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  "body": "\n## Definition\n\nLet $X$ be a set, let $f \\colon X \\to X$ be a [[function|0EPAT51DXQ]], and let $\\lambda \\in \\C$.\n*Schröder's equation* for $f$ and $\\lambda$ is the [[functional equation|SRAN4EKWS0]]\n$$\\Psi(f(x)) = \\lambda \\, \\Psi(x) \\quad \\text{for all } x \\in X,$$\nin which the unknown is a function $\\Psi \\colon X \\to \\C$.\nIn the main case, $X$ is a neighbourhood of a [[fixed point|R6QVS6P21N]] $0$ of a holomorphic map $f$, and $\\lambda = f'(0)$.\nThen one asks for a holomorphic $\\Psi$ with $\\Psi(0) = 0$ and $\\Psi'(0) = 1$.\n\n## Remarks\n\nExample: $f(x) = x^2 + 2x$ on $X = (-1, \\infty)$, with $\\lambda = 2$.\nThe fixed point is $0$, and $f'(0) = 2$.\nThe function $\\Psi(x) = \\log(1 + x)$ is a solution with $\\Psi(0) = 0$ and $\\Psi'(0) = 1$, since $\\Psi(f(x)) = \\log\\big((1+x)^2\\big) = 2 \\log(1 + x)$.\n\nNon-example: for the same $f$, the function $\\Psi(x) = x$ is not a solution, since $f(x) = x^2 + 2x \\ne 2x$ for $x \\ne 0$.\n\nIf $\\Psi$ is invertible, the equation says $f = \\Psi^{-1} \\circ (\\lambda \\Psi)$, so $f^n = \\Psi^{-1} \\circ (\\lambda^n \\Psi)$ for every $n \\ge 0$.\nThe function $\\Psi$ is called a Schröder function of $f$.\nIf $\\Psi$ is a solution, so is $c \\Psi$ for every constant $c$; the condition $\\Psi'(0) = 1$ fixes this freedom.\n",
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