颤振涡旋模空间的体积

Kazutoshi Ohta, N. Sakai
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引用次数: 4

摘要

研究了紧致黎曼曲面上颤振规范理论中BPS涡的模空间体积。BPS涡旋的存在对颤振规范理论提出了限制。我们证明了在超对称颤振规范理论中,一个合适的上同算子(体积算子)的vev给出了模空间体积,其中嵌入了涡旋的BPS方程。在超对称规范理论中,利用局部化将模空间体积精确地计算为轮廓积分。图论对于构造超对称颤振规范理论和导出体积公式都是有用的。体积的轮廓积分公式(对Jeffrey-Kirwan残量公式的推广)导致了Bradlow边界(涡度的上界由黎曼曲面的面积除以涡的固有尺寸)。给出了各种颤振规范理论的一些例子,并讨论了这些理论中模空间体积的性质。我们的公式应用于具有$CP^N$目标空间的测量非线性sigma模型的涡旋模空间的体积,该模型是由母颤振规范理论的强耦合极限得到的。我们还讨论了颤振规范理论的非阿贝尔推广和体积公式的“阿贝尔化”。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The volume of the quiver vortex moduli space
We study the moduli space volume of BPS vortices in quiver gauge theories on compact Riemann surfaces. The existence of BPS vortices imposes constraints on the quiver gauge theories. We show that the moduli space volume is given by a vev of a suitable cohomological operator (volume operator) in a supersymmetric quiver gauge theory, where BPS equations of the vortices are embedded. In the supersymmetric gauge theory, the moduli space volume is exactly evaluated as a contour integral by using the localization. Graph theory is useful to construct the supersymmetric quiver gauge theory and to derive the volume formula. The contour integral formula of the volume (generalization of the Jeffrey-Kirwan residue formula) leads to the Bradlow bounds (upper bounds on the vorticity by the area of the Riemann surface divided by the intrinsic size of the vortex). We give some examples of various quiver gauge theories and discuss properties of the moduli space volume in these theories. Our formula are applied to the volume of the vortex moduli space in the gauged non-linear sigma model with $CP^N$ target space, which is obtained by a strong coupling limit of a parent quiver gauge theory. We also discuss a non-Abelian generalization of the quiver gauge theory and "Abelianization" of the volume formula.
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