Hermitian properties of the gamma matrices

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SUMMARY

The gamma matrices ##\gamma^{\mu}## are defined by the anti-commutation relation $$\{\gamma^{\mu},\gamma^{\nu}\}=2g^{\mu\nu}$$ and can be represented in various bases, including the Dirac and Weyl bases. The discussion centers on the proof of the relation $$(\gamma^{\mu})^{\dagger}\gamma^{0}=\gamma^{0}\gamma^{\mu}$$ without referencing a specific representation. It is concluded that such a proof is not feasible since any set of matrices satisfying the anti-commutation relations can be transformed by an arbitrary matrix ##\hat{A}##, and the preservation of pseudohermiticity requires ##\hat{A}## to be unitary.

PREREQUISITES
  • Understanding of gamma matrices and their properties in quantum field theory
  • Familiarity with the Dirac and Weyl representations of gamma matrices
  • Knowledge of anti-commutation relations in linear algebra
  • Basic concepts of unitary transformations in matrix theory
NEXT STEPS
  • Study the representation theory of the Lorentz group and its implications for gamma matrices
  • Explore the properties of pseudohermiticity in quantum mechanics
  • Learn about the implications of unitary transformations on matrix representations
  • Investigate the mathematical foundations of bispinor representations in quantum field theory
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The discussion is beneficial for theoretical physicists, particularly those specializing in quantum field theory, as well as mathematicians interested in the algebraic structures of gamma matrices and their applications in particle physics.

spaghetti3451
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The gamma matrices ##\gamma^{\mu}## are defined by

$$\{\gamma^{\mu},\gamma^{\nu}\}=2g^{\mu\nu}.$$

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There exist representations of the gamma matrices such as the Dirac basis and the Weyl basis.

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Is it possible to prove the relation

$$(\gamma^{\mu})^{\dagger}\gamma^{0}=\gamma^{0}\gamma^{\mu}$$

without alluding to a specific representation?
 
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I don't think so, because given any set of matrices fulfilling the anti-commutation relations, any other set
$$\tilde{\gamma}^{\mu} = \hat{A} \gamma^{\mu} \hat{A}^{-1},$$
where ##\hat{A}## is an arbitrary ##\mathbb{C}^{4 \times 4}## matrix also fulfills them. It's of course more natural to use a simple set of matrices as suggested by the representation theory of the Lorentz group behind the bispinor representation, e.g., the chiral (or Weyl) representation. The pseudohermiticity relations, are only preserved with ##\hat{A}## unitary.
 

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