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  "body": "\n## Summary\n\nClifford analysis extends complex analysis to $\\R^n$ by letting functions take values in a [[Clifford algebra|A38B1QFK20]].\nIts central objects are the [[monogenic functions|646PNPT1R6]], the functions annihilated by a [[Dirac operator|3DXGJTEQZH]].\nThe square of the Dirac operator is the Laplacian up to sign.\nSo the theory refines harmonic analysis, as holomorphic functions refine harmonic functions in the plane.\nIt has a Cauchy integral formula, Taylor and Laurent series, and links to singular integrals, spin geometry and representation theory.\nIt grew out of [[quaternionic analysis|SAT7ST5WP7]], which is closely related to its low-dimensional cases.\n\n## Explanations\n\n### L1 human\n\nIn the plane, holomorphic functions are the solutions of the Cauchy–Riemann equations, a first-order system whose \"square\" is the Laplace equation.\nIn higher dimensions there is no such system with complex numbers alone.\nA Clifford algebra supplies anticommuting units $e_1, \\ldots, e_n$ with $e_j^2 = -1$, and with them the operator $\\sum_j e_j \\partial_{x_j}$ squares to minus the Laplacian.\nFunctions killed by this operator behave much like holomorphic functions: they have an integral formula, power series, and a maximum principle.\n",
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