From dyadic $\Lambda_{\alpha}$ to $\Lambda_{\alpha}$
| Autor: | Wael Abu-Shammala, Alberto Torchinsky |
|---|---|
| Jazyk: | angličtina |
| Rok vydání: | 2008 |
| Předmět: |
Polynomial
Mathematics::Functional Analysis Lipschitz class 42B30 42B35 General Mathematics Mathematics::Classical Analysis and ODEs Haar Hardy space Bounded mean oscillation Mathematics - Functional Analysis Combinatorics symbols.namesake Mathematics - Classical Analysis and ODEs symbols Maximal function Locally integrable function Affine transformation 42B30 Mathematics 42B35 |
| Zdroj: | Illinois J. Math. 52, no. 2 (2008), 681-689 |
| Popis: | In this paper we show how to compute the �� norm , �� 0, using the dyadic grid. This result is a consequence of the description of the Hardy spaces H p (R N ) in terms of dyadic and special atoms. Recently, several novel methods for computing the BMO norm of a function f in two dimensions were discussed in (9). Given its importance, it is also of interest to explore the possibility of computing the norm of a BMO function, or more generally a function in the Lipschitz class �α, using the dyadic grid in R N. It turns out that the BMO question is closely related to that of approximating functions in the Hardy space H 1 (R N ) by the Haar system. The approximation in H 1 (R N ) by affine systems was proved in (2), but this result does not apply to the Haar system. Now, if H A (R) denotes the closure of the Haar system in H 1 (R), it is not hard to see that the distance d(f, H A ) of f ∈ H 1 (R) to H A is ∼ � R ∞ 0 f(x) dx �, see (1). Thus, neither dyadic atoms suffice to describe the Hardy spaces, nor the evaluation of thenorm in BMO can be reduced to a straightforward computation using the dyadic intervals. In this paper we address both of these issues. First, we give a characterization of the Hardy spaces H p (R N ) in terms of dyadic and special atoms, and then, by a duality argument, we show how to compute the norm in �α(R N ), α ≥ 0, using the dyadic grid. We begin by introducing some notations. Let J denote a family of cubes Q in R N , and Pd the collection of polynomials in R N of degree less than or equal to d. Given α ≥ 0, Q ∈ J, and a locally integrable function g, let pQ(g) denote the unique polynomial in P(α) such that (g − pQ(g)) χQ has vanishing moments up to order (α). For a locally square-integrable function g, we consider the maximal function M ♯,2 α,J g(x) given by |
| Databáze: | OpenAIRE |
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