flike_mcw06#cl8.dat

Resolved Specific Ion Data Collections

Ion
Cl8+
Temperature Range
1.396 eV → 1.396 x 104 eV

ADF04

Filename
flike_mcw06#cl8.dat
Full Path
adf04/copaw#f/flike_mcw06#cl8.dat
Download data
  • Spontaneous Emission: Cl+8(i) → Cl+8(j) + hv
  • Electron Impact Excitation: Cl+8(i) + e → Cl+8(j) + e
2s2 2p5 2P1.5 0.0 cm-1
2s2 2p5 2P0.5 14397.0 cm-1
2s1 2p6 2S0.5 573116.0 cm-1
2s2 2p4 3s1 4P2.5 1877720.0 cm-1
2s2 2p4 3s1 4P1.5 1885440.0 cm-1
2s2 2p4 3s1 4P0.5 1890440.0 cm-1
2s2 2p4 3s1 2P1.5 1902110.0 cm-1
2s2 2p4 3s1 2P0.5 1911330.0 cm-1
2s2 2p4 3s1 2D2.5 1951360.0 cm-1
2s2 2p4 3s1 2D1.5 1951590.0 cm-1
2s2 2p4 3p1 4P2.5 1995140.0 cm-1
2s2 2p4 3p1 4P1.5 1997130.0 cm-1
2s2 2p4 3p1 4P0.5 2001040.0 cm-1
2s2 2p4 3p1 4D3.5 2010490.0 cm-1
2s2 2p4 3p1 4D2.5 2014270.0 cm-1
2s2 2p4 3p1 4D1.5 2018850.0 cm-1
2s2 2p4 3p1 4D0.5 2020820.0 cm-1
2s2 2p4 3p1 2D2.5 2024980.0 cm-1
2s2 2p4 3p1 2P0.5 2025630.0 cm-1
2s2 2p4 3p1 2D1.5 2030000.0 cm-1
2s2 2p4 3p1 2P1.5 2034570.0 cm-1
2s2 2p4 3p1 4S1.5 2036090.0 cm-1
2s2 2p4 3p1 2S0.5 2038150.0 cm-1
2s2 2p4 3s1 2S0.5 2041170.0 cm-1
2s2 2p4 3p1 2F2.5 2073820.0 cm-1
2s2 2p4 3p1 2F3.5 2075820.0 cm-1
2s2 2p4 3p1 2D1.5 2089880.0 cm-1
2s2 2p4 3p1 2D2.5 2091210.0 cm-1
2s2 2p4 3p1 2P1.5 2125550.0 cm-1
2s2 2p4 3p1 2P0.5 2131150.0 cm-1
2s2 2p4 3d1 4D3.5 2162780.0 cm-1
2s2 2p4 3d1 4D2.5 2163540.0 cm-1
2s2 2p4 3d1 4D1.5 2165070.0 cm-1
2s2 2p4 3d1 4D0.5 2166740.0 cm-1
2s2 2p4 3p1 2P1.5 2175740.0 cm-1
2s2 2p4 3p1 2P0.5 2177290.0 cm-1
2s2 2p4 3d1 4F4.5 2177710.0 cm-1
2s2 2p4 3d1 4F3.5 2181900.0 cm-1
2s2 2p4 3d1 4P0.5 2185990.0 cm-1
2s2 2p4 3d1 4F2.5 2186280.0 cm-1
2s2 2p4 3d1 4F1.5 2188530.0 cm-1
2s2 2p4 3d1 4P1.5 2189510.0 cm-1
2s2 2p4 3d1 2F3.5 2190830.0 cm-1
2s2 2p4 3d1 4P2.5 2193240.0 cm-1
2s2 2p4 3d1 2P0.5 2196260.0 cm-1
2s2 2p4 3d1 2F2.5 2197010.0 cm-1
2s2 2p4 3d1 2D1.5 2200650.0 cm-1
2s2 2p4 3d1 2P1.5 2207830.0 cm-1
2s2 2p4 3d1 2D2.5 2208280.0 cm-1
2s2 2p4 3d1 2G3.5 2238770.0 cm-1
2s2 2p4 3d1 2G4.5 2239190.0 cm-1
2s2 2p4 3d1 2S0.5 2252300.0 cm-1
2s2 2p4 3d1 2F2.5 2255050.0 cm-1
2s2 2p4 3d1 2F3.5 2256270.0 cm-1
2s2 2p4 3d1 2P1.5 2260410.0 cm-1
2s2 2p4 3d1 2D2.5 2262480.0 cm-1
2s2 2p4 3d1 2P0.5 2265160.0 cm-1
2s2 2p4 3d1 2D1.5 2266880.0 cm-1
2s2 2p4 3d1 2D2.5 2340670.0 cm-1
2s2 2p4 3d1 2D1.5 2341800.0 cm-1
2s1 2p5 3s1 4P2.5 2381390.0 cm-1
2s1 2p5 3s1 4P1.5 2388800.0 cm-1
2s1 2p5 3s1 4P0.5 2394070.0 cm-1
2s1 2p5 3s1 2P1.5 2417390.0 cm-1
2s1 2p5 3s1 2P0.5 2426160.0 cm-1
2s1 2p5 3p1 4S1.5 2490650.0 cm-1
2s1 2p5 3p1 4D3.5 2508240.0 cm-1
2s1 2p5 3p1 4D2.5 2509040.0 cm-1
2s1 2p5 3p1 4D1.5 2513130.0 cm-1
2s1 2p5 3p1 4P2.5 2514590.0 cm-1
2s1 2p5 3p1 4D0.5 2516890.0 cm-1
2s1 2p5 3p1 4P1.5 2519840.0 cm-1
2s1 2p5 3p1 4P0.5 2521530.0 cm-1
2s1 2p5 3p1 2D2.5 2525860.0 cm-1
2s1 2p5 3p1 2P1.5 2526380.0 cm-1
2s1 2p5 3p1 2P0.5 2532230.0 cm-1
2s1 2p5 3p1 2D1.5 2534100.0 cm-1
2s2 2p4 4s1 4P2.5 2541300.0 cm-1
2s2 2p4 4s1 2P1.5 2541400.0 cm-1
2s2 2p4 4s1 2P0.5 2549770.0 cm-1
2s2 2p4 4s1 4P1.5 2549970.0 cm-1
2s2 2p4 4s1 4P0.5 2552870.0 cm-1
2s2 2p4 4p1 4P2.5 2576450.0 cm-1
2s2 2p4 4p1 4P1.5 2577440.0 cm-1
2s2 2p4 4p1 4D3.5 2578970.0 cm-1
2s1 2p5 3s1 2P0.5 2579280.0 cm-1
2s2 2p4 4p1 2D2.5 2581270.0 cm-1
2s1 2p5 3p1 2S0.5 2582140.0 cm-1
2s1 2p5 3s1 2P1.5 2582330.0 cm-1
2s2 2p4 4p1 4P0.5 2584900.0 cm-1
2s2 2p4 4p1 4D1.5 2587930.0 cm-1
2s2 2p4 4p1 4D2.5 2589940.0 cm-1
2s2 2p4 4p1 4D0.5 2590780.0 cm-1
2s2 2p4 4p1 2S0.5 2592240.0 cm-1
2s2 2p4 4p1 4S1.5 2593570.0 cm-1
2s2 2p4 4p1 2D1.5 2594290.0 cm-1
2s2 2p4 4s1 2D2.5 2596760.0 cm-1
2s2 2p4 4s1 2D1.5 2596930.0 cm-1
2s2 2p4 4p1 2P1.5 2610030.0 cm-1
2s2 2p4 4p1 2P0.5 2612040.0 cm-1
2s2 2p4 4d1 4D3.5 2635840.0 cm-1
2s2 2p4 4d1 4D2.5 2636360.0 cm-1
2s2 2p4 4d1 4D1.5 2637630.0 cm-1
2s2 2p4 4d1 4D0.5 2639400.0 cm-1
2s2 2p4 4d1 4F4.5 2639580.0 cm-1
2s2 2p4 4d1 2F3.5 2642060.0 cm-1
2s2 2p4 4d1 4P0.5 2644440.0 cm-1
2s2 2p4 4p1 2F2.5 2644500.0 cm-1
2s2 2p4 4p1 2F3.5 2645240.0 cm-1
2s2 2p4 4d1 4F2.5 2646770.0 cm-1
2s2 2p4 4f1 4F4.5 2647010.0 cm-1
2s2 2p4 4d1 4P1.5 2647040.0 cm-1
2s2 2p4 4f1 4F3.5 2648320.0 cm-1
2s2 2p4 4f1 4F2.5 2649790.0 cm-1
2s2 2p4 4d1 4F3.5 2650010.0 cm-1
2s2 2p4 4p1 2D1.5 2650070.0 cm-1
2s2 2p4 4p1 2D2.5 2650550.0 cm-1
2s2 2p4 4d1 4F1.5 2651560.0 cm-1
2s2 2p4 4f1 4F1.5 2651700.0 cm-1
2s2 2p4 4d1 4P2.5 2652120.0 cm-1
2s2 2p4 4d1 2P0.5 2653350.0 cm-1
2s2 2p4 4d1 2F2.5 2653430.0 cm-1
2s2 2p4 4d1 2P1.5 2655890.0 cm-1
2s2 2p4 4f1 2F3.5 2656200.0 cm-1
2s2 2p4 4f1 2F2.5 2657090.0 cm-1
2s2 2p4 4f1 4D0.5 2657150.0 cm-1
2s2 2p4 4f1 4D1.5 2658100.0 cm-1
2s2 2p4 4p1 2P1.5 2658640.0 cm-1
2s1 2p5 3d1 4P0.5 2659860.0 cm-1
2s2 2p4 4d1 2D2.5 2661680.0 cm-1
2s2 2p4 4p1 2P0.5 2662150.0 cm-1
2s1 2p5 3d1 4P1.5 2662340.0 cm-1
2s2 2p4 4f1 4D2.5 2662880.0 cm-1
2s2 2p4 4f1 4G5.5 2663350.0 cm-1
2s2 2p4 4f1 2G4.5 2663460.0 cm-1
2s2 2p4 4d1 2D1.5 2663770.0 cm-1
2s2 2p4 4f1 2D1.5 2664580.0 cm-1
2s2 2p4 4f1 4D3.5 2665590.0 cm-1
2s1 2p5 3d1 4P2.5 2666820.0 cm-1
2s2 2p4 4f1 4G4.5 2669710.0 cm-1
2s2 2p4 4f1 2D2.5 2669950.0 cm-1
2s2 2p4 4f1 4G3.5 2670810.0 cm-1
2s2 2p4 4f1 4G2.5 2674680.0 cm-1
2s2 2p4 4f1 2G3.5 2674830.0 cm-1
2s1 2p5 3d1 4F4.5 2684170.0 cm-1
2s2 2p4 4s1 2S0.5 2684490.0 cm-1
2s1 2p5 3d1 4F3.5 2685070.0 cm-1
2s1 2p5 3d1 4F2.5 2686830.0 cm-1
2s1 2p5 3d1 4F1.5 2689130.0 cm-1
2s1 2p5 3d1 2F3.5 2693460.0 cm-1
2s1 2p5 3d1 4D0.5 2696290.0 cm-1
2s1 2p5 3d1 4D2.5 2697360.0 cm-1
2s1 2p5 3d1 4D1.5 2697840.0 cm-1
2s1 2p5 3d1 4D3.5 2699500.0 cm-1
2s1 2p5 3d1 2F2.5 2700260.0 cm-1
2s2 2p4 4d1 2G3.5 2704260.0 cm-1
2s2 2p4 4d1 2G4.5 2704440.0 cm-1
2s1 2p5 3d1 2D1.5 2705050.0 cm-1
2s1 2p5 3d1 2D2.5 2707190.0 cm-1
2s2 2p4 4d1 2P1.5 2708650.0 cm-1
2s2 2p4 4d1 2D2.5 2709290.0 cm-1
2s1 2p5 3p1 2D1.5 2709710.0 cm-1
2s2 2p4 4d1 2P0.5 2709980.0 cm-1
2s2 2p4 4d1 2F3.5 2710300.0 cm-1
2s2 2p4 4d1 2F2.5 2710390.0 cm-1
2s2 2p4 4d1 2S0.5 2712010.0 cm-1
2s2 2p4 4d1 2D1.5 2716690.0 cm-1
2s1 2p5 3p1 2D2.5 2716840.0 cm-1
2s1 2p5 3d1 2P0.5 2718690.0 cm-1
2s2 2p4 4f1 2P1.5 2722390.0 cm-1
2s2 2p4 4f1 2P0.5 2723000.0 cm-1
2s1 2p5 3p1 2P0.5 2723980.0 cm-1
2s1 2p5 3p1 2P1.5 2724240.0 cm-1
2s1 2p5 3d1 2P1.5 2725300.0 cm-1
2s2 2p4 4f1 2D2.5 2726550.0 cm-1
2s2 2p4 4f1 2D1.5 2727160.0 cm-1
2s2 2p4 4f1 2H4.5 2727810.0 cm-1
2s2 2p4 4f1 2H5.5 2727890.0 cm-1
2s2 2p4 4f1 2F2.5 2729520.0 cm-1
2s2 2p4 4f1 2F3.5 2729540.0 cm-1
2s2 2p4 4f1 2G3.5 2731090.0 cm-1
2s2 2p4 4f1 2G4.5 2731170.0 cm-1
2s2 2p4 4p1 2P0.5 2739320.0 cm-1
2s2 2p4 4p1 2P1.5 2739410.0 cm-1
2s1 2p5 3p1 2S0.5 2746370.0 cm-1
2s2 2p4 4d1 2D2.5 2798960.0 cm-1
2s2 2p4 4d1 2D1.5 2799470.0 cm-1
2s2 2p4 4f1 2F2.5 2817720.0 cm-1
2s2 2p4 4f1 2F3.5 2817750.0 cm-1
2s1 2p5 3d1 2F2.5 2875820.0 cm-1
2s1 2p5 3d1 2F3.5 2876180.0 cm-1
2s1 2p5 3d1 2P1.5 2884630.0 cm-1
2s1 2p5 3d1 2P0.5 2885240.0 cm-1
2s1 2p5 3d1 2D1.5 2886390.0 cm-1
2s1 2p5 3d1 2D2.5 2886610.0 cm-1
L+ 8        17         9       3186697.(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 = 1.4365
         2S = 1.1917
         2P = 1.1351
         3S = 1.1098
         3P = 1.0614
         3D = 1.0845
         4S = 1.1236
         4P = 1.0701
         4D = 1.0849
         4F = 1.0774

 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 (0.0435392 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.870784 eV) was used
 from the last threshold up to 1.361187 Z**2 Rydbergs (1185.3 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (0.870784 eV) was used
 from first threshold up to 1.361187 Z**2 Rydbergs (1185.3 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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