lilike_lgy10#ne7.dat

Resolved Specific Ion Data Collections

Ion
Ne7+
Temperature Range
1.103 eV → 1.103 x 104 eV

ADF04

Filename
lilike_lgy10#ne7.dat
Full Path
adf04/copaw#li/lilike_lgy10#ne7.dat
Download data
  • Spontaneous Emission: Ne+7(i) → Ne+7(j) + hv
  • Electron Impact Excitation: Ne+7(i) + e → Ne+7(j) + e
2s1 2S0.5 0.0 cm-1
2p1 2P0.5 129000.0 cm-1
2p1 2P1.5 130625.0 cm-1
3s1 2S0.5 1099310.0 cm-1
3p1 2P0.5 1134450.0 cm-1
3p1 2P1.5 1134930.0 cm-1
3d1 2D1.5 1146730.0 cm-1
3d1 2D2.5 1146880.0 cm-1
4s1 2S0.5 1468910.0 cm-1
4p1 2P0.5 1483280.0 cm-1
4p1 2P1.5 1483480.0 cm-1
4d1 2D1.5 1488400.0 cm-1
4d1 2D2.5 1488460.0 cm-1
4f1 2F2.5 1488670.0 cm-1
4f1 2F3.5 1488700.0 cm-1
5s1 2S0.5 1636710.0 cm-1
5p1 2P0.5 1643960.0 cm-1
5p1 2P1.5 1644060.0 cm-1
5d1 2D1.5 1646560.0 cm-1
5d1 2D2.5 1646590.0 cm-1
5f1 2F2.5 1646710.0 cm-1
5f1 2F3.5 1646720.0 cm-1
5g1 2G3.5 1646730.0 cm-1
5g1 2G4.5 1646740.0 cm-1
1s1 2s2 2S0.5 7206180.0 cm-1
1s1 2s1 2p1 4P0.5 7242500.0 cm-1
1s1 2s1 2p1 4P1.5 7243080.0 cm-1
1s1 2s1 2p1 4P2.5 7244050.0 cm-1
1s1 2s1 2p1 2P0.5 7338290.0 cm-1
1s1 2s1 2p1 2P1.5 7339040.0 cm-1
1s1 2p2 4P0.5 7381250.0 cm-1
1s1 2p2 4P1.5 7381840.0 cm-1
1s1 2p2 4P2.5 7382790.0 cm-1
1s1 2s1 2p1 2P0.5 7393900.0 cm-1
1s1 2s1 2p1 2P1.5 7394330.0 cm-1
1s1 2p2 2D1.5 7444620.0 cm-1
1s1 2p2 2D2.5 7444680.0 cm-1
1s1 2p2 2P0.5 7459580.0 cm-1
1s1 2p2 2P1.5 7460770.0 cm-1
1s1 2p2 2S0.5 7542420.0 cm-1
1s1 2s1 3s1 4S1.5 8372200.0 cm-1
1s1 2s1 3s1 2S0.5 8406570.0 cm-1
1s1 2s1 3p1 4P0.5 8419530.0 cm-1
1s1 2s1 3p1 4P1.5 8419550.0 cm-1
1s1 2s1 3p1 4P2.5 8419910.0 cm-1
1s1 2s1 3p1 2P0.5 8419920.0 cm-1
1s1 2s1 3p1 2P1.5 8419940.0 cm-1
1s1 2s1 3d1 4D0.5 8443740.0 cm-1
1s1 2s1 3d1 4D1.5 8443790.0 cm-1
1s1 2s1 3d1 4D2.5 8443880.0 cm-1
1s1 2s1 3d1 4D3.5 8444000.0 cm-1
1s1 2s1 3s1 2S0.5 8458330.0 cm-1
1s1 2s1 3d1 2D2.5 8461420.0 cm-1
1s1 2s1 3d1 2D1.5 8461420.0 cm-1
1s1 2p1 3s1 4P0.5 8479280.0 cm-1
1s1 2p1 3s1 4P1.5 8479800.0 cm-1
1s1 2p1 3s1 4P2.5 8480700.0 cm-1
1s1 2s1 3p1 2P0.5 8489040.0 cm-1
1s1 2s1 3p1 2P1.5 8489360.0 cm-1
1s1 2p1 3p1 4D0.5 8499740.0 cm-1
1s1 2p1 3p1 4D1.5 8500120.0 cm-1
1s1 2p1 3p1 4D2.5 8500730.0 cm-1
1s1 2p1 3p1 4D3.5 8501520.0 cm-1
1s1 2p1 3p1 2P0.5 8503020.0 cm-1
1s1 2p1 3p1 2P1.5 8503130.0 cm-1
1s1 2p1 3p1 4S1.5 8514430.0 cm-1
1s1 2p1 3s1 2P0.5 8516960.0 cm-1
1s1 2p1 3s1 2P1.5 8518260.0 cm-1
1s1 2s1 3d1 2D1.5 8523060.0 cm-1
1s1 2s1 3d1 2D2.5 8523270.0 cm-1
1s1 2p1 3d1 4F1.5 8524220.0 cm-1
1s1 2p1 3d1 4F2.5 8524560.0 cm-1
1s1 2p1 3d1 4F3.5 8525040.0 cm-1
1s1 2p1 3d1 4F4.5 8525660.0 cm-1
1s1 2p1 3p1 4P0.5 8527010.0 cm-1
1s1 2p1 3p1 4P1.5 8527360.0 cm-1
1s1 2p1 3p1 4P2.5 8527880.0 cm-1
1s1 2p1 3d1 2D1.5 8529690.0 cm-1
1s1 2p1 3d1 2D2.5 8529840.0 cm-1
1s1 2p1 3p1 2D1.5 8536880.0 cm-1
1s1 2p1 3p1 2D2.5 8538060.0 cm-1
1s1 2p1 3s1 2P1.5 8542870.0 cm-1
1s1 2p1 3s1 2P0.5 8543120.0 cm-1
1s1 2p1 3d1 4D0.5 8544960.0 cm-1
1s1 2p1 3d1 4D1.5 8545060.0 cm-1
1s1 2p1 3d1 4D2.5 8545250.0 cm-1
1s1 2p1 3d1 4D3.5 8545550.0 cm-1
1s1 2p1 3d1 2F2.5 8549810.0 cm-1
1s1 2p1 3d1 2F3.5 8551060.0 cm-1
1s1 2p1 3d1 4P2.5 8552480.0 cm-1
1s1 2p1 3d1 4P1.5 8552810.0 cm-1
1s1 2p1 3d1 4P0.5 8553000.0 cm-1
1s1 2p1 3p1 2S0.5 8555870.0 cm-1
1s1 2p1 3d1 2P1.5 8571390.0 cm-1
1s1 2p1 3d1 2P0.5 8572100.0 cm-1
1s1 2p1 3p1 2D2.5 8574640.0 cm-1
1s1 2p1 3p1 2D1.5 8574660.0 cm-1
1s1 2p1 3p1 2P0.5 8574690.0 cm-1
1s1 2p1 3p1 2P1.5 8575260.0 cm-1
1s1 2p1 3d1 2D1.5 8590870.0 cm-1
1s1 2p1 3d1 2D2.5 8591060.0 cm-1
1s1 2p1 3p1 2S0.5 8598900.0 cm-1
1s1 2p1 3d1 2F3.5 8599720.0 cm-1
1s1 2p1 3d1 2F2.5 8600050.0 cm-1
1s1 2p1 3d1 2P0.5 8614420.0 cm-1
1s1 2p1 3d1 2P1.5 8614750.0 cm-1
1s1 2s1 4s1 4S1.5 8777870.0 cm-1
1s1 2s1 4s1 2S0.5 8788620.0 cm-1
1s1 2s1 4p1 4P0.5 8794070.0 cm-1
1s1 2s1 4p1 4P1.5 8794110.0 cm-1
1s1 2s1 4p1 4P2.5 8794190.0 cm-1
1s1 2s1 4p1 2P1.5 8798340.0 cm-1
1s1 2s1 4p1 2P0.5 8798380.0 cm-1
1s1 2s1 4d1 4D0.5 8803960.0 cm-1
1s1 2s1 4d1 4D1.5 8803970.0 cm-1
1s1 2s1 4d1 4D2.5 8803990.0 cm-1
1s1 2s1 4d1 4D3.5 8804020.0 cm-1
1s1 2s1 4d1 2D2.5 8809560.0 cm-1
1s1 2s1 4d1 2D1.5 8809570.0 cm-1
1s1 2s1 4f1 4F1.5 8812210.0 cm-1
1s1 2s1 4f1 4F2.5 8812220.0 cm-1
1s1 2s1 4f1 4F3.5 8812230.0 cm-1
1s1 2s1 4f1 4F4.5 8812250.0 cm-1
1s1 2s1 4f1 2F3.5 8814450.0 cm-1
1s1 2s1 4f1 2F2.5 8814460.0 cm-1
1s1 2s1 4s1 2S0.5 8855010.0 cm-1
1s1 2s1 4p1 2P0.5 8867450.0 cm-1
1s1 2s1 4p1 2P1.5 8867640.0 cm-1
1s1 2p1 4s1 4P0.5 8867740.0 cm-1
1s1 2p1 4s1 4P1.5 8868240.0 cm-1
1s1 2p1 4s1 4P2.5 8869040.0 cm-1
1s1 2p1 4p1 4D0.5 8878050.0 cm-1
1s1 2p1 4p1 4D1.5 8878350.0 cm-1
1s1 2p1 4s1 2P0.5 8878760.0 cm-1
1s1 2p1 4p1 4D2.5 8878850.0 cm-1
1s1 2p1 4p1 4D3.5 8879580.0 cm-1
1s1 2s1 4d1 2D1.5 8879630.0 cm-1
1s1 2s1 4d1 2D2.5 8879680.0 cm-1
1s1 2p1 4s1 2P1.5 8879810.0 cm-1
1s1 2p1 4p1 2P0.5 8880870.0 cm-1
1s1 2p1 4p1 2P1.5 8881180.0 cm-1
1s1 2p1 4p1 4S1.5 8883460.0 cm-1
1s1 2p1 4p1 4P0.5 8884320.0 cm-1
1s1 2p1 4p1 4P1.5 8884840.0 cm-1
1s1 2p1 4p1 4P2.5 8885120.0 cm-1
1s1 2s1 4f1 2F2.5 8886450.0 cm-1
1s1 2s1 4f1 2F3.5 8886540.0 cm-1
1s1 2p1 4d1 4F1.5 8887560.0 cm-1
1s1 2p1 4d1 4F2.5 8887890.0 cm-1
1s1 2p1 4d1 4F3.5 8888360.0 cm-1
1s1 2p1 4d1 2D1.5 8888930.0 cm-1
1s1 2p1 4d1 4F4.5 8888970.0 cm-1
1s1 2p1 4d1 2D2.5 8889130.0 cm-1
1s1 2p1 4p1 2D1.5 8890330.0 cm-1
1s1 2p1 4p1 2D2.5 8891260.0 cm-1
1s1 2p1 4d1 4D0.5 8892710.0 cm-1
1s1 2p1 4d1 4D1.5 8892790.0 cm-1
1s1 2p1 4d1 4D2.5 8892950.0 cm-1
1s1 2p1 4d1 4D3.5 8893280.0 cm-1
1s1 2p1 4f1 2F2.5 8894370.0 cm-1
1s1 2p1 4f1 2F3.5 8894540.0 cm-1
1s1 2p1 4f1 4F1.5 8894710.0 cm-1
1s1 2p1 4f1 4F2.5 8894740.0 cm-1
1s1 2p1 4f1 4F3.5 8894840.0 cm-1
1s1 2p1 4f1 4F4.5 8895000.0 cm-1
1s1 2p1 4d1 4P2.5 8895640.0 cm-1
1s1 2p1 4d1 4P1.5 8895980.0 cm-1
1s1 2p1 4d1 4P0.5 8896180.0 cm-1
1s1 2p1 4f1 4G2.5 8897230.0 cm-1
1s1 2p1 4f1 4G3.5 8897530.0 cm-1
1s1 2p1 4f1 4G4.5 8897940.0 cm-1
1s1 2p1 4f1 4G5.5 8898400.0 cm-1
1s1 2p1 4f1 2G3.5 8899330.0 cm-1
1s1 2p1 4d1 2F2.5 8899520.0 cm-1
1s1 2p1 4f1 2G4.5 8900120.0 cm-1
1s1 2p1 4d1 2F3.5 8900480.0 cm-1
1s1 2p1 4f1 4D3.5 8900670.0 cm-1
1s1 2p1 4p1 2S0.5 8900840.0 cm-1
1s1 2p1 4f1 4D2.5 8901030.0 cm-1
1s1 2p1 4f1 4D1.5 8901310.0 cm-1
1s1 2p1 4f1 4D0.5 8901480.0 cm-1
1s1 2p1 4f1 2D2.5 8902520.0 cm-1
1s1 2p1 4d1 2P1.5 8902930.0 cm-1
1s1 2p1 4f1 2D1.5 8903050.0 cm-1
1s1 2p1 4d1 2P0.5 8903560.0 cm-1
1s1 2p1 4s1 2P0.5 8921100.0 cm-1
1s1 2p1 4s1 2P1.5 8921110.0 cm-1
1s1 2p1 4p1 2D1.5 8932980.0 cm-1
1s1 2p1 4p1 2D2.5 8933000.0 cm-1
1s1 2p1 4p1 2P0.5 8933170.0 cm-1
1s1 2p1 4p1 2P1.5 8933360.0 cm-1
1s1 2p1 4p1 2S0.5 8940320.0 cm-1
1s1 2p1 4d1 2D1.5 8941020.0 cm-1
1s1 2p1 4d1 2D2.5 8941090.0 cm-1
1s1 2p1 4d1 2F3.5 8942650.0 cm-1
1s1 2p1 4d1 2F2.5 8942810.0 cm-1
1s1 2p1 4f1 2F2.5 8944000.0 cm-1
1s1 2p1 4f1 2F3.5 8944030.0 cm-1
1s1 2p1 4f1 2G4.5 8947700.0 cm-1
1s1 2p1 4f1 2G3.5 8947700.0 cm-1
1s1 2p1 4d1 2P0.5 8948280.0 cm-1
1s1 2p1 4d1 2P1.5 8948420.0 cm-1
1s1 2p1 4f1 2D1.5 8950750.0 cm-1
1s1 2p1 4f1 2D2.5 8950800.0 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 = 1.27799
         2S = 1.02346
         2P = 0.91350
         3S = 1.01200
         3P = 0.90786
         3D = 0.83823
         4S = 1.00986
         4P = 0.90769
         4D = 0.83982
         4F = 0.82573
         5S = 1.01195
         5P = 0.90920
         5D = 0.84313
         5F = 0.81985
         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.

 63 continuum basis orbitals were used, giving a smallest maximum
 basis-orbital energy of 244.8167 Rydbergs (3330.976020 eV)

 A fine energy mesh of 0.000004 Z**2 Rydbergs (0.002666776 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (6.66694 eV) was used
 from the last threshold up to 3.586353 Z**2 Rydbergs (2391 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (6.66694 eV) was used
 from first threshold up to 3.586353 Z**2 Rydbergs (2391 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:        14/10/10
------------------------------------------------------------------------
        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 = 1.28169
         2S = 1.02607
         2P = 0.91728
         3S = 1.01437
         3P = 0.90966
         3D = 0.84264
         4S = 1.01437
         4P = 0.91067
         4D = 0.84821
         4F = 0.99000

 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.

 45 continuum basis orbitals were used, giving a smallest maximum
 basis-orbital energy of 254.5793 Rydbergs (3463.805956 eV)

 A fine energy mesh of 0.000010 Z**2 Rydbergs (0.00666694 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (6.66694 eV) was used
 from the last threshold up to 3.586353 Z**2 Rydbergs (2391 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (6.66694 eV) was used
 from first threshold up to 3.586353 Z**2 Rydbergs (2391 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   1.167806
  3   1.182836
  4  10.022899
  5  10.341418
  6  10.345867
  7  10.45540
  8  10.45673
  9  13.39213
 10  13.52240
 11  13.52427
 12  13.56971
 13  13.57028
 14  13.57274
 15  13.57302
 16  14.92163
 17  14.98728
 18  14.98823
 19  15.01128
 20  15.01158
 21  15.012949
 22  15.013095
 23  15.01322
 25   65.52557
 26   65.84492
 27   65.84899
 28   65.85894
 29   66.72935
 31   67.09804
 32   67.10482
 33   67.11270
 34   67.17132
 36   67.64700
 38   67.77093
 40   68.51452
 41   76.09481
 42   76.37329
 43   76.50087
 46   76.55554
 48   76.73160
 52   76.81070
 53   76.87996
 55   76.99004
 58   77.18432
 60   77.22806
 66   77.33923
 67   77.33012
 69   77.47592
 71   77.43519
 75   77.38298
 78   77.48249
 80   77.53060
 82   77.69463
 84   77.60077
 90   77.67002
 93   77.71285
 96   77.91333
 103  78.10470
 107  79.77870
 114  79.99904
 118  80.04570
 120  80.07814
 124  80.09163
 129  80.54872
 132  80.60941
 143  80.67721
 153  80.76286
 160  80.78346
 162  80.78027
 166  80.78018
 169  80.79640
 173  80.80752
 179  80.82191

 Produced by: Guiyun Liang
 Date:        01/09/10
------------------------------------------------------------------------

Contributors

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

Data Classes