A particle of mass m is subjected to a potential V(x). If its wavefunction is given by
\(\psi(x,t) = \alpha x^2 e^{-\beta x} e^{i\gamma t/\hbar}, x>0\)
\(\psi(x,t) = 0, x \le 0\),
then V(x) is (\(\alpha\), \(\beta\) and \(\gamma\) are constants of appropriate dimensions)