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Lanczos tridiagonalization of a symmetric matrix

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1: 35.1 Special Notation
a , b complex variables.
𝐙 complex symmetric matrix.
The main functions treated in this chapter are the multivariate gamma and beta functions, respectively Γ m ( a ) and B m ( a , b ) , and the special functions of matrix argument: Bessel (of the first kind) A ν ( 𝐓 ) and (of the second kind) B ν ( 𝐓 ) ; confluent hypergeometric (of the first kind) F 1 1 ( a ; b ; 𝐓 ) or F 1 1 ( a b ; 𝐓 ) and (of the second kind) Ψ ( a ; b ; 𝐓 ) ; Gaussian hypergeometric F 1 2 ( a 1 , a 2 ; b ; 𝐓 ) or F 1 2 ( a 1 , a 2 b ; 𝐓 ) ; generalized hypergeometric F q p ( a 1 , , a p ; b 1 , , b q ; 𝐓 ) or F q p ( a 1 , , a p b 1 , , b q ; 𝐓 ) . An alternative notation for the multivariate gamma function is Π m ( a ) = Γ m ( a + 1 2 ( m + 1 ) ) (Herz (1955, p. 480)). Related notations for the Bessel functions are 𝒥 ν + 1 2 ( m + 1 ) ( 𝐓 ) = A ν ( 𝐓 ) / A ν ( 𝟎 ) (Faraut and Korányi (1994, pp. 320–329)), K m ( 0 , , 0 , ν | 𝐒 , 𝐓 ) = | 𝐓 | ν B ν ( 𝐒 𝐓 ) (Terras (1988, pp. 49–64)), and 𝒦 ν ( 𝐓 ) = | 𝐓 | ν B ν ( 𝐒 𝐓 ) (Faraut and Korányi (1994, pp. 357–358)).
2: 35.5 Bessel Functions of Matrix Argument
§35.5 Bessel Functions of Matrix Argument
§35.5(i) Definitions
§35.5(ii) Properties
§35.5(iii) Asymptotic Approximations
For asymptotic approximations for Bessel functions of matrix argument, see Herz (1955) and Butler and Wood (2003).
3: 35.6 Confluent Hypergeometric Functions of Matrix Argument
§35.6 Confluent Hypergeometric Functions of Matrix Argument
§35.6(i) Definitions
Laguerre Form
§35.6(ii) Properties
§35.6(iii) Relations to Bessel Functions of Matrix Argument
4: 35.8 Generalized Hypergeometric Functions of Matrix Argument
§35.8 Generalized Hypergeometric Functions of Matrix Argument
§35.8(i) Definition
The generalized hypergeometric function F q p with matrix argument 𝐓 𝓢 , numerator parameters a 1 , , a p , and denominator parameters b 1 , , b q is …
Convergence Properties
A similar result for the F 1 0 function of matrix argument is given in Faraut and Korányi (1994, p. 346). …
5: 35.7 Gaussian Hypergeometric Function of Matrix Argument
§35.7 Gaussian Hypergeometric Function of Matrix Argument
§35.7(i) Definition
Jacobi Form
Let f : 𝛀 (a) be orthogonally invariant, so that f ( 𝐓 ) is a symmetric function of t 1 , , t m , the eigenvalues of the matrix argument 𝐓 𝛀 ; (b) be analytic in t 1 , , t m in a neighborhood of 𝐓 = 𝟎 ; (c) satisfy f ( 𝟎 ) = 1 . Subject to the conditions (a)–(c), the function f ( 𝐓 ) = F 1 2 ( a , b ; c ; 𝐓 ) is the unique solution of each partial differential equation …
6: 19.16 Definitions
§19.16(i) Symmetric Integrals
A fourth integral that is symmetric in only two variables is defined by … which is homogeneous and of degree a in the z ’s, and unchanged when the same permutation is applied to both sets of subscripts 1 , , n . … …
§19.16(iii) Various Cases of R a ( 𝐛 ; 𝐳 )
7: 3.2 Linear Algebra
§3.2(ii) Gaussian Elimination for a Tridiagonal Matrix
§3.2(vi) Lanczos Tridiagonalization of a Symmetric Matrix
Define the Lanczos vectors 𝐯 j and coefficients α j and β j by 𝐯 0 = 𝟎 , a normalized vector 𝐯 1 (perhaps chosen randomly), α 1 = 𝐯 1 T 𝐀 𝐯 1 , β 1 = 0 , and for j = 1 , 2 , , n 1 by the recursive scheme …The tridiagonal matrixLanczos’ method is related to Gauss quadrature considered in §3.5(v). …
8: 1.2 Elementary Algebra
A matrix 𝐀 is: a diagonal matrix if …a real symmetric matrix if …a tridiagonal matrix if … Equation (3.2.7) displays a tridiagonal matrix in index form; (3.2.4) does the same for a lower triangular matrix. …
9: 30.16 Methods of Computation
For d sufficiently large, construct the d × d tridiagonal matrix 𝐀 = [ A j , k ] with nonzero elements …The eigenvalues of 𝐀 can be computed by methods indicated in §§3.2(vi), 3.2(vii). … The coefficients a n , r m ( γ 2 ) are computed as the recessive solution of (30.8.4) (§3.6), and normalized via (30.8.5). A fourth method, based on the expansion (30.8.1), is as follows. Let 𝐀 be the d × d matrix given by (30.16.1) if n m is even, or by (30.16.6) if n m is odd. …
10: 31.5 Solutions Analytic at Three Singularities: Heun Polynomials
Let α = n , n = 0 , 1 , 2 , , and q n , m , m = 0 , 1 , , n , be the eigenvalues of the tridiagonal matrix
31.5.1 [ 0 a γ 0 0 P 1 Q 1 R 1 0 0 P 2 Q 2 R n 1 0 0 P n Q n ] ,
31.5.2 𝐻𝑝 n , m ( a , q n , m ; n , β , γ , δ ; z ) = H ( a , q n , m ; n , β , γ , δ ; z )
is a polynomial of degree n , and hence a solution of (31.2.1) that is analytic at all three finite singularities 0 , 1 , a . …