ADOPTED LEVELS, GAMMAS for 208Bi

Author: M. J. Martin |  Citation: Nucl. Data Sheets 108,1583 (2007) |  Cutoff date: 1-Jun-2007 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-1400.6 keV 24S(n)= 6887 keV 3S(p)= 3707.2 keV 20Q(α)= 3051.0 keV 20
Reference: 2012WA38

References:
  A  206Pb(α,d)  B  207Pb(3He,d),(α,t)
  C  208Pb(p,nγ)  D  208Pb(48Ca,xγ)
  E  209Bi(p,d)  F  209Bi(d,t),(3He,α)
  G  209Bi(d,tγ)  H  210Bi(p,t): TARGET=9- ISOMER
  I  208Bi IT decay  J  208Po ε decay
  K  212At α decay (0.314 S)  L  212At α decay (0.119 S)
  M  207Pb(p,p’),(pol p,p’) IAR  N  207Pb(7Li,α2nγ)
  O  208Pb(π+,PI0)  P  208Pb(p,n),(p,NP’)
  Q  208Pb(3He,t),(3He,TP),(3He,TN)  R  209Bi(γ,n)
  S  209Bi(n,2nγ)  T  209Bi(17O,18OG)
  U  208Pb(6Li,6He) 








E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
      0.0ABC EFGHIJKL N   RSTU 5+ 3.68×10+5 y 4 
% ε = 100
     
     63.02 4 ABC EFGHIJKL N   RSTU 4+       63.00 6 
 
M1(+E2)
      0.0
5+
    510.28 7 A C EFGHI KL N   RSTU 6+ 118 ps 14     447.3 1 
   510.15 15 
     4.0 11 
   100
[E2]
E2(+M1)
     63.02
      0.0
4+
5+
    601.46 4  BC EFGH JKL N   RSTU 4+ 5.5 ps 21     538.41 6 
   601.49 6 
    51.8 11 
   100
M1
M1
     63.02
      0.0
4+
5+
    628.33 6 ABC EFGH   L N    ST  5+       26.91 11 
   118.2 2 
   565.23 8 
     0.41 5 
     4.2 12 
   100 7 

M1

    601.46
    510.28
     63.02
4+
6+
4+
    633.14 5 ABC EFGH JK  N   RST  3+       31.7 1 
   570.09 6 
   633.0 2 
     2.4 6 
   100.0 24 
     1.3 1 
M1(+E2)
M1

    601.46
     63.02
      0.0
4+
4+
5+
    650.57 10 A C EFGHI  L N   RST  7+ > 1.0 ns    140.08 12 
   650.60 16 
    52 16 
   100
M1
E2
    510.28
      0.0
6+
5+
    886.36 8 A C EFGH  KL N   RS   5+ 0.18 ps +8-6     823.25 14 
   886.4 2 
   100
    96 9 


     63.02
      0.0
4+
5+
    924.85 6   C EFGH JK       S   2+      291.77 6 
   861.83 7 
   925.11 13 ?
   100
    28.8 17 
    <0.14
M1+E2
[E2]

    633.14
     63.02
      0.0
3+
4+
5+
    936.27 6 ABC    H  K  N   RS   3+ > 1.7 ps    303.1 1 
   873.3 2 
   936.3 2 
     1.0 1 
   100 3 
     1.7 4 



    633.14
     63.02
      0.0
3+
4+
5+
    958.99 7   C EFGH  KL N   R    4+      325.74 9 
   330.6 2 
   896.0 2 
   959.0 2 
    11.6 7 
     4.2 9 
   100 6 
    36 3 




    633.14
    628.33
     63.02
      0.0
3+
5+
4+
5+
   1033.26 6 ABC EF    K  N   RS   4+ 0.72 ps +26-17     146.6 2 
   400.0 2 
   431.4 2 
   970.25 14 
  1033.31 14 
     1.0 2 
     2.0 3 
    <0.3
    41.5 8 
   100.0 25 
M1




    886.36
    633.14
    601.46
     63.02
      0.0
5+
3+
4+
4+
5+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   1069.11 6   C EFG   K  N   RS   3+ 0.44 ps +21-12     110.0 2 
   435.7 2 
   467.37 15 
  1006.23 15 
  1069.3 2 
     0.6 2 
     9.0 7 
     9.0 7 
   100 6 
     2.8 4 
M1




    958.99
    633.14
    601.46
     63.02
      0.0
4+
3+
4+
4+
5+
   1095.06 14   C EFGH   L N   R    6+ 0.13 ps +5-4     207.8?
  1094.9 2 
 
 


    886.36
      0.0
5+
5+
   1469.47 11 A C  F       N    S   4+,5+,6+      435.9 2 
   841.0 3 
   959.0 2 
    18 4 
     9 6 
   100 14 



   1033.26
    628.33
    510.28
4+
5+
6+
   1529.40 7 A C EF                3+,4+      496.1 1 
   592.9 2 
   896.2 2 
   927.97 15 
  1466.4 2 
  1529.4 3 
   100 4 
    17 6 
    44 8 
    98 3 
    59 4 
    28 4 






   1033.26
    936.27
    633.14
    601.46
     63.02
      0.0
4+
3+
3+
4+
4+
5+
   1539.39 7   C          N        2+,3+ > 1.2 ps    470.06 15 
   602.88 15 
   614.22 15 
   906.32 15 
   937.8 2 
  1476.5 2 
     3.0 2 
    20.3 12 
     7.4 5 
   100.0 6 
     3.0 2 
    12.0 8 






   1069.11
    936.27
    924.85
    633.14
    601.46
     63.02
3+
3+
2+
3+
4+
4+
   1563.45 9  BC                   3+,4+      494.1 3 
   529.9 2 
   627.13 13 
   677.1 2 
   935.2 2 
     1.7 10 
    25 8 
   100 20 
     3 1 
    67 14 





   1069.11
   1033.26
    936.27
    886.36
    628.33
3+
4+
3+
5+
5+
   1571.1 4 A  DEF HI         S   10- 2.58 ms 4 
% IT = 100
   920.5 3 
 
E3(+M4)
    650.57
7+
   1603 5      F                       
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   1624.68 11 ABC EF                6-      530.4 4 
   738.2 2 
   973.9 2 
   996.2 2 
     4.5 8 
    14 1 
    59 12 
   100 20 




   1095.06
    886.36
    650.57
    628.33
6+
5+
7+
5+
   1657.47 22   C EF H              8-     1006.9 2 
 

    650.57
7+
   1666.58 16 ABC                   7-     1015.9 2 
  1156.4 2 
    70 40 
   100 40 


    650.57
    510.28
7+
6+
   1703.35 7   C EF                5-      233.7 3 
   669.9 2 
   744.2 2 
  1074.9 2 
  1640.5 1 
  1703.2 2 
     0.30 10 
     6 4 
    26 3 
     9 2 
   100 4 
    32 2 






   1469.47
   1033.26
    958.99
    628.33
     63.02
      0.0
4+,5+,6+
4+
4+
5+
4+
5+
   1715.66 19 ABC EF H              6-,7-     1064.9 2 
  1205.8 3 
   100 50 
    80 40 


    650.57
    510.28
7+
6+
   1716.17 25 ABC EF H              6-,7-      621.1 2 
 

   1095.06
6+
   1731 5      F                       
   1786.1 15     EF H              9-        
   1802.09 8 ABC            PQ     1+      262.50 15 
   865.84 15 
   877.2 2 
  1169.07 15 
   100 5 
    16.3 10 
    17.3 10 
     6.8 4 




   1539.39
    936.27
    924.85
    633.14
2+,3+
3+
2+
3+
   1824.45 16   C                        354.9 2 
  1761.5 2 
   100
    87 11 


   1469.47
     63.02
4+,5+,6+
4+
   1836 4 A                     (5+,6+,7+)        
   1839.03 9   C EF                4-      135.6 2 
   805.6 2 
   879.9 2 
   902.9 3 
   952.5 3 
  1205.9 2 
  1210.9 2 
  1775.7 3 
    51 13 
    13 8 
    18 4 
    44 3 
     6.6 22 
    56 10 
    10 8 
   100 6 
M1







   1703.35
   1033.26
    958.99
    936.27
    886.36
    633.14
    628.33
     63.02
5-
4+
4+
3+
5+
3+
5+
4+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   1870.77 10   C EF                3+,4+      307.0 2 
   331.0 2 
   837.7 2 
   934.7 2 
   946.0 2 
     7.5 18 
     5.5 17 
   100 7 
    69 12 
    15 3 





   1563.45
   1539.39
   1033.26
    936.27
    924.85
3+,4+
2+,3+
4+
3+
2+
   1882.14 11 ABC                   2+,3,4,5+      412.5 2 
   812.9 2 
   849.0 2 
   923.3 3 
   946.0 2 
    25 4 
    18.2 11 
     3.6 18 
     6 2 
   100 10 





   1469.47
   1069.11
   1033.26
    958.99
    936.27
4+,5+,6+
3+
4+
4+
3+
   1919.97 7   C EF                3-       80.7 2 
   390.2 2 
   886.7 2 
   960.8 2 
   983.7 2 
   995.1 2 
  1287.0 3 
  1318.6 2 
     5 2 
     7.8 7 
    <8
     9.9 11 
    50 3 
   100 7 
     5.4 7 
    31 5 
M1







   1839.03
   1529.40
   1033.26
    958.99
    936.27
    924.85
    633.14
    601.46
4-
3+,4+
4+
4+
3+
2+
3+
4+
   2077.66 8   C                   0-,1-,2-      275.26 15 
  1141.4 2 
  1152.84 10 
   100 6 
     1.0 2 
     0.8 2 
E1


   1802.09
    936.27
    924.85
1+
3+
2+
   2126.90 8  BC                   2+,3,4+      255.7 2 
   597.2 2 
  1057.5 3 
  1093.4 8 
  1190.77 12 
  1202.1 2 
  1493.8 2 
    13.7 11 
    13 2 
     3.5 7 
     4.4 8 
   100 3 
    12.6 8 
    13.8 11 







   1870.77
   1529.40
   1069.11
   1033.26
    936.27
    924.85
    633.14
3+,4+
3+,4+
3+
4+
3+
2+
3+
   2132 7        H                     
   2160 7        H                     
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   2179.42 20   C                   4+,5,6,7+     1083.8 4 
  1293.2 2 
 
 


   1095.06
    886.36
6+
5+
   2180.04 21   C                   4+,5,6,7+     1084.9 2 
  2180.3 4 
    32 7 
   100


   1095.06
      0.0
6+
5+
   2202.89 12   C                   1-,2-,3-      125.3 2 
   663.3 2 
   100
    51 12 
M1

   2077.66
   1539.39
0-,1-,2-
2+,3+
   2246 5 A                            
   2308.08 9   C                   2+,3,4      388.1 1 
   838.1 3 
  1239.09 12 
     6.2 8 
     4.2 12 
   100 3 



   1919.97
   1469.47
   1069.11
3-
4+,5+,6+
3+
   2340.1 4   C EF H              7+     1829.8 4 
 

    510.28
6+
   2358.47 20   C                   2+,3,4,5+     1725.2 2 
  1758.1 6 
   100
    16 8 


    633.14
    601.46
3+
4+
   2383.86 19   C EF                4+,5+     1750 1 
  1754.8 6 
  1782.5 2 
    53 3 
    16 7 
   100 48 



    633.14
    628.33
    601.46
3+
5+
4+
   2385.97 15   C EF                4+,5+      856.7 3 
  1753.0 3 
  1757.6 2 
  1784.1 4 
     5 5 
    50 50 
   100 9 
  <220




   1529.40
    633.14
    628.33
    601.46
3+,4+
3+
5+
4+
   2404.2 5   C                       1771.1 5 
 

    633.14
3+
   2407 5 A      H              9-        
   2409.10 18 A C EF                6+     1780.4 3 
  1807.5 3 
  1899.3 3 
 
 
 



    628.33
    601.46
    510.28
5+
4+
6+
   2415.72 12   C                   1+,2,3,4-      337.9 2 
 

   2077.66
0-,1-,2-
   2426.7 4  B DEF H              11-      855.7 2 
 

   1571.1
10-
   2436.87 19   C                        873.3 2 
 

   1563.45
3+,4+
   2457.38 10   C EF                3+      918.0 2 
  1388.6
  1532.6 2 
  1824.13 14 
  1856.0 2 
    27 2 
     6.6 17 
    50 4 
   100 8 
    73 6 





   1539.39
   1069.11
    924.85
    633.14
    601.46
2+,3+
3+
2+
3+
4+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   2470 5 A      H              9-        
   2478.49 12   C                   2,3,4      275.3 2 
   558.5 2 
  1845.5 2 
 
   100 7 
    20.5 17 



   2202.89
   1919.97
    633.14
1-,2-,3-
3-
3+
   2495.53 11   C                   4,5+      293.5 5 
   656.2 4 
   792.1 2 
  1559.2 2 
  1609.1 4 
  1862.5 2 
  1894.0 3 
    25 2 
    62 5 
    60 5 
    48 4 
    35 12 
   100 8 
    66 6 







   2202.89
   1839.03
   1703.35
    936.27
    886.36
    633.14
    601.46
1-,2-,3-
4-
5-
3+
5+
3+
4+
   2501.56 11 A C EF                2+     1432.2 2 
  1576.7 2 
  1868.3 2 
    18 6 
    88 5 
   100 7 



   1069.11
    924.85
    633.14
3+
2+
3+
   2513.51 10 A C                   2+,3,4,5+     1444.2 2 
  1480.0 2 
  1554.5 2 
  1577.5 2 
  1880.5 4 
  1912.2 2 
    47 4 
    18.5 14 
   100 6 
    13.7 24 
    41 4 
    42 4 






   1069.11
   1033.26
    958.99
    936.27
    633.14
    601.46
3+
4+
4+
3+
3+
4+
   2544.83 14   C                        467.21 12 
 

   2077.66
0-,1-,2-
   2554 5        H                     
   2556.45 9   C                   2,3,4      636.2 2 
  1487.4 1 
  1620.0 3 
  1923.3 2 
    42 4 
   100 6 
    23.7 15 
    86 6 




   1919.97
   1069.11
    936.27
    633.14
3-
3+
3+
3+
   2564.79 14   C                   3+      149.4 4 
  1936.6 2 
  1963.4 3 
     3.9 15 
   100 11 
   <17



   2415.72
    628.33
    601.46
1+,2,3,4-
5+
4+
   2570.31 13   C                   1,2,3      154.6 2 
   492.6 2 
  1645.6 2 
     6 5 
    72 10 
   100 7 



   2415.72
   2077.66
    924.85
1+,2,3,4-
0-,1-,2-
2+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   2586.58 11   C                   3+,4,5+     1627.4 2 
  1700.5 2 
  1953.4 2 
  1984.9 3 
  2523.5 3 
    59 6 
    71 6 
    64 6 
    21 4 
   100 8 





    958.99
    886.36
    633.14
    601.46
     63.02
4+
5+
3+
4+
4+
   2605 6 A                            
   2612.63 14   C                   4+,5+     1653.6 2 
  1676.4 3 
  1979 1 
  2011.3 3 
  2102.3 3 
    45 3 
    13 3 
   <30
   100 8 
    37 3 





    958.99
    936.27
    633.14
    601.46
    510.28
4+
3+
3+
4+
6+
   2631.02 16   C                   5,6,7-      928.1 3 
  1006.3 2 
  1535.8 2 
    60 20 
 
   100 11 



   1703.35
   1624.68
   1095.06
5-
6-
6+
   2636.34 14 A C                   2+,3,4,5+     1677.3 2 
  2003.2 3 
  2034.9 2 
    78 9 
    92 8 
   100 8 



    958.99
    633.14
    601.46
4+
3+
4+
   2657.29 24   C                        454.4 2 
 

   2202.89
1-,2-,3-
   2660.7 4   C EF H              8+     2010.1 3 
 

    650.57
7+
   2679.42 11   C  F                1+,2,3      601.3 2 
  1610.4 2 
  1754.8 2 
  2046.4 2 
 
   100 5 
    39 9 
 




   2077.66
   1069.11
    924.85
    633.14
0-,1-,2-
3+
2+
3+
   2693.78 12   C  F                2+,3,4,5+      149.4 4 
  1624.8 2 
  1660.9 4 
  1757.4 3 
  2060.3 3 
  2630.6 2 
 
    42 3 
     4.6 7 
     0.29 3 
    45 3 
   100 8 






   2544.83
   1069.11
   1033.26
    936.27
    633.14
     63.02

3+
4+
3+
3+
4+
   2718.55 12   C EF                2,3,4      798.42 15 
   848.7 4 
  1189.7 3 
  1649.2 3 
  1782.2 2 
   100 7 
    42 3 
     3.5 9 
    11.0 9 
     0.12 2 





   1919.97
   1870.77
   1529.40
   1069.11
    936.27
3-
3+,4+
3+,4+
3+
3+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   2719 6 A                     (6-)        
   2733.04 14   C                        254.4 2 
   530.2 2 
  1808.3 2 
 
 
 



   2478.49
   2202.89
    924.85
2,3,4
1-,2-,3-
2+
   2739.52 12   C                   3,4,5     1114.6 2 
  1780.4 3 
  1814.9 2 
  1853.2 2 
    64 7 
    46 10 
   100 12 
    82 9 




   1624.68
    958.99
    924.85
    886.36
6-
4+
2+
5+
   2804 6 A                     (10-)        
   2826 6 A                     (6-,7-,8-)        
   2838.89 11   C                   1+,2,3      268.8 3 
   282.2 2 
   423.1 1 
   761.3 2 
  1914.4 2 
    15.7 14 
    13.2 12 
    39 4 
   100 4 
    20 2 





   2570.31
   2556.45
   2415.72
   2077.66
    924.85
1,2,3
2,3,4
1+,2,3,4-
0-,1-,2-
2+
   2843 7        H                     
   2843.36 22   C                        765.7 2 
 

   2077.66
0-,1-,2-
   2869.57 11   C                   3+,4,5,6+     2806.50 16 
  2869.57 15 
    28.0 15 
   100 5 


     63.02
      0.0
4+
5+
   2879.66 15   C                   2+,3,4,5+     1340.1 2 
  1846.6 2 
    59 10 
   100 13 


   1539.39
   1033.26
2+,3+
4+
   2881.30 20 A C                   3+,4,5+      294.6 3 
  1812.1 5 
  1994.6 6 
  2818.5 3 
 
   100 14 
    51 7 
 




   2586.58
   1069.11
    886.36
     63.02
3+,4,5+
3+
5+
4+
   2884.07 16 A C EF                1+      382.5 2 
  1815.1 3 
  1959.1 3 
    71.0 7 
   100 21 
    71 29 



   2501.56
   1069.11
    924.85
2+
3+
2+
   2886.77 12 ABC                        330.5 2 
   578.7 2 
  2285.0 2 
 
    99 8 
   100 8 



   2556.45
   2308.08
    601.46
2,3,4
2+,3,4
4+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   2888.47 16 ABC                       2888.45 16 
 

      0.0
5+
   2893.76 13 A C E          PQ     2-      973.8 2 
  1091.6 2 
  1364.1 4 
  1957.6 2 
   100 60 
     8 7 
     8 7 
    13 13 




   1919.97
   1802.09
   1529.40
    936.27
3-
1+
3+,4+
3+
   2903.58 16   C                   0+,1,2,3+     1101.6 2 
  1978.9 4 
   100
    21 4 


   1802.09
    924.85
1+
2+
   2912 10 ?     F                       
   2932.84 13   C                   3+,4,5+     1996.4 2 
  2046.4 2 
  2331.6 2 
    36 2 
   100 7 
    19.7 16 



    936.27
    886.36
    601.46
3+
5+
4+
   2942.88 16  BC                   2+     2879.84 15 
 

     63.02
4+
   2950.96 11   C                   2+,3      873.3 2 
  1411.3 3 
  1992.3 2 
  2026.1 2 
  2317.6 2 
 
    32 2 
    22 2 
   100 8 
    26 8 





   2077.66
   1539.39
    958.99
    924.85
    633.14
0-,1-,2-
2+,3+
4+
2+
3+
   3049 3     E                        
   3069.34 12  BC EF                2+      632.2 3 
  1267.6 2 
  1529.9 2 
  1539.7 3 
  2036.2 3 
  2132.7 3 
 
   100 6 
    81 11 
    22 8 
    29 7 
     0.39 7 






   2436.87
   1802.09
   1539.39
   1529.40
   1033.26
    936.27

1+
2+,3+
3+,4+
4+
3+
   3091 5 A      H              (8)-        
   3114 3     E                 3+,4+,5+,6+        
   3141 3     E                 3+,4+,5+,6+        
   3154 5        H              -        
   3154.98 22   C                        846.9 2 
 

   2308.08
2+,3,4
   3165.93 14   C                   1+,2,3,4+      262.5 2 
   601.4 2 
   664.0 2 
  1626.4 3 
 
 
 
 




   2903.58
   2564.79
   2501.56
   1539.39
0+,1,2,3+
3+
2+
2+,3+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   3171 5 AB             PQ     1+        
   3201.1 4    D                  (12+)      774.4 3 
  1629.9 3 
   100
    57


   2426.7
   1571.1
11-
10-
   3207 7 A                            
   3212 3     E                        
   3240 3     E                        
   3246 7 A                            
   3257 5  B                    1+,2+        
   3271 3     EF                +        
   3286.38 9  BC                   2+     1159.35 12 
  1757.2 2 
  2217.2 3 
  2253.1 2 
  2361.5 2 
  2652.8 4 
  2685.2 2 
    77 6 
    41 7 
    14 2 
    64 6 
    91 11 
    64 11 
   100 8 







   2126.90
   1529.40
   1069.11
   1033.26
    924.85
    633.14
    601.46
2+,3,4+
3+,4+
3+
4+
2+
3+
4+
   3300 7 A      H              -        
   3318 3     EF                +        
   3327 3 A   E                 4-,5-        
   3332 7 A      H                     
   3347 3     E                 4-,5-        
   3351.34 20   C                        738.8 4 
   935.7 3 
  1821.8 3 
 
 
 



   2612.63
   2415.72
   1529.40
4+,5+
1+,2,3,4-
3+,4+
   3362 3     EF                +        
   3379 7 A                            
   3387 3     EF                       
   3390.9 4   C                        440.2 6 
   496 2 
  2454.6 4 
    24.0 10 
   <10
   100 6 



   2950.96
   2893.76
    936.27
2+,3
2-
3+
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   3407 5  B                    1+,2+        
   3411 10        H                     
   3412 3     EF                +        
   3425.08 12   C                        538.2 2 
   545.6 4 
  1117.2 3 
  2488.9 2 
  2791.8 2 
 
 
 
 
 





   2886.77
   2879.66
   2308.08
    936.27
    633.14

2+,3,4,5+
2+,3,4
3+
3+
   3427.2 4   C                        862.4 3 
 

   2564.79
3+
   3449.4 5    D           P      (13+)      248.4 3 
 
M1
   3201.1
(12+)
   3453 5 A      H              -        
   3457 5 AB                    1+,2+        
   3461 3     EF                +        
   3499.7 8 A  D                  (11+)     1928.6 10 
 

   1571.1
10-
   3521 7        H              9-        
   3524 3  B  EF                +        
   3532 5  B                           
   3541 3     E                 +        
   3547 7 A                            
   3563 5        H              -        
   3565 3     EF                +        
   3600.6 5 A  D                  (12+)      101S
  1173.9 4 
 
 


   3499.7
   2426.7
(11+)
11-
   3611 3  B  E                 1+,2+        
   3631 7        H                     
   3662 3     EF                       
   3688 3     EF                       
   3718 5     EF                +        
   3742 3     E                        
   3751 7        H                     
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   3766 3     E                        
   3767 10        H                     
   3795 8 A                            
   3851 5        H                     
   3854 8 A                            
   3863 25                PQ     1+        
   3886 3     E                 (+)        
   3905 8 A                            
   3906 10        H                     
   3967 8 A                            
   4013 10        H                     
   4015 4     E                 +        
   4015 8 A                            
   4043 25                 Q     1+        
   4049 8 A                            
   4087 10        H                     
   4137 10        H                     
   4156 9 A                            
   4159.1 5    D                  (13+)      558.8 8 
   709.7 3 
   957.8 5 
  2588 1 
     2.7
   100
    35
     5.4




   3600.6
   3449.4
   3201.1
   1571.1
(12+)
(13+)
(12+)
10-
   4183 4     E                        
   4236 9 A                            
   4238 5        H                     
   4284 9 A                            
   4291.0 5    D                  (13)      690.3 4 
   841.7 4 
    70
   100


   3600.6
   3449.4
(12+)
(13+)
   4357 9 A                            
   4399 9 A                            
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
   4448 9 A                            
   4484.3 5    D                  (14+)      325.2 3 
  1034.9 5 
   100
    14


   4159.1
   3449.4
(13+)
(13+)
   4543 4     E                 +        
   4556 4     E                 +        
   4587 4     E                 +        
   4617 4     E          PQ     1+        
   4635.3 5    D                  (15+)      151.0 5 
   475.9 6 
  1185.9 4 
   100
   100
   100



   4484.3
   4159.1
   3449.4
(14+)
(13+)
(13+)
   4652 10 A                            
   4697?A                            
   4836.2 5 A  D                  (14-)      545.2 4 
   677.2 4 
  1336?
  1386.7 4 
   100
    38
    <8
    62




   4291.0
   4159.1
   3499.7
   3449.4
(13)
(13+)
(11+)
(13+)
   4885 10 A                            
   5008 10 A                            
   5067 10 A                            
   5463.0 6 A  D                  (15-)      626.8 4 
  2262.0 8 
   100
    20


   4836.2
   3201.1
(14-)
(12+)
   5552 11 ?A                            
   5626.6 6    D                  (16-)      163.7 5 
   990.8 7 
  2178 1 
   100
    36
     9.1



   5463.0
   4635.3
   3449.4
(15-)
(15+)
(13+)
      5.9E+3 2                PQ     1+        
      7.13E+3 10                P             
      8.19E+3 10                PQ     1+        
  ≈9000   D                  ≈ 40 ns      
      9.16E+3 10                P      (1)+        
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
      9.8E+3 2                 Q     1+        
     10.38E+3 10                P      (1)+        
  15165 6             M  PQ     0+ 231 keV 6       
     15.6E+3 2                PQ     1+        
  17780            M         3- 166 keV 47       
  18363            M         5- 234 keV 19       
  18640            M         4- 242 keV 18       
  18874            M         5- 195 keV 51       
  19085            M         4- 245 keV 67       
  19126            M         5- 281 keV 70       
  19161            M         6- 285 keV 85       
  19203            M         7- 277 keV 67       
  19216            M         3- 339 keV 54       
  19290            M         4- 261 keV 61       
  19345            M         5- 306 keV 56       
  19371            M         6- 226 keV 42       
  19395            M         2- 336 keV 72       
  19420            M         3- 312 keV 42       
  19462            M         5- 289 keV 51       
  19524            M         4- 319 keV 51       
  19646            M         6- 329 keV 78       
  19776            M         7+        
  19863            M         3- 301 keV 30       
  20026            M         7+        
  20139            M         2- 247 keV 12       
  20203            M         3- 262 keV 25       
  20292            M         2- 318 keV 16       
  20410            M         3- 272 keV 10       
  20445            M         1- 285 keV 19       
  20539            M         2- 290 keV 15       
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
  20647            M         5- 225 keV 51       
  20677            M         1- 291 keV 38       
  20860            M         5- 328 keV 76       
  20943            M         (2-) 298 keV 32       
  21039            M         3- 281 keV 20       
  21089            M         2- 252 keV 78       
     21.1E+3 80                PQ     0-,1-,2- 10 MeV 3       
  21112            M         1- 268 keV 19       
  21134            M         3-        
  21175            M         4-        
  21252            M         2-        
  21428            M         1-        
  21479            M         1-        
     22.90E+3 20                P      (1)+ ≈ 670 keV      
  23500               P      0-,1-,2- 2.9 MeV      
     24.60E+3 20                P      (1)+ 1.2 MeV      
  28000               P      (2)+ 14 MeV      

E(level): From a least-squares fit to the adopted Eγ. Energies for levels not deexcited by gammas are averages from all reactions populating the level. Note that values from (p,d), from (3He,d),(α,t), from (d,t),(3He,α) and from (p,t) have been adjusted as noted in the source datasets. Above about 2500, the association of levels seen in the different reactions, except where Jπ information is known, is uncertain. The evaluator has chosen to show separate levels in such cases. It is possible that some of these levels that overlap in energy are the same. For E(level)>15.6 MeV, energies are from 207Pb(p,p’),(pol p,p’). These levels are probable IAR of 208Pb levels. For data on the Gamow-Teller resonance at 15.6 MeV, and on resonances above 21 MeV, see 208Pb(3He,t),(3He,tp),(3He,tn), 208Pb(p,n),(p,np’), and 208Pb(π+,π0)

Jπ(level): 2006Bo08, in (p,nγ), compare the experimental energies with a shell-model calculation (see 2006Bo08 for details). Their calculation gives agreement with the Jπ and configuration assignments for the levels seen previously in transfer reactions, and their observed γ branchings are consistent with the assignments. In addition, the authors propose assignments for five of the six members of the π2f7/2ν2f5/2-1 multiplet, and three of the four members of the π2f7/2ν3p3/2-1 multiplet. They suggest that the 1824 level could Be the 6+ member of the first of these multiplets, or the 5+ member of the second multiplet. Their calculations confirm the 1802 level as the 1+ member of the f7/2-f5/2 multiplet. These assignments are given in comments. Assignments for E(level)>15 MeV are from σ and analyzing power in 207Pb(p,p’),(pol p,p’) IAR

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Additional Gamma Data:















E(level)
(keV)		Jπ(level)T1/2(level)E(γ)
(keV)		MultipolarityMixing
Ratio		Conversion
Coefficient		Additional Data
     63.02 4+       63.00 6 M1(+E2)0.14 LT7.8α=7.8 5
    510.28 6+ 118 ps 14     447.3 1 [E2] 0.0410B(E2)(W.u.)=0.10 3, α=0.0410
6+ 118 ps 14     510.15 15 E2(+M1)1.3 GT0.044B(E2)(W.u.)=1.5 5, α=0.044 15
    601.46 4+ 5.5 ps 21     538.41 6 M1 0.0964α=0.0964
4+ 5.5 ps 21     601.49 6 M1 0.0720B(M1)(W.u.)=0.008 +6-4, α=0.0720
    633.14 3+       31.7 1 M1(+E2)0.10 LT62α=62 7
3+      570.09 6 M1 0.0829α=0.0829
    650.57 7+ > 1.0 ns    140.08 12 M1 4.09B(M1)(W.u.)≤0.0012, α=4.09
7+ > 1.0 ns    650.60 16 E2 0.0169B(E2)(W.u.)≤0.017, α=0.0169
    886.36 5+ 0.18 ps +8-6     823.25 14   B(E2)(W.u.)≤77, B(M1)(W.u.)≤0.15
5+ 0.18 ps +8-6     886.4 2   B(E2)(W.u.)≤36, B(M1)(W.u.)≤0.08
    924.85 2+      291.77 6 M1+E20.57 260.41α=0.41
2+      861.83 7 [E2] 0.0095α=0.0095
   1033.26 4+ 0.72 ps +26-17     970.25 14   B(E2)(W.u.)≤2.4, B(M1)(W.u.)≤0.0064
4+ 0.72 ps +26-17    1033.31 14   B(E2)(W.u.)≤4.3, B(M1)(W.u.)≤0.013
   1069.11 3+ 0.44 ps +21-12    1069.3 2   B(E2)(W.u.)=0.25 +11-8
   1095.06 6+ 0.13 ps +5-4    1094.9 2   B(E2)(W.u.)≤55, B(M1)(W.u.)≤0.17
   1571.1 10- 2.58 ms 4 
% IT = 100
   920.5 3 E3(+M4)0.05 LT0.0200B(E3)(W.u.)=3.21E-4 5, α=0.0200 2
   2077.66 0-,1-,2-      275.26 15 E1 0.0372α=0.0372
   3449.4 (13+)      248.4 3 M1 0.8α=0.8 2

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
      0.05+ 3.68×10+5 y 4 
% ε = 100
Q=-0.51 7, μ=+4.578 13
Isotope shift measured (1983LaZZ, 2000Pe30, 2007Me09).
     63.024+   configuration=π1h9/2ν3p1/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
    510.286+ 118 ps 14  configuration=π1h9/2ν2f5/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
    601.464+ 5.5 ps 21  configuration=π1h9/2ν2f5/2-1 + π2f7/2ν3p1/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
    628.335+   configuration=π1h9/2ν2f5/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
    633.143+   configuration=π1h9/2ν2f5/2-1 + π2f7/2ν3p1/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
    650.577+ > 1.0 ns configuration=π1h9/2ν2f5/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
    886.365+ 0.18 ps +8-6  configuration=π1h9/2ν3p3/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
    924.852+   configuration=π1h9/2ν2f5/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
    936.273+ > 1.7 ps configuration=π2f7/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
    958.994+   configuration=π1h9/2ν3p3/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   1033.264+ 0.72 ps +26-17  configuration=π2f7/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
   1069.113+ 0.44 ps +21-12  configuration=π1h9/2ν3p3/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   1095.066+ 0.13 ps +5-4  configuration=π1h9/2ν3p3/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   1469.474+,5+,6+   configuration=π2f7/2ν2f5/2-1.
   1571.110- 2.58 ms 4 
% IT = 100
μ=2.672 14 (1974Hu11,1985No09,2005St24)
configuration=π1h9/2ν1i13/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   1624.686-   configuration=π1i13/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
   1657.478-   configuration=π1h9/2ν1i13/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   1666.587-   configuration=π1i13/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
   1703.355-   configuration=π1h9/2ν1i13/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available. J(1703) and J(1839) are reversed from the values suggested by 1971Al05 in 209Bi(d,t).
   1715.666-,7-   configuration=π1h9/2ν1i13/2-1.
E(level): Weighted average from (p,nγ) and ε decay. Weighted average from (p,nγ), (n,2nγ), and IT decay. Doublet in 209Bi(p,d), 209Bi(d,t), and 207Pb(3He,d),(α,t) on the basis of strength. No broadening observed in (p,d), thus the levels are <3 keV apart. Doublet resolved in (p,nγ).
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   1716.176-,7-   configuration=π1h9/2ν1i13/2-1.
E(level): Weighted average from (p,nγ) and ε decay. Weighted average from (p,nγ), (n,2nγ), and IT decay. Doublet in 209Bi(p,d), 209Bi(d,t), and 207Pb(3He,d),(α,t) on the basis of strength. No broadening observed in (p,d), thus the levels are <3 keV apart. Doublet resolved in (p,nγ).
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   1786.19-   configuration: based on L-transfer in 209Bi(p,d). However, observation that L=0 in 210Bi(9-)(p,t), with configuration=π1h9/2ν2g9/2-1 for the 210Bi target requires the presence of core-excited components in the wavefunction (1979Er11).
   1802.091+   configuration=π2f7/2ν2f5/2-1.
Jπ(level): From L(3He,t)=0 at E=200 and 450 MeV, and the assumption that possible 0+ anti-analog states below the analog of the 208Pb g.s. will not Be populated at the bombarding energies used (1991Ja04).
   1839.034-   configuration=π1h9/2ν1i13/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available. J(1703) and J(1839) are reversed from the values suggested by 1971Al05 in 209Bi(d,t).
E(level)Jπ(level)T1/2(level)Comments
   1870.773+,4+   configuration=π2f7/2ν3p3/2-1.
   1919.973-   configuration=π1h9/2ν1i13/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   2077.660-,1-,2-   Jπ(level): 2006Bo08 in (p,nγ) suggest that the 2078 level is a two-particle two-hole excitation and that the lowest such state is expected to have Jπ=1-. The 2208 level deexcites via an E1 γ to 1+ and so has Jπ=0-, 1-, or 2-. The 1141γ to 3+ suggests Jπ=2-; however, as pointed out by the authors, the branching of this transition is small, and is not inconsistent with mult=M2, allowing Jπ=1-. The evaluator notes that the 1141γ could also Be E3, in which case Jπ=0- is also not ruled out. 2006Bo08 further suggest that the states at 2203, 2416, and 2478 are probably also two-particle two-hole states. See 2006Bo08 for a discussion of these configurations.
   2126.902+,3,4+   configuration=π2f7/2ν3p3/2-1.
   2202.891-,2-,3-   Jπ(level): 2006Bo08 in (p,nγ) suggest that the 2078 level is a two-particle two-hole excitation and that the lowest such state is expected to have Jπ=1-. The 2208 level deexcites via an E1 γ to 1+ and so has Jπ=0-, 1-, or 2-. The 1141γ to 3+ suggests Jπ=2-; however, as pointed out by the authors, the branching of this transition is small, and is not inconsistent with mult=M2, allowing Jπ=1-. The evaluator notes that the 1141γ could also Be E3, in which case Jπ=0- is also not ruled out. 2006Bo08 further suggest that the states at 2203, 2416, and 2478 are probably also two-particle two-hole states. See 2006Bo08 for a discussion of these configurations.
   2340.17+   configuration=π1h9/2ν2f7/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   2383.864+,5+   configuration=π1h9/2ν2f7/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available. In (p,d) a level at 2385.3 22 is proposed as a 4+, 5+ doublet. The 2383.8 and 2386.0 levels both deexcite to levels with Jπ=3+ and 5+. The evaluator assigns these levels as the components of the doublet.
   2385.974+,5+   configuration=π1h9/2ν2f7/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available. In (p,d) a level at 2385.3 22 is proposed as a 4+, 5+ doublet. The 2383.8 and 2386.0 levels both deexcite to levels with Jπ=3+ and 5+. The evaluator assigns these levels as the components of the doublet.
   24079-   configuration: from 206Pb(α,d) and 210Bi(9-)(p,t).
   2409.106+   configuration=π1h9/2ν2f7/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   2415.721+,2,3,4-   Jπ(level): 2006Bo08 in (p,nγ) suggest that the 2078 level is a two-particle two-hole excitation and that the lowest such state is expected to have Jπ=1-. The 2208 level deexcites via an E1 γ to 1+ and so has Jπ=0-, 1-, or 2-. The 1141γ to 3+ suggests Jπ=2-; however, as pointed out by the authors, the branching of this transition is small, and is not inconsistent with mult=M2, allowing Jπ=1-. The evaluator notes that the 1141γ could also Be E3, in which case Jπ=0- is also not ruled out. 2006Bo08 further suggest that the states at 2203, 2416, and 2478 are probably also two-particle two-hole states. See 2006Bo08 for a discussion of these configurations.
   2426.711-   configuration=π1h9/2ν1i13/2-1.
   2457.383+   configuration=π1h9/2ν2f7/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   24709-   configuration: from 206Pb(α,d) and 210Bi(9-)(p,t).
   2501.562+   configuration=π1h9/2ν2f7/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   2660.78+   configuration=π1h9/2ν2f7/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   2718.552,3,4   Jπ(level): Suggested by 1971Al05 in (d,t) as possible Jπ=2- member of the configuration=π1h9/2ν1i13/2-1 multiplet; however, the level is weakly populated and no L values was determined. The 2- member of that multiplet is now known to Be at 2894.
   2804(10-)   configuration=206Pb(0+)π1h9/2ν1i11/2.
Jπ(level): From 1977Da05 in 206Pb(α,d) based on similarity of Q value, L value and σ with levels in 206Bi and 210Bi; and assumption that the levels are two-particle+(206Pb core) states with J(π)+J(ν)=J(max).
   2884.071+   configuration=π1h9/2ν2f7/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   2886.77   Jπ(level): 1971Al05 report Jπ=3+ with configuration=π2f5/2ν3p1/2-1 \ for a peak at 2887 5. This could correspond to either the 2886.6 level or the 2888.4 level.
   2888.47   Jπ(level): 1971Al05 report Jπ=3+ with configuration=π2f5/2ν3p1/2-1 \ for a peak at 2887 5. This could correspond to either the 2886.6 level or the 2888.4 level.
   2893.762-   configuration=π1h9/2ν1i13/2-1.
   2942.882+   configuration=π2f5/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
   3069.342+   configuration=π3p3/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
   3091(8)-   configuration: from 206Pb(α,d) and 210Bi(p,t).
Jπ(level): From 1977Da05 in 206Pb(α,d) based on similarity of Q value, L value and σ with levels in 206Bi and 210Bi; and assumption that the levels are two-particle+(206Pb core) states with J(π)+J(ν)=J(max).
E(level)Jπ(level)T1/2(level)Comments
   3154-   configuration=206Pb(2+)π1h9/2ν2g9/2-1.
   31711+   configuration=π3p3/2ν3p1/2-1.
Jπ(level): From L(3He,t)=0 at E=200 and 450 MeV, and the assumption that possible 0+ anti-analog states below the analog of the 208Pb g.s. will not Be populated at the bombarding energies used (1991Ja04).
   32571+,2+   configuration=π3p3/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
   3271+   configuration: the level appears to have a ν2f7/2-1 component also.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   3286.382+   configuration=π3p3/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
   3300-   configuration=206Pb(2+)π1h9/2ν2g9/2.
   3318+   configuration=π1h9/2ν1h9/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   33274-,5-   configuration=π1h9/2ν3s1/2-1.
   33474-,5-   configuration=π1h9/2ν3s1/2-1.
   3362+   configuration: the level appears to have a ν2f7/2-1 component also.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   34071+,2+   configuration=π3p3/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
   3412+   configuration=π1h9/2ν1h9/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   3449.4(13+)   configuration: from 208Pb(p,n) (E=3400).
   3453-   configuration=206Pb(2+)π1h9/2ν2g9/2.
   34571+,2+   configuration=π3p3/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
   3461+   configuration=π1h9/2ν1h9/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   3499.7(11+)   conf=206Pb(0+)π1i13/2π2g9/2.
Jπ(level): From 1977Da05 in 206Pb(α,d) based on similarity of Q value, L value and σ with levels in 206Bi and 210Bi; and assumption that the levels are two-particle+(206Pb core) states with J(π)+J(ν)=J(max).
   35219-   configuration=206Pb(0+)π1h9/2ν2g9/2.
   3524+   configuration=π1h9/2ν1h9/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   3541+   configuration=π1h9/2ν1h9/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   3563-   configuration=206Pb(2+)π1h9/2ν2g9/2.
   3565+   configuration=π1h9/2ν1h9/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   3600.6(12+)   configuration=206Pb(0+)π1h9/2ν1j15/2.
Jπ(level): From 1977Da05 in 206Pb(α,d) based on similarity of Q value, L value and σ with levels in 206Bi and 210Bi; and assumption that the levels are two-particle+(206Pb core) states with J(π)+J(ν)=J(max).
   36111+,2+   configuration=π3p3/2ν3p1/2-1.
Jπ(level): From 1971Al05 in 207Pb(3He,d) based on L-transfer and σ. This reaction populates levels with configuration=πnljν3p1/2-1J where the proton particle states involved are 1h9/2 (L=5), 2f7/2 (L=3), 1i13/2 (L=6), 2f5/2 (L=3), and 3p3/2 (L=1). As long as the full strength is seen for a multiplet, then this strength must Be distributed among the members of that multiplet in proportion to 2J+1. The authors note that the total strength in each multiplet is close to that expected on the basis of sum rule limits. The L=1 states are fragmented so only the combination 1+,2+ can Be established. Supporting arguments are given where available.
   3662   XREF: F(3649).
E(level)Jπ(level)T1/2(level)Comments
   3718+   configuration=π1h9/2ν1h9/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   38631+   Jπ(level): From L(3He,t)=0 at E=200 and 450 MeV, and the assumption that possible 0+ anti-analog states below the analog of the 208Pb g.s. will not Be populated at the bombarding energies used (1991Ja04).
   3886(+)   configuration=π1h9/2ν1h9/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   4015+   configuration=π1h9/2ν2f7/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   40431+   Jπ(level): From L(3He,t)=0 at E=200 and 450 MeV, and the assumption that possible 0+ anti-analog states below the analog of the 208Pb g.s. will not Be populated at the bombarding energies used (1991Ja04).
   4159.1(13+)   Jπ(level): Proposed by 2003Fo03 on the basis of the agreement of energy with calculations using the shell model, and the observed γ decay modes.
   4291.0(13)   Jπ(level): Proposed by 2003Fo03 on the basis of the agreement of energy with calculations using the shell model, and the observed γ decay modes.
   4484.3(14+)   Jπ(level): Proposed by 2003Fo03 on the basis of the agreement of energy with calculations using the shell model, and the observed γ decay modes.
   4543+   configuration=π1h9/2ν2f7/2-1.
E(level): Weighted average from (p,nγ) and ε decay.
Jπ(level): From L and σ in (p,d) (1973Cr05). This reaction populates levels with configuration=π1h9/2ν(nlj)-1J where the hole states involved are 3p1/2, 2f5/2, 3p3/2, 1i13/2, 2f7/2, 1h9/2, and 3s1/2. The energies of these hole states are well known in 207Pb. As long as the full pick-up strength for a given L transfer is observed, then the pickup strength must Be distributed among the various possible J values in proportion to 2J+1. See 1973Cr05 in 209Bi(p,d) and also 1971Al05 in 209Bi(d,t),(3He,α). The 628 and 633 levels are an unresolved doublet with Jπ=3+ and 5+. The 633 level is assigned as the 3+ member of the doublet on the basis of its strong γ feeding from the 2+ level at 925. For the L=5 levels, and for the levels above 3800, only π can Be established. Supporting arguments are given where available.
   46171+   configuration=π1h9/2ν2f7/2-1.
Jπ(level): From L(3He,t)=0 at E=200 and 450 MeV, and the assumption that possible 0+ anti-analog states below the analog of the 208Pb g.s. will not Be populated at the bombarding energies used (1991Ja04).
   4635.3(15+)   Jπ(level): Proposed by 2003Fo03 on the basis of the agreement of energy with calculations using the shell model, and the observed γ decay modes.
   4836.2(14-)   configuration=206Pb(0+)π1i13/2ν1j15/2.
Jπ(level): From 1977Da05 in 206Pb(α,d) based on similarity of Q value, L value and σ with levels in 206Bi and 210Bi; and assumption that the levels are two-particle+(206Pb core) states with J(π)+J(ν)=J(max).
   5463.0(15-)   Jπ(level): Proposed by 2003Fo03 on the basis of the agreement of energy with calculations using the shell model, and the observed γ decay modes.
   5626.6(16-)   Jπ(level): Proposed by 2003Fo03 on the basis of the agreement of energy with calculations using the shell model, and the observed γ decay modes.
      5.9E+31+   Jπ(level): From L(3He,t)=0 at E=200 and 450 MeV, and the assumption that possible 0+ anti-analog states below the analog of the 208Pb g.s. will not Be populated at the bombarding energies used (1991Ja04).
      8.19E+31+   Jπ(level): From L(3He,t)=0 at E=200 and 450 MeV, and the assumption that possible 0+ anti-analog states below the analog of the 208Pb g.s. will not Be populated at the bombarding energies used (1991Ja04).
   9000 ≈ 40 ns 2003Fo03 in 208Pb(48Ca,Xγ) state that they have established the presence of an isomer at about 9 MeV with a half-life of the order of 40 ns.
      9.8E+31+   Jπ(level): From L(3He,t)=0 at E=200 and 450 MeV, and the assumption that possible 0+ anti-analog states below the analog of the 208Pb g.s. will not Be populated at the bombarding energies used (1991Ja04).
  151650+ 231 keV 6  Γ(p)=130 4; Γ(p 3p1/2)=51.6 17; Γ(p 2f5/2)=20.6 17; Γ(p 3p3/2)=58 3; Γ(p 2f7/2)|<4.
E(level): Γ(p)=130 4; Γ(p 3p1/2)=51.6 17; Γ(p 2f5/2)=20.6 17; Γ(p 3p3/2)=58 3; Γ(p 2f7/2)|<4.
     15.6E+31+   Γp=184 49
Γp=58 keV 20, 102 keV 31, 8 keV 9, and 16 keV 8 for proton decay to the 3p1/2, 2f7/2 + 3p3/2, 1i13/2, and 2f7/2 neutron hole states, respectively, in 207Pb.
     21.1E+30-,1-,2- 10 MeV 3  configuration=isovector spin-flip dipole resonance.

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Additional Gamma Comments:

E(level)E(gamma)Comments
     63.02     63.00E(γ): weighted average of 62.94 5 from 0.119S 212At(α), 63.13 10 from 208Po ε decay, and 63.1 1 from (p,nγ)
M(γ): From ε decay
    510.28    447.3I(γ): Weighted average from (p,nγ), (d,tγ), and IT decay
    510.15I(γ): Weighted average from (p,nγ), (d,tγ), and IT decay
M(γ): From IT decay
    601.46    538.41E(γ): Weighted average from (p,nγ) and ε decay
I(γ): Weighted average from (p,nγ), (d,tγ), and ε decay
M(γ): From ε decay
    601.49E(γ): Weighted average from (p,nγ) and ε decay
I(γ): Weighted average from (p,nγ), (d,tγ), and ε decay
M(γ): From ε decay
    628.33    118.2M(γ): From (p,nγ)
    633.14     31.7E(γ): Weighted average from (p,nγ) and ε decay
    570.09E(γ): Weighted average from (p,nγ) and ε decay
M(γ): From ε decay
    650.57    140.08E(γ): Weighted average from (p,nγ) and IT decay
I(γ): Iγ/Iγ(651γ)=0.85 10 in (d,tγ). Weighted average from (p,nγ) and IT decay
M(γ): From (p,nγ)
    650.60E(γ): Weighted average from (p,nγ) and IT decay
I(γ): Weighted average from (p,nγ) and IT decay
M(γ): From IT decay
    886.36    886.4I(γ): Weighted average from (p,nγ) and (d,tγ)
    924.85    291.77E(γ): Weighted average from (p,nγ) and ε decay
I(γ): Weighted average from (p,nγ) and ε decay
M(γ): From ε decay
    861.83E(γ): Weighted average from (p,nγ) and ε decay
I(γ): Weighted average from (p,nγ) and ε decay
    925.11I(γ): Iγ=2.3 11 is reported in ε decay; however, the transition is not seen in (p,nγ) where the adopted limit is reported
    958.99    959.0I(γ): Weighted average from (p,nγ) and (d,tγ)
   1033.26    146.6M(γ): From (p,nγ)
    431.4I(γ): from 1971Pr02 in (p,nγ). 2006Bo08 report 1.2 3
   1069.11    110.0M(γ): From (p,nγ)
    467.37I(γ): Iγ/Iγ(1006γ)=0.19 4 is reported in 209Bi(d,tγ)
   1095.06    207.8E(γ): from the E(level) difference. Eγ=208 is reported in (d,tγ)
I(γ): Iγ/Iγ(1095γ)=0.02 1 is reported in (d,tγ). In (p,nγ) 1971Pr02 report a ratio of <0.06, and 2006Bo08 do not see the transition
   1571.1    920.5E(γ): Weighted average from (p,nγ), (n,2nγ), and IT decay. Doublet in 209Bi(p,d), 209Bi(d,t), and 207Pb(3He,d),(α,t) on the basis of strength. No broadening observed in (p,d), thus the levels are <3 keV apart. Doublet resolved in (p,nγ)
   1839.03    135.6M(γ): From (p,nγ)
   1919.97     80.7M(γ): From (p,nγ)
   2077.66    275.26M(γ): From (p,nγ)
   2202.89    125.3M(γ): From (p,nγ)
E(level)E(gamma)Comments
   3600.6    101E(γ): not observed, but required by coincidence data in 208Pb(48Ca,Xγ). The energy is from the E(level) difference

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