Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
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... Green's function for a broad set of fragments . Figure 1 shows the first three collisional contributions to the Green's function for producing 52 Cr . In the figure , the atomic weight of each projectile ( Ap ) is truncated to the ...
... Green's function for a broad set of fragments . Figure 1 shows the first three collisional contributions to the Green's function for producing 52 Cr . In the figure , the atomic weight of each projectile ( Ap ) is truncated to the ...
Página 81
G. Rickayzen. FIG.3.16. The one-particle Green's function G(1,2) (the thick line here) represented in terms of proper self-energies. This general result can be related to the Green's function given by equation (3.55) which was derived ...
G. Rickayzen. FIG.3.16. The one-particle Green's function G(1,2) (the thick line here) represented in terms of proper self-energies. This general result can be related to the Green's function given by equation (3.55) which was derived ...
Página 173
... Green's function formulation of many - body quantum transport theory for multi - band semiconductor systems with a phonon bath . The equations are expressed exactly in terms of single particle nonequilibrium Green's functions and self ...
... Green's function formulation of many - body quantum transport theory for multi - band semiconductor systems with a phonon bath . The equations are expressed exactly in terms of single particle nonequilibrium Green's functions and self ...
Contenido
34 | 12 |
Solution for Diagonalizable Matrices | 21 |
The Evaluation of a Function of a Matrix for an Arbitrary Matrix | 38 |
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approximation arbitrary ax² basis Bessel functions boundary conditions Chap coefficients column consider constant continuous systems contour coordinates corresponding cylindrical functions d²/dx² defined definition denoted determinant diagonal differential equation Dirac notation domain eigencolumns eigenfunctions eigenvectors elements evaluate expansion F₁ finite number follows formula Fourier given Green's function Hence Hermitian Hermitian matrix Hermitian operator infinite integral inverse Laplacian linear operator linearly independent lowest eigenvalue Mathematical matrix McGraw-Hill Book Company method multiplication nonsingular normal number of degrees obtained orthonormality conditions Physics problem relations representation result Ritz method scattering sinh solution solve spherical spherical harmonics string Substitution theorem transform trial functions vanish variable vector space Verify w₁ wave write written x₁ Y₁ yields York zero ηπχ ди ду дх