论分数平均曲率为零的有边界超曲面的形状

Fumihiko Onoue
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引用次数: 0

摘要

我们考虑边界在 \({\mathbb {R}}^N\) 中的紧凑超曲面,它们是 Paroni 等人引入的分数面积的临界点(Commun Pure Appl Anal 17:709-727, 2018)。具体而言,我们在几个简单的设置中研究了此类超曲面的形状。首先,我们考虑临界点,临界点的边界是维数为(N-2\)的光滑、可定向、封闭流形\(\Gamma \),并且位于超平面\(H \subset {mathbb {R}}^N\) 中。然后我们证明临界点与一个维数为 \(N-1\) 的光滑流形 \({\mathcal {N}}\subset H\) 重合,并且 \(\partial {mathcal {N}}= \Gamma \)。其次,我们考虑临界点,临界点的边界由两个光滑的、可定向的、封闭的流形组成,维数为(N-2),假设(\(\Gamma _1\)位于垂直于(x_N)轴的超平面H中,并且(\(\Gamma _2 = \Gamma _1 + d\, e_N\)((d >;0) and\(e_N = (0,\cdots ,0,1) \in {\mathbb {R}}^N\).然后,假设\(\Gamma _1\)有一个非负的平均曲率,我们证明临界点与两个光滑流形\({\mathcal {N}}_1 \subset H\) 和\({\mathcal {N}}_2 \subset H + d \、e_N\) of dimension\(N-1\) with\(Partial {\mathcal {N}}_i =\Gamma _i\) for \(i \in \{1,2\}\).此外,临界点的内部并不与\({\mathbb {R}}^N\) 中的\({\mathbb {R}}^N\) 的\(\Gamma _1\)和\(\Gamma _2\)的凸壳的边界相交,而这可能发生在迪皮埃罗等人所考虑的一维情况下(Proc Am Math Soc 150:2223-2237, 2022)。我们还得到了一个定量约束,它可以告诉我们临界点与\({\mathcal {N}}_1 \cup\ {mathcal {N}}_2\) 有多大不同。最后,在与第二种情况相同的环境下,我们证明了如果 d 足够大,那么临界点是断开的;如果 d 足够小,那么当 \(N \ge 3\) 时,\(\γ_1\)和\(\γ_2\)处于临界点的同一个连通部分。此外,通过计算边界为 \(\Gamma _1 \cup \Gamma _2\)的圆锥的分数平均曲率,我们还可以得到,如果临界点包含在圆锥的内部或外部,那么临界点的内部并不接触圆锥。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

On the Shape of Hypersurfaces with Boundary Which Have Zero Fractional Mean Curvature

On the Shape of Hypersurfaces with Boundary Which Have Zero Fractional Mean Curvature

We consider compact hypersurfaces with boundary in \({\mathbb {R}}^N\) that are the critical points of the fractional area introduced by Paroni et al. (Commun Pure Appl Anal 17:709–727, 2018). In particular, we study the shape of such hypersurfaces in several simple settings. First we consider the critical points whose boundary is a smooth, orientable, closed manifold \(\Gamma \) of dimension \(N-2\) and lies in a hyperplane \(H \subset {\mathbb {R}}^N\). Then we show that the critical points coincide with a smooth manifold \({\mathcal {N}}\subset H\) of dimension \(N-1\) with \(\partial {\mathcal {N}}= \Gamma \). Second we consider the critical points whose boundary consists of two smooth, orientable, closed manifolds \(\Gamma _1\) and \(\Gamma _2\) of dimension \(N-2\) and suppose that \(\Gamma _1\) lies in a hyperplane H perpendicular to the \(x_N\)-axis and that \(\Gamma _2 = \Gamma _1 + d \, e_N\) (\(d >0\) and \(e_N = (0,\cdots ,0,1) \in {\mathbb {R}}^N\)). Then, assuming that \(\Gamma _1\) has a non-negative mean curvature, we show that the critical points do not coincide with the union of two smooth manifolds \({\mathcal {N}}_1 \subset H\) and \({\mathcal {N}}_2 \subset H + d \, e_N\) of dimension \(N-1\) with \(\partial {\mathcal {N}}_i = \Gamma _i\) for \(i \in \{1,2\}\). Moreover, the interior of the critical points does not intersect the boundary of the convex hull in \({\mathbb {R}}^N\) of \(\Gamma _1\) and \(\Gamma _2\), while this can occur in the codimension-one situation considered by Dipierro et al. (Proc Am Math Soc 150:2223–2237, 2022). We also obtain a quantitative bound which may tell us how different the critical points are from \({\mathcal {N}}_1 \cup {\mathcal {N}}_2\). Finally, in the same setting as in the second case, we show that, if d is sufficiently large, then the critical points are disconnected and, if d is sufficiently small, then \(\Gamma _1\) and \(\Gamma _2\) are in the same connected component of the critical points when \(N \ge 3\). Moreover, by computing the fractional mean curvature of a cone whose boundary is \(\Gamma _1 \cup \Gamma _2\), we also obtain that the interior of the critical points does not touch the cone if the critical points are contained in either the inside or the outside of the cone.

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