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  "body": "\n## Summary\n\nThe fractional Fourier transform is a family of unitary operators $\\mathcal{F}_\\alpha$ on $L^2(\\R)$, indexed by an angle $\\alpha$.\nHere $\\mathcal{F}_0$ is the identity and $\\mathcal{F}_{\\pi/2}$ is the [[Fourier transform|DPVM34ADZV]].\nThe family is a group: $\\mathcal{F}_\\alpha \\mathcal{F}_\\beta = \\mathcal{F}_{\\alpha + \\beta}$, so the Fourier transform has a square root, a cube root, and so on.\nIn the time-frequency plane, $\\mathcal{F}_\\alpha$ acts as a rotation by the angle $\\alpha$.\nIt is used in optics and signal processing to analyse chirps and other signals whose frequency changes in time.\n\n## Explanations\n\n### L1 human\n\nDoing the Fourier transform four times gives back the original function, so it behaves like a rotation by a quarter turn.\nThe fractional Fourier transform fills in the rotations by all the other angles.\nA signal is then seen from a direction between pure time and pure frequency.\nFor example, the Gaussian $e^{-x^2/2}$ is unchanged by every $\\mathcal{F}_\\alpha$, just as a round disc is unchanged by every rotation.\n",
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