The general solution to the Schrodinger equation is a linear combination of steady states Y(x, t) = _ Cnun(x)e iEn t n=1 where the un (x) represent the time independent, position function, In = Onehi represent the total wave function solution, also known as separable solutions, and En is the corresponding energy. There can be an infinite set of solutions to the Schrodinger equation . Problem 88. Suppose a particular solution starts out in a linear combination of just two stationary states: Y(x, 0) = C141(x) + C24/2(x). Find the full wave function F (x, t)