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Emergence of non-centrosymmetric topologicalinsulating phase in BiTeI under pressure

机译:BiTeI中非中心对称拓扑绝缘相在压力下的出现

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摘要

The spin–orbit interaction affects the electronic structure of solids in various ways. Topologicalinsulators are one example in which the spin–orbit interaction leads the bulk bands to havea non-trivial topology, observable as gapless surface or edge states. Another example is theRashba effect, which lifts the electron-spin degeneracy as a consequence of the spin–orbitinteraction under broken inversion symmetry. It is of particular importance to know how thesetwo effects, that is, the non-trivial topology of electronic states and the Rashba spin splitting,interplay with each other. Here we show through sophisticated first-principles calculations thatBiTeI, a giant bulk Rashba semiconductor, turns into a topological insulator under a reasonablepressure. This material is shown to exhibit several unique features, such as a highly pressuretunable giant Rashba spin splitting, an unusual pressure-induced quantum phase transition,and more importantly, the formation of strikingly different Dirac surface states at oppositesides of the material.
机译:自旋轨道相互作用以各种方式影响固体的电子结构。拓扑绝缘子是一个示例,其中自旋-轨道相互作用导致体带具有不平凡的拓扑,可观察为无间隙的表面或边缘状态。另一个例子是拉什巴效应(Rashba effect),由于破坏了反演对称性,自旋-轨道相互作用导致了电子自旋简并性。了解这两种效应(即电子状态的非平凡拓扑和Rashba自旋分裂,相互影响)如何特别重要。在这里,我们通过复杂的第一性原理计算表明,巨大的Rashba体半导体BiTeI在合理的压力下变成了拓扑绝缘体。该材料显示出一些独特的特征,例如,高度可调的巨型Rashba自旋分裂,异常的压力诱导的量子相变,更重要的是,在材料的相对侧形成了明显不同的Dirac表面态。

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