[Paper Review] Symmetry and linear stability in Serrin's overdetermined problem via the stability of the parallel surface problem
This paper establishes optimal linear stability for Serrin's overdetermined problem by linking it to the stability of the parallel surface problem. Using a novel strategy based on Lipschitz regularity estimates on parallel surfaces, the authors prove that if the normal derivative is constant on the boundary, the domain must be a ball, and provide a sharp linear stability estimate in $C^{2, au}$ domains.
We consider the solution of the problem $$ -Δu=f(u) \ \mbox{ and } \ u>0 \ \ \mbox{ in } \ Ω, \ \ u=0 \ \mbox{ on } \ Γ, $$ where $Ω$ is a bounded domain in $\mathbb{R}^N$ with boundary $Γ$ of class $C^{2,τ}$, $00$, where $r_e$ and $r_i$ are the radii of a spherical annulus containing $Γ$, $Γ^δ$ is a surface parallel to $Γ$ at distance $δ$ and sufficiently close to $Γ$, and $[u]_{Γ^δ}$ is the Lipschitz semi-norm of $u$ on $Γ^δ$; secondly, if in addition $u_ν$ is constant on $Γ$, show that $$ [u]_{Γ^δ}=o(C_δ)\ \mbox{ as } \ δ o 0^+. $$ In this paper, we prove that this strategy is successful. As a by-product of this method, for $C^{2,τ}$-regular domains, we also obtain a linear stability estimate for Serrin's symmetry result. Our result is optimal and greatly improves the similar logarithmic-type estimate of [ABR] and the Hölder estimate of [CMV] that was restricted to convex domains.
Motivation & Objective
- To resolve a conjecture in [CMS2] that Serrin’s symmetry theorem can be derived via stability of the parallel surface problem.
- To establish a linear stability estimate for Serrin’s overdetermined problem in $C^{2, au}$-regular domains.
- To improve upon prior logarithmic and H"older-type stability estimates by achieving optimal linear bounds.
- To connect the stability of the parallel surface problem to the symmetry and stability of Serrin’s problem through geometric and analytic techniques.
Proposed method
- Derive a Lipschitz regularity estimate for the solution $u$ on a parallel surface $\Gamma^\delta$ at distance $\delta$ from $\Gamma$, using Taylor expansion and curvature bounds.
- Establish the key inequality (5.1) relating the Lipschitz seminorm $[u]_{\Gamma^\delta}$ to the seminorms of $u_\nu$ and $u_{\nu\nu}$ on $\Gamma$ and $\Gamma^t$.
- Use the $C^{2,\tau}$ regularity of $u$ to control the decay of $[u_{\nu\nu}]_{\Gamma^t}$ as $t \to 0^+$, ensuring integrability.
- Apply Theorem 4.2 on parallel surface stability to derive a quantitative annular containment $B_{r_i} \subset \Omega \subset B_{r_e}$ with $r_e - r_i$ bounded by an integral of $[u_{\nu\nu}]_{\Gamma^t}$.
- Pass to the limit as $\delta \to 0^+$ to obtain the linear stability estimate $r_e - r_i \leq 2C [u_\nu]_\Gamma$.
- Leverage the fact that $[u_{\nu\nu}]_{\Gamma^t} = O(t^{\tau-1})$ to ensure the integral vanishes in the limit, yielding symmetry when $u_\nu$ is constant.
Experimental results
Research questions
- RQ1Can Serrin’s symmetry theorem be derived via a stability argument based on the parallel surface problem?
- RQ2What is the optimal quantitative stability estimate for Serrin’s overdetermined problem in $C^{2,\tau}$ domains?
- RQ3How does the Lipschitz regularity of $u$ on parallel surfaces $\Gamma^\delta$ control the geometry of $\Omega$?
- RQ4Can the stability estimate be improved beyond logarithmic or H"older-type bounds to achieve linear stability?
- RQ5What role does the $C^{2,\tau}$ regularity of $u$ play in the decay of $[u_{\nu\nu}]_{\Gamma^t}$ as $t \to 0^+$?
Key findings
- The authors confirm the conjecture in [CMS2] that Serrin’s symmetry result can be derived via stability of the parallel surface problem.
- A sharp linear stability estimate is established: $r_e - r_i \leq 2C [u_\nu]_\Gamma$, where $C$ is a universal constant depending only on $N$ and $\tau$.
- The stability estimate is optimal and improves upon the logarithmic estimate in [ABR] and the H"older estimate in [CMV], which required convexity.
- The method yields symmetry as a consequence of stability: if $u_\nu$ is constant on $\Gamma$, then $\Omega$ is a ball.
- The proof relies on a new estimate (5.1) that bounds the Lipschitz seminorm of $u$ on $\Gamma^\delta$ in terms of the normal derivatives on $\Gamma$ and $\Gamma^t$.
- The decay rate $[u_{\nu\nu}]_{\Gamma^t} = O(t^{\tau-1})$ ensures the integral term vanishes as $\delta \to 0^+$, enabling the linear bound.
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This review was created by AI and reviewed by human editors.