Perturbation Theory (Non-Degenerate)

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Discussion Overview

The discussion revolves around the application of perturbation theory to a quantum mechanical system described by a modified harmonic oscillator potential. Participants explore how to derive the Hamiltonian, the ground state wave function, and the energy corrections using first-order perturbation theory.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Homework-related

Main Points Raised

  • One participant presents the potential V(x) and seeks guidance on deriving the Hamiltonian H₀ and the ground state wave function.
  • Another participant suggests that the Hamiltonian can be expressed as H = H₀ + Hₚ, where Hₚ represents the perturbation term.
  • There is a question about whether the Hamiltonian includes both the unperturbed and perturbation terms, with a specific form proposed.
  • A participant points out the need to use the ground state wave function of the unperturbed harmonic oscillator to evaluate the energy corrections.
  • One participant expresses uncertainty about the ground state wave function, indicating this as a barrier to solving the problem.
  • A link to an external resource is provided for further reference on the harmonic oscillator.
  • A question is raised about the applicability of the discussed approach to an anharmonic oscillator.
  • Another participant clarifies that the unperturbed harmonic oscillator wave function should be used for the calculations.

Areas of Agreement / Disagreement

Participants generally agree on the need to use the unperturbed harmonic oscillator wave function for calculations. However, there is uncertainty regarding the specific details of the Hamiltonian and the ground state wave function, indicating that the discussion remains unresolved.

Contextual Notes

Some participants express uncertainty about the ground state wave function, which may affect their ability to proceed with the calculations. The discussion also touches on the distinction between harmonic and anharmonic oscillators, but does not resolve how the perturbation theory applies in both cases.

Who May Find This Useful

This discussion may be useful for students or researchers interested in quantum mechanics, particularly those studying perturbation theory and its applications to harmonic and anharmonic oscillators.

jhosamelly
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If I have V(x)=\frac{1}{2}m\omega^{2}x^{2} (1+ \frac{x^{2}}{L^{2}})

How do I start to solve for the hamiltonian Ho, the ground state wave function ?? Calculate for the energy of the quantum ground state using first order perturbation theory?
 
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H= H_{0} + H_{p}

So basically, you have an aditional term, H_{p} = \frac{1}{2L^{2}}mω^2 x^4, that perturbates your hamiltonian.
You already know the solution for the harmonic oscillator, H= H_{0} = \hbarω(n + \frac{1}{2}), so you just have to find the corrections for the H_{p}.

hope i made myself clear ( ;
 
so does this mean my hamiltonian would be H= \hbarω(n + \frac{1}{2}) + \frac{1}{2L^{2}}mω^2 x^4 ?
 
Don't you know the ground state wave function of unperturbed oscillator.you can see them elsewhere and then just evaluate(with normalized eigenfunctions)
<E>=∫ψ0*(Hp0
 
I actually don't know the wave function.. That's also my prob... if i only know the wave function I'll be able to solve this.
 
Last edited:
Is this the same for an anharmonic oscillator? That is the problem about.
 
No,you use unpertubed harmonic oscillator wave function for calculation.
 

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