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  "body": "\n## Summary\n\nA unitary representation of a [[topological group|92700QAB5Y]] $G$ is a homomorphism from $G$ to the [[unitary operators|MM0EJ2GDE4]] on a [[Hilbert space|HM2HHE3J51]].\nIt must be continuous in the strong operator topology.\nIt is the kind of [[group representation|WYGRXCG2RN]] used for infinite groups in analysis and physics, because unitary operators preserve lengths and angles.\nHarmonic analysis on a locally compact group is largely the study of its unitary representations.\nIn quantum mechanics, symmetry groups act on state spaces in this way.\n\n## Explanations\n\n### L1 human\n\nA unitary operator is a rotation of a possibly infinite-dimensional space: it keeps all lengths and angles.\nA unitary representation assigns such a rotation to each element of a group, so that the product of two elements goes to the composition of their rotations.\nFor example, the real line acts on the space $L^2(\\R)$ of square-integrable functions by shifting: the number $t$ sends $f$ to the function $x \\mapsto f(x - t)$.\nShifting does not change the integral of $\\abs{f}^2$, so each shift is unitary, and shifting by a small amount changes $f$ only a little.\n",
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