Abstract

We present a comprehensive analysis of the implications of conformal invariance for 3-point functions of the stress-energy tensor, conserved currents and scalar operators in general dimension and in momentum space. Our starting point is a novel and very effective decomposition of tensor correlators which reduces their computation to that of a number of scalar form factors. For example, the most general 3-point function of a conserved and traceless stress-energy tensor is determined by only five form factors. Dilatations and special conformal Ward identities then impose additional conditions on these form factors. The special conformal Ward identities become a set of first and second order differential equations, whose general solution is given in terms of integrals involving a product of three Bessel functions (`triple-K integrals'). All in all, the correlators are completely determined up to a number of constants, in agreement with well-known position space results. We develop systematic methods for explicitly evaluating the triple-K integrals. In odd dimensions they are given in terms of elementary functions while in even dimensions the results involve dilogarithms. In some cases, the triple-K integrals diverge and subtractions are necessary and we show how such subtractions are related to conformal anomalies. This paper contains two parts that can be read independently of each other. In the first part, we explain the method that leads to the solution for the correlators in terms of triple-K integrals and how to evaluate these integrals, while the second part contains a self-contained presentation of all results. Readers interested only in results may directly consult the second part of the paper.

Highlights

  • Introduction and summary of resultsIt is well known that conformal invariance imposes strong constraints on correlation functions

  • We present a comprehensive analysis of the implications of conformal invariance for 3-point functions of the stress-energy tensor, conserved currents and scalar operators in general dimension and in momentum space

  • The second part is completely self-contained and can be used without reference to the first part of the paper. This second part starts with a collection of all basic definitions and a summary of conventions, followed by a list of all results for all 3point functions involving the stress-energy tensor, conserved currents and scalar operators. For each such correlator we list: (i) the relevant trace and transverse Ward identities, (ii) the reconstruction formula that yield the complete correlator from its transverse(-traceless) part, (iii) the tensorial decomposition of the transverse(-traceless) part, (iv) how to extract the form factors from the complete correlator, (v) the primary conformal Ward identities (CWIs) and their solution in terms of triple-K integrals, (vi) the secondary Ward identities and the relations they impose on the integration constants of the primary Ward identities, (vii) evaluation of the triple-K integrals in dimensions d = 3, 5

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Summary

Introduction and summary of results

It is well known that conformal invariance imposes strong constraints on correlation functions. This second part starts with a collection of all basic definitions and a summary of conventions, followed by a list of all results for all 3point functions involving the stress-energy tensor, conserved currents and scalar operators For each such correlator we list: (i) the relevant trace and transverse Ward identities, (ii) the reconstruction formula that yield the complete correlator from its transverse(-traceless) part, (iii) the tensorial decomposition of the transverse(-traceless) part, (iv) how to extract the form factors from the complete correlator, (v) the primary CWIs and their solution in terms of triple-K integrals, (vi) the secondary Ward identities and the relations they impose on the integration constants of the primary Ward identities (the primary constants), (vii) evaluation of the triple-K integrals in dimensions d = 3, 5.

Part I
Scalar 2-point function
Tensorial 2-point functions
From position to momentum space
Conformal Ward identities
Uniqueness of the solution
Decomposition of tensors
Representations of tensor structures
Decomposition of tμ1ν1 tμ2ν2 tμ3ν3
Finding the form factors
Example
Conformal Ward identities in momentum space
From position space to momentum space
Dilatation Ward identity
Special conformal Ward identities
Primary conformal Ward identities
Secondary conformal Ward identities
Transverse Ward identities
Solutions to conformal Ward identities
Triple-K integrals
Region of validity and regularisation
Basic properties
Dilatation degree of the triple-K integral
Triple-K integrals and 2-point functions
Solutions to the primary conformal Ward identities
More on T μ1ν1 T μ2ν2 O
Solutions to the secondary conformal Ward identities
T μ1ν1 T μ2ν2 O for free scalars
Simplifications in the generic case
Worked example: T μ1ν1J μ2J μ3
Extensions
List of results
A Decomposition of T T T μ1ν1 μ2ν2 μ3ν3 in non-conformal case
F Triviality of T μ1ν1J μ2O

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