Electron impact collision strengths and spontaneous radiative decay rates are calculated for Fe XI. The data pertain to the 96 levels of the configurations 3s 2 3p 4 , 3s3p 5 , 3s 2 3p 3 3d, 3p 6 , 3s 2 3p 3 4s, and 3s 2 3p 3 4d. Collision strengths are calculated at 10 incident electron energies: 1
Atomic data and spectral line intensities for Ni XXI
β Scribed by A.K. Bhatia; E. Landi; H.E. Mason
- Publisher
- Elsevier Science
- Year
- 2003
- Tongue
- English
- Weight
- 334 KB
- Volume
- 83
- Category
- Article
- ISSN
- 0092-640X
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β¦ Synopsis
Electron impact collision strengths, energy levels, oscillator strengths and spontaneous radiative decay rates are calculated for Ni XXI. The configurations used are 2s 2 2p 4 , 2s2p 5 , 2p 6 , 2s 2 2p 3 3s, and 2s 2 3p 3 3d giving rise to 58 fine-structure levels in intermediate coupling. Collision strengths are calculated at five incident energies, 85, 170, 255, 340, and 425 Ry. Excitation rate coefficients are calculated by assuming a Maxwellian electron velocity distribution at an electron temperature of log T e Γ°KΓ ΒΌ 6:9, corresponding to maximum abundance of Ni XXI. Using the excitation rate coefficients and the radiative transition rates, statistical equilibrium equations for level populations are solved at electron densities 10 8 -10 14 cm Γ3 . Relative spectral line intensities are calculated. Proton excitation rates between the lowest three levels have been included in the statistical equilibrium equations. The predicted intensity ratios are compared with available observations.
π SIMILAR VOLUMES
Electron collision strengths for Mg VI, calculated in the distorted-wave approximation, are presented for all transitions between the 23 levels of the 2s 2 2p 3 , 2s2p 4 , 2p 5 , and 2s 2 2p 2 3s configurations. Radiative data have been calculated utilizing the same four-configuration model of the i
Electron impact collision strengths, energy levels, oscillator strengths, and spontaneous radiative decay rates are calculated for the O-like ion S IX. The configurations used are 2s 2 2p 4 , 2s2p 5 , 2p 6 , 2s 2 2p 3 3s, 2s 2 2p 3 3p, and 2s 2 2p 3 3d giving rise to 86 fine-structure levels in inte