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Weihong Xie

Publications and source records attributed to Weihong Xie.

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Serrin's Problem under Dirichlet Perturbations: Geometric Compactness and Sharp Planar Stability

In earlier work [21], we posed a stability question for Serrin's overdetermined problem under Dirichlet perturbations and proved that the answer is negative in dimensions $n\ge3$. Here we resolve the question in the planar convex class and obtain a sharp quantitative theory without any a priori geometric nondegeneracy. Let $u_Ω$ solve \[ -Δu_Ω=1\ \text{in }Ω,\qquad \partial_νu_Ω=-\frac{|Ω|}{P(Ω)}\ \text{on }\partialΩ, \qquad \int_{\partialΩ}u_Ω\,dσ=0, \] and set $O(Ω):=\text{osc}_{\partial Ω}u_Ω$. We construct fixed-area annuli with $O(Ω_k)\to0$ that remain far from every disk, showing that convexity is essential in dimension two. By contrast, if $Ω_k\subset\mathbb R^2$ are convex, $|Ω_k|=π$, and $O(Ω_k)\to0$, then, up to translations, $Ω_k$ converges in Hausdorff distance to the unit disk. Moreover, \[ R_Ω-r_Ω+\inf_{z\in\mathbb R^2}d_H(Ω,B_1(z)) \le C\,O(Ω) \] for all planar convex $Ω$ with $|Ω|=π$ and sufficiently small $O(Ω)$, and the linear order is optimal. The proof combines a new mechanism excluding long-thin degeneration, the rough-domain Serrin rigidity theorem of Figalli--Zhang, new tangential-gradient and linear boundary-growth estimates, a boundary $P$-function estimate, and the reverse-Serrin identity of Magnanini--Molinarolo--Poggesi. We also study the weaker deficit \[ A(Ω):=\frac1{P(Ω)}\int_{\partialΩ}u_Ω,dσ-\min_{\partialΩ}u_Ω. \] In the planar convex class, $A(Ω_k)\to0$ still forces convergence to a disk, and \[ R_Ω-r_Ω+\inf_z d_H(Ω,B_1(z)) \le C A(Ω)^{2/3} \] for $|Ω|=π$ and sufficiently small $A(Ω)$.

math.AP

Torsion energy with boundary mean zero condition

Motivated by establishing Neumann Talenti type comparison results, we concern the minimization of the following shape functional under volume constraint: \begin{align*} T(Ω):=\inf\left\{\frac12 \int_Ω |\nabla u|^2\,dx -\int_Ωu\,dx: u\in H^1(Ω),\ \int_{\partial Ω}udσ=0 \right\}. \end{align*} We prove that ball is a local minimizer to $T(\cdot)$ under smooth perturbation, but quite surprisingly, ball is not locally minimal to $T(\cdot)$ under Lipschitz perturbation. In fact, let $P_N$ be the regular polygon in $\mathbb{R}^2$ with $N$ sides and area $π$, then we prove that $T(P_N)$ is a strictly increasing function with respect to $N$ and $\lim_{N\rightarrow \infty}T(P_N)=T(B)$ where $B$ is the unit disk. As another side result, we prove that in dimension bigger than or equal to three, rigidity results of Serrin's seminal overdetermined system is not stable under Dirichlet perturbations, in contrast to the stability of rigidity under Neumann perturbation.

math.AP

Improved Beckner's inequality for axially symmetric functions on $\mathbb{S}^4$

We show that axially symmetric solutions on $\mathbb{S}^4$ to a constant $Q$-curvature type equation (it may also be called fourth order mean field equation) must be constant, provided that the parameter $α$ in front of the Paneitz operator belongs to $[\frac{473 + \sqrt{209329}}{1800}\approx0.517, 1)$. This is in contrast to the case $α=1$, where a family of solutions exist, known as standard bubbles. The phenomenon resembles the Gaussian curvature equation on $ \mathbb{S}^2$. As a consequence, we prove an improved Beckner's inequality on $\mathbb{S}^4$ for axially symmetric functions with their centers of mass at the origin. Furthermore, we show uniqueness of axially symmetric solutions when $α=\frac15$ by exploiting Pohozaev-type identities, and prove existence of a non-constant axially symmetric solution for $α\in (\frac15, \frac12)$ via a bifurcation method.

math.AP

Improved Beckner's inequality for axially symmetric functions on $\mathbb{S}^n$

In this article we present various uniqueness and existence results for Q-curvature type equations with a Paneitz operator on $\s^n$ in axially symmetric function spaces. In particular, we show uniqueness results for $n=6, 8$ and improve the best constant of Beckner's inequality in these dimensions for axially symmetric functions under the constraint that their centers of mass are at the origin. As a consequence, the associated first Szegö limit theorem is also proven for axially symmetric functions.

math.AP

Infinitely many solutions for Schrödinger-Newton equations

We prove the existence of infinitely many non-radial positive solutions for the Schrödinger-Newton system $$ \left\{\begin{array}{ll} Δu- V(|x|)u + Ψu=0, &x\in\mathbb{R}^3,\newline ΔΨ+\frac12 u^2=0, &x\in\mathbb{R}^3, \end{array}\right. $$ provided that $V(r)$ has the following behavior at infinity: $$ V(r)=V_0+\frac{a}{r^m}+O\left(\frac{1}{r^{m+θ}}\right) \quad\mbox{ as } r\rightarrow\infty, $$ where $\frac12\le m<1$ and $a, V_0, θ$ are some positive constants. In particular, for any $s$ large we use a reduction method to construct $s-$bump solutions lying on a circle of radius $r\sim (s\log s)^{\frac{1}{1-m}}$.

math.AP