A symmetry condition for genus zero free boundary minimal surfaces attaining the first eigenvalue of one
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 boundary components, in the 3-ball has distinct reflection planes, then one is the first eigenvalue of the surface.
Key words and phrases:
minimal surface, Steklov eigenvalue problem, free boundary problem2020 Mathematics Subject Classification:
Primary 53A10; Secondary 58C40, 52A101. Introduction
Let be the standard Euclidean 3-ball. A surface with boundary is a free boundary minimal surface in if the mean curvature of is everywhere zero and meets perpendicularly along . This is equivalent to the requirements that be a critical point of the area functional among all variations of in whose boundaries are contained in . For general references to this topic, we refer the reader to [14, 2].
Free boundary minimal surfaces in 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 in a Riemannian manifold is to find for which there exists a function satisfying
(1.3) |
where is the outward unit conormal vector of along . We call an Steklov eigenfunction and an Steklov eigenvalue. It is known that the eigenvalues form a sequence . See [10, 5] for general surveys. Fraser and Schoen observed that every coordinate function of a free boundary minimal surface in satisfies (1.3) with [8]. Thus, the coordinate functions are Steklov eigenfunctions with eigenvalue 1.
In [7], Fraser and Li proposed the following conjecture.
Conjecture 1.
Let be an embedded free boundary minimal hypersurface in . Then, the first Steklov eigenvalue is 1.
Note that without the embeddedness assumption, there are some examples with by FernΓ‘ndez-Hauswirth-Mira [6] and Kapouleas-McGrath [11]. This conjecture can be seen as an analog of Yauβs conjecture for closed minimal hypersurfaces in [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 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 . 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 be an embedded free boundary minimal surface of genus zero with boundary components in the unit ball . If has reflection symmetries, then .
The main idea of the proof involves associating the boundary components with distinct points in (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 authorβs previous work on free boundary minimal annuli [19] to free boundary minimal surfaces of genus zero with 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 has distinct reflection planes sharing a common axis, then .
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 be a compact embedded free boundary minimal surface of any topological type in . 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 is not homeomorphic to a disk. Then, a coordinate plane dissects by exactly two components.
From now on, a reflection means a mapping from to itself that is an isometry with a plane as a set of fixed points. We denote by the reflection through a plane .
Lemma 2.2.
-
(1)
Let be two distinct points. If two reflections map into , then the two reflection planes are identical.
-
(2)
A reflection plane of passes through the origin.
Proof.
For (1), let and be such two reflection planes. Clearly, and is a rotation about an axis. The axis is the intersection of and , so it does not contain . Since, , is the identical map. Thus . For (2), let be a reflection plane of . If is an equatorial disk, passes through the origin. Otherwise, we can take two distinct points such that and . Using (1), should be a coordinate plane passing through the midpoint of and , which completes the proof. β
2.2. Properties for genus zero
In the proof of the following lemmas, we use the fact that has genus zero.
Lemma 2.3.
satisfies the followings.
-
(1)
(transversality) If a coordinate plane meets , it intersects transversely. In particular, , where is the origin.
-
(2)
(radial graphicality) If a ray from the origin meets , it intersects at a single point transversely.
Proof.
We denote by
the components of .
Let be the position vector in . For , let
(2.1) |
Lemma 2.4.
Assume . Each , satisfies the followings.
-
(1)
is a strictly convex curve in . In other words, a plane passing through the origin intersects in at most two points.
-
(2)
There is a small neighborhood of in that is contained outside of the convex cone over .
-
(3)
A plane parallel to the line passing through and the origin intersects in at most two points.
-
(4)
Let be a first Steklov eigenfunction of . Then, contains at most two nodal points of .
2.3. Properties under
Lemma 2.5.
-
(1)
Any coordinate functions , are Steklov eigenfunctions of with eigenvalue 1. In particular, .
-
(2)
Let be a first Steklov eigenfunction of . Then,
If , we have
Proof.
See, for example, [19, Lemma 2.1]. β
Note that Lemma 2.5 holds for all compact immersed free boundary minimal submanfolds in with all coordinate functions .
Lemma 2.6 (symmetry of a first eigenfunction, [16, Lemma 3.2]).
Assume . Let be a first Steklov eigenfunction of . If , is invariant under .
Lemma 2.7 (constant sign).
Assume . If a boundary component is invariant under the reflections through the two distinct planes, a first Steklov eigenfunction of has a constant sign on .
Proof.
Let and be two distinct reflection planes for . By symmetry principle [19, Theorem 1.4] and Lemma 2.2 (2), and are two reflection planes for passing through the origin. Since , they also pass through . By a similar argument in Case 1 in the proof of [19, Theorem 1.2], the first eigenfunction has a constant sign on . β
3. Main proof
Let be the convex sets in bounded by , respectively. Note that each of is well-defined by Lemma 2.4 (1). The following theorem insists that no two nested convex sets exist among .
Theorem 3.1.
There are no two distinct such that or .
Proof.
Assume . Take a coordinate plane that meets transversely and meets and . Let be the boundary components of that has an intersection with , and we denote by and for all .
We consider a graph whose vertex set is
(3.1) |
and the edges are the arcs in whose endpoints are contained in . 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)
Take the edge containing and give a direction from . Let be the other vertex in the edge.
-
(2)
Take the vertex which is contained in the same boundary component with but not identical to .
-
(3)
Repeat the first and second steps until the vertex comes out.
By the two-piece property (Theorem 2.1) with the fact that has genus zero, every edge has a direction.
We claim that the directed graph from escapes the convex cone over by an edge. Note the fact that a small part of an arc of from each of vertices and is contained outside of the convex cone over by Lemma 2.4 (2). Since we can give directions on every edge, the directed graph from escapes the convex cone over . On the other hand, the embeddedness of implies that for every , we have either or . Therefore, the directed graph escapes by an edge that meets one of the line segments and 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 that meets at least twice. It contracts the radial graphicality of (Lemma 2.3 (2)).
β
Corollary 3.2.
has distinct elements.
Proof.
Suppose for . If , we can find a coordinate plane that separates and . Then, , a contradiction. On the other hand, we consider . Since is embedded, we have either or , which contradicts Theorem 3.1. β
Corollary 3.3.
Let be a reflection plane of . Then, for , if and only if .
Proof.
It is clear that implies . Now suppose . We note that is a boundary component of , say . Then, , and by the assumption, . By Corollary 3.2, we have and . β
Lemma 3.4.
Let be distinct reflection planes of . Then, the reflection group generated by acts transitively on . Equivalently, the reflection group acts transitively on .
Proof.
Suppose the first statement is not true. We consider a graph with vertices and edges if there is a plane such that . By the assumption, this graph has at least two components. Take one of the smallest components with vertices. Then, .
We show that . Suppose and let be such vertex. Then, every reflection, , maps into . This reflections map into . If , by Corollary 3.2, only one coordinate plane passes through and . It implies that there is at most one reflection in that map into . In addition, using Lemma 2.2 (1), there are at most reflections that map into . Thus, there are at most distinct reflections in , a contradiction. Thus, . In a similar argument, we can show that , which is . It contradicts Corollary 3.2. Therefore, .
Let be the vertex set of the smallest component. By Lemma 2.2 (1), there are at most reflection planes in that do not pass through . Therefore, there must be at least reflection planes in that pass through . Suppose and . In this case, there is exactly one reflection plane in that does not pass through . Because every reflection plane passing through maps into , Lemma 2.2 further implies that there can be at most distinct reflection planes passing through in . Then, there are at most reflections in , contrary to Corollary 3.2. Therefore we can take , and we can assume is connected to by an edge. By Lemma 2.2 (1), the reflection planes in that pass through maps one-to-one into . Thus, there are at most such reflections. However, leads to a contradiction.
The second statement follows from the first statement with an argument in the proof of Corollary 3.3. β
Now we prove the main theorem.
Proof of Theorem 1.1.
The case for is trivial by the classical work by Nitsche [18]. For , our theorem is known in [19, Theorem 1.2]. Thus, we only need to consider . We prove this theorem by proof by contradiction. We assume . We will obtain a contradiction by following the steps.
Step 1. Let be the given reflection planes of . We show that for each , there is such that . By Corollary 3.3 and Lemma 2.2 (1), it is sufficient to prove that there is exactly one reflection plane in that passes through each . Suppose there are no reflection planes in that pass through . Then, by Lemma 2.2 (1), there are at most distinct reflections in , a contradiction. If there are two reflections in that pass through , by Lemma 2.7, a first eigenfunction has a constant sign on . By Lemma 3.4 with Corollary 3.3 and Lemma 2.6, has a constant sign on . It contradicts Lemma 2.5 (2).
By Step 1, for each , we can define and such that
(3.2) |
In addition, we show that each of the boundary components of has exactly two nodal points of . By Lemma 2.6 and Lemma 2.5 (2), changes its sign on each of the boundary components. In addition, every has the same number of nodal points of , and the number is at least two. By Lemma 2.4 (4), the number should be two.
Let be the nodal point of in . Then, by Lemma 2.6, . Otherwise, and . Then, by Lemma 2.6 again, cannot change its sign on , a contradiction. These nodal points divide each of the boundary components into two arcs.
Step 2. We show that the two arcs of are not congruent. Suppose not. Then, either a nontrivial rotation or a reflection that maps one component of into the other and vice versa. If there is such a reflection, it cannot be . By Lemma 2.7, has a constant sign on , a contradiction. If there is such a rotation , and . For the case of and , the rotation axis for passes through and . Since the axis meets at exactly two points, should be either or . However, lies in the interior of [19, Proposition 3.5], a contradiction. For the case of and , we note that is the 180Β°rotation through the axis passing through the origin and . Together with , has a reflection symmetry distinct from . Lemma 2.7 again gives a contradiction.
We prove the following step using an argument on arcs.
Step 3. We show that share a common axis. By the previous step, let and be the components of . Furthermore, we define an arc of that is congruent to . Clearly,
(3.3) |
Then, we have
(3.4) |
For simplicity, let and let . Then, and is either or . Note that , , and are all rotations along axes passing through the origin. Then, is a rotation along the axis passing through the origin and . Suppose is not the identity map. Since the axis and are invariant under and , each of components of lies in a plane that passes through the axis. Similarly, lies in two planes passing through the axis. Since is real analytic (see [13, Section 6]), this boundary component lies in a plane, so it is a circle. By [19, Remark 6.2], is congruent to one of an equatorial disk and a critical catenoid. It contradicts . Thus is the identity map. Then, the rotation axes of and are identical. Since each of these axes is the intersection of the two reflection planes, and contain a common axis. Since is arbitrary and
(3.5) |
we obtained our desired conclusion.
Step 4. Let -axis be the common axis of as in the previous step. By Step 1 and Lemma 2.6, every nodal point of in has the same -coordinates, say . Moreover, using (2.2), we have
(3.6) |
By Lemma 2.4 (3), does not change its sign on each of and . Thus, we have
(3.7) |
β
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 has reflection symmetries, the first Steklov eigenspace for is spanned by the three coordinate functions of .
References
- [1] Simon Brendle, Minimal surfaces in : a survey of recent results, Bull. Math. Sci. 3 (2013), no.Β 1, 133β171. MR 3061135
- [2] Alessandro Carlotto, Free boundary minimal surfaces: a survey of recent results, Rend. Accad. Sci. Fis. Mat., Napoli (4) 86 (2019), 103β121 (English).
- [3] Jaigyoung Choe, Minimal surfaces in and Yauβs conjecture, Proceedings of the 10th international workshop on differential geometry, Taegu, Korea, November 10β11, 2005, Taegu: Kyungpook National University, 2006, pp.Β 183β188 (English).
- [4] Jaigyoung Choe and Marc Soret, First eigenvalue of symmetric minimal surfaces in , Indiana Univ. Math. J. 58 (2009), no.Β 1, 269β281 (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, 1β161 (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, 183β200.
- [8] Ailana Fraser and Richard Schoen, The first Steklov eigenvalue, conformal geometry, and minimal surfaces, Adv. Math. 226 (2011), no.Β 5, 4011β4030.
- [9] by same author, Sharp eigenvalue bounds and minimal surfaces in the ball, Invent. Math. 203 (2016), no.Β 3, 823β890.
- [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 120β148.
- [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), 1β13.
- [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 401β435.
- [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, 1661β1686.
- [16] Peter McGrath, A characterization of the critical catenoid, Indiana Univ. Math. J. 67 (2018), no.Β 2, 889β897.
- [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, 1β19.
- [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. Γcole Norm. Sup. (3) 19 (1902), 455β490.
- [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, 6174β6199. 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, 521β540. 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.