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Holographic Aspects of Four Dimensional ${\cal N }=2$ SCFTs and their Marginal Deformations

Carlos Nunez, Dibakar Roychowdhury, Stefano Speziali, Salomon Zacarias

TL;DR

The paper develops a holographic dictionary for four-dimensional ${\

Abstract

We study the holographic description of ${\cal N}=2$ Super Conformal Field Theories in four dimensions first given by Gaiotto and Maldacena. We present new expressions that holographically calculate characteristic numbers of the CFT and associated Hanany-Witten set-ups, or more dynamical observables, like the central charge. A number of examples of varying complexity are studied and some proofs for these new expressions are presented. We repeat this treatment for the case of the marginally deformed Gaiotto-Maldacena theories, presenting an infinite family of new solutions and compute some of its observables. These new backgrounds rely on the solution of a Laplace equation and a boundary condition, encoding the kinematics of the original conformal field theory.

Holographic Aspects of Four Dimensional ${\cal N }=2$ SCFTs and their Marginal Deformations

TL;DR

The paper develops a holographic dictionary for four-dimensional ${\

Abstract

We study the holographic description of Super Conformal Field Theories in four dimensions first given by Gaiotto and Maldacena. We present new expressions that holographically calculate characteristic numbers of the CFT and associated Hanany-Witten set-ups, or more dynamical observables, like the central charge. A number of examples of varying complexity are studied and some proofs for these new expressions are presented. We repeat this treatment for the case of the marginally deformed Gaiotto-Maldacena theories, presenting an infinite family of new solutions and compute some of its observables. These new backgrounds rely on the solution of a Laplace equation and a boundary condition, encoding the kinematics of the original conformal field theory.

Paper Structure

This paper contains 41 sections, 179 equations, 15 figures, 2 tables.

Figures (15)

  • Figure 1: The quiver and Hanany-Witten set-up for a generic situation. The vertical lines denote individual Neveu-Schwarz branes extended on the $(x_4,x_5)$ space. The horizontal ones D4 branes, that extend on $x_6$, in between five branes and the crossed-circles D6 branes, that extend on the $(x_7,x_8,x_9)$ directions. All the branes share the Minkowski directions. This realises the isometries $SO(1,3) \times SO(3)\times SO(2)$.
  • Figure 2: A generic quiver. The squares indicate flavour groups and the circles gauge groups.
  • Figure 3: The quiver and Hanany-Witten set-up for the profile in eq.(\ref{['profile1']}). The vertical lines denote individual Neveu-Schwarz branes. The horizontal lines D4 branes and the crossed circles D6 branes.
  • Figure 4: The quiver and Hanany-Witten set-up for the profile in eq.(\ref{['profile2']}).
  • Figure 5: The two operations preserving conformality and $SU(2)_R\times U(1)_r$ as discussed in the text
  • ...and 10 more figures