In physics intros to 2d conformal field theory, people often talk about the "group of conformal transformations". Of course, that's not a group but rather a pseudo-group... that's not what my question is about.
I care about a certain group $G$, which I'll define in a moment. My question is: Is it the trivial group?
Fix, once and for all, a small number $\varepsilon$.
For $j\in\{1,2,3\}$,
let $D_j\subset \mathbb C$ be the disc of radius $1+j\varepsilon$ around the origin of the complex plane, so that
$D_1\subset D_2 \subset D_3\subset \mathbb C$.
I'll define my group $G$ by generators and relations:
Generators:
The set $X$ of generators of $G$ is the set of injective holomorphic maps $f:D_2\to D_3$ satisfying $D_1\subset f(D_2)$
For $f\in X$, I'll write $[f]$ for the corresponding generator of $G$.Relations:
Note that if $f,g\in X$, then $f\circ g$ is defined on $D_1$.
Whenever $f,g,h\in X$ satisfy $f|_{D_1}=(g\circ h)|_{D_1}$, then we declare $[f] = [g][h]$ in $G$.
Is $G$ trivial?
What I know so far about this problem:
I know a bunch of elements of $X$ that are trivial in $G$.
Here's a proof that for any (small enough) scalar $a$, the element $(z\mapsto z+a)\in X$ is trivial in $G$.
Proof. Consider the map $D_3\to\mathbb CP^1$ given by $z\mapsto \exp\big(2\pi i z\big/\frac a2\big)$.
Pull back the Lie algebra of holomorphic vector fields on $\mathbb CP^1$ along that map to produce a subalgebra of the Lie algebra of vector fields on $D_3$ isomorphic to $\mathfrak{sl}(2,\mathbb C)$.
By small-time-exponentiating these vector fields, one gets an embedding $U\hookrightarrow X$ from some neighbourhood $U$ of the origin of $SL(2,\mathbb C)$ into the set $X$ of generators of $G$.
The universal group associated to the local Lie group $U$ is $SL(2,\mathbb C)$.
So one gets a homomorphism $\psi:SL(2,\mathbb C)\to G$.
The one-parameter group $t\mapsto (z\mapsto z+at)\in G$ is the composite of a certain one-parameter group $\gamma:\mathbb R\to SL(2,\mathbb C)$ with the homomorphism $\psi$.
Since $\gamma$ is not injective, neither is the composite $\psi\circ \gamma$.
The map $(z\mapsto z+a)$ is in the kernel. q.e.d.