Sobolev spaces and trace theorem on the Sierpinski gasket

preprint2020arXivOpen access

Abstract

On the Sierpinski gasket SG\mathcal{SG}, we consider Sobolev spaces Lσ2(SG)L^2_σ(\mathcal{SG}) associated with the standard Laplacian ΔΔ with order σ≥0σ\geq 0. When σ∈Z+σ\in\mathbb{Z}^+, Lσ2(SG)L^2_σ(\mathcal{SG}) consists of functions equipped with L2L^2 norms of the function itself and its Laplacians up to σσ order; when σ∉Z+σ\notin \mathbb{Z}^+, we fill up the gaps between integer orders by using complex interpolation. Let Lσ,D2(SG)=(I−ΔD)−σL2(SG)L^2_{σ, D}(\mathcal{SG})=(I-Δ_D)^{-σ}L^2(\mathcal{SG}) where ΔDΔ_D is the Dirichlet Laplacian associated with ΔΔ. Let {pn}n≥0\{p_n\}_{n\geq 0} be a collection of countably many points located along one of the symmetrical axes of SG\mathcal{SG}. We make a full characterization of the trace spaces of Lσ2(SG)L^2_σ(\mathcal{SG}) and Lσ,D2(SG)L^2_{σ,D}(\mathcal{SG}) to {pn}n≥0\{p_n\}_{n\geq 0}. Using this, we get a full description of the relationship between Lσ2(SG)L^2_σ(\mathcal{SG}) and Lσ,D2(SG)L^2_{σ,D}(\mathcal{SG}) for σ≥0σ\geq 0. The result indicates that when σ−log⁡32log⁡5∈Z+σ-\frac{\log 3}{2\log5}\in \mathbb{Z}^+, Lσ,D2(SG)L^2_{σ, D}(\mathcal{SG}) is not closed in Lσ2(SG)L^2_σ(\mathcal{SG}) and has an infinite codimension. Otherwise, Lσ,D2(SG)L^2_{σ, D}(\mathcal{SG}) is closed in Lσ2(SG)L^2_σ(\mathcal{SG}) with a finite codimension. Similar result holds for the Neumann case. Another consequence of the trace result is that the Sobolev spaces Lσ2(SG)L^2_σ(\mathcal{SG}) are stable under complex interpolation for σ≥0σ\geq 0 although they are defined by piecewise interpolation between integer orders.

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