ADOPTED LEVELS, GAMMAS for 140Ce

Author: N. Nica |  Citation: Nucl. Data Sheets 154, 1 (2018) |  Cutoff date: 20-Nov-2018 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-3388 keV 6S(n)= 9200 keV 7S(p)= 8138.8 keV 17Q(α)= -1614.1 keV 16
Reference: 2017WA10

References:
  A  140La β- decay  B  140Pr ε decay
  C  144Nd α decay  D  138Ba(3He,n)
  E  138Ba(α,2nγ)  F  138Ce(t,p)
  G  139La(3He,d)  H  140Ce(γ,γ’)
  I  140Ce(E,E’)  J  140Ce(n,n’γ)
  K  140Ce(p,p’)  L  140Ce(α,α’)
  M  140Ce(α,α’γ)  N  140Ce(17O,17O’γ)
  O  141Pr(d,3He)  P  142Ce(p,t)
  Q  142Nd(14C,16O)  R  143Nd(n,α),(n,αγ)
  S  144Nd(d,6Li)  T  238U(12C,Fγ)
  U  Coulomb Excitation 

General Comments:

Measured nuclear charge radii and isotopes shifts: 2000Ga58, 1999GaZU, 1999Is02, 1997Is06, 1997IsZY.










E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
     0.0ABCDEFGHIJKLMNOPQRSTU 0+ STABLE      
  1596.233 23 AB DEFGHIJKL NOPQRSTU 2+ 0.0910 ps +48-44    1596.210 35 
  100
E2
     0.0
0+
  1903.31 6 AB  EF   JK  NOP R    0+ 0.40 ns 3     306.9 2 
  1903.5
  100
 
E2
E0
  1596.233
     0.0
2+
0+
  2083.259 24 A   E G IJKL  OPQR T  4+ 3.45 ns 3     487.021 12 
  2083.2 5 
  100.0 13 
    0.03 2 
E2
E4
  1596.233
     0.0
2+
0+
  2107.854 24 A   E   IJ    OP   T  6+ 7.3 µs 15      24.595 4 
  100
E2
  2083.259
4+
  2347.881 24 AB  E   IJ L  O  R    2+ ≤ 0.2 ns    445.5 5 
   751.637 18 
  2347.88 5 
    0.07 2 
  100 1 
   19.6 7 
[E2]
M1+E2
E2
  1903.31
  1596.233
     0.0
0+
2+
0+
  2349.805 25 A   E   IJ L  O  R    5+ ≤ 12 ps    241.933 30 
   266.543 12 
   88.9 17 
  100.0 16 
M1+E2
M1+E2
  2107.854
  2083.259
6+
4+
  2412.013 24 A   E G  J    O  R    3+ 1.3 ps 4      64.135 10 
   328.762 8 
   815.772 19 
    0.06 1 
   87.3 17 
  100.0 9 
M1
M1+E2
M1(+E2)
  2347.881
  2083.259
  1596.233
2+
4+
2+
  2464.08 3 A   EFG IJKL N PQR  U 3- 0.15 ps 3     867.846 20 
  2464.1 5 
  100 1 
    0.21 3 
E1
[E3]
  1596.233
     0.0
2+
0+
  2480.925 24 A   E    J            4+ 22 ps 7      68.916 6 
   131.117 8 
   397.52 5 
   16.1 5 
  100 2 
   15.7 10 
M1
M1+E2
(E2)
  2412.013
  2349.805
  2083.259
3+
5+
4+
  2515.76 3 A   E G  J    OP R    4+ ≤ 2.5 ps    432.493 12 
   919.550 23 
  100 1 
   92 1 
M1+E2
E2
  2083.259
  1596.233
4+
2+
  2521.428 24 AB DE G  J    OP      2+ ≤ 2.4 ps    109.422 11 
   173.543 9 
   438.5 5 
   618.12 5 
   925.189 21 
  2521.40 5 
    3.18 6 
    1.84 6 
    0.57 14 
    0.54 6 
  100 1 
   50.2 6 
M1+E2
M1


E2+M1
E2
  2412.013
  2347.881
  2083.259
  1903.31
  1596.233
     0.0
3+
2+
4+
0+
2+
0+
  2547.23 4 AB       J       R    1+ 0.19 ps +11-5     950.987 26 
  2547.34 11 
  100 1 
   19.5 6 
M1(+E2)
M1
  1596.233
     0.0
2+
0+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  2628.81 4     E G  J            6+      278.84 13 
   520.964 25 
   12.7 16 
  100 5 
M1,E2
E2+M1
  2349.805
  2107.854
5+
6+
  2658.3 10 ?    E    J                 575?
  100

  2083.259
4+
  2899.59 4 AB    GHIJKL  OP      2+ 49 fs 9     996.2 3 
  1303.38 5 
  2899.55 4 
    3.2 8 
   53 3 
  100 5 

M1+E2
E2
  1903.31
  1596.233
     0.0
0+
2+
0+
  3001.12 14 A        J    O       2+ 0.16 ps +10-5    1097.20 23 
  1405.20 17 
   39 8 
  100 12 

(M1+E2)
  1903.31
  1596.233
0+
2+
  3016.9 5  B   F   J     P      0+ ≥ 0.14 ps   1420.7 5 
  3016.3 12 
  100 15 
 
E2
E0
  1596.233
     0.0
2+
0+
  3039.0 4          J L          3-        
  3118.55 16 AB   FGHIJKL NOP      2+ 27.5 fs 85    3118.51 16 
  100
(E2)
     0.0
0+
  3120.34 20 ?         J            2+     3120.3 2 ?
  100
E2
     0.0
0+
  3122.11 5          J            4+      657.5 4 
   772.50 13 
  1525.85 4 
    2.9 10 
   23 2 
  100 5 


E2
  2464.08
  2349.805
  1596.233
3-
5+
2+
  3168.3 10 ?    E                     1085?
  100

  2083.259
4+
  3219.95 11          J            (0+)     1623.71 10 
  100

  1596.233
2+
  3226 2      F         P      0+        
  3255.70 5     E G  JKL          5-      739.94 4 
   774.8 3 
  100 6 
   22 4 
(E1)

  2515.76
  2480.925
4+
4+
  3319.65 6 AB     HIJ            2+ 58 fs +19-12     772.50 13 ?
  1235.8 6 ?
  1724.7?
  3319.61 6 
   39 3 
   11 4 
   52 3 
  100 6 



E2
  2547.23
  2083.259
  1596.233
     0.0
1+
4+
2+
0+
  3335.47 11      FG  J L   P      4+      855.1 4 
   985.63 22 
  1227.71 16 ?
  1252.12 13 
  1739.4 3 
   18 4 
    9 3 
   43 5 
  100 8 
   23 4 





  2480.925
  2349.805
  2107.854
  2083.259
  1596.233
4+
5+
6+
4+
2+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  3360.24 18          J                1010.45 19 
  1276.9 4 
  100 10 
   27 8 


  2349.805
  2083.259
5+
4+
  3391.09 8     E    J                1307.73 10 
  1794.93 10 
  100 8 
   79 5 


  2083.259
  1596.233
4+
2+
  3394.92 7 A     G  JK           (4-) 0.042 ps +49-21     982.89?
  1045.11 7 
  1287.03 19 
  1311.56 19 ?
  100 6 
   74 5 
   22 3 
   22 3 




  2412.013
  2349.805
  2107.854
  2083.259
3+
5+
6+
4+
  3395.1 10 ?    E                 (4+)      983.1?
  100
M1,E2
  2412.013
3+
  3408.02 15          J            (2+) ≥ 0.062 ps    886.42 22 
   944.0 3 
   996.2 3 
  1811.0 3 ?
  3408.1 4 
  100 11 
   41 7 
   27 7 
   49 7 
   57 7 





  2521.428
  2464.08
  2412.013
  1596.233
     0.0
2+
3-
3+
2+
0+
  3424.6 3     E G IJ     P   T  7-     1316.8 3 
  100
E1
  2107.854
6+
  3432.8 10     E                 7+     1083.0
  100
E2
  2349.805
5+
  3436.54 7          J            (2+,1)     1088.65 6 
  1533.2 4 ?
  3436.8 8 
  100 5 
    6.2 11 
    5.4 12 



  2347.881
  1903.31
     0.0
2+
0+
0+
  3471.21 11          J            (2+) 0.097 ps +76-35    1568.1 5 
  3471.15 11 
   16 4 
  100 6 

(E2)
  1903.31
     0.0
0+
0+
  3473.75 4 A     G  JK           3- 0.066 ps +21-13     992.9 5 
  1125.64 22 
  1877.51 3 
   33 12 
   22 3 
  100 10 



  2480.925
  2347.881
  1596.233
4+
2+
2+
  3476.3 3     E              T  8-       51.7 1 
   848.2
  100
 


  3424.6
  2628.81
7-
6+
  3484.2 10     E                 6+     1134.4
  100
E2
  2349.805
5+
  3491.2 3 ?         J                 944.0 3 
  3491.2 7 
  100 18 
   79 18 


  2547.23
     0.0
1+
0+
  3492.23 25     E              T  9- 1.7 ns 2      15.7
    69.5
  1384.2 3 
 
 
 



  3476.3
  3424.6
  2107.854
8-
7-
6+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  3512.3 3     E              T  8+     1404.4 3 
  100
E2
  2107.854
6+
  3520.87 14 A                     (4+)     1924.62 13 
  100

  1596.233
2+
  3522.2 10     E G               (5)     1041.3
 

  2480.925
4+
  3534.6 10     E      L          (3,4)     1184.8
  100

  2349.805
5+
  3539.1 3          J            2+ ≥ 0.21 ps   3539.1 3 
  100
E2
     0.0
0+
  3551 3      F    K    P      2+,3-        
  3567.5 3          J            (2+)     1484.3 3 
  3567.0 10 
  100 13 
   55 16 


  2083.259
     0.0
4+
0+
  3602        I                    
  3620.7 6     E                 8+      992.2
  1512.9
 
 


  2628.81
  2107.854
6+
6+
  3642.8 3        H J  MN        1- 1.45 fs 19    1739.4 3 ?
  3642.7 3 
   22 4 
  100 7 

E1
  1903.31
     0.0
0+
0+
  3646.7 6          J            (1,2+) ≥ 0.062 ps   1743.31 22 ?
  3646.6 6 
   75 11 
  100 18 


  1903.31
     0.0
0+
0+
  3648.23 14          J            (2+,3,4+)     1564.92 16 
  2052.07 22 
  100 8 
   69 7 


  2083.259
  1596.233
4+
2+
  3653 3      F    K    P      2+,3-        
  3657.64 18 ?         J            (4+,5,6+)     1307.73 10 ?
  1549.76 19 
  1574.5 5 
  100 3 
   45 5 
   12 4 



  2349.805
  2107.854
  2083.259
5+
6+
4+
  3661.5 10     E                 (7,8)     1032.7
 

  2628.81
6+
  3684.2 6          J            (1-,2+)     1220.5 3 ?
  3684.1 6 
  100 14 
   76 12 


  2464.08
     0.0
3-
0+
  3708.60 13          J            (2+)     1227.71 16 
  2112.30 19 
  3708.1 11 
   81 10 
  100 8 
   33 8 



  2480.925
  1596.233
     0.0
4+
2+
0+
  3710 4      FG   K    P      5-        
  3714.3 3     E              T  10+ 23.1 ns 4     202.0 3 
   222.0 3 
   54 12 
  100 15 
E2
E1
  3512.3
  3492.23
8+
9-
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  3723.54 17          J            (2+) ≥ 0.097 ps   1311.56 19 
  3723.4 3 
   45 7 
  100 7 

(E2)
  2412.013
     0.0
3+
0+
  3729 2      F         P      2+        
  3735.3 4          J            (1,2+)     3735.2 4 
  100

     0.0
0+
  3746 2      F         P             
  3767.97 10          J            (2+,3+,4+)     1220.5 3 
  1252.12 13 ?
  1287.03 19 
  1684.4 3 
  2171.82 13 
   34 5 
   98 8 
   36 5 
   23 3 
  100 6 





  2547.23
  2515.76
  2480.925
  2083.259
  1596.233
1+
4+
4+
4+
2+
  3780     FG               (3+,4+)        
  3792.72 15          JK    P      3-      893.7 3 
  1276.9 4 
  1311.56 19 
  2196.6 6 
  100 13 
   48 14 
   94 14 
   93 10 




  2899.59
  2515.76
  2480.925
  1596.233
2+
4+
4+
2+
  3836.1 5 ?         J            (2+,3,4+)     1753.1 4 ?
  2239.8 5 
   32 10 
  100 17 


  2083.259
  1596.233
4+
2+
  3847.10 14          J            (4+,5,6+)      808.1 3 
  1497.31 22 
  1739.4 3 
  1763.6 3 
   49 7 
  100 10 
   38 6 
   47 6 




  3039.0
  2349.805
  2107.854
  2083.259
3-
5+
6+
4+
  3853.2 5          J            (1,2+)     2256.8 7 
  3853.3 6 
   30 8 
  100 11 


  1596.233
     0.0
2+
0+
  3879.3 8          J            (1,2+)     3879.2 8 
  100

     0.0
0+
  3894.5 6     E                 9+      180.0
   274.2
   382.3
 
 
 



  3714.3
  3620.7
  3512.3
10+
8+
8+
  3910.93 23          J                2314.68 22 
  100

  1596.233
2+
  3911 10      FG        P      5-        
  3912 4           K           2-        
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  3956 4           K                  
  3957.93 18          J                1493.6 3 
  2361.80 22 
   69 9 
  100 9 


  2464.08
  1596.233
3-
2+
  3970.8 10 ?    E                     1621.0?
 

  2349.805
5+
  3980           L   P      3-        
  3984.20 16          J            (2+,3,4+)     1901.4 5 
  2387.90 16 
   87 19 
  100 15 


  2083.259
  1596.233
4+
2+
  4000 4           K           4-        
  4017 10       G        P             
  4053       H              (1)     4053
  100
(D)
     0.0
0+
  4061        I                    
  4125 10    D FG        P      2+        
  4158 4    D      K           2-        
  4164.0 3          J            (1,2+)     2567.8 3 
  4163.5 9 
  100 16 
   53 18 


  1596.233
     0.0
2+
0+
  4171.1 7      FG  J            (2+,1)     2576.1 6 ?
  4171.0 7 
   31 10 
  100 14 


  1596.233
     0.0
2+
0+
  4173.6 8        H    MN        1(-) 3.6 fs 7    4173.5 8 
  100
[E1]
     0.0
0+
  4182 4           K           1-        
  4183 10                P      2+,(3-,4+)        
  4208 6           K                  
  4242 10      FG        P      2+        
  4262.5 7     E                 10+      368.1
   548.3
 
 


  3894.5
  3714.3
9+
10+
  4279.9 4          J            (2+,3,4+)     2196.6 4 
  2683.6 7 
   74 8 
  100 12 


  2083.259
  1596.233
4+
2+
  4296 6         I K    P      3-,4+        
  4331       H              (1)     4331
  100
(D)
     0.0
0+
  4340 10           K    P      (1-)        
  4354.9 7        H     N        1 3.7 fs 8    4354.8 7 
  100
D
     0.0
0+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  4360 10       G        P      +        
  4364 4           K           1-        
  4371       H              (1)     4371
  100
(D)
     0.0
0+
  4388       H              (1)     4388
  100
(D)
     0.0
0+
  4424 4           K    P      2+,3-        
  4437       H              (1)     4437
  100
(D)
     0.0
0+
  4448.5 11     E                 (9,11)      734.2
  100

  3714.3
10+
  4450 10           K                  
  4485 10           K                  
  4514.9 9        H    MN        1(-) 2.7 fs 5    4514.8 9 
  100
[E1]
     0.0
0+
  4538 4           K    P      3-        
  4571.3 13 ?    E                 (8+,10+)     1058.4?
 

  3512.3
8+
  4580 4           K           2-        
  4640 10           K                  
  4655       H              (1)     4655
  100
(D)
     0.0
0+
  4660 15           K                  
  4700 10         I K                  
  4720 15           K                  
  4748 4           K    P      2-        
  4760 15           K                  
  4770 10           K           1-        
  4787.8 9        H    MN        1(-) 2.3 fs 4    4787.7 9 
  100
[E1]
     0.0
0+
  4790 15           K                  
  4827 10                P      2+,3-        
  4851.1 4     E              T  12+      588.8
  1136.8 3 
 
  100

E2
  4262.5
  3714.3
10+
10+
  4860 10           K                  
  4875       H              (1)     4875
  100
(D)
     0.0
0+
  4880 15           K                  
  4883       H              (1)     4883
  100
(D)
     0.0
0+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  4904.6 5     E              T  11-     1190.3 4 
  100
E1
  3714.3
10+
  4910 15           K                  
  4951       H              (1)     4951
  100
(D)
     0.0
0+
  4958.0 8     E                 (11+)     1465.9
  100

  3492.23
9-
  4979 10              N P      2+,3-        
  5000 15           K                  
  5026 6         I K           2-,3-        
  5050 15           K                  
  5069.5 11     E                 (9,11)     1355.2
  100
D
  3714.3
10+
  5093.4 7     E              T  (12-)      135.3
   188.9 5 
 
  100


  4958.0
  4904.6
(11+)
11-
  5101 10           K    P      GE 5        
  5102.1 5     E              T  13-      250.9 3 
  100
E1
  4851.1
12+
  5140 15           K                  
  5157.3 12        H    M  P      1(-) 2.6 fs 5    5157.2 12 
  100
[E1]
     0.0
0+
  5160 15           K  N P             
  5190.2 10        H    MN        1(-) 2.1 fs 4    5190.1 10 
  100
[E1]
     0.0
0+
  5196 6           K           2-,3-        
  5211.6 14        H    MN        1(-) 3.6 fs 9    5211.5 14 
  100
[E1]
     0.0
0+
  5230 15           K    P             
  5245       H              (1)     5245
  100
(D)
     0.0
0+
  5295 10                P      5-,6+        
  5330       H              (1)     5330
  100
(D)
     0.0
0+
  5335.0 9     E                 (12-)      232.6
   377.4
 
 


  5102.1
  4958.0
13-
(11+)
  5337.3 9        H    MN        1(-) 1.8 fs 4    5337.2 9 
  100
[E1]
     0.0
0+
  5377 10         I      P      4+,5-        
  5419.0 4                    T  (14-)      318.0 4 
  100

  5101
GE 5
  5424 6           K           2-,3-        
  5449 10                P             
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  5466 6           K           2-,3-        
  5470       H              (1)     5470
  100
(D)
     0.0
0+
  5494       H              (1)     5494
  100
(D)
     0.0
0+
  5548.4 7        H    MN        1(-) 0.97 fs 17    5548.3 7 
  100
[E1]
     0.0
0+
  5573.8 14        H    MN        1(-) 1.7 fs 4    5573.7 14 
  100
[E1]
     0.0
0+
  5574 15                P      (0+)        
  5624       H              (1)     5624
 
(D)
     0.0
0+
  5650 15                P      2+,3-        
  5659.9 6        H    MN        1- 0.0121 eV 29    5659.8 6 
  100
E1
     0.0
0+
  5693.3 5                    T       592.3 5 
  100

  5101
GE 5
  5703 15                P      1-,2+        
  5721       H              (1)     5721
  100
(D)
     0.0
0+
  5759       H              (1)     5759
  100
(D)
     0.0
0+
  5789 15                P             
  5809       H              (1)     5809
  100
(D)
     0.0
0+
  5823       H              (1)     5823
  100
(D)
     0.0
0+
  5896 15                P      1-,2+        
  5928.6 10        H    M         1(-) 1.16 fs 24    5928.5 10 
  100
[E1]
     0.0
0+
  5940       H              (1)     5940
  100
(D)
     0.0
0+
  5989 15                P      (3-,4+)        
  6029       H              (1)     6029
  100
(D)
     0.0
0+
  6078 15                P      2+,3-        
  6119.1 15        H              1- 0.69 fs 12    6119.0 15 
  100
E1
     0.0
0+
  6130.6 12        H              1 1.5 fs 3    6130.5 12 
  100
D
     0.0
0+
  6161.7 14        H    MN        1(-) 1.08 fs 20    6161.6 14 
  100
[E1]
     0.0
0+
  6187 15                P      2+,3-        
  6226       H              (1)     6226
  100
(D)
     0.0
0+
  6233        I                    
  6245       H              (1)     6245
  100
(D)
     0.0
0+
  6255       H              (1)     6255
  100
(D)
     0.0
0+
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  6268 15                P             
  6273.6 10        H              1 1.05 fs 20    6273.4 10 
  100
D
     0.0
0+
  6295.3 8        H              1- 0.46 fs 8    6295.1 8 
  100
E1
     0.0
0+
  6303.6 3                    T  (15-)     1202.6 3 
  100

  5101
GE 5
  6327.8 12        H              1 1.3 fs 5    6327.6 12 
  100
D
     0.0
0+
  6343.3 11        H              1 0.78 fs 15    6343.1 11 
  100
D
     0.0
0+
  6352.7 10        H              1 0.69 fs 13    6352.5 10 
  100
D
     0.0
0+
  6364 15                P      3-,4+        
  6397.2 8        H              1- 0.28 fs 5    6397.0 8 
  100
E1
     0.0
0+
  6439.9 14        H              1(-) 0.53 fs 9    6439.7 14 
  100
(E1)
     0.0
0+
  6449.9 15        H              1(-) 0.90 fs 18    6449.7 15 
  100
(E1)
     0.0
0+
  6458.5 15        H              1(-) 1.00 fs 20    6458.3 15 
  100
(E1)
     0.0
0+
  6484.8 10        H              1 1.00 fs 20    6484.6 10 
  100
D
     0.0
0+
  6497.0 7        H              1- 0.33 fs 6    6496.8 7 
  100
E1
     0.0
0+
  6535.8 6        H              1- 0.22 fs 3    6535.6 6 
  100
E1
     0.0
0+
  6549.1 11        H              1 1.3 fs 3    6548.9 11 
  100
D
     0.0
0+
  6574.9 15        H              1 1.16 fs 23    6574.7 15 
  100
D
     0.0
0+
  6605.5 10        H              1(-) 0.69 fs 12    6605.3 10 
  100
(E1)
     0.0
0+
  6616.2 10        H              1(-) 0.74 fs 13    6616.0 10 
  100
(E1)
     0.0
0+
  6678        I                    
  6771.7 14        H              (2+)     6771.5 14 
  100
(E2)
     0.0
0+
  6781.9 15        H              1 0.85 fs 19    6781.7 15 
  100
D
     0.0
0+
  6796.6 5                    T  (16-)      493.0 4 
  100

  6303.6
(15-)
  6841.8 12        H              1 0.79 fs 22    6841.6 12 
  100
D
     0.0
0+
  6862.4 7        H              1- 0.24 fs 4    6862.2 7 
  100
E1
     0.0
0+
  6889.2 8                    T  (15,16)     1470.2 7 
  100

  5419.0
(14-)
  6905.9 15        H              1 0.45 fs 10    6905.7 15 
  100
D
     0.0
0+
  6932.6 14        H              1 0.52 fs 11    6932.4 14 
  100
D
     0.0
0+
  6960.4 12        H              1 0.47 fs 10    6960.2 12 
  100
D
     0.0
0+
  7038.2 6                    T  (17-)      734.6 5 
  100

  6303.6
(15-)
E(level)
(keV)
XREFJπ(level) T1/2(level)E(γ)
(keV)
I(γ)M(γ)Final Levels
  7050        I                    
  7206.0 14        H              1 0.31 fs 5    7205.8 14 
  100
D
     0.0
0+
  7214.8 15        H              1 0.34 fs 6    7214.6 15 
  100
D
     0.0
0+
  7341.5 14        H              1 0.9 fs 2    7341.3 14 
  100
D
     0.0
0+
  7370   D                  0+        
  7673.4 12        H              1 0.76 fs 18    7673.2 12 
  100
D
     0.0
0+

E(level): From least-squares fit to γ energies

M(γ): From α(K)exp, γ(θ), γγ(θ), linear pol in β- and ε decay and in different nuclear reactions

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Band Transitions:

E(level)
(keV)
Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - γ.S. band
     0.0 0+ STABLE      
  1596.233 23  2+ 0.0910 ps +48-44    1596.210 35 
  100
E2
     0.0
0+
  2083.259 24  4+ 3.45 ns 3     487.021 12 
  2083.2 5 
  100.0 13 
    0.03 2 
E2
E4
  1596.233
     0.0
2+
0+
  2107.854 24  6+ 7.3 µs 15      24.595 4 
  100
E2
  2083.259
4+
  3512.3 3  8+     1404.4 3 
  100
E2
  2107.854
6+
  3714.3 3  10+ 23.1 ns 4     202.0 3 
   222.0 3 
   54 12 
  100 15 
E2
E1
  3512.3
  3492.23
8+
9-
  4851.1 4  12+      588.8
  1136.8 3 
 
  100

E2
  4262.5
  3714.3
10+
10+

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Additional Gamma Data:















E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
  1596.233 2+ 0.0910 ps +48-44    1596.210 35 E2 8.98×10-4B(E2)(W.u.)=13.9 7, α=8.98E-4, α(K)=0.000676 10, α(L)=8.63E-5 12, α(M)=1.79E-5 3, α(N)=3.97E-6 6, α(O)=6.45E-7 9, α(P)=4.92E-8 7
  1903.31 0+ 0.40 ns 3     306.9 2 E2 0.0454B(E2)(W.u.)=7.4 10, α=0.0454, α(K)=0.0365 6, α(L)=0.00697 10, α(M)=0.001498 22, α(N)=0.000327 5, α(O)=4.98E-5 7, α(P)=2.42E-6 4
  2083.259 4+ 3.45 ns 3     487.021 12 E2 0.01159B(E2)(W.u.)=0.1370 12, α=0.01159, α(K)=0.00966 14, α(L)=0.001527 22, α(M)=0.000324 5, α(N)=7.11E-5 10, α(O)=1.113E-5 16, α(P)=6.77E-7 10
4+ 3.45 ns 3    2083.2 5 E4 1.36×10-3B(E4)(W.u.)=14 10, α=1.36E-3, α(K)=0.001162 17, α(L)=0.0001598 23, α(M)=3.35E-5 5, α(N)=7.43E-6 11, α(O)=1.198E-6 17, α(P)=8.83E-8 13
  2107.854 6+ 7.3 µs 15      24.595 4 E2 697B(E2)(W.u.)=0.29 +8-5, α=697, α(L)=545 8, α(M)=122.0 18, α(N)=25.9 4, α(O)=3.52 5, α(P)=0.000945 14
  2347.881 2+ ≤ 0.2 ns    445.5 5 [E2] 0.01486α=0.01486, α(K)=0.01232 18, α(L)=0.00201 3, α(M)=0.000427 7, α(N)=9.36×10-5 14, α(O)=1.458E-5 21, α(P)=8.56E-7 13
2+ ≤ 0.2 ns    751.637 18 M1+E2+0.38 40.00548α=0.00548 9, α(K)=0.00471 8, α(L)=0.000613 10, α(M)=0.0001277 20, α(N)=2.83×10-5 5, α(O)=4.60E-6 8, α(P)=3.54E-7 6
2+ ≤ 0.2 ns   2347.88 5 E2 8.45×10-4α=8.45×10-4, α(K)=0.000333 5, α(L)=4.15E-5 6, α(M)=8.60E-6 12, α(N)=1.91E-6 3, α(O)=3.11E-7 5, α(P)=2.42E-8 4
  2349.805 5+ ≤ 12 ps    241.933 30 M1+E2-0.04 +3-60.1020α=0.1020, α(K)=0.0872 13, α(L)=0.01171 17, α(M)=0.00245 4, α(N)=0.000543 8, α(O)=8.81×10-5 13, α(P)=6.70E-6 10
5+ ≤ 12 ps    266.543 12 M1+E2-0.04 40.0787α=0.0787, α(K)=0.0673 10, α(L)=0.00902 13, α(M)=0.00188 3, α(N)=0.000418 6, α(O)=6.78×10-5 10, α(P)=5.17E-6 8
  2412.013 3+ 1.3 ps 4      64.135 10 M1 4.26B(M1)(W.u.)=0.020 +14-8, α=4.26, α(K)=3.63 5, α(L)=0.499 7, α(M)=0.1046 15, α(N)=0.0232 4, α(O)=0.00375 6, α(P)=0.000281 4
3+ 1.3 ps 4     328.762 8 M1+E2-0.049 60.0453B(E2)(W.u.)=2.9 +24-12, B(M1)(W.u.)=0.22 +10-5, α=0.0453, α(K)=0.0388 6, α(L)=0.00516 8, α(M)=0.001078 15, α(N)=0.000239 4, α(O)=3.88E-5 6, α(P)=2.97E-6 5
3+ 1.3 ps 4     815.772 19 M1(+E2)-0.03 10.00470B(E2)(W.u.)=0.013 +21-9, B(M1)(W.u.)=0.016 +8-4, α=0.00470, α(K)=0.00404 6, α(L)=0.000521 8, α(M)=0.0001085 16, α(N)=2.41E-5 4, α(O)=3.92E-6 6, α(P)=3.05E-7 5
  2464.08 3- 0.15 ps 3     867.846 20 E1 1.11×10-3B(E1)(W.u.)=0.0026 +6-4, α=1.11E-3, α(K)=0.000959 14, α(L)=0.0001200 17, α(M)=2.49E-5 4, α(N)=5.51E-6 8, α(O)=8.92E-7 13, α(P)=6.80E-8 10
3- 0.15 ps 3    2464.1 5 [E3] 9.28×10-4B(E3)(W.u.)=26 +12-8, α=9.28E-4, α(K)=0.000514 8, α(L)=6.61E-5 10, α(M)=1.375E-5 20, α(N)=3.05E-6 5, α(O)=4.95E-7 7, α(P)=3.81E-8 6
  2480.925 4+ 22 ps 7      68.916 6 M1 3.46B(M1)(W.u.)=0.20 +11-6, α=3.46, α(K)=2.95 5, α(L)=0.405 6, α(M)=0.0848 12, α(N)=0.0188 3, α(O)=0.00304 5, α(P)=0.000228 4
4+ 22 ps 7     131.117 8 M1+E2-0.13 +2-50.553B(E2)(W.u.)=1.1×102 +20-5, B(M1)(W.u.)=0.18 +9-5, α=0.553 9, α(K)=0.470 7, α(L)=0.0661 22, α(M)=0.0139 5, α(N)=0.00307 11, α(O)=0.000495 15, α(P)=3.61E-5 6
4+ 22 ps 7     397.52 5 (E2) 0.0206B(E2)(W.u.)=3.9 +23-12, α=0.0206, α(K)=0.01699 24, α(L)=0.00289 4, α(M)=0.000616 9, α(N)=0.0001349 19, α(O)=2.09E-5 3, α(P)=1.166E-6 17
  2515.76 4+ ≤ 2.5 ps    432.493 12 M1+E2-0.04 20.0224α=0.0224, α(K)=0.0192 3, α(L)=0.00253 4, α(M)=0.000527 8, α(N)=0.0001170 17, α(O)=1.90×10-5 3, α(P)=1.461E-6 21
4+ ≤ 2.5 ps    919.550 23 E2 0.00242α=0.00242, α(K)=0.00207 3, α(L)=0.000281 4, α(M)=5.87×10-5 9, α(N)=1.298E-5 19, α(O)=2.08E-6 3, α(P)=1.496E-7 21
  2521.428 2+ ≤ 2.4 ps    109.422 11 M1+E2+0.26 50.952α=0.952 20, α(K)=0.790 12, α(L)=0.128 9, α(M)=0.0271 19, α(N)=0.0060 4, α(O)=0.00094 6, α(P)=5.98×10-5 9
2+ ≤ 2.4 ps    173.543 9 M1 0.252α=0.252, α(K)=0.215 3, α(L)=0.0291 4, α(M)=0.00609 9, α(N)=0.001351 19, α(O)=0.000219 3, α(P)=1.658×10-5 24
2+ ≤ 2.4 ps    925.189 21 E2+M1-0.22 40.00344α=0.00344 6, α(K)=0.00296 5, α(L)=0.000381 6, α(M)=7.92×10-5 12, α(N)=1.76E-5 3, α(O)=2.86E-6 5, α(P)=2.22E-7 4
2+ ≤ 2.4 ps   2521.40 5 E2 8.81×10-4α=8.81×10-4, α(K)=0.000293 5, α(L)=3.65E-5 6, α(M)=7.55E-6 11, α(N)=1.676E-6 24, α(O)=2.73E-7 4, α(P)=2.13E-8 3
  2547.23 1+ 0.19 ps +11-5     950.987 26 M1(+E2)+0.01 70.00327B(M1)(W.u.)=0.112 42, α=0.00327, α(K)=0.00282 4, α(L)=0.000361 5, α(M)=7.52×10-5 11, α(N)=1.669E-5 24, α(O)=2.72E-6 4, α(P)=2.12E-7 3
1+ 0.19 ps +11-5    2547.34 11 M1 9.62×10-4B(M1)(W.u.)=0.00114 +46-44, α=9.62×10-4, α(K)=0.000318 5, α(L)=3.97E-5 6, α(M)=8.24E-6 12, α(N)=1.83E-6 3, α(O)=2.99E-7 5, α(P)=2.36E-8 4
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
  2628.81 6+      278.84 13 M1,E2 0.066α=0.066 5, α(K)=0.054 6, α(L)=0.0089 10, α(M)=0.00190 23, α(N)=0.00042 5, α(O)=6.5×10-5 5, α(P)=3.9E-6 7
6+      520.964 25 E2+M1-0.19 60.01387α=0.01387 22, α(K)=0.01189 20, α(L)=0.001563 24, α(M)=0.000326 5, α(N)=7.23×10-5 11, α(O)=1.175E-5 18, α(P)=9.01E-7 15
  2899.59 2+ 49 fs 9    1303.38 5 M1+E2-1.5 +10-40.00132B(E2)(W.u.)=17 +8-13, B(M1)(W.u.)=0.021 +51-10, α=0.00132 21, α(K)=0.00111 18, α(L)=0.000143 22, α(M)=3.0E-5 5, α(N)=6.6E-6 10, α(O)=1.07E-6 17, α(P)=8.2E-8 15
2+ 49 fs 9    2899.55 4 E2 9.79×10-4B(E2)(W.u.)=0.83 +23-16, α=9.79E-4, α(K)=0.000230 4, α(L)=2.84E-5 4, α(M)=5.88E-6 9, α(N)=1.306E-6 19, α(O)=2.13E-7 3, α(P)=1.669E-8 24
  3001.12 2+ 0.16 ps +10-5    1405.20 17 (M1+E2)+0.7 30.00127B(E2)(W.u.)=3.5 +50-27, B(M1)(W.u.)=0.024 +25-14, α=0.00127 7, α(K)=0.00106 6, α(L)=0.000135 7, α(M)=2.80E-5 15, α(N)=6.2E-6 4, α(O)=1.01E-6 6, α(P)=7.8E-8 5
  3016.9 0+ ≥ 0.14 ps   1420.7 5 E2 1.03×10-3α=1.03×10-3, α(K)=0.000846 12, α(L)=0.0001089 16, α(M)=2.27E-5 4, α(N)=5.02E-6 7, α(O)=8.13E-7 12, α(P)=6.15E-8 9
  3118.55 2+ 27.5 fs 85    3118.51 16 (E2) 1.04×10-3B(E2)(W.u.)=1.6 +7-4, α=1.04E-3, α(K)=0.000203 3, α(L)=2.50E-5 4, α(M)=5.18E-6 8, α(N)=1.149E-6 16, α(O)=1.87E-7 3, α(P)=1.472E-8 21
  3120.34 2+     3120.3 2 E2 1.04×10-3α=1.04×10-3, α(K)=0.000203 3, α(L)=2.50E-5 4, α(M)=5.17E-6 8, α(N)=1.148E-6 16, α(O)=1.87E-7 3, α(P)=1.470E-8 21
  3122.11 4+     1525.85 4 E2 9.43×10-4α=9.43×10-4, α(K)=0.000737 11, α(L)=9.44E-5 14, α(M)=1.96E-5 3, α(N)=4.35E-6 6, α(O)=7.05E-7 10, α(P)=5.36E-8 8
  3255.70 5-      739.94 4 (E1) 1.53×10-3α=1.53×10-3, α(K)=0.001319 19, α(L)=0.0001662 24, α(M)=3.45E-5 5, α(N)=7.63E-6 11, α(O)=1.234E-6 18, α(P)=9.33E-8 13
  3319.65 2+ 58 fs +19-12    3319.61 6 E2 1.10×10-3B(E2)(W.u.)=0.29 9, α=1.10E-3, α(K)=0.000182 3, α(L)=2.24E-5 4, α(M)=4.64E-6 7, α(N)=1.031E-6 15, α(O)=1.680E-7 24, α(P)=1.322E-8 19
  3395.1 (4+)      983.1M1,E2 0.0026α=0.0026 5, α(K)=0.0022 5, α(L)=0.00029 5, α(M)=6.0×10-5 10, α(N)=1.33E-5 22, α(O)=2.1E-6 4, α(P)=1.6E-7 4
  3424.6 7-     1316.8 3 E1 6.01×10-4α=6.01×10-4, α(K)=0.000444 7, α(L)=5.48E-5 8, α(M)=1.134E-5 16, α(N)=2.51E-6 4, α(O)=4.08E-7 6, α(P)=3.16E-8 5
  3432.8 7+     1083.0E2 1.70×10-3α=1.70×10-3, α(K)=0.001459 21, α(L)=0.000194 3, α(M)=4.04E-5 6, α(N)=8.94E-6 13, α(O)=1.440E-6 21, α(P)=1.059E-7 15
  3471.21 (2+) 0.097 ps +76-35    3471.15 11 (E2) 1.15×10-3B(E2)(W.u.)=0.23 +15-11, α=1.15E-3, α(K)=0.0001690 24, α(L)=2.08E-5 3, α(M)=4.30E-6 6, α(N)=9.54E-7 14, α(O)=1.556E-7 22, α(P)=1.226E-8 18
  3484.2 6+     1134.4E2 1.55×10-3α=1.55×10-3, α(K)=0.001325 19, α(L)=0.0001749 25, α(M)=3.65E-5 6, α(N)=8.07E-6 12, α(O)=1.302E-6 19, α(P)=9.63E-8 14
  3512.3 8+     1404.4 3 E2 1.05×10-3α=1.05×10-3, α(K)=0.000865 13, α(L)=0.0001115 16, α(M)=2.32E-5 4, α(N)=5.14E-6 8, α(O)=8.32E-7 12, α(P)=6.29E-8 9
  3539.1 2+ ≥ 0.21 ps   3539.1 3 E2 1.17×10-3α=1.17×10-3, α(K)=0.0001636 23, α(L)=2.01E-5 3, α(M)=4.16E-6 6, α(N)=9.23E-7 13, α(O)=1.505E-7 21, α(P)=1.186E-8 17
  3642.8 1- 1.45 fs 19    3642.7 3 E1 1.61×10-3B(E1)(W.u.)=0.0030 5, α=1.61E-3, α(K)=9.12E-5 13, α(L)=1.102E-5 16, α(M)=2.28E-6 4, α(N)=5.05E-7 7, α(O)=8.24E-8 12, α(P)=6.50E-9 10
  3714.3 10+ 23.1 ns 4     202.0 3 E2 0.178B(E2)(W.u.)=0.55 14, α=0.178, α(K)=0.1351 20, α(L)=0.0335 5, α(M)=0.00731 12, α(N)=0.001583 24, α(O)=0.000234 4, α(P)=8.31E-6 13
10+ 23.1 ns 4     222.0 3 E1 0.0274B(E1)(W.u.)=6.0E-7 10, α=0.0274, α(K)=0.0235 4, α(L)=0.00311 5, α(M)=0.000646 10, α(N)=0.0001423 21, α(O)=2.26E-5 4, α(P)=1.555E-6 23
  3723.54 (2+) ≥ 0.097 ps   3723.4 3 (E2) 1.23×10-3α=1.23×10-3, α(K)=0.0001502 21, α(L)=1.84E-5 3, α(M)=3.81E-6 6, α(N)=8.46E-7 12, α(O)=1.381E-7 20, α(P)=1.089E-8 16
  4173.6 1(-) 3.6 fs 7    4173.5 8 [E1] 0.00180B(E1)(W.u.)=9.6E-4 +23-16, α=0.00180, α(K)=7.56E-5 11, α(L)=9.12E-6 13, α(M)=1.88E-6 3, α(N)=4.18E-7 6, α(O)=6.81E-8 10, α(P)=5.39E-9 8
  4514.9 1(-) 2.7 fs 5    4514.8 9 [E1] 0.00192B(E1)(W.u.)=0.00101 +23-16, α=0.00192, α(K)=6.80E-5 10, α(L)=8.19E-6 12, α(M)=1.691E-6 24, α(N)=3.75E-7 6, α(O)=6.12E-8 9, α(P)=4.84E-9 7
  4787.8 1(-) 2.3 fs 4    4787.7 9 [E1] 0.00201B(E1)(W.u.)=9.9E-4 +21-15, α=0.00201, α(K)=6.28E-5 9, α(L)=7.57E-6 11, α(M)=1.562E-6 22, α(N)=3.47E-7 5, α(O)=5.65E-8 8, α(P)=4.47E-9 7
E(level)
(keV)
Jπ(level)T1/2(level)E(γ)
(keV)
MultipolarityMixing
Ratio
Conversion
Coefficient
Additional Data
  4851.1 12+     1136.8 3 E2 1.54×10-3α=1.54×10-3, α(K)=0.001320 19, α(L)=0.0001741 25, α(M)=3.63E-5 5, α(N)=8.03E-6 12, α(O)=1.296E-6 19, α(P)=9.59E-8 14
  4904.6 11-     1190.3 4 E1 6.38×10-4α=6.38×10-4, α(K)=0.000530 8, α(L)=6.57E-5 10, α(M)=1.360E-5 19, α(N)=3.01E-6 5, α(O)=4.90E-7 7, α(P)=3.78E-8 6
  5102.1 13-      250.9 3 E1 0.0198α=0.0198, α(K)=0.01700 25, α(L)=0.00224 4, α(M)=0.000465 7, α(N)=0.0001024 15, α(O)=1.632×10-5 24, α(P)=1.137E-6 17
  5157.3 1(-) 2.6 fs 5    5157.2 12 [E1] 0.00211B(E1)(W.u.)=7.0E-4 +17-11, α=0.00211, α(K)=5.70E-5 8, α(L)=6.85E-6 10, α(M)=1.414E-6 20, α(N)=3.14E-7 5, α(O)=5.12E-8 8, α(P)=4.05E-9 6
  5190.2 1(-) 2.1 fs 4    5190.1 10 [E1] 0.00212B(E1)(W.u.)=8.5E-4 +20-14, α=0.00212, α(K)=5.65E-5 8, α(L)=6.80E-6 10, α(M)=1.402E-6 20, α(N)=3.11E-7 5, α(O)=5.08E-8 8, α(P)=4.02E-9 6
  5211.6 1(-) 3.6 fs 9    5211.5 14 [E1] 0.00213B(E1)(W.u.)=4.9E-4 +17-10, α=0.00213, α(K)=5.62E-5 8, α(L)=6.76E-6 10, α(M)=1.395E-6 20, α(N)=3.09E-7 5, α(O)=5.05E-8 7, α(P)=4.00E-9 6
  5337.3 1(-) 1.8 fs 4    5337.2 9 [E1] 0.00217B(E1)(W.u.)=9.1E-4 +26-17, α=0.00217, α(K)=5.45E-5 8, α(L)=6.55E-6 10, α(M)=1.351E-6 19, α(N)=3.00E-7 5, α(O)=4.89E-8 7, α(P)=3.87E-9 6
  5548.4 1(-) 0.97 fs 17    5548.3 7 [E1] 0.00223B(E1)(W.u.)=0.00151 +32-23, α=0.00223, α(K)=5.18E-5 8, α(L)=6.22E-6 9, α(M)=1.284E-6 18, α(N)=2.85E-7 4, α(O)=4.65E-8 7, α(P)=3.68E-9 6
  5573.8 1(-) 1.7 fs 4    5573.7 14 [E1] 0.00223B(E1)(W.u.)=8.5E-4 +26-16, α=0.00223, α(K)=5.15E-5 8, α(L)=6.19E-6 9, α(M)=1.276E-6 18, α(N)=2.83E-7 4, α(O)=4.62E-8 7, α(P)=3.66E-9 6
  5659.9 1- 0.0121 eV 29    5659.8 6 E1 0.00226B(E1)(W.u.)=3.7E-5 9, α=0.00226, α(K)=5.05E-5 7, α(L)=6.06E-6 9, α(M)=1.251E-6 18, α(N)=2.78E-7 4, α(O)=4.53E-8 7, α(P)=3.59E-9 5
  5928.6 1(-) 1.16 fs 24    5928.5 10 [E1] 0.00233B(E1)(W.u.)=0.00104 +27-18, α=0.00233, α(K)=4.75E-5 7, α(L)=5.71E-6 8, α(M)=1.178E-6 17, α(N)=2.61E-7 4, α(O)=4.27E-8 6, α(P)=3.38E-9 5
  6119.1 1- 0.69 fs 12    6119.0 15 E1 B(E1)(W.u.)=0.00159 +34-24
  6161.7 1(-) 1.08 fs 20    6161.6 14 [E1] B(E1)(W.u.)=9.9E-4 +23-16
  6295.3 1- 0.46 fs 8    6295.1 8 E1 B(E1)(W.u.)=0.00219 +46-33
  6397.2 1- 0.28 fs 5    6397.0 8 E1 B(E1)(W.u.)=0.0034 +8-5
  6439.9 1(-) 0.53 fs 9    6439.7 14 (E1) B(E1)(W.u.)=0.00177 +37-26
  6449.9 1(-) 0.90 fs 18    6449.7 15 (E1) B(E1)(W.u.)=0.00104 +26-17
  6458.5 1(-) 1.00 fs 20    6458.3 15 (E1) B(E1)(W.u.)=9.3E-4 +23-16
  6497.0 1- 0.33 fs 6    6496.8 7 E1 B(E1)(W.u.)=0.0028 +6-4
  6535.8 1- 0.22 fs 3    6535.6 6 E1 B(E1)(W.u.)=0.0041 +7-5
  6605.5 1(-) 0.69 fs 12    6605.3 10 (E1) B(E1)(W.u.)=0.00126 +27-19
  6616.2 1(-) 0.74 fs 13    6616.0 10 (E1) B(E1)(W.u.)=0.00117 +25-18
  6862.4 1- 0.24 fs 4    6862.2 7 E1 B(E1)(W.u.)=0.0032 +7-5

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0.00+ STABLE E(level): From 140Pr ε Decay. γ.S. band.
  1596.2332+ 0.0910 ps +48-44  μ=+1.9 2 (2014StZZ)
RMS charge radius <r2>1/2=4.8771 fm 18 (2013An02).
E(level): From 140Pr ε Decay. γ.S. band.
  2083.2594+ 3.45 ns 3  μ=+4.20 15, Q=0.35 7 (2013StZZ,2014StZZ)
E(level): From 140Pr ε Decay. γ.S. band.
  2107.8546+ 7.3 µs 15  E(level): From 140Pr ε Decay. γ.S. band.
  3120.342+   Extra 2+ level found only by 1985Di11 about 2 keV higher in energy than the previous 2+, 3118.5 level found only by 1993Go23, both levels being mainly determined by a γ transition to g.s., which suggests that this can be a same level.
  32260+   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  3255.705-   Jπ(level): From L in (p,p’) (1977Sh06).
  3394.92(4-) 0.042 ps +49-21  E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  3395.1(4+)   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  3473.753- 0.066 ps +21-13  E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  3476.38-   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  3484.26+   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  3492.239- 1.7 ns 2  Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  3512.38+   E(level): From 140Pr ε Decay. γ.S. band.
Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  3534.6(3,4)   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  35512+,3-   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  3620.78+   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  36532+,3-   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  37105-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  3714.310+ 23.1 ns 4  μ=+10.3 4 (2014StZZ,1988Ka04)
E(level): From 140Pr ε Decay. γ.S. band.
Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  3792.723-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  3894.59+   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  39122-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  40004-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  4053(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
E(level)Jπ(level)T1/2(level)Comments
  41252+   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  41582-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  4173.61(-) 3.6 fs 7  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  41821-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  4262.510+   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  42963-,4+   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  4331(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  4340(1-)   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  4354.91 3.7 fs 8  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  43641-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  4371(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  4388(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  44242+,3-   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  4437(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  4448.5(9,11)   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  4514.91(-) 2.7 fs 5  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  45383-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  45802-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  4655(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  47482-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  47701-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  4787.81(-) 2.3 fs 4  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  48272+,3-   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  4851.112+   E(level): From 140Pr ε Decay. γ.S. band.
Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  4875(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
E(level)Jπ(level)T1/2(level)Comments
  4883(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  4904.611-   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  4951(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  4958.0(11+)   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  49792+,3-   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  50262-,3-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  5069.5(9,11)   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  5093.4(12-)   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  5101GE 5   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  5102.113-   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  5157.31(-) 2.6 fs 5  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  5190.21(-) 2.1 fs 4  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  51962-,3-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  5211.61(-) 3.6 fs 9  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  5245(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  52955-,6+   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  5330(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  5335.0(12-)   Jπ(level): From multipolarities deduced from α(K)exp and γ(θ) in (α,2nγ) (1979BiZN).
  5337.31(-) 1.8 fs 4  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  53774+,5-   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  5419.0(14-)   Jπ(level): From 238U(12C,Fγ) dataset tentatively assigned by 2012As06 based on the following criteria: (i) Spin values increase with excitation energy, (ii) High-energy (low-energy) transitions likely have an E2 (M1) character, and (iii) Measured branching ratios as well as the existence or the absence of cross-over transitions place some conditions on the multipolarities.
  54242-,3-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  54662-,3-   E(level): From (α,α’γ) and (γ,γ’) datasets.
Jπ(level): From analysis of (p,p’) via IAR decay (1969He13,1970He05).
  5470(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  5494(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
E(level)Jπ(level)T1/2(level)Comments
  5548.41(-) 0.97 fs 17  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  5573.81(-) 1.7 fs 4  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  5574(0+)   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  5624(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  56502+,3-   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  57031-,2+   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  5721(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  5759(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  5809(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  5823(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  58961-,2+   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  5928.61(-) 1.16 fs 24  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  5940(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  5989(3-,4+)   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  6029(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  60782+,3-   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  6119.11- 0.69 fs 12  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6130.61 1.5 fs 3  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6161.71(-) 1.08 fs 20  Jπ(level): From 140Ce(α,α’γ) dataset based on measured γ-ray multipolarity (αγ(θ)); only natural parities are excited under the kinematic conditions of the experiment.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  61872+,3-   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  6226(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  6245(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  6255(1)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  6273.61 1.05 fs 20  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6295.31- 0.46 fs 8  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
E(level)Jπ(level)T1/2(level)Comments
  6303.6(15-)   Jπ(level): From 238U(12C,Fγ) dataset tentatively assigned by 2012As06 based on the following criteria: (i) Spin values increase with excitation energy, (ii) High-energy (low-energy) transitions likely have an E2 (M1) character, and (iii) Measured branching ratios as well as the existence or the absence of cross-over transitions place some conditions on the multipolarities.
  6327.81 1.3 fs 5  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6343.31 0.78 fs 15  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6352.71 0.69 fs 13  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  63643-,4+   E(level): From 140Ce(γ,γ’) dataset.
Jπ(level): From L in (p,t) (1977Sh06).
  6397.21- 0.28 fs 5  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6439.91(-) 0.53 fs 9  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6449.91(-) 0.90 fs 18  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6458.51(-) 1.00 fs 20  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6484.81 1.00 fs 20  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6497.01- 0.33 fs 6  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6535.81- 0.22 fs 3  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6549.11 1.3 fs 3  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6574.91 1.16 fs 23  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6605.51(-) 0.69 fs 12  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6616.21(-) 0.74 fs 13  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6771.7(2+)   Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
  6781.91 0.85 fs 19  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6796.6(16-)   Jπ(level): From 238U(12C,Fγ) dataset tentatively assigned by 2012As06 based on the following criteria: (i) Spin values increase with excitation energy, (ii) High-energy (low-energy) transitions likely have an E2 (M1) character, and (iii) Measured branching ratios as well as the existence or the absence of cross-over transitions place some conditions on the multipolarities.
  6841.81 0.79 fs 22  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6862.41- 0.24 fs 4  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6889.2(15,16)   Jπ(level): From 238U(12C,Fγ) dataset tentatively assigned by 2012As06 based on the following criteria: (i) Spin values increase with excitation energy, (ii) High-energy (low-energy) transitions likely have an E2 (M1) character, and (iii) Measured branching ratios as well as the existence or the absence of cross-over transitions place some conditions on the multipolarities.
  6905.91 0.45 fs 10  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6932.61 0.52 fs 11  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  6960.41 0.47 fs 10  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
E(level)Jπ(level)T1/2(level)Comments
  7038.2(17-)   Jπ(level): From 238U(12C,Fγ) dataset tentatively assigned by 2012As06 based on the following criteria: (i) Spin values increase with excitation energy, (ii) High-energy (low-energy) transitions likely have an E2 (M1) character, and (iii) Measured branching ratios as well as the existence or the absence of cross-over transitions place some conditions on the multipolarities.
  7206.01 0.31 fs 5  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  7214.81 0.34 fs 6  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  7341.51 0.9 fs 2  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.
  7673.41 0.76 fs 18  Jπ(level): Based on measured multipolarity and parity of γ-ray that decays to 0+ g.s. in 140Ce(γ,γ’) dataset.
T1/2(level): From 140Ce(γ,γ’) dataset, deduced from Γ02/Γ values in 2006Vo11, when available, assuming Γ0=Γ based on the observation of only the ground-state transitions. As no transitions other than those to the ground-state were observed, it is a reasonable approximation.

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Additional Gamma Comments:

E(level)E(gamma)Comments
  2628.81   278.84E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
   520.964E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  2899.59   996.2E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1303.38E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  2899.55E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3016.9  1420.7E(γ): From 140Pr ε Decay
I(γ): From 140Pr ε Decay
  3016.3E(γ): From 140Pr ε Decay
I(γ): From 140Pr ε Decay
  3120.34  3120.3E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3122.11   657.5E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
   772.50E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1525.85E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3168.3  1085E(γ): γ peak confounded with first Ge escape of intense 1596γ (1993Go23, (n,n’γ))
  3219.95  1623.71E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3255.70   739.94E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
   774.8E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3319.65   772.50E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1235.8E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1724.7E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3319.61E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3335.47   855.1E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
   985.63E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1227.71E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1252.12E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1739.4E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3360.24  1010.45E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1276.9E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
E(level)E(gamma)Comments
  3391.09  1307.73E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1794.93E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3394.92   982.89E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1045.11E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1287.03E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1311.56E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3424.6  1316.8E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  3436.54  1088.65E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1533.2E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3436.8E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3471.21  1568.1E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3471.15E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3473.75  1125.64E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3476.3    51.7E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  3491.2   944.0E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3491.2E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3492.23  1384.2E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  3512.3  1404.4E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  3567.5  1484.3E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3567.0E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3642.8  1739.4E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3642.7E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
M(γ): from γ(θ) and linear pol in (γ,γ’)
  3646.7  1743.31E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3646.6E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3648.23  1564.92E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  2052.07E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
E(level)E(gamma)Comments
  3657.64  1307.73E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1549.76E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1574.5E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3684.2  1220.5E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3684.1E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3708.60  1227.71E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  2112.30E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3708.1E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3714.3   202.0E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
   222.0E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  3723.54  1311.56E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3723.4E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3735.3  3735.2E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3767.97  1220.5E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1252.12E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1287.03E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1684.4E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  2171.82E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3792.72   893.7E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1276.9E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1311.56E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  2196.6E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3836.1  1753.1E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  2239.8E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3847.10   808.1E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1497.31E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1739.4E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  1763.6E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
E(level)E(gamma)Comments
  3853.2  2256.8E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3853.3E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3879.3  3879.2E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3910.93  2314.68E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3957.93  1493.6E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  2361.80E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  3984.20  1901.4E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  2387.90E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  4053  4053E(γ): From 140Ce(γ,γ’) dataset
  4164.0  2567.8E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  4163.5E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  4171.1  2576.1E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  4171.0E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  4173.6  4173.5E(γ): from (α,α’γ) and (γ,γ’)
  4279.9  2196.6E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  2683.6E(γ): From 140Ce(n,n’γ)
I(γ): From 140Ce(n,n’γ)
  4331  4331E(γ): From 140Ce(γ,γ’) dataset
  4354.9  4354.8E(γ): From 140Ce(γ,γ’) dataset
  4371  4371E(γ): From 140Ce(γ,γ’) dataset
  4388  4388E(γ): From 140Ce(γ,γ’) dataset
  4437  4437E(γ): From 140Ce(γ,γ’) dataset
  4514.9  4514.8E(γ): From (α,α’γ) and (γ,γ’) datasets
  4655  4655E(γ): From 140Ce(γ,γ’) dataset
  4787.8  4787.7E(γ): From (α,α’γ) and (γ,γ’) datasets
  4851.1  1136.8E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
E(level)E(gamma)Comments
  4875  4875E(γ): From 140Ce(γ,γ’) dataset
  4883  4883E(γ): From 140Ce(γ,γ’) dataset
  4904.6  1190.3E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  4951  4951E(γ): From 140Ce(γ,γ’) dataset
  5093.4   188.9E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  5102.1   250.9E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  5157.3  5157.2E(γ): From (α,α’γ) and (γ,γ’) datasets
  5190.2  5190.1E(γ): From (α,α’γ) and (γ,γ’) datasets
  5211.6  5211.5E(γ): From (α,α’γ) and (γ,γ’) datasets
  5245  5245E(γ): From 140Ce(γ,γ’) dataset
  5330  5330E(γ): From 140Ce(γ,γ’) dataset
  5337.3  5337.2E(γ): From (α,α’γ) and (γ,γ’) datasets
  5419.0   318.0E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  5470  5470E(γ): From 140Ce(γ,γ’) dataset
  5494  5494E(γ): From 140Ce(γ,γ’) dataset
  5548.4  5548.3E(γ): From (α,α’γ) and (γ,γ’) datasets
  5573.8  5573.7E(γ): From (α,α’γ) and (γ,γ’) datasets
  5624  5624E(γ): From 140Ce(γ,γ’) dataset
  5659.9  5659.8E(γ): From (α,α’γ) and (γ,γ’) datasets
M(γ): from γ(θ) and linear pol in (γ,γ’)
  5693.3   592.3E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  5721  5721E(γ): From 140Ce(γ,γ’) dataset
  5759  5759E(γ): From 140Ce(γ,γ’) dataset
  5809  5809E(γ): From 140Ce(γ,γ’) dataset
  5823  5823E(γ): From 140Ce(γ,γ’) dataset
  5928.6  5928.5E(γ): From (α,α’γ) and (γ,γ’) datasets
E(level)E(gamma)Comments
  5940  5940E(γ): From 140Ce(γ,γ’) dataset
  6029  6029E(γ): From 140Ce(γ,γ’) dataset
  6119.1  6119.0E(γ): From 140Ce(γ,γ’) dataset
  6130.6  6130.5E(γ): From 140Ce(γ,γ’) dataset
  6161.7  6161.6E(γ): From (α,α’γ) and (γ,γ’) datasets
  6226  6226E(γ): From 140Ce(γ,γ’) dataset
  6245  6245E(γ): From 140Ce(γ,γ’) dataset
  6255  6255E(γ): From 140Ce(γ,γ’) dataset
  6273.6  6273.4E(γ): From 140Ce(γ,γ’) dataset
  6295.3  6295.1E(γ): From 140Ce(γ,γ’) dataset
  6303.6  1202.6E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  6327.8  6327.6E(γ): From 140Ce(γ,γ’) dataset
  6343.3  6343.1E(γ): From 140Ce(γ,γ’) dataset
  6352.7  6352.5E(γ): From 140Ce(γ,γ’) dataset
  6397.2  6397.0E(γ): From 140Ce(γ,γ’) dataset
  6439.9  6439.7E(γ): From 140Ce(γ,γ’) dataset
  6449.9  6449.7E(γ): From 140Ce(γ,γ’) dataset
  6458.5  6458.3E(γ): From 140Ce(γ,γ’) dataset
  6484.8  6484.6E(γ): From 140Ce(γ,γ’) dataset
  6497.0  6496.8E(γ): From 140Ce(γ,γ’) dataset
  6535.8  6535.6E(γ): From 140Ce(γ,γ’) dataset
  6549.1  6548.9E(γ): From 140Ce(γ,γ’) dataset
  6574.9  6574.7E(γ): From 140Ce(γ,γ’) dataset
  6605.5  6605.3E(γ): From 140Ce(γ,γ’) dataset
  6616.2  6616.0E(γ): From 140Ce(γ,γ’) dataset
E(level)E(gamma)Comments
  6771.7  6771.5E(γ): From 140Ce(γ,γ’) dataset
  6781.9  6781.7E(γ): From 140Ce(γ,γ’) dataset
  6796.6   493.0E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  6841.8  6841.6E(γ): From 140Ce(γ,γ’) dataset
  6862.4  6862.2E(γ): From 140Ce(γ,γ’) dataset
  6889.2  1470.2E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  6905.9  6905.7E(γ): From 140Ce(γ,γ’) dataset
  6932.6  6932.4E(γ): From 140Ce(γ,γ’) dataset
  6960.4  6960.2E(γ): From 140Ce(γ,γ’) dataset
  7038.2   734.6E(γ): From 238U(12C,Fγ))
I(γ): From 238U(12C,Fγ))
  7206.0  7205.8E(γ): From 140Ce(γ,γ’) dataset
  7214.8  7214.6E(γ): From 140Ce(γ,γ’) dataset
  7341.5  7341.3E(γ): From 140Ce(γ,γ’) dataset
  7673.4  7673.2E(γ): From 140Ce(γ,γ’) dataset

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