Some Mathematical Methods of Physics |
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It is clear that if f ( A ) is a known matrix , the value of f ( A ) u is known for arbitrary u , since the indicated multiplication can be carried out . Simi- larly , if the value of f ( A ) u is known for arbitrary u , f ( A ) may be ...
It is clear that if f ( A ) is a known matrix , the value of f ( A ) u is known for arbitrary u , since the indicated multiplication can be carried out . Simi- larly , if the value of f ( A ) u is known for arbitrary u , f ( A ) may be ...
Página 57
... 4.4 Linear Operators An operator L , in a vector space , is an entity which , acting upon an arbitrary vector x , converts it into a vector y : y = Lx ( 4.15 ) L is a known operator if and only if , given x , y is determined .
... 4.4 Linear Operators An operator L , in a vector space , is an entity which , acting upon an arbitrary vector x , converts it into a vector y : y = Lx ( 4.15 ) L is a known operator if and only if , given x , y is determined .
Página 257
One type of singularity is known as a branch point . By definition , a point z = a is a branch point of f ( z ) if f ( z ) fails to return to its original value when z moves around « in a circle of arbitrarily small ( nonzero ) radius .
One type of singularity is known as a branch point . By definition , a point z = a is a branch point of f ( z ) if f ( z ) fails to return to its original value when z moves around « in a circle of arbitrarily small ( nonzero ) radius .
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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 |
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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