flike_mcw06#v14.dat

Resolved Specific Ion Data Collections

Ion
V14+
Temperature Range
3.878 eV → 3.878 x 104 eV

ADF04

Filename
flike_mcw06#v14.dat
Full Path
adf04/copaw#f/flike_mcw06#v14.dat
Download data
  • Spontaneous Emission: V+14(i) → V+14(j) + hv
  • Electron Impact Excitation: V+14(i) + e → V+14(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 59979.0 cm-1
2s1 2p6 2S0.5 894686.0 cm-1
2s2 2p4 3s1 4P2.5 4506600.0 cm-1
2s2 2p4 3s1 4P1.5 4528800.0 cm-1
2s2 2p4 3s1 4P0.5 4556270.0 cm-1
2s2 2p4 3s1 2P1.5 4564270.0 cm-1
2s2 2p4 3s1 2P0.5 4588950.0 cm-1
2s2 2p4 3s1 2D2.5 4639390.0 cm-1
2s2 2p4 3s1 2D1.5 4641340.0 cm-1
2s2 2p4 3p1 4P2.5 4708430.0 cm-1
2s2 2p4 3p1 4P1.5 4708960.0 cm-1
2s2 2p4 3p1 4P0.5 4728220.0 cm-1
2s2 2p4 3p1 4D3.5 4733820.0 cm-1
2s2 2p4 3p1 2D2.5 4738280.0 cm-1
2s2 2p4 3p1 2P0.5 4763370.0 cm-1
2s2 2p4 3p1 4D1.5 4766770.0 cm-1
2s2 2p4 3p1 4D0.5 4772160.0 cm-1
2s2 2p4 3s1 2S0.5 4780530.0 cm-1
2s2 2p4 3p1 2P1.5 4781010.0 cm-1
2s2 2p4 3p1 4D2.5 4781640.0 cm-1
2s2 2p4 3p1 4S1.5 4793280.0 cm-1
2s2 2p4 3p1 2S0.5 4801880.0 cm-1
2s2 2p4 3p1 2D1.5 4804080.0 cm-1
2s2 2p4 3p1 2F2.5 4844060.0 cm-1
2s2 2p4 3p1 2F3.5 4854680.0 cm-1
2s2 2p4 3p1 2D1.5 4871750.0 cm-1
2s2 2p4 3p1 2D2.5 4878600.0 cm-1
2s2 2p4 3p1 2P1.5 4929740.0 cm-1
2s2 2p4 3p1 2P0.5 4946130.0 cm-1
2s2 2p4 3d1 4D3.5 4986530.0 cm-1
2s2 2p4 3d1 4D2.5 4986720.0 cm-1
2s2 2p4 3d1 4D1.5 4990960.0 cm-1
2s2 2p4 3d1 4D0.5 4998050.0 cm-1
2s2 2p4 3p1 2P1.5 5008170.0 cm-1
2s2 2p4 3d1 4F4.5 5009470.0 cm-1
2s2 2p4 3p1 2P0.5 5017410.0 cm-1
2s2 2p4 3d1 2F3.5 5019070.0 cm-1
2s2 2p4 3d1 4P0.5 5028790.0 cm-1
2s2 2p4 3d1 4P1.5 5040050.0 cm-1
2s2 2p4 3d1 4F2.5 5042270.0 cm-1
2s2 2p4 3d1 2P0.5 5048080.0 cm-1
2s2 2p4 3d1 4F1.5 5054760.0 cm-1
2s2 2p4 3d1 4F3.5 5055690.0 cm-1
2s2 2p4 3d1 4P2.5 5057460.0 cm-1
2s2 2p4 3d1 2D1.5 5062650.0 cm-1
2s2 2p4 3d1 2F2.5 5071170.0 cm-1
2s2 2p4 3d1 2P1.5 5085210.0 cm-1
2s2 2p4 3d1 2D2.5 5093220.0 cm-1
2s2 2p4 3d1 2G3.5 5122330.0 cm-1
2s2 2p4 3d1 2G4.5 5124500.0 cm-1
2s2 2p4 3d1 2S0.5 5147080.0 cm-1
2s2 2p4 3d1 2F2.5 5148140.0 cm-1
2s2 2p4 3d1 2F3.5 5154750.0 cm-1
2s2 2p4 3d1 2P1.5 5169420.0 cm-1
2s2 2p4 3d1 2D2.5 5172040.0 cm-1
2s2 2p4 3d1 2D1.5 5188840.0 cm-1
2s2 2p4 3d1 2P0.5 5190260.0 cm-1
2s2 2p4 3d1 2D2.5 5284250.0 cm-1
2s1 2p5 3s1 4P2.5 5289440.0 cm-1
2s2 2p4 3d1 2D1.5 5293130.0 cm-1
2s1 2p5 3s1 4P1.5 5314370.0 cm-1
2s1 2p5 3s1 4P0.5 5339100.0 cm-1
2s1 2p5 3s1 2P1.5 5355990.0 cm-1
2s1 2p5 3s1 2P0.5 5388680.0 cm-1
2s1 2p5 3p1 4S1.5 5478390.0 cm-1
2s1 2p5 3p1 4D2.5 5506220.0 cm-1
2s1 2p5 3p1 4D3.5 5506960.0 cm-1
2s1 2p5 3p1 4D1.5 5520700.0 cm-1
2s1 2p5 3p1 2D2.5 5531290.0 cm-1
2s1 2p5 3p1 4D0.5 5536990.0 cm-1
2s1 2p5 3p1 2P1.5 5548520.0 cm-1
2s1 2p5 3p1 4P2.5 5557170.0 cm-1
2s1 2p5 3p1 4P1.5 5560670.0 cm-1
2s1 2p5 3p1 4P0.5 5561920.0 cm-1
2s1 2p5 3p1 2P0.5 5566480.0 cm-1
2s1 2p5 3p1 2D1.5 5585540.0 cm-1
2s1 2p5 3s1 2P1.5 5601210.0 cm-1
2s1 2p5 3s1 2P0.5 5604400.0 cm-1
2s1 2p5 3p1 2S0.5 5632050.0 cm-1
2s1 2p5 3d1 4P0.5 5750710.0 cm-1
2s1 2p5 3d1 4P1.5 5757150.0 cm-1
2s1 2p5 3d1 4F4.5 5764600.0 cm-1
2s1 2p5 3d1 4P2.5 5768430.0 cm-1
2s1 2p5 3d1 4F3.5 5772600.0 cm-1
2s1 2p5 3d1 4F2.5 5785580.0 cm-1
2s1 2p5 3d1 4F1.5 5796980.0 cm-1
2s1 2p5 3p1 2D1.5 5800930.0 cm-1
2s1 2p5 3d1 4D3.5 5801240.0 cm-1
2s1 2p5 3p1 2D2.5 5812520.0 cm-1
2s1 2p5 3d1 4D0.5 5819270.0 cm-1
2s1 2p5 3p1 2P0.5 5820590.0 cm-1
2s1 2p5 3d1 4D2.5 5825420.0 cm-1
2s1 2p5 3p1 2P1.5 5826080.0 cm-1
2s1 2p5 3d1 2F3.5 5827360.0 cm-1
2s1 2p5 3d1 4D1.5 5828260.0 cm-1
2s1 2p5 3d1 2D2.5 5829630.0 cm-1
2s1 2p5 3d1 2D1.5 5841940.0 cm-1
2s1 2p5 3d1 2F2.5 5858400.0 cm-1
2s1 2p5 3p1 2S0.5 5861620.0 cm-1
2s1 2p5 3d1 2P0.5 5871720.0 cm-1
2s1 2p5 3d1 2P1.5 5903130.0 cm-1
2s1 2p5 3d1 2F2.5 6071970.0 cm-1
2s1 2p5 3d1 2F3.5 6073360.0 cm-1
2s1 2p5 3d1 2P1.5 6089640.0 cm-1
2s2 2p4 4s1 4P2.5 6091280.0 cm-1
2s1 2p5 3d1 2P0.5 6094220.0 cm-1
2s1 2p5 3d1 2D1.5 6094640.0 cm-1
2s1 2p5 3d1 2D2.5 6094980.0 cm-1
2s2 2p4 4s1 2P1.5 6098920.0 cm-1
2s2 2p4 4s1 4P1.5 6140620.0 cm-1
2s2 2p4 4s1 4P0.5 6140870.0 cm-1
2s2 2p4 4s1 2P0.5 6150000.0 cm-1
2s2 2p4 4p1 4P2.5 6173740.0 cm-1
2s2 2p4 4p1 4P1.5 6175020.0 cm-1
2s2 2p4 4p1 4D3.5 6180530.0 cm-1
2s2 2p4 4p1 2D2.5 6182460.0 cm-1
2s2 2p4 4p1 2S0.5 6185420.0 cm-1
2s2 2p4 4p1 2P1.5 6202430.0 cm-1
2s2 2p4 4s1 2D2.5 6216630.0 cm-1
2s2 2p4 4s1 2D1.5 6217180.0 cm-1
2s2 2p4 4p1 4P0.5 6221560.0 cm-1
2s2 2p4 4p1 4D0.5 6226180.0 cm-1
2s2 2p4 4p1 4D1.5 6227620.0 cm-1
2s2 2p4 4p1 4D2.5 6227770.0 cm-1
2s2 2p4 4p1 4S1.5 6232630.0 cm-1
2s2 2p4 4p1 2D1.5 6241670.0 cm-1
2s2 2p4 4p1 2P0.5 6243350.0 cm-1
2s2 2p4 4d1 4D3.5 6274870.0 cm-1
2s2 2p4 4d1 4D2.5 6275340.0 cm-1
2s2 2p4 4d1 4D1.5 6277530.0 cm-1
2s2 2p4 4d1 4P0.5 6280910.0 cm-1
2s2 2p4 4d1 4F4.5 6280920.0 cm-1
2s2 2p4 4d1 2F3.5 6285020.0 cm-1
2s2 2p4 4d1 2P0.5 6291870.0 cm-1
2s2 2p4 4p1 2F2.5 6298680.0 cm-1
2s2 2p4 4d1 4P1.5 6299060.0 cm-1
2s2 2p4 4d1 2F2.5 6299990.0 cm-1
2s2 2p4 4p1 2F3.5 6302870.0 cm-1
2s2 2p4 4p1 2D1.5 6307270.0 cm-1
2s2 2p4 4p1 2D2.5 6309940.0 cm-1
2s2 2p4 4p1 2P1.5 6315060.0 cm-1
2s2 2p4 4d1 4D0.5 6325750.0 cm-1
2s2 2p4 4d1 4F3.5 6327340.0 cm-1
2s2 2p4 4p1 2P0.5 6328270.0 cm-1
2s2 2p4 4d1 4F1.5 6328700.0 cm-1
2s2 2p4 4d1 4F2.5 6328780.0 cm-1
2s2 2p4 4f1 4F4.5 6329900.0 cm-1
2s2 2p4 4f1 4F3.5 6329970.0 cm-1
2s2 2p4 4f1 4F2.5 6330760.0 cm-1
2s2 2p4 4d1 2D1.5 6331740.0 cm-1
2s2 2p4 4f1 4G5.5 6331840.0 cm-1
2s2 2p4 4f1 2F3.5 6331850.0 cm-1
2s2 2p4 4f1 2G4.5 6331860.0 cm-1
2s2 2p4 4f1 4D1.5 6332600.0 cm-1
2s2 2p4 4d1 4P2.5 6333450.0 cm-1
2s2 2p4 4f1 2F2.5 6333900.0 cm-1
2s2 2p4 4f1 4D0.5 6334860.0 cm-1
2s2 2p4 4f1 2D1.5 6335890.0 cm-1
2s2 2p4 4d1 2D2.5 6346320.0 cm-1
2s2 2p4 4d1 2P1.5 6348610.0 cm-1
2s2 2p4 4s1 2S0.5 6357530.0 cm-1
2s2 2p4 4f1 4F1.5 6378230.0 cm-1
2s2 2p4 4f1 4G4.5 6378400.0 cm-1
2s2 2p4 4f1 4G3.5 6378440.0 cm-1
2s2 2p4 4f1 4D2.5 6379240.0 cm-1
2s2 2p4 4f1 4G2.5 6380570.0 cm-1
2s2 2p4 4f1 2G3.5 6381270.0 cm-1
2s2 2p4 4f1 2D2.5 6383480.0 cm-1
2s2 2p4 4f1 4D3.5 6383520.0 cm-1
2s2 2p4 4d1 2G3.5 6399970.0 cm-1
2s2 2p4 4d1 2G4.5 6400930.0 cm-1
2s2 2p4 4d1 2F2.5 6408680.0 cm-1
2s2 2p4 4d1 2S0.5 6410340.0 cm-1
2s2 2p4 4d1 2F3.5 6411110.0 cm-1
2s2 2p4 4d1 2P1.5 6412280.0 cm-1
2s2 2p4 4d1 2D2.5 6413910.0 cm-1
2s2 2p4 4d1 2D1.5 6420780.0 cm-1
2s2 2p4 4d1 2P0.5 6422710.0 cm-1
2s2 2p4 4p1 2P0.5 6446850.0 cm-1
2s2 2p4 4p1 2P1.5 6447600.0 cm-1
2s2 2p4 4f1 2H4.5 6450280.0 cm-1
2s2 2p4 4f1 2H5.5 6450770.0 cm-1
2s2 2p4 4f1 2P0.5 6453190.0 cm-1
2s2 2p4 4f1 2P1.5 6453600.0 cm-1
2s2 2p4 4f1 2D1.5 6455880.0 cm-1
2s2 2p4 4f1 2D2.5 6455890.0 cm-1
2s2 2p4 4f1 2G3.5 6456670.0 cm-1
2s2 2p4 4f1 2G4.5 6457210.0 cm-1
2s2 2p4 4f1 2F2.5 6457480.0 cm-1
2s2 2p4 4f1 2F3.5 6457690.0 cm-1
2s2 2p4 4d1 2D2.5 6548330.0 cm-1
2s2 2p4 4d1 2D1.5 6551110.0 cm-1
2s2 2p4 4f1 2F2.5 6595650.0 cm-1
2s2 2p4 4f1 2F3.5 6596100.0 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 = 1.4199
         2S = 1.2038
         2P = 1.1426
         3S = 1.1261
         3P = 1.0764
         3D = 1.1081
         4S = 1.1416
         4P = 1.0876
         4D = 1.1096
         4F = 1.1126

 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 (0.02666776 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (2.666776 eV) was used
 from the last threshold up to 1.052732 Z**2 Rydbergs (2807.4 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (2.666776 eV) was used
 from first threshold up to 1.052732 Z**2 Rydbergs (2807.4 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

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