Ehrenfest theorem and Hamiltonian operator

AI Thread Summary
The discussion revolves around applying the generalized Ehrenfest theorem to demonstrate that for a free particle with the Hamiltonian operator H = p^2/2m, the second derivative of the expectation value of position squared, d^2<x^2>/dt^2, equals (2/m)<p^2>. Participants explore the necessary commutation relations and the application of the theorem, specifically focusing on the operator A being either position x or momentum p. There is confusion regarding the evaluation of commutators and the correct application of the theorem, with users seeking clarification on the steps involved. The conversation highlights the importance of understanding the relationship between operators and their commutation properties in quantum mechanics. Overall, the thread emphasizes the complexities of applying theoretical concepts to practical problems in quantum physics.
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Homework Statement



Use the generalized Ehrenfest theorem to show that any free particle with the one-dimensional Hamiltonian operator

H= p^2/2m obeys

d^2<x^2> / dt^2 = (2/m)<p^2>,



Homework Equations



The commutation relation xp - px = ih(bar)



The Attempt at a Solution




d^2<x^2> / dt^2 = (1/m)(d<p^2>/dt)


H = p^2/2m + V(x)

then [x^2,H] = x^2[(p^2/2m) + V(x)) - ((p^2/2m) + V(x))x^2 = (1/2m)[x^2,p^2]


[x^2,p^2] = xxpp - ppxx = 2ih(bar)(xp + px)

I'm stuck at this point?

am i on the right track?

the < > brackets represent the expectation value
 
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You're not using the generalized Ehrenfest theorem from the looks of it. T

The theorem you want to use is:
<br /> \frac{d \langle A \rangle}{dt}=\frac{1}{i \hbar}\langle [A,H] \rangle+\left\langle \frac{dA}{dt} \right\rangle<br />

With A an operator in the Schrodinger picture. Now use A=x and A=p.
 
According to my textbook the generalized Ehrenfest theorem is

what you have put but without the derivative term of A at the end
 
Don't forget the tex bracket. Well you could write it like that, because the last term in my expression is usually zero for operators in the Schrodinger picture.

It wasn't clear from your original post that you were actually using that one however.

That said can you evaluate the equation for x and p?
 
Which x and p ?

the term (xp + px) ?

I really thought i was on the right track.

I'm not sure where to go now. Pointers?
 
If

[x^2,p^2] = xxpp - ppxx = 2ih(bar)(xp + px)

Then how do I find the term (xp + px) ?
 
Write the commutator as [x^2,pp] and use the commutator identity [A,BC]=[A,B]C+B[A,C] then do the same for the x^2.
 
I'm still not following

I'm given the commutation relations in my text as


[x^2,p^2] = xxpp - ppxx = 2ih(bar)(xp + px)

[xp,p^2] = xxpp - ppxx = 2ih(bar)(p^2)

[px,p^2] = xxpp - ppxx = 2ih(bar)(p^2)
 
You can let a test function work on it. Evaluate (xp+px)f(x).
 
  • #10
This makes no sense to me. I think I'm going to call it a day. Thanks for all your help Cyosis
 
  • #11
Do you know how you can show that [x,p]=i \hbar in the first place?
 
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