Commutation Relations, 2D Harmonic Oscillator

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SUMMARY

The discussion focuses on the calculation of the commutation relations involving the Hamiltonian ##\hat H_0 = \hbar \omega (\hat a_x \hat a_x^{\dagger} + \hat a_y \hat a_y^{\dagger} + 1)## and the angular momentum operator ##\hat L = i \hbar (\hat a_y^{\dagger} \hat a_x - \hat a_x^{\dagger} \hat a_y)## for a two-dimensional harmonic oscillator. The user seeks a more efficient method to compute ##\hat H_0 \hat L | n_1, n_2 \rangle## and ##\hat L \hat H_0 | n_1, n_2 \rangle##, expressing concerns about the complexity of the calculations. The discussion highlights the relationship between the Hamiltonian and the total quantum numbers ##n_1 + n_2##, suggesting that the operator ##\hat L## does not change this total.

PREREQUISITES
  • Understanding of quantum mechanics, specifically harmonic oscillators
  • Familiarity with operator algebra in quantum mechanics
  • Knowledge of commutation relations and eigenstates
  • Experience with the ladder operators ##\hat a_x## and ##\hat a_y##
NEXT STEPS
  • Explore the derivation of commutation relations for angular momentum operators
  • Study the properties of number states in quantum mechanics
  • Investigate the implications of the total quantum number conservation in harmonic oscillators
  • Learn about the simplification techniques for operator products in quantum mechanics
USEFUL FOR

Students and researchers in quantum mechanics, particularly those studying harmonic oscillators and angular momentum, will benefit from this discussion. It is also valuable for anyone looking to enhance their understanding of operator algebra in quantum systems.

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Homework Statement


Consider a two-dimensional harmonic oscillator, described by the Hamiltonian

##\hat H_0 = \hbar \omega (\hat a_x \hat a_x ^{\dagger} + \hat a_y \hat a_y^{\dagger} + 1)##

Calculate ##\hat H_0 \hat L | n_1, n_2 \rangle## and ##\hat L \hat H_0 |n_1, n_2 \rangle##. What does this imply for ##[\hat H_0 , \hat L]##

Homework Equations

The Attempt at a Solution


[/B]
I can solve this problem by "brute force", having shown that ##\hat L = \hat x \hat P_y - \hat y \hat P_x = i \hbar (\hat a_y^{\dagger} \hat a_x - \hat a_x ^{\dagger} \hat a_y)##. I can apply one operator and then the other, but the results are messy making me think this can be done in a smarter manner.

Trying to combine these operators into a single simplified operator gives me

##H_0 \hat L = i \hbar^2 \omega (\hat a_x ^{\dagger} \hat a_x (\hat a_y ^{\dagger} \hat a_x - \hat a_x ^{\dagger} \hat a_y) + \hat a_y^{\dagger} \hat a_y (\hat a_y^{\dagger} \hat a_x - \hat a_x^{\dagger} \hat a_y) + (\hat a_y^{\dagger} \hat a_x - \hat a_x^{\dagger} \hat a_y))##

I need to deal with this ##(\hat a_y ^{\dagger} \hat a_x - \hat a_x ^{\dagger} \hat a_y)## term but I am unsure of how to do it. I know that ##[\hat a_i, \hat a_i^{\dagger}] = 1## and that the x and y operators are mutually commuting.

If I set ##\hat N = \hat a_y^{\dagger} \hat a_x##, then ##(\hat a_y ^{\dagger} \hat a_x - \hat a_x ^{\dagger} \hat a_y) = [\hat N, \hat N^{\dagger}]## but the numbered states or not eigenstates of my invented operator...

So, is there anything I can realize to make this problem less of an accounting exercise?

I hope it's clear what I'm asking; I can solve this problem, but it does not feel efficient.

Thank you for your help!
 
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Do you realize that the Hamiltonian on a number state ##\mid n_1,n_2\rangle ## has eigenvalue related to the total ##n_1+n_2##?
\begin{align*} H& = \hbar \omega (a_x ^{\dagger}a_x + a_y^{\dagger}a_y \ + 1) \\
H &= \hbar\omega(N_x + N_y + 1)\\
H|n_1, n_2> &= \hbar\omega(n_1 + n_2+1)|n_1, n_2>\end{align*}
So a question you can ask is "does ##L## change the total ##n_1 + n_2## ?"
You can examine the operator ##L## or try it out.
 

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