Running Coupling: QF Theory, Asymptotic Freedom & RG Law

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SUMMARY

The discussion centers on the concept of renormalization in Quantum Field (QF) theory, specifically addressing the introduction of a renormalization scale μ and its relationship with the coupling g(μ) as dictated by the Renormalization Group (RG) law. It highlights the paradox of how physical phenomena can vary significantly along the RG trajectory despite μ being non-physical. The conversation emphasizes that while μ does not represent the physical energy of a process, selecting μ close to the relevant energy scale can yield accurate predictions if g(μ) is small, allowing low-order perturbation theory to effectively describe physical interactions.

PREREQUISITES
  • Understanding of Quantum Field Theory (QFT)
  • Familiarity with Renormalization Group (RG) concepts
  • Knowledge of perturbation theory in quantum physics
  • Basic principles of Quantum Chromodynamics (QCD)
NEXT STEPS
  • Study the implications of Renormalization Group flow in Quantum Field Theory
  • Explore the concept of asymptotic freedom in Quantum Chromodynamics (QCD)
  • Learn about the mathematical formulation of perturbation theory
  • Investigate the physical significance of renormalization scales in particle physics
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Physicists, particularly those specializing in Quantum Field Theory and Quantum Chromodynamics, as well as students and researchers interested in the mathematical foundations and implications of renormalization and coupling behavior in high-energy physics.

anthony2005
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First a little intro.

The process of renormalization introduces in a QF theory a renormalization scale μ. Physical quantities do not depend on it, as a change of μ comes along with the change of the coupling g(μ) according to the RG law.

But why then the physics can change so drastically along the RG trajectory? For instance, why asymptotic freedom in QCD is attributed to the unphysical ( μ,g(μ) ) RG behaviour? The μ is not introduced as the physical energy of a given process.

Thanks
 
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Physics changes with the physical energy scale, not with μ. But if you choose μ near the relevant physical energy scale, and g(μ) happens to be small, then low orders of perturbation theory will give a good description of physics at that physical energy scale. If not, not.
 

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