• Chinese Physics B
  • Vol. 29, Issue 9, (2020)
Changlin Yan1、2, Cong Wang2, Linwei Zhou2, Pengjie Guo2, Kai Liu2, Zhong-Yi Lu2, Zhihai Cheng2, Yang Chai3, Anlian Pan4, and Wei Ji2、†
Author Affiliations
  • 1School of Physics and Electronics, Hunan University, Changsha 40082, China
  • 2Beijing Key Laboratory of Optoelectronic Functional Materials & Micro-Nano Devices, Department of Physics, Renmin University of China, Beijing 10087, China
  • 3The Hong Kong Polytechnic University, Hung Hom, Kowloon, Hong Kong, China
  • 4Key Laboratory for Micro-Nano Physics and Technology of Hunan Province, College of Materials Science and Engineering, Hunan University, Changsha 10082, China
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    DOI: 10.1088/1674-1056/aba606 Cite this Article
    Changlin Yan, Cong Wang, Linwei Zhou, Pengjie Guo, Kai Liu, Zhong-Yi Lu, Zhihai Cheng, Yang Chai, Anlian Pan, Wei Ji. Two ultra-stable novel allotropes of tellurium few-layers[J]. Chinese Physics B, 2020, 29(9): Copy Citation Text show less
    (a) and (b) Top- and side-view of the bilayer α and δ phases, respectively. (c)–(f) Top- and side-views of monolayer Te in γ, β, ε, and ζ phases, respectively. Orange, red, and blue balls represent Te atoms in different sublayers along the interlayer direction z. (g)–(h) Total energies per Te atom and surface energies per unit area in different phases as a function of number of sublayers, respectively. The monolayer Te in α, γ, δ, ε, and ζ are presented with green, magenta, blue, orange, red, and black symbols, respectively.
    Fig. 1. (a) and (b) Top- and side-view of the bilayer α and δ phases, respectively. (c)–(f) Top- and side-views of monolayer Te in γ, β, ε, and ζ phases, respectively. Orange, red, and blue balls represent Te atoms in different sublayers along the interlayer direction z. (g)–(h) Total energies per Te atom and surface energies per unit area in different phases as a function of number of sublayers, respectively. The monolayer Te in α, γ, δ, ε, and ζ are presented with green, magenta, blue, orange, red, and black symbols, respectively.
    Structure evolution of ζ Te after layer stacking. (a) Bond lengths as a function of the number of sublayers. The blue and red lines correspond to intra- and average interlayer Te–Te bond lengths, respectively. (b) The evolution of layer heights in ζ few-layer with respect to sublayer number. The layers marked in red dotted rectangular frame tend to form a dimer or trimer when stacking together.
    Fig. 2. Structure evolution of ζ Te after layer stacking. (a) Bond lengths as a function of the number of sublayers. The blue and red lines correspond to intra- and average interlayer Te–Te bond lengths, respectively. (b) The evolution of layer heights in ζ few-layer with respect to sublayer number. The layers marked in red dotted rectangular frame tend to form a dimer or trimer when stacking together.
    Topological properties of tri-sublayer ζ Te. (a) The orbital projection of the tri-sublayer ζ without SOC. (b) The band structure of the tri-sublayer ζ with SOC. Red dashed rectangles mark the location of the band inversion and band opening with the SOC effect. The four time-reversal invariant points are labeled as Γ, X, Y and S. (c) The parities of filled states of tri-sublayer ζ at four time-reversal-invariant points in the Brillouin zone. The “+” and “–” correspond to even and odd parity, respectively. (d) Edge states of the ribbon ζ. Red and blue lines represent the ribbon and bulk states, respectively.
    Fig. 3. Topological properties of tri-sublayer ζ Te. (a) The orbital projection of the tri-sublayer ζ without SOC. (b) The band structure of the tri-sublayer ζ with SOC. Red dashed rectangles mark the location of the band inversion and band opening with the SOC effect. The four time-reversal invariant points are labeled as Γ, X, Y and S. (c) The parities of filled states of tri-sublayer ζ at four time-reversal-invariant points in the Brillouin zone. The “+” and “–” correspond to even and odd parity, respectively. (d) Edge states of the ribbon ζ. Red and blue lines represent the ribbon and bulk states, respectively.
    Phase diagram of Te under charge doping. Relative total energy of mono- (a), bi- (b), and four-layer (c) Te in different phases as a function of electron/hole doping level. The total energies of the ζ phase were chosen as the energy reference. Lines with different colors correspond to the relative energies of different phases: α, black; β, red; γ, blue; δ, dark cyan; ε, magenta; ζ, dark gray.
    Fig. 4. Phase diagram of Te under charge doping. Relative total energy of mono- (a), bi- (b), and four-layer (c) Te in different phases as a function of electron/hole doping level. The total energies of the ζ phase were chosen as the energy reference. Lines with different colors correspond to the relative energies of different phases: α, black; β, red; γ, blue; δ, dark cyan; ε, magenta; ζ, dark gray.
    Changlin Yan, Cong Wang, Linwei Zhou, Pengjie Guo, Kai Liu, Zhong-Yi Lu, Zhihai Cheng, Yang Chai, Anlian Pan, Wei Ji. Two ultra-stable novel allotropes of tellurium few-layers[J]. Chinese Physics B, 2020, 29(9):
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