Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
Dentro del libro
Resultados 1-3 de 17
Página 13
... differences all arise from the definition of the product of two matrices . The first difference to be considered is the noncommutativity of matrix multiplication . That is , there are matrices p and m such that mp #pm In fact , an ...
... differences all arise from the definition of the product of two matrices . The first difference to be considered is the noncommutativity of matrix multiplication . That is , there are matrices p and m such that mp #pm In fact , an ...
Página 80
... difference operator d2 with boundary conditions ( 6.9 ) and ( 6.10 ) has been intro- duced . i Such a procedure , of writing a difference equation y1 = Dx , and boundary conditions to eliminate auxiliary variables xo , x_1 , ... , etc ...
... difference operator d2 with boundary conditions ( 6.9 ) and ( 6.10 ) has been intro- duced . i Such a procedure , of writing a difference equation y1 = Dx , and boundary conditions to eliminate auxiliary variables xo , x_1 , ... , etc ...
Página 296
... Difference equation , 75 from variational principle , 239-241 Difference operator , 79-80 adjoint of , 80 Differential operator , 108-109 Differential scattering cross section , 184 Diffraction , order of , 196 Dirac , P. A. M. , 67 ...
... Difference equation , 75 from variational principle , 239-241 Difference operator , 79-80 adjoint of , 80 Differential operator , 108-109 Differential scattering cross section , 184 Diffraction , order of , 196 Dirac , P. A. M. , 67 ...
Contenido
Perturbation of Eigenvalues | 14 |
The Laplacian v2 in One Dimension | 18 |
Solution for Diagonalizable Matrices | 21 |
Derechos de autor | |
Otras 19 secciones no mostradas
Otras ediciones - Ver todas
Términos y frases comunes
approximate arbitrary ax² basis Bessel function boundary conditions chap coefficients column consider constant continuous systems contour coordinates corresponding cylindrical functions d²/dx² defined denoted determinant diagonal differential equation Dirac notation domain eigen eigencolumns eigenfunctions eigenvalue equation eigenvector eikr evaluate expansion finite number follows Fourier given Green's function Hence Hermitian Hermitian matrix Hermitian operator infinite integral inverse Laplace transform Laplacian linear operator linearly independent lowest eigenvalue matrix membrane method multiplication nonsingular normal obtained orthonormality conditions plane problem procedure relations representation result satisfies the boundary scattering sinh solve spherical spherical harmonics string Substitution theorem trial functions vanish variable vector space Verify wave write written y₁ yields York zero ηπχ πο ποχ ди ду дх