Show, from it's definition,
\psi(x,t) = \int dx' G(x,t;x',t_0) \psi(x',t_0)
G(x,t;x',t_0)= \langle x | U(t,t_0) | x' \rangle
that the propagator G(x,t;x',t') is the Green Function of the Time-Dependent Schrodinger Equation,
\left ( H_x - i \hbar \frac{\partial}{\partial t} \right )...