Abstract

In a series of recent papers, a special kind of AdS2/CFT1 duality was observed: the boundary correlators of elementary fields that appear in the Lagrangian of a 2d conformal theory in rigid AdS2 background are the same as the correlators of the corresponding primary operators in the chiral half of that 2d CFT in flat space restricted to the real line. The examples considered were: (i) the Liouville theory where the operator dual to the Liouville scalar in AdS2 is the stress tensor; (ii) the abelian Toda theory where the operators dual to the Toda scalars are the mathcal{W} -algebra generators; (iii) the non-abelian Toda theory where the Liouville field is dual to the stress tensor while the extra gauged WZW theory scalars are dual to non-abelian parafermionic operators. By direct Witten diagram com- putations in AdS2 one can check that the structure of the boundary correlators is indeed consistent with the Virasoro (or higher) symmetry. Here we consider a supersymmetric generalization: the mathcal{N} = 1 superconformal Liouville theory in AdS2. We start with the super Liouville theory coupled to 2d supergravity and show that a consistent restriction to rigid AdS2 background requires a non-zero value of the supergravity auxiliary field and thus a modification of the Liouville potential from its familiar flat-space form. We show that the Liouville scalar and its fermionic partner are dual to the chiral half of the stress tensor and the supercurrent of the super Liouville theory on the plane. We perform tests supporting the duality by explicitly computing AdS2 Witten diagrams with bosonic and fermionic loops.

Highlights

  • Introduction and summaryRecent investigations of correlators of operators on 1/2 BPS Wilson loop at strong coupling using AdS5 × S5 superstring action motivate the study of boundary correlators in conformal quantum field theories in AdS2 space

  • In a series of recent papers, a special kind of AdS2/CFT1 duality was observed: the boundary correlators of elementary fields that appear in the Lagrangian of a 2d conformal theory in rigid AdS2 background are the same as the correlators of the corresponding primary operators in the chiral half of that 2d CFT in flat space restricted to the real line

  • The examples considered were: (i) the Liouville theory where the operator dual to the Liouville scalar in AdS2 is the stress tensor; (ii) the abelian Toda theory where the operators dual to the Toda scalars are the W-algebra generators; (iii) the non-abelian Toda theory where the Liouville field is dual to the stress tensor while the extra gauged WZW theory scalars are dual to non-abelian parafermionic operators

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Summary

Introduction and summary

Recent investigations of correlators of operators on 1/2 BPS Wilson loop at strong coupling using AdS5 × S5 superstring action (see [1, 2] and refs. there) motivate the study of boundary correlators in conformal quantum field theories in AdS2 space. While for a general QFT in AdS2 one expects the boundary correlators to be covariant under the isometry of AdS2 or the 1d conformal group SO(2, 1), in the case of a conformal (Weylcovariant) theory one may expect this symmetry to be enhanced to the infinite-dimensional Virasoro symmetry (or reparametrizations of 1d boundary) putting strong constraints on the structure of the boundary correlators This was studied recently on the examples of the Liouville and Toda theories [3,4,5,6]. The expected Virasoro symmetry of the boundary scalar correlators implies that they should be proportional to the correlators of the holomorphic stress tensor of the original Liouville theory on the complex w-plane formally restricted to the real line (boundary of half-plane).1 This correspondence (dubbed “AdS2/CFT12/2 duality”) extends to the case of higher spin W-symmetry generators in Toda theories.

Bosonic Liouville theory
Superconformal Liouville theory in flat space
Scalar multiplet theory in 2d supergravity background and restriction to AdS2
Super Weyl invariance conditions
Action for super Liouville theory in AdS2
Super Liouville theory
Duality predictions for the boundary correlation functions
Perturbation theory in AdS2
Two-point functions
Scalar propagator correction
Fermion propagator correction
Three-point functions
Tree level
One-loop correction to three-scalar correlator
Four-point functions
A Majorana fermion action in Euclidean AdS2
B Propagators in AdS
Component form of fermion propagator in AdS2
C Tree-level calculation of Φ2Ψ2 boundary correlation function
Findings
Φ2Ψ2 correlator in super Liouville theory in AdS2
Full Text
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