Hopf hypersurfaces in nonflat complex space forms
Makoto Kimura
Department of Mathematics, Ibaraki University, Mito, Ibaraki 310-8512, Japan
e-mail : [email protected] (2010 Mathematics Subject Classification : 53C40.)
Abstract. We study Hopf hypersurfaces in non-flat complex space forms by using some Gauss maps from a real hypersurface to complex (either positive definite or indefinite) 2-plane Grassmannian and quaternionic (para-)K¨ahler structures.
1 Introduction
Among real hypersurfaces in complex space forms, Hopf hypersurfaces have good geometric properties and studied widely. A real hypersurfaceM in a complex space form Mf(c) (of constant holomorphic sectional curvature 4c) is called Hopf if the structure vector ξ=−J N is an eigenvector of the shape operatorA of M. We say that the (constant) eigenvalue µ with Aξ =µξ a Hopf curvature of Hopf hypersurface M. Whenc >0, Cecil and Ryan [4] proved that a Hopf hypersurface M with Hopf curvature µ = 2 cot 2r (0 < r < π/2) lies on the tube of radius r over a complex submanifold in CPn, provided that the focal mapφr :M →CPn, φr(x) = expx(rNx) (x ∈ M, Nx ∈ Tx⊥M, |Nx| = 1) has constant rank on M. After that Montiel [15] proved similar result for Hopf hypersurfaces withlarge Hopf curvature, (i.e., |µ|>2) in complex hyperbolic spaceCHn (with c=−1). On the other hand, Ivey [7] and Ivey-Ryan [8] proved that a Hopf hypersurface with|µ|<2 in CHn may be constructed from an arbitrary pair of Legendrian submanifolds in S2n−1.
Here we will study (Hopf) hypersurfacesM inCPn (resp. CHn) by using some Gauss map G(resp. G) frome M to complex 2-plane GrassmannianG2(Cn+1) (resp.
Grassmannian G1,1(Cn+11 ) of 2-planes with signature (1,1) in Cn+11 ), which maps each point of M to the 2-plane spanned by position vector and structure vector
Key words and phrases:
* This work was supported by grant Proj. No. 24540080 from Grants-in-Aid for Scientific Research, the Ministry of Education, Science, Sports and Culture, Japan.
25
at the point in M. We see that: If M is a Hopf hypersurface in CPn, then the Gauss imageG(M) is a real (2n−2)-dimensionaltotally complex submanifold with respect to quaternionic K¨ahler structure in G2(Cn+1) (Theorem 4.1). If M is a Hopf hypersurface inCHn with (constant) Hopf curvatureµ, then the Gauss image G(Me ) is a real (2n−2)-dimensional submanifold and invariant under a quaternionic (para-)K¨ahler structureI ofG1,1(Cn+11 ) satisfying
1. I2=−1 provided|µ|>2, 2. I2= 1 provided|µ|<2, 3. I2= 0 provided|µ|= 2
(Theorem 6.1). Detailed descriptions will appear elsewhere.
The author would like to thank Professor Young Jin Suh for inviting me to this international workshop.
2 Real hypersurfaces in CPn and CHn
First we recall the Fubini-Study metric on the complex projective space CPn (cf. [4, 11]). The Euclidean metric h, ion Cn+1 is given byhz, wi= Re(tzw) for¯ z, w∈Cn+1. The unit sphereS2n+1 inCn+1 is the principal fiber bundle overCPn with the structure groupS1 and the Hopf fibrationπ:S2n+1→CPn. The tangent space ofS2n+1 at a pointz is
TzS2n+1={w∈Cn+1|hz, wi= 0}.
Let
Tz0 ={w∈Cn+1|hz, wi=hiz, wi= 0}.
With respect to the principal fiber bundle S2n+1(CPn, S1), there is a connection such that Tz0 is the horizontal subspace at z. Then the Fubini-Study metric g of constant holomorphic sectional curvature 4 is given byg(X, Y) =hX∗, Y∗i, where X, Y ∈TxCPn, andX∗, Y∗ are respectively their horizontal lifts at a pointz with π(z) =x. The complex structure onT0 defined by multiplication by√
−1 induces a canonical complex structureJ onCPn throughπ∗.
Next we recall the metric of negative constant holomorphic sectional curvature on the complex hyperbolic space CHn (cf. [15, 11]). The indefinite metrich, iof index 2 onCn+1 is given by
hz, wi= Re −z0w¯0+
n
X
k=1
zkw¯k
!
for z = (z0, z1, . . . , zn), w= (w0, w1, . . . , wn)∈ Cn+1. The anti de Sitter space is defined by
H12n+1={z∈Cn+1| hz, zi=−1}.
H12n+1 is the principal fiber bundle overCHn with the structure group S1 and the fibrationπ:H12n+1 →CHn. The tangent space ofH12n+1 at a pointzis
TzH12n+1={w∈Cn+1|hz, wi= 0}.
Let
Tz0 ={w∈Cn+1|hz, wi=hiz, wi= 0}.
We observe that the restriction ofh, ito Tz0 is positive-definite. The distribution Tz0 defines a connection in the principal fiber bundleH12n+1(CHn, S1), becauseTz0 is complementary to the subspace {iz} tangent to the fibre throughz, and invariant under theS1-action. Then the metricgof constant holomorphic sectional curvature
−4 is given byg(X, Y) =hX∗, Y∗i, whereX, Y ∈TxCHn, andX∗, Y∗ are respec- tively their horizontal lifts at a point z withπ(z) =x. The complex structure on T0 defined by multiplication by √
−1 induces a canonical complex structureJ on CHn throughπ∗.
We recall some facts about real hypersurfaces in complex space forms. Let Mfn(c) be a space of constant holomorphic sectional curvature 4cwith real dimension 2n. LetJ:TMf→Mfbe the complex structure with properties J2=−1,∇Je = 0, and hJ X, J Yi=hX, Yi, where∇e is the Levi-Civita connection of Mf. LetM2n−1 be a real hypersurface inMf(c) and letN be a local unit normal vector field ofM in Mf. We definestructure vector ofM asξ=−J N.
Ifξis a principal vector, i.e.,Aξ=µξholds for the shape operator ofM inMf, M is called a Hopf hypersurface and µ is called Hopf curvature. It is well known ([13], [12]) that Hopf curvature µof Hopf hypersurface M is constant for non flat complex space forms. We note that µ is not constant for Hopf hypersurfaces in Cn+1in general ([16], Theorem 2.1).
Fundamental result for Hopf hypersurfaces in complex projective spaceCPnwas proved by Cecil-Ryan [4]:
Theorem 2.1. Let M be a connected, orientable Hopf hypersurface of CPn with Hopf curvature µ = 2 cot 2r (0 < r < π/2). Suppose the focal map φr(x) = expx(rNx)(x∈M,Nx∈Tx⊥M,|Nx|= 1) has constant rank qon M. Then:
1. q is even and every point x0 ∈ M has a neighborhood U such that φrU is an embedded complex(q/2)-dimensional submanifold ofCPn.
2. For each pointxin such a neighborhoodU, the leaf of the foliationT0 throughx intersects U in an open subset of a geodesic hypersphere in the totally geodesic CP(m−q/2)orthogonal toTp(φrU)atp=φr(x). ThusU lies on the tube of radius r overφrU.
Similar result for Hopf hypersurfaces with large Hopf curvature in complex hyperbolic spaceCHn was proved by Montiel [15]:
Theorem 2.2. Let M be an orientable Hopf hypersurface ofCHn and we assume that φr (r >0) has constant rank q on M. Then, if µ = 2 coth 2r (hence µ > 2), for every x0 ∈M there exists an open neighbourhood W of x0 such that φrW is a (q/2)-dimensional complex submanifold embedded in CHn. Moreover W lies in a tube of radius roverφrW.
On the other hand, with respect to Hopf hypersurfaces with small Hopf curva- ture inCHn, Ivey [7] and Ivey-Ryan [8] proved that a Hopf hypersurface with|µ|<2 in CHn may be constructed from an arbitrary pair of Legendrian submanifolds in S2n−1.
3 Totally complex submanifolds in Quaternionic K¨ahler manifolds
We recall the basic definitions and facts on totally complex submanifolds of a quaternionic K¨ahler manifold (cf. [18]) Let (Mf4m,g, Q) be a quaternionic K¨˜ ahler manifold with the quaternionic K¨ahler structure (˜g, Q), that is, ˜gis the Riemannian metric on MfandQis a rank 3 subbundle of EndTMfwhich satisfies the following conditions:
1. For each p∈Mf, there is a neighborhood U of pover which there exists a local frame field{I˜1,I˜2,I˜3} ofQsatisfying
I˜12= ˜I22= ˜I32=−1, I˜1I˜2=−I˜2I˜1= ˜I3, I˜2I˜3=−I˜3I˜2= ˜I1, I˜3I˜1=−I˜1I˜3= ˜I2.
2. For any elementL∈Qp, ˜gpis invariant byL, i.e., ˜gp(LX, Y) + ˜gp(X, LY) = 0 forX, Y ∈TpMf,p∈Mf.
3. The vector bundleQis parallel in EndTMfwith respect to the Riemannian connection∇e associated with ˜g.
A submanifoldM2mofMfis said to bealmost Hermitian if there exists a section ˜I of the bundleQ|M such that (1) ˜I2=−1, (2) ˜IT M =T M (cf. D.V. Alekseevsky and S. Marchiafava [1]). We denote by I the almost complex structure on M induced from ˜I. Evidently (M, I) with the induced metricgis an almost Hermitian manifold. If (M, g, I) is K¨ahler, we call it aK¨ahler submanifold of a quaternionic K¨ahler manifoldMf. An almost Hermitian submanifoldM together with a section ˜I ofQ|M is said to betotally complex if at each pointp∈M we haveLTpM ⊥TpM, for each L ∈ Qp with ˜g(L,I˜p) = 0 (cf. S. Funabashi [5]). It is known that a 2m (m≥2)-dimensional almost Hermitian submanifoldM2mis K¨ahler if and only if it is totally complex ([1] Theorem 1.12).
4 Gauss map of real hypersurfaces inCPn
We recall complex Grassmann manifoldG2(Cn+1) according to [11], Example 10.8. Let M0 = M0(n+ 1,2;C) be the space of complex matrices Z with n+ 1 rows and 2 columns such thattZZ¯ =E2 (or, equivalently, the 2 column vectors are orthonormal with respect to the standard inner product inCn+1). M0 is identified with complex Stiefel manifoldV2(Cn+1). The groupU(2) acts freely onM0 on the right: Z7→ZB, whereB∈U(2). We may consider complex 2-plane Grassmannian G2(Cn+1) as the base space of the principal fiber bundleM0 with groupU(2).
For eachZ ∈M0, the tangent spaceTZ(M0) is
TZ(M0) ={W ∈M(n+ 1,2;C)|tW Z+tZW = 0}.
In TZ(M0) we have an inner product g(W1, W2) = Re trace tW2W1. Let TZ00 = {ZA| A ∈ u(2)} ⊂ TZ(M0) and let TZ0 be the orthogonal complement of TZ00 in TZ(M0) with respect tog. The subspaceTZ0 admits a complex structureW 7→iW. We see that ˜π : M0 → G2(Cn+1) induces a linear isomorphism of TZ0 onto Tπ(Z)˜ (G2(Cn+1)). By transferring the complex structure i and the inner prod- uct g on TZ0 by ˜π∗ we get the usual complex structure J on G2(Cn+1) and the Hermitian metric on G2(Cn+1), respectively. Note that G2(Cn+1) is a complex 2n−2-dimensional Hermitian symmetric space.
Let U be an open subset in G2(Cn+1) and let ˜Z : U → π˜−1(U) be a cross section with respect to the fibration ˜π:M0→G2(Cn+1). Then for eachp∈U, the subspace T0˜
Z(p) admits 3 linear endomorphismsI1, I2, I3: I1:W 7→W
−i 0
0 i
, I2:W 7→W
0 −1
1 0
, I3:W 7→W
0 i i 0
. By transferring I1, I2, I3 on T0˜
Z(p) (p ∈ U) by ˜π∗ we get local basis ˜I1,I˜2,I˜3 of quaternionic K¨ahler structureQp onU ⊂G2(Cn+1) (cf. [2, 19]).
Let M2n−1 be a real hypersurface in complex projective space CPn and let w ∈S2n+1 with π(w) = xforx ∈M. We denote ξw0 as the horizontal lift of the structure vector ξatxtoTw0 with respect to the Hopf fibrationπ:S2n+1→CPn. Then theGauss map G:M2n−1→G2(Cn+1) ofM is defined by
(4.1) G(x) = ˜π(w, ξw0 ),
where ˜π: M0 =V2(Cn+1) → G2(Cn+1) given as above. It is seen that G is well defined.
Theorem 4.1. Let M be a real hypersurface in CPn and let G : M2n−1 → G2(Cn+1)be the Gauss map defined by (4.1). SupposeM is a Hopf hypersurface.
Then the image G(M) is a real (2n−2)-dimensional totally complex submanifold of G2(Cn+1).
5 Totally (para-)complex submanifolds in Quaternionic Para-K¨ahler manifolds
We recall real Clifford algebras (cf. [6, 14]) and (quaternionic) para-complex structure (cf. [14]). Let (V =R(p, q),h, i) be a real symmetric inner product space of signaturep, q. The Clifford algebraC(p, q) is the quotient⊗V /I(V), whereI(V) is the two-sided ideal in⊗V generated by all elements:
x⊗x+hx, xi withx∈V.
Examples of Clifford algebras are:
1. C=C(0,1), Complex numbers: z=x+iy,i2=−1,|z|2=x2+y2, there is no zero divisors.
2. Ce =C(1,0), Para-complex numbers: z=x+jy, j2= 1, |z|2=x2−y2, there exists zero divisors.
3. H=C(0,2),Quaternions: q=q0+iq1+jq2+kq3,i2=j2=k2=−1,|q|2= q¯q=q20+q12+q22+q32, there is no zero divisors,H∼=C2,q=z1(q) +jz2(q).
4. He =C(2,0) =C(1,1),Para-quaternions: q=q0+iq1+jq2+kq3,i2=−1, j2 = k2 = 1, |q|2 = q20+q12−q22−q23, there exists zero divisors, He ∼=C2, q=z1(q) +jz2(q).
There is a natural correspondence between complex numbersCand Euclidean plane R2, and para-complex numbersCe are naturally identified with real symmetric inner product space R(1,1) of signature (1,1). Also there is a natural correspondence between quaternionsHand Euclidean 4-spaceR4, and para-quaternionsHe are nat- urally identified with real symmetric inner product spaceR(2,2) of signature (2,2).
Let M be a differentiable manifold. We consider the following structures on a real vector space V =TxM, x ∈ M, where one assumes that I, J, K are given endomorphisms:
1. Complex: J2=−1,V ⊗C=VJ+⊕VJ−,VJ±={u∈V ⊗C| J u=±iu}, 2. Para-complex: J2= 1, V ⊗C=VJ+⊕VJ−,VJ±={u∈V ⊗C|J u=±iu},
dimVJ+= dimVJ−,
3. Hypercomplex: H = (I, J, K), I2 = J2 = K2 = −1, IJ = −J I = K (J K=−KJ=I,KI =−IK =J),
4. Para-hypercomplex: He = (I, J, K),I2=−1,J2=K2= 1,IJ =−J I = K (J K =−KJ =−I,KI =−IK =J).
It is known that the space of (oriented) geodesics (i.e., great circles S1) in round sphere Sn is naturally identified with (oriented) real 2-plane Grassmannian G2(Rn+1), and it has complex structure. On the other hand, the space of (ori- ented) geodesics (i.e., hyperbolic linesH1) in hyperbolic spaceHn is naturally iden- tified with (oriented) GrassmannianG1,1(Rn+11 ) of 2-plane with signature (1,1) in Minkowski spaceRn+11 , and it has para-complex structure [3, 9, 10].
A (para-)hypercomplex structure on V generates respectively a structure:
1. Quaternionic, generated by H = (I, J, K): Q = hHi = RI+RJ +RK, (I, J, K) determined up toA∈SO(3),S(Q) ={L∈Q| kLk2= 1},
2. Para-quaternionic, generated byHe = (I, J, K): Qe=hHei=RI+RJ+RK, (I, J, K) determined up toA∈SO(2,1), S(Q) =e S+(Q)e ∪S−(Q),e S+(Q) = {L∈Q|e L2= 1},S−(Q) ={L∈Q|e L2=−1}.
To treat the quaternionic and para-quaternionic case simultaneously, we setη= 1 orη=−1 and (1, 2, 3) = (−1,−1,−1) or (1, 2, 3) = (−1,1,1) respectively for hypercomplex or para-hypercomplex structure (I1, I2, I3): then the multiplication table looks
Iα2 =α1, IαIβ=−IβIα=ηγIγ (α= 1,2,3) where (α, β, γ) is any circular permutation of (1,2,3).
Analmost (para-)quaternionic structure on a differentiable manifold M4n is a rank 3 subbundleQ⊂End(T M), which is locally spanned by a fieldH = (I1, I2, I3) of (para-)hypercomplex structures. Such a locally defined triple H = (Iα), α = 1,2,3, will be called a(local) admissible basis ofQ.
Analmost (para-)quaternionic connection is a linear connection ∇ which pre- serves Q; equivalently, for any local admissible basisH = (Iα) ofQ, one has
∇Iα=−βωγ⊗Iβ+γωβ⊗Iγ (P.C.)
where (P.C.) means that (α, β, γ) is any circular permutation of (1,2,3).
An almost (para-)quaternionic structureQis called a(para-)quaternionic struc- ture if M admits a(para-)quaternionic connection, i.e. a torsion-free almost (para- )quaternionic connection. An(almost) (para-)quaternionic manifold (M4n, Q) is a manifoldM4n endowed with an (almost) (para-)quaternionic structureQ.
Analmost (para-)quaternionic Hermitian manifold(M, Q, g) is an almost (para- )quaternionic manifold (M, Q) endowed with a pseudo Riemannian metricgwhich is Q-Hermitian, i.e. any endomorphism ofQisg-skew-symmetric. (M, Q, g), (n >1), is called a (para-)quaternionic K¨ahler manifold if the Levi-Civita connection of g preserves Q, i.e. ∇g is a (para-)quaternionic connection.
Let (fM4m,˜g, Q) be a para-quaternionic K¨ahler manifold with the para- quaternionic K¨ahler structure (˜g, Q). A submanifoldM2mofMfis said to bealmost Hermitian (resp. almost para-Hermitian) if there exists a section ˜I of the bundle Q|M such that (1) ˜I2 =−1 (resp. ˜I2 = 1), (2) ˜IT M =T M. An almost (para- )Hermitian submanifold M together with a section ˜I of Q|M is said to be totally (para-)complex if at each pointp ∈ M we haveLTpM ⊥ TpM, for each L ∈ Qp
with ˜g(L,I˜p) = 0.
6 Gauss map of real hypersurfaces inCHn
We consider Grassmann manifold G1,1(Cn+11 ) of 2-planes with signature (1,1) inCn+11 . We putn×nmatrixJn as
Jn =
−1 0 · · · 0 0 1 · · · 0 ... ... . .. ... 0 0 · · · 1
.
Let Mf0 = Mf0(n+ 1,2;C) be the space of complex matrices Z with n+ 1 rows and 2 columns such that tZJ¯ n+1Z = J2 (or, equivalently, the 2 column vectors are orthonormal with respect to the inner product inCn+11 ). Mf0 is identified with complex (indefinite) Stiefel manifold V1,1(Cn+11 ). The groupU(1,1) acts freely on Mf0 on the right: Z 7→ZB, where B ∈U(1,1). We may consider complex (1,1)- plane GrassmannianG1,1(Cn+11 ) as the base space of the principal fiber bundle Mf0 with groupU(1,1).
For each Z∈Mf0, the tangent spaceTZ(Mf0) is
TZ(Mf0) ={W ∈M(n+ 1,2;C)|tW Jn+1Z+tZJn+1W = 0}.
InTZ(M0) we have an inner producteg(W1, W2) = Re tracetW2Jn+1W1. LetTZ00= {ZA| A ∈ u(1,1)} ⊂TZ(M0) and let TZ0 be the orthogonal complement of TZ00 in TZ(M0) with respect to eg. The subspace TZ0 admits a complex structure W 7→
iW. We see that ˜π : Mf0 →G1,1(Cn+11 ) induces a linear isomorphism of TZ0 onto T˜π(Z)(G1,1(Cn+11 )). By transferring the complex structureiand the inner product g onTZ0 by ˜π∗ we get the complex structureJ onG1,1(Cn+11 ) and the (indefinite) Hermitian metric onG1,1(Cn+11 ), respectively.
Let U be an open subset in G1,1(Cn+11 ) and let ˜Z : U → π˜−1(U) be a cross section with respect to the fibration ˜π :Mf0 → G1,1(Cn+11 ). Then for each p∈U, the subspaceTZ(p)0˜ admits 3 linear endomorphismsI1, I2, I3:
I1:W 7→W
−i 0 0 i
, I2:W 7→W 0 1
1 0
, I3:W 7→W
0 −i i 0
.
By transferring I1, I2, I3 on TZ(p)0˜ (p ∈ U) by ˜π∗ we get local basis ˜I1,I˜2,I˜3 of quaternionic para-K¨ahler structureQp onU ⊂G1,1(Cn+11 ).
Let M2n−1 be a real hypersurface in complex hyperbolic space CHn and let w∈ H12n+1 with π(w) =xforx∈M. We denote ξ0w as the horizontal lift of the structure vectorξatxtoTw0 with respect to the fibrationπ:H12n+1→CHn. Then theGauss map Ge:M2n−1→G1,1(Cn+11 ) ofM is defined by
(6.1) G(x) = ˜e π(w, ξ0w),
where ˜π:Mf0 =V1,1(Cn+11 )→G1,1(Cn+11 ) given as above. It is seen thatGe is well defined.
Theorem 6.1. Let M2n−1 be a real hypersurface in CHn and let Ge : M → G1,1(Cn+11 ) be the Gauss map defined by (6.1). Suppose M is a Hopf hypersur- face with Hopf curvature µ. Then the imageG(M) is a real (2n−2)-dimensional submanifold of G1,1(Cn+11 )such that
1. G(M)is totally complex provided |µ|>2, 2. G(M)is totally para-complex provided|µ|<2,
3. There exists a sectionI˜of the bundleQ|G(M) satisfyingI˜2= 0andIT G(M˜ ) = T G(M)provided|µ|= 2.
References
[1] D. V. Alekseevsky and S. Marchiafava,Hermitian and Kahler submanifolds of a quaternionic Kahler manifold, Osaka J. Math.38(2001), no. 4, 869–904.
[2] J. Berndt,Riemannian geometry of complex two-plane Grassmannians, Rend.
Sem. Mat. Univ. Politec. Torino55(1997), no. 1, 19–83.
[3] V. Cruceanu, P. Fortuny and P. M. Gadea,A survey on paracomplex geometry, Rocky Mountain J.26(1996), 83-115.
[4] T. E. Cecil and P. J. Ryan,Focal sets and real hypersurfaces in complex pro- jective space, Trans. Amer. Math. Soc.269(1982), no. 2, 481–499.
[5] S. Funabashi,Totally complex submanifolds of a quaternionic Kaehlerian man- ifold, Kodai Math. J.2(1979), no. 3, 314–336.
[6] F. R. Harvey, Spinors and calibrations, Perspectives in Mathematics, 9. Aca- demic Press, Inc., Boston, MA, 1990. xiv+323 pp. ISBN: 0-12-329650-1 [7] T. E. Ivey, A d’Alembert formula for Hopf hypersurfaces, Results Math. 60
(2011), no. 1-4, 293–309.
[8] T. E. Ivey and P. J. Ryan,Hopf hypersurfaces of small Hopf principal curvature inCH2, Geom. Dedicata 141(2009), 147–161.
[9] M. Kimura,Space of geodesics in hyperbolic spaces and Lorentz numbers, Mem.
Fac. Sci. Eng. Shimane Univ. Ser. B Math. Sci.36(2003), 61–67.
[10] S. Kaneyuki and M. Kozai, Paracomplex structures and affine symmetric spaces, Tokyo J. Math. 8(1985), 81-98.
[11] S. Kobayashi and K. Nomizu,Foundations of differential geometry. Vol. II, In- terscience Tracts in Pure and Applied Mathematics, No. 15 Vol. II Interscience Publishers John Wiley & Sons, Inc., New York-London-Sydney 1969 xv+470 pp
[12] U.-H. Ki and Y. J. Suh,On real hypersurfaces of a complex space form, Math.
J. Okayama Univ. 32(1990), 207–221.
[13] Y. Maeda,On real hypersurfaces of a complex projective space, J. Math. Soc.
Japan 28(1976), 529–540.
[14] S. Marchiafava, Submanifolds of (para-)quaternionic Kahler manifolds, Note Mat. 28(2009), [2008 on verso], suppl. 1, 295–316.
[15] S. Montiel, Real hypersurfaces of a complex hyperbolic space, J. Math. Soc.
Japan 37(1985), no. 3, 515–535.
[16] R. Niebergall and P. J. Ryan,Real hypersurfaces in complex space forms, Tight and taut submanifolds (Berkeley, CA, 1994), 233?305, Math. Sci. Res. Inst.
Publ., 32, Cambridge Univ. Press, Cambridge, 1997.
[17] M. Takeuchi,Totally complex submanifolds of quaternionic symmetric spaces, Japan. J. Math. (N.S.)12 (1986), no. 1, 161–189.
[18] K. Tsukada, Fundamental theorem for totally complex submanifolds, (English summary) Hokkaido Math. J. 36(2007), no. 3, 641–668.
[19] J. A. Wolf, Complex homogeneous contact manifolds and quaternionic sym- metric spaces, J. Math. Mech. 14(1965), 1033-1047.