Notation: B(a, r) = \{z \in \mathbb{C}: |z - a| < r \}, B = B(0, 1), \mathbb{S} is the Riemann sphere.
Let \mathcal{S} be the collection of all injective analytic function f on the unit disk with f(0) = 0 and f'(0) = 1. We know from the Open Mapping Theorem that f(B) must contain a disk B(0, r_f). For the class \mathcal{S}, there is a universal r > 0 such that f(B) contains B(0, r) for all f \in S.
Theorem (Koebe's 1/4-Theorem). If f \in \mathcal{S} then B(0, 1/4) \subseteq f(B).
We need to the following result, which is of independent interest.
Theorem (The Area Theorem). Let g: B \backslash \{0\} \rightarrow \mathbb{C} be an injective analytic function with Laurent series expansion at 0 g(z) = \frac{1}{z} + c_0 + c_1 z + c_2 z^2 + \cdots. Then \sum_{n = 1}^\infty n|c_n|^2 \leq 1.
Proof: Note that g is a conformal equivalence between B and g(B) \subseteq \mathbb{S} and \infty \in g(B). Fix any 0 < r < 1. Consider U_r = \mathbb{S} \backslash \overline{B(0, r)}. It is an open set in \mathbb{C} with boundary \gamma parametrized by \theta \mapsto h(re^{i\theta}) where \theta runs from 2\pi to 0. The area of U_r is given by \begin{align*}
\mathrm{Area}(U_r) &= \frac{1}{2i}\int_\gamma \bar{w} dw = -\frac{1}{2i} \int_0^{2\pi} \overline{h(re^{i\theta})}h'(re^{i\theta})ire^{i\theta}d\theta \\
&= - \frac{1}{2i} \int_0^{2\pi} [ \left(-\frac{1}{r^2} + |c_1|^2 + 2|c_2|^2 + 3|c_3|^2 + \cdots \right)r^2 \\
&{\,\,} + \textrm{ terms with nonzero integral powers of } e^{i\theta} ] \\
&= \pi \left(\frac{1}{r^2} - \sum_{n = 1}^\infty n|c_n|^2 r^2 \right).
\end{align*}
Since area is always non-negative, let r \rightarrow 1 and we are done.
Proof of Koebe's Theorem: Let f \in \mathcal{S}. Then f omits some w_0 \in \mathbb{C} (or otherwise f^{-1} is a bounded entire function, which is then constant by Liouville's Theorem, contradiction), so h = 1/f omits 0 and 1/w_0. Observe that the Taylor series of f at 0 takes the form f(z) = z + a_2 z^2 + a_3 z^3 + \cdots, so h(z) = \frac{1}{z + a_2 z^2 + \cdots} = \frac{1}{z} + c_0 + c_1 z + c_2 z^2 + \cdots. Let z_0 = 0 \textrm{ or } 1/w_0. We have g(z) = \frac{1}{h(z) - z_0} = \frac{z}{1 + (c_0 - z_0)z + c_1 z^2 + \cdots} = z + (z_0 - c_0)z^2 + \cdots. In particular, g(0) = 0 and g'(0) = 1. Also note that g is injective. Thus g \in \mathcal{S}.
We claim that there exists some u \in \mathcal{S} such that u(z)^2 = g(z^2). Since g is injective and g(0) = 0, the analytic function g(z)/z omits 0 on B, we can find some analytic function \varphi on B such that \varphi(z)^2 = g(z)/z and \varphi(0) = 1. Let u(z) = z\varphi(z^2). Then g(z^2) = z^2 \cdot g(z^2)/z^2 = z^2\varphi(z^2)^2 = u(z)^2. Since \varphi(0) = 1 and \varphi'(0) = \frac{1}{2}(g(z)/z)^{-1/2}\frac{d}{dz}(g(z)/z)|_{z = 0} = \frac{1}{2} (z_0 - c_0), u(z) = z\varphi(z^2) = z + \frac{1}{2}(z_0 - c_0)z^3 + \cdots. Hence u(0) = 0 and u'(0) = 1. To show that u \in \mathcal{S} it remains to prove that u is injective. Suppose u(z) = u(w). Then g(z^2) = g(w^2). By injectivity of g, z^2 = w^2 or z = \pm w. If z = -w, then u(w) = u(z) = u(-w) = -u(w), so g(w^2) = u(w)^2 = 0 and w^2 = 0 by injectivity of g again, i.e. w = z = 0. In any case we have z = w.
Now consider the Laurent expansion of 1/u at 0, we have \frac{1}{u(z)} = \frac{1}{z + \frac{1}{2}(z_0 - c_0)z^3 + \cdots} = \frac{1}{z}(1 - \frac{1}{2}(z_0 - c_0)z^2 + \cdots) = \frac{1}{z} - \frac{1}{2}(z_0 - c_0)z + \cdots. By the Area Theorem, |-\frac{1}{2}(z_0 - c_0)| \leq 1, or |z_0 - c_0| \leq 2. Therefore |1/w_0| \leq |1/w_0 - c_0| + |0 - c_0| \leq 2 + 2 = 4, or |w_0| \geq 1/4. It follows that \mathbb{C} \backslash f(B) \subseteq \{w \in \mathbb{C}: |w| \geq 1/4\}, so B(0, 1/4) \subseteq f(B). QED.
Reference:
Andersson - Topics in Complex Analysis
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