  The {\it{Polaron measure}} is defined as the transformed path measure
  $$\widehat{\mathbb P}_{\epsilon,T}= Z_{\epsilon,T}^{-1}\,\,
\exp\bigg\{\frac{1}{2}\int_{-T}^T\int_{-T}^T\frac{\epsilon\e^{-\epsilon|t-s|}}{|\omega(t)-\omega(s)|}
\,\d s \,\d t\bigg\}\d\mathbb P$$ with respect to the law $\mathbb P$ of three
dimensional Brownian increments on a finite interval $[-T,T]$, and $
Z_{\epsilon,T}$ is the partition function with $\epsilon>0$ being a constant.
The logarithmic asymptotic behavior of the partition function $Z_{\epsilon,T}$
was analyzed in \cite{DV83} showing that $$ g_0=\lim_{\epsilon \to
0}\bigg[\lim_{T\to\infty}\frac{\log Z_{\eps,T}}{2T}\bigg]=\sup_{\heap{\psi\in
H^1(\R^3)}{\|\psi\|_2=1}} \bigg\{\int_{\mathbb R^3}\int_{\mathbb R^3}\d x\d
y\,\frac {\psi^2(x) \psi^2(y)}{|x-y|} -\frac 12\big\|\nabla
\psi\big\|_2^2\bigg\}. $$ In \cite{MV18} we analyzed the actual path measures
and showed that the limit ${\widehat {\mathbb
P}}_{\eps}=\lim_{T\to\infty}\widehat{\mathbb P}_{\eps,T}$ exists and identified
this limit explicitly, and as a corollary, we also deduced the central limit
theorem for
  $(2T)^{-1/2}(\omega(T)-\omega(-T))$ under $\widehat{\mathbb P}_{\eps,T}$ and
obtained an expression for the limiting variance $\sigma^2(\eps)$.
  In the present article, we investigate the {\it{strong coupling limit}}
$\lim_{\eps\to 0} \lim_{T\to\infty} \widehat{\mathbb P}_{\eps,T}=\lim_{\eps\to
0} \widehat {\mathbb P}_\eps$ and show that this limit coincides with the
increments of the stationary Pekar process with generator
  $$
  \frac 12 \Delta+ \bigg(\frac{\nabla\psi}\psi\bigg)\cdot \nabla
  $$ for any maximizer $\psi$ of the free enrgy $g_0$. The Pekar process was
also earlier identified in \cite{MV14}, \cite{KM15} and \cite{BKM15} as the
limiting object of the {\it{mean-field Polaron}} measures.}
