lilike_lgy10#fe23.dat

Resolved Specific Ion Data Collections

Ion
Fe23+
Temperature Range
9.909 eV → 9.909 x 104 eV

ADF04

Filename
lilike_lgy10#fe23.dat
Full Path
adf04/copaw#li/lilike_lgy10#fe23.dat
Download data
  • Spontaneous Emission: Fe+23(i) → Fe+23(j) + hv
  • Electron Impact Excitation: Fe+23(i) + e → Fe+23(j) + e
2s1 2S0.5 0.0 cm-1
2p1 2P0.5 392244.0 cm-1
2p1 2P1.5 519199.0 cm-1
3s1 2S0.5 9273970.0 cm-1
3p1 2P0.5 9382640.0 cm-1
3p1 2P1.5 9419480.0 cm-1
3d1 2D1.5 9462840.0 cm-1
3d1 2D2.5 9474830.0 cm-1
4s1 2S0.5 12467000.0 cm-1
4p1 2P0.5 12511700.0 cm-1
4p1 2P1.5 12526900.0 cm-1
4d1 2D1.5 12544800.0 cm-1
4d1 2D2.5 12549900.0 cm-1
4f1 2F2.5 12550800.0 cm-1
4f1 2F3.5 12553400.0 cm-1
5s1 2S0.5 13932300.0 cm-1
5p1 2P0.5 13954900.0 cm-1
5p1 2P1.5 13962400.0 cm-1
5d1 2D1.5 13971500.0 cm-1
5d1 2D2.5 13974100.0 cm-1
5f1 2F2.5 13974600.0 cm-1
5f1 2F3.5 13975900.0 cm-1
5g1 2G3.5 13975900.0 cm-1
5g1 2G4.5 13976700.0 cm-1
1s1 2s2 2S0.5 53342000.0 cm-1
1s1 2s1 2p1 4P0.5 53436600.0 cm-1
1s1 2s1 2p1 4P1.5 53472900.0 cm-1
1s1 2s1 2p1 4P2.5 53555900.0 cm-1
1s1 2s1 2p1 2P0.5 53761900.0 cm-1
1s1 2s1 2p1 2P1.5 53833300.0 cm-1
1s1 2p2 4P0.5 53902600.0 cm-1
1s1 2s1 2p1 2P0.5 53945400.0 cm-1
1s1 2p2 4P1.5 53960000.0 cm-1
1s1 2s1 2p1 2P1.5 53967900.0 cm-1
1s1 2p2 4P2.5 54015900.0 cm-1
1s1 2p2 2D1.5 54165100.0 cm-1
1s1 2p2 2P0.5 54185500.0 cm-1
1s1 2p2 2D2.5 54212900.0 cm-1
1s1 2p2 2P1.5 54313100.0 cm-1
1s1 2p2 2S0.5 54476400.0 cm-1
1s1 2s1 3s1 4S1.5 62772800.0 cm-1
1s1 2s1 3s1 2S0.5 62878100.0 cm-1
1s1 2s1 3p1 4P0.5 62910300.0 cm-1
1s1 2s1 3p1 4P1.5 62914900.0 cm-1
1s1 2s1 3p1 4P2.5 62942700.0 cm-1
1s1 2s1 3p1 2P1.5 62951200.0 cm-1
1s1 2s1 3p1 2P0.5 62951600.0 cm-1
1s1 2s1 3d1 4D0.5 63018300.0 cm-1
1s1 2s1 3d1 4D1.5 63022400.0 cm-1
1s1 2s1 3d1 4D2.5 63028700.0 cm-1
1s1 2s1 3d1 4D3.5 63037100.0 cm-1
1s1 2s1 3s1 2S0.5 63042600.0 cm-1
1s1 2p1 3s1 4P0.5 63073900.0 cm-1
1s1 2s1 3d1 2D2.5 63082400.0 cm-1
1s1 2s1 3d1 2D1.5 63082900.0 cm-1
1s1 2p1 3s1 4P1.5 63102100.0 cm-1
1s1 2s1 3p1 2P0.5 63139600.0 cm-1
1s1 2p1 3p1 4D0.5 63139800.0 cm-1
1s1 2p1 3p1 4D1.5 63161000.0 cm-1
1s1 2s1 3p1 2P1.5 63175700.0 cm-1
1s1 2p1 3s1 4P2.5 63188100.0 cm-1
1s1 2p1 3s1 2P0.5 63194600.0 cm-1
1s1 2p1 3p1 2P1.5 63211500.0 cm-1
1s1 2p1 3p1 4D2.5 63211800.0 cm-1
1s1 2p1 3p1 2P0.5 63236600.0 cm-1
1s1 2p1 3p1 4P0.5 63251600.0 cm-1
1s1 2p1 3d1 4F1.5 63252000.0 cm-1
1s1 2p1 3p1 2D1.5 63270700.0 cm-1
1s1 2p1 3d1 4F2.5 63272300.0 cm-1
1s1 2s1 3d1 2D1.5 63280900.0 cm-1
1s1 2s1 3d1 2D2.5 63289800.0 cm-1
1s1 2p1 3p1 4D3.5 63291200.0 cm-1
1s1 2p1 3s1 2P1.5 63291400.0 cm-1
1s1 2p1 3d1 2D2.5 63308500.0 cm-1
1s1 2p1 3d1 4F3.5 63309100.0 cm-1
1s1 2p1 3p1 4P1.5 63311100.0 cm-1
1s1 2p1 3d1 2D1.5 63320400.0 cm-1
1s1 2p1 3p1 4S1.5 63329700.0 cm-1
1s1 2p1 3p1 4P2.5 63330300.0 cm-1
1s1 2p1 3d1 4D0.5 63343000.0 cm-1
1s1 2p1 3d1 4D1.5 63345600.0 cm-1
1s1 2p1 3d1 2F2.5 63349600.0 cm-1
1s1 2p1 3s1 2P1.5 63365000.0 cm-1
1s1 2p1 3s1 2P0.5 63372400.0 cm-1
1s1 2p1 3d1 4F4.5 63380100.0 cm-1
1s1 2p1 3p1 2D2.5 63393200.0 cm-1
1s1 2p1 3d1 4D2.5 63405600.0 cm-1
1s1 2p1 3p1 2S0.5 63412100.0 cm-1
1s1 2p1 3d1 4D3.5 63419300.0 cm-1
1s1 2p1 3d1 4P1.5 63438400.0 cm-1
1s1 2p1 3d1 4P2.5 63439300.0 cm-1
1s1 2p1 3d1 4P0.5 63443000.0 cm-1
1s1 2p1 3d1 2F3.5 63459100.0 cm-1
1s1 2p1 3d1 2P1.5 63466900.0 cm-1
1s1 2p1 3p1 2P0.5 63468000.0 cm-1
1s1 2p1 3p1 2D1.5 63468600.0 cm-1
1s1 2p1 3p1 2D2.5 63482300.0 cm-1
1s1 2p1 3d1 2P0.5 63509700.0 cm-1
1s1 2p1 3p1 2P1.5 63510100.0 cm-1
1s1 2p1 3p1 2S0.5 63556300.0 cm-1
1s1 2p1 3d1 2D1.5 63561100.0 cm-1
1s1 2p1 3d1 2D2.5 63567000.0 cm-1
1s1 2p1 3d1 2F3.5 63583500.0 cm-1
1s1 2p1 3d1 2F2.5 63604400.0 cm-1
1s1 2p1 3d1 2P0.5 63610900.0 cm-1
1s1 2p1 3d1 2P1.5 63633300.0 cm-1
1s1 2s1 4s1 4S1.5 66063600.0 cm-1
1s1 2s1 4s1 2S0.5 66098200.0 cm-1
1s1 2s1 4p1 4P0.5 66114100.0 cm-1
1s1 2s1 4p1 4P1.5 66116900.0 cm-1
1s1 2s1 4p1 4P2.5 66126500.0 cm-1
1s1 2s1 4p1 2P1.5 66138300.0 cm-1
1s1 2s1 4p1 2P0.5 66140700.0 cm-1
1s1 2s1 4d1 4D0.5 66159700.0 cm-1
1s1 2s1 4d1 4D1.5 66160700.0 cm-1
1s1 2s1 4d1 4D2.5 66162300.0 cm-1
1s1 2s1 4d1 4D3.5 66165100.0 cm-1
1s1 2s1 4d1 2D2.5 66179400.0 cm-1
1s1 2s1 4d1 2D1.5 66180500.0 cm-1
1s1 2s1 4f1 4F1.5 66190000.0 cm-1
1s1 2s1 4f1 4F2.5 66190500.0 cm-1
1s1 2s1 4f1 4F3.5 66191200.0 cm-1
1s1 2s1 4f1 4F4.5 66192700.0 cm-1
1s1 2s1 4f1 2F3.5 66196600.0 cm-1
1s1 2s1 4f1 2F2.5 66197300.0 cm-1
1s1 2s1 4s1 2S0.5 66308200.0 cm-1
1s1 2p1 4s1 4P0.5 66315800.0 cm-1
1s1 2p1 4s1 4P1.5 66338100.0 cm-1
1s1 2p1 4p1 4D0.5 66347300.0 cm-1
1s1 2s1 4p1 2P0.5 66349700.0 cm-1
1s1 2p1 4s1 2P0.5 66364600.0 cm-1
1s1 2p1 4p1 4D1.5 66365500.0 cm-1
1s1 2s1 4p1 2P1.5 66367200.0 cm-1
1s1 2p1 4p1 4S1.5 66378000.0 cm-1
1s1 2p1 4p1 4D2.5 66390400.0 cm-1
1s1 2p1 4d1 4F1.5 66393200.0 cm-1
1s1 2p1 4p1 4P0.5 66393800.0 cm-1
1s1 2s1 4d1 2D1.5 66400200.0 cm-1
1s1 2p1 4p1 2P0.5 66404600.0 cm-1
1s1 2p1 4d1 4F2.5 66406700.0 cm-1
1s1 2s1 4d1 2D2.5 66406700.0 cm-1
1s1 2p1 4p1 2D1.5 66410200.0 cm-1
1s1 2p1 4d1 4D2.5 66415800.0 cm-1
1s1 2p1 4f1 4G2.5 66421600.0 cm-1
1s1 2p1 4f1 2G3.5 66425100.0 cm-1
1s1 2s1 4f1 2F2.5 66425500.0 cm-1
1s1 2s1 4f1 2F3.5 66428400.0 cm-1
1s1 2p1 4d1 4F3.5 66431200.0 cm-1
1s1 2p1 4d1 4D1.5 66431400.0 cm-1
1s1 2p1 4s1 4P2.5 66435600.0 cm-1
1s1 2p1 4d1 2D1.5 66436300.0 cm-1
1s1 2p1 4d1 4D0.5 66436400.0 cm-1
1s1 2p1 4d1 2F2.5 66445600.0 cm-1
1s1 2p1 4f1 4G3.5 66445800.0 cm-1
1s1 2p1 4f1 4F1.5 66446800.0 cm-1
1s1 2p1 4f1 2F2.5 66447900.0 cm-1
1s1 2p1 4f1 4G4.5 66449800.0 cm-1
1s1 2p1 4f1 2D2.5 66452800.0 cm-1
1s1 2p1 4f1 4D3.5 66455600.0 cm-1
1s1 2p1 4s1 2P1.5 66461600.0 cm-1
1s1 2p1 4p1 4D3.5 66481600.0 cm-1
1s1 2p1 4p1 4P1.5 66482000.0 cm-1
1s1 2p1 4p1 4P2.5 66484800.0 cm-1
1s1 2p1 4p1 2P1.5 66495400.0 cm-1
1s1 2p1 4p1 2D2.5 66512900.0 cm-1
1s1 2p1 4d1 4F4.5 66517500.0 cm-1
1s1 2p1 4d1 2D2.5 66523300.0 cm-1
1s1 2p1 4d1 4D3.5 66525000.0 cm-1
1s1 2p1 4p1 2S0.5 66525800.0 cm-1
1s1 2p1 4d1 4P1.5 66531900.0 cm-1
1s1 2p1 4d1 4P2.5 66533800.0 cm-1
1s1 2p1 4d1 4P0.5 66534300.0 cm-1
1s1 2p1 4d1 2P1.5 66541200.0 cm-1
1s1 2p1 4f1 2F3.5 66543400.0 cm-1
1s1 2p1 4f1 4F4.5 66545300.0 cm-1
1s1 2p1 4f1 4F2.5 66546400.0 cm-1
1s1 2p1 4f1 4F3.5 66548200.0 cm-1
1s1 2p1 4d1 2F3.5 66548200.0 cm-1
1s1 2p1 4f1 4G5.5 66550800.0 cm-1
1s1 2p1 4f1 4D1.5 66552100.0 cm-1
1s1 2p1 4f1 2G4.5 66553600.0 cm-1
1s1 2p1 4f1 4D2.5 66554000.0 cm-1
1s1 2p1 4f1 4D0.5 66556100.0 cm-1
1s1 2p1 4d1 2P0.5 66557300.0 cm-1
1s1 2p1 4f1 2D1.5 66560900.0 cm-1
1s1 2p1 4s1 2P0.5 66588900.0 cm-1
1s1 2p1 4s1 2P1.5 66589500.0 cm-1
1s1 2p1 4p1 2P0.5 66627100.0 cm-1
1s1 2p1 4p1 2D1.5 66627700.0 cm-1
1s1 2p1 4p1 2D2.5 66636200.0 cm-1
1s1 2p1 4p1 2P1.5 66642400.0 cm-1
1s1 2p1 4p1 2S0.5 66654700.0 cm-1
1s1 2p1 4d1 2D1.5 66667200.0 cm-1
1s1 2p1 4d1 2D2.5 66670100.0 cm-1
1s1 2p1 4d1 2F3.5 66670700.0 cm-1
1s1 2p1 4d1 2F2.5 66679000.0 cm-1
1s1 2p1 4f1 2F2.5 66682500.0 cm-1
1s1 2p1 4d1 2P0.5 66683100.0 cm-1
1s1 2p1 4f1 2F3.5 66684800.0 cm-1
1s1 2p1 4d1 2P1.5 66691500.0 cm-1
1s1 2p1 4f1 2G3.5 66693600.0 cm-1
1s1 2p1 4f1 2G4.5 66694300.0 cm-1
1s1 2p1 4f1 2D1.5 66698800.0 cm-1
1s1 2p1 4f1 2D2.5 66701900.0 cm-1
 Update: Guiyun Liang, 03/12/10
         Added the '-' sign for dipole transition
        Result of ICFT R-matrix calculation for outer shell excitation

        Result of ICFT R-matrix calculation
        +++++++++++++++++++++++++++++++++++

 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 = 1.28261
         2S = 1.04660
         2P = 0.94896
         3S = 1.03313
         3P = 0.94135
         3D = 0.87877
         4S = 1.03167
         4P = 0.94084
         4D = 0.88032
         4F = 1.04433
         5S = 1.03370
         5P = 0.94207
         5D = 0.88450
         5F = 0.85595
         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 1979.6869 Rydbergs (26935.619961 eV)

 A fine energy mesh of 0.000010 Z**2 Rydbergs (0.07197574 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (71.97574 eV) was used
 from the last threshold up to 2.813448 Z**2 Rydbergs (20250 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (71.97574 eV) was used
 from first threshold up to 2.813448 Z**2 Rydbergs (20250 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:        15/03/10
 Update: Guiyun Liang, 03/12/10
         Added the '-' sign for dipole transition
------------------------------------------------------------------------
        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 = 1.28785
         2S = 1.04836
         2P = 0.95095
         3S = 1.03526
         3P = 0.94230
         3D = 0.88497
         4S = 1.03517
         4P = 0.94333
         4D = 0.88903
         4F = 1.03849

 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 (0.07197574 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (71.97574 eV) was used
 from the last threshold up to 2.813448 Z**2 Rydbergs (20250 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.010000 Z**2 Rydbergs (71.97574 eV) was used
 from first threshold up to 2.813448 Z**2 Rydbergs (20250 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    3.57201
  3    4.74549
  4   84.49724
  5   85.46045
  6   85.81493
  7   86.19675
  8   86.32068
  9  113.58397
 10  113.98948
 11  114.13529
 12  114.26560
 13  114.32027
 14  114.34214
 15  114.37860
 16  126.89804
 17  127.06161
 18  127.13633
 19  127.21744
 20  127.26118
 25   485.12030
 26   486.09718
 27   486.31589
 29   489.02144
 30   489.64383
 31   490.30724
 32   490.70911
 33   490.91779
 34   490.90867
 35   491.33697
 36   492.63826
 37   492.77677
 38   493.10392
 39   494.08444
 40   495.48870
 43   572.18458
 57   573.82486
 81   576.65890
 83   576.00279
 93   577.29314
 96   577.30590
 97   577.45262
 100  579.31069

 Produced by: Guiyun Liang
 Date:        03/08/10
------------------------------------------------------------------------

Contributors

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

Data Classes