Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
Dentro del libro
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Página 20
... chap . 5 , McGraw - Hill Book Company , Inc. , New York , 1940 . Margenau , H. , and G. M. Murphy : " The Mathematics of Physics and Chemistry , " chap . 10 , D. Van Nostrand Company , Inc. , Princeton , N.J. , 1943 . Jeffreys , H ...
... chap . 5 , McGraw - Hill Book Company , Inc. , New York , 1940 . Margenau , H. , and G. M. Murphy : " The Mathematics of Physics and Chemistry , " chap . 10 , D. Van Nostrand Company , Inc. , Princeton , N.J. , 1943 . Jeffreys , H ...
Página 197
... chap . V and chap . VII , sec . 26 , McGraw - Hill Book Company , Inc. , New York , 1949 . Sommerfeld , A .: " Partial Differential Equations in Physics , " chap . V , Academic Press , Inc. , New York , 1949 . Morse , P. M. , and H ...
... chap . V and chap . VII , sec . 26 , McGraw - Hill Book Company , Inc. , New York , 1949 . Sommerfeld , A .: " Partial Differential Equations in Physics , " chap . V , Academic Press , Inc. , New York , 1949 . Morse , P. M. , and H ...
Página 266
... Chap . 5 , which dealt with finite dimensional spaces only , to cover the infinite dimensional spaces as well . The reader is therefore advised to refresh his knowledge of the contents of the first two sections of Chap . 5 before ...
... Chap . 5 , which dealt with finite dimensional spaces only , to cover the infinite dimensional spaces as well . The reader is therefore advised to refresh his knowledge of the contents of the first two sections of Chap . 5 before ...
Contenido
Solution for Diagonalizable Matrices | 21 |
12 | 37 |
Vector Spaces and Linear Operators | 50 |
Derechos de autor | |
Otras 33 secciones no mostradas
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Términos y frases comunes
analytic approximate arbitrary asymptotic ax² Bessel function boundary conditions chap coefficients consider constant contour coordinates corresponding cylindrical functions d₁ d²/dx² defined denotes determinant diagonal differential equation Dirac notation ei(p eigen eigencolumn eigenfunctions eigenvalue equation eigenvalue problem eigenvector eikr element evaluate expansion finite number follows Fourier integral theorem function f(x given Green's function Hence Hermitian Hermitian matrix Hermitian operator infinite integral representation integrand inverse Laplacian linear lowest eigenvalue matrix method multiplication notation obtained operator orthonormality conditions perturbation plane relations result Ritz method row or column saddle point saddle-point method satisfy the orthonormality scattering sinh solution solve spherical spherical harmonics substitution transformation functions trial functions vanish variable vector vector space verified wave written yields zero ηπχ πρ ди ду дх