# Variant of the Riemann Mapping Theorem for $Conf(\mathbb H^2)$?

According to the Riemann mapping theorem it is possible to map a simply connected open subset $B \subset \mathbb C$ into any other $B' \subset \mathbb C$ by a (bi-)holomorphic mapping. Moreover, such a mapping is unique.

Now I'm interested in the related case of the infinite dimensional Lie group $Conf(\mathbb H^2)$ that maps the upper half plane to itself. The Lie group is locally isomorphic to $Diff(S^1)$ (I think... some details may vary), so it should be clear that there are subsets $B' \subset \mathbb H^2$ that cannot be mapped from $B$ by a $Conf(\mathbb H^2)$ transformation.

Specifically, I'm interested in some kind of intuition about the possible forms of allowed mappings as above, i.e. some "number" of possible images of such mappings. Clearly the answer will involve $Diff(S^1)$ in some important way...

In short:

-$Diff(\mathbb C)$ maps $B$ to any $B'$ in infinite number of possible ways

-$Conf(\mathbb C)$ maps $B$ to any $B'$ in a unique way

-$Conf(\mathbb H^2)$ maps $B$ to some subsets $B'$... but what kind of $B'$s??

I actually have in mind a way to "number" such maps, but there are probably much better mathematical expositions/proofs lying around somewhere...

EDIT: OK I just knew I should've stuck with infinite dimensional Lie algebras instead of Lie groups (as per Robert Bryant's comment below)... so here are some corrections (I'll leave the above stuff intact for the sake of my own public humiliation):

1) Yes indeed I meant a proper subset which is connected and simply connected

2) OK so the Riemann Mapping is unique up to $PSL(2;\mathbb R)$... didn't realize that!

3) So instead of "$Conf(\mathbb H^2)$" let's think about holomorphic vector fields on $\mathbb H^2$, e.g.

$V = \xi(z) \partial_z + \xi(\bar z) \partial_{\bar z}$.

As $Im(z) \to 0$, these tend to $\xi(x) \partial_x \in Vect(S^1)$ (the boundary of $\mathbb H^2$ is $S^1$). I think it's safe to say that there are flows at least for some $\xi$ such that the resulting mapping is a conformal transformation? That's what I meant by $Conf(\mathbb H^2)$, which was probably wrong in many ways...

So the question then applies to flows of $V$... I hope it's clearer now!

• You've got some things mixed up here. Even assuming, in stating the Riemann Mapping Theorem, that your notation '$B\subset \mathbb{C}$' means that $B$ is a proper subset of $\mathbb{C}$, you left out the 'connected' hypothesis (unless you include that in your definition of 'simply connected'), and even then, the mapping is never unique; it is only unique up to composition with an element of $Conf(B)\simeq \mathrm{PSL}(2,\mathbb{R})$. Similarly, you seem not to realize that $Conf(\mathbb{H}^2)$ is not infinite dimensional at all, but is, in fact, of dimension $3$. Try again? – Robert Bryant Mar 22 '13 at 18:10
• Ah... I could map $B \to \mathbb D \to B'$ and $\mathbb D$ is invariant under $PSL(2;\mathbb R)$. Silly me! Anyway, I edited the question. – H. Arponen Mar 22 '13 at 20:01
• Arponen: you did not edit your question sufficiently. Especially about "infinite-dimensional $Conf(H^2)$". I do not understand at all what is this. – Alexandre Eremenko Mar 23 '13 at 3:09
• Arponen: Also your definition of holomorphic vector fields is wrong. All in all, I do not think you have a real question here. Please read "how to ask" on MO FAQ. Voting to close. – Misha Mar 23 '13 at 3:30
• Eremenko: forget about $Conf(\mathbb H^2)$ but think of $Diff(S^1)$ instead and the corresponding Lie algebra $Vect(S^1)$ (or maybe it's better to denote it as $diff(S^1)$). Then expand $\xi$ as Fourier series. Misha: a holomorphic vector field isn't such that $\bar \partial \xi = 0$ when $\xi : \mathbb C \to \mathbb C$? OK maybe I got that wrong too. Just call it a "vector field" then. I'm currently too tired to completely edit the question. Close it if you will, I'll leave it up to the community. – H. Arponen Mar 23 '13 at 7:57

Anyway, to get to your question: It seems that, by $Conf(\mathbb{H}^2)$, you mean the (real) vector fields on $\mathbb{H}^2$ whose (local) flows are holomorphic. Such a vector field $X$ is the real part of a unique holomorphic vector field $Z$ of the form $$Z = h(z)\ \frac{\partial\ }{\partial z} = h(x+iy)\ \frac12\left(\frac{\partial\ }{\partial x}-i\frac{\partial\ }{\partial y}\right)$$ where $h$ is holomorphic in the upper half plane. People frequently write $Z$ when they mean $X = Z +\bar Z$, which is why some folks were confused by your expression for an element of $Conf(\mathbb{H}^2)$.
The problem with thinking of this infinite dimensional vector space as the Lie algebra of a Lie group is that most of these vector fields only define local flows on $\mathbb{H}^2$, not global ones, so they don't really generate automorphisms of $\mathbb{H}^2$. In fact, it's a theorem that the only ones that do are the ones for which
$$h(z) = a + bz + cz^2$$ where $a$, $b$, and $c$ are real numbers, and this is a Lie algebra isomorphic to ${\frak{sl}}(2,\mathbb{R})$. The flows that are generated in this way generate the Lie group of linear fractional transformations that carry $\mathbb{H}^2$ into itself, and this happens to be the group of automorphisms of $\mathbb{H}^2$ as a complex manifold.
Given this, it seems that, instead, you want $Conf(\mathbb{H}^2)$ to mean something else, namely the Lie algebra of vector fields of the above form in which $h$ is holomorphic on the entire complex plane $\mathbb{C}$ and real-valued on $\mathbb{R}$. In other words, $h$ should have its power series in $z$ have all real coefficients and have infinite radius of convergence. Then, indeed, $Conf(\mathbb{H}^2)$ injects into (but not onto) the Lie algebra $\frak{X}(\mathbb{R})$ of real analytic vector fields on $\mathbb{R}$.
By the way, if $B\subset\mathbb{C}$ is a connected and simply connected open subset, then the set of all holomorphic vector fields on $B$ will still be of the above form for some set of $h\in\mathcal{O}(B)$ (the holomorphic functions on $B$), but picking out the $3$-dimensional subalgebra whose flows generate the automorphisms of $B$ (which, by the Riemann Mapping Theorem, is a $3$-dimensional Lie subalgebra of this space) is, generally, a very difficult thing to do.
• Thanks Robert for yet another great explanation and my apologies to all for mildly flipping out like that and wasting everyone's time with a poorly laid out question... Anyway, the flows and specifically their actions on open sets as Ben McKay describes above are what I'm interested in. By the way Ben McKay (and Robert), what exactly do you mean by "finding invariants of the open sets"? Is it related to what Robert writes about the automorphisms of $B$? I can't see how the automorphisms are related to the problem... – H. Arponen Mar 25 '13 at 18:12