Relationship between bare and renormalized beta functions

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SUMMARY

The discussion focuses on the proof of beta function universality in ##\phi^4## theory, specifically examining the relationship between bare and renormalized beta functions. It establishes that the renormalized coupling ##\lambda## is independent of the cutoff ##\Lambda##, leading to the equation $$0= \Lambda \frac {\text{d} \lambda}{\text{d} \Lambda} = -\mu \frac{\partial \lambda}{\partial \mu} + \beta^{(\text{B})}(\lambda) \frac{\partial \lambda}{\partial \lambda_0}$$. The participants seek clarification on the derivation of this relationship and inquire about the renormalization scheme utilized. A reference to RG applications in ##\phi^4## theory is provided for further reading.

PREREQUISITES
  • Understanding of quantum field theory (QFT)
  • Familiarity with renormalization group (RG) techniques
  • Knowledge of beta functions in field theories
  • Basic concepts of coupling constants in quantum physics
NEXT STEPS
  • Study the derivation of beta functions in quantum field theories
  • Explore the implications of renormalization schemes in QFT
  • Review the provided reference on RG applications in ##\phi^4## theory
  • Investigate the relationship between bare and renormalized parameters in field theories
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Researchers, theoretical physicists, and students specializing in quantum field theory, particularly those interested in renormalization techniques and beta function analysis.

Siupa
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I'm looking at a proof of beta function universality in ##\phi^4## theory, and at one point they do the following step: after imposing that the renormalized coupling ##\lambda## is independent of the cutoff ##\Lambda##, we have
$$0= \Lambda \frac {\text{d} \lambda}{\text{d} \Lambda} = \Lambda \frac {\partial \lambda}{\partial \Lambda} + \Lambda \frac{\partial \lambda_0}{\partial \Lambda} \frac{\partial \lambda}{\partial \lambda_0} \implies 0 = - \mu \frac{\partial \lambda}{\partial \mu} + \beta^{(\text{B})}(\lambda) \frac{\partial \lambda}{\partial \lambda_0}$$
This seems to imply
$$\Lambda \frac{\partial \lambda}{\partial \Lambda} = -\mu \frac{\partial \lambda}{\partial \mu}$$
Why is this true? Where does it come from? ##\lambda_0## is the bare coupling and ##\mu## the arbitrary mass scale
 
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@Siupa inline LaTeX needs to be enclosed in double dollar signs, not single ones. I have used magic moderator powers to edit your OP to fix this.
 

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