Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
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Página 49
... Transformation , " Dover Publications , New York , 1944 . Campbell , G. A. and R. M. Foster : " Fourier Integrals for Practical Applications , " D. Van Nostrand Company , Inc. , Princeton , N. J. , 1948 . Parodi , M .: “ Applications ...
... Transformation , " Dover Publications , New York , 1944 . Campbell , G. A. and R. M. Foster : " Fourier Integrals for Practical Applications , " D. Van Nostrand Company , Inc. , Princeton , N. J. , 1948 . Parodi , M .: “ Applications ...
Página 101
... transformation of a function ƒ into a function Fas given by a matrix S : or F ( v ) = √s ( v , x ) f ( x ) dx F = Sf The inverse transformation is given by a matrix T : or f ( x ) = ft ( x , y ) F ( v ) dy f = TF Substitution of ( 8.18 ) ...
... transformation of a function ƒ into a function Fas given by a matrix S : or F ( v ) = √s ( v , x ) f ( x ) dx F = Sf The inverse transformation is given by a matrix T : or f ( x ) = ft ( x , y ) F ( v ) dy f = TF Substitution of ( 8.18 ) ...
Página 267
... transformation to another basis , say the μ basis , the expression for > becomes | > = \ μ > < μ | λ2 > < 2 | > ( 2B.2 ) in which denotes the base kets and < u > is the transformation function for the change from the λ basis to the μ ...
... transformation to another basis , say the μ basis , the expression for > becomes | > = \ μ > < μ | λ2 > < 2 | > ( 2B.2 ) in which denotes the base kets and < u > is the transformation function for the change from the λ basis to the μ ...
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