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扭曲双层石墨烯中量子反常霍尔铁磁体的集体激发

Collective Excitations of Quantum Anomalous Hall Ferromagnets in Twisted Bilayer Graphene.

作者信息

Wu Fengcheng, Das Sarma Sankar

机构信息

Condensed Matter Theory Center and Joint Quantum Institute, Department of Physics, University of Maryland, College Park, Maryland 20742, USA.

出版信息

Phys Rev Lett. 2020 Jan 31;124(4):046403. doi: 10.1103/PhysRevLett.124.046403.

Abstract

We present a microscopic theory for collective excitations of quantum anomalous Hall ferromagnets (QAHF) in twisted bilayer graphene. We calculate the spin magnon and valley magnon spectra by solving Bethe-Salpeter equations and verify the stability of QAHF. We extract the spin stiffness from the gapless spin wave dispersion and estimate the energy cost of a skyrmion-antiskyrmion pair, which is found to be comparable in energy with the Hartree-Fock gap. The valley wave mode is gapped, implying that the valley polarized state is more favorable compared to the valley coherent state. Using a nonlinear sigma model, we estimate the valley ordering temperature, which is considerably reduced from the mean-field transition temperature due to thermal excitations of valley waves.

摘要

我们提出了一种关于扭曲双层石墨烯中量子反常霍尔铁磁体(QAHF)集体激发的微观理论。我们通过求解贝特 - 萨尔皮特方程来计算自旋磁振子和能谷磁振子谱,并验证了QAHF的稳定性。我们从无隙自旋波色散中提取出自旋刚度,并估计了一个斯格明子 - 反斯格明子对的能量成本,发现其能量与哈特里 - 福克能隙相当。能谷波模式是有能隙的,这意味着与能谷相干态相比,能谷极化态更有利。使用非线性西格玛模型,我们估计了能谷有序温度,由于能谷波的热激发,该温度比平均场转变温度大幅降低。

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