Volume 2023, Issue 1 2347915
Research Article
Open Access

Some New Characterizations of Real Hypersurfaces with Isometric Reeb Flow in Complex Two-Plane Grassmannians

Dehe Li

Corresponding Author

Dehe Li

School of Mathematics and Statistics, Anyang Normal University, Anyang 455000, China aynu.edu.cn

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Bo Li

Bo Li

School of Mathematics and Statistics, Anyang Normal University, Anyang 455000, China aynu.edu.cn

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Lifen Zhang

Lifen Zhang

School of Mathematics and Statistics, Anyang Normal University, Anyang 455000, China aynu.edu.cn

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First published: 10 March 2023
Academic Editor: Manuel De Leon

Abstract

In this note, we establish an integral inequality for compact and orientable real hypersurfaces in complex two-plane Grassmannians G2(m+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(m+2) with isometric Reeb flow can be presented.

1. Introduction

The complex two-plane Grassmannian G2(m+2) consists of all complex two-dimensional linear subspaces in m+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(3) is isometric to the two-dimensional complex projective space P2(8) with constant holomorphic sectional curvature 8, whereas when m = 2, G2(4) can be identified with the real Grassmannian manifold of oriented two-dimensional linear subspace in 6 (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(m+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(m+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, 616] and the references therein. In [1], Berndt and Suh considered the real hypersurfaces in G2(m+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(m+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(m+1) in G2(m+2)

  • (B)

    m is even, say m = 2n, and M is an open part of a tube around a totally geodesic Pn in G2(m+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(m+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(m+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(m+1) in G2(m+2).

In this note, motivated by this line, we establish an integral inequality for these compact real hypersurfaces in G2(m+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(m+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:

(1)
where H = trA denotes the mean curvature of M and ‖·‖ is the tensorial norm with respect to the induced metric g of M.

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(m+1) in G2(m+2).

Then, for closed orientable real hypersurfaces in G2(m+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(m+2), m ≥ 3. If on M it holds

(2)
then it must be the case that ‖A2Hg(Aξ, ξ) = 4m and M is a tube around a totally geodesic G2(m+1) in G2(m+2).

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(m+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 ‖A2 ≤ 4m holds on a closed minimal orientable real hypersurface M in G2(m+2) for m ≥ 3, then ‖A2 = 4m and M is a tube around a totally geodesic G2(m+1) in G2(m+2) with radius .

2. Preliminaries

In this section, we review some basic geometric properties of real hypersurfaces in complex two-plane Grassmannians G2(m+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].

Let M be a connected and oriented real hypersurface isometrically immersed in G2(m+2) equipped with a Kähler structure J and a quaternionic Kähler structure not containing J. Denote by the Levi-Civita connection of the Riemannian metric g on G2(m+2) and by ∇ the Levi-Civita connection of the induced metric denoted still by g on M, respectively. Then, for a unit normal vector field N of M, the formulas of Gauss and Weingarten are given by
(3)
where A denotes the shape operator of M and X, Y are tangent vector fields on M.
For any XTM, we can decompose JXTG2(m+2) as
(4)
where ϕ denotes a tensor field of type (1) on M and η is the 1-form over M, corresponding to the Reeb vector field ξ. Then, the almost contact metric structure (ϕ, ξ, η, g) induced from J satisfies the following relations:
(5)
Choose {J1, J2, J3} to be a canonical local basis of , and for a ∈ {1, 2, 3}, put
(6)
This induces a local almost contact metric 3-structure (ϕa, ξa, ηa, g) on M satisfying
(7)
From the relation JaJa+1 = Ja+2 = −Ja+1Ja, we further obtain
(8)
where the index is taken modulo three.
Noting that JJa = JaJ, we have the relationships between these two almost contact metric structures (ϕ, ξ, η, g) and (ϕa, ξa, ηa, g) as below:
(9)
Moreover, for X, Y, ZTM, the Gauss equation of M in G2(m+2) is given by
(10)
By contracting Y and Z in (10), we have the following expression of the Ricci tensor of M:
(11)
where H = trA is the mean curvature of the real hypersurface M in G2(m+2).

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(m+1) in G2(m+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. ξ denotes quaternionic span of the Reeb vector field ξ.

Table 1. Principal curvatures and corresponding eigenspaces.
Principal curvature Eigenspace Multiplicity
Span{ξ1} 1
Span{ξ2, ξ3} 2
{X|Xξ, JX = J1X} 2m − 2
0 {X|Xξ, 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

(12)
where is the Lie derivative of g with respect to X and ‖·‖ denotes the length with respect to g.

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

(13)

By using the Ricci identity , we get

(14)

Similarly, straightforward calculations give

(15)

From the above calculations, the assertion (12) follows immediately.

3.1. Completion of the Proof of Theorem 3.

With the help of the formulas of Gauss and Weingarten in (3), we derive from and (4) that for XTM, it holds
(16)
Then, for the convenience of calculation, we choose to be an orthonormal basis of TxM for any point xM. Using (16), by definition, we obtain
(17)
which is equivalent to
(18)
From (5) and (16), it follows that
(19)
Noting that the structure tensor ϕ and the shape operator A of M is skew-symmetric and symmetric with respect to the induced metric g on M, respectively, from (16), we calculate
(20)
Moreover, by virtue of (11), we have
(21)
Thus, by putting X = ξ in (12) and applying equations (18)–(21), we derive from Lemma 8 that
(22)
By the compactness of M, we integrate the above equation and a divergence theorem for compact manifolds yields
(23)
where . In particular, the above equality holds if and only if Aϕ = ϕA and , or equivalently, and . Hence, the assertion follows from the combination of Theorem 2 and Remark 5.
On the other hand, according to Table 1 in Proposition 7, a direct calculation gives us that in a tube of radius , it holds
(24)
which implies that ‖A2 = 4m + Hg(Aξ, ξ) holds identically. In particular, it can be checked that the mean curvature H vanishes if and only if , which belongs to the interval when m ≥ 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).

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