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Acta Universitatis Apulensis ISSN: 1582-5329 No. 30/2012 pp. 143-150 ON COMPLETE SPACELIKE HYPERSURFACES IN ANTI-DE SITTER SPACE H

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ON COMPLETE SPACELIKE HYPERSURFACES IN ANTI-DE SITTER SPACE H1N+1(−1)

Yingbo Han and Shuxiang Feng

Abstract. In this paper, we investigate complete spacelike hypersurfaces with constant mean curvature in anti-de Sitter spaceH1n+1(−1). Some rigidity theorems are obtained for these hypersurfaces.

2000Mathematics Subject Classification: 53C42, 53B30.

1. Introduction

Let M1n+1(c) denote an (n+ 1)-dimensional Lorentzian manifold of constant curvature c, which is called a Lorentzian space form.Then an (n+ 1)-dimensional Lorentzian space form M1n+1(c) is said to be a de Sitter space S1n+1(c), a Lorentzian Minkowski space Ln+1 or an anti-de Sitter spaceH1n+1(c) respectively, according to its sectional curvature c > 0, c = 0 or c < 0. A hypersuface M in a Lorentizian space formM1n+1(c) is said to be spacelike if the induced metric onM from that of M1n+1(c) is positive definite.

In recent years, the study of spacelike hypersurfaces in semi-Riemannian ambi- ents has got increasing interesting motivated by their importance in problems related to Physics, more specifically in the theory of general relativity.

E.Calabi [1] first studied the Bernstein problem for maximal spacelike entire graphs in Rn+11 ,n ≤4, and proved that it must be hyperplane. Later S.Y. Cheng and S.T. Yau [2] showed that this conclusion remains true for arbitrary n. In [4] T.

Ishihara proved that complete maximal spacelike hypersurfaces of M1n+1(c), c≥0, are totally geodesic. Further, in the same paper, T. Ishihara also proved the following result:

Theorem 1.1.[4]. Let Mn be an n-dimensional complete maximal spacelike hypersurface in anti-de Sitter space H1n+1(−1), then the norm square of the second fundamental form of M satisfiesS ≤nand S =nif and only if Mn =Hm(−mn)× Hn−m(−n−mn ), (1≤m≤n−1).

In [3], L.F. Cao and G.X. Wei gave a new characterization of hyperbolic cylinder Mn=Hm(−mn)×Hn−m(−n−mn ) in anti-de Sitter spaceH1n+1(−1).

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Theorem 1.2.[3]. Let Mn be an n-dimensional (n ≥ 3) complete maximal spacelike hyperusrface with two distinct principal curvatureλandµin anti-de Sitter spaceH1n+1(−1). If inf|λ−µ|>0, then Mn=Hm(−mn)×Hn−m(−n−mn ), (1≤m≤ n−1).

In [5], C.X.Nie studied complete spacelike hypersurfaces with constant mean curvature in anti-de Sitter space H1n+1(−1) and gave the following result:

Theorem 1.3.[5]. Let Mn be an n-dimensional (n ≥ 3) complete spacelike hyperusrface with constant mean curvature and two distinct principal curvature λ and µin anti-de Sitter spaceH1n+1(−1). If inf|λ−µ|>0, then Mn=Hm(−a12)× Hn−m(−1−a1 2), (1≤m≤n−1).

In this note, we also investigate complete spacelike hypersurfaces with constant mean curvature inH1n+1(−1). More precisely, we prove the following results:

Theorem 1.4. Let Mn (n ≥ 3) be a complete spacelike hypersurface with constant mean curvature H in H1n+1(−1). Assume that Mn has n−1 principal curvatures with the same sign everywhere. If the Ricci curvature RicM of Mn and S satisfy the following:

RicM ≥ −n(n−2)

n−1 [1 + n2H2 2(n−1)−

pn2H4+ 4(n−1)H2

2(n−1) ] =−C(H) S ≤ n+ n3H2

2(n−1)+n(n−2) 2(n−1)

q

n2H4+ 4(n−1)H2=S+(H),

then S is constant,S =S+(H) and Mn=H1(−a12)×Hn−1(−1−a1 2) witha2n1. Corollary 1.5. Let Mn (n≥3) be a complete maximal spacelike hypersurface in H1n+1(−1). Assume that Mn has n−1 principal curvatures with the same sign everywhere. If RicM ≥ −n(n−2)n−1 , then S=n and Mn=H1(−n)×Hn−1(−n−1n ).

Theorem 1.6. Let Mn (n ≥ 3) be a complete spacelike hypersurface with constant mean curvature H in H1n+1(−1). Assume that Mn has n−1 principal curvatures with the same sign everywhere. If −C(H) ≤ RicM ≤ 0, then S is constant, S =S+(H) andMn=H1(−a12)×Hn−1(−1−a1 2) witha2n1.

2.Preliminaries

Let Mn be an n-dimensional spacelike hypersurface of H1n+1(−1). We choose a local field of semi-Riemannian orthonormal frames {e1,· · ·, en, en+1} in H1n+1(−1) such that, restricted to Mn, e1,· · ·, en are tangent to Mn. Let ω1,· · ·, ωn+1 be

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its dual frame field such that the semi-Riemannian metric of H1n+1(c) is given by ds2=Pn+1A=1AA)2, wherei = 1,i= 1,· · ·, nandn+1 =−1 . Then the structure equations of S1n+1(1) are given by

A=X

B

BωAB∧ωB, ωABBA= 0, (1) dωAB =X

C

CωAC∧ωCB −1 2

X

CD

KABCDωC∧ωD, (2) KABCD =−ABACδBD−δADδBC). (3) We restrict these forms to Mn, thenωn+1= 0 and the Riemannian metric ofMn is written as ds2 =Piω2i. Since

0 =dωn+1 =X

i

ωn+1,i∧ωi, (4)

by Cartan’s lemma we may write ωn+1,i=X

j

hijωj, hij =hji. (5) From these formulas, we obtain the structure equations of Mn:

i =X

j

ωij ∧ωj, ωijji = 0, dωij =X

k

ωik∧ωkj−1 2

X

k,l

Rijklωk∧ωl,

Rijkl=−(δikδjl−δilδjk)−(hikhjl−hilhjk), (6) where Rijkl are the components of curvature tensor of Mn. We call

B =X

i,j

hijωi⊗ωj⊗en+1 (7) the second fundamental form of Mn.

From the above equation, we have

R=−n(n−1)−n2H2+S, (8) whereRis the scalar curvature andS is the norm square of the second fundamental form and H is the mean curvature, then we have

S =X

ij

h2, H = 1 n

X

i

hii.

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Now, we compute some local formulas. For any fixed point x inM, we can choose a local frame field {e1,· · ·, en}, such that

hij(x) =λi(x)δij, i, j= 1,· · ·, n.

where λi are principal curvatures.

Example 1. Let M =H1(−a12)×Hn−1(−1−a1 2) (a >0) be a spacelike hyper- surface of H1n+1(−1). ThenM has two distinct constant principal curvatures

λ1 =

√ 1−a2

a , λ2 =· · ·=λn=− a

√ 1−a2. and constant mean curvature H = 1nPλi = 1−na2

na 1−a2. Ifa2< 1n, then we have

S =n+ n3H2

2(n−1)+n(n−2) 2(n−1)

q

n2H4+ 4(n−1)H2 =S+(H) and the infremum of Ricci curvature of Mn is given by

−C(H) =−n(n−2)

n−1 [1 + n2H2 2(n−1)−

pn2H4+ 4(n−1)H2 2(n−1) ] Ifa2 = 1n, then we haveH = 0,S =n

and the infremum of Ricci curvature ofMn is given by −n(n−2)n−1 . If 1> a2> 1n, then we have

S =n+ n3H2

2(n−1)−n(n−2) 2(n−1)

q

n2H4+ 4(n−1)H2 =S(H) and the infremum of Ricci curvature of Mn is given by

−C+(H) =−n(n−2)

n−1 [1 + n2H2 2(n−1)+

pn2H4+ 4(n−1)H2 2(n−1) ].

3.Proof of Theorems

By renumbering the principal directionse1,· · ·, en, if necessary, we may assume that the principal curvature satisfy

λn≤λn−1 ≤ · · · ≤λ1

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Then we have

S =

n

X

i=1

λ2i, nH =X

i

λi (9)

Rijkl = −δikδjl−δilδjk−λiλjδikδjliλjδilδjk (10) Ricii =

n

X

k=1

Rikik =−(n−1)−nHλi2i (11) Set

P(t) =t2−nHt−(n−1), (12)

It has two real roots Λ±= nH+

n2H2+4(n−1)

2 . From (11) and (12), we have

Ricii=P(λi). (13)

In the next part, we give the proof of Theorem 1.4.

Proof of Theorem 1.4:

AssumeH ≥0. From (1) and (8), we have R = −n(n−1)−n2H2+S

≤ −n(n−1)−n2H2+n+ n3H2

2(n−1)+n(n−2) 2(n−1)

q

n2H4+ 4(n−1)H2

= −n(n−2)[1 + n2H2 2(n−1)−

pn2H4+ 4(n−1)H2 2(n−1) ]

= −(n−1)C(H).

By using the conditions R =PiRicii and Ricii ≥ −C(H), we have Ricii ≤0 for i∈ {1,· · ·, n}. From (13), we have

P(λi)≤0, fori= 1,· · ·, n. So we have

Λ≤λn≤λn−1 ≤ · · · ≤λ1 ≤Λ+. Denote µ= nH−

n2H2+4(n−1)

2(n−1) , we have P(µ) =P(nH −µ) =−C(H). Since Mn has (n−1) principal curvatures with the same sign everywhere andRicii≥ −C(H), then we have the following possible case.

Case A:

Λ ≤λn≤λn−1≤ · · · ≤λ2 ≤µ <0< nH−µ≤λ1≤Λ+.

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Case B:

Λ ≤λn≤µ <0< nH−µ≤λn−1 ≤ · · · ≤λ2 ≤λ1≤Λ+. If the principal curvatures satisfy Case A, then we have

λn≤λn−1 ≤ · · · ≤λ2≤µ <0, On the other hand, we have

n

X

i=2

λi=nH−λ1 ≥nH−Λ+= nH −pn2H2+ 4(n−1)

2 = (n−1)µ.

So we have

λn=· · ·=λ2 =µ, λ1 = nH+pn2H2+ 4(n−1)

2 ,

S = n+ n3H2

2(n−1)+n(n−2) 2(n−1)

q

n2H4+ 4(n−1)H2 and

inf|λ1−λ2|= (2n−3)nH+npn2H2+ 4(n−1)

2(n−1) >0.

then from Theorem 1.3 and Example 1, we know thatMn=H1(−a12)×Hn−1(−1−a12) with a2n1.

If the principal curvatures satisfy Case B, then we have

n−1

X

i=1

λi=nH−λn

≤ nH −nH−pn2H2+ 4(n−1) 2

= nH +pn2H2+ 4(n−1)

2 . (14)

On other hand, we have

n−1

X

i=1

λi≥(n−1)(nH−µ) = (2n−3)nH +pn2H2+ 4(n−1)

2 (15)

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From (14) and (15), we have

(2n−3)nH+pn2H2+ 4(n−1)

2 ≤ nH+pn2H2+ 4(n−1)

2 ,

so

H ≤0.

Since H ≥0, thenH = 0. So the case B turns into the following:

−√

n−1≤λn≤ − 1

√n−1 <0< 1

√n−1 ≤λn−1 ≤ · · · ≤λ1 ≤√

n−1. (16) then we have

(n−1) 1

√n−1 =√

n−1≤

n−1

X

i=1

λi =−λn≤√

n−1. (17)

From (16) and (17), we have

λ1 =· · ·=λn−1 = 1

√n−1 and

λn=−√ n−1.

So

S =

n

X

i=1

λ2i =n

From Theorem 1.1 and S =n, we know thatMn=H1(−n)×Hn−1(−n−1n ). Thus we complete the proof of Theorem 1.4.

Proof of Corollary 1.5: Since Mn is a complete maximal spacelike hypersur- face of H1n+1(−1), then we know that S ≤ n from Theorem 1.1. So we know that Mn satisfies the following:

RicM ≥ −n(n−2) n−1 and

S≤n.

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From Theorem 1.4, we know that S is constant, S = n and Mn = H1(−n)× Hn−1(−n−1n ). This completes the proof of Corollary 1.5.

Proof of Theorem 1.6: Since−C(H)≤RicM ≤0, then we have

−C(H)≤P(λi) =λ2i −nHλi−(n−1)≤0

So we know that the principal curvatures satisfy the Case A or Case B. From the proof of Theorem 1.4, we know that Theorem 1.6 is true.

Acknowledgements: This project is supported by the National Natural Science Foundation of China ( Grant Nos. 11201400, 10971029, 11026062), Project of Henan Provincial Department of Education (Grant No. 2011A110015) and Talent youth teacher fund of Xinyang Normal University.

References

[1] E. Calabi, Examples of Bernstein problems for nonlinear equations, Proc.

Sympos. Pure Math. 15(1970), 223-230.

[2] S.Y. Cheng, S.T. Yau,Maximal space-like hypersurfaces in the Lorentz Minkowski space, Ann. of Math. 104(1976), 407-419.

[3] L.F. Cao, G.X. Wei,A new characterization of hyperbolic cylinder in anti-de Sitter space H1n+1(−1), J.Math.Anal. and Appl. 329(2007), 408-414.

[4] T. Ishihara, Maximal spacelike submanifolds of a pseudo-Riemannian space form of constant curvature, Michigan Math J. 35(1988), 345-352.

[5] C.X. Nie, An application of maximum principle to space-like hypersurfaces with constant mean curvature in anti-de Sitter space, Monatsh Math. 168(2012), 65-73.

[6] S. Nishikawa,On maximal spacelike hypersurfaces in a Lorentzian manifolds, Nagoya Math. J. 95(1984), 117-124.

[7] B.Y. Wu,On complete spacelike hypersurfaces with constant m-th mean cur- vature in an anti-de Sitter space, Inter.J.Math. 21(2010), 551-569.

[8] B.Y. Wu, On complete spacelike hypersurfaces with two distinct principal curvatures in Lorentz-Minkowski space, J.Geo.Phys. 60(2010), 43-52.

Yingbo Han and Shuxiang Feng

College of Mathematics and Information Science Xinyang Normal University

Xinyang, 464000, Henan, P. R. China

email:[email protected]; [email protected]

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