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The Seiberg-Witten Kahler Potential as a Two-Sphere Partition Function

Daniel S. Park, Jaewon Song

TL;DR

This work shows that the Seiberg–Witten Kahler potential for 4D ${\cal N}=2$ $SU(2)$ SYM can be obtained from the two-sphere partition function of a GLSM describing the non-compact Calabi–Yau $\mathcal{O}(-2,-2)\rightarrow \mathbb{P}^1\times\mathbb{P}^1$, by taking a field-theory limit of the Kahler parameters. A small positive R-charge $\mathfrak{q}$ is introduced to regulate the non-compact direction, and the leading behavior of $Z_{S^2}$ as $\epsilon\to 0$ and $\mathfrak{q}\to 0^+$ yields $-\pi \partial\bar{\partial} K_{SW}(u,\Lambda)$ up to the prescribed identifications $q_b=\epsilon^4\Lambda^4$ and $q_f=\tfrac{1}{4}-\epsilon^2 u$. The method leverages the known relation between $S^2$ partition functions and Kahler potentials for Calabi–Yau geometries, and interprets the result in terms of the mirror coordinate $u$ on the Seiberg–Witten curve. The authors outline a generalization to other theories engineered by toric Calabi–Yau threefolds, providing a concrete program for obtaining gauge-theory Kahler potentials from $S^2$ partition functions, while noting subtleties in field-theory limits and R-charge choices for more complex cases.

Abstract

Recently it has been shown that the two-sphere partition function of a gauged linear sigma model of a Calabi-Yau manifold yields the exact quantum Kahler potential of the Kahler moduli space of that manifold. Since four-dimensional N=2 gauge theories can be engineered by non-compact Calabi-Yau threefolds, this implies that it is possible to obtain exact gauge theory Kahler potentials from two-sphere partition functions. In this paper, we demonstrate that the Seiberg-Witten Kahler potential can indeed be obtained as a two-sphere partition function. To be precise, we extract the quantum Kahler metric of 4D N=2 SU(2) Super-Yang-Mills theory by taking the field theory limit of the Kahler parameters of the O(-2,-2) bundle over P1 x P1. We expect this method of computing the Kahler potential to generalize to other four-dimensional N=2 gauge theories that can be geometrically engineered by toric Calabi-Yau threefolds.

The Seiberg-Witten Kahler Potential as a Two-Sphere Partition Function

TL;DR

This work shows that the Seiberg–Witten Kahler potential for 4D SYM can be obtained from the two-sphere partition function of a GLSM describing the non-compact Calabi–Yau , by taking a field-theory limit of the Kahler parameters. A small positive R-charge is introduced to regulate the non-compact direction, and the leading behavior of as and yields up to the prescribed identifications and . The method leverages the known relation between partition functions and Kahler potentials for Calabi–Yau geometries, and interprets the result in terms of the mirror coordinate on the Seiberg–Witten curve. The authors outline a generalization to other theories engineered by toric Calabi–Yau threefolds, providing a concrete program for obtaining gauge-theory Kahler potentials from partition functions, while noting subtleties in field-theory limits and R-charge choices for more complex cases.

Abstract

Recently it has been shown that the two-sphere partition function of a gauged linear sigma model of a Calabi-Yau manifold yields the exact quantum Kahler potential of the Kahler moduli space of that manifold. Since four-dimensional N=2 gauge theories can be engineered by non-compact Calabi-Yau threefolds, this implies that it is possible to obtain exact gauge theory Kahler potentials from two-sphere partition functions. In this paper, we demonstrate that the Seiberg-Witten Kahler potential can indeed be obtained as a two-sphere partition function. To be precise, we extract the quantum Kahler metric of 4D N=2 SU(2) Super-Yang-Mills theory by taking the field theory limit of the Kahler parameters of the O(-2,-2) bundle over P1 x P1. We expect this method of computing the Kahler potential to generalize to other four-dimensional N=2 gauge theories that can be geometrically engineered by toric Calabi-Yau threefolds.

Paper Structure

This paper contains 6 sections, 80 equations, 2 tables.