Symmetry properties for positive solutions of mixed boundary value problems in a sub-spherical sector
Ruofei Yao
TL;DR
This work studies symmetry and monotonicity of positive solutions to $\Delta u + f(u)=0$ in planar sub-spherical sectors under mixed Dirichlet–Neumann boundaries. It advances the moving-plane method by developing a maximum principle tailored to mixed boundary problems and by incorporating Hartman–Wintner angular-derivative analysis to secure non-vanishing tangential derivatives on the Neumann part. Through a careful analysis of angle relations and a continuation of moving planes in multiple directions, the authors establish axial symmetry and monotonicity for all admissible openings with $\beta\le 2\pi/3$, including detailed handling of challenging regimes $\pi/3<\beta<\pi/2$ via double-domain techniques. The results extend classical symmetry theory to mixed-boundary elliptic problems in symmetric domains, providing new tools for qualitative PDE analysis in sectors and related geometries.
Abstract
In this paper, we investigate the symmetry properties of positive solutions $u$ to a semilinear elliptic equation under mixed Dirichlet-Neumann boundary conditions in symmetric domains. First, we establish a maximum principle tailored to mixed-boundary problems in domains of either small volume or narrow width, thereby enabling the application of the moving plane method. Secondly, in contrast to the purely Dirichlet case, a key challenge is to establish the non-vanishing of the tangential derivative of $u$ along the Neumann boundary. To address this, we employ local analysis techniques of angular derivatives, as introduced by Hartman and Wintner [Amer. J. Math., 1953]. Thirdly, we identify the signs of directional derivatives of $u$ along sections of the moving line. Using a planar sub-spherical sector as an example, we illustrate how these new innovative techniques and the moving plane method can be combined to derive symmetry and monotonicity results, particularly when the amplitude is less than or equal to $2π/3$.
