Research article

Biharmonic submanifolds of Kaehler product manifolds

  • Received: 07 May 2021 Accepted: 08 June 2021 Published: 22 June 2021
  • MSC : 53C15, 53C40, 53C42, 53C43

  • In this paper, the authors have established the necessary and sufficient conditions for the submanifolds of Kaehler product manifolds to be biharmonic. Moreover, the magnitude of scalar curvature for the hypersurfaces in a product of two unit spheres has been derived. Also, for the same product, the magnitude of the mean curvature vector for Lagrangian submanifolds has been estimated. Finally, the non-existence condition for totally complex Lagrangian submanifolds in a product of unit sphere and a hyperbolic space has been proved.

    Citation: Yanlin Li, Mehraj Ahmad Lone, Umair Ali Wani. Biharmonic submanifolds of Kaehler product manifolds[J]. AIMS Mathematics, 2021, 6(9): 9309-9321. doi: 10.3934/math.2021541

    Related Papers:

    [1] Mohd. Aquib, Amira A. Ishan, Meraj Ali Khan, Mohammad Hasan Shahid . A characterization for totally real submanifolds using self-adjoint differential operator. AIMS Mathematics, 2022, 7(1): 104-120. doi: 10.3934/math.2022006
    [2] Ali H. Alkhaldi, Meraj Ali Khan, Shyamal Kumar Hui, Pradip Mandal . Ricci curvature of semi-slant warped product submanifolds in generalized complex space forms. AIMS Mathematics, 2022, 7(4): 7069-7092. doi: 10.3934/math.2022394
    [3] Aliya Naaz Siddiqui, Mohammad Hasan Shahid, Jae Won Lee . On Ricci curvature of submanifolds in statistical manifolds of constant (quasi-constant) curvature. AIMS Mathematics, 2020, 5(4): 3495-3509. doi: 10.3934/math.2020227
    [4] Noura Alhouiti, Fatemah Mofarreh, Fatemah Abdullah Alghamdi, Akram Ali, Piscoran-Ioan Laurian . Geometric topology of CR-warped products in six-dimensional sphere. AIMS Mathematics, 2024, 9(9): 25114-25126. doi: 10.3934/math.20241224
    [5] Fatemah Mofarreh, S. K. Srivastava, Anuj Kumar, Akram Ali . Geometric inequalities of PR-warped product submanifold in para-Kenmotsu manifold. AIMS Mathematics, 2022, 7(10): 19481-19509. doi: 10.3934/math.20221069
    [6] Mehmet Gülbahar . Qualar curvatures of pseudo Riemannian manifolds and pseudo Riemannian submanifolds. AIMS Mathematics, 2021, 6(2): 1366-1376. doi: 10.3934/math.2021085
    [7] Tanumoy Pal, Ibrahim Al-Dayel, Meraj Ali Khan, Biswabismita Bag, Shyamal Kumar Hui, Foued Aloui . Generalized warped product submanifolds of Lorentzian concircular structure manifolds. AIMS Mathematics, 2024, 9(7): 17997-18012. doi: 10.3934/math.2024877
    [8] Mohammad Aamir Qayyoom, Rawan Bossly, Mobin Ahmad . On CR-lightlike submanifolds in a golden semi-Riemannian manifold. AIMS Mathematics, 2024, 9(5): 13043-13057. doi: 10.3934/math.2024636
    [9] Amira A. Ishan, Meraj Ali Khan . Chen-Ricci inequality for biwarped product submanifolds in complex space forms. AIMS Mathematics, 2021, 6(5): 5256-5274. doi: 10.3934/math.2021311
    [10] Meraj Ali Khan, Ali H. Alkhaldi, Mohd. Aquib . Estimation of eigenvalues for the α-Laplace operator on pseudo-slant submanifolds of generalized Sasakian space forms. AIMS Mathematics, 2022, 7(9): 16054-16066. doi: 10.3934/math.2022879
  • In this paper, the authors have established the necessary and sufficient conditions for the submanifolds of Kaehler product manifolds to be biharmonic. Moreover, the magnitude of scalar curvature for the hypersurfaces in a product of two unit spheres has been derived. Also, for the same product, the magnitude of the mean curvature vector for Lagrangian submanifolds has been estimated. Finally, the non-existence condition for totally complex Lagrangian submanifolds in a product of unit sphere and a hyperbolic space has been proved.



    For any two manifolds (M, g) and (N, h), a harmonic map ψ is the critical point of the energy functional defined as

    E(ψ)=12M|dψ|2dvg.

    The natural generalization of the harmonic maps was given by J. Eells and J. H. Sampson [1]. The established map ψ is called biharmonic if it is the critical point of energy functional

    E2(ψ)=12M|τ(ψ)|2dvg.

    with τ(ψ)=tr(dψ) as the vanishing tensor field for any harmonic map. For the above established E2, the first and second variation was studied by G. Y. Jiang [2]. For the same bi-harmonic functional, the associated Euler-Lagrange equation is τ2(ψ)=0, where τ2(ψ) is called bi-tension field and is defined as

    τ2(ψ)=Δτ(ψ)tr(RN(dψ,τ(ψ))dψ.

    In the above equation, Δ is the rough Laplacian acting on the sections of ψ1(TN) and RN is the curvature tensor for N. For any VΓ(ψ1(TN)) and X, Y Γ(TN), the definitions of Δ and RN are given by

    ΔV=tr(Δ2V),
    RN(X,Y)=[NX,NY]N[X,Y].

    A large number of studies have been done on biharmonic submanifolds [3,4,5,6,7,8]. It is a general fact that every harmonic map is biharmonic, but the vice-versa isn't true. The biharmonic maps, which are not harmonic, are called proper-biharmonic maps. If the harmonic map ψ is isometric immersion from the manifold (M,g) into (N,h), then the manifold M is called minimal submanifold of N. From the definition of proper biharmonic maps, it can be concluded that these are those submanifolds that aren't harmonic. Biharmonic submanifolds in different ambient spaces for different space forms have been extensively studied in the last few decades. Caddeo R. et al. [9] studied biharmonic submanifolds in spheres. Fetcu D. et al. [10,11,12] studied these submanifolds in complex, Sasakian and the product of sphere and real line space forms. J. Roth and A. Upadhyay [13,14] studied the biharmonic submanifolds on product spaces and generalized space forms. Chen B. Y. proved Chen's biharmonic conjecture stating that biharmonic surfaces do not exist in any Euclidean space with parallel normalized mean curvature vectors [15]. Yu F. et al. proved the same conjecture for hypersurfaces in R5 [16].

    The present study establishes the necessary and sufficient conditions for the submanifolds of Kaehler product manifolds to be biharmonic. Our future work then combines the work done in this paper with the techniques of singularity theory presented in [17,18,19,20]. We have derived the magnitude of scalar curvature for the hypersurfaces in a product of two spheres. We have also estimated the magnitude of the mean curvature vector for Lagrangian submanifolds in a product of two spheres. Finally, we proved the non-existence condition for totally complex Lagrangian submanifolds in a product of unit sphere and hyperbolic space.

    Let ˆMn and ˆMp be any Kehlerian manifolds of dimensions n (real dimension 2n) and p (real dimension 2p) respectively. Let us further assume Jn and Jp denote the almost complex structures of ˆMn and ˆMp, respectively. Suppose, ˆMn and ˆMp are complex space forms with constant holomorphic sectional curvatures c1 and c2, respectively. The Riemannian curvature tensor ˆRn of ˆMn(c1) is given by

    ˆRn(X,Y)Z = 14c1[gn(Y,Z)Xgn(X,Z)Y]

    + 14c1[gn(JnY,Z)JnXgn(JnX,Z)JnY+2gn(X,JnY)JnZ].

    Similarly, the Riemannian curvature tensor ˆRp of ˆMp(c2) is given by

    ˆRp(X,Y)Z = 14c2[gp(Y,Z)Xgp(X,Z)Y]

    + 14c2[gp(JpY,Z)JpXgp(JpX,Z)JpY+2gp(X,JpY)JpZ].

    For any generalized submanifold M of any complex space form N, the almost complex structure J induces the existence of four operators on M, namely

    j:TMTM,k:TMNM,l:NMTM,m:NMNM,

    defined for all X TM (tangent bundle) and ζNM (normal bundle) by

    JX=jX+kX,Jζ=lζ+mζ. (2.1)

    Since J is the almost complex structure, it satisfies J2 = Id. For any X, Y tangent to N, we also have g(JX,Y)=g(X,JY). Using the above properties of J, the relations for the operators, j, k, l and m are given as

    j2X+lkX+X=0, (2.2)
    m2ζ+klζ+ζ=0, (2.3)
    jlζ+lmζ=0, (2.4)
    kjX+mkX=0, (2.5)
    g(kX,ζ)+g(X,lζ)=0. (2.6)

    for all X Γ(TM) and ζΓ(NM). Also, j and m are skew-symmetric.

    Now, let us consider the Kaehler product manifold ˆMn(c1)׈Mp(c2) denoted by ˆM. If P and Q denote projection operators of the tangent spaces of ˆMn(c1) and ˆMp(c2), then we always have P2=P, Q2=Q and PQ=QP. If we put F=PQ, the properties of P and Q establish F2=I. This F is almost product structure of ˆMn(c1)׈Mp(c2). Moreover, we define a Riemannian metric g on ˆM as

    g(X, Y) = gn(PX,PY) + gp(QX,QY).

    Where X and Y are vector fields on ˆM. It further follows, g(FX,Y)=g(X,FY). If we put JX=JnPX+JpQX, we get JnP=PJ, JpQ=QJ, FJ=JF, g(JX,JY)=g(X,Y), ˆJ = 0. Thus J is the Kaehlerian structure on ˆM. The Riemannian curvature tensor ˆR of the product manifold ˆM is given as [21]

    R(X,Y)Z=c1+c216[g(Y,Z)Xg(X,Z)Y+g(JY,Z)JXg(JX,Z)JY+2g(X,JY)JZ+g(FY,Z)FXg(FX,Z)FY+g(FJY,Z)FJXg(FJX,Z)FJY+g(FZ,JY)FJZ]+c1c216[g(FY,Z)Xg(FX,Z)Y+g(Y,Z)FXg(X,Z)FY+g(FJY,Z)JXg(FJX,Z)JY+g(JY,Z)FJXg(JX,Z)FJY+2g(FX,JY)JZ+2g(X,JY)JFZ]. (2.7)

    The product structure F induces the existence of four operators:

    f:TMTM,h:TMNM,s:NMTMandt:NMNM,

    defined for all X TM (tangent bundle) and ζNM (normal bundle) by

    FX=fX+hX,Fζ=sζ+tζ. (2.8)

    These four operators follow the following relations

    f2X+shX=X, (2.9)
    t2ζ+hsζ=ζ, (2.10)
    fsζ+stζ=0, (2.11)
    hfX+thX=0, (2.12)
    g(hX,ζ)=g(X,sζ). (2.13)

    for all X Γ(TM) and ζΓ(NM). Also, f and t are symmetric.

    The first theorem gives necessary and sufficient condition for the manifold to be biharmonic.

    Theorem 3.1. Let M be a u-dimensional submanifold of the Kaehler product manifold ˆM = ˆMn(c1)׈Mp(c2) with A, B and H, respectively denoting the shape operator, second fundamental form and mean curvature vector. Then, this submanifold is biharmonic if and only if the following equations are satisfied:

    H+tr(B(.,AH.))+c1+c216[uH+3klH+hsHtr(f)tH+2(hjflH+tkflH+hjsmH+tksmH)tr(fj+sk)(hlH+tmH)]+c1c216[tr(f)HutH+3(kflH+ksmH)tr(fj+sk)(mH)+3(hjlH+tklH)]=0. (3.1)
    u2grad|H|2+2tr(AH(.))+c1+c28[3jlH+fsHtr(f)sH+2(fjflH+skflH+fjsmH+sksmH)tr(fj+sk)(flH+smH)]+c1c28[sHusH+3(jflH+jsmH)tr(fj+sk)(lH)+3(fjlH+sklH)]=0. (3.2)

    Proof. The equations of biharmonicity have been already established in [12,22,23]. Projection of the equation τ(ψ)=0 on both tangential and normal bundles establishes the following equations

    H+tr(B(.,AH.))+tr(ˉR(.,H.)=0,u2grad|H|2+2tr(AH(.))+2tr(ˉR(.,H.)=0. (3.3)

    Suppose that {Xi}ui=1 is a local orthonormal frame for TM, then by using the Eq 2.7 of curvarture tensor ˉR, we have

    tr(ˉR(.,H.)=ui=1ˉR(Xi,H)Xi, (3.4)

    tr(ˉR(.,H.) = ui=1{c1+c216[g(H,Xi)Xig(Xi,Xi)H+g(JH,Xi)JXi

    g(JXi,Xi)JH+2g(Xi,JH)JXi+g(FH,Xi)FXig(FXi,Xi)FH

    +g(FJH,Xi)FJXig(FJXi,Xi)FJH+g(FXi,JH)FJXi]

    +c1c216[g(FH,Xi)Xig(FXi,Xi)H+g(H,Xi)FXig(Xi,Xi)FH

    +g(FJH,Xi)JXig(FJXi,Xi)JH+g(JH,Xi)FJXig(JXi,Xi)FJH

    +2g(FXi,JH)JXi+2g(Xi,JH)JFXi]},

    Introducing the established sets of four operators, j, k, l and m and f, h, s and t for J and F respectively, we get the simplified equation as

    tr(ˉR(.,H.) = c1+c216[uH+ui=1g(lH,Xi)JXi+ui=12g(Xi,lH)JXi

    +F(FH)tr(f)FH+FJ(FJH)tr(fj+sk)FJH+FJ(FJH)]

    +c1c216[(FH)tr(f)HuFH+J(FJH)tr(fj+sk)JH

    +ui=1g(lH,Xi)FJXi+2J(FJH)+ui=12g(Xi,lH)JFXi],

    or tr(ˉR(.,H.) = c1+c216[uH+3JlH+fsH+hsHtr(f)sHtr(f)tH

    +2FJ(flH+smH)tr(fj+sk)FJH]

    +c1c216[sHtr(f)HuFH+J(flH+smH)tr(fj+sk)JH+

    3FJlH+2J(flH+smH)],

    tr(ˉR(.,H.) = c1+c216[uH+3jlH+3klH+fsH+hsHtr(f)sHtr(f)tH

    + 2(fjflH+hjflH+skflH+tkflH+fjsmH+hjsmH+sksmH+tksmH)

    tr(fj+sk)(flH+hlH+smH+tmH)]

    + c1c216[sHtr(f)HushutH+3(jflH+kflH+jsmH+ksmH)

    tr(fj+sk)(lH+mH)+3(fjlH+hjlH+sklH+tklH)].

    By identification of tangential and normal parts, we get the required equations.

    Corollary 3.2. If M is a u-dimensional totally real submanifold of the Kaehler product manifold ˆM = ˆMn(c1)׈Mp(c2). Then, this submanifold is biharmonic if and only if the following equations are satisfied

    H+tr(B(.,AH.))+c1+c216[uH+3klH+hsHtr(f)tH+2(tkflH+tksmH)tr(sk)(hlH+tmH)]+c1c216[tr(f)HutH+3(kflH+ksmH)tr(sk)(mH)+3(tklH)]=0. (3.5)
    u2grad|H|2+2tr(AH(.))+c1+c28[fsHtr(f)sH+2(skflH+sksmH)tr(sk)(flH+smH)]+c1c28[sHusHtr(sk)(lH)+3(sklH)]=0. (3.6)

    Proof. If M is a totally real submanifold, then we know that for any XΓ(TM), we have

    JX=kX,

    In other words, jX=0. Using this fact in Theorem 3.1, we get the required equations.

    Corollary 3.3. a): If M is any hypersurface of the Kaehler product manifold

    ˆM=ˆMp(c1)׈Mnp(c2).

    Then, M is biharmonic if and only if the following equations are satisfied

    H+tr(B(.,AH.))+c1+c216[(n2)H+hsHtr(f)tH+2(hjflH+tkflH)tr(fj+sk)(hlH)]+c1c216[tr(f)H(n1)tH+3(kflH)+3(tklH)]=0. (3.7)
    n12grad|H|2+2tr(AH(.))+c1+c28[fsHtr(f)sH+2(fjflH+skflH)tr(fj+sk)(flH)]+c1c28[sH(n1)sH+3(jflH)tr(fj+sk)(lH)3sH]=0. (3.8)

    b): If M is any totally real hypersurface of the Kaehler product manifold

    ˆM=ˆMp(c1)׈Mnp(c2).

    Then, M is biharmonic if and only if the following equations are satisfied:

    H+tr(B(.,AH.))+c1+c216[(n2)H+hsHtr(f)tH+2(tkflH)tr(sk)(hlH)]+c1c216[tr(f)H(n1)tH+3(kflH)+3(tklH)]=0. (3.9)
    n12grad|H|2+2tr(AH(.))+c1+c28[fsHtr(f)sH+2(skflH)tr(sk)(flH)]+c1c28[sH(n1)sHtr(sk)(lH)3sH]=0. (3.10)

    Proof. a): For any hypersurface M,J maps normal vectors to tangent vectors as such m=0. Using this fact with the Eqs 2.3 and 2.4 for H, we get the required equations from Theorem 3.1.

    b): For any totally real hypersurface M, we have j=0 and m=0.

    Corollary 3.4. If M is a u-dimensional Lagrangian manifold of the Kaehler product manifold

    ˆM=ˆMn(c1)׈Mp(c2).

    Then, M is biharmonic if and only if the following equations are satisfied

    H+tr(B(.,AH.))+c1+c216[(u+3)H+hsHtr(f)tH+2(tkflH)tr(sk)(hlH)]+c1c216[tr(f)HutH+3(kflH)+3(tklH)]=0. (3.11)
    u2grad|H|2+2tr(AH(.))+c1+c28[fsHtr(f)sH+2(skflH)tr(sk)(flH)]+c1c28[sHusHtr(sk)(lH)3(sH)]=0. (3.12)

    Proof. If M is a Lagrangian manifold, then j=0 and m=0. Using this fact with Eq 2.3, we get the required equations from Theorem 3.1.

    From now on, the authors will consider the ambient space to be product of two 2-spheres of same radius (for simplicity radius equals 1 unit). The reason for taking 2-sphere follows from[24] as it is the only sphere which accepts Kaehler structure. In the following equations, we will have

    c1+c216=c18=18andc1c28=b=0.

    To estimate the magnitude of mean curvature vector and scalar curvature, the authors will further assume the cases where F will map the whole of tangent bundle or normal vectors to respective bundles only. The reason being the equations involve the product of almost complex structure J and product structure F. As such it isn't possible to get simpler equations involving dimensions of submanifolds and mean curvature vector only.

    Proposition 3.5. Let M be any hypersurface of S2×S2 with non-zero constant mean curvature such that FXΓ(TM) and FNΓ(TM) for any XΓ(TM) and NΓ(TM). Then M is biharmonic if we have

    |B|2=18[1+1|H|2tr(sk)FJH,H]. (3.13)

    Proof. By the established hypothesis on F, we have f=0 and t=0. Using these equations along with Eqs 2.9 and 2.10 in Eq 3.7, we get

    H+tr(B(.,AH.))18[H+tr(sk)(hlH)]=0, (3.14)

    Since M is a hypersurface, the above equation becomes,

    tr(B(.,AH.))18[H+tr(sk)(hlH)]=0, (3.15)

    Since tr(B(.,AH.)) = |B|2H, on further simplifying, we get,

    |B|2H2=18[H2+tr(sk)hlH,H], (3.16)

    or

    |B|2=18[1+1|H|2tr(sk)FJH,H]. (3.17)

    Remark 3.6. It can be easily concluded from above proposition that there doesn't exist any hypersurface of S2×S2 when FXΓ(TM) and FNΓ(TM) for any XΓ(TM) and NΓ(TM) for

    tr(sk)FJH,H+|H|20.

    The above proposition can be used to derive the value of scalar curvature for biharmonic hypersurface M when FXΓ(TM) and FNΓ(TM) for any XΓ(TM) and NΓ(TM).

    Proposition 3.7. Let M be any proper-biharmonic hypersurface of S2×S2 with non-zero constant mean curvature such that FXΓ(TM) and FNΓ(TM) for any XΓ(TM) and NΓ(TM). Then the scalar curvature τ of M is given by

    τM=18[5+tr(sk)21|H|2tr(sk)FJH,H]+3|H|2.

    Proof. By the equation of Gauss, we have,

    τM=n1i,j=1ˉR(Xi,Xj)Xj,Xi|B|2+(n1)|H|2,

    The curvature tensor ˆR for S2×S2 is given by Eq 2.7 with

    c1+c216=c18=18andc1c28=0.

    And,

    ˆR(Xi,Xj)Xj,Xi=18[1+FXj,XjFXi,XiFXi,Xj2+FJXj,XjFXi,Xi], (3.18)

    Since FXiΓ(TM) and f=0. We have

    n1i,j=1ˆR(Xi,Xj)Xj,Xi=18[6+tr(sk)2]. (3.19)

    Using the value of |B|2 gives the required equation.

    Proposition 3.8. Let M be any totally complex-hypersurface of S2×S2 with non-zero constant mean curvature such that FXΓ(TM) and FNΓ(TM) for any XΓ(TM) and NΓ(TM). Then for trivially biharmonic M, we have

    |B|2=18. (3.20)

    Proof. By the established hypothesis on F, we have f=0 and t=0. Using these equations along with Eqs 2.9 and 2.10 in Theorem 3.1, we get

    H+tr(B(.,AH.))18H=0, (3.21)

    Since M is a hypersurface, the above equation becomes

    tr(B(.,AH.))18H=0. (3.22)

    Since tr(B(.,AH.)) = |B|2H. On further simplifying, we get the required equation.

    Proposition 3.9. Let M be any proper-biharmonic totally complex-hypersurface of S2×S2 with non-zero constant mean curvature such that FXΓ(TM) and FNΓ(TM) for any XΓ(TM) and NΓ(TM). Then the scalar curvature τ of M is given as

    τM=18[5+tr(sk)2]+3|H|2. (3.23)

    Proof. By the equation of Gauss, we have

    τM=n1i,j=1ˆR(Xi,Xj)Xj,Xi|B|2+(n1)|H|2,

    The curvature tensor ˆR for S2×S2 is given by Eq 2.7 with

    c1+c216=c18=18andc1c28=0.

    Then,

    ˆR(Xi,Xj)Xj,Xi=18[1+FXj,XjFXi,XiFXi,Xj2+FJXj,XjFXi,Xi]. (3.24)

    Since FXiΓ(TM) and f=0. We have

    n1i,j=1ˆR(Xi,Xj)Xj,Xi=18[6+tr(sk)2]. (3.25)

    Using the value of |B|2 gives the required equation.

    Corollary 3.10. Let M be u-dimensional Lagrangian submanifold of S2×S2 with non-zero constant mean curvature such that FXΓ(TM) and FNΓ(TM) for any XΓ(TM) and NΓ(TM). Let us further assume [tr(sk)FJH,H]0 Then we have

    a): If M is a proper-biharmonic, then 0<|H|2u+28u.

    b): If |H|2=u+28u, then M is biharmonic if and only if it is pseudo-umbilical manifold, H=0 and tr(sk) = 0.

    Proof. By the given hypothesis for F, we have f=0 and t=0.

    Implementing the above conditions along with Eq 2.9 in Corollary 3.4 a), we get,

    ΔH+tr(B(.,AH.))18[(u+2)Htr(sk)(hlH)]=0. (3.26)

    By taking the inner product with H, we get

    ΔH,H+|AH|218[(u+2)|H|2+tr(sk)FJH,H)]=0, (3.27)

    where AH is the shape operator associated with mean curvature vector H.

    Using Bochner formula, we get

    18(u+2)|H|2=|AH|2+|H|2+18tr(sk)FJH,H). (3.28)

    By the Cauchy-Schwarz inequality, we have |AH|2u|H|4. Using this fact, we have

    18(u+2)|H|2u|H|4+|H|2+18tr(sk)FJH,H)u|H|4+18tr(sk)FJH,H)u|H|4. (3.29)

    Since H is a non-zero constant, we have

    0<|H|2u+28u.

    If |H|2u+28u and M is proper-biharmonic, all of the above inequalities become equalities. Thus, we have H|2=0 and tr(sk)=0 as FJ is an isometry. Since the Cuachy-Schwarz inequality becomes equality, we have M as pseudo-umbilical.

    Remark 3.11. The cases for which FXΓ(TM) and FNΓ(TM) for any XΓ(TM) and NΓ(TM) establish the results comparable to those established in this paper. The proofs of all those results follow a similar procedure; thus, they haven't been discussed here.

    Finally, we discuss a non-existence case for the product of a unit sphere and a hyperbolic space. Out of all the discussed cases, the non-existence result can be found only for totally-complex Lagrangian submanifolds. Same has been discussed here:

    Proposition 3.12. There doesn't exist any proper biharmonic totally complex Lagrangian submanifold (dimension 2) with parallel mean curvature in S2×Hn2 such that FXΓ(TM) and FNΓ(TM) for any XΓ(TM) and NΓ(TM).

    Proof. Since mean curvature H is parallel and not identically zero. Therefore, FH isn't zero identically.

    M is trivially biharmonic, according to Theorem 3.1, we have

    u2grad|H|2+2tr(AH(.))+c1+c28[fsHtr(f)sH]+c1c28[sHusH3(sH)]=0. (3.30)

    For the above equation, we have c1+c2=0 and c1c2=2,

    or

    u2grad|H|2+2tr(AH(.))+14[(u+2)sH]=0. (3.31)

    Using the hypothesis, we have sH=0 or FH=0, which isn't possible.

    We established the necessary and sufficient conditions for the submanifolds of Kaehler product manifolds to be biharmonic. And we derived the magnitude of scalar curvature for the hypersurfaces in a product of two unit spheres. Also, for the same product, the magnitude of the mean curvature vector for Lagrangian submanifolds has been estimated. Finally, we proved the non-existence condition for totally complex Lagrangian submanifolds in a product of unit sphere and a hyperbolic space.

    The authors declare no conflict of interest.



    [1] J. Eells, J. H. Sampson, Harmonic mappings of Riemannian manifolds, Am. J. Math., 86 (1964), 109–160. doi: 10.2307/2373037
    [2] G. Y. Jiang, 2-Harmonic maps and their first and second variational formulas, Chin. Ann. Math. Ser. A, 7 (1986), 389–402.
    [3] R. I. Caddeo, S. Montaldo, M. P. Piu, On biharmonic maps, Int. Congr. Differ. Geom., Amer. Math. Soc., 288 (2001), 286–290.
    [4] J. Inoguchi, Submanifolds with harmonic mean curvature vector field in contact 3-manifolds, Colloq. Math., 100 (2004), 163–179. doi: 10.4064/cm100-2-2
    [5] S. Maeta, H. Urakawa, Biharmonic Lagrangian submanifolds in Kaehler manifolds, Glasgow Math. J., 55 (2013), 465–480. doi: 10.1017/S0017089512000730
    [6] S. Montaldo, C. Oniciuc, A short survey on biharmonic maps between Riemannian manifolds, Rev. Union Mat. Argent., 47 (2006), 1–22.
    [7] Y. L. Ou, Biharmonic hypersurfaces in Riemannian manifolds, Pacific J. Math., 248 (2010), 217–232. doi: 10.2140/pjm.2010.248.217
    [8] H. Urakawa, Sasaki manifolds, Kaehler cone manifolds and biharmonic submanifolds, Illinois J. Math., 58 (2014), 521–535.
    [9] R. Caddeo, S. Montaldo, C. Oniciuc, Biharmonic submanifolds in spheres, Israel J. Math., 130 (2002), 109–123. doi: 10.1007/BF02764073
    [10] D. Fetcu, E. Loubeau, S. Motaldo, C. Oniciuc, Biharmonic submanifolds of CPn, Math. Z., 266 (2010), 505–531. doi: 10.1007/s00209-009-0582-z
    [11] D. Fetcu, C. Oniciuc, Explicit formulas for biharmonic submanifolds in Sasakian space forms, Pacific J. Math., 240 (2009), 85–107. doi: 10.2140/pjm.2009.240.85
    [12] D. Fetcu, C. Oniciuc, H. Rosenberg, Biharmonic submanifolds with parallel mean curvature in Sn× R, J. Geom. Anal., 23 (2013), 2158–2176. doi: 10.1007/s12220-012-9323-3
    [13] J. Roth, A note on biharmonic submanifolds of product spaces, J. Geom., 104 (2013), 375–381. doi: 10.1007/s00022-013-0168-0
    [14] J. Roth, A. Upadhaya, Biharmonic submanifolds of generalized space forms, Differ. Geom. Appl., 50 (2017), 88–104. doi: 10.1016/j.difgeo.2016.11.003
    [15] B. Y. Chen, Chen's biharmonic conjecture and submanifolds with parallel normalized mean curvature vector, Mathematics, 7 (2019), 710. doi: 10.3390/math7080710
    [16] Y. Fu, M. Hang, X. Zhan, On Chen's conjecture for hypersurfaces in R5, 2020. arXiv: 2006.07612v3.
    [17] Y. Li, S. Liu, Z. Wang, Tangent developables and Darboux developables of framed curves, Topol. Appl., (2020), 107526.
    [18] Y. Li, Z. Wang, Lightlike tangent developables in de Sitter 3-space, J. Geom. Phys., 164 (2021), 1–11.
    [19] Y. Li, Z. Wang, T. Zhao, Geometric algebra of singular ruled surfaces, Adv. Appl. Clifford Algebras., 31 (2021), 1–19. doi: 10.1007/s00006-020-01101-8
    [20] Y. Li, Y. Zhu, Q. Sun, Singularities and dualities of pedal curves in pseudo-hyperbolic and de Sitter space, Int. J. Geom. Methods Mod. Phys., 18 (2021), 1–31.
    [21] K. Yano, M. Kon, Structures on manifolds, World Scientific Publishing Co., Singapore., 1984.
    [22] A. Balmus, S. Montaldo, C. Oniciuc, Biharmonic PNMC submanifolds in spheres, Ark. Mat., 51 (2013), 197–221. doi: 10.1007/s11512-012-0169-5
    [23] B. Y. Chen, Total mean curvature and submanifolds of finite type, World Scientific Publishing Co., Singapore, 1984.
    [24] R. L. Bishop, S. I. Goldberg, On the topology of positively curved Kaehler manifolds II, Tohoku Math. J., 17 (1962), 310–318.
  • This article has been cited by:

    1. Yanlin Li, Mohan Khatri, Jay Prakash Singh, Sudhakar K. Chaubey, Improved Chen’s Inequalities for Submanifolds of Generalized Sasakian-Space-Forms, 2022, 11, 2075-1680, 324, 10.3390/axioms11070324
    2. Yanlin Li, Ali Uçum, Kazım İlarslan, Çetin Camcı, A New Class of Bertrand Curves in Euclidean 4-Space, 2022, 14, 2073-8994, 1191, 10.3390/sym14061191
    3. Nadia Alluhaibi, Rashad A. Abdel-Baky, Kinematic Geometry of Timelike Ruled Surfaces in Minkowski 3-Space E13, 2022, 14, 2073-8994, 749, 10.3390/sym14040749
    4. Yanlin Li, Santu Dey, Sampa Pahan, Akram Ali, Geometry of conformal η-Ricci solitons and conformal η-Ricci almost solitons on paracontact geometry, 2022, 20, 2391-5455, 574, 10.1515/math-2022-0048
    5. Yongqiao Wang, Lin Yang, Pengcheng Li, Yuan Chang, Singularities of Osculating Developable Surfaces of Timelike Surfaces along Curves, 2022, 14, 2073-8994, 2251, 10.3390/sym14112251
    6. Rashad A. Abdel-Baky, Fatemah Mofarreh, A Study on the Bertrand Offsets of Timelike Ruled Surfaces in Minkowski 3-Space, 2022, 14, 2073-8994, 783, 10.3390/sym14040783
    7. Sachin Kumar Srivastava, Fatemah Mofarreh, Anuj Kumar, Akram Ali, Characterizations of PR-Pseudo-Slant Warped Product Submanifold of Para-Kenmotsu Manifold with Slant Base, 2022, 14, 2073-8994, 1001, 10.3390/sym14051001
    8. Yanlin Li, Pişcoran Laurian-Ioan, Akram Ali, Ali H. Alkhaldi, Null Homology Groups and Stable Currents in Warped Product Submanifolds of Euclidean Spaces, 2021, 13, 2073-8994, 1587, 10.3390/sym13091587
    9. Sushil Kumar, Mohd Bilal, Rajendra Prasad, Abdul Haseeb, Zhizhi Chen, V-Quasi-Bi-Slant Riemannian Maps, 2022, 14, 2073-8994, 1360, 10.3390/sym14071360
    10. Xiaoming Fan, Yanlin Li, Prince Majeed, Mehraj Ahmad Lone, Sandeep Sharma, Geometric Classification of Warped Products Isometrically Immersed into Conformal Sasakian Space Froms, 2022, 14, 2073-8994, 608, 10.3390/sym14030608
    11. Yanlin Li, Rajendra Prasad, Abdul Haseeb, Sushil Kumar, Sumeet Kumar, A Study of Clairaut Semi-Invariant Riemannian Maps from Cosymplectic Manifolds, 2022, 11, 2075-1680, 503, 10.3390/axioms11100503
    12. Nadia Alluhaibi, Rashad A. Abdel-Baky, Monia Naghi, On the Bertrand Offsets of Timelike Ruled Surfaces in Minkowski 3-Space, 2022, 14, 2073-8994, 673, 10.3390/sym14040673
    13. Yanlin Li, Akram Ali, Fatemah Mofarreh, Abimbola Abolarinwa, Rifaqat Ali, Umair Ali, Some Eigenvalues Estimate for the ϕ -Laplace Operator on Slant Submanifolds of Sasakian Space Forms, 2021, 2021, 2314-8888, 1, 10.1155/2021/6195939
    14. Rashad Abdel-Satar Abdel-Baky, Mohamed Khalifa Saad, Singularities of Non-Developable Ruled Surface with Space-like Ruling, 2022, 14, 2073-8994, 716, 10.3390/sym14040716
    15. Pengfei Zhang, Yanlin Li, Soumendu Roy, Santu Dey, Geometry of α-Cosymplectic Metric as ∗-Conformal η-Ricci–Yamabe Solitons Admitting Quarter-Symmetric Metric Connection, 2021, 13, 2073-8994, 2189, 10.3390/sym13112189
    16. Qiming Zhao, Lin Yang, Yongqiao Wang, Geometry of Developable Surfaces of Frenet Type Framed Base Curves from the Singularity Theory Viewpoint, 2022, 14, 2073-8994, 975, 10.3390/sym14050975
    17. Haibo Yu, Liang Chen, Singularities of Slant Focal Surfaces along Lightlike Locus on Mixed Type Surfaces, 2022, 14, 2073-8994, 1203, 10.3390/sym14061203
    18. Yanlin Li, Dipen Ganguly, Santu Dey, Arindam Bhattacharyya, Conformal η-Ricci solitons within the framework of indefinite Kenmotsu manifolds, 2022, 7, 2473-6988, 5408, 10.3934/math.2022300
    19. Haiming Liu, Jiajing Miao, Extended Legendrian Dualities Theorem in Singularity Theory, 2022, 14, 2073-8994, 982, 10.3390/sym14050982
    20. Pengfei Zhang, Yanlin Li, Soumendu Roy, Santu Dey, Arindam Bhattacharyya, Geometrical Structure in a Perfect Fluid Spacetime with Conformal Ricci–Yamabe Soliton, 2022, 14, 2073-8994, 594, 10.3390/sym14030594
    21. Sümeyye Gür Mazlum, Süleyman Şenyurt, Luca Grilli, The Dual Expression of Parallel Equidistant Ruled Surfaces in Euclidean 3-Space, 2022, 14, 2073-8994, 1062, 10.3390/sym14051062
    22. Yanlin Li, Akram Ali, Fatemah Mofarreh, Nadia Alluhaibi, Bibhas Ranjan Majhi, Homology Groups in Warped Product Submanifolds in Hyperbolic Spaces, 2021, 2021, 2314-4785, 1, 10.1155/2021/8554738
    23. Yongqiao Wang, Lin Yang, Yuxin Liu, Yuan Chang, Singularities for Focal Sets of Timelike Sabban Curves in de Sitter 3-Space, 2022, 14, 2073-8994, 2471, 10.3390/sym14122471
    24. Yanlin Li, Abimbola Abolarinwa, Shahroud Azami, Akram Ali, Yamabe constant evolution and monotonicity along the conformal Ricci flow, 2022, 7, 2473-6988, 12077, 10.3934/math.2022671
    25. Nasser Bin Turki, A Note on Incompressible Vector Fields, 2023, 15, 2073-8994, 1479, 10.3390/sym15081479
    26. S. K. Yadav, D. L. Suthar, Kählerian Norden spacetime admitting conformal η-Ricci–Yamabe metric, 2024, 21, 0219-8878, 10.1142/S0219887824502347
  • Reader Comments
  • © 2021 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(2849) PDF downloads(100) Cited by(26)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog