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  "body": "\n## Statement\n\nLet $\\mathbb{D}$ be the [[unit disc|8G5ABXRK85]], and let $f \\colon \\mathbb{D} \\to \\C$ be a [[univalent function|R91E83SDBD]].\nThen the image $f(\\mathbb{D})$ contains the open disc with centre $f(0)$ and radius $\\abs{f'(0)}/4$.\n\n## Remarks\n\nAfter replacing $f$ by $(f - f(0))/f'(0)$, one may assume $f(z) = z + a_2 z^2 + \\cdots$ is in the class $S$.\nIf $w \\notin f(\\mathbb{D})$, then $g = wf/(w - f)$ is again in $S$, and its second coefficient is $a_2 + 1/w$.\nBieberbach's inequality $\\abs{a_2} \\le 2$ for functions in $S$, which follows from the [[Grönwall area theorem|BYZDAZNHP4]], gives $\\abs{a_2 + 1/w} \\le 2$ and $\\abs{a_2} \\le 2$, hence $\\abs{1/w} \\le 4$, that is, $\\abs{w} \\ge 1/4$.\nThe constant $1/4$ is sharp: the [[Koebe function|EZQFWKF03Q]] $k(z) = z/(1-z)^2$ is in $S$ and omits the value $-1/4$.\nInjectivity is necessary: $f(z) = (e^{Nz} - 1)/N$ has $f(0) = 0$ and $f'(0) = 1$, but omits the value $-1/N$, which is close to $0$ for large $N$.\n\n## Explanations\n\n### L1 human\n\nA univalent function on the unit disc cannot squeeze its image too much near the image of the centre.\nAfter normalising so that $f(0) = 0$ and $f'(0) = 1$, the image always contains the disc of radius $1/4$ around $0$.\nThe Koebe function shows that a quarter is the best one can say.\n\n### L2 human\n\nThe theorem is the basic covering theorem of univalent function theory.\nIt gives the distance estimate $\\frac{1}{4}\\abs{f'(z)}(1 - \\abs{z}^2) \\le \\operatorname{dist}(f(z), \\partial f(\\mathbb{D})) \\le \\abs{f'(z)}(1 - \\abs{z}^2)$ for univalent $f$, where the upper bound comes from the Schwarz lemma.\nThis compares the hyperbolic metric of a simply connected domain with the reciprocal of the distance to its boundary, up to a factor $4$.\nTogether with the Koebe distortion theorem, it gives the compactness of the class $S$ in the topology of locally uniform convergence.\nFor maps that need not be injective, [[Bloch's theorem|KW31KDX7TB]] gives a much weaker covering result.\n",
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