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Persistence of Monoclinic Crystal Structure in 3D Second-Order Topological Insulator Candidate 1T'-MoTe2 Thin Flake Without Structural Phase Transition.
Su, Bo; Huang, Yuan; Hou, Yan Hui; Li, Jiawei; Yang, Rong; Ma, Yongchang; Yang, Yang; Zhang, Guangyu; Zhou, Xingjiang; Luo, Jianlin; Chen, Zhi-Guo.
Affiliation
  • Su B; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Huang Y; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100190, China.
  • Hou YH; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Li J; Songshan Lake Materials Laboratory, Dongguan, 523808, China.
  • Yang R; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Ma Y; School of Materials Science and Engineering, Tianjin University of Technology, Tianjin, 300384, China.
  • Yang Y; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Zhang G; School of Physical Sciences, University of Chinese Academy of Sciences, Beijing, 100190, China.
  • Zhou X; Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing, 100190, China.
  • Luo J; Songshan Lake Materials Laboratory, Dongguan, 523808, China.
  • Chen ZG; School of Materials Science and Engineering, Tianjin University of Technology, Tianjin, 300384, China.
Adv Sci (Weinh) ; 9(5): e2101532, 2022 Feb.
Article in En | MEDLINE | ID: mdl-34923770
ABSTRACT
A van der Waals material, MoTe2 with a monoclinic 1T' crystal structure is a candidate for 3D second-order topological insulators (SOTIs) hosting gapless hinge states and insulating surface states. However, due to the temperature-induced structural phase transition, the monoclinic 1T' structure of MoTe2 is transformed into the orthorhombic Td structure as the temperature is lowered, which hinders the experimental verification and electronic applications of the predicted SOTI state at low temperatures. Here, systematic Raman spectroscopy studies of the exfoliated MoTe2 thin flakes with variable thicknesses at different temperatures, are presented. As a spectroscopic signature of the orthorhombic Td structure of MoTe2 , the out-of-plane vibration mode D at ≈ 125 cm-1 is always visible below a certain temperature in the multilayer flakes thicker than ≈ 27.7 nm, but vanishes in the temperature range from 80 to 320 K when the flake thickness becomes lower than ≈ 19.5 nm. The absence of the out-of-plane vibration mode D in the Raman spectra here demonstrates not only the disappearance of the monoclinic-to-orthorhombic phase transition but also the persistence of the monoclinic 1T' structure in the MoTe2 thin flakes thinner than ≈ 19.5 nm at low temperatures down to 80 K, which may be caused by the high enough density of the holes introduced during the gold-enhanced exfoliation process and exposure to air. The MoTe2 thin flakes with the low-temperature monoclinic 1T' structure provide a material platform for realizing SOTI states in van der Waals materials at low temperatures, which paves the way for developing a new generation of electronic devices based on SOTIs.
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Full text: 1 Collection: 01-internacional Database: MEDLINE Type of study: Prognostic_studies Language: En Journal: Adv Sci (Weinh) Year: 2022 Document type: Article Affiliation country: China

Full text: 1 Collection: 01-internacional Database: MEDLINE Type of study: Prognostic_studies Language: En Journal: Adv Sci (Weinh) Year: 2022 Document type: Article Affiliation country: China