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  "body": "\n## Definition\n\nLet $P$ be a monic [[polynomial|1G0B73WPX8]] of degree $d \\ge 2$ whose filled Julia set $K$ is connected.\nLet $\\overline{\\mathbb{D}}$ be the closed unit disc.\nBy [[Böttcher's theorem|YBBDYHBADD]] there is a unique [[conformal map|0YYT36R4YD]] $\\varphi \\colon \\C \\setminus K \\to \\C \\setminus \\overline{\\mathbb{D}}$ with $\\varphi(z)/z \\to 1$ as $z \\to \\infty$.\nIt satisfies $\\varphi(P(z)) = \\varphi(z)^d$.\nFor $\\theta \\in \\R/\\Z$, the *external ray of angle* $\\theta$ is\n$$R_\\theta = \\varphi^{-1}\\big(\\set{r e^{2\\pi i \\theta} : r \u003e 1}\\big).$$\nThe ray $R_\\theta$ *lands* at $z_0 \\in \\partial K$ if $\\varphi^{-1}(r e^{2\\pi i \\theta}) \\to z_0$ as $r \\to 1^+$.\n\n## Remarks\n\nThe relation $\\varphi \\circ P = \\varphi^d$ gives $P(R_\\theta) = R_{d\\theta}$.\nExample: for $P(z) = z^2$, $K$ is the closed unit disc and $\\varphi$ is the identity.\nSo $R_\\theta$ is the half-line $\\set{r e^{2\\pi i \\theta} : r \u003e 1}$, and it lands at $e^{2\\pi i \\theta}$.\nNon-example: for $P(z) = z^2$, the spiral $\\set{r e^{2\\pi i (\\theta + \\log r)} : r \u003e 1}$ is not an external ray, since $\\varphi$ maps it to a curve whose angle varies.\nDouady and Hubbard showed that every ray with a rational angle lands, at a periodic or preperiodic point of the [[Julia set|5M4S7P04GR]].\nFor the [[quadratic family|WDZFV2ACXR]], external rays of the Mandelbrot set are defined in the same way, with the conformal map from its complement onto $\\C \\setminus \\overline{\\mathbb{D}}$.\n",
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