• 検索結果がありません。

RICCI CURVATURE OF SUBMANIFOLDS IN KENMOTSU SPACE FORMS

N/A
N/A
Protected

Academic year: 2022

シェア "RICCI CURVATURE OF SUBMANIFOLDS IN KENMOTSU SPACE FORMS"

Copied!
9
0
0

読み込み中.... (全文を見る)

全文

(1)

http://ijmms.hindawi.com

© Hindawi Publishing Corp.

RICCI CURVATURE OF SUBMANIFOLDS IN KENMOTSU SPACE FORMS

KADRI ARSLAN, RIDVAN EZENTAS, ION MIHAI, CENGIZHAN MURATHAN, and CIHAN ÖZGÜR Received 20 April 2001 and in revised form 21 August 2001

In 1999, Chen established a sharp relationship between the Ricci curvature and the squared mean curvature for a submanifold in a Riemannian space form with arbitrary codimension.

Similar problems for submanifolds in complex space forms were studied by Matsumoto et al. In this paper, we obtain sharp relationships between the Ricci curvature and the squared mean curvature for submanifolds in Kenmotsu space forms.

2000 Mathematics Subject Classification: 53C25, 53C40.

1. Preliminaries. Let(M, <, >)˜ be a Hermitian manifold and denote byJthe canon- ical almost complex structure on ˜M. According to the behavior of the tangent bundle T Mwith respect to the action ofJ, we may distinguish two special classes of subman- ifoldsMin ˜M:

(a) complex submanifolds, that is,J(TpM)=TpM, for allp∈M.

(b) totally real submanifolds, that is,J(TpM)⊂TpM, for all p∈M, whereTpM (resp.,TpM) is the tangent (resp., the normal) vector space ofMatp. Such submani- folds were defined and studied by Chen and Ogiue [4].

On the other hand, Yano and Ishihara [8] considered a submanifoldMwhose tan- gent bundleT M splits into a complex subbundleᏰand a totally real subbundleᏰ. Later, such a submanifold was called a CR-submanifold [1, 2]. Blair and Chen [1]

proved that aCR-submanifold of a locally conformal Kaehler manifold is a Cauchy- Riemann manifold in the sense of Greenfield.

The first main result on CR-submanifolds was obtained by Chen [2]: any CR- submanifold of a Kaehler manifold is foliated by totally real submanifolds (i.e., the totally real subbundle is involutive).

As nontrivial examples ofCR-submanifolds, we can mention the (real) hypersur- faces of Hermitian manifolds.

2. Kenmotsu manifolds and their submanifolds. Tanno [7] has classified, into three classes, the connected almost contact Riemannian manifolds whose automor- phisms groups have the maximum dimensions:

(1) homogeneous normal contact Riemannian manifolds with constant φ- holomorphic sectional curvature;

(2) global Riemannian products of a line or circle and a Kaehlerian space form;

(3) warped product spacesfF, whereLis a line andF a Kaehlerian manifold.

(2)

Kenmotsu [5] studied the third class and characterized it by tensor equations. Later, such a manifold was called a Kenmotsu manifold.

A(2m+1)-dimensional Riemannian manifold(M, g)˜ is said to be a Kenmotsu man- ifold if it admits an endomorphismφof its tangent bundleTM, a vector field˜ ξ, and a 1-formη, which satisfy:

φ2= −Id+η⊗ξ, η(ξ)=1, φξ=0, η◦φ=0, g(φX, φY )=g(X, Y )−η(X)η(Y ), η(X)=g(X, ξ),

Xφ

Y= −g(X, φY )ξ−η(Y )φX,

Xξ=X−η(X),

(2.1)

for any vector fieldsX, Y on ˜M, where ˜∇denotes the Riemannian connection with respect tog.

We denote byωthe fundamental 2-form of ˜M, that is, ω(X, Y )=g(φX, Y ), for allX, Y Γ(TM). It was proved that the pairing˜ (ω, η)defines a locally conformal cosymplectic structure, that is,

dω=∧η, dη=0. (2.2)

A Kenmotsu manifold with constantφ-holomorphic sectional curvaturecis called a Kenmotsu space form and it is denoted by ˜M(c). Then its curvature tensor ˜R is expressed by (cf. [5])

4 ˜R(X, Y )Z=(c−3)

g(Y , Z)X−g(X, Z)Y +(c+1)

η(X)Y−η(Y )X

η(Z)+

g(X, Z)η(Y )−g(Y , Z)η(X) ξ +ω(Y , Z)φX−ω(X, Z)φY−2ω(X, Y )φZ

.

(2.3)

Let ˜Mbe a Kenmotsu manifold andMann-dimensional submanifold tangent toξ.

For any vector fieldXtangent toM, we put

φX=P X+F X, (2.4)

whereP X(resp.,F X) denotes the tangential (resp., normal) component ofφX. ThenP is an endomorphism of tangent bundleT MandF is a normal bundle valued 1-form onT M.

The equation of Gauss is given by R(X, Y , Z, W )˜ =R(X, Y , Z, W )+g

h(X, W ), h(Y , Z) −g

h(X, Z), h(Y , W ) , (2.5) for any vectorsX,Y,Z,W tangent toM.

We denote byHthe mean curvature vector, that is, H(p)= 1

n n i=1

h

ei, ei , (2.6)

where{e1, . . . , en}is an orthonormal basis of the tangent spaceTpM,p∈M.

(3)

Also, we set

hrij=g h

ei, ej , er ,

h2= n i,j=1

g h

ei, ej , h ei, ej

. (2.7)

Let{e1, . . . , en}be an orthonormal basis ofTpM. We put P2=

n i,j=1

g2

P ei, ej . (2.8)

By analogy with submanifolds in a Kaehler manifold, different classes of submani- folds in a Kenmotsu manifold were considered (cf. [6]).

A submanifoldMtangent toξis said to be invariant (resp., anti-invariant) ifφ(TpM)

⊂TpM, for allp∈M(resp.,φ(TpM)⊂TpM, for allp∈M).

A submanifoldMtangent toξis called a contactCR-submanifold [9] if there exists a pair of orthogonal differentiable distributionsᏰandᏰonM, such that,

(i) T M=⊕{ξ}, where{ξ}is the 1-dimensional distribution spanned byξ;

(ii) Ᏸis invariant byφ, that is,φ(p)⊂p, for allp∈M;

(iii) Ᏸis anti-invariant byφ, that is,φ(p)⊂TpM, for allp∈M.

In particular, ifᏰ= {0}(resp., Ᏸ= {0}),M is an invariant (resp., anti-invariant) submanifold.

Next, recall some notions introduced by Chen (see [3]).

LetLbe ak-plane section ofTpMandXa unit vector inL. We choose an orthonormal basis{e1, . . . , ek}ofLsuch thate1=X.

Define the Ricci curvature RicLofLatXby

RicL(X)=K12+K13+···+K1k, (2.9) whereKijdenotes the sectional curvature of the 2-plane section spanned byei,ej. We simply called such a curvature ak-Ricci curvature.

The scalar curvatureτ of thek-plane sectionLis given by τ(L)=

1i<jk

Kij. (2.10)

For each integerk, 2≤k≤n, the Riemannian invariantΘk on ann-dimensional Riemannian manifoldMis defined by

Θk(p)= 1 k−1inf

L,XRicL(X), p∈M, (2.11)

whereLruns over allk-plane sections inTpMandXruns over all unit vectors inL.

Recall that for a submanifoldMin a Riemannian manifold, the relative null space ofMat a pointp∈Mis defined by

p=

X∈TpM|h(X, Y )=0, Y∈TpM

. (2.12)

(4)

3. Ricci curvature and squared mean curvature. Chen established a sharp rela- tionship between the Ricci curvature and the squared mean curvature for submani- folds in real space forms (see [3]).

We prove similar inequalities for certain submanifolds of a Kenmotsu space form M(c). We will consider submanifolds˜ Mtangent to the Reeb vector fieldξ.

Theorem3.1. LetM(c)˜ be a(2m+1)-dimensional Kenmotsu space form andMan n-dimensional submanifold tangent toξ. Then

(i) for each unit vectorX∈TpMorthogonal toξ, Ric(X)1

4

(n−1)(c3)+1 2

3P X22 (c+1)+n2H2

; (3.1)

(ii) ifH(p)=0, then a unit tangent vectorX∈TpM orthogonal toξsatisfies the equality case of (3.1) if and only ifX∈p;

(iii) the equality case of (3.1) holds identically for all unit tangent vectors orthogonal toξatpif and only ifpis a totally geodesic point.

Proof. LetX∈TpMbe a unit tangent vectorXatp. We choose an orthonormal basise1, . . . , en=ξ,en+1, . . . , e2m+1inTpM(c)˜ such thate1, . . . , enare tangent toMatp, withe1=X.

Then, from the equation of Gauss, we have n2H2=+h2−n(n−1)c−3

4

3P22n+2 c+1

4 . (3.2)

From (3.2), we get n2H2=+

2m+1 r=n+1

hr11 2+

hr22+···+hrnn 2+2

i<j

hrij2

2

2m+1

r=n+1

2≤i<j≤n

hriihrjj−n(n−1)c−3 4

3P22n+2 c+1 4

=+1 2

2m+1 r=n+1

hr11+···+hrnn 2+

hr11−hr22−···−hrnn 2 +2

2m+1 r=n+1

i<j

hrij2

2

2m+1 r=n+1

2i<jn

hriihrjj

−n(n−1)c−3 4

3P22n+2 c+1 4 .

(3.3)

From the equation of Gauss, we find

2i<jn

Kij=

2m+1

r=n+1

2i<jn

hriihrjj hrij2 +(n−1)(n2)

2

c−3 4 +

3P23P e122n+4 c+1 8 .

(3.4)

(5)

Substituting (3.4) in (3.3), we get 1

2n2H2=2 Ric(X)+1 2

2m+1

r=n+1

hr11−hr22−···−hrnn 2

+

2m+1 r=n+1

n j=1

hr1j2

2(n1)c−3 4

3P X22 c+1 4

2 Ric(X)2(n1)c−3 4

3P X22 c+1 4 ,

(3.5)

which is equivalent to (3.1).

For (ii) assume thatH(p)=0. Equality holds in (3.1) if and only if

hr12= ··· =hr1n=0, hr11=hr22+···+hrnn=0, r∈ {n+1, . . . ,2m}. (3.6) Thenhr1j=0, for allj∈ {1, . . . , n},r∈ {n+1, . . . ,2m}, that is,X∈p.

For (iii) the equality case of (3.1) holds for all unit tangent vectors atpif and only if

hrij=0, ij, r∈ {n+1, . . . ,2m},

hr11+hr22+···+hrnn2hrii=0, i∈ {1, . . . , n}, r∈ {n+1, . . . ,2m}. (3.7) It follows thatpis a totally geodesic point.

The converse is trivial.

Corollary3.2. LetMbe ann-dimensional invariant submanifold tangent toξin a Kenmotsu space formM(c). Then,˜

(i) for each unit vectorX∈TpMorthogonal toξ, we have Ric(X)1

4

(n−1)(c3)+1 2(c+1)

; (3.8)

(ii) a unit tangent vectorX∈TpMorthogonal toξsatisfies the equality case of (3.8) if and only ifX∈p;

(iii) the equality case of (3.8) holds identically for all unit tangent vectors orthogonal toξatpif and only ifpis a totally geodesic point.

Proof. It is known that every invariant submanifold of a Kenmotsu space form is minimal (cf. [6]).

On the other hand, for any unit tangent vectorX∈TpM orthogonal toξ, we have P X = φX = X =1.

Then, the inequality (3.1) implies (3.8).

Similarly, we can prove the following results.

Corollary3.3. LetMbe ann-dimensional anti-invariant submanifold tangent toξ in a Kenmotsu space formM(c). Then,˜

(i) for each unit vectorX∈TpMorthogonal toξ, we have Ric(X)1

4

(n−1)(c3)−(c+1)+n2H2

; (3.9)

(6)

(ii) ifH(p)=0, then a unit tangent vectorX∈TpM orthogonal toξsatisfies the equality case of (3.9) if and only ifX∈p;

(iii) the equality case of (3.9) holds identically for all unit tangent vectors orthogonal toξatpif and only ifpis a totally geodesic point.

Corollary3.4. LetMbe ann-dimensional contactCR-submanifold of a Kenmotsu space formM(c). Then˜

(i) for each unit vectorX∈p, Ric(X)1

4

(n−1)(c−3)+1

2(c+1)+n2H2

; (3.10)

(ii) for each unit vectorX∈p, we have Ric(X)1

4

(n−1)(c3)−(c+1)+n2H2

. (3.11)

4. k-Ricci curvature. In this section, we prove a relationship between thek-Ricci curvature and the squared mean curvature for submanifolds tangent toξin a Ken- motsu space form.

Theorem4.1. LetM(c)˜ be a Kenmotsu space form andM ann-dimensional sub- manifold tangent toξ. Then we have

H2

n(n−1)−c−3 4

3P X22(n1) n(n−1)

c+1

4 . (4.1)

Proof. We choose an orthonormal basis{e1, . . . , en, en+1, . . . , e2m+1=ξ}atpsuch thaten+1is parallel to the mean curvature vectorH(p), ande1, . . . , endiagonalize the shape operatorAn+1. Then the shape operators take the forms

An+1=







a1 0 0 ··· 0 0 a2 0 ··· 0 ... ... ... ··· ... 0 0 0 ··· an







Ar= hrij

, i, j=1, . . . , n;r=n+2, . . . ,2m, traceAr= n i=1

hrii=0.

(4.2)

From (3.2), we get

n2H2=+ n i=1

a2i+

2m

r=n+2

n i,j=1

hrij2

−n(n−1)c−3 4

3P X22(n1) c+1 4 .

(4.3)

On the other hand, since 0

i<j

ai−aj

2=(n−1)

i

a2i2

i<j

aiaj, (4.4)

(7)

we obtain

n2H2=

n

i=1

ai

2

= n i=1

a2i+2

i<j

aiaj≤n n i=1

a2i, (4.5) which implies that

n i=1

a2i≥nH2. (4.6)

We have from (4.3)

n2H2+nH2−n(n−1)c+3 4

3P X22(n1) c+1

4 , (4.7) which is equivalent to (4.1).

UsingTheorem 4.1, we obtain the following.

Theorem4.2. LetM(c)˜ be a Kenmotsu space form andM ann-dimensional sub- manifold tangent toξ. Then, for any integerk,2≤k≤n, and any pointp∈M, we have

H2(p)≥Θk(p)−c−3 4

3P22n+2 (c+1)

4n(n−1) . (4.8)

Proof. Let{e1, . . . , en}be an orthonormal basis ofTpM. Denote byLi1···ik thek- plane section spanned byei1, . . . , eik. It follows from (2.9) and (2.10) that

τ

Li1···ik =1 2

i∈{i1,...,ik}

RicLi 1···ik

ei ,

τ(p)= 1 Cn−2k−2

1≤i1<···<ik≤n

τ Li1···ik .

(4.9)

Combining (2.11) and (4.9), we find

τ(p)≥n(n−1)

2 Θk(p). (4.10)

From (4.1) and (4.10), we obtain (4.8).

In particular, we obtain the following.

Corollary4.3. LetMbe ann-dimensional invariant submanifold tangent toξin a Kenmotsu space formM(c). Then, for any integer˜ k,2≤k≤n, and any pointp∈M,

Θk(p)≤c−3 4 +c+1

4n . (4.11)

Corollary 4.4. LetM be an n-dimensional anti-invariant submanifold tangent toξin a Kenmotsu space formM(c). Then, for any integer˜ k,2≤k≤n, and any point p∈M,

H2(p)≥Θk(p)−c−3 4 +c+1

2n . (4.12)

(8)

Corollary4.5. LetMbe ann-dimensional contactCR-submanifold of a Kenmotsu space formM(c). Then, for any integer˜ k,2≤k≤n, and any pointp∈M,

H2(p)≥Θk(p)−c−3

4 −(3h−n+1)(c+1)

2n(n1) , (4.13)

where2h=dimᏰ.

Acknowledgments. The authors are very indebted to the referee for valuable suggestions. This paper is prepared during the third named author’s visit to the Uludag University, Bursa, Turkey in July 2000. The third author is supported by the Scientific and Technical Research Council of Turkey (TÜBITAK) for NATO-PC Advanced Fellowships Programme.

References

[1] D. E. Blair and B.-Y. Chen,On CR-submanifolds of Hermitian manifolds, Israel J. Math.34 (1979), no. 4, 353–363.

[2] B.-Y. Chen,CR-submanifolds of a Kaehler manifold. I, J. Differential Geom.16(1981), no. 2, 305–322.

[3] ,Relations between Ricci curvature and shape operator for submanifolds with arbi- trary codimensions, Glasgow Math. J.41(1999), no. 1, 33–41.

[4] B.-Y. Chen and K. Ogiue,On totally real submanifolds, Trans. Amer. Math. Soc.193(1974), 257–266.

[5] K. Kenmotsu,A class of almost contact Riemannian manifolds, Tôhoku Math. J. (2)24 (1972), 93–103.

[6] K. Matsumoto, I. Mihai, and R. Ro¸sca,A certain locally conformal almost cosymplectic man- ifold and its submanifolds, Tensor (N.S.)51(1992), no. 1, 91–102.

[7] S. Tanno, The automorphism groups of almost contact Riemannian manifolds, Tôhoku Math. J. (2)21(1969), 21–38.

[8] K. Yano and S. Ishihara,Thef-structure induced on submanifolds of complex and almost complex spaces, K¯odai Math. Sem. Rep.18(1966), 120–160.

[9] K. Yano and M. Kon,Structures on Manifolds, Series in Pure Mathematics, vol. 3, World Scientific Publishing, Singapore, 1984.

Kadri Arslan: Department of Mathematics, Faculty of Arts and Sciences, Uludag University, Görükle16059, Bursa, Turkey

E-mail address:[email protected]

Ridvan Ezentas, Cengizhan Murathan, and Cihan Özgür: Department of Mathemat- ics, Faculty of Arts and Sciences, Uludag University, Görükle16059, Bursa, Turkey

Ion Mihai: Faculty of Mathematics, University of Bucharest, Str. Academiei14, 70109Bucharest, Romania

E-mail address:[email protected]

(9)

Special Issue on

Time-Dependent Billiards

Call for Papers

This subject has been extensively studied in the past years for one-, two-, and three-dimensional space. Additionally, such dynamical systems can exhibit a very important and still unexplained phenomenon, called as the Fermi acceleration phenomenon. Basically, the phenomenon of Fermi accelera- tion (FA) is a process in which a classical particle can acquire unbounded energy from collisions with a heavy moving wall.

This phenomenon was originally proposed by Enrico Fermi in 1949 as a possible explanation of the origin of the large energies of the cosmic particles. His original model was then modified and considered under different approaches and using many versions. Moreover, applications of FA have been of a large broad interest in many different fields of science including plasma physics, astrophysics, atomic physics, optics, and time-dependent billiard problems and they are useful for controlling chaos in Engineering and dynamical systems exhibiting chaos (both conservative and dissipative chaos).

We intend to publish in this special issue papers reporting research on time-dependent billiards. The topic includes both conservative and dissipative dynamics. Papers dis- cussing dynamical properties, statistical and mathematical results, stability investigation of the phase space structure, the phenomenon of Fermi acceleration, conditions for having suppression of Fermi acceleration, and computational and numerical methods for exploring these structures and applications are welcome.

To be acceptable for publication in the special issue of Mathematical Problems in Engineering, papers must make significant, original, and correct contributions to one or more of the topics above mentioned. Mathematical papers regarding the topics above are also welcome.

Authors should follow the Mathematical Problems in Engineering manuscript format described at

http://www .hindawi.com/journals/mpe/. Prospective authors should

submit an electronic copy of their complete manuscript through the journal Manuscript Tracking System at

http://

mts.hindawi.com/

according to the following timetable:

Manuscript Due December 1, 2008 First Round of Reviews March 1, 2009 Publication Date June 1, 2009

Guest Editors

Edson Denis Leonel,

Departamento de Estatística, Matemática Aplicada e Computação, Instituto de Geociências e Ciências Exatas, Universidade Estadual Paulista, Avenida 24A, 1515 Bela Vista, 13506-700 Rio Claro, SP, Brazil ; [email protected]

Alexander Loskutov,

Physics Faculty, Moscow State University, Vorob’evy Gory, Moscow 119992, Russia;

[email protected]

Hindawi Publishing Corporation http://www.hindawi.com

参照

関連したドキュメント

Papaghiuc [18] introduced a class of submanifolds in an almost Hermitian manifold, called the semi-slant submanifolds which include proper CR-submanifolds and proper slant

In the present paper, we establish an inequality between the warping func- tion f (intrinsic structure) and the squared mean curvature kH k 2 and the holomorphic sectional curvature

In section 5, first we establish a basic inequality involving sectional curvatures and the squared mean curvature for subman- ifolds of a Riemannian manifold, then by applying