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Chiral flavors and M2-branes at toric CY4 singularities

Francesco Benini, Cyril Closset, Stefano Cremonesi

TL;DR

The paper develops a comprehensive framework for 3d $\mathcal{N}=2$ quiver CS theories describing M2-branes on toric CY$_4$ cones with codimension-two degenerations, i.e., flavored theories arising from D6-branes. It combines a top-down M-theory reduction to IIA with D6-branes and a bottom-up flavored quiver approach, positing a holomorphic quantum relation $T^{(n)}T^{(-n)}=(\prod X_\alpha^{h_\alpha})^{|n|}$ for diagonal monopoles that fixes the flavored moduli space as a toric CY$_4$. The authors provide a general recipe to derive the flavored mesonic moduli space, show its toric nature via auxiliary A-theory brane tilings, and verify it across many explicit examples, including the $Q^{1,1,1}$ geometry. They also relate real and complex masses to geometric deformations of the IIA/M-theory background and discuss shifts in Chern-Simons levels induced by D6-branes. Overall, the work extends the AdS$_4$/CFT$_3$ dictionary to a broad class of flavored toric CY$_4$ singularities and offers concrete tools to engineer and study new holographic duals.

Abstract

We extend the stringy derivation of N=2 AdS4/CFT3 dualities to cases where the M-theory circle degenerates at complex codimension-two submanifolds of a toric conical CY4. The type IIA backgrounds include D6-branes, and the dual N=2 quiver gauge theories contain chiral flavors. We provide a general recipe to derive the geometric moduli space of flavored versions of Abelian toric quiver gauge theories. The CY4 cone is reproduced thanks to a non-trivial quantum F-term relation between diagonal monopole operators and bifundamental fields. We find new field theory duals to many geometries, including Q111.

Chiral flavors and M2-branes at toric CY4 singularities

TL;DR

The paper develops a comprehensive framework for 3d quiver CS theories describing M2-branes on toric CY cones with codimension-two degenerations, i.e., flavored theories arising from D6-branes. It combines a top-down M-theory reduction to IIA with D6-branes and a bottom-up flavored quiver approach, positing a holomorphic quantum relation for diagonal monopoles that fixes the flavored moduli space as a toric CY. The authors provide a general recipe to derive the flavored mesonic moduli space, show its toric nature via auxiliary A-theory brane tilings, and verify it across many explicit examples, including the geometry. They also relate real and complex masses to geometric deformations of the IIA/M-theory background and discuss shifts in Chern-Simons levels induced by D6-branes. Overall, the work extends the AdS/CFT dictionary to a broad class of flavored toric CY singularities and offers concrete tools to engineer and study new holographic duals.

Abstract

We extend the stringy derivation of N=2 AdS4/CFT3 dualities to cases where the M-theory circle degenerates at complex codimension-two submanifolds of a toric conical CY4. The type IIA backgrounds include D6-branes, and the dual N=2 quiver gauge theories contain chiral flavors. We provide a general recipe to derive the geometric moduli space of flavored versions of Abelian toric quiver gauge theories. The CY4 cone is reproduced thanks to a non-trivial quantum F-term relation between diagonal monopole operators and bifundamental fields. We find new field theory duals to many geometries, including Q111.

Paper Structure

This paper contains 39 sections, 122 equations, 16 figures.

Figures (16)

  • Figure 1: Vertical projection from the 3d toric diagram of $Y_4$ to the 2d toric diagram of $Y_3$. The three aligned points give rise to two D6-branes.
  • Figure 2: Deformation of the unflavored theory to construct the A-theory.
  • Figure 3: Quivers for flavored SQED. Circles are gauge groups, squares are flavor groups. Colored arrows indicate bifundamental fields coupled to flavors via a superpotential term.
  • Figure 4: Toric diagrams corresponding to some flavors for the $\mathbb{C}^3$ quiver.
  • Figure 5: Toric diagrams of $\mathbb{C}^2\times \mathbb{C}^2/\mathbb{Z}_h$, for $h=3$.
  • ...and 11 more figures