flike_mcw06#sc12.dat

Resolved Specific Ion Data Collections

Ion
Sc12+
Temperature Range
2.912 eV → 2.912 x 104 eV

ADF04

Filename
flike_mcw06#sc12.dat
Full Path
adf04/copaw#f/flike_mcw06#sc12.dat
Download data
  • Spontaneous Emission: Sc+12(i) → Sc+12(j) + hv
  • Electron Impact Excitation: Sc+12(i) + e → Sc+12(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 39348.0 cm-1
2s1 2p6 2S0.5 781586.0 cm-1
2s2 2p4 3s1 4P2.5 3508540.0 cm-1
2s2 2p4 3s1 4P1.5 3525990.0 cm-1
2s2 2p4 3s1 4P0.5 3542060.0 cm-1
2s2 2p4 3s1 2P1.5 3550560.0 cm-1
2s2 2p4 3s1 2P0.5 3570770.0 cm-1
2s2 2p4 3s1 2D2.5 3617480.0 cm-1
2s2 2p4 3s1 2D1.5 3618580.0 cm-1
2s2 2p4 3p1 4P2.5 3681120.0 cm-1
2s2 2p4 3p1 4P1.5 3683020.0 cm-1
2s2 2p4 3p1 4P0.5 3695700.0 cm-1
2s2 2p4 3p1 4D3.5 3702960.0 cm-1
2s2 2p4 3p1 2D2.5 3708150.0 cm-1
2s2 2p4 3p1 2P0.5 3724670.0 cm-1
2s2 2p4 3p1 4D1.5 3725070.0 cm-1
2s2 2p4 3p1 4D0.5 3729560.0 cm-1
2s2 2p4 3p1 4D2.5 3734860.0 cm-1
2s2 2p4 3p1 2P1.5 3738000.0 cm-1
2s2 2p4 3s1 2S0.5 3739050.0 cm-1
2s2 2p4 3p1 4S1.5 3747660.0 cm-1
2s2 2p4 3p1 2D1.5 3753560.0 cm-1
2s2 2p4 3p1 2S0.5 3753710.0 cm-1
2s2 2p4 3p1 2F2.5 3794420.0 cm-1
2s2 2p4 3p1 2F3.5 3800950.0 cm-1
2s2 2p4 3p1 2D1.5 3818000.0 cm-1
2s2 2p4 3p1 2D2.5 3822320.0 cm-1
2s2 2p4 3p1 2P1.5 3869650.0 cm-1
2s2 2p4 3p1 2P0.5 3881520.0 cm-1
2s2 2p4 3d1 4D3.5 3921650.0 cm-1
2s2 2p4 3d1 4D2.5 3922340.0 cm-1
2s2 2p4 3d1 4D1.5 3925760.0 cm-1
2s2 2p4 3d1 4D0.5 3930760.0 cm-1
2s2 2p4 3p1 2P1.5 3934820.0 cm-1
2s2 2p4 3p1 2P0.5 3940830.0 cm-1
2s2 2p4 3d1 4F4.5 3942500.0 cm-1
2s2 2p4 3d1 4F3.5 3950690.0 cm-1
2s2 2p4 3d1 4P0.5 3957490.0 cm-1
2s2 2p4 3d1 4F2.5 3965100.0 cm-1
2s2 2p4 3d1 4P1.5 3965510.0 cm-1
2s2 2p4 3d1 2P0.5 3971490.0 cm-1
2s2 2p4 3d1 4F1.5 3972980.0 cm-1
2s2 2p4 3d1 2F3.5 3973130.0 cm-1
2s2 2p4 3d1 4P2.5 3976730.0 cm-1
2s2 2p4 3d1 2D1.5 3982330.0 cm-1
2s2 2p4 3d1 2F2.5 3985470.0 cm-1
2s2 2p4 3d1 2P1.5 3998890.0 cm-1
2s2 2p4 3d1 2D2.5 4004050.0 cm-1
2s2 2p4 3d1 2G3.5 4033810.0 cm-1
2s2 2p4 3d1 2G4.5 4035150.0 cm-1
2s2 2p4 3d1 2S0.5 4055120.0 cm-1
2s2 2p4 3d1 2F2.5 4057140.0 cm-1
2s2 2p4 3d1 2F3.5 4061290.0 cm-1
2s2 2p4 3d1 2P1.5 4073450.0 cm-1
2s2 2p4 3d1 2D2.5 4075320.0 cm-1
2s2 2p4 3d1 2P0.5 4087090.0 cm-1
2s2 2p4 3d1 2D1.5 4087320.0 cm-1
2s2 2p4 3d1 2D2.5 4173790.0 cm-1
2s2 2p4 3d1 2D1.5 4178830.0 cm-1
2s1 2p5 3s1 4P2.5 4193230.0 cm-1
2s1 2p5 3s1 4P1.5 4211190.0 cm-1
2s1 2p5 3s1 4P0.5 4226710.0 cm-1
2s1 2p5 3s1 2P1.5 4247800.0 cm-1
2s1 2p5 3s1 2P0.5 4270220.0 cm-1
2s1 2p5 3p1 4S1.5 4354470.0 cm-1
2s1 2p5 3p1 4D3.5 4379010.0 cm-1
2s1 2p5 3p1 4D2.5 4380480.0 cm-1
2s1 2p5 3p1 4D1.5 4390290.0 cm-1
2s1 2p5 3p1 2D2.5 4400030.0 cm-1
2s1 2p5 3p1 4D0.5 4400840.0 cm-1
2s1 2p5 3p1 2P1.5 4412000.0 cm-1
2s1 2p5 3p1 4P2.5 4416030.0 cm-1
2s1 2p5 3p1 4P1.5 4419000.0 cm-1
2s1 2p5 3p1 4P0.5 4419030.0 cm-1
2s1 2p5 3p1 2P0.5 4426490.0 cm-1
2s1 2p5 3p1 2D1.5 4435680.0 cm-1
2s1 2p5 3s1 2P1.5 4468290.0 cm-1
2s1 2p5 3s1 2P0.5 4470220.0 cm-1
2s1 2p5 3p1 2S0.5 4484720.0 cm-1
2s1 2p5 3d1 4P0.5 4591620.0 cm-1
2s1 2p5 3d1 4P1.5 4596250.0 cm-1
2s1 2p5 3d1 4F4.5 4602280.0 cm-1
2s1 2p5 3d1 4P2.5 4604570.0 cm-1
2s1 2p5 3d1 4F3.5 4608650.0 cm-1
2s1 2p5 3d1 4F2.5 4617540.0 cm-1
2s1 2p5 3d1 4F1.5 4625560.0 cm-1
2s1 2p5 3d1 4D3.5 4632600.0 cm-1
2s1 2p5 3p1 2D1.5 4640720.0 cm-1
2s1 2p5 3d1 4D0.5 4644260.0 cm-1
2s1 2p5 3d1 4D2.5 4647200.0 cm-1
2s1 2p5 3p1 2D2.5 4647740.0 cm-1
2s1 2p5 3d1 4D1.5 4648580.0 cm-1
2s1 2p5 3d1 2F3.5 4649710.0 cm-1
2s1 2p5 3d1 2D2.5 4653220.0 cm-1
2s1 2p5 3p1 2P0.5 4656870.0 cm-1
2s1 2p5 3p1 2P1.5 4660190.0 cm-1
2s1 2p5 3d1 2D1.5 4663670.0 cm-1
2s1 2p5 3d1 2F2.5 4672040.0 cm-1
2s1 2p5 3p1 2S0.5 4691570.0 cm-1
2s1 2p5 3d1 2P0.5 4691880.0 cm-1
2s1 2p5 3d1 2P1.5 4711620.0 cm-1
2s2 2p4 4s1 4P2.5 4738840.0 cm-1
2s2 2p4 4s1 2P1.5 4745540.0 cm-1
2s2 2p4 4s1 4P1.5 4770890.0 cm-1
2s2 2p4 4s1 4P0.5 4771820.0 cm-1
2s2 2p4 4s1 2P0.5 4780300.0 cm-1
2s2 2p4 4p1 4P2.5 4808920.0 cm-1
2s2 2p4 4p1 4P1.5 4810680.0 cm-1
2s2 2p4 4p1 4D3.5 4814380.0 cm-1
2s2 2p4 4p1 2D2.5 4816660.0 cm-1
2s2 2p4 4p1 2S0.5 4818920.0 cm-1
2s2 2p4 4p1 4S1.5 4831500.0 cm-1
2s2 2p4 4p1 4P0.5 4840730.0 cm-1
2s2 2p4 4s1 2D2.5 4841250.0 cm-1
2s2 2p4 4s1 2D1.5 4841500.0 cm-1
2s2 2p4 4p1 4D2.5 4844640.0 cm-1
2s2 2p4 4p1 4D0.5 4845530.0 cm-1
2s2 2p4 4p1 4D1.5 4846670.0 cm-1
2s2 2p4 4p1 2D1.5 4848980.0 cm-1
2s2 2p4 4p1 2P1.5 4858670.0 cm-1
2s2 2p4 4p1 2P0.5 4860300.0 cm-1
2s1 2p5 3d1 2F2.5 4868680.0 cm-1
2s1 2p5 3d1 2F3.5 4869590.0 cm-1
2s1 2p5 3d1 2P1.5 4883160.0 cm-1
2s1 2p5 3d1 2P0.5 4885420.0 cm-1
2s1 2p5 3d1 2D1.5 4887730.0 cm-1
2s1 2p5 3d1 2D2.5 4888340.0 cm-1
2s2 2p4 4d1 4D3.5 4895330.0 cm-1
2s2 2p4 4d1 4D2.5 4895940.0 cm-1
2s2 2p4 4d1 4D1.5 4897960.0 cm-1
2s2 2p4 4d1 4F4.5 4900730.0 cm-1
2s2 2p4 4d1 2P0.5 4900960.0 cm-1
2s2 2p4 4d1 2F3.5 4904500.0 cm-1
2s2 2p4 4d1 4P0.5 4909860.0 cm-1
2s2 2p4 4p1 2F2.5 4914420.0 cm-1
2s2 2p4 4d1 4P1.5 4915340.0 cm-1
2s2 2p4 4d1 4P2.5 4915570.0 cm-1
2s2 2p4 4p1 2F3.5 4917060.0 cm-1
2s2 2p4 4p1 2D1.5 4919270.0 cm-1
2s2 2p4 4p1 2D2.5 4921170.0 cm-1
2s2 2p4 4p1 2P1.5 4926230.0 cm-1
2s2 2p4 4d1 4F3.5 4930260.0 cm-1
2s2 2p4 4d1 4D0.5 4930370.0 cm-1
2s2 2p4 4d1 4F1.5 4932840.0 cm-1
2s2 2p4 4d1 4F2.5 4932930.0 cm-1
2s2 2p4 4d1 2D1.5 4935290.0 cm-1
2s2 2p4 4p1 2P0.5 4935440.0 cm-1
2s2 2p4 4d1 2F2.5 4935480.0 cm-1
2s2 2p4 4f1 4F4.5 4941130.0 cm-1
2s2 2p4 4f1 4F3.5 4941370.0 cm-1
2s2 2p4 4f1 4F2.5 4942270.0 cm-1
2s2 2p4 4f1 4G5.5 4942380.0 cm-1
2s2 2p4 4f1 2G4.5 4942510.0 cm-1
2s2 2p4 4f1 2F3.5 4942640.0 cm-1
2s2 2p4 4f1 4D1.5 4944050.0 cm-1
2s2 2p4 4f1 2F2.5 4944690.0 cm-1
2s2 2p4 4f1 4D0.5 4946010.0 cm-1
2s2 2p4 4f1 2D1.5 4946680.0 cm-1
2s2 2p4 4d1 2D2.5 4947620.0 cm-1
2s2 2p4 4d1 2P1.5 4950000.0 cm-1
2s2 2p4 4s1 2S0.5 4962520.0 cm-1
2s2 2p4 4f1 4G4.5 4972060.0 cm-1
2s2 2p4 4f1 4G3.5 4972180.0 cm-1
2s2 2p4 4f1 4F1.5 4972570.0 cm-1
2s2 2p4 4f1 4D2.5 4973210.0 cm-1
2s2 2p4 4f1 4G2.5 4974140.0 cm-1
2s2 2p4 4f1 2G3.5 4974480.0 cm-1
2s2 2p4 4f1 2D2.5 4978710.0 cm-1
2s2 2p4 4f1 4D3.5 4978770.0 cm-1
2s2 2p4 4d1 2G3.5 4997380.0 cm-1
2s2 2p4 4d1 2G4.5 4997960.0 cm-1
2s2 2p4 4d1 2F2.5 5005210.0 cm-1
2s2 2p4 4d1 2S0.5 5006750.0 cm-1
2s2 2p4 4d1 2F3.5 5006810.0 cm-1
2s2 2p4 4d1 2P1.5 5008370.0 cm-1
2s2 2p4 4d1 2D2.5 5009490.0 cm-1
2s2 2p4 4d1 2D1.5 5014310.0 cm-1
2s2 2p4 4d1 2P0.5 5015430.0 cm-1
2s2 2p4 4f1 2H4.5 5038480.0 cm-1
2s2 2p4 4p1 2P0.5 5038560.0 cm-1
2s2 2p4 4f1 2H5.5 5038780.0 cm-1
2s2 2p4 4p1 2P1.5 5038880.0 cm-1
2s2 2p4 4f1 2G3.5 5043900.0 cm-1
2s2 2p4 4f1 2G4.5 5044220.0 cm-1
2s2 2p4 4f1 2F2.5 5045620.0 cm-1
2s2 2p4 4f1 2F3.5 5045870.0 cm-1
2s2 2p4 4f1 2P0.5 5045880.0 cm-1
2s2 2p4 4f1 2P1.5 5046000.0 cm-1
2s2 2p4 4f1 2D1.5 5046220.0 cm-1
2s2 2p4 4f1 2D2.5 5046370.0 cm-1
2s2 2p4 4d1 2D2.5 5125590.0 cm-1
2s2 2p4 4d1 2D1.5 5127330.0 cm-1
2s2 2p4 4f1 2F2.5 5164310.0 cm-1
2s2 2p4 4f1 2F3.5 5164610.0 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 = 1.4242
         2S = 1.2007
         2P = 1.1406
         3S = 1.1220
         3P = 1.0725
         3D = 1.1024
         4S = 1.1371
         4P = 1.0832
         4D = 1.1037
         4F = 1.1039

 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 (0.01959264 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (1.959264 eV) was used
 from the last threshold up to 1.123432 Z**2 Rydbergs (2201.1 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (1.959264 eV) was used
 from first threshold up to 1.123432 Z**2 Rydbergs (2201.1 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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