Gromov boundary

In mathematics, the Gromov boundary of a δ-hyperbolic space (especially a hyperbolic group) is an abstract concept generalizing the boundary sphere of hyperbolic space. Conceptually, the Gromov boundary is the set of all points at infinity. For instance, the Gromov boundary of the real line is two points, corresponding to positive and negative infinity.

The Cayley graph of a free group with two generators. This is a hyperbolic group whose Gromov boundary is a Cantor set. Hyperbolic groups and their boundaries are important topics in geometric group theory, as are Cayley graphs.
The (6,4,2) triangular hyperbolic tiling. The triangle group corresponding to this tiling has a circle as its Gromov boundary.

Definition

There are several equivalent definitions of the Gromov boundary of a geodesic and proper δ-hyperbolic space. One of the most common uses equivalence classes of geodesic rays.[1]

Pick some point of a hyperbolic metric space to be the origin. A geodesic ray is a path given by an isometry such that each segment is a path of shortest length from to .

Two geodesics are defined to be equivalent if there is a constant such that for all . The equivalence class of is denoted .

The Gromov boundary of a geodesic and proper hyperbolic metric space is the set is a geodesic ray in .

Topology

It is useful to use the Gromov product of three points. The Gromov product of three points in a metric space is . In a tree (graph theory), this measures how long the paths from to and stay together before diverging. Since hyperbolic spaces are tree-like, the Gromov product measures how long geodesics from to and stay close before diverging.

Given a point in the Gromov boundary, we define the sets there are geodesic rays with and . These open sets form a basis for the topology of the Gromov boundary.

These open sets are just the set of geodesic rays which follow one fixed geodesic ray up to a distance before diverging.

This topology makes the Gromov boundary into a compact metrizable space.

The number of ends of a hyperbolic group is the number of components of the Gromov boundary.

Properties of the Gromov boundary

The Gromov boundary has several important properties. One of the most frequently used properties in group theory is the following: if a group acts geometrically on a δ-hyperbolic space, then is hyperbolic group and and have homeomorphic Gromov boundaries.[2]

One of the most important properties is that it is a quasi-isometry invariant; that is, if two hyperbolic metric spaces are quasi-isometric, then the quasi-isometry between them gives a homeomorphism between their boundaries.[3][4] This is important because homeomorphisms of compact spaces are much easier to understand than quasi-isometries of spaces.

Examples

Generalizations

Visual boundary of CAT(0) space

For a complete CAT(0) space X, the visual boundary of X, like the Gromov boundary of δ-hyperbolic space, consists of equivalence class of asymptotic geodesic rays. However, the Gromov product cannot be used to define a topology on it. For example, in the case of a flat plane, any two geodesic rays issuing from a point not heading in opposite directions will have infinite Gromov product with respect to that point. The visual boundary is instead endowed with the cone topology. Fix a point o in X. Any boundary point can be represented by a unique geodesic ray issuing from o. Given a ray issuing from o, and positive numbers t > 0 and r > 0, a neighborhood basis at the boundary point is given by sets of the form

The cone topology as defined above is independent of the choice of o.

If X is proper, then the visual boundary with the cone topology is compact. When X is both CAT(0) and proper geodesic δ-hyperbolic space, the cone topology coincides with the topology of Gromov boundary.[6]

Cannon's Conjecture

Cannon's conjecture concerns the classification of groups with a 2-sphere at infinity:

Cannon's conjecture: Every Gromov hyperbolic group with a 2-sphere at infinity acts geometrically on hyperbolic 3-space.[7]

The analog to this conjecture is known to be true for 1-spheres and false for spheres of all dimension greater than 2.

Notes

References

  • Bridson, Martin R.; Haefliger, André (1999), Metric spaces of non-positive curvature, Grundlehren der Mathematischen Wissenschaften, vol. 319, Springer-Verlag, ISBN 3-540-64324-9, MR 1744486
  • Cannon, James W. (1994), "The combinatorial Riemann mapping theorem", Acta Mathematica, 173 (2): 155–234, doi:10.1007/bf02398434
  • Champetier, C. (1995), "Propriétés statistiques des groupes de presentation finie", Advances in Mathematics, 116: 197–262, doi:10.1006/aima.1995.1067
  • Coornaert, M.; Delzant, T.; Papadopoulos, A. (1990), Géométrie et théorie des groupes. Les groupes hyperboliques de Gromov, Lecture Notes in Mathematics (in French), vol. 1441, Springer-Verlag, ISBN 3-540-52977-2
  • de la Harpe, Pierre; Ghys, Etienne (1990), Sur les groupes hyperboliques d'après Mikhael Gromov (in French), Birkhäuser
  • Gromov, M. (1987), "Hyperbolic groups", in S. Gersten (ed.), Essays in group theory, Math. Sci. Res. Inst. Publ., vol. 8, Springer, pp. 75–263
  • Kapovich, Ilya; Benakli, Nadia (2002), "Boundaries of hyperbolic groups", Combinatorial and geometric group theory, Contemporary Mathematics, vol. 296, pp. 39–93
  • Roe, John (2003), Lectures on Coarse Geometry, University Lecture Series, vol. 31, American Mathematical Society, ISBN 978-0-8218-3332-2
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