Some Mathematical Methods of Physics |
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Página 9
To illustrate the method of writing the equations of motion suggested by the matrix notation , Eqs . ( 1.6 ) are ... it is desirable to introduce a notation which enables one to write the required relations in concise and clear form .
To illustrate the method of writing the equations of motion suggested by the matrix notation , Eqs . ( 1.6 ) are ... it is desirable to introduce a notation which enables one to write the required relations in concise and clear form .
Página 80
If M M + , one can write D = D + , BC BC + , and vice versa . ... The equation y + Mx - ( M + y ) + x = 0 for arbitrary x and y may be considered a definition of M + , as is seen by writing the equation in detailed form = 0 = ΣΜ - ΣΜήνα ...
If M M + , one can write D = D + , BC BC + , and vice versa . ... The equation y + Mx - ( M + y ) + x = 0 for arbitrary x and y may be considered a definition of M + , as is seen by writing the equation in detailed form = 0 = ΣΜ - ΣΜήνα ...
Página 177
For example , one might write in place of Eq . ( 13.1 ) c2V2 - a 2 3 ] 4 ′ ( x , 1 ) = c2S ( 1,1 ) ( ~ 212 + n ) 3 ] ¥ ( x , 1 ) where n > 0. A solution of ( 13.4 ) is , for large r , η r ¥ ~ [ e ̄ ( nr / c ) ƒ1 ( r — ct ) + e ‹ nr / c ) ...
For example , one might write in place of Eq . ( 13.1 ) c2V2 - a 2 3 ] 4 ′ ( x , 1 ) = c2S ( 1,1 ) ( ~ 212 + n ) 3 ] ¥ ( x , 1 ) where n > 0. A solution of ( 13.4 ) is , for large r , η r ¥ ~ [ e ̄ ( nr / c ) ƒ1 ( r — ct ) + e ‹ nr / c ) ...
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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 |
Derechos de autor | |
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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