Zhang Ya-Hui
William H. Miller III Department of Physics and Astronomy, <a href="https://ror.org/00za53h95">Johns Hopkins University</a>, Baltimore, Maryland, 21218, USA.
Phys Rev Lett. 2024 Sep 6;133(10):106502. doi: 10.1103/PhysRevLett.133.106502.
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.
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。