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Optimal quadratures for analytic functions
Authors:M M Chawla  B L Raina
Institution:(1) Department of Mathematics, Indian Institute of Technology, Hauz Khas, New Delhi-29, India
Abstract:For integralsint –1 1 w(x)f(x)dx with 
$$w(x) = (1 - x)^{ \pm \tfrac{1}{2}} (1 + x)^{ \pm \tfrac{1}{2}} $$
and with analytic integrands, we consider the determination of ldquooptimalrdquo abscissasx i o and weightsA i o , for a fixedn, which minimize the errorE n (f)=int –1 1 w(x)f(x)dxSgr i =1n A i f(x i ) over an appropriate Hilbert spaceH 2(E rgr ; midw(z)mid) of analytic functions. Simultaneously, we consider the simpler problem of determining ldquointermediate-optimalrdquo weightsA i *, corresponding to (preassigned) Gaussian abscissasx i G , which minimize the quadrature error. For eachw(x), the intermediate-optimal weightsA i * are obtained explicitly, and these come out proportional to the corresponding Gaussian weightsA i G . In each case,A i G =A i *+O(rhov –4n ),rhov rarr infin. For 
$$w(x) = (1 - x^2 )^{ \pm \tfrac{1}{2}} $$
, a complete explicit solution for optimal abscissas and weights is given; in fact, the set {x i G ,A i *;i=1,...,n} to provides the optimal abscissas and weights. For otherw(x), we study the closeness of the set {x i G ,A i *;i=1,...,n} to the optimal solution {x i o ,A i o ;i=1,...,n} in terms ofepsi n (rhov), the maximum absolute remainder in the second set ofn normal equations. In each case,epsi n (rhov) is, at least, of the order ofrhov –4n for largerhov.
Keywords:
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