Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
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Página 191
... replaced by since 1 [ d d x + 1 ) + ] r2 dr 7.2 dr 2 + k2 fi , out = u ( r ) fi ( 13.66 ) 7.2 +2 k2 ] . + kafi , inc = 0 d d 1 ( 1 + 1 ) Lr2 dr dr The Then , replacing f , in the right - hand member of ( 13.66 ) by fi , inc = ji ( kr ) ...
... replaced by since 1 [ d d x + 1 ) + ] r2 dr 7.2 dr 2 + k2 fi , out = u ( r ) fi ( 13.66 ) 7.2 +2 k2 ] . + kafi , inc = 0 d d 1 ( 1 + 1 ) Lr2 dr dr The Then , replacing f , in the right - hand member of ( 13.66 ) by fi , inc = ji ( kr ) ...
Página 228
... replaced by the problem L ̄1y = λ ̄1y -1 ( 16.8 ) Clearly , the largest eigenvalue of L - 1 to which the iteration method con- verges yields the lowest eigenvalue of L. Unfortunately , the labor of inverting in the case of discrete ...
... replaced by the problem L ̄1y = λ ̄1y -1 ( 16.8 ) Clearly , the largest eigenvalue of L - 1 to which the iteration method con- verges yields the lowest eigenvalue of L. Unfortunately , the labor of inverting in the case of discrete ...
Página 282
... the direction of the real axis , in which the plus and minus signs are for the upper and lower half planes . In the convergence considerations sin § is replaced by sin ( 8 ) . Since a change of 2 " in the path of 282 APPENDIX 2c.
... the direction of the real axis , in which the plus and minus signs are for the upper and lower half planes . In the convergence considerations sin § is replaced by sin ( 8 ) . Since a change of 2 " in the path of 282 APPENDIX 2c.
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