flike_mcw06#cr15.dat

Resolved Specific Ion Data Collections

Ion
Cr15+
Temperature Range
4.412 eV → 4.412 x 104 eV

ADF04

Filename
flike_mcw06#cr15.dat
Full Path
adf04/copaw#f/flike_mcw06#cr15.dat
Download data
  • Spontaneous Emission: Cr+15(i) → Cr+15(j) + hv
  • Electron Impact Excitation: Cr+15(i) + e → Cr+15(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 72910.0 cm-1
2s1 2p6 2S0.5 954067.0 cm-1
2s2 2p4 3s1 4P2.5 5051200.0 cm-1
2s2 2p4 3s1 2P1.5 5075460.0 cm-1
2s2 2p4 3s1 4P0.5 5110420.0 cm-1
2s2 2p4 3s1 4P1.5 5119280.0 cm-1
2s2 2p4 3s1 2P0.5 5145430.0 cm-1
2s2 2p4 3s1 2D2.5 5198130.0 cm-1
2s2 2p4 3s1 2D1.5 5200620.0 cm-1
2s2 2p4 3p1 4P1.5 5267520.0 cm-1
2s2 2p4 3p1 4P2.5 5268090.0 cm-1
2s2 2p4 3p1 4P0.5 5290420.0 cm-1
2s2 2p4 3p1 4D3.5 5295470.0 cm-1
2s2 2p4 3p1 2D2.5 5299200.0 cm-1
2s2 2p4 3p1 2P0.5 5331020.0 cm-1
2s2 2p4 3p1 4D1.5 5334880.0 cm-1
2s2 2p4 3p1 4D0.5 5340250.0 cm-1
2s2 2p4 3p1 2P1.5 5350030.0 cm-1
2s2 2p4 3s1 2S0.5 5350760.0 cm-1
2s2 2p4 3p1 4D2.5 5353730.0 cm-1
2s2 2p4 3p1 4S1.5 5364020.0 cm-1
2s2 2p4 3p1 2S0.5 5374360.0 cm-1
2s2 2p4 3p1 2D1.5 5377680.0 cm-1
2s2 2p4 3p1 2F2.5 5416780.0 cm-1
2s2 2p4 3p1 2F3.5 5430110.0 cm-1
2s2 2p4 3p1 2D1.5 5446780.0 cm-1
2s2 2p4 3p1 2D2.5 5455190.0 cm-1
2s2 2p4 3p1 2P1.5 5507260.0 cm-1
2s2 2p4 3p1 2P0.5 5526610.0 cm-1
2s2 2p4 3d1 4D2.5 5565280.0 cm-1
2s2 2p4 3d1 4D3.5 5565490.0 cm-1
2s2 2p4 3d1 4D1.5 5569800.0 cm-1
2s2 2p4 3d1 4D0.5 5577840.0 cm-1
2s2 2p4 3d1 4F4.5 5589290.0 cm-1
2s2 2p4 3p1 2P1.5 5594870.0 cm-1
2s2 2p4 3d1 2F3.5 5599340.0 cm-1
2s2 2p4 3p1 2P0.5 5605620.0 cm-1
2s2 2p4 3d1 4P0.5 5610850.0 cm-1
2s2 2p4 3d1 4P1.5 5623780.0 cm-1
2s2 2p4 3d1 4F2.5 5627760.0 cm-1
2s2 2p4 3d1 2P0.5 5634940.0 cm-1
2s2 2p4 3d1 4F1.5 5643270.0 cm-1
2s2 2p4 3d1 4P2.5 5645560.0 cm-1
2s2 2p4 3d1 4F3.5 5645750.0 cm-1
2s2 2p4 3d1 2D1.5 5651440.0 cm-1
2s2 2p4 3d1 2F2.5 5662800.0 cm-1
2s2 2p4 3d1 2P1.5 5676950.0 cm-1
2s2 2p4 3d1 2D2.5 5686180.0 cm-1
2s2 2p4 3d1 2G3.5 5715160.0 cm-1
2s2 2p4 3d1 2G4.5 5717880.0 cm-1
2s2 2p4 3d1 2S0.5 5741520.0 cm-1
2s2 2p4 3d1 2F2.5 5741990.0 cm-1
2s2 2p4 3d1 2F3.5 5750060.0 cm-1
2s2 2p4 3d1 2P1.5 5765360.0 cm-1
2s2 2p4 3d1 2D2.5 5768660.0 cm-1
2s2 2p4 3d1 2D1.5 5788070.0 cm-1
2s2 2p4 3d1 2P0.5 5790640.0 cm-1
2s1 2p5 3s1 4P2.5 5885700.0 cm-1
2s2 2p4 3d1 2D2.5 5889560.0 cm-1
2s2 2p4 3d1 2D1.5 5900840.0 cm-1
2s1 2p5 3s1 4P1.5 5914330.0 cm-1
2s1 2p5 3s1 4P0.5 5945030.0 cm-1
2s1 2p5 3s1 2P1.5 5959300.0 cm-1
2s1 2p5 3s1 2P0.5 5998140.0 cm-1
2s1 2p5 3p1 4S1.5 6088870.0 cm-1
2s1 2p5 3p1 4D2.5 6117300.0 cm-1
2s1 2p5 3p1 4D3.5 6119810.0 cm-1
2s1 2p5 3p1 4D1.5 6134620.0 cm-1
2s1 2p5 3p1 2D2.5 6145740.0 cm-1
2s1 2p5 3p1 4D0.5 6154270.0 cm-1
2s1 2p5 3p1 2P1.5 6166210.0 cm-1
2s1 2p5 3p1 4P2.5 6177830.0 cm-1
2s1 2p5 3p1 4P1.5 6181550.0 cm-1
2s1 2p5 3p1 4P0.5 6183910.0 cm-1
2s1 2p5 3p1 2P0.5 6185660.0 cm-1
2s1 2p5 3p1 2D1.5 6211870.0 cm-1
2s1 2p5 3s1 2P1.5 6217070.0 cm-1
2s1 2p5 3s1 2P0.5 6221090.0 cm-1
2s1 2p5 3p1 2S0.5 6255950.0 cm-1
2s1 2p5 3d1 4P0.5 6379100.0 cm-1
2s1 2p5 3d1 4P1.5 6386530.0 cm-1
2s1 2p5 3d1 4F4.5 6394700.0 cm-1
2s1 2p5 3d1 4P2.5 6399330.0 cm-1
2s1 2p5 3d1 4F3.5 6403420.0 cm-1
2s1 2p5 3d1 4F2.5 6418780.0 cm-1
2s1 2p5 3p1 2D1.5 6430420.0 cm-1
2s1 2p5 3d1 4F1.5 6432030.0 cm-1
2s1 2p5 3d1 2F3.5 6434440.0 cm-1
2s1 2p5 3p1 2D2.5 6444940.0 cm-1
2s1 2p5 3p1 2P0.5 6452300.0 cm-1
2s1 2p5 3d1 4D0.5 6456400.0 cm-1
2s1 2p5 3p1 2P1.5 6459080.0 cm-1
2s1 2p5 3d1 4D2.5 6464670.0 cm-1
2s1 2p5 3d1 4D3.5 6466300.0 cm-1
2s1 2p5 3d1 2D2.5 6467600.0 cm-1
2s1 2p5 3d1 4D1.5 6468800.0 cm-1
2s1 2p5 3d1 2D1.5 6480670.0 cm-1
2s1 2p5 3p1 2S0.5 6496310.0 cm-1
2s1 2p5 3d1 2F2.5 6502770.0 cm-1
2s1 2p5 3d1 2P0.5 6510570.0 cm-1
2s1 2p5 3d1 2P1.5 6549440.0 cm-1
2s1 2p5 3d1 2F2.5 6722060.0 cm-1
2s1 2p5 3d1 2F3.5 6723810.0 cm-1
2s1 2p5 3d1 2P1.5 6741660.0 cm-1
2s1 2p5 3d1 2D1.5 6747060.0 cm-1
2s1 2p5 3d1 2D2.5 6747160.0 cm-1
2s1 2p5 3d1 2P0.5 6747680.0 cm-1
2s2 2p4 4s1 4P2.5 6829730.0 cm-1
2s2 2p4 4s1 2P1.5 6837820.0 cm-1
2s2 2p4 4s1 4P0.5 6889070.0 cm-1
2s2 2p4 4s1 4P1.5 6890170.0 cm-1
2s2 2p4 4s1 2P0.5 6898990.0 cm-1
2s2 2p4 4p1 4P2.5 6918460.0 cm-1
2s2 2p4 4p1 4P1.5 6919390.0 cm-1
2s2 2p4 4p1 4D3.5 6926040.0 cm-1
2s2 2p4 4p1 2D2.5 6927690.0 cm-1
2s2 2p4 4p1 2S0.5 6930990.0 cm-1
2s2 2p4 4p1 2P1.5 6950370.0 cm-1
2s2 2p4 4s1 2D2.5 6968920.0 cm-1
2s2 2p4 4s1 2D1.5 6969660.0 cm-1
2s2 2p4 4p1 4P0.5 6976580.0 cm-1
2s2 2p4 4p1 4D0.5 6979990.0 cm-1
2s2 2p4 4p1 4D1.5 6982290.0 cm-1
2s2 2p4 4p1 4D2.5 6984300.0 cm-1
2s2 2p4 4p1 4S1.5 6989370.0 cm-1
2s2 2p4 4p1 2D1.5 6997240.0 cm-1
2s2 2p4 4p1 2P0.5 6999680.0 cm-1
2s2 2p4 4d1 4D3.5 7027200.0 cm-1
2s2 2p4 4d1 4D2.5 7027550.0 cm-1
2s2 2p4 4d1 4D1.5 7029740.0 cm-1
2s2 2p4 4d1 4P0.5 7033260.0 cm-1
2s2 2p4 4d1 4F4.5 7033520.0 cm-1
2s2 2p4 4d1 2F3.5 7037700.0 cm-1
2s2 2p4 4d1 2P0.5 7045300.0 cm-1
2s2 2p4 4d1 4P1.5 7053390.0 cm-1
2s2 2p4 4d1 2F2.5 7054740.0 cm-1
2s2 2p4 4p1 2F2.5 7056760.0 cm-1
2s2 2p4 4p1 2F3.5 7061990.0 cm-1
2s2 2p4 4p1 2D1.5 7066420.0 cm-1
2s2 2p4 4p1 2D2.5 7069660.0 cm-1
2s2 2p4 4p1 2P1.5 7074050.0 cm-1
2s2 2p4 4f1 4F3.5 7086940.0 cm-1
2s2 2p4 4f1 4F4.5 7086970.0 cm-1
2s2 2p4 4f1 4F2.5 7087720.0 cm-1
2s2 2p4 4d1 4D0.5 7088430.0 cm-1
2s2 2p4 4f1 2G4.5 7089100.0 cm-1
2s2 2p4 4f1 4G5.5 7089140.0 cm-1
2s2 2p4 4f1 2F3.5 7089150.0 cm-1
2s2 2p4 4p1 2P0.5 7089440.0 cm-1
2s2 2p4 4f1 4D1.5 7089640.0 cm-1
2s2 2p4 4d1 4F1.5 7090430.0 cm-1
2s2 2p4 4d1 4F2.5 7090800.0 cm-1
2s2 2p4 4d1 4F3.5 7090860.0 cm-1
2s2 2p4 4f1 2F2.5 7091280.0 cm-1
2s2 2p4 4f1 4D0.5 7092030.0 cm-1
2s2 2p4 4f1 2D1.5 7093270.0 cm-1
2s2 2p4 4d1 2D1.5 7094920.0 cm-1
2s2 2p4 4d1 4P2.5 7097440.0 cm-1
2s2 2p4 4d1 2D2.5 7110010.0 cm-1
2s2 2p4 4d1 2P1.5 7112480.0 cm-1
2s2 2p4 4s1 2S0.5 7121220.0 cm-1
2s2 2p4 4f1 4F1.5 7146160.0 cm-1
2s2 2p4 4f1 4G3.5 7146540.0 cm-1
2s2 2p4 4f1 4G4.5 7146640.0 cm-1
2s2 2p4 4f1 4D2.5 7147290.0 cm-1
2s2 2p4 4f1 4G2.5 7147860.0 cm-1
2s2 2p4 4f1 2G3.5 7149060.0 cm-1
2s2 2p4 4f1 4D3.5 7150270.0 cm-1
2s2 2p4 4f1 2D2.5 7150520.0 cm-1
2s2 2p4 4d1 2G3.5 7166050.0 cm-1
2s2 2p4 4d1 2G4.5 7167260.0 cm-1
2s2 2p4 4d1 2F2.5 7175180.0 cm-1
2s2 2p4 4d1 2S0.5 7176890.0 cm-1
2s2 2p4 4d1 2F3.5 7178060.0 cm-1
2s2 2p4 4d1 2P1.5 7178910.0 cm-1
2s2 2p4 4d1 2D2.5 7180840.0 cm-1
2s2 2p4 4d1 2D1.5 7188840.0 cm-1
2s2 2p4 4d1 2P0.5 7191280.0 cm-1
2s2 2p4 4p1 2P0.5 7217170.0 cm-1
2s2 2p4 4p1 2P1.5 7218270.0 cm-1
2s2 2p4 4f1 2H4.5 7221070.0 cm-1
2s2 2p4 4f1 2H5.5 7221700.0 cm-1
2s2 2p4 4f1 2P0.5 7223120.0 cm-1
2s2 2p4 4f1 2P1.5 7223640.0 cm-1
2s2 2p4 4f1 2D2.5 7226400.0 cm-1
2s2 2p4 4f1 2D1.5 7226440.0 cm-1
2s2 2p4 4f1 2G3.5 7227920.0 cm-1
2s2 2p4 4f1 2F2.5 7228560.0 cm-1
2s2 2p4 4f1 2G4.5 7228600.0 cm-1
2s2 2p4 4f1 2F3.5 7228790.0 cm-1
2s2 2p4 4d1 2D2.5 7326120.0 cm-1
2s2 2p4 4d1 2D1.5 7329510.0 cm-1
2s2 2p4 4f1 2F2.5 7377920.0 cm-1
2s2 2p4 4f1 2F3.5 7378470.0 cm-1
R+15        24        16       8380101.(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 = 1.4179
         2S = 1.2052
         2P = 1.1434
         3S = 1.1277
         3P = 1.0780
         3D = 1.1104
         4S = 1.1435
         4P = 1.0895
         4D = 1.1121
         4F = 1.1160

 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 (0.0306135 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (3.06135 eV) was used
 from the last threshold up to 1.018178 Z**2 Rydbergs (3117 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (3.06135 eV) was used
 from first threshold up to 1.018178 Z**2 Rydbergs (3117 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
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  • Comments
  • Origins

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