Complete Hypersurfaces in a Real Space Form

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Дата:2008
Автор: Shu, Sh.
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Опубліковано: Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України 2008
Назва видання:Журнал математической физики, анализа, геометрии
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Цитувати:Complete Hypersurfaces in a Real Space Form / Sh. Shu // Журнал математической физики, анализа, геометрии. — 2008. — Т. 4, № 2. — С. 294-304. — Бібліогр.: 12 назв. — англ.

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spelling irk-123456789-1065082016-10-06T00:28:12Z Complete Hypersurfaces in a Real Space Form Shu, Sh. 2008 Article Complete Hypersurfaces in a Real Space Form / Sh. Shu // Журнал математической физики, анализа, геометрии. — 2008. — Т. 4, № 2. — С. 294-304. — Бібліогр.: 12 назв. — англ. 1812-9471 http://dspace.nbuv.gov.ua/handle/123456789/106508 en Журнал математической физики, анализа, геометрии Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
format Article
author Shu, Sh.
spellingShingle Shu, Sh.
Complete Hypersurfaces in a Real Space Form
Журнал математической физики, анализа, геометрии
author_facet Shu, Sh.
author_sort Shu, Sh.
title Complete Hypersurfaces in a Real Space Form
title_short Complete Hypersurfaces in a Real Space Form
title_full Complete Hypersurfaces in a Real Space Form
title_fullStr Complete Hypersurfaces in a Real Space Form
title_full_unstemmed Complete Hypersurfaces in a Real Space Form
title_sort complete hypersurfaces in a real space form
publisher Фізико-технічний інститут низьких температур ім. Б.І. Вєркіна НАН України
publishDate 2008
url http://dspace.nbuv.gov.ua/handle/123456789/106508
citation_txt Complete Hypersurfaces in a Real Space Form / Sh. Shu // Журнал математической физики, анализа, геометрии. — 2008. — Т. 4, № 2. — С. 294-304. — Бібліогр.: 12 назв. — англ.
series Журнал математической физики, анализа, геометрии
work_keys_str_mv AT shush completehypersurfacesinarealspaceform
first_indexed 2025-07-07T18:35:03Z
last_indexed 2025-07-07T18:35:03Z
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fulltext Journal of Mathematical Physics, Analysis, Geometry 2008, vol. 4, No. 2, pp. 294�304 Complete Hypersurfaces in a Real Space Form Shu Shichang Department of Mathematics, Xianyang Teachers University Xianyang, 712000, Shaanxi, Peoples Republic of China E-mail:shushichang@126.com Received February 24, 2007 Let Mn be an n-dimensional complete hypersurface with the scalar cur- vature n(n � 1)R and the mean curvature H being linearly related, that is, n(n � 1)R = k0H(k0 > 0) in a real space form Rn+1(c). Assume that the mean curvature is positive and obtains its maximum on Mn. We show that (1) if c = 1; k0 � 2n p n(n� 1), for any i, P j 6=i �2 j > n(n � 1) and jhj2 � nH2 + (B+ H )2, then Mn is totally umbilical, or (i) n � 3;Mn is lo- cally an H(r)-torus with r2 < n�1 n , (ii) n = 2;Mn is locally an H(r)-torus with r2 6= n�1 n ; (2) if c = 0 and jhj2 � nH2+( eB+ H )2, thenMn is isometric to a standard round sphere, a hyperplane Rn or Sn�1(c1) � R1; (3) if c = �1 and jhj2 � nH2 + ( bB+ H )2, then Mn is totally umbilical or is isometric to Sn�1(r) �H1(�1=(r2 + 1)) for some r > 0, where jhj2 denotes the squared norm of the second fundamental form of Mn; B+ H ; eB+ H and bB+ H are denoted by (1.1), (1.2) and (1.3). Key words: hypersurface, mean curvature, scalar curvature, real space form. Mathematics Subject Classi�cation 2000: 53C40 (primary); 53C20 (secondary). 1. Introduction Let Rn+1(c) be an (n+ 1)-dimensional connected Riemannian manifold with constant sectional curvature c. We also call it a real space form. According to c > 0, c = 0 or c < 0, it is called sphere space, Euclidean space or hyperbolic space, respectively, and it is denoted by Sn+1(c); Rn+1 and Hn+1(c). As it is well- known that there are many rigidity results for hypersurfaces with constant mean curvature or with constant scalar curvature in Sn+1(c); Rn+1 and Hn+1(c), for example, see [1�3, 5] and [12] etc., but fewer ones are obtained for hypersurfaces This work is supported in part by the Natural Science Foundation of China and NSF of Shaanxi, China. c Shu Shichang, 2008 Complete Hypersurfaces in a Real Space Form with the scalar curvature and the mean curvature being linearly related. We know that an H(r)-torus in a unit sphere Sn+1(1) is the product immersion Sn�1(r)� S1( p 1� r2) ,! Rn�R2, where Sn�1(r) � Rn; S1( p 1� r2) � R2, 0 < r < 1, are standard immersions. In some orientation, H(r)-torus has principal curvatures given by �1 = � � � = �n�1 = p 1�r2 r and �n = � rp 1�r2 . In [12], the authors obtained the following: Theorem 1.1. Let Mn be an n-dimensional complete hypersurface with con- stant mean curvature H in a unit sphere Sn+1(1). (1) If jhj2 < D0(n;H), then Mn is totally umbilical. (2) If jhj2 = D0(n;H), then (i) when H = 0;Mn is locally a Cli�ord torus; (ii) when H 6= 0; n � 3;Mn is locally an H(r)-torus with r2 < n�1 n ; (iii) when H 6= 0; n = 2;Mn is locally an H(r)-torus with r2 6= n�1 n , where D0(n;H) = n+ n3H2 2(n� 1) � (n� 2)nH 2(n� 1) [n2H2 + 4(n� 1)] 1 2 : In [6], S.Y. Cheng and S.T. Yau obtained the following: Theorem 1.2. Let Mn be a complete hypersurface with constant mean cur- vature in Rn+1. If the sectional curvature of Mn is nonnegative, then Mn is isometric to a standard round sphere, a hyperplane Rn or a Riemannian product Sk(c1)�Rn�k, 1 � k � n� 1. In this paper, we study the hypersurfaces in a real space form Rn+1(c) with scalar curvature n(n � 1)R and the mean curvature H being linearly related. We obtain the following theorems: Theorem 1.3. Let Mn be an n-dimensional complete hypersurface with n(n� 1)R = k0H in a unit sphere Sn+1(1), where k0(� 2n p n(n� 1)) is a positive constant. Assume that the mean curvature H is positive and obtains its maximum on Mn and for any i, P j 6=i � 2 j > n(n� 1), where �j(j = 1; : : : ; i� 1; i+1; : : : ; n) are the principal curvatures onMn. If the squared norm of the second fundamental form jhj2 satis�es jhj2 � nH2 + (B+ H )2 on Mn, then Mn is totally umbilical, or (i) n � 3;Mn is locally an H(r)-torus with r2 < n�1 n ; (ii) n = 2;Mn is locally an H(r)-torus with r2 6= n�1 n , where B+ H = �1 2 (n� 2) r n n� 1 H + s n3H2 4(n� 1) + n: (1:1) Theorem 1.4. Let Mn be an n-dimensional complete hypersurface with n(n� 1)R = k0H in a Euclidean space Rn+1, where k0 is a positive constant. Assume Journal of Mathematical Physics, Analysis, Geometry, 2008, vol. 4, No. 2 295 Shu Shichang that the mean curvature H is positive and obtains its maximum on Mn. If the squared norm of the second fundamental form jhj2 satis�es jhj2 � nH2 + ( eB+ H )2 on Mn, then Mn is isometric to a standard round sphere, a hyperplane Rn or a Riemannian product Sn�1(c1)�R1, where eB+ H = r n n� 1 H: (1:2) Theorem 1.5. Let Mn be an n-dimensional complete hypersurface with n(n� 1)R = k0H in a hyperbolic space Hn+1(�1), where k0 is a positive constant. Assume that the mean curvature H is positive and obtains its maximum on Mn. If the squared norm of the second fundamental form jhj2 satis�es jhj2 � nH2 + ( bB+ H )2 on Mn, then Mn is totally umbilical or is isometric to Sn�1(r)�H1(�1=(r2+1)) for some r > 0, where bB+ H = �1 2 (n� 2) r n n� 1 H + s n3H2 4(n� 1) � n; (n2H2 � 4(n� 1)): (1:3) 2. Preliminaries Let Mn be an n-dimensional hypersurface in Rn+1(c). For any p 2 Mn we choose a local orthonormal frame e1; : : : ; en; en+1 in Rn+1(c) around p such that e1; : : : ; en are tangential to Mn. Take the corresponding dual co-frame f!1; : : : ; !n; !n+1g. In this paper we make the following convention on the range of indices, 1 � A;B;C � � � � n+ 1; 1 � i; j; k; � � � � n: The structure equations of Rn+1(c) are d!A = P B !AB ^ !B ; !AB = �!BA; d!AB = P c !AC ^ !CB � c!A ^ !B: If we denote by the same letters the restrictions of !A; !AB to Mn, we have d!i = X j !ij ^ !j; !ij = �!ji; (2:1) 296 Journal of Mathematical Physics, Analysis, Geometry, 2008, vol. 4, No. 2 Complete Hypersurfaces in a Real Space Form d!ij = X k !ik ^ !kj � 1 2 X k;l Rijkl!k ^ !l; (2:2) where Rijkl is the curvature tensor of the induced metric on Mn. Restricted to Mn; !n+1 = 0, thus 0 = d!n+1 = X i !n+1i ^ !i; (2:3) and by Cartan's lemma we can write !in+1 = X j hij!j; hij = hji: (2:4) The quadratic form h = P i;j hij!i !j is the second fundamental form of Mn. The Gauss equation is Rijkl = c(ÆikÆjl � ÆilÆjk) + hikhjl � hilhjk; (2:5) n(n� 1)R = n(n� 1)c+ n2H2 � jhj2; (2:6) where R is the normalized scalar curvature, H = (1=n) P i hii the mean curvature and jhj2 = P i;j h2 ij the squared norm of the second fundamental form of Mn, respectively. The Codazzi equation and Ricci identity are hijk = hikj ; (2:7) hijkl � hijlk = X m hmjRmikl + X m himRmjkl; (2:8) where the �rst and the second covariant derivatives of the second fundamental form are de�ned byX k hijk!k = dhij + X k hkj!ki + X k hik!kj; (2:9) X l hijkl!l = dhijk + X m hmjk!mi + X m himk!mj + X m hijm!mk: (2:10) In order to represent our theorems, we need some notations, for details see H.B. Lawson [9] and P.J. Ryan [11]. First we give a description of the real hyper- bolic space Hn+1(c) of constant curvature c(< 0). For any two vectors x and y in Rn+2, we set g(x; y) = x1y1 + : : :+ xn+1yn+1 � xn+2yn+2; Journal of Mathematical Physics, Analysis, Geometry, 2008, vol. 4, No. 2 297 Shu Shichang (Rn+2; g) is the so-called Minkowski space-time. Denote � = p �1=c. We de�ne Hn+1(c) = fx 2 Rn+2 j g(x; x) = ��2; xn+2 > 0g: Then Hn+1(c) is a simply-connected hypersurface of Rn+2. Hence, we obtain a model of a real hyperbolic space. We de�ne M1 = fx 2 Hn+1(c) j x1 = 0g; M2 = fx 2 Hn+1(c) j x1 = r > 0g; M3 = fx 2 Hn+1(c) j xn+2 = xn+1 + �g; M4 = fx 2 Hn+1(c) j x21 + : : :+ x2 n+1 = r2 > 0g; M5 = fx 2 Hn+1(c) j x21 + : : :+ x2 k+1 = r2 > 0; x2 k+2 + : : :+ x2 n+1 � x2 n+2 = ��2 � r2g: M1; : : : ;M5 are often called the standard examples of complete hypersurfaces in Hn+1(c) with at most two distinct constant principal curvatures. It is obvious that M1; : : : ;M4 are totally umbilical. In the sense of Chen [7], they are called the hyperspheres of Hn+1(c). M3 is called the horosphere and M4 � the geodesic distance sphere of Hn+1(c). P.J. Ryan [11] obtained the following: Lemma 2.1([11]). Let Mn be a complete hypersurface in Hn+1(c). Suppose that, under a suitable choice of a local orthonormal tangent frame �eld of TMn, the shape operator over TMn is expressed as a matrix A. If Mn has at most two distinct constant principal curvatures, then it is congruent to one of the following: (1) M1. In this case, A = 0, andM1 is totally geodesic. Hence M1 is isometric to Hn(c). (2) M2. In this case, A = 1=�2p 1=�2+1=r2 In, where In denotes the identity matrix of degree n, and M2 is isometric to Hn(�1=(r2 + �2)). (3) M3. In this case, A = 1 � In, and M3 is isometric to a Euclidean space Rn. (4) M4. In this case, A = p 1=r2 + 1=�2In;M4 is isometric to a round sphere Sn(r) of radius r. (5) M5. In this case, A = �Ik � �In�k, where � = p 1=�2 + 1=r2, and � = 1=�2p 1=r2+1=�2 ;M5 is isometric to Sk(r)�Hn�k(�1=(r2 + �2)). We also need the following algebraic Lemma due to [10] and [1]. Lemma 2.2([10, 1]). Let �i; i = 1; : : : ; n be real numbers, with P i �i = 0 and P i �2 i = �2 � 0. Then � n� 2p n(n� 1) �3 � X i �3i � n� 2p n(n� 1) �3; (2:11) 298 Journal of Mathematical Physics, Analysis, Geometry, 2008, vol. 4, No. 2 Complete Hypersurfaces in a Real Space Form and equality holds if and only if either (n � 1) of the numbers �i are equal to �= p n(n� 1) or (n� 1) of the numbers �i are equal to ��= p n(n� 1). 3. Proof of Theorems In order to prove our theorems, we introduce an operator 2 due to S.Y. Cheng and S.T. Yau [5] by 2f = X i;j (nHÆij � hij)fij; (3:1) where f is a C2-function on Mn, the gradient and Hessian (fij) are de�ned by df = X i fi!i; X j fij!j = dfi + X j fj!ji: (3:2) The Laplacian of f is de�ned by �f = P i fii. We choose a local frame �eld e1; : : : ; en at each point of Mn, such that hij = �iÆij . From (3.1) and (2.6), we have 2(nH) = nH�(nH)� P i �i(nH)ii = 1 2 �(nH)2 � P i (nH)2 i � P i �i(nH)ii = 1 2 n(n� 1)�R+ 1 2 �jhj2 � n2jrHj2 � P i �i(nH)ii: (3.3) From (2.7) and (2.8), by a standard and direct calculation, we have 1 2 �jhj2 = X i;j;k h2ijk + X i �i(nH)ii + 1 2 X i;j Rijij(�i � �j) 2; (3:4) where Rijij = c + �i�j(i 6= j) denotes the sectional curvature of the section spanned by fei; ejg: From (3.3) and (3.4), we get 2(nH) = 1 2 n(n� 1)�R+ jrhj2 � n2jrHj2 + 1 2 X i;j (c+ �i�j)(�i � �j) 2: (3:5) By making use of the similar method in [4], we can prove the following: Proposition 3.1. Let Mn be an n-dimensional hypersurface in a real space form Rn+1(c) with n(n� 1)R = k0H, k0 = constant > 0. Assume that the mean curvature H > 0. Then we have the operator L = 2� (k0=2n)� Journal of Mathematical Physics, Analysis, Geometry, 2008, vol. 4, No. 2 299 Shu Shichang (1) if c > 0 and for any i, P j 6=i � 2 j > n(n� 1)c; L is elliptic; (2) if c � 0; L is elliptic. P r o o f. We choose an orthonormal frame �eld fejg at each point in Mn so that hij = �iÆij. For any i, (nH � �i � k0=2n) = P j �j � �i � (1=2)[� P j �2 j + n2H2 + n(n� 1)c]=(nH) = [( P j �j) 2 � �i P j �j � (1=2) P l 6=j �l�j � (1=2)n(n� 1)c](nH)�1 = [ P j �2 j + (1=2) P l 6=j �l�j � �i P j �j � (1=2)n(n � 1)c](nH)�1 = [ P i6=j �2 j + (1=2) P l6=j l;j 6=i �l�j � (1=2)n(n � 1)c](nH)�1 = (1=2)[ P j 6=i �2 j + ( P j 6=i �j) 2 � n(n� 1)c](nH)�1: (3.6) (1) If c > 0 and for any i, P j 6=i �2 j > n(n� 1)c; from (3.6), we have (nH � �i � k0=2n) � (1=2)[ X j 6=i �2j � n(n� 1)c](nH)�1 > 0: Therefore, we know that L is an elliptic operator. (2) If c � 0, from (3.6) again, we have (nH � �i � k0=2n) > 0: Therefore, we also know that L is an elliptic operator. This completes the proof of Prop. 3.1. We can also prove the following: Proposition 3.2. Let Mn be an n-dimensional hypersurface in a real space form Rn+1(c) with n(n� 1)R = k0H, k0 = constant > 0. Assume that the mean curvature H > 0. Then we have: (1) if c > 0 and k0 � 2n p n(n� 1)c, then jrhj2 � n2jrHj2; (2) if c � 0, for all k0 > 0, then jrhj2 � n2jrHj2: 300 Journal of Mathematical Physics, Analysis, Geometry, 2008, vol. 4, No. 2 Complete Hypersurfaces in a Real Space Form P r o o f. Since H > 0, we have jhj2 6= 0. In fact, if jhj2 = P i �2 i = 0 at a point of Mn, then �i = 0, i = 1; 2; : : : ; n, at this point. Therefore H = 0 at this point. This is impossible. From (2.6) and n(n� 1)R = k0H, we have k0riH = 2n2HriH � 2 P j;k hkjhkji; (1 2 k0 � n2H)riH = � P j;k hkjhkji; (1 2 k0 � n2H)2jrHj2 = P i ( P j;k hkjhkji) 2 � P i;j h2 ij P i;j;k h2 ijk = jhj2jrhj2: Therefore, we have jrhj2 � n2jrHj2 � [( k0 2 � n2H)2 � n2jhj2]jrHj2 1 jhj2 = [ (k0)2 4 � n3(n� 1)c]jrHj2 1 jhj2 : (3.7) (1)If c > 0 and k0 � 2n p n(n� 1)c, from (3.7), we have jrhj2 � n2jrHj2 � 0: (2) If c � 0, from (3.7), we also have jrhj2 � n2jrHj2 � 0: This completes the proof of Prop. 3.2. Proposition 3.3. Let Mn be an n-dimensional hypersurface in a real space form Rn+1(c) with n(n� 1)R = k0H, k0 = constant > 0. Then we have nLH � (jrhj2 � n2jrHj2) + jgj2fnc+ nH2 � n(n� 2)p n(n� 1) jHjjgj � jgj2g; where jgj2 is a nonnegative C2-function on Mn de�ned by jgj2 = jhj2 � nH2. P r o o f. From (3.5) we have nLH = n[2H � (k0=2n)�H] = 2(nH)� (1=2)�[n(n� 1)R] = jrhj2 � n2jrHj2 + 1 2 P i;j (c+ �i�j)(�i � �j) 2 = jrhj2 � n2jrHj2 + ncjhj2 � n2H2c� jhj4 + nH P i �3 i : (3.8) Journal of Mathematical Physics, Analysis, Geometry, 2008, vol. 4, No. 2 301 Shu Shichang Let jgj2 be a nonnegative C2-function on Mn de�ned by jgj2 = jhj2 � nH2. Since P i (H � �i) = 0, P i (H � �i) 2 = jhj2 � nH2 = jgj2, by Lem. 2.2 we get nH P i �3 i = 3nH2jhj2 � 2n2H4 � nH P i (H � �i) 3 � 3nH2jgj2 + n2H4 � njHj n� 2p n(n� 1) jgj3: (3.9) Therefore, from (3.8) and (3.9), we have nLH � jrhj2 � n2jrHj2 + jgj2fnc+ nH2 � n(n� 2)p n(n� 1) jHjjgj � jgj2g: This completes the proof of Prop. 3.3. P r o o f o f T h e o r e m 1.3. From the assumption of Th. 1.3, Prop. 3.2 and Prop. 3.3 for c = 1, we have nLH � jgj2fn+ nH2 � n(n�2)p n(n�1) Hjgj � jgj2g = jgj2PH(jgj); (3:10) where PH(jgj) = n+ nH2 � n(n� 2)p n(n� 1) Hjgj � jgj2: PH(jgj) has two real roots B� H and B+ H given by B� H = �1 2 (n� 2) r n n� 1 H � s n3H2 4(n� 1) + n: Therefore, we know that PH(jgj) = (jgj �B� H )(�jgj +B+ H ): Clearly, we know that jgj�B� H > 0. From the assumption of Th. 1.3, we infer that PH(jgj) � 0 onMn. This implies that the right-hand side of (3.10) is nonnegative. Since, from Prop. 3.1, the operator L is elliptic, and H obtains its maximum on Mn, from (3.10) we know that H = const on Mn. Therefore, we know that Mn is an n-dimensional complete hypersurface with constant mean curvature H(> 0) in a unit sphere Sn+1(1). By the assumption of Th. 1.3 and the result of Th. 1.1, we can check directly that jhj2 � nH2 + (B+ H )2 = n+ n 3 H 2 2(n�1) � (n�2)nH 2(n�1) [n2H2 + 4(n � 1)] 1 2 = D0(n;H). Therefore we have either Mn is totally umbilical, or (i) n � 3;Mn is locally an H(r)-torus with r2 < n�1 n ; (ii) n = 2;Mn is locally an H(r)-torus with r2 6= n�1 n . This completes the proof of Th. 1.3. 302 Journal of Mathematical Physics, Analysis, Geometry, 2008, vol. 4, No. 2 Complete Hypersurfaces in a Real Space Form P r o o f o f T h e o r e m 1.4. From the assumption of Th. 1.4, Prop. 3.2 and Prop. 3.3, for c = 0, we have nLH � jgj2fnH2 � n(n�2)p n(n�1) Hjgj � jgj2g = jgj2QH(jgj); (3:11) where QH(jgj) = nH2 � n(n� 2)p n(n� 1) Hjgj � jgj2: QH(jgj) has two real roots eB� H and eB+ H given by eB� H = �(n� 1) r n n� 1 H; eB+ H = r n n� 1 H: Therefore, we know that QH(jgj) = (jgj � eB� H )(�jgj + eB+ H ): Clearly, we know that jgj � eB� H > 0. From the assumption of Th. 1.4, we infer that QH(jgj) � 0 on Mn. This implies that the right-hand side of (3.11) is nonnegative. From Proposition 3.1, we know that L is elliptic, and H obtains its maximum on Mn. From (3.11), we have H = const on Mn. From (3.11) again, we get jgj2QH(jgj) = 0. We infer that the equality holds in Lem. 2.2. Therefore, we know that (n � 1) of the numbers H � �i are equal to jgj= p n(n� 1). This implies that Mn has (n � 1) principal curvatures equal and constant. As H is constant, the other principal curvature is constant as well. From an inequality of Chen�Okumura [8], we know that jhj2 � n2H2=(n� 1) implies that the sectional curvature K of Mn is nonnegative. Therefore, we know that Mn is a complete hypersurface in Rn+1 with constant mean curvature and nonnegative sectional curvature. From Theorem 1.2, we have either Mn is isometric to a standard round sphere, a hyperplane Rn or a Riemannian product Sn�1(c1) � R1. This completes the proof of Th. 1.4. P r o o f o f T h e o r e m 1.5. From the assumption of Th. 1.5, Prop. 3.2 and Prop. 3.3, for c = �1, we have nLH � jgj2f�n+ nH2 � n(n�2)p n(n�1) Hjgj � jgj2g = jgj2RH(jgj); (3:12) where RH(jgj) = �n+ nH2 � n(n� 2)p n(n� 1) Hjgj � jgj2: RH(jgj) has two real roots bB� H and bB+ H given by bB� H = �1 2 (n� 2) r n n� 1 H � s n3H2 4(n� 1) � n; n2H2 � 4(n� 1): Journal of Mathematical Physics, Analysis, Geometry, 2008, vol. 4, No. 2 303 Shu Shichang Therefore, we know that RH(jgj) = (jgj � bB� H )(�jgj + bB+ H ): Clearly, we know that jgj� bB� H > 0. From the assumption of Th. 1.5, we infer that RH(jgj) � 0 onMn. This implies that the right-hand side of (3.12) is nonnegative. From Proposition 3.1, we know that L is elliptic. Since H obtains its maximum on Mn, from (3.12), we have H = const on Mn. From (3.12) again, we get jgj2RH(jgj) = 0, so jgj2 = 0, and Mn is totally umbilical, or RH(jgj) = 0. In the latter case, we know that (n�1) of the numbers H��i are equal to jgj= p n(n� 1). This implies thatMn has (n�1) principal curvatures equal and constant. As H is constant, the other principal curvature is constant as well, soMn is isoparametric. From the result of Lem. 2.1, Mn is isometric to Sn�1(r) �H1(�1=(r2 + 1)) for some r > 0. This completes the proof of Th. 1.5. References [1] H. Alencar and M.P. do Carmo, Hypersurfaces with Constant Mean Curvature in Sphere. � Proc. Amer. Math. Soc. 120 (1994), 1223�1229. [2] Q.M. Cheng, Complete Hypersurfaces in Euclidean Space Rn+1 with Constant Scalar Curvature. � Indiana Univ. Math. J. 51 (2002), 53�68. [3] Q.M. Cheng, Hypersurfaces in a Unit Shere Sn+1(1) with Constant Scalar Curva- ture. � J. London Math. Soc. 64 (2001), 755�768. [4] Q.M. Cheng, Complete Space-Like Hypersurfaces of a de Sitter Space with r = kH . � Mem. Fac. Sci. Kyushu Univ. 44 (1990), 67�77. [5] S.Y. Cheng and S.T. Yau, Hypersurfaces with Constant Scalar Curvature. � Math. Ann. 225 (1977), 195�204. [6] S.Y. Cheng and S.T. Yau, Di�erential Equations on Riemannian Manifolds and their Geometric Applications. � Comm. Pure Appl. Math. 28 (1975), 333�354. [7] B.Y. Chen, Totally Mean Curvature and Submanifolds of Finite Type. World Sci., Singapore, 1984. [8] B.Y. Chen and M. Okumura, Scalar Curvature, Inequality and Submanifold. � Proc. Amer. Math. Soc. 38 (1973), 605�608. [9] H.B. Lawson, Jr., Local Rigidity Theorems for Minimal Hypersurfaces. � Ann. Math. 89(2) (1969), 187�197. [10] M. Okumura, Hypersurfaces and a Pinching Problem on the Second Fundamental Tensor. � Amer. J. Math. 96 (1974), 207�213. [11] P.J. Ryan, Hypersurfaces with Parallel Ricci Tensor. � Osaka J. Math. 8 (1971), 251�259. [12] S.C. Shu, Complete Hypersurfaces with Constant Mean Curvature in Locally Sym- metric Manifold. � Adv. Math. Chinese 33 (2004), 563�569. 304 Journal of Mathematical Physics, Analysis, Geometry, 2008, vol. 4, No. 2