Some Mathematical Methods of Physics |
Dentro del libro
Resultados 1-3 de 76
Página 26
Since the above two results are fundamental , it is desirable to consider them at some length . Let the eigencolumns of A , belonging to the eigenvalues 21 , be written ass . Then , as follows from ( 2.8 ) , ƒ ( A ) s.
Since the above two results are fundamental , it is desirable to consider them at some length . Let the eigencolumns of A , belonging to the eigenvalues 21 , be written ass . Then , as follows from ( 2.8 ) , ƒ ( A ) s.
Página 61
The representation of the operator L in the basis v , defined by the relations is + uz = VjSjl and ut = Σ suve From ( 4.31 ) it follows that L = = Σv1 ( sus ) v ls L = Σulu + n = integer ( 4.33 ) ( 4.34 ) ( 4.35 ) so that for any power ...
The representation of the operator L in the basis v , defined by the relations is + uz = VjSjl and ut = Σ suve From ( 4.31 ) it follows that L = = Σv1 ( sus ) v ls L = Σulu + n = integer ( 4.33 ) ( 4.34 ) ( 4.35 ) so that for any power ...
Página 247
which is clearly its cofactor Dnn . That the coefficient of d , is its cofactor D1 , may be seen as follows : In | D | interchange the nth and ith rows and then the nth and jth columns , so as to make the element a ,, the lower right ...
which is clearly its cofactor Dnn . That the coefficient of d , is its cofactor D1 , may be seen as follows : In | D | interchange the nth and ith rows and then the nth and jth columns , so as to make the element a ,, the lower right ...
Comentarios de la gente - Escribir un comentario
No encontramos ningún comentario en los lugares habituales.
Contenido
Solution for Diagonalizable Matrices | 21 |
The Evaluation of a Function of a Matrix for an Arbitrary Matrix | 38 |
13 | 44 |
Derechos de autor | |
Otras 25 secciones no mostradas
Otras ediciones - Ver todas
Términos y frases comunes
applied approaches approximate arbitrary basis becomes Bessel boundary conditions called chap chapter Clearly coefficients column complete consider constant continuous contour coordinates corresponding defined definition demonstrated denoted derived determinant difference differential equation direction discussed eigencolumn eigenfunctions eigenvalue element equal equation evaluate example exists expansion expression finite follows Fourier function given Green's function Hence independent infinite integral introduce known limit linear lowest matrix method multiplication normalized notation Note obtained operator orthonormality path Physics plane positive problem procedure reduces relations replaced representation represented result satisfies scattering solution solve space string Substitution Suppose theorem transformation unique vanish variable vector verified wave write written yields York zero ду