Research article

The Lawson-Simons' theorem on warped product submanifolds with geometric information

  • Received: 14 January 2021 Accepted: 14 March 2021 Published: 26 March 2021
  • MSC : 53B50, 53C20, 53C40

  • The main objective of this paper is to investigate topological properties from the view point of compact warped product submanifolds of a space form with the vanishing constant sectional curvature. That is, we prove the non-existence of stable integral p-currents in a compact oriented warped product pointwise semi-slant submanifold Mn in the Euclidean space Rp+2q which satisfies an operative condition involving the Laplacian of a warped function and a pointwise slant function, and show that their homology groups are zero on this operative condition. Moreover, under the assumption of extrinsic conditions, we derive new topological sphere theorems on a warped product submanifold Mn, and prove that Mn is homeomorphic to Sn if n=4, and Mn is homotopic to Sn if n=3. Furthermore, the same results are generalized for CR-warped products and our results recovered [17].

    Citation: Ali H. Alkhaldi, Akram Ali, Jae Won Lee. The Lawson-Simons' theorem on warped product submanifolds with geometric information[J]. AIMS Mathematics, 2021, 6(6): 5886-5895. doi: 10.3934/math.2021348

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  • The main objective of this paper is to investigate topological properties from the view point of compact warped product submanifolds of a space form with the vanishing constant sectional curvature. That is, we prove the non-existence of stable integral p-currents in a compact oriented warped product pointwise semi-slant submanifold Mn in the Euclidean space Rp+2q which satisfies an operative condition involving the Laplacian of a warped function and a pointwise slant function, and show that their homology groups are zero on this operative condition. Moreover, under the assumption of extrinsic conditions, we derive new topological sphere theorems on a warped product submanifold Mn, and prove that Mn is homeomorphic to Sn if n=4, and Mn is homotopic to Sn if n=3. Furthermore, the same results are generalized for CR-warped products and our results recovered [17].



    The theory of integral currents was introduced by Federer-Fleming [8]. The notion of an integral current plays an important role in providing tooplogical information by combining the geometric structure of differentiable manifolds and homology groups with integral coefficients. In 1970 s, Lawson-Simons [11] provided the optimization for the nonexistence of stable currents in submanifolds of the sphere Sn with pinched the second fundamental form.

    On the other hand, vanishing homology and non-existence of stable integral currents in warped product submanifolds in an odd dimensional sphere were constructed in [15]. By taking the help of Lawson-Simons' results [11], they proved that the homology groups were trivial and did not exist stable currents of a contact CR-warped product submanifold in an odd dimentional sphere (see [15] for more detail). Later on, F. Şahin [17,18] proved similar results for CR-warped product submanifold in Euclidean spaces and in the near Kaehler six sphere S6. Motivated by previous development, Ali et al. [1] optimized the warped function and pointwise slant functions for a warped product submanifold in the unit sphere with trivial homology groups on the pointwise slant fiber. Inspired by the results [7] on a hyperbolic space for negative constant sectional curvature, Ali et al. [3] derived the results for non-existence stable currents and vanishing homology groups for CR-warped product in complex hyperbolic spaces. As applications, some topological sphere theorems have been proved in [3]. The same study has been extended for Lagrangian warped product submanifolds of the near Kaehler six sphere S6 in [2], and similar results in a generalized complex space can be found in [13]. By imposing certain conditions on the second fundamental form in ([12,14,20,21,22]), several mathematicians obtained many results for topological and differentiable structures of submanifolds.

    In this work, we provide these results in non-trivial warped product pointwise semi-slant submanifold in Kaehler manifold with zero holomorphic sectional curvature, which generalizes a CR-warped product submanifold class, proved by B. Sahin [16]. Moreover, we show that our results are an extension of F. Sahin in [17].

    A Kaehler manifold ˜M of dimension 2m with an almost complex structure J and a Riemannian metric g satisfies

    J2=Ig(JU,JV)=g(U,V)(˜UJ)V=0 (2.1)

    for all vector fields U,VX(T˜M), where X(T˜M) denotes the collection of all sections on the tangent bundle T˜M on ˜M and ˜ denotes the covariant differential operator on ˜M with respect to the Riemannian metric g [23].

    If and are the induced Riemannian connections on the tangent bundle TM and the normal bundle TM of a submanifold M, respectively, then the following formulas are recognized as Gauss and Weingarten

    ˜UV=UV+h(U,V), (2.2)
    ˜UN=ANU+UN (2.3)

    for U,VX(TM) and NX(TM). If the tangential and normal components of JU(JN) are represented by PU(tN) and FU(fN) respectively, then they are related as:

    (i)JU=PU+FU,(ii)JN=tN+fN (2.4)

    Here, a totally real submanifold M provides P is identically zero and a holomorphic submanifold characterizes F is identically zero. If the curvature tensors of ˜M and M are symbolized ˜R and R, respectively, the Gauss equation for a submanifold M is given as:

    ˜R(X,Y,Z,W)=R(X,Y,Z,W)+g(h(X,Z),h(Y,W))g(h(X,W),h(Y,Z)) (2.5)

    for X,Y,Z,WX(TM). Several classes of a submanifold M of Kaehler manifold ˜M are categorised as in the following by the behaviour of almost complex structure J:

    (ⅰ) M is holomorphic if J(TxM)TxM and totally real if J(TxM)TM at each xM [5].

    (ⅱ) A submanifold M is a CR-submanifold if the tangent space TM of M is expressed as TM=DTD for a totally real distribution D, i.e., J(D)(TM) and a holomorphic distribution DT, that is, J(DT)DT [5].

    (ⅲ) If the Wirtinger angle θ(X) between JX and TxM for any nonzero vector XTxM and xM provides θ:TMR is a real-valued function, then M is called a pointwise slant submanifold [6]. If the angle θ(X) is globally constant then M is slant submanifold. The necessary and sufficent condition for M to be pointwise slant if the tangential endomorphism P is satisfied the following

    P2=λI. (2.6)

    for λ[0,1] such that λ=cos2θ. The following formulas can be constructed by using (2.4) and (2.6) as:

    g(PU,PV)=cos2θg(U,V), (2.7)
    g(FU,FV)=sin2θg(U,V) (2.8)

    for any U,VX(TDθ).

    (ⅳ) If the tangent space TM of M is disintegrated as TM=DTDθ for the poinwise slant distribution Dθ, then it is called a pointwise semi-slant submanifold [16]. Moreover, if μ is an invariant subspace under J of the normal bundle TM, then the normal bundle TM can be decomposed as TM=FDθμ.

    If p and q are the ranks of the complex distribution DT and the pointwise slant distribution Dθ of a pointwise semi-slant submanifold in a Kaehler manifold ˜M, respectively, then the following remarks hold:

    Remark 1. M is invariant if q=0 and pointwise slant if p=0.

    Remark 2. If we consider the slant function θ:MR is globally constant on M and θ=π2, then M is a CR-submanifold.

    Remark 3. If the slant function θ:M(0,π2), then M is called a proper pointwise semi-slant submanifold.

    Moreover, there are some examples and related problems of a pointwise semi-slant submanifold in a Kaehler manifold in [16]. Furthermore, the initial concept of a warped product manifold is given by Bishop and O'Neill [4]. The product manifold of the form Np1×fNq2 with the metric g=g1+f2g2 of two Riemannian manifolds Np1 and Nq2 is called a warped product manifold and f denotes the warping function on the base Np1. Now we have

    ZX=XZ=(Xlnf)Z (2.9)

    for any XΓ(TN1) and ZΓ(TN2), where the gradient (lnf) of lnf is given by

    g(lnf,X)=X(lnf). (2.10)

    The following relation is proved in [4]

    R(X,Z)Y=Hf(X,Y)fZ (2.11)

    where Hf is a Hessian tensor of f.

    Remark 4. A warped product manifold Mn=Np1×fNq2 is trivial if and only if f is constant along Np1.

    For the Laplacian Δ(lnf) of the warping function f, we have

    Δ(lnf)=div(ff)=g(1f,f)1fdiv(f)=lnf2+ff. (2.12)

    From (2.12), we get

    Δff=Δ(lnf)||(lnf)||2. (2.13)

    To prove our main results, we need the following which was obtained by Lawson and Simons [11], we summarize these result as follows;

    Lemma 3.1. [11,20] For the second fundamental form h and any positive integers p and q with p+q=n, if the inequality

    pα=1nβ=p+1(2||h(eα,eβ)||2g(h(eα,eα),h(eβ,eβ)))<pqc (3.1)

    is satisfied for an n-dimensional compact submanifold Mn in a space form ˜M(c) of constant curvature c0, then there is no stable p-currents in Mn and Hp(Mn,Z)=Hq(Mn,Z)=0, where Hα(Mn,Z) is the α-th homology group of Mn with integer coefficients and {eα}1αn are orthonormal basis of Mn.

    From the generalized Poincare conjecture, it was proved in [11] that if the second fundamental form bounded above of an n-dimensional compact submanifold Mn in the unit sphere Sn+p, then Mn is either homeomorphic to a sphere Sn for n3 or homotopic to a sphere Sn for n=3. In [19], if an n-dimensional compact oriented submanifold Mn of the (n+k)-dimensional Euclidean space En+k satisfies the pinching condition Ric(X)>δ1(n)g(AHX,X), where the Ricci curvature Ric and the shape operator AH with respect to the mean curvature H, and δ1(n) is constant given by δ1(n)=n(n3)n1 if n is odd and δ1(n)=n2 if n is even, then there are no stable currents in Mn, and also Mn is homeomorphic to Sn.

    In the case study of the present paper, we consider the only non-trvial warped product pointwise semi-slant submanifold of the form NpT×fNqθ in a Kaehler manifold because other warped product submanifolds are trivial (see [16] for detail). Before proceeding to the main theorem, we recall that the following result [16]:

    Lemma 3.2. Let Mn=NpT×fNqθ be a warped product pointwise semi-slant submanifold of a Kaehler manifold ˜M. Then

    g(h(X,Z),FPZ)=(Xlnf)cos2θ||Z||2 (3.2)
    g(h(Z,JX),FZ)=(Xlnf)||Z||2 (3.3)

    for X,YX(TNT) and ZX(TNθ).

    Let Cq be a complex vector space, which is identified with a real vector space R2q, expressed as (z1,,zq)(x1,xq,y1yq) with zβ=xβ+iyβ, for β=1,q. With the standard metric in R2q, it becomes the Euclidean 2qspace, denoted by R2q. Therefore, with the standard flat Kaehlerian metric, an almost complex structure J on R2q is said to be compatible if (R2q,J) is analytically isometric to the complex number space Cq. From now on, we denote the Euclidean 2qspace with compatible almost complex structure J by R2q. Thus, (R2q,J) is a Kaehler manifold with zero constant sectional curvature. Therefore, we have nonexistence stable integral pcurrents theorem for a warped product pointwise semi-slant submanifold in a flat space or the Euclidean space Rp+2q as follows;

    Theorem 3.3. Let Mn=NpT×fNqθ be a compact, oriented warped product pointwise semi-slant submanifold in the Euclidean space Rp+2q with n=p+q. If the following condition is satisfied

    Δ(lnf)>(1q+csc2θ+cot2θ)||(lnf)||2 (3.4)

    then there does not exist stable integral p-currents in Mn and

    Hp(Mn,Z)=Hq(Mn,Z)=0,

    where Hi(Mn,Z) is the i-th homology group of Mn with integer coefficients.

    Proof. Let dim(NT)=p=2α and dim(Nθ)=q=2β, where Nθ and NT are integral manifolds of Dθ and D, respectively.

    Consider {e1,e2,,eα,eα+1=Je1,,e2α=Jeα} and {e2α+1=e1,,e2α+β=eβ,e2α+β+1=eβ+1=secθPe1,,ep+q=eq=secθPeβ} to be orthonormal frames of TNT and TNθ, respectively. Thus the orthonormal frames of the normal subbundles FDθ is {en+1=ˉe1=cscθFe1,,en+β=ˉeβ=cscθFe1,en+β+1=ˉeβ+1=cscθsecθFPe1,,en+2β=ˉe2β=cscθsecθFPeβ}. Thus, we have

    pi=1nj=p+1{2||h(ei,ej)||2g(h(ei,ei),h(ej,ej))}=p+2qr=n+1pi=1nj=p+1(hrij)2+pi=1nj=p+1{||h(ei,ej)||2g(h(ei,ei),h(ej,ej))}. (3.5)

    Then from Gauss Eq (2.5) for the Euclidean space Rp+2q, we get

    pi=1nj=p+1{2||h(ei,ej)||2g(h(ei,ei),h(ej,ej))}=p+2qr=n+1pi=1nj=p+1(hrij)2+pi=1qj=1g(R(ei,ej)ei,ej). (3.6)

    From R(ei,ej)ei=Hf(ei,ei)fej in (2.11), we derive

    pi=1qj=1g(R(ei,ej)ei,ej)=qfpi=1g(eif,ei). (3.7)

    Combining (3.6) and (3.7), we derive

    pi=1nj=p+1{2||h(ei,ej)||2g(h(ei,ei),h(ej,ej))}=qfpi=1g(eif,ei)+p+2qr=n+1pi=1nj=p+1(hrij)2. (3.8)

    First we compute the term Δf, that is the Laplacian of f, one derives

    Δf=nk=1g(ek(f),ek)=pi=1g(ei(f),ei)qj=1g(ej(f),ej).

    The above equation can be expressed as components of Nqθ from adapted orthonormal frame, one obtains

    Δf=pi=1g(ei(f),ei)βj=1g(ej(f),ej)sec2θβj=1g(Pej(f),Pej).

    Since NpT is totally geodesic in Mn, gradlnfX(TNT), we obtain

    Δf=1fβj=1(g(ej,ej)||(f)||2+sec2θg(Pej,Pej)||f||2)pi=1g(ei(f),ei).

    Multiply to above equation by 1f, and from (2.7), we get:

    Δff=1fpi=1g(ei(f),ei)q||(lnf)||2.

    Making use of (2.13), we find that

    1fpi=1g(ei(f),ei)=Δ(lnf)+(1q)||lnf||2. (3.9)

    Thus from (3.8) and (3.9), we compute that

    pi=1nj=p+1{2||h(ei,ej)||2g(h(ei,ei),h(ej,ej))}=q(1q)||(lnf)||2qΔ(lnf)+p+2qr=n+1pi=1nj=p+1(hrij)2. (3.10)

    Now, let X=eα(1αp) and Z=eβ(1βq), we have

    p+2qr=n+1pi=1nj=p+1(hrij)2=2βr=1pi=1qj=1g(h(ei,ej),ˉer)2=pi=1βj,r=1{g(h(ei,ej),cscθFer)2+g(h(ei,ej),cscθsecθFPer)2}.

    At the above equation, the term in the right hand side is FDθ-component and for pointwise semi-slant, the fact PDθDθ and t(TM)=Dθ. Then using (3.2) and (3.3) of Lemma 3.2 in the above equations, after summation over the vector fields on NT and Nθ, we derive

    p+2qr=n+1pi=1nj=p+1(hrij)2=2(csc2θ+cot2θ)αi=1βj=1(eilnf))2g(ej,ej)2+2(csc2θ+cot2θ)αi=1βj=1(Jeilnf))2g(ej,ej)2

    The last equation can be expressed as:

    p+2qr=n+1pi=1nj=p+1(hrij)2=2(csc2θ+cot2θ)pi=1(eilnf)2βj=1g(ej,ej)2,

    which implies

    p+2qr=n+1pi=1nj=p+1(hrij)2=q(csc2θ+cot2θ)||lnf||2. (3.11)

    Following from (3.10) and (3.11), we arrive at

    qΔ(lnf)+q(1q)||(lnf)||2+q(csc2θ+cot2θ)||(lnf)||2=pi=1nj=p+1{2||h(ei,ej)||2g(h(ei,ei),h(ej,ej))}. (3.12)

    If (3.4) in Theorem 3.3 is satisfied, then from above equation, we get

    pi=1nj=p+1{2||h(ei,ej)||2g(h(ei,ei),h(ej,ej))}<0 (3.13)

    Applying Lemma 3.1, for Euclidean space c=0, we get the final conclusion of our theorem.

    In particular, when the slant function is constant with θ=π2 in Theorem 3.3, a warped product pointwise semi-slant submanifold Mn=NpT×fNqθ becomes a CR-warped product in a Kaehler manifold such that NpT and Nqθ=Nq are holomorphic and totally real submanifolds, respectively. Therefore, due to the studied of Chen [5], we prove the nonexistence of a stable integrable p-currents for CR-warped products in Euclidean space Rp+2q as a consequence of Theorem 3.3.

    Theorem 3.4. [17] Let Mn=NpT×fNq be a compact CR-warped product submanifold in Euclidean space Rp+2q with n=p+q. If the following condition is satisfied

    Δ(lnf)>(2q)||(lnf)||2, (3.14)

    then there does not exist a stable integral p-currents in Mn and

    Hp(Mn,Z)=Hq(Mn,Z)=0,

    where Hi(Mn,Z) is the i-th homology group of Mn with integer coefficients.

    Then we state next sphere theorem as follows;

    Theorem 3.5. Let Mn=NpT×fNqθ be a compact oriented warped product pointwise semi-slant submanifold in Rp+2q with n=p+q, if the following condition is satisfied

    Δ(lnf)>(1q+csc2θ+cot2θ)||(lnf)||2, (3.15)

    Then Mp+q is homeomorphic to Sn when p+q=4 and if p+q=3, then Mp+q is homotopic to Sn.

    Proof. From Theorem 3.3, there does not exist stable integral p-currents in a warped product pointwise semi-slant submanifold M and their homology group zero for all positive integer p,q such that p+q=n3, that is, Hq(M,Z)=Hq(M,Z)=0. Therefore, M is a homology sphere. By choosing a Riemannian universal covering of ambient manifold ˜M of M together with compactness of M and (3.12), ˜M is compact due to Myer's theorem. Thus the above justification can be imposed to the Riemannian universal covering ˜M of M to show that M is a homology sphere. As ˜M is a homology sphere with fundamental group π1(˜M)=0 and it is also a homotopy sphere. Therefore, applying the generalized Poincarẽ's conjecture (Smale n5 [14], Freedman n=4 [9]), we get that M is homotopy to the Euclidean sphere Sn.

    On other hand, if n=3, using the result of R. S. Hamilton [10], we conclude that M3 is a three dimensional spherical space form and hence π1(M)=0, it is homotopic to a Euclidean sphere S3. The proof of completed.

    From Theorem 3.4, there is a consequence of Theorem 3.5 as the sphere theorem for compact CR-warped products in Rp+2q;

    Theorem 3.6. [17] Let Mn=NpT×fNq be a compact, oriented CR-warped product submanifold in Rp+2q with n=p+q, if the following is satisfied

    Δ(lnf)>(2q)||(lnf)||2, (3.16)

    then Mp+q is homeomorphic to Sn when p+q=4 and if p+q=3, then Mp+q is homotopic to Sn.

    Remark 5. Theorems 3.5 and 3.6 are topological sphere theorems for warped product submanifolds without the assumption that Mn is simply connected. Moreover, our results become more significant due to involving the new pinching conditions in terms of a pointwise slant function and the Laplacian of a warping function.

    Remark 6. It noted that our results are generalized all results which were proved in [17].

    The authors would like to express their gratitude to Deanship of Scientific Research at King Khalid University, Saudi Arabia for providing funding research group under the research grant R. G. P. 1/186/41. Jae Won Lee was supported by the National Research Foundation of Korea(NRF) grant funded by the Korea government(MSIT) (2020R1F1A1A01069289).

    The authors declare that they have no competing interests.



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    1. Meraj Khan, Cenep Ozel, Mohd Siddiqi, Sudhakar Chaubeyi, Sadia Ali, Analysis of stable currents and homology of biwarped product submanifolds in the Euclidean space, 2023, 37, 0354-5180, 7105, 10.2298/FIL2321105K
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