flike_mcw06#ne1.dat
Resolved Specific Ion Data Collections
- Ion
- Ne1+
- Temperature Range
- 0.069 eV → 689 eV
ADF04
- Filename
- flike_mcw06#ne1.dat
- Full Path
- adf04/copaw#f/flike_mcw06#ne1.dat
Download data
- Spontaneous Emission: Ne+1(i) → Ne+1(j) + hv
- Electron Impact Excitation: Ne+1(i) + e → Ne+1(j) + e
| 2s2 2p5 2P1.5 | 0.0 cm-1 |
| 2s2 2p5 2P0.5 | 890.0 cm-1 |
| 2s2 2p4 3s1 4P2.5 | 196018.0 cm-1 |
| 2s2 2p4 3s1 4P1.5 | 196526.0 cm-1 |
| 2s2 2p4 3s1 4P0.5 | 196836.0 cm-1 |
| 2s2 2p4 3s1 2P1.5 | 201063.0 cm-1 |
| 2s2 2p4 3s1 2P0.5 | 201676.0 cm-1 |
| 2s2 2p4 3p1 4P2.5 | 222672.0 cm-1 |
| 2s2 2p4 3p1 4P1.5 | 222902.0 cm-1 |
| 2s2 2p4 3p1 4P0.5 | 223080.0 cm-1 |
| 2s2 2p4 3s1 2D2.5 | 225193.0 cm-1 |
| 2s2 2p4 3s1 2D1.5 | 225194.0 cm-1 |
| 2s2 2p4 3p1 4D3.5 | 225325.0 cm-1 |
| 2s2 2p4 3p1 4D2.5 | 225663.0 cm-1 |
| 2s2 2p4 3p1 4D1.5 | 225918.0 cm-1 |
| 2s2 2p4 3p1 4D0.5 | 226069.0 cm-1 |
| 2s2 2p4 3p1 2D2.5 | 227148.0 cm-1 |
| 2s2 2p4 3p1 2D1.5 | 227661.0 cm-1 |
| 2s2 2p4 3p1 2S0.5 | 228952.0 cm-1 |
| 2s2 2p4 3p1 4S1.5 | 228993.0 cm-1 |
| 2s2 2p4 3p1 2P1.5 | 233160.0 cm-1 |
| 2s2 2p4 3p1 2P0.5 | 233175.0 cm-1 |
| 2s1 2p6 2S0.5 | 239585.0 cm-1 |
| 2s2 2p4 3p1 2F2.5 | 252436.0 cm-1 |
| 2s2 2p4 3p1 2F3.5 | 252467.0 cm-1 |
| 2s2 2p4 3d1 4D3.5 | 254643.0 cm-1 |
| 2s2 2p4 3d1 4D2.5 | 254722.0 cm-1 |
| 2s2 2p4 3d1 4D1.5 | 254824.0 cm-1 |
| 2s2 2p4 3d1 4D0.5 | 254917.0 cm-1 |
| 2s2 2p4 3p1 2D1.5 | 255208.0 cm-1 |
| 2s2 2p4 3p1 2D2.5 | 255233.0 cm-1 |
| 2s2 2p4 3d1 4F4.5 | 255741.0 cm-1 |
| 2s2 2p4 3d1 4F3.5 | 255920.0 cm-1 |
| 2s2 2p4 3d1 2D2.5 | 256005.0 cm-1 |
| 2s2 2p4 3d1 2D1.5 | 256192.0 cm-1 |
| 2s2 2p4 3d1 4P0.5 | 256266.0 cm-1 |
| 2s2 2p4 3d1 2F3.5 | 256333.0 cm-1 |
| 2s2 2p4 3d1 4F2.5 | 256399.0 cm-1 |
| 2s2 2p4 3d1 4P1.5 | 256464.0 cm-1 |
| 2s2 2p4 3p1 2P1.5 | 256516.0 cm-1 |
| 2s2 2p4 3d1 4F1.5 | 256586.0 cm-1 |
| 2s2 2p4 3d1 4P2.5 | 256627.0 cm-1 |
| 2s2 2p4 3p1 2P0.5 | 256805.0 cm-1 |
| 2s2 2p4 3d1 2F2.5 | 256822.0 cm-1 |
| 2s2 2p4 3d1 2P0.5 | 257037.0 cm-1 |
| 2s2 2p4 3d1 2P1.5 | 257419.0 cm-1 |
| 2s2 2p4 4s1 4P2.5 | 257625.0 cm-1 |
| 2s2 2p4 4s1 4P1.5 | 258018.0 cm-1 |
| 2s2 2p4 4s1 4P0.5 | 258325.0 cm-1 |
| 2s2 2p4 4s1 2P1.5 | 259021.0 cm-1 |
| 2s2 2p4 4s1 2P0.5 | 259583.0 cm-1 |
| 2s2 2p4 4p1 4P2.5 | 266042.0 cm-1 |
| 2s2 2p4 4p1 4P1.5 | 266250.0 cm-1 |
| 2s2 2p4 3s1 2S0.5 | 266284.0 cm-1 |
| 2s2 2p4 4p1 4P0.5 | 266473.0 cm-1 |
| 2s2 2p4 4p1 4D3.5 | 266663.0 cm-1 |
| 2s2 2p4 4p1 4D2.5 | 266949.0 cm-1 |
| 2s2 2p4 4p1 4D1.5 | 267268.0 cm-1 |
| 2s2 2p4 4p1 4D0.5 | 267439.0 cm-1 |
| 2s2 2p4 4p1 2D2.5 | 267454.0 cm-1 |
| 2s2 2p4 4p1 2D1.5 | 267880.0 cm-1 |
| 2s2 2p4 4p1 2S0.5 | 267971.0 cm-1 |
| 2s2 2p4 4p1 4S1.5 | 268023.0 cm-1 |
| 2s2 2p4 4p1 2P1.5 | 273690.0 cm-1 |
| 2s2 2p4 4p1 2P0.5 | 273856.0 cm-1 |
| 2s2 2p4 4d1 4D3.5 | 277113.0 cm-1 |
| 2s2 2p4 4d1 4D2.5 | 277165.0 cm-1 |
| 2s2 2p4 4d1 4D1.5 | 277256.0 cm-1 |
| 2s2 2p4 4d1 4D0.5 | 277367.0 cm-1 |
| 2s2 2p4 4d1 4F4.5 | 277465.0 cm-1 |
| 2s2 2p4 4d1 2F3.5 | 277569.0 cm-1 |
| 2s2 2p4 4d1 2D2.5 | 277663.0 cm-1 |
| 2s2 2p4 4d1 4P0.5 | 277765.0 cm-1 |
| 2s2 2p4 4d1 2D1.5 | 277772.0 cm-1 |
| 2s2 2p4 4f1 4F4.5 | 277909.0 cm-1 |
| 2s2 2p4 4f1 2F3.5 | 277912.0 cm-1 |
| 2s2 2p4 4f1 4F3.5 | 277922.0 cm-1 |
| 2s2 2p4 4f1 4F2.5 | 277922.0 cm-1 |
| 2s2 2p4 4f1 4D1.5 | 277978.0 cm-1 |
| 2s2 2p4 4f1 2F2.5 | 277980.0 cm-1 |
| 2s2 2p4 4f1 4G5.5 | 278021.0 cm-1 |
| 2s2 2p4 4f1 2G4.5 | 278022.0 cm-1 |
| 2s2 2p4 4d1 4F3.5 | 278035.0 cm-1 |
| 2s2 2p4 4f1 4D0.5 | 278062.0 cm-1 |
| 2s2 2p4 4f1 2D1.5 | 278064.0 cm-1 |
| 2s2 2p4 4d1 4P1.5 | 278125.0 cm-1 |
| 2s2 2p4 4d1 4F2.5 | 278137.0 cm-1 |
| 2s2 2p4 4d1 2P0.5 | 278203.0 cm-1 |
| 2s2 2p4 4d1 4P2.5 | 278242.0 cm-1 |
| 2s2 2p4 4d1 4F1.5 | 278249.0 cm-1 |
| 2s2 2p4 4d1 2F2.5 | 278469.0 cm-1 |
| 2s2 2p4 4f1 4F1.5 | 278568.0 cm-1 |
| 2s2 2p4 4f1 4D2.5 | 278570.0 cm-1 |
| 2s2 2p4 4f1 4G4.5 | 278595.0 cm-1 |
| 2s2 2p4 4f1 4G3.5 | 278596.0 cm-1 |
| 2s2 2p4 4d1 2P1.5 | 278652.0 cm-1 |
| 2s2 2p4 4f1 4D3.5 | 278663.0 cm-1 |
| 2s2 2p4 4f1 2D2.5 | 278664.0 cm-1 |
| 2s2 2p4 4f1 2G3.5 | 278909.0 cm-1 |
| 2s2 2p4 4f1 4G2.5 | 278909.0 cm-1 |
| 2s2 2p4 3d1 2G3.5 | 282644.0 cm-1 |
| 2s2 2p4 3d1 2G4.5 | 282647.0 cm-1 |
| 2s2 2p4 3d1 2P1.5 | 282761.0 cm-1 |
| 2s2 2p4 3d1 2P0.5 | 282785.0 cm-1 |
| 2s2 2p4 3d1 2D2.5 | 283556.0 cm-1 |
| 2s2 2p4 3d1 2D1.5 | 283575.0 cm-1 |
| 2s2 2p4 3d1 2F2.5 | 283959.0 cm-1 |
| 2s2 2p4 3d1 2F3.5 | 283963.0 cm-1 |
| 2s2 2p4 3d1 2S0.5 | 285197.0 cm-1 |
| 2s2 2p4 4s1 2D2.5 | 285437.0 cm-1 |
| 2s2 2p4 4s1 2D1.5 | 285437.0 cm-1 |
| 2s2 2p4 4p1 2F2.5 | 294047.0 cm-1 |
| 2s2 2p4 4p1 2F3.5 | 294057.0 cm-1 |
| 2s2 2p4 3p1 2P0.5 | 294801.0 cm-1 |
| 2s2 2p4 3p1 2P1.5 | 294812.0 cm-1 |
| 2s2 2p4 4p1 2D1.5 | 294837.0 cm-1 |
| 2s2 2p4 4p1 2D2.5 | 294839.0 cm-1 |
| 2s2 2p4 4p1 2P1.5 | 296572.0 cm-1 |
| 2s2 2p4 4p1 2P0.5 | 296771.0 cm-1 |
| 2s2 2p4 4d1 2G3.5 | 304726.0 cm-1 |
| 2s2 2p4 4d1 2G4.5 | 304727.0 cm-1 |
| 2s2 2p4 4d1 2P1.5 | 304818.0 cm-1 |
| 2s2 2p4 4d1 2P0.5 | 304830.0 cm-1 |
| 2s2 2p4 4d1 2D2.5 | 305140.0 cm-1 |
| 2s2 2p4 4d1 2D1.5 | 305149.0 cm-1 |
| 2s2 2p4 4d1 2F2.5 | 305247.0 cm-1 |
| 2s2 2p4 4d1 2F3.5 | 305249.0 cm-1 |
| 2s2 2p4 4f1 2P0.5 | 305277.0 cm-1 |
| 2s2 2p4 4f1 2P1.5 | 305278.0 cm-1 |
| 2s2 2p4 4f1 2H4.5 | 305379.0 cm-1 |
| 2s2 2p4 4f1 2H5.5 | 305379.0 cm-1 |
| 2s2 2p4 4f1 2D1.5 | 305393.0 cm-1 |
| 2s2 2p4 4f1 2D2.5 | 305393.0 cm-1 |
| 2s2 2p4 4d1 2S0.5 | 305393.0 cm-1 |
| 2s2 2p4 4f1 2F2.5 | 305527.0 cm-1 |
| 2s2 2p4 4f1 2F3.5 | 305528.0 cm-1 |
| 2s2 2p4 4f1 2G3.5 | 305562.0 cm-1 |
| 2s2 2p4 4f1 2G4.5 | 305562.0 cm-1 |
| 2s2 2p4 3d1 2D2.5 | 323959.0 cm-1 |
| 2s2 2p4 3d1 2D1.5 | 323963.0 cm-1 |
| 2s2 2p4 4s1 2S0.5 | 326327.0 cm-1 |
| 2s2 2p4 4p1 2P1.5 | 335250.0 cm-1 |
| 2s2 2p4 4p1 2P0.5 | 335258.0 cm-1 |
| 2s2 2p4 4d1 2D2.5 | 345686.0 cm-1 |
| 2s2 2p4 4d1 2D1.5 | 345687.0 cm-1 |
| 2s2 2p4 4f1 2F2.5 | 346167.0 cm-1 |
| 2s2 2p4 4f1 2F3.5 | 346167.0 cm-1 |
| 2s1 2p5 3s1 4P2.5 | 411624.0 cm-1 |
| 2s1 2p5 3s1 4P1.5 | 412130.0 cm-1 |
| 2s1 2p5 3s1 4P0.5 | 412444.0 cm-1 |
| 2s1 2p5 3s1 2P1.5 | 420635.0 cm-1 |
| 2s1 2p5 3s1 2P0.5 | 421230.0 cm-1 |
| 2s1 2p5 3p1 4S1.5 | 436289.0 cm-1 |
| 2s1 2p5 3p1 4D3.5 | 439408.0 cm-1 |
| 2s1 2p5 3p1 4D2.5 | 439710.0 cm-1 |
| 2s1 2p5 3p1 4D1.5 | 439965.0 cm-1 |
| 2s1 2p5 3p1 4D0.5 | 440135.0 cm-1 |
| 2s1 2p5 3p1 2D2.5 | 441936.0 cm-1 |
| 2s1 2p5 3p1 4P2.5 | 442216.0 cm-1 |
| 2s1 2p5 3p1 4P1.5 | 442346.0 cm-1 |
| 2s1 2p5 3p1 4P0.5 | 442479.0 cm-1 |
| 2s1 2p5 3p1 2D1.5 | 442509.0 cm-1 |
| 2s1 2p5 3p1 2P1.5 | 443385.0 cm-1 |
| 2s1 2p5 3p1 2P0.5 | 443619.0 cm-1 |
| 2s1 2p5 3p1 2S0.5 | 460751.0 cm-1 |
| 2s1 2p5 3d1 4P0.5 | 469028.0 cm-1 |
| 2s1 2p5 3d1 4P1.5 | 469149.0 cm-1 |
| 2s1 2p5 3d1 4P2.5 | 469376.0 cm-1 |
| 2s1 2p5 3d1 4F4.5 | 469482.0 cm-1 |
| 2s1 2p5 3d1 4F3.5 | 469679.0 cm-1 |
| 2s1 2p5 3d1 4F2.5 | 469917.0 cm-1 |
| 2s1 2p5 3d1 2F3.5 | 470103.0 cm-1 |
| 2s1 2p5 3d1 4F1.5 | 470137.0 cm-1 |
| 2s1 2p5 3d1 2F2.5 | 470524.0 cm-1 |
| 2s1 2p5 3d1 2P0.5 | 470755.0 cm-1 |
| 2s1 2p5 3d1 2P1.5 | 470893.0 cm-1 |
| 2s1 2p5 3d1 4D3.5 | 470973.0 cm-1 |
| 2s1 2p5 3d1 4D2.5 | 471081.0 cm-1 |
| 2s1 2p5 3d1 4D1.5 | 471230.0 cm-1 |
| 2s1 2p5 3d1 4D0.5 | 471268.0 cm-1 |
| 2s1 2p5 3d1 2D2.5 | 471340.0 cm-1 |
| 2s1 2p5 3d1 2D1.5 | 471620.0 cm-1 |
| 2s1 2p5 3s1 2P1.5 | 512902.0 cm-1 |
| 2s1 2p5 3s1 2P0.5 | 512921.0 cm-1 |
| 2s1 2p5 3p1 2D1.5 | 539117.0 cm-1 |
| 2s1 2p5 3p1 2D2.5 | 539148.0 cm-1 |
| 2s1 2p5 3p1 2P0.5 | 540613.0 cm-1 |
| 2s1 2p5 3p1 2P1.5 | 540628.0 cm-1 |
| 2s1 2p5 3p1 2S0.5 | 542389.0 cm-1 |
| 2s1 2p5 3d1 2P1.5 | 568241.0 cm-1 |
| 2s1 2p5 3d1 2P0.5 | 568243.0 cm-1 |
| 2s1 2p5 3d1 2F2.5 | 568368.0 cm-1 |
| 2s1 2p5 3d1 2F3.5 | 568370.0 cm-1 |
| 2s1 2p5 3d1 2D1.5 | 569258.0 cm-1 |
| 2s1 2p5 3d1 2D2.5 | 569261.0 cm-1 |
Contributors
- Mike Witthoeft
- Allan Whiteford
- Nigel Badnell
------------------------------------------------------------------------ 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 = 1.4842 2S = 1.1510 2P = 1.1081 3S = 1.0323 3P = 1.0060 3D = 0.9941 4S = 1.0389 4P = 1.0058 4D = 0.9385 4F = 0.8990 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. 50 continuum basis orbitals were used, giving a smallest maximum basis-orbital energy of 21.2982 Rydbergs (289.783309 eV) A fine energy mesh of 0.000100 Z**2 Rydbergs (0.0013606 eV) was used between the first and last thresholds for the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (0.13606 eV) was used from the last threshold up to 9.032192 Z**2 Rydbergs (122.892 eV) in the excitation calculation. A coarse energy mesh of 0.010000 Z**2 Rydbergs (0.13606 eV) was used from first threshold up to 9.032192 Z**2 Rydbergs (122.892 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 Note that this file is for a near neutral ion but the results are from a sequence calculation. Care should be taken when using this data. 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 Added warning/caution comment ------------------------------------------------------------------------