# Free particle wave function confusion.

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Hi! I'm currently studying Griffith's fantastic book on QM, and I'm confused for a bit about the wave function for a free particle.
Here's what I think so far; for a free particle, there are no stationary states, so therefore we can't solve the SE with
ψ(x)=Aeikx+Be-ikx

That is, we can't write a discrete sum. But We can have solutions as:

ψ(x,t)=∫dkφ(k)ei(kx-ωt)

I don't know if my understanding is correct, so please tell me so. Now, I assume that this understanding is correct and get to the question: If the solutions can only be the latter, then why was the solution from the book for the scattering states in the delta function potential a sum of stationary states and not the continuous sum? Also, why is it the same for the bound states if we are solving for the free particle when x<0 and x>0? Is it because it has a potential at x=0?

Orodruin
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Here's what I think so far; for a free particle, there are no stationary states, so therefore we can't solve the SE with
ψ(x)=Aeikx+Be-ikx
These functions do solve the Schrödinger equation, but they are not normalisable and therefore not actually in the relevant Hilbert space of square integrable functions.

If the solutions can only be the latter, then why was the solution from the book for the scattering states in the delta function potential a sum of stationary states and not the continuous sum?
Generally, in scattering theory, you will look at an in-state of definite momentum. Of course, the actual physical state is a superposition of such states and not a plane wave. However, in many cases, looking at just an incoming plane wave solution is a sufficiently accurate description.

Also, why is it the same for the bound states if we are solving for the free particle when x<0 and x>0? Is it because it has a potential at x=0?