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The data in the above table shows that: 1, the ions from the high spectral line very intensive, and some energy difference of 0.01 au. When the number of electrons in a long time, the line to the long-wave energy that is moving low. The so-intensive lines, experiments using only high-resolution equipment and advanced tools can be observed that this experiment will undoubtedly bring a high degree of difficulty. We adopted strict calculated precise spectral data for the experimental work can provide a useful reference. 2, in the spectrum, on the same between the two electronic states in terms of the transition from high multiple of the spectrum transition to a low degree of multiple spectra of the energy spectra obtained from multiple often than the low degree spectra of the transition to high multiple of the spectrum by the spectrum of energy to be small. This is 3.1-3.3 in the same table can be seen. 3, in the line, on a line of the case, with the principal quantum number increases, the transition probabilities and oscillator strength reduced, but the rate of decrease transition probabilities than oscillator strength is smaller. By definition, the transition probabilities level spacing, transitions and radial type parameters of the three points, despite the energy interval with the increase in the principal quantum number, but the radial integral had been falling, and the decline rate faster than the increase in energy interval rate. The oscillator strength is proportional and integral radial, and energy is inversely proportional spacing, oscillator strength transition probabilities than the rate of the decrease is reasonable. 4, atom (ion) of the spin - orbit coupling is essentially a relativistic effect, and for highly ionized atoms state, the valence electrons are lining of the shielding role of the smaller electronic, atomic number of effective nuclear charge bigger, more valence electron in the field of nuclear power movement, relativistic effect more visible and thus have a stronger rotation - Orbit role. Therefore, in such circumstances, we have adopted a jj coupling, rather than LS coupling, as a violation of this rule LS coupling transitions (¡÷ S = 0) s-2p transition is a reasonable existence. 5, and found that: 1 s-2p (r = 1-6) to 1 s-3p transition of the energy transition probabilities, the oscillator strength and intensity to the line, but the difference is very small. For example: r = 1, 1s-2p, E = 226.0334au, A = 9.7643,; 1s-3p, E = 223.4706au, A = 8.7643,. Accordingly the former than the latter slightly higher. We know that the level of different transitions spectral data, select a transition and a strong interaction between the energy electron configuration not the same, these electronic configuration formed by the configuration state function CSF is not the same, thus the CSF on atomic ASF contribution to the state does not function like this, and eventually will have an impact on the calculation of spectral data results. So that we can draw: 2 s full shell did not affect CSF on atomic state function ASF contribution, that is 2 s for its shell outside the Shell 2 p little impact on the electronics.
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