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Recipe for generating Weyl semimetals with extended topologically protected features

机译:生成具有扩展的拓扑保护功能的Weyl半金属的配方

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摘要

We present a recipe that leads to Weyl semimetals with extended topologically protected features. We show that compounds in a family that possess time-reversal symmetry and share a noncentrosymmetric cubic structure with the space group F-43m (no. 216) host robust Weyl fermions with extended and easily measurable protected features. The candidates in this family are compounds with different chemical formulas, AB_2, ABC, ABC_2, and ABCD, and their Fermi levels are predominantly populated by nontrivial Weyl fermions. Symmetry of the system requires that the Weyl nodes with opposite chirality are well separated in momentum space. Adjacent Weyl points have the same chirality; thus these Weyl nodes would not annihilate each other with respect to lattice perturbations. As Fermi arcs and surface states connect Weyl nodes with opposite chirality, the large separation of the latter in momentum space guarantees the appearance of very long arcs and surface states. This work demonstrates that the use of system symmetry by first-principles calculations is a powerful approach for discovering new Weyl semimetals with attractive features whose protected fermions may be candidates of many applications.
机译:我们提出了一种配方,该配方导致具有扩展的拓扑保护功能的Weyl半金属。我们表明,具有时间反转对称性并且与空间群F-43m(编号216)共享一个非中心对称立方结构的化合物可以容纳具有扩展且易于测量的受保护特征的坚固的Weyl费米子。该族的候选化合物是具有不同化学式AB_2,ABC,ABC_2和ABCD的化合物,其费米水平主要由非平凡的魏尔费米子组成。系统的对称性要求手性相反的Weyl节点在动量空间中要很好地分开。相邻的Weyl点具有相同的手性;因此,这些Weyl节点不会因晶格扰动而相互消灭。当费米弧和表面态以相反的手性连接Weyl节点时,后者在动量空间中的较大分隔保证了非常长的弧和表面态的出现。这项工作表明,通过第一性原理计算使用系统对称性是发现具有有吸引力特征的新型韦尔半金属的有力方法,其受保护的费米子可能是许多应用的候选人。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2017年第12期|121104.1-121104.5|共5页
  • 作者单位

    Department of Physics, South University of Science and Technology of China, Shenzhen 518055, Peoples Republic of China,Institute for Structure and Function & Department of Physics, Chongqing University, Chongqing 400044, Peoples Republic of China;

    Department of Physics, South University of Science and Technology of China, Shenzhen 518055, Peoples Republic of China,Dalian Institute of Chemical Physics, Chinese Academy of Sciences, 116023 Dalian, Peoples Republic of China;

    Department of Physics, South University of Science and Technology of China, Shenzhen 518055, Peoples Republic of China;

    Department of Physics, South University of Science and Technology of China, Shenzhen 518055, Peoples Republic of China;

    Department of Physics, South University of Science and Technology of China, Shenzhen 518055, Peoples Republic of China,Key Laboratory of Advanced Technology of Materials (Ministry of Education), Superconductivity and New Energy R&D Center, Southwest Jiaotong University, Chengdu, 610031 Sichuan, Peoples Republic of China;

    Department of Physics, South University of Science and Technology of China, Shenzhen 518055, Peoples Republic of China,Institute for Structure and Function & Department of Physics, Chongqing University, Chongqing 400044, Peoples Republic of China;

    Department of Physics, South University of Science and Technology of China, Shenzhen 518055, Peoples Republic of China;

    Department of Physics, South University of Science and Technology of China, Shenzhen 518055, Peoples Republic of China,School of Science and Engineering, The Chinese University of Hong Kong (Shenzhen), 518172 Shenzhen, Peoples Republic of China;

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