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31: 35.7 Gaussian Hypergeometric Function of Matrix Argument
Case m = 2
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 . …
32: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
Self-Adjoint and Symmetric Operators
§1.18(vii) Continuous Spectra: More General Cases
A linear operator T with dense domain is called symmetric if …
Self-adjoint extensions of a symmetric Operator
By Weyl’s alternative n 1 equals either 1 (the limit point case) or 2 (the limit circle case), and similarly for n 2 . …
33: 3.1 Arithmetics and Error Measures
In the case of the normalized binary interchange formats, the representation of data for binary32 (previously single precision) ( N = 32 , p = 24 , E min = 126 , E max = 127 ), binary64 (previously double precision) ( N = 64 , p = 53 , E min = 1022 , E max = 1023 ) and binary128 (previously quad precision) ( N = 128 , p = 113 , E min = 16382 , E max = 16383 ) are as in Figure 3.1.1. …
Rounding
Symmetric rounding or rounding to nearest of x gives x or x + , whichever is nearer to x , with maximum relative error equal to the machine precision 1 2 ϵ M = 2 p . … Also in this arithmetic generalized precision can be defined, which includes absolute error and relative precision (§3.1(v)) as special cases. …
34: 21.7 Riemann Surfaces
In contrast, a g -dimensional Riemann theta function arising from a compact Riemann surface of genus g ( > 1 ) depends on at most 3 g 3 complex parameters (one complex parameter for the case g = 1 ). … Fay derives (21.7.10) as a special case of a more general class of addition theorems for Riemann theta functions on Riemann surfaces. …
21.7.12 T 1 T 2 = ( T 1 T 2 ) ( T 1 T 2 ) .
21.7.14 𝜼 ( T 1 T 2 ) = 𝜼 ( T 1 ) + 𝜼 ( T 2 ) ,
21.7.15 4 𝜼 1 ( T ) 𝜼 2 ( T ) = 1 2 ( | T U | g 1 ) ( mod 2 ) ,
35: 21.5 Modular Transformations
( 𝐁 symmetric with integer elements and even diagonal elements.) …( 𝐁 symmetric with integer elements.) … For explicit results in the case g = 1 , see §20.7(viii).
36: 2.6 Distributional Methods
2.6.6 S ( x ) 2 π 3 s = 0 ( 1 ) s ( 1 3 s ) x s ( 1 / 3 ) , x .
Similarly, in the case α = 1 , we define …In either case, we define the distribution associated with f n ( t ) by …
2.6.32 0 f ( t ) ( t + z ) ρ d t , ρ > 0 ,
An application has been given by López (2000) to derive asymptotic expansions of standard symmetric elliptic integrals, complete with error bounds; see §19.27(vi). …
37: 3.5 Quadrature
When f C , the Romberg method affords a means of obtaining high accuracy in many cases with a relatively simple adaptive algorithm. … The Gauss nodes x k (the zeros of p n ) are the eigenvalues of the (symmetric tridiagonal) Jacobi matrix of order n × n : … For these cases the integration path may need to be deformed; see §3.5(ix). … The integrand can be extended as a periodic C function on with period 2 π and as noted in §3.5(i), the trapezoidal rule is exceptionally efficient in this case. … A special case is the rule for Hilbert transforms (§1.14(v)): …
38: 19.3 Graphics
See accompanying text
Figure 19.3.6: Π ( ϕ , 2 , k ) as a function of k 2 and sin 2 ϕ for 1 k 2 3 , 0 sin 2 ϕ < 1 . …The function tends to + as sin 2 ϕ 1 2 , except in the last case below. … Magnify 3D Help
See accompanying text
Figure 19.3.9: ( K ( k ) ) as a function of complex k 2 for 2 ( k 2 ) 2 , 2 ( k 2 ) 2 . The real part is symmetric under reflection in the real axis. … Magnify 3D Help
See accompanying text
Figure 19.3.11: ( E ( k ) ) as a function of complex k 2 for 2 ( k 2 ) 2 , 2 ( k 2 ) 2 . The real part is symmetric under reflection in the real axis. … Magnify 3D Help
39: 1.2 Elementary Algebra
Special cases are the Euclidean length or l 2 norma real symmetric matrix if …
40: 18.28 Askey–Wilson Class
The Askey–Wilson class OP’s comprise the four-parameter families of Askey–Wilson polynomials and of q -Racah polynomials, and cases of these families obtained by specialization of parameters. … y ) such that P n ( z ) = p n ( 1 2 ( z + z 1 ) ) in the Askey–Wilson case, and P n ( y ) = p n ( q y + c q y + 1 ) in the q -Racah case, and both are eigenfunctions of a second order q -difference operator similar to (18.27.1). … The polynomials p n ( x ; a , b , c , d | q ) are symmetric in the parameters a , b , c , d . … For further nondegenerate cases see Chihara and Ismail (1993) and Christiansen and Ismail (2006). … These systems are the q -Racah polynomials and its limit cases. …