Show that $\mathcal{L}\{t^{1/2}\}=\sqrt{\pi}/(2s^{3/2}), \: s>0$
By the definition of Laplace transform we get:
$$\mathcal{L}\{t^{1/2}\} = \int_0^\infty t^{1/2}e^{-st} \, dt = \{x = \sqrt{st} \} = \dfrac{2}{s^{3/2}} \int_0^\infty e^{-x^2} x^2 \, dx. $$
A known and easily proved result is $\int_0^\infty e^{-x^2} \, dx = \dfrac{\sqrt{\pi}}{2}$. How (if possible) can I use this result to determine the integral above? I was thinking either integration by parts or perhaps a suitable coordinate transformation (e.g. polar coordinates) but my attempts failed.
Rewrite the integral as $$\int\limits_0^\infty-\frac{x}{2} \left(-2xe^{-x^2}\right)dx$$ and use integration by parts with $f(x) = -\frac{x}{2}$ and $g(x) = e^{-x^2}$ to obtain $$\left. -\frac x 2 e^{-x^2}\right|_0^\infty + \frac{1}{2} \int\limits_0^\infty e^{-x^2}dx = \frac{\sqrt{\pi}}{4}$$