Abstract

The spectral problem for the AdS5×S5 superstring and its dual planar maximally supersymmetric Yang–Mills theory can be efficiently solved through a set of functional equations known as the quantum spectral curve. We discuss how the same concepts apply to the η-deformed AdS5×S5 superstring, an integrable deformation of the AdS5×S5 superstring with quantum group symmetry. This model can be viewed as a trigonometric version of the AdS5×S5 superstring, like the relation between the XXZ and XXX spin chains, or the sausage and the S2 sigma models for instance. We derive the quantum spectral curve for the η-deformed string by reformulating the corresponding ground-state thermodynamic Bethe ansatz equations as an analytic Y system, and map this to an analytic T system which upon suitable gauge fixing leads to a Pμ system – the quantum spectral curve. We then discuss constraints on the asymptotics of this system to single out particular excited states. At the spectral level the η-deformed string and its quantum spectral curve interpolate between the AdS5×S5 superstring and a superstring on “mirror” AdS5×S5, reflecting a more general relationship between the spectral and thermodynamic data of the η-deformed string. In particular, the spectral problem of the mirror AdS5×S5 string, and the thermodynamics of the undeformed AdS5×S5 string, are described by a second rational limit of our trigonometric quantum spectral curve, distinct from the regular undeformed limit.

Highlights

  • The discovery of integrable models in the planar limit of the AdS/CFT correspondence has led to remarkable advances in this area [1, 2]

  • We discuss how the same concepts apply to the η-deformed AdS5 × S5 superstring, an integrable deformation of the AdS5 × S5 superstring with quantum group symmetry

  • Using well-known tools of integrability,1 it is for instance possible to find a closed set of functional equations that nonperturbatively describe the spectrum of scaling dimensions in planar N = 4 supersymmetric Yang-Mills theory, or equivalently the energy spectrum of a superstring moving in AdS5 × S5

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Summary

Introduction

The discovery of integrable models in the planar limit of the AdS/CFT correspondence has led to remarkable advances in this area [1, 2]. The solution of the AdS5 × S5 spectral problem involves fixing a light-cone gauge, doing a double Wick rotation to arrive at the so-called mirror model [5], and using its exact S matrix as input for the thermodynamic Bethe ansatz (TBA) [6, 7, 8, 9] This results in an involved set of infinitely many coupled integral equations, encoding the spectrum. Our equations describe the spectrum of the classically light-cone gauge-fixed η-deformed sigma model, a quantum deformation of the AdS5 × S5 superstring spectrum interpolating between AdS5 × S5 and its mirror version.5 This interpolation reflects a curious property of the full η-deformed model, dubbed mirror duality [41]: performing a double Wick rotation in the light-cone gauge, is equivalent to inverting the deformation parameter in a suitable parametrisation. In the conclusions we discuss various interesting open questions and possible future directions

Basic parametrisation of the η-deformed string
Quantum spectral curve for the η-deformed string
Deriving the QSC
From TBA to analytic Y system
Simplification and Y system
Deriving the analyticity conditions
Treating the YQs
From analytic Y system to analytic T system
Constructing the T gauges
Introducing the Pμ system
Deducing analytic properties of μ from TBA
Periodicity properties of μ12
Switching conventions
The Qω system
H symmetry and reality
Selecting the right solution
Deriving the asymptotics
Left-right symmetric sector
Weak coupling Bethe equations
Mirror duality and the undeformed mirror limit
Conclusions
Parameters of the η model
Kernels
Contribution of the dressing phase
Rederiving the TBA equation from the discontinuities
Reconstructing the YQ TBA equation
Driving term EQ
Define the T gauge directly in terms of the T gauge
Constructing T
Solving periodic difference equations: constructing f
Constructing TR and TL
The T gauge is analytic
So is T really Z4-symmetric?
Full Text
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