Let's start by noting that
$$
F(x)=\sum_{k=-\infty}^{+\infty} f(x+2kL) \tag{1}
$$
is a periodic function with period $2L$:
$$
F(x+2L)=\sum_{k=-\infty}^{+\infty} f(x+2L+2kL)=\sum_{k'=-\infty}^{+\infty} f(x+2k'L)=F(x). \tag{2}
$$
Therefore, it can be represented as a Fourier series in the interval $[-L,L]$:
$$
F(x)=\sum_{n=-\infty}^{\infty}F_n\,e^{in\pi x/L}, \tag{3}
$$
where
\begin{align*}
F_n&=\frac{1}{2L}\int_{-L}^{L}F(x)\,e^{-in\pi x/L}\,dx \\
&=\frac{1}{2L}\int_{-L}^{L}\sum_{k=-\infty}^{\infty}f(x+2kL)\,
e^{-in\pi x/L}\,dx \\
&=\frac{1}{2L}\sum_{k=-\infty}^{\infty}\int_{(2k-1)L}^{(2k+1)L}
f(y)\,e^{-in\pi(y-2kL)/L}\,dy \\
&=\frac{1}{2L}\int_{-\infty}^{\infty}f(y)\,e^{-in\pi y/L}\,dy
=\frac{\sqrt{2\pi}}{2L}\hat{f}\left(\frac{n\pi}{L}\right), \tag{4}
\end{align*}
where $\hat{f}$ is the Fourier transform of $f$.
Combining $(1)$, $(3)$ and $(4)$ we finally obtain
$$
\sum_{k=-\infty}^{+\infty} f(x+2kL)=\frac{\sqrt{2\pi}}{2L}
\sum_{n=-\infty}^{+\infty} \hat{f}\left(\frac{n\pi}{L}\right)e^{in\pi x/L}.
\tag{5}
$$