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Introduction and statement of results

Complex hyperbolic space tex2html_wrap_inline949 is a complete Riemannian manifold with sectional curvature pinched between -2 and -1/2. A standard model for it is the unit ball tex2html_wrap_inline997 ( tex2html_wrap_inline999 ) with the Bergman metric. For the case d=1 note that tex2html_wrap_inline1003 is isomorphic to the real hyperbolic plane tex2html_wrap_inline1005 . As a complex manifold, tex2html_wrap_inline949 admits a natural Kähler structure, and therefore also a symplectic structure.

The group of holomorphic isometries of tex2html_wrap_inline949 is the Lie group PU(1,d). G. D. Mostow [19] established that finite covolume discrete subgroups of PU(1,d) are rigid. Recent work has shown that interesting phenomona still arise in connection with deformations of smaller discrete subgroups. (See for example [8], [9].)

At the same time, a successful theory of quasiconformal mapping on complex hyperbolic space and its boundary has been developed by Korányi, Reimann, Pansu and others. (See for example [15] and [20].) Moreover, as in real hyperbolic geometry, there seems to be much fertile ground for the application of quasiconformal mappings to deformation questions about complex hyperbolic groups. Indeed, Mostow's rigidity theorem involves quasiconformal mapping in a vital way. In this article, we offer another application of quasiconformal mapping to deformation theory of groups that are far from having finite covolume. Specifically, we show that smooth deformations of complex hyperbolic Schottky groups are quasiconformally stable in an appropriate sense.

For comparison recall the definition of quasiconformal stability from the theory of Kleinian groups as given by Bers in [2]. Let G be any subgroup of tex2html_wrap_inline1017 . A homomorphism tex2html_wrap_inline1019 will be called allowable if it preserves the square traces of parabolic and elliptic elements. Say that tex2html_wrap_inline1021 is a quasiconformal deformation of G if there exists a quasiconformal mapping tex2html_wrap_inline1025 such that tex2html_wrap_inline1027 for all tex2html_wrap_inline1029 . A finitely generated Kleinian group tex2html_wrap_inline1031 is then called quasiconformally stable if every allowable homomorphism sufficiently close to the identity is a quasiconformal deformation. In [2], Bers described a criterion (involving the quadratic differentials for tex2html_wrap_inline1031 ) to determine whether a group tex2html_wrap_inline1031 is quasiconformally stable. As a consequence of this criterion, it follows that Fuchsian groups, Schottky groups, groups of Schottky type and certain non-degenerate B-groups are all quasiconformally stable [3].

As with real hyperbolic isometries, elements of PU(1,d) can be classified as loxodromic, parabolic or elliptic. Let tex2html_wrap_inline1041 be a discrete group generated by n loxodromic elements. The Dirichlet domain (fundamental polyhedron) of tex2html_wrap_inline1031 with respect to the point tex2html_wrap_inline1047 is given by

displaymath985

In analogy with Kleinian groups, if the sides of D do not intersect and are not asymptotic, we call tex2html_wrap_inline1031 a Schottky group of rank n. The space of such groups (modulo conjugation) has real dimension 4+d(nd+2n-6). Namely, by [4, Lemma 3.2.2,], a loxodromic element with given fixed points has tex2html_wrap_inline1059 real parameters left. Every fixed point contributes 2d-1 real parameters, and three fixed points can be normalized by Cartan's angular invariant (see e.g. [7, §7,]). The limit set

displaymath986

of such a group is closed and totally disconnected (i.e. a Cantor set) (see e.g. [21, Theorem 12.1.21,]).

We consider a family tex2html_wrap_inline1065 of Schottky groups with generators tex2html_wrap_inline1067 , depending tex2html_wrap_inline959 on t, i.e.\ tex2html_wrap_inline1073 with tex2html_wrap_inline1075 of class tex2html_wrap_inline959 . Note that the tex2html_wrap_inline1079 are all isomorphic to the free group on n generators (cf. [21, Theorem 12.1.19,]), hence there are canonical isomorphisms

displaymath987

We show that smooth deformations of Schottky groups are quasiconformally stable in the following sense.

   thm110

Note that the boundary tex2html_wrap_inline1097 of complex hyperbolic space can be identified with the one-point compactification of the Heisenberg group tex2html_wrap_inline1099 , see e.g. [7, §2.1,], [13] or the next section. The Heisenberg metric on tex2html_wrap_inline1101 is also defined in the next section.

Because two Schottky groups of the same rank can clearly be connected by a smooth family of such groups, we have the following corollary.

cor123

In particular, the limit sets tex2html_wrap_inline1117 and tex2html_wrap_inline1119 are quasiconformally equivalent: tex2html_wrap_inline1121 . Because the image of a Schottky group under a homomorphism close to the identity is again a Schottky group of the same rank, the quasiconformal stability expressed by Theorem 1.1 includes quasiconformal stability in the sense of Bers.

In real hyperbolic space tex2html_wrap_inline1123 , the following is known. For d=3, members of a continuously parametrized family of finitely generated discrete groups are canonically isomorphic to each other, [12, Theorem 3,]. Again for d=3, using the generalized tex2html_wrap_inline1129 -lemma of holomorphic motions, one can show: If tex2html_wrap_inline1131 is a holomorphic family of finitely generated Kleinian groups such that no new parabolic elements are created as z varies in the unit disk, then the tex2html_wrap_inline1135 are canonically quasiconformally conjugate on their limit sets, [1]. In fact, the equivariant version of the generalized tex2html_wrap_inline1129 -lemma by Earle, Kra and Krushkal' [6] shows that the groups tex2html_wrap_inline1135 are quasiconformally conjugate on tex2html_wrap_inline1141 .

The method used in the present paper yields analogous results for Schottky groups in tex2html_wrap_inline1123 for tex2html_wrap_inline1145 . Use the ball tex2html_wrap_inline1147 as a model for real hyperbolic space and on its boundary tex2html_wrap_inline1097 use the euclidean (chordal) metric to define quasiconformality. In the interior, it does not matter whether one uses the hyperbolic or the euclidean metric to define quasiconformality, because these metrics are conformally equivalent.

  thm142

As a corollary, Schottky groups of equal rank n (acting on tex2html_wrap_inline1171 , tex2html_wrap_inline1145 ) are quasiconformally conjugate. The hyperbolic quotient manifolds tex2html_wrap_inline1175 and tex2html_wrap_inline1177 are quasiconformally equivalent. By [17, VIII.D.1,], for d=3 these manifolds are `handlebodies of genus n'.

By the known rigidity of quaternionic hyperbolic space and the Cayley plane, analogous results for Schottky groups on these spaces cannot hold. Namely, as P. Pansu has shown, every quasiconformal map on the boundary of quaternionic hyperbolic space or the Cayley plane is the extension of an isometry (Corollary 11.2 and Proposition 11.5 in [20]). Thus, for the result to hold, the space of Schottky groups modulo conjugation by isometries would have to reduce to a point, which of course is not the case. However, in the quaternionic and Cayley cases our construction still yields an equivariant homeomorphism of hyperbolic space and its boundary which is a diffeomorphism in the interior.

In the general case of negatively curved groups, Martin [16] has shown the existence of a quasisymmetric conjugacy on the limit set.

Section 2 contains introductory material and some lemmas which are used in section 3 to proof the theorems. It is a pleasure for us to thank Martin Reimann for many helpful discussions.


next up previous
Next: Notation and preliminaries Up: Deformation of Schottky groups Previous: Deformation of Schottky groups

Robert Miner
Wed Jan 22 10:50:29 CST 1997