flike_mcw06#k10.dat

Resolved Specific Ion Data Collections

Ion
K10+
Temperature Range
2.085 eV → 2.085 x 104 eV

ADF04

Filename
flike_mcw06#k10.dat
Full Path
adf04/copaw#f/flike_mcw06#k10.dat
Download data
  • Spontaneous Emission: K+10(i) → K+10(j) + hv
  • Electron Impact Excitation: K+10(i) + e → K+10(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 24564.0 cm-1
2s1 2p6 2S0.5 674837.0 cm-1
2s2 2p4 3s1 4P2.5 2632160.0 cm-1
2s2 2p4 3s1 4P1.5 2644480.0 cm-1
2s2 2p4 3s1 4P0.5 2653520.0 cm-1
2s2 2p4 3s1 2P1.5 2663840.0 cm-1
2s2 2p4 3s1 2P0.5 2678380.0 cm-1
2s2 2p4 3s1 2D2.5 2721850.0 cm-1
2s2 2p4 3s1 2D1.5 2722400.0 cm-1
2s2 2p4 3p1 4P2.5 2776650.0 cm-1
2s2 2p4 3p1 4P1.5 2778940.0 cm-1
2s2 2p4 3p1 4P0.5 2786380.0 cm-1
2s2 2p4 3p1 4D3.5 2795240.0 cm-1
2s2 2p4 3p1 4D2.5 2800120.0 cm-1
2s2 2p4 3p1 4D1.5 2809260.0 cm-1
2s2 2p4 3p1 4D0.5 2812360.0 cm-1
2s2 2p4 3p1 2P0.5 2812840.0 cm-1
2s2 2p4 3p1 2D2.5 2816530.0 cm-1
2s2 2p4 3p1 2P1.5 2821310.0 cm-1
2s2 2p4 3s1 2S0.5 2826770.0 cm-1
2s2 2p4 3p1 4S1.5 2828560.0 cm-1
2s2 2p4 3p1 2D1.5 2831100.0 cm-1
2s2 2p4 3p1 2S0.5 2832940.0 cm-1
2s2 2p4 3p1 2F2.5 2871410.0 cm-1
2s2 2p4 3p1 2F3.5 2875180.0 cm-1
2s2 2p4 3p1 2D1.5 2891190.0 cm-1
2s2 2p4 3p1 2D2.5 2893700.0 cm-1
2s2 2p4 3p1 2P1.5 2935260.0 cm-1
2s2 2p4 3p1 2P0.5 2943680.0 cm-1
2s2 2p4 3d1 4D3.5 2980540.0 cm-1
2s2 2p4 3d1 4D2.5 2981390.0 cm-1
2s2 2p4 3d1 4D1.5 2983820.0 cm-1
2s2 2p4 3d1 4D0.5 2986900.0 cm-1
2s2 2p4 3p1 2P1.5 2991660.0 cm-1
2s2 2p4 3p1 2P0.5 2994970.0 cm-1
2s2 2p4 3d1 4F4.5 2998720.0 cm-1
2s2 2p4 3d1 4F3.5 3004980.0 cm-1
2s2 2p4 3d1 4P0.5 3010010.0 cm-1
2s2 2p4 3d1 4F2.5 3013190.0 cm-1
2s2 2p4 3d1 4P1.5 3015090.0 cm-1
2s2 2p4 3d1 4F1.5 3018080.0 cm-1
2s2 2p4 3d1 2F3.5 3018870.0 cm-1
2s2 2p4 3d1 2P0.5 3021760.0 cm-1
2s2 2p4 3d1 4P2.5 3022320.0 cm-1
2s2 2p4 3d1 2F2.5 3028090.0 cm-1
2s2 2p4 3d1 2D1.5 3029170.0 cm-1
2s2 2p4 3d1 2P1.5 3040390.0 cm-1
2s2 2p4 3d1 2D2.5 3042900.0 cm-1
2s2 2p4 3d1 2G3.5 3073220.0 cm-1
2s2 2p4 3d1 2G4.5 3074000.0 cm-1
2s2 2p4 3d1 2S0.5 3090770.0 cm-1
2s2 2p4 3d1 2F2.5 3093350.0 cm-1
2s2 2p4 3d1 2F3.5 3095730.0 cm-1
2s2 2p4 3d1 2P1.5 3104170.0 cm-1
2s2 2p4 3d1 2D2.5 3105930.0 cm-1
2s2 2p4 3d1 2P0.5 3112570.0 cm-1
2s2 2p4 3d1 2D1.5 3113730.0 cm-1
2s2 2p4 3d1 2D2.5 3193610.0 cm-1
2s2 2p4 3d1 2D1.5 3196160.0 cm-1
2s1 2p5 3s1 4P2.5 3224300.0 cm-1
2s1 2p5 3s1 4P1.5 3236320.0 cm-1
2s1 2p5 3s1 4P0.5 3245630.0 cm-1
2s1 2p5 3s1 2P1.5 3268960.0 cm-1
2s1 2p5 3s1 2P0.5 3283490.0 cm-1
2s1 2p5 3p1 4S1.5 3358930.0 cm-1
2s1 2p5 3p1 4D3.5 3379960.0 cm-1
2s1 2p5 3p1 4D2.5 3382210.0 cm-1
2s1 2p5 3p1 4D1.5 3388500.0 cm-1
2s1 2p5 3p1 4D0.5 3394760.0 cm-1
2s1 2p5 3p1 4P2.5 3397270.0 cm-1
2s1 2p5 3p1 2P1.5 3405340.0 cm-1
2s1 2p5 3p1 2D2.5 3406610.0 cm-1
2s1 2p5 3p1 4P0.5 3408330.0 cm-1
2s1 2p5 3p1 4P1.5 3409040.0 cm-1
2s1 2p5 3p1 2P0.5 3416520.0 cm-1
2s1 2p5 3p1 2D1.5 3420150.0 cm-1
2s1 2p5 3s1 2P1.5 3464860.0 cm-1
2s1 2p5 3s1 2P0.5 3465940.0 cm-1
2s1 2p5 3p1 2S0.5 3468930.0 cm-1
2s2 2p4 4s1 4P2.5 3552460.0 cm-1
2s2 2p4 4s1 2P1.5 3557240.0 cm-1
2s1 2p5 3d1 4P0.5 3560780.0 cm-1
2s1 2p5 3d1 4P1.5 3563690.0 cm-1
2s1 2p5 3d1 4F4.5 3568320.0 cm-1
2s1 2p5 3d1 4P2.5 3568980.0 cm-1
2s2 2p4 4s1 4P1.5 3572140.0 cm-1
2s1 2p5 3d1 4F3.5 3572820.0 cm-1
2s2 2p4 4s1 4P0.5 3573130.0 cm-1
2s1 2p5 3d1 4F2.5 3578490.0 cm-1
2s2 2p4 4s1 2P0.5 3579520.0 cm-1
2s1 2p5 3d1 4F1.5 3583610.0 cm-1
2s1 2p5 3d1 4D3.5 3589870.0 cm-1
2s1 2p5 3d1 4D0.5 3597300.0 cm-1
2s1 2p5 3d1 4D2.5 3597520.0 cm-1
2s1 2p5 3d1 4D1.5 3598950.0 cm-1
2s1 2p5 3d1 2F3.5 3601800.0 cm-1
2s1 2p5 3d1 2D2.5 3604230.0 cm-1
2s1 2p5 3p1 2D1.5 3605690.0 cm-1
2s1 2p5 3p1 2D2.5 3608610.0 cm-1
2s1 2p5 3d1 2D1.5 3611530.0 cm-1
2s2 2p4 4p1 4P2.5 3611540.0 cm-1
2s2 2p4 4p1 4P1.5 3613320.0 cm-1
2s1 2p5 3d1 2F2.5 3614720.0 cm-1
2s2 2p4 4p1 2S0.5 3618320.0 cm-1
2s2 2p4 4p1 4D3.5 3618820.0 cm-1
2s2 2p4 4p1 2D2.5 3623960.0 cm-1
2s1 2p5 3p1 2P0.5 3624730.0 cm-1
2s1 2p5 3p1 2P1.5 3626650.0 cm-1
2s2 2p4 4p1 4D1.5 3629300.0 cm-1
2s2 2p4 4p1 4P0.5 3630950.0 cm-1
2s2 2p4 4p1 4S1.5 3636040.0 cm-1
2s2 2p4 4p1 4D0.5 3636320.0 cm-1
2s2 2p4 4p1 4D2.5 3636350.0 cm-1
2s1 2p5 3d1 2P0.5 3638200.0 cm-1
2s2 2p4 4p1 2P1.5 3639140.0 cm-1
2s2 2p4 4s1 2D1.5 3641420.0 cm-1
2s2 2p4 4s1 2D2.5 3642380.0 cm-1
2s2 2p4 4p1 2D1.5 3643020.0 cm-1
2s1 2p5 3p1 2S0.5 3651140.0 cm-1
2s2 2p4 4p1 2P0.5 3652320.0 cm-1
2s1 2p5 3d1 2P1.5 3658080.0 cm-1
2s2 2p4 4d1 4D3.5 3682380.0 cm-1
2s2 2p4 4d1 4D2.5 3682990.0 cm-1
2s2 2p4 4d1 4D1.5 3684690.0 cm-1
2s2 2p4 4d1 4F4.5 3687020.0 cm-1
2s2 2p4 4d1 4D0.5 3687150.0 cm-1
2s2 2p4 4d1 2F3.5 3690230.0 cm-1
2s2 2p4 4p1 2F2.5 3691670.0 cm-1
2s2 2p4 4p1 2F3.5 3693020.0 cm-1
2s2 2p4 4d1 4P0.5 3694040.0 cm-1
2s2 2p4 4d1 4F2.5 3697820.0 cm-1
2s2 2p4 4d1 4P1.5 3697970.0 cm-1
2s2 2p4 4p1 2D1.5 3699080.0 cm-1
2s2 2p4 4p1 2D2.5 3699950.0 cm-1
2s2 2p4 4d1 4F3.5 3705010.0 cm-1
2s2 2p4 4d1 2P0.5 3706860.0 cm-1
2s2 2p4 4d1 4F1.5 3707310.0 cm-1
2s2 2p4 4p1 2P1.5 3707550.0 cm-1
2s2 2p4 4d1 4P2.5 3707640.0 cm-1
2s2 2p4 4d1 2F2.5 3709360.0 cm-1
2s2 2p4 4d1 2D1.5 3710590.0 cm-1
2s2 2p4 4p1 2P0.5 3713830.0 cm-1
2s2 2p4 4f1 4G4.5 3719560.0 cm-1
2s2 2p4 4f1 4G5.5 3719600.0 cm-1
2s2 2p4 4d1 2D2.5 3719680.0 cm-1
2s2 2p4 4f1 4F3.5 3719800.0 cm-1
2s2 2p4 4f1 2G4.5 3719820.0 cm-1
2s2 2p4 4f1 4F2.5 3720650.0 cm-1
2s2 2p4 4f1 2F3.5 3720950.0 cm-1
2s2 2p4 4f1 4D1.5 3721980.0 cm-1
2s2 2p4 4d1 2P1.5 3722090.0 cm-1
2s2 2p4 4f1 4D2.5 3722440.0 cm-1
2s2 2p4 4f1 4D0.5 3723520.0 cm-1
2s2 2p4 4f1 2D1.5 3723750.0 cm-1
2s2 2p4 4f1 4F4.5 3738000.0 cm-1
2s2 2p4 4f1 4G3.5 3738060.0 cm-1
2s2 2p4 4f1 4G2.5 3739450.0 cm-1
2s2 2p4 4f1 4F1.5 3739520.0 cm-1
2s2 2p4 4f1 2G3.5 3739790.0 cm-1
2s2 2p4 4f1 2F2.5 3739970.0 cm-1
2s2 2p4 4s1 2S0.5 3741930.0 cm-1
2s2 2p4 4f1 2D2.5 3744290.0 cm-1
2s2 2p4 4f1 4D3.5 3744420.0 cm-1
2s2 2p4 4d1 2G3.5 3766010.0 cm-1
2s2 2p4 4d1 2G4.5 3766350.0 cm-1
2s2 2p4 4d1 2F2.5 3772800.0 cm-1
2s2 2p4 4d1 2F3.5 3773740.0 cm-1
2s2 2p4 4d1 2S0.5 3774320.0 cm-1
2s2 2p4 4f1 2P1.5 3775200.0 cm-1
2s2 2p4 4d1 2P1.5 3775420.0 cm-1
2s2 2p4 4f1 2P0.5 3775440.0 cm-1
2s2 2p4 4d1 2D2.5 3776160.0 cm-1
2s2 2p4 4d1 2D1.5 3779260.0 cm-1
2s2 2p4 4d1 2P0.5 3779840.0 cm-1
2s2 2p4 4f1 2D2.5 3784330.0 cm-1
2s2 2p4 4f1 2D1.5 3784570.0 cm-1
2s2 2p4 4f1 2F3.5 3788780.0 cm-1
2s2 2p4 4f1 2F2.5 3789080.0 cm-1
2s2 2p4 4f1 2H4.5 3798180.0 cm-1
2s2 2p4 4f1 2H5.5 3798340.0 cm-1
2s2 2p4 4f1 2G3.5 3802530.0 cm-1
2s2 2p4 4f1 2G4.5 3802710.0 cm-1
2s2 2p4 4p1 2P0.5 3803350.0 cm-1
2s2 2p4 4p1 2P1.5 3803500.0 cm-1
2s1 2p5 3d1 2F2.5 3822320.0 cm-1
2s1 2p5 3d1 2F3.5 3822940.0 cm-1
2s1 2p5 3d1 2D1.5 3840620.0 cm-1
2s1 2p5 3d1 2D2.5 3841190.0 cm-1
2s1 2p5 3d1 2P1.5 3844300.0 cm-1
2s1 2p5 3d1 2P0.5 3845030.0 cm-1
2s2 2p4 4d1 2D2.5 3876780.0 cm-1
2s2 2p4 4d1 2D1.5 3877770.0 cm-1
2s2 2p4 4f1 2F2.5 3908060.0 cm-1
2s2 2p4 4f1 2F3.5 3908290.0 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 = 1.4297
         2S = 1.1968
         2P = 1.1382
         3S = 1.1168
         3P = 1.0677
         3D = 1.0949
         4S = 1.1313
         4P = 1.0775
         4D = 1.0959
         4F = 1.0927

 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 0.000050 Z**2 Rydbergs (0.06803 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (1.3606 eV) was used
 from the last threshold up to 1.217551 Z**2 Rydbergs (1656.6 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (1.3606 eV) was used
 from first threshold up to 1.217551 Z**2 Rydbergs (1656.6 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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