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III. The excitation and ionization of helium by electrons of moderate velocity. Proc Roy Soc 1933; A 140(842): 613-36. Fano U, Macek JH. Impact excitation and polarization of the emitted light. Rev Mod Phys 1973; 45(4): 553-73. Botero J, Macek JH. Coulomb-Born calculation of the triple-differential cross section for inner-shell electronimpact ionization of carbon. Phys Rev A 1992; 45(1): 154-65. Berakdar J, Briggs JS. Three-body coulomb continuum problem. Phys Rev Lett 1994; 72(24): 3799-02. 28 Dynamical Processes in Atomic and Molecular Physics     Joseph H.
It is, thus, possible that some intermediate states contribute both to Ф and to 2q h1 p expansions, leading to 2q h1 p 0 . This does not lead to complications as the Fano formalism that we are using does not assume the orthogonality of the bound and the continuum components. g. those in which the ionized inner-shell orbital is delocalized due to inversion symmetry. As has been shown in Ref. , this difficulty can be circumvented by using the appropriate linear combinations of the "standard" configurations.
This asymptotic behavior of the decay width can be explained by a physically appealing virtual photon transfer model which represents the decay process as an emission of a virtual photon by the inner-shell-ionized atom followed by its absorption by a neighboring neutral. 40 Dynamical Processes in Atomic and Molecular Physics Averbukh et al. Figure 5: Doubly logarithmic plot of the total ICD width of Ne 2s vacancy in MgNe cluster as a function of internuclear separation. Full line- ADC(2)x result; dashed line – virtual photon transfer prediction .