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

Manuel Calixto, A. Mayorgas, J. Guerrero
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引用次数: 0

摘要

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