Table of Contents
Fetching ...

Seiberg Duality, 5d SCFTs and Nekrasov Partition Functions

Masato Taki

TL;DR

This work demonstrates that Seiberg-like dualities in 5d SCFTs arise from Picard–Lefschetz moves of affine $E_N$ 7-brane backgrounds, leading to multiple Type IIB 5-brane webs and toric/pseudo del Pezzo duals describing the same fixed points. The authors conjecture and test a unifying relation between Nekrasov partition functions across toric and pseudo del Pezzo phases, $Z_{dP_k} = Z_{PdP_k^{p}} / Z^{PdP_k^{p}}_{ ext{extra}}$, where $Z^{PdP_k^{p}}_{ ext{extra}}$ captures non-full spin content from stacks of parallel external legs. Using refined topological vertex techniques, they perform explicit one-instanton (and some higher) checks for $E_1$ through $E_5$ theories, showing that the extra factors precisely account for the discrepancies and render the partition functions equivalent. The results classify 5d SCFTs with one-dimensional Coulomb branches into eight distinct theories, reveal deep links to the 4d Seiberg duality via 7-brane moves, and suggest promising directions toward non-toric vertex constructions and 5d AGT relations.

Abstract

It is known that a 4d N = 1 SCFT lives on D3-branes probing a local del Pezzo Calabi-Yau singularity. The Seiberg (or toric) duality of this SCFT arises from the Picard-Lefshetz transformation of the affine E_N 7-brane background that is associated with the Calabi-Yau threefold. In this paper we study the duality of the affine E_N background itself and a 5-brane probing it. We then find that many different Type IIB 5-brane webs describe the same SCFT in 5d. We check this duality by comparing the Nekrasov partition functions of these 5-brane web configurations.

Seiberg Duality, 5d SCFTs and Nekrasov Partition Functions

TL;DR

This work demonstrates that Seiberg-like dualities in 5d SCFTs arise from Picard–Lefschetz moves of affine 7-brane backgrounds, leading to multiple Type IIB 5-brane webs and toric/pseudo del Pezzo duals describing the same fixed points. The authors conjecture and test a unifying relation between Nekrasov partition functions across toric and pseudo del Pezzo phases, , where captures non-full spin content from stacks of parallel external legs. Using refined topological vertex techniques, they perform explicit one-instanton (and some higher) checks for through theories, showing that the extra factors precisely account for the discrepancies and render the partition functions equivalent. The results classify 5d SCFTs with one-dimensional Coulomb branches into eight distinct theories, reveal deep links to the 4d Seiberg duality via 7-brane moves, and suggest promising directions toward non-toric vertex constructions and 5d AGT relations.

Abstract

It is known that a 4d N = 1 SCFT lives on D3-branes probing a local del Pezzo Calabi-Yau singularity. The Seiberg (or toric) duality of this SCFT arises from the Picard-Lefshetz transformation of the affine E_N 7-brane background that is associated with the Calabi-Yau threefold. In this paper we study the duality of the affine E_N background itself and a 5-brane probing it. We then find that many different Type IIB 5-brane webs describe the same SCFT in 5d. We check this duality by comparing the Nekrasov partition functions of these 5-brane web configurations.

Paper Structure

This paper contains 16 sections, 172 equations, 37 figures.

Figures (37)

  • Figure 1: The left hand side is the 5-brane web dual to the local $\mathbb{CP}^2$ geometry. We regularize an external leg by terminating it on a 7-brane. A colored circle is a 7-brane, and a dashed lines is branch cut arising from it. Moving these three 7-branes inside the 5-brane loop yields the right hand side through the Hanany-Witten effect.
  • Figure 2: All the $GL(2,\mathbb{Z})$-inequivalent convex lattice polygons with single internal point and their dual web diagrams.
  • Figure 3: Blowup in a toric web diagram. The local Calabi-Yau for the first del Pezzo ${\mathcal{B}}_1$ is the one point blowup of the local $\,\mathbb{P}^2$. The resulting three toric diagrams are equivalent up to the $SL(2,\mathbb{Z})$ symmetry transformation.
  • Figure 4: The two toric phases of the local geometry of the another first del Pezzo $\tilde{\mathcal{B}}_1$.
  • Figure 5: The left hand side is the 5-brane loop probe of $\,\,\bf \hat{E}_1$ 7-brane configuration. Since all the 7-branes are not collapsible, only a sub-algebra $E_1$ is realized on the 5-brane. The right hand side is the corresponding web diagram which is obtained by moving a 7-brane the outside of the loop along the associated geodesic.
  • ...and 32 more figures