Can there by a theory that is both UV and IR stable?

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SUMMARY

The discussion confirms that a theory can be both ultraviolet (UV) and infrared (IR) stable, specifically citing the ##g\phi^4## theory in three dimensions as a concrete example. The 1-loop beta function for the coupling constant ##g## is defined as $$ \beta(g) = \frac{1}{16\pi^2} ( - g + 3 g^2)$$, which reveals two fixed points: the free theory at ##g=0## and the interacting theory at ##g\sim 1/3##. The analysis shows that as the scale ##\mu## approaches infinity, the coupling constant approaches zero, indicating UV stability, while as ##\mu## approaches zero, the coupling constant approaches ##1/3##, indicating IR stability, known as the Wilson-Fisher fixed point.

PREREQUISITES
  • Understanding of quantum field theory concepts
  • Familiarity with renormalization group (RG) flow
  • Knowledge of beta functions and fixed points
  • Basic mathematical skills in calculus and differential equations
NEXT STEPS
  • Study the implications of the Wilson-Fisher fixed point in quantum field theory
  • Explore higher-loop corrections in the ##g\phi^4## theory
  • Learn about the renormalization group flow in different dimensions
  • Investigate other models that exhibit both UV and IR stability
USEFUL FOR

The discussion is beneficial for theoretical physicists, particularly those specializing in quantum field theory, as well as graduate students seeking to deepen their understanding of stability in quantum theories.

metroplex021
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The question is in the title: is it possible for a theory to be both UV and IR stable? And concrete models would be much appreciated!
 
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If you mean: can a theory have a stable RG fixed point in both the UV and IR, the answer is yes. A concrete example is ##g\phi^4## theory in 3 dimensions. The 1-loop beta function for ##g## is

$$ \beta(g) = \frac{1}{16\pi^2} ( - g + 3 g^2).$$

There are 2 fixed points: the free theory at ##g=0## and an interacting theory at ##g\sim 1/3## (higher loops would be expected to change the position slightly). We can integrate the beta function to get

$$ g(\mu) = \frac{ 16\pi^2 g(\Lambda) }{ 48\pi^2 g(\Lambda) - \frac{\mu}{\Lambda} ( g(\Lambda) -1)}.$$

For fixed ##\Lambda##, we see that taking the scale to ##\mu \rightarrow \infty## sends ##g(\mu) \rightarrow 0##, so this fixed point corresponds to the UV. Similarly, sending ##\mu\rightarrow 0## takes us to ##g(\mu)\rightarrow 1/3##, so this is an IR fixed point (generally known as the Wilson-Fisher fixed point).
 
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