Quantitative bounds on rates of approximation by linear combinations of Heaviside plane waves are obtained for sufficiently differentiable functions f which vanish rapidly enough at infinity: for d odd and f ∈ Cd(Rd), with lower-order partials vanishing at infinity and dth-order partials vanishing as x −(d+1+ε), ε > 0, on any domain ⊂ Rd with unit Lebesgue measure, the L2( )-error in approximating f by a linear combination of n Heaviside plane waves is bounded above by kd f d,1,∞n−1/2, where kd ∼ ( d)1/2(e/2 )d/2 and f d,1,∞ is the Sobolev seminorm determined by the largest of the L1-norms of the dth-order partials of f on Rd. In particular, for d odd and f (x)=exp(− x 2), the L2( )-approximation error is at most (2 d)3/4n−1/2 and the sup-norm approximation error on Rd is at most 68 √ 2(n−1)−1/2(2 d)3/4 √ d + 1, n 2. © 2007 Published by Elsevier Inc.
Paul C. Kainen, Vera Kurková, Andrew Vogt