Some Mathematical Methods of PhysicsMcGraw-Hill, 1960 - 300 páginas |
Dentro del libro
Resultados 1-3 de 34
Página 7
... called the elements of the matrix m . For the purpose of display of the matrix m one writes mil m12 m13 Min M2n M21 ... called a diagonal matrix . = = m11 , i ‡ j , is called FORMULATION OF THE PROBLEM AND DEVELOPMENT OF NOTATION 7.
... called the elements of the matrix m . For the purpose of display of the matrix m one writes mil m12 m13 Min M2n M21 ... called a diagonal matrix . = = m11 , i ‡ j , is called FORMULATION OF THE PROBLEM AND DEVELOPMENT OF NOTATION 7.
Página 67
... called base ket vectors , or simply base kets . The base vectors in the dual space , ut , are called base bra vectors , or base bras , and are denoted by < il , the mirror image of the symbol for the base kets . Using the convention ...
... called base ket vectors , or simply base kets . The base vectors in the dual space , ut , are called base bra vectors , or base bras , and are denoted by < il , the mirror image of the symbol for the base kets . Using the convention ...
Página 92
... called the ( finite ) Fourier sine transform of g ( x ) , and g ( x ) is called the inverse transform of G .. To evaluate f ( d2 / dx2 ) g ( x ) one may use the transform of g ( x ) . Thus , from ( 7.17 ) f ( d2 / dx2 ) g ( x ) = £ ƒ ...
... called the ( finite ) Fourier sine transform of g ( x ) , and g ( x ) is called the inverse transform of G .. To evaluate f ( d2 / dx2 ) g ( x ) one may use the transform of g ( x ) . Thus , from ( 7.17 ) f ( d2 / dx2 ) g ( x ) = £ ƒ ...
Contenido
34 | 12 |
The Laplacian V² in One Dimension | 18 |
Solution for Diagonalizable Matrices | 21 |
Derechos de autor | |
Otras 31 secciones no mostradas
Otras ediciones - Ver todas
Términos y frases comunes
approximate arbitrary asymptotic ax² base vectors basis Bessel functions boundary conditions Chap coefficients consider constant continuous systems contour corresponding cylindrical functions d²/dx² defined definition denoted determinant diagonal diagonalizable differential equation Dirac notation eigen eigencolumns eigenfunctions eigenvalue problem eigenvectors elements evaluate expansion finite number follows formula given Green's function Hence Hermitian matrix Hermitian operator infinite integral representation integral theorem inverse Laplace transform linear operator linearly independent lowest eigenvalue matrix McGraw-Hill Book Company method multiplication nonsingular normal matrix obtained orthonormality conditions perturbation procedure relations result Ritz method satisfies scattering sinh solution solve spherical substitution transformation functions trial functions vanish variable vector space Verify wave whence write written x₁ y₁ yields York zero ηπχ παχ ди ду дх