Undergrad The propagator of the gauge field

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SUMMARY

The discussion focuses on deriving the propagator of the gauge field from the free massive vector boson Lagrangian, specifically given by 𝓛W = - \frac{1}{4} (\partial_\mu W^\dagger_\nu - \partial_\nu W_\mu^\dagger ) (\partial^\mu W^\nu - \partial^\nu W^\mu ) + M^2_W W^\dagger_\mu W^\mu. The propagator in momentum space is expressed as i Δμν = - i \frac{gμν - kμ kν/M^2_W}{k² - M²_W}. The discussion emphasizes the need to apply the textbook formula for Green functions and perform a Fourier transformation to switch to momentum representation.

PREREQUISITES
  • Understanding of Quantum Field Theory (QFT)
  • Familiarity with Lagrangian mechanics
  • Knowledge of Fourier transformations
  • Concept of Green functions in quantum physics
NEXT STEPS
  • Study the derivation of propagators in Quantum Field Theory
  • Learn about the application of Fourier transformations in physics
  • Explore the concept of Green functions and their significance in QFT
  • Review standard textbooks on Quantum Field Theory for detailed examples
USEFUL FOR

Students and researchers in theoretical physics, particularly those focusing on Quantum Field Theory and gauge theories, will benefit from this discussion.

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Hi,

I read in a QFT book that the free massive vector boson Lagrangian is

## \mathcal{L}_W = - \frac{1}{4} (\partial_\mu W^\dagger_\nu - \partial_\nu W_\mu^\dagger ) (\partial^\mu W^\nu - \partial^\nu W^\mu ) + M^2_W W^\dagger_\mu W^\mu ##

gives the propagator in momentum space by:

## i \Delta_{\mu\nu} = - i \frac{g_{\mu\nu - k_\mu k_\nu/M^2_W}}{k^2-M^2_W} ##

Any help how to derive the formula of the propagator from the Lagrangian ?
 
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This is standard textbook material. The propagator is the unconnected two point Green function. To obtain Green functions from the action you need to apply the textbook formula and then switch to momentum representation via a Fouriert transformation of the propagator in the coordinate representation.
 
Ok, I'm asking how to do so, or please mention a good reference for ..
 

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