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Three dimensional canonical singularity and five dimensional N=1 SCFT

Dan Xie, Shing-Tung Yau

TL;DR

We address the problem of engineering five-dimensional $\mathcal{N}=1$ SCFTs from geometry by proposing that M-theory on a 3-fold canonical singularity $X$ yields a 5d SCFT. The main approach ties flavor symmetry to the ADE structure over one-dimensional singular loci and identifies the Coulomb-branch data with crepant resolutions: the prepotential is cubic, $${\cal F}=\frac{1}{6}(\sum_i \phi_i D_i)^3$, and the full Coulomb branch is the nef-cone fan formed by all flop-related resolutions. The paper provides concrete geometric frameworks for toric, quotient, and hypersurface singularities, detailing how to compute flavor symmetries, Coulomb-branch dimensions, prepotentials, and gauge-theory limits via nef/Mori data and triangulations, often connecting to $(p,q)$-web constructions. This geometric program yields a unifying lens to classify and compute 5d SCFT data, with explicit methods to access non-abelian flavor enhancements, Coulomb-branch chambers, and BPS spectra, and suggests extensions to non-toric and Fano geometries and to circle compactifications that bridge to Seiberg-Witten-type descriptions.

Abstract

We conjecture that every three dimensional canonical singularity defines a five dimensional N=1 SCFT. Flavor symmetry can be found from singularity structure: non-abelian flavor symmetry is read from the singularity type over one dimensional singular locus. The dimension of Coulomb branch is given by the number of compact crepant divisors from a crepant resolution of singularity. The detailed structure of Coulomb branch is described as follows: a): A chamber of Coulomb branch is described by a crepant resolution, and this chamber is given by its Nef cone and the prepotential is computed from triple intersection numbers; b): Crepant resolution is not unique and different resolutions are related by flops; Nef cones from crepant resolutions form a fan which is claimed to be the full Coulomb branch.

Three dimensional canonical singularity and five dimensional N=1 SCFT

TL;DR

We address the problem of engineering five-dimensional SCFTs from geometry by proposing that M-theory on a 3-fold canonical singularity yields a 5d SCFT. The main approach ties flavor symmetry to the ADE structure over one-dimensional singular loci and identifies the Coulomb-branch data with crepant resolutions: the prepotential is cubic, $, and the full Coulomb branch is the nef-cone fan formed by all flop-related resolutions. The paper provides concrete geometric frameworks for toric, quotient, and hypersurface singularities, detailing how to compute flavor symmetries, Coulomb-branch dimensions, prepotentials, and gauge-theory limits via nef/Mori data and triangulations, often connecting to -web constructions. This geometric program yields a unifying lens to classify and compute 5d SCFT data, with explicit methods to access non-abelian flavor enhancements, Coulomb-branch chambers, and BPS spectra, and suggests extensions to non-toric and Fano geometries and to circle compactifications that bridge to Seiberg-Witten-type descriptions.

Abstract

We conjecture that every three dimensional canonical singularity defines a five dimensional N=1 SCFT. Flavor symmetry can be found from singularity structure: non-abelian flavor symmetry is read from the singularity type over one dimensional singular locus. The dimension of Coulomb branch is given by the number of compact crepant divisors from a crepant resolution of singularity. The detailed structure of Coulomb branch is described as follows: a): A chamber of Coulomb branch is described by a crepant resolution, and this chamber is given by its Nef cone and the prepotential is computed from triple intersection numbers; b): Crepant resolution is not unique and different resolutions are related by flops; Nef cones from crepant resolutions form a fan which is claimed to be the full Coulomb branch.

Paper Structure

This paper contains 19 sections, 1 theorem, 77 equations, 17 figures, 2 tables.

Key Result

Theorem 2

X is terminal if and only if (up to permutations of $(x,y,z)$ and symmetries of $\mu_r$) $X=C^3/\mu_r$ of type ${1\over r}(a, -a, 1)$ with $a$ coprime to $r$, where $\mu_r$ is the cyclic group of order $r$.

Figures (17)

  • Figure 1: A toric diagram and one of its partial resolution, and we also write down a gauge theory description.
  • Figure 2: Two different resolutions of a lattice polygon can be related by sequence of flops shown above.
  • Figure 3: Quadrilaterals in a triangulation of a polygon $P$.
  • Figure 4: One toric diagram and its crepant resolution.
  • Figure 5: Three toric diagrams which have pure SU(2) gauge theory description along certain locus of Coulomb branch.
  • ...and 12 more figures

Theorems & Definitions (4)

  • Conjecture 1
  • Definition 1
  • Theorem 2
  • Conjecture 2