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Annals of Mathematics The Clifford-Klein Space Forms of Indefinite Metric Author(s): Joseph A. Wolf Reviewed work(s): Source: The Annals of Mathematics, Second Series, Vol. 75, No. 1 (Jan., 1962), pp. 77-80 Published by: Annals of Mathematics Stable URL: http://www.jstor.org/stable/1970420. Accessed: 03/05/2012 14:54 Your use of the JSTOR archive indicates your acceptance of the Terms & Conditions of Use, available at. http://www.jstor.org/page/info/about/policies/terms.jsp JSTOR is a not-for-profit service that helps scholars, researchers, and students discover, use, and build upon a wide range of content in a trusted digital archive. We use information technology and tools to increase productivity and facilitate new forms of scholarship. For more information about JSTOR, please contact support@jstor.org. Annals of Mathematics is collaborating with JSTOR to digitize, preserve and extend access to The Annals of Mathematics. http://www.jstor.org

ANNAL!S OF MIATHEMATICS Vol. 75, No. 1, January, 1962 Printed in Japan THE CLIFFORD-KLEIN SPACE FORMS OF INDEFINITE METRIC BY JOSEPH A. WOLF* (Received February 24, 1961) 1. Introduction The spherical space form problem of Clifford-Klein is the classification problem for complete connected riemannian manifolds of constant positive curvature. E. Calabi and L. Markus have recently considered the classification problem for complete connected Lorenz n-manifolds M," of constant positive curvature, and have [1; Theorems 2 and 3] reduced it to the spherical space form problem for riemannian (n - 1)-manifolds, when n? 3. We will extend their ideas to more general signatures of metric, and reduce the classification problem for complete connected pseudoriemannian n-manifolds M,, of constant positive curvature, and with s # n - 1 and 2s < n, to the spherical space form problem for riemannian (n - s)-manifolds. As the spherical space form problem is solved in dimension 3 [3], and is trivial in even dimensions, this gives a classification (up to global isometry) of the complete connected pseudo-riemannian manifolds M8' of constant positive curvature with s # n - 1, 2s < n, and either n - s = 3 or n - s even. I am indebted to L. Markus and E. Calabi for showing me the manuscript of their paper [1], which is the basis for this note. 2. Pseudo-riemannian manifolds In order to establish terminology and notation, we recall some basic facts about pseudo-riemannian manifolds. A pseudo-riemannian metric Q on a differentiable manifold Mis a differentiable field of non-degenerate bilinear forms Qp on the tangent-spaces Mp of M; a pseudo-riemannian manifold is a differentiable manifold with a pseudo-riemannian metric. We will consider only those pseudo-riemannian manifolds (M, Q) where each Qp has the same signature', say -dxi - * - dx' + dx'l1 + *** + dx2; (M, Q) is then denoted MS". In the riemannian case (s = 0), we will simply write Mn. A pseudo-riemannian manifold Msn carries a unique linear connection-the Levi-Civita connection on the tangent-bundle of M8n-with torsion zero, and such that parallel translation is an isometry of tangentspaces. In local coordinates x-(x1,..., xn), we set qij(x) = Qx((&I8xi), (0/1xj)) * The author is grateful for National Science Foundation Fellowship support while writ- ing this paper. This is automatic if M is connected. 77

78 JOSEPH A. WOLF and lower indices of the curvature tensor Ri k,(x) of the Levi-Civita connection, using the classical formula Rijkl(X) = :qjm(x)ri kt(x); M7 has constant curvature K if RijkZ(X) = K[qik(x)qi,(x) - qik(x)qj,(x)] identically in x, for every (i, j, k, 1) and every local coordinate system. M." is complete if its Levi-Civita connection is complete, i.e., if every geodesic can be extended to arbitrary values of the affine parameter. An isometry is a diffeomorphism d: N,4-+Mf" where every tangent map is a linear isometry; a pseudo-riemannian covering is a covering f: Nn -+ M;' of connected pseudo-riemannian manifolds where every tangent map is a linear isometry. The indefinite orthogonal group Os(n + 1) is the group of all linear transformations of the real vector space R"+' which preserve the bilinear form bn(x, y) = -x-y-* * *-x~y. + x,+ly+y + *** + x,+ly?1+y. The quadric bl(x, x) = 1 carries a pseudo-riemannian metric such that it is a pseudoriemannian manifold Sn of constant curvature +1, and Os(n + 1) is its full group of isometries [4,? 4]. We define Ss to be Ss if s < n - 1, Sn-_ to be the universal pseudo-riemannian covering manifold of SnU1, and Sn to be the component of (0, **, 0, 1) in Sn. We have proved [4, Theorem 5] that every complete connected pseudo-riemannian manifold Mn of constant curvature +1 admits a universal pseudo-riemannian covering f: Sn -* M, and is thus isometric to the quotient manifold SSID where the subgroup D of the group of isometries of S9n is just the group of deck transformations of f. Thus we define a pseudo-spherical space form of signature (s, n - s) to be a complete connected pseudo-riemannian manifold Mst of constant curvature + 1. A spherical space form is just a pseudospherical space form M" = Mn, and, in the terminology of [1], a relativistic spherical space form is a pseudo-spherical space form Ml. 3. The reduction This reduction was inspired by that of Calabi and Markus [1] where they do the case s = 1; the proof of our Theorem 1 being virtually identical to their proof for s = 1, while the methods of our Theorem 2 are different from their quite geometric techniques. THEOREM 1. Let M: be a pseudo-spherical space form with s # n - 1 and 2s? n. Then Mn has finite fundamental group. PROOF. Sn = 9Sn because s < n - 1, so we have a universal pseudoriemannian covering f: Sn -* M84. The group D of deck transformations of the covering is isomorphic to the fundamental group of Mn, so we must

CLIFFORD-KLEIN SPACE FORMS 79 prove that D is finite. S: is given by -EIxI + EI+IX2 =1 where the x; are coordinates in R71+ relative to a basis {v1,***, v,,1}. Let V be the subspace spanned by {vats, *., v,?1}. If g is any non-singular linear transformation of R n+1' then 2s < n < n + 1 gives us dim (Vn gv)?2 dim V- (n + 1) > 0. If Sn5 denotes the "equatorial sphere" xi = x. =s = 0, Es+lxj = 1 in S8", and if g e D, it follows that g(sn-s) meets Sn-s The rest of the argument follows [1]. If D were infinite, compactness of Sn-s would give a point p e 5n-S, a sequence {gij of distinct elements of D, and a sequence {pi} in Sn-s such that each gi(pi) e Sn-s and {gi(pi)}-*p We may pass to a subsequence and assume {pi} p' e Sn-S. This gives an element g e D with g(p') = p; so {g-1gi(pj} -* g-1(p) = p'. As all the gi are distinct, we may assume that none of the g-1gi is 1 e D. Thus every neighborhood of p' in Ssn meets one of its transforms by an element #1 of D. This is impossible because D, being a group of deck transformations, acts freely and properly discontinuously on Ss. q.e.d. Notice that the product 0(s) x 0(n - s + 1) is a maximal compact subgroup of Os(n + 1), where 0(s) is the ordinary orthogonal group on the first s coordinates in Rn+1 and 0(n - s + 1) is the ordinary orthogonal group on the last n - s + 1 coordinates in R LEMMA (E. Cartan). Every compact subgroup of Os(n + 1) is conjugate to a subgroup of 0(s) x 0(n - s + 1). PROOF. This follows from a technique of E. Cartan [2,? 16]. Also, A. Borel has remarked that the lemma is just simultaneous diagonalization of two quadratic forms. q.e.d. THEOREM 2. Let Sn-sIG be a spherical space form, view G as the image of a faithful orthogonal representation f: H-* 0(n - s + 1) of an abstract finite group H, let g: H-* 0(s) be any orthogonal representation of H. and set D = (g + f)(h) c0 (s) x 0(n-s + 1) c Os(n + 1). Then D is free and properly discontinuous on Sn, SSnJD is a pseudo-spherical space form, and S,,/D has finite fundamental group if s # n -1. Conversely, let Mn be a pseudo-spherical space form with s # n - 1 and with finite fundamental group (automatic if 2s? n). Then Mn is isometric to one of the manifolds SS'7D described above. PROOF. D is finite, thus properly discontinuous on Sn. If h e H and (g + f )(h) has an eigenvalue + 1, then either h = 1 or the corresponding eigenvector lies in the span of the first s coordinates on Rn l. Thus D acts freely on SSn. This shows that S,,/D is a pseudo-spherical space form.

80 JOSEPH A. WOLF If s * n - 1, then S." is simply connected, and the fundamental group of S.:/D is finite. For the second part of the theorem, let f: S." -- M." be the universal pseudo-riemannian covering, and let D be the group of deck transformations. As s * n - 1, D is a subgroup of 08(n + 1). D was assumed finite, thus compact, although this is automatic if 2s < n. Using the lemma, we may replace D by a conjugate, thereby changing M," by an isometry, and assume D c 0(s) x 0(n - s + 1). Now write every a e D in the form (al, a2) with a, e 0(s) and a2 G 0(n - s + 1). The {a2} generate a subgroup G of 0(n - s + 1) which acts freely on the equatorial sphere So-* in S."; thus S''-/G is a spherical space form. Set H = D, f(a)= a and g(a) = a,, and the theorem is proved. q.e.d. Theorems 1 and 2 reduce the classification problem for complete connected pseudo-riemannian manifolds M." (s # n - 1 and 2s < n) of constant positive curvature to the classification problem for complete connected riemannian manifolds M,,-' of constant positive curvature. INSTITUTE FOR ADVANCED STUDY REFERENCES 1. E. CALABi and L. MARKUS, Relativistic space forms, Ann. of Math., 75 (1962), 63-76. 2. :. CARTAN, Groupes simples coe et ouverts et la giometrie riemoannienne, J. Math. Pures Appl., 8 (1929), 1-33; OEuvres completes, part. 1, vol. 2, 1011-1044. 3. W. THRELFALL and H. SEFERT, Topologische Untersuchung der Diskontinuititsbereiche endlicher Bewegungsgruppen des dreidimensionalen sphiriachen Baume", Math. Ann., 104 (1930), 1-70; ibid, 107 (1932), 543-586. 4. J. A. WOLF, Homogeneous manifolds of constant curvature, Comment. Math. Helv., to appear.