Hilbert space structure and classical limit of the low energy sector of U(N) quantum Hall ferromagnets

Manuel Calixto, A. Mayorgas, J. Guerrero
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Abstract

Using the Lieb–Mattis ordering theorem of electronic energy levels, we identify and construct the Hilbert space of the low energy sector of U(N) quantum Hall/Heisenberg ferromagnets at filling factor M for L Landau/lattice sites. The carrier Hilbert space of irreducible representations of U(N) is described by rectangular Young tableaux of M rows and L columns, and associated with Grassmannian phase spaces U(N)/U(M)×U(N-M). Replacing U(N)-spin operators by their expectation values in a Grassmannian coherent state allows for a semi-classical treatment of the low energy U(N)-spin-wave coherent excitations (skyrmions) of U(N) quantum Hall ferromagnets in terms of Grasmannian nonlinear sigma models.
U(N)量子霍尔铁磁体的希尔伯特空间结构和低能段的经典极限
利用电子能级的利布-马蒂斯排序定理,我们确定并构建了 L 个兰道/晶格位点填充因子为 M 的 U(N) 量子霍尔/海森堡铁磁体低能段的希尔伯特空间。U(N) 不可还原表征的载波希尔伯特空间由 M 行 L 列的矩形杨表描述,并与格拉斯曼相空间 U(N)/U(M)×U(N-M) 相关联。用它们在格拉斯曼相干态中的期望值代替 U(N)-spin 算子,就可以用格拉斯曼非线性西格玛模型对 U(N) 量子霍尔铁磁体的低能 U(N)-spin 波相干激发(skyrmions)进行半经典处理。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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