Why the density function of a random variable $X$ that follow the normal law $\mathcal N(0,\sigma ^2)$ is $\frac{1}{\sigma \sqrt{2\pi}}e^{-\frac{x^2}{2\sigma ^2}}$ and not $\frac{1}{\sigma \sqrt{\pi}}e^{-\frac{x^2}{\sigma ^2}}$ ? Indeed, this could work since $$\int_{\mathbb R}\frac{1}{\sigma \sqrt\pi}e^{-\frac{x^2}{\sigma ^2}}dx=1.$$
So why adding the $2$ in $$\frac{1}{\sigma \sqrt{2\pi}}e^{-\frac{x^2}{2\sigma ^2}}\ \ ?$$
The function $\frac1{\sigma\sqrt\pi}e^{-\frac{x^2}{\sigma^2}}$ is a PDF for positive $\sigma$, and this for random variables that have normal distribution with mean $0$.
However if we calculate the corresponding variance on base of this PDF then the answer is not $\sigma^2$.
So we are not dealing with $\mathcal N(0,\sigma^2)$.