Concept:
The integral
\[
\int_{-\infty}^{\infty} e^{-x^2}\,dx
\]
is known as the Gaussian integral. It plays a fundamental role in probability theory, especially in the Normal distribution.
A well-known result from calculus states:
\[
\int_{-\infty}^{\infty} e^{-x^2}\,dx = \sqrt{\pi}
\]
This result is usually derived by squaring the integral and converting it into polar coordinates.
Step 1: Define the integral.
Let
\[
I = \int_{-\infty}^{\infty} e^{-x^2}\,dx
\]
Step 2: Square the integral.
\[
I^2 =
\left(\int_{-\infty}^{\infty} e^{-x^2}\,dx\right)
\left(\int_{-\infty}^{\infty} e^{-y^2}\,dy\right)
\]
\[
=
\int_{-\infty}^{\infty}\int_{-\infty}^{\infty}
e^{-(x^2+y^2)}\,dx\,dy
\]
Step 3: Convert to polar coordinates.
Using \(x^2 + y^2 = r^2\) and \(dx\,dy = r\,dr\,d\theta\):
\[
I^2 =
\int_{0}^{2\pi} \int_{0}^{\infty} e^{-r^2} r\,dr\,d\theta
\]
\[
=
2\pi \int_{0}^{\infty} e^{-r^2} r\,dr
\]
Let \(u=r^2\), \(du=2r\,dr\):
\[
\int_{0}^{\infty} e^{-r^2} r\,dr = \frac{1}{2}
\]
Thus,
\[
I^2 = 2\pi \times \frac{1}{2} = \pi
\]
Step 4: Take the square root.
\[
I = \sqrt{\pi}
\]
\[
\therefore \int_{-\infty}^{\infty} e^{-x^2}\,dx = \sqrt{\pi}
\]