Probability of perturbed harmonic oscillator

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SUMMARY

The discussion focuses on calculating the probabilities of a perturbed harmonic oscillator transitioning to its ground state and second excited state after a sudden displacement of the potential center. The experiment involves a particle of mass m initially in the first excited state, with the potential modified by a small displacement 'a'. Using perturbation theory, the potential is expressed as V = (1/2)mω²(x-a)² - (1/2)mω²x², and the wavefunction is expanded to first order in 'a'. The calculations yield the probabilities for the transitions, emphasizing the importance of sudden approximations in the analysis.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically harmonic oscillators.
  • Familiarity with perturbation theory in quantum mechanics.
  • Knowledge of wavefunction expansion techniques.
  • Proficiency in mathematical concepts involving operators and eigenstates.
NEXT STEPS
  • Study the application of perturbation theory in quantum mechanics.
  • Learn about sudden approximation techniques in quantum systems.
  • Explore the mathematical derivation of wavefunction expansions.
  • Investigate the implications of potential modifications on quantum states.
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This discussion is beneficial for quantum mechanics students, physicists specializing in theoretical physics, and researchers exploring quantum state transitions in perturbed systems.

phyzzydud
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An experimenter has carefully prepared a particle of mass m in the first excited state of a one dimensional harmonic oscillator. Suddenly he coughs and knocks the center of the potential a small distance, a, to one side. It takes him a time T to recover and when he has done so he immediately puts the center back where it was.
A) Find, to lowest order in a, the probability that the oscillator will now be in its ground state.
B) Find, to lowest order in a, the probability that the oscillator will now be in its second excited state.


I know that there are two sudden approximations that can be made, the first after he coughs, and the second after he moves the center back. I was thinking Hi = -hbar^2/2m * d^2 phi/dx^2 + 1/2 m w^2 x^2. For the first sudden approximation, the x^2 would be replaced by (x-a)^2, and then it would return to x^2 for the second approximation. I think I'm not sure where the a fits into the calculation, and how to find the answer to the lowest order in a.
 
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First step, you will need to find the first order expansion using perturbation theory. Use the perturbed potential:

[tex]V = \frac{1}{2}m\omega^2 (x-a)^2- \frac{1}{2}m\omega^2x^2[/tex]

And expand the the wavefunction to first order in 'a' by finding,

[tex]|n'> = |n>+\sum_{k\ne n}|k>\frac{<k|V|n>}{E_n - E_k}[/tex]

Once you have that you will have to make use of the fact that the change in the potential was sudden.
 
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