  It was recently found that the classical 3d O$(N)$ model in the semi-infinite
geometry can exhibit an "extraordinary-log" boundary universality class, where
the spin-spin correlation function on the boundary falls off as $\langle
\vec{S}(x) \cdot \vec{S}(0)\rangle \sim \frac{1}{(\log x)^q}$. This
universality class exists for a range $2 \leq N < N_c$ {and Monte-Carlo
simulations and conformal bootstrap} indicate $N_c > 3$. In this work, we
extend this result to the 3d O$(N)$ model in an infinite geometry with a plane
defect. We use renormalization group (RG) to show that in this case the
extraordinary-log universality class is present for any finite $N \ge 2$. We
additionally show, in agreement with our RG analysis, that the line of defect
fixed points which is present at $N = \infty$ is lifted to the ordinary,
special (no defect) and extraordinary-log universality classes by $1/N$
corrections. We study the `"central charge" $a$ for the $O(N)$ model in the
boundary and interface geometries and provide a non-trivial detailed check of
an $a$-theorem by Jensen and O'Bannon. Finally, we revisit the problem of the
O$(N)$ model in the semi-infinite geometry. We find evidence that at $N = N_c$
the extraordinary and special fixed points annihilate and only the ordinary
fixed point is left for $N > N_c$.
