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Exploring the ground state spectrum of γ-deformed N = 4 SYM

A bstract We study the γ -deformation of the planar N = 4 super Yang-Mills theory which breaks all supersymmetries but is expected to preserve integrability of the model. We focus on the operator Tr ( ϕ 1 ϕ 1 ) built from two scalars, whose integrability description has been questioned before due to...

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Published in:The journal of high energy physics 2022-06, Vol.2022 (6), p.146-24, Article 146
Main Authors: Levkovich-Maslyuk, Fedor, Preti, Michelangelo
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description A bstract We study the γ -deformation of the planar N = 4 super Yang-Mills theory which breaks all supersymmetries but is expected to preserve integrability of the model. We focus on the operator Tr ( ϕ 1 ϕ 1 ) built from two scalars, whose integrability description has been questioned before due to contributions from double-trace counterterms. We show that despite these subtle effects, the integrability-based Quantum Spectral Curve (QSC) framework works perfectly for this state and in particular reproduces the known 1-loop prediction. This resolves an earlier controversy concerning this operator and provides further evidence that the γ -deformed model is an integrable CFT at least in the planar limit. We use the QSC to compute the first 5 weak coupling orders of the anomalous dimension analytically, matching known results in the fishnet limit, and also compute it numerically all the way from weak to strong coupling. We also utilize this data to extract a new coefficient of the beta function of the double-trace operator couplings.
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subjects AdS-CFT Correspondence
Classical and Quantum Gravitation
Couplings
Deformation
Elementary Particles
High energy physics
High Energy Physics - Theory
Integrable Field Theories
Mathematical analysis
Physics
Physics and Astronomy
Quantum Field Theories
Quantum Field Theory
Quantum Physics
Regular Article - Theoretical Physics
Relativity Theory
Scalars
String Theory
Supersymmetry
Yang-Mills theory
title Exploring the ground state spectrum of γ-deformed N = 4 SYM
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