flike_mcw06#fe17.dat

Resolved Specific Ion Data Collections

Ion
Fe17+
Temperature Range
5.584 eV → 5.584 x 104 eV

ADF04

Filename
flike_mcw06#fe17.dat
Full Path
adf04/copaw#f/flike_mcw06#fe17.dat
Download data
  • Spontaneous Emission: Fe+17(i) → Fe+17(j) + hv
  • Electron Impact Excitation: Fe+17(i) + e → Fe+17(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 104941.0 cm-1
2s1 2p6 2S0.5 1079520.0 cm-1
2s2 2p4 3s1 4P2.5 6231320.0 cm-1
2s2 2p4 3s1 2P1.5 6259140.0 cm-1
2s2 2p4 3s1 4P0.5 6311980.0 cm-1
2s2 2p4 3s1 4P1.5 6326440.0 cm-1
2s2 2p4 3s1 2P0.5 6353970.0 cm-1
2s2 2p4 3s1 2D2.5 6412090.0 cm-1
2s2 2p4 3s1 2D1.5 6415870.0 cm-1
2s2 2p4 3p1 4P1.5 6475610.0 cm-1
2s2 2p4 3p1 4P2.5 6479080.0 cm-1
2s2 2p4 3p1 4P0.5 6506540.0 cm-1
2s2 2p4 3p1 4D3.5 6511340.0 cm-1
2s2 2p4 3p1 2D2.5 6513020.0 cm-1
2s2 2p4 3p1 2P0.5 6563900.0 cm-1
2s2 2p4 3p1 4D1.5 6565290.0 cm-1
2s2 2p4 3p1 4D0.5 6569100.0 cm-1
2s2 2p4 3p1 2P1.5 6583360.0 cm-1
2s2 2p4 3s1 2S0.5 6592650.0 cm-1
2s2 2p4 3p1 4D2.5 6596440.0 cm-1
2s2 2p4 3p1 4S1.5 6602080.0 cm-1
2s2 2p4 3p1 2S0.5 6617650.0 cm-1
2s2 2p4 3p1 2D1.5 6622480.0 cm-1
2s2 2p4 3p1 2F2.5 6658950.0 cm-1
2s2 2p4 3p1 2F3.5 6679250.0 cm-1
2s2 2p4 3p1 2D1.5 6694440.0 cm-1
2s2 2p4 3p1 2D2.5 6706440.0 cm-1
2s2 2p4 3p1 2P1.5 6758000.0 cm-1
2s2 2p4 3p1 2P0.5 6785540.0 cm-1
2s2 2p4 3d1 4D2.5 6815250.0 cm-1
2s2 2p4 3d1 4D3.5 6816650.0 cm-1
2s2 2p4 3d1 4D1.5 6819970.0 cm-1
2s2 2p4 3d1 4D0.5 6829610.0 cm-1
2s2 2p4 3d1 4F4.5 6841830.0 cm-1
2s2 2p4 3d1 2F3.5 6852210.0 cm-1
2s2 2p4 3d1 4P0.5 6867770.0 cm-1
2s2 2p4 3p1 2P1.5 6871210.0 cm-1
2s2 2p4 3p1 2P0.5 6883790.0 cm-1
2s2 2p4 3d1 4P1.5 6884140.0 cm-1
2s2 2p4 3d1 2F2.5 6892260.0 cm-1
2s2 2p4 3d1 2P0.5 6907580.0 cm-1
2s2 2p4 3d1 4F1.5 6915150.0 cm-1
2s2 2p4 3d1 4F2.5 6917770.0 cm-1
2s2 2p4 3d1 4F3.5 6924700.0 cm-1
2s2 2p4 3d1 2D1.5 6927830.0 cm-1
2s2 2p4 3d1 4P2.5 6944920.0 cm-1
2s2 2p4 3d1 2P1.5 6959050.0 cm-1
2s2 2p4 3d1 2D2.5 6969520.0 cm-1
2s2 2p4 3d1 2G3.5 6999150.0 cm-1
2s2 2p4 3d1 2G4.5 7003400.0 cm-1
2s2 2p4 3d1 2F2.5 7027820.0 cm-1
2s2 2p4 3d1 2S0.5 7028600.0 cm-1
2s2 2p4 3d1 2F3.5 7039180.0 cm-1
2s2 2p4 3d1 2P1.5 7054330.0 cm-1
2s2 2p4 3d1 2D2.5 7059510.0 cm-1
2s2 2p4 3d1 2D1.5 7084680.0 cm-1
2s2 2p4 3d1 2P0.5 7090180.0 cm-1
2s1 2p5 3s1 4P2.5 7175370.0 cm-1
2s2 2p4 3d1 2D2.5 7203240.0 cm-1
2s1 2p5 3s1 4P1.5 7211530.0 cm-1
2s2 2p4 3d1 2D1.5 7219910.0 cm-1
2s1 2p5 3s1 4P0.5 7257140.0 cm-1
2s1 2p5 3s1 2P1.5 7265740.0 cm-1
2s1 2p5 3s1 2P0.5 7319460.0 cm-1
2s1 2p5 3p1 4S1.5 7407580.0 cm-1
2s1 2p5 3p1 4D2.5 7436740.0 cm-1
2s1 2p5 3p1 4D3.5 7444390.0 cm-1
2s1 2p5 3p1 4D1.5 7461000.0 cm-1
2s1 2p5 3p1 2D2.5 7473440.0 cm-1
2s1 2p5 3p1 4D0.5 7488150.0 cm-1
2s1 2p5 3p1 2P1.5 7501580.0 cm-1
2s1 2p5 3p1 4P2.5 7520590.0 cm-1
2s1 2p5 3p1 2P0.5 7523070.0 cm-1
2s1 2p5 3p1 4P1.5 7524660.0 cm-1
2s1 2p5 3p1 4P0.5 7530710.0 cm-1
2s1 2p5 3s1 2P1.5 7549250.0 cm-1
2s1 2p5 3s1 2P0.5 7555520.0 cm-1
2s1 2p5 3p1 2D1.5 7569420.0 cm-1
2s1 2p5 3p1 2S0.5 7606130.0 cm-1
2s1 2p5 3d1 4P0.5 7734760.0 cm-1
2s1 2p5 3d1 4P1.5 7744340.0 cm-1
2s1 2p5 3d1 4F4.5 7754160.0 cm-1
2s1 2p5 3d1 4P2.5 7760190.0 cm-1
2s1 2p5 3d1 4F3.5 7764020.0 cm-1
2s1 2p5 3d1 4F2.5 7784730.0 cm-1
2s1 2p5 3p1 2D1.5 7790080.0 cm-1
2s1 2p5 3d1 2F3.5 7799960.0 cm-1
2s1 2p5 3d1 4F1.5 7801920.0 cm-1
2s1 2p5 3p1 2D2.5 7812040.0 cm-1
2s1 2p5 3p1 2P0.5 7817420.0 cm-1
2s1 2p5 3p1 2P1.5 7827290.0 cm-1
2s1 2p5 3d1 4D0.5 7831330.0 cm-1
2s1 2p5 3d1 4D2.5 7844780.0 cm-1
2s1 2p5 3d1 2D2.5 7844970.0 cm-1
2s1 2p5 3d1 4D3.5 7845960.0 cm-1
2s1 2p5 3d1 4D1.5 7852900.0 cm-1
2s1 2p5 3d1 2D1.5 7859240.0 cm-1
2s1 2p5 3p1 2S0.5 7866900.0 cm-1
2s1 2p5 3d1 2P0.5 7887470.0 cm-1
2s1 2p5 3d1 2F2.5 7896370.0 cm-1
2s1 2p5 3d1 2P1.5 7945140.0 cm-1
2s1 2p5 3d1 2F2.5 8124140.0 cm-1
2s1 2p5 3d1 2F3.5 8126880.0 cm-1
2s1 2p5 3d1 2P1.5 8147130.0 cm-1
2s1 2p5 3d1 2D2.5 8153660.0 cm-1
2s1 2p5 3d1 2D1.5 8154260.0 cm-1
2s1 2p5 3d1 2P0.5 8156780.0 cm-1
2s2 2p4 4s1 4P2.5 8431040.0 cm-1
2s2 2p4 4s1 2P1.5 8439950.0 cm-1
2s2 2p4 4s1 4P0.5 8511100.0 cm-1
2s2 2p4 4s1 4P1.5 8519580.0 cm-1
2s2 2p4 4s1 2P0.5 8527280.0 cm-1
2s2 2p4 4p1 4P2.5 8532520.0 cm-1
2s2 2p4 4p1 4P1.5 8532540.0 cm-1
2s2 2p4 4p1 4D3.5 8542150.0 cm-1
2s2 2p4 4p1 2D2.5 8543160.0 cm-1
2s2 2p4 4p1 2S0.5 8546950.0 cm-1
2s2 2p4 4p1 2P1.5 8571260.0 cm-1
2s2 2p4 4s1 2D2.5 8603650.0 cm-1
2s2 2p4 4s1 2D1.5 8604800.0 cm-1
2s2 2p4 4p1 4D0.5 8612250.0 cm-1
2s2 2p4 4p1 4P0.5 8618020.0 cm-1
2s2 2p4 4p1 4D1.5 8619690.0 cm-1
2s2 2p4 4p1 4D2.5 8628370.0 cm-1
2s2 2p4 4p1 4S1.5 8633260.0 cm-1
2s2 2p4 4p1 2D1.5 8637860.0 cm-1
2s2 2p4 4p1 2P0.5 8643480.0 cm-1
2s2 2p4 4d1 4D2.5 8657090.0 cm-1
2s2 2p4 4d1 4D3.5 8657140.0 cm-1
2s2 2p4 4d1 4D1.5 8659180.0 cm-1
2s2 2p4 4d1 4P0.5 8662910.0 cm-1
2s2 2p4 4d1 4F4.5 8663940.0 cm-1
2s2 2p4 4d1 2F3.5 8668070.0 cm-1
2s2 2p4 4d1 2P0.5 8677200.0 cm-1
2s2 2p4 4d1 4P1.5 8687170.0 cm-1
2s2 2p4 4d1 2F2.5 8689460.0 cm-1
2s2 2p4 4p1 2F2.5 8703330.0 cm-1
2s2 2p4 4p1 2F3.5 8711270.0 cm-1
2s2 2p4 4p1 2D1.5 8715320.0 cm-1
2s2 2p4 4p1 2D2.5 8719880.0 cm-1
2s2 2p4 4p1 2P1.5 8722240.0 cm-1
2s2 2p4 4f1 4F3.5 8726270.0 cm-1
2s2 2p4 4f1 4F4.5 8726550.0 cm-1
2s2 2p4 4f1 4F2.5 8727030.0 cm-1
2s2 2p4 4f1 2G4.5 8728810.0 cm-1
2s2 2p4 4f1 4G5.5 8729080.0 cm-1
2s2 2p4 4f1 4D1.5 8729080.0 cm-1
2s2 2p4 4f1 2F3.5 8729230.0 cm-1
2s2 2p4 4f1 2F2.5 8731490.0 cm-1
2s2 2p4 4f1 4D0.5 8731630.0 cm-1
2s2 2p4 4f1 2D1.5 8733410.0 cm-1
2s2 2p4 4d1 4F1.5 8740480.0 cm-1
2s2 2p4 4p1 2P0.5 8742490.0 cm-1
2s2 2p4 4d1 4F2.5 8742560.0 cm-1
2s2 2p4 4d1 4D0.5 8744900.0 cm-1
2s2 2p4 4d1 4F3.5 8749060.0 cm-1
2s2 2p4 4d1 2D1.5 8752420.0 cm-1
2s2 2p4 4d1 4P2.5 8756580.0 cm-1
2s2 2p4 4d1 2D2.5 8767270.0 cm-1
2s2 2p4 4d1 2P1.5 8771030.0 cm-1
2s2 2p4 4s1 2S0.5 8783530.0 cm-1
2s2 2p4 4f1 4G2.5 8806480.0 cm-1
2s2 2p4 4f1 2G3.5 8807650.0 cm-1
2s2 2p4 4f1 4F1.5 8813290.0 cm-1
2s2 2p4 4f1 4G3.5 8814420.0 cm-1
2s2 2p4 4f1 4G4.5 8814440.0 cm-1
2s2 2p4 4f1 4D2.5 8815100.0 cm-1
2s2 2p4 4f1 2D2.5 8818020.0 cm-1
2s2 2p4 4f1 4D3.5 8818320.0 cm-1
2s2 2p4 4d1 2G3.5 8829020.0 cm-1
2s2 2p4 4d1 2G4.5 8830890.0 cm-1
2s2 2p4 4d1 2F2.5 8839040.0 cm-1
2s2 2p4 4d1 2S0.5 8840780.0 cm-1
2s2 2p4 4d1 2P1.5 8842780.0 cm-1
2s2 2p4 4d1 2F3.5 8842860.0 cm-1
2s2 2p4 4d1 2D2.5 8845400.0 cm-1
2s2 2p4 4d1 2D1.5 8855800.0 cm-1
2s2 2p4 4d1 2P0.5 8859490.0 cm-1
2s2 2p4 4p1 2P0.5 8892560.0 cm-1
2s2 2p4 4f1 2H4.5 8893690.0 cm-1
2s2 2p4 4p1 2P1.5 8894580.0 cm-1
2s2 2p4 4f1 2H5.5 8894660.0 cm-1
2s2 2p4 4f1 2P0.5 8895080.0 cm-1
2s2 2p4 4f1 2P1.5 8896100.0 cm-1
2s2 2p4 4f1 2D2.5 8898940.0 cm-1
2s2 2p4 4f1 2D1.5 8899080.0 cm-1
2s2 2p4 4f1 2G3.5 8901350.0 cm-1
2s2 2p4 4f1 2F2.5 8901910.0 cm-1
2s2 2p4 4f1 2F3.5 8902230.0 cm-1
2s2 2p4 4f1 2G4.5 8902420.0 cm-1
2s2 2p4 4d1 2D2.5 9017400.0 cm-1
2s2 2p4 4d1 2D1.5 9022080.0 cm-1
2s2 2p4 4f1 2F2.5 9078360.0 cm-1
2s2 2p4 4f1 2F3.5 9079180.0 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 = 1.4147
         2S = 1.2075
         2P = 1.1449
         3S = 1.1307
         3P = 1.0808
         3D = 1.1143
         4S = 1.1467
         4P = 1.0928
         4D = 1.1162
         4F = 1.1224

 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.

 30 continuum basis orbitals were used.

 A fine energy mesh of 0.000010 Z**2 Rydbergs (0.03932134 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (3.932134 eV) was used
 from the last threshold up to 0.978858 Z**2 Rydbergs (3849 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (3.932134 eV) was used
 from first threshold up to 0.978858 Z**2 Rydbergs (3849 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:
      M C Witthoeft, A D Whiteford and N R Badnell
      J Phys B 40 2969-2993 (2007)
      DOI: 10.1088/0953-4075/40/15/001

 Produced by: Mike Witthoeft
 Date:        18/07/06

 Update: Allan Whiteford, 14/03/08 
         Added Journal reference
         Removed incomplete comment about basis orbitals
         Added parent specification

------------------------------------------------------------------------
 Update: Martin O'Mullane, 04-11-2010
         Update ionisation potential from NIST database.

------------------------------------------------------------------------

Contributors

  • Mike Witthoeft
  • Allan Whiteford
  • Nigel Badnell
  • Martin O'Mullane
  • Processes
  • States
  • Comments
  • Origins

Data Classes