Some Mathematical Methods of Physics |
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It will now be shown that an arbitrary column u may be written as a linear combination of the eigencolumns of A if and only if A has n linearly independent eigencolumns . Thus , if A has less than n linearly independ- ent eigencolumns ...
It will now be shown that an arbitrary column u may be written as a linear combination of the eigencolumns of A if and only if A has n linearly independent eigencolumns . Thus , if A has less than n linearly independ- ent eigencolumns ...
Página 28
It will now be shown that A has at least as many linearly independent eigencolumns as it has distinct eigenvalues . Thus , let these distinct eigenvalues be denoted 2 ,, with i taking on a value for each distinct eigen- value , and let ...
It will now be shown that A has at least as many linearly independent eigencolumns as it has distinct eigenvalues . Thus , let these distinct eigenvalues be denoted 2 ,, with i taking on a value for each distinct eigen- value , and let ...
Página 53
This extension is carried out as follows : Let u ; ( i = 1 , 2 , ... , n ) be a set of linearly independent vectors in an n - dimensional vector space . Any vector x may be written as2 X = n Συχ i = 1 ( 4.6 ) The set of vectors u ...
This extension is carried out as follows : Let u ; ( i = 1 , 2 , ... , n ) be a set of linearly independent vectors in an n - dimensional vector space . Any vector x may be written as2 X = n Συχ i = 1 ( 4.6 ) The set of vectors u ...
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Contenido
Solution for Diagonalizable Matrices | 21 |
The Evaluation of a Function of a Matrix for an Arbitrary Matrix | 38 |
13 | 44 |
Derechos de autor | |
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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