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  "body": "\n## Statement\n\nLet $a \u003c b$ and let $K \\colon [a, b] \\times [a, b] \\to \\C$ be a [[continuous kernel|ZM5G144PZG]] that is [[Hermitian|2ZB3NFZ94T]]: $K(y, x) = \\overline{K(x, y)}$ for all $x, y$.\nLet $(\\varphi_n)_{n \\in N}$ be an orthonormal family of [[eigenfunctions|4NSACSWRJZ]] of $T_K \\varphi = \\int_a^b K(\\cdot, y) \\varphi(y) \\, dy$, with real nonzero eigenvalues $\\mu_n$.\nAssume that, for each nonzero eigenvalue, the $\\varphi_n$ with that eigenvalue form a basis of its eigenspace.\nThese eigenfunctions are continuous, since $\\varphi_n = \\mu_n^{-1} T_K \\varphi_n$.\nLet $h \\in L^2[a, b]$ and $f = T_K h$, that is,\n$$f(x) = \\int_a^b K(x, y) \\, h(y) \\, dy.$$\nThen for every $x \\in [a, b]$,\n$$f(x) = \\sum_{n \\in N} \\ip{f}{\\varphi_n} \\varphi_n(x) = \\sum_{n \\in N} \\mu_n \\ip{h}{\\varphi_n} \\varphi_n(x),$$\nwhere $\\ip{u}{v} = \\int_a^b u \\overline{v}$, and the series converges absolutely and [[uniformly|08VZ57PT26]] on $[a, b]$.\n\n## Remarks\n\nFor fixed $x$, the numbers $\\mu_n \\overline{\\varphi_n(x)}$ are the Fourier coefficients of the function $y \\mapsto \\overline{K(x, y)}$, so [[Bessel's inequality|0RBT5PB74K]] gives $\\sum_n \\mu_n^2 \\abs{\\varphi_n(x)}^2 \\le \\int_a^b \\abs{K(x, y)}^2 \\, dy \\le C$ for a constant $C$ independent of $x$.\nThe Cauchy–Schwarz inequality then bounds the tail $\\sum_{n \\ge m} \\abs{\\mu_n \\ip{h}{\\varphi_n} \\varphi_n(x)}$ by $\\sqrt{C} \\left(\\sum_{n \\ge m} \\abs{\\ip{h}{\\varphi_n}}^2\\right)^{1/2}$, which tends to $0$ uniformly in $x$.\nBy the [[spectral theorem for compact self-adjoint operators|A1G25R99PY]], the series converges to $f$ in $L^2$; the uniform limit is continuous and so is $f$, hence they agree everywhere.\n\nExample: for $K(x, y) = \\min(x, y)$ on $[0, 1]$, the eigenfunctions are $\\sqrt{2} \\sin\\left((n - \\tfrac12) \\pi x\\right)$.\nEvery function $f = T_K h$ with $h \\in L^2[0, 1]$ is continuous with $f(0) = 0$, and its expansion in these sines converges uniformly on $[0, 1]$.\n\nThe hypothesis $f = T_K h$ matters.\nFor a general function $f \\in L^2[a, b]$, the eigenfunction series converges only in $L^2$.\nIts sum is the orthogonal projection of $f$ onto the closed span of the $\\varphi_n$, which may differ from $f$.\n\n## Explanations\n\n### L1 human\n\nThe eigenfunctions of a symmetric kernel are like the axes of an ellipse.\nAny function produced by the integral operator can be written as a sum of these eigenfunctions.\nThe theorem says that this sum converges in the strongest usual sense, uniformly at every point.\n\n### L2 human\n\nThis is the classical form of the [[spectral theorem for compact self-adjoint operators|A1G25R99PY]], adapted to continuous kernels.\nIt is used to solve the Fredholm equation of the second kind with a symmetric kernel: the solution of $\\varphi - \\lambda T_K \\varphi = f$, for $\\lambda$ not a characteristic value, is $\\varphi = f + \\lambda \\sum_n \\frac{\\mu_n \\ip{f}{\\varphi_n}}{1 - \\lambda \\mu_n} \\varphi_n$.\nThrough Green's functions it gives the uniform convergence of eigenfunction expansions for Sturm–Liouville problems.\n",
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