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Titlebook: Non-perturbative Description of Quantum Systems; Ilya Feranchuk,Alexey Ivanov,Alexander Ulyanenkov Book 2015 Springer International Publis

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Ilya Feranchuk,Alexey Ivanov,Van-Hoang Le,Alexander Ulyanenkovanging from 19 to 83. In view of the large amount of data available some of the information is given on the CD ROM only. The data for nuclei with Z up to 18 has been published in Subvolume I/19A1. Parameters fo978-3-540-31656-5Series ISSN 1615-1844 Series E-ISSN 1616-9522
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0075-8450 lustrate the basic principles of the method which are further used for the solution of complex problems of quantum theory for many-particle systems. The results obtained are supplemented by numerical calculations, presented as tables and figures.978-3-319-13005-7978-3-319-13006-4Series ISSN 0075-8450 Series E-ISSN 1616-6361
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https://doi.org/10.1007/978-3-319-13006-4Anharmonic Oscillator; Atoms in a Strong External Field; Coupled Anharmonic Oscillators; Multi-electron
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Many-Electron Atoms,, biology and condensed matter physics by using density functional theory (DFT), introduced in pioneering works [1, 2]. This approach is used as a basis for ab initio calculations for complex molecular systems and the details of the method are presented in numerous monographs and reviews [3–6].
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Ilya Feranchuk,Alexey Ivanov,Alexander UlyanenkovGives a detailed introduction and comprehensive description of non-perturbative operator method.Provides an extended review of other non-perturbative methods for description of quantum systems.Display
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978-3-319-13005-7Springer International Publishing Switzerland 2015
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Applications of OM for One-Dimensional Systems,The extended analysis of various physical problems related to anharmonic oscillator performed in previous chapter makes it possible to sort out the capabilities of the operator method, which are not exclusively related to QAO and can be exploited for description of more complex quantum systems.
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Operator Method for Quantum Statistics,The construction of the uniformly available approximation (UAA) for thermodynamical functions has two specific features, which differ it from the solution of the Schrödinger equation for stationary states. First of all, these functions depend both on Hamiltonian parameters and on the temperature ..
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