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Kyungpook Mathematical Journal 2017; 57(4): 683-699

Published online December 23, 2017

Copyright © Kyungpook Mathematical Journal.

Real Hypersurfaces in the Complex Hyperbolic Quadric with Killing Shape Operator

Imsoon Jeong1
Young Jin Suh2

Division of Future Capability Education, Pai Chai University, Daejeon 35345, Republic of Korea1
Department of Mathematics & Research Institute of Real and Complex Manifolds, Kyungpook National University, Daegu 41566, Republic of Korea2

Received: April 24, 2017; Accepted: June 26, 2017

We introduce the notion of Killing shape operator for real hypersurfaces in the complex hyperbolic quadric Qm* = SOm,2/SOmSO2. The Killing shape operator implies that the unit normal vector field N becomes -principal or -isotropic. Then according to each case, we give a complete classification of real hypersurfaces in Qm* = SOm,2/SOmSO2 with Killing shape operator.

Keywords: Killing shape operator, $mathfrak A$-isotropic, $mathfrak A$-principal, K"{a}hler structure, complex conjugation, complex quadric

As examples of some Hermitian symmetric spaces of rank 2, usually we can consider Riemannian symmetric spaces SUm+2/S(U2Um) and SU2,m/S(U2Um), which are said to be complex two-plane Grassmannians and complex hyperbolic two-plane Grassmannians respectively (see [1], [2], [3], [6], [7], [8], [16], [17] and [23]). Those are said to be Hermitian symmetric spaces and quaternionic Kähler symmetric spaces equipped with the Kähler structure J and the quaternionic Kähler structure = Span{J1, J2, J3} on SU2,m/S(U2Um). The rank of SU2,m/S(U2Um) is 2 and there are exactly two types of singular tangent vectors X of SU2,m/S(U2Um) which are characterized by the geometric properties and respectively.

As another example of Hermitian symmetric space with rank 2 of compact type different from the above ones, we could give a complex quadric Qm = SOm+2/SO2SOm, which is a complex hypersurface in complex projective space CPm (see Reckziegel [14], Suh [19], [20], [22] and Smyth [15]). The complex quadric also can be regarded as a kind of real Grassmann manifolds of compact type with rank 2 (see Kobayashi and Nomizu [10]). Accordingly, the complex quadric admits two important geometric structures that a complex conjugation structure A and a Kähler structure J, which anti-commute with each other, that is, AJ = −JA. Then for m≥2 the triple (Qm, J, g) is a Hermitian symmetric space of compact type with rank 2 and its maximal sectional curvature is equal to 4 (see Klein [9] and Reckziegel [14]).

About the latter part of twentieth century, many geometers have investigated some real hypersurfaces in Hermitian symmetric spaces of rank 1 like the complex projective space ℂPm or the complex hyperbolic space ℂHm. For the complex projective space ℂPm and the quaternionic projective space ℚPm a characterization with isometric Reeb flow was obtained by Okumura [11], -parallel shape operator = 0 by Pérez [12], and -parallel curvature tensor = 0 by Pérez and Suh [13], respectively, where = Span{ξ1, ξ2, ξ3}, ξi = −JiN, i = 1, 2, 3.

Now let us introduce a complex hyperbolic quadric Qm*=SOm,2o/SO2SOm, which can be regarded as a Hermitian symmetric space with rank 2 of noncompact type. Here we consider a real hypersurface M in Qm* with shape operator of Codazzi type, that is, (∇XS)Y = (∇Y S)X for the shape operator S and any vector fields X and Y on M in Qm*. In Suh [18] we gave a non-existence property for real hypersurfaces of Codazzi type in the complex quadric Qm* as follows:

Theorem A

There do not exist any Hopf real hypersurfaces in complex quadric Qm*, m ≥ 3, with shape operator of Codazzi type.

Next we have considered the notion of parallel shape operator for real hypersurfaces M in Qm*. Usually, parallelism is naturally included in the notion of shape operator of Codazzi type. So by Theorem A we can assert the following

Theorem B

There do not exist any Hopf real hypersurfaces in complex quadric Qm*, m ≥ 3, with parallel shape operator.

Apart from the complex structure J there is another distinguished geometric structure on Qm*. Namely, a vector subbundle = {Aλ|λ ∈ S1C}, [z] ∈ Qm*, which consists of all complex conjugations defined on the complex quadric Qm*. The vector bundle contains a S1-bundle of real structures, that is, complex conjugations A on the tangent spaces of Qm* and becomes a parallel rank 2-subbundle of of End TQm*. This geometric structure determines a maximal -invariant sub-bundle of the tangent bundle TM of a real hypersurface M in Qm*.

Recall that a nonzero tangent vector WTzQm* is called singular if it is tangent to more than one maximal flat in Qm*. Here maximal flat means a 2-dimensional curvature flat maximal totally geodesic submanifold in Qm*. Such a maximal flat always exists, because the rank of Qm* is 2. There are two types of singular tangent vectors for the complex quadric Qm* as follows:

  • If there exists a conjugation such that WV (A), then W is singular. Such a singular tangent vector is called -principal.

  • If there exist a conjugation and orthonormal vectors X, YV (A) such that W/W=(X+JY)/2, then W is singular. Such a singular tangent vector is called -isotropic.

Here we note that the unit normal N is said to be -principal if N is invariant under the complex conjugation A, that is, AN = N.

Moreover, the derivative of the complex conjugation A on Qm* is defined by

(¯XA)Y=q(X)JAY

for any vector fields X and Y on M and q denotes a certain 1-form defined on M.

Recall that a nonzero tangent vector WT[z]Qm* is called singular if it is tangent to more than one maximal flat in Qm*. There are two types of singular tangent vectors for the complex quadric Qm*:

  • If there exists a conjugation such that WV (A), then W is singular. Such a singular tangent vector is called -principal.

  • If there exist a conjugation and orthonormal vectors X, YV (A) such that W/W=(X+JY)/2, then W is singular. Such a singular tangent vector is called -isotropic.

The shape operator S of M in Qm* is said to be Killing if the operator S satisfies

(XS)Y+(YS)X=0

for any X, YTzM, zM. The equation is equivalent to (∇XS)X = 0 for any XTzM, zM, because of linearization. Moreover, we can give the geometric meaning of Killing Jacobi tensor as follows:

When we consider a geodesic γ with initial conditions such that γ(0) = z and γ̇ (0) = X. Then the transformed vector field Sγ̇ is Levi-Civita parallel along the geodesic γ of the vector field X (see Blair [5] and Tachibana [24]).

In the study of real hypersurfaces in the complex quadric Qm we considered the notion of parallel Ricci tensor, that is, ∇Ric = 0 (see Suh [19]). But from the assumption of Ricci being parallel, it was difficult for us to derive the fact that either the unit normal N is -isotropic or -principal. So in [19] we gave a classification with the further assumption of -isotropic. But fortunately, when we consider Killing shape operator for real hypersurfaces in the complex hyperbolic quadric Qm*, first we can assert that the unit normal vector field N becomes either -isotropic or -principal as follows:

Main Theorem 1

Let M be a Hopf real hypersurface in the complex hyperbolic quadric Qm*, m≥3, with Killing shape operator. Then the unit normal vector field N is singular, that is, N is-isotropic or-principal.

Then motivated by such a result, next we give a complete classification for real hypersurfaces in the complex hyperbolic quadric Qm* with Killing shape operator as follows:

Main Theorem 2

Let M be a real hypersurface in the complex hyperbolic quadric Qm*, m≥4, with Killing shape operator. Then M is locally congruent to a horosphere or has 6 distinct constant principal curvatures given by

α0,β=γ=0,λ1=(α2-1)+(α2-1)2-2α22α,

and

λ2=(α2-1)-(α2-1)2-2α22α

with corresponding principal curvature spaces respectively

Tα=[ξ],Tβ=[AN],Tγ=[Aξ],φ(Tλi)=Tμi,

and

dim (Tλ1+Tλ2)=dim (Tμ1+Tμ2)=m-2.

Let us denote by C1m+2 an indefinite complex Euclidean space ℂm+2, on which the indefinite Hermitian product

H(z,w)=-z1w¯1+z2w¯2++zn+2w¯n+2

is negative definite.

The homogeneous quadratic equation z12++zm2-zm+12-zm+22=0 consists of the points in 1m+2 defines a noncompact complex hyperbolic quadric Q*m=SO2,mo/SO2SOm which can be immersed in the (m + 1)-dimensional in complex hyperbolic space ℂHm+1 = SU1,m+1/S(Um+1U1). The complex hypersurface Qm* in ℂHm+1 is known as the m-dimensional complex hyperbolic quadric. The complex structure J on ℂHm+1 naturally induces a complex structure on Q*m which we will denote by J as well. We equip Qm* with the Riemannian metric g which is induced from the Begerman metric on ℂHm+1 with constant holomorphic sectional curvature 4. For m ≥ 2 the triple (Qm*, J, g) is a Hermitian symmetric space of rank two and its minimal sectional curvature is equal to −4. The 1-dimensional quadric Q1* is isometric to the 2-dimensional real hyperbolic space H2=SO1,2o/SO1SO2. The 2-dimensional complex quadric Q2* is isometric to the Riemannian product of complex hyperbolic spaces ℂH1×H1. We will assume m ≥ 3 for the main part of this paper.

For a nonzero vector z1m+2 we denote by [z] the complex span of z, that is, [z] = {λz | λ ∈ ℂ}. Note that by definition [z] is a point in ℂHm+1. As usual, for each [z] ∈ ℂHm+1 we identify T[z]Hm+1 with the orthogonal complement 1m+2[z] of [z] in 1m+2. For [z] ∈ Qm* the tangent space T[z]Qm* can then be identified canonically with the orthogonal complement 1m+2([z][z¯]) in 1m+2. Note that ν[z]Qm* is a unit normal vector of Qm* in ℂHm+1 at the point [z].

We denote by A the shape operator of Qm* in ℂHm+1 with respect to . Then we have Aw = w for all wT[z]Qm*, that is, A is just complex conjugation restricted to T[z]Qm*. The shape operator A is an antilinear involution on the complex vector space T[z]Q*m and

T[z]Qm*=V(Az¯)JV(Az¯),

where V(Az¯)=1m+2T[z]Qm* is the (+1)-eigenspace and JV(Az¯)=i1m+2T[z]Qm* is the (−1)-eigenspace of A. Geometrically this means that the shape operator A defines a real structure on the complex vector space T[z]Qm*. Recall that a real structure on a complex vector space V is by definition an antilinear involution A : VV. Since the normal space ν[z]Qm* of Qm* in H1m+1 at [z] is a complex subspace of T[z]Hm+1 of complex dimension one, every normal vector in ν[z]Qm* can be written as λ with some λ ∈ ℂ. The shape operators Aλ of Qm* define a rank two vector subbundle of the endomorphism bundle End(TQm*). Since the second fundamental form of the embedding Qm* ⊂ ℂHm+1 is parallel (see e.g. [15]), is a parallel subbundle of End(TQm*). For λ ∈ S1 ⊂ ℂ we again get a real structure Aλ on T[z]Qm* and we have V (Aλ) = λV (A). We thus have an S1-subbundle of consisting of real structures on the tangent spaces of Qm*.

The Gauss equation for the complex hypersurface Qm* ⊂ ℂHm+1 implies that the Riemannian curvature tensor of Qm* can be expressed in terms of the Riemannian metric g, the complex structure J and a generic real structure A in :

R¯(X,Y)Z=-g(Y,Z)X+g(X,Z)Y-g(JY,Z)JX+g(JX,Z)JY+2g(JX,Y)JZ-g(AY,Z)AX+g(AX,Z)AY-g(JAY,Z)JAX+g(JAX,Z)JAY.

Note that the complex structure J anti-commutes with each endomorphism , that is, AJ = −JA.

A nonzero tangent vector WT[z]Qm* is called singular if it is tangent to more than one maximal flat in Qm*. There are two types of singular tangent vectors for the complex quadric Qm*:

  • If there exists a real structure such that WV (A), then W is singular. Such a singular tangent vector is called -principal.

  • If there exist a real structure and orthonormal vectors X, YV (A) such that W/W=(X+JY)/2, then W is singular. Such a singular tangent vector is called -isotropic.

Basic complex linear algebra shows that for every unit tangent vector WT[z]Qm* there exist a real structure and orthonormal vectors X, YV (A) such that

W=cos(t)X+sin(t)JY

for some t ∈ [0, π/4]. The singular tangent vectors correspond to the values t = 0 and t = π/4.

Let M be a real hypersurface in Qm* and denote by (φ, ξ, η, g) the induced almost contact metric structure on M and by ∇ the induced Riemannian connection on M. Note that ξ = −JN, where N is a (local) unit normal vector field of M. The vector field ξ is known as the Reeb vector field of M. If the integral curves of ξ are geodesics in M, the hypersurface M is called a Hopf hypersurface. The integral curves of ξ are geodesics in M if and only if ξ is a principal curvature vector of M everywhere. The tangent bundle TM of M splits orthogonally into , where = ker(η) is the maximal complex subbundle of TM and ℱ = ℝξ. The structure tensor field φ restricted to coincides with the complex structure J restricted to , and we have φξ = 0. We denote by νM the normal bundle of M.

We first introduce some notations. For a fixed real structure and XT[z]M we decompose AX into its tangential and normal component, that is,

AX=BX+ρ(X)N

where BX is the tangential component of AX and

ρ(X)=g(AX,N)=g(X,AN)=g(X,AJξ)=g(JX,Aξ).

Since JX = φX + η(X)N and = + ρ(ξ)N we also have

ρ(X)=g(φX,Bξ)+η(X)ρ(ξ)=η(BφX)+η(X)ρ(ξ).

We also define

δ=g(N,AN)=g(JN,JAN)=-g(JN,AJN)=-g(ξ,Aξ).

At each point [z] ∈ M we define

Q[z]={XT[z]MAXT[z]Mfor all AA[z]},

which is the maximal -invariant subspace of T[z]M. Then by using the same method for real hypersurfaces in Q*m as in Berndt and Suh [4] we get the following

Lemma 2.1

Let M be a real hypersurface in the complex hyperbolic quadric Qm*. Then the following statements are equivalent:

  • The normal vector N[z]of M is-principal,

  • ,

  • There exists a real structuresuch that AN[z] ∈ ℂν[z]M.

Assume now that the normal vector N[z] of M is not -principal. Then there exists a real structure such that

N[z]=cos(t)Z1+sin(t)JZ2

for some orthonormal vectors Z1, Z2V (A) and 0<tπ4. This implies

N[z]=cos(t)Z1+sin(t)JZ2,AN[z]=cos(t)Z1-sin(t)JZ2,ξ[z]=sin(t)Z2-cos(t)JZ1,Aξ[z]=sin(t)Z2+cos(t)JZ1,

and therefore = T[z]Qm ⊝ ([Z1] ⊕ [Z2]) is strictly contained in . Moreover, we have

Aξ[z]=Bξ[z]and ρ(ξ[z])=0.

We have

g(Bξ[z]+δξ[z],N[z])=0,g(Bξ[z]+δξ[z],δ[z])=0,g(Bξ[z]+δξ[z],Bξ[z]+δξ[z])=sin2(2t),

where the function δ denotes δ = −g(ξ, Aξ) = −(sin2t − cos2t) = cos2t. Therefore

U[z]=1sin(2t)(Bξ[z]+δξ[z])

is a unit vector in and

C[z]=Q[z][U[z]](orthogonal sum).

If N[z] is not -principal at [z], then N is not -principal in an open neighborhood of [z], and therefore U is a well-defined unit vector field on that open neighborhood. We summarize this in the following

Lemma 2.2

Let M be a real hypersurface in the complex hyperbolic quadric Qm* whose unit normal N[z]is not-principal at [z]. Then there exists an open neighborhood of [z] in M and a section A inon that neighborhood consisting of real structures such that

  • = Bξ and ρ(ξ) = 0,

  • U = ( + δξ)/||Bξ + δξ|| is a unit vector field tangent to,

  • ⊕ [U].

From the explicit expression of the Riemannian curvature tensor of the complex hyperbolic quadric Qm* we can easily derive the Codazzi equation for a real hypersurface MQ*m:

g((XS)Y-(YS)X,Z)=-η(X)g(φY,Z)+η(Y)g(φX,Z)+2η(Z)g(φX,Y)-ρ(X)g(BY,Z)+ρ(Y)g(BX,Z)+η(BX)g(BY,φZ)+η(BX)ρ(Y)η(Z)-η(BY)g(BX,φZ)-η(BY)ρ(X)η(Z).

We now assume that M is a Hopf hypersurface. Then the shape operator S of M in Qm* satisfies

Sξ=αξ

with the smooth function α = g(Sξ, ξ) on M. Inserting Z = ξ into the Codazzi equation leads to

g((XS)Y-(YS)X,ξ)=2g(φX,Y)-2ρ(X)η(BY)+2ρ(Y)η(BX).

On the other hand, we have

g((XS)Y-(YS)X,ξ)=g((XS)ξ,Y)-g((YS)ξ,X)=dα(X)η(Y)-dα(Y)η(X)+αg((Sφ+φS)X,Y)-2g(SφSX,Y).

Comparing the previous two equations and putting X = ξ yields

dα(Y)=dα(ξ)η(Y)+2δρ(Y),

where δ denotes δ = −g(Aξ, ξ). Reinserting this into the previous equation yields

g((XS)Y-(YS)X,ξ)=-2δη(X)ρ(Y)+2δρ(X)η(Y)+αg((φS+Sφ)X,Y)-2g(SφSX,Y).

Altogether this implies

0=2g(SφSX,Y)-αg((φS+Sφ)X,Y)+2g(φX,Y)-2δρ(X)η(Y)-2ρ(X)η(BY)+2ρ(Y)η(BX)+2δη(X)ρ(Y)=g((2SφS-α(φS+Sφ)+2φ)X,Y)-2ρ(X)η(BY+δY)+2ρ(Y)η(BX+δX)=g((2SφS-α(φS+Sφ)+2φ)X,Y)-2ρ(X)g(Y,Bξ+δξ)+2g(X,Bξ+δξ)ρ(Y).

If AN = N we have ρ = 0, otherwise we can use Lemma 2.2 to calculate ρ(Y) = g(Y,AN) = g(Y, AJξ) = −g(Y, JAξ) = −g(Y, JBξ) = −g(Y, φBξ). Thus we have proved

Lemma 3.1

Let M be a Hopf hypersurface in the complex hyperbolic quadric Qm*, m ≥ 3. Then we have

(2SφS-α(φS+Sφ)+2φ)X=2ρ(X)(Bξ+δξ)+2g(X,Bξ+δξ)φBξ.

If the unit normal vector field N is -principal, we can choose a real structure such that AN = N. Then we have ρ = 0 and φBξ = −φξ = 0, and therefore

2SφS-α(φS+Sφ)=-2φ.

If N is not -principal, we can choose a real structure as in Lemma 2.2 and get

ρ(X)(Bξ+δξ)+g(X,Bξ+δξ)φBξ=-g(X,φ(Bξ+δξ))(Bξ+δξ)+g(X,Bξ+δξ)φ(Bξ+δξ)=Bξ+δξ2(g(X,U)φU-g(X,φU)U)=sin2(2t)(g(X,U)φU-g(X,φU)U),

which is equal to 0 on and equal to sin2(2t)φX on . Altogether we have proved:

Lemma 3.2

Let M be a Hopf hypersurface in the complex hyperbolic quadric Qm*, m ≥ 3. Then the tensor field

2SφS-α(φS+Sφ)

leavesandinvariant and we have

2SφS-α(φS+Sφ)=-2φon Q

and

2SφS-α(φS+Sφ)=-2δ2φon CQ,

where δ = −g(Aξ, ξ) = cos2t as in Section 3.

Let us put AX = BX + ρ(X)N for any vector field XTzQm*, zM, ρ(X) = g(AX,N), where BX and ρ(X)N respectively denote the tangential and normal component of the vector field AX. Then = + ρ(ξ)N and ρ(ξ) = g(Aξ,N) = 0. Then it follows that

AN=AJξ=-JAξ=-J(Bξ+ρ(ξ)N)=-(φBξ+η(Bξ)N).

The shape operator S of M in the complex hyperbolic quadric Qm* is said to be Killing if the operator S satisfies

(XS)Y+(YS)X=0

for any X, YTzM, zM.

From (4.1), together with the equation of Codazzi, it follows that

2g((XS)Y,Z)=-η(X)g(φY,Z)+η(Y)g(φX,Z)+2η(Z)g(φX,Y)-g(X,AN)g(AY,Z)+g(Y,AN)g(AX,Z)-g(X,Aξ)g(JAY,Z)+g(Y,Aξ)g(JAX,Z).

Since we have assumed the real hypersurface M in Qm* is Hopf, then = αξ. This gives

(XS)ξ=(Xα)ξ+αφSX-SφSX.

From this, let us put Y = ξ in (4.2) and use g(Aξ,N) = 0, we see that

2g((Xα)ξ+αφSX-SφSX,Z)=g(φX,Z)-g(X,AN)g(Aξ,Z)-g(X,Aξ)g(JAξ,Z)+g(ξ,Aξ)g(JAX,Z).

Here, let us put X = ξ in (4.3) and also use g(ξ,AN) = 0, we have

2(ξα)η(Z)=-g(ξ,Aξ)g(JAξ,Z)+g(ξ,Aξ)g(JAξ,Z)=0.

From this we get ξα = 0. Then the derivative Y α in Section 3 becomes

Yα=-2g(Y,AN)g(ξ,Aξ).

From this, together with (4.3), it follows that

2g(-2g(X,AN)g(ξ,Aξ)ξ+αφSX-SφSX,Z)=g(φX,Z)-g(X,AN)g(Aξ,Z)-g(X,Aξ)g(JAξ,Z)+g(ξ,Aξ)g(JAX,Z).

Then by putting Z = ξ into (4.3), we have

-4g(X,AN)g(ξ,Aξ)=-g(X,AN)g(Aξ,ξ)-g(X,Aξ)g(JAξ,ξ)+g(ξ,Aξ)g(JAX,ξ)=-2g(X,AN)g(Aξ,ξ).

Since g(Aξ,N) = 0, (4.6) gives that

g(Aξ,ξ)g(AN,X)=0.

Then we have g(Aξ, ξ) = 0 or (AN)T = 0, where (AN)T denotes the tangential part of the vector AN.

Summing up above discussions, we conclude the following

Lemma 4.1

Let M be a Hopf real hypersurface in the complex hyperbolic quadric Qm*, m≥3, with Killing shape operator. Then the unit normal vector field N is singular, that is, N is-isotropic or-principal.

Proof

In above discussion, let us consider the first case g(Aξ, ξ) = 0. Then it implies that

0=g(Aξ,ξ)=g(AJN,JN)=-g(JAN,JN)=-g(AN,N).

If we insert N = costZ1 + sintJZ2 for Z1, Z2V (A) into the above equation, we have cos2t−sin2t = 0. Then by Section 2, we have t=π4, that is, N=12(X+JY) for some X, YV (A). So the unit normal N is -isotropic.

Next we consider the case that (AN)T = 0. Then AN = (AN)T+g(AN,N)N = g(AN,N)N. So it follows that

N=A2N=g(AN,N)AN=g2(AN,N)N.

So g(AN,N) = ±1 gives that AN = ±N.

That is, the unit normal N is -principal.

Then we are able to consider the classification of Killing shape operator S of M in Qm* into two cases that the unit normal N is -principal or N is -isotropic. In Section 5 we will discuss a classification of real hypersurfaces in Qm* with Killing shape operator and -isotropic unit normal and in Section 6 a non-existence of Killing shape operator for hypersurfaces in Qm when N is -principal will be explained in detail.

In this section let us assume that the unit normal vector field N is -isotropic. Then the normal vector field N can be written

N=12(Z1+JZ2)

for Z1, Z2V (A), where V (A) denotes the (+1)-eigenspace of the complex conjugation . Then it follows that

AN=12(Z1-JZ2),AJN=-12(JZ1+Z2),and JN=12(JZ1-Z2).

From this, together with anti-commuting AJ = −JA, it follows that

g(ξ,Aξ)=g(JN,AJN)=0,g(ξ,AN)=0and g(AN,N)=0.

Then (4.3) gives the following for any X,ZTzM, zM

2g(αφSX-SφSX,Z)=g(φX,Z)-g(X,AN)g(Aξ,Z)-g(X,Aξ)g(JAξ,Z)=g(φX,Z)-g(X,AN)g(Aξ,Z)+g(X,Aξ)g(AN,Z).

Since Aξ,ANTzM, zM, it implies

2(αφSX-SφSX)=φX-g(X,AN)Aξ+g(X,Aξ)AN.

On the other hand, we have the following from Lemma 3.1 in Section 3 a Hopf real hypersurface M with -isotropic unit normal N

2SφSX=α(Sφ+φS)X-2φX+2g(X,AN)Aξ-2g(X,Aξ)AN.

Then by virtue of (5.2) and (5.3), first we have

-SφSX=-2αφSX+α2(φS+Sφ)X.

Then naturally it follows that

-2SφSX=αSφX-3αφSX.

We know that the tangent space TzM, zM is decomposed as follows:

TzM=[ξ][Aξ,AN]Q,

where = Span[Aξ,AN].

Lemma 5.1

Let M be a Hopf real hypersurface in the complex hyperbolic quadric Qm*, m≥3, with-isotropic unit normal vector field. Then

SAN=0,         and         SAξ=0.
Proof

Let us denote by = Span[Aξ,AN]. Since N is isotropic, g(AN,N) = 0 and g(Aξ, ξ) = 0. By differentiating g(AN,N) = 0 and using (∇̄XA)Y = q(X)JAY and the equation of Weingarten, we know that

0=g(¯X(AN),N)+g(AN,¯XN)=g(q(X)JAN-ASX,N)-g(AN,SX)=-2g(ASX,N).

Then SAN = 0. Moreover, by differentiating g(Aξ,N) = 0 and using g(AN,N) = 0, we have the following formula

0=g(¯X(Aξ),N)+g(Aξ,¯XN)=g(q(X)JAξ+A(φSX+g(SX,ξ)N),N)-g(SAξ,X)=-2g(SAξ,X)

for any XTzM, zM, where in the third equality we have used φAN = JAN = −AJN = . Then it follows that

SAξ=0.

It completes the proof of our assertion.

By Lemma 5.1 we know that the distribution for a Hopf real hypersurface M in Qm* is invariant by the shape operator S, so the distribution is also S invariant. From this fact we may consider a principal curvature vector such that SX = λX, because the distribution can be diagonalized. Then (5.4) gives

SφX=3αλ2λ+αφX.

In fact, if 2λ + α = 0, then 0 = αλ = −2λ2. This implies α = λ = 0. Then (5.3) gives φX = 0 for . This leads a contradiction.

For , we knowthat g(X,AN) = g(X,Aξ) = 0. So (5.3) gives the following

2SφSX=α(Sφ+φS)X-2φX.

Then we consider two cases for or .

As a first, for such that SX = λX the formula (5.6) gives

2λSφX=αSφX+(αλ-2)φX.

Then we can consider two cases as follows:

Case 1. α = 2λ

Then αλ = 2 gives α = 2 and λ = 1 with multiplicities 1 and 2(m − 2) respectively. This case implies that the shape operator commutes with the structure tensor, that is, = φS. Then by a result due to Suh [21], M is locally congruent to a horosphere.

Case 2. α = 2λ

Then (5.7) gives that

SφX=μφX         where μ=αλ-22λ-α.

Then (5.5) and (5.8) give

αλ-22λ-αφX=2αλ2λ+αφX.

From this, any principal curvatures λ and μ of the distribition satisfy the following quadratic equation

2αλ2-2(α2-1)λ+α=0.

The solutions become the following constant principal curvatures given by

λ1,λ2=(α2-1)±(α2-1)2-2α22α,

because the Reeb function α is constant for -isotropic unit normal N. Here we note that the Reeb function α can not vanishing. If the function α identically vanishes, then (5.9) gives λ = 0. From this, together with (5.7), we have φX = 0, which implies a contradiction.

From this, together with Lemma 5.1, the expression of the shape operator becomes the following

S=[α00000000000000000000000λi0000000λi0000000μi0000000μi].

Here the principal curvatures λ1 and λ2 are given by (5.10) with multiplicities p + q = m − 2 where dimTλ1 = p and dimTλ2 = q, respectively. Moreover, the principal curvatures μi (i = 1, 2) with respect to the eigenspaces Tμi = φ(Tλi) satisfy μi=αλi-22λi-α, respectively.

Summing up the above discussions, we give the following

Theorem 5.2

Let M be a real hypersurface in the complex hyperbolic quadric Qm* with-isotropic unit normal vector field. Then M is locally congruent to a horosphere or M has 4 distinct constant principal curvatures given by

α0,β=γ=0,λ1=(α2-1)+(α2-1)2-2α22α,andλ2=(α2-1)-(α2-1)2-2α22α

with corresponding principal curvature spaces respectively

Tα=[ξ],Tβ=[AN],Tγ=[Aξ],φ(Tλi)=Tμi,

and

dim (Tλ1+Tλ2)=dim (Tμ1+Tμ2)=m-2.

In this section let us consider a real hypersurface M in the complex hyperbolic quadric Qm* with Killing shape operator for the case that the unit normal N is -principal. In this case the Killing shape operator (4.3) gives that

2g({αφSX-SφSX},Z)=g(φX,Z)-g(φAX,Z),

where we have used g(ξ,Aξ) = −1 and JAX = φAX + η(AX)N. Then it follows that

2(αφSX-SφSX)=φX-φAX.

Since the unit normal vector field N is -principal, = −ξ. Then differentiating this and using Gauss equation give

X(Aξ)=¯X(Aξ)-g(SX,Aξ)N=-q(X)N+AφSX+2αη(X)N,

where q denotes a certain 1-form defined on M as in the introduction. From this, together with ∇X() = −∇Xξ = −φSX, it follows that

-φSX=-q(X)N+AφSX+2αη(X)N.

By taking the inner product of (6.3) with the unit normal N, we have q(X) = 2αη(X). From this, we know

AφSX=-φSX.

So when we consider SX = λX for and λ = 0, (6.4) becomes AφX = −φX, where the distribution denotes the orthogonal complement of the Reeb vector field ξ. When the principal curvature λ = 0, SX = 0 in (6.1) gives that

φAX=φX.

Accordingly, for any cases we know that

AX=X-2η(X)ξ.

Then we have

TrA=g(AN,N)+i=12m-1g(Aei,ei)=1+i=12m-1g(ei-2η(ei)ξ,ei)=2(m-1).

But TrA = 0, because TzQm = V (A) ⊕ JV (A), where V (A) = {XTzQm*|AX = X} and JV (A) = {XTzQm|AX = −X}. This leads to a contradiction, which implies another theorem as follows:

Theorem 6.1

There do not exist any real hypersurface in the complex hyperbolic quadric Qm* with Killing shape operator if the unit normal vector field is-principal.

Summing up all of discussions including Sections 4 and 5, by Lemma 4.1, Theorems 5.2 and 6.1, we give a complete proof of our Main Theorem 2 in the introduction.

This work was supported by grant Proj. No. NRF-2015-R1A2A1A-01002459 from National Research Foundation of Korea. The first author was supported by NRF-2017-R1A2B4005317.

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