Geometric Analysis

15-Math-8002

Gromov Hyperbolicity


Department of

Mathematical

Sciences

This page is a work in progress! All information is subject to change (Last revised 23 January 2015)

Instructor Prof David A Herron
4514 French Hall, 556-4075
Office Hours
Mon 1:20-2:15,Wed & Fri 11:15-12:00, and by appt
E-mail me at David's e-address
My web page is at David's w-address



Basic Course Description

Geodesic triangles in the hyperbolic plane have the property that every point on a given side is at most distance two from one of the other sides, regardless of how big the triangle is. A Gromov hyperbolic metric space is a metric space with this thin triangles property. Amazingly, this simple definition leads to deep mathematics, particularly in relation to group theory. Gromov hyperbolic groups have good algebraic properties (for example, solvable word problem) and are "generic": if you pick a group at random, it will be Gromov hyperbolic.

Hyperbolic space \(\mathbb{H}^{n+1}\) has an $n$-sphere \(\mathbb{S}^{n}\) at infinity which has a conformal structure. This was used, for example, in the original proof of Mostow rigidity. Likewise, a Gromov hyperbolic space \(X\) has a boundary at infinity \(\partial_\infty X\) which carries a canonical topological (in fact, conformal) structure. However, unlike the usual sphere, this boundary will often have fractal like properties.

The aim of this course is to give an introduction to Gromov hyperbolic metric spaces and to explore some of the connections between the geometry of the boundary at infinity and quasiconformal function theory.

Here is a preliminary outline of topics that we intend to cover.

References

No textbook is required, but here are some helpful references.