# What is the connection between Conformal Field Theory and Renormalization group in QFT?

As I know, the fundamental concept of QFT is Renormalization Group and RG flow. It is defined by making 2 steps:

1. We introduce cutting-off and then integrating over "fast" fields $\widetilde{\phi}$, where $\phi=\phi_{0}+\widetilde{\phi}$.

2. We are doing rescaling: $x\to x/L$: $\phi_{0}(x)\to Z^{-1/2}(L)\phi(x)$.

This procedure defines RG flow on the manifold of quasi local actions: $\frac{dA_{l}}{dl}=B\{A_{l}\}$.

In this approach we have such notions as crytical points $A_{*}$, relevant and irrelevant fields, Callan–Symanzik equation etc, and we can apply it, say, to phase transitions.

Also we can introduce stress-energy tensor $T^{\mu\nu}$. And, as far as i know, if we consider scale transformations $x^{\mu} \to x^{\mu}+\epsilon x^{\mu}$ , we can obtain Callan–Symanzik equation, and if the theory have a crytical point: $\beta^{k}(\lambda^{k})=0$, then trace of stress energy tensor $\Theta(x)=T^{\mu}_{\mu}=0$, so our correlation functions have symmetry at scaling transformation.

So the question is: As far as I know, at this point they somehow introduce conformal transformations and Conformal Field Theory. Can you explain, what place in Quantum Field Theory CFT takes? (I mean connection between them, sorry if the question is a little vague or stupid). How it relates to the RG approach exactly? (This point is very important for me). Maybe some good books?

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Well it seems that you have all pretty much figured out: conformal field theories are a subset of quantum field theories corresponding to the point(s) at which the beta function vanishes. It may seem not much interesting to look at subset of 'vanishing measure' in the space of quantum field theories but actually: conformal symmetry is a really strong constraint and is enough to solve exactly some theories in 2d, and you can derive results near critical points from the so called conformal perturbation theory. The main references are Ginsparg lecture notes (arXiv) and thee book by DiFran & al. –  Learning is a mess Apr 21 '14 at 22:23
@Learningisamess: There's a lot of good writing about CFT which doesn't stick to the comforts of 2 dimensions. See, e.g., sites.google.com/site/slavarychkov or physics.ipm.ac.ir/phd-courses/semester7/CFT-course-2013.pdf –  user1504 Apr 22 '14 at 0:12
@Learningisamess Thanks for explanation. Correct me please if I've misunderstood something: when we analyze QFT renormalization using RG approach, we obtain important notion as critical points. Then we introduce stress-energy tensor and obtain that it's trace equals to zero at them. But this condition allows us to introduce conformal symmetry preserving the vanishing trace and therefore Conformal Field Theory at critical points. Am I right? If so, why it wasn't introduced some analog of RG analysis based on conformal symmetry(not only in critical points)? This is due to technical difficulties? –  xxxxx Apr 24 '14 at 17:33

• Any quantum field theory which has hope of having an UV-completion can be viewed as as effective theory at point in the RG flow from an UV complete theory.

• Field theories at the UV fixed point are conformal.

• Hence all 'well-defined' field theories are either CFTs or points in the RG flow from one (UV) CFT to another CFT.

So in a sense, in Kaplan's words:

studying the space of CFTs basically amounts to studying the space of all well-defined QFTs

So that's one way of seeing the place of CFTs in general QFTs.

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