flike_mcw06#ti13.dat

Resolved Specific Ion Data Collections

Ion
Ti13+
Temperature Range
3.378 eV → 3.378 x 104 eV

ADF04

Filename
flike_mcw06#ti13.dat
Full Path
adf04/copaw#f/flike_mcw06#ti13.dat
Download data
  • Spontaneous Emission: Ti+13(i) → Ti+13(j) + hv
  • Electron Impact Excitation: Ti+13(i) + e → Ti+13(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 48851.0 cm-1
2s1 2p6 2S0.5 837258.0 cm-1
2s2 2p4 3s1 4P2.5 3992360.0 cm-1
2s2 2p4 3s1 4P1.5 4012280.0 cm-1
2s2 2p4 3s1 4P0.5 4033460.0 cm-1
2s2 2p4 3s1 2P1.5 4041420.0 cm-1
2s2 2p4 3s1 2P0.5 4064100.0 cm-1
2s2 2p4 3s1 2D2.5 4112560.0 cm-1
2s2 2p4 3s1 2D1.5 4114050.0 cm-1
2s2 2p4 3p1 4P2.5 4179420.0 cm-1
2s2 2p4 3p1 4P1.5 4180780.0 cm-1
2s2 2p4 3p1 4P0.5 4196620.0 cm-1
2s2 2p4 3p1 4D3.5 4202980.0 cm-1
2s2 2p4 3p1 2D2.5 4207940.0 cm-1
2s2 2p4 3p1 2P0.5 4228010.0 cm-1
2s2 2p4 3p1 4D1.5 4230160.0 cm-1
2s2 2p4 3p1 4D0.5 4235210.0 cm-1
2s2 2p4 3p1 4D2.5 4242080.0 cm-1
2s2 2p4 3s1 2S0.5 4243440.0 cm-1
2s2 2p4 3p1 2P1.5 4243680.0 cm-1
2s2 2p4 3p1 4S1.5 4254550.0 cm-1
2s2 2p4 3p1 2S0.5 4261750.0 cm-1
2s2 2p4 3p1 2D1.5 4262750.0 cm-1
2s2 2p4 3p1 2F2.5 4303320.0 cm-1
2s2 2p4 3p1 2F3.5 4311700.0 cm-1
2s2 2p4 3p1 2D1.5 4328900.0 cm-1
2s2 2p4 3p1 2D2.5 4334390.0 cm-1
2s2 2p4 3p1 2P1.5 4383910.0 cm-1
2s2 2p4 3p1 2P0.5 4397850.0 cm-1
2s2 2p4 3d1 4D3.5 4438590.0 cm-1
2s2 2p4 3d1 4D2.5 4439080.0 cm-1
2s2 2p4 3d1 4D1.5 4442940.0 cm-1
2s2 2p4 3d1 4D0.5 4449000.0 cm-1
2s2 2p4 3p1 2P1.5 4454990.0 cm-1
2s2 2p4 3d1 4F4.5 4460550.0 cm-1
2s2 2p4 3p1 2P0.5 4462600.0 cm-1
2s2 2p4 3d1 2F3.5 4469530.0 cm-1
2s2 2p4 3d1 4P0.5 4477660.0 cm-1
2s2 2p4 3d1 4P1.5 4487280.0 cm-1
2s2 2p4 3d1 4F2.5 4488030.0 cm-1
2s2 2p4 3d1 2P0.5 4493720.0 cm-1
2s2 2p4 3d1 4F1.5 4497990.0 cm-1
2s2 2p4 3d1 4F3.5 4498240.0 cm-1
2s2 2p4 3d1 4P2.5 4501220.0 cm-1
2s2 2p4 3d1 2D1.5 4506400.0 cm-1
2s2 2p4 3d1 2F2.5 4512140.0 cm-1
2s2 2p4 3d1 2P1.5 4525940.0 cm-1
2s2 2p4 3d1 2D2.5 4532550.0 cm-1
2s2 2p4 3d1 2G3.5 4561960.0 cm-1
2s2 2p4 3d1 2G4.5 4563670.0 cm-1
2s2 2p4 3d1 2S0.5 4585020.0 cm-1
2s2 2p4 3d1 2F2.5 4586610.0 cm-1
2s2 2p4 3d1 2F3.5 4591910.0 cm-1
2s2 2p4 3d1 2P1.5 4605510.0 cm-1
2s2 2p4 3d1 2D2.5 4607660.0 cm-1
2s2 2p4 3d1 2D1.5 4621990.0 cm-1
2s2 2p4 3d1 2P0.5 4622480.0 cm-1
2s2 2p4 3d1 2D2.5 4712500.0 cm-1
2s2 2p4 3d1 2D1.5 4719290.0 cm-1
2s1 2p5 3s1 4P2.5 4725340.0 cm-1
2s1 2p5 3s1 4P1.5 4746690.0 cm-1
2s1 2p5 3s1 4P0.5 4766390.0 cm-1
2s1 2p5 3s1 2P1.5 4785590.0 cm-1
2s1 2p5 3s1 2P0.5 4812820.0 cm-1
2s1 2p5 3p1 4S1.5 4900310.0 cm-1
2s1 2p5 3p1 4D3.5 4926770.0 cm-1
2s1 2p5 3p1 4D2.5 4927340.0 cm-1
2s1 2p5 3p1 4D1.5 4939320.0 cm-1
2s1 2p5 3p1 2D2.5 4949460.0 cm-1
2s1 2p5 3p1 4D0.5 4952570.0 cm-1
2s1 2p5 3p1 2P1.5 4963870.0 cm-1
2s1 2p5 3p1 4P2.5 4969990.0 cm-1
2s1 2p5 3p1 4P1.5 4973240.0 cm-1
2s1 2p5 3p1 4P0.5 4973750.0 cm-1
2s1 2p5 3p1 2P0.5 4980140.0 cm-1
2s1 2p5 3p1 2D1.5 4993620.0 cm-1
2s1 2p5 3s1 2P1.5 5018390.0 cm-1
2s1 2p5 3s1 2P0.5 5020880.0 cm-1
2s1 2p5 3p1 2S0.5 5041760.0 cm-1
2s1 2p5 3d1 4P0.5 5154970.0 cm-1
2s1 2p5 3d1 4P1.5 5160470.0 cm-1
2s1 2p5 3d1 4F4.5 5167220.0 cm-1
2s1 2p5 3d1 4P2.5 5170260.0 cm-1
2s1 2p5 3d1 4F3.5 5174420.0 cm-1
2s1 2p5 3d1 4F2.5 5185250.0 cm-1
2s1 2p5 3d1 4F1.5 5194900.0 cm-1
2s1 2p5 3d1 4D3.5 5200720.0 cm-1
2s1 2p5 3p1 2D1.5 5204500.0 cm-1
2s1 2p5 3p1 2D2.5 5213610.0 cm-1
2s1 2p5 3d1 4D0.5 5215340.0 cm-1
2s1 2p5 3d1 4D2.5 5219700.0 cm-1
2s1 2p5 3d1 4D1.5 5221660.0 cm-1
2s1 2p5 3d1 2F3.5 5221950.0 cm-1
2s1 2p5 3p1 2P0.5 5222240.0 cm-1
2s1 2p5 3d1 2D2.5 5224960.0 cm-1
2s1 2p5 3p1 2P1.5 5226600.0 cm-1
2s1 2p5 3d1 2D1.5 5236390.0 cm-1
2s1 2p5 3d1 2F2.5 5248320.0 cm-1
2s1 2p5 3p1 2S0.5 5260160.0 cm-1
2s1 2p5 3d1 2P0.5 5265580.0 cm-1
2s1 2p5 3d1 2P1.5 5290660.0 cm-1
2s2 2p4 4s1 4P2.5 5394300.0 cm-1
2s2 2p4 4s1 2P1.5 5401470.0 cm-1
2s2 2p4 4s1 4P1.5 5434240.0 cm-1
2s2 2p4 4s1 4P0.5 5435050.0 cm-1
2s2 2p4 4s1 2P0.5 5443840.0 cm-1
2s1 2p5 3d1 2F2.5 5454770.0 cm-1
2s1 2p5 3d1 2F3.5 5455840.0 cm-1
2s2 2p4 4p1 4P2.5 5470360.0 cm-1
2s1 2p5 3d1 2P1.5 5470410.0 cm-1
2s2 2p4 4p1 4P1.5 5472040.0 cm-1
2s1 2p5 3d1 2P0.5 5473870.0 cm-1
2s1 2p5 3d1 2D1.5 5475590.0 cm-1
2s1 2p5 3d1 2D2.5 5476040.0 cm-1
2s2 2p4 4p1 4D3.5 5476910.0 cm-1
2s2 2p4 4p1 2D2.5 5479150.0 cm-1
2s2 2p4 4p1 2S0.5 5481420.0 cm-1
2s2 2p4 4p1 2D1.5 5496190.0 cm-1
2s2 2p4 4s1 2D2.5 5507440.0 cm-1
2s2 2p4 4s1 2D1.5 5507830.0 cm-1
2s2 2p4 4p1 4P0.5 5509650.0 cm-1
2s2 2p4 4p1 4D2.5 5514620.0 cm-1
2s2 2p4 4p1 4D0.5 5514660.0 cm-1
2s2 2p4 4p1 4D1.5 5515760.0 cm-1
2s2 2p4 4p1 4S1.5 5519220.0 cm-1
2s2 2p4 4p1 2P1.5 5528940.0 cm-1
2s2 2p4 4p1 2P0.5 5530310.0 cm-1
2s2 2p4 4d1 4D3.5 5564250.0 cm-1
2s2 2p4 4d1 4D2.5 5564810.0 cm-1
2s2 2p4 4d1 4D1.5 5566930.0 cm-1
2s2 2p4 4d1 4F4.5 5569990.0 cm-1
2s2 2p4 4d1 4P0.5 5570150.0 cm-1
2s2 2p4 4d1 2F3.5 5573950.0 cm-1
2s2 2p4 4d1 2P0.5 5580070.0 cm-1
2s2 2p4 4p1 2F2.5 5584020.0 cm-1
2s2 2p4 4d1 4P1.5 5586380.0 cm-1
2s2 2p4 4d1 4P2.5 5586930.0 cm-1
2s2 2p4 4p1 2F3.5 5587350.0 cm-1
2s2 2p4 4p1 2D1.5 5591380.0 cm-1
2s2 2p4 4p1 2D2.5 5593560.0 cm-1
2s2 2p4 4p1 2P1.5 5599150.0 cm-1
2s2 2p4 4d1 4D0.5 5606460.0 cm-1
2s2 2p4 4d1 4F3.5 5607210.0 cm-1
2s2 2p4 4d1 4F1.5 5609460.0 cm-1
2s2 2p4 4d1 4F2.5 5609490.0 cm-1
2s2 2p4 4p1 2P0.5 5610340.0 cm-1
2s2 2p4 4d1 2D1.5 5611940.0 cm-1
2s2 2p4 4d1 2F2.5 5612870.0 cm-1
2s2 2p4 4f1 4F4.5 5614620.0 cm-1
2s2 2p4 4f1 4F3.5 5614770.0 cm-1
2s2 2p4 4f1 4F2.5 5615580.0 cm-1
2s2 2p4 4f1 4G5.5 5616250.0 cm-1
2s2 2p4 4f1 2F3.5 5616340.0 cm-1
2s2 2p4 4f1 2G4.5 5616340.0 cm-1
2s2 2p4 4f1 4D1.5 5617340.0 cm-1
2s2 2p4 4f1 2F2.5 5618330.0 cm-1
2s2 2p4 4f1 4D0.5 5619470.0 cm-1
2s2 2p4 4f1 2D1.5 5620300.0 cm-1
2s2 2p4 4d1 2D2.5 5625560.0 cm-1
2s2 2p4 4d1 2P1.5 5627860.0 cm-1
2s2 2p4 4s1 2S0.5 5638110.0 cm-1
2s2 2p4 4f1 4G4.5 5653610.0 cm-1
2s2 2p4 4f1 4G3.5 5653690.0 cm-1
2s2 2p4 4f1 4F1.5 5653750.0 cm-1
2s2 2p4 4f1 4D2.5 5654570.0 cm-1
2s2 2p4 4f1 4G2.5 5655820.0 cm-1
2s2 2p4 4f1 2G3.5 5656270.0 cm-1
2s2 2p4 4f1 2D2.5 5659770.0 cm-1
2s2 2p4 4f1 4D3.5 5659880.0 cm-1
2s2 2p4 4d1 2G3.5 5677150.0 cm-1
2s2 2p4 4d1 2G4.5 5677900.0 cm-1
2s2 2p4 4d1 2F2.5 5685440.0 cm-1
2s2 2p4 4d1 2S0.5 5687030.0 cm-1
2s2 2p4 4d1 2F3.5 5687430.0 cm-1
2s2 2p4 4d1 2P1.5 5688840.0 cm-1
2s2 2p4 4d1 2D2.5 5690200.0 cm-1
2s2 2p4 4d1 2D1.5 5696010.0 cm-1
2s2 2p4 4d1 2P0.5 5697500.0 cm-1
2s2 2p4 4p1 2P0.5 5720830.0 cm-1
2s2 2p4 4p1 2P1.5 5721330.0 cm-1
2s2 2p4 4f1 2H4.5 5722830.0 cm-1
2s2 2p4 4f1 2H5.5 5723210.0 cm-1
2s2 2p4 4f1 2P0.5 5727210.0 cm-1
2s2 2p4 4f1 2P1.5 5727500.0 cm-1
2s2 2p4 4f1 2G3.5 5728740.0 cm-1
2s2 2p4 4f1 2D1.5 5729010.0 cm-1
2s2 2p4 4f1 2D2.5 5729080.0 cm-1
2s2 2p4 4f1 2G4.5 5729160.0 cm-1
2s2 2p4 4f1 2F2.5 5729870.0 cm-1
2s2 2p4 4f1 2F3.5 5730060.0 cm-1
2s2 2p4 4d1 2D2.5 5814990.0 cm-1
2s2 2p4 4d1 2D1.5 5817210.0 cm-1
2s2 2p4 4f1 2F2.5 5857940.0 cm-1
2s2 2p4 4f1 2F3.5 5858310.0 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 = 1.4219
         2S = 1.2023
         2P = 1.1417
         3S = 1.1241
         3P = 1.0745
         3D = 1.1054
         4S = 1.1395
         4P = 1.0855
         4D = 1.1069
         4F = 1.1085

 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 (0.02299414 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (2.299414 eV) was used
 from the last threshold up to 1.085233 Z**2 Rydbergs (2495.4 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (2.299414 eV) was used
 from first threshold up to 1.085233 Z**2 Rydbergs (2495.4 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
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