Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
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Página 22
... Eigenvalues and Eigencolumns If there exist a number λ and a column u such that Au = λι ( 2.7 ) λ then 2 is said to be an eigenvalue of A , u is said to be an eigen column of A , and the eigencolumn u and the eigenvalue 2 are said to ...
... Eigenvalues and Eigencolumns If there exist a number λ and a column u such that Au = λι ( 2.7 ) λ then 2 is said to be an eigenvalue of A , u is said to be an eigen column of A , and the eigencolumn u and the eigenvalue 2 are said to ...
Página 225
... eigenvalue and the corresponding eigencolumn of a ( matrix ) operator L. It proceeds as follows : It is desired to solve the eigenvalue problem Ly = hy ' m ( 16.1 ) for its largest ( in magnitude ) eigenvalue 2 , and its corresponding eigen ...
... eigenvalue and the corresponding eigencolumn of a ( matrix ) operator L. It proceeds as follows : It is desired to solve the eigenvalue problem Ly = hy ' m ( 16.1 ) for its largest ( in magnitude ) eigenvalue 2 , and its corresponding eigen ...
Página 227
... eigenvalue and its eigen- column are determined , whereas in many problems it is the lowest eigen- value and its eigencolumn which are of interest ; the method cannot be applied to continuous systems involving differential operators ...
... eigenvalue and its eigen- column are determined , whereas in many problems it is the lowest eigen- value and its eigencolumn which are of interest ; the method cannot be applied to continuous systems involving differential operators ...
Contenido
Solution for Diagonalizable Matrices | 21 |
The Evaluation of a Function of a Matrix for an Arbitrary Matrix | 38 |
13 | 44 |
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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