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Titlebook: Atomic Photoeffect; M. Ya. Amusia Book 1990 Springer Science+Business Media New York 1990 Plasma.astrophysics.atom.atoms.electronics.energ

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The Random-Phase Approximation with Exchange,tion amplitude becomes the sum of two terms. The first of these arises from the electron being removed by means of its direct interaction with the electromagnetic field, while the second describes an electron ejected as a result of the change in the self-consistent field.
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Double-Vacancy States, one-electron ionization accompanied by excitation. In the first experiments [192] on double-electron ionization, one electron was removed from an inner shell, while the other was removed from an outer shell. The results were explained by the “shake-off” model, according to which the change in the a
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Estimate , from a Normal Population,tomic self-consistent field caused by removal of one of the inner electrons leads, in turn, to the removal of an outer electron. The situation became markedly more complex when data were obtained for removal of two electrons from the same shell, and especially on removal from an outer one [26].
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The Structure of the Atom and Its Interaction with an Electromagnetic Field,esented are of Coulombic origin. The state of an atom is determined by its wavefunction Ψ.(.. ⋯ ..), which is a solution of the stationary Schrödinger equation:.where Ψ. depends on the spatial coordinates and spin projection of each electron, i.e., .. ≡ .., σ..
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Double-Vacancy States,tomic self-consistent field caused by removal of one of the inner electrons leads, in turn, to the removal of an outer electron. The situation became markedly more complex when data were obtained for removal of two electrons from the same shell, and especially on removal from an outer one [26].
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