Loop Grassmannian of quivers and Compactified Coulomb branch of quiver gauge theory with no framing

Fuente: arXiv
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Autor principal: Dong, Zhijie
Formato: Preprint
Publicado: 2024
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author Dong, Zhijie
author_facet Dong, Zhijie
contents Mirković introduced the notion of loop Grassmannian for symmetric integer matrix $κ$. It is a two-step limit of the local projective space $Z_κ^α$, which generalizes the usual Zastava for a simply laced group $G$. The usual loop Grassmannian of $G$ is recovered when the matrix $κ$ is the Cartan matrix of $G$. On the other hand, Braverman, Finkelberg, and Nakajima showed that the Compactified Coulomb branch $\mathbf{M}_{Q}^α$ for the quiver gauge theory with no framing also generalizes the usual Zastava. We show that in the case when $κ$ is the associated matrix of the quiver $Q$, these two generalizations of Zastava coincide, i.e $\mathbf{M}_{Q}^α\cong Z_{κ(Q)}^α$.
format Preprint
id arxiv_https___arxiv_org_abs_2408_05458
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Loop Grassmannian of quivers and Compactified Coulomb branch of quiver gauge theory with no framing
Dong, Zhijie
Representation Theory
Algebraic Geometry
Mirković introduced the notion of loop Grassmannian for symmetric integer matrix $κ$. It is a two-step limit of the local projective space $Z_κ^α$, which generalizes the usual Zastava for a simply laced group $G$. The usual loop Grassmannian of $G$ is recovered when the matrix $κ$ is the Cartan matrix of $G$. On the other hand, Braverman, Finkelberg, and Nakajima showed that the Compactified Coulomb branch $\mathbf{M}_{Q}^α$ for the quiver gauge theory with no framing also generalizes the usual Zastava. We show that in the case when $κ$ is the associated matrix of the quiver $Q$, these two generalizations of Zastava coincide, i.e $\mathbf{M}_{Q}^α\cong Z_{κ(Q)}^α$.
title Loop Grassmannian of quivers and Compactified Coulomb branch of quiver gauge theory with no framing
topic Representation Theory
Algebraic Geometry
url https://arxiv.org/abs/2408.05458