blike_lgy12#f4.dat

Resolved Specific Ion Data Collections

Ion
F4+
Temperature Range
0.431 eV → 4308 eV

ADF04

Filename
blike_lgy12#f4.dat
Full Path
adf04/copaw#b/blike_lgy12#f4.dat
Download data
  • Spontaneous Emission: F+4(i) → F+4(j) + hv
  • Electron Impact Excitation: F+4(i) + e → F+4(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 744.5 cm-1
2s1 2p2 4P0.5 85790.2 cm-1
2s1 2p2 4P1.5 86043.5 cm-1
2s1 2p2 4P2.5 86407.0 cm-1
2s1 2p2 2D1.5 152875.0 cm-1
2s1 2p2 2D2.5 152899.0 cm-1
2s1 2p2 2S0.5 197566.0 cm-1
2s1 2p2 2P0.5 214880.0 cm-1
2s1 2p2 2P1.5 215348.0 cm-1
2p3 4S1.5 276414.0 cm-1
2p3 2D1.5 307227.0 cm-1
2p3 2D2.5 307275.0 cm-1
2p3 2P0.5 347420.0 cm-1
2p3 2P1.5 347442.0 cm-1
2s2 3s1 2S0.5 522088.0 cm-1
2s2 3p1 2P0.5 562900.0 cm-1
2s2 3p1 2P1.5 563091.0 cm-1
2s2 3d1 2D1.5 601165.0 cm-1
2s2 3d1 2D2.5 601211.0 cm-1
2s1 2p1 3s1 4P0.5 619568.0 cm-1
2s1 2p1 3s1 4P1.5 619829.0 cm-1
2s1 2p1 3s1 4P2.5 620269.0 cm-1
2s1 2p1 3s1 2P0.5 640501.0 cm-1
2s1 2p1 3s1 2P1.5 640994.0 cm-1
2s1 2p1 3p1 2P0.5 654784.0 cm-1
2s1 2p1 3p1 2P1.5 655007.0 cm-1
2s1 2p1 3p1 4D0.5 656715.0 cm-1
2s1 2p1 3p1 4D1.5 656863.0 cm-1
2s1 2p1 3p1 4D2.5 657118.0 cm-1
2s1 2p1 3p1 4D3.5 657495.0 cm-1
2s1 2p1 3p1 4S1.5 664535.0 cm-1
2s1 2p1 3p1 4P0.5 669144.0 cm-1
2s1 2p1 3p1 4P1.5 669326.0 cm-1
2s1 2p1 3p1 4P2.5 669596.0 cm-1
2s1 2p1 3p1 2D1.5 676357.0 cm-1
2s1 2p1 3p1 2D2.5 676801.0 cm-1
2s1 2p1 3p1 2S0.5 689088.0 cm-1
2s1 2p1 3d1 4F1.5 692188.0 cm-1
2s1 2p1 3d1 4F2.5 692334.0 cm-1
2s1 2p1 3d1 4F3.5 692542.0 cm-1
2s1 2p1 3d1 4F4.5 692813.0 cm-1
2s1 2p1 3d1 4D0.5 700230.0 cm-1
2s1 2p1 3d1 4D1.5 700274.0 cm-1
2s1 2p1 3d1 4D2.5 700356.0 cm-1
2s1 2p1 3d1 4D3.5 700489.0 cm-1
2s1 2p1 3d1 2D1.5 702781.0 cm-1
2s1 2p1 3d1 2D2.5 702862.0 cm-1
2s1 2p1 3d1 4P2.5 704241.0 cm-1
2s1 2p1 3d1 4P1.5 704398.0 cm-1
2s1 2p1 3d1 4P0.5 704496.0 cm-1
2s2 4s1 2S0.5 715119.0 cm-1
2s1 2p1 3d1 2F2.5 719169.0 cm-1
2s1 2p1 3s1 2P1.5 719547.0 cm-1
2s1 2p1 3s1 2P0.5 719558.0 cm-1
2s1 2p1 3d1 2F3.5 719595.0 cm-1
2s1 2p1 3d1 2P1.5 724084.0 cm-1
2s1 2p1 3d1 2P0.5 724287.0 cm-1
2s2 4p1 2P0.5 733506.0 cm-1
2s2 4p1 2P1.5 733569.0 cm-1
2s2 4d1 2D1.5 746204.0 cm-1
2s2 4d1 2D2.5 746222.0 cm-1
2s2 4f1 2F2.5 748978.0 cm-1
2s2 4f1 2F3.5 748988.0 cm-1
2s1 2p1 3p1 2D1.5 760177.0 cm-1
2s1 2p1 3p1 2D2.5 760252.0 cm-1
2s1 2p1 3p1 2P0.5 760456.0 cm-1
2s1 2p1 3p1 2P1.5 760606.0 cm-1
2s1 2p1 3p1 2S0.5 772012.0 cm-1
2p2 3s1 4P0.5 785599.0 cm-1
2p2 3s1 4P1.5 785861.0 cm-1
2p2 3s1 4P2.5 786294.0 cm-1
2s1 2p1 3d1 2F2.5 798020.0 cm-1
2s1 2p1 3d1 2F3.5 798024.0 cm-1
2s1 2p1 3d1 2D1.5 799539.0 cm-1
2s1 2p1 3d1 2D2.5 799609.0 cm-1
2p2 3s1 2P0.5 803058.0 cm-1
2p2 3s1 2P1.5 803526.0 cm-1
2s1 2p1 3d1 2P0.5 808430.0 cm-1
2s1 2p1 3d1 2P1.5 808496.0 cm-1
2p2 3p1 2S0.5 811914.0 cm-1
2s1 2p1 4s1 4P0.5 813775.0 cm-1
2s1 2p1 4s1 4P1.5 813996.0 cm-1
2s1 2p1 4s1 4P2.5 814385.0 cm-1
2p2 3s1 2D1.5 818890.0 cm-1
2p2 3s1 2D2.5 818954.0 cm-1
2p2 3p1 4D0.5 819306.0 cm-1
2p2 3p1 4D1.5 819468.0 cm-1
2p2 3p1 4D2.5 819736.0 cm-1
2p2 3p1 4D3.5 820105.0 cm-1
2s1 2p1 4s1 2P0.5 820833.0 cm-1
2s1 2p1 4s1 2P1.5 821276.0 cm-1
2p2 3p1 4P0.5 827051.0 cm-1
2p2 3p1 4P1.5 827217.0 cm-1
2p2 3p1 4P2.5 827498.0 cm-1
2s1 2p1 4p1 4D0.5 829655.0 cm-1
2s1 2p1 4p1 4D1.5 829785.0 cm-1
2s1 2p1 4p1 4D2.5 830006.0 cm-1
2s1 2p1 4p1 4D3.5 830322.0 cm-1
2p2 3p1 2D1.5 831138.0 cm-1
2p2 3p1 2D2.5 831597.0 cm-1
2s1 2p1 4p1 4S1.5 833046.0 cm-1
2s1 2p1 4p1 4P0.5 834896.0 cm-1
2s1 2p1 4p1 4P1.5 835062.0 cm-1
2s1 2p1 4p1 4P2.5 835259.0 cm-1
2s1 2p1 4p1 2P0.5 836632.0 cm-1
2s1 2p1 4p1 2P1.5 836862.0 cm-1
2s1 2p1 4f1 4F1.5 840802.0 cm-1
2s1 2p1 4f1 4F2.5 840890.0 cm-1
2s1 2p1 4f1 4F3.5 841015.0 cm-1
2s1 2p1 4f1 4F4.5 841180.0 cm-1
2s1 2p1 4p1 2D1.5 841332.0 cm-1
2s1 2p1 4p1 2D2.5 841652.0 cm-1
2s1 2p1 4d1 4F1.5 842747.0 cm-1
2s1 2p1 4d1 4F2.5 842883.0 cm-1
2s1 2p1 4d1 4F3.5 843082.0 cm-1
2s1 2p1 4d1 4F4.5 843352.0 cm-1
2p2 3p1 2P1.5 843444.0 cm-1
2p2 3p1 2P0.5 843467.0 cm-1
2s1 2p1 4f1 2F2.5 844101.0 cm-1
2s1 2p1 4f1 2F3.5 844280.0 cm-1
2p2 3p1 4S1.5 845705.0 cm-1
2s1 2p1 4d1 4D0.5 845765.0 cm-1
2s1 2p1 4d1 4D1.5 845787.0 cm-1
2s1 2p1 4d1 4D2.5 845841.0 cm-1
2s1 2p1 4p1 2S0.5 845964.0 cm-1
2s1 2p1 4d1 4D3.5 846016.0 cm-1
2s1 2p1 4d1 4P2.5 846833.0 cm-1
2s1 2p1 4d1 4P1.5 847014.0 cm-1
2s1 2p1 4d1 4P0.5 847106.0 cm-1
2s1 2p1 4f1 4D3.5 847495.0 cm-1
2s1 2p1 4f1 4D2.5 847573.0 cm-1
2s1 2p1 4f1 4D1.5 847629.0 cm-1
2s1 2p1 4f1 4D0.5 847662.0 cm-1
2s1 2p1 4d1 2D1.5 847753.0 cm-1
2s1 2p1 4d1 2D2.5 847888.0 cm-1
2s1 2p1 4f1 2D2.5 851174.0 cm-1
2s1 2p1 4f1 2D1.5 851393.0 cm-1
2s1 2p1 4f1 4G2.5 851770.0 cm-1
2s1 2p1 4f1 4G3.5 851895.0 cm-1
2s1 2p1 4f1 4G4.5 852084.0 cm-1
2s1 2p1 4f1 4G5.5 852335.0 cm-1
2s1 2p1 4f1 2G3.5 852617.0 cm-1
2s1 2p1 4d1 2F2.5 852625.0 cm-1
2s1 2p1 4d1 2F3.5 852959.0 cm-1
2s1 2p1 4f1 2G4.5 852988.0 cm-1
2s1 2p1 4d1 2P1.5 855271.0 cm-1
2s1 2p1 4d1 2P0.5 855519.0 cm-1
2p2 3p1 2F2.5 857712.0 cm-1
2p2 3p1 2F3.5 857918.0 cm-1
2p2 3d1 2P1.5 858991.0 cm-1
2p2 3d1 2P0.5 859380.0 cm-1
2p2 3d1 4F1.5 860853.0 cm-1
2p2 3d1 4F2.5 860944.0 cm-1
2p2 3d1 4F3.5 861077.0 cm-1
2p2 3d1 4F4.5 861260.0 cm-1
2p2 3d1 4D1.5 864829.0 cm-1
2p2 3d1 4D0.5 864830.0 cm-1
2p2 3d1 4D2.5 864832.0 cm-1
2p2 3d1 4D3.5 864857.0 cm-1
2p2 3d1 4P2.5 867116.0 cm-1
2p2 3d1 4P1.5 867288.0 cm-1
2p2 3d1 4P0.5 867385.0 cm-1
2p2 3d1 2F2.5 867573.0 cm-1
2p2 3d1 2F3.5 867961.0 cm-1
2p2 3p1 2D2.5 871897.0 cm-1
2p2 3p1 2D1.5 871930.0 cm-1
2p2 3p1 2P0.5 881350.0 cm-1
2p2 3p1 2P1.5 881612.0 cm-1
2p2 3d1 2G3.5 884253.0 cm-1
2p2 3d1 2G4.5 884284.0 cm-1
2p2 3s1 2S0.5 884903.0 cm-1
2p2 3d1 2D2.5 887467.0 cm-1
2p2 3d1 2D1.5 887493.0 cm-1
2p2 3d1 2D1.5 894216.0 cm-1
2p2 3d1 2D2.5 894412.0 cm-1
2p2 3d1 2F3.5 894984.0 cm-1
2p2 3d1 2F2.5 895099.0 cm-1
2p2 3d1 2P0.5 903111.0 cm-1
2p2 3d1 2P1.5 903276.0 cm-1
2p2 3d1 2S0.5 909112.0 cm-1
2s1 2p1 4s1 2P0.5 914517.0 cm-1
2s1 2p1 4s1 2P1.5 914550.0 cm-1
2p2 3p1 2P0.5 927794.0 cm-1
2p2 3p1 2P1.5 927878.0 cm-1
2s1 2p1 4p1 2D1.5 928958.0 cm-1
2s1 2p1 4p1 2D2.5 928994.0 cm-1
2s1 2p1 4p1 2P0.5 932085.0 cm-1
2s1 2p1 4p1 2P1.5 932150.0 cm-1
2s1 2p1 4p1 2S0.5 936624.0 cm-1
2s1 2p1 4f1 2D2.5 940254.0 cm-1
2s1 2p1 4f1 2D1.5 940268.0 cm-1
2s1 2p1 4d1 2F3.5 942358.0 cm-1
2s1 2p1 4d1 2F2.5 942361.0 cm-1
2s1 2p1 4d1 2D1.5 943164.0 cm-1
2s1 2p1 4d1 2D2.5 943188.0 cm-1
2s1 2p1 4d1 2P0.5 946590.0 cm-1
2s1 2p1 4d1 2P1.5 946610.0 cm-1
2s1 2p1 4f1 2F2.5 948030.0 cm-1
2s1 2p1 4f1 2F3.5 948038.0 cm-1
2s1 2p1 4f1 2G3.5 951547.0 cm-1
2s1 2p1 4f1 2G4.5 951558.0 cm-1
2p2 3d1 2D2.5 967505.0 cm-1
2p2 3d1 2D1.5 967536.0 cm-1
------------------------------------------------------------------------

        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 = 1.40597
         2S = 1.24278
         2P = 1.17399
         3S = 1.64015
         3P = 1.34575
         3D = 1.43378
         4S = 1.54779
         4P = 1.33411
         4D = 1.48348
         4F = 2.31452

 An exchange calculation was performed up to J=12
 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 86.8959 Rydbergs (1182.305615 eV)

 A fine energy mesh of 0.000010 Z**2 Rydbergs (0.00217696 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.217696 eV) was used
 from the last threshold up to 1.574305 Z**2 Rydbergs (342.72 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.217696 eV) was used
 from first threshold up to 1.574305 Z**2 Rydbergs (342.72 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

 See:
      G Y Liang, N R Badnell and G Zhao
      A&A 547, A87 (2012)
      DOI: 10.1051/0004-6361/201220277

 Produced by: Guiyun Liang
 Date:        13/06/12

 Those data points with same collision strength in OMEGAU at higher energies
 are deleted. The adf04 file is generated based upon this correction.

 Date:  Tue May 28 19:59:27 2013
----------------------------------------------------------------------------

Contributors

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

Data Classes