Orlicz-Hardy Spaces Associated with Divergence Operators on Unbounded Strongly Lipschitz Domains of Rn\mathbb{R}^n

preprint2012arXivOpen access

Abstract

Let ΩΩ be either Rn\mathbb{R}^n or an unbounded strongly Lipschitz domain of Rn\mathbb{R}^n, and ΦΦ be a continuous, strictly increasing, subadditive and positive function on (0,∞)(0,\infty) of upper type 1 and of strictly critical lower type pΦ∈(n/(n+1),1]p_Φ\in(n/(n+1),1]. Let LL be a divergence form elliptic operator on L2(Ω)L^2 (Ω) with the Neumann boundary condition and the heat semigroup generated by LL have the Gaussian property (G∞)(G_{\infty}). In this paper, the authors introduce the Orlicz-Hardy space HΦ, L(Ω)H_{Φ,\,L}(Ω) via the nontangential maximal function associated with {e−tL}t≥0\{e^{-t\sqrt{L}}\}_{t\ge0}, and establish its equivalent characterization in terms of the Lusin area function associated with {e−tL}t≥0\{e^{-t\sqrt{L}}\}_{t\ge0}. The authors also introduce the "geometrical" Orlicz-Hardy space HΦ, z(Ω)H_{Φ,\,z}(Ω) via the classical Orlicz-Hardy space HΦ(Rn)H_Φ(\mathbb{R}^n), and prove that the spaces HΦ, L(Ω)H_{Φ,\,L}(Ω) and HΦ, z(Ω)H_{Φ,\,z}(Ω) coincide with equivalent norms, from which, characterizations of HΦ, L(Ω)H_{Φ,\,L}(Ω), including the vertical and the nontangential maximal function characterizations associated with {e−tL}t≥0\{e^{-tL}\}_{t\ge0}, and the Lusin area function characterization associated with {e−tL}t≥0\{e^{-tL}\}_{t\ge0}, are deduced. All the above results generalize the well-known results of P. Auscher and E. Russ by taking Φ(t)≡tΦ(t)\equiv t for all t∈(0,∞)t\in(0,\infty).

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