How to solve an anharmonic oscillator perturbation problem?

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SUMMARY

The discussion centers on solving an anharmonic oscillator perturbation problem, specifically focusing on the quantum states defined by Ej = jhf - (lambda)(jhf)^2. The user seeks guidance on calculating the partition function Zj = sum(e^(-(beta)Ej)) and determining the free energy F, which is expressed as F ≈ Fo + (lambda)F1. A participant confirms that the problem is indeed a perturbation issue and suggests that the eigenvalue format allows for direct relation to the unperturbed harmonic oscillator without needing the perturbing potential V1.

PREREQUISITES
  • Understanding of quantum mechanics, specifically anharmonic oscillators
  • Familiarity with perturbation theory in quantum systems
  • Knowledge of partition functions in statistical mechanics
  • Experience with free energy calculations in thermodynamics
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  • Study perturbation theory applications in quantum mechanics
  • Learn how to derive partition functions for anharmonic oscillators
  • Research free energy calculations in statistical mechanics
  • Explore the relationship between eigenvalues and unperturbed systems
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Students and researchers in quantum mechanics, particularly those dealing with anharmonic oscillators and statistical mechanics, will benefit from this discussion.

leright
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I have a homework problem that is kinda driving me nuts...

Consider the case of an anharmonic oscillator with microsystem quantum states given by Ej = jhf - (lambda)(jhf)^2.

Using the known harmonic expressions as a starting point, determine the corresponding expression for F1 and for F, which is about equal to Fo + (lambda)F1.

Can someone give me a hint on how to approach this problem? I figure I could find the partition function easily enough since Zj = sum(e^(-(beta)Ej)). I can then plug in Ej into the Zj function. However, I am not sure how to determine that sum. Am I even approaching this problem in the right way?

Thanks.
 
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IF you have the partition function, how do you get the F ?

Daniel.
 
Hi leright,
This
looks like a perturbation problem to me. You don't need the perturbing potential V1 since you have the eigenvalue given in the form of an unperturbed part (relate that to the unperturbed H.O.) and a perturbation of strength lambda.
 

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