lilike_lgy10#cr21.dat

Resolved Specific Ion Data Collections

Ion
Cr21+
Temperature Range
8.341 eV → 8.341 x 104 eV

ADF04

Filename
lilike_lgy10#cr21.dat
Full Path
adf04/copaw#li/lilike_lgy10#cr21.dat
Download data
  • Spontaneous Emission: Cr+21(i) → Cr+21(j) + hv
  • Electron Impact Excitation: Cr+21(i) + e → Cr+21(j) + e
2s1 2S0.5 0.0 cm-1
2p1 2P0.5 357874.0 cm-1
2p1 2P1.5 447633.0 cm-1
3s1 2S0.5 7806360.0 cm-1
3p1 2P0.5 7905500.0 cm-1
3p1 2P1.5 7931610.0 cm-1
3d1 2D1.5 7970860.0 cm-1
3d1 2D2.5 7979320.0 cm-1
4s1 2S0.5 10491600.0 cm-1
4p1 2P0.5 10532400.0 cm-1
4p1 2P1.5 10543200.0 cm-1
4d1 2D1.5 10559500.0 cm-1
4d1 2D2.5 10563000.0 cm-1
4f1 2F2.5 10563900.0 cm-1
4f1 2F3.5 10565700.0 cm-1
5s1 2S0.5 11723500.0 cm-1
5p1 2P0.5 11744100.0 cm-1
5p1 2P1.5 11749500.0 cm-1
5d1 2D1.5 11757800.0 cm-1
5d1 2D2.5 11759600.0 cm-1
5f1 2F2.5 11760100.0 cm-1
5f1 2F3.5 11761000.0 cm-1
5g1 2G3.5 11761000.0 cm-1
5g1 2G4.5 11761500.0 cm-1
1s1 2s2 2S0.5 45199100.0 cm-1
1s1 2s1 2p1 4P0.5 45286000.0 cm-1
1s1 2s1 2p1 4P1.5 45312800.0 cm-1
1s1 2s1 2p1 4P2.5 45370100.0 cm-1
1s1 2s1 2p1 2P0.5 45579800.0 cm-1
1s1 2s1 2p1 2P1.5 45628000.0 cm-1
1s1 2p2 4P0.5 45700100.0 cm-1
1s1 2s1 2p1 2P0.5 45733500.0 cm-1
1s1 2p2 4P1.5 45738300.0 cm-1
1s1 2s1 2p1 2P1.5 45750700.0 cm-1
1s1 2p2 4P2.5 45780800.0 cm-1
1s1 2p2 2D1.5 45925800.0 cm-1
1s1 2p2 2P0.5 45951100.0 cm-1
1s1 2p2 2D2.5 45954100.0 cm-1
1s1 2p2 2P1.5 46038100.0 cm-1
1s1 2p2 2S0.5 46196800.0 cm-1
1s1 2s1 3s1 4S1.5 53152100.0 cm-1
1s1 2s1 3s1 2S0.5 53247200.0 cm-1
1s1 2s1 3p1 4P0.5 53277300.0 cm-1
1s1 2s1 3p1 4P1.5 53280900.0 cm-1
1s1 2s1 3p1 4P2.5 53300000.0 cm-1
1s1 2s1 3p1 2P1.5 53307500.0 cm-1
1s1 2s1 3p1 2P0.5 53308000.0 cm-1
1s1 2s1 3d1 4D0.5 53369700.0 cm-1
1s1 2s1 3d1 4D1.5 53372700.0 cm-1
1s1 2s1 3d1 4D2.5 53377200.0 cm-1
1s1 2s1 3d1 4D3.5 53383300.0 cm-1
1s1 2s1 3s1 2S0.5 53397000.0 cm-1
1s1 2s1 3d1 2D2.5 53426100.0 cm-1
1s1 2p1 3s1 4P0.5 53426100.0 cm-1
1s1 2s1 3d1 2D1.5 53426300.0 cm-1
1s1 2p1 3s1 4P1.5 53447800.0 cm-1
1s1 2s1 3p1 2P0.5 53484200.0 cm-1
1s1 2p1 3p1 4D0.5 53487000.0 cm-1
1s1 2p1 3p1 4D1.5 53503400.0 cm-1
1s1 2p1 3s1 4P2.5 53506400.0 cm-1
1s1 2s1 3p1 2P1.5 53508900.0 cm-1
1s1 2p1 3s1 2P0.5 53536700.0 cm-1
1s1 2p1 3p1 4D2.5 53539900.0 cm-1
1s1 2p1 3p1 2P1.5 53544100.0 cm-1
1s1 2p1 3p1 2P0.5 53561100.0 cm-1
1s1 2p1 3p1 4P0.5 53580900.0 cm-1
1s1 2p1 3d1 4F1.5 53581800.0 cm-1
1s1 2p1 3p1 4D3.5 53593400.0 cm-1
1s1 2p1 3p1 4S1.5 53593900.0 cm-1
1s1 2p1 3d1 4F2.5 53597400.0 cm-1
1s1 2p1 3s1 2P1.5 53605000.0 cm-1
1s1 2s1 3d1 2D1.5 53605600.0 cm-1
1s1 2s1 3d1 2D2.5 53611700.0 cm-1
1s1 2p1 3p1 4P1.5 53621200.0 cm-1
1s1 2p1 3d1 4F3.5 53624500.0 cm-1
1s1 2p1 3d1 2D2.5 53629600.0 cm-1
1s1 2p1 3p1 2D1.5 53634300.0 cm-1
1s1 2p1 3d1 2D1.5 53636200.0 cm-1
1s1 2p1 3p1 4P2.5 53636400.0 cm-1
1s1 2p1 3d1 4D0.5 53660100.0 cm-1
1s1 2p1 3d1 4D1.5 53662400.0 cm-1
1s1 2p1 3d1 4D2.5 53666400.0 cm-1
1s1 2p1 3d1 4F4.5 53671400.0 cm-1
1s1 2p1 3s1 2P1.5 53671600.0 cm-1
1s1 2p1 3s1 2P0.5 53678300.0 cm-1
1s1 2p1 3p1 2D2.5 53688500.0 cm-1
1s1 2p1 3d1 2F2.5 53699500.0 cm-1
1s1 2p1 3d1 4D3.5 53710600.0 cm-1
1s1 2p1 3p1 2S0.5 53713300.0 cm-1
1s1 2p1 3d1 4P2.5 53727500.0 cm-1
1s1 2p1 3d1 4P1.5 53728900.0 cm-1
1s1 2p1 3d1 4P0.5 53732400.0 cm-1
1s1 2p1 3d1 2F3.5 53744500.0 cm-1
1s1 2p1 3d1 2P1.5 53758100.0 cm-1
1s1 2p1 3p1 2P0.5 53764600.0 cm-1
1s1 2p1 3p1 2D1.5 53765900.0 cm-1
1s1 2p1 3p1 2D2.5 53774000.0 cm-1
1s1 2p1 3d1 2P0.5 53791600.0 cm-1
1s1 2p1 3p1 2P1.5 53795200.0 cm-1
1s1 2p1 3p1 2S0.5 53841000.0 cm-1
1s1 2p1 3d1 2D1.5 53842100.0 cm-1
1s1 2p1 3d1 2D2.5 53847100.0 cm-1
1s1 2p1 3d1 2F3.5 53863500.0 cm-1
1s1 2p1 3d1 2F2.5 53879100.0 cm-1
1s1 2p1 3d1 2P0.5 53891000.0 cm-1
1s1 2p1 3d1 2P1.5 53907400.0 cm-1
1s1 2s1 4s1 4S1.5 55927300.0 cm-1
1s1 2s1 4s1 2S0.5 55958600.0 cm-1
1s1 2s1 4p1 4P0.5 55973200.0 cm-1
1s1 2s1 4p1 4P1.5 55975400.0 cm-1
1s1 2s1 4p1 4P2.5 55981900.0 cm-1
1s1 2s1 4p1 2P1.5 55992900.0 cm-1
1s1 2s1 4p1 2P0.5 55994800.0 cm-1
1s1 2s1 4d1 4D0.5 56012200.0 cm-1
1s1 2s1 4d1 4D1.5 56012900.0 cm-1
1s1 2s1 4d1 4D2.5 56014100.0 cm-1
1s1 2s1 4d1 4D3.5 56016000.0 cm-1
1s1 2s1 4d1 2D2.5 56029600.0 cm-1
1s1 2s1 4d1 2D1.5 56030300.0 cm-1
1s1 2s1 4f1 4F1.5 56038900.0 cm-1
1s1 2s1 4f1 4F2.5 56039300.0 cm-1
1s1 2s1 4f1 4F3.5 56039900.0 cm-1
1s1 2s1 4f1 4F4.5 56040900.0 cm-1
1s1 2s1 4f1 2F3.5 56044700.0 cm-1
1s1 2s1 4f1 2F2.5 56045200.0 cm-1
1s1 2s1 4s1 2S0.5 56149600.0 cm-1
1s1 2p1 4s1 4P0.5 56157400.0 cm-1
1s1 2p1 4s1 4P1.5 56175000.0 cm-1
1s1 2s1 4p1 2P0.5 56186300.0 cm-1
1s1 2p1 4p1 4D0.5 56186400.0 cm-1
1s1 2s1 4p1 2P1.5 56199600.0 cm-1
1s1 2p1 4p1 4D1.5 56200000.0 cm-1
1s1 2p1 4s1 2P0.5 56200500.0 cm-1
1s1 2p1 4p1 4S1.5 56211500.0 cm-1
1s1 2p1 4p1 4D2.5 56219600.0 cm-1
1s1 2p1 4p1 4P0.5 56223900.0 cm-1
1s1 2p1 4d1 4F1.5 56225200.0 cm-1
1s1 2s1 4d1 2D1.5 56230600.0 cm-1
1s1 2p1 4p1 2P0.5 56232100.0 cm-1
1s1 2s1 4d1 2D2.5 56234900.0 cm-1
1s1 2p1 4d1 4F2.5 56235200.0 cm-1
1s1 2p1 4p1 2D1.5 56238200.0 cm-1
1s1 2p1 4s1 4P2.5 56240200.0 cm-1
1s1 2p1 4d1 4D2.5 56246200.0 cm-1
1s1 2p1 4f1 4G2.5 56250400.0 cm-1
1s1 2p1 4f1 4F3.5 56253100.0 cm-1
1s1 2s1 4f1 2F2.5 56254000.0 cm-1
1s1 2p1 4d1 4F3.5 56254700.0 cm-1
1s1 2s1 4f1 2F3.5 56255100.0 cm-1
1s1 2p1 4d1 2D1.5 56255600.0 cm-1
1s1 2p1 4d1 4D0.5 56260800.0 cm-1
1s1 2p1 4d1 4D1.5 56260900.0 cm-1
1s1 2p1 4s1 2P1.5 56266500.0 cm-1
1s1 2p1 4d1 2F2.5 56268000.0 cm-1
1s1 2p1 4f1 4G3.5 56269100.0 cm-1
1s1 2p1 4f1 4F1.5 56269600.0 cm-1
1s1 2p1 4f1 2F2.5 56270200.0 cm-1
1s1 2p1 4f1 4G4.5 56272000.0 cm-1
1s1 2p1 4f1 2D2.5 56275600.0 cm-1
1s1 2p1 4f1 4D3.5 56277700.0 cm-1
1s1 2p1 4p1 4D3.5 56280800.0 cm-1
1s1 2p1 4p1 4P1.5 56284100.0 cm-1
1s1 2p1 4p1 4P2.5 56286300.0 cm-1
1s1 2p1 4p1 2P1.5 56293700.0 cm-1
1s1 2p1 4p1 2D2.5 56310200.0 cm-1
1s1 2p1 4d1 4F4.5 56312400.0 cm-1
1s1 2p1 4d1 2D2.5 56319100.0 cm-1
1s1 2p1 4d1 4D3.5 56320000.0 cm-1
1s1 2p1 4p1 2S0.5 56323300.0 cm-1
1s1 2p1 4d1 4P1.5 56326900.0 cm-1
1s1 2p1 4d1 4P2.5 56327700.0 cm-1
1s1 2p1 4d1 4P0.5 56328900.0 cm-1
1s1 2p1 4d1 2P1.5 56335100.0 cm-1
1s1 2p1 4f1 2F3.5 56336200.0 cm-1
1s1 2p1 4f1 4F4.5 56337400.0 cm-1
1s1 2p1 4f1 4F2.5 56339000.0 cm-1
1s1 2p1 4f1 2G3.5 56340100.0 cm-1
1s1 2p1 4d1 2F3.5 56341200.0 cm-1
1s1 2p1 4f1 4G5.5 56342300.0 cm-1
1s1 2p1 4f1 4D1.5 56344300.0 cm-1
1s1 2p1 4f1 2G4.5 56345200.0 cm-1
1s1 2p1 4f1 4D2.5 56345500.0 cm-1
1s1 2p1 4f1 4D0.5 56347800.0 cm-1
1s1 2p1 4d1 2P0.5 56349400.0 cm-1
1s1 2p1 4f1 2D1.5 56351700.0 cm-1
1s1 2p1 4s1 2P0.5 56384800.0 cm-1
1s1 2p1 4s1 2P1.5 56385400.0 cm-1
1s1 2p1 4p1 2P0.5 56419500.0 cm-1
1s1 2p1 4p1 2D1.5 56420000.0 cm-1
1s1 2p1 4p1 2D2.5 56425600.0 cm-1
1s1 2p1 4p1 2P1.5 56430400.0 cm-1
1s1 2p1 4p1 2S0.5 56443100.0 cm-1
1s1 2p1 4d1 2D1.5 56453200.0 cm-1
1s1 2p1 4d1 2D2.5 56455500.0 cm-1
1s1 2p1 4d1 2F3.5 56456300.0 cm-1
1s1 2p1 4d1 2F2.5 56462700.0 cm-1
1s1 2p1 4f1 2F2.5 56466000.0 cm-1
1s1 2p1 4f1 2F3.5 56467600.0 cm-1
1s1 2p1 4d1 2P0.5 56468700.0 cm-1
1s1 2p1 4d1 2P1.5 56474900.0 cm-1
1s1 2p1 4f1 2G3.5 56476300.0 cm-1
1s1 2p1 4f1 2G4.5 56476700.0 cm-1
1s1 2p1 4f1 2D1.5 56481500.0 cm-1
1s1 2p1 4f1 2D2.5 56483800.0 cm-1
R+21        24        22      13800147.(  )
------------------------------------------------------------------------

        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 = 1.28236
         2S = 1.04549
         2P = 0.94745
         3S = 1.03251
         3P = 0.93970
         3D = 0.87677
         4S = 1.03066
         4P = 0.93913
         4D = 0.87820
         4F = 1.03462
         5S = 1.03234
         5P = 0.94087
         5D = 0.88204
         5F = 0.85563
         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 1671.4105 Rydbergs (22741.211263 eV)

 A fine energy mesh of 0.000004 Z**2 Rydbergs (0.024000984 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (60.00246 eV) was used
 from the last threshold up to 2.851550 Z**2 Rydbergs (17110 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (60.00246 eV) was used
 from first threshold up to 2.851550 Z**2 Rydbergs (17110 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 = 1.28744
         2S = 1.04729
         2P = 0.94961
         3S = 1.03408
         3P = 0.94043
         3D = 0.88409
         4S = 1.03412
         4P = 0.94162
         4D = 0.88829
         4F = 1.03573

 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 1499.8035 Rydbergs (20406.326421 eV)

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.03000123 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (60.00246 eV) was used
 from the last threshold up to 2.851550 Z**2 Rydbergs (17110 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (60.00246 eV) was used
 from first threshold up to 2.851550 Z**2 Rydbergs (17110 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    3.25756
   3    4.08607
   4   71.10243
   5   72.00541
   6   72.25090
   7   72.59445
   8   72.67172
   9   95.557285
  10   95.936555
  11   96.040075
  12   96.184784
  13   96.217407
  16  106.78355
  17  106.97719
  18  107.03014
  19  107.10413
  20  107.12090
  25  411.12724
  26  411.94738
  27  412.14786
  29  414.60828
  30  415.06392
  31  415.72914
  32  416.01163
  33  416.13921
  34  416.17566
  35  416.46727
  36  417.77949
  37  417.92529
  38  418.00731
  39  418.81834
  40  420.21258
  84  488.44825
  96  489.08614
  97  489.16815
  99  489.32307
 102  489.85160
 103  490.00652
 190  513.35318

 Produced by: Guiyun Liang
 Date:        23/08/10
------------------------------------------------------------------------

Contributors

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

Data Classes