  We take an open regular domain $\Omega$ in $\mathbb{R}^n$ with $n\ge 3$. We
introduce a pair of positive parameters $\epsilon_1$ and $\epsilon_2$ and we
set $\epsilon\equiv(\epsilon_1,\epsilon_2)$. Then we define the perforated
domain $\Omega_\epsilon$ by making in $\Omega$ a small hole of size
$\epsilon_1\epsilon_2$ at distance $\epsilon_1$ from the boundary. When
$\epsilon\rightarrow(0, 0)$, the hole approaches the boundary while its size
shrinks at a faster rate. In $\Omega_\epsilon$ we consider a Dirichlet problem
for the Laplace equation and we denote its solution by $u_\epsilon$. By an
approach based on functional analysis and on the introduction of special layer
potentials we show that the map which takes $\epsilon$ to (a restriction of)
$u_\epsilon$ has a real analytic continuation in a neighbourhood of $(0, 0)$.
