<p>We perform a complete classification of AdS<sub>2</sub> solutions of Type II supergravity realising <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <mi mathvariant="script">N</mi> </math></EquationSource> <EquationSource Format="TEX">\( \mathcal{N} \)</EquationSource> </InlineEquation> = 6 supersymmetry and OSp(6|2) superconformal symmetry on backgrounds that are foliations of AdS<sub>2</sub> × ℂℙ<sup>3</sup> over a Riemann surface Σ<sub>2</sub>. Such solutions only exist in type IIB supergravity and are in 1 to 1 correspondence with a fourth order PDE that can be locally solved in terms of two holomorphic functions. Particular solutions in the class are the T-duals of the AdS<sub>3</sub> × ℂℙ<sup>3</sup> and AdS<sub>2</sub> × S<sup>7</sup> solutions to massive Type IIA supergravity found in the literature. We discuss the field theory interpretation of the two sub-classes of solutions related to AdS<sub>3</sub> × ℂℙ<sup>3</sup> by Abelian and non-Abelian T-duality, which provide explicit examples for the Riemann surface an annulus or a strip. In the second case we interpret the solutions as holographic duals to baryon vertex configurations realised in D2-brane box models.</p>

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\( \mathcal{N} \) = 6 supersymmetric AdS2 × ℂℙ3 × Σ2

  • Andrea Conti,
  • Yolanda Lozano,
  • Niall T. Macpherson

摘要

We perform a complete classification of AdS2 solutions of Type II supergravity realising N \( \mathcal{N} \) = 6 supersymmetry and OSp(6|2) superconformal symmetry on backgrounds that are foliations of AdS2 × ℂℙ3 over a Riemann surface Σ2. Such solutions only exist in type IIB supergravity and are in 1 to 1 correspondence with a fourth order PDE that can be locally solved in terms of two holomorphic functions. Particular solutions in the class are the T-duals of the AdS3 × ℂℙ3 and AdS2 × S7 solutions to massive Type IIA supergravity found in the literature. We discuss the field theory interpretation of the two sub-classes of solutions related to AdS3 × ℂℙ3 by Abelian and non-Abelian T-duality, which provide explicit examples for the Riemann surface an annulus or a strip. In the second case we interpret the solutions as holographic duals to baryon vertex configurations realised in D2-brane box models.