The main objective of this paper is to achieve the Chen-Ricci inequality for biwarped product submanifolds isometrically immersed in a complex space form in the expressions of the squared norm of mean curvature vector and warping functions.The equality cases are likewise discussed. In particular, we also derive Chen-Ricci inequality for CR-warped product submanifolds and point wise semi slant warped product submanifolds.
Citation: Amira A. Ishan, Meraj Ali Khan. Chen-Ricci inequality for biwarped product submanifolds in complex space forms[J]. AIMS Mathematics, 2021, 6(5): 5256-5274. doi: 10.3934/math.2021311
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The main objective of this paper is to achieve the Chen-Ricci inequality for biwarped product submanifolds isometrically immersed in a complex space form in the expressions of the squared norm of mean curvature vector and warping functions.The equality cases are likewise discussed. In particular, we also derive Chen-Ricci inequality for CR-warped product submanifolds and point wise semi slant warped product submanifolds.
The accoplishment of warped product manifolds came into existent after the study of Bishop and O'Neill [1] on the manifolds of negative curvature. Examining the fact that a Riemannian product of manifolds can not have negative curvature, they constructed the model of warped product manifolds for the class of manifolds of negative (or non positive) curvature which is defined as follows:
Let (U1,g1) and (U2,g2) be two Riemannian manifolds with Riemannian metrics g1 and g2 respectively and ψ be a positive differentiable function on U1. If ξ:U1×U2→U1 and η:U1×U2→U2 are the projection maps given by ξ(p,q)=p and η(p,q)=q for every (p,q)∈U1×U2, then the warped product manifold is the product manifold U1×U2 equipped with the Riemannian structure such that
g(V1,V2)=g1(ξ∗V1,ξ∗V2)+(ξ∘π)2g2(η∗V1,η∗V2), |
for all V1,V2∈TU. The function ψ is called the warping function of the warped product manifold. If the warping function is constant, then the warped product is trivial i.e., simply Riemannian product. On the basis of the fact that warped product manifolds admit a number of applications in Physics and theory of relativity [2], this has been a topic of extensive research. Warped products provide many fundamental solutions to Einstein field equations [2]. The concept of modelling of space-time near black holes adopts the idea of warped product manifolds [3]. Schwartzschild space-time is an example of warped product U×rK2, where the base U=R×R+ is a half plane r>0 and the fibre K2 is the unit sphere. Under certain conditions, the Schwartzchild space-time becomes the black hole. A cosmological model to represent the universe as a space-time known as Robertson-Walker model is a warped product [4].
In [1] authors have studied some fundamental features of warped product manifolds. An extrinsic study on warped product submanifolds of the kaehler manifolds was performed by B. Y. Chen ([5,6]). Since then, many geometers have explored warped product manifolds in different settings like almost complex and almost contact manifolds and various existence results have been investigated (see the survey article [7]).
In 1999, Chen [8] discovered a relationship between Ricci curvature and squared mean curvature vector for an arbitrary Riemannian manifold. On the line of Chen a series of articles have been appeared to formulate the relationship between Ricci curvature and squared mean curvature in the setting of some important structures on Riemannian manifolds (see [9,10,11,12,13,14]). Recently, Mustafa et al. [15] proved a relationship between Ricci curvature and squared mean curvature for warped product submanifolds of a semi-slant submanifold of Kenmotsu space forms.
In this paper, our aim is to obtain a relationship between Ricci curvature and squared mean curvature for biwarped product submanifolds in the setting of complex space forms.
Let ˉU be an almost Hermitian manifold with an almost complex structure J and a Hermitian metric g, i.e., J2=−I and g(JV1,JV2)=g(V1,V2), for all vector fields V1,V2 on ˉU. If J is parallel with respect to the Levi-Civita connection ˉD on ˉU, that mean
(ˉDV1J)V2=0, | (2.1) |
for all V1,V2∈TˉU, then (ˉU,J,g,ˉD) is called a Kaehler manifold. A Kaehler manifold ˉU is called a complex space form if it has constant holomorphic sectional curvature denoted by ˉU(c). The curvature tensor of the complex space form ˉU(c) is given by
ˉR(V1,V2,V2,V4)=c4[g(V2,V3)g(V1,V4)−g(V1,V3)g(V2,V4)+g(V1,JV3)g(JV2,V4)−g(V2,JV3)g(JV1,V4)+2g(V1,JV2)g(JV3,V4)], | (2.2) |
for any V1,V2,V3,V4∈TˉU.
Let U be an n−dimensional Riemannian manifold isometrically immersed in a m−dimensional Riemannian manifold ˉU. Then the Gauss and Weingarten formulas are ˉDV1V2=DV1V2+h(V1,V2) and ˉDV1ξ=−AξV1+D⊥V1ξ respectively, for all V1,V2∈TU and ξ∈T⊥U. Where D is the induced Levi-civita connection on U, ξ is a vector field normal to U, h is the second fundamental form of U, D⊥ is the normal connection in the normal bundle T⊥U and Aξ is the shape operator of the second fundamental form. The second fundamental form h and the shape operator are associated by the following formula
g(h(V1,V2),ξ)=g(AξV1,V2). | (2.3) |
The equation of Gauss is given by
R(V1,V2,V3,V4)=ˉR(V1,V2,V3,V4)+g(h(V1,V4),h(V2,V3))−g(h(V1,V3),h(V2,V4)), | (2.4) |
for all V1,V2,V3,V4∈TU. Where, ˉR and R are the curvature tensors of ˉU and U respectively.
For any V∈TU and N∈T⊥U, JV1 and JN can be decomposed as follows
JV1=PV1+FV1 | (2.5) |
and
JN=tN+fN, | (2.6) |
where PV1 (resp. tN) is the tangential and FV1 (resp. fN) is the normal component of JV1 (resp. JN).
For any orthonormal basis {e1,e2,…,ek} of the tangent space TxU, the mean curvature vector H(x) and its squared norm are defined as follows
H(x)=1nk∑i=1h(ei,ei),‖H‖2=1k2k∑i,j=1g(h(ei,ei),h(ej,ej)), | (2.7) |
where k is the dimension of U. If h=0 then the submanifold is said to be totally geodesic and minimal if H=0. If h(V1,V2)=g(V1,V2)H for all V1,V2∈TU, then U is called totally umbilical.
The scalar curvature of ˉU is denoted by ˉτ(ˉU) and is defined as
ˉτ(ˉU)=∑1≤p<q≤mˉκpq, | (2.8) |
where ˉκpq=ˉκ(ep∧eq) and m is the dimension of the Riemannian manifold ˉM. Throughout this study, we shall use the equivalent version of the above equation, which is given by
2ˉτ(ˉU)=∑1≤p<q≤mˉκpq. | (2.9) |
In a similar way, the scalar curvature ˉτ(Lx) of a L−plane is given by
ˉτ(Lx)=∑1≤p<q≤mˉκpq. | (2.10) |
Let {e1,…,ek} be an orthonormal basis of the tangent space TxU and if er belongs to the orthonormal basis {ek+1,…em} of the normal space T⊥U, then we have
hrpq=g(h(ep,eq),er) | (2.11) |
and
‖h‖2=n∑p,q=1g(h(ep,eq),h(ep,eq)). | (2.12) |
Let κpq and ˉκpq be the sectional curvatures of the plane sections spanned by ep and eq at x in the submanifold Uk and in the Riemannian space form ˉUm(c), respectively. Thus by Gauss equation, we have
κpq=ˉκpq+m∑r=k+1(hrpphrqq−(hrpq)2). | (2.13) |
The global tensor field for orthonormal frame of vector field {e1,…,ek} on Uk is defined as
ˉT(V1,V2)=k∑i=1{g(ˉR(ei,V1)V2,ei)}, | (2.14) |
for all V1,V2∈TxUk. The above tensor is called the Ricci tensor. If we fix a distinct vector eu from {e1,…,ek} on Uk, which is governed by χ. Then the Ricci curvature is defined by
R(χ)=k∑p=1p≠uκ(ep∧eu). | (2.15) |
For a smooth function ψ on a Riemannian manifold U with Riemannian metric g, the gradient of ψ is denoted by ∇ψ and is defined as
g(∇ψ,U1)=U1ψ, | (2.16) |
for all U1∈TU.
Let the dimension of U is k and {e1,e2,…,ek} be a basis of TU. Then as a result of (2.16), we get
‖∇ψ‖2=k∑i=1(ei(ψ))2. | (2.17) |
The Laplacian of ψ is defined by
Δψ=k∑i=1{(∇eiei)ψ−eieiψ}. | (2.18) |
B. Y. Chen and F. Dillen [16] generalize the definition of warped product submanifold to multiply warped product manifolds as follows.
Let {Ui},i=1,2,…,k be Riemannian manifolds with respective Riemannian metrics {gi}i=1,2,…,k and {ψ}i=2,3,…,k are positive valued functions on U1. Then the product manifold U=U1×U2×⋯×Uk endowed with the Riemannian metric g given by
g=h∗1(g1)+k∑i=2(ψi∘h1)2h∗i(gi) |
is called multiply warped product manifold and denoted by U=U1×f2U2×⋯×fkUk where hi(i=1,2,…,k) are the projection maps of U onto Ui respectively. The functions fi are known as the warping functions [16]. If the warping functions are constants, the warped product is simply Riemannian product of manifolds. As a paricular case of multiply warped product manifolds, we can define biwarped product manifolds for i=3. For i=2, multiply warped product manifold reduces to single warped product manifold. Consider the biwarped product manifold U=U0×f1U1×f2U2 with the Levi-civita connection of Ui for i=0,1,2. Now, we have the following result for biwarped product submanifold.
Lemma 3.1. [17] Let U=U0×f1U1×f2U2 be a biwarped product manifold. Then we have
DV1V2=DV2V1=V1(lnfi)V2 | (3.1) |
for V1∈TU0 and V2∈TUi, for i=1,2.
Recently, H. M. Tastan [18] studied biwarped submanifolds in the Kaehler manifolds and this was followed by M. A. Khan and K. Khan [19]. Basically, M. A. Khan and K. Khan explored biwarped product submnaifolds of the type U=UT×f1U⊥×f2Uθ in the setting of complex space forms. Where UT, U⊥ and Uθ are the invarianat, totally real and pointwise slant submanifolds respectively. Throughout this study we consider k−dimensional biwarped product submanifold Uk=Uk1T×f2Uk2⊥×f3Uk3θ of a complex space form, where k1, k2,k3 are the dimensions of the invariant, totally real and pointwise slant submanifolds. If Uk3θ={0} then the biwarped product submanifold becomes the CR-warped product submanifold. Similarly, if Uk2⊥={0} then the biwarped product submanifold reduced to pointwise semi-slant warped product submanifold.
For a biwarped product submanifold Uk=Uk1T×f2Uk2⊥×f3Uk3θ of a Riemannian manifold from Eq (3.5) of [16] one can conclude the following result
Δf2f2+Δf3f3=k1∑i=1k2∑j=1κ(ei,ej)+k1∑i=1k3∑k=1κ(ei,ek). | (3.2) |
Now, we have the following initial result.
Lemma 3.2. Let Uk=Uk1T×f2Uk2⊥×f3Uk3θ be a biwarped product submanifold isometrically immersed in a Kaehler manifold ˉU. Then
(i) g(h(V1,V2),FV3)=0,
(ii) g(h(V1,V2),JV4)=0,
(iii) g(h(JV1,JV1),N)=−g(h(V1,V1),N),
for any V1,V2∈TUk1T, V4∈TUk2⊥, V3∈TUk3θ and N belongs to invariant subbundle of T⊥U.
Proof. By using Gauss and Weingarten formulae in Eq (2.1), we have
DV1PV3+h(V1,PV3)−AFV3V1+D⊥V1FV3+JDV1V3+DV3JV1+Jh(V1,V3)=0, |
taking inner product with V2 and using 3.1, we get the required result. In a similar way, we can prove the part (ii).
To prove (iii), for any V1∈TUT we have
ˉDV1JV1=JˉDV1V1, |
using Gauss formula and (2.1), we get
DV1JV1+h(JV1,V1)=JDV1V1+Jh(V1,V1), |
taking inner product with JN, above equation yields
g(h(JV1,V1),JN)=g(h(V1,V1),N), | (3.3) |
interchanging V1 by JV1 the above equation gives
g(h(JV1,V1),JN)=−g(h(JV1,JV1),N). | (3.4) |
From (3.3) and (3.4), we get the required result.
Definition 3.1. The warped product U1×f2U2×f3U3 isometrically immersed in a Riemannian manifold ˉU is called Ui totally geodesic if the partial second fundamental form hi vanishes identically. It is called Ui-minimal if the partial mean curvature vector Hi becomes zero for i=1,2,3.
Assumme that the distributions corresponding to the submanifolds Uk1T, Uk2⊥ and Uk3θ are S, S⊥ and Sθ respectively. From the Lemma 3.2 it is evident that the isometric immersion Uk1T×f2Uk2⊥×f3Uk3θ into a Kaehler manifold is D− minimal. The S− minimality property provides us a useful relationship between the biwarped product submanifold Uk1T×f2Uk2⊥×f3Uk3θ and the equation of Gauss.
Let {e1,…,ep,ep+1=Je1,…,ek1=Jep,ek1+1,…,ek2,ek2+1=e1, …,ek2+q=eq,ek2+q+1=eq+1=secθPe1,…e(k3=2q)=ek3=secθPeq} be a local orthonormal frame of vector fields on the biwarped product submanifold Uk1T×f2Uk2⊥×f3Uk3θ such that the set {e1,…,ep,ep+1=Je1,…,ek1=Jep} is tangent to Uk1T, the set {ek1+1,…,ek2} is tangent to Uk2⊥ and the set {ek2+1,…,ek2+q,…ek3} is tangent to Uk3θ. Moreover, {ek+1=Jek1+1,…ek+k2=Jek2,ek+k2+1=cscθFe1,…,ek+k3=cscθFeq,ek+k2+k3+1=ˉe1,…,em=ˉek} is a basis for the normal bundle T⊥U, such that the sets {ek+1=Jek1+1,…ek+k2=Jek2} is tangent to JS⊥, {ek+1=cscθFe1,…,ek+k2=cscθFeq} is tangent to FSθ and {ˉe1,…,ˉel} is tangent to the complementary invariant subbundle μ with even dimension l.
From Lemma 3.2, it is easy to conclude that
m∑r=k+1k1∑i,j=1g(h(ei,ej),er)=0. | (3.5) |
Thus it follows that the trace of h due to Uk1T becomes zero. Hence in view of the Definition 3.1, we obtain the following important result.
Theorem 3.3. Let Uk=Uk1T×f2Uk2⊥×f3Uk3θ be a biwarped product submanifold isometrically immersed in a Kaehler manifold. Then Uk is S− minimal.
So, it is easy to conclude the following
‖H‖2=1k2m∑r=k+1(hrk1+1k1+1+⋯+hrk2k2+⋯+hrkk)2, | (3.6) |
where ‖H‖2 is the squared mean curvature.
In this section, we investigate Ricci curvature in terms of the squared norm of mean curvature and the warping functions as follows.
Theorem 4.1. Let Uk=Uk1T×f2Uk2⊥×f3Uk3θ be a biwarped product submanifold isometrically immersed in a complex space form ˉU(c). Then for each orthogonal unit vector field χ∈TxU, either tangent to Uk1T, Uk2⊥ or Uk3θ, we have
(1) The Ricci curvature satisfy the following inequalities
(i) If χ is tangent to Uk1T, then
14k2‖H‖2≥R(χ)+k2Δf2f2+k3Δf3f3+c4(k−k1k2−k2k3−k1k3−12). | (4.1) |
(ii) If χ is tangent to Uk2⊥, then
14k2‖H‖2≥R(χ)+k2Δf2f2+k3Δf3f3+c4(k−k1k2−k2k3−k1k3+1). | (4.2) |
(iii)χ is tangent to Uk2θ, then
14k2‖H‖2≥R(χ)+k2Δf2f2+k3Δf3f3+c4(k−k1k2−k2k3−k1k3+1−32cos2θ). | (4.3) |
(2) If H(x)=0, then each point x∈Uk there is a unit vector field χ which satisfies the equality case of (1) if and only if Uk is mixed totally geodesic and χ lies in the relative null space Nx at x.
(3) For the equality case we have
(a) The equality case of (4.1) holds identically for all unit vector fields tangent to Uk1T at each x∈Uk if and only if Uk is mixed totally geodesic and S−totally geodesic biwarped product submanifold in ˉUm(c).
(b) The equality case of (4.2) holds identically for all unit vector fields tangent to Uk2⊥ at each x∈Uk if and only if U is mixed totally geodesic and either Uk is S⊥- totally geodesic biwarped product or Uk is a S⊥ totally umbilical in ˉSm(c) with dim S⊥=2.
(c) The equality case of (4.3) holds identically for all unit vector fields tangent to Uk3θ at each x∈Uk if and only if U is mixed totally geodesic and either Uk is Sθ- totally geodesic biwarped product submanifold or Uk is a Sθ totally umbilical in ˉUm(c) with dim Sθ=2.
(d) The equality case of (1) holds identically for all unit tangent vectors to Uk at each x∈Uk if and only if either Uk is totally geodesic submanifold or Uk is a mixed totally geodesic totally umbilical and S− totally geodesic submanifold with dim Uθ=2 and dim U⊥=2
where k1, k2, and k3 are the dimensions of Uk1T, Uk2⊥, and Uk3θ respectively.
Proof. Suppose that Uk=Uk1T×f2Uk2⊥×f3Uk3θ be a biwarped product submanifold of a complex space form. From Gauss equation, we have
k2‖H‖2=2τ(Uk)+‖h‖2−2ˉτ(Uk). | (4.4) |
Let {e1,…,ek1,ek1+1,…,ek2,…ek} be a local orthonormal frame of vector fields on Uk such that {e1,…,ek1} are tangent to Uk1T, {ek1+1,…,ek2} are tangent to Uk2⊥ and {ek2+1,…,ek} are tangent to Uk3θ. So, the unit tangent vector χ=eA∈{e1,…,ek} can be expanded (4.4) as follows
k2‖H‖2=2τ(Uk)+12m∑r=k+1{(hr11+…hrk2k2+⋯+hrkk−hrAA)2+(hrAA)2} |
−m∑r=k+1∑1≤i≠j≤khriihrjj−2ˉτ(Uk). | (4.5) |
The above expression can be written as follows
k2‖H‖2=2τ(Uk)+12m∑r=k+1{(hr11+…hrk2k2+⋯+hrkk)2+(2hrAA−(hr11+⋯+hrkk))2}+2m∑r=k+1∑1≤i<j≤k(hrij)2−2m∑r=k+1∑1≤i<j≤ki,j≠Ahriihrjj−2ˉτ(Uk). |
In view of the Lemma 3.2, the preceding expression takes the form
k2‖H‖2=2τ(Uk)+12m∑r=k+1{(hrk1+1k1+1+…hrk2k2+⋯+hrkk)2+12m∑r=k+1(2hrAA−(hrk1+1k1+1+…hrk2k2+⋯+hrkk))2+2m∑r=k+1∑1≤i<j≤k(hrij)2−2m∑r=k+1∑1≤i<j≤ki,j≠Ahriihrjj−2ˉτ(Uk). | (4.6) |
Considering unit tangent vector χ=eA, we have three choices χ is either tangent to the base manifold Uk1T or to the fibers Uk2⊥ and Uk3θ.
Case 1: If χ is tangent to Uk1T, then we need to choose a unit vector field from {e1,…,ek1}. Let χ=e1. Then from (2.14) and (3.5) we have
k2‖H‖2≥R(χ)+12m∑r=k+1{(hrk1+1k1+1+…hrk2k2+⋯+hrkk)2+k2Δf2f2+k3Δf3f3+12m∑r=k+1(2hr11−(hrk1+1k1+1+…hrk2k2+⋯+hrkk))2+m∑r=k+1∑1≤α<β≤k1(hrααhrββ−(hrαβ)2)+m∑r=k+1∑k1+1≤p<q≤k2(hrpphrqq−(hrpq)2)+m∑r=k+1∑k2+1≤s<t≤k(hrsshrtt−(hrst)2)+m∑r=k+1∑1≤i<j≤k(hrij)2−m∑r=k+1∑2≤i<j≤k(hriihrjj)−2ˉτ(U)+∑2≤i<j≤kˉκ(ei,ej)+ˉτ(Uk1T)+ˉτ(Uk2⊥)+ˉτ(Uk3θ). | (4.7) |
Putting V1,V4=ei and V2,V3=ej in the formula (2.2), we have
2ˉτ(U)=c4[k(k−1)+3k1+3k3cos2θ] | (4.8) |
∑2≤i<j≤kˉκ(ei,ej)=c8[(k−1)(k−2)+3(k1−1)+3k3cos2θ] |
ˉτ(Uk1T)=c8[k1(k1−1)+3k1] |
ˉτ(Uk2⊥)=c8[k2(k2−1)] |
ˉτ(Uk3θ)=c8[k3(k3−1)+3k3cos2θ]. |
Using these values in (4.7), we get
k2‖H‖2≥R(χ)+12k2‖H‖2+12m∑r=k+1(2hr11−(hrk1+1k1+1+⋯+hrkk))2+k2Δf2f2+k3Δf3f3+m∑r=k+1k1∑i=1k2∑j=k1+1(hrij)2+m∑r=k+1k1∑i=1k∑k=k2+1(hrik)2+m∑r=k+1k1∑β=2hr11hrββ−m∑r=k+1k1∑i=2k2∑j=k1+1hriihrjj−m∑r=k+1k1∑i=2n∑n=k2+1hriihrnn+c4(k−k1k2−k2k3−k3k1−12). | (4.9) |
In view of Lemma 3.1
m∑r=k+1k1∑β=2hr11hrββ=m∑r=k+1(hr11)2 |
−m∑r=k+1k1∑i=2[k2∑j=k1+1hriihrjj+k∑n=k2+1hriihrnn]=m∑r=k+1n∑j=k1+1hr11hrjj. |
Utilizing in (4.9), we have
k2‖H‖2≥R(χ)+12k2‖H‖2+12m∑r=k+1(2hr11−(hrk1+1k1+1+⋯+hrkk))2+k2Δf2f2+k3Δf3f3+m∑r=k+1k1∑i=1k2∑j=k1+1(hrij)2+m∑r=k+1k1∑i=1k∑k=k2+1(hrik)2−m∑r=k+1(hr11)2+k1∑i=1k∑j=k1+1hriihrjj+c4(k−k1k2−k2k3−k3k1−12). | (4.10) |
The third term on the right hand side can be written as
12m∑r=k+1(2hr11−(hrk1+1k1+1+⋯+hrk2k2+⋯+hrkk))2=2m∑r=k+1(hr11)2+12k2‖H‖2−2m∑r=k+1[k2∑j=k1+1hr11hrjj+k∑n=k2+1hr11hrnn]. | (4.11) |
Combining above two expressions, we have
12k2‖H‖2≥R(χ)+m∑r=k+1(hr11)2−m∑r=k+1k∑j=k1+1hr11hrjj+12m∑r=k+1(hrk1+1k1+1+⋯+hrk2k2+⋯+hrkk)2+m∑r=k+1k1∑i=1k∑j=k1+1(hrij)2+k2Δf2f2+k3Δf3f3+c4(k−k1k2−k2k3−k3k1−12). | (4.12) |
Or equivalently
14k2‖H‖2≥R(χ)+14m∑r=k+1(2hr11−(hrk1+1k1+1+⋯+hrk2k2+⋯+hrkk))2+m∑r=k+1k1∑i=1k∑j=k1+1(hrij)2+k2Δf2f2+k3Δf3f3+c4(k−k1k2−k2k3−k3k1−12), | (4.13) |
which gives the inequality (i) of (1).
Case 2. If χ is tangent to Uk2⊥, we chose the unit vector from {ek1+1,…,ek2}. Suppose χ=ek2, then from (4.6), we deduce
k2‖H‖2≥R(χ)+12m∑r=k+1(hrk1+1k1+1+…hrk2k2+⋯+hrkk)2+k2Δf2f2+k3Δf3f3+12m∑r=k+1((hrk1+1k1+1+…hrk2k2+⋯+hrkk)−2hrk2k2)2+m∑r=k+1∑1≤α<β≤k1(hrααhrββ−(hrαβ)2)+m∑r=k+1∑k1+1≤s<t≤k2(hrsshrtt−(hrst)2)+m∑r=k+1∑k2+1≤p<q≤k(hrpphrqq−(hrpq)2)+m∑r=k+1∑1≤i<j≤k(hrij)2−m∑r=k+1∑1≤i<j≤ki,j≠k2(hriihrjj)−2ˉτ(U)+∑1≤i<j≤ki,j≠k2ˉκ(ei,ej)+ˉτ(Uk1T)+ˉτ(Uk2⊥)+ˉτ(Uk3θ). | (4.14) |
From (2.2) by putting V1,V4=ei and V2,V3=ej, one can compute
∑1≤i<j≤ki,j≠k2ˉκ(ei,ej)=c8[(k−1)(k−2)+3k1+3k3cos2θ] |
ˉτ(Uk1T)=c8[k1(k1−1)+3k1] |
ˉτ(Uk2⊥)=c8[k2(k2−1)] |
ˉτ(Uk3θ)=c8[k3(k3−1)+3k3cos2θ]. |
Using these values together with (4.8) in (4.14) and applying similar techniques as in Case 1, we obtain
k2‖H‖2≥R(χ)+12m∑r=k+1((hrk1+1k1+1+…hrk2k2+⋯+hrkk)−2hrk2k2))2+12k2‖H‖2+k2Δf2f2+k3Δf3f3+m∑r=k+1∑1≤i<j≤k(hrij)2+m∑r=k+1[k2−1∑t=k1+1hrk2k2hrtt+k∑l=k2+1hrk2k2hrll]m∑r=1k1∑i=1[k2−1∑j=k1+1hriihrjj+k∑n=k2+1hriihrnn]+c4(k−k1k2−k2k3−k3k1+1). | (4.15) |
By the Lemma 3.1, one can conclude
m∑r=1k1∑i=1[k2−1∑j=k1+1hriihrjj+k∑n=k2+1hriihrnn]=0. |
The second and seventh terms on right hand side of (4.15) can be solved as follows
12m∑r=k+1((hrk1+1k1+1+⋯+hrkk)−2hrk2k2))2+m∑r=k+1[k2−1∑t=k1+1hrk2k2hrtt+k∑l=k2+1hrk2k2hrll]=12m∑r=k+1(hrk1+1k1+1+⋯+hrkk)2+2m∑r=k+1(hrk2k2)2−2m∑r=k+1k∑j=k1+1hrk2k2hrjj+m∑r=k+1k∑t=k1+1hrk2k2hrtt−m∑r=k+1(hrk2k2)2=12m∑r=k+1(hrk1+1k1+1+⋯+hrkk)2+m∑r=k+1(hrk2k2)2−m∑r=k+1k∑j=k1+1hrkkhrjj. | (4.16) |
Utilizing these two values in (4.15), we arrive
12k2‖H‖2≥R(χ)+m∑r=k+1(hrk2k2)2−m∑r=k+1k∑i=k1+1hrkkhrjj+12m∑r=k+1(hrk1+1k1+1+⋯+hrkk)2+12k2‖H‖2+k2Δf2f2+k3Δf3f3+m∑r=k+1k1∑i=1k∑j=k1+1(hrij)2+c4(k−k1k2−k2k3−k3k1+1). | (4.17) |
By using similar steps as in Case 1, the above inequality can be written as
14k2‖H‖2≥R(χ)+14m∑r=k+1(2hrk2k2−(hrk1+1k1+1+⋯+hrkk))2+k2Δf2f2+k3Δf3f3+c4(k−k1k2−k2k3−k1k3+1). | (4.18) |
The last inequality leads to inequality (ii) of (1).
Case 3. If χ is tangent to Uk3θ, then we choose the unit vector field from {ek2+1,…,ek}. Suppose the vector χ is ek. Then from (4.6)
k2‖H‖2≥R(χ)+12m∑r=k+1(hrk1+1k1+1+…hrk2k2+⋯+hrkk)2+k2Δf2f2+k3Δf3f3+12m∑r=k+1((hrk1+1k1+1+…hrk2k2+⋯+hrkk)−2hrkk)2+m∑r=k+1∑1≤α<β≤k1(hrααhrββ−(hrαβ)2)+m∑r=k+1∑k1+1≤s<t≤k2(hrsshrtt−(hrst)2)+m∑r=k+1∑k2+1≤p<q≤k(hrpphrqq−(hrpq)2)+m∑r=k+1∑1≤i<j≤k(hrij)2−m∑r=k+1∑1≤i<j≤k−1hriihrjj−2ˉτ(U)+∑1≤i<j≤k−1ˉκ(ei,ej)+ˉτ(Uk1T)+ˉτ(Uk2⊥)+ˉτ(Uk3θ). | (4.19) |
From (2.2), one can compute
∑1≤i<j≤k−1ˉκ(ei,ej)=c8[(k−1)(k−2)+3k1+3(k3−1)cos2θ] |
ˉτ(Uk1T)=c8[k1(k1−1)+3k1] |
ˉτ(Uk2⊥)=c8[k2(k2−1)] |
ˉτ(Uk3θ)=c8[k3(k3−1)+3k3cos2θ]. |
By usage of these values together with (4.8) in (4.19) and analogous to case 1 and case 2, we obtain
k2‖H‖2≥R(χ)+12k2‖H‖2+12m∑r=k+1((hrk1+1k1+1+…hrk2k2+⋯+hrkk)−2hrkk)2+k2Δf2f2+k3Δf3f3+m∑r=k+1∑1≤i<j≤k(hrij)2+m∑r=k+1k−1∑q=k1+1hrkkhrqq−m∑r=k+1k1∑i=1k−1∑j=k1+1hriihrjj+c4(k−k1k2−k2k3−k1k3+1−32cos2θ). | (4.20) |
On applying the Lemma 3.1, it is easy to verify
m∑r=k+1k1∑i=1k−1∑j=k1+1hriihrjj=0. | (4.21) |
Using in (4.20), we obtain
k2‖H‖2≥R(χ)+12k2‖H‖2+12m∑r=k+1((hrk1+1k1+1+…hrk2k2+⋯+hrkk)−2hrkk)2+k2Δf2f2+k3Δf3f3+m∑r=k+1∑1≤i<j≤k(hrij)2+m∑r=k+1k−1∑q=k1+1hrkkhrqq+c4(k−k1k2−k2k3−k1k3+1−32cos2θ). | (4.22) |
The third and seventh terms on the right hand side of (4.22) in a similar way as in case 1 and case 2 can be simplified as
12m∑r=k+1((hrk1+1k1+1+…hrk2k2+⋯+hrkk)−2hrkk)2+m∑r=k+1k−1∑q=k1+1hrkhrqq=12m∑r=k+1(hrk1+1k1+1+…hrk2k2+⋯+hrkk)2+m∑r=k+1(hrkk)2−m∑r=k+1k∑j=k1+1hrkkhrjj. | (4.23) |
By combining (4.22) and (4.23) and using similar techniques as used in case 1 and case 2, we can derive
14k2‖H‖2≥R(χ)+14m∑r=k+1(2hrkk−(hrk1+1k1+1+⋯+hrkk))2+k2Δf2f2+k3Δf3f3+c4(k−k1k2−k2k3−k1k3+1−32cos2θ). | (4.24) |
The last inequality leads to inequality (iii) in (1).
Next, we explore the equality cases of (1). First, we redefine the notion of the relative null space Nx of the submanifold Uk in the complex space form ˉUm(c) at any point x∈Uk, the relative null space was defined by B. Y. Chen [8], as follows
Nx={V1∈TxUk:h(V1,V2)=0,∀V2∈TxUk}. |
For A∈{1,…,k} a unit vector field eA tangent to Uk at x satisfies the equality sign of (4.1) identically if and only if
(i)k1∑p=1k∑q=k1+1hrpq=0(ii)k∑b=1n∑A=1b≠AhrbA=0(iii)2hrAA=k∑q=k1+1hrqq, | (4.25) |
holds for r∈{k+1,…m}, which implies that Uk is mixed totally geodesic biwarped product submanifold. Combining statements (ii) and (iii) with the fact that Uk is biwarped product submanifold, we get that the unit vector field χ=eA belongs to the relative null space Nx. The converse is trivial, this proves statement (2).
For a biwarped product submanifold, the equality sign of (4.1) holds identically for all unit tangent vector belong to UT at x if and only if
(i)k1∑p=1k∑q=k1+1hrpq=0(ii)k∑b=1k1∑A=1b≠AhrbA=0(iii)2hrpp=k∑q=k1+1hrqq, | (4.26) |
where p∈{1,…,k1} and r∈{k+1,…,m}. Since Uk is biwarped product submanifold, the third condition implies that hrpp=0,p∈{1,…,k1}. Using this in the condition (ii), we conclude that Uk is S−totally geodesic biwarped product submanifold in ˉUm(c) and mixed totally geodesicness follows from the condition (i). Which proves (a) in the statement (3).
For a biwarped product submanifold, the equality sign of (4.2) holds identically for all unit tangent vector fields tangent to U⊥ at x if and only if
(i)k1∑p=1n∑q=k1+1hrpq=0(ii)k∑b=1k2∑A=k1+1b≠AhrbA=0(iii)2hrKK=k∑q=k1+1hrqq, | (4.27) |
such that K∈{k1+1,…,k2} and r∈{k+1,…,m}. From the condition (iii) two cases emerge, that is
hrLL=0,∀L∈{k1+1,…,k2}andr∈{k+1,…,m}ordimU⊥=2. | (4.28) |
If the first case of (4.27) satisfies, then by virtue of condition (ii), it is easy to conclude that Uk is a S⊥− totally geodesic biwarped product submanifold in ˉUm(c). This is the first case of part (b) of statement (3).
For a biwarped product submanifold, the equality sign of (4.3) holds identically for all unit tangent vector fields tangent to Uk3θ at x if and only if
(i)k1∑p=1k∑q=k1+1hrpq=0(ii)n∑b=1k3∑A=k2+1b≠AhrbA=0(iii)2hrLL=n∑q=k1+1hrqq, | (4.29) |
such that L∈{k2+1,…,k} and r∈{k+1,…,m}. From the condition (iii) two cases arise, that is
hrLL=0,∀L∈{k2+1,…,n}andr∈{k+1,…,m}ordimUθ=2. | (4.30) |
If the first case of (4.29) satisfies, then by virtue of condition (ii), it is easy to conclude that Uk is a Sθ− totally geodesic biwarped product submanifold in ˉUm(c). This is the first case of part (c) of statement (3).
For the other case, assume that Uk is not Sθ−totally geodesic biwarped product submanifold and dim Uθ=2. Then condition (ii) of (4.29) implies that Uk is Sθ− totally umbilical biwarped product submanifold in ˉU(c), which is second case of this part. This verifies part (c) of (3).
To prove (d) using parts (a),(b) and (c) of (3), we combine (4.26), (4.27) and (4.29). For the first case of this part, assume that dimU⊥≠2 and dimUθ≠2. Since from parts (a), (b) and (c) of statement (3) we conclude that Uk is S−totally geodesic, S⊥− totally geodesic and Sθ− totally geodesic submanifolds in ˉUm(c). Hence Uk is a totally geodesic submanifold in ˉUm(c).
For another case, suppose that first case does not satisfy. Then parts (a), (b) and (c) provide that Uk is mixed totally geodesic and S− totally geodesic submanifold of ˉUm(c) with dimU⊥=2 and dimUθ=2. From the conditions (b) and (c) it follows that Uk is S⊥− and Dθ−totally umbilical biwarped product submanifolds and from (a) it is S−totally geodesic, which is part (d). This proves the theorem.
If Uk2⊥={0}, then the biwarped product submanifold becomes the Point wise semi-slant warped product submanifold that is Uk=Uk1T×f2Uk3θ. Now, we have the following corollary which can be deduced from the Theorem 4.2.
Corollary 4.2. Let Uk=Uk1T×f3Uk3θ be a pointwise semi-slant warped product submanifold isometrically immersed in a complex space form ˉU(c). Then for each orthogonal unit vector field χ∈TxU, either tangent to Uk1T or Uk3θ, we have
(1) The Ricci curvature satisfy the following inequalities
(i) If χ is tangent to Uk1T, then
14k2‖H‖2≥R(χ)+k3Δf3f3+c4(k−k1k3−12). | (4.31) |
(ii) χ is tangent to Uk3θ, then
14k2‖H‖2≥R(χ)+k3Δf3f3+c4(k−k1k3+1−32cos2θ). | (4.32) |
(2) If H(x)=0, then each point x∈Uk there is a unit vector field χ which satisfies the equality case of (1) if and only if Uk is mixed totally geodesic and χ lies in the relative null space Nx at x.
(3) For the equality case we have
(a) The equality case of (4.31) holds identically for all unit vector fields tangent to UT at each x∈Uk if and only if Uk is mixed totally geodesic and S−totally geodesic point wise semi slant warped product submanifold in ˉUm(c).
(b) The equality case of (4.32) holds identically for all unit vector fields tangent to Uk3θ at each x∈Uk if and only if S is mixed totally geodesic and either Uk is Dθ- totally geodesic point wise semi slant warped product submanifold or Uk is a Sθ totally umbilical in ˉUm(c) with dim Sθ=2.
(c) The equality case of (1) holds identically for all unit tangent vectors to Uk at each x∈Uk if and only if either Uk is totally geodesic submanifold or Uk is a mixed totally geodesic totally umbilical and S− totally geodesic submanifold with dim Uθ=2.
where k1 and k3 are the dimensions of Uk1T and Uk3θ respectively.
Now, we have another case that is if Uk3θ={0} then the biwarped product submanifold becomes the CR-warped product submanifold. In this case we have the following corollary.
Corollary 4.3. Let Uk=Uk1T×f2Uk2⊥ be a CR-warped product submanifold isometrically immersed in a complex space form ˉUm(c). Then for each orthogonal unit vector field χ∈TxU, either tangent to Uk1T or Uk2⊥, we have
(1) The Ricci curvature satisfy the following inequalities
(i) If χ is tangent to Uk1T, then
14k2‖H‖2≥R(χ)+U2Δf2f2+c4(k−k1k2−12). | (4.33) |
(ii) If χ is tangent to Uk2⊥, then
14k2‖H‖2≥R(χ)+k2Δf2f2+c4(k−k1k2+1). | (4.34) |
(2)If H(x)=0, then each point x∈Uk there is a unit vector field χ which satisfies the equality case of (1) if and only if Uk is mixed totally geodesic and χ lies in the relative null space Nx at x.
(3) For the equality case we have
(a) The equality case of (4.33) holds identically for all unit vector fields tangent to UT at each x∈Uk if and only if Uk is mixed totally geodesic and S−totally geodesic CR-warped product submanifold in ˉUm(c).
(b) The equality case of (4.34) holds identically for all unit vector fields tangent to Uk2⊥ at each x∈Uk if and only if U is mixed totally geodesic and either Uk is S⊥- totally geodesic biwarped product or Uk is a S⊥ totally umbilical in ˉUm(c) with dim S⊥=2.
(c)The equality case of (1) holds identically for all unit tangent vectors to Uk at each x∈Uk if and only if either Uk is totally geodesic submanifold or Uk is a mixed totally geodesic totally umbilical and S− totally geodesic submanifold with dim U⊥=2.
where k1 and k2 are the dimensions of Uk1T and Uk2⊥ respectively.
The authors are highly thankful to anonymous referees and the handling editor for theirs valuable suggestions and comments which have improved the contents of the paper. This work was supported by Taif University Researchers Supporting Project number (TURSP-2020/223), Taif University, Taif, Saudi Arabia.
The authors declare that they have no any conflict of interest.
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