
  7185
  7273
  7633
  7648
  8040
  8635
  8697
  8788
    8
    3
    5
    8
    5
    5
    5
    5
    5
    3
    5
   11
    5
   16
  100
   38
   32

















   3388
   3242
   3224
   3017.3
   2680.0
   2408.3
   2388.0
   2309.4
   2182.0
   1602.68
   1514.54
   1155.32
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2,5/2-)
(3/2,5/2,7/2-)
(1/2,3/2,5/2-)

(7/2,9/2)
(7/2-)
5/2+
3/2-
7/2-
7/2+
5/2-
9/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8851.5 21    DE        (5/2-,7/2-)     4723
  4940
  5464
  5628
  5835
  6046
  6444
  6464
  6617
  7248
  7336
  7696
  7711
  8698
  8760
  8851
    6
    6
   16
    6
    9
   12
    6
   25
   25
    3
    9
    3
   41
  100
    3
   22
















   4129
   3912
   3388
   3224
   3017.3
   2808.3
   2408.3
   2388.0
   2234.0
   1602.68
   1514.54
   1155.32
   1140.53
    152.9282
     90.6392
      0.0
(5/2)-
(3/2)-
(3/2,5/2-)
(1/2,3/2,5/2-)

5/2+
(7/2-)
5/2+
5/2
7/2+
5/2-
9/2-
5/2+
3/2-
5/2-
7/2-
   8867.2 21    DE        (5/2)     4955
  5026
  5126
  5229
  5403
  5479
  5625
  5733
  5850
  6459
  6479
  6557
  6602
  6632
  6871
  7204
  7263
  7351
  7726
  8118
  8713
  8775
  8866
    9
    9
    9
    4
    4
    4
    4
   13
    4
    4
    4
   22
    9
    9
    4
   48
    4
   17
   35
   52
  100
   22
   35























   3912
   3841
   3741
   3639.8
   3462.9
   3388
   3242
   3134.0
   3017.3
   2408.3
   2388.0
   2309.4
   2265.3
   2234.0
   1994.7
   1661.40
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2)-
1/2(+),3/2,5/2-
1/2-,3/2-
(7/2-)
(3/2+ TO 9/2+)
(3/2,5/2-)
(3/2,5/2,7/2-)
7/2,9/2(+)

(7/2-)
5/2+
3/2-
5/2-
5/2
3/2(+)
3/2-
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8877.0 21    DE        (5/2)     5489
  5552
  5638
  5653
  5743
  5860
  6066
  6489
  6567
  6642
  7214
  7361
  7736
  8128
  8723
  8785
  8876
    3
    3
    3
    3
    3
    3
    3
   12
    3
   12
    6
    6
   64
   33
   18
   27
  100

















   3388
   3325
   3239.5
   3224
   3134.0
   3017.3
   2810.9
   2388.0
   2309.4
   2234.0
   1661.40
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2,5/2-)
(1/2+ TO 7/2+)
7/2-
(1/2,3/2,5/2-)
7/2,9/2(+)

5/2-,7/2-
5/2+
3/2-
5/2
3/2-
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8880.9 21    DE        (5/2)     4879
  4969
  5040
  5065
  5187
  5417
  5493
  5864
  6473
  6571
  6646
  6698
  6885
  7234
  7277
  7365
  7740
  8789
  8880
    4
    4
    4
    4
    4
   13
    9
   22
    4
   13
   13
   22
   22
   17
    9
   13
   13
  100
   52



















   4002
   3912
   3841
   3816
   3694
   3462.9
   3388
   3017.3
   2408.3
   2309.4
   2234.0
   2182.0
   1994.7
   1646.43
   1602.68
   1514.54
   1140.53
     90.6392
      0.0
(3/2)-
(3/2)-
1/2(+),3/2,5/2-
(LE 7/2-)
3/2+,5/2+
(3/2+ TO 9/2+)
(3/2,5/2-)

(7/2-)
3/2-
5/2
7/2-
3/2(+)
(1/2+)
7/2+
5/2-
5/2+
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8890.7 21    DE        (3/2-)     4256
  4518
  4621
  4638
  4793
  4931
  5050
  5075
  5150
  5197
  5503
  6581
  6626
  6656
  6895
  7228
  7244
  8142
  8737
  8799
  8890
    7
    7
    7
    3
    3
    3
    3
    3
   10
    3
    7
   10
   13
    7
   10
   13
   43
  100
   50
   23
    7





















   4635
   4373
   4270
   4253
   4098
   3960
   3841
   3816
   3741
   3694
   3388
   2309.4
   2265.3
   2234.0
   1994.7
   1661.40
   1646.43
    748.27
    152.9282
     90.6392
      0.0
(5/2)-
1/2-,3/2-

1/2-,3/2-
(LE 7/2-)
(3/2-,5/2,7/2-)
1/2(+),3/2,5/2-
(LE 7/2-)
1/2-,3/2-
3/2+,5/2+
(3/2,5/2-)
3/2-
5/2-
5/2
3/2(+)
3/2-
(1/2+)
3/2+
3/2-
5/2-
7/2-
   8893.6 21    DE        (5/2-)     4496
  4634
  4764
  4981
  5152
  5255
  6082
  6087
  6583
  6628
  6658
  6710
  6897
  7230
  7289
  7377
  7737
  7752
  8144
  8739
  8801
  8892
    3
    3
    3
    6
    3
    3
    3
    3
    6
    9
   18
    6
    9
   12
    9
    9
    3
   18
   12
   21
   38
  100






















   4397
   4259
   4129
   3912
   3741
   3639.8
   2810.9
   2808.3
   2309.4
   2265.3
   2234.0
   2182.0
   1994.7
   1661.40
   1602.68
   1514.54
   1155.32
   1140.53
    748.27
    152.9282
     90.6392
      0.0
5/2-,7/2-
(3/2,5/2,7/2)
(5/2)-
(3/2)-
1/2-,3/2-
(7/2-)
5/2-,7/2-
5/2+
3/2-
5/2-
5/2
7/2-
3/2(+)
3/2-
7/2+
5/2-
9/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8895.6 21    DE        (5/2)     4636
  5507
  5653
  6630
  6899
  7232
  7291
  7379
  7754
  8146
  8741
  8803
  8894
    7
    7
    7
   10
    7
   31
    7
   14
   41
  100
   59
   41
   14













   4259
   3388
   3242
   2265.3
   1994.7
   1661.40
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2,5/2,7/2)
(3/2,5/2-)
(3/2,5/2,7/2-)
5/2-
3/2(+)
3/2-
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8902.5 21    DE        (5/2)     4614
  5664
  5886
  6593
  6668
  6907
  7256
  7259
  7387
  7762
  8154
  8749
  8811
  8902
    5
   20
   10
   15
   30
   20
   10
   35
   10
   30
   65
   95
   55
  100














   4289
   3239.5
   3017.3
   2309.4
   2234.0
   1994.7
   1646.43
   1643.19
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
3/2+,5/2+
7/2-

3/2-
5/2
3/2(+)
(1/2+)
(3/2-,5/2)
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8912.2 21    DE        (5/2)     4515
  4783
  5000
  5218
  5309
  5524
  5673
  6101
  6504
  6602
  6647
  6677
  6916
  7249
  7265
  7396
  7771
  8163
  8758
  8820
  8911
    5
    3
    5
    3
    3
    3
    3
   10
    5
    5
    5
    8
    8
    8
    3
    3
    8
   13
   21
   49
  100





















   4397
   4129
   3912
   3694
   3603
   3388
   3239.5
   2810.9
   2408.3
   2309.4
   2265.3
   2234.0
   1994.7
   1661.40
   1646.43
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
5/2-,7/2-
(5/2)-
(3/2)-
3/2+,5/2+

(3/2,5/2-)
7/2-
5/2-,7/2-
(7/2-)
3/2-
5/2-
5/2
3/2(+)
3/2-
(1/2+)
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8921.1 21    D         (5/2+)     6612
  6739
  6743
  6926
  7275
  7318
  7406
  7781
  8173
  8768
  8831
  8921
   42
   16
   16
   21
   42
   53
   21
   16
   42
  100
   68
   89












   2309.4
   2182.0
   2178.3
   1994.7
   1646.43
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
3/2-
7/2-
9/2+
3/2(+)
(1/2+)
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8925.0 21    D         (7/2-)     4290
  4890
  5143
  5537
  6690
  7262
  7321
  7409
  7784
  8771
  8833
  8924
    2
    2
    4
    4
    4
    4
   15
    4
    6
   49
   13
  100












   4635
   4035
   3782
   3388
   2234.0
   1661.40
   1602.68
   1514.54
   1140.53
    152.9282
     90.6392
      0.0
(5/2)-
(3/2- TO 9/2+)
(GE 9/2)
(3/2,5/2-)
5/2
3/2-
7/2+
5/2-
5/2+
3/2-
5/2-
7/2-
   8927.9 21    DE        (5/2)     5540
  5911
  6618
  6693
  6932
  7265
  7281
  7324
  7412
  7787
  8179
  8774
  8836
  8927
   22
   33
   22
   39
   11
   56
   83
   11
   11
   56
   22
   50
   39
  100














   3388
   3017.3
   2309.4
   2234.0
   1994.7
   1661.40
   1646.43
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2,5/2-)

3/2-
5/2
3/2(+)
3/2-
(1/2+)
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8942.6 21    D         (5/2)     5249
  5926
  6555
  6633
  6708
  6947
  7280
  7296
  7339
  7427
  7802
  8194
  8789
  8851
  8942
   14
   10
   14
   29
    5
   14
   62
   62
   14
   14
   10
   29
   48
   52
  100















   3694
   3017.3
   2388.0
   2309.4
   2234.0
   1994.7
   1661.40
   1646.43
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
3/2+,5/2+

5/2+
3/2-
5/2
3/2(+)
3/2-
(1/2+)
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   8945 25          J   (1/2+)        
   8965.1 21    D         (5/2+)     4712
  4747
  4877
  5005
  5038
  5053
  5149
  5224
  5577
  5741
  5831
  5948
  6285
  6557
  6785
  7449
  7824
  8216
  8811
  8873
  8964
    4
    4
    4
    8
    8
    8
    8
   17
   12
    4
    8
   12
    8
    8
    8
   38
  100
   42
   42
   50
   21





















   4253
   4218
   4088
   3960
   3927
   3912
   3816
   3741
   3388
   3224
   3134.0
   3017.3
   2680.0
   2408.3
   2178.3
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
1/2-,3/2-
(3/2)-
3/2(-),5/2,7/2-
(3/2-,5/2,7/2-)
(1/2+ TO 9/2+)
(3/2)-
(LE 7/2-)
1/2-,3/2-
(3/2,5/2-)
(1/2,3/2,5/2-)
7/2,9/2(+)

(7/2,9/2)
(7/2-)
9/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   8998.5 21    D         (1/2-)     6733
  7351
  8249
  8844
   27
   11
   19
  100




   2265.3
   1646.43
    748.27
    152.9282
5/2-
(1/2+)
3/2+
3/2-
   9008.2 21    D         (5/2+)     4920
  5006
  5096
  5237
  5267
  5330
  5337
  5666
  5991
  6600
  6620
  6698
  7012
  7361
  7404
  7867
  8259
  8854
  8916
  9007
    6
    9
   14
    6
    9
    9
    9
    9
   11
    6
   29
   11
   14
    3
    3
   14
   14
  100
    9
    9




















   4088
   4002
   3912
   3771
   3741
   3678
   3671
   3342
   3017.3
   2408.3
   2388.0
   2309.4
   1994.7
   1646.43
   1602.68
   1140.53
    748.27
    152.9282
     90.6392
      0.0
3/2(-),5/2,7/2-
(3/2)-
(3/2)-
(1/2+ TO 9/2+)
1/2-,3/2-
(7/2)-
(1/2+ TO 9/2+)
(1/2+ TO 9/2+)

(7/2-)
5/2+
3/2-
3/2(+)
(1/2+)
7/2+
5/2+
3/2+
3/2-
5/2-
7/2-
   9029.8 21    D         (5/2)     4490
  5359
  5427
  5642
  5791
  5896
  6013
  6622
  6642
  6720
  6794
  7034
  7367
  7386
  7426
  7889
  8281
  8876
  8938
  9029
    4
    2
    2
    2
    9
    2
    7
    2
    4
    2
    7
   11
    7
   16
    2
    4
    7
   11
    9
  100




















   4540
   3671
   3603
   3388
   3239.5
   3134.0
   3017.3
   2408.3
   2388.0
   2309.4
   2234.0
   1994.7
   1661.40
   1643.19
   1602.68
   1140.53
    748.27
    152.9282
     90.6392
      0.0

(1/2+ TO 9/2+)

(3/2,5/2-)
7/2-
7/2,9/2(+)

(7/2-)
5/2+
3/2-
5/2
3/2(+)
3/2-
(3/2-,5/2)
7/2+
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   9037.6 21    D         (5/2)     7897
  8289
  8884
  8946
  9037
   96
   22
   93
  100
   59





   1140.53
    748.27
    152.9282
     90.6392
      0.0
5/2+
3/2+
3/2-
5/2-
7/2-
   9044.5 21    D         (7/2-)     5084
  5132
  5528
  5785
  6373?
  6373?
  6734
  6808
  6860
  7528
  7903
  8890
  8952
  9043
   13
   13
   13
   25
   19
   19
   69
   44
   69
   19
   81
   94
   69
  100














   3960
   3912
   3516
   3259.5
   2671.3
   2671.0
   2309.4
   2234.0
   2182.0
   1514.54
   1140.53
    152.9282
     90.6392
      0.0
(3/2-,5/2,7/2-)
(3/2)-
(3/2- TO 9/2)
(GE 9/2)
7/2-,9/2,11/2+
(11/2)-
3/2-
5/2
7/2-
5/2-
5/2+
3/2-
5/2-
7/2-
   9056.2 21    D         (5/2)     6747
  7061
  7394
  7541
  7916
  8308
  8903
  8965
  9056
   23
   20
   10
   10
    7
   27
  100
   53
   83









   2309.4
   1994.7
   1661.40
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
3/2-
3/2(+)
3/2-
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   9071.9 21    D         (5/2)     5551
  5684
  6055
  6261
  6684
  6761
  6836
  6888
  7076
  7409
  7425
  7468
  7556
  7931
  8323
  8918
  8980
  9071
   14
    5
   10
    5
   10
   48
    5
   10
   19
   24
   29
   10
   10
   19
   24
   81
  100
   57


















   3516
   3388
   3017.3
   2810.9
   2388.0
   2309.4
   2234.0
   2182.0
   1994.7
   1661.40
   1646.43
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2- TO 9/2)
(3/2,5/2-)

5/2-,7/2-
5/2+
3/2-
5/2
7/2-
3/2(+)
3/2-
(1/2+)
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   9075.8 21    D         (5/2)     5116
  5164
  5355
  5382
  5751
  6059
  6668
  6765
  6892
  7080
  7413
  7432
  7472
  7560
  7935
  8327
  8922
  8984
  9075
    5
   11
    5
    5
   11
   16
   11
   32
   11
   32
   32
   32
   26
   37
   37
   11
   53
   63
  100



















   3960
   3912
   3721
   3694
   3325
   3017.3
   2408.3
   2309.4
   2182.0
   1994.7
   1661.40
   1643.19
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2-,5/2,7/2-)
(3/2)-
(LE 7/2)-
3/2+,5/2+
(1/2+ TO 7/2+)

(7/2-)
3/2-
7/2-
3/2(+)
3/2-
(3/2-,5/2)
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   9078.8 21    D         (3/2-)     6062
  6691
  7416
  7435
  7563
  8330
  8925
  8987
  9078
    5
   10
    7
    7
   10
  100
   16
    9
    9









   3017.3
   2388.0
   1661.40
   1643.19
   1514.54
    748.27
    152.9282
     90.6392
      0.0

5/2+
3/2-
(3/2-,5/2)
5/2-
3/2+
3/2-
5/2-
7/2-
   9082.7 21    D     J   (3/2+)     7420
  7439
  7942
  8334
  8929
  8993
   27
   43
   57
   53
   13
  100






   1661.40
   1643.19
   1140.53
    748.27
    152.9282
     90.6392
3/2-
(3/2-,5/2)
5/2+
3/2+
3/2-
5/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   9089.5 21    D         (3/2-,5/2)     6702
  7443
  8341
  8936
  8998
  9089
    7
    3
   10
  100
   33
    5






   2388.0
   1646.43
    748.27
    152.9282
     90.6392
      0.0
5/2+
(1/2+)
3/2+
3/2-
5/2-
7/2-
   9094.4 21    D         (5/2)     5183
  5354
  5401
  6078
  6784
  6859
  7448
  7579
  7954
  8346
  8941
  9003
  9094
    7
    7
    7
   14
    7
   11
   36
   21
   36
  100
   25
   82
    4













   3912
   3741
   3694
   3017.3
   2309.4
   2234.0
   1643.19
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2)-
1/2-,3/2-
3/2+,5/2+

3/2-
5/2
(3/2-,5/2)
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   9118.0 21    D         (5/2)     5730
  6101
  6312
  6807
  6882
  7122
  7514
  7602
  7977
  8369
  8964
  9026
  9117
    5
   33
   24
   10
   52
   48
   14
  100
   29
   24
   29
   81
   29













   3388
   3017.3
   2808.3
   2309.4
   2234.0
   1994.7
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(3/2,5/2-)

5/2+
3/2-
5/2
3/2(+)
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   9131.7 21    D         (5/2)     6821
  6866
  7469
  7485
  7528
  8383
  8978
  9040
  9131
    9
   13
    9
   24
   17
   11
  100
   24
   11









   2309.4
   2265.3
   1661.40
   1646.43
   1602.68
    748.27
    152.9282
     90.6392
      0.0
3/2-
5/2-
3/2-
(1/2+)
7/2+
3/2+
3/2-
5/2-
7/2-
   9135.6 21    D         (5/2)     7472
  7488
  8386
  8981
  9043
  9134
   38
   21
   28
  100
   21
   49






   1661.40
   1646.43
    748.27
    152.9282
     90.6392
      0.0
3/2-
(1/2+)
3/2+
3/2-
5/2-
7/2-
   9148.3 21    D         (5/2)     5618
  6760
  6965
  7153
  7545
  7633
  8400
  8995
  9057
  9148
   25
   35
   35
   65
   60
   50
  100
   45
   65
   20










   3531
   2388.0
   2182.0
   1994.7
   1602.68
   1514.54
    748.27
    152.9282
     90.6392
      0.0
(LE 7/2-)
5/2+
7/2-
3/2(+)
7/2+
5/2-
3/2+
3/2-
5/2-
7/2-
   9154.2 21    D         (5/2+)     5915
  5930
  6348
  6843
  6888
  6974
  7491
  7507
  7638
  8405
  9000
  9062
  9153
    9
    5
   14
   59
   23
   14
   36
   23
   59
  100
   50
   41
   23













   3239.5
   3224
   2808.3
   2309.4
   2265.3
   2178.3
   1661.40
   1646.43
   1514.54
    748.27
    152.9282
     90.6392
      0.0
7/2-
(1/2,3/2,5/2-)
5/2+
3/2-
5/2-
9/2+
3/2-
(1/2+)
5/2-
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   9161.1 21    D         (1/2-,3/2)     5937
  6895
  6925
  7517
  8412
  9007
  9069
    5
    7
   16
   19
    9
  100
   19







   3224
   2265.3
   2234.0
   1643.19
    748.27
    152.9282
     90.6392
(1/2,3/2,5/2-)
5/2-
5/2
(3/2-,5/2)
3/2+
3/2-
5/2-
   9167.9 21    D         (5/2)     4533
  4746
  4809
  5133
  5208
  5427
  5474
  5490
  5565
  5780
  5926
  6151
  6362
  6759
  6779
  6857
  6902
  6932
  7172
  7505
  7524
  7564
  7652
  8027
  8419
  9014
  9076
  9167
    8
    8
   15
    8
   15
    8
    8
    8
    8
   15
   15
   15
   23
   15
   15
   62
   15
    8
    8
   69
   62
   54
   46
   31
   23
   77
   31
  100




























   4635
   4422
   4359
   4035
   3960
   3741
   3694
   3678
   3603
   3388
   3242
   3017.3
   2808.3
   2408.3
   2388.0
   2309.4
   2265.3
   2234.0
   1994.7
   1661.40
   1643.19
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(5/2)-


(3/2- TO 9/2+)
(3/2-,5/2,7/2-)
1/2-,3/2-
3/2+,5/2+
(7/2)-

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

5/2+
(7/2-)
5/2+
3/2-
5/2-
5/2
3/2(+)
3/2-
(3/2-,5/2)
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   9168.9 21    D         (3/2-)     5428
  5781
  5945
  6858
  7173
  7506
  7525
  7565
  7653
  9015
  9077
  9168
    2
    2
    3
    5
    7
    5
   12
    3
    3
  100
    3
    7












   3741
   3388
   3224
   2309.4
   1994.7
   1661.40
   1643.19
   1602.68
   1514.54
    152.9282
     90.6392
      0.0
1/2-,3/2-
(3/2,5/2-)
(1/2,3/2,5/2-)
3/2-
3/2(+)
3/2-
(3/2-,5/2)
7/2+
5/2-
3/2-
5/2-
7/2-
   9174.8 21    D         (5/2)     6157
  6863
  7511
  7570
  8033
  8425
  9020
  9082
  9173
   14
    9
   23
   11
   23
   40
   49
   17
  100









   3017.3
   2309.4
   1661.40
   1602.68
   1140.53
    748.27
    152.9282
     90.6392
      0.0

3/2-
3/2-
7/2+
5/2+
3/2+
3/2-
5/2-
7/2-
   9182.6 21    D         (5/2)     7667
  8042
  8434
  9091
  9182
    7
  100
   74
   47
    5





   1514.54
   1140.53
    748.27
     90.6392
      0.0
5/2-
5/2+
3/2+
5/2-
7/2-
   9193.4 21    D         (5/2,7/2+)     7197
  7546
  8444
  9101
  9192
  100
   42
  100
   92
   83





   1994.7
   1646.43
    748.27
     90.6392
      0.0
3/2(+)
(1/2+)
3/2+
5/2-
7/2-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
   9195.3 21    D         (5/2)     5674
  6178
  6786
  6806
  6884
  7532
  7591
  7679
  8054
  8446
  9041
  9103
  9194
   14
   14
   14
   14
   14
   38
   19
   38
   76
   90
   19
   24
  100













   3521
   3017.3
   2408.3
   2388.0
   2309.4
   1661.40
   1602.68
   1514.54
   1140.53
    748.27
    152.9282
     90.6392
      0.0
(LE 9/2)

(7/2-)
5/2+
3/2-
3/2-
7/2+
5/2-
5/2+
3/2+
3/2-
5/2-
7/2-
   9568 10     E        (1/2-)        
   9662 10     E        3/2-        
  10230 10     E        (5/2)-        
  10925 7     E        (5/2)+        
  11150 7     E        (9/2+)        

E(level): From a least-squares fit to Eγ except as noted in the XREF column, comments, or footnotes. Resonance E(level)=(0.97955873 4)E(p)+S(p) with S(p)=6758.2 8 (2003Au03)

Jπ(level): From angular momentum transfer in (3He,d), except as noted

T1/2(level): From (α,pγ), except as noted; see discussion of discrepancies there and in (p,nγ). Γ’s from Γp and Γγ in (p,γ)

Back to top

Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - 7/2- GS yrast band
      0.0 7/2- 330 d 15 
% ε = 100
     
     90.6392 17  5/2- 228 ps 13      90.639 2 
  100
M1
      0.0
7/2-
   1021.62 11  11/2- 3.4 ps 6    1021.63 14 
  100
E2
      0.0
7/2-
   1155.32 10  9/2- 1.1 ps 3     133.80 17 
  1064.63 17 
  1155.33 17 
    3.9 8 
   30.0 6 
  100.0 10 
(M1(+E2))
E2
M1+E2
   1021.62
     90.6392
      0.0
11/2-
5/2-
7/2-
   2263.30 21  15/2- 0.65 ps +38-19    1241.69 18 
  100
E2
   1021.62
11/2-
   2861.5 5  13/2- 0.10 ps 6     134 1 ?
   598.3 7 
  1706 1 
  1840 1 ?
 
   28.2 13 
  100 6 
 
(M1(+E2))
(M1(+E2))
E2(+M3)
D,E2
   2727.5
   2263.30
   1155.32
   1021.62
15/2-
15/2-
9/2-
11/2-
   3325.2 4  (17/2-)      464 1 
   597.1 5 
  1061.9 5 
   36.84
   21.05
  100
D,Q
D
D
   2861.5
   2727.5
   2263.30
13/2-
15/2-
15/2-
   3742.4 6  (19/2-)        
   5529.7 7  (21/2-)     1787 1 
  2204 1 
  100
   43
D

   3742.4
   3325.2
(19/2-)
(17/2-)
   5689.9 8  (23/2-)      160 1 
  1947 1 
    2.7
  100

D,Q
   5529.7
   3742.4
(21/2-)
(19/2-)
   7801.4 8  (25/2-)        
   8416.1 9  (27/2-)      613 1 
  5690 1 
  100
   45
D
(Q)
   7801.4
   2727.5
(25/2-)
15/2-
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - Kπ=3/2+ ROTATIONAL band
    748.27 9  3/2+ 5.3 ps 6       
   1140.53 11  5/2+ 1.3 ps 6     392.7 6 
   987.61 26 
  1049.79 17 
  1140.7 3 
   10.5 10 
   31.4 17 
   44.5 21 
  100 4 
M1+E2
(E1(+M2))
E1+M2
E1(+M2)
    748.27
    152.9282
     90.6392
      0.0
3/2+
3/2-
5/2-
7/2-
   1602.68 12  7/2+ 0.47 ps 22     447.4 3 
   462.2 2 
   854.5 3 
  1512.0 3 
  1602.6 2 
    1.6 8 
   13.5 17 
   15 4 
  100 8 
   49.3 20 
(E1)
M1(+E2)
(E2)
(E1)
(E1+M2)
   1155.32
   1140.53
    748.27
     90.6392
      0.0
9/2-
5/2+
3/2+
5/2-
7/2-
   2178.3 4  9/2+ 0.56 ps +49-28     575.4 9 
  1023 1 ?
  1037.4 5 
  1157.0 7 
  2178.3 8 
   11.3 17 
 
   33.9 17 
   16.1 17 
  100 5 
D(+Q)
D,Q
E2
D
D(+Q)
   1602.68
   1155.32
   1140.53
   1021.62
      0.0
7/2+
9/2-
5/2+
11/2-
7/2-
   2741.0 5  11/2+ 0.39 ps +36-17     562.5 7 
  1138.9 9 
  1585.8 9 
  1719.0 15 ?
   27.1 21 
  100 5 
   81 5 
  <10
D,E2
(E2)
(E1(+M2))
(E1(+M2))
   2178.3
   1602.68
   1155.32
   1021.62
9/2+
7/2+
9/2-
11/2-
   3341.8 7  (13/2+)      601.0 8 
   670.5 8 
  1163.0 10 
   72.5 25 
   78 5 
  100 5 
D,E2
D,E2
D,Q
   2741.0
   2671.0
   2178.3
11/2+
(11/2)-
9/2+
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 3 - Kπ=1/2+ ROTATIONAL BAND?
   1646.43 21  (1/2+) 6.6 ps 10       
   1994.7 4  3/2(+) 0.49 ps 21     854.5 4 
  1246.8 10 
  1841.0 8 
  1903.4 8 
   85 21 
   46 5 
  100 5 
   62 5 
(M1+E2)
D,E2
(E1+M2)
(E1(+M2))
   1140.53
    748.27
    152.9282
     90.6392
5/2+
3/2+
3/2-
5/2-
   2388.0 5  5/2+ 57 fs 20     393.6 15 ?
  1247.8 12 ?
  1639.3 6 
  2235.5 16 ?
  2298.6 15 
  2388.6 14 
   16.9 17 
   11.9 17 
  100 5 
   <8.5
   28.8 17 
   11.9 17 
(M1(+E2))
D,E2
M1+E2

(E1(+M2))
(E1(+M2))
   1994.7
   1140.53
    748.27
    152.9282
     90.6392
      0.0
3/2(+)
5/2+
3/2+
3/2-
5/2-
7/2-
E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 4 - NEGATIVE-PARITY SIDE band
   2671.0 3  (11/2)- < 11 fs      
   2727.5 3  15/2- 0.10 ps 4     464.2 3 
  1705.5 7 
  100
  100
M1(+E2)
(E2)
   2263.30
   1021.62
15/2-
11/2-
   2810.9 5  5/2-,7/2- < 12 fs    628.4 10 
  1673 2 ?
  2720.3 19 
  2810.9 5 
   33 5 
   25 6 
  100 5 
   75 5 
M1
D,E2
D,E2
D,E2
   2182.0
   1140.53
     90.6392
      0.0
7/2-
5/2+
5/2-
7/2-
   6844.9 8  (23/2-)     1155 1 
  1315 1 
  3102 1 
  100
    6.2
   12.5
D


   5689.9
   5529.7
   3742.4
(23/2-)
(21/2-)
(19/2-)

Back to top

Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
     90.6392 5/2- 228 ps 13      90.639 2 M1 0.0287B(M1)(W.u.)=0.126 8, α=0.0287, α(K)=0.0259 4, α(L)=0.00245 4, α(M)=0.000320 5, α(N)=1.629×10-5 23, α(N+)=1.629E-5 23
    152.9282 3/2- 19.90 ns 24      62.289 2 (M1) 0.0787B(M1)(W.u.)=0.00176 8, α=0.0787, α(K)=0.0710 10, α(L)=0.00676 10, α(M)=0.000885 13, α(N)=4.47×10-5 7, α(N+)=4.47E-5 7
3/2- 19.90 ns 24     152.928 2 E2 0.0725B(E2)(W.u.)=17.4 7, α=0.0725, α(K)=0.0654 10, α(L)=0.00623 9, α(M)=0.000808 12, α(N)=3.91E-5 6, α(N+)=3.91E-5 6
    748.27 3/2+ 5.3 ps 6     595.35 14 (E1(+M2))-0.02 20.000184B(E1)(W.u.)=0.00024 3, B(M2)(W.u.)=1.3 +26-13, α=0.000184 3, α(K)=0.0001664 25, α(L)=1.514E-5 23, α(M)=1.98E-6 3, α(N)=1.030E-7 16, α(N+)=1.030E-7 16
3/2+ 5.3 ps 6     657.60 14 (E1(+M2))-0.01 20.0001450B(E1)(W.u.)=0.000154 18, B(M2)(W.u.)=0.16 +66-16, α=0.0001450 21, α(K)=0.0001317 19, α(L)=1.197E-5 18, α(M)=1.567E-6 23, α(N)=8.15E-8 12, α(N+)=8.15E-8 12
   1021.62 11/2- 3.4 ps 6    1021.63 14 E2 0.0001310B(E2)(W.u.)=14.0 25, α=0.0001310 19, α(K)=0.0001184 17, α(L)=1.079E-5 16, α(M)=1.413E-6 20, α(N)=7.35E-8 11, α(N+)=7.35E-8 11
   1140.53 5/2+ 1.3 ps 6     392.7 6 M1+E2 0.0015α=0.0015 8, α(K)=0.0013 7, α(L)=0.00012 6, α(M)=1.6×10-5 8, α(N)=8.E-7 4, α(N+)=8.E-7 4
5/2+ 1.3 ps 6     987.61 26 (E1(+M2))-0.04 86.16×10-5B(E1)(W.u.)=7.E-5 4, B(M2)(W.u.)=0.5 +21-5, α=6.16E-5 25, α(K)=5.59E-5 22, α(L)=5.07E-6 21, α(M)=6.6E-7 3, α(N)=3.46E-8 14, α(N+)=3.46E-8 14
5/2+ 1.3 ps 6    1049.79 17 E1+M2 0.00013B(E1)(W.u.)=8.E-5 4, α=0.00013 8, α(K)=0.00012 7, α(L)=1.1E-5 7, α(M)=1.4E-6 9, α(N)=7.E-8 5, α(N+)=7.E-8 5
5/2+ 1.3 ps 6    1140.7 3 E1(+M2)-0.05 67.00×10-5B(E1)(W.u.)=0.00014 7, B(M2)(W.u.)=1.2 +30-12, α=7.00E-5 14, α(K)=4.27E-5 13, α(L)=3.87E-6 12, α(M)=5.07E-7 15, α(N)=2.65E-8 8, α(N+)=2.30E-5 4
   1155.32 9/2- 1.1 ps 3     133.80 17 (M1(+E2))-0.15 150.013B(E2)(W.u.)=7.×102 +15-7, B(M1)(W.u.)=0.24 9, α=0.013 7, α(K)=0.012 6, α(L)=0.0011 6, α(M)=0.00014 8, α(N)=7.E-6 4, α(N+)=7.E-6 4
9/2- 1.1 ps 3    1064.63 17 E2 0.0001180B(E2)(W.u.)=7.9 22, α=0.0001180 17, α(K)=0.0001073 15, α(L)=9.77E-6 14, α(M)=1.280E-6 18, α(N)=6.66E-8 10, α(N+)=6.66E-8 10
9/2- 1.1 ps 3    1155.33 17 M1+E2+0.70 78.89×10-5B(E2)(W.u.)=5.8 18, B(M1)(W.u.)=0.0065 19, α=8.89E-5 16, α(K)=7.78E-5 14, α(L)=7.07E-6 12, α(M)=9.26E-7 16, α(N)=4.84E-8 9, α(N+)=3.11E-6 8
   1514.54 5/2- 31 fs 12     766 1 (E1(+M2)) 0.00028B(E1)(W.u.)=0.006 3, α=0.00028 18, α(K)=0.00025 16, α(L)=2.3E-5 15, α(M)=3.0E-6 20, α(N)=1.6E-7 10, α(N+)=1.6E-7 10
5/2- 31 fs 12    1361.61 7 M1+E2-0.57 59.57×10-5B(E2)(W.u.)=42 18, B(M1)(W.u.)=0.10 4, α=9.57E-5 16, α(K)=5.53E-5 9, α(L)=5.02E-6 8, α(M)=6.58E-7 10, α(N)=3.44E-8 6, α(N+)=3.47E-5 7
5/2- 31 fs 12    1423.6 3 (M1(+E2))-0.6 +6-211.06×10-4B(E2)(W.u.)=7 +12-7, B(M1)(W.u.)=0.017 12, α=1.06E-4 16, α(K)=5.1E-5 5, α(L)=4.6E-6 5, α(M)=6.1E-7 6, α(N)=3.2E-8 3, α(N+)=4.9E-5 11
   1602.68 7/2+ 0.47 ps 22     447.4 3 (E1) 0.000376B(E1)(W.u.)=0.00011 8, α=0.000376 6, α(K)=0.000340 5, α(L)=3.10E-5 5, α(M)=4.05E-6 6, α(N)=2.10E-7 3, α(N+)=2.10E-7 3
7/2+ 0.47 ps 22     462.2 2 M1(+E2)-0.05 210.00053B(E2)(W.u.)=1.0 +85-10, B(M1)(W.u.)=0.036 18, α=0.00053 5, α(K)=0.00048 4, α(L)=4.4E-5 4, α(M)=5.8E-6 5, α(N)=3.01E-7 25, α(N+)=3.01E-7 25
7/2+ 0.47 ps 22     854.5 3 (E2) 0.000205B(E2)(W.u.)=21 12, α=0.000205 3, α(K)=0.000185 3, α(L)=1.692E-5 24, α(M)=2.22E-6 4, α(N)=1.149E-7 17, α(N+)=1.149E-7 17
7/2+ 0.47 ps 22    1512.0 3 (E1) 0.000300B(E1)(W.u.)=0.00017 9, α=0.000300 5, α(K)=2.61E-5 4, α(L)=2.36E-6 4, α(M)=3.10E-7 5, α(N)=1.620E-8 23, α(N+)=0.000271 4
7/2+ 0.47 ps 22    1602.6 2 (E1+M2)+0.29 113.50×10-4B(E1)(W.u.)=7.E-5 4, B(M2)(W.u.)=10 9, α=3.50E-4 16, α(K)=2.8E-5 3, α(L)=2.5E-6 3, α(M)=3.3E-7 4, α(N)=1.71E-8 19, α(N+)=0.000320 19
   1646.43 (1/2+) 6.6 ps 10    1493.6 3 (E1(+M2)) 0.00020B(E1)(W.u.)=1.2E-5 3, α=0.00020 9, α(K)=6.E-5 3, α(L)=5.E-6 3, α(M)=7.E-7 4, α(N)=3.5E-8 18, α(N+)=0.00014 12
   1661.40 3/2- 16 fs 7     912.3 10 (E1(+M2)) 0.00018B(E1)(W.u.)=0.0021 10, α=0.00018 11, α(K)=0.00016 10, α(L)=1.5E-5 10, α(M)=2.0E-6 12, α(N)=1.0E-7 7, α(N+)=1.0E-7 7
3/2- 16 fs 7    1570.83 17 M1(+E2)-0.04 91.33×10-4B(E2)(W.u.)=0.3 +13-3, B(M1)(W.u.)=0.18 8, α=1.33E-4 2, α(K)=4.11E-5 6, α(L)=3.72E-6 6, α(M)=4.88E-7 7, α(N)=2.56E-8 4, α(N+)=8.74E-5 13
3/2- 16 fs 7    1661.4 10 (E2(+M3)) 0.00018B(E2)(W.u.)=24 11, α=0.00018 3, α(K)=8.E-5 4, α(L)=7.E-6 4, α(M)=9.E-7 5, α(N)=4.9E-8 23, α(N+)=9.E-5 7
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
   1994.7 3/2(+) 0.49 ps 21     854.5 4 (M1+E2)-0.22 161.47×10-4B(E2)(W.u.)=3 +5-3, B(M1)(W.u.)=0.020 10, α=1.47E-4 6, α(K)=0.000133 5, α(L)=1.21E-5 5, α(M)=1.59E-6 6, α(N)=8.3E-8 3, α(N+)=8.3E-8 3
3/2(+) 0.49 ps 21    1841.0 8 (E1+M2)-0.17 95.35×10-4B(E1)(W.u.)=5.5E-5 24, B(M2)(W.u.)=2.1 +24-2, α=5.35E-4 16, α(K)=2.02E-5 13, α(L)=1.83E-6 12, α(M)=2.39E-7 15, α(N)=1.25E-8 8, α(N+)=0.000512 17
3/2(+) 0.49 ps 21    1903.4 8 (E1(+M2)) 0.00038B(E1)(W.u.)=3.2E-5 14, α=0.00038 22, α(K)=3.4E-5 17, α(L)=3.1E-6 15, α(M)=4.1E-7 20, α(N)=2.1E-8 10, α(N+)=0.00034 24
   2178.3 9/2+ 0.56 ps +49-28     575.4 9 D(+Q)-0.07 15 
9/2+ 0.56 ps +49-28    1037.4 5 E2 0.0001260B(E2)(W.u.)=17 +9-15, α=0.0001260 18, α(K)=0.0001141 16, α(L)=1.040E-5 15, α(M)=1.361E-6 20, α(N)=7.08E-8 10, α(N+)=7.08E-8 10
9/2+ 0.56 ps +49-28    2178.3 8 D(+Q)-0.02 5 
   2182.0 7/2- 33 fs 12    1026.8 7 (M1(+E2)) 1.00×10-4B(M1)(W.u.)=0.14 6, α=1.00×10-4 2, α(K)=9.09E-5 13, α(L)=8.26E-6 12, α(M)=1.083E-6 16, α(N)=5.66E-8 8, α(N+)=5.66E-8 8
7/2- 33 fs 12    2090.7 7 (M1+E2)-0.09 40.000318B(E2)(W.u.)=0.23 23, B(M1)(W.u.)=0.052 20, α=0.000318 5, α(K)=2.50E-5 4, α(L)=2.26E-6 4, α(M)=2.97E-7 5, α(N)=1.556E-8 22, α(N+)=0.000290 5
   2234.0 5/2 12 fs 8    2142.9 10 D(+Q)+0.04 14 
   2263.30 15/2- 0.65 ps +38-19    1241.69 18 E2 9.96×10-5B(E2)(W.u.)=28 +8-17, α=9.96E-5 14, α(K)=7.55E-5 11, α(L)=6.86E-6 10, α(M)=8.99E-7 13, α(N)=4.69E-8 7, α(N+)=1.637E-5 24
   2309.4 3/2- 14 fs 7    1560(E1(+M2)) 0.00023B(E1)(W.u.)=0.0007 4, α=0.00023 11, α(K)=5.E-5 3, α(L)=4.6E-6 24, α(M)=6.E-7 4, α(N)=3.2E-8 17, α(N+)=0.00017 14
3/2- 14 fs 7    2310.6 14 (E2) 0.000490B(E2)(W.u.)=12 6, α=0.000490 7, α(K)=2.24E-5 4, α(L)=2.03E-6 3, α(M)=2.66E-7 4, α(N)=1.393E-8 20, α(N+)=0.000465 7
   2353.4 9/2- 33 fs 12    1331.7 7 (M1+E2)-0.19 168.79×10-5B(E2)(W.u.)=4 +8-4, B(M1)(W.u.)=0.09 4, α=8.79E-5 20, α(K)=5.58E-5 11, α(L)=5.06E-6 10, α(M)=6.64E-7 13, α(N)=3.47E-8 7, α(N+)=2.64E-5 9
9/2- 33 fs 12    2262.2 20 (E2(+M3)) 0.00033B(E2)(W.u.)=1.6 7, α=0.00033 14, α(K)=3.9E-5 16, α(L)=3.6E-6 15, α(M)=4.7E-7 20, α(N)=2.4E-8 10, α(N+)=0.00029 16
9/2- 33 fs 12    2353.2 7 M1+E2-0.54 234.44×10-4B(E2)(W.u.)=2.9 22, B(M1)(W.u.)=0.022 10, α=4.44E-4 14, α(K)=2.08E-5 4, α(L)=1.88E-6 3, α(M)=2.47E-7 4, α(N)=1.294E-8 21, α(N+)=0.000421 14
   2388.0 5/2+ 57 fs 20     393.6 15 (M1(+E2))-0.0 40.00076B(M1)(W.u.)=0.62 23, α=0.00076 20, α(K)=0.00069 18, α(L)=6.3×10-5 17, α(M)=8.3E-6 22, α(N)=4.3E-7 11, α(N+)=4.3E-7 11
5/2+ 57 fs 20    1639.3 6 M1+E2-0.36 151.57×10-4B(E2)(W.u.)=5 5, B(M1)(W.u.)=0.045 17, α=1.57E-4 5, α(K)=3.86E-5 7, α(L)=3.49E-6 6, α(M)=4.58E-7 8, α(N)=2.40E-8 5, α(N+)=0.000115 4
5/2+ 57 fs 20    2298.6 15 (E1(+M2)) 0.0006B(E1)(W.u.)=0.00012 5, α=0.0006 3, α(K)=2.4E-5 11, α(L)=2.2E-6 10, α(M)=2.9E-7 13, α(N)=1.5E-8 7, α(N+)=0.0005 3
5/2+ 57 fs 20    2388.6 14 (E1(+M2)) 0.0006B(E1)(W.u.)=4.5E-5 17, α=0.0006 4, α(K)=2.3E-5 10, α(L)=2.0E-6 9, α(M)=2.7E-7 12, α(N)=1.4E-8 6, α(N+)=0.0006 4
   2408.3 (7/2-) < 8 fs   2408.4 4 D(+Q)+0.02 15 
   2671.0 (11/2)- < 11 fs   1649.2 3 M1+E2-0.41 61.61×10-4B(E2)(W.u.)>32, B(M1)(W.u.)>0.28, α=1.61E-4 3, α(K)=3.83E-5 6, α(L)=3.47E-6 5, α(M)=4.54E-7 7, α(N)=2.38E-8 4, α(N+)=0.0001193 22
   2727.5 15/2- 0.10 ps 4     464.2 3 M1(+E2) 0.0009B(E2)(W.u.)<1.2×102 5, B(M1)(W.u.)=1.1 5, α=0.0009 4, α(K)=0.0008 4, α(L)=7.E-5 3, α(M)=1.0E-5 4, α(N)=5.0E-7 20, α(N+)=5.0E-7 20
15/2- 0.10 ps 4    1705.5 7 (E2) 0.000218B(E2)(W.u.)=18 8, α=0.000218 4, α(K)=3.91E-5 6, α(L)=3.55E-6 5, α(M)=4.65E-7 7, α(N)=2.43E-8 4, α(N+)=0.0001749 25
   2741.0 11/2+ 0.39 ps +36-17    1138.9 9 (E2) 0.0001040B(E2)(W.u.)=33 +15-33, α=0.0001040 15, α(K)=9.17E-5 13, α(L)=8.34E-6 12, α(M)=1.093E-6 16, α(N)=5.69E-8 8, α(N+)=2.73E-6 7
11/2+ 0.39 ps +36-17    1585.8 9 (E1(+M2)) 0.00024B(E1)(W.u.)=0.00012 +6-12, α=0.00024 12, α(K)=4.9E-5 25, α(L)=4.5E-6 23, α(M)=6.E-7 3, α(N)=3.1E-8 16, α(N+)=0.00018 15
11/2+ 0.39 ps +36-17    1719.0 15 (E1(+M2)) 0.00029B(E1)(W.u.)=6.E-6 +7-6, α=0.00029 17, α(K)=4.2E-5 21, α(L)=3.8E-6 19, α(M)=5.0E-7 25, α(N)=2.6E-8 13, α(N+)=0.00025 19
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
   2808.3 5/2+ 0.32 ps 6    2655.7 20 (E1(+M2)) 0.0007B(E1)(W.u.)=2.5E-5 6, α=0.0007 4, α(K)=1.9E-5 8, α(L)=1.7E-6 7, α(M)=2.2E-7 9, α(N)=1.2E-8 5, α(N+)=0.0007 4
5/2+ 0.32 ps 6    2808.5 20 (E1(+M2)) 0.0008B(E1)(W.u.)=2.4E-5 6, α=0.0008 4, α(K)=1.7E-5 7, α(L)=1.5E-6 6, α(M)=2.0E-7 8, α(N)=1.1E-8 4, α(N+)=0.0008 4
   2810.9 5/2-,7/2- < 12 fs    628.4 10 M1 0.000273B(M1)(W.u.)>1.0, α=0.000273 4, α(K)=0.000247 4, α(L)=2.25×10-5 4, α(M)=2.95E-6 5, α(N)=1.540E-7 23, α(N+)=1.540E-7 23
   2861.5 13/2- 0.10 ps 6     134 1 (M1(+E2)) 0.07B(M1)(W.u.)≥0.26 16 LE 11, α=0.07 6, α(K)=0.06 5, α(L)=0.006 5, α(M)=0.0007 7, α(N)=4.E-5 3, α(N+)=4.E-5 3
13/2- 0.10 ps 6     598.3 7 (M1(+E2)) 0.00043B(M1)(W.u.)=0.22 17, α=0.00043 13, α(K)=0.00039 12, α(L)=3.6×10-5 11, α(M)=4.7E-6 14, α(N)=2.4E-7 7, α(N+)=2.4E-7 7
13/2- 0.10 ps 6    1706 1 E2(+M3)-0.09 172.18×10-4B(E2)(W.u.)=28 18, B(M3)(W.u.)=6.×105 +21-6, α=2.18E-4 5, α(K)=4.0E-5 4, α(L)=3.6E-6 4, α(M)=4.7E-7 5, α(N)=2.46E-8 24, α(N+)=0.000174 9
   3134.0 7/2,9/2(+) < 33.3 ps   3133.4 10 D+Q+0.26 12 
   3742.4 (19/2-)      416.9 5 D+Q-2.0 4 
   3912 (3/2)-     3761D(+Q)-1.3 20 
   7745.0 3/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
  3658D(+Q)0.00 3 
3/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
  3830D(+Q)+0.01 2 
3/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
  3999D(+Q)-0.01 2 
3/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
  5363(E1(+M2)) 0.0016B(E1)(W.u.)=0.00062, α=0.0016 5, α(K)=6.3E-6 16, α(L)=5.7E-7 14, α(M)=7.4E-8 19, α(N)=3.9E-9 10, α(N+)=0.0016 5
3/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
  6104D+Q+0.038 25 
3/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
  6995(E1(+M2)) B(E1)(W.u.)=0.00028
3/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
  7592(M1+E2)-0.023 14B(E2)(W.u.)=0.0004 +5-4, B(M1)(W.u.)=0.017 5
3/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
  7654(M1(+E2))-0.01 2B(E2)(W.u.)=5.E-5 +20-5, B(M1)(W.u.)=0.012 4
3/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
  7745E2+M3-0.02 1B(E2)(W.u.)=0.036 11, B(M3)(W.u.)=1.7 +18-17
   7750 3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  3664D(+Q)+0.01 3 
3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  3746(M1(+E2))-0.01 20.000967B(E2)(W.u.)=0.0011 +44-11, B(M1)(W.u.)=0.064 19, α=0.000967 14, α(K)=9.96E-6 14, α(L)=9.00E-7 13, α(M)=1.179E-7 17, α(N)=6.19E-9 9, α(N+)=0.000956 14
3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  3836(M1(+E2))-0.01 20.001000B(E2)(W.u.)=0.0007 +28-7, B(M1)(W.u.)=0.041 12, α=0.001000 14, α(K)=9.62E-6 14, α(L)=8.69E-7 13, α(M)=1.139E-7 16, α(N)=5.98E-9 9, α(N+)=0.000990 14
3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  4005(M1(+E2))+0.01 20.001060B(E2)(W.u.)=0.0007 +29-7, B(M1)(W.u.)=0.047 14, α=0.001060 15, α(K)=9.03E-6 13, α(L)=8.16E-7 12, α(M)=1.069E-7 15, α(N)=5.61E-9 8, α(N+)=0.001050 15
3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  5448(M1+E2)-0.09 60.001480B(E2)(W.u.)=0.007 +10-7, B(M1)(W.u.)=0.010 3, α=0.001480 21, α(K)=5.85E-6 9, α(L)=5.28E-7 8, α(M)=6.92E-8 10, α(N)=3.64E-9 5, α(N+)=0.001473 21
3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  6111(E1(+M2))+0.02 3B(E1)(W.u.)=0.00037 11, B(M2)(W.u.)=0.018 +55-18
3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  6611(E1) B(E1)(W.u.)=2.6E-5 8
3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  7001(E1(+M2))+0.07 25B(E1)(W.u.)=2.2E-5 7, B(M2)(W.u.)=0.010 +72-10
3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  7660(M1+E2)+0.03 2B(E2)(W.u.)=0.0008 +12-8, B(M1)(W.u.)=0.022 7
3/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
  7752E2(+M3)-0.03 38B(E2)(W.u.)=0.029 9, B(M3)(W.u.)=3 +76-3
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
   8092.6 (1/2-) 53 eV 15 
% IT = 4.8 19
% p = 95.2 19
  3456(E2(+M3)) 0.00074B(E2)(W.u.)=12, α=0.00074 25, α(K)=1.7E-5 6, α(L)=1.5E-6 5, α(M)=2.0E-7 7, α(N)=1.1E-8 4, α(N+)=0.0007 3
(1/2-) 53 eV 15 
% IT = 4.8 19
% p = 95.2 19
  6447(E1) B(E1)(W.u.)=0.00063 18
(1/2-) 53 eV 15 
% IT = 4.8 19
% p = 95.2 19
  7341(E1) B(E1)(W.u.)=7.2E-5 21
(1/2-) 53 eV 15 
% IT = 4.8 19
% p = 95.2 19
  7999(E2+(M3)) B(E2)(W.u.)=0.092
   8117.5 3/2     6978D+Q-0.11 8 
3/2     7370D+Q+0.10 4 
3/2     8027D(+Q)+0.14 15 
3/2     8118Q+O-0.29 15 

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
      0.07/2- 330 d 15 
% ε = 100
μ=4.47 5 (2005St24,1957We17), T=3/2
E(level): 7/2- GS yrast band. From β+ decay.
     90.63925/2- 228 ps 13  E(level): 7/2- GS yrast band. From β+ decay.
    748.273/2+ 5.3 ps 6  T=3/2
E(level): Kπ=3/2+ ROTATIONAL band.
   1021.6211/2- 3.4 ps 6  E(level): 7/2- GS yrast band. From β+ decay.
   1140.535/2+ 1.3 ps 6  E(level): Kπ=3/2+ ROTATIONAL band.
   1155.329/2- 1.1 ps 3  E(level): 7/2- GS yrast band. From β+ decay.
   1602.687/2+ 0.47 ps 22  E(level): Kπ=3/2+ ROTATIONAL band.
   1610(9/2-,11/2-)   Jπ(level): From angular momentum transfer in (t,α).
   1646.43(1/2+) 6.6 ps 10  E(level): Kπ=1/2+ ROTATIONAL BAND?.
   1994.73/2(+) 0.49 ps 21  E(level): Kπ=1/2+ ROTATIONAL BAND?.
   2178.39/2+ 0.56 ps +49-28  E(level): Kπ=3/2+ ROTATIONAL band.
   2182.07/2- 33 fs 12  Jπ(level): From angular momentum transfer in (p,t).
   2263.3015/2- 0.65 ps +38-19  E(level): 7/2- GS yrast band. From β+ decay.
   2388.05/2+ 57 fs 20  E(level): Kπ=1/2+ ROTATIONAL BAND?.
   2671.0(11/2)- < 11 fs E(level): NEGATIVE-PARITY SIDE band.
   2671.37/2-,9/2,11/2+ < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   2727.515/2- 0.10 ps 4  E(level): NEGATIVE-PARITY SIDE band.
   2741.011/2+ 0.39 ps +36-17  E(level): Kπ=3/2+ ROTATIONAL band.
   2810.95/2-,7/2- < 12 fs E(level): NEGATIVE-PARITY SIDE band.
   2861.513/2- 0.10 ps 6  E(level): 7/2- GS yrast band. From β+ decay.
   3017.3 < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3134.07/2,9/2(+) < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3224(1/2,3/2,5/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3239.57/2- < 33.3 ps Jπ(level): From angular momentum transfer in (p,t).
T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3242(3/2,5/2,7/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
E(level)Jπ(level)T1/2(level)Comments
   32481/2+   Jπ(level): From angular momentum transfer in (t,α).
   3259.5(GE 9/2)   T1/2>2 ps,T1/2<0.7 ns.
   3303.23/2-,5/2,7/2,9/2 < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3325(1/2+ TO 7/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   3325.2(17/2-)   E(level): 7/2- GS yrast band. From β+ decay.
   3340.5 < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3341.8(13/2+)   T1/2>3.5 ps, T1/2<0.7 ns.
E(level): Kπ=3/2+ ROTATIONAL band.
   3342(1/2+ TO 9/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3388(3/2,5/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3388.55/2,7/2 < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3405(3/2)-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3462.9(3/2+ TO 9/2+) < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3479(7/2-)   Jπ(level): From angular momentum transfer in (p,t).
   3500.6 < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3516(3/2- TO 9/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   3521(LE 9/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   3531(LE 7/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   3531.15/2-,7/2,9/2+ < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3603   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3609(7/2-)   Jπ(level): From angular momentum transfer in (p,t).
   3623.9LE 9/2 < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3639.8(7/2-) < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3665.911/2 < 33.3 ps T1/2(level): From γ(t) in (p,nγ). Upper limit on the mean lives for these transitions was approximately 10 to 48 ps.
   3671(1/2+ TO 9/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3678(7/2)-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
E(level)Jπ(level)T1/2(level)Comments
   36943/2+,5/2+   E(level): From (p,α).
Jπ(level): From angular momentum transfer in (t,α).
   3721(LE 7/2)-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   37411/2-,3/2-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3742.4(19/2-)   E(level): 7/2- GS yrast band. From β+ decay.
   37575/2-,7/2-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3771(1/2+ TO 9/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   3782(GE 9/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3795(-)   Jπ(level): From angular momentum transfer in (p,t).
   3816(LE 7/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3825(-)   Jπ(level): From angular momentum transfer in (p,t).
   38411/2(+),3/2,5/2-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   3912(3/2)-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): L(3He,d)=1; 3/2 from deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   3927(1/2+ TO 9/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   3960(3/2-,5/2,7/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   3975(-)   Jπ(level): From angular momentum transfer in (p,t).
   4002(3/2)-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): L(3He,d)=1; 3/2 from deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   4035(3/2- TO 9/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   40883/2(-),5/2,7/2-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   4098(LE 7/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   4129(5/2)-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   4152   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   4218(3/2)-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): L(3He,d)=1; 3/2 from deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   42531/2-,3/2-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   4259(3/2,5/2,7/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From deexcitation of resonances assuming d,E2 for strong transitions and multidimensional nonmetric scaling analysis.
   4270   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
E(level)Jπ(level)T1/2(level)Comments
   42893/2+,5/2+   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From angular momentum transfer in (t,α).
   4359   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   43731/2-,3/2-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   43975/2-,7/2-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From angular momentum transfer in (t,α).
   4422   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   4436   E(level): From (p,α).
   44985/2(-),7/2(-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   45021/2-,3/2-   E(level): From (3He,d).
   4540   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   4590   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   4635(5/2)-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   46623/2+,5/2+   E(level): From (p,α).
Jπ(level): From angular momentum transfer in (t,α).
   47403/2+,5/2+   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): From angular momentum transfer in (t,α).
   48401/2-,3/2-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   4863   E(level): From (p,α).
   4885   E(level): From (p,α).
   49471/2-,3/2-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   49591/2+   Jπ(level): From angular momentum transfer in (t,α).
   50105/2-,7/2-   E(level): From (p,α).
Jπ(level): From angular momentum transfer in (t,α).
   5042   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   50723/2+,5/2+   Jπ(level): From angular momentum transfer in (t,α).
   5134   E(level): From (p,α).
   52121/2-,3/2-   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   5230   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   52921/2+   E(level): From (p,α).
Jπ(level): From angular momentum transfer in (t,α).
E(level)Jπ(level)T1/2(level)Comments
   5347(3/2+,5/2+)   E(level): From (p,α).
Jπ(level): From angular momentum transfer in (t,α).
   53871/2-,3/2-   E(level): From (p,α).
Jπ(level): From angular momentum transfer in (t,α).
   54115/2-,7/2-   E(level): From (p,α).
   55221/2+   Jπ(level): From angular momentum transfer in (t,α).
   5529.7(21/2-)   E(level): 7/2- GS yrast band. From β+ decay.
Jπ(level): From stretched (ΔJ=1) dipole or stretched (ΔJ=2) quadrupole cascade and membership in 7/2- g.s. yrast band.
   55971/2-,3/2-   E(level): From (3He,d).
   5631(3/2+,5/2+)   Jπ(level): From angular momentum transfer in (t,α).
   5689.9(23/2-)   E(level): 7/2- GS yrast band. From β+ decay.
Jπ(level): From stretched (ΔJ=1) dipole or stretched (ΔJ=2) quadrupole cascade and membership in 7/2- g.s. yrast band.
   58891/2-,3/2-   E(level): From (3He,d).
   5931(3/2+,5/2+)   Jπ(level): From angular momentum transfer in (t,α).
   59871/2-,3/2-   E(level): From (3He,d).
   6058(3/2+,5/2+)   Jπ(level): From angular momentum transfer in (t,α).
   6184   E(level): From (3He,d).
   62201/2-,3/2-   E(level): From (3He,d).
   63331/2-,3/2-   E(level): From (3He,d).
   6368   E(level): From (3He,d).
   6430   E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
Jπ(level): Jp=7/2-, t=5/2, IAS(49Ti g.s.) for 6446 25 in (p,|A).
   6474   E(level): From (3He,d). t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
Jπ(level): Jp=7/2-, t=5/2, IAS(49Ti g.s.) for 6446 25 in (p,|A).
   6521   E(level): From (3He,d).
   6563(3/2+,5/2+)   Jπ(level): From angular momentum transfer in (t,α).
   6844.9(23/2-)   E(level): NEGATIVE-PARITY SIDE band.
   7745.03/2- 8.9 eV 30 
% IT = 10 4
% p = 90 4
T=5/2, Γγ=0.88 25, Γp=8 3
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
   77503/2- 6.7 eV 20 
% IT = 10 4
% p = 90 4
T=5/2, Γγ=0.70 20, Γp=6 2
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
   7801.4(25/2-)   E(level): 7/2- GS yrast band. From β+ decay.
Jπ(level): From stretched (ΔJ=1) dipole or stretched (ΔJ=2) quadrupole cascade and membership in 7/2- g.s. yrast band.
   7838.7(1/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 1/2-,3/2,5/2 from γ’s to 3/2-, 3/2+, and 5/2- assuming d,E2; 1/2,3/2 from multidimensional nonmetric scaling analysis.
E(level)Jπ(level)T1/2(level)Comments
   7910.2(1/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 1/2-,3/2,5/2 from γ’s to 3/2-, 3/2+, and 5/2- assuming d,E2; 1/2,3/2 from multidimensional nonmetric scaling analysis.
   7943.5(3/2-)   T=5/2
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis.
   8013.0(3/2-)   T=5/2
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis.
   8058.1(3/2,5/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   8071.8(5/2)   T=5/2
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. From (p,γ) E=960-2488 keV res.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   8092.6(1/2-) 53 eV 15 
% IT = 4.8 19
% p = 95.2 19
T=5/2, Γγ=2.5 7, Γp=50 15
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
   8104.23/2(-),5/2   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   8117.53/2   Γγ=0.33 9
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   8131.5(3/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis.
   8290.33/2(-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   8416.1(27/2-)   E(level): 7/2- GS yrast band. From β+ decay.
Jπ(level): From stretched (ΔJ=1) dipole or stretched (ΔJ=2) quadrupole cascade and membership in 7/2- g.s. yrast band.
   8525.3(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   8628.2(3/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis.
   8633.1(5/2)   T=5/2
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   8640.9(3/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis.
   8642.9(3/2-,5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   8682.0(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (p,γ) E=960-2488 keV res.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   8784.9(5/2)   T=5/2
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. From (p,γ) E=960-2488 keV res.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   8788.8(5/2-)   T=5/2
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
   8851.5(5/2-,7/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   8867.2(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   8877.0(5/2)   T=5/2
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. From (p,γ) E=960-2488 keV res.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   8880.9(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   8890.7(3/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis.
   8893.6(5/2-)   T=5/2
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
E(level)Jπ(level)T1/2(level)Comments
   8895.6(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   8902.5(5/2)   T=(5/2)
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. From (p,γ) E=960-2488 keV res.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. Jp=5/2-, t=5/2 from IAS identification in (3He,pd).
   8912.2(5/2)   T=(5/2)
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents. From (p,γ) E=960-2488 keV res.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. Jp=5/2-, t=5/2 from IAS identification in (3He,pd).
   8921.1(5/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (α,pγ).
Jπ(level): 5/2+ from γ’s to 3/2-, 3/2+, and 9/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   8925.0(7/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   8927.9(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis. Jp=5/2-, t=5/2 from IAS identification in (3He,pd).
   8942.6(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   8945(1/2+)   T=(5/2)
E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
   8965.1(5/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (α,pγ).
Jπ(level): 5/2+ from γ’s to 3/2-, 3/2+, and 9/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   8998.5(1/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   9008.2(5/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9029.8(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9037.6(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (p,γ) E=960-2488 keV res.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9044.5(7/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   9056.2(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (p,γ) E=960-2488 keV res.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9071.9(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9075.8(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9078.8(3/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 3/2 from multidimensional nonmetric scaling analysis.
   9082.7(3/2+)   T=(5/2)
E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
   9089.5(3/2-,5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   9094.4(5/2)   E(level): From (p,γ) E=960-2488 keV res.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9118.0(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9131.7(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9135.6(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (p,γ) E=960-2488 keV res.
Jπ(level): 3/2-,5/2 from γ’s to 3/2-, 3/2+, and 7/2- assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9148.3(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
E(level)Jπ(level)T1/2(level)Comments
   9154.2(5/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (α,pγ).
Jπ(level): 5/2+ from γ’s to 3/2-, 3/2+, and 9/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9161.1(1/2-,3/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 1/2-,3/2,5/2 from γ’s to 3/2-, 3/2+, and 5/2- assuming d,E2; 1/2,3/2 from multidimensional nonmetric scaling analysis.
   9167.9(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9168.9(3/2-)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   9174.8(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9182.6(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   9193.4(5/2,7/2+)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
   9195.3(5/2)   E(level): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies.
Jπ(level): 5/2 from γ’s to 3/2-, 3/2+, 7/2-, and 7/2+ assuming d,E2; 5/2 from multidimensional nonmetric scaling analysis.
   9568(1/2-)   T=(5/2)
E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
   96623/2-   T=5/2
E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
  10230(5/2)-   T=5/2
E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
  10925(5/2)+   T=5/2
E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.
  11150(9/2+)   T=5/2
E(level): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents.

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Additional Gamma Comments:

E(level)E(gamma)Comments
     90.6392     90.639E(γ): From β+ decay
M(γ): from α(exp) in (p,nγ) and comparison to RUL. Δπ=1 d γ from recoil-γ(θ) in (40C,3pγ)
    152.9282     62.289E(γ): From β+ decay
I(γ): weighted av of Iγ(62γ)/Iγ(153γ)=72.4 35/100.0 52 from (α,pγ) and 68.9 32/100.0 32 from (p,nγ). Iγ(62γ)/Iγ(153γ)=54.0 7/100.0 4 from B=decay and 100/92 from (p,γ) discrepant
M(γ): d from comparison to RUL. Δπ=no from the level scheme
    152.928E(γ): From β+ decay
I(γ): From β+ decay
M(γ): from α(exp) in (p,nγ) and comparison to RUL
    748.27    595.35M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=yes from level scheme
    657.60M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=yes from level scheme
   1021.62   1021.63M(γ): Q(+O) from pγ(θ) in (α,pγ). Ne M2(+E3) from comparison to RUL. ΔJ=2 Q or ΔJ=0 d γ from recoil-γ(θ) in (40Ca,3pγ)
   1140.53    392.7E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies
M(γ): D+Q from pγ(θ) in (α,pγ). E1+M2 excluded by δ and comparison to RUL
    987.61M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=yes from level scheme
   1049.79M(γ): from α(exp) and γ(θ) in (p,nγ)
   1140.7E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies
M(γ): from α(exp) in (p,nγ) and pγ(θ) in (α,pγ)
   1155.32    133.80E(γ): From (p,α)
M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme
   1064.63M(γ): Q from pγ(θ) in (α,pγ). Ne M2 from comparison to RUL
   1155.33M(γ): ΔJ=1 d γ from recoil-γ(θ) in (40Ca,3pγ). D+Q from pγ(θ) in (α,pγ). E1+M2 excluded by δ and comparison to RUL
   1514.54    766M(γ): d from comparison to RUL. Δπ=yes from level scheme
   1361.61E(γ): From β+ decay
M(γ): D+Q from pγ(θ) in (α,pγ). E1+M2 excluded by δ and comparison to RUL
   1423.6E(γ): From (p,α). t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents
M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme
   1514.4E(γ): From (3He,d). t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents
M(γ): From comparison to RUL
   1602.68    447.4I(γ): Results from (40Ca,3pγ), (α,pγ), and other (p,nγ) measurements are discrepant. This may Be due, in part, to the bombarding energies and the higher-lying states excited. Note, for example, the 463γ.
M(γ): d,E2 from α(exp) in (p,nγ). Δπ=yes from level scheme
    462.2I(γ): Results from (40Ca,3pγ), (α,pγ), and other (p,nγ) measurements are discrepant. This may Be due, in part, to the bombarding energies and the higher-lying states excited. Note, for example, the 463γ.
M(γ): d(+Q) from pγ(θ) in (α,pγ). Ne E1+M2 from α(exp) in (p,nγ)
    854.5E(γ): Multiply placed with intensity suitably divided
I(γ): Multiply placed with intensity suitably divided. Results from (40Ca,3pγ), (α,pγ), and other (p,nγ) measurements are discrepant. This may Be due, in part, to the bombarding energies and the higher-lying states excited. Note, for example, the 463γ.
M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme
   1512.0I(γ): Results from (40Ca,3pγ), (α,pγ), and other (p,nγ) measurements are discrepant. This may Be due, in part, to the bombarding energies and the higher-lying states excited. Note, for example, the 463γ.
M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   1602.6I(γ): Results from (40Ca,3pγ), (α,pγ), and other (p,nγ) measurements are discrepant. This may Be due, in part, to the bombarding energies and the higher-lying states excited. Note, for example, the 463γ.
M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=yes from level scheme
   1643.19   1490.24I(γ): From (p,γ) E=960-2488 keV res
M(γ): from pγ(θ) in (α,pγ)
   1553E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   1646.43    898.06I(γ): Unweighted average of Iγ(898γ)/Iγ(1493γ)=53% 3/47% 2 from (α,pγ) and 40% 4/60% 5 from (p,nγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=21% 1:79% 4:<5% from (α,pγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=25% 1:66% 1:9% 1 from (p,nγ)
   1493.6E(γ): From (α,pγ)
I(γ): Unweighted average of Iγ(898γ)/Iγ(1493γ)=53% 3/47% 2 from (α,pγ) and 40% 4/60% 5 from (p,nγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=21% 1:79% 4:<5% from (α,pγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=25% 1:66% 1:9% 1 from (p,nγ)
M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
E(level)E(gamma)Comments
   1661.40    912.3M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   1508.37E(γ): From (3He,d)
M(γ): From comparison to RUL
   1570.83E(γ): From (p,α)
M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme
   1661.4M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme
   1994.7    854.5E(γ): Multiply placed with intensity suitably divided. From (p,α)
I(γ): Multiply placed with intensity suitably divided
M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme
   1246.8E(γ): Multiply placed with intensity suitably divided. From (3He,d)
I(γ): Multiply placed with intensity suitably divided
M(γ): From comparison to RUL
   1841.0M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=yes from level scheme
   1903.4M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   2178.3    575.4I(γ): From (α,pγ)
   1023E(γ): From (3He,d). From (40Ca,3pγ)
I(γ): from Iγ(1023γ)/Iγ(1157γ)=5/11 and Iγ(1023γ)/Iγ(2178γ)=5/2 in (40Ca,3pγ)
M(γ): From comparison to RUL
   1037.4I(γ): From (α,pγ)
M(γ): from pγ(θ) in (α,pγ) and α(exp) in (p,nγ)
   1157.0I(γ): From (α,pγ)
M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ)
   2178.3I(γ): From (α,pγ)
   2182.0   1026.8I(γ): Unweighted average of Iγ(898γ)/Iγ(1493γ)=53% 3/47% 2 from (α,pγ) and 40% 4/60% 5 from (p,nγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=21% 1:79% 4:<5% from (α,pγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=25% 1:66% 1:9% 1 from (p,nγ)
M(γ): d,E2 from comparison to RUL. Δπ=no from level scheme. d,E2 from comparison to RUL. Δπ=yes from level scheme
   2090.7E(γ): From (p,α). t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents
I(γ): Unweighted average of Iγ(898γ)/Iγ(1493γ)=53% 3/47% 2 from (α,pγ) and 40% 4/60% 5 from (p,nγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=21% 1:79% 4:<5% from (α,pγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=25% 1:66% 1:9% 1 from (p,nγ)
M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme
   2181.6E(γ): From (3He,d)
I(γ): Unweighted average of Iγ(898γ)/Iγ(1493γ)=53% 3/47% 2 from (α,pγ) and 40% 4/60% 5 from (p,nγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=21% 1:79% 4:<5% from (α,pγ) and Iγ(1027γ):Iγ(2089γ):Iγ(2187γ)=25% 1:66% 1:9% 1 from (p,nγ)
M(γ): From comparison to RUL
   2234.0    572.5E(γ): From (3He,d). t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents
I(γ): Note that Iγ(572γ) from (p,nγ) may have an unresolved component from 2178 state and that Iγ(2233γ) from (α,pγ) may have an unresolved component from the 3388 state discrepant.
M(γ): From comparison to RUL
   2142.9E(γ): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents
   2234.4E(γ): t=5/2 isobaric analog resonances. See (p,γ),(3He,pd), (p,α), below, for correspondence with 49Ti parents
I(γ): Note that Iγ(572γ) from (p,nγ) may have an unresolved component from 2178 state and that Iγ(2233γ) from (α,pγ) may have an unresolved component from the 3388 state discrepant.
   2263.30   1241.69M(γ): from α(exp) in (p,nγ) and comparison to RUL. ΔJ=2 Q or ΔJ=0 d from recoil-γ(θ) in (40Ca,3pγ)
   2265.3    621E(γ): From (3He,d). From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
M(γ): From comparison to RUL
   2112.3E(γ): From (α,pγ)
I(γ): From (p,γ) E=960-2488 keV res
   2309.4   1560E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   2310.6M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme
   2353.4   1198.9E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (3He,d)
M(γ): From comparison to RUL
   1331.7E(γ): From (p,α)
M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme
   2262.2M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme
   2353.2E(γ): From (α,pγ)
M(γ): D+Q from pγ(θ) in (α,pγ). E1+M2 excluded by δ and comparison to RUL
E(level)E(gamma)Comments
   2388.0    393.6E(γ): From (p,α). From (α,pγ)
I(γ): From (α,pγ)
M(γ): D+Q or d(+Q) from pγ(θ) in (α,pγ). Δπ=no from level scheme
   1247.8E(γ): Multiply placed with intensity suitably divided. From (3He,d). From (α,pγ)
I(γ): Multiply placed with intensity suitably divided. From (α,pγ)
M(γ): From comparison to RUL
   1639.3I(γ): From (α,pγ)
M(γ): D+Q from pγ(θ) in (α,pγ). E1+M2 excluded by δ and comparison to RUL
   2235.5I(γ): From (α,pγ)
   2298.6I(γ): From (α,pγ)
M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   2388.6I(γ): From (α,pγ)
M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   2408.3    229.2E(γ): From (α,pγ)
I(γ): From (α,pγ)
   1252.9E(γ): From (3He,d)
M(γ): From comparison to RUL
   1268E(γ): From (3He,d). From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
M(γ): From comparison to RUL
   1385.7E(γ): From (3He,d)
M(γ): From comparison to RUL
   2408.4E(γ): From (α,pγ)
   2671.0   1517E(γ): From (3He,d). From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): From comparison to RUL
   1649.2E(γ): From (α,pγ)
I(γ): From (40Ca,3pγ)
M(γ): D+Q from pγ(θ) in (α,pγ). δ(9/2,11/2,13/2) and comparison to RUL exclude E1+M2
   2671.3   1649.3E(γ): From (3He,d)
M(γ): From comparison to RUL
   2579.2E(γ): From (3He,d)
M(γ): From comparison to RUL
   2727.5    464.2E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies
I(γ): From (40Ca,3pγ)
M(γ): d(+Q) from pγ(θ) in (α,pγ). Ne E1 from comparison to RUL. ΔJ=2 Q or ΔJ=0 d γ from recoil-γ(θ) in (40Ca,3pγ)
   1705.5I(γ): From (40Ca,3pγ)
M(γ): d,E2 from comparison to RUL. ΔJ=2 Q or ΔJ=0 d from recoil-γ(θ) in (40Ca,3pγ). ΔJπ=2,no from level scheme
   2741.0    562.5E(γ): From (3He,d)
I(γ): From (α,pγ)
M(γ): From comparison to RUL
   1138.9E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies
I(γ): From (α,pγ)
M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme
   1585.8I(γ): From (α,pγ)
M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   1719.0E(γ): From (α,pγ)
I(γ): From (α,pγ)
M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   2786.4   1184.3E(γ): From (3He,d)
M(γ): From comparison to RUL
   1764.5M(γ): D+Q,Q from pγ(θ) in (α,pγ). Ne M2 from comparison to RUL
   2697.2E(γ): From (3He,d)
M(γ): From comparison to RUL
   2786.4E(γ): From (α,pγ)
M(γ): D+Q,Q from pγ(θ) in (α,pγ). δ(9/2) and comparison to RUL exclude E1+M2; Ne M2 from comparison to RUL
E(level)E(gamma)Comments
   2808.3   1206.6E(γ): From (3He,d)
M(γ): From comparison to RUL
   1666.7E(γ): From (3He,d)
M(γ): From comparison to RUL
   2058E(γ): From (3He,d). From (α,pγ)
I(γ): From (α,pγ)
M(γ): From comparison to RUL
   2655.7M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   2808.5M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   2810.9    628.4E(γ): From (3He,d)
M(γ): From comparison to RUL
   1673E(γ): From (3He,d)
M(γ): From comparison to RUL
   2720.3E(γ): From (3He,d). From (α,pγ)
M(γ): From comparison to RUL
   2810.9E(γ): From (3He,d). From (α,pγ)
M(γ): From comparison to RUL
   2861.5    134E(γ): From (40Ca,3pγ)
I(γ): from Iγ(134γ)/Iγ(599γ)=0.0125 and Iγ(134γ)/Iγ(1707γ)=0.025 in (40Ca,3pγ)
M(γ): d from comparison to RUL. Δπ=no from the level scheme
    598.3E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies
M(γ): ΔJ=1 d transition from recoil-γ(θ) in (40Ca,3pγ). Δπ=no from level scheme
   1706E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies
M(γ): Q+O from pγ(θ) in (α,pγ). Ne M2+E3 from comparison to RUL. ΔJ=2 Q or ΔJ=0 d from recoil-γ(θ) in (40Ca,3pγ)
   1840E(γ): From (3He,d). From (40Ca,3pγ)
I(γ): from Iγ(1840γ)/Iγ(599γ)=1.4 and Iγ(1840γ)/Iγ(1707γ)=10 in (40Ca,3pγ)
M(γ): From comparison to RUL
   3017.3   1414.1E(γ): From (3He,d)
M(γ): From comparison to RUL
   3133.9    462.9E(γ): From (3He,d). From (α,pγ)
I(γ): From (α,pγ)
M(γ): From comparison to RUL
   3134.0   1979.5E(γ): From (p,γ). Excluded from the least-squares adjustment since the connecting transitions have no uncertainties on Eγ or were obtained from the adopted excitation energies. From (3He,d)
M(γ): From comparison to RUL
   2112.8E(γ): From (3He,d)
M(γ): From comparison to RUL
   2385.7E(γ): From (3He,d)
M(γ): From comparison to RUL
   3224   1566E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3074E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3239.5   1725.2E(γ): From (3He,d)
M(γ): From comparison to RUL
   3238.2E(γ): From (3He,d)
M(γ): From comparison to RUL
   3259.5    473.1E(γ): From (α,pγ)
I(γ): From (α,pγ)
   3303.2   1121.0E(γ): From (3He,d)
M(γ): From comparison to RUL
   3213.5E(γ): From (3He,d)
M(γ): From comparison to RUL
E(level)E(gamma)Comments
   3325.2    464E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): Stretched (ΔJ=2) quadrupole or ΔJ=0 dipole transition from recoil-γ(θ) in (40Ca,3pγ)
    597.1E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ)
   1061.9E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ)
   3341.8    601.0E(γ): From (3He,d). From (α,pγ)
I(γ): From (α,pγ)
M(γ): From comparison to RUL
    670.5E(γ): From (3He,d). From (α,pγ)
I(γ): From (α,pγ)
M(γ): From comparison to RUL
   1163.0E(γ): From (3He,d). From (α,pγ)
I(γ): From (α,pγ)
M(γ): From comparison to RUL
   3388   1729E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   1876E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3531   1870E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   1887E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3378E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3531.1   1178.4E(γ): From (3He,d)
M(γ): From comparison to RUL
   1348.4E(γ): From (3He,d)
M(γ): From comparison to RUL
   2015.6E(γ): From (3He,d)
M(γ): From comparison to RUL
   3378.5E(γ): From (3He,d)
M(γ): From comparison to RUL
   3623.9   2483.3E(γ): From (3He,d)
M(γ): From comparison to RUL
   3639.8   1461.5E(γ): From (3He,d)
M(γ): From comparison to RUL
   2123.8E(γ): From (3He,d)
M(γ): From comparison to RUL
   2618.1E(γ): From (3He,d)
M(γ): From comparison to RUL
   3665.9   1312.1E(γ): From (3He,d)
M(γ): From comparison to RUL
   1402.7E(γ): From (3He,d)
M(γ): From comparison to RUL
   3666.7E(γ): From (3He,d)
M(γ): From comparison to RUL
   3741   2230E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3591E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3653E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
E(level)E(gamma)Comments
   3742.4    416.9E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
   1479.1E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): Stretched (ΔJ=2) quadrupole or ΔJ=0 dipole transition from recoil-γ(θ) in (40Ca,3pγ)
   3816   3725E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3841   2180E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   2197E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3912   1650E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   2270E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3761E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4002   1693E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   2358E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4088   1855E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   2576E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   3937E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4090E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4129   3380E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4253   2589E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   2606E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4373   2064E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   2138E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   2712E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4498   3343E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4345E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4590   2355E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4635   4548E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   4639E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
E(level)E(gamma)Comments
   4947   4853E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   5212   2903E(γ): From (p,γ) E=960-2488 keV res
I(γ): From (p,γ) E=960-2488 keV res
   5529.7   1787E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): from recoil-γ(θ) in (40Ca,3pγ)
   2204E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
   5689.9    160E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
   1947E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): Stretched (ΔJ=2) quadrupole or ΔJ=0 dipole transition from recoil-γ(θ) in (40Ca,3pγ)
   6844.9   1155E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ)
   1315E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
   3102E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
   7745.0   3111E(γ): From (3He,d)
M(γ): From comparison to RUL
   3249E(γ): From (3He,d)
M(γ): From comparison to RUL
   3620E(γ): From (3He,d)
M(γ): From comparison to RUL
   3741E(γ): From (3He,d)
M(γ): From comparison to RUL
   3931E(γ): From (3He,d)
M(γ): From comparison to RUL
   4355E(γ): From (3He,d)
M(γ): From comparison to RUL
   5363M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   5486E(γ): From (3He,d)
M(γ): From comparison to RUL
   6995E(γ): From (3He,d)
M(γ): From comparison to RUL. d,E2 from comparison to RUL. Δπ=yes from level scheme
   7592M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme
   7654M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme
   7745M(γ): Q+O from γ(θ) in (p,γ). Ne M2+E3 from comparison to RUL
   7750   3116E(γ): From (3He,d)
M(γ): From comparison to RUL
   3627E(γ): From (3He,d)
M(γ): From comparison to RUL
   3746M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme
   3836M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme
   3993E(γ): From (3He,d)
M(γ): From comparison to RUL
   4005M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme
   4343E(γ): From (3He,d)
M(γ): From comparison to RUL
   4360E(γ): From (3He,d)
M(γ): From comparison to RUL
   5448M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme
   5491E(γ): From (3He,d)
M(γ): From comparison to RUL
   6111M(γ): d(+Q) from γ(θ) in (p,γ). Δπ=yes from level scheme
   6611M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   7001M(γ): d(+Q) from γ(θ) in (p,γ). Δπ=yes from level scheme
   7660M(γ): D+Q or d(+Q) from γ(θ) in (p,γ). Δπ=no from level scheme
   7752M(γ): Q(+O) from γ(θ) in (p,γ). Ne M2 from comparison to RUL
E(level)E(gamma)Comments
   7801.4    956E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ)
   2111E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ)
   2271E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
   8092.6   3456M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme
   3718E(γ): From (3He,d)
M(γ): From comparison to RUL
   4089E(γ): From (3He,d)
M(γ): From comparison to RUL
   4179E(γ): From (3He,d)
M(γ): From comparison to RUL
   4249E(γ): From (3He,d)
M(γ): From comparison to RUL
   4349E(γ): From (3He,d)
M(γ): From comparison to RUL
   4851E(γ): From (3He,d)
M(γ): From comparison to RUL
   4866E(γ): From (3He,d)
M(γ): From comparison to RUL
   6429E(γ): From (3He,d)
M(γ): From comparison to RUL
   6447M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   7341M(γ): d,E2 from comparison to RUL. Δπ=yes from level scheme
   7936M(γ): from comparison to RUL. γ(θ) isotropic in (p,γ)
   7999M(γ): d,E2 from comparison to RUL. ΔJ=2 from level scheme
   8117.5   3743E(γ): From (3He,d)
M(γ): From comparison to RUL
   4114E(γ): From (3He,d)
M(γ): From comparison to RUL
   4728E(γ): From (3He,d)
M(γ): From comparison to RUL
   4892E(γ): From (3He,d)
M(γ): From comparison to RUL
   5730E(γ): From (3He,d)
M(γ): From comparison to RUL
   5808E(γ): From (3He,d)
M(γ): From comparison to RUL
   5853E(γ): From (3He,d)
M(γ): From comparison to RUL
   5884E(γ): From (3He,d)
M(γ): From comparison to RUL
   6601E(γ): From (3He,d)
M(γ): From comparison to RUL
E(level)E(gamma)Comments
   8416.1    613E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): Stretched (ΔJ=1) dipole transition from recoil-γ(θ) in (40Ca,3pγ)
   5690E(γ): From (40Ca,3pγ)
I(γ): From (40Ca,3pγ)
M(γ): Stretched (ΔJ=2) quadrupole or ΔJ=0 dipole transition from recoil-γ(θ) in (40Ca,3pγ)
   9044.5   6373E(γ): Multiply placed with undivided intensity
I(γ): Multiply placed with undivided intensity
   6373E(γ): Multiply placed with undivided intensity
I(γ): Multiply placed with undivided intensity

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