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  "body": "\n## Summary\n\nA linear canonical transformation is an integral transform of functions on $\\R$ attached to a real $2 \\times 2$ matrix of determinant $1$.\nIt includes the [[Fourier transform|DPVM34ADZV]], the [[fractional Fourier transform|28VV812XWQ]], the Fresnel transform, scalings and multiplication by chirps as special cases.\nComposing two such transforms gives, up to a sign, the transform of the product matrix.\nSo they form a projective unitary representation of $SL(2, \\R)$, which is a genuine representation of the [[metaplectic group|8B0JM2YDE2]].\nIn optics it describes the propagation of light through lenses and free space in the paraxial approximation.\n\n## Explanations\n\n### L1 human\n\nA signal can be pictured in a plane with time along one axis and frequency along the other.\nLinear maps of this plane that keep areas and orientation are given by matrices $\\begin{pmatrix} a \u0026 b \\\\ c \u0026 d \\end{pmatrix}$ with $ad - bc = 1$.\nFor each such map there is a transform of signals that moves their picture in the plane accordingly.\nThe Fourier transform is the quarter-turn rotation, a scaling of time is a squeeze of the plane, and multiplying by $e^{i\\pi c t^2}$ is a shear.\n",
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