Resolved Specific Ion Data Collections

Temperature Range
4.980 eV → 4.980 x 104 eV


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  • Spontaneous Emission: Sc+16(i) → Sc+16(j) + hv
  • Electron Impact Excitation: Sc+16(i) + e → Sc+16(j) + e
2s2 2p1 2P0.5 0.0 cm-1
2s2 2p1 2P1.5 45636.4 cm-1
2s1 2p2 4P0.5 288244.0 cm-1
2s1 2p2 4P1.5 306782.0 cm-1
2s1 2p2 4P2.5 329322.0 cm-1
2s1 2p2 2D1.5 516643.0 cm-1
2s1 2p2 2D2.5 520627.0 cm-1
2s1 2p2 2S0.5 632153.0 cm-1
2s1 2p2 2P0.5 682436.0 cm-1
2s1 2p2 2P1.5 694955.0 cm-1
2p3 4S1.5 896916.0 cm-1
2p3 2D1.5 1008090.0 cm-1
2p3 2D2.5 1015250.0 cm-1
2p3 2P0.5 1129040.0 cm-1
2p3 2P1.5 1142540.0 cm-1
2s2 3s1 2S0.5 4944340.0 cm-1
2s2 3p1 2P0.5 5082460.0 cm-1
2s2 3p1 2P1.5 5095090.0 cm-1
2s1 2p1 3s1 4P0.5 5222850.0 cm-1
2s2 3d1 2D1.5 5225030.0 cm-1
2s2 3d1 2D2.5 5228970.0 cm-1
2s1 2p1 3s1 4P1.5 5236390.0 cm-1
2s1 2p1 3s1 4P2.5 5265140.0 cm-1
2s1 2p1 3s1 2P0.5 5295000.0 cm-1
2s1 2p1 3s1 2P1.5 5326350.0 cm-1
2s1 2p1 3p1 4D0.5 5346200.0 cm-1
2s1 2p1 3p1 4D1.5 5358160.0 cm-1
2s1 2p1 3p1 2P0.5 5374740.0 cm-1
2s1 2p1 3p1 2P1.5 5376510.0 cm-1
2s1 2p1 3p1 4D2.5 5378320.0 cm-1
2s1 2p1 3p1 4D3.5 5403940.0 cm-1
2s1 2p1 3p1 4S1.5 5406250.0 cm-1
2s1 2p1 3p1 4P0.5 5407590.0 cm-1
2s1 2p1 3p1 4P1.5 5427390.0 cm-1
2s1 2p1 3p1 4P2.5 5435750.0 cm-1
2s1 2p1 3p1 2D1.5 5436370.0 cm-1
2s1 2p1 3p1 2D2.5 5462470.0 cm-1
2s1 2p1 3d1 4F1.5 5472470.0 cm-1
2s1 2p1 3d1 4F2.5 5480880.0 cm-1
2s1 2p1 3d1 4F3.5 5493810.0 cm-1
2s1 2p1 3p1 2S0.5 5494530.0 cm-1
2s1 2p1 3d1 4F4.5 5515080.0 cm-1
2s1 2p1 3d1 4D2.5 5515640.0 cm-1
2s1 2p1 3s1 2P0.5 5516550.0 cm-1
2s1 2p1 3s1 2P1.5 5517460.0 cm-1
2s1 2p1 3d1 4D1.5 5518880.0 cm-1
2s1 2p1 3d1 4D0.5 5519840.0 cm-1
2s1 2p1 3d1 2D1.5 5533560.0 cm-1
2s1 2p1 3d1 2D2.5 5539730.0 cm-1
2s1 2p1 3d1 4D3.5 5542760.0 cm-1
2s1 2p1 3d1 4P2.5 5552630.0 cm-1
2s1 2p1 3d1 4P1.5 5554150.0 cm-1
2s1 2p1 3d1 4P0.5 5555630.0 cm-1
2s1 2p1 3d1 2F2.5 5597600.0 cm-1
2s1 2p1 3d1 2P1.5 5620110.0 cm-1
2s1 2p1 3d1 2F3.5 5623790.0 cm-1
2s1 2p1 3d1 2P0.5 5635010.0 cm-1
2s1 2p1 3p1 2P0.5 5652890.0 cm-1
2s1 2p1 3p1 2D1.5 5656820.0 cm-1
2s1 2p1 3p1 2D2.5 5664490.0 cm-1
2s1 2p1 3p1 2P1.5 5666450.0 cm-1
2s1 2p1 3p1 2S0.5 5697060.0 cm-1
2p2 3s1 4P0.5 5718020.0 cm-1
2p2 3s1 4P1.5 5734630.0 cm-1
2p2 3s1 4P2.5 5757080.0 cm-1
2s1 2p1 3d1 2F3.5 5785380.0 cm-1
2s1 2p1 3d1 2F2.5 5786330.0 cm-1
2p2 3s1 2P0.5 5796290.0 cm-1
2s1 2p1 3d1 2D1.5 5798670.0 cm-1
2s1 2p1 3d1 2D2.5 5803850.0 cm-1
2p2 3s1 2P1.5 5817160.0 cm-1
2s1 2p1 3d1 2P0.5 5820230.0 cm-1
2s1 2p1 3d1 2P1.5 5827230.0 cm-1
2p2 3p1 2S0.5 5829150.0 cm-1
2p2 3p1 4D0.5 5838850.0 cm-1
2p2 3p1 4D1.5 5844340.0 cm-1
2p2 3s1 2D2.5 5857410.0 cm-1
2p2 3p1 4D2.5 5861970.0 cm-1
2p2 3s1 2D1.5 5862980.0 cm-1
2p2 3p1 4P1.5 5870450.0 cm-1
2p2 3p1 4P0.5 5873240.0 cm-1
2p2 3p1 4P2.5 5882680.0 cm-1
2p2 3p1 4D3.5 5883560.0 cm-1
2p2 3p1 2D1.5 5890380.0 cm-1
2p2 3p1 2D2.5 5921240.0 cm-1
2p2 3p1 2P1.5 5932460.0 cm-1
2p2 3p1 4S1.5 5939260.0 cm-1
2p2 3p1 2P0.5 5942390.0 cm-1
2p2 3d1 4F1.5 5947190.0 cm-1
2p2 3d1 4F2.5 5956470.0 cm-1
2p2 3d1 4F3.5 5970600.0 cm-1
2p2 3p1 2F2.5 5977240.0 cm-1
2p2 3d1 2P1.5 5980770.0 cm-1
2p2 3d1 4D0.5 5983770.0 cm-1
2p2 3p1 2F3.5 5986050.0 cm-1
2p2 3d1 4D2.5 5987430.0 cm-1
2p2 3d1 4F4.5 5988170.0 cm-1
2p2 3d1 4D3.5 5997790.0 cm-1
2p2 3d1 4D1.5 5999300.0 cm-1
2p2 3d1 2F2.5 6003410.0 cm-1
2p2 3p1 2D1.5 6021300.0 cm-1
2p2 3d1 2P0.5 6022230.0 cm-1
2p2 3p1 2D2.5 6025970.0 cm-1
2p2 3d1 4P2.5 6031570.0 cm-1
2p2 3s1 2S0.5 6032960.0 cm-1
2p2 3d1 2F3.5 6034210.0 cm-1
2p2 3d1 4P1.5 6039530.0 cm-1
2p2 3d1 4P0.5 6044090.0 cm-1
2p2 3p1 2P0.5 6047440.0 cm-1
2p2 3p1 2P1.5 6072040.0 cm-1
2p2 3d1 2G3.5 6086730.0 cm-1
2p2 3d1 2D2.5 6091880.0 cm-1
2p2 3d1 2G4.5 6092820.0 cm-1
2p2 3d1 2D1.5 6093860.0 cm-1
2p2 3d1 2D1.5 6117550.0 cm-1
2p2 3d1 2D2.5 6124900.0 cm-1
2p2 3d1 2F3.5 6138740.0 cm-1
2p2 3d1 2P0.5 6151170.0 cm-1
2p2 3d1 2F2.5 6152980.0 cm-1
2p2 3d1 2P1.5 6165810.0 cm-1
2p2 3d1 2S0.5 6171650.0 cm-1
2p2 3p1 2P0.5 6172330.0 cm-1
2p2 3p1 2P1.5 6178270.0 cm-1
2p2 3d1 2D2.5 6291370.0 cm-1
2p2 3d1 2D1.5 6296110.0 cm-1
2s2 4s1 2S0.5 6711150.0 cm-1
2s2 4p1 2P0.5 6767700.0 cm-1
2s2 4p1 2P1.5 6772890.0 cm-1
2s2 4d1 2D1.5 6820000.0 cm-1
2s2 4d1 2D2.5 6821590.0 cm-1
2s2 4f1 2F2.5 6848780.0 cm-1
2s2 4f1 2F3.5 6849520.0 cm-1
2s1 2p1 4s1 4P0.5 6987690.0 cm-1
2s1 2p1 4s1 4P1.5 7000220.0 cm-1
2s1 2p1 4s1 2P0.5 7017470.0 cm-1
2s1 2p1 4s1 4P2.5 7029860.0 cm-1
2s1 2p1 4p1 4D0.5 7038600.0 cm-1
2s1 2p1 4p1 4D1.5 7047380.0 cm-1
2s1 2p1 4s1 2P1.5 7049490.0 cm-1
2s1 2p1 4p1 2P1.5 7055300.0 cm-1
2s1 2p1 4p1 4D2.5 7060000.0 cm-1
2s1 2p1 4p1 2P0.5 7061680.0 cm-1
2s1 2p1 4p1 4P0.5 7066160.0 cm-1
2s1 2p1 4p1 2D1.5 7072310.0 cm-1
2s1 2p1 4p1 4D3.5 7086720.0 cm-1
2s1 2p1 4d1 4F1.5 7087620.0 cm-1
2s1 2p1 4p1 4P1.5 7091390.0 cm-1
2s1 2p1 4d1 4F2.5 7093500.0 cm-1
2s1 2p1 4p1 4P2.5 7093720.0 cm-1
2s1 2p1 4p1 4S1.5 7095420.0 cm-1
2s1 2p1 4d1 4F3.5 7104550.0 cm-1
2s1 2p1 4d1 4P2.5 7105340.0 cm-1
2s1 2p1 4p1 2D2.5 7108330.0 cm-1
2s1 2p1 4d1 4D1.5 7109080.0 cm-1
2s1 2p1 4d1 4D0.5 7110680.0 cm-1
2s1 2p1 4d1 2D1.5 7118650.0 cm-1
2s1 2p1 4p1 2S0.5 7119550.0 cm-1
2s1 2p1 4f1 4G2.5 7122000.0 cm-1
2s1 2p1 4f1 4D3.5 7123040.0 cm-1
2s1 2p1 4d1 2D2.5 7124840.0 cm-1
2s1 2p1 4d1 4F4.5 7129900.0 cm-1
2s1 2p1 4f1 4F1.5 7133460.0 cm-1
2s1 2p1 4f1 4G4.5 7134720.0 cm-1
2s1 2p1 4f1 4F2.5 7134770.0 cm-1
2s1 2p1 4f1 4G3.5 7135210.0 cm-1
2s1 2p1 4d1 4D3.5 7136920.0 cm-1
2s1 2p1 4f1 2F2.5 7139570.0 cm-1
2s1 2p1 4f1 2G3.5 7139890.0 cm-1
2s1 2p1 4d1 4D2.5 7139980.0 cm-1
2s1 2p1 4d1 4P1.5 7141820.0 cm-1
2s1 2p1 4d1 4P0.5 7142650.0 cm-1
2s1 2p1 4d1 2F2.5 7150870.0 cm-1
2s1 2p1 4d1 2P1.5 7160030.0 cm-1
2s1 2p1 4f1 4F4.5 7165240.0 cm-1
2s1 2p1 4f1 4F3.5 7165590.0 cm-1
2s1 2p1 4d1 2F3.5 7165740.0 cm-1
2s1 2p1 4f1 4D2.5 7167480.0 cm-1
2s1 2p1 4f1 4G5.5 7168160.0 cm-1
2s1 2p1 4f1 2F3.5 7168460.0 cm-1
2s1 2p1 4d1 2P0.5 7169300.0 cm-1
2s1 2p1 4f1 4D1.5 7170320.0 cm-1
2s1 2p1 4f1 2G4.5 7171910.0 cm-1
2s1 2p1 4f1 4D0.5 7172170.0 cm-1
2s1 2p1 4f1 2D2.5 7172260.0 cm-1
2s1 2p1 4f1 2D1.5 7176480.0 cm-1
2s1 2p1 4s1 2P0.5 7275900.0 cm-1
2s1 2p1 4s1 2P1.5 7276640.0 cm-1
2s1 2p1 4p1 2D1.5 7330150.0 cm-1
2s1 2p1 4p1 2P0.5 7332180.0 cm-1
2s1 2p1 4p1 2D2.5 7333470.0 cm-1
2s1 2p1 4p1 2P1.5 7336950.0 cm-1
2s1 2p1 4p1 2S0.5 7345580.0 cm-1
2s1 2p1 4d1 2F2.5 7381240.0 cm-1
2s1 2p1 4d1 2F3.5 7381240.0 cm-1
2s1 2p1 4d1 2D1.5 7381910.0 cm-1
2s1 2p1 4d1 2D2.5 7383950.0 cm-1
2s1 2p1 4d1 2P0.5 7392850.0 cm-1
2s1 2p1 4d1 2P1.5 7394510.0 cm-1
2s1 2p1 4f1 2F2.5 7403030.0 cm-1
2s1 2p1 4f1 2F3.5 7403790.0 cm-1
2s1 2p1 4f1 2G3.5 7411270.0 cm-1
2s1 2p1 4f1 2G4.5 7411970.0 cm-1
2s1 2p1 4f1 2D1.5 7416580.0 cm-1
2s1 2p1 4f1 2D2.5 7417230.0 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 = 1.38253
         2S = 1.25020
         2P = 1.17403
         3S = 1.59051
         3P = 1.36923
         3D = 1.48216
         4S = 1.49331
         4P = 1.37751
         4D = 1.53545
         4F = 1.53287

 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 943.0712 Rydbergs (12831.426747 eV)

 A fine energy mesh of 0.000002 Z**2 Rydbergs (0.006966272 eV) was used
 between the first and last thresholds for the excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (3.483136 eV) was used
 from the last threshold up to 0.942254 Z**2 Rydbergs (3282 eV) in the
 excitation calculation.

 A coarse energy mesh of 0.001000 Z**2 Rydbergs (3.483136 eV) was used
 from first threshold up to 0.942254 Z**2 Rydbergs (3282 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:        25/04/12


  • Guiyun Liang
  • Nigel Badnell
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