Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
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Página 12
Gerald Goertzel, Nunzio Tralli. its elements along the main diagonal ( the elements I ) are unity and all others are zero ... element of x ; then multiply the second element from the left of z by the second element from the top of x ...
Gerald Goertzel, Nunzio Tralli. its elements along the main diagonal ( the elements I ) are unity and all others are zero ... element of x ; then multiply the second element from the left of z by the second element from the top of x ...
Página 246
... element of any row ( or column ) of a determinant is multiplied by a given number λ and added to ( or subtracted from ) the corresponding element of another row ( or column ) , the value of the determinant is un- changed . Apply ...
... element of any row ( or column ) of a determinant is multiplied by a given number λ and added to ( or subtracted from ) the corresponding element of another row ( or column ) , the value of the determinant is un- changed . Apply ...
Página 247
... element a ,, the lower right element in the new determinant . According to property II there have been ( ni ) + ( n − j ) changes of sign . It follows , therefore , that the coefficient of d , is the product of its minor by ( −1 ) 2n ...
... element a ,, the lower right element in the new determinant . According to property II there have been ( ni ) + ( n − j ) changes of sign . It follows , therefore , that the coefficient of d , is the product of its minor by ( −1 ) 2n ...
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