强磁场中带电任意子气体基态能量的解析方法

B. Abdullaev, U. Rößler, C. Park, M. Musakhanov
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引用次数: 0

摘要

本文给出了二维任意子气体在强磁场中(朗道能级填充因子νL≤1)基态能量的解析公式。该公式是通过将消失约束的谐波势正则化应用于谐波约束的库仑任意子气体得到的。在没有库仑相互作用的情况下,我们的分析结果提供了一个精确解。它包含由任意子参数ν和ν l表征的任意子规范场的贡献。在存在库仑相互作用的情况下,我们引入了一个依赖于参数ν, ν l和密度参数rs的函数。该函数是通过拟合自旋极化电子分数量子霍尔效应域中的fino - ortolani插值方程以及在强磁场中二维库仑玻色气体基态能量与已知结果的一致性要求来确定的。我们证明了我们的公式不仅对费米子(ν = 1)有效,而且对任何子(0≤ν≤1)都有效。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Analytic approach to ground state energy of charged anyon gas in strong magnetic field
We present analytic formulas for the ground state energy of two-dimensional (2D) anyon gas in strong magnetic field (Landau level filling factor νL ≤ 1). The formulas are obtained by applying harmonic potential regularization for the vanishing confinement to harmonically confined Coulomb anyon gas. In a case of absence of the Coulomb interaction our analytic result provides an exact solution. It contains a contribution of the anyon gauge field characterized by the anyon parameters ν and νL. In a case of presence of the Coulomb interaction we introduce a function depending on the parameters ν, νL and the density parameter rs. The function is determined by fitting the Fano-Ortolani interpolation equation in the fractional quantum Hall effect regime for spinpolarized electrons and by consistence requirement with known results for the ground state energy of the 2D Coulomb Bose gas in strong magnetic field. We show that our formulas are valid not only for fermions (ν = 1) but quite generally for anyons (0 ≤ ν ≤ 1).
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