Quantum harmonic oscillator with harmonic perturbation

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SUMMARY

The discussion focuses on deriving the ground state energy series E(a) for a harmonic oscillator with a harmonic perturbation described by the Hamiltonian H = p²/2 + x²/2 + a x²/2. The exact solution is known to converge to 1/2√(1+a) for |a| < 1. Participants confirm the applicability of Rayleigh-Schrödinger perturbation theory, noting the complexity of calculating higher-order corrections beyond the second order. The conversation emphasizes the need for a more straightforward method to obtain the n-th order perturbation series without relying on diagrams.

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically harmonic oscillators.
  • Familiarity with perturbation theory, particularly Rayleigh-Schrödinger theory.
  • Knowledge of ladder operators and their application in quantum mechanics.
  • Basic proficiency in series convergence and mathematical analysis.
NEXT STEPS
  • Explore advanced techniques in perturbation theory, focusing on Kato's theory.
  • Research ladder operator methods for calculating matrix elements in quantum systems.
  • Study the derivation of higher-order corrections in perturbation series.
  • Investigate alternative approaches to perturbation theory that simplify calculations.
USEFUL FOR

Students and researchers in quantum mechanics, particularly those studying perturbation theory and harmonic oscillators, will benefit from this discussion.

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Homework Statement



Let's consider a harmonic oscillator with a harmonic perturbation:
H = \frac{p^2}{2} + \frac{x^2}{2} + a \frac{x^2}{2}.
Exact solution is known, but we want to derive it using perturbation theory. More specifically, suppose we want to obtain a series for the ground state energy E(a). This series is known to be a convegent one (when |a| &lt; 1) with sum equal to the exact answer (1/2 \sqrt{1+a}). We want to comfirm this fact by a direct calculation.

Homework Equations

and

The Attempt at a Solution



Well-knows recurrence relations of Rayleigh-Schrödinger theory are applicable, and I've manually checked first five orders. The calculations quickly become very cumbersome, and there seems to be no easy way to obtain a general expression for n-th order (known in advance from the exact answer).

What is the most straightforward way to obtain this series? Will the Kato's theory be of any help in this case?

Thank you in advance.
 
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Are you using a ladder operator approach ? The calculations should be the simplest.
 
Sure, I use them to calculate matrix elements of perturbation. This part of calculation is indeed simple. What seems to be not simple is the calculation of the n-th order of perturbation series and not just 1st and 2nd like most textbooks do.

1st order correction is A |2\rangle, 2nd order - B |2\rangle + C |4\rangle, 3rd order - D |2\rangle + F |4\rangle + G |6\rangle and so on. The number of terms grows with n.

There should be an elegant way to do the calculation even in the framework of an "old" perturbation theory. I deliberately avoid using diagramms here.
 

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