What i tried was:
$\int_{-\infty}^{\infty} exp(-\sqrt{2\pi}x-\dfrac{(y-x)^2}{2})dy = -\dfrac{1}{y-x}exp(-\sqrt{2\pi}x-\dfrac{(y-x)^2}{2})|_{-\infty}^{\infty}$
The exp dominates the expression so it goes faster to $0$ for $y$ that approaches infinity or negative infinity, so the expression will be zero. However when i use wolfram to solve this integral i get: $\sqrt{2\pi}exp(-\sqrt{2\pi}x)$. Going to polar representation doesn't seem to be effective here. How did they come by this result?