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Toric Calabi-Yau four-folds dual to Chern-Simons-matter theories

Kazushi Ueda, Masahito Yamazaki

TL;DR

This work addresses constructing gravity duals for 3d Chern-Simons–matter theories by identifying the Calabi–Yau 4-fold cone $C(Y_7)$ with a branch of the moduli space, realized through toric, torus-based dimer models. It introduces a concrete forward algorithm that extracts the toric data of $C(Y_7)$ from the quiver, superpotential, and CS levels by analyzing perfect matchings on brane tilings, yielding the convex hull of vectors $v^{\alpha}$ as the CY$_4$ toric diagram. The authors validate the method with examples, reproducing known toric data for cases like $Y^{p,k}(\mathbb{CP}^2)$ and identifying limitations for $Y^{p,k}(\mathbb{CP}^1\times\mathbb{CP}^1)$, where the conjectured toric data fails to match and Seiberg duality does not commute with the construction. Overall, the paper provides a practical, systematic bridge between 3d CS–matter theories and M-theory backgrounds, enabling the generation of gravity duals and guiding future investigations into dualities and extensions such as orientifolds and marginal deformations.

Abstract

We propose a new method to find gravity duals to a large class of three-dimensional Chern-Simons-matter theories, using techniques from dimer models. The gravity dual is given by M-theory on AdS_4\times Y_7, where Y_7 is an arbitrary seven-dimensional toric Sasaki-Einstein manifold. The cone of Y_7 is a toric Calabi-Yau 4-fold, which coincides with a branch of the vacuum moduli space of Chern-Simons-matter theories.

Toric Calabi-Yau four-folds dual to Chern-Simons-matter theories

TL;DR

This work addresses constructing gravity duals for 3d Chern-Simons–matter theories by identifying the Calabi–Yau 4-fold cone with a branch of the moduli space, realized through toric, torus-based dimer models. It introduces a concrete forward algorithm that extracts the toric data of from the quiver, superpotential, and CS levels by analyzing perfect matchings on brane tilings, yielding the convex hull of vectors as the CY toric diagram. The authors validate the method with examples, reproducing known toric data for cases like and identifying limitations for , where the conjectured toric data fails to match and Seiberg duality does not commute with the construction. Overall, the paper provides a practical, systematic bridge between 3d CS–matter theories and M-theory backgrounds, enabling the generation of gravity duals and guiding future investigations into dualities and extensions such as orientifolds and marginal deformations.

Abstract

We propose a new method to find gravity duals to a large class of three-dimensional Chern-Simons-matter theories, using techniques from dimer models. The gravity dual is given by M-theory on AdS_4\times Y_7, where Y_7 is an arbitrary seven-dimensional toric Sasaki-Einstein manifold. The cone of Y_7 is a toric Calabi-Yau 4-fold, which coincides with a branch of the vacuum moduli space of Chern-Simons-matter theories.

Paper Structure

This paper contains 9 sections, 30 equations, 9 figures.

Figures (9)

  • Figure 1: The bipartite graph (a), quiver diagram (b,d) and toric diagram (c) corresponding to the Suspended Pinched Point.
  • Figure 2: The perfect matchings of bipartite graphs and their height functions. The height functions gives the coordinates of the toric diagram.
  • Figure 3: The choices of paths $p_1,\dots, p_4$ (left) and Chern-Simons levels for SPP (right). On the right figure the flow of the Chern-Simons charge is represented as a green arrow.
  • Figure 4: The bipartite graph (a), thee toric diagram (c) and the quiver diagram (b,d) for $C(Y_5)=K_{\mathbb{CP}^2}$.
  • Figure 5: The choice of paths $p_1,\dots, p_4$, flow of CS cherge (above) and perfect matchings with corresponding coordinate of the lattice point of convex polytope (below) in the case of $C(Y_5)=K_{\mathbb{CP}^2}$.
  • ...and 4 more figures