Ehrenfest theorem and Hamiltonian operator

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Homework Help Overview

The discussion revolves around applying the generalized Ehrenfest theorem to demonstrate a relationship involving the Hamiltonian operator for a free particle in one dimension. The original poster attempts to derive the second time derivative of the expectation value of position squared in terms of the expectation value of momentum squared.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the application of the Ehrenfest theorem, discussing the necessary commutation relations and the implications of the Hamiltonian operator. There are questions about the correct form of the theorem and how to evaluate specific terms in the equations presented.

Discussion Status

The discussion is ongoing, with participants providing guidance on the application of the theorem and commutation relations. Some express uncertainty about their progress, while others suggest methods to evaluate specific terms, indicating a collaborative effort to clarify the problem.

Contextual Notes

There is mention of differing interpretations of the generalized Ehrenfest theorem and its components, as well as the importance of the commutation relations provided in the original post. The original poster also notes a lack of clarity in their understanding of the next steps.

cleggy
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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 Schrödinger 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 Schrödinger 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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