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莫尔陈带中具有分数量子自旋霍尔效应的涡旋自旋液体

Vortex Spin Liquid with Fractional Quantum Spin Hall Effect in Moiré Chern Bands.

作者信息

Zhang Ya-Hui

机构信息

William H. Miller III Department of Physics and Astronomy, <a href="https://ror.org/00za53h95">Johns Hopkins University</a>, Baltimore, Maryland, 21218, USA.

出版信息

Phys Rev Lett. 2024 Sep 6;133(10):106502. doi: 10.1103/PhysRevLett.133.106502.

Abstract

Recently there is a report of the experimental signatures of a fractional quantum spin hall (FQSH) state at hole filling n=3 in a twisted MoTe_{2} bilayer. Previous theories of FQSH phases simply considered a decoupled pair of a fractional quantum Hall phase and its time reversal partner. Here, we show the first construction of an FQSH phase beyond the decoupling picture. We consider a pair of half-filled C=±1 Chern bands in the two valleys, similar to the well-studied quantum Hall bilayer, but now with opposite chiralities. Because of the strong intervalley repulsion, we expect a charge gap to open with low-energy physics dominated by the neutral intervalley excitons. However, the presence of an effective "flux" frustrates exciton condensation by proliferating vortices. Here, we construct a vortex liquid of excitons dubbed a vortex spin liquid, formed from exciton pairing of the composite fermions in the decoupled composite Fermi liquid phase. This insulator is a quantum spin liquid with gapless spin excitations carried by the flux of an emergent U(1) gauge field. Additionally, there exist neutral and spinless Fermi surfaces formed by fermionic vortices of a nearby intervalley-coherent order. Unlike a conventional Mott insulator, the vortex spin liquid phase also exhibits a quantized FQSH effect with gapless helical charge modes along the edge. Our work demonstrates the possibility of nontrivial FQSH phases and provides predictions to detect them in future experiments.

摘要

最近有报道称,在扭曲的二碲化钼双层中,空穴填充率n = 3时出现了分数量子自旋霍尔(FQSH)态的实验特征。先前关于FQSH相的理论仅考虑了分数量子霍尔相及其时间反演伙伴的解耦对。在此,我们展示了超越解耦图景的FQSH相的首次构建。我们考虑在两个谷中一对半填充的C = ±1陈数带,类似于经过充分研究的量子霍尔双层,但现在具有相反的手性。由于强烈的谷间排斥,我们预计会打开一个电荷能隙,其低能物理由中性谷间激子主导。然而,有效“磁通”的存在通过增殖涡旋阻碍了激子凝聚。在此,我们构建了一种激子涡旋液体,称为涡旋自旋液体,它由解耦的复合费米液体相中复合费米子的激子配对形成。这种绝缘体是一种量子自旋液体,具有由涌现的U(1)规范场的磁通携带的无隙自旋激发。此外,还存在由附近谷间相干序的费米子涡旋形成的中性和无自旋费米面。与传统的莫特绝缘体不同,涡旋自旋液体相还表现出沿边缘具有无隙螺旋电荷模式的量化FQSH效应。我们的工作证明了非平凡FQSH相的可能性,并为未来实验中检测它们提供了预测。

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