Department of Physics, Kyoto University, Kyoto, Japan.
Department of Advanced Materials Science, University of Tokyo, Chiba, Japan.
Nature. 2018 Jul;559(7713):227-231. doi: 10.1038/s41586-018-0274-0. Epub 2018 Jul 11.
The quantum Hall effect in two-dimensional electron gases involves the flow of topologically protected dissipationless charge currents along the edges of a sample. Integer or fractional electrical conductance is associated with edge currents of electrons or quasiparticles with fractional charges, respectively. It has been predicted that quantum Hall phenomena can also be created by edge currents with a fundamentally different origin: the fractionalization of quantum spins. However, such quantization has not yet been observed. Here we report the observation of this type of quantization of the Hall effect in an insulating two-dimensional quantum magnet, α-RuCl, with a dominant Kitaev interaction (a bond-dependent Ising-type interaction) on a two-dimensional honeycomb lattice. We find that the application of a magnetic field parallel to the sample destroys long-range magnetic order, leading to a field-induced quantum-spin-liquid ground state with substantial entanglement of local spins. In the low-temperature regime of this state, the two-dimensional thermal Hall conductance reaches a quantum plateau as a function of the applied magnetic field and has a quantization value that is exactly half of the two-dimensional thermal Hall conductance of the integer quantum Hall effect. This half-integer quantization of the thermal Hall conductance in a bulk material is a signature of topologically protected chiral edge currents of charge-neutral Majorana fermions (particles that are their own antiparticles), which have half the degrees of freedom of conventional fermions. These results demonstrate the fractionalization of spins into itinerant Majorana fermions and Z fluxes, which is predicted to occur in Kitaev quantum spin liquids. Above a critical magnetic field, the quantization disappears and the thermal Hall conductance goes to zero rapidly, indicating a topological quantum phase transition between the states with and without chiral Majorana edge modes. Emergent Majorana fermions in a quantum magnet are expected to have a great impact on strongly correlated quantum matter, opening up the possibility of topological quantum computing at relatively high temperatures.
二维电子气中的量子霍尔效应涉及拓扑保护无耗散电荷电流沿样品边缘流动。整数或分数电导率分别与具有分数电荷的电子或准粒子的边缘电流相关联。有人预测,量子霍尔现象也可以通过具有根本不同起源的边缘电流来产生:量子自旋的分数化。然而,这种量化尚未被观察到。在这里,我们报告了在二维量子磁体 α-RuCl 中观察到这种类型的霍尔效应的量子化,该磁体在二维蜂窝晶格上具有主导的 Kitaev 相互作用(依赖于键的各向异性 Ising 型相互作用)。我们发现,平行于样品施加磁场会破坏长程磁有序,导致磁场诱导的量子自旋液体基态,其中局部自旋具有大量纠缠。在该状态的低温区,二维热霍尔电导率作为外加磁场的函数达到量子平台,并且具有与整数量子霍尔效应的二维热霍尔电导率精确一半的量子化值。大块材料中热霍尔电导率的这种半整数量子化是电荷中性马约拉纳费米子(其自身反粒子的粒子)的拓扑保护手征边缘电流的特征,其自由度是传统费米子的一半。这些结果证明了自旋分数化为巡游马约拉纳费米子和 Z 通量,这被预测在 Kitaev 量子自旋液体中发生。在临界磁场以上,量子化消失,热霍尔电导率迅速降至零,表明具有手征马约拉纳边缘模式和无手征马约拉纳边缘模式的状态之间存在拓扑量子相变。量子磁体中的涌现马约拉纳费米子有望对强关联量子物质产生重大影响,为在相对较高温度下实现拓扑量子计算开辟了可能性。