flike_mcw06#cu20.dat

Resolved Specific Ion Data Collections

Ion
Cu20+
Temperature Range
7.600 eV → 7.600 x 104 eV

ADF04

Filename
flike_mcw06#cu20.dat
Full Path
adf04/copaw#f/flike_mcw06#cu20.dat
Download data
  • Spontaneous Emission: Cu+20(i) → Cu+20(j) + hv
  • Electron Impact Excitation: Cu+20(i) + e → Cu+20(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 171486.0 cm-1
2s1 2p6 2S0.5 1287720.0 cm-1
2s2 2p4 3s1 4P2.5 8228460.0 cm-1
2s2 2p4 3s1 2P1.5 8260560.0 cm-1
2s2 2p4 3s1 4P0.5 8343200.0 cm-1
2s2 2p4 3s1 4P1.5 8382600.0 cm-1
2s2 2p4 3s1 2P0.5 8410520.0 cm-1
2s2 2p4 3s1 2D2.5 8477380.0 cm-1
2s2 2p4 3s1 2D1.5 8483490.0 cm-1
2s2 2p4 3p1 4P1.5 8514850.0 cm-1
2s2 2p4 3p1 4P2.5 8523600.0 cm-1
2s2 2p4 3p1 2P0.5 8560910.0 cm-1
2s2 2p4 3p1 2D2.5 8565100.0 cm-1
2s2 2p4 3p1 4D3.5 8567100.0 cm-1
2s2 2p4 3p1 4D0.5 8640150.0 cm-1
2s2 2p4 3p1 4S1.5 8644480.0 cm-1
2s2 2p4 3p1 4P0.5 8660850.0 cm-1
2s2 2p4 3p1 4D1.5 8672360.0 cm-1
2s2 2p4 3p1 2P1.5 8702420.0 cm-1
2s2 2p4 3p1 4D2.5 8710580.0 cm-1
2s2 2p4 3s1 2S0.5 8717170.0 cm-1
2s2 2p4 3p1 2S0.5 8732980.0 cm-1
2s2 2p4 3p1 2D1.5 8738150.0 cm-1
2s2 2p4 3p1 2F2.5 8767000.0 cm-1
2s2 2p4 3p1 2F3.5 8802740.0 cm-1
2s2 2p4 3p1 2D1.5 8814480.0 cm-1
2s2 2p4 3p1 2D2.5 8832710.0 cm-1
2s2 2p4 3p1 2P1.5 8876500.0 cm-1
2s2 2p4 3d1 4D2.5 8922900.0 cm-1
2s2 2p4 3p1 2P0.5 8924280.0 cm-1
2s2 2p4 3d1 4D1.5 8926990.0 cm-1
2s2 2p4 3d1 4D3.5 8927130.0 cm-1
2s2 2p4 3d1 2P0.5 8938460.0 cm-1
2s2 2p4 3d1 4F4.5 8953870.0 cm-1
2s2 2p4 3d1 2F3.5 8963250.0 cm-1
2s2 2p4 3d1 4P0.5 8986080.0 cm-1
2s2 2p4 3d1 4P1.5 9007920.0 cm-1
2s2 2p4 3d1 2F2.5 9022810.0 cm-1
2s2 2p4 3p1 2P1.5 9052450.0 cm-1
2s2 2p4 3d1 4F1.5 9058310.0 cm-1
2s2 2p4 3p1 2P0.5 9061930.0 cm-1
2s2 2p4 3d1 4F2.5 9065920.0 cm-1
2s2 2p4 3d1 4D0.5 9067890.0 cm-1
2s2 2p4 3d1 2D1.5 9093470.0 cm-1
2s2 2p4 3d1 4F3.5 9094500.0 cm-1
2s2 2p4 3d1 4P2.5 9119360.0 cm-1
2s2 2p4 3d1 2P1.5 9133670.0 cm-1
2s2 2p4 3d1 2D2.5 9141200.0 cm-1
2s2 2p4 3d1 2G3.5 9175030.0 cm-1
2s2 2p4 3d1 2G4.5 9182920.0 cm-1
2s2 2p4 3d1 2F2.5 9207000.0 cm-1
2s2 2p4 3d1 2S0.5 9208940.0 cm-1
2s2 2p4 3d1 2F3.5 9223550.0 cm-1
2s2 2p4 3d1 2P1.5 9235330.0 cm-1
2s2 2p4 3d1 2D2.5 9243820.0 cm-1
2s2 2p4 3d1 2D1.5 9279610.0 cm-1
2s2 2p4 3d1 2P0.5 9290560.0 cm-1
2s1 2p5 3s1 4P2.5 9355840.0 cm-1
2s1 2p5 3s1 4P1.5 9402920.0 cm-1
2s2 2p4 3d1 2D2.5 9441280.0 cm-1
2s2 2p4 3d1 2D1.5 9465620.0 cm-1
2s1 2p5 3s1 4P0.5 9477680.0 cm-1
2s1 2p5 3s1 2P1.5 9478680.0 cm-1
2s1 2p5 3s1 2P0.5 9564280.0 cm-1
2s1 2p5 3p1 4S1.5 9632710.0 cm-1
2s1 2p5 3p1 4D2.5 9662150.0 cm-1
2s1 2p5 3p1 4D3.5 9682370.0 cm-1
2s1 2p5 3p1 4D1.5 9700920.0 cm-1
2s1 2p5 3p1 4P2.5 9716000.0 cm-1
2s1 2p5 3p1 4P0.5 9740670.0 cm-1
2s1 2p5 3p1 2P1.5 9757690.0 cm-1
2s1 2p5 3p1 2P0.5 9779250.0 cm-1
2s1 2p5 3p1 2D2.5 9792040.0 cm-1
2s1 2p5 3p1 2D1.5 9796530.0 cm-1
2s1 2p5 3s1 2P1.5 9804980.0 cm-1
2s1 2p5 3p1 4D0.5 9813030.0 cm-1
2s1 2p5 3s1 2P0.5 9816500.0 cm-1
2s1 2p5 3p1 4P1.5 9875010.0 cm-1
2s1 2p5 3p1 2S0.5 9893290.0 cm-1
2s1 2p5 3d1 4P0.5 10019500.0 cm-1
2s1 2p5 3d1 4P1.5 10032600.0 cm-1
2s1 2p5 3d1 4F4.5 10045800.0 cm-1
2s1 2p5 3d1 4P2.5 10053000.0 cm-1
2s1 2p5 3d1 4F3.5 10056300.0 cm-1
2s1 2p5 3d1 4F2.5 10086200.0 cm-1
2s1 2p5 3p1 2D1.5 10087700.0 cm-1
2s1 2p5 3d1 2F3.5 10100400.0 cm-1
2s1 2p5 3d1 4D1.5 10109900.0 cm-1
2s1 2p5 3p1 2D2.5 10125700.0 cm-1
2s1 2p5 3p1 2P0.5 10126600.0 cm-1
2s1 2p5 3p1 2P1.5 10142300.0 cm-1
2s1 2p5 3d1 4D0.5 10149600.0 cm-1
2s1 2p5 3d1 2D2.5 10168700.0 cm-1
2s1 2p5 3d1 4D2.5 10173300.0 cm-1
2s1 2p5 3d1 4D3.5 10174200.0 cm-1
2s1 2p5 3d1 2D1.5 10181100.0 cm-1
2s1 2p5 3p1 2S0.5 10182100.0 cm-1
2s1 2p5 3d1 4F1.5 10194800.0 cm-1
2s1 2p5 3d1 2P0.5 10205100.0 cm-1
2s1 2p5 3d1 2F2.5 10256700.0 cm-1
2s1 2p5 3d1 2P1.5 10302900.0 cm-1
2s1 2p5 3d1 2F2.5 10490200.0 cm-1
2s1 2p5 3d1 2F3.5 10495300.0 cm-1
2s1 2p5 3d1 2P1.5 10517900.0 cm-1
2s1 2p5 3d1 2D2.5 10527200.0 cm-1
2s1 2p5 3d1 2D1.5 10528900.0 cm-1
2s1 2p5 3d1 2P0.5 10534200.0 cm-1
2s2 2p4 4s1 4P2.5 11144400.0 cm-1
2s2 2p4 4s1 2P1.5 11154300.0 cm-1
2s2 2p4 4s1 4P0.5 11255000.0 cm-1
2s2 2p4 4p1 4P1.5 11263700.0 cm-1
2s2 2p4 4p1 4P2.5 11265200.0 cm-1
2s2 2p4 4p1 4D3.5 11279700.0 cm-1
2s2 2p4 4p1 2D2.5 11279700.0 cm-1
2s2 2p4 4p1 2S0.5 11283900.0 cm-1
2s2 2p4 4s1 4P1.5 11293100.0 cm-1
2s2 2p4 4s1 2P0.5 11300600.0 cm-1
2s2 2p4 4p1 2P1.5 11315600.0 cm-1
2s2 2p4 4p1 4D0.5 11373600.0 cm-1
2s2 2p4 4s1 2D2.5 11384700.0 cm-1
2s2 2p4 4s1 2D1.5 11386700.0 cm-1
2s2 2p4 4p1 4D1.5 11391100.0 cm-1
2s2 2p4 4p1 4P0.5 11408700.0 cm-1
2s2 2p4 4d1 4D2.5 11415000.0 cm-1
2s2 2p4 4d1 4D3.5 11416000.0 cm-1
2s2 2p4 4d1 4D1.5 11416600.0 cm-1
2s2 2p4 4d1 4P0.5 11420600.0 cm-1
2s2 2p4 4d1 4F4.5 11423500.0 cm-1
2s2 2p4 4p1 4S1.5 11424800.0 cm-1
2s2 2p4 4p1 4D2.5 11425900.0 cm-1
2s2 2p4 4d1 2F3.5 11427000.0 cm-1
2s2 2p4 4p1 2D1.5 11433600.0 cm-1
2s2 2p4 4d1 2P0.5 11438700.0 cm-1
2s2 2p4 4p1 2P0.5 11441500.0 cm-1
2s2 2p4 4d1 2D1.5 11451600.0 cm-1
2s2 2p4 4d1 2D2.5 11455300.0 cm-1
2s2 2p4 4f1 4F3.5 11499400.0 cm-1
2s2 2p4 4f1 4F2.5 11499900.0 cm-1
2s2 2p4 4f1 4F4.5 11500300.0 cm-1
2s2 2p4 4f1 4D1.5 11502300.0 cm-1
2s2 2p4 4f1 2G4.5 11502400.0 cm-1
2s2 2p4 4p1 2F2.5 11502800.0 cm-1
2s2 2p4 4f1 4G5.5 11503200.0 cm-1
2s2 2p4 4f1 2F3.5 11503800.0 cm-1
2s2 2p4 4f1 4D0.5 11505000.0 cm-1
2s2 2p4 4f1 2F2.5 11506200.0 cm-1
2s2 2p4 4f1 2D1.5 11507800.0 cm-1
2s2 2p4 4p1 2F3.5 11516500.0 cm-1
2s2 2p4 4p1 2P1.5 11519100.0 cm-1
2s2 2p4 4p1 2D1.5 11524300.0 cm-1
2s2 2p4 4p1 2D2.5 11526200.0 cm-1
2s2 2p4 4d1 4F1.5 11529400.0 cm-1
2s2 2p4 4d1 4F2.5 11536000.0 cm-1
2s2 2p4 4p1 2P0.5 11553000.0 cm-1
2s2 2p4 4d1 4D0.5 11561200.0 cm-1
2s2 2p4 4d1 4F3.5 11568300.0 cm-1
2s2 2p4 4d1 4P1.5 11570400.0 cm-1
2s2 2p4 4d1 4P2.5 11577200.0 cm-1
2s2 2p4 4d1 2F2.5 11584000.0 cm-1
2s2 2p4 4d1 2P1.5 11591400.0 cm-1
2s2 2p4 4f1 4G2.5 11608900.0 cm-1
2s2 2p4 4f1 2G3.5 11611000.0 cm-1
2s2 2p4 4s1 2S0.5 11622900.0 cm-1
2s2 2p4 4f1 4F1.5 11646100.0 cm-1
2s2 2p4 4f1 4G3.5 11647900.0 cm-1
2s2 2p4 4f1 4G4.5 11648400.0 cm-1
2s2 2p4 4f1 4D2.5 11648900.0 cm-1
2s2 2p4 4f1 2D2.5 11652300.0 cm-1
2s2 2p4 4f1 4D3.5 11653200.0 cm-1
2s2 2p4 4d1 2G3.5 11654700.0 cm-1
2s2 2p4 4d1 2G4.5 11658100.0 cm-1
2s2 2p4 4d1 2D2.5 11666400.0 cm-1
2s2 2p4 4d1 2S0.5 11668000.0 cm-1
2s2 2p4 4d1 2P1.5 11669600.0 cm-1
2s2 2p4 4d1 2F3.5 11671600.0 cm-1
2s2 2p4 4d1 2F2.5 11673200.0 cm-1
2s2 2p4 4d1 2D1.5 11687600.0 cm-1
2s2 2p4 4d1 2P0.5 11693700.0 cm-1
2s2 2p4 4f1 2P0.5 11734300.0 cm-1
2s2 2p4 4f1 2H4.5 11734500.0 cm-1
2s2 2p4 4f1 2P1.5 11735800.0 cm-1
2s2 2p4 4f1 2H5.5 11736200.0 cm-1
2s2 2p4 4f1 2D2.5 11740200.0 cm-1
2s2 2p4 4f1 2D1.5 11740500.0 cm-1
2s2 2p4 4f1 2G3.5 11743200.0 cm-1
2s2 2p4 4f1 2F2.5 11744000.0 cm-1
2s2 2p4 4f1 2F3.5 11744600.0 cm-1
2s2 2p4 4f1 2G4.5 11745100.0 cm-1
2s2 2p4 4p1 2P0.5 11753400.0 cm-1
2s2 2p4 4p1 2P1.5 11759000.0 cm-1
2s2 2p4 4d1 2D2.5 11903100.0 cm-1
2s2 2p4 4d1 2D1.5 11909300.0 cm-1
2s2 2p4 4f1 2F2.5 11978100.0 cm-1
2s2 2p4 4f1 2F3.5 11979500.0 cm-1
U+20        29        21      13493656.(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 = 1.4105
         2S = 1.2103
         2P = 1.1466
         3S = 1.1341
         3P = 1.0842
         3D = 1.1189
         4S = 1.1505
         4P = 1.0968
         4D = 1.1209
         4F = 1.1302

 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 0.000005 Z**2 Rydbergs (0.027212 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (5.4424 eV) was used
 from the last threshold up to 0.922203 Z**2 Rydbergs (5019 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (5.4424 eV) was used
 from first threshold up to 0.922203 Z**2 Rydbergs (5019 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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