ls#ge18.dat

Resolved Specific Ion Data Collections

Ion
Ge18+
Temperature Range
6.221 eV → 6.842 x 104 eV

ADF04

Filename
ls#ge18.dat
Full Path
adf04/copmm#32/ls#ge18.dat
Download data
  • Spontaneous Emission: Ge+18(i) → Ge+18(j) + hv
  • Electron Impact Excitation: Ge+18(i) + e → Ge+18(j) + e
24525 3P4.0 0.0 cm-1
24525 1D2.0 63759.0 cm-1
24525 1S0.0 123100.0 cm-1
14535 5S2.0 305276.0 cm-1
14535 3D7.0 423536.0 cm-1
14535 3P4.0 481926.0 cm-1
14535 1D2.0 551146.0 cm-1
14535 3S1.0 576436.0 cm-1
24515516 3F10.0 616186.0 cm-1
14535 1P1.0 631816.0 cm-1
24515516 3P4.0 665476.0 cm-1
24515516 1D2.0 674896.0 cm-1
24515516 3D7.0 688006.0 cm-1
24515516 1F3.0 768816.0 cm-1
24515516 1P1.0 773886.0 cm-1
24515517 3P4.0 2567640.0 cm-1
24515517 1P1.0 2598740.0 cm-1
24515518 1P1.0 2726440.0 cm-1
24515518 3D7.0 2740040.0 cm-1
24515518 3P4.0 2760340.0 cm-1
24515518 3S1.0 2774440.0 cm-1
24515518 1D2.0 2795140.0 cm-1
24515518 1S0.0 2825840.0 cm-1
24515519 3D7.0 2972040.0 cm-1
24515519 3F10.0 2973140.0 cm-1
24515519 1D2.0 2992440.0 cm-1
24515519 3P4.0 3005840.0 cm-1
24515519 1F3.0 3010040.0 cm-1
24515519 1P1.0 3020140.0 cm-1
2451551a 3G13.0 3116540.0 cm-1
2451551a 3F10.0 3119240.0 cm-1
2451551a 1F3.0 3139340.0 cm-1
2451551a 3D7.0 3155340.0 cm-1
2451551a 1G4.0 3174440.0 cm-1
2451551a 1D2.0 3176740.0 cm-1
--------------------------------------------------------------------------------

             Configuration
       Eissner            == Standard           R Parentage

   1   24525              == 3S2 3P2              1 3P  3P/
   2   24525              == 3S2 3P2              2 1D  1D/
   3   24525              == 3S2 3P2              3 1S  1S/
   4   14535              == 3S1 3P3              1 2S  2S/ 1 4S  5S/
   5   14535              == 3S1 3P3              1 2S  2S/ 2 2D  3D/
   6   14535              == 3S1 3P3              1 2S  2S/ 3 2P  3P/
   7   14535              == 3S1 3P3              1 2S  2S/ 2 2D  1D/
   8   14535              == 3S1 3P3              1 2S  2S/ 1 4S  3S/
   9   24515516           == 3S2 3P1 3D1          1 2P  2P/ 1 2D  3F/
  10   14535              == 3S1 3P3              1 2S  2S/ 3 2P  1P/
  11   24515516           == 3S2 3P1 3D1          1 2P  2P/ 1 2D  3P/
  12   24515516           == 3S2 3P1 3D1        * 1 2P  2P/ 1 2D  1D/
  13   24515516           == 3S2 3P1 3D1          1 2P  2P/ 1 2D  3D/
  14   24515516           == 3S2 3P1 3D1          1 2P  2P/ 1 2D  1F/
  15   24515516           == 3S2 3P1 3D1          1 2P  2P/ 1 2D  1P/
  16   24515517           == 3S2 3P1 4S1          1 2P  2P/ 1 2S  3P/
  17   24515517           == 3S2 3P1 4S1          1 2P  2P/ 1 2S  1P/
  18   24515518           == 3S2 3P1 4P1        * 1 2P  2P/ 1 2P  1P/
  19   24515518           == 3S2 3P1 4P1          1 2P  2P/ 1 2P  3D/
  20   24515518           == 3S2 3P1 4P1          1 2P  2P/ 1 2P  3P/
  21   24515518           == 3S2 3P1 4P1          1 2P  2P/ 1 2P  3S/
  22   24515518           == 3S2 3P1 4P1          1 2P  2P/ 1 2P  1D/
  23   24515518           == 3S2 3P1 4P1          1 2P  2P/ 1 2P  1S/
  24   24515519           == 3S2 3P1 4D1          1 2P  2P/ 1 2D  3D/
  25   24515519           == 3S2 3P1 4D1          1 2P  2P/ 1 2D  3F/
  26   24515519           == 3S2 3P1 4D1          1 2P  2P/ 1 2D  1D/
  27   24515519           == 3S2 3P1 4D1          1 2P  2P/ 1 2D  3P/
  28   24515519           == 3S2 3P1 4D1          1 2P  2P/ 1 2D  1F/
  29   24515519           == 3S2 3P1 4D1          1 2P  2P/ 1 2D  1P/
  30   2451551A           == 3S2 3P1 4F1          1 2P  2P/ 1 2F  3G/
  31   2451551A           == 3S2 3P1 4F1          1 2P  2P/ 1 2F  3F/
  32   2451551A           == 3S2 3P1 4F1          1 2P  2P/ 1 2F  1F/
  33   2451551A           == 3S2 3P1 4F1          1 2P  2P/ 1 2F  3D/
  34   2451551A           == 3S2 3P1 4F1          1 2P  2P/ 1 2F  1G/
  35   2451551A           == 3S2 3P1 4F1          1 2P  2P/ 1 2F  1D/

 (R) - Levels (or levels within a term) have been reassigned
       from their principal component.

--------------------------------------------------------------------------------

 IC Level list :

        1     2     3     4     5     6     7     8     9    10
       11    12    13    14    15    16    17    18    19    20
       21    22    23    24    25    26    27    28    29    30
       31    32    33    34    35    36    37    38    39    40
       41    42    43    44    45    46    47    48    49    50
       51    52    53    54    55    56    57    58    59    60
       61    62    63    64    65

 Map to LS levels :

        1     1     1     2     3     4     5     5     5     6
        6     6     7     8     9     9    10     9    11    13
       12    11    11    13    13    14    15    16    16    16
       17    19    19    20    18    20    20    19    21    22
       23    25    24    24    25    26    24    25    27    27
       28    27    29    30    31    30    31    32    31    30
       33    33    33    34    35

--------------------------------------------------------------------------------

   Generated from Cowan Atomic Structure Program

   From IFG file : ./ifg#ge32-18_adf34.dat

   Options in effect

   Coupling    Avalue   numtemps   Lweight   Isonuclear   Comment Level
   LS          YES      14         NO        YES          2


   Cowan code options
   ------------------
                                                                          
      Cowan plane wave Born method                                        
                                                                          
      Scale factors 85 95 85 85 50                                        
                                                                          
   Parity 1    Parity 2    Allowed
        259         555        617     initially
         93         175        257     reduced

   Note: The Born method does NOT calculate spin changing transitions
   correctly. You should supplement for important transitions of this type.

--------------------------------------------------------------------------------

   Code     : ADAS801
   Producer : Martin O'Mullane
   Date     : 27/02/06

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Contributors

  • Martin O'Mullane
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