How Do You Solve for the Propagator in Momentum Space Under Constant Force?

[WarnK]

Homework Statement

(this is from R. Shankar, Principles of Quantum Mechanics, 2nd ed, exercise 5.4.3)
Consider a particle subject to a constant force f in one dimension. Solve for the propagator in momentum space and get

U(p,t;p',0) = \delta (p-p'-ft) e^{ i(p'^3-p^3)/6m\hbar f }

Homework Equations

The Attempt at a Solution

I write a hamiltonian H = p^2/2m + fx, plug that into H|p>=E|p>, with the x operator in momentum space being ih d/dp, it's all nice and seperable and I get

\psi(p) = A exp \left( i \frac{p^3-6mEp}{6m\hbar f} \right)

but what do I do now? I'm not sure how to go about normalizing this.

 

[Avodyne]

First of all, you don't really mean H|p>=E|p>; |p> is an eigenstate of the momentum operator, but not of H; you mean H|E>=E|E>, where <p|E> is your momentum-space wave function.

You want to normalize it so that you can write a completeness statement in the form
\int_{-\infty}^{+\infty}dE\;|E\rangle\langle E| = I,
where I is the identity operator.

 

[WarnK]

Thanks!
It's a bit much too write everything as tex but I ended up with
A = \left( \frac{1}{2 \pi \hbar f} \right)^{1/2}
Now, how do I get a propagator out of this!

 

[Avodyne]

The propagator is <p'|e^(-iHt/hbar)|p>. Can you think of a use for the completeness statement?

 

[WarnK]

<br /> \langle p&#039;| e^{-iHt/ \hbar} |p\rangle = \int_{-\infty}^{+\infty}dE \langle p&#039;|E \rangle \langle E| e^{-iHt/ \hbar} |p\rangle = \int_{-\infty}^{+\infty}dE \langle p&#039;|E \rangle \langle E|p-ft\rangle<br />
and I can plug in my expression for psi, do the integral and out comes the given answer.
But how come e^(-iHt/hbar)|p> = |p-ft>? I just guessed it from experience of doing lots of integrals like these.

 

[Avodyne]

You don't need to guess it, and in fact it's not correct; evaluating your final expression does not yield the given result (so you made a mistake somewhere when you evaluated it).

In your middle expression, you can replace H with E, since H is sitting next to one of its eigenstates. Then the integral over E will generate the given answer.

 

[cybla]

Hi, i have a quick question on middle part of the integral. How do you evaluate <E|e^{-iEt/h}|p> ?