At time t = 0 a particle in the potential V(x) = mω2x2/2 is described by the wave function
\(\psi(x, 0) = A\sum\limits_n (1/\sqrt 2)^n\psi_n(x)\),
where \(\psi_n(x)\) are eigenstates of the energy with eigenvalues En = (n + 1/2)hω. You are given that \((\psi_n, \psi_{n'})= \delta_{nn'}\).
(a) Find the normalization constant A.
(b) Write an expression for \(\psi\)(x, t) for t > 0.
(c) Show that |\(\psi\)(x, t)|2 is a periodic function of time and indicate the longest period \(\tau\).
(d) Find the expectation value of the energy at t = 0.