lilike_lgy10#ar15.dat

Resolved Specific Ion Data Collections

Ion
Ar15+
Temperature Range
4.412 eV → 4.412 x 104 eV

ADF04

Filename
lilike_lgy10#ar15.dat
Full Path
adf04/copaw#li/lilike_lgy10#ar15.dat
Download data
  • Spontaneous Emission: Ar+15(i) → Ar+15(j) + hv
  • Electron Impact Excitation: Ar+15(i) + e → Ar+15(j) + e
2s1 2S0.5 0.0 cm-1
2p1 2P0.5 257751.0 cm-1
2p1 2P1.5 283061.0 cm-1
3s1 2S0.5 4176520.0 cm-1
3p1 2P0.5 4247710.0 cm-1
3p1 2P1.5 4255120.0 cm-1
3d1 2D1.5 4282320.0 cm-1
3d1 2D2.5 4284680.0 cm-1
4s1 2S0.5 5606430.0 cm-1
4p1 2P0.5 5635710.0 cm-1
4p1 2P1.5 5638800.0 cm-1
4d1 2D1.5 5650090.0 cm-1
4d1 2D2.5 5651080.0 cm-1
4f1 2F2.5 5651660.0 cm-1
4f1 2F3.5 5652160.0 cm-1
5s1 2S0.5 6261140.0 cm-1
5p1 2P0.5 6275930.0 cm-1
5p1 2P1.5 6277500.0 cm-1
5d1 2D1.5 6283230.0 cm-1
5d1 2D2.5 6283740.0 cm-1
5f1 2F2.5 6284060.0 cm-1
5f1 2F3.5 6284310.0 cm-1
5g1 2G3.5 6284320.0 cm-1
5g1 2G4.5 6284470.0 cm-1
1s1 2s2 2S0.5 24874300.0 cm-1
1s1 2s1 2p1 4P0.5 24938700.0 cm-1
1s1 2s1 2p1 4P1.5 24947000.0 cm-1
1s1 2s1 2p1 4P2.5 24962300.0 cm-1
1s1 2s1 2p1 2P0.5 25142900.0 cm-1
1s1 2s1 2p1 2P1.5 25154900.0 cm-1
1s1 2p2 4P0.5 25218400.0 cm-1
1s1 2p2 4P1.5 25227900.0 cm-1
1s1 2s1 2p1 2P0.5 25241400.0 cm-1
1s1 2p2 4P2.5 25241600.0 cm-1
1s1 2s1 2p1 2P1.5 25247300.0 cm-1
1s1 2p2 2D1.5 25361300.0 cm-1
1s1 2p2 2D2.5 25365300.0 cm-1
1s1 2p2 2P0.5 25390100.0 cm-1
1s1 2p2 2P1.5 25411400.0 cm-1
1s1 2p2 2S0.5 25546100.0 cm-1
1s1 2s1 3s1 4S1.5 29164600.0 cm-1
1s1 2s1 3s1 2S0.5 29232200.0 cm-1
1s1 2s1 3p1 4P0.5 29255200.0 cm-1
1s1 2s1 3p1 4P1.5 29256500.0 cm-1
1s1 2s1 3p1 4P2.5 29261300.0 cm-1
1s1 2s1 3p1 2P1.5 29265500.0 cm-1
1s1 2s1 3p1 2P0.5 29265800.0 cm-1
1s1 2s1 3d1 4D0.5 29312000.0 cm-1
1s1 2s1 3d1 4D1.5 29312900.0 cm-1
1s1 2s1 3d1 4D2.5 29314200.0 cm-1
1s1 2s1 3d1 4D3.5 29316100.0 cm-1
1s1 2s1 3s1 2S0.5 29339400.0 cm-1
1s1 2s1 3d1 2D1.5 29349400.0 cm-1
1s1 2s1 3d1 2D2.5 29349400.0 cm-1
1s1 2p1 3s1 4P0.5 29363000.0 cm-1
1s1 2p1 3s1 4P1.5 29370400.0 cm-1
1s1 2p1 3s1 4P2.5 29385300.0 cm-1
1s1 2s1 3p1 2P0.5 29399900.0 cm-1
1s1 2s1 3p1 2P1.5 29405900.0 cm-1
1s1 2p1 3p1 4D0.5 29407700.0 cm-1
1s1 2p1 3p1 4D1.5 29413300.0 cm-1
1s1 2p1 3p1 4D2.5 29423600.0 cm-1
1s1 2p1 3p1 2P1.5 29431900.0 cm-1
1s1 2p1 3p1 2P0.5 29433400.0 cm-1
1s1 2p1 3p1 4D3.5 29436900.0 cm-1
1s1 2p1 3s1 2P0.5 29443400.0 cm-1
1s1 2p1 3p1 4S1.5 29454100.0 cm-1
1s1 2p1 3s1 2P1.5 29462700.0 cm-1
1s1 2p1 3p1 4P0.5 29462800.0 cm-1
1s1 2p1 3d1 4F1.5 29463900.0 cm-1
1s1 2p1 3d1 4F2.5 29469100.0 cm-1
1s1 2p1 3p1 4P1.5 29471000.0 cm-1
1s1 2p1 3p1 4P2.5 29475900.0 cm-1
1s1 2s1 3d1 2D1.5 29476800.0 cm-1
1s1 2p1 3d1 4F3.5 29477200.0 cm-1
1s1 2s1 3d1 2D2.5 29480700.0 cm-1
1s1 2p1 3d1 2D1.5 29486300.0 cm-1
1s1 2p1 3d1 2D2.5 29486900.0 cm-1
1s1 2p1 3d1 4F4.5 29488100.0 cm-1
1s1 2p1 3p1 2D1.5 29491000.0 cm-1
1s1 2p1 3p1 2D2.5 29509000.0 cm-1
1s1 2p1 3s1 2P1.5 29511000.0 cm-1
1s1 2p1 3d1 4D0.5 29511100.0 cm-1
1s1 2p1 3d1 4D1.5 29513100.0 cm-1
1s1 2p1 3d1 4D2.5 29514800.0 cm-1
1s1 2p1 3s1 2P0.5 29515100.0 cm-1
1s1 2p1 3d1 4D3.5 29522800.0 cm-1
1s1 2p1 3d1 2F2.5 29523700.0 cm-1
1s1 2p1 3d1 4P2.5 29533800.0 cm-1
1s1 2p1 3d1 4P1.5 29536500.0 cm-1
1s1 2p1 3d1 4P0.5 29538100.0 cm-1
1s1 2p1 3p1 2S0.5 29539800.0 cm-1
1s1 2p1 3d1 2F3.5 29541700.0 cm-1
1s1 2p1 3d1 2P1.5 29567700.0 cm-1
1s1 2p1 3p1 2P0.5 29577000.0 cm-1
1s1 2p1 3p1 2D1.5 29577800.0 cm-1
1s1 2p1 3d1 2P0.5 29578400.0 cm-1
1s1 2p1 3p1 2D2.5 29579000.0 cm-1
1s1 2p1 3p1 2P1.5 29586000.0 cm-1
1s1 2p1 3d1 2D1.5 29620200.0 cm-1
1s1 2p1 3d1 2D2.5 29622400.0 cm-1
1s1 2p1 3p1 2S0.5 29626500.0 cm-1
1s1 2p1 3d1 2F3.5 29637400.0 cm-1
1s1 2p1 3d1 2F2.5 29642300.0 cm-1
1s1 2p1 3d1 2P0.5 29661600.0 cm-1
1s1 2p1 3d1 2P1.5 29666500.0 cm-1
1s1 2s1 4s1 4S1.5 30661400.0 cm-1
1s1 2s1 4s1 2S0.5 30683600.0 cm-1
1s1 2s1 4p1 4P0.5 30694100.0 cm-1
1s1 2s1 4p1 4P1.5 30694900.0 cm-1
1s1 2s1 4p1 4P2.5 30696500.0 cm-1
1s1 2s1 4p1 2P1.5 30705000.0 cm-1
1s1 2s1 4p1 2P0.5 30705600.0 cm-1
1s1 2s1 4d1 4D0.5 30718100.0 cm-1
1s1 2s1 4d1 4D1.5 30718300.0 cm-1
1s1 2s1 4d1 4D2.5 30718700.0 cm-1
1s1 2s1 4d1 4D3.5 30719200.0 cm-1
1s1 2s1 4d1 2D2.5 30729800.0 cm-1
1s1 2s1 4d1 2D1.5 30730000.0 cm-1
1s1 2s1 4f1 4F1.5 30735900.0 cm-1
1s1 2s1 4f1 4F2.5 30736000.0 cm-1
1s1 2s1 4f1 4F3.5 30736200.0 cm-1
1s1 2s1 4f1 4F4.5 30736500.0 cm-1
1s1 2s1 4f1 2F3.5 30739800.0 cm-1
1s1 2s1 4f1 2F2.5 30739900.0 cm-1
1s1 2s1 4s1 2S0.5 30820200.0 cm-1
1s1 2p1 4s1 4P0.5 30828700.0 cm-1
1s1 2p1 4s1 4P1.5 30835100.0 cm-1
1s1 2s1 4p1 2P0.5 30844000.0 cm-1
1s1 2s1 4p1 2P1.5 30848900.0 cm-1
1s1 2p1 4p1 4D0.5 30849700.0 cm-1
1s1 2p1 4s1 4P2.5 30851600.0 cm-1
1s1 2p1 4p1 4D1.5 30854200.0 cm-1
1s1 2p1 4s1 2P0.5 30856900.0 cm-1
1s1 2p1 4p1 4D2.5 30861300.0 cm-1
1s1 2p1 4p1 4S1.5 30862400.0 cm-1
1s1 2p1 4p1 2P0.5 30866000.0 cm-1
1s1 2p1 4p1 4P0.5 30869700.0 cm-1
1s1 2p1 4d1 4F1.5 30872700.0 cm-1
1s1 2p1 4s1 2P1.5 30872800.0 cm-1
1s1 2s1 4d1 2D1.5 30873800.0 cm-1
1s1 2s1 4d1 2D2.5 30874600.0 cm-1
1s1 2p1 4p1 2P1.5 30874800.0 cm-1
1s1 2p1 4p1 4D3.5 30875500.0 cm-1
1s1 2p1 4d1 4F2.5 30877100.0 cm-1
1s1 2p1 4d1 2D2.5 30883000.0 cm-1
1s1 2p1 4p1 4P1.5 30883200.0 cm-1
1s1 2p1 4d1 4F3.5 30883400.0 cm-1
1s1 2p1 4p1 4P2.5 30883400.0 cm-1
1s1 2p1 4d1 2D1.5 30885100.0 cm-1
1s1 2p1 4p1 2D1.5 30887300.0 cm-1
1s1 2s1 4f1 2F2.5 30888300.0 cm-1
1s1 2s1 4f1 2F3.5 30889200.0 cm-1
1s1 2p1 4f1 4G2.5 30890000.0 cm-1
1s1 2p1 4d1 4D0.5 30890200.0 cm-1
1s1 2p1 4d1 4D1.5 30890700.0 cm-1
1s1 2p1 4f1 4F3.5 30891100.0 cm-1
1s1 2p1 4d1 4D2.5 30894600.0 cm-1
1s1 2p1 4f1 2F2.5 30895400.0 cm-1
1s1 2p1 4f1 4F1.5 30895600.0 cm-1
1s1 2p1 4f1 2F3.5 30896000.0 cm-1
1s1 2p1 4d1 4F4.5 30896500.0 cm-1
1s1 2p1 4f1 4F4.5 30897000.0 cm-1
1s1 2p1 4p1 2D2.5 30897900.0 cm-1
1s1 2p1 4f1 4F2.5 30901600.0 cm-1
1s1 2p1 4f1 2G3.5 30902100.0 cm-1
1s1 2p1 4d1 4D3.5 30903500.0 cm-1
1s1 2p1 4d1 2F2.5 30906000.0 cm-1
1s1 2p1 4d1 4P2.5 30908900.0 cm-1
1s1 2p1 4d1 4P1.5 30909200.0 cm-1
1s1 2p1 4d1 4P0.5 30910300.0 cm-1
1s1 2p1 4p1 2S0.5 30912400.0 cm-1
1s1 2p1 4f1 4G4.5 30914000.0 cm-1
1s1 2p1 4f1 4G3.5 30914100.0 cm-1
1s1 2p1 4f1 4D3.5 30916400.0 cm-1
1s1 2p1 4f1 2D2.5 30916900.0 cm-1
1s1 2p1 4f1 4G5.5 30917000.0 cm-1
1s1 2p1 4d1 2P1.5 30917300.0 cm-1
1s1 2p1 4d1 2F3.5 30918800.0 cm-1
1s1 2p1 4f1 2G4.5 30919900.0 cm-1
1s1 2p1 4f1 4D1.5 30920200.0 cm-1
1s1 2p1 4f1 4D2.5 30920700.0 cm-1
1s1 2p1 4f1 4D0.5 30922100.0 cm-1
1s1 2p1 4d1 2P0.5 30924400.0 cm-1
1s1 2p1 4f1 2D1.5 30924500.0 cm-1
1s1 2p1 4s1 2P0.5 30960700.0 cm-1
1s1 2p1 4s1 2P1.5 30960900.0 cm-1
1s1 2p1 4p1 2P0.5 30985100.0 cm-1
1s1 2p1 4p1 2D1.5 30985200.0 cm-1
1s1 2p1 4p1 2D2.5 30986400.0 cm-1
1s1 2p1 4p1 2P1.5 30988200.0 cm-1
1s1 2p1 4p1 2S0.5 31000300.0 cm-1
1s1 2p1 4d1 2D1.5 31004900.0 cm-1
1s1 2p1 4d1 2D2.5 31005800.0 cm-1
1s1 2p1 4d1 2F3.5 31007400.0 cm-1
1s1 2p1 4d1 2F2.5 31009500.0 cm-1
1s1 2p1 4f1 2F2.5 31012200.0 cm-1
1s1 2p1 4f1 2F3.5 31012700.0 cm-1
1s1 2p1 4d1 2P0.5 31017900.0 cm-1
1s1 2p1 4f1 2G3.5 31019800.0 cm-1
1s1 2p1 4d1 2P1.5 31019800.0 cm-1
1s1 2p1 4f1 2G4.5 31019900.0 cm-1
1s1 2p1 4f1 2D1.5 31024600.0 cm-1
1s1 2p1 4f1 2D2.5 31025300.0 cm-1
------------------------------------------------------------------------

        Result of ICFT R-matrix calculation for outer shell excitation
        +++++++++++++++++++++++++++++++++++

 Calculation automated by offline ADAS code ADAS8#3

     Summary Information
     +++++++++++++++++++

 *  Ionisation energy taken from ADAS adf00 files

 *  Energy levels calculated by AUTOSTRUCTURE

 *  Radiative rates calculated by AUTOSTRUCTURE

 *  Effective collision strengths calculated by ICFT
    R-matrix calculation using target structure from
    AUTOSTRUCTURE.

     Calculation details
     +++++++++++++++++++

 The following scaling parameters on bound orbitals were used:

         1S = 1.28136
         2S = 1.04052
         2P = 0.93965
         3S = 1.02761
         3P = 0.93258
         3D = 0.86682
         4S = 1.02632
         4P = 0.93219
         4D = 0.86863
         4F = 1.01227
         5S = 1.02802
         5P = 0.93350
         5D = 0.87282
         5F = 0.85031
         5G = 1.00000

 An exchange calculation was performed up to J=10
 A non-exchange calculation was then performed up to J=40
 Followed by a top-up calculation to J -> infinity.

 60 continuum basis orbitals were used, giving a smallest maximum
 basis-orbital energy of 883.0170 Rydbergs (12014.329302 eV)

 A fine energy mesh of 0.000004 Z**2 Rydbergs (0.0122454 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (30.6135 eV) was used
 from the last threshold up to 3.067274 Z**2 Rydbergs (9390 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (30.6135 eV) was used
 from first threshold up to 3.067274 Z**2 Rydbergs (9390 eV) in the
 non-exchange calculation.

 Dipole and Born limits were used from the last calculated energy points
 up to infinite energy to complete the effective collision strengths

  Produced by: Guiyun Liang
 Date:        13/10/10
------------------------------------------------------------------------
        Result of ICFT R-matrix calculation for core-excitation
   G.Y. Liang, and N.R. Badnell, A&A (2010)
        +++++++++++++++++++++++++++++++++++

 Calculation automated by offline ADAS code ADAS8#3

     Summary Information
     +++++++++++++++++++

 *  Ionisation energy taken from ADAS adf00 files

 *  Energy levels calculated by AUTOSTRUCTURE

 *  Radiative rates calculated by AUTOSTRUCTURE

 *  Effective collision strengths calculated by ICFT
    R-matrix calculation using target structure from
    AUTOSTRUCTURE.

     Calculation details
     +++++++++++++++++++

 The following scaling parameters on bound orbitals were used:

         1S = 1.28617
         2S = 1.04253
         2P = 0.94219
         3S = 1.03003
         3P = 0.93419
         3D = 0.87071
         4S = 1.03023
         4P = 0.93503
         4D = 0.87574
         4F = 0.98643

 An exchange calculation was performed up to J=10
 A non-exchange calculation was then performed up to J=40
 Followed by a top-up calculation to J -> infinity.

 40 continuum basis orbitals were used, giving a smallest maximum
 basis-orbital energy of 0 Rydbergs (0.000000 eV)

 A fine energy mesh of 0.000010 Z**2 Rydbergs (0.0306135 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (30.6135 eV) was used
 from the last threshold up to 2.999940 Z**2 Rydbergs (9183.86502 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (30.6135 eV) was used
 from first threshold up to 2.999940 Z**2 Rydbergs (9183.86502 eV) in the
 non-exchange calculation.

 Dipole and Born limits were used from the last calculated energy points
 up to infinite energy to complete the effective collision strengths

  NIST v4 energy  (Ryd)
  2   2.34219
  3   2.57527
  4  38.0548
  5  38.6966
  6  38.7658
  7  39.0129
  8  39.0347
  9  51.0833
 10  51.3477
 11  51.3766
 12  51.4777
 13  51.487
 16  57.041
 17  57.180
 18  57.195
 19  57.247
 20  57.251
 25  226.30
 26  226.90
 27  226.96
 28  227.12
 31  229.45
 32  229.55
 33  229.61
 34  229.67
 35  229.67
 36  230.72
 37  230.73

 Produced by: Guiyun Liang
 Date:        24/11/10
------------------------------------------------------------------------

Contributors

  • Guiyun Liang
  • Nigel Badnell
  • Processes
  • States
  • Comments
  • Origins

Data Classes