Here is another possibility to find a bijective conformal mapping from the complex plane minus the closed unit disk, the segment $[-2, -1]$, and $[1, \infty)$ onto the unit disk.
We use the transformation $ \frac{1}{z} $ that you wanted. This maps your original region to the interior of the unit disk minus the segments $[-1, -1/2]$ and $[0, 1]$ as you remarked.
We now use our good old friend $\frac{iz + i}{-z + 1} $ to map the region to the upper half-plane. This maps our region to: $ \mathbb{H} \setminus \left( i[0, 1/3] \cup i[1, \infty] \right)$ We rotate the plane by $ e^{-i\pi/2} $ to transform it to another half-plane minus the segments: $
\left( [0, 1/3] \cup [1, \infty] \right)
$. Squaring yields $
\mathbb{C} \setminus \left( (-\infty, 1/9] \cup [1, \infty) \right)
$.
We are almost done if we remember how $\sin(z)$ works. In my edition of Stein's complex analysis there is a nice composition which yields $\sin(z)$ on the section named "The Dirichlet problem in a strip ". In any case the following trasnformations are motivated by having seen this in Stein.
If we displace and dilate the region by using the transformation $\frac{9}{4}(z - 5/9) $: $
\mathbb{C} \setminus \left( (-\infty, -1] \cup [1, \infty) \right)
$. We now use Stein's trick and apply the $\arcsin(z)$ function, which maps the region to the infinite strip:
$
\{ -\pi/2 < \Re(z) < \pi/2 \}
$. Now we are almost done, we shift and rotate the strip using $ e^{i\pi/2}z + \pi i/2 $ to get: $
\{ 0 < \Im(z) < \pi \}
$. Take the exponential of this region to map it to the upper half-plane.
Finally, use once more our good old friend $ \frac{z - i}{z + i} $ to map the upper half-plane to the unit disk.