flike_mcw06#zn21.dat

Resolved Specific Ion Data Collections

Ion
Zn21+
Temperature Range
8.341 eV → 8.341 x 104 eV

ADF04

Filename
flike_mcw06#zn21.dat
Full Path
adf04/copaw#f/flike_mcw06#zn21.dat
Download data
  • Spontaneous Emission: Zn+21(i) → Zn+21(j) + hv
  • Electron Impact Excitation: Zn+21(i) + e → Zn+21(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 199494.0 cm-1
2s1 2p6 2S0.5 1363430.0 cm-1
2s2 2p4 3s1 4P2.5 8954590.0 cm-1
2s2 2p4 3s1 2P1.5 8987940.0 cm-1
2s2 2p4 3s1 4P0.5 9080280.0 cm-1
2s2 2p4 3s1 4P1.5 9134190.0 cm-1
2s2 2p4 3s1 2P0.5 9162380.0 cm-1
2s2 2p4 3s1 2D2.5 9231850.0 cm-1
2s2 2p4 3s1 2D1.5 9238820.0 cm-1
2s2 2p4 3p1 4P1.5 9255090.0 cm-1
2s2 2p4 3p1 4P2.5 9265570.0 cm-1
2s2 2p4 3p1 2P0.5 9307380.0 cm-1
2s2 2p4 3p1 2D2.5 9311260.0 cm-1
2s2 2p4 3p1 4D3.5 9314390.0 cm-1
2s2 2p4 3p1 4D0.5 9391110.0 cm-1
2s2 2p4 3p1 4S1.5 9399480.0 cm-1
2s2 2p4 3p1 4P0.5 9426180.0 cm-1
2s2 2p4 3p1 4D1.5 9432120.0 cm-1
2s2 2p4 3p1 2P1.5 9468160.0 cm-1
2s2 2p4 3p1 4D2.5 9483070.0 cm-1
2s2 2p4 3s1 2S0.5 9497280.0 cm-1
2s2 2p4 3p1 2S0.5 9506010.0 cm-1
2s2 2p4 3p1 2D1.5 9511030.0 cm-1
2s2 2p4 3p1 2F2.5 9535830.0 cm-1
2s2 2p4 3p1 2F3.5 9578310.0 cm-1
2s2 2p4 3p1 2D1.5 9588750.0 cm-1
2s2 2p4 3p1 2D2.5 9609140.0 cm-1
2s2 2p4 3p1 2P1.5 9648380.0 cm-1
2s2 2p4 3d1 4D2.5 9687670.0 cm-1
2s2 2p4 3d1 4D1.5 9691330.0 cm-1
2s2 2p4 3d1 4D3.5 9693140.0 cm-1
2s2 2p4 3d1 2P0.5 9703340.0 cm-1
2s2 2p4 3p1 2P0.5 9705380.0 cm-1
2s2 2p4 3d1 4F4.5 9720360.0 cm-1
2s2 2p4 3d1 2F3.5 9729020.0 cm-1
2s2 2p4 3d1 4P0.5 9754590.0 cm-1
2s2 2p4 3d1 4P1.5 9778340.0 cm-1
2s2 2p4 3d1 2D2.5 9795460.0 cm-1
2s2 2p4 3d1 4F1.5 9834990.0 cm-1
2s2 2p4 3d1 4F2.5 9845450.0 cm-1
2s2 2p4 3p1 2P1.5 9853140.0 cm-1
2s2 2p4 3d1 4D0.5 9856050.0 cm-1
2s2 2p4 3p1 2P0.5 9859450.0 cm-1
2s2 2p4 3d1 2D1.5 9883370.0 cm-1
2s2 2p4 3d1 4F3.5 9886000.0 cm-1
2s2 2p4 3d1 4P2.5 9912300.0 cm-1
2s2 2p4 3d1 2P1.5 9926900.0 cm-1
2s2 2p4 3d1 2F2.5 9932180.0 cm-1
2s2 2p4 3d1 2G3.5 9968080.0 cm-1
2s2 2p4 3d1 2G4.5 9977650.0 cm-1
2s2 2p4 3d1 2F2.5 10001600.0 cm-1
2s2 2p4 3d1 2S0.5 10003500.0 cm-1
2s2 2p4 3d1 2F3.5 10019800.0 cm-1
2s2 2p4 3d1 2P1.5 10029800.0 cm-1
2s2 2p4 3d1 2D2.5 10039300.0 cm-1
2s2 2p4 3d1 2D1.5 10079200.0 cm-1
2s2 2p4 3d1 2P0.5 10092100.0 cm-1
2s1 2p5 3s1 4P2.5 10149100.0 cm-1
2s1 2p5 3s1 4P1.5 10199700.0 cm-1
2s2 2p4 3d1 2D2.5 10261300.0 cm-1
2s1 2p5 3s1 2P1.5 10284700.0 cm-1
2s1 2p5 3s1 4P0.5 10285500.0 cm-1
2s2 2p4 3d1 2D1.5 10287600.0 cm-1
2s1 2p5 3s1 2P0.5 10384700.0 cm-1
2s1 2p5 3p1 4S1.5 10441100.0 cm-1
2s1 2p5 3p1 4D2.5 10470500.0 cm-1
2s1 2p5 3p1 4D3.5 10496400.0 cm-1
2s1 2p5 3p1 4D1.5 10515500.0 cm-1
2s1 2p5 3p1 4P2.5 10531600.0 cm-1
2s1 2p5 3p1 4P0.5 10559600.0 cm-1
2s1 2p5 3p1 2P1.5 10577900.0 cm-1
2s1 2p5 3p1 2P0.5 10598700.0 cm-1
2s1 2p5 3p1 2D2.5 10618700.0 cm-1
2s1 2p5 3p1 2D1.5 10623400.0 cm-1
2s1 2p5 3s1 2P1.5 10627400.0 cm-1
2s1 2p5 3s1 2P0.5 10641300.0 cm-1
2s1 2p5 3p1 4D0.5 10644900.0 cm-1
2s1 2p5 3p1 4P1.5 10717300.0 cm-1
2s1 2p5 3p1 2S0.5 10727100.0 cm-1
2s1 2p5 3d1 4P0.5 10849200.0 cm-1
2s1 2p5 3d1 4P1.5 10863600.0 cm-1
2s1 2p5 3d1 4F4.5 10878200.0 cm-1
2s1 2p5 3d1 4P2.5 10885500.0 cm-1
2s1 2p5 3d1 4F3.5 10888600.0 cm-1
2s1 2p5 3d1 4F2.5 10921800.0 cm-1
2s1 2p5 3p1 2D1.5 10924300.0 cm-1
2s1 2p5 3d1 2F3.5 10935600.0 cm-1
2s1 2p5 3d1 4D1.5 10947700.0 cm-1
2s1 2p5 3p1 2P0.5 10968200.0 cm-1
2s1 2p5 3p1 2D2.5 10969200.0 cm-1
2s1 2p5 3p1 2P1.5 10986100.0 cm-1
2s1 2p5 3d1 4D0.5 10991600.0 cm-1
2s1 2p5 3d1 2D2.5 11013000.0 cm-1
2s1 2p5 3d1 2F2.5 11019300.0 cm-1
2s1 2p5 3d1 4D3.5 11020400.0 cm-1
2s1 2p5 3p1 2S0.5 11024900.0 cm-1
2s1 2p5 3d1 2D1.5 11025100.0 cm-1
2s1 2p5 3d1 2P0.5 11046100.0 cm-1
2s1 2p5 3d1 4F1.5 11046100.0 cm-1
2s1 2p5 3d1 4D2.5 11117700.0 cm-1
2s1 2p5 3d1 2P1.5 11161200.0 cm-1
2s1 2p5 3d1 2F2.5 11351200.0 cm-1
2s1 2p5 3d1 2F3.5 11357500.0 cm-1
2s1 2p5 3d1 2P1.5 11380600.0 cm-1
2s1 2p5 3d1 2D2.5 11391000.0 cm-1
2s1 2p5 3d1 2D1.5 11393000.0 cm-1
2s1 2p5 3d1 2P0.5 11399300.0 cm-1
2s2 2p4 4s1 4P2.5 12132000.0 cm-1
2s2 2p4 4s1 2P1.5 12142300.0 cm-1
2s2 2p4 4s1 4P0.5 12252300.0 cm-1
2s2 2p4 4p1 4P1.5 12257200.0 cm-1
2s2 2p4 4p1 4P2.5 12259200.0 cm-1
2s2 2p4 4p1 2D2.5 12275700.0 cm-1
2s2 2p4 4p1 4D3.5 12275900.0 cm-1
2s2 2p4 4p1 2S0.5 12279900.0 cm-1
2s2 2p4 4s1 4P1.5 12306400.0 cm-1
2s2 2p4 4s1 2P0.5 12314100.0 cm-1
2s2 2p4 4p1 2P1.5 12314100.0 cm-1
2s2 2p4 4p1 4D0.5 12376900.0 cm-1
2s2 2p4 4p1 4S1.5 12398100.0 cm-1
2s2 2p4 4s1 2D2.5 12400500.0 cm-1
2s2 2p4 4s1 2D1.5 12402900.0 cm-1
2s2 2p4 4d1 4D2.5 12418100.0 cm-1
2s2 2p4 4d1 4D3.5 12419600.0 cm-1
2s2 2p4 4d1 4D1.5 12419600.0 cm-1
2s2 2p4 4d1 4P0.5 12423600.0 cm-1
2s2 2p4 4d1 4F4.5 12427300.0 cm-1
2s2 2p4 4p1 4P0.5 12427900.0 cm-1
2s2 2p4 4d1 2F3.5 12430400.0 cm-1
2s2 2p4 4d1 2P0.5 12443100.0 cm-1
2s2 2p4 4p1 4D1.5 12443900.0 cm-1
2s2 2p4 4p1 4D2.5 12447800.0 cm-1
2s2 2p4 4p1 2D1.5 12455700.0 cm-1
2s2 2p4 4d1 2D1.5 12457000.0 cm-1
2s2 2p4 4d1 2D2.5 12461300.0 cm-1
2s2 2p4 4p1 2P0.5 12463800.0 cm-1
2s2 2p4 4f1 4F3.5 12507900.0 cm-1
2s2 2p4 4f1 4F2.5 12508400.0 cm-1
2s2 2p4 4f1 4F4.5 12508900.0 cm-1
2s2 2p4 4f1 4D1.5 12510700.0 cm-1
2s2 2p4 4f1 2G4.5 12510900.0 cm-1
2s2 2p4 4f1 4G5.5 12512000.0 cm-1
2s2 2p4 4f1 2F3.5 12512700.0 cm-1
2s2 2p4 4f1 4D0.5 12513500.0 cm-1
2s2 2p4 4f1 2F2.5 12515100.0 cm-1
2s2 2p4 4f1 2D1.5 12516700.0 cm-1
2s2 2p4 4p1 2F2.5 12524700.0 cm-1
2s2 2p4 4p1 2F3.5 12541100.0 cm-1
2s2 2p4 4d1 4F1.5 12542500.0 cm-1
2s2 2p4 4p1 2P1.5 12542800.0 cm-1
2s2 2p4 4p1 2D1.5 12547600.0 cm-1
2s2 2p4 4d1 4F2.5 12550700.0 cm-1
2s2 2p4 4p1 2D2.5 12551100.0 cm-1
2s2 2p4 4p1 2P0.5 12579300.0 cm-1
2s2 2p4 4d1 4D0.5 12589500.0 cm-1
2s2 2p4 4d1 4F3.5 12597800.0 cm-1
2s2 2p4 4d1 4P1.5 12599300.0 cm-1
2s2 2p4 4d1 4P2.5 12607100.0 cm-1
2s2 2p4 4d1 2F2.5 12612800.0 cm-1
2s2 2p4 4d1 2P1.5 12621500.0 cm-1
2s2 2p4 4f1 4G2.5 12626800.0 cm-1
2s2 2p4 4f1 2G3.5 12629300.0 cm-1
2s2 2p4 4s1 2S0.5 12663900.0 cm-1
2s2 2p4 4f1 4F1.5 12680100.0 cm-1
2s2 2p4 4f1 4G3.5 12682100.0 cm-1
2s2 2p4 4f1 4G4.5 12682900.0 cm-1
2s2 2p4 4f1 4D2.5 12683200.0 cm-1
2s2 2p4 4d1 2G3.5 12686100.0 cm-1
2s2 2p4 4f1 2D2.5 12686900.0 cm-1
2s2 2p4 4f1 4D3.5 12687900.0 cm-1
2s2 2p4 4d1 2G4.5 12690200.0 cm-1
2s2 2p4 4d1 2D2.5 12698600.0 cm-1
2s2 2p4 4d1 2S0.5 12700000.0 cm-1
2s2 2p4 4d1 2P1.5 12701400.0 cm-1
2s2 2p4 4d1 2F3.5 12704100.0 cm-1
2s2 2p4 4d1 2F2.5 12705300.0 cm-1
2s2 2p4 4d1 2D1.5 12721100.0 cm-1
2s2 2p4 4d1 2P0.5 12728200.0 cm-1
2s2 2p4 4f1 2P0.5 12770800.0 cm-1
2s2 2p4 4f1 2H4.5 12771100.0 cm-1
2s2 2p4 4f1 2P1.5 12772500.0 cm-1
2s2 2p4 4f1 2H5.5 12773200.0 cm-1
2s2 2p4 4f1 2D2.5 12777000.0 cm-1
2s2 2p4 4f1 2D1.5 12777400.0 cm-1
2s2 2p4 4f1 2G3.5 12780200.0 cm-1
2s2 2p4 4f1 2F2.5 12781100.0 cm-1
2s2 2p4 4f1 2F3.5 12781800.0 cm-1
2s2 2p4 4f1 2G4.5 12782400.0 cm-1
2s2 2p4 4p1 2P0.5 12801500.0 cm-1
2s2 2p4 4p1 2P1.5 12808900.0 cm-1
2s2 2p4 4d1 2D2.5 12960500.0 cm-1
2s2 2p4 4d1 2D1.5 12967100.0 cm-1
2s2 2p4 4f1 2F2.5 13040200.0 cm-1
2s2 2p4 4f1 2F3.5 13041900.0 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 = 1.4093
         2S = 1.2111
         2P = 1.1471
         3S = 1.1350
         3P = 1.0851
         3D = 1.1202
         4S = 1.1515
         4P = 1.0979
         4D = 1.1223
         4F = 1.1321

 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 (0.03000123 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (6.000246 eV) was used
 from the last threshold up to 0.914962 Z**2 Rydbergs (5490 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (6.000246 eV) was used
 from first threshold up to 0.914962 Z**2 Rydbergs (5490 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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