Abstract

We define GCR-lightlike submanifolds of indefinite cosymplectic manifolds and give an example. Then, we study mixed geodesic GCR-lightlike submanifolds of indefinite cosymplectic manifolds and obtain some characterization theorems for a GCR-lightlike submanifold to be a GCR-lightlike product.

1. Introduction

To fill the gaps in the general theory of submanifolds, Duggal and Bejancu [1] introduced lightlike (degenerate) geometry of submanifolds. Since the geometry of 𝐶𝑅-submanifolds has potential for applications in mathematical physics, particularly in general relativity, and the geometry of lightlike submanifolds has extensive uses in mathematical physics and relativity, Duggal and Bejancu [1] clubbed these two topics and introduced the theory of 𝐶𝑅-lightlike submanifolds of indefinite Kaehler manifolds and then Duggal and Sahin [2], introduced the theory of 𝐶𝑅-lightlike submanifolds of indefinite Sasakian manifolds, which were further studied by Kumar et al. [3]. But 𝐶𝑅-lightlike submanifolds do not include the complex and real subcases contrary to the classical theory of 𝐶𝑅-submanifolds [4]. Thus, later on, Duggal and Sahin [5] introduced a new class of submanifolds, generalized-Cauchy-Riemann- (GCR-) lightlike submanifolds of indefinite Kaehler manifolds and then of indefinite Sasakian manifolds in [6]. This class of submanifolds acts as an umbrella of invariant, screen real, contact 𝐶𝑅-lightlike subcases and real hypersurfaces. Therefore, the study of 𝐺𝐶𝑅-lightlike submanifolds is the topic of main discussion in the present scenario. In [7], the present authors studied totally contact umbilical 𝐺𝐶𝑅-lightlike submanifolds of indefinite Sasakian manifolds.

In present paper, after defining 𝐺𝐶𝑅-lightlike submanifolds of indefinite cosymplectic manifolds, we study mixed geodesic 𝐺𝐶𝑅-lightlike submanifolds of indefinite cosymplectic manifolds. In [8, 9], Kumar et al. obtained some necessary and sufficient conditions for a 𝐺𝐶𝑅-lightlike submanifold of indefinite Kaehler and Sasakian manifolds to be a 𝐺𝐶𝑅-lightlike product, respectively. Thus, in this paper, we obtain some characterization theorems for a 𝐺𝐶𝑅-lightlike submanifold of indefinite cosymplectic manifold to be a 𝐺𝐶𝑅-lightlike product.

2. Lightlike Submanifolds

Let 𝑉 be a real 𝑚-dimensional vector space with a symmetric bilinear mapping 𝑔𝑉×𝑉. The mapping 𝑔 is called degenerate on 𝑉 if there exists a vector 𝜉0 of 𝑉 such that 𝑔(𝜉,𝑣)=0,𝑣𝑉,(2.1) otherwise 𝑔 is called nondegenerate. It is important to note that a non-degenerate symmetric bilinear form on 𝑉 may induce either a non-degenerate or a degenerate symmetric bilinear form on a subspace of 𝑉. Let 𝑊 be a subspace of 𝑉 and 𝑔𝑤   degenerate; then 𝑊 is called a degenerate (lightlike) subspace of 𝑉.

Let (𝑀,𝑔) be a real (𝑚+𝑛)-dimensional semi-Riemannian manifold of constant index 𝑞 such that 𝑚,𝑛1, 1𝑞𝑚+𝑛1, and let (𝑀,𝑔) be an 𝑚-dimensional submanifold of 𝑀 and 𝑔 the induced metric of 𝑔 on 𝑀. Thus, if 𝑔 is degenerate on the tangent bundle 𝑇𝑀 of 𝑀, then 𝑀 is called a lightlike (degenerate) submanifold of 𝑀 (for detail see [1]). For a degenerate metric 𝑔 on 𝑀, 𝑇𝑀 is also a degenerate 𝑛-dimensional subspace of 𝑇𝑥𝑀. Thus, both 𝑇𝑥𝑀 and 𝑇𝑥𝑀 are degenerate orthogonal subspaces but no longer complementary. In this case, there exists a subspace Rad𝑇𝑥𝑀=𝑇𝑥𝑀𝑇𝑥𝑀, which is known as radical (null) subspace. If the mapping Rad𝑇𝑀𝑥𝑀Rad𝑇𝑥𝑀 defines a smooth distribution on 𝑀 of rank 𝑟>0, then the submanifold 𝑀 of 𝑀 is called an 𝑟-lightlike submanifold and Rad𝑇𝑀 is called the radical distribution on 𝑀. Then, there exists a non-degenerate screen distribution 𝑆(𝑇𝑀) which is a complementary vector subbundle to Rad𝑇𝑀 in 𝑇𝑀. Therefore, 𝑇𝑀=Rad𝑇𝑀𝑆(𝑇𝑀),(2.2) where denotes orthogonal direct sum. Let 𝑆(𝑇𝑀), called screen transversal vector bundle, be a non-degenerate complementary vector subbundle to Rad𝑇𝑀 in 𝑇𝑀. Let tr(𝑇𝑀) and ltr(𝑇𝑀) be complementary (but not orthogonal) vector bundles to 𝑇𝑀 in 𝑇𝑀|𝑀 and to Rad𝑇𝑀 in 𝑆(𝑇𝑀), called transversal vector bundle and lightlike transversal vector bundle of 𝑀, respectively. Then, we have tr(𝑇𝑀)=ltr(𝑇𝑀)𝑆𝑇𝑀𝑇,(2.3)𝑀|𝑀=𝑇𝑀tr(𝑇𝑀)=(Rad𝑇𝑀ltr(𝑇𝑀))𝑆(𝑇𝑀)𝑆𝑇𝑀.(2.4)

Let 𝑢 be a local coordinate neighborhood of 𝑀 and consider the local quasiorthonormal fields of frames of 𝑀 along 𝑀 on 𝑢 as {𝜉1,,𝜉𝑟,𝑊𝑟+1,,𝑊𝑛,𝑁1,,𝑁𝑟,𝑋𝑟+1,,𝑋𝑚}, where {𝜉1,,𝜉𝑟}and{𝑁1,,𝑁𝑟} are local lightlike bases of Γ(Rad𝑇𝑀|𝑢) and Γ(ltr(𝑇𝑀)|𝑢) and {𝑊𝑟+1,,𝑊𝑛}and{𝑋𝑟+1,,𝑋𝑚} are local orthonormal bases of Γ(𝑆(𝑇𝑀)|𝑢) and Γ(𝑆(𝑇𝑀)|𝑢), respectively. For these quasiorthonormal fields of frames, we have the following theorem.

Theorem 2.1 (see [1]). Let (𝑀,𝑔,𝑆(𝑇𝑀),𝑆(𝑇𝑀)) be an 𝑟-lightlike submanifold of a semi-Riemannian manifold (𝑀,𝑔). Then there, exist a complementary vector bundle ltr(TM) of Rad TM in 𝑆(𝑇𝑀) and a basis of Γ(ltr(𝑇𝑀)|𝑢) consisting of smooth section {𝑁𝑖} of 𝑆(𝑇𝑀)|𝑢, where 𝑢 is a coordinate neighborhood of 𝑀, such that 𝑔𝑁𝑖,𝜉𝑗=𝛿𝑖𝑗,𝑔𝑁𝑖,𝑁𝑗=0,forany𝑖,𝑗{1,2,,𝑟},(2.5) where {𝜉1,,𝜉𝑟} is a lightlike basis of Γ(Rad(𝑇𝑀)).

Let be the Levi-Civita connection on 𝑀. Then, according to decomposition (2.4), the Gauss and Weingarten formulas are given by 𝑋𝑌=𝑋𝑌+(𝑋,𝑌),𝑋𝑈=𝐴𝑈𝑋+𝑋𝑈,(2.6) for any 𝑋,𝑌Γ(𝑇𝑀) and 𝑈Γ(tr(𝑇𝑀)), where {𝑋𝑌,𝐴𝑈𝑋} and {(𝑋,𝑌),𝑋𝑈} belong to Γ(𝑇𝑀) and Γ(tr(𝑇𝑀)), respectively. Here is a torsion-free linear connection on 𝑀, is a symmetric bilinear form on Γ(𝑇𝑀) that is called second fundamental form, and 𝐴𝑈 is a linear operator on 𝑀, known as shape operator.

According to (2.3), considering the projection morphisms 𝐿 and 𝑆 of tr(𝑇𝑀) on ltr(𝑇𝑀) and 𝑆(𝑇𝑀), respectively, then (2.6) gives 𝑋𝑌=𝑋𝑌+𝑙(𝑋,𝑌)+𝑠(𝑋,𝑌),𝑋𝑈=𝐴𝑈𝑋+𝐷𝑙𝑋𝑈+𝐷𝑠𝑋𝑈,(2.7) where we put 𝑙(𝑋,𝑌)=𝐿((𝑋,𝑌)),𝑠(𝑋,𝑌)=𝑆((𝑋,𝑌)),𝐷𝑙𝑋𝑈=𝐿(𝑋𝑈), 𝐷𝑠𝑋𝑈=𝑆(𝑋𝑈).

As 𝑙 and 𝑠 are Γ(ltr(𝑇𝑀))-valued and Γ(𝑆(𝑇𝑀))-valued, respectively, they are called the lightlike second fundamental form and the screen second fundamental form on 𝑀. In particular, 𝑋𝑁=𝐴𝑁𝑋+𝑙𝑋𝑁+𝐷𝑠(𝑋,𝑁),𝑋𝑊=𝐴𝑊𝑋+𝑠𝑋𝑊+𝐷𝑙(𝑋,𝑊),(2.8) where 𝑋Γ(𝑇𝑀),𝑁Γ(ltr(𝑇𝑀)), and 𝑊Γ(𝑆(𝑇𝑀)). By using (2.3)-(2.4) and (2.7)-(2.8), we obtain 𝑔𝑠+(𝑋,𝑌),𝑊𝑔𝑌,𝐷𝑙𝐴(𝑋,𝑊)=𝑔𝑊,𝑋,𝑌(2.9)𝑔𝑙+(𝑋,𝑌),𝜉𝑔𝑌,𝑙(𝑋,𝜉)+𝑔𝑌,𝑋𝜉=0,(2.10) for any 𝜉Γ(Rad𝑇𝑀), 𝑊Γ(𝑆(𝑇𝑀)), and 𝑁,𝑁Γ(ltr(𝑇𝑀)).

Let 𝑃 be the projection morphism of 𝑇𝑀 on 𝑆(𝑇𝑀). Then, using (2.2), we can induce some new geometric objects on the screen distribution 𝑆(𝑇𝑀) on 𝑀 as 𝑋𝑃𝑌=𝑋𝑃𝑌+(𝑋,𝑌),𝑋𝜉=𝐴𝜉𝑋+𝑋𝑡𝜉,(2.11) for any 𝑋,𝑌Γ(𝑇𝑀) and 𝜉Γ(Rad𝑇𝑀), where {𝑋𝑃𝑌,𝐴𝜉𝑋} and {(𝑋,𝑌),𝑋𝑡𝜉} belong to Γ(𝑆(𝑇𝑀)) and Γ(Rad𝑇𝑀), respectively. and 𝑡 are linear connections on complementary distributions 𝑆(𝑇𝑀) and Rad𝑇𝑀, respectively. Then, using (2.7), (2.8), and (2.11), we have 𝑔𝑙𝐴(𝑋,𝑃𝑌),𝜉=𝑔𝜉,𝑋,𝑃𝑌𝑔𝐴(𝑋,𝑃𝑌),𝑁=𝑔𝑁𝑋,𝑃𝑌.(2.12)

Next, an odd-dimensional semi-Riemannian manifold 𝑀 is said to be an indefinite almost contact metric manifold if there exist structure tensors (𝜙,𝑉,𝜂,𝑔), where 𝜙 is a (1,1) tensor field, 𝑉 is a vector field called structure vector field, 𝜂 is a 1-form, and 𝑔 is the semi-Riemannian metric on 𝑀 satisfying (see [10]) 𝑔(𝜙𝑋,𝜙𝑌)=𝑔(𝑋,𝑌)𝜂(𝑋)𝜂(𝑌),𝜙𝑔(𝑋,𝑉)=𝜂(𝑋),2𝑋=𝑋+𝜂(𝑋)𝑉,𝜂𝜙=0,𝜙𝑉=0,𝜂(𝑉)=1,(2.13) for any 𝑋,𝑌Γ(𝑇𝑀).

An indefinite almost contact metric manifold 𝑀 is called an indefinite cosymplectic manifold if (see [11]) 𝑋𝜙=0,(2.14)𝑋𝑉=0.(2.15)

3. Generalized Cauchy-Riemann Lightlike Submanifolds

Calin [12] proved that if the characteristic vector field 𝑉 is tangent to (𝑀,𝑔,𝑆(𝑇𝑀)), then it belongs to 𝑆(𝑇𝑀). We assume that the characteristic vector 𝑉 is tangent to 𝑀 throughout this paper. Thus, we define the generalized Cauchy-Riemann lightlike submanifolds of an indefinite cosymplectic manifold as follows.

Definition 3.1. Let (𝑀,𝑔,𝑆(𝑇𝑀),𝑆(𝑇𝑀)) be a real lightlike submanifold of an indefinite cosymplectic manifold (𝑀,𝑔) such that the structure vector field 𝑉 is tangent to 𝑀; then 𝑀 is called a generalized-Cauchy-Riemann- (GCR-) lightlike submanifold if the following conditions are satisfied:(A)there exist two subbundles 𝐷1 and 𝐷2 of Rad(𝑇𝑀) such that Rad(𝑇𝑀)=𝐷1𝐷2𝐷,𝜙1=𝐷1𝐷,𝜙2𝑆(𝑇𝑀),(3.1)(B)there exist two subbundles 𝐷0 and 𝐷 of 𝑆(𝑇𝑀) such that 𝑆(𝑇𝑀)=𝜙𝐷2𝐷𝐷0𝑉,𝜙𝐷=𝐿𝑆,(3.2) where 𝐷0 is invariant nondegenerate distribution on 𝑀, {𝑉} is one-dimensional distribution spanned by 𝑉, and 𝐿 and 𝑆 are vector subbundles of ltr(𝑇𝑀) and 𝑆(𝑇𝑀), respectively.

Therefore, the tangent bundle 𝑇𝑀 of 𝑀 is decomposed as 𝑇𝑀=𝐷𝐷{𝑉},𝐷=Rad(𝑇𝑀)𝐷0𝐷𝜙2.(3.3) A contact 𝐺𝐶𝑅-lightlike submanifold is said to be proper if 𝐷0{0},𝐷1{0},𝐷2{0}, and 𝐿{0}. Hence, from the definition of 𝐺𝐶𝑅-lightlike submanifolds, we have that (a)condition (A) implies that dim(Rad𝑇𝑀)3,(b)condition (B) implies that dim(𝐷)2𝑠6 and dim(𝐷2)=dim(𝑆), and thus dim(𝑀)9 and dim(𝑀)13. (c)any proper 9-dimensional contact 𝐺𝐶𝑅-lightlike submanifold is 3-lightlike, (d)(a) and contact distribution (𝜂=0) imply that index (𝑀)4.The following proposition shows that the class of 𝐺𝐶𝑅-lightlike submanifolds is an umbrella of invariant, contact 𝐶𝑅 and contact 𝑆𝐶𝑅-lightlike submanifolds.

Proposition 3.2. A 𝐺𝐶𝑅-lightlike submanifold 𝑀 of an indefinite cosymplectic manifold 𝑀 is contact 𝐶𝑅-submanifold (resp., contact 𝑆𝐶𝑅-lightlike submanifold) if and only if 𝐷1={0} (resp., 𝐷2={0}).

Proof. Let 𝑀 be a contact 𝐶𝑅-lightlike submanifold; then 𝜙Rad𝑇𝑀 is a distribution on 𝑀 such that Rad𝑇𝑀𝜙Rad𝑇𝑀={0}. Therefore, 𝐷2=Rad𝑇𝑀 and 𝐷1={0}. Since ltr(𝑇𝑀)𝜙(ltr(𝑇𝑀))={0}, this implies that 𝜙(ltr(𝑇𝑀))𝑆(𝑇𝑀). Conversely, suppose that 𝑀 is a 𝐺𝐶𝑅-lightlike submanifold of an indefinite Cosymplectic manifold such that 𝐷1={0}. Then, from (3.1), we have 𝐷2=Rad(𝑇𝑀), and therefore Rad𝑇𝑀𝜙Rad𝑇𝑀={0}. Hence, 𝜙Rad𝑇𝑀 is a vector subbundle of 𝑆(𝑇𝑀). This implies that 𝑀 is a contact 𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold. Similarly the other assertion follows.
The following construction helps in understanding the example of 𝐺𝐶𝑅-lightlike submanifold. Let (𝑅𝑞2𝑚+1,𝜙0,𝑉,𝜂,𝑔) be with its usual Cosymplectic structure and given by 𝜂=𝑑𝑧,𝑉=𝜕𝑧,𝑔=𝜂𝜂𝑞/2𝑖=1𝑑𝑥𝑖𝑑𝑥𝑖+𝑑𝑦𝑖𝑑𝑦𝑖+𝑚𝑖=𝑞+1𝑑𝑥𝑖𝑑𝑥𝑖+𝑑𝑦𝑖𝑑𝑦𝑖,𝜙0𝑋1,𝑋2,,𝑋𝑚1,𝑋𝑚,𝑌1,𝑌2,,𝑌𝑚1,𝑌𝑚=,𝑍𝑋2,𝑋1,,𝑋𝑚,𝑋𝑚1,𝑌2,𝑌1,,𝑌𝑚,𝑌𝑚1,,0(3.4) where (𝑥𝑖;𝑦𝑖;𝑧) are the Cartesian coordinates.

Example 3.3. Let 𝑀=(𝑅413,𝑔) be a semi-Euclidean space and 𝑀 a 9-dimensional submanifold of 𝑀 that is given by 𝑥4=𝑥1cos𝜃𝑦1sin𝜃,𝑦4=𝑥1sin𝜃+𝑦1𝑥cos𝜃,2=𝑦3,𝑥5=𝑦1+52,(3.5) where 𝑔 is of signature (,,+,+,+,+,,,+,+,+,+,+) with respect to the canonical basis {𝜕𝑥1,𝜕𝑥2,𝜕𝑥3,𝜕𝑥4,𝜕𝑥5,𝜕𝑥6,𝜕𝑦1,𝜕𝑦2,𝜕𝑦3,𝜕𝑦4,𝜕𝑦5,𝜕𝑦6,𝜕𝑧}. Then, the local frame of 𝑇𝑀 is given by 𝜉1=𝜕𝑥1+cos𝜃𝜕𝑥4+sin𝜃𝜕𝑦4,𝜉2=sin𝜃𝜕𝑥4+𝜕𝑦1+cos𝜃𝜕𝑦4,𝜉3=𝜕𝑥2+𝜕𝑦3,𝑋1=𝜕𝑥3𝜕𝑦2,𝑋2=𝜕𝑥6,𝑋3=𝜕𝑦6,𝑋4=𝑦5𝜕𝑥5+𝑥5𝜕𝑦5,𝑋5=𝜕𝑥3+𝜕𝑦2,𝑋6=𝑉=𝜕𝑧.(3.6) Hence, 𝑀 is a 3-lightlike as Rad𝑇𝑀=span{𝜉1,𝜉2,𝜉3}. Also, 𝜙0𝜉1=𝜉2 and 𝜙0𝜉3=𝑋1; these imply that 𝐷1=span{𝜉1,𝜉2} and 𝐷2=span{𝜉3}, respectively. Since 𝜙0𝑋2=𝑋3,  𝐷0=span{𝑋2,𝑋3}. By straightforward calculations, we obtain 𝑆𝑇𝑀=span𝑊=𝑥5𝜕𝑥5𝑦5𝜕𝑦5,(3.7) where 𝜙0(𝑊)=𝑋4; this implies that 𝑆=𝑆(𝑇𝑀). Moreover, the lightlike transversal bundle ltr(𝑇𝑀) is spanned by 𝑁1=12𝜕𝑥1+cos𝜃𝜕𝑥4+sin𝜃𝜕𝑦4,𝑁2=12sin𝜃𝜕𝑥4𝜕𝑦1+cos𝜃𝜕𝑦4,𝑁3=12𝜕𝑥2+𝜕𝑦3,(3.8) where 𝜙0(𝑁1)=𝑁2 and 𝜙0(𝑁3)=𝑋5. Hence, 𝐿=span{𝑁3}. Therefore, 𝐷=span{𝜙0(𝑁3),𝜙0(𝑊)}. Thus, 𝑀 is a 𝐺𝐶𝑅-lightlike submanifold of 𝑅413.
Let 𝑄, 𝑃1, 𝑃2 be the projection morphism on 𝐷, 𝜙𝑆=𝑀2, 𝜙𝐿=𝑀1, respectively; therefore 𝑋=𝑄𝑋+𝑉+𝑃1𝑋+𝑃2𝑋,(3.9) for 𝑋Γ(𝑇𝑀). Applying 𝜙 to (3.9), we obtain 𝜙𝑋=𝑓𝑋+𝜔𝑃1𝑋+𝜔𝑃2𝑋,(3.10) where 𝑓𝑋Γ(𝐷), 𝜔𝑃1𝑋Γ(𝐿), and 𝜔𝑃2𝑋Γ(𝑆), or, we can write (3.10) as 𝜙𝑋=𝑓𝑋+𝜔𝑋,(3.11) where 𝑓𝑋 and 𝜔𝑋 are the tangential and transversal components of 𝜙𝑋, respectively.
Similarly, 𝜙𝑈=𝐵𝑈+C𝑈,𝑈Γ(tr(𝑇𝑀)),(3.12) where 𝐵𝑈 and 𝐶𝑈 are the sections of 𝑇𝑀 and tr(𝑇𝑀), respectively. Differentiating (3.10) and using (2.8)–(2.10) and (3.12), we have 𝐷𝑠𝑋,𝜔𝑃2𝑌=𝑠𝑋𝜔𝑃1𝑌+𝜔𝑃1𝑋𝑌𝑠(𝑋,𝑓𝑌)+𝐶𝑠𝐷(𝑋,𝑌),𝑙𝑋,𝜔𝑃1𝑌=𝑙𝑋𝜔𝑃2𝑌+𝜔𝑃2𝑋𝑌𝑙(𝑋,𝑓𝑌)+𝐶𝑙(𝑋,𝑌),(3.13) for all 𝑋,𝑌Γ(𝑇𝑀). By using, cosymplectic property of with (2.7), we have the following lemmas.

Lemma 3.4. Let 𝑀 be a 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀; then one has 𝑋𝑓𝑌=𝐴𝜔𝑌𝑋+𝐵(𝑋,𝑌),𝑡𝑋𝜔𝑌=𝐶(𝑋,𝑌)(𝑋,𝑓𝑌),(3.14) where 𝑋,𝑌Γ(𝑇𝑀) and 𝑋𝑓𝑌=𝑋𝑓𝑌𝑓𝑋𝑌,𝑡𝑋𝜔𝑌=𝑡𝑋𝜔𝑌𝜔𝑋𝑌.(3.15)

Lemma 3.5. Let 𝑀 be a 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀; then one has 𝑋𝐵𝑈=𝐴𝐶𝑈𝑋𝑓𝐴𝑈𝑋,𝑡𝑋𝐶U=𝜔𝐴𝑈𝑋(𝑋,𝐵𝑈),(3.16) where 𝑋Γ(𝑇𝑀) and 𝑈Γ(tr(𝑇𝑀)) and 𝑋𝐵𝑈=𝑋𝐵𝑈𝐵𝑡𝑋𝑈,𝑡𝑋𝐶𝑈=𝑡𝑋𝐶𝑈𝐶𝑡𝑋𝑈.(3.17)

4. Mixed Geodesic GCR-Lightlike Submanifolds

Definition 4.1. A 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold is called mixed geodesic 𝐺𝐶𝑅-lightlike submanifold if its second fundamental form satisfies (𝑋,𝑌)=0, for any 𝑋Γ(𝐷𝑉) and 𝑌Γ(𝐷).

Definition 4.2. A 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold is called 𝐷 geodesic 𝐺𝐶𝑅-lightlike submanifold if its second fundamental form satisfies (𝑋,𝑌)=0, for any 𝑋,𝑌Γ(𝐷).

Theorem 4.3. Let 𝑀 be a 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. Then, 𝑀 is mixed geodesic if and only if 𝐴𝜉𝑋 and 𝐴𝑊𝑋Γ(𝑀2𝜙𝐷2), for any 𝑋Γ(𝐷𝑉),𝑊Γ(𝑆(𝑇𝑀)) and 𝜉Γ(Rad(𝑇𝑀)).

Proof. Using, definition of 𝐺𝐶𝑅-lightlike submanifolds, 𝑀 is mixed geodesic if and only if 𝑔((𝑋,𝑌),𝑊)=𝑔((𝑋,𝑌),𝜉)=0, for 𝑋Γ(𝐷𝑉),𝑌Γ(𝐷),𝑊Γ(𝑆(𝑇𝑀)), and 𝜉Γ(Rad(𝑇𝑀)). Using (2.8) and (2.11), we get 𝑔((𝑋,𝑌),𝑊)=𝑔𝑋𝑌,𝑊=𝑔𝑌,𝑋𝑊=𝑔𝑌,𝐴𝑊𝑋,𝑔((𝑋,𝑌),𝜉)=𝑔𝑋𝑌,𝜉=𝑔𝑌,𝑋𝜉=𝑔𝑌,𝐴𝜉𝑋.(4.1) Therefore, from (4.1), the proof is complete.

Theorem 4.4. Let 𝑀 be a 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. Then, 𝑀 is 𝐷 geodesic if and only if 𝐴𝜉𝑋 and 𝐴𝑊𝑋Γ(𝑀2𝜙𝐷2), for any 𝑋Γ(𝐷),𝜉ΓRad(𝑇𝑀), and 𝑊Γ(𝑆(𝑇𝑀)).

Proof. The proof is similar to the proof of Theorem 4.3.

Lemma 4.5. Let 𝑀 be a mixed geodesic 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. Then 𝐴𝜉𝑋Γ(𝜙𝐷2), for any 𝑋Γ(𝐷), 𝜉Γ(𝐷2).

Proof. For 𝑋Γ(𝐷) and 𝜉Γ(𝐷2), using (2.7) we have (𝜙𝜉,𝑋)=𝑋𝜙𝜉𝑋𝜙𝜉=𝜙𝑋𝜉+𝜙(𝑋,𝜉)𝑋𝜙𝜉.(4.2) Since 𝑀 is mixed geodesic, we obtain 𝜙𝑋𝜉=𝑋𝜙𝜉. Here, using (2.11), we get 𝜙(𝐴𝜉𝑋+𝑋𝑡𝜉)=𝑋𝜙𝜉+(𝑋,𝜙𝜉), and then, by virtue of (3.11), we obtain 𝑓𝐴𝜉𝑋𝜔𝐴𝜉𝑋+𝜙(𝑋𝑡𝜉)=𝑋𝜙𝜉+(𝑋,𝜙𝜉). Comparing the transversal components, we get 𝜔𝐴𝜉𝑋=0; this implies that 𝐴𝜉𝐷𝑋Γ0𝐷{𝑉}𝜙2.(4.3) If 𝐴𝜉𝑋𝐷0, then the nondegeneracy of 𝐷0 implies that there must exist a 𝑍0𝐷0 such that 𝑔(𝐴𝜉𝑋,𝑍0)0. But using the hypothesis that 𝑀 is a mixed geodesic with (2.7) and (2.11), we get 𝑔𝐴𝜉𝑋,𝑍0=𝑔𝑋𝜉,𝑍0=𝑔𝜉,𝑋𝑍0=𝑔𝜉,𝑋𝑍0+𝑋,𝑍0=0.(4.4) Therefore, 𝐴𝜉𝐷𝑋Γ0.(4.5) Also using (2.13), and (2.15), we get 𝑔𝐴𝜉𝑋,𝑉=𝑔𝑋=𝜉,𝑉𝑔𝜉,𝑋𝑉=0.(4.6) Therefore, 𝐴𝜉𝑋{𝑉}.(4.7) Hence, from (4.3), (4.5), and (4.7), the result follows.

Corollary 4.6. Let 𝑀 be a mixed geodesic 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. Then, 𝑔(𝑙(𝑋,𝑌),𝜉)=0, for any 𝑋Γ(𝐷),𝑌Γ(𝑀2) and 𝜉Γ(𝐷2).

Proof. The result follows from (2.12) and Lemma 4.5.

Theorem 4.7. Let 𝑀 be a mixed geodesic 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. Then, 𝐴𝑈𝑋Γ(𝐷{𝑉}) and 𝑡𝑋𝑈Γ(𝐿𝑆), for any 𝑋Γ(𝐷{𝑉}) and 𝑈Γ(𝐿𝑆).

Proof. Since 𝑀 is mixed geodesic 𝐺𝐶𝑅-lightlike submanifold (𝑋,𝑌)=0 for any 𝑋Γ(𝐷{𝑉}),𝑌Γ(𝐷), and thus (2.6) implies that 0=𝑋𝑌𝑋𝑌.(4.8) Since 𝐷 is an anti-invariant distribution there exists a vector field 𝑈Γ(𝐿𝑆) such that 𝜙𝑈=𝑌. Thus, from (2.8), (2.14), (3.11), and (3.12), we get 0=𝑋𝜙𝑈𝑋𝑌=𝜙𝐴𝑈𝑋+𝑡𝑋𝑈𝑋𝑌=𝑓𝐴𝑈𝑋𝜔𝐴𝑈𝑋+𝐵𝑡𝑋𝑈+𝐶𝑡𝑋𝑈𝑋𝑌.(4.9) Comparing the transversal components, we get 𝜔𝐴𝑈𝑋=𝐶𝑡𝑋𝑈. Since 𝜔𝐴𝑈𝑋Γ(𝐿𝑆) and 𝐶𝑡𝑋𝑈Γ(𝐿𝑆), this implies that 𝜔𝐴𝑈𝑋=0 and 𝐶𝑡𝑋𝑈=0. Hence, 𝐴𝑈𝑋Γ(𝐷{𝑉}) and 𝑡𝑋𝑈Γ(𝐿𝑆).

5. GCR-Lightlike Product

Definition 5.1. 𝐺𝐶𝑅-lightlike submanifold 𝑀 of an indefinite cosymplectic manifold 𝑀 is called 𝐺𝐶𝑅-lightlike product if both the distributions 𝐷{𝑉} and 𝐷 define totally geodesic foliation in 𝑀.

Theorem 5.2. Let 𝑀 be a 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. Then, the distribution 𝐷{𝑉} define a totally geodesic foliation in 𝑀 if and only if 𝐵(𝑋,𝜙𝑌)=0, for any 𝑋,𝑌𝐷{𝑉}.

Proof. Since 𝐷=𝜙(𝐿𝑆), 𝐷{𝑉} defines a totally geodesic foliation in 𝑀 if and only if 𝑔(𝑋𝑌,𝜙𝜉)=𝑔(𝑋𝑌,𝜙𝑊)=0, for any 𝑋,𝑌Γ(𝐷{𝑉}), 𝜉Γ(𝐷2), and 𝑊Γ(𝑆). Using (2.7) and (2.14), we have 𝑔𝑋𝑌,𝜙𝜉=𝑔𝑋𝜙𝑌,𝜉=𝑔𝑙𝑔(𝑋,𝑓𝑌),𝜉,(5.1)𝑋𝑌,𝜙𝑊=𝑔𝑋𝜙𝑌,𝑊=𝑔𝑠(𝑋,𝑓𝑌),𝑊.(5.2) Hence, from (5.1) and (5.2), the assertion follows.

Theorem 5.3. Let 𝑀 be a 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. Then, the distribution 𝐷 defines a totally geodesic foliation in 𝑀 if and only if 𝐴𝑁𝑋 has no component in 𝜙𝑆𝜙𝐷2 and 𝐴𝜔𝑌𝑋 has no component in 𝐷2𝐷0, for any 𝑋,𝑌Γ(𝐷) and 𝑁Γ(ltr(𝑇𝑀)).

Proof. From the definition of a 𝐺𝐶𝑅-lightlike submanifold, we know that 𝐷 defines a totally geodesic foliation in 𝑀 if and only if 𝑔𝑋𝑌,𝑁=𝑔𝑋𝑌,𝜙𝑁1=𝑔𝑋𝑌,𝑉=𝑔𝑋𝑌,𝜙𝑍=0,(5.3) for 𝑋,𝑌Γ(𝐷),𝑁Γ(ltr(𝑇𝑀)),𝑍Γ(𝐷0) and 𝑁1Γ(𝐿). Using (2.7) and (2.8), we have 𝑔𝑋=𝑌,𝑁𝑔𝑋𝑌,𝑁=𝑔𝑌,𝑋𝑁=𝑔𝑌,𝐴𝑁𝑋.(5.4) Using (2.7), (2.15), and (2.14), we obtain 𝑔𝑋𝑌,𝜙𝑁1𝜙=𝑔𝑋𝑌,𝑁1=𝑔𝑋𝜔𝑌,𝑁1𝐴=𝑔𝜔𝑌𝑋,𝑁1𝑔,(5.5)𝑋𝜙𝑌,𝜙𝑍=𝑔𝑋𝑌,𝑍=𝑔𝑋𝐴𝜔𝑌,𝑍=𝑔𝜔𝑌𝑔𝑋,𝑍,(5.6)𝑋𝑌,𝑉=𝑔𝑋𝑌,𝑉=𝑔𝑌,𝑋𝑉=0.(5.7) Thus, from (5.4)–(5.7), the result follows.

Theorem 5.4. Let 𝑀 be a 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. If (𝑋𝑓)𝑌=0, then 𝑀 is a 𝐺𝐶𝑅 lightlike product.

Proof. Let 𝑋,𝑌Γ(𝐷); therefore 𝑓𝑌=0. Then using (3.15) with the hypothesis, we get 𝑓𝑋𝑌=0. Therefore the distribution 𝐷 defines a totally geodesic foliation. Next, let 𝑋,𝑌𝐷{𝑉}; therefore 𝜔𝑌=0. Then using (3.14), we get 𝐵(𝑋,𝑌)=0. Therefore, 𝐷{𝑉} defines a totally geodesic foliation in 𝑀. Hence, 𝑀 is a 𝐺𝐶𝑅 lightlike product.

Definition 5.5. A lightlike submanifold 𝑀 of a semi-Riemannian manifold is said to be an irrotational submanifold if 𝑋𝜉Γ(𝑇𝑀), for any 𝑋Γ(𝑇𝑀) and 𝜉ΓRad(𝑇𝑀). Thus, 𝑀 is an irrotational lightlike submanifold if and only if 𝑙(𝑋,𝜉)=0 and 𝑠(𝑋,𝜉)=0.

Theorem 5.6. Let 𝑀 be an irrotational 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. Then, 𝑀 is a 𝐺𝐶𝑅 lightlike product if the following conditions are satisfied:(A)𝑋𝑈Γ(𝑆(𝑇𝑀)),forall𝑋Γ(𝑇𝑀),and𝑈Γ(tr(𝑇𝑀)), (B)𝐴𝜉𝑌Γ(𝜙(𝑆)),forall𝑌Γ(𝐷).

Proof. Let (𝐴) hold; then, using (2.8), we get 𝐴𝑁𝑋=0,𝐴𝑊𝑋=0, 𝐷𝑙(𝑋,𝑊)=0, and 𝑙𝑋𝑁=0 for 𝑋Γ(𝑇𝑀). These equations imply that the distribution 𝐷 defines a totally geodesic foliation in 𝑀, and, with (2.9), we get 𝑔(𝑠(𝑋,𝑌),𝑊)=0. Hence, the non degeneracy of 𝑆(𝑇𝑀) implies that 𝑠(𝑋,𝑌)=0. Therefore, 𝑠(𝑋,𝑌) has no component in 𝑆. Finally, from (2.10) and the hypothesis that 𝑀 is irrotational, we have 𝑔(𝑙(𝑋,𝑌),𝜉)=𝑔(𝑌,𝐴𝜉𝑋), for 𝑋Γ(𝑇𝑀) and 𝑌Γ(𝐷). Assume that (𝐵) holds; then 𝑙(𝑋,𝑌)=0. Therefore, 𝑙(𝑋,𝑌) has no component in 𝐿. Thus, the distribution 𝐷{𝑉} defines a totally geodesic foliation in 𝑀. Hence, 𝑀 is a 𝐺𝐶𝑅 lightlike product.

Definition 5.7 (see [13]). If the second fundamental form of a submanifold, tangent to characteristic vector field 𝑉, of a Sasakian manifold 𝑀 is of the form (𝑋,𝑌)={𝑔(𝑋,𝑌)𝜂(𝑋)𝜂(𝑌)}𝛼+𝜂(𝑋)(𝑌,𝑉)+𝜂(𝑌)(𝑋,𝑉),(5.8) for any 𝑋,𝑌Γ(𝑇𝑀), where 𝛼 is a vector field transversal to 𝑀, then 𝑀 is called a totally contact umbilical submanifold of a Sasakian manifold.

Theorem 5.8. Let 𝑀 be a totally contact umbilical 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. Then, 𝑀 is a 𝐺𝐶𝑅-lightlike product if 𝐵(𝑋,𝑌)=0, for any 𝑋,𝑌Γ(𝑇𝑀).

Proof. Let 𝑋,𝑌Γ(𝐷{𝑉}); then the hypothesis that 𝐵(𝑋,𝑌)=0 implies that the distribution 𝐷{𝑉} defines a totally geodesic foliation in 𝑀.
If we assume that 𝑋,𝑌Γ(𝐷), then, using (3.14), we have 𝑓𝑋𝑌=𝐴𝜔𝑌𝑋+𝐵(𝑋,𝑌), and taking inner product with 𝑍Γ(𝐷0) and using (2.6) and (2.14), we obtain 𝑔𝑓𝑋𝐴𝑌,𝑍=𝑔𝜔𝑌𝑋+𝐵(𝑋,𝑌),𝑍=𝑔𝑋𝑌,𝜙𝑍=𝑔𝑌,𝑋𝑍,(5.9) where 𝜙𝑍=𝑍Γ(𝐷0). For any 𝑋Γ(𝐷) from (3.14), we have 𝜔𝑃𝑋𝑍=(𝑋,𝑓𝑍)𝐶(𝑋,𝑍). Therefore, using the hypothesis with (5.8), we get 𝜔𝑃𝑋𝑍=0; this implies that 𝑋𝑍Γ(𝐷), and thus (5.9) becomes 𝑔(𝑓𝑋𝑌,𝑍)=0. Then, the nondegeneracy of the distribution 𝐷0 implies that the distribution 𝐷 defines a totally geodesic foliation in 𝑀. Hence, the assertion follows.

Theorem 5.9. Let 𝑀 be a totally geodesic 𝐺𝐶𝑅-lightlike submanifold of an indefinite cosymplectic manifold 𝑀. Suppose that there exists a transversal vector bundle of 𝑀 which is parallel along 𝐷 with respect to Levi-Civita connection on 𝑀, that is, 𝑋𝑈Γ(tr(𝑇𝑀)), for any 𝑈Γ(tr(𝑇𝑀)), 𝑋Γ(𝐷). Then, 𝑀 is a 𝐺𝐶𝑅-lightlike product.

Proof. Since 𝑀 is a totally geodesic 𝐺𝐶𝑅-lightlike 𝐵(𝑋,𝑌)=0, for 𝑋,𝑌Γ(𝐷{𝑉}); this implies 𝐷{𝑉} defines a totally geodesic foliation in 𝑀.
Next 𝑋𝑈Γ(tr(𝑇𝑀)) implies 𝐴𝑈𝑋=0, and hence, by Theorem 5.3, the distribution 𝐷 defines a totally geodesic foliation in 𝑀. Hence, the result follows.

Acknowledgment

The authors would like to thank the anonymous referee for his/her comments that helped them to improve this paper.