lilike_lgy10#na8.dat

Resolved Specific Ion Data Collections

Ion
Na8+
Temperature Range
1.396 eV → 1.396 x 104 eV

ADF04

Filename
lilike_lgy10#na8.dat
Full Path
adf04/copaw#li/lilike_lgy10#na8.dat
Download data
  • Spontaneous Emission: Na+8(i) → Na+8(j) + hv
  • Electron Impact Excitation: Na+8(i) + e → Na+8(j) + e
2s1 2S0.5 0.0 cm-1
2p1 2P0.5 144927.0 cm-1
2p1 2P1.5 147517.0 cm-1
3s1 2S0.5 1375420.0 cm-1
3p1 2P0.5 1415020.0 cm-1
3p1 2P1.5 1415780.0 cm-1
3d1 2D1.5 1429460.0 cm-1
3d1 2D2.5 1429690.0 cm-1
4s1 2S0.5 1839680.0 cm-1
4p1 2P0.5 1855900.0 cm-1
4p1 2P1.5 1856220.0 cm-1
4d1 2D1.5 1861920.0 cm-1
4d1 2D2.5 1862010.0 cm-1
4f1 2F2.5 1862260.0 cm-1
4f1 2F3.5 1862310.0 cm-1
5s1 2S0.5 2050860.0 cm-1
5p1 2P0.5 2059040.0 cm-1
5p1 2P1.5 2059200.0 cm-1
5d1 2D1.5 2062100.0 cm-1
5d1 2D2.5 2062150.0 cm-1
5f1 2F2.5 2062290.0 cm-1
5f1 2F3.5 2062320.0 cm-1
5g1 2G3.5 2062320.0 cm-1
5g1 2G4.5 2062330.0 cm-1
1s1 2s2 2S0.5 8831110.0 cm-1
1s1 2s1 2p1 4P0.5 8870790.0 cm-1
1s1 2s1 2p1 4P1.5 8871710.0 cm-1
1s1 2s1 2p1 4P2.5 8873260.0 cm-1
1s1 2s1 2p1 2P0.5 8979640.0 cm-1
1s1 2s1 2p1 2P1.5 8980830.0 cm-1
1s1 2p2 4P0.5 9025680.0 cm-1
1s1 2p2 4P1.5 9026610.0 cm-1
1s1 2p2 4P2.5 9028120.0 cm-1
1s1 2s1 2p1 2P0.5 9040080.0 cm-1
1s1 2s1 2p1 2P1.5 9040750.0 cm-1
1s1 2p2 2D1.5 9098010.0 cm-1
1s1 2p2 2D2.5 9098130.0 cm-1
1s1 2p2 2P0.5 9115400.0 cm-1
1s1 2p2 2P1.5 9117320.0 cm-1
1s1 2p2 2S0.5 9206470.0 cm-1
1s1 2s1 3s1 4S1.5 10279300.0 cm-1
1s1 2s1 3s1 2S0.5 10317700.0 cm-1
1s1 2s1 3p1 4P0.5 10331900.0 cm-1
1s1 2s1 3p1 4P1.5 10332000.0 cm-1
1s1 2s1 3p1 4P2.5 10332500.0 cm-1
1s1 2s1 3p1 2P1.5 10332900.0 cm-1
1s1 2s1 3p1 2P0.5 10333000.0 cm-1
1s1 2s1 3d1 4D0.5 10359700.0 cm-1
1s1 2s1 3d1 4D1.5 10359800.0 cm-1
1s1 2s1 3d1 4D2.5 10359900.0 cm-1
1s1 2s1 3d1 4D3.5 10360100.0 cm-1
1s1 2s1 3s1 2S0.5 10376300.0 cm-1
1s1 2s1 3d1 2D1.5 10379700.0 cm-1
1s1 2s1 3d1 2D2.5 10379700.0 cm-1
1s1 2p1 3s1 4P0.5 10397300.0 cm-1
1s1 2p1 3s1 4P1.5 10398100.0 cm-1
1s1 2p1 3s1 4P2.5 10399600.0 cm-1
1s1 2s1 3p1 2P0.5 10410500.0 cm-1
1s1 2s1 3p1 2P1.5 10411100.0 cm-1
1s1 2p1 3p1 4D0.5 10420900.0 cm-1
1s1 2p1 3p1 4D1.5 10421500.0 cm-1
1s1 2p1 3p1 4D2.5 10422500.0 cm-1
1s1 2p1 3p1 4D3.5 10423800.0 cm-1
1s1 2p1 3p1 2P0.5 10425400.0 cm-1
1s1 2p1 3p1 2P1.5 10425500.0 cm-1
1s1 2p1 3p1 4S1.5 10437900.0 cm-1
1s1 2p1 3s1 2P0.5 10440400.0 cm-1
1s1 2p1 3s1 2P1.5 10442500.0 cm-1
1s1 2p1 3d1 4F1.5 10448600.0 cm-1
1s1 2p1 3d1 4F2.5 10449200.0 cm-1
1s1 2s1 3d1 2D1.5 10449500.0 cm-1
1s1 2s1 3d1 2D2.5 10449800.0 cm-1
1s1 2p1 3d1 4F3.5 10450000.0 cm-1
1s1 2p1 3p1 4P0.5 10450800.0 cm-1
1s1 2p1 3d1 4F4.5 10451000.0 cm-1
1s1 2p1 3p1 4P1.5 10451300.0 cm-1
1s1 2p1 3p1 4P2.5 10452200.0 cm-1
1s1 2p1 3d1 2D1.5 10455100.0 cm-1
1s1 2p1 3d1 2D2.5 10455400.0 cm-1
1s1 2p1 3p1 2D1.5 10463100.0 cm-1
1s1 2p1 3p1 2D2.5 10465000.0 cm-1
1s1 2p1 3s1 2P1.5 10470500.0 cm-1
1s1 2p1 3s1 2P0.5 10470900.0 cm-1
1s1 2p1 3d1 4D0.5 10472100.0 cm-1
1s1 2p1 3d1 4D1.5 10472300.0 cm-1
1s1 2p1 3d1 4D2.5 10472600.0 cm-1
1s1 2p1 3d1 4D3.5 10473100.0 cm-1
1s1 2p1 3d1 2F2.5 10478000.0 cm-1
1s1 2p1 3d1 2F3.5 10480000.0 cm-1
1s1 2p1 3d1 4P2.5 10480700.0 cm-1
1s1 2p1 3d1 4P1.5 10481200.0 cm-1
1s1 2p1 3d1 4P0.5 10481400.0 cm-1
1s1 2p1 3p1 2S0.5 10485100.0 cm-1
1s1 2p1 3d1 2P1.5 10502000.0 cm-1
1s1 2p1 3d1 2P0.5 10503100.0 cm-1
1s1 2p1 3p1 2P0.5 10506200.0 cm-1
1s1 2p1 3p1 2D1.5 10506200.0 cm-1
1s1 2p1 3p1 2D2.5 10506200.0 cm-1
1s1 2p1 3p1 2P1.5 10507100.0 cm-1
1s1 2p1 3d1 2D1.5 10525200.0 cm-1
1s1 2p1 3d1 2D2.5 10525500.0 cm-1
1s1 2p1 3p1 2S0.5 10533400.0 cm-1
1s1 2p1 3d1 2F3.5 10535200.0 cm-1
1s1 2p1 3d1 2F2.5 10535700.0 cm-1
1s1 2p1 3d1 2P0.5 10551200.0 cm-1
1s1 2p1 3d1 2P1.5 10551800.0 cm-1
1s1 2s1 4s1 4S1.5 10783500.0 cm-1
1s1 2s1 4s1 2S0.5 10795600.0 cm-1
1s1 2s1 4p1 4P0.5 10801700.0 cm-1
1s1 2s1 4p1 4P1.5 10801800.0 cm-1
1s1 2s1 4p1 4P2.5 10801900.0 cm-1
1s1 2s1 4p1 2P1.5 10806600.0 cm-1
1s1 2s1 4p1 2P0.5 10806700.0 cm-1
1s1 2s1 4d1 4D0.5 10813200.0 cm-1
1s1 2s1 4d1 4D1.5 10813200.0 cm-1
1s1 2s1 4d1 4D2.5 10813200.0 cm-1
1s1 2s1 4d1 4D3.5 10813300.0 cm-1
1s1 2s1 4d1 2D2.5 10819500.0 cm-1
1s1 2s1 4d1 2D1.5 10819500.0 cm-1
1s1 2s1 4f1 4F1.5 10822500.0 cm-1
1s1 2s1 4f1 4F2.5 10822500.0 cm-1
1s1 2s1 4f1 4F3.5 10822600.0 cm-1
1s1 2s1 4f1 4F4.5 10822600.0 cm-1
1s1 2s1 4f1 2F3.5 10824900.0 cm-1
1s1 2s1 4f1 2F2.5 10824900.0 cm-1
1s1 2s1 4s1 2S0.5 10870700.0 cm-1
1s1 2p1 4s1 4P0.5 10882500.0 cm-1
1s1 2p1 4s1 4P1.5 10883300.0 cm-1
1s1 2s1 4p1 2P0.5 10884600.0 cm-1
1s1 2p1 4s1 4P2.5 10884800.0 cm-1
1s1 2s1 4p1 2P1.5 10885000.0 cm-1
1s1 2p1 4p1 4D0.5 10894300.0 cm-1
1s1 2p1 4p1 4D1.5 10894800.0 cm-1
1s1 2p1 4s1 2P0.5 10895600.0 cm-1
1s1 2p1 4p1 4D2.5 10895600.0 cm-1
1s1 2p1 4p1 4D3.5 10896800.0 cm-1
1s1 2p1 4s1 2P1.5 10897300.0 cm-1
1s1 2p1 4p1 2P0.5 10897900.0 cm-1
1s1 2p1 4p1 2P1.5 10898400.0 cm-1
1s1 2s1 4d1 2D1.5 10898700.0 cm-1
1s1 2s1 4d1 2D2.5 10898800.0 cm-1
1s1 2p1 4p1 4S1.5 10900800.0 cm-1
1s1 2p1 4p1 4P0.5 10901500.0 cm-1
1s1 2p1 4p1 4P1.5 10902500.0 cm-1
1s1 2p1 4p1 4P2.5 10902800.0 cm-1
1s1 2p1 4d1 4F1.5 10905200.0 cm-1
1s1 2p1 4d1 4F2.5 10905800.0 cm-1
1s1 2s1 4f1 2F2.5 10906400.0 cm-1
1s1 2p1 4d1 4F3.5 10906500.0 cm-1
1s1 2s1 4f1 2F3.5 10906600.0 cm-1
1s1 2p1 4d1 2D1.5 10907200.0 cm-1
1s1 2p1 4d1 2D2.5 10907500.0 cm-1
1s1 2p1 4d1 4F4.5 10907500.0 cm-1
1s1 2p1 4p1 2D1.5 10908600.0 cm-1
1s1 2p1 4p1 2D2.5 10910000.0 cm-1
1s1 2p1 4d1 4D0.5 10911400.0 cm-1
1s1 2p1 4d1 4D1.5 10911500.0 cm-1
1s1 2p1 4d1 4D2.5 10911700.0 cm-1
1s1 2p1 4d1 4D3.5 10912300.0 cm-1
1s1 2p1 4f1 2F2.5 10913300.0 cm-1
1s1 2p1 4f1 2F3.5 10913600.0 cm-1
1s1 2p1 4f1 4F2.5 10913700.0 cm-1
1s1 2p1 4f1 4F1.5 10913700.0 cm-1
1s1 2p1 4f1 4F3.5 10913900.0 cm-1
1s1 2p1 4f1 4F4.5 10914200.0 cm-1
1s1 2p1 4d1 4P2.5 10914900.0 cm-1
1s1 2p1 4d1 4P1.5 10915400.0 cm-1
1s1 2p1 4d1 4P0.5 10915700.0 cm-1
1s1 2p1 4f1 4G2.5 10916500.0 cm-1
1s1 2p1 4f1 4G3.5 10916900.0 cm-1
1s1 2p1 4f1 4G4.5 10917600.0 cm-1
1s1 2p1 4f1 4G5.5 10918300.0 cm-1
1s1 2p1 4d1 2F2.5 10919000.0 cm-1
1s1 2p1 4f1 2G3.5 10919000.0 cm-1
1s1 2p1 4f1 4D3.5 10920200.0 cm-1
1s1 2p1 4f1 2G4.5 10920400.0 cm-1
1s1 2p1 4p1 2S0.5 10920500.0 cm-1
1s1 2p1 4d1 2F3.5 10920500.0 cm-1
1s1 2p1 4f1 4D2.5 10920900.0 cm-1
1s1 2p1 4f1 4D1.5 10921400.0 cm-1
1s1 2p1 4f1 4D0.5 10921700.0 cm-1
1s1 2p1 4f1 2D2.5 10922500.0 cm-1
1s1 2p1 4d1 2P1.5 10922900.0 cm-1
1s1 2p1 4f1 2D1.5 10923300.0 cm-1
1s1 2p1 4d1 2P0.5 10923900.0 cm-1
1s1 2p1 4s1 2P0.5 10944500.0 cm-1
1s1 2p1 4s1 2P1.5 10944500.0 cm-1
1s1 2p1 4p1 2D1.5 10957900.0 cm-1
1s1 2p1 4p1 2D2.5 10957900.0 cm-1
1s1 2p1 4p1 2P0.5 10958100.0 cm-1
1s1 2p1 4p1 2P1.5 10958400.0 cm-1
1s1 2p1 4p1 2S0.5 10966100.0 cm-1
1s1 2p1 4d1 2D1.5 10967200.0 cm-1
1s1 2p1 4d1 2D2.5 10967300.0 cm-1
1s1 2p1 4d1 2F3.5 10968900.0 cm-1
1s1 2p1 4d1 2F2.5 10969200.0 cm-1
1s1 2p1 4f1 2F2.5 10970600.0 cm-1
1s1 2p1 4f1 2F3.5 10970700.0 cm-1
1s1 2p1 4f1 2G4.5 10974800.0 cm-1
1s1 2p1 4f1 2G3.5 10974800.0 cm-1
1s1 2p1 4d1 2P0.5 10975200.0 cm-1
1s1 2p1 4d1 2P1.5 10975500.0 cm-1
1s1 2p1 4f1 2D1.5 10978100.0 cm-1
1s1 2p1 4f1 2D2.5 10978200.0 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 = 1.27871
         2S = 1.02718
         2P = 0.91907
         3S = 1.01537
         3P = 0.91386
         3D = 0.84411
         4S = 1.01393
         4P = 0.91293
         4D = 0.84623
         4F = 0.90169
         5S = 1.01539
         5P = 0.91441
         5D = 0.84784
         5F = 0.83768
         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 311.7242 Rydbergs (4241.319465 eV)

 A fine energy mesh of 0.000004 Z**2 Rydbergs (0.003483136 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (8.70784 eV) was used
 from the last threshold up to 3.701262 Z**2 Rydbergs (3223 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (8.70784 eV) was used
 from first threshold up to 3.701262 Z**2 Rydbergs (3223 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 = 1.28265
         2S = 1.02943
         2P = 0.92257
         3S = 1.01811
         3P = 0.91491
         3D = 0.84839
         4S = 1.01778
         4P = 0.91587
         4D = 0.85351
         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 322.1583 Rydbergs (4383.285830 eV)

 A fine energy mesh of 0.000010 Z**2 Rydbergs (0.00870784 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (8.70784 eV) was used
 from the last threshold up to 3.701262 Z**2 Rydbergs (3223 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (8.70784 eV) was used
 from first threshold up to 3.701262 Z**2 Rydbergs (3223 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   1.31279
  3   1.33672
  4  12.5386
  5  12.8978
  6  12.9047
  7  13.031
  8  13.033
  9  16.7705
 10  16.9171
 11  16.9201
 12  16.9701
 13  16.9730
 14  16.9763
 15  16.9767
 16  18.6948
 17  18.7685
 18  18.7685
 19  18.7982
 20  18.7986
 25  80.334
 26  80.688
 27  80.694
 28  80.711
 29  81.683
 30  81.697
 31  82.087
 32  82.098
 33  82.110
 34  82.168
 35  82.174
 36  82.703
 37  82.710
 38  82.881
 39  82.904
 40  83.644

 Produced by: Guiyun Liang
 Date:        20/05/10
------------------------------------------------------------------------

Contributors

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

Data Classes