Abstract

In this work, building up on [1] we present momentum space Ward identities related to broken higher spin symmetry as an alternate approach to computing correlators of spinning operators in interacting theories such as the quasi-fermionic and quasi-bosonic theories. The direct Feynman diagram approach to computing correlation functions is intricate and in general has been performed only in specific kinematic regimes. We use higher spin equations to obtain the parity even and parity odd contributions to two-, three- and four-point correlators involving spinning and scalar operators in a general kinematic regime, and match our results with existing results in the literature for cases where they are available.One of the interesting facts about higher spin equations is that one can use them away from the conformal fixed point. We illustrate this by considering mass deformed free boson theory and solving for two-point functions of spinning operators using higher spin equations.

Highlights

  • Conformal Field Theory (CFT) is one of the cornerstones of theoretical physics

  • In this work, building up on [1] we present momentum space Ward identities related to broken higher spin symmetry as an alternate approach to computing correlators of spinning operators in interacting theories such as the quasi-fermionic and quasi-bosonic theories

  • The authors showed that three-point correlators in an interacting theory with broken higher spin symmetry can be fixed in terms of three-point functions of the free fermion theory, free boson theory and a parity odd part and they fixed the coefficients of these terms

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Summary

Introduction

Conformal Field Theory (CFT) is one of the cornerstones of theoretical physics. Among other things, it plays an important role in the well celebrated gauge-gravity correspondence, in explaining critical phenomena at phase transitions, and in defining quantum field theories as deformations of theories with conformal symmetry. See the very recent work [39] in which we computed parity odd correlators by solving momentum space conformal Ward identities and using weight-shifting and spin-raising operators. Parity odd correlators are important as they arise in the study of the free fermion theory and theories with slightly broken higher spin symmetry. In appendix F we give some details involved in the computation of correlators in the free massive bosonic theory

Free theories
Free boson theory
Free fermion theory
Interacting theories
Critical bosonic theory
Quasi-fermionic theory
Quasi-bosonic theory with conformal given by: d12
Higher spin equations in momentum space
Two-point functions
Three-point functions
Four-point functions
Three-point function
A Fourier transform of the above equation gives in momentum space the following:
Quasi-bosonic theory
Four-point function
Higher spin equations away from conformal fixed point
Summary
J1J1J0 in quasi-bosonic theory In the quasi-bosonic theory we have
Conclusion and discussion
Full Text
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