Show that ${\mathcal L} {\lbrace t^{n-\frac{1}{2}}\rbrace}=\frac{(2n-1)!!}{2^n}\frac{1}{s^n} \sqrt{\frac{\pi}{s}}$
My Attempt:
${\mathcal L} {\lbrace t^{n-\frac{1}{2}}\rbrace}=\int_{0}^{\infty}\mathcal e^{-st}t^{n-\frac{1}{2}}dt$
Integration by parts gives:
${\mathcal L} {\lbrace t^{n-\frac{1}{2}}\rbrace}=\frac{(2n-1)}{2s}{\mathcal L} {\lbrace t^{n-\frac{3}{2}}\rbrace}$
${\mathcal L} {\lbrace t^{n-\frac{3}{2}}\rbrace}=\frac{(2n-3)}{2s}{\mathcal L} {\lbrace t^{n-\frac{5}{2}}\rbrace}$
${\mathcal L} {\lbrace t^{n-\frac{5}{2}}\rbrace}=\frac{(2n-5)}{2s}{\mathcal L} {\lbrace t^{n-\frac{7}{2}}\rbrace}$
I start to see the $\frac{(2n-1)!!}{2^n}\frac{1}{s^n}$, but not the $\sqrt{\frac{\pi}{s}}$
Thanks, in advance.
The Laplace Transform of $t^{n-1/2}$ is given by
$$\mathscr{L}\left(t^{n-1/2}\right)(s)=\int_0^\infty t^{n-1/2}\,e^{-st}\,dt$$
Now, enforce the substitution $st\to t$ reveals
$$\begin{align} \mathscr{L}\left(t^{n-1/2}\right)(s)&=\left(\frac{1}{s}\right)^{n+1/2}\int_0^\infty t^{n-1/2}\,e^{-t}\,dt\\\\ &=\left(\frac{1}{s}\right)^{n+1/2}\Gamma(n+1/2)\tag 1 \end{align}$$
where $\Gamma(z)\equiv \int_0^\infty t^{z-1}\,e^{-t}\,dt$ is the Gamma Function.
The Gamma function satisfies the Functional Relationship $\Gamma(z+1)=z\Gamma (z)$. Applying this functional relationship repeatedly to the right-hand side of $(1)$ yields
$$\begin{align} \mathscr{L}\left(t^{n-1/2}\right)(s)&=\left(\frac{1}{s}\right)^{n+1/2}\left(\frac12\,\cdot \frac32\,\cdot\frac52\,\cdots\frac{2n-1}{2}\right)\Gamma(1/2)\\\\ &=\frac{(2n-1)!!}{2^n}\left(\frac{1}{s}\right)^{n}\sqrt{\frac{\pi}{s}} \end{align}$$
where we used $\Gamma(1/2)=\int_0^\infty t^{-1/2}e^{-t}\,dt=\sqrt{\pi}$. Note that this integral can be evaluated by enforcing the substitution $t\to t^2$, which results in the well-know Gaussian integral.