Corrector for the Ehrenfets equation

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SUMMARY

The discussion centers on the calculation of the lowest corrector for the Ehrenfest equation, specifically addressing the potential V(x) and its slow variation relative to the wavefunction's wavelength. Participants express confusion regarding the term "corrector" in the context of the Ehrenfest theorem, which relates to the classical equation of motion. The Ehrenfest theorem is highlighted as m(d²/dt²) = -⟨dV/dx⟩, equating expectation values with classical mechanics. References to classical mechanics and quantum mechanics textbooks, including works by Eugen Merzbacher and Prof. Fitzpatrick, provide context for the discussion.

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  • Familiarity with classical mechanics equations of motion
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  • Basic concepts of expectation values in quantum mechanics
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Students and researchers in quantum mechanics, particularly those exploring the intersection of classical and quantum dynamics, as well as educators seeking to clarify the Ehrenfest theorem and its applications.

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Homework Statement



The potential V(x) in the equation
m\frac{d^2}{dt^2}=-\left \langle \frac{d\hat{V}}{dx} \right \rangle
changes very slowly for the typical wavelength wavefunction. Calculate the lowest corrector for the classical equation of motion.

Homework Equations


The Ehrenfest Theorem
m\frac{d^2}{dt^2}=-\left \langle \frac{d\hat{V}}{dx} \right \rangle

The Attempt at a Solution


I don't understand the question. I can't find in any book a mention of a corrector for the Ehrenfest equation. And what does it mean with the wavelentgh of the wavefunction?

Thank you for your time.
 
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Funny, your only relevant equation is also a given in this exercise. My (very old ) QM book has ## {d\over dt}<{\bf p}> = -\int \Psi^* (\nabla V)\Psi\, d\tau = -<\nabla V> = <{\bf F}> ##as Ehrenfest's theorem; with the comment: "this is simply Newton's law, but now for expectation values".

Must say my book is easier to understand for me than your rendering of he exercise: ## m\frac{d^2}{dt^2}\,## looks like an operator to me, not an expectation value like ## -\left \langle \frac{d\hat{V}}{dx} \right \rangle\,##.

So I am on your side in "not understanding the question". I need some reassurance this really is exactly how the exercise was formulated...

This link, by prof. Fitzpatrick, Texas university Austin, sides with Eugen Merzbacher. It makes me think a <x> fell by the wayside somewhere...

Wavelength of the wave function generally has a ##\hbar## in it somewhere, making the wavelength real small compared to change in V.
 

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