What's the proof that $\int_0^\infty \tan x\,dx=\ln 2$?

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The $0$-at-$0$ antiderivative $\ln|\sec x|$ is periodic with mean $\frac{1}{\pi}\int_0^\pi\ln\sec xdx$, which is famously $\ln 2$. If we regard the antiderivative as equal to its own mean at infinity, $\int_0^\infty\tan xdx=\ln 2$.