Solve by integration
$$\int_{-\infty}^\infty e^{-iαx-α^2 t} dα$$
solve by integration , this integral is - infinity to infinity and exponent value
Solve by integration
$$\int_{-\infty}^\infty e^{-iαx-α^2 t} dα$$
solve by integration , this integral is - infinity to infinity and exponent value
This question has a short answer and a long one.
completing the square you have: $$ e^{−iαx−α^2t}=e^{-t(\alpha+\frac{ix}{2t})} \,e^{\frac{-x^2}{4t}} \\ \Rightarrow \int_{-\infty}^{\infty} e^{−iαx−α^2t}\, d \alpha=e^{\frac{-x^2}{4t}} \, \int_{-\infty}^{\infty}e^{-t(\alpha+\frac{ix}{2t})^2} \,d\alpha \\=e^{\frac{-x^2}{4t}} \, \int_{-\infty}^{\infty}e^{-t\alpha^2} \,d\alpha \\=e^{\frac{-x^2}{4t}} \sqrt{\frac{\pi}{t}} $$
But in the complete answer, we have to prove that
$$ \int_{-\infty}^{\infty}e^{-t(\alpha+b)^2} \,d\alpha=\int_{-\infty}^{\infty}e^{-t\alpha^2} \,d\alpha $$
For that we can just use a change of variable, but $b$ is imaginary and that means that the limits of integration would change to a line in the complex plane.
So to prove that we need another approach and what is commonly done is to use the fact $e^{z^2}$ is an entire function, so any closed line integral in the complex plane will be $0$. So you choose a rectangle whose segments parallel to the real line go from $-\infty$ to $\infty$ , and the other segments go from $0$ to some $ic$. Then you solve the 4 integrals for each segment and using that the sum of the 4 of them is $0$, you should get the desired result, that is, it is fine to complete the squares even if you have to deal with an imaginary term.
Although this isn't quite the Fourier transform of a Gaussian, this link helps illustrate @Mhenni's idea:
http://www4.ncsu.edu/~franzen/public_html/CH795Z/math/ft/gaussian.html
Hint: Complete the square in the argument of the exponential in terms of $\alpha$ and then use Gaussian integrals.
Added: Note that, you need to make a change of variables after completing the square. See here.