Consider a state described by \[ \psi(x, t) = \psi_2(x, t) + \psi_4(x, t), \] where} \( \psi_2(x, t) \) and \( \psi_4(x, t) \) are respectively the second and fourth normalized harmonic oscillator wave functions and \( \omega \) is the angular frequency of the harmonic oscillator. The wave function \( \psi(x, t = 0) \) will be orthogonal to \( \psi(x, t) \) at time \( t \) equal to