Calculating Beta Function for Scalar QCD Theory

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SUMMARY

The discussion focuses on calculating the beta function for scalar Quantum Chromodynamics (QCD) theory, specifically at one loop for general SU(N) groups. The Lagrangian for scalar QCD is established as: (\partial_\mu \phi^a)^\dagger (\partial^\mu \phi^a) - m^2 \phi^{a \dagger} \phi^a - \frac{\lambda}{4}(\phi^{a\dagger} \phi^a)^2, which is modified by replacing partial derivatives with covariant derivatives. The gauge field Lagrangian is also included to complete the formulation. Srednicki's textbook is recommended for further insights into scalar electrodynamics.

PREREQUISITES
  • Understanding of Lagrangian mechanics in quantum field theory
  • Familiarity with SU(N) symmetry groups
  • Knowledge of Feynman rules and diagram calculations
  • Basic principles of gauge theory
NEXT STEPS
  • Study the derivation of the Lagrangian for scalar QCD in detail
  • Learn how to calculate one-loop diagrams using Feynman rules
  • Explore the beta function in quantum field theories
  • Read Srednicki's textbook chapters on scalar electrodynamics for comparative insights
USEFUL FOR

The discussion is beneficial for theoretical physicists, graduate students in quantum field theory, and researchers focusing on gauge theories and their applications in particle physics.

abrata
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Hi all,

I am currently trying to calculate the beta function for scalar QCD theory (one loop for general su(n)).

I therefore need to calculate the Feynman rules in order to apply them to the one loop diagrams. Unfortunately I am getting very confused with what the Lagrangian for scalar QCD should be. If anyone knows of some clear examples of this Lagrangian and possibly the derivation of the corresponding Feynman rules and diagrams I would be very appreciated.

Many thanks
Abrata
 
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First start with the Lagrangian for a scalar field with an internal SU(N) symmetry:

(\partial_\mu \phi^a)^\dagger (\partial^\mu \phi^a) - m^2 \phi^{a \dagger} \phi^a - \frac{\lambda}{4}(\phi^{a\dagger} \phi^a)^2

Then replace the partial derivatives with covariant derivatives:

(D_\mu \phi^a)^\dagger (D^\mu \phi^a) - m^2 \phi^{a \dagger} \phi^a - \frac{\lambda}{4}(\phi^{a\dagger} \phi^a)^2

where ##D_\mu \phi^a = \partial_\mu \phi^a - i g T^{a b} \phi^b##. Add in the gauge field Lagrangian and you have the Lagrangian for scalar QCD.

Srednicki's textbook has some chapters on scalar electrodynamics, which might help you.
 

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