(a) Show by direct substitution in the Schrodinger equation for the one-dimensional harmonic oscillator that the wave function ψ0 (x) = A0e – a2x2/2, where a2 = mw/h, is a solution with energy corresponding to n = 0 in Eq. (40.22). (b) Find the normalization constant A0. (c) Find the classical turning points and show, in contrast, that the probability density has a maximum at x = 0.