Conformal map from a lune to the unit disc in $\mathbb{C}$ On my complex analysis prelim this morning I was asked to give a conformal map from the region $L=\{z\in\mathbb{C}:|z-i|<\sqrt{2},|z+i|<\sqrt{2}\}$, a lune with vertices at $-1$ and $1$ to the unit disc $\mathbb{D}=\{z:|z|<1\}$.  I tried to send $L$ to the upper half plane by the Möbius transform sending $(-1,0,1)$ to $(0,i,\infty)$.  Then I composed with the Cayley transformation to get to the unit disc.
My question is: does my first map do what I want it to(presuming I calculated it correctly)?
To be brief, does the Möbius transform which takes $(-1,0,1)$ to $(0,i,\infty)$ send $L$ to the upper half plane?
 A: Just to put everyone's answers together and finish things off, $f:z\mapsto
\frac{1+z}{1-z}$ sends $-1$ to $0$ and $1$ to $\infty$.  Because $f:(-1,1)\to(0,+\infty)$, the sector is symmetric about $\mathbb{R}^+$.  Since $f$ is conformal, it preserves the right angle at which the circles cross, so the sector has a right angle. Therefore, $g:z\mapsto z^2$ maps the sector to the right half-plane.  Then, $h:z\mapsto\frac{z-1}{z+1}$ maps the right half-plane to the unit disk. Thus,
$$
h\circ g\circ f:z\mapsto\frac{2z}{1+z^2}
$$
should map the given lune to the unit disk.
A: Theo is right.  For a general lune: First apply a linear fractional transformation mapping the two corners (vertices, horns, whatever you call them) to $0$ and $\infty$.  The result is a sector.  Then apply a power to get a half-plane.  Then appy a linear fractional transformation to get a disk.
A: Your map sending $(-1,0,1)$ to $(0,i,\infty)$ is given by $i = e^{i\pi/2}$ times the cross ratio $[z,0,-1,1] = \frac{z+1}{z - 1} : \frac{1}{-1}$, so it is $$\tilde{\phi}(z) =  e^{i\pi/2}\cdot \frac{1+z}{1-z}.$$
It is easy to see geometrically (or by a direct calculation) that $\tilde\phi(L)$  is the quadrant $\{z:\,\operatorname{Im}{z} \gt |\operatorname{Re}{z}|\}$ since the circles $|z-i|=\sqrt{2}$ and $|z+i|=\sqrt{2}$ are sent to the lines $\{\operatorname{Im}{z} = \operatorname{Re}{z}\}$ and $\{\operatorname{Im}{z} = -\operatorname{Re}{z}\}$. Note that the angles at the vertices of the lune are equal to $\pi/2$.
It is more convenient to work with $\displaystyle\phi(z) = e^{i\pi/4}\cdot \frac{1+z}{1-z}$ which sends $L$ to the quadrant $\{z:\operatorname{Re}{z}, \, \operatorname{Im}{z}\gt 0\}$, then square to get to the upper half plane and apply the Cayley-transfom
$\displaystyle\kappa(z) = \frac{z-i}{z+i}$ to get to the unit disk.
The solution to your problem then is $\kappa((\phi(z))^2)$, which you can compute yourself if needed.

The general procedure is succinctly explained in GEdgar's answer.
