4.6 Article

Quantum spin Hall effect in tilted penta silicene and its isoelectronic substitutions

Journal

PHYSICAL CHEMISTRY CHEMICAL PHYSICS
Volume 24, Issue 25, Pages 15201-15207

Publisher

ROYAL SOC CHEMISTRY
DOI: 10.1039/d2cp01390h

Keywords

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Funding

  1. National Natural Science Foundation of China [11874307, 22073076]
  2. Fundamental Research Funds for the Central Universities of China [20720210023]

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In this study, a new topological allotrope of silicene, named tilted penta silicene, is discovered using an adaptive genetic algorithm. The geometric and electronic properties of this allotrope and its isoelectronic substitutions (Ge, Sn) are investigated. The results show that tilted penta silicene exhibits topological insulator behavior and remains stable after isoelectronic substitutions.
Silicene, a competitive two-dimensional (2D) material for future electronic devices, has attracted intensive attention in condensed matter physics. Utilizing an adaptive genetic algorithm (AGA), we identify a topological allotrope of silicene, named tilted penta (tPenta) silicene. Based on first-principles calculations, the geometric and electronic properties of tPenta silicene and its isoelectronic substitutions (Ge, Sn) are investigated. Our results indicate that tPenta silicene exhibits a semimetallic state with distorted Dirac cones in the absence of spin-orbit coupling (SOC). When SOC is considered, it shows semiconducting behavior with a gap opening of 2.4 meV at the Dirac point. Based on the results of Z(2) invariant (Z(2) = 1) and the helical edge states, we demonstrate that tPenta silicene is a topological insulator. Furthermore, the effect of isoelectronic substitutions on tPenta silicene is studied. Two stoichiometric phases, i.e., tPenta Si0.333Ge0.667 and tPenta Si0.333Sn0.667 are found to retain the geometric framework of tPenta silicene and exhibit high stabilities. Our calculations show that both tPenta Si(0.333)Ge(0.66)7 and tPenta Si0.333Sn0.667 are QSH insulators with enlarged band gaps of 32.5 meV and 94.3 meV, respectively, at the HSE06 level, offering great potential for practical applications at room temperature.

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