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Untitled - Cdm.unimo.it

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122 Polynomial Approximation of Differential Equations<br />

Taking into account lemma 6.7.4, theorems 6.2.6 and 6.3.5 are respectively generalized<br />

to the case of Herm<strong>it</strong>e functions as follows.<br />

Theorem 6.7.5 - Let k ∈ N, then there exists a constant C > 0 such that, for any<br />

g ∈ H k v (R), one has<br />

(6.7.9) g − Π ∗ v,ng L 2 v (R) ≤ C<br />

k 1<br />

√n<br />

g H k v (R), ∀n > k.<br />

Theorem 6.7.6 - We can find a constant C > 0 such that, for any n ≥ 1<br />

(6.7.10) q ′ L 2 w (R) ≤ C √ n q L 2 w (R), ∀q ∈ Sn.<br />

We finally define I ∗ v,n : C 0 (R) → Sn−1, n ≥ 1, such that<br />

(6.7.11) I ∗ v,n := [Iw,n(gv)]w, ∀g ∈ C 0 (R).<br />

A theoretical convergence analysis for the operator I ∗ v,n for n → +∞ is considered in<br />

funaro and kavian(1988). Here we state the main result (we recall that the Sobolev<br />

spaces w<strong>it</strong>h real exponent have been introduced in section 5.6).<br />

Theorem 6.7.7 - Let ǫ > 0 and s ≥ 1 + ǫ. Then there exists a constant C > 0 such<br />

that, for any g ∈ H s v(R), we have<br />

(6.7.12) g − I ∗ v,ng L 2 v (R) ≤ C<br />

s−1−ǫ 1<br />

√n gHs v (R), ∀n ≥ 1.<br />

Other results, concerning the rate of convergence of the so called normalized Herm<strong>it</strong>e<br />

functions, are provided in boyd(1984).

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