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  "body": "\n## Summary\n\nPoincaré's functional equation asks for a function $\\Psi$ with $\\Psi(\\lambda z) = f(\\Psi(z))$, where $f$ is a given holomorphic map with a [[fixed point|R6QVS6P21N]] at $0$ and $\\lambda = f'(0)$.\nIt is the inverse form of [[Schröder's equation|VTJV7JVJEA]]: if $\\Phi$ solves Schröder's equation and is invertible, then $\\Psi = \\Phi^{-1}$ solves Poincaré's equation.\nFor a repelling fixed point of an entire map, the solution extends to an entire function on all of $\\C$, the Poincaré function.\nPoincaré functions parametrise the dynamics of $f$ near the repelling point and are used to study Julia sets.\n\n## Explanations\n\n### L1 human\n\nSchröder's equation looks for a coordinate in which the map $f$ becomes multiplication by $\\lambda$.\nPoincaré's equation looks at the same change of coordinates in the other direction: it maps the simple picture, multiplication by $\\lambda$, onto the complicated one.\nFor $f(w) = w^2 + 2w$ and $\\lambda = 2$, the function $\\Psi(z) = e^z - 1$ works, since $f(e^z - 1) = e^{2z} - 1 = \\Psi(2z)$.\nFor the logistic map $f(w) = 4w(1 - w)$ and $\\lambda = 4$, the function $\\Psi(z) = \\sin^2 \\sqrt{z}$ works, by the double-angle formula.\n",
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