Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
Dentro del libro
Resultados 1-3 de 14
Página 169
... Green's function now becomes 1 G ( x , x ' ) = 2α Lelo e số lần ( x −x ) + elac lan ( x − x ) ] which is identical with the previously obtained result ( 12.13 ) . An interesting property of the first derivative of the Green's function ...
... Green's function now becomes 1 G ( x , x ' ) = 2α Lelo e số lần ( x −x ) + elac lan ( x − x ) ] which is identical with the previously obtained result ( 12.13 ) . An interesting property of the first derivative of the Green's function ...
Página 172
... Green's function may be written +1 G ( r , r ' ) = Σ8ı ( r , r ' ) Σ ¥ ‚ TM ( 0 ′ , q ' ) Y ; TM ( 0 , q ) m = -l = { 8 ( r , r ) √21 + 1 yo ( tr ) 4πT ( 12.33 ) ( 12.34 ) by the use of ( 11.87 ) . The auxiliary Green's function g1 ( r ...
... Green's function may be written +1 G ( r , r ' ) = Σ8ı ( r , r ' ) Σ ¥ ‚ TM ( 0 ′ , q ' ) Y ; TM ( 0 , q ) m = -l = { 8 ( r , r ) √21 + 1 yo ( tr ) 4πT ( 12.33 ) ( 12.34 ) by the use of ( 11.87 ) . The auxiliary Green's function g1 ( r ...
Página 178
... Green's function G is a possibility . The Green's function is given by where -1 G ( r , r ' ) = ( V2 + k。3 ) ̃1 d ( r — r ′ ) = Σgir , r ' ) Y ( 0 ' , ' ) Y2 TM ( 0 , q ) 1 , m ( 13.11 ) gi ( r , r ' ) = 2 ' j¿ ( λr ) j¿ ( λr ' ) TT00 ...
... Green's function G is a possibility . The Green's function is given by where -1 G ( r , r ' ) = ( V2 + k。3 ) ̃1 d ( r — r ′ ) = Σgir , r ' ) Y ( 0 ' , ' ) Y2 TM ( 0 , q ) 1 , m ( 13.11 ) gi ( r , r ' ) = 2 ' j¿ ( λr ) j¿ ( λr ' ) TT00 ...
Contenido
Solution for Diagonalizable Matrices | 21 |
12 | 37 |
Vector Spaces and Linear Operators | 50 |
Derechos de autor | |
Otras 33 secciones no mostradas
Otras ediciones - Ver todas
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