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

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期刊全稱(chēng)Atomic Many-Body Theory
影響因子2023Ingvar Lindgren,John Morrison
視頻videohttp://file.papertrans.cn/165/164741/164741.mp4
學(xué)科分類(lèi)Springer Series in Chemical Physics
圖書(shū)封面Titlebook: Atomic Many-Body Theory;  Ingvar Lindgren,John Morrison Book 19821st edition Springer-Verlag Berlin Heidelberg 1982 Atommodell.Body.N-K?rpe
影響因子This book has developed through a series of lectures on atomic theory given these last eight years at Chalmers University of Technology and several oth- er research centers. These courses were intended to make the basic elements of atomic theory available to experimentalists working with the hyperfine structure and the optical properties of atoms and to provide some insight into recent developments in the theory. The original intention of this book has gradually extended to include a wide range of topics. We have tried to provide a complete description of atomic theory, bridging the gap between introductory books on quantum mechanics - such as the book by Merzbacher, for instance - and present- day research in the field. Our presentation is 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.
Pindex Book 19821st edition
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書(shū)目名稱(chēng)Atomic Many-Body Theory影響因子(影響力)




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Angular-Momentum and Spherical Tensor Operators appears in the present chapter is treated more extensively in several monographs that are devoted entirely to angular-momentum theory [. 1957; . 1957; . and . 1959; . and . 1968] and the reader is referred to these books for further details. We have tried, however, to include all the material we ne
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The Central-Field Modelage field due to the nucleus and the other electrons. This assumption reduces the many-electron problem to a number of independent single-electron problems, and it leads to the general unrestricted Hartree-Fock model. For an arbitrary potential the single-particle functions can have quite a complica
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