We are asked to evaluate the integral:
\[ I = \int_0^\infty e^{-x^2} \, dx \]
Step 1: Recognize the Gaussian integral
The Gaussian integral is a well-known result. For the entire range from \(-\infty\) to \(\infty\), we know that:
\[ \int_{-\infty}^\infty e^{-x^2} \, dx = \sqrt{\pi} \]
Step 2: Use symmetry of the function
The function \(e^{-x^2}\) is symmetric around \(x = 0\), which means:
\[ \int_{-\infty}^\infty e^{-x^2} \, dx = 2 \int_0^\infty e^{-x^2} \, dx \]
Thus, we can express the integral over \(0\) to \(\infty\) as half of the integral over the entire real line:
\[ I = \frac{1}{2} \int_{-\infty}^\infty e^{-x^2} \, dx \]
Step 3: Substitution from the known result
From Step 1, we know the value of the full Gaussian integral:
\[ \int_{-\infty}^\infty e^{-x^2} \, dx = \sqrt{\pi} \]
Therefore, substituting this result into the equation for \(I\):
\[ I = \frac{1}{2} \times \sqrt{\pi} = \frac{\sqrt{\pi}}{2} \]