3-d harmonic oscillator and SU(3) - how to imagine it?

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Discussion Overview

The discussion centers on the relationship between the 3-dimensional harmonic oscillator and its SU(3) symmetry. Participants explore how the symmetry manifests in the context of the oscillator's eigenstates and the role of the Gell-Mann generators. The conversation includes theoretical considerations and references to literature.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • François states that the 3-dimensional harmonic oscillator exhibits SU(3) symmetry due to its spherical symmetry and questions how the eight generators of SU(3) act on the eigenstates.
  • Another participant provides links to resources that may help in understanding the topic but does not elaborate further.
  • A participant clarifies that the generators are elements of the Lie algebra su(3) and that they correspond to infinitesimal symmetry transformations of the Hamiltonian, which may not necessarily transform eigenstates to eigenstates.
  • François mentions that the Gell-Mann matrices are one representation of the SU(3) generators and questions the reason for having eight generators.
  • François references D M Fradkin's work, explaining that the eight generators arise from the symmetries of angular momentum and the Runge-Lentz tensor, which together account for the eight generators in the context of the harmonic oscillator.
  • Another participant notes that while the SU(N) symmetry is evident in the holomorphic representation of the Hamiltonian, it does not provide much insight into the underlying physics and mentions the presence of su(2) sub-algebras within su(3).

Areas of Agreement / Disagreement

Participants express various viewpoints regarding the nature of the SU(3) symmetry and the role of its generators, indicating that multiple competing views remain. The discussion does not reach a consensus on the specifics of how the generators act on the eigenstates.

Contextual Notes

The discussion highlights the complexity of the relationship between the harmonic oscillator and its symmetry, with references to different representations and the mathematical structure of SU(3). There are unresolved aspects regarding the transformation properties of the eigenstates and the implications of the generators.

franoisbelfor
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The 3-dimensional harmonic oscillator has SU(3) symmetry. This is stated in many papers. It seems to be due to the spherical symmetry of the system. (After all, the idea of a 3d harmonic oscillator is that a mass is attached to the origin with a spring, and that the mass can move in 3 dimensions, with no gravity involved.)

But I have an issue. If this system has SU(3) symmetry, the 8 generators of SU(3) must somehow act on the various eigenstates. How exactly does this happen? Is there a book or a paper on this?

For example, the eight Gell-Mann generators of SU(3) must transform the states of the harmonic oscillator. What do they do? Do they rotate the state? How? Why are there 8 of them?

Thank you for any advice in this matter.

Cheers

François
 
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franoisbelfor said:
But I have an issue. If this system has SU(3) symmetry, the 8 generators of SU(3) must somehow act on the various eigenstates.

The generators are elements of the lie algebra su(3), not the group SU(3). If we take a step away from matrices and imagine the actions of the generators as abstract operators then the generators correspond to infinitesimal symmetry transformations of the Hamiltonian, therefore they do not necessarily transform eigenstates to eigenstates.

For example, the eight Gell-Mann generators of SU(3) must transform the states of the harmonic oscillator.

I just want to point out that the Gell-Mann matrices are one of many equivalent representations for the generators of SU(3).

Why are there 8 of them?

Why 8 generators? Determine the dimension of SU(3), and determine the dimension of the tangent space at the identity, and tell me how many vectors are needed to span this tangent space (the answer is 8).
 
franoisbelfor said:
But I have an issue. If this system has SU(3) symmetry, the 8 generators of SU(3) must somehow act on the various eigenstates. How exactly does this happen? Is there a book or a paper on this?

For example, the eight Gell-Mann generators of SU(3) must transform the states of the harmonic oscillator. What do they do? Do they rotate the state? How? Why are there 8 of them?

Thank you for any advice in this matter.

Cheers

François

D M Fradkin discussed the physics very clearly in the 1964 American Journal of Physics, I found out. The symmetries are the angular momentum and the Runge-Lentz tensor (for the harmonic oscillator in 3d, it is a tensor, not a vector). That makes 3+5=8 generators

The generators shift energy among the 3 linearly independent oscillators, keeping the total energy constant.

François
 
Thanks, François. That's insightful.

In any case, it's easy to see where the SU(N) comes from, but not terribly illuminating. If you work in the holomorphic representation, then the Hamiltonian is H = a^\dagger a which clearly has an SU(N) symmetry. This is also a very elaborate way of determining the degeneracy of such a harmonic oscillator.

Of course, there's the unrelated issue that su(3) contains a bunch of su(2) sub-algebras.
 

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