Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
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Página 18
... introduce the concept of linear inde- pendence . A set of n columns is said to be linearly independent if there exists no linear combination of these columns which vanishes ; that is , the kn - columns m , are linearly independent if ...
... introduce the concept of linear inde- pendence . A set of n columns is said to be linearly independent if there exists no linear combination of these columns which vanishes ; that is , the kn - columns m , are linearly independent if ...
Página 53
... introduce the concept of a dual space : To each vector x in the space determined by the basis u , there corresponds a vector x + in the dual space determined by the basis ut such that + X n - Σxu == i = 1 + where x , is the complex ...
... introduce the concept of a dual space : To each vector x in the space determined by the basis u , there corresponds a vector x + in the dual space determined by the basis ut such that + X n - Σxu == i = 1 + where x , is the complex ...
Página 243
... introduce the with the understanding that this is an abbreviation and that the value of [ A ] is obtained by evaluating the sum | A | = where € 12 - 1 , E21 = —1 , and € 11 & , 91,925 = 822 == 0. A = lal is called the determinant of the ...
... introduce the with the understanding that this is an abbreviation and that the value of [ A ] is obtained by evaluating the sum | A | = where € 12 - 1 , E21 = —1 , and € 11 & , 91,925 = 822 == 0. A = lal is called the determinant of the ...
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