Le'ts consider a discrete spectrum of the Hamiltonian of some system. A solution of the TDSE, can be a superposition of eigenstates of H, and can be written :
$\Psi(\vec r,t)=\sum_n c_n \phi_n(\vec r)e^{-i\frac{E_n}{\hbar}t}$.
This expression was the result of the consideration that the potential was time independent, which then allowed me to use separation of variables.
But, there is also this expression:
$\Psi(\vec r,t)=\sum_n c_n(t_0)e^{-i\frac{E_n}{\hbar}(t-t_0)}\phi_n(\vec r)$