• Chinese Physics B
  • Vol. 29, Issue 9, (2020)
Long Lin1, Yi-Peng Guo1, Chao-Zheng He2、†, Hua-Long Tao3, Jing-Tao Huang1, Wei-Yang Yu4, Rui-Xin Chen1, Meng-Si Lou1, and Long-Bin Yan1
Author Affiliations
  • 1Cultivating Base for Key Laboratory of Environment-Friendly Inorganic Materials in Henan Province, School of Materials Science and Engineering, Henan Polytechnic University, Jiaozuo 454000, China
  • 2Institute of Environmental and Energy Catalysis, School of Materials Science and Chemical Engineering, Xi’an Technological University, Xi’an 71001, China
  • 3Liaoning Key Materials Laboratory for Railway, School of Materials Science and Engineering, Dalian Jiaotong University, Dalian 116028, China
  • 4School of Physics and Electronic Information Engineering, Henan Polytechnic University, Jiaozuo 5003, China
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    DOI: 10.1088/1674-1056/ab9741 Cite this Article
    Long Lin, Yi-Peng Guo, Chao-Zheng He, Hua-Long Tao, Jing-Tao Huang, Wei-Yang Yu, Rui-Xin Chen, Meng-Si Lou, Long-Bin Yan. First-principles study of magnetism of 3d transition metals and nitrogen co-doped monolayer MoS2[J]. Chinese Physics B, 2020, 29(9): Copy Citation Text show less
    Structure of the supercell used for the calculation, showing top view and side view of (a) intrinsic MoS2, (b) TM-MoS2, (c) (TM, N) co-doped MoS2 and (d) (2Fe, N) co-doped MoS2, respectively. Mo atoms replace Fe atoms, which is indicated by 1–9.
    Fig. 1. Structure of the supercell used for the calculation, showing top view and side view of (a) intrinsic MoS2, (b) TM-MoS2, (c) (TM, N) co-doped MoS2 and (d) (2Fe, N) co-doped MoS2, respectively. Mo atoms replace Fe atoms, which is indicated by 1–9.
    Band structure of intrinsic MoS2.
    Fig. 1. Band structure of intrinsic MoS2.
    TDOS and PDOS for (a) Fe, (b) Co, and (c) Ni-doped MoS2, calculated by using PBE functional, with Fermi level set to be 0 eV.
    Fig. 2. TDOS and PDOS for (a) Fe, (b) Co, and (c) Ni-doped MoS2, calculated by using PBE functional, with Fermi level set to be 0 eV.
    Band structure for (a) Fe, (b) Co, (c) Ni-doped MoS2.
    Fig. 2. Band structure for (a) Fe, (b) Co, (c) Ni-doped MoS2.
    TDOSs and PDOSs for (a) Fe–N, (b) Co–N, and (c) Ni–N co-doped monolayer MoS2, with Fermi level set to be 0 eV.
    Fig. 3. TDOSs and PDOSs for (a) Fe–N, (b) Co–N, and (c) Ni–N co-doped monolayer MoS2, with Fermi level set to be 0 eV.
    Band structure of (a) Fe–N, (b) Co–N, and (c) Ni–N co-doped MoS2.
    Fig. 3. Band structure of (a) Fe–N, (b) Co–N, and (c) Ni–N co-doped MoS2.
    Band structure of (2Fe, N) co-doped monolayer MoS2: (a) FM, (b) AFM, respectively.
    Fig. 4. Band structure of (2Fe, N) co-doped monolayer MoS2: (a) FM, (b) AFM, respectively.
    TDOSs and PDOSs for (2Fe, N) co-doped monolayer MoS2, with Fermi level set to be 0 eV.
    Fig. 4. TDOSs and PDOSs for (2Fe, N) co-doped monolayer MoS2, with Fermi level set to be 0 eV.
    Spin density distribution of (2Fe, N) co-doped MoS2 in FM coupling, with isovalue set to be 0.02 e/Å3.
    Fig. 5. Spin density distribution of (2Fe, N) co-doped MoS2 in FM coupling, with isovalue set to be 0.02 e/Å3.
    Dopant siteBond length/ÅMagnetic moments/μB
    dS – ModS – TMTotalSMoTM
    MoS22.4080.000.000.00
    Fe2.4122.2832.020.010.131.17
    Co2.4162.2932.930.040.300.86
    Ni2.3982.4054.050.290.161.11
    Table 1. Calculation results of intrinsic MoS2 and TM-doped MoS2, S–Mo, and S–TM bond lengths, and total magnetic moment, and magnetic moment of S, Mo, and TM atoms, respectively.
    Dopant sitedTM – NTotal/μBTM/μBEform/eV
    Mo-richS-rich
    Fe1.9651.000.642.64–0.06
    Co1.9751.980.733.911.21
    Ni1.9391.110.184.722.22
    Table 2. Calculation results of (TM, N) co-doped MoS2, TM–N bond length, total magnetic moment, the local magnetic moment of TM atom, and formation energy.
    Configurationd (Fe–Fe)/ÅΔE/eVΔEFM/meVMagnetic moment/μB
    (a, b)AFMFMTotalFe1Fe2NMoS
    (2, 4)3.2863.29442.53.261.771.77–0.03–0.01–0.06
    (1, 2)3.4283.425–0.482.23.001.961.74–0.09–0.100.00
    (2, 6)5.2555.2750.68–4.83.402.052.050.03–0.010.00
    (1, 5)5.4955.4870.14–29.13.021.871.80–0.060.38–0.05
    (3, 8)5.5355.5080.59–1.13.321.811.78–0.01–0.040.00
    (1, 3)6.2896.242–0.6864.23.471.851.85–0.030.040.00
    (3, 7)6.2536.2800.33–92.33.442.082.03–0.020.010.00
    (1, 9)10.92310.9180.38–14.83.051.841.85–0.080.000.00
    Table 3. Calculation results of 8 configurations for (2Fe, N) co-doped MoS2. Fe–Fe distance, Δ E, ΔEFM, total magnetic moment, and magnetic moment of Fe1, Fe2, N, Mo, and S atoms, respectively.
    Long Lin, Yi-Peng Guo, Chao-Zheng He, Hua-Long Tao, Jing-Tao Huang, Wei-Yang Yu, Rui-Xin Chen, Meng-Si Lou, Long-Bin Yan. First-principles study of magnetism of 3d transition metals and nitrogen co-doped monolayer MoS2[J]. Chinese Physics B, 2020, 29(9):
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