Two dimensional asymmetric harmonic oscillator

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SUMMARY

The discussion centers on the two-dimensional asymmetric harmonic oscillator, specifically addressing the potential defined by V = 1/2m(Omegax)x^2 + 1/2m(Omegay)y^2. The energy of the system is expressed as E = (Nx + 1/2)hbarOmegax + (Ny + 1/2)hbarOmegay when Omegax and Omegay are unequal. Participants confirm that this formulation is correct by considering separable solutions of the wave function, ψ(x,y) = X(x)Y(y). This clarification is essential for understanding energy calculations in asymmetric systems.

PREREQUISITES
  • Understanding of harmonic oscillators in quantum mechanics
  • Familiarity with the Schrödinger equation
  • Knowledge of quantum numbers (Nx, Ny)
  • Basic concepts of wave functions and separability
NEXT STEPS
  • Study the implications of varying frequencies in two-dimensional quantum systems
  • Explore the derivation of the Schrödinger equation for asymmetric potentials
  • Learn about the role of quantum numbers in energy levels of oscillators
  • Investigate the concept of separable solutions in multi-dimensional quantum mechanics
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Students and researchers in quantum mechanics, particularly those focusing on harmonic oscillators and energy calculations in multi-dimensional systems.

JackPunchedJi
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Let's say I have a 2D harmonic oscillator:

Homework Statement


The potential is of course defined by: V = 1/2m(Omegax)x^2 + 1/2m(Omegay)y^2

Homework Equations



Generally when doing a harmonic oscillator we find that in two dimensions the energy is just:

(Nx+Ny+1)hbarOmega is the energy.

How does this change when the Omegax and Omegay are not equal?

The Attempt at a Solution



Do we simply get the energy as...

E = (Nx+1/2)hbarOmegax + (Ny+1/2)hhbarOmegay ?

That would seem logical, but would like the clarification.
 
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Your intuition is correct. You can work it out by considering a separable solution of the form \psi(x,y)= X(x)Y(y).
 

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