Resolved Specific Ion Data Collections

Temperature Range
2.085 eV → 2.085 x 104 eV


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  • Spontaneous Emission: P+10(i) → P+10(j) + hv
  • Electron Impact Excitation: P+10(i) + e → P+10(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 9698.6 cm-1
2s1 2p2 4P0.5 177177.0 cm-1
2s1 2p2 4P1.5 180671.0 cm-1
2s1 2p2 4P2.5 185631.0 cm-1
2s1 2p2 2D1.5 316807.0 cm-1
2s1 2p2 2D2.5 316905.0 cm-1
2s1 2p2 2S0.5 403322.0 cm-1
2s1 2p2 2P0.5 426877.0 cm-1
2s1 2p2 2P1.5 432160.0 cm-1
2p3 4S1.5 558973.0 cm-1
2p3 2D1.5 631961.0 cm-1
2p3 2D2.5 632164.0 cm-1
2p3 2P0.5 709666.0 cm-1
2p3 2P1.5 710749.0 cm-1
2s2 3s1 2S0.5 2173040.0 cm-1
2s2 3p1 2P0.5 2262080.0 cm-1
2s2 3p1 2P1.5 2264740.0 cm-1
2s2 3d1 2D1.5 2348980.0 cm-1
2s2 3d1 2D2.5 2349760.0 cm-1
2s1 2p1 3s1 4P0.5 2359500.0 cm-1
2s1 2p1 3s1 4P1.5 2362690.0 cm-1
2s1 2p1 3s1 4P2.5 2368450.0 cm-1
2s1 2p1 3s1 2P0.5 2404750.0 cm-1
2s1 2p1 3s1 2P1.5 2411180.0 cm-1
2s1 2p1 3p1 2P0.5 2439030.0 cm-1
2s1 2p1 3p1 4D1.5 2442020.0 cm-1
2s1 2p1 3p1 4D0.5 2444600.0 cm-1
2s1 2p1 3p1 2P1.5 2445880.0 cm-1
2s1 2p1 3p1 4D2.5 2447350.0 cm-1
2s1 2p1 3p1 4D3.5 2452430.0 cm-1
2s1 2p1 3p1 4S1.5 2463530.0 cm-1
2s1 2p1 3p1 4P0.5 2472460.0 cm-1
2s1 2p1 3p1 4P1.5 2475450.0 cm-1
2s1 2p1 3p1 4P2.5 2478300.0 cm-1
2s1 2p1 3p1 2D1.5 2486890.0 cm-1
2s1 2p1 3p1 2D2.5 2492780.0 cm-1
2s1 2p1 3d1 4F1.5 2515600.0 cm-1
2s1 2p1 3d1 4F2.5 2517500.0 cm-1
2s1 2p1 3p1 2S0.5 2518170.0 cm-1
2s1 2p1 3d1 4F3.5 2520290.0 cm-1
2s1 2p1 3d1 4F4.5 2524180.0 cm-1
2s1 2p1 3d1 4D0.5 2539770.0 cm-1
2s1 2p1 3d1 4D1.5 2539950.0 cm-1
2s1 2p1 3d1 4D2.5 2540270.0 cm-1
2s1 2p1 3d1 4D3.5 2543780.0 cm-1
2s1 2p1 3d1 2D1.5 2544100.0 cm-1
2s1 2p1 3d1 2D2.5 2544980.0 cm-1
2s1 2p1 3s1 2P0.5 2548080.0 cm-1
2s1 2p1 3s1 2P1.5 2548400.0 cm-1
2s1 2p1 3d1 4P2.5 2550070.0 cm-1
2s1 2p1 3d1 4P1.5 2551010.0 cm-1
2s1 2p1 3d1 4P0.5 2551750.0 cm-1
2s1 2p1 3d1 2F2.5 2587600.0 cm-1
2s1 2p1 3d1 2F3.5 2593360.0 cm-1
2s1 2p1 3d1 2P1.5 2598020.0 cm-1
2s1 2p1 3d1 2P0.5 2601310.0 cm-1
2s1 2p1 3p1 2P0.5 2635220.0 cm-1
2s1 2p1 3p1 2P1.5 2636690.0 cm-1
2s1 2p1 3p1 2D1.5 2638750.0 cm-1
2s1 2p1 3p1 2D2.5 2639000.0 cm-1
2s1 2p1 3p1 2S0.5 2660270.0 cm-1
2p2 3s1 4P0.5 2680650.0 cm-1
2p2 3s1 4P1.5 2684070.0 cm-1
2p2 3s1 4P2.5 2689400.0 cm-1
2s1 2p1 3d1 2F3.5 2714000.0 cm-1
2s1 2p1 3d1 2F2.5 2714160.0 cm-1
2s1 2p1 3d1 2D1.5 2725250.0 cm-1
2s1 2p1 3d1 2D2.5 2726310.0 cm-1
2p2 3s1 2P0.5 2730120.0 cm-1
2p2 3s1 2P1.5 2735900.0 cm-1
2s1 2p1 3d1 2P0.5 2741240.0 cm-1
2s1 2p1 3d1 2P1.5 2742270.0 cm-1
2p2 3p1 2S0.5 2744120.0 cm-1
2p2 3p1 4D0.5 2754620.0 cm-1
2p2 3p1 4D1.5 2756720.0 cm-1
2p2 3s1 2D2.5 2757810.0 cm-1
2p2 3s1 2D1.5 2758050.0 cm-1
2p2 3p1 4D2.5 2760260.0 cm-1
2p2 3p1 4D3.5 2765150.0 cm-1
2p2 3p1 4P0.5 2768650.0 cm-1
2p2 3p1 4P1.5 2769880.0 cm-1
2p2 3p1 4P2.5 2772810.0 cm-1
2p2 3p1 2D1.5 2781070.0 cm-1
2p2 3p1 2D2.5 2787530.0 cm-1
2p2 3p1 2P1.5 2804500.0 cm-1
2p2 3p1 2P0.5 2805440.0 cm-1
2p2 3p1 4S1.5 2809710.0 cm-1
2p2 3d1 4F1.5 2822470.0 cm-1
2p2 3d1 4F2.5 2824370.0 cm-1
2p2 3d1 4F3.5 2827130.0 cm-1
2p2 3d1 4F4.5 2830840.0 cm-1
2p2 3p1 2F2.5 2833600.0 cm-1
2p2 3p1 2F3.5 2835620.0 cm-1
2p2 3d1 4D1.5 2839880.0 cm-1
2p2 3d1 4D0.5 2840060.0 cm-1
2p2 3d1 4D2.5 2842250.0 cm-1
2p2 3d1 4D3.5 2843700.0 cm-1
2p2 3d1 2P1.5 2844190.0 cm-1
2p2 3d1 2F2.5 2849130.0 cm-1
2p2 3d1 2P0.5 2849220.0 cm-1
2p2 3d1 2F3.5 2855850.0 cm-1
2p2 3d1 4P2.5 2864740.0 cm-1
2p2 3p1 2D1.5 2865240.0 cm-1
2p2 3p1 2D2.5 2865330.0 cm-1
2p2 3d1 4P1.5 2866900.0 cm-1
2p2 3d1 4P0.5 2868010.0 cm-1
2p2 3s1 2S0.5 2877740.0 cm-1
2p2 3p1 2P0.5 2884130.0 cm-1
2p2 3p1 2P1.5 2888290.0 cm-1
2p2 3d1 2G3.5 2900040.0 cm-1
2p2 3d1 2G4.5 2900900.0 cm-1
2p2 3d1 2D2.5 2903930.0 cm-1
2p2 3d1 2D1.5 2904160.0 cm-1
2p2 3d1 2D1.5 2921220.0 cm-1
2p2 3d1 2D2.5 2923730.0 cm-1
2p2 3d1 2F3.5 2928300.0 cm-1
2p2 3d1 2F2.5 2930560.0 cm-1
2p2 3d1 2P0.5 2943790.0 cm-1
2p2 3d1 2P1.5 2946380.0 cm-1
2p2 3d1 2S0.5 2954830.0 cm-1
2s2 4s1 2S0.5 2958870.0 cm-1
2p2 3p1 2P0.5 2966410.0 cm-1
2p2 3p1 2P1.5 2967490.0 cm-1
2s2 4p1 2P0.5 2994440.0 cm-1
2s2 4p1 2P1.5 2995530.0 cm-1
2s2 4d1 2D1.5 3024820.0 cm-1
2s2 4d1 2D2.5 3025120.0 cm-1
2p2 3d1 2D2.5 3036500.0 cm-1
2p2 3d1 2D1.5 3037590.0 cm-1
2s2 4f1 2F2.5 3042520.0 cm-1
2s2 4f1 2F3.5 3042650.0 cm-1
2s1 2p1 4s1 4P0.5 3144640.0 cm-1
2s1 2p1 4s1 4P1.5 3147620.0 cm-1
2s1 2p1 4s1 4P2.5 3153370.0 cm-1
2s1 2p1 4s1 2P0.5 3161580.0 cm-1
2s1 2p1 4s1 2P1.5 3168060.0 cm-1
2s1 2p1 4p1 4D0.5 3177240.0 cm-1
2s1 2p1 4p1 4D1.5 3179220.0 cm-1
2s1 2p1 4p1 4D2.5 3182250.0 cm-1
2s1 2p1 4p1 2P0.5 3184010.0 cm-1
2s1 2p1 4p1 2P1.5 3184090.0 cm-1
2s1 2p1 4p1 4D3.5 3187070.0 cm-1
2s1 2p1 4p1 4S1.5 3188830.0 cm-1
2s1 2p1 4p1 4P0.5 3189310.0 cm-1
2s1 2p1 4p1 4P1.5 3193430.0 cm-1
2s1 2p1 4p1 4P2.5 3194510.0 cm-1
2s1 2p1 4p1 2D1.5 3198260.0 cm-1
2s1 2p1 4p1 2D2.5 3203290.0 cm-1
2s1 2p1 4d1 4F1.5 3205560.0 cm-1
2s1 2p1 4d1 4F2.5 3207150.0 cm-1
2s1 2p1 4d1 4F3.5 3209680.0 cm-1
2s1 2p1 4p1 2S0.5 3213200.0 cm-1
2s1 2p1 4d1 4F4.5 3214010.0 cm-1
2s1 2p1 4d1 4D2.5 3214260.0 cm-1
2s1 2p1 4d1 4D1.5 3214860.0 cm-1
2s1 2p1 4d1 4D0.5 3215130.0 cm-1
2s1 2p1 4d1 2D1.5 3218540.0 cm-1
2s1 2p1 4d1 4D3.5 3219480.0 cm-1
2s1 2p1 4d1 2D2.5 3220090.0 cm-1
2s1 2p1 4d1 4P2.5 3221800.0 cm-1
2s1 2p1 4d1 4P1.5 3222340.0 cm-1
2s1 2p1 4d1 4P0.5 3222790.0 cm-1
2s1 2p1 4f1 4G2.5 3227320.0 cm-1
2s1 2p1 4f1 4F3.5 3227560.0 cm-1
2s1 2p1 4f1 4F1.5 3229200.0 cm-1
2s1 2p1 4f1 4F4.5 3229720.0 cm-1
2s1 2p1 4f1 4F2.5 3230220.0 cm-1
2s1 2p1 4f1 2F3.5 3230960.0 cm-1
2s1 2p1 4f1 2G3.5 3232660.0 cm-1
2s1 2p1 4f1 2F2.5 3232720.0 cm-1
2s1 2p1 4d1 2F2.5 3233610.0 cm-1
2s1 2p1 4f1 4G4.5 3236060.0 cm-1
2s1 2p1 4f1 4G3.5 3236960.0 cm-1
2s1 2p1 4f1 4G5.5 3237330.0 cm-1
2s1 2p1 4d1 2P1.5 3237680.0 cm-1
2s1 2p1 4f1 4D3.5 3238340.0 cm-1
2s1 2p1 4d1 2F3.5 3238400.0 cm-1
2s1 2p1 4f1 4D2.5 3238520.0 cm-1
2s1 2p1 4f1 2G4.5 3239650.0 cm-1
2s1 2p1 4f1 4D1.5 3239750.0 cm-1
2s1 2p1 4f1 4D0.5 3240450.0 cm-1
2s1 2p1 4d1 2P0.5 3240570.0 cm-1
2s1 2p1 4f1 2D2.5 3241240.0 cm-1
2s1 2p1 4f1 2D1.5 3243230.0 cm-1
2s1 2p1 4s1 2P0.5 3330100.0 cm-1
2s1 2p1 4s1 2P1.5 3330280.0 cm-1
2s1 2p1 4p1 2D1.5 3363680.0 cm-1
2s1 2p1 4p1 2D2.5 3364280.0 cm-1
2s1 2p1 4p1 2P0.5 3365590.0 cm-1
2s1 2p1 4p1 2P1.5 3366470.0 cm-1
2s1 2p1 4p1 2S0.5 3372720.0 cm-1
2s1 2p1 4d1 2F3.5 3393820.0 cm-1
2s1 2p1 4d1 2F2.5 3393840.0 cm-1
2s1 2p1 4d1 2D1.5 3395020.0 cm-1
2s1 2p1 4d1 2D2.5 3395420.0 cm-1
2s1 2p1 4d1 2P0.5 3402110.0 cm-1
2s1 2p1 4d1 2P1.5 3402440.0 cm-1
2s1 2p1 4f1 2F2.5 3407160.0 cm-1
2s1 2p1 4f1 2F3.5 3407300.0 cm-1
2s1 2p1 4f1 2G3.5 3412660.0 cm-1
2s1 2p1 4f1 2G4.5 3412800.0 cm-1
2s1 2p1 4f1 2D1.5 3416650.0 cm-1
2s1 2p1 4f1 2D2.5 3416760.0 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 = 1.38951
         2S = 1.24743
         2P = 1.17236
         3S = 1.60821
         3P = 1.36083
         3D = 1.47206
         4S = 1.46557
         4P = 1.35802
         4D = 1.51540
         4F = 1.33250

 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 409.4653 Rydbergs (5571.184872 eV)

 A fine energy mesh of 0.000005 Z**2 Rydbergs (0.006803 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 1.086138 Z**2 Rydbergs (1477.8 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 1.086138 Z**2 Rydbergs (1477.8 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:        09/05/12


  • Guiyun Liang
  • Nigel Badnell
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