Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
Dentro del libro
Resultados 1-3 de 13
Página v
... theory , and reactor physics . In an attempt to develop this background in one coherent manner , rather than have it appear in bits and pieces in various courses , one of us introduced and taught a graduate course , entitled ...
... theory , and reactor physics . In an attempt to develop this background in one coherent manner , rather than have it appear in bits and pieces in various courses , one of us introduced and taught a graduate course , entitled ...
Página 38
... theory.1 f ( A ) = 1 f ( Z ) dz 2πi Jc Z A ( 3.1 ) This formula may be applied to matrices2 as well as to numbers , provided the contour C encloses all eigenvalues of A and no singularities of f ( Z ) . A proof is indicated in Sec . 3.3 ...
... theory.1 f ( A ) = 1 f ( Z ) dz 2πi Jc Z A ( 3.1 ) This formula may be applied to matrices2 as well as to numbers , provided the contour C encloses all eigenvalues of A and no singularities of f ( Z ) . A proof is indicated in Sec . 3.3 ...
Página 209
... theory , starting with the unloaded string . 5. Use perturbation theory to evaluate the eigenvalues of the matrix 21 α 0 0 α 22 B 0 Ο β3 γ 0 0 γλ assuming α , ẞ , and y are small . = M References Schiff , L. I .: " Quantum Mechanics ...
... theory , starting with the unloaded string . 5. Use perturbation theory to evaluate the eigenvalues of the matrix 21 α 0 0 α 22 B 0 Ο β3 γ 0 0 γλ assuming α , ẞ , and y are small . = M References Schiff , L. I .: " Quantum Mechanics ...
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