Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
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Página 109
... reduces to the conventional - Lf ( r ) = g ( r ) ( ordinary or partial ) differential equation D ( r ) f ( r ) = g ( r ) Similarly , the equation a f ( r , t ) = Lf ( r , t ) Ət a reduces to f ( r , t ) = D ( r ) f ( r , t ) Ət It is ...
... reduces to the conventional - Lf ( r ) = g ( r ) ( ordinary or partial ) differential equation D ( r ) f ( r ) = g ( r ) Similarly , the equation a f ( r , t ) = Lf ( r , t ) Ət a reduces to f ( r , t ) = D ( r ) f ( r , t ) Ət It is ...
Página 139
... reduces to and wx or eix = eir cos e = Σ infn , 1 n = -∞ + ∞0 eir cos e = Σ inJ ( r ) eino ( 10.40 ) n = -∞∞ By equating the real and imaginary parts of both sides of ( 10.40 ) it is found that and cos ( r cos 0 ) = Jo ( r ) + 2 Σ i ...
... reduces to and wx or eix = eir cos e = Σ infn , 1 n = -∞ + ∞0 eir cos e = Σ inJ ( r ) eino ( 10.40 ) n = -∞∞ By equating the real and imaginary parts of both sides of ( 10.40 ) it is found that and cos ( r cos 0 ) = Jo ( r ) + 2 Σ i ...
Página 205
... reduces to σ ( 8L ) f + L df = ( 82 ) £ ̧ + 2 , df One now seeks a left multiplier such that the terms - L df . — 2 , df = ( L — 2 ̧ ) df 。 are annihilated . Use gt such that and obtain or + g + ( L — 2 ) = 0 g + ( 8L ) f = g + ( 82 ) ...
... reduces to σ ( 8L ) f + L df = ( 82 ) £ ̧ + 2 , df One now seeks a left multiplier such that the terms - L df . — 2 , df = ( L — 2 ̧ ) df 。 are annihilated . Use gt such that and obtain or + g + ( L — 2 ) = 0 g + ( 8L ) f = g + ( 82 ) ...
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