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  "body": "\n## Summary\n\nThe Dirichlet-to-Neumann operator of a domain sends boundary values to normal derivatives.\nGiven a function $f$ on the boundary, it solves the [[Dirichlet problem|8D56GQ4AG8]] for [[Laplace's equation|S8RG6N1PRT]] with data $f$.\nThen it returns the normal derivative of the solution on the boundary; conductivity equations work the same way.\nIt is a basic example of a [[pseudo-differential operator|FF27N0BWTP]] on the boundary.\nIt carries the boundary measurements of electrical impedance tomography, in the [[Calderón problem|R8Y8DDTWBM]], and its eigenvalues are the Steklov eigenvalues.\n\n## Explanations\n\n### L1 human\n\nFix the temperature, or the voltage, on the boundary of a body and let it settle to equilibrium inside.\nThen measure how much heat, or current, flows out through each part of the boundary.\nThe Dirichlet-to-Neumann operator is the rule that turns the first list of numbers into the second.\nOn the unit disk, the boundary data $\\cos(k\\theta)$ extend to the harmonic function $r^k \\cos(k\\theta)$, whose radial derivative at $r = 1$ is $k \\cos(k\\theta)$.\nSo on the disk the operator multiplies the $k$-th Fourier mode by $\\abs{k}$.\n",
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