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  "body": "\n## Summary\n\nThe Borel functional calculus assigns an operator $f(N)$ to a normal or self-adjoint operator $N$ and a Borel function $f$ on its spectrum.\nIt is defined by integrating $f$ against the projection-valued measure given by the spectral theorem.\nIt extends the continuous functional calculus to discontinuous functions, such as indicator functions, which produce the spectral projections of $N$.\n\n## Explanations\n\n### L1 human\n\nFor a diagonal matrix, applying a function to the matrix means applying it to each diagonal entry.\nThe spectral theorem says that normal operators are diagonal in a generalized sense, with a measure in place of a list of eigenvalues.\nThe Borel functional calculus applies a function to an operator in the same way, entry by entry along the spectrum.\nFor the matrix $\\operatorname{diag}(1, 2)$ and the indicator function $f$ of the set $\\set{2}$, the result is $f(N) = \\operatorname{diag}(0, 1)$, the projection onto the eigenspace of $2$.\n",
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