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  "body": "\n## Summary\n\nA de Branges space is a Hilbert space of [[entire functions|0419794R0T]] built from one entire function $E$.\nThe function $E$ must be larger at each point of the upper half-plane than at the mirror point in the lower half-plane.\nIts elements are the entire functions $F$ such that $F/E$ and $F^\\#/E$ lie in the Hardy space of the [[upper half-plane|X6XGGH5FPW]].\nThe norm of $F$ is the $L^2$ norm of $F/E$ on the real line.\nIt is a [[reproducing kernel Hilbert space|4CK2GSRAGD]] with an explicit kernel, and it generalises the Paley–Wiener spaces.\nDe Branges used these spaces in the spectral theory of canonical systems.\n\n## Explanations\n\n### L1 human\n\nChoose an entire function $E$ with $\\abs{E(\\bar z)} \u003c \\abs{E(z)}$ whenever $z$ is in the upper half-plane.\nThe space $\\mathcal{H}(E)$ collects entire functions that are \"no larger than $E$\" in a precise square-integrable sense.\nFor $E(z) = e^{-iaz}$ with $a \u003e 0$, one gets the Paley–Wiener space of square-integrable band-limited functions, whose Fourier transforms live on $[-a, a]$.\nEach point evaluation $F \\mapsto F(w)$ is a bounded functional, given by an inner product with an explicit kernel.\n",
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