In general you have the following: if $\mathcal{D}_{\alpha}f(x) = f(\alpha x)$ where $\alpha >0$, then
$$\mathcal{F}\mathcal{D}_{\alpha}f(y) = \frac{1}{\alpha} \mathcal{D}_{\alpha^{-1}}\mathcal{F}f(y).$$
You can see this by doing a change of variable $x' = \alpha x$:
$$\mathcal{F}\mathcal{D}_{\alpha}f(y) = \int_{-\infty}^{\infty} e^{-ixy} f(\alpha x)\,dx = \int_{-\infty}^{\infty} e^{-ix'\frac{y}{\alpha}} f(x')\,\frac{1}{\alpha}dx' = \frac{1}{\alpha} \mathcal{F}f\left(\frac{y}{\alpha}\right)$$
which is of course equal to $\frac{1}{\alpha}\mathcal{D}_{\alpha^{-1}}\mathcal{F}f(y)$. What this says is that if you know $\mathcal{F}f$, then you can easily compute the Fourier transform of a dilation of $f$. In your case, we know what the Fourier transform of $g(n) = e^{-n^2}$ is. To get $f$, note that $f(n) = g(\sqrt{\pi x} n)$ and use the above relationship.