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Robustness of topological states with respect to lattice instability in the nonsymmorphic topological insulator KHgSb

机译:非对杂拓扑绝缘体Khgsb中拓扑状态对晶格不稳定的鲁棒性

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摘要

We report a polarized Raman scattering study of nonsymmorphic topological insulator KHgSb with hourglasslike electronic dispersion. Supported by theoretical calculations, we show that the lattice of the previously assigned space group P6_3/mmc (No. 194) is unstable in KHgSb. While we observe one of two calculated Raman active E_(2g) phonons of space group P63/mmc at room temperature, an additional A_(1g) peak appears at 99.5 cm~(-1) upon cooling below T* = 150 K, which suggests a lattice distortion. Several weak peaks associated with two-phonon excitations emerge with this lattice instability. We also show that the sample is very sensitive to high temperature and high laser power, conditions under which it quickly decomposes, leading to the formation of Sb. Our first-principles calculations indicate that space group P6_(3mc) (No. 186), corresponding to a vertical displacement of the Sb atoms with respect to the Hg atoms that breaks the inversion symmetry, is lower in energy than the presumed P6_3/mmc structure and preserves the glide-plane symmetry necessary to the formation of hourglass fermions.
机译:我们报道了具有沙漏电子分散的非无约态拓扑绝缘体Khgsb的极化拉​​曼散射研究。通过理论计算支持,我们表明先前分配的空间组P6_3 / MMC(194年)的晶格在KHGSB中不稳定。虽然我们在室温下观察到空间组P63 / MMC的两个计算的拉曼有源E_(2G)声子,但在冷却下方T * = 150 k以下时,额外的A_(1G)峰值出现在99.5cm〜(-1)。建议格子扭曲。与双声子激发相关的几个弱峰值出现了这种晶格不稳定。我们还表明,样品对高温和高激光功率非常敏感,它迅速分解的条件,导致形成SB。我们的第一原理计算表明,对应于SB原子的垂直位移的空间组P6_(3MC)(No.186)相对于断裂反转对称的HG原子,能量低于假定的P6_3 / MMC结构并保留形成沙漏码头所需的滑动平面对称性。

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  • 来源
    《Physical Review. B, Condensed Matter》 |2017年第6期|064102.1-064102.8|共8页
  • 作者单位

    Beijing National Laboratory for Condensed Matter Physics and Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Beijing National Laboratory for Condensed Matter Physics and Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Beijing National Laboratory for Condensed Matter Physics and Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Beijing National Laboratory for Condensed Matter Physics and Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Department of Physics & Astronomy Rutgers University Piscataway New Jersey 08854 USA;

    Beijing National Laboratory for Condensed Matter Physics and Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China;

    Beijing National Laboratory for Condensed Matter Physics and Institute of Physics Chinese Academy of Sciences Beijing 100190 China;

    Beijing National Laboratory for Condensed Matter Physics and Institute of Physics Chinese Academy of Sciences Beijing 100190 China Collaborative Innovation Center of Quantum Matter Beijing China;

    Beijing National Laboratory for Condensed Matter Physics and Institute of Physics Chinese Academy of Sciences Beijing 100190 China Collaborative Innovation Center of Quantum Matter Beijing China;

    Beijing National Laboratory for Condensed Matter Physics and Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China Collaborative Innovation Center of Quantum Matter Beijing China;

    Beijing National Laboratory for Condensed Matter Physics and Institute of Physics Chinese Academy of Sciences Beijing 100190 China School of Physical Sciences University of Chinese Academy of Sciences Beijing 100049 China Collaborative Innovation Center of Quantum Matter Beijing China;

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