Near the beginning of the book A Primer on Mapping Class Groups it’s shown that the center of the fundamental group of a hyperbolic surface of finite volume must be trivial. I had a hard time understanding the proof until I got help from someone. There’s some important and basic stuff involved in it.
Let be a hyperbolic surface, not necessarily of finite volume (for now). So
is the quotient of
by a subgroup
of
acting freely and properly discontinuously, where
. What we’ll show is:
If not equal to the identity, and
is a subgroup of
which contains
and satisfies that every element of
commutes with
then
must be cyclic.
In other words such an exists only if it really must. I’ll say later how this implies the trivial center thing if
has finite volume.
So, fix our Suppose
commutes with
and isn’t the identity.
Fact numero uno: and
have the same fixed points in
Proof: Say is a fixed point of
Then
meaning that if
is a fixed point of
then so is
Remember from the classification of isometries that every isometry has zero (elliptic), one (parabolic), or two (hyperbolic) fixed points on the boundary, and nothing in
is elliptic. If we’re in the case that both
and
are hyperbolic, then say their fixed points are the reds and the blues respectively.

From the above, we know that sends fixed points of
to fixed points of
so it must send the red points to the red points. We want it to be that the red and blue points are actually the same. If not, then either
fixes three points, so is the identity, or
fixes three points and is the identity. But even in the latter case we must have that
is the identity. This follows from thinking about how any hyperbolic isometry is conjugate to the typical one:
This kind of reasoning shows that the fixed points of
and
are the same, with there not being much different when one (and hence both) are parabolic.
So, they have the same fixed points at infinity. The next observation is that this means and
leave invariant the same “copy of
“. In the case that they’re hyperbolic, it’s the geodesic joining the two fixed points. In the case that they’re parabolic, it’s any horocycle tangent to the fixed point.

Each of those is isometric to In the case of the vertical line geodesic in the upper half plane, the isometry with
is given by natural log, in the case of a horocycle, just think of one of the horocycles tangent to the point at infinity in the upper half plane, so a horizontal line. At height
that horocycle really is exactly
Fact numero dos: The as above gives rise to a group of isometries of
with its usual metric, which is cyclic.
Proof: As we saw above, each element of gives an isometry of
And this has to actually be a translation of
as opposed to a reflection or something. As usual you see this by thinking about the “typical” hyperbolic and parabolic isometries,
and
and knowing that really any hyperbolic and parabolic isometry behaves the same way since it’ll be conjugate to one of those.
So, gives a group of translations
It turns out we can pick an
so that
for all non-zero
If we weren’t able to do that, it would contradict the discreteness of
i.e. that it’s supposed to act freely and properly discontinuously. Now we want to prove that
generates the group. Fix any
assuming for now that
Choose the smallest
so that
If
is strictly greater than
then their difference satisfies
but
is in the group, which contradicts
being the smallest.

So and we conclude that the group is cyclic.
And that’s it! Since restricted to the geodesic or the horocycle is cyclic,
must actually be cyclic. Though you might have to think about that for a little bit.
So why does that mean the center of is trivial if
has finite volume? Well, if the center is nontrivial then it has some non-identity element
and everything in
commutes with
so
must be cyclic. But that means
is “too small” for
to be finite volume. For example, the fundamental regions might look like the following.

Each of those has infinite volume. And for the general case of any hyperbolic/parabolic isometry, you again just say it’s the same picture “up to conjugation”.
This kind of restriction on commuting elements can be thought of as support for the saying that the fundamental group of a hyperbolic surface has to be complicated. And this gives a way of seeing that the torus can’t be given a hyperbolic structure, without using the Gauss-Bonnet theorem, since the torus has fundamental group Since this is abelian (and not cyclic, regardless of what we think the volume should be) by what we’ve seen here it’s too simple for hyperbolic aspirations.