Resolved Specific Ion Data Collections

Temperature Range
2.482 eV → 2.482 x 104 eV


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  • Spontaneous Emission: S+11(i) → S+11(j) + hv
  • Electron Impact Excitation: S+11(i) + e → S+11(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 13135.0 cm-1
2s1 2p2 4P0.5 193882.0 cm-1
2s1 2p2 4P1.5 198675.0 cm-1
2s1 2p2 4P2.5 205425.0 cm-1
2s1 2p2 2D1.5 346704.0 cm-1
2s1 2p2 2D2.5 347005.0 cm-1
2s1 2p2 2S0.5 439575.0 cm-1
2s1 2p2 2P0.5 464755.0 cm-1
2s1 2p2 2P1.5 471431.0 cm-1
2p3 4S1.5 610075.0 cm-1
2p3 2D1.5 689907.0 cm-1
2p3 2D2.5 690478.0 cm-1
2p3 2P0.5 774021.0 cm-1
2p3 2P1.5 775805.0 cm-1
2s2 3s1 2S0.5 2556600.0 cm-1
2s2 3p1 2P0.5 2653720.0 cm-1
2s2 3p1 2P1.5 2657320.0 cm-1
2s2 3d1 2D1.5 2749200.0 cm-1
2s2 3d1 2D2.5 2750280.0 cm-1
2s1 2p1 3s1 4P0.5 2758140.0 cm-1
2s1 2p1 3s1 4P1.5 2762390.0 cm-1
2s1 2p1 3s1 4P2.5 2770240.0 cm-1
2s1 2p1 3s1 2P0.5 2807590.0 cm-1
2s1 2p1 3s1 2P1.5 2816330.0 cm-1
2s1 2p1 3p1 4D0.5 2845030.0 cm-1
2s1 2p1 3p1 4D1.5 2848960.0 cm-1
2s1 2p1 3p1 2P0.5 2852620.0 cm-1
2s1 2p1 3p1 2P1.5 2854280.0 cm-1
2s1 2p1 3p1 4D2.5 2855640.0 cm-1
2s1 2p1 3p1 4D3.5 2862590.0 cm-1
2s1 2p1 3p1 4S1.5 2873410.0 cm-1
2s1 2p1 3p1 4P0.5 2882280.0 cm-1
2s1 2p1 3p1 4P1.5 2886580.0 cm-1
2s1 2p1 3p1 4P2.5 2890210.0 cm-1
2s1 2p1 3p1 2D1.5 2898210.0 cm-1
2s1 2p1 3p1 2D2.5 2906190.0 cm-1
2s1 2p1 3d1 4F1.5 2928900.0 cm-1
2s1 2p1 3d1 4F2.5 2931460.0 cm-1
2s1 2p1 3p1 2S0.5 2933210.0 cm-1
2s1 2p1 3d1 4F3.5 2935250.0 cm-1
2s1 2p1 3d1 4F4.5 2940630.0 cm-1
2s1 2p1 3d1 4D0.5 2956270.0 cm-1
2s1 2p1 3d1 4D1.5 2956400.0 cm-1
2s1 2p1 3d1 4D2.5 2956510.0 cm-1
2s1 2p1 3d1 2D1.5 2961190.0 cm-1
2s1 2p1 3d1 4D3.5 2961890.0 cm-1
2s1 2p1 3s1 2P0.5 2962520.0 cm-1
2s1 2p1 3d1 2D2.5 2962700.0 cm-1
2s1 2p1 3s1 2P1.5 2963140.0 cm-1
2s1 2p1 3d1 4P2.5 2968700.0 cm-1
2s1 2p1 3d1 4P1.5 2969730.0 cm-1
2s1 2p1 3d1 4P0.5 2970620.0 cm-1
2s1 2p1 3d1 2F2.5 3008830.0 cm-1
2s1 2p1 3d1 2F3.5 3016640.0 cm-1
2s1 2p1 3d1 2P1.5 3020670.0 cm-1
2s1 2p1 3d1 2P0.5 3025120.0 cm-1
2s1 2p1 3p1 2P0.5 3057620.0 cm-1
2s1 2p1 3p1 2P1.5 3059470.0 cm-1
2s1 2p1 3p1 2D1.5 3062110.0 cm-1
2s1 2p1 3p1 2D2.5 3062290.0 cm-1
2s1 2p1 3p1 2S0.5 3085810.0 cm-1
2p2 3s1 4P0.5 3106510.0 cm-1
2p2 3s1 4P1.5 3111160.0 cm-1
2p2 3s1 4P2.5 3118300.0 cm-1
2s1 2p1 3d1 2F3.5 3144650.0 cm-1
2s1 2p1 3d1 2F2.5 3144900.0 cm-1
2s1 2p1 3d1 2D1.5 3156390.0 cm-1
2s1 2p1 3d1 2D2.5 3157840.0 cm-1
2p2 3s1 2P0.5 3160570.0 cm-1
2p2 3s1 2P1.5 3168160.0 cm-1
2s1 2p1 3d1 2P0.5 3173760.0 cm-1
2s1 2p1 3d1 2P1.5 3175210.0 cm-1
2p2 3p1 2S0.5 3177390.0 cm-1
2p2 3p1 4D0.5 3187410.0 cm-1
2p2 3p1 4D1.5 3190240.0 cm-1
2p2 3s1 2D2.5 3191910.0 cm-1
2p2 3s1 2D1.5 3192420.0 cm-1
2p2 3p1 4D2.5 3195070.0 cm-1
2p2 3p1 4D3.5 3201670.0 cm-1
2p2 3p1 4P0.5 3203900.0 cm-1
2p2 3p1 4P1.5 3205250.0 cm-1
2p2 3p1 4P2.5 3209090.0 cm-1
2p2 3p1 2D1.5 3217160.0 cm-1
2p2 3p1 2D2.5 3226050.0 cm-1
2p2 3p1 2P1.5 3243460.0 cm-1
2p2 3p1 2P0.5 3244920.0 cm-1
2p2 3p1 4S1.5 3248710.0 cm-1
2p2 3d1 4F1.5 3262160.0 cm-1
2p2 3d1 4F2.5 3264740.0 cm-1
2p2 3d1 4F3.5 3268500.0 cm-1
2p2 3d1 4F4.5 3273570.0 cm-1
2p2 3p1 2F2.5 3274690.0 cm-1
2p2 3p1 2F3.5 3277420.0 cm-1
2p2 3d1 4D1.5 3281510.0 cm-1
2p2 3d1 4D0.5 3281930.0 cm-1
2p2 3d1 4D2.5 3284660.0 cm-1
2p2 3d1 4D3.5 3286740.0 cm-1
2p2 3d1 2P1.5 3287260.0 cm-1
2p2 3d1 2F2.5 3292130.0 cm-1
2p2 3d1 2P0.5 3294010.0 cm-1
2p2 3d1 2F3.5 3301270.0 cm-1
2p2 3p1 2D1.5 3308940.0 cm-1
2p2 3p1 2D2.5 3309260.0 cm-1
2p2 3d1 4P2.5 3309670.0 cm-1
2p2 3d1 4P1.5 3312520.0 cm-1
2p2 3d1 4P0.5 3313930.0 cm-1
2p2 3s1 2S0.5 3321220.0 cm-1
2p2 3p1 2P0.5 3329280.0 cm-1
2p2 3p1 2P1.5 3335130.0 cm-1
2p2 3d1 2G3.5 3347980.0 cm-1
2p2 3d1 2G4.5 3349220.0 cm-1
2p2 3d1 2D2.5 3352660.0 cm-1
2p2 3d1 2D1.5 3353120.0 cm-1
2p2 3d1 2D1.5 3370880.0 cm-1
2p2 3d1 2D2.5 3374190.0 cm-1
2p2 3d1 2F3.5 3379920.0 cm-1
2p2 3d1 2F2.5 3383180.0 cm-1
2p2 3d1 2P0.5 3395510.0 cm-1
2p2 3d1 2P1.5 3399120.0 cm-1
2p2 3d1 2S0.5 3407610.0 cm-1
2p2 3p1 2P0.5 3418000.0 cm-1
2p2 3p1 2P1.5 3419490.0 cm-1
2s2 4s1 2S0.5 3478360.0 cm-1
2p2 3d1 2D2.5 3495420.0 cm-1
2p2 3d1 2D1.5 3496940.0 cm-1
2s2 4p1 2P0.5 3517440.0 cm-1
2s2 4p1 2P1.5 3518920.0 cm-1
2s2 4d1 2D1.5 3551420.0 cm-1
2s2 4d1 2D2.5 3551850.0 cm-1
2s2 4f1 2F2.5 3570590.0 cm-1
2s2 4f1 2F3.5 3570780.0 cm-1
2s1 2p1 4s1 4P0.5 3679200.0 cm-1
2s1 2p1 4s1 4P1.5 3683160.0 cm-1
2s1 2p1 4s1 4P2.5 3691060.0 cm-1
2s1 2p1 4s1 2P0.5 3697720.0 cm-1
2s1 2p1 4s1 2P1.5 3706570.0 cm-1
2s1 2p1 4p1 4D0.5 3714840.0 cm-1
2s1 2p1 4p1 4D1.5 3717540.0 cm-1
2s1 2p1 4p1 4D2.5 3721590.0 cm-1
2s1 2p1 4p1 2P1.5 3722910.0 cm-1
2s1 2p1 4p1 2P0.5 3723300.0 cm-1
2s1 2p1 4p1 4D3.5 3728290.0 cm-1
2s1 2p1 4p1 4P0.5 3728780.0 cm-1
2s1 2p1 4p1 4S1.5 3729260.0 cm-1
2s1 2p1 4p1 4P1.5 3734800.0 cm-1
2s1 2p1 4p1 4P2.5 3735950.0 cm-1
2s1 2p1 4p1 2D1.5 3738940.0 cm-1
2s1 2p1 4p1 2D2.5 3745500.0 cm-1
2s1 2p1 4d1 4F1.5 3746230.0 cm-1
2s1 2p1 4d1 4F2.5 3748320.0 cm-1
2s1 2p1 4d1 4F3.5 3751710.0 cm-1
2s1 2p1 4p1 2S0.5 3755810.0 cm-1
2s1 2p1 4d1 4D2.5 3756070.0 cm-1
2s1 2p1 4d1 4D1.5 3757020.0 cm-1
2s1 2p1 4d1 4D0.5 3757460.0 cm-1
2s1 2p1 4d1 4F4.5 3757800.0 cm-1
2s1 2p1 4d1 2D1.5 3761450.0 cm-1
2s1 2p1 4d1 4D3.5 3763640.0 cm-1
2s1 2p1 4d1 2D2.5 3763750.0 cm-1
2s1 2p1 4d1 4P2.5 3766110.0 cm-1
2s1 2p1 4d1 4P1.5 3766850.0 cm-1
2s1 2p1 4d1 4P0.5 3767370.0 cm-1
2s1 2p1 4f1 4G2.5 3770120.0 cm-1
2s1 2p1 4f1 4F3.5 3770450.0 cm-1
2s1 2p1 4f1 4F1.5 3772900.0 cm-1
2s1 2p1 4f1 4F4.5 3773520.0 cm-1
2s1 2p1 4f1 4F2.5 3773940.0 cm-1
2s1 2p1 4f1 2F3.5 3774660.0 cm-1
2s1 2p1 4f1 2F2.5 3776860.0 cm-1
2s1 2p1 4f1 2G3.5 3776890.0 cm-1
2s1 2p1 4d1 2F2.5 3778050.0 cm-1
2s1 2p1 4f1 4G4.5 3782060.0 cm-1
2s1 2p1 4f1 4G3.5 3782850.0 cm-1
2s1 2p1 4d1 2P1.5 3782940.0 cm-1
2s1 2p1 4f1 4G5.5 3783600.0 cm-1
2s1 2p1 4d1 2F3.5 3784340.0 cm-1
2s1 2p1 4f1 4D3.5 3784470.0 cm-1
2s1 2p1 4f1 4D2.5 3784500.0 cm-1
2s1 2p1 4f1 4D1.5 3786020.0 cm-1
2s1 2p1 4f1 2G4.5 3786180.0 cm-1
2s1 2p1 4d1 2P0.5 3786700.0 cm-1
2s1 2p1 4f1 4D0.5 3786890.0 cm-1
2s1 2p1 4f1 2D2.5 3787480.0 cm-1
2s1 2p1 4f1 2D1.5 3789850.0 cm-1
2s1 2p1 4s1 2P0.5 3880050.0 cm-1
2s1 2p1 4s1 2P1.5 3880290.0 cm-1
2s1 2p1 4p1 2D1.5 3916980.0 cm-1
2s1 2p1 4p1 2D2.5 3917830.0 cm-1
2s1 2p1 4p1 2P0.5 3918960.0 cm-1
2s1 2p1 4p1 2P1.5 3920180.0 cm-1
2s1 2p1 4p1 2S0.5 3926910.0 cm-1
2s1 2p1 4d1 2F3.5 3950310.0 cm-1
2s1 2p1 4d1 2F2.5 3950340.0 cm-1
2s1 2p1 4d1 2D1.5 3951510.0 cm-1
2s1 2p1 4d1 2D2.5 3952060.0 cm-1
2s1 2p1 4d1 2P0.5 3959260.0 cm-1
2s1 2p1 4d1 2P1.5 3959720.0 cm-1
2s1 2p1 4f1 2F2.5 3965010.0 cm-1
2s1 2p1 4f1 2F3.5 3965210.0 cm-1
2s1 2p1 4f1 2G3.5 3970970.0 cm-1
2s1 2p1 4f1 2G4.5 3971160.0 cm-1
2s1 2p1 4f1 2D1.5 3975160.0 cm-1
2s1 2p1 4f1 2D2.5 3975320.0 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

     Calculation details

 The following scaling parameters on bound orbitals were used:

         1S = 1.38787
         2S = 1.24802
         2P = 1.17263
         3S = 1.60433
         3P = 1.36255
         3D = 1.47452
         4S = 1.47343
         4P = 1.36462
         4D = 1.53091
         4F = 1.39692

 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 479.8587 Rydbergs (6528.957472 eV)

 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 1.049974 Z**2 Rydbergs (1728.6 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 1.049974 Z**2 Rydbergs (1728.6 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

      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:        29/05/11


  • Guiyun Liang
  • Nigel Badnell
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