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Non-conformality of gamma_i-deformed N=4 SYM theory

Jan Fokken, Christoph Sieg, Matthias Wilhelm

TL;DR

The paper demonstrates that the three-parameter gamma_i deformation of N=4 SYM is not conformally invariant, due to a running double-trace coupling whose beta-function is generically nonzero in the 't Hooft limit. By systematically introducing and classifying tree-level and multi-trace couplings consistent with renormalizability and planarity, the authors show that conformality cannot be restored by such deformations. They explicitly compute the one-loop running of a key double-trace coupling, finding a nonzero beta-function unless the deformation angles coincide in a specific way, and discuss implications for the integrability-based finite-size problem and potential tachyonic instabilities in the dual string background. The work suggests that the gamma_i-deformed background may lack a conformal Lagrangian dual with the same field content as N=4 SYM, or that the AdS5 factor acquires corrections that destabilize the background. A concrete test is proposed to clarify the origin of observed divergences in integrability-based descriptions and to distinguish between potential scenarios for the dual theory.

Abstract

We show that the gamma_i-deformation, which was proposed as candidate gauge theory for a non-supersymmetric three-parameter deformation of the AdS/CFT correspondence, is not conformally invariant due to a running double-trace coupling - not even in the 't Hooft limit. Moreover, this non-conformality cannot be cured when we extend the theory by adding at tree-level arbitrary multi-trace couplings that obey certain minimal consistency requirements. Our findings suggest a possible connection between this breakdown of conformal invariance and a puzzling divergence recently encountered in the integrability-based descriptions of two-loop finite-size corrections for the single-trace operator of two identical chiral fields. We propose a test to clarify this.

Non-conformality of gamma_i-deformed N=4 SYM theory

TL;DR

The paper demonstrates that the three-parameter gamma_i deformation of N=4 SYM is not conformally invariant, due to a running double-trace coupling whose beta-function is generically nonzero in the 't Hooft limit. By systematically introducing and classifying tree-level and multi-trace couplings consistent with renormalizability and planarity, the authors show that conformality cannot be restored by such deformations. They explicitly compute the one-loop running of a key double-trace coupling, finding a nonzero beta-function unless the deformation angles coincide in a specific way, and discuss implications for the integrability-based finite-size problem and potential tachyonic instabilities in the dual string background. The work suggests that the gamma_i-deformed background may lack a conformal Lagrangian dual with the same field content as N=4 SYM, or that the AdS5 factor acquires corrections that destabilize the background. A concrete test is proposed to clarify the origin of observed divergences in integrability-based descriptions and to distinguish between potential scenarios for the dual theory.

Abstract

We show that the gamma_i-deformation, which was proposed as candidate gauge theory for a non-supersymmetric three-parameter deformation of the AdS/CFT correspondence, is not conformally invariant due to a running double-trace coupling - not even in the 't Hooft limit. Moreover, this non-conformality cannot be cured when we extend the theory by adding at tree-level arbitrary multi-trace couplings that obey certain minimal consistency requirements. Our findings suggest a possible connection between this breakdown of conformal invariance and a puzzling divergence recently encountered in the integrability-based descriptions of two-loop finite-size corrections for the single-trace operator of two identical chiral fields. We propose a test to clarify this.

Paper Structure

This paper contains 18 sections, 55 equations, 1 figure.

Figures (1)

  • Figure 1: Complete list of contributions (up to conjugation) to $\bar{\phi}_i^a\bar{\phi}_i^b\phi^{i,c}\phi^{i,d}(ab)(cd)$ that deviate from the ones in the undeformed $\mathcal{N}=4$ SYM theory. The diagrams are displayed in double-line notation with central plain and dashed flavor lines for scalar and fermionic fields, respectively. Flavor-neutral gauge boson lines appear without central line. \ref{['ss4s4']}, \ref{['us4s4']}: diagrams with two F-term-type single-trace interactions; \ref{['ts4s4']}: diagram with two F-term-type double-trace interactions; \ref{['tDs4s4']}: diagram with one F-term-type double-trace and one D-term-type single trace interaction; \ref{['s4gg2']}, \ref{['s4gg3']}: F-term-type double-trace interaction with gauge boson exchange; \ref{['fbox1']}, \ref{['fbox2']}, \ref{['fbox3']}: fermion box with four Yukawa-type interactions.