Untitled - Cdm.unimo.it
Untitled - Cdm.unimo.it
Untitled - Cdm.unimo.it
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124 Polynomial Approximation of Differential Equations<br />
w<strong>it</strong>h different techniques, shows a faster convergence behavior. Although the inequal<strong>it</strong>y<br />
(6.6.7) ensures the same kind of convergence, <strong>it</strong> requires f to be more regular. In<br />
nevai(1976) numerous extensions are provided, and in maday(1991) an estimate like<br />
(6.6.4) is proven for Legendre Gauss-Lobatto points.<br />
For analytic functions, the error estimates for the interpolation operator are expected<br />
to exhib<strong>it</strong> an exponential decay. Results in this direction are given in tadmor(1986)<br />
for Chebyshev expansions. Various improvements and estimates in different weighted<br />
spaces are considered in d<strong>it</strong>zian and totik(1987).<br />
To give an idea of the difficulties one may face when working w<strong>it</strong>h the interpolation<br />
operators, we note for instance that an inequal<strong>it</strong>y like (6.2.7) is not verified, when<br />
replacing Πw,n by Iw,n. This shows that the operator Iw,n is not continuous in<br />
the L2 w(I) norm, even if f ∈ C0 ( Ī). To check this fact, we construct a sequence of<br />
functions fk ∈ C0 (n)<br />
( Ī), k ∈ N, such that fk(ξ j ) = 1, 1 ≤ j ≤ n, ∀k ∈ N. Therefore,<br />
one has Iw,nfk ≡ 1, ∀k ∈ N, which implies that Iw,nfkL2 w (I) = 0 is constant w<strong>it</strong>h<br />
respect to k. On the other hand, every fk can be defined at the remaining points in<br />
such a way that limk→+∞ fk L 2 w (I) = 0. This is in contrast w<strong>it</strong>h the claim that Iw,n<br />
is continuous. Nevertheless, Iw,n is continuous in the norm of C0 ( Ī), i.e., for any n ≥ 1,<br />
we can find γ ≡ γ(n) such that<br />
(6.8.2) Iw,nf C 0 (Ī) ≤ γ f C 0 (Ī), ∀f ∈ C 0 ( Ī).<br />
In fact, for any f ∈ C0 ( Ī), (3.9.5) yields<br />
(6.8.3) Iw,nf C 0 (Ī) ≤ γ |||Iw,nf|||w,n = γ max<br />
1≤j≤n |f(ξ(n)<br />
j )| ≤ γ f C 0 (Ī).<br />
This is why the natural domain for Iw,n is the space of continuous functions. Unfor-<br />
tunately, the constant γ grows w<strong>it</strong>h n.<br />
* * * * * * * * * * * *<br />
W<strong>it</strong>h the conclusion of this chapter, we have finished the first part of the book. Having<br />
established the structure of the approximating functions we intend to use, as well as their<br />
properties, we now turn our efforts toward the discretization of derivative operators, and<br />
their associated problems.