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  "body": "\n## Definition\n\nLet $n \\ge 2$ and let $\\Omega \\subseteq \\R^n$ be open.\nAn *integro-partial differential equation* on $\\Omega$ is an equation for an unknown function $u \\colon \\Omega \\to \\R$ (or $\\C$, or $\\R^m$) such that:\n\n1. at least one partial derivative of $u$ appears in it, and\n2. at least one integral of $u$, or of a derivative of $u$, with respect to one or more of the variables appears in it.\n\nA typical linear form is\n$$\\sum_{\\abs{\\alpha} \\le k} a_\\alpha(x) \\, \\partial^\\alpha u(x) + \\int_{\\Omega} K(x, y) \\, u(y) \\, dy = f(x), \\quad x \\in \\Omega,$$\nwith given coefficients $a_\\alpha$, kernel $K$ and right side $f$.\n\n## Remarks\n\nExample: let $J \\colon \\R \\to [0, \\infty)$ be even and integrable, and consider $\\partial_t u(x, t) = \\int_{\\R} J(x - y) \\big(u(y, t) - u(x, t)\\big) \\, dy$ on $\\R \\times (0, \\infty)$.\nWrite $\\hat J(\\omega) = \\int_{\\R} J(z) \\cos(\\omega z) \\, dz$.\nThen $u(x, t) = e^{(\\hat J(\\omega) - \\hat J(0)) t} \\cos(\\omega x)$ is a solution, because $\\int_{\\R} J(x - y) \\cos(\\omega y) \\, dy = \\hat J(\\omega) \\cos(\\omega x)$ for even $J$.\n\nNon-example: the heat equation $\\partial_t u = \\partial_x^2 u$ contains no integral of $u$, so it fails clause 2 and is a [[partial differential equation|GC5BDZ6QBC]].\nThe equation $x'(t) = \\int_0^t x(s) \\, ds$ has an unknown of one variable only, so it is an [[integro-differential equation|YRKW2KX2CW]] but not a partial one.\n",
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