Ghorashi Sayed Ali Akbar, Li Tianhe, Hughes Taylor L
Department of Physics, William & Mary, Williamsburg, Virginia 23187, USA.
Department of Physics and Institute for Condensed Matter Theory, University of Illinois at Urbana-Champaign, Illinois 61801, USA.
Phys Rev Lett. 2020 Dec 31;125(26):266804. doi: 10.1103/PhysRevLett.125.266804.
We investigate higher-order Weyl semimetals (HOWSMs) having bulk Weyl nodes attached to both surface and hinge Fermi arcs. We identify a new type of Weyl node, which we dub a 2nd-order Weyl node, that can be identified as a transition in momentum space in which both the Chern number and a higher order topological invariant change. As a proof of concept we use a model of stacked higher order quadrupole insulators (QI) to identify three types of WSM phases: 1st order, 2nd order, and hybrid order. The model can also realize type-II and hybrid-tilt WSMs with various surface and hinge arcs. After a comprehensive analysis of the topological properties of various HOWSMs, we turn to their physical implications that show the very distinct behavior of 2nd-order Weyl nodes when they are gapped out. We obtain three remarkable results: (i) the coupling of a 2nd-order Weyl phase with a conventional 1st-order one can lead to a hybrid-order topological insulator having coexisting surface cones and flat hinge arcs that are independent and not attached to each other. (ii) A nested 2nd-order inversion-symmetric WSM by a charge-density wave (CDW) order generates an insulating phase having coexisting flatband surface and hinge states all over the Brillouin zone. (iii) A CDW order in a time-reversal symmetric higher-order WSM gaps out a 2nd-order node with a 1st-order node and generates an insulating phase having coexisting surface Dirac cone and hinge arcs. Moreover, we show that a measurement of charge density in the presence of magnetic flux can help to identify some classes of 2nd-order WSMs. Finally, we show that periodic driving can be utilized as a way for generating HOWSMs. Our results are relevant to metamaterials as well as various phases of Cd_{3}As_{2}, KMgBi, and rutile-structure PtO_{2} that have been predicted to realize higher order Dirac semimetals.
我们研究了具有与表面和棱边费米弧相连的体 Weyl 节点的高阶 Weyl 半金属(HOWSMs)。我们识别出一种新型的 Weyl 节点,我们将其称为二阶 Weyl 节点,它可被视为动量空间中的一种转变,其中陈数和一个高阶拓扑不变量都会发生变化。作为概念验证,我们使用堆叠高阶四极绝缘体(QI)模型来识别三种类型的 Weyl 半金属相:一阶、二阶和混合阶。该模型还可以实现具有各种表面和棱边弧的 II 型和混合倾斜 Weyl 半金属。在对各种 HOWSMs 的拓扑性质进行全面分析之后,我们转向它们的物理意义,这表明二阶 Weyl 节点在能隙化时具有非常独特的行为。我们得到了三个显著的结果:(i)二阶 Weyl 相与传统一阶相的耦合可以导致一种混合阶拓扑绝缘体,其共存的表面锥和扁平棱边弧相互独立且不相连。(ii)由电荷密度波(CDW)序嵌套的二阶反演对称 Weyl 半金属会产生一个绝缘相,在整个布里渊区共存着平带表面态和棱边态。(iii)时间反演对称高阶 Weyl 半金属中的 CDW 序会使一个二阶节点与一个一阶节点能隙化,并产生一个共存表面狄拉克锥和棱边弧的绝缘相。此外,我们表明在存在磁通量的情况下测量电荷密度有助于识别某些类型的二阶 Weyl 半金属。最后,我们表明周期性驱动可以用作产生 HOWSMs 的一种方式。我们的结果与超材料以及 Cd₃As₂、KMgBi 和金红石结构的 PtO₂ 的各种相相关,这些材料已被预测可实现高阶狄拉克半金属。