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JD_PM
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- TL;DR Summary
- I want to understand the usefulness of obtaining the Cartan subalgebra
I was studying the ##n##-dimensional harmonic oscillator, whose Hamiltonian is
$$\hat H = \sum_{j=1}^{n} \Big( \frac{1}{2m} \hat p_j^2 + \frac{\omega^2 m}{2} \hat q_j^2 \Big)$$
The ladder operators are
$$a_{\pm} = \frac{1}{\sqrt{2 \hbar m \omega}} ( \mp ip + m \omega q)$$
And came across an exercise related to it that states the following:
'Determine the Cartan subalgebra (i.e. the maximal abelian subset of these operators; the maximal number of operators ##a_i^{\dagger} a_j## which mutually commute). Hint: there are ##n## of them. Show also that the energy eigenstates are also eigenstates of the elements of this abelian subset.'
Before even attempting the exercise I need to understand the usefulness of determining the Cartan subalgebra.
Could you please shed some light on why is useful to determine it (i.e. why is it useful to determine the maximal number of operators ##a_i^{\dagger} a_j## which mutually commute)?
Thank you.
$$\hat H = \sum_{j=1}^{n} \Big( \frac{1}{2m} \hat p_j^2 + \frac{\omega^2 m}{2} \hat q_j^2 \Big)$$
The ladder operators are
$$a_{\pm} = \frac{1}{\sqrt{2 \hbar m \omega}} ( \mp ip + m \omega q)$$
And came across an exercise related to it that states the following:
'Determine the Cartan subalgebra (i.e. the maximal abelian subset of these operators; the maximal number of operators ##a_i^{\dagger} a_j## which mutually commute). Hint: there are ##n## of them. Show also that the energy eigenstates are also eigenstates of the elements of this abelian subset.'
Before even attempting the exercise I need to understand the usefulness of determining the Cartan subalgebra.
Could you please shed some light on why is useful to determine it (i.e. why is it useful to determine the maximal number of operators ##a_i^{\dagger} a_j## which mutually commute)?
Thank you.