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发表于 2025-3-21 18:00:07 | 显示全部楼层 |阅读模式
书目名称Green’s Functions in Quantum Physics
编辑Eleftherios N. Economou
视频video
丛书名称Springer Series in Solid-State Sciences
图书封面Titlebook: ;
出版日期Book 19791st edition
版次1
doihttps://doi.org/10.1007/978-3-662-11900-6
isbn_ebook978-3-662-11900-6Series ISSN 0171-1873 Series E-ISSN 2197-4179
issn_series 0171-1873
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发表于 2025-3-21 21:39:15 | 显示全部楼层
发表于 2025-3-22 02:43:44 | 显示全部楼层
Social Science and OR Technologyfect periodic lattice. The hamiltonian is given by .. + .. where .. is a periodic TBH of the type studied in Chap.5 and .. describes the change of the potential as a result of the impurity and is given by ..
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https://doi.org/10.1007/978-1-4615-5747-0in Chap.2, corresponding to a second-order (in time) differential equation. For a translationally invariant system the Fourier transforms of the g’s and g’s can be expressed in terms of a single real quantity A(.,ω) which can be interpreted as 2π times a generalized density of states in .-ω-space.
发表于 2025-3-22 20:16:39 | 显示全部楼层
Green’s Functions and Perturbation Theoryenvalues and eigenfunctions can be easily determined. This problem will be solved by: 1) calculating ..(z) corresponding to .. ; 2) expressing .(z) in terms of ..(z) and .., where .(z) is the Green’s function associated with .; and 3) extracting from .(z) information about the eigenvalues and eigenf
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Two or More Impurities; Disordered Systemssociated with the two impurities is not simply the sum of t-matrices of each impurity but includes infinitely many terms which correspond physically to multiple scattering events. A diagrammatic representation of this fact is shown in Fig.7.1, where the propagation from site i to site . [described b
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