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Titlebook: Atomic Many-Body Theory; Ingvar Lindgren,John Morrison Book 19821st edition Springer-Verlag Berlin Heidelberg 1982 Atommodell.Body.N-Körpe

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楼主: Braggart
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Weldon A. Lodwick,Elizabeth Untiedt developed in the previous chapters, we shall still separate the single-particle states into . categories, which can be referred to as “particle” and “hole” states, respectively. In this formalism we have the option of treating the valence shell(s) either as particles or as holes, which gives some additional flexibility.
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Studies in Fuzziness and Soft Computing considering one- and two-particle equations, it is possible to treat the dominating correlation effect, namely the ., in a complete way. This appears to be a very promising approach for an accurate treatment of the electron correlation for atomic and molecular systems.
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Introductionrons. The first direct evidence of atomic shell structure was given by optical spectroscopy and x-ray absorption data. Nowadays, modern techniques, such as x-ray photoelectron spectroscopy and laser spectroscopy, provide us with a wide variety of accurate information about the structure of the atom.
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The Independent-Particle Modelerically symmetric. This is the central-field model, which together with the variation principle leads to the restricted Hartree-Fock equations. The central-field model forms the basis of the atomic shell structure and the chemical regularity of the elements.
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Application of Perturbation Theory to Open-Shell Systems developed in the previous chapters, we shall still separate the single-particle states into . categories, which can be referred to as “particle” and “hole” states, respectively. In this formalism we have the option of treating the valence shell(s) either as particles or as holes, which gives some additional flexibility.
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The Pair-Correlation Problem and the Coupled-Cluster Approach considering one- and two-particle equations, it is possible to treat the dominating correlation effect, namely the ., in a complete way. This appears to be a very promising approach for an accurate treatment of the electron correlation for atomic and molecular systems.
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Book 19821st edition limited to static atomic prop­ erties, such as the effective electron-electron interaction, but the formalism can be extended without major difficulties to include dynamic properties, such as transition probabilities and dynamic polarizabilities.
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https://doi.org/10.1007/978-3-642-57949-3the previous chapter. This process leads to the ordinary Hartree-Fock (HF) model, and it is often called the “restricted” HF procedure, in order to distinguish it from the more general or “unrestricted” HF method, discussed in Chap. 5.
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