Titlebook: Collisions of Electrons with Atoms and Molecules; G. F. Drukarev Book 1987 Plenum Press, New York 1987 Cross section.Plasma.atomic collisi

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Introduction,ve certain momenta and projection of their spin on some specified fixed direction, and the target is in a certain state of internal motion specified by a set of quantum numbers. After the collision all momenta, spin projections and other quantum numbers will be changed (in general). Moreover the str

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Scattering of a Particle by a Potential,ain initial form of it. This initial form corresponds to a particle localized at a given time in the source far from the target. The time evolution of the wave function is governed by the Schrödinger equation

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Ionization,the ejected) near threshold is low and the energy dependence of the cross section is determined mainly by the motion of the electron far away from the nucleus. In this case the motion of the electrons can be treated using classical mechanics. This was done by Wannier (1953) and later by Vinkaln and

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Dissociation of Molecules,of the incident electron exceeds the reaction threshold. Some characteristic features of this process can be demonstrated when the H. molecule is the target. The experimental data were summarized by Schulz (1973). In Figure 9.1 the energy dependence of the total cross section for dissociative attach

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Inference Control for relational databasesthe ejected) near threshold is low and the energy dependence of the cross section is determined mainly by the motion of the electron far away from the nucleus. In this case the motion of the electrons can be treated using classical mechanics. This was done by Wannier (1953) and later by Vinkaln and Gailitis (1967).