Beta functions and relevant/irrelevant operators

eherrtelle59
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Ok, I'm having some conceptual difficulty here. When discussing beta functions and the relation how these differential equations flow, I still don't quite get the difference between relevant vs. marginally relevant and irrelevant vs. marginally irrelevant.

For instance, take the β function with coupling g_s

[itex]\frac{dg^2_s}{d\ln M} = -\frac{14}{16\pi^2}g^4_s[/itex]

The solution is [itex]\frac{1}{g^2_s}=\frac{14}{16\pi^2} \ln(M/M')[/itex]
such that the theory diverges at M'. The theory's obviously asymptotically free, as when the scale M grows, the coupling g_s decreases.

So, since the beta function is negative, I know this is either irrelevant or marginally irrelevant. What's the difference?
 
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Actually, I'm wrong above.

At lower and lower energy scales M, g becomes larger and larger and therefore relevant. Why is it marginally relevant instead of relevant?
 
In case I'm being to obscure above, let's just work with QED vs. QCD.

How do you know these theories are marginally (ir)relevant as opposed to (ir)relevant?

Thanks
 

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