Representation symmetric, antisymmetric or mixed

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SUMMARY

This discussion focuses on determining the nature of representations in the context of Lie groups, specifically SO(5). The key takeaway is that a representation is symmetric if the parameter b equals zero and antisymmetric if a equals zero, as per the tensor product notation (a,b) = ⊗_a (1,0) ⊗_b (0,1). The conversation also highlights the process of forming higher rank tensors from the vector representation and the importance of the invariant totally antisymmetric quantity εabcde for further reduction of representations.

PREREQUISITES
  • Understanding of Lie groups and their representations
  • Familiarity with tensor products in the context of representation theory
  • Knowledge of the symmetric group Sk and Young's diagrams
  • Experience with Georgi's "Lie Algebras in Particle Physics" for foundational concepts
NEXT STEPS
  • Study the properties of the invariant totally antisymmetric tensor εabcde in detail
  • Learn about the reduction of representations using traces and symmetrization techniques
  • Explore the implications of Young's diagrams for representations of the symmetric group Sk
  • Read additional texts on representation theory beyond Georgi's book for broader insights
USEFUL FOR

This discussion is beneficial for physicists, mathematicians, and students specializing in representation theory, particularly those focusing on Lie groups and their applications in particle physics.

JorisL
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Hi,

While studying Lie groups and in particular the representations I have some trouble with determining whether a representation is a symmetric, antisymmetric or mixed tensor product of the fundamental representations. I'm working with SO(5) to get an understanding about the actual mechanisms.

I used Georgi's book Lie Algebras in Particle Physics. Do I understand correctly when saying that a representation, (a,b) = \bigotimes_a (1,0)\bigotimes_b (0,1) is symmetric if b = 0, antisymmetric if a = 0? Or is there more to it?


Joris
 
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JorisL said:
While studying Lie groups and in particular the representations I have some trouble with determining whether a representation is a symmetric, antisymmetric or mixed tensor product of the fundamental representations. I'm working with SO(5) to get an understanding about the actual mechanisms.

For SO(n), start with the vector representation, Va, a = 1,... n. Form higher rank tensors by taking tensor products, Vabc... k. These representations are reducible, and may be reduced by taking traces and by symmetrizing the indices in all possible ways. For example for two indices, Vab may be reduced into a symmetric part (Vab + Vab)/2 and an antisymmetric part (Vab - Vab)/2.

In general, each part of a k-rank tensor corresponds to a representation of the symmetric group Sk. For more than two indices, some of these representations have "mixed" symmetry.

In particular for SO(5) there is an invariant totally antisymmetric quantity εabcde that may be used for further reduction. Multiplication by this quantity will convert a totally antisymmetric set of three indices to an antisymmetric set of only two. In terms of Sk this means that the Young's diagrams are restricted to having at most two rows.
 
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So if I can show that the contractition of the totally antisymmetric tensor with the rep vanishes I'd know I'm dealing with a totally symmetric rep? Or is there a more suitable way?

Also, can you recommend an extra text? Because the Georgi text is suitable for examples, the generalities I find less obvious.
 

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