In dynamics, we have the notion of a "hyperbolic set" for a diffeomorphism $f:M\to M$ of a Riemannian manifold. I am trying to connect this to my existing ideas surrounding the term "hyperbolic". To my understanding, $M$ itself need not be a hyperbolic manifold$^*$, but maybe there is some more distant connection$^{**}$ at work?
$^*$Consider the action of $\begin{pmatrix}2&1\\1&1\end{pmatrix}$ on the torus.
$^{**}$Heh
[EDIT] Someone wanted to know what a hyperbolic set was so I'm adding the definition here. Let $M$ be a Riemannian manifold and let $f:M\to M$ be a diffeomorphism. Then $\Lambda \subset M$ is hyperbolic if there are constants $C> 0$ and $\lambda \in (0,1)$ such that for every $x\in \Lambda$, we can write $T_xM = E^u(x) \oplus E^s(x)$. We require that $\|df^n_x v\| \le C\lambda^n \|v\|$ for $v\in E^s(x)$ and $n\ge 0$, $\|df^{-n}_x v\| \le C\lambda^n \|v\|$ for $v\in E^u(x)$ and $n\ge 0$, $df_x(E^u(x)) = E^u(f(x))$, and $df_x(E^s(x)) = E^s(f(x))$.
In English, we have expanding and contracting directions. Standard example is, give me some $A\in GL_n(\mathbb{Z})$ with no eigenvalues on the unit circle. It'll induce an automorphism of the torus $\mathbb{R}^n/\mathbb{Z}^n$. Then $\mathbb{T}^n$ is a hyperbolic set with respect to this automorphism, with the expanding directions being the sum of eigenspaces with eigenvalue $> 1$, and the contracting directions being the sum of eigenspaces with eigenvalue $< 1$.