Torsion functions and the Cheeger problem: a fractional approach

preprint2020arXivOpen access

Abstract

Let ΩΩ be a Lipschitz bounded domain of RN\mathbb{R}^N , N≥2N\geq2. The fractional Cheeger constant hs(Ω)h_s (Ω), 0<s<10<s<1, is defined by hs(Ω)=inf⁡E⊂ΩPs(E)∣E∣,  where  Ps(E)=∫RN∫RN∣χE(x)−χE(y)∣∣x−y∣N+sdxdy,h_s(Ω)=\inf_{E\subsetΩ}\frac{P_s(E)}{|E|},\: \text{ where } \: P_s (E)=\int_{\mathbb{R}^N }\int_{\mathbb{R}^N }\frac{|χ_{E}(x)-χ_{E}(y)|}{|x-y|^{N+s}} dx dy, with χEχ_{E} denoting the characteristic function of the smooth subdomain EE. The main purpose of this paper is to show that lim⁡p→1+∣ϕps∣L∞(Ω)1−p=hs(Ω)=lim⁡p→1+∣ϕps∣L1(Ω)1−p,\lim_{p\rightarrow1^+}\left|ϕ_p^s\right|_{L^{\infty}(Ω)}^{1-p}=h_s (Ω)=\lim_{p\rightarrow1^+}\left|ϕ_p^s\right|_{L^1(Ω)}^{1-p}, where ϕpsϕ_p^s is the fractional (s,p)(s,p)-torsion function of ΩΩ, that is, the solution of the Dirichlet problem for the fractional pp-Laplacian: −(Δ)ps u=1-(Δ)_p^s\,u=1 in ΩΩ, u=0u=0 in RN∖Ω\mathbb{R}^N \setminusΩ. For this, we derive suitable bounds for the first eigenvalue λ1,ps(Ω)λ_{1,p}^s(Ω) of the fractional pp-Laplacian operator in terms of ϕpsϕ_p^s. We also show that ϕpsϕ_p^s minimizes the (s,p)(s,p)-Gagliardo seminorm in RN\mathbb{R}^N , among the functions normalized by the L1L^1-norm.

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