This paper was converted on www.awesomepapers.org from LaTeX by an anonymous user.
Want to know more? Visit the Converter page.

A symmetry condition for genus zero free boundary minimal surfaces attaining the first eigenvalue of one

Dong-Hwi Seo Research Institute of Mathematics, Seoul National University, 1 Gwanak-ro, Gwanak-gu, Seoul 08826, Republic of Korea [email protected]
Abstract.

An embedded free boundary minimal surface in the 3-ball has a Steklov eigenvalue of one due to its coordinate functions. Fraser and Li conjectured that whether one is the first nonzero Steklov eigenvalue. In this paper, we show that if an embedded free boundary minimal surface of genus zero, with nn boundary components, in the 3-ball has nn distinct reflection planes, then one is the first eigenvalue of the surface.

Key words and phrases:
minimal surface, Steklov eigenvalue problem, free boundary problem
2020 Mathematics Subject Classification:
Primary 53A10; Secondary 58C40, 52A10

1. Introduction

Let 𝔹3\mathbb{B}^{3} be the standard Euclidean 3-ball. A surface M2M^{2} with boundary βˆ‚M\partial M is a free boundary minimal surface in 𝔹3\mathbb{B}^{3} if the mean curvature of MM is everywhere zero and MM meets βˆ‚π”Ή3\partial\mathbb{B}^{3} perpendicularly along βˆ‚M\partial M. This is equivalent to the requirements that MM be a critical point of the area functional among all variations of MM in 𝔹3\mathbb{B}^{3} whose boundaries are contained in βˆ‚π”Ή3\partial\mathbb{B}^{3}. For general references to this topic, we refer the reader to [14, 2].

Free boundary minimal surfaces in 𝔹3\mathbb{B}^{3} have an interesting connection with the Steklov eigenvalue problem, initially investigated by Fraser and Scheon [8]. The Steklov eigenvalue problem [20] of a smooth bounded domain Ξ©\Omega in a Riemannian manifold is to find Οƒβˆˆβ„\sigma\in\mathbb{R} for which there exists a function u∈Cβˆžβ€‹(Ξ©)u\in C^{\infty}(\Omega) satisfying

(1.3) {Δ​u=0inΒ β€‹Ξ©βˆ‚uβˆ‚Ξ·=σ​uonΒ β€‹βˆ‚Ξ©,\displaystyle\left\{\begin{array}[]{rcll}\Delta u&=&0&\text{in }\Omega\\ \frac{\partial u}{\partial\eta}&=&\sigma u&\text{on }\partial\Omega\end{array}\right.,

where Ξ·\eta is the outward unit conormal vector of Ξ©\Omega along βˆ‚Ξ©\partial\Omega. We call uu an Steklov eigenfunction and Οƒ\sigma an Steklov eigenvalue. It is known that the eigenvalues form a sequence 0=Οƒ0<Οƒ1β‰€β€¦β†’βˆž0=\sigma_{0}<\sigma_{1}\leq\dots\rightarrow\infty. See [10, 5] for general surveys. Fraser and Schoen observed that every coordinate function of a free boundary minimal surface in 𝔹n\mathbb{B}^{n} satisfies (1.3) with Οƒ=1\sigma=1 [8]. Thus, the coordinate functions are Steklov eigenfunctions with eigenvalue 1.

In [7], Fraser and Li proposed the following conjecture.

Conjecture 1.

Let NN be an embedded free boundary minimal hypersurface in 𝔹n\mathbb{B}^{n}. Then, the first Steklov eigenvalue Οƒ1​(N)\sigma_{1}(N) is 1.

Note that without the embeddedness assumption, there are some examples with Οƒ1​(M)<1\sigma_{1}(M)<1 by FernΓ‘ndez-Hauswirth-Mira [6] and Kapouleas-McGrath [11]. This conjecture can be seen as an analog of Yau’s conjecture for closed minimal hypersurfaces in π•Šn\mathbb{S}^{n} [23]. See surveys in [3, 1] and related results in [4, 22, 21].

Conjecture 1 has been studied by several authors. McGrath showed that if an embedded free boundary minimal annulus in 𝔹3\mathbb{B}^{3} has the reflection symmetries by three orthogonal planes passing through the origin, then the surface supports the conjecture [16]. In this work and his following work with Kusner [12], he showed that the conjecture holds for various classes of embedded free boundary minimal surfaces in 𝔹3\mathbb{B}^{3}. In particular, Kusner and McGrath showed that if an embedded free boundary minimal annulus has antipodal symmetry, the surface satisfies the conjecture. Additionally, the author showed that the conjecture holds for several symmetric free boundary minimal annuli [19]. For example, if an embedded free boundary minimal annulus has two distinct reflection planes, then the surface has the first eigenvalue of one [19, Theorem 1.2]. Here, we remark that there were no restrictions on reflection planes.

The main theorem in this paper is as follows.

Theorem 1.1.

Let Ξ£\Sigma be an embedded free boundary minimal surface of genus zero with nn boundary components in the unit ball 𝔹3\mathbb{B}^{3}. If Ξ£\Sigma has nn reflection symmetries, then Οƒ1​(Ξ£)=1\sigma_{1}(\Sigma)=1.

The main idea of the proof involves associating the boundary components with nn distinct points in π•Š2\mathbb{S}^{2} (Corollary 3.2). These points are derived from (2.2), which is motivated by the flux of a minimal surface. This idea, combined with a basic linear algebraic observation, simplifies the analysis of reflections (for example, see Corollary 3.3). Building on established techniques for genus zero free boundary minimal surfaces (Section 2), we can obtain the main theorem.

This theorem can be viewed as an extension of the author’s previous work on free boundary minimal annuli [19] to free boundary minimal surfaces of genus zero with nn boundary components. Since there are no restrictions on reflection planes, the theorem includes a new symmetry criterion on a surface to achieve the first Steklov eigenvalue of one. For example, the theorem explains that if Ξ£\Sigma has nn distinct reflection planes sharing a common axis, then Οƒ1​(Ξ£)=1\sigma_{1}(\Sigma)=1.

Acknowledgments

This work was supported by the National Research Foundation of Korea (NRF) grant funded by the Korean Government (MSIT) (No. 2021R1C1C2005144).

2. Preliminaries

2.1. General properties

Let MM be a compact embedded free boundary minimal surface of any topological type in 𝔹3\mathbb{B}^{3}. In this paper, we define a coordinate plane as a plane passing through the origin.

Theorem 2.1 (two-piece property, [15, Theorem A]).

Suppose MM is not homeomorphic to a disk. Then, a coordinate plane dissects MM by exactly two components.

From now on, a reflection means a mapping from ℝ3\mathbb{R}^{3} to itself that is an isometry with a plane as a set of fixed points. We denote by RΞ R_{\Pi} the reflection through a plane Ξ \Pi.

Lemma 2.2.
  1. (1)

    Let p1,p2βˆˆπ•Š2p_{1},p_{2}\in\mathbb{S}^{2} be two distinct points. If two reflections map p1p_{1} into p2p_{2}, then the two reflection planes are identical.

  2. (2)

    A reflection plane of MM passes through the origin.

Proof.

For (1), let Ξ 1\Pi_{1} and Ξ 2\Pi_{2} be such two reflection planes. Clearly, p1βˆ‰Ξ 1,Ξ 2p_{1}\notin\Pi_{1},\Pi_{2} and RΞ 1βˆ’1∘RΞ 2R_{\Pi_{1}}^{-1}\circ R_{\Pi_{2}} is a rotation about an axis. The axis is the intersection of Ξ 1\Pi_{1} and Ξ 2\Pi_{2}, so it does not contain p1p_{1}. Since, RΞ 1∘RΞ 2βˆ’1​(p1)=p1R_{\Pi_{1}}\circ R_{\Pi_{2}}^{-1}(p_{1})=p_{1}, RΞ 1βˆ’1∘RΞ 2R_{\Pi_{1}}^{-1}\circ R_{\Pi_{2}} is the identical map. Thus Ξ 1=Ξ 2\Pi_{1}=\Pi_{2}. For (2), let Ξ \Pi be a reflection plane of MM. If MM is an equatorial disk, Ξ \Pi passes through the origin. Otherwise, we can take two distinct points p1,p2βˆˆπ•Š2p_{1},p_{2}\in\mathbb{S}^{2} such that RΠ​(p1)=p2R_{\Pi}(p_{1})=p_{2} and p2β‰ βˆ’p1p_{2}\neq-p_{1}. Using (1), Ξ \Pi should be a coordinate plane passing through the midpoint of p1p_{1} and p2p_{2}, which completes the proof. ∎

2.2. Properties for genus zero

In the proof of the following lemmas, we use the fact that Ξ£\Sigma has genus zero.

Lemma 2.3.

Ξ£\Sigma satisfies the followings.

  1. (1)

    (transversality) If a coordinate plane meets Ξ£\Sigma, it intersects transversely. In particular, oβˆ‰Ξ£o\notin\Sigma, where oo is the origin.

  2. (2)

    (radial graphicality) If a ray from the origin meets Ξ£\Sigma, it intersects at a single point transversely.

Proof.

Every statement can be found in the proof of [9, Proposition 8.1]. For detailed proof, see [19, Corollary 4.5] for (1) and [17, Lemma 2.1] for (2). ∎

We denote by

(βˆ‚Ξ£)1,…,(βˆ‚Ξ£)n,\displaystyle(\partial\Sigma)_{1},\dots,(\partial\Sigma)_{n},

the components of βˆ‚Ξ£\partial\Sigma.

Let xx be the position vector in ℝ3\mathbb{R}^{3}. For i=1,…,ni=1,\dots,n, let

(2.1) Fi:=∫(βˆ‚Ξ£)ixi,andfi:=∫(βˆ‚Ξ£)ixi|∫(βˆ‚Ξ£)ixi|βˆˆπ•Š2.\displaystyle F_{i}:=\int_{(\partial\Sigma)_{i}}x_{i},\quad\text{and}\quad f_{i}:=\frac{\int_{(\partial\Sigma)_{i}}x_{i}}{\left|\int_{(\partial\Sigma)_{i}}x_{i}\right|}\in\mathbb{S}^{2}.

Using Lemma 2.5, we have

𝟎=βˆ«βˆ‚Ξ£x=βˆ«βˆ‚Ξ£(x1,x2,x3).\displaystyle\mathbf{0}=\int_{\partial\Sigma}x=\int_{\partial\Sigma}(x_{1},x_{2},x_{3}).

Thus we have

(2.2) F1+…​Fn=0.\displaystyle F_{1}+\dots F_{n}=0.
Lemma 2.4.

Assume nβ‰₯2n\geq 2. Each (βˆ‚Ξ£)i,i=1,…,n(\partial\Sigma)_{i},i=1,\dots,n, satisfies the followings.

  1. (1)

    (βˆ‚Ξ£)i(\partial\Sigma)_{i} is a strictly convex curve in π•Š2\mathbb{S}^{2}. In other words, a plane passing through the origin intersects (βˆ‚Ξ£)i(\partial\Sigma)_{i} in at most two points.

  2. (2)

    There is a small neighborhood of (βˆ‚Ξ£)i(\partial\Sigma)_{i} in Ξ£\Sigma that is contained outside of the convex cone over (βˆ‚Ξ£)i(\partial\Sigma)_{i}.

  3. (3)

    A plane parallel to the line passing through fif_{i} and the origin intersects (βˆ‚Ξ£)i(\partial\Sigma)_{i} in at most two points.

  4. (4)

    Let uu be a first Steklov eigenfunction of Ξ£\Sigma. Then, (βˆ‚Ξ£)i(\partial\Sigma)_{i} contains at most two nodal points of uu.

Proof.

For the proof of (1), see [19, Lemma 4.2] or [12, Corollary 4.2]. The major tool of the proof is the two-piece property (Theorem 2.1). For (2), see [19, Lemma 6.4]. (3) and (4) follow from [19, Proposition 3.6] and [19, Remark 4.4], respectively. ∎

2.3. Properties under Οƒ1​(M)<1\sigma_{1}(M)<1

Lemma 2.5.
  1. (1)

    Any coordinate functions xi,i=1,2,3x_{i},i=1,2,3, are Steklov eigenfunctions of MM with eigenvalue 1. In particular, Οƒ1​(M)≀1\sigma_{1}(M)\leq 1.

  2. (2)

    Let uu be a first Steklov eigenfunction of MM. Then,

    βˆ«βˆ‚Mu=0.\displaystyle\int_{\partial M}u=0.

    If Οƒ1​(M)<1\sigma_{1}(M)<1, we have

    βˆ«βˆ‚Mu​xi=0.\displaystyle\int_{\partial M}ux_{i}=0.
Proof.

See, for example, [19, Lemma 2.1]. ∎

Note that Lemma 2.5 holds for all compact immersed free boundary minimal submanfolds in 𝔹m\mathbb{B}^{m} with all coordinate functions x1,…,xmx_{1},\dots,x_{m}.

Lemma 2.6 (symmetry of a first eigenfunction, [16, Lemma 3.2]).

Assume Οƒ1​(M)<1\sigma_{1}(M)<1. Let uu be a first Steklov eigenfunction of MM. If RΠ​(M)=MR_{\Pi}(M)=M, uu is invariant under RΞ R_{\Pi}.

Lemma 2.7 (constant sign).

Assume Οƒ1​(Ξ£)<1\sigma_{1}(\Sigma)<1. If a boundary component (βˆ‚Ξ£)i(\partial\Sigma)_{i} is invariant under the reflections through the two distinct planes, a first Steklov eigenfunction of Ξ£\Sigma has a constant sign on (βˆ‚Ξ£)i(\partial\Sigma)_{i}.

Proof.

Let Ξ 1\Pi_{1} and Ξ 2\Pi_{2} be two distinct reflection planes for (βˆ‚Ξ£)i(\partial\Sigma)_{i}. By symmetry principle [19, Theorem 1.4] and Lemma 2.2 (2), Ξ 1\Pi_{1} and Ξ 2\Pi_{2} are two reflection planes for Ξ£\Sigma passing through the origin. Since RΞ 1​(fi)=RΞ 2​(fi)=fiR_{\Pi_{1}}(f_{i})=R_{\Pi_{2}}(f_{i})=f_{i}, they also pass through fif_{i}. By a similar argument in Case 1 in the proof of [19, Theorem 1.2], the first eigenfunction has a constant sign on (βˆ‚Ξ£)i(\partial\Sigma)_{i}. ∎

3. Main proof

Let Di,i=1,…,nD_{i},i=1,\dots,n be the convex sets in π•Š2\mathbb{S}^{2} bounded by (βˆ‚Ξ£)i(\partial\Sigma)_{i}, respectively. Note that each of Di,i=1,…,nD_{i},i=1,\dots,n is well-defined by Lemma 2.4 (1). The following theorem insists that no two nested convex sets exist among DiD_{i}.

Theorem 3.1.

There are no two distinct i,j∈{1,…,n}i,j\in\{1,\dots,n\} such that Di⊊DjD_{i}\subsetneq D_{j} or Dj⊊DiD_{j}\subsetneq D_{i}.

Proof.

Assume D1βŠ‚D2D_{1}\subset D_{2}. Take a coordinate plane Ξ \Pi that meets βˆ‚Ξ£\partial\Sigma transversely and meets (βˆ‚Ξ£)1(\partial\Sigma)_{1} and (βˆ‚Ξ£)2(\partial\Sigma)_{2}. Let {(βˆ‚Ξ£)1,…​(βˆ‚Ξ£)m}\{(\partial\Sigma)_{1},\dots(\partial\Sigma)_{m}\} be the boundary components of Ξ£\Sigma that has an intersection with Ξ \Pi, and we denote (βˆ‚Ξ£)i∩Π(\partial\Sigma)_{i}\cap\Pi by vi1v_{i}^{1} and vi2v_{i}^{2} for all i=1,2,…,mi=1,2,\dots,m.

We consider a graph whose vertex set is

(3.1) {v11,…,vm1}βˆͺ{v12,…,vm2}\displaystyle\{v_{1}^{1},\dots,v_{m}^{1}\}\cup\{v_{1}^{2},\dots,v_{m}^{2}\}

and the edges are the arcs in Π∩Σ\Pi\cap\Sigma whose endpoints are contained in βˆ‚Ξ£\partial\Sigma. By the transversality property (Lemma 2.3 (1)), every vertex is contained in exactly one edge. Furthermore, we give a direction on the edge set by following the procedure.

  1. (1)

    Take the edge containing v12v_{1}^{2} and give a direction from v12v_{1}^{2}. Let vv be the other vertex in the edge.

  2. (2)

    Take the vertex ww which is contained in the same boundary component with vv but not identical to vv.

  3. (3)

    Repeat the first and second steps until the vertex v11v_{1}^{1} comes out.

By the two-piece property (Theorem 2.1) with the fact that Ξ£\Sigma has genus zero, every edge has a direction.

We claim that the directed graph from v12v_{1}^{2} escapes the convex cone over D2∩ΠD_{2}\cap\Pi by an edge. Note the fact that a small part of an arc of Π∩Σ\Pi\cap\Sigma from each of vertices vi1v_{i}^{1} and vi2v_{i}^{2} is contained outside of the convex cone over Di∩ΠD_{i}\cap\Pi by Lemma 2.4 (2). Since we can give directions on every edge, the directed graph from v12v_{1}^{2} escapes the convex cone over D2∩ΠD_{2}\cap\Pi. On the other hand, the embeddedness of Ξ£\Sigma implies that for every ii, we have either vi1,vi2∈int​(D2)v_{i}^{1},v_{i}^{2}\in\text{int}(D_{2}) or vi1,vi2βˆ‰int​(D2)v_{i}^{1},v_{i}^{2}\notin\text{int}(D_{2}). Therefore, the directed graph escapes by an edge that meets one of the line segments o​v21ov_{2}^{1} and o​v22ov_{2}^{2} transversely by Lemma 2.3 (1), which completes that proof.

By the previous claim and the fact in the proof, there is a ray from oo that meets Ξ£\Sigma at least twice. It contracts the radial graphicality of Ξ£\Sigma (Lemma 2.3 (2)).

∎

Corollary 3.2.

{f1,…,fn}\{f_{1},\dots,f_{n}\} has nn distinct elements.

Proof.

Suppose fi=fjf_{i}=f_{j} for iβ‰ ji\neq j. If Di∩Dj=βˆ…D_{i}\cap D_{j}=\emptyset, we can find a coordinate plane that separates DiD_{i} and DjD_{j}. Then, fiβ‰ fjf_{i}\neq f_{j}, a contradiction. On the other hand, we consider Di∩Djβ‰ βˆ…D_{i}\cap D_{j}\neq\emptyset. Since Ξ£\Sigma is embedded, we have either Di⊊DjD_{i}\subsetneq D_{j} or Dj⊊DiD_{j}\subsetneq D_{i}, which contradicts Theorem 3.1. ∎

Corollary 3.3.

Let Ξ \Pi be a reflection plane of Ξ£\Sigma. Then, for 1≀i≀j≀n1\leq i\leq j\leq n, RΠ​((βˆ‚Ξ£)i)=(βˆ‚Ξ£)jR_{\Pi}((\partial\Sigma)_{i})=(\partial\Sigma)_{j} if and only if RΠ​(fi)=fjR_{\Pi}(f_{i})=f_{j}.

Proof.

It is clear that RΠ​((βˆ‚Ξ£)i)=(βˆ‚Ξ£)jR_{\Pi}((\partial\Sigma)_{i})=(\partial\Sigma)_{j} implies RΠ​(fi)=fjR_{\Pi}(f_{i})=f_{j}. Now suppose RΠ​(fi)=fjR_{\Pi}(f_{i})=f_{j}. We note that RΠ​((βˆ‚Ξ£)i)R_{\Pi}((\partial\Sigma)_{i}) is a boundary component of Ξ£\Sigma, say (βˆ‚Ξ£)k(\partial\Sigma)_{k}. Then, fk=RΠ​(fi)f_{k}=R_{\Pi}(f_{i}), and by the assumption, fk=fjf_{k}=f_{j}. By Corollary 3.2, we have k=jk=j and RΠ​((βˆ‚Ξ£)i)=(βˆ‚Ξ£)jR_{\Pi}((\partial\Sigma)_{i})=(\partial\Sigma)_{j}. ∎

Lemma 3.4.

Let Ξ 1,…,Ξ n\Pi_{1},\dots,\Pi_{n} be distinct reflection planes of Ξ£\Sigma. Then, the reflection group generated by RΞ 1,…,RΞ nR_{\Pi_{1}},\dots,R_{\Pi_{n}} acts transitively on {f1,…,fn}\{f_{1},\dots,f_{n}\}. Equivalently, the reflection group acts transitively on {(βˆ‚Ξ£)1,…,(βˆ‚Ξ£)n}\{(\partial\Sigma)_{1},\dots,(\partial\Sigma)_{n}\}.

Proof.

Suppose the first statement is not true. We consider a graph with vertices {f1,…,fn}\{f_{1},\dots,f_{n}\} and edges (fi​fj),1≀i,j≀n(f_{i}f_{j}),1\leq i,j\leq n if there is a plane Π∈{Ξ 1,…,Ξ n}\Pi\in\{\Pi_{1},\dots,\Pi_{n}\} such that RΠ​(fi)=fjR_{\Pi}(f_{i})=f_{j}. By the assumption, this graph has at least two components. Take one of the smallest components with kk vertices. Then, k≀nβˆ’kk\leq n-k.

We show that kβ‰₯2k\geq 2. Suppose k=1k=1 and let f1f_{1} be such vertex. Then, every reflection, RΞ 1,…,RΞ nR_{\Pi_{1}},\dots,R_{\Pi_{n}}, maps f1f_{1} into f1f_{1}. This nn reflections map f2f_{2} into {f1,…,fn}βˆ–{f1}\{f_{1},\dots,f_{n}\}\setminus\{f_{1}\}. If f2β‰ βˆ’f1f_{2}\neq-f_{1}, by Corollary 3.2, only one coordinate plane passes through f1f_{1} and f2f_{2}. It implies that there is at most one reflection in {RΞ 1,…,RΞ n}\{R_{\Pi_{1}},\dots,R_{\Pi_{n}}\} that map f2f_{2} into f2f_{2}. In addition, using Lemma 2.2 (1), there are at most nβˆ’2n-2 reflections that map f2f_{2} into {f1,…,fn}βˆ–{f1,f2}\{f_{1},\dots,f_{n}\}\setminus\{f_{1},f_{2}\}. Thus, there are at most nβˆ’1n-1 distinct reflections in {RΞ 1,…,RΞ n}\{R_{\Pi_{1}},\dots,R_{\Pi_{n}}\}, a contradiction. Thus, f2=βˆ’f1f_{2}=-f_{1}. In a similar argument, we can show that f2=f3=β‹―=fnf_{2}=f_{3}=\cdots=f_{n}, which is βˆ’f1-f_{1}. It contradicts Corollary 3.2. Therefore, kβ‰₯2k\geq 2.

Let {f1,…,fk}\{f_{1},\dots,f_{k}\} be the vertex set of the smallest component. By Lemma 2.2 (1), there are at most kβˆ’1k-1 reflection planes in {Ξ 1,…,Ξ n}\{\Pi_{1},\dots,\Pi_{n}\} that do not pass through f1f_{1}. Therefore, there must be at least nβˆ’k+1n-k+1 reflection planes in {Ξ 1,…,Ξ n}\{\Pi_{1},\dots,\Pi_{n}\} that pass through f1f_{1}. Suppose k=2k=2 and f2=βˆ’f1f_{2}=-f_{1}. In this case, there is exactly one reflection plane in {Ξ 1,…,Ξ n}\{\Pi_{1},\dots,\Pi_{n}\} that does not pass through f1f_{1}. Because every reflection plane passing through f1f_{1} maps f3f_{3} into {f3,…,fn}\{f_{3},\dots,f_{n}\}, Lemma 2.2 further implies that there can be at most nβˆ’2n-2 distinct reflection planes passing through f1f_{1} in {Ξ 1,…,Ξ n}\{\Pi_{1},\dots,\Pi_{n}\}. Then, there are at most nβˆ’1n-1 reflections in {Ξ 1,…,Ξ n}\{\Pi_{1},\dots,\Pi_{n}\}, contrary to Corollary 3.2. Therefore we can take f2β‰ βˆ’f1f_{2}\neq-f_{1}, and we can assume f2f_{2} is connected to f1f_{1} by an edge. By Lemma 2.2 (1), the reflection planes in {Ξ 1,…,Ξ n}\{\Pi_{1},\dots,\Pi_{n}\} that pass through f1f_{1} maps f2f_{2} one-to-one into {f2,…,fk}\{f_{2},\dots,f_{k}\}. Thus, there are at most kβˆ’1k-1 such reflections. However, nβˆ’k+1>kβˆ’1n-k+1>k-1 leads to a contradiction.

The second statement follows from the first statement with an argument in the proof of Corollary 3.3. ∎

Now we prove the main theorem.

Proof of Theorem 1.1.

The case for n=1n=1 is trivial by the classical work by Nitsche [18]. For n=2n=2, our theorem is known in [19, Theorem 1.2]. Thus, we only need to consider n>2n>2. We prove this theorem by proof by contradiction. We assume Οƒ1​(Ξ£)<1\sigma_{1}(\Sigma)<1. We will obtain a contradiction by following the steps.

Step 1. Let Ξ 1,…,Ξ n\Pi_{1},\dots,\Pi_{n} be the given reflection planes of Ξ£\Sigma. We show that for each 1≀i,j≀n1\leq i,j\leq n, there is Π∈{Ξ 1,…,Ξ n}\Pi\in\{\Pi_{1},\dots,\Pi_{n}\} such that RΠ​((βˆ‚Ξ£)i)=(βˆ‚Ξ£)jR_{\Pi}((\partial\Sigma)_{i})=(\partial\Sigma)_{j}. By Corollary 3.3 and Lemma 2.2 (1), it is sufficient to prove that there is exactly one reflection plane in {Ξ 1,…,Ξ n}\{\Pi_{1},\dots,\Pi_{n}\} that passes through each fif_{i}. Suppose there are no reflection planes in {Ξ 1,…,Ξ n}\{\Pi_{1},\dots,\Pi_{n}\} that pass through fif_{i}. Then, by Lemma 2.2 (1), there are at most nβˆ’1n-1 distinct reflections in {RΞ 1,…,RΞ n}\{R_{\Pi_{1}},\dots,R_{\Pi_{n}}\}, a contradiction. If there are two reflections in {RΞ 1,…,RΞ n}\{R_{\Pi_{1}},\dots,R_{\Pi_{n}}\} that pass through fif_{i}, by Lemma 2.7, a first eigenfunction uu has a constant sign on (βˆ‚Ξ£)i(\partial\Sigma)_{i}. By Lemma 3.4 with Corollary 3.3 and Lemma 2.6, uu has a constant sign on βˆ‚Ξ£\partial\Sigma. It contradicts Lemma 2.5 (2).

By Step 1, for each 1≀i,j≀n1\leq i,j\leq n, we can define Ξ i​j∈{Ξ 1,…,Ξ n}\Pi_{ij}\in\{\Pi_{1},\dots,\Pi_{n}\} and Ri​j:=RΞ i​jR_{ij}:=R_{\Pi_{ij}} such that

(3.2) Ri​j​((βˆ‚Ξ£)i)=(βˆ‚Ξ£)j.\displaystyle R_{ij}((\partial\Sigma)_{i})=(\partial\Sigma)_{j}.

In addition, we show that each of the boundary components of Ξ£\Sigma has exactly two nodal points of uu. By Lemma 2.6 and Lemma 2.5 (2), uu changes its sign on each of the boundary components. In addition, every (βˆ‚Ξ£)i(\partial\Sigma)_{i} has the same number of nodal points of uu, and the number is at least two. By Lemma 2.4 (4), the number should be two.

Let pi1,pi2p_{i}^{1},p_{i}^{2} be the nodal point of uu in (βˆ‚Ξ£)i(\partial\Sigma)_{i}. Then, by Lemma 2.6, Ri​i​(pi1)=pi2R_{ii}(p_{i}^{1})=p_{i}^{2}. Otherwise, Ri​i​(pi1)=pi1R_{ii}(p_{i}^{1})=p_{i}^{1} and Ri​i​(pi2)=pi2R_{ii}(p_{i}^{2})=p_{i}^{2}. Then, by Lemma 2.6 again, uu cannot change its sign on (βˆ‚Ξ£)i(\partial\Sigma)_{i}, a contradiction. These nodal points divide each of the boundary components into two arcs.

Step 2. We show that the two arcs of (βˆ‚Ξ£)iβˆ–{pi1,pi2}(\partial\Sigma)_{i}\setminus\{p_{i}^{1},p_{i}^{2}\} are not congruent. Suppose not. Then, either a nontrivial rotation or a reflection that maps one component of (βˆ‚Ξ£)iβˆ–{pi1,pi2}(\partial\Sigma)_{i}\setminus\{p_{i}^{1},p_{i}^{2}\} into the other and vice versa. If there is such a reflection, it cannot be Ri​iR_{ii}. By Lemma 2.7, uu has a constant sign on (βˆ‚Ξ£)i(\partial\Sigma)_{i}, a contradiction. If there is such a rotation AA, A​(fi)=fiA(f_{i})=f_{i} and A​({pi1,pi2})={pi1,pi2}A(\{p_{i}^{1},p_{i}^{2}\})=\{p_{i}^{1},p_{i}^{2}\}. For the case of A​(pi1)=pi1A(p_{i}^{1})=p_{i}^{1} and A​(pi2)=pi2A(p_{i}^{2})=p_{i}^{2}, the rotation axis for AA passes through fi,pi1,f_{i},p_{i}^{1}, and pi2p_{i}^{2}. Since the axis meets π•Š2\mathbb{S}^{2} at exactly two points, fif_{i} should be either pi1p_{i}^{1} or pi2p_{i}^{2}. However, fif_{i} lies in the interior of DiD_{i} [19, Proposition 3.5], a contradiction. For the case of A​(pi1)=pi2A(p_{i}^{1})=p_{i}^{2} and A​(pi2)=pi1A(p_{i}^{2})=p_{i}^{1}, we note that AA is the 180Β°rotation through the axis passing through the origin and fif_{i}. Together with Ri​iR_{ii}, (βˆ‚Ξ£)i(\partial\Sigma)_{i} has a reflection symmetry distinct from Ri​iR_{ii}. Lemma 2.7 again gives a contradiction.

We prove the following step using an argument on arcs.

Step 3. We show that Ξ 1,…,Ξ n\Pi_{1},\dots,\Pi_{n} share a common axis. By the previous step, let p11​p12^\widehat{p_{1}^{1}p_{1}^{2}} and p11​p12^β€²\widehat{p_{1}^{1}p_{1}^{2}}^{\prime} be the components of (βˆ‚Ξ£)1βˆ–{p11,pi2}(\partial\Sigma)_{1}\setminus\{p_{1}^{1},p_{i}^{2}\}. Furthermore, we define an arc pi1​pi2^\widehat{p_{i}^{1}p_{i}^{2}} of (βˆ‚Ξ£)i(\partial\Sigma)_{i} that is congruent to p11​p12^\widehat{p_{1}^{1}p_{1}^{2}}. Clearly,

(3.3) Ri​j​(pi1​pi2^)=pj1​pj2^.\displaystyle R_{ij}\left(\widehat{p_{i}^{1}p_{i}^{2}}\right)=\widehat{p_{j}^{1}p_{j}^{2}}.

Then, we have

(3.4) R2​i∘R12​(p11​p12^)=R1​i∘R11​(p11​p12^)=pi1​pi2^.\displaystyle R_{2i}\circ R_{12}\left(\widehat{p_{1}^{1}p_{1}^{2}}\right)=R_{1i}\circ R_{11}\left(\widehat{p_{1}^{1}p_{1}^{2}}\right)=\widehat{p_{i}^{1}p_{i}^{2}}.

For simplicity, let A:=(R2​i∘R12)βˆ’1∘(R1​i∘R11)A:=(R_{2i}\circ R_{12})^{-1}\circ(R_{1i}\circ R_{11}) and let q1:=p11​p12^∩Π11q_{1}:=\widehat{p_{1}^{1}p_{1}^{2}}\cap\Pi_{11}. Then, A​(q1)=q1A(q_{1})=q_{1} and A​(p11)A(p_{1}^{1}) is either p11p_{1}^{1} or p12p_{1}^{2}. Note that R2​i∘R12R_{2i}\circ R_{12}, R1​i∘R11R_{1i}\circ R_{11}, and AA are all rotations along axes passing through the origin. Then, AA is a rotation along the axis passing through the origin and q1q_{1}. Suppose AA is not the identity map. Since the axis and p11​p12^\widehat{p_{1}^{1}p_{1}^{2}} are invariant under AA and R11R_{11}, each of components of p11​p12^βˆ–{q1}\widehat{p_{1}^{1}p_{1}^{2}}\setminus\{q_{1}\} lies in a plane that passes through the axis. Similarly, p11​p12^β€²\widehat{p_{1}^{1}p_{1}^{2}}^{\prime} lies in two planes passing through the axis. Since (βˆ‚Ξ£)1(\partial\Sigma)_{1} is real analytic (see [13, Section 6]), this boundary component lies in a plane, so it is a circle. By [19, Remark 6.2], Ξ£\Sigma is congruent to one of an equatorial disk and a critical catenoid. It contradicts n>2n>2. Thus AA is the identity map. Then, the rotation axes of R2​i∘R12R_{2i}\circ R_{12} and R1​i∘R11R_{1i}\circ R_{11} are identical. Since each of these axes is the intersection of the two reflection planes, Ξ 11,Ξ 12,\Pi_{11},\Pi_{12}, and Ξ 1​i\Pi_{1i} contain a common axis. Since ii is arbitrary and

(3.5) {Ξ 11,…,Ξ 1​n}={Ξ 1,…,Ξ n},\displaystyle\left\{\Pi_{11},\dots,\Pi_{1n}\right\}=\left\{\Pi_{1},\dots,\Pi_{n}\right\},

we obtained our desired conclusion.

Step 4. Let x3x_{3}-axis be the common axis of Ξ 1,…,Ξ n\Pi_{1},\dots,\Pi_{n} as in the previous step. By Step 1 and Lemma 2.6, every nodal point of uu in βˆ‚Ξ£\partial\Sigma has the same x3x_{3}-coordinates, say cc. Moreover, using (2.2), we have

(3.6) f1,f2,…,fn∈{x3=0}\displaystyle f_{1},f_{2},\dots,f_{n}\in\{x_{3}=0\}

By Lemma 2.4 (3), uu does not change its sign on each of βˆ‚Ξ£βˆ©{x3>c}\partial\Sigma\cap\{x_{3}>c\} and βˆ‚Ξ£βˆ©{x3<c}\partial\Sigma\cap\{x_{3}<c\}. Thus, we have

(3.7) βˆ«βˆ‚Ξ£u​(x3βˆ’c)β‰ 0,\displaystyle\int_{\partial\Sigma}u(x_{3}-c)\neq 0,

which contradicts Lemma 2.5 (2).

Throughout the steps, we obtained a contradiction by assuming Οƒ1​(Ξ£)<1\sigma_{1}(\Sigma)<1. By Lemma 2.5 (1), we have Οƒ1​(Ξ£)=1\sigma_{1}(\Sigma)=1.

∎

For a surface of genus zero, the first eigenvalue of this surface has multiplicity at most 3 [9, Theorem 2.3]. Main theorem implies the following.

Corollary 3.5.

If Ξ£\Sigma has nn reflection symmetries, the first Steklov eigenspace for Ξ£\Sigma is spanned by the three coordinate functions of ℝ3\mathbb{R}^{3}.

References

  • [1] Simon Brendle, Minimal surfaces in S3S^{3}: a survey of recent results, Bull. Math. Sci. 3 (2013), no.Β 1, 133–171. MR 3061135
  • [2] Alessandro Carlotto, Free boundary minimal surfaces: a survey of recent results, Rend. Accad. Sci. Fis. Mat., Napoli (4) 86 (2019), 103–121 (English).
  • [3] Jaigyoung Choe, Minimal surfaces in π•Š3\mathbb{S}^{3} and Yau’s conjecture, Proceedings of the 10th international workshop on differential geometry, Taegu, Korea, November 10–11, 2005, Taegu: Kyungpook National University, 2006, pp.Β 183–188 (English).
  • [4] Jaigyoung Choe and Marc Soret, First eigenvalue of symmetric minimal surfaces in π•Š3\mathbb{S}^{3}, Indiana Univ. Math. J. 58 (2009), no.Β 1, 269–281 (English).
  • [5] Bruno Colbois, Alexandre Girouard, Carolyn Gordon, and David Sher, Some recent developments on the Steklov eigenvalue problem, Rev. Mat. Complut. 37 (2024), no.Β 1, 1–161 (English).
  • [6] Isabel FernΓ‘ndez, Laurent Hauswirth, and Pablo Mira, Free boundary minimal annuli immersed in the unit ball, Arch. Ration. Mech. Anal. 247 (2023), no.Β 6, 44 (English), Id/No 108.
  • [7] Ailana Fraser and Martin Man-chun Li, Compactness of the space of embedded minimal surfaces with free boundary in three-manifolds with nonnegative Ricci curvature and convex boundary, J. Differential Geom. 96 (2014), no.Β 2, 183–200.
  • [8] Ailana Fraser and Richard Schoen, The first Steklov eigenvalue, conformal geometry, and minimal surfaces, Adv. Math. 226 (2011), no.Β 5, 4011–4030.
  • [9] by same author, Sharp eigenvalue bounds and minimal surfaces in the ball, Invent. Math. 203 (2016), no.Β 3, 823–890.
  • [10] A.Β Girouard and I.Β Polterovich, Spectral geometry of the Steklov problem, Shape optimization and spectral theory, De Gruyter Open, Warsaw, 2017, pp.Β 120–148.
  • [11] Nikolaos Kapouleas and Peter McGrath, Free boundary minimal annuli immersed in the unit 3-ball, arXiv:2212.09680 [math.DG].
  • [12] Robert Kusner and Peter McGrath, On Steklov eigenspaces for free boundary minimal surfaces in the unit ball, Amer. J. Math. (to appear), arXiv:2011.06884.
  • [13] Hans Lewy, On mimimal surfaces with partially free boundary, Comm. Pure Appl. Math. 4 (1951), 1–13.
  • [14] Martin Man-chun Li, Free boundary minimal surfaces in the unit ball: recent advances and open questions, Proceedings of the International Consortium of Chinese Mathematicians 2017, Int. Press, Boston, MA, [2020] Β©2020, pp.Β 401–435.
  • [15] Vanderson Lima and Ana Menezes, A two-piece property for free boundary minimal surfaces in the ball, Trans. Amer. Math. Soc. 374 (2021), no.Β 3, 1661–1686.
  • [16] Peter McGrath, A characterization of the critical catenoid, Indiana Univ. Math. J. 67 (2018), no.Β 2, 889–897.
  • [17] Peter McGrath and Jiahua Zou, On the areas of genus zero free boundary minimal surfaces embedded in the unit 3-ball, J. Geom. Anal. 34 (2024), no.Β 9, Paper No. 274, 14. MR 4765852
  • [18] Johannes C.Β C. Nitsche, Stationary partitioning of convex bodies, Arch. Rational Mech. Anal. 89 (1985), no.Β 1, 1–19.
  • [19] Dong-Hwi Seo, Sufficient symmetry conditions for free boundary minimal annuli to be the critical catenoid, arXiv:2112.11877 [math.DG].
  • [20] W.Β Stekloff, Sur les problΓ¨mes fondamentaux de la physique mathΓ©matique (suite et fin), Ann. Sci. Γ‰cole Norm. Sup. (3) 19 (1902), 455–490.
  • [21] Zizhou Tang, Yuquan Xie, and Wenjiao Yan, Isoparametric foliation and Yau conjecture on the first eigenvalue, II, J. Funct. Anal. 266 (2014), no.Β 10, 6174–6199. MR 3188712
  • [22] Zizhou Tang and Wenjiao Yan, Isoparametric foliation and Yau conjecture on the first eigenvalue, J. Differential Geom. 94 (2013), no.Β 3, 521–540. MR 3080491
  • [23] Shing-Tung Yau, Problem section of the seminar in differential geometry at Tokyo, Semin. differential geometry, Ann. Math. Stud. 102, 669-706 (1982)., 1982.