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  "body": "\n## Summary\n\nThe classical orthogonal polynomials are the three families of Jacobi, Laguerre and [[Hermite polynomials|MGACY98E9H]].\nThey include special cases such as the Gegenbauer, Legendre and [[Chebyshev polynomials|M6EAR1JHPP]].\nEach family is orthogonal for a weight on an interval.\nThe weights are of beta type on $(-1, 1)$, of gamma type on $(0, \\infty)$, and Gaussian on $\\R$.\nThey are the only orthogonal polynomial families that are eigenfunctions of a second-order differential operator, and they have Rodrigues formulas and explicit recurrences.\nThey are the basic tools of approximation, Gaussian quadrature, and separation of variables in mathematical physics.\n\n## Explanations\n\n### L1 human\n\nTwo polynomials are orthogonal for a weight when the integral of their product times the weight is zero, like perpendicular vectors.\nFor a given weight, the Gram–Schmidt process applied to $1, x, x^2, \\dots$ gives one orthogonal polynomial of each degree.\nFor three kinds of weight this produces families with especially nice formulas, and these are the classical ones.\nFor example, the weight $e^{-x^2}$ on the whole line gives the Hermite polynomials $1$, $2x$, $4x^2 - 2$, and so on.\n",
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