
Chiral limit of $$ \mathcal{N} $$ = 4 SYM and ABJM and integrable Feynman graphs
Author(s) -
João Caetano,
Ömer Gürdoğan,
Владимир Казаков
Publication year - 2018
Publication title -
the journal of high energy physics/the journal of high energy physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.998
H-Index - 261
eISSN - 1126-6708
pISSN - 1029-8479
DOI - 10.1007/jhep03(2018)077
Subject(s) - feynman diagram , scalar (mathematics) , mathematical physics , bethe ansatz , integrable system , scaling limit , gauge theory , physics , coupling constant , conformal map , quantum mechanics , scaling , mathematics , mathematical analysis , geometry
A bstract We consider a special double scaling limit, recently introduced by two of the authors, combining weak coupling and large imaginary twist, for the γ-twisted $$ \mathcal{N} $$ N = 4 SYM theory. We also establish the analogous limit for ABJM theory. The resulting non-gauge chiral 4D and 3D theories of interacting scalars and fermions are integrable in the planar limit. In spite of the breakdown of conformality by double-trace interactions, most of the correlators for local operators of these theories are conformal, with non-trivial anomalous dimensions defined by specific, integrable Feynman diagrams. We discuss the details of this diagrammatics. We construct the doubly-scaled asymptotic Bethe ansatz (ABA) equations for multi-magnon states in these theories. Each entry of the mixing matrix of local conformal operators in the simplest of these theories — the bi-scalar model in 4D and tri-scalar model in 3D — is given by a single Feynman diagram at any given loop order. The related diagrams are in principle computable, up to a few scheme dependent constants, by integrability methods (quantum spectral curve or ABA). These constants should be fixed from direct computations of a few simplest graphs. This integrability-based method is advocated to be able to provide information about some high loop order graphs which are hardly computable by other known methods. We exemplify our approach with specific five-loop graphs.