Proving the Isomorphism Property of the Spinor Map in SL(2,C) and SO(3,1)

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SUMMARY

The discussion focuses on proving the isomorphism property of the spinor map between SL(2,C) and SO(3,1). The explicit forms of the isomorphism are given by the equations \textbf{x}=\overline{\sigma}_{\mu}x^{\mu} and x^{\mu}=\frac{1}{2}tr(\sigma^{\mu}\textbf{x}). The linear map is defined as \textbf{x}'=A\textbf{x}A^{\dagger}, leading to the relationship x'^{\mu}=\phi(A)^{\mu}_{\nu}x^{\nu}. The user seeks to prove that \phi(AB)=\phi(A)\phi(B), referencing Mueller-Kirsten and Wiedemann's book "Supersymmetry" for further details.

PREREQUISITES
  • Understanding of group theory, specifically SL(2,C) and SO(3,1)
  • Familiarity with linear algebra concepts, including matrix operations and traces
  • Knowledge of spinor representation and its applications in physics
  • Basic understanding of homomorphisms in mathematical structures
NEXT STEPS
  • Study the properties of the spinor map in detail
  • Review the proof of the isomorphism property in Mueller-Kirsten and Wiedemann's "Supersymmetry"
  • Explore applications of SL(2,C) and SO(3,1) in theoretical physics
  • Learn about the implications of the isomorphism in quantum mechanics and relativity
USEFUL FOR

The discussion is beneficial for theoretical physicists, mathematicians specializing in group theory, and students studying the relationship between spinors and spacetime symmetries.

gentsagree
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In the context of the homomorphism between SL(2,C) and SO(3,1), I have that

\textbf{x}=\overline{\sigma}_{\mu}x^{\mu}

x^{\mu}=\frac{1}{2}tr(\sigma^{\mu}\textbf{x})

give the explicit form of the isomorphism, where \textbf{x} is a 2x2 matrix of SL(2,C) and x^{\mu} a 4-vector of SO(3,1).

Considering the linear map (the spinor map)

\textbf{x}\rightarrow\textbf{x}'=A\textbf{x}A^{\dagger}

one can show that the 4-vectors on the SO(3,1) side are also linearly related by

x'^{\mu}=\phi(A)^{\mu}_{\nu}x^{\nu}

where it is easy to show that

\phi(A)^{\mu}_{\nu}=\frac{1}{2}tr(\sigma^{\mu}A\overline{\sigma}_{\nu}A^{\dagger})

I understand all this, but I want to prove that \phi(AB)=\phi(A)\phi(B). How would I go about doing this? I tried a few things but not very successfully.
 
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I can't copy paste the proof here, I can only tell you where to find it: Mueller-Kirsten + Wiedemann's <Supersymmetry> (WS, 1987), pages 66 and 67.
 
Thanks a lot dextercioby, the book is really helpful!
 

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