Not sure if I correctly understood but this can be done as follows.
Start writing the series obtained convoluting as
$$ \sum_{k=0}^{\infty} \frac{1}{(k+1)!} \sum_{\ell=0}^{k} \left( a_{\ell}\ a_{k-\ell}\ \ell!\ (k-\ell)! \right) x^{k+1} $$
Note that this is a power series with coefficients $A_k = \dfrac{1}{(k+1)!} \sum_\limits{\ell=0}^{k} \left( a_{\ell}\ a_{k-\ell}\ \ell!\ (k-\ell)! \right)$.
We want to write $\sum_\limits{k=0}^{\infty} A_k\ x^{k+1} = \sum_\limits{k=0}^{\infty} \sum_\limits{\ell=0}^{k} b_l\ c_{k-l}\ x^k = \left( \sum_\limits{m=0}^{\infty} b_m\ x^m \right) \left( \sum_\limits{n=0}^{\infty} c_n\ x^n \right) $, which still also a power series with coefficients $P_k = \sum_\limits{\ell=0}^{k} b_l\ c_{k-l}$.
Since a power series uniquely determines a function, it follows that the coeffiecients of both must be equal. That is, $P_0 = 0$ and $ P_{k+1} = A_k $. Also, because $P_0 = b_0 c_0$ we have that $b_0 = 0$ or $c_0 = 0$. Without loss of generality suppose that $b_0 \neq 0$; then $c_0 = 0$.
We gonna write $c_n$ as a function of $a_k$ and $b_m$.
For $k = 0$
$$ A_0 = a_{0}^2 = P_1 = b_0 c_1 + b_1 c_0 = b_0 c_1 \implies c_1 = \frac{a_0^2}{b_0} $$
For $k = 1$
$$ A_1 = \frac{1}{2} \left( a_{0} a_{1} + a_{1} a_{0} \right) = a_{0} a_{1} = P_2 = b_0 c_2 + b_1 c_1 + b_2 c_0 = b_0 c_2 + b_1 c_1\\
\implies c_2 = \frac{1}{b_0} \left( a_{0} a_{1} - b_1 c_1 \right) $$
For $k = 2$
$$ A_2 = \frac{1}{3} \left( 4 a_0 a_2 + a_1^2 \right) = P_3 = b_0 c_3 + b_1 c_2 + b_2 c_1\\
\implies c_3 = \frac{1}{b_0} \left( \frac{1}{3} \left( 4 a_0 a_2 + a_1^2 \right) - b_1 c_2 - b_2 c_1 \right) $$
And so on... Hence
$$ c_{n+1} = \frac{1}{b_0} \left( A_n - \sum_{\ell=1}^{k-1} b_{\ell}\ c_{k-\ell} \right) $$
This means that $b_n$ is a sequence that we are free to determine as long as we choose $c_n$ as above. Thus we may choose a sequence which make its respective power series to have infinite radius of convergence to avoid any problem, say $b_m = \dfrac{1}{m!}$; so $\sum_\limits{m=0}^{\infty} b_i\ x^i = e^x$. We are done.