Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
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Página 20
... Verify the distributive law 15. Verify that ( MN ) P MP + NP = ( AB ) T = BTAT 16. Show that if M = AA " , then M = MT and hence Mis a symmetric matrix . 17. Show that a nonsquare matrix cannot have an inverse . 18. Verify that the ...
... Verify the distributive law 15. Verify that ( MN ) P MP + NP = ( AB ) T = BTAT 16. Show that if M = AA " , then M = MT and hence Mis a symmetric matrix . 17. Show that a nonsquare matrix cannot have an inverse . 18. Verify that the ...
Página 123
... verify completeness one must show that + Σ $ „ ( x ) S „ ( x ' ) = d ( x − x ' ) 0 < x , x ' < L ( 9.49 ) n = 1 ... verified . The result 1 + ∞o Σ ei ( 2xn / L ) ( x − x ' ) = d ( x − x ' ) 0 < x , x ' < L ( 9.49a ) L n = -∞o is ...
... verify completeness one must show that + Σ $ „ ( x ) S „ ( x ' ) = d ( x − x ' ) 0 < x , x ' < L ( 9.49 ) n = 1 ... verified . The result 1 + ∞o Σ ei ( 2xn / L ) ( x − x ' ) = d ( x − x ' ) 0 < x , x ' < L ( 9.49a ) L n = -∞o is ...
Página 276
Gerald Goertzel, Nunzio Tralli. The verification of ( 2B.43 ) has been carried out in Sec . 10.5 of the text . The verification of ( 2B.44 ) is left as an exercise for the reader . - Let < r , 0 > = f ( r , 0 ) and < k , n | > = g ( k ) ...
Gerald Goertzel, Nunzio Tralli. The verification of ( 2B.43 ) has been carried out in Sec . 10.5 of the text . The verification of ( 2B.44 ) is left as an exercise for the reader . - Let < r , 0 > = f ( r , 0 ) and < k , n | > = g ( k ) ...
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