Abstract

After showing how to prove the integrated c-theorem within the functional RG framework based on the effective average action, we derive an exact RG flow equation for Zamolodchikov's c-function in two dimensions by relating it to the flow of the effective average action. In order to obtain a non-trivial flow for the c-function, we will need to understand the general form of the effective average action away from criticality, where nonlocal invariants, with beta functions as coefficients, must be included in the ansatz to be consistent. We then apply our construction to several examples: exact results, local potential approximation and loop expansion. In each case we construct the relative approximate c-function and find it to be consistent with Zamolodchikov's c-theorem. Finally, we present a relation between the c-function and the (matter induced) beta function of Newton's constant, allowing us to use heat kernel techniques to compute the RG running of the c-function.

Highlights

  • The renormalization group (RG) underlies most of our modern understanding of quantum and statistical field theories [1, 2]

  • The main purpose of this paper is to move the first steps necessary in order to give a bridge between these two general results: the c-theorem and the computation of universal quantities related to the integrated flow between fixed points, and the functional renormalization group (fRG) formalism based on the exact flow for the effective average action (EAA)

  • In this work we have explored a new way to study the flow of the c-function within the framework of the functional RG based on the effective average action (EAA)

Read more

Summary

Introduction

The renormalization group (RG) underlies most of our modern understanding of quantum and statistical field theories [1, 2]. Note that the difference between the two central charges is an intrinsic quantity (intrinsic meaning independent of spurious contributions like scheme dependence of the renormalization procedure), so the content of the theorem is highly nontrivial In this case a complete RG analysis requires the ability to follow the flow arbitrarily far away from a fixed point. The main purpose of this paper is to move the first steps necessary in order to give a bridge between these two general results: the c-theorem and the computation of universal quantities related to the integrated flow between fixed points (that is, to global properties of theory space), and the fRG formalism based on the exact flow for the EAA.

The integrated c-theorem
Weyl-invariant quantization and functional measures
CFT action on curved background
Anomaly matching from the path-integral
Proof of the integrated c-theorem
Flow equation for the c-function
The fRG flow equation for the c-function
General form of the effective average action
The local ansatz and its limitations
Nonlocal ansatz and the scale anomaly
Checking exact results
Massive deformation of the Gaussian fixed point
G m 2k
Massive deformation of the Ising fixed point
The c-function in the local potential approximation
Flow between the Gaussian and Ising fixed points
Sine-Gordon model
The c-function in the loop expansion
Zamolodchikov’s metric: diagrammatics
Non-unitary theories
Relation between ck and βGk
Minimally coupled scalar
Self-interacting scalar
Conclusions
A Loop expansion from the fRG
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call