首页> 外文期刊>International journal of computational materials science and engineering >Structural, electronic and magnetic properties of S sites vacancy defects graphene/MoS_2 van der Waals heterostructures: First-principles study
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Structural, electronic and magnetic properties of S sites vacancy defects graphene/MoS_2 van der Waals heterostructures: First-principles study

机译:Structural, electronic and magnetic properties of S sites vacancy defects graphene/MoS_2 van der Waals heterostructures: First-principles study

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摘要

In this work, we investigated the geometrical structures, electronic and magnetic properties of S sites vacancy defects in heterostructure graphene/molybdenum disulphide ((HS)G/MoS_2) material by performing first-principles calculations based on spin polarized Density Functional Theory (DFT) method within van der Waals (vdW) corrections (DFT-D2) approach. All the structures are optimized and relaxed by BFGS method using computational tool Quantum ESPRESSO (QE) package. We found that both (HS)G/MoS_2 and S sites vacancy defects in (HS)G/MoS_2 (D1S-(HS)G/MoS_2, U1S-(HS)G/MoS_2, 2S-(HS)G/MoS_2 and 3S-(HS)G/MoS_2) are stable materials, and atoms in defects structures are more compact than in pristine (HS)G/MoS_2 structure. From band structure calculations, we found that (HS)G/MoS_2, (DlS-(HS)G/MoS_2, U1S-(HS)G/MoS_2, 2S-(HS)G/MoS_2 and 3S-(HS)G/MoS_2) materials have n-type Schottky contact. The Dirac cone is formed in conduction band of the materials mentioned above. The barrier height of Dirac cones from Fermi energy level of (HS)G/MoS_2, (D1S-(HS)G/MoS_2, U1S-(HS)G/MoS_2, 2S-(HS)G/MoS_2 and 3S-(HS)G/MoS_2) materials have values 0.56 eV, 0.62 eV, 0.62 eV, 0.64 eV and 0.65 eV, respectively, which means they have metallic properties. To study the magnetic properties of materials, we have carried out DoS and PDoS calculations. We found that (HS)G/MoS_2, D1S-(HS)G/MoS_2 and U1S-(HS)G/MoS_2 materials have non-magnetic properties, and 2S-(HS)G/MoS_2 and 3S-(HS)G/MoS_2 materials have magnetic properties. Therefore, the non-magnetic (HS)G/MoS_2 changes to magnetic 2S-(HS)G/MoS_2 and 3S-(HS)G/MoS_2 materials due to 2S and 3S atoms vacancy defects, respectively, in (HS)G/MoS_2 material. Magnetic moment obtained in 2S-(HS)G/MoS_2 and 3S-(HS)G/MoS_2 materials due to the unequal distribution of up and down spin states of electrons in 2s and 2p orbitals of C atoms; 4p, 4d and 5s orbitals of Mo atoms; and 3s and 3p orbitals of S atoms in structures. Magnetic moment of 2S-(HS)G/MoS_2 and 3S-(HS)G/MoS_2 materials is -0.11μ_B/cell and -0.29μ_B/cell, respectively, and spins of 2p orbital of C atoms, 3p orbital of S atoms and 4d orbital of Mo atoms have dominant role to create magnetism in 2S-(HS)G/MoS_2 and 3S-(HS)G/MoS_2 materials.

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