Gauge Boson Propagators in Spontaneously Broken Gauge Theories

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SUMMARY

The discussion focuses on the propagator for gauge bosons in spontaneously broken non-abelian gauge theories, specifically in the R_\xi gauge. The propagator is expressed as \tilde{D}^{\mu\nu}_F(k)^{ab}=\frac{-i}{k^2-M^{ab}}\left[g^{\mu\nu}-(1-\xi)\frac{k^\mu k^\nu}{k^2-\xi M^{ab}}\right], where M^{ab} is the gauge boson mass matrix and \xi is the gauge fixing parameter. The author seeks to rationalize the propagator to have matrices in the numerator and questions whether this is feasible without diagonalizing the mass matrix. The consensus indicates that diagonalization is necessary for perturbative calculations.

PREREQUISITES
  • Understanding of gauge theories, particularly non-abelian gauge theories
  • Familiarity with the R_\xi gauge and its implications
  • Knowledge of propagators in quantum field theory
  • Experience with matrix diagonalization techniques
NEXT STEPS
  • Study Peskin and Schroeder's treatment of gauge boson propagators in quantum field theory
  • Learn about diagonalization of matrices in the context of quantum field theory
  • Explore perturbative calculations in spontaneously broken gauge theories
  • Investigate alternative gauge fixing methods and their effects on propagators
USEFUL FOR

The discussion is beneficial for theoretical physicists, particularly those specializing in quantum field theory, gauge theories, and particle physics. It is also relevant for graduate students and researchers looking to deepen their understanding of gauge boson dynamics in spontaneously broken gauge theories.

TriTertButoxy
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The propagator for gauge bosons in a spontaneously broken (non-abelian) gauge theory in the R_\xi gauge is (see Peskin and Schroeder eqn. 21.53)

<br /> \tilde{D}^{\mu\nu}_F(k)^{ab}=\frac{-i}{k^2-M^{ab}}\left[g^{\mu\nu}-(1-\xi)\frac{k^\mu k^\nu}{k^2-\xi M^{ab}}\right]\,,<br />​

where M^{ab} is the gauge boson mass matrix, and \xi is the gauge fixing parameter. The matrices in the denominator should be interpreted as matrix inverses. To make perturbative calculations, I am supposed to diagonalize the mass matrix M^{ab}, and write the propagator in terms of the eigenvalues.

I would like to make my calculations as general as possible, and avoid having to go to a particular model to diagonalize the mass matrix. Is there a way to rationalize the propagator above so that the matrices are in the numerator?
 
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I would like to write the propagator as\tilde{D}^{\mu\nu}_F(k)^{ab}=\frac{-i}{k^2}\left[g^{\mu\nu}+(1-\xi)\frac{M^{ab}}{k^2-\xi M^{ab}}k^\mu k^\nu\right]\,.If this is not possible, what is the best way to proceed? Is it just necessary to choose a particular model and diagonalize the mass matrix?
 

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