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June 2016

RADICAL TRANSVERSAL SCREEN SEMI-SLANT LIGHTLIKE SUBMANIFOLDS OF INDEFINITE KAEHLER MANIFOLDS

S. S. Shukla and Akhilesh Yadav

Abstract. In this paper, we introduce the notion of radical transversal screen semi-slant lightlike submanifolds of indefinite Kaehler manifolds giving characterization theorem with some non-trivial examples of such submanifolds. Integrability conditions of distributionsD1,D2 and RadT Mon radical transversal screen semi-slant lightlike submanifolds of indefinite Kaehler man- ifolds have been obtained. Further, we obtain necessary and sufficient conditions for foliations determined by above distributions to be totally geodesic.

1. Introduction

The theory of lightlike submanifolds of a semi-Riemannian manifold was intro- duced by Duggal and Bejancu [2]. A submanifoldM of a semi-Riemannian manifold M is said to be lightlike submanifold if the induced metricgonM is degenerate, i.e., there exists a non-zeroX∈Γ(T M) such that g(X, Y) = 0, ∀Y Γ(T M). Various classes of lightlike submanifolds of indefinite Kaehler manifolds have been defined according to the behaviour of distributions on these submanifolds with respect to the action of (1,1) tensor field J in Kaehler structure of the ambient manifolds.

Such submanifolds have been studied in [3, 7].

The geometry of slant submanifolds of Kaehler manifolds was studied by B.

Y. Chen in [1] and the geometry of semi-slant submanifolds of Kaehler manifolds was studied by N. Papaghuic in [5]. In [6], Sahin studied screen-slant lightlike submanifolds of an indefinite Hermitian manifold. The theory of radical transver- sal, transversal, semi-transversal lightlike submanifolds has been studied in [8]. In [9–11], the authors studied lightlike submanifolds, radical transversal lightlike sub- manifolds and radical transversal screen semi-slant lightlike submanifolds. In this paper, we introduce the notion of radical transversal screen semi-slant lightlike submanifolds of indefinite Kaehler manifolds. This new class of lightlike submani- folds of an indefinite Kaehler manifold includes radical transversal and transversal lightlike submanifolds as its sub-cases.

2010 Mathematics Subject Classification: 53C15, 53C40, 53C50

Keywords and phrases: Semi-Riemannian manifold; degenerate metric; radical distribution;

screen distribution; screen transversal vector bundle; lightlike transversal vector bundle; Gauss and Weingarten formulae.

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The paper is arranged as follows. There are some basic results in Section 2. In Section 3, we introduce radical transversal screen semi-slant lightlike submanifolds of an indefinite Kaehler manifold, giving some examples. Section 4 is devoted to the study of foliations determined by distributions on radical transversal screen semi-slant lightlike submanifolds of indefinite Kaehler manifolds.

2. Preliminaries

A submanifold (Mm, g) immersed in a semi-Riemannian manifold (Mm+n, g) is called a lightlike submanifold [2] if the metric g induced from g is degenerate and the radical distribution RadT M is of rank r, where 1≤r ≤m. Let S(T M) be a screen distribution which is a semi-Riemannian complementary distribution ofRadT M in TM, that is

T M =RadT M⊕orthS(T M).

Now consider a screen transversal vector bundle S(T M), which is a semi- Riemannian complementary vector bundle ofRadT M inT M. Since for any local basisi} of RadT M, there exists a local null frame{Ni}of sections with values in the orthogonal complement of S(T M) in [S(T M)] such thatg(ξi, Nj) =δij

and g(Ni, Nj) = 0, it follows that there exists a lightlike transversal vector bun- dle ltr(T M) locally spanned by {Ni}. Let tr(T M) be complementary (but not orthogonal) vector bundle toT M inT M|M. Then

tr(T M) =ltr(T M)orthS(T M), T M|M =T M⊕tr(T M),

T M|M =S(T M)orth[RadT M⊕ltr(T M)]orthS(T M).

Following are four cases of a lightlike submanifold¡

M, g, S(T M), S(T M)¢ : Case 1. r-lightlike ifr <min (m, n),

Case 2. co-isotropic ifr=n < m,S¡ T M¢

={0}, Case 3. isotropic ifr=m < n, S(T M) ={0},

Case 4. totally lightlike ifr=m=n,S(T M) =S(T M) ={0}.

The Gauss and Weingarten formulae are given as

XY =XY +h(X, Y), (2.1)

XV =−AVX+tXV, (2.2)

for all X, Y Γ(T M) andV Γ(tr(T M)), where XY, AVX belong to Γ(T M) and h(X, Y),tXV belong to Γ(tr(T M)). and tare linear connections on M and on the vector bundle tr(T M) respectively. The second fundamental form h is a symmetric F(M)-bilinear form on Γ(T M) with values in Γ(tr(T M)) and the shape operatorAV is a linear endomorphism of Γ(T M). From (2.1) and (2.2), for

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anyX, Y Γ(T M),N Γ(ltr(T M)) andW Γ(S(T M)), we have

XY =XY +hl(X, Y) +hs(X, Y), (2.3)

XN =−ANX+lXN+Ds(X, N), (2.4)

XW =−AWX+sXW+Dl(X, W), (2.5) where hl(X, Y) = L(h(X, Y)), hs(X, Y) = S(h(X, Y)), Dl(X, W) = L(∇tXW), Ds(X, N) = S(∇tXN). L and S are the projection morphisms of tr(T M) on ltr(T M) andS(T M) respectively. landsare linear connections onltr(T M) and S(T M) called the lightlike connection and screen transversal connection on M respectively.

Now by using (2.1), (2.3)–(2.5) and metric connection∇, we obtain g(hs(X, Y), W) +g(Y, Dl(X, W)) =g(AWX, Y),

g(Ds(X, N), W) =g(N, AWX).

Denote the projection of T M on S(T M) by P. Then from the decomposition of the tangent bundle of a lightlike submanifold, for any X, Y Γ(T M) and ξ Γ(RadT M), we have

XP Y =XP Y +h(X, P Y),

Xξ=−AξX+∗tXξ, By using the above equations, we obtain

g(hl(X, P Y), ξ) =g(AξX, P Y), g(h(X, P Y), N) =g(ANX, P Y),

g(hl(X, ξ), ξ) = 0, Aξξ= 0.

It is important to note that in general is not a metric connection. Since is metric connection, by using (2.3), we get

(∇Xg)(Y, Z) =g(hl(X, Y), Z) +g(hl(X, Z), Y).

An indefinite almost Hermitian manifold (M , g, J) is a 2m-dimensional semi- Riemannian manifold M with semi-Riemannian metric g of constant index q, 0 < q < 2m and a (1, 1) tensor field J on M such that following conditions are satisfied:

J2X=−X,

g(JX, JY) =g(X, Y), (2.6) for allX, Y Γ(T M).

An indefinite almost Hermitian manifold (M , g, J) is called an indefinite Kaehler manifold ifJ is parallel with respect to∇, i.e.,

(∇XJ)Y = 0, (2.7)

for allX, Y Γ(T M), where is Levi-Civita connection with respect tog.

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3. Radical transversal screen semi-slant lightlike submanifolds In this section, we introduce the notion of radical transversal screen semi- slant lightlike submanifolds of indefinite Kaehler manifolds. At first, we state the following lemma for later use:

Lemma 3.1. Let M be a 2q-lightlike submanifold of an indefinite Kaehler manifold M, of index 2q such that 2q < dim(M). Then the screen distribution S(T M)on lightlike submanifold M is Riemannian.

The proof of above Lemma follows as in Lemma 3.1 of [6], so we omit it.

Definition 3.1. LetM be a 2q-lightlike submanifold of an indefinite Kaehler manifoldM of index 2qsuch that 2q < dim(M). Then we say thatM is a radical transversal screen semi-slant lightlike submanifold ofM if the following conditions are satisfied:

(i) J(RadT M) =ltr(T M),

(ii) there exist non-degenerate orthogonal distributionsD1andD2onM such that S(T M) =D1orthD2,

(iii) the distributionD1 is an invariant, i.e. JD1=D1,

(iv) the distributionD2 is slant with angle θ(6= 0), i.e. for eachx∈M and each non-zero vectorX (D2)x, the angle θbetweenJX and the vector subspace (D2)xis a non-zero constant, which is independent of the choice ofx∈M and X (D2)x.

This constant angle θ is called the slant angle of distributionD2. A radical transversal screen semi-slant lightlike submanifold is said to be proper ifD16={0}, D26={0}andθ6= π2.

From the above definition, we have the following decomposition T M =RadT M⊕orthD1orthD2.

Let (R2m2q , g, J) denote the manifoldR2m2q with its usual Kaehler structure given by g= 14(−Pq

i=1dxi⊗dxi+dyi⊗dyi+Pm

i=q+1dxi⊗dxi+dyi⊗dyi), J(Pm

i=1(Xi∂xi+Yi∂yi)) =Pm

i=1(Yi∂xi−Xi∂yi),

where (xi, yi) are the cartesian coordinates onR2m2q . Now we construct some exam- ples of radical transversal screen semi-slant lightlike submanifolds of an indefinite Kaehler manifold.

Example 1. Let (R122 , g, J) be an indefinite Kaehler manifold, where g is of signature (−,+,+,+,+,+,−,+,+,+,+,+) with respect to the canonical basis {∂x1, ∂x2, ∂x3, ∂x4, ∂x5, ∂x6, ∂y1, ∂y2, ∂y3, ∂y4, ∂y5, ∂y6}.

SupposeM is a submanifold of R122 given byx1=−y2=u1,x2=−y1=u2, x3 = u3cosβ, y3 = −u4cosβ, x4 =u4sinβ, y4 = u3sinβ, x5 = u5sinu6, y5 = u5cosu6,x6= sinu5,y6= cosu5.

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The local frame ofT M is given by{Z1, Z2, Z3, Z4, Z5, Z6}, where Z1= 2(∂x1−∂y2),Z2= 2(∂x2−∂y1),

Z3= 2(cosβ∂x3+ sinβ∂y4),Z4= 2(sinβ∂x4cosβ∂y3), Z5= 2(sinu6∂x5+ cosu6∂y5+ cosu5∂x6sinu5∂y6), Z6= 2(u5cosu6∂x5−u5sinu6∂y5).

HenceRadT M =span{Z1, Z2} andS(T M) =span{Z3, Z4, Z5, Z6}.

Nowltr(T M) is spanned byN1=−∂x1−∂y2,N2=−∂x2−∂y1andS(T M) is spanned by

W1= 2(sinβ∂x3cosβ∂y4),W2= 2(cosβ∂x4+ sinβ∂y3), W3= 2(sinu6∂x5+ cosu6∂y5cosu5∂x6+ sinu5∂y6), W4= 2(u5sinu5∂x6+u5cosu5∂y6).

It follows that JZ1 = 2N2 and JZ2 = 2N1, which implies that JRadT M = ltr(T M). On the other hand, we can see that D1 = span{Z3, Z4} such that JZ3 =Z4 and JZ4 =−Z3, which implies that D1 is invariant with respect to J andD2=span{Z5, Z6}is a slant distribution with slant angleπ/4. HenceM is a radical transversal screen semi-slant 2-lightlike submanifold ofR122 .

Example 2. Let (R122 , g, J) be an indefinite Kaehler manifold, where g is of signature (−,+,+,+,+,+,−,+,+,+,+,+) with respect to the canonical basis {∂x1, ∂x2, ∂x3, ∂x4, ∂x5, ∂x6, ∂y1, ∂y2, ∂y3, ∂y4, ∂y5, ∂y6}.

Suppose M is a submanifold of R122 given by x1 = u1, y1 = −u2, x2 = u1cosα−u2sinα, y2 = u1sinα+u2cosα, x3 = y4 = u3, x4 = −y3 = u4, x5=u5cosθ,y5=u6cosθ,x6=u6sinθ, y6=u5sinθ.

The local frame ofT M is given by{Z1, Z2, Z3, Z4, Z5, Z6}, where Z1= 2(∂x1+ cosα∂x2+ sinα∂y2),Z2= 2(−∂y1sinα∂x2+ cosα∂y2), Z3= 2(∂x3+∂y4),Z4= 2(∂x4−∂y3),

Z5= 2(cosθ∂x5+ sinθ∂y6),Z6= 2(sinθ∂x6+ cosθ∂y5).

HenceRadT M =span{Z1, Z2} andS(T M) =span{Z3, Z4, Z5, Z6}.

Now ltr(T M) is spanned by N1 =−∂x1+ cosα∂x2+ sinα∂y2, N2 =∂y1 sinα∂x2+ cosα∂y2 andS(T M) is spanned by

W1= 2(∂x3−∂y4),W2= 2(∂x4+∂y3),

W3= 2(sinθ∂x5cosθ∂y6),W4= 2(cosθ∂x6sinθ∂y5).

It follows thatJZ1=−2N2,JZ2= 2N1, which implies thatJRadT M=ltr(T M).

On the other hand, we can see thatD1=span{Z3, Z4}such thatJZ3=Z4,JZ4=

−Z3, which implies thatD1is invariant with respect toJ andD2=span{Z5, Z6} is a slant distribution with slant angle 2θ. HenceM is a radical transversal screen semi-slant 2-lightlike submanifold ofR122 .

Now, for any vector fieldX tangent toM, we putJX=P X+F X, whereP X and F X are tangential and transversal parts of JX respectively. We denote the

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projections on RadT M, D1 and D2 in T M by P1, P2 and P3 respectively. Then for anyX Γ(T M), we get

X =P1X+P2X+P3X. (3.1)

Now applyingJ to (3.1), we have

JX=JP1X+JP2X+JP3X, which gives

JX =JP1X+JP2X+f P3X+F P3X, (3.2) where f P3X (resp.F P3X) denotes the tangential (resp. transversal) component of JP3X. Thus we get JP1X Γ(ltr(T M)), JP2X Γ(D1), f P3X Γ(D2) and F P3X Γ(S(T M)).

Similarly, we denote the projections oftr(T M) on ltr(T M) andS(T M) by Q1and Q2 respectively. Then for anyW Γ(tr(T M)), we have

W =Q1W+Q2W. (3.3)

ApplyingJ to (3.3), we obtain

JW =JQ1W +JQ2W, which gives

JW =JQ1W+BQ2W+CQ2W, (3.4)

whereBQ2W (resp. CQ2W) denotes the tangential (resp. transversal) component of JQ2W. Thus we get JQ1W Γ(RadT M), BQ2W Γ(D2) and CQ2W Γ(S(T M)).

Now, by using (2.7), (3.2), (3.4) and (2.3)–(2.5) and identifying the components onRadT M,D1,D2,ltr(T M) andS(T M), we obtain

P1(∇XJP2Y) +P1(∇Xf P3Y) =P1(AJP

1YX) +P1(AF P3YX) +Jhl(X, Y), P2(∇XJP2Y) +P2(∇Xf P3Y) =P2(AF P3YX) +P2(AJP

1YX) +JP2XY, (3.5) P3(∇XJP2Y) +P3(∇Xf P3Y)

=P3(AF P3YX) +P3(AJP1YX) +f P3XY +Bhs(X, Y), (3.6)

lXJP1Y +hl(X, JP2Y) +hl(X, f P3Y) =JP1XY −Dl(X, F P3Y), (3.7) Ds(X, JP1Y) +hs(X, JP2Y) +hs(X, f P3Y)

=Chs(X, Y)− ∇sXF P3Y +F P3XY. (3.8) Theorem 3.2. Let M be a 2q-lightlike submanifold of an indefinite Kaehler manifoldM. ThenM is a radical transversal screen semi-slant lightlike submanifold if and only if

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(i) Jltr(T M)is a distribution onM such thatJltr(T M) =RadT M, (ii) distributionD1 is invariant with respect toJ, i.e. JD1=D1, (iii) there exists a constant λ∈[0,1)such that P2X =−λX.

Moreover, there also exists a constant µ∈ (0,1] such that BF X =−µX, for all X Γ(D2), whereD1 andD2 are non-degenerate orthogonal distributions on M such that S(T M) =D1orthD2 andλ= cos2θ,θ is slant angle of D2.

Proof. LetM be a radical transversal screen semi-slant lightlike submanifold of an indefinite Kaehler manifoldM. Then distributionD1is invariant with respect to J andJRadT M =ltr(T M). ThusJX∈ltr(T M), for allX Γ(RadT M). Hence J(JX)∈J(ltr(T M)), which implies−X ∈J(ltr(T M)), for allX Γ(RadT M), which proves (i) and (ii).

Now for anyX Γ(D2), we have|P X|=|JX|cosθ, which implies cosθ= |P X|

|JX|. (3.9)

In view of (3.9), we get cos2θ=|P X||JX|22 = g(P X,P X)g(JX,JX) =g(X,P2X)

g(X,J2X), which gives g(X, P2X) = cos2θ g(X, J2X). (3.10) Since M is radical transversal screen semi-slant lightlike submanifold, cos2θ = λ(constant)∈[0,1) and therefore from (3.14), we getg(X, P2X) =λg(X, J2X) = g(X, λJ2X), which implies

g(X,(P2−λJ2)X) = 0.

Now for anyX Γ(D2), we haveJ2(X) =P2X+F P X+BF X+CF X. Taking the tangential component, we get P2X = −X −BF X Γ(D2), for any X Γ(D2). Thus (P2−λJ2)X Γ(D2). Since the induced metric g = g|D2×D2 is non-degenerate(positive definite), by the facts above, we have (P2−λJ2)X = 0, which implies

P2X =λJ2X=−λX. (3.11)

Now, for any vector fieldX∈Γ(D2), we have

JX=P X+F X, (3.12)

whereP X andF X are tangential and transversal parts ofJX respectively.

ApplyingJ to (3.12) and taking tangential component, we get

−X =P2X+BF X. (3.13)

From (3.11) and (3.13), we getBF X =−µX, where 1−λ=µ(constant)∈(0,1].

This proves (iii).

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Conversely suppose that conditions (i), (ii) and (iii) are satisfied. From (i), we have JN ∈RadT M, for all N Γ(ltr(T M)). HenceJ(JN)∈J(RadT M), which implies−N J(RadT M), for all N Γ(ltr(T M)). ThusJRadT M =ltr(T M).

From (3.18), for anyX Γ(D2), we get−X =P2X−µX, which impliesP2X =

−λX, where 1−µ=λ(constant)∈[0,1).

Now cosθ= g(JX,P X)|JX||P X| =g(X,JP X)|JX||P X| =g(X,P|JX||P X|2X) =−λg(X,J|JX||P X|2X) =λg(JX,JX)|JX||P X|. From the above equation, we get

cosθ=λ|JX|

|P X|. (3.14)

Therefore (3.9) and (3.14) give cos2θ=λ(constant).

HenceM is a radical transversal screen semi-slant lightlike submanifold.

Corollary 3.1. Let M be a radical transversal screen semi-slant lightlike submanifold of an indefinite Kaehler manifold M with slant angleθ, then for any X, Y Γ(D2), we have

(i) g(P X, P Y) = cos2θ g(X, Y), (ii) g(F X, F Y) = sin2θ g(X, Y).

The proof of above Corollary follows by using similar steps as in proof of Corollary 3.2 of [6].

Theorem 3.3. Let M be a radical transversal screen semi-slant lightlike sub- manifold of an indefinite Kaehler manifoldM with structure vector field tangent to M. Then RadT M is integrable if and only if

(i) P2(AJP

1YX) =P2(AJP

1XY)andP3(AJP

1YX) =P3(AJP

1XY), (ii) Ds(Y, JP1X) =Ds(X, JP1Y), for allX, Y Γ(RadT M).

Proof. Let M be a radical transversal screen semi-slant lightlike submani- fold of an indefinite Kaehler manifold M. Let X, Y Γ(RadT M). From (3.8), we have Ds(X, JP1Y) = Chs(X, Y) +F P3XY, which gives Ds(X, JP1Y) Ds(Y, JP1X) =F P3[X, Y]. In view of (3.5), we haveP2(AJP1YX)+JP2XY = 0, which implies P2(AJP

1XY)−P2(AJP

1YX) = JP2[X, Y]. Also from (3.6), we have P3(AJP

1YX) + Bhs(X, Y) +f P3XY = 0, which gives P3(AJP

1XY) P3(AJP

1YX) =f P3[X, Y]. This concludes the theorem.

Theorem 3.4. Let M be a radical transversal screen semi-slant lightlike sub- manifold of an indefinite Kaehler manifold M. Then D1 is integrable if and only if

(i) hl(Y, JP2X) =hl(X, JP2Y)andhs(Y, JP2X) =hs(X, JP2Y), (ii) P3(∇XJP2Y) =P3(∇YJP2X), for allX, Y Γ(D1).

Proof. Let M be a radical transversal screen semi-slant lightlike subman- ifold of an indefinite Kaehler manifold M. Let X, Y Γ(D1). From (3.8),

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we have hs(X, JP2Y) = Chs(X, Y) +F P3XY, which implies hs(X, JP2Y) hs(Y, JP2X) = F P3[X, Y]. In view of (3.7), we have hl(X, JP2Y) = JP1XY, which gives hl(X, JP2Y)−hl(Y, JP2X) = JP1[X, Y]. From (3.6), we obtain P3(∇XJP2Y) = f P3XY + Bhs(X, Y), which implies P3(∇XJP2Y) P3(∇YJP2X) =f P3[X, Y]. This proves the theorem.

Theorem 3.5. Let M be a radical transversal screen semi-slant lightlike sub- manifold of an indefinite Kaehler manifold M. Then D2 is integrable if and only if

(i) hl(X, f P3Y) +Dl(X, F P3Y) =hl(Y, f P3X) +Dl(Y, F P3X), (ii) P2(∇Xf P3Y − ∇Yf P3X) =P2(AF P3YX−AF P3XY), for allX, Y Γ(D2).

Proof. Let M be a radical transversal screen semi-slant lightlike subman- ifold of an indefinite Kaehler manifold M. Let X, Y Γ(D2). From (3.7), we have hl(X, f P3Y) +Dl(X, F P3Y) = JP1XY, which gives hl(X, f P3Y) + Dl(X, F P3Y)−hl(Y, f P3X)−Dl(Y, F P3X) = JP1[X, Y]. Also from (35), we obtain P2(∇Xf P3Y) = P2(AF P3YX) +JP2XY, which implies P2(∇Xf P3Y

Yf P3X) =P2(AF P3YX−AF P3XY) +JP2[X, Y]. Thus, we obtain the required results.

Theorem 3.6. Let M be a radical transversal screen semi-slant lightlike sub- manifold of an indefinite Kaehler manifold M. Then the induced connection∇ is a metric connection if and only if

(i) BDs(X, N) =f P3ANX,

(ii) JP2ANX = 0, for all X∈Γ(T M) andN∈Γ(ltr(T M)).

Proof. LetM be a radical transversal screen semi-slant lightlike submanifold of an indefinite Kaehler manifoldM. Then the induced connectiononM is a metric connection if and only ifRadT Mis parallel distribution with respect to[2]. From (2.3), (2.4) and (2.7), we obtain XJN +hl(X, JN) +hs(X, JN) =−JANX + J∇lXN+JDs(X, N). Now, on comparing tangential components of both sides of above equation, we getXJN=−JP2ANX−f P3ANX+J∇lXN+BDs(X, N), which completes the proof.

4. Foliations determined by distributions

In this section, we obtain necessary and sufficient conditions for foliations determined by distributions on a radical transversal screen semi-slant lightlike sub- manifold of an indefinite Kaehler manifold to be totally geodesic.

Definition 4.1. An equivalence relation on ann-dimensional semi-Rieman- nian manifold (M , g) in which the equivalence classes are connected, immersed submanifolds (called the leaves of the foliation) of a common dimensionk, 0< k≤n is called a foliation on M. If each leaf of a foliation F on a semi-Riemannian

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manifold (M , g) is totally geodesic submanifold of M, we say that F is a totally geodesic foliation.

Theorem 4.1. Let M be a radical transversal screen semi-slant lightlike sub- manifold of an indefinite Kaehler manifold M. Then RadT M defines a totally geodesic foliation if and only ifg(AF P3ZX, JY) =g(∇XJP2Z+Xf P3Z, JY), for allX, Y Γ(RadT M)andZ Γ(S(T M)).

Proof. Let M be a radical transversal screen semi-slant lightlike subman- ifold of an indefinite Kaehler manifold M. To prove RadT M defines a total- ly geodesic foliation, it is sufficient to show that XY Γ(RadT M), for all X, Y Γ(RadT M). Since is metric connection, using (2.3), (2.6), (2.7) and (3.2), for any X, Y Γ(RadT M) and Z Γ(S(T M)), we obtain g(∇XY, Z) =

−g(∇X(JP2Z+f P3Z+F P3Z), JY), which impliesg(∇XY, Z) =g(P1AF P3ZX− P1XJP2Z−P1Xf P3Z, JY). This proves the theorem.

Theorem 4.2. Let M be a radical transversal screen semi-slant lightlike sub- manifold of an indefinite Kaehler manifoldM. Then D1 defines a totally geodesic foliation if and only if

(i) g(AF ZX, JY) =g(∇Xf Z, JY), for allX, Y Γ(D1)andZ Γ(D2), (ii) AJN vanishes onD1, for all N∈Γ(ltr(T M)).

Proof. LetM be a radical transversal screen semi-slant lightlike submanifold of an indefinite Kaehler manifoldM. The distribution D1 defines a totally geodesic foliation if and only if XY Γ(D1), for all X, Y Γ(D1). Since is metric connection, from (2.3), (2.6) and (2.7), for any X, Y Γ(D1) and Z Γ(D2), we obtain g(∇XY, Z) =−g(∇XJZ, JY), which implies g(∇XY, Z) = g(AF ZX

Xf Z, JY). Also, from (2.3), (2.6) and (2.7), for any X, Y Γ(D1) and N Γ(ltr(T M)), we have g(∇XY, N) = −g(JY,∇XJN), which gives g(∇XY, N) =

−g(JY,∇XJN) =g(JY, AJNX). This concludes the theorem.

Theorem 4.3. Let M be a radical transversal screen semi-slant lightlike sub- manifold of an indefinite Kaehler manifoldM. Then D2 defines a totally geodesic foliation if and only if

(i) g(f Y,∇XJZ) =−g(F Y, hs(X, JZ)), (ii) g(f Y,∇XJN) =−g(F Y, hs(X, JN)),

for allX, Y Γ(D2),Z∈Γ(D1)andN Γ(ltr(T M)).

Proof. LetM be a radical transversal screen semi-slant lightlike submanifold of an indefinite Kaehler manifoldM. The distribution D2 defines a totally geodesic foliation if and only if XY Γ(D2), for all X, Y Γ(D2). Since is metric connection, using (2.3), (2.6) and (2.7), for any X, Y Γ(D2) andZ Γ(D1), we get g(∇XY, Z) = −g(JY,∇XJZ), which implies g(∇XY, Z) = −g(f Y,∇XJZ)− g(F Y, hs(X, JZ)). Now, from (2.3), (2.6) and (2.7), for anyX, Y Γ(D2) andN∈

(11)

Γ(ltr(T M)), we have g(∇XY, N) = −g(JY,∇XJN), which gives g(∇XY, N) =

−g(f Y,∇XJN)−g(F Y, hs(X, JN)). Thus, we obtain the required results.

Acknowledgement: Akhilesh Yadav gratefully acknowledges the financial support provided by the Council of Scientific and Industrial Research (C.S.I.R.), India.

REFERENCES

[1] B.Y. Chen,Geometry of Slant Submanifolds, Katholieke Universiteit, Leuven, 1990.

[2] K.L. Duggal and A. Bejancu,Lightlike Submanifolds of Semi-Riemannian Manifolds and Applications, Vol. 364 of Mathematics and its applications, Kluwer Academic Publishers, Dordrecht, The Netherlands, 1996.

[3] K.L. Duggal and B. Sahin,Differential Geomety of Lightlike Submanifolds, Birkh¨auser Verlag AG, Basel, Boston, Berlin, 2010.

[4] B. O’Neill,Semi-Riemannian Geometry with Applications to Relativity, Academic Press New York, 1983.

[5] N. Papaghiuc, Semi-slant submanifolds of a Kaehlerian manifold, An. Stiint. Al.I.Cuza.

Univ. Iasi,40, (1994), 55–61.

[6] B. Sahin, B.,Screen slant lightlike submanifolds, Int. Electronic J. Geometry,2(2009), 41–54.

[7] B. Sahin,Slant lightlike submanifolds of indefinite Hermitian manifolds, Balkan J. Geometry Appl.,13(1) (2008), 107–119.

[8] B. Sahin,Transversal lightlike submanifolds of indefinite Kaehler manifolds, Analele. Univ.

Timisoara,44(1), (2006), 119–145.

[9] S.S. Shukla and A. Yadav,Lightlike submanifolds of indefinite para-Sasakian manifolds, Mat.

Vesnik,66(4) (2014), 371–386.

[10] S.S. Shukla and A. Yadav, Radical transversal lightlike submanifolds of indefinite para- Sasakian manifolds, Demonstratio Math.,47(4) (2014), 994–1011.

[11] S.S. Shukla and A. Yadav,Radical transversal screen semi-slant lightlike submanifolds of indefinite Sasakian manifolds, Lobachevskii J. Math.36(2) (2015), 160–168.

(received 13.05.2015; in revised form 17.01.2016; available online 03.02.2016) Department of Mathematics, University of Allahabad, Allahabad-211002, India E-mail:ssshukla [email protected], akhilesh [email protected]

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