Atomic Physics With Heavy Ions 1999
DOI: 10.1007/978-3-642-58580-7_12
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Electron-Impact Ionization and Recombination of Highly Charged Ions

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Cited by 5 publications
(2 citation statements)
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“…The experimental data points in the corresponding energy range were excluded from the fit in figure 2. By fitting the Rydberg formula to the tabulated n = 4, 5, 6 resonance positions the following quantum defects and series limits were obtained: for the 2pnp 3 D series µ = 0.282( 2) and E ∞ = 26.545(3) eV, for the 2pnp 3 P series µ = 0.180 (1) and E ∞ = 26.536 (1) eV. These values for the series limits are up to 25 meV higher than the spectroscopic values.…”
Section: Fit Of Individual Resonancesmentioning
confidence: 99%
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“…The experimental data points in the corresponding energy range were excluded from the fit in figure 2. By fitting the Rydberg formula to the tabulated n = 4, 5, 6 resonance positions the following quantum defects and series limits were obtained: for the 2pnp 3 D series µ = 0.282( 2) and E ∞ = 26.545(3) eV, for the 2pnp 3 P series µ = 0.180 (1) and E ∞ = 26.536 (1) eV. These values for the series limits are up to 25 meV higher than the spectroscopic values.…”
Section: Fit Of Individual Resonancesmentioning
confidence: 99%
“…By extending photoionization (PI) experiments to include ions in addition to atoms, systematic studies of PI along isoelectronic sequences become feasible. The sequence of berylliumlike ions has already received much attention in, for example, electron impact ionization or electron-ion recombination studies [1]. Beryllium-like ions on the one hand are relatively simple systems, so that one may hope to gain a detailed understanding of the observed atomic processes.…”
Section: Introductionmentioning
confidence: 99%