Logarithmic singularity
= Logarithmic singularity
{title2=$a\log(z-z_0)$}
A logarithmic singularity behaves locally like $a\log(z-z_0)$ with $a\ne0$, on a chosen branch. Although unbounded at the endpoint, it is integrable along a finite ray. In a rapidly oscillating endpoint integral its contour rotation produces a logarithm of the large parameter and a branch-angle contribution; this differs from the ordinary smooth-amplitude <Watson lemma>.