blike_lgy12#si9.dat

Resolved Specific Ion Data Collections

Ion
Si9+
Temperature Range
1.723 eV → 1.723 x 104 eV

ADF04

Filename
blike_lgy12#si9.dat
Full Path
adf04/copaw#b/blike_lgy12#si9.dat
Download data
  • Spontaneous Emission: Si+9(i) → Si+9(j) + hv
  • Electron Impact Excitation: Si+9(i) + e → Si+9(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 6990.6 cm-1
2s1 2p2 4P0.5 161010.0 cm-1
2s1 2p2 4P1.5 163490.0 cm-1
2s1 2p2 4P2.5 167060.0 cm-1
2s1 2p2 2D1.5 287850.0 cm-1
2s1 2p2 2D2.5 287880.0 cm-1
2s1 2p2 2S0.5 367670.0 cm-1
2s1 2p2 2P0.5 390040.0 cm-1
2s1 2p2 2P1.5 394030.0 cm-1
2p3 4S1.5 509330.0 cm-1
2p3 2D1.5 575430.0 cm-1
2p3 2D2.5 575450.0 cm-1
2p3 2P0.5 646760.0 cm-1
2p3 2P1.5 647390.0 cm-1
2s2 3s1 2S0.5 1820590.0 cm-1
2s2 3p1 2P0.5 1901580.0 cm-1
2s2 3p1 2P1.5 1903480.0 cm-1
2s2 3d1 2D1.5 1980090.0 cm-1
2s2 3d1 2D2.5 1980640.0 cm-1
2s1 2p1 3s1 4P0.5 1992060.0 cm-1
2s1 2p1 3s1 4P1.5 1994380.0 cm-1
2s1 2p1 3s1 4P2.5 1998510.0 cm-1
2s1 2p1 3s1 2P0.5 2033170.0 cm-1
2s1 2p1 3s1 2P1.5 2037790.0 cm-1
2s1 2p1 3p1 2P0.5 2064170.0 cm-1
2s1 2p1 3p1 2P1.5 2066380.0 cm-1
2s1 2p1 3p1 4D0.5 2068320.0 cm-1
2s1 2p1 3p1 4D1.5 2069290.0 cm-1
2s1 2p1 3p1 4D2.5 2070720.0 cm-1
2s1 2p1 3p1 4D3.5 2074350.0 cm-1
2s1 2p1 3p1 4S1.5 2085370.0 cm-1
2s1 2p1 3p1 4P0.5 2094060.0 cm-1
2s1 2p1 3p1 4P1.5 2096110.0 cm-1
2s1 2p1 3p1 4P2.5 2098270.0 cm-1
2s1 2p1 3p1 2D1.5 2107140.0 cm-1
2s1 2p1 3p1 2D2.5 2111370.0 cm-1
2s1 2p1 3d1 4F1.5 2133760.0 cm-1
2s1 2p1 3p1 2S0.5 2134960.0 cm-1
2s1 2p1 3d1 4F2.5 2135140.0 cm-1
2s1 2p1 3d1 4F3.5 2137140.0 cm-1
2s1 2p1 3d1 4F4.5 2139890.0 cm-1
2s1 2p1 3d1 4D0.5 2154920.0 cm-1
2s1 2p1 3d1 4D1.5 2155120.0 cm-1
2s1 2p1 3d1 4D2.5 2155520.0 cm-1
2s1 2p1 3d1 4D3.5 2157720.0 cm-1
2s1 2p1 3d1 2D1.5 2158700.0 cm-1
2s1 2p1 3d1 2D2.5 2159260.0 cm-1
2s1 2p1 3d1 4P2.5 2163550.0 cm-1
2s1 2p1 3d1 4P1.5 2164350.0 cm-1
2s1 2p1 3d1 4P0.5 2164940.0 cm-1
2s1 2p1 3s1 2P0.5 2165320.0 cm-1
2s1 2p1 3s1 2P1.5 2165500.0 cm-1
2s1 2p1 3d1 2F2.5 2198010.0 cm-1
2s1 2p1 3d1 2F3.5 2202160.0 cm-1
2s1 2p1 3d1 2P1.5 2207200.0 cm-1
2s1 2p1 3d1 2P0.5 2209560.0 cm-1
2s1 2p1 3p1 2P0.5 2244530.0 cm-1
2s1 2p1 3p1 2P1.5 2245650.0 cm-1
2s1 2p1 3p1 2D1.5 2247270.0 cm-1
2s1 2p1 3p1 2D2.5 2247520.0 cm-1
2s1 2p1 3p1 2S0.5 2266410.0 cm-1
2p2 3s1 4P0.5 2286500.0 cm-1
2p2 3s1 4P1.5 2288950.0 cm-1
2p2 3s1 4P2.5 2292830.0 cm-1
2s1 2p1 3d1 2F3.5 2315200.0 cm-1
2s1 2p1 3d1 2F2.5 2315300.0 cm-1
2s1 2p1 3d1 2D1.5 2325960.0 cm-1
2s1 2p1 3d1 2D2.5 2326710.0 cm-1
2p2 3s1 2P0.5 2331380.0 cm-1
2p2 3s1 2P1.5 2335650.0 cm-1
2s1 2p1 3d1 2P0.5 2340470.0 cm-1
2s1 2p1 3d1 2P1.5 2341190.0 cm-1
2p2 3p1 2S0.5 2342940.0 cm-1
2p2 3p1 4D0.5 2353620.0 cm-1
2p2 3p1 4D1.5 2355130.0 cm-1
2p2 3s1 2D2.5 2355920.0 cm-1
2p2 3s1 2D1.5 2356010.0 cm-1
2p2 3p1 4D2.5 2357670.0 cm-1
2p2 3p1 4D3.5 2361190.0 cm-1
2p2 3p1 4P0.5 2365560.0 cm-1
2p2 3p1 4P1.5 2366590.0 cm-1
2p2 3p1 4P2.5 2368770.0 cm-1
2p2 3p1 2D1.5 2377110.0 cm-1
2p2 3p1 2D2.5 2381690.0 cm-1
2p2 3p1 2P1.5 2397830.0 cm-1
2p2 3p1 2P0.5 2398420.0 cm-1
2p2 3p1 4S1.5 2403040.0 cm-1
2p2 3d1 4F1.5 2414750.0 cm-1
2p2 3d1 4F2.5 2416110.0 cm-1
2p2 3d1 4F3.5 2418090.0 cm-1
2p2 3d1 4F4.5 2420740.0 cm-1
2p2 3p1 2F2.5 2424790.0 cm-1
2p2 3p1 2F3.5 2426250.0 cm-1
2p2 3d1 4D1.5 2430350.0 cm-1
2p2 3d1 4D0.5 2430370.0 cm-1
2p2 3d1 4D2.5 2432020.0 cm-1
2p2 3d1 4D3.5 2433040.0 cm-1
2p2 3d1 2P1.5 2433530.0 cm-1
2p2 3d1 2P0.5 2437210.0 cm-1
2p2 3d1 2F2.5 2438430.0 cm-1
2p2 3d1 2F3.5 2443240.0 cm-1
2p2 3d1 4P2.5 2452210.0 cm-1
2p2 3p1 2D2.5 2453760.0 cm-1
2p2 3p1 2D1.5 2453780.0 cm-1
2p2 3d1 4P1.5 2453790.0 cm-1
2p2 3d1 4P0.5 2454640.0 cm-1
2p2 3s1 2S0.5 2466450.0 cm-1
2p2 3p1 2P0.5 2471030.0 cm-1
2p2 3p1 2P1.5 2473910.0 cm-1
2s2 4s1 2S0.5 2481430.0 cm-1
2p2 3d1 2G3.5 2484560.0 cm-1
2p2 3d1 2G4.5 2485140.0 cm-1
2p2 3d1 2D2.5 2487470.0 cm-1
2p2 3d1 2D1.5 2487540.0 cm-1
2p2 3d1 2D1.5 2503910.0 cm-1
2p2 3d1 2D2.5 2505690.0 cm-1
2p2 3d1 2F3.5 2509150.0 cm-1
2p2 3d1 2F2.5 2510690.0 cm-1
2s2 4p1 2P0.5 2513530.0 cm-1
2s2 4p1 2P1.5 2514310.0 cm-1
2p2 3d1 2P0.5 2524410.0 cm-1
2p2 3d1 2P1.5 2526230.0 cm-1
2p2 3d1 2S0.5 2534580.0 cm-1
2s2 4d1 2D1.5 2540690.0 cm-1
2s2 4d1 2D2.5 2540920.0 cm-1
2p2 3p1 2P0.5 2547110.0 cm-1
2p2 3p1 2P1.5 2547880.0 cm-1
2s2 4f1 2F2.5 2556650.0 cm-1
2s2 4f1 2F3.5 2556740.0 cm-1
2p2 3d1 2D2.5 2609560.0 cm-1
2p2 3d1 2D1.5 2610330.0 cm-1
2s1 2p1 4s1 4P0.5 2652160.0 cm-1
2s1 2p1 4s1 4P1.5 2654330.0 cm-1
2s1 2p1 4s1 4P2.5 2658420.0 cm-1
2s1 2p1 4s1 2P0.5 2667690.0 cm-1
2s1 2p1 4s1 2P1.5 2672310.0 cm-1
2s1 2p1 4p1 4D0.5 2681690.0 cm-1
2s1 2p1 4p1 4D1.5 2683100.0 cm-1
2s1 2p1 4p1 4D2.5 2685310.0 cm-1
2s1 2p1 4p1 2P0.5 2687170.0 cm-1
2s1 2p1 4p1 2P1.5 2687480.0 cm-1
2s1 2p1 4p1 4D3.5 2688690.0 cm-1
2s1 2p1 4p1 4S1.5 2690920.0 cm-1
2s1 2p1 4p1 4P0.5 2692140.0 cm-1
2s1 2p1 4p1 4P1.5 2694840.0 cm-1
2s1 2p1 4p1 4P2.5 2695820.0 cm-1
2s1 2p1 4p1 2D1.5 2700220.0 cm-1
2s1 2p1 4p1 2D2.5 2703910.0 cm-1
2s1 2p1 4d1 4F1.5 2706980.0 cm-1
2s1 2p1 4d1 4F2.5 2708160.0 cm-1
2s1 2p1 4d1 4F3.5 2710000.0 cm-1
2s1 2p1 4d1 4F4.5 2712990.0 cm-1
2s1 2p1 4p1 2S0.5 2713340.0 cm-1
2s1 2p1 4d1 4D2.5 2714700.0 cm-1
2s1 2p1 4d1 4D1.5 2715020.0 cm-1
2s1 2p1 4d1 4D0.5 2715180.0 cm-1
2s1 2p1 4d1 2D1.5 2718110.0 cm-1
2s1 2p1 4d1 4D3.5 2718150.0 cm-1
2s1 2p1 4d1 2D2.5 2719030.0 cm-1
2s1 2p1 4d1 4P2.5 2720330.0 cm-1
2s1 2p1 4d1 4P1.5 2720650.0 cm-1
2s1 2p1 4d1 4P0.5 2721030.0 cm-1
2s1 2p1 4f1 4F2.5 2726700.0 cm-1
2s1 2p1 4f1 4F3.5 2726860.0 cm-1
2s1 2p1 4f1 4F1.5 2727910.0 cm-1
2s1 2p1 4f1 4F4.5 2728320.0 cm-1
2s1 2p1 4f1 4G2.5 2728910.0 cm-1
2s1 2p1 4f1 2F3.5 2729660.0 cm-1
2s1 2p1 4f1 2G3.5 2730820.0 cm-1
2s1 2p1 4f1 2F2.5 2731020.0 cm-1
2s1 2p1 4d1 2F2.5 2731900.0 cm-1
2s1 2p1 4f1 4G4.5 2732940.0 cm-1
2s1 2p1 4f1 4G5.5 2733950.0 cm-1
2s1 2p1 4f1 4G3.5 2733950.0 cm-1
2s1 2p1 4f1 4D3.5 2735130.0 cm-1
2s1 2p1 4d1 2P1.5 2735290.0 cm-1
2s1 2p1 4f1 4D2.5 2735410.0 cm-1
2s1 2p1 4d1 2F3.5 2735430.0 cm-1
2s1 2p1 4f1 2G4.5 2735990.0 cm-1
2s1 2p1 4f1 4D1.5 2736360.0 cm-1
2s1 2p1 4f1 4D0.5 2736890.0 cm-1
2s1 2p1 4d1 2P0.5 2737450.0 cm-1
2s1 2p1 4f1 2D2.5 2737950.0 cm-1
2s1 2p1 4f1 2D1.5 2739570.0 cm-1
2s1 2p1 4s1 2P0.5 2822660.0 cm-1
2s1 2p1 4s1 2P1.5 2822800.0 cm-1
2s1 2p1 4p1 2D1.5 2852910.0 cm-1
2s1 2p1 4p1 2D2.5 2853330.0 cm-1
2s1 2p1 4p1 2P0.5 2854760.0 cm-1
2s1 2p1 4p1 2P1.5 2855380.0 cm-1
2s1 2p1 4p1 2S0.5 2861130.0 cm-1
2s1 2p1 4d1 2F3.5 2879940.0 cm-1
2s1 2p1 4d1 2F2.5 2879960.0 cm-1
2s1 2p1 4d1 2D1.5 2881150.0 cm-1
2s1 2p1 4d1 2D2.5 2881430.0 cm-1
2s1 2p1 4d1 2P0.5 2887610.0 cm-1
2s1 2p1 4d1 2P1.5 2887840.0 cm-1
2s1 2p1 4f1 2F2.5 2891930.0 cm-1
2s1 2p1 4f1 2F3.5 2892030.0 cm-1
2s1 2p1 4f1 2G3.5 2896980.0 cm-1
2s1 2p1 4f1 2G4.5 2897080.0 cm-1
2s1 2p1 4f1 2D1.5 2900810.0 cm-1
2s1 2p1 4f1 2D2.5 2900890.0 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 = 1.39126
         2S = 1.24678
         2P = 1.17212
         3S = 1.61234
         3P = 1.35881
         3D = 1.46915
         4S = 1.45299
         4P = 1.35280
         4D = 1.53085
         4F = 1.22926

 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.

 40 continuum basis orbitals were used, giving a smallest maximum
 basis-orbital energy of 339.2886 Rydbergs (4616.360692 eV)

 A fine energy mesh of 0.000010 Z**2 Rydbergs (0.01102086 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (1.102086 eV) was used
 from the last threshold up to 1.092584 Z**2 Rydbergs (1204.122 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (1.102086 eV) was used
 from first threshold up to 1.092584 Z**2 Rydbergs (1204.122 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:
      G Y Liang, N R Badnell and G Zhao
      A&A 547, A87 (2012)
      DOI: 10.1051/0004-6361/201220277

 Produced by: Guiyun Liang
 Date:        29/03/12

 Those data points with same collision strength in OMEGAU at higher energies
 are deleted. The adf04 file is generated based upon this correction.

 Date:  Tue May 28 21:07:12 2013
----------------------------------------------------------------------------

Contributors

  • Guiyun Liang
  • Nigel Badnell
  • Processes
  • States
  • Comments
  • Origins

Data Classes