Time Evolution for particle with potential suddenly removed

[Xyius]

Homework Statement

This is a problem from my Statistical Mechanics book by Pathria.
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At $t=0$, the ground state wavefunction of a one-dimensional quantum harmonic oscillator with potential $V(x)=\frac{1}{2}\omega_0^2 x^2$ is given by,

\psi(x,0)=\frac{1}{\pi^{1/4} \sqrt{a}}e^{-\frac{x^2}{2a^2}}

where $a=\sqrt{\frac{\hbar}{m \omega_0}}$. At $t=0$, the harmonic potential is abruptly removed. Use the momentum representation of the wavefunction at $t=0$ and the time-dependent Schrodinger equation to determine the spatial wavefunction and density at time $t>0$.

Homework Equations

i\hbar \frac{\partial}{\partial t}\psi=\hat{H} \psi

The Attempt at a Solution

So first I took the Fourier transform of the wave function given at $t=0$ to get,

\Phi(k,0)=-\frac{\sqrt{a}}{\pi^{1/4}}e^{\frac{1}{2}i a ^2 k^2}

So now that at $t>0$ the potential is removed, the new Hamiltonian is that of a free particle. I want to see how the original wave function evolves with time with this new potential. So I will multiply it by the time evolution operator.

\Phi(k,t)=\Phi(k,0)e^{-i \frac{\hat{H}t}{\hbar}}=\Phi(k,0)e^{-i \frac{\hat{p}^2 t}{2m\hbar}}

Generally, we can write this as,

|\psi(t)>=e^{-i \frac{\hat{p}^2 t}{2m\hbar}}|\psi_0>

The whole goal is to find the spatial wave function so let's project it onto $x$.

<x|\psi(t)>=<x|e^{-i \frac{\hat{p}^2 t}{2m\hbar}}|\psi_0>

What is given in the beginning of the problem is $<x|\psi_0>$ so I do the following.

&lt;x|\psi(t)&gt;=\int &lt;x|e^{-i \frac{\hat{p}^2 t}{2m\hbar}}|x&#039;&gt;&lt;x&#039;|\psi_0&gt;dx&#039;

Now, the Hamiltonian in the exponential purely depends on the momentum operator, so it would be easiest to deal with momentum eigenkets. So I will insert two more identities in there.

&lt;x|\psi(t)&gt;=\int &lt;x|p&#039;&gt;&lt;p&#039;|e^{-i \frac{\hat{p}^2 t}{2m\hbar}}|p&gt;&lt;p|x&#039;&gt;&lt;x&#039;|\psi_0&gt;dx&#039;dpdp&#039;

&lt;x|\psi(t)&gt;=\int &lt;x|p&#039;&gt;e^{-i \frac{p^2 t}{2m\hbar}}\delta(p&#039;-p)&lt;p|x&#039;&gt;&lt;x&#039;|\psi_0&gt;dx&#039;dpdp&#039;

&lt;x|\psi(t)&gt;=\int &lt;x|p&gt;e^{-i \frac{p^2 t}{2m\hbar}}&lt;p|x&#039;&gt;&lt;x&#039;|\psi_0&gt;dx&#039;dp

My problem is, I do not know what $<x|p>$ and $<p|x'>$ are. I remember back when I took quantum mechanics dealing with these types of terms but for the life of me I cannot remember what their value is or why! If anyone can help I would greatly appreciate it!

EDIT:
A ha! I just realized that these terms are simply the plane wave solution to the free particle! I will go though it now to make sure I have no other issues.

 

[Goddar]

Hi. I think you're taking a detour here...
You obtained the full wave function in momentum space:
Φ(k,t ) = Φ(k,0)⋅exp(–ik²t/2m)
(remember in momentum space p-hat is just p, not a differential operator)
So to get the spatial wave function, just take the inverse Fourier transform.