Conformal Anomaly Actions and Dilaton Interactions

Abstract

A number of computational results concerning quantum conformal symmetry is presented. After a review of the connection between conformal symmetry for a Lagrangian field theory in flat space and Weyl symmetry for the same system embedded in a gravitational background, which is discussed in chapter 1, in chapter 2 the 3 energy momentum tensors correlation function is explicitly computed in three free field theories in 4 dimensions; the result is given for two of the three operators on the mass-shell. In chapter 3 a general method to map Green functions built in position space on the ground of symmetry requirements to momentum space, where they can be computed in terms of Feynman diagrams, is developed and discussed: an "integrability" condition, allowing to decide whether a certain correlator can exist within a Lagrangian theory, is derived. Chapter 4 discusses the possible phenomenological implications of the conformal anomaly pole which shows up in the 3 point Green function of one energy momentum tensor with two gauge currents and is interpreted as the perturbative signature of the pseudo-Goldstone boson of conformal symmetry, the dilaton. In chapter 5 we present the computation of the completely traced 4 point function of the energy momentum tensor with a method that exploits the relation between 1-loop counterterms and conformal anomalies, completely bypassing perturbative computations with Feynman diagrams. Later in chapter 6, an algorithm is developed which allows to compute recursively the completely traced Green functions of any number of energy momentum tensors in any renormalization scheme, starting from the dilaton Wess-Zumino action for conformal anomalies. This is derived by applying the Weyl-gauging procedure to the 1-loop counterterms in dimensional regularization. The result is explicitly derived and tested in 2, 4 and 6 dimensions.