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TBA, NLO Luscher correction, and double wrapping in twisted AdS/CFT

Changrim Ahn, Zoltan Bajnok, Diego Bombardelli, Rafael I. Nepomechie

TL;DR

This work develops a complete, cross-validated framework for finite-volume ground-state energies in integrable theories with twists. By deriving both LO and NLO Lüscher corrections and twisted TBA equations (with a universal Y-system), it shows exact agreement between the two approaches for the O(4) model and the γ-deformed AdS/CFT theory. The NLO (double-wrapping) corrections are computed explicitly, including a full treatment of the AdS/CFT bound-state spectrum and dressing factors, yielding a six-loop prediction for Tr Z^3 in the twisted theory. The analysis confirms that twists influence the asymptotics but not the local TBA/Y-system structure, and it establishes a solid foundation for extending to excited states and higher-wrapping orders. Overall, the results provide a highly nontrivial consistency check of the integrable S-matrix and the finite-size framework in twisted AdS/CFT.

Abstract

The ground-state energy of integrably-twisted theories is analyzed in finite volume. We derive the leading and next-to-leading order (NLO) Lüscher-type corrections for large volumes of the vacuum energy for integrable theories with twisted boundary conditions and twisted S-matrix. We then derive the twisted thermodynamic Bethe ansatz (TBA) equations to describe exactly the ground state, from which we obtain an untwisted Y-system. The two approaches are compared by expanding the TBA equations to NLO, and exact agreement is found. We give explicit results for the O(4) model and for the three-parameter family of $γ$-deformed (non-supersymmetric) planar AdS/CFT model, where the ground-state energy can be nontrivial and can acquire finite-size corrections. The NLO corrections, which correspond to double-wrapping diagrams, are explicitly evaluated for the latter model at six loops.

TBA, NLO Luscher correction, and double wrapping in twisted AdS/CFT

TL;DR

This work develops a complete, cross-validated framework for finite-volume ground-state energies in integrable theories with twists. By deriving both LO and NLO Lüscher corrections and twisted TBA equations (with a universal Y-system), it shows exact agreement between the two approaches for the O(4) model and the γ-deformed AdS/CFT theory. The NLO (double-wrapping) corrections are computed explicitly, including a full treatment of the AdS/CFT bound-state spectrum and dressing factors, yielding a six-loop prediction for Tr Z^3 in the twisted theory. The analysis confirms that twists influence the asymptotics but not the local TBA/Y-system structure, and it establishes a solid foundation for extending to excited states and higher-wrapping orders. Overall, the results provide a highly nontrivial consistency check of the integrable S-matrix and the finite-size framework in twisted AdS/CFT.

Abstract

The ground-state energy of integrably-twisted theories is analyzed in finite volume. We derive the leading and next-to-leading order (NLO) Lüscher-type corrections for large volumes of the vacuum energy for integrable theories with twisted boundary conditions and twisted S-matrix. We then derive the twisted thermodynamic Bethe ansatz (TBA) equations to describe exactly the ground state, from which we obtain an untwisted Y-system. The two approaches are compared by expanding the TBA equations to NLO, and exact agreement is found. We give explicit results for the O(4) model and for the three-parameter family of -deformed (non-supersymmetric) planar AdS/CFT model, where the ground-state energy can be nontrivial and can acquire finite-size corrections. The NLO corrections, which correspond to double-wrapping diagrams, are explicitly evaluated for the latter model at six loops.

Paper Structure

This paper contains 32 sections, 217 equations, 1 figure, 3 tables.

Figures (1)

  • Figure 1: Two possible locations of a defect. On the left it is located in space, and it introduces a twisted boundary condition. On the right it is located in (Euclidean) time, and it acts as an operator on the periodic Hilbert space.