Having trouble with time (in)dependant solutions

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Hey all -

I'm taking my first quantum class this year, and I'm still on really shaky ground about time-dependent and time-independent solutions of the Schrödinger equation. I understand that the time independent Schrödinger equation comes from separating your space and time variables, but I have trouble interpreting the meanings of both types of solutions. Particularly, why can you reconstruct any arbitrary \Psi(x,t) out of the time-independent solutions? Rather, why can an electron in, say, an infinite square well potential have different \Psi's?
 
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Solve the time-dependent Schroedinger equation i\hbar\frac{\partial}{\partial t}\Psi(x,t) = H\Psi(x,t) by separation of variables to give the following particular solutions (which have the counterintuitive property of predicting time-independent observables):

<br /> \Psi(x,t) = \phi_E(x)e^{-\frac{i}{\hbar}Et}\;\;\;\;\;\;\;\;|\Psi(x,t)|^2 = |\phi_E(x)|^2<br />

Where has the time gone? It is restored to us by a general solution to the TDSE - an arbitrary superposition of the particular solutions:

<br /> \Psi(x,t) = \sum_{n=1}^{\infty} a_n\phi_n(x) e^{-\frac{i}{\hbar}E_nt} \;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\;\text{\mathrm{(discrete\;spectrum)}}<br />

<br /> \Psi(x,t) = \int_0^{\infty} a(E)\phi_E(x) e^{-\frac{i}{\hbar}Et}\;dE \;\;\;\;\;\;\;\;\text{\mathrm{(continuous \; spectrum)}}<br />

Quite generally, a wave packet - a superposition of states having different energies - is required in order to have a time-dependence in the probability density and in other observable quantities, such as the average position or momentum of a particle.
Simplest example: a linear combination of just two particular solutions

\Psi(x,t) = a\phi_E(x) e^{-\frac{i}{\hbar}Et} + b\phi_{E&#039;}(x) e^{-\frac{i}{\hbar}E&#039;t}.

The probability density is given by:

<br /> |\Psi(x,t)|^2 = |a|^2|\phi_E(x)|^2 + |b|^2|\Psi_{E&#039;}(x)|^2 + 2\mathrm{Re}\left\{a^*b\phi_E^*(x)\phi_{E&#039;}(x)\mathrm{e}^{-i\frac{(E&#039;-E)t}{\hbar}}\right\}<br />

All the time-dependence is contained in the interference term.
 
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