flike_mcw06#co18.dat

Resolved Specific Ion Data Collections

Ion
Co18+
Temperature Range
6.221 eV → 6.221 x 104 eV

ADF04

Filename
flike_mcw06#co18.dat
Full Path
adf04/copaw#f/flike_mcw06#co18.dat
Download data
  • Spontaneous Emission: Co+18(i) → Co+18(j) + hv
  • Electron Impact Excitation: Co+18(i) + e → Co+18(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 124440.0 cm-1
2s1 2p6 2S0.5 1146010.0 cm-1
2s2 2p4 3s1 4P2.5 6866810.0 cm-1
2s2 2p4 3s1 2P1.5 6896170.0 cm-1
2s2 2p4 3s1 4P0.5 6958840.0 cm-1
2s2 2p4 3s1 4P1.5 6978940.0 cm-1
2s2 2p4 3s1 2P0.5 7006640.0 cm-1
2s2 2p4 3s1 2D2.5 7067730.0 cm-1
2s2 2p4 3s1 2D1.5 7072240.0 cm-1
2s2 2p4 3p1 4P1.5 7125100.0 cm-1
2s2 2p4 3p1 4P2.5 7130270.0 cm-1
2s2 2p4 3p1 2P0.5 7160560.0 cm-1
2s2 2p4 3p1 4D3.5 7165630.0 cm-1
2s2 2p4 3p1 2D2.5 7166090.0 cm-1
2s2 2p4 3p1 2P1.5 7227340.0 cm-1
2s2 2p4 3p1 4D0.5 7228060.0 cm-1
2s2 2p4 3p1 4P0.5 7230900.0 cm-1
2s2 2p4 3p1 4D1.5 7247830.0 cm-1
2s2 2p4 3s1 2S0.5 7265400.0 cm-1
2s2 2p4 3p1 4D2.5 7267550.0 cm-1
2s2 2p4 3p1 4S1.5 7269640.0 cm-1
2s2 2p4 3p1 2S0.5 7289080.0 cm-1
2s2 2p4 3p1 2D1.5 7294240.0 cm-1
2s2 2p4 3p1 2F2.5 7328790.0 cm-1
2s2 2p4 3p1 2F3.5 7353500.0 cm-1
2s2 2p4 3p1 2D1.5 7367660.0 cm-1
2s2 2p4 3p1 2D2.5 7381670.0 cm-1
2s2 2p4 3p1 2P1.5 7431610.0 cm-1
2s2 2p4 3p1 2P0.5 7464710.0 cm-1
2s2 2p4 3d1 4D2.5 7486740.0 cm-1
2s2 2p4 3d1 4D3.5 7488940.0 cm-1
2s2 2p4 3d1 4D1.5 7491370.0 cm-1
2s2 2p4 3d1 2P0.5 7501680.0 cm-1
2s2 2p4 3d1 4F4.5 7514680.0 cm-1
2s2 2p4 3d1 2F3.5 7524930.0 cm-1
2s2 2p4 3d1 4P0.5 7542750.0 cm-1
2s2 2p4 3d1 4P1.5 7560900.0 cm-1
2s2 2p4 3p1 2P1.5 7562100.0 cm-1
2s2 2p4 3d1 2F2.5 7571260.0 cm-1
2s2 2p4 3p1 2P0.5 7574600.0 cm-1
2s2 2p4 3d1 4D0.5 7593920.0 cm-1
2s2 2p4 3d1 4F1.5 7598300.0 cm-1
2s2 2p4 3d1 4F2.5 7601940.0 cm-1
2s2 2p4 3d1 4F3.5 7614160.0 cm-1
2s2 2p4 3d1 2D1.5 7615980.0 cm-1
2s2 2p4 3d1 4P2.5 7635970.0 cm-1
2s2 2p4 3d1 2P1.5 7650070.0 cm-1
2s2 2p4 3d1 2D2.5 7660250.0 cm-1
2s2 2p4 3d1 2G3.5 7690860.0 cm-1
2s2 2p4 3d1 2G4.5 7696110.0 cm-1
2s2 2p4 3d1 2F2.5 7720480.0 cm-1
2s2 2p4 3d1 2S0.5 7721800.0 cm-1
2s2 2p4 3d1 2F3.5 7733580.0 cm-1
2s2 2p4 3d1 2P1.5 7747980.0 cm-1
2s2 2p4 3d1 2D2.5 7754260.0 cm-1
2s2 2p4 3d1 2D1.5 7782670.0 cm-1
2s2 2p4 3d1 2P0.5 7789890.0 cm-1
2s1 2p5 3s1 4P2.5 7869190.0 cm-1
2s1 2p5 3s1 4P1.5 7909070.0 cm-1
2s2 2p4 3d1 2D2.5 7912920.0 cm-1
2s2 2p4 3d1 2D1.5 7932340.0 cm-1
2s1 2p5 3s1 4P0.5 7963590.0 cm-1
2s1 2p5 3s1 2P1.5 7969400.0 cm-1
2s1 2p5 3s1 2P0.5 8032200.0 cm-1
2s1 2p5 3p1 4S1.5 8116170.0 cm-1
2s1 2p5 3p1 4D2.5 8145500.0 cm-1
2s1 2p5 3p1 4D3.5 8156640.0 cm-1
2s1 2p5 3p1 4D1.5 8173980.0 cm-1
2s1 2p5 3p1 2D2.5 8187220.0 cm-1
2s1 2p5 3p1 4P0.5 8205200.0 cm-1
2s1 2p5 3p1 2P1.5 8219700.0 cm-1
2s1 2p5 3p1 2P0.5 8241620.0 cm-1
2s1 2p5 3p1 4P2.5 8243200.0 cm-1
2s1 2p5 3p1 4P1.5 8247410.0 cm-1
2s1 2p5 3p1 4D0.5 8256220.0 cm-1
2s1 2p5 3s1 2P1.5 8266390.0 cm-1
2s1 2p5 3s1 2P0.5 8274130.0 cm-1
2s1 2p5 3p1 2D1.5 8301560.0 cm-1
2s1 2p5 3p1 2S0.5 8333210.0 cm-1
2s1 2p5 3d1 4P0.5 8462570.0 cm-1
2s1 2p5 3d1 4P1.5 8473300.0 cm-1
2s1 2p5 3d1 4F4.5 8484090.0 cm-1
2s1 2p5 3d1 4P2.5 8490660.0 cm-1
2s1 2p5 3d1 4F3.5 8494330.0 cm-1
2s1 2p5 3d1 4F2.5 8517950.0 cm-1
2s1 2p5 3p1 2D1.5 8521070.0 cm-1
2s1 2p5 3d1 2F3.5 8532860.0 cm-1
2s1 2p5 3d1 4F1.5 8537240.0 cm-1
2s1 2p5 3p1 2D2.5 8547660.0 cm-1
2s1 2p5 3p1 2P0.5 8551750.0 cm-1
2s1 2p5 3p1 2P1.5 8563420.0 cm-1
2s1 2p5 3d1 4D0.5 8569700.0 cm-1
2s1 2p5 3d1 2D2.5 8584800.0 cm-1
2s1 2p5 3d1 4D2.5 8586350.0 cm-1
2s1 2p5 3d1 4D3.5 8587280.0 cm-1
2s1 2p5 3d1 4D1.5 8596090.0 cm-1
2s1 2p5 3d1 2D1.5 8600760.0 cm-1
2s1 2p5 3p1 2S0.5 8603600.0 cm-1
2s1 2p5 3d1 2P0.5 8626090.0 cm-1
2s1 2p5 3d1 2F2.5 8646630.0 cm-1
2s1 2p5 3d1 2P1.5 8695380.0 cm-1
2s1 2p5 3d1 2F2.5 8877230.0 cm-1
2s1 2p5 3d1 2F3.5 8880620.0 cm-1
2s1 2p5 3d1 2P1.5 8901780.0 cm-1
2s1 2p5 3d1 2D2.5 8909100.0 cm-1
2s1 2p5 3d1 2D1.5 8910090.0 cm-1
2s1 2p5 3d1 2P0.5 8913560.0 cm-1
2s2 2p4 4s1 4P2.5 9293960.0 cm-1
2s2 2p4 4s1 2P1.5 9303240.0 cm-1
2s2 2p4 4s1 4P0.5 9384340.0 cm-1
2s2 2p4 4s1 4P1.5 9399920.0 cm-1
2s2 2p4 4p1 4P1.5 9401370.0 cm-1
2s2 2p4 4p1 4P2.5 9401860.0 cm-1
2s2 2p4 4s1 2P0.5 9407390.0 cm-1
2s2 2p4 4p1 4D3.5 9412840.0 cm-1
2s2 2p4 4p1 2D2.5 9413510.0 cm-1
2s2 2p4 4p1 2S0.5 9417480.0 cm-1
2s2 2p4 4p1 2P1.5 9444280.0 cm-1
2s2 2p4 4s1 2D2.5 9486560.0 cm-1
2s2 2p4 4s1 2D1.5 9487960.0 cm-1
2s2 2p4 4p1 4D0.5 9491290.0 cm-1
2s2 2p4 4p1 4D1.5 9501820.0 cm-1
2s2 2p4 4p1 4P0.5 9503990.0 cm-1
2s2 2p4 4p1 4D2.5 9516420.0 cm-1
2s2 2p4 4p1 4S1.5 9520160.0 cm-1
2s2 2p4 4p1 2D1.5 9524550.0 cm-1
2s2 2p4 4p1 2P0.5 9531580.0 cm-1
2s2 2p4 4d1 4D2.5 9534530.0 cm-1
2s2 2p4 4d1 4D3.5 9534850.0 cm-1
2s2 2p4 4d1 4D1.5 9536520.0 cm-1
2s2 2p4 4d1 4P0.5 9540320.0 cm-1
2s2 2p4 4d1 4F4.5 9541880.0 cm-1
2s2 2p4 4d1 2F3.5 9545870.0 cm-1
2s2 2p4 4d1 2P0.5 9555820.0 cm-1
2s2 2p4 4d1 2D1.5 9566760.0 cm-1
2s2 2p4 4d1 2F2.5 9569530.0 cm-1
2s2 2p4 4p1 2F2.5 9592250.0 cm-1
2s2 2p4 4p1 2F3.5 9601880.0 cm-1
2s2 2p4 4p1 2D1.5 9605590.0 cm-1
2s2 2p4 4f1 4F3.5 9608760.0 cm-1
2s2 2p4 4f1 4F4.5 9609170.0 cm-1
2s2 2p4 4f1 4F2.5 9609470.0 cm-1
2s2 2p4 4p1 2D2.5 9610900.0 cm-1
2s2 2p4 4f1 2G4.5 9611410.0 cm-1
2s2 2p4 4f1 4D1.5 9611450.0 cm-1
2s2 2p4 4f1 4G5.5 9611840.0 cm-1
2s2 2p4 4f1 2F3.5 9612110.0 cm-1
2s2 2p4 4p1 2P1.5 9612110.0 cm-1
2s2 2p4 4f1 4D0.5 9614190.0 cm-1
2s2 2p4 4f1 2F2.5 9614430.0 cm-1
2s2 2p4 4f1 2D1.5 9616270.0 cm-1
2s2 2p4 4d1 4F1.5 9628410.0 cm-1
2s2 2p4 4d1 4F2.5 9631830.0 cm-1
2s2 2p4 4p1 2P0.5 9634900.0 cm-1
2s2 2p4 4d1 4D0.5 9639200.0 cm-1
2s2 2p4 4d1 4F3.5 9644270.0 cm-1
2s2 2p4 4d1 4P1.5 9647250.0 cm-1
2s2 2p4 4d1 4P2.5 9652260.0 cm-1
2s2 2p4 4d1 2D2.5 9661650.0 cm-1
2s2 2p4 4d1 2P1.5 9666490.0 cm-1
2s2 2p4 4s1 2S0.5 9683300.0 cm-1
2s2 2p4 4f1 4G2.5 9698690.0 cm-1
2s2 2p4 4f1 2G3.5 9700130.0 cm-1
2s2 2p4 4f1 4F1.5 9713010.0 cm-1
2s2 2p4 4f1 4G3.5 9714340.0 cm-1
2s2 2p4 4f1 4G4.5 9714520.0 cm-1
2s2 2p4 4f1 4D2.5 9715110.0 cm-1
2s2 2p4 4f1 2D2.5 9718200.0 cm-1
2s2 2p4 4f1 4D3.5 9718680.0 cm-1
2s2 2p4 4d1 2G3.5 9726460.0 cm-1
2s2 2p4 4d1 2G4.5 9728760.0 cm-1
2s2 2p4 4d1 2F2.5 9736990.0 cm-1
2s2 2p4 4d1 2S0.5 9738690.0 cm-1
2s2 2p4 4d1 2P1.5 9740620.0 cm-1
2s2 2p4 4d1 2F3.5 9741270.0 cm-1
2s2 2p4 4d1 2D2.5 9743590.0 cm-1
2s2 2p4 4d1 2D1.5 9755260.0 cm-1
2s2 2p4 4d1 2P0.5 9759680.0 cm-1
2s2 2p4 4f1 2H4.5 9796090.0 cm-1
2s2 2p4 4f1 2P0.5 9796190.0 cm-1
2s2 2p4 4f1 2H5.5 9797280.0 cm-1
2s2 2p4 4f1 2P1.5 9797470.0 cm-1
2s2 2p4 4p1 2P0.5 9800120.0 cm-1
2s2 2p4 4f1 2D2.5 9801420.0 cm-1
2s2 2p4 4f1 2D1.5 9801620.0 cm-1
2s2 2p4 4p1 2P1.5 9802910.0 cm-1
2s2 2p4 4f1 2G3.5 9804120.0 cm-1
2s2 2p4 4f1 2F2.5 9804700.0 cm-1
2s2 2p4 4f1 2F3.5 9805110.0 cm-1
2s2 2p4 4f1 2G4.5 9805420.0 cm-1
2s2 2p4 4d1 2D2.5 9932150.0 cm-1
2s2 2p4 4d1 2D1.5 9937450.0 cm-1
2s2 2p4 4f1 2F2.5 9997760.0 cm-1
2s2 2p4 4f1 2F3.5 9998760.0 cm-1
O+18        27        19      11380483.(1S)
------------------------------------------------------------------------

        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 = 1.4131
         2S = 1.2085
         2P = 1.1455
         3S = 1.1319
         3P = 1.0820
         3D = 1.1160
         4S = 1.1480
         4P = 1.0942
         4D = 1.1179
         4F = 1.1251

 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 (0.04408344 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (4.408344 eV) was used
 from the last threshold up to 0.960225 Z**2 Rydbergs (4233 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (4.408344 eV) was used
 from first threshold up to 0.960225 Z**2 Rydbergs (4233 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

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

Contributors

  • Mike Witthoeft
  • Allan Whiteford
  • Nigel Badnell
  • Processes
  • States
  • Comments
  • Origins

Data Classes