Solution.
D is the unit of two circles which intersect at i and −i at an angle of 2π. First, we translate so one of the intersection points is at the origin:
φ1:D→Ω1=D+i,φ1(z)=z+i.
Next, we send the other intersection point 2i to ∞ in a symmetric way. More specifically, we want 0↦0, i↦i, and 2i↦∞, so we get
φ2:Ω1→Ω2,φ2(z)=2i−ziz.
Observe that
φ2(z)=∣2i−z∣2iz(−2i−z)=∣2i−z∣22z−i∣z∣2=∣2i−z∣22Rez+i(∣2i−z∣22Imz−∣z∣2).
In other words, because D+i was symmetric about Rez=0, it follows that Ω2 is also symmetric about Rez=0. Since angles are preserved by conformal mappings, we see that the circles are mapped to half-lines containing 0 which intersect at an angle of 2π. Again by symmetry, we see that Ω2={4π<Argz<43π}, where we take the standard branch (0,2π). After the rotation
φ3:Ω2→Ω3={0<Argz<2π},φ3(z)=e−iπ/4z,
we get the first quadrant. Thus, we can complete the problem with
φ4φ5:Ω3→Ω4=H,:Ω4→Ω5=D,φ4(z)=z2φ5(z)=z+iz−i,
so the desired conformal mapping is φ5∘⋯∘φ1.