Some New Characterizations of Real Hypersurfaces with Isometric Reeb Flow in Complex Two-Plane Grassmannians
Abstract
In this note, we establish an integral inequality for compact and orientable real hypersurfaces in complex two-plane Grassmannians G2(ℂm+2), involving the shape operator A and the Reeb vector field ξ. Moreover, this integral inequality is optimal in the sense that the real hypersurfaces attaining the equality are completely determined. As direct consequences, some new characterizations of the real hypersurfaces in G2(ℂm+2) with isometric Reeb flow can be presented.
1. Introduction
The complex two-plane Grassmannian G2(ℂm+2) consists of all complex two-dimensional linear subspaces in ℂm+2 and is of complex dimension 2m. It is known as the unique compact irreducible Hermitian symmetric space of rank two equipped with a Kähler structure J and a quaternionic Kähler structure satisfying JJa = JaJ for a ∈ {1, 2, 3} (cf. [1, 2]). When m = 1, G2(ℂ3) is isometric to the two-dimensional complex projective space ℂP2(8) with constant holomorphic sectional curvature 8, whereas when m = 2, G2(ℂ4) can be identified with the real Grassmannian manifold of oriented two-dimensional linear subspace in ℝ6 (cf. [3, 4]). For the purpose of this note, we shall assume m ≥ 3.
Let M be a connected and orientable real hypersurface isometrically immersed in G2(ℂm+2) for m ≥ 3 and N be a unit normal vector field along M. Then, the almost contact structure vector field ξ defined by ξ = −JN is said to be the Reeb vector field. In particular, such a hypersurface is called Hopf if its shape operator A satisfies Aξ = αξ with α = g(Aξ, ξ), where g is the induced metric on M. Moreover, we denote by {ξ1, ξ2, ξ3} the almost contact 3-structure vector fields, where ξa = −JaN for a ∈ {1, 2, 3} and {Ja} is a canonical local basis of . For the real hypersurface M in G2(ℂm+2), there exist naturally two distributions, which we write as [ξ] = Span{ξ} and , respectively.
The study of real hypersurfaces in initiated by Berndt and Suh [1, 5] is an attractive geometric topic, and many interesting results have been established in the last few decades; for details, see, e.g., [4, 6–16] and the references therein. In [1], Berndt and Suh considered the real hypersurfaces in G2(ℂm+2) for m ≥ 3 such that both [ξ] and are invariant under the shape operator A and they obtained the following well-known classification result:
Theorem 1. Let M be a connected real hypersurface in G2(ℂm+2), m ≥ 3. Then, both [ξ] and are invariant under the shape operator of M if and only if one of the following holds:
- (A)
M is an open part of a tube around a totally geodesic G2(ℂm+1) in G2(ℂm+2)
- (B)
m is even, say m = 2n, and M is an open part of a tube around a totally geodesic ℍPn in G2(ℂm+2)
Since then, a number of interesting characterization results related to these Hopf hypersurfaces of types (A) and (B) have been obtained. For instance, it was proved in [17] that a Hopf hypersurface in G2(ℂm+2) for m ≥ 3 must be the one of type (B) if and only if the Reeb vector ξ belongs to the orthogonal complement of . In addition, more characterizations of real hypersurfaces of type (B) can be found in [18, 19]. On the other hand, for the real hypersurface M of type (A), Berndt and Suh also gave a characterization under the assumption that the shape operator A commutes with the structure tensor ϕ, i.e., Aϕ = ϕA. This is equivalent to the condition that the Reeb flow on M is isometric, which means with the Lie derivative in the direction of ξ. More precisely, it can be stated as follows:
Theorem 2. Let M be a connected real hypersurface in G2(ℂm+2), m ≥ 3. Then, the Reeb flow on M is isometric if and only if M is an open part of a tube around a totally geodesic G2(ℂm+1) in G2(ℂm+2).
In this note, motivated by this line, we establish an integral inequality for these compact real hypersurfaces in G2(ℂm+2) for m ≥ 3, and its equality case provides a new characterization of real hypersurfaces with isometric Reeb flow.
Theorem 3. Let M be a compact orientable real hypersurface in G2(ℂm+2), m ≥ 3. Then, in terms of the shape operator A and the Reeb vector field ξ of M, we have the following integral inequality of Simons’ type:
Moreover, the equality in (1) holds if and only if M has isometric Reeb flow and M is a tube around a totally geodesic G2(ℂm+1) in G2(ℂm+2).
Then, for closed orientable real hypersurfaces in G2(ℂm+2) with m ≥ 3, Theorem 3 immediately gives the following rigidity theorem, involving the shape operator A and the Reeb vector field ξ.
Corollary 4. Let M be a compact orientable real hypersurface in G2(ℂm+2), m ≥ 3. If on M it holds
Remark 5. To obtain the inequality in (1), the key idea is to apply the classical Yano’s formula as it has been dealt with for hypersurfaces of other ambient spaces [20, 21]. Specifically, for such real hypersurfaces in G2(ℂm+2)(m ≥ 3) with isometric Reeb flow, the Reeb vector filed ξ belongs to the distribution (cf. [22]).
Remark 6. According to Corollary 4, it is known that, if ‖A‖2 ≤ 4m holds on a closed minimal orientable real hypersurface M in G2(ℂm+2) for m ≥ 3, then ‖A‖2 = 4m and M is a tube around a totally geodesic G2(ℂm+1) in G2(ℂm+2) with radius .
2. Preliminaries
In this section, we review some basic geometric properties of real hypersurfaces in complex two-plane Grassmannians G2(ℂm+2) and also derive some fundamental equations which shall be used in the proof of Theorem 3. More details can be found in the references [3, 23, 24].
3. Proof of Theorem 3
To complete the proof and obtain new characterizations, in this section, we first recall an important property related to the principal curvatures of such special real hypersurfaces of type (A). It is stated as follows (cf. [1, 22]).
Proposition 7. Let M be the tube of radius around the totally geodesic G2(ℂm+1) in G2(ℂm+2) for m ≥ 3. Choose to be the almost Hermitian structure such that JN = J1N. Then, M has three (if ) or four (otherwise) distinct constant principal curvatures. Their values and corresponding principal curvature spaces and multiplicities are given in Table 1. ℍξ denotes quaternionic span of the Reeb vector field ξ.
Principal curvature | Eigenspace | Multiplicity |
---|---|---|
|
Span{ξ1} | 1 |
|
Span{ξ2, ξ3} | 2 |
|
{X|X⊥ℍξ, JX = J1X} | 2m − 2 |
0 | {X|X⊥ℍξ, JX = −J1X} | 2m − 2 |
Next, as a crucial step towards the proof of Theorem 3, we introduce the classical formula in Riemannian geometry, which was first proved by Yano [25] using tensor analysis. For reader’s convenience, we include a proof here (cf. [20, 21]).
Lemma 8. Let (M, g) be a Riemannian manifold with Levi-Civita connection ∇. Then, for any tangent vector field X on M, it holds that
Proof. Choose {ei} to be an orthonormal basis of M and assume that X = ∑iXiei. Then, by adopting the usual notations for components of the covariant derivatives and the Riemannian curvature tensor, we have
By using the Ricci identity , we get
Similarly, straightforward calculations give
From the above calculations, the assertion (12) follows immediately.
3.1. Completion of the Proof of Theorem 3.
This completes the proof of Theorem 3.
Conflicts of Interest
The authors declare that they have no competing interests.
Acknowledgments
This project was supported by grant of the NSFC (No. 11801011) and the Key Scientific Research Projects of Colleges and Universities of Henan Province (No. 23A110001).
Open Research
Data Availability
No data were used to support this study.