flike_mcw06#ca11.dat

Resolved Specific Ion Data Collections

Ion
Ca11+
Temperature Range
2.482 eV → 2.482 x 104 eV

ADF04

Filename
flike_mcw06#ca11.dat
Full Path
adf04/copaw#f/flike_mcw06#ca11.dat
Download data
  • Spontaneous Emission: Ca+11(i) → Ca+11(j) + hv
  • Electron Impact Excitation: Ca+11(i) + e → Ca+11(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 31306.0 cm-1
2s1 2p6 2S0.5 727507.0 cm-1
2s2 2p4 3s1 4P2.5 3055120.0 cm-1
2s2 2p4 3s1 4P1.5 3070000.0 cm-1
2s2 2p4 3s1 4P0.5 3082090.0 cm-1
2s2 2p4 3s1 2P1.5 3091450.0 cm-1
2s2 2p4 3s1 2P0.5 3108880.0 cm-1
2s2 2p4 3s1 2D2.5 3153960.0 cm-1
2s2 2p4 3s1 2D1.5 3154750.0 cm-1
2s2 2p4 3p1 4P2.5 3213520.0 cm-1
2s2 2p4 3p1 4P1.5 3215720.0 cm-1
2s2 2p4 3p1 4P0.5 3225580.0 cm-1
2s2 2p4 3p1 4D3.5 3233720.0 cm-1
2s2 2p4 3p1 4D2.5 3238870.0 cm-1
2s2 2p4 3p1 4D1.5 3251460.0 cm-1
2s2 2p4 3p1 2P0.5 3253010.0 cm-1
2s2 2p4 3p1 4D0.5 3255280.0 cm-1
2s2 2p4 3p1 2D2.5 3259740.0 cm-1
2s2 2p4 3p1 2P1.5 3263910.0 cm-1
2s2 2p4 3s1 2S0.5 3266940.0 cm-1
2s2 2p4 3p1 4S1.5 3272390.0 cm-1
2s2 2p4 3p1 2D1.5 3276360.0 cm-1
2s2 2p4 3p1 2S0.5 3277500.0 cm-1
2s2 2p4 3p1 2F2.5 3317170.0 cm-1
2s2 2p4 3p1 2F3.5 3322170.0 cm-1
2s2 2p4 3p1 2D1.5 3338820.0 cm-1
2s2 2p4 3p1 2D2.5 3342160.0 cm-1
2s2 2p4 3p1 2P1.5 3386800.0 cm-1
2s2 2p4 3p1 2P0.5 3396850.0 cm-1
2s2 2p4 3d1 4D3.5 3435650.0 cm-1
2s2 2p4 3d1 4D2.5 3436450.0 cm-1
2s2 2p4 3d1 4D1.5 3439380.0 cm-1
2s2 2p4 3d1 4D0.5 3443370.0 cm-1
2s2 2p4 3p1 2P1.5 3447180.0 cm-1
2s2 2p4 3p1 2P0.5 3451730.0 cm-1
2s2 2p4 3d1 4F4.5 3455230.0 cm-1
2s2 2p4 3d1 4F3.5 3462510.0 cm-1
2s2 2p4 3d1 4P0.5 3468280.0 cm-1
2s2 2p4 3d1 4F2.5 3473490.0 cm-1
2s2 2p4 3d1 4P1.5 3474770.0 cm-1
2s2 2p4 3d1 4F1.5 3479700.0 cm-1
2s2 2p4 3d1 2F3.5 3480090.0 cm-1
2s2 2p4 3d1 2P0.5 3480950.0 cm-1
2s2 2p4 3d1 4P2.5 3483800.0 cm-1
2s2 2p4 3d1 2D1.5 3490030.0 cm-1
2s2 2p4 3d1 2F2.5 3490870.0 cm-1
2s2 2p4 3d1 2P1.5 3503780.0 cm-1
2s2 2p4 3d1 2D2.5 3507550.0 cm-1
2s2 2p4 3d1 2G3.5 3537640.0 cm-1
2s2 2p4 3d1 2G4.5 3538670.0 cm-1
2s2 2p4 3d1 2S0.5 3557100.0 cm-1
2s2 2p4 3d1 2F2.5 3559460.0 cm-1
2s2 2p4 3d1 2F3.5 3562640.0 cm-1
2s2 2p4 3d1 2P1.5 3573050.0 cm-1
2s2 2p4 3d1 2D2.5 3574800.0 cm-1
2s2 2p4 3d1 2P0.5 3583850.0 cm-1
2s2 2p4 3d1 2D1.5 3584610.0 cm-1
2s2 2p4 3d1 2D2.5 3667620.0 cm-1
2s2 2p4 3d1 2D1.5 3671260.0 cm-1
2s1 2p5 3s1 4P2.5 3692930.0 cm-1
2s1 2p5 3s1 4P1.5 3707770.0 cm-1
2s1 2p5 3s1 4P0.5 3719860.0 cm-1
2s1 2p5 3s1 2P1.5 3742350.0 cm-1
2s1 2p5 3s1 2P0.5 3760530.0 cm-1
2s1 2p5 3p1 4S1.5 3840720.0 cm-1
2s1 2p5 3p1 4D3.5 3863470.0 cm-1
2s1 2p5 3p1 4D2.5 3865490.0 cm-1
2s1 2p5 3p1 4D1.5 3873410.0 cm-1
2s1 2p5 3p1 4D0.5 3881620.0 cm-1
2s1 2p5 3p1 2D2.5 3882720.0 cm-1
2s1 2p5 3p1 2P1.5 3892610.0 cm-1
2s1 2p5 3p1 4P2.5 3895000.0 cm-1
2s1 2p5 3p1 4P0.5 3897360.0 cm-1
2s1 2p5 3p1 4P1.5 3897680.0 cm-1
2s1 2p5 3p1 2P0.5 3905340.0 cm-1
2s1 2p5 3p1 2D1.5 3911320.0 cm-1
2s1 2p5 3s1 2P1.5 3950560.0 cm-1
2s1 2p5 3s1 2P0.5 3952030.0 cm-1
2s1 2p5 3p1 2S0.5 3960550.0 cm-1
2s1 2p5 3d1 4P0.5 4060390.0 cm-1
2s1 2p5 3d1 4P1.5 4064190.0 cm-1
2s1 2p5 3d1 4F4.5 4069460.0 cm-1
2s1 2p5 3d1 4P2.5 4071090.0 cm-1
2s1 2p5 3d1 4F3.5 4074950.0 cm-1
2s1 2p5 3d1 4F2.5 4082150.0 cm-1
2s1 2p5 3d1 4F1.5 4088640.0 cm-1
2s1 2p5 3d1 4D3.5 4096410.0 cm-1
2s1 2p5 3d1 4D0.5 4105530.0 cm-1
2s1 2p5 3d1 4D2.5 4107370.0 cm-1
2s1 2p5 3d1 4D1.5 4108390.0 cm-1
2s1 2p5 3p1 2D1.5 4108880.0 cm-1
2s1 2p5 3d1 2F3.5 4110170.0 cm-1
2s1 2p5 3d1 2D2.5 4113870.0 cm-1
2s1 2p5 3p1 2D2.5 4113920.0 cm-1
2s1 2p5 3d1 2D1.5 4123210.0 cm-1
2s1 2p5 3p1 2P0.5 4123770.0 cm-1
2s1 2p5 3p1 2P1.5 4123850.0 cm-1
2s2 2p4 4s1 4P2.5 4125160.0 cm-1
2s1 2p5 3d1 2F2.5 4128870.0 cm-1
2s2 2p4 4s1 2P1.5 4133550.0 cm-1
2s1 2p5 3d1 2P0.5 4150160.0 cm-1
2s2 2p4 4s1 4P1.5 4150690.0 cm-1
2s2 2p4 4s1 4P0.5 4151020.0 cm-1
2s1 2p5 3p1 2S0.5 4154960.0 cm-1
2s2 2p4 4s1 2P0.5 4160220.0 cm-1
2s1 2p5 3d1 2P1.5 4165310.0 cm-1
2s2 2p4 4p1 4P2.5 4189030.0 cm-1
2s2 2p4 4p1 4P1.5 4190820.0 cm-1
2s2 2p4 4p1 4D3.5 4194210.0 cm-1
2s2 2p4 4p1 2D2.5 4196620.0 cm-1
2s2 2p4 4p1 2S0.5 4198030.0 cm-1
2s2 2p4 4p1 4D1.5 4208740.0 cm-1
2s2 2p4 4p1 4P0.5 4214700.0 cm-1
2s2 2p4 4p1 4D2.5 4217880.0 cm-1
2s2 2p4 4s1 2D2.5 4218230.0 cm-1
2s2 2p4 4s1 2D1.5 4218280.0 cm-1
2s2 2p4 4p1 4D0.5 4219070.0 cm-1
2s2 2p4 4p1 4S1.5 4220250.0 cm-1
2s2 2p4 4p1 2D1.5 4221960.0 cm-1
2s2 2p4 4p1 2P1.5 4231810.0 cm-1
2s2 2p4 4p1 2P0.5 4233220.0 cm-1
2s2 2p4 4d1 4D3.5 4268050.0 cm-1
2s2 2p4 4d1 4D2.5 4268670.0 cm-1
2s2 2p4 4d1 4D1.5 4270540.0 cm-1
2s2 2p4 4d1 4F4.5 4273080.0 cm-1
2s2 2p4 4d1 4D0.5 4273300.0 cm-1
2s2 2p4 4p1 2F2.5 4276580.0 cm-1
2s2 2p4 4d1 2F3.5 4276590.0 cm-1
2s2 2p4 4p1 2F3.5 4278240.0 cm-1
2s2 2p4 4d1 4P0.5 4281180.0 cm-1
2s2 2p4 4d1 4P1.5 4285860.0 cm-1
2s2 2p4 4d1 4F2.5 4285860.0 cm-1
2s2 2p4 4p1 2D1.5 4286480.0 cm-1
2s2 2p4 4p1 2D2.5 4287590.0 cm-1
2s2 2p4 4p1 2P1.5 4295350.0 cm-1
2s2 2p4 4d1 4F3.5 4296260.0 cm-1
2s2 2p4 4d1 2P0.5 4297240.0 cm-1
2s2 2p4 4d1 4F1.5 4298800.0 cm-1
2s2 2p4 4d1 4P2.5 4299010.0 cm-1
2s2 2p4 4d1 2F2.5 4301050.0 cm-1
2s2 2p4 4d1 2D1.5 4301580.0 cm-1
2s2 2p4 4p1 2P0.5 4303220.0 cm-1
2s2 2p4 4f1 4F3.5 4309380.0 cm-1
2s2 2p4 4f1 4F4.5 4309410.0 cm-1
2s2 2p4 4f1 4F2.5 4309640.0 cm-1
2s2 2p4 4f1 4G5.5 4310170.0 cm-1
2s2 2p4 4f1 2G4.5 4310320.0 cm-1
2s2 2p4 4f1 2F3.5 4310720.0 cm-1
2s2 2p4 4f1 2D1.5 4310950.0 cm-1
2s2 2p4 4f1 4D2.5 4311820.0 cm-1
2s2 2p4 4f1 4D1.5 4311980.0 cm-1
2s2 2p4 4f1 4D0.5 4311990.0 cm-1
2s2 2p4 4d1 2D2.5 4312350.0 cm-1
2s2 2p4 4d1 2P1.5 4314780.0 cm-1
2s1 2p5 3d1 2F2.5 4325430.0 cm-1
2s1 2p5 3d1 2F3.5 4325760.0 cm-1
2s1 2p5 3d1 2P1.5 4326210.0 cm-1
2s1 2p5 3d1 2P0.5 4327100.0 cm-1
2s2 2p4 4s1 2S0.5 4330410.0 cm-1
2s2 2p4 4f1 4F1.5 4332730.0 cm-1
2s2 2p4 4f1 4G4.5 4333560.0 cm-1
2s1 2p5 3d1 2D2.5 4333810.0 cm-1
2s2 2p4 4f1 4G3.5 4333820.0 cm-1
2s2 2p4 4f1 2F2.5 4335220.0 cm-1
2s2 2p4 4f1 4G2.5 4335830.0 cm-1
2s2 2p4 4f1 2G3.5 4335840.0 cm-1
2s1 2p5 3d1 2D1.5 4336220.0 cm-1
2s2 2p4 4f1 4D3.5 4340240.0 cm-1
2s2 2p4 4f1 2D2.5 4340590.0 cm-1
2s2 2p4 4d1 2G3.5 4360400.0 cm-1
2s2 2p4 4d1 2G4.5 4360840.0 cm-1
2s2 2p4 4d1 2F2.5 4367730.0 cm-1
2s2 2p4 4d1 2F3.5 4368980.0 cm-1
2s2 2p4 4d1 2S0.5 4369250.0 cm-1
2s2 2p4 4d1 2P1.5 4370620.0 cm-1
2s2 2p4 4d1 2D2.5 4371540.0 cm-1
2s2 2p4 4d1 2D1.5 4375450.0 cm-1
2s2 2p4 4d1 2P0.5 4376260.0 cm-1
2s2 2p4 4f1 2H4.5 4397000.0 cm-1
2s2 2p4 4f1 2H5.5 4397220.0 cm-1
2s2 2p4 4p1 2P0.5 4399480.0 cm-1
2s2 2p4 4p1 2P1.5 4399690.0 cm-1
2s2 2p4 4f1 2G3.5 4401890.0 cm-1
2s2 2p4 4f1 2G4.5 4402130.0 cm-1
2s2 2p4 4f1 2F2.5 4405530.0 cm-1
2s2 2p4 4f1 2F3.5 4405850.0 cm-1
2s2 2p4 4f1 2D1.5 4410020.0 cm-1
2s2 2p4 4f1 2D2.5 4410360.0 cm-1
2s2 2p4 4f1 2P1.5 4412740.0 cm-1
2s2 2p4 4f1 2P0.5 4412880.0 cm-1
2s2 2p4 4d1 2D2.5 4479650.0 cm-1
2s2 2p4 4d1 2D1.5 4480980.0 cm-1
2s2 2p4 4f1 2F2.5 4514360.0 cm-1
2s2 2p4 4f1 2F3.5 4514610.0 cm-1
A+11        20        12       5174047.(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 = 1.4268
         2S = 1.1988
         2P = 1.1395
         3S = 1.1195
         3P = 1.0702
         3D = 1.0990
         4S = 1.1344
         4P = 1.0805
         4D = 1.1001
         4F = 1.0989

 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 (0.01646326 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (1.646326 eV) was used
 from the last threshold up to 1.168967 Z**2 Rydbergs (1924.5 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (1.646326 eV) was used
 from first threshold up to 1.168967 Z**2 Rydbergs (1924.5 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
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