Proofs of Group Theory for Theoretical Physicists - Daniel

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SUMMARY

This discussion focuses on the need for rigorous mathematical proofs related to group theory concepts relevant to theoretical physics. Key points include the lack of nontrivial finite dimensional unitary linear irreducible representations (irreps) for noncompact Lie groups, the full reducibility of linear representations of simply connected Lie groups, and the bijective correspondence between unitary linear irreps and self-adjoint irreps of the corresponding Lie algebra. The discussion highlights the importance of these concepts in understanding space-time symmetries in quantum mechanics, particularly through the Wigner-Weyl method. A recommended resource is "Representation Theory (A First Course)" by Fulton and Harris, specifically Lecture 8 onwards.

PREREQUISITES
  • Understanding of Lie groups and Lie algebras
  • Familiarity with unitary representations in quantum mechanics
  • Knowledge of the Wigner-Weyl method in quantum mechanics
  • Basic concepts of representation theory
NEXT STEPS
  • Study the proofs of theorems related to noncompact Lie groups and their representations
  • Explore the full reducibility of representations in simply connected Lie groups
  • Investigate the correspondence between unitary linear irreps and self-adjoint irreps
  • Read "Representation Theory (A First Course)" by Fulton and Harris, focusing on Lecture 8
USEFUL FOR

Theoretical physicists, mathematicians specializing in representation theory, and students seeking a deeper understanding of the mathematical foundations of quantum mechanics.

dextercioby
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It's always annoying when one finds in books (written by (theoretical) physicists for (theoretical) physics students) statements like those below without a mere cross-reference for a mathematically-rigurous proof. And that's what I'm searching for right now: either point me to some books, or post the proofs right here (that would be perfect). So here's what's been bugging me lately:

1. A noncompact Lie group has no nontrivial finite dimensional unitary linear irreps.
2. The linear representations of a simply connected Lie group are fully reducible.
3. The unitary linear irreps of a simply connected Lie group can be put in bijective correspondence with (essentially) selfadjoint irreps of the corresponding Lie algebra.
4. The Theorem of Nelson. The only reference for a proof that i found is the original article by Nelson, but, unfortunately, it's not within my reach.

The relevance of this thread: these mathematical results are fundamental in understanding the concept of implementing space-time symmetries in the Hilbert space language of QM through the so-called "Wigner-Weyl method".

Daniel.
 
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The underlying idea is the following:

any lie group homomorphism is determined uniquely by the induced lie algebra map.

See Fulton and Harris, Representation Theory (A First Course) Springer GTM 129 (1991) Lecture 8 onwards.

I don't know that it'll answer all your questions, but it seems like it'll be a start in the right direction. It is quite a cheap and readily available book. You library should have a copy.
 

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