• Acta Physica Sinica
  • Vol. 69, Issue 11, 117101-1 (2020)
Hao-Hao Ma*, Xian-Bin Zhang*, Xu-Yan Wei, and Jia-Meng Cao
Author Affiliations
  • School of Science, Xi’an University of Technology, Xi’an 710048, China
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    DOI: 10.7498/aps.69.20200080 Cite this Article
    Hao-Hao Ma, Xian-Bin Zhang, Xu-Yan Wei, Jia-Meng Cao. Theoretical study on Schottky regulation of WSe2/graphene heterostructure doped with nonmetallic elements [J]. Acta Physica Sinica, 2020, 69(11): 117101-1 Copy Citation Text show less
    Top views of monolayer WSe2 doping: (a) Top view of single layer WSe2 3 × 3 × 1 supercell boron doped; (b) top view of single layer WSe2 3 × 3 × 1 supercell carbon doped; (c) top view of single layer WSe2 3 × 3 × 1 supercell nitrogen doped; (d) top view of single layer WSe2 3 × 3 × 1 supercell oxygen doped.
    Fig. 1. Top views of monolayer WSe2 doping: (a) Top view of single layer WSe2 3 × 3 × 1 supercell boron doped; (b) top view of single layer WSe2 3 × 3 × 1 supercell carbon doped; (c) top view of single layer WSe2 3 × 3 × 1 supercell nitrogen doped; (d) top view of single layer WSe2 3 × 3 × 1 supercell oxygen doped.
    Energy band structures of (a) monolayer WSe2, (b) grapheme, and (c) WSe2/graphene heterostructure. The n-type (p-type) SBH are indicated between the Fermi level and the conduction band minimum (the valence band maximum) of the WSe2 layer. The Fermi level is set to zero and marked by red dotted lines.
    Fig. 2. Energy band structures of (a) monolayer WSe2, (b) grapheme, and (c) WSe2/graphene heterostructure. The n-type (p-type) SBH are indicated between the Fermi level and the conduction band minimum (the valence band maximum) of the WSe2 layer. The Fermi level is set to zero and marked by red dotted lines.
    Three-dimensional charge density difference plots of WSe2/graphene heterostructure: (a) Side view; (b) top view.
    Fig. 3. Three-dimensional charge density difference plots of WSe2/graphene heterostructure: (a) Side view; (b) top view.
    Calculated total density of states and the corresponding partial density of states of WSe2/graphene heterostructure.
    Fig. 4. Calculated total density of states and the corresponding partial density of states of WSe2/graphene heterostructure.
    Band structures: (a) W9Se17O1; (b) W9Se17N1; (c) W9Se17C1; (d) W9Se17B1.
    Fig. 5. Band structures: (a) W9Se17O1; (b) W9Se17N1; (c) W9Se17C1; (d) W9Se17B1.
    Band structures: (a) W9Se17O1/graphene; (b) W9Se17N1/graphen; (c) W9Se17C1/graphen; (d) W9Se17B1/graphen.
    Fig. 6. Band structures: (a) W9Se17O1/graphene; (b) W9Se17N1/graphen; (c) W9Se17C1/graphen; (d) W9Se17B1/graphen.
    a1/nm a2/nm σ/% Ef/eV Ecoh/eV·nm–2ΔEmismatch/eV·nm–2
    W9Se180.9900.9840.6250–1.791–1.690
    W9Se17O10.9790.9840.5000.373–3.000–6.896
    W9Se17N10.9830.9840.0200.732–1.992–7.022
    W9Se17C10.9870.9840.3042.650–1.905–6.923
    W9Se17B10.9890.9840.5865.430–2.662–6.500
    Table 1.

    Lattice mismatch rate, formation energy, cohesive energy, and lattice mismatch energy parameters of WSe2/graphene heterojunction doped with different nonmetallic elements.

    不同非金属元素掺杂WSe2/graphene异质结的晶格失配率、形成能、结合能、晶格失配能参数

    Hao-Hao Ma, Xian-Bin Zhang, Xu-Yan Wei, Jia-Meng Cao. Theoretical study on Schottky regulation of WSe2/graphene heterostructure doped with nonmetallic elements [J]. Acta Physica Sinica, 2020, 69(11): 117101-1
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