Show explicitly that the eigenfunctions
$\psi_0(x) = (\frac{\alpha}{\pi})^{1/4} e^{-\frac{\alpha x^2}{2}}$
$\psi_1(x) = (\frac{4\alpha^3}{\pi})^{1/4} x e^{-\frac{\alpha x^2}{2}}$
$\psi_2(x) = (\frac{\alpha}{\pi})^{1/4} (2\alpha x^2 - 1) e^{-\frac{\alpha x^2}{2}}$
satisfy the time independent Schrödinger equation for the harmonic oscillator.