Abstract

Many CFT problems, e.g. ones with global symmetries, have correlation functions with a crossing antisymmetric sector. We show that such a crossing antisymmetric function can be expanded in terms of manifestly crossing antisymmetric objects, which we call the ‘+ type Polyakov blocks’. These blocks are built from AdSd+1 Witten diagrams. In 1d they encode the ‘+ type’ analytic functionals which act on crossing antisymmetric functions. In general d we establish this Witten diagram basis from a crossing antisymmetric dispersion relation in Mellin space. Analogous to the crossing symmetric case, the dispersion relation imposes a set of independent ‘locality constraints’ in addition to the usual CFT sum rules given by the ‘Polyakov conditions’. We use the Polyakov blocks to simplify more general analytic functionals in d > 1 and global symmetry functionals.

Highlights

  • One of the most important tools available to theoretical physicists in CFT problems is crossing symmetry or the Conformal Bootstrap

  • The latter is an idea that a crossing symmetric correlator can be expanded in terms of a manifestly crossing symmetric sum of Witten diagrams which must be equal to the usual conformal block expansion [11,12,13]

  • For this we show that a crossing antisymmetric function can be obtained from a dispersion relation in Mellin space

Read more

Summary

Introduction

The analytic functionals are perhaps most well understood in 1d, where they are related to another formulation of crossing symmetry: the Polyakov bootstrap [10] The latter is an idea that a crossing symmetric correlator can be expanded in terms of a manifestly crossing symmetric sum of Witten diagrams (a Polyakov block) which must be equal to the usual conformal block expansion [11,12,13]. The idea of a + type Polyakov block is extended to general dimensions, which requires an infinite number of exchange Witten diagrams and crossing antisymmetric contact diagrams For this we show that a crossing antisymmetric function can be obtained from a dispersion relation in Mellin space. This, rather counter-intuitive, notation is for consistency with the analytic functional literature

Basic kinematics
Fermionic case
Bosonic case
General d Polyakov blocks and dispersion relation
Crossing antisymmetric Polyakov block
Contact diagrams
Dispersion relation
Polyakov conditions
Product functionals in even d
Global symmetry — simple functionals
General d
Conclusion
Holographic correlators
A Details of Witten diagrams
General case — review
C Checks with the dispersion relation
Numerical checks
Bounds with product functionals

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

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.