Abstract

A new class of conformal field theories is presented, where the background gravitational field is conformally flat. Conformally flat (CF) spacetimes enjoy conformal properties quite similar to the ones of flat spacetime. The conformal isometry group is of maximal rank and the conformal Killing vectors in conformally flat coordinates are {\em exactly} the same as the ones of flat spacetime. In this work, a new concept of distance is introduced, the {\em conformal distance}, which transforms covariantly under all conformal isometries of the CF space. It is shown that precisely for CF spacetimes, an adequate power of the said conformal distance is a solution of the non-minimal d'Alembert equation.

Highlights

  • The importance of flat spacetime conformal field theories (CFT) in theoretical physics can be hardly exaggerated

  • The present paper aims to generalize this whole setup of conformal field theories to a particular instance of curved spacetimes, namely to conformally flat (CF) spacetimes

  • When the spacetime is such that there exists a nonvanishing set of conformal Killing vectors (CKV), there is another definition, which coincides with a function of the former in flat spacetime as well as in spacetimes of constant curvature

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Summary

INTRODUCTION

The importance of flat spacetime conformal field theories (CFT) in theoretical physics can be hardly exaggerated (cf. for example, [1,2]). They are fixed points of the renormalization group, and as such, they are in some sense, the simplest of all quantum field theories. III, we discuss a new concept of distance, which related to the geodesic distance (Synge’s world function) is not identical to it This distance, dubbed by us as conformal distance, transforms covariantly under all conformal isometries of the CF space, and gets a very simple expression in the natural coordinate system. We end up with our conclusions and suggestions for future work

THE GROUP OF CONFORMAL ISOMETRIES OF CF SPACETIMES
CONFORMAL DISTANCE
CONFORMAL FIELDS IN CF SPACETIMES
Þμ : ð4:6Þ
DIRAC FERMIONS
CFT CORRELATORS
CONCLUSIONS
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