Journal of Semiconductors, Volume. 44, Issue 4, 042101(2023)

A family of flexible two-dimensional semiconductors: MgMX2Y6 (M = Ti/Zr/Hf; X = Si/Ge; Y = S/Se/Te)

Junhui Yuan1, Kanhao Xue1,2、*, Xiangshui Miao1,2, and Lei Ye1,2、**
Author Affiliations
  • 1School of Integrated Circuits, School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan 430074, China
  • 2Hubei Yangtze Memory Laboratories, Wuhan 430205, China
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    Figures & Tables(12)
    (Color online) (a) The top view and (b, c) side view of monolayer MgMX2Y6. (d) The corresponding first Brillouin zone of MgMX2Y6 monolayers.
    (Color online) Phonon dispersion of ML MgMX2Y6 and In2X2Y6.
    (Color online) AIMD simulation results of MgMX2Y6 MLs at 300 K.
    (Color online) Calculated cohesive energies of MgMX2Y6 and In2X2Y6 MLs.
    (Color online) Tensile stress σ, as a function of uniaxial strain, ε, along the (a) x- and (b) y-directions and (c) of biaxial strain, respectively, for ML MgMX2Y6 and In2X2Y6.
    (Color online) Projected electronic band structures of MgMX2Y6 MLs based on HSE06+SOC calculation.
    (Color online) Projected electronic band structures of In2X2Y6 MLs based on HSE06+SOC calculation.
    (Color online) The band edges of MgMX2Y6 and In2X2Y6 MLs. The vacuum level is set to zero. The work functions of Ag, Ti, Cu, Au and Pt have been marked in the figure.
    (Color online) Optical absorption coefficient of MgMX2Y6 and In2X2Y6 MLs based on HSE06+SOC calculations.
    • Table 0. Calculated elastic constant C11/C22/C12/C66 (N/m), axial Young’s modulus Y11/Y22 (N/m), Poisson’s ratio v11/v22, ultimate strength σ* (N/m), ultimate strain ε*, corresponding to the ultimate strength for x, y, and biaxial tensions of MgMX2Y6 and In2X2Y6 MLs.

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      Table 0. Calculated elastic constant C11/C22/C12/C66 (N/m), axial Young’s modulus Y11/Y22 (N/m), Poisson’s ratio v11/v22, ultimate strength σ* (N/m), ultimate strain ε*, corresponding to the ultimate strength for x, y, and biaxial tensions of MgMX2Y6 and In2X2Y6 MLs.

      MaterialC11/C22C12C66C112C122Y11/Y22v11/v22xyBiaxial
      σ*ε*σ*ε*σ*ε*
      MgTiSi2S671.8820.3525.764752.3166.120.285.670.144.770.118.950.17
      MgTiSi2Se659.6917.2721.213264.2554.690.294.930.163.700.106.230.12
      MgTiSi2Te645.5613.5116.031893.4141.560.304.160.202.530.084.830.12
      MgTiGe2S666.5519.8223.364036.0860.650.305.460.153.850.086.920.12
      MgTiGe2Se655.2716.5419.372781.0450.320.304.630.183.320.106.070.14
      MgTiGe2Te641.0911.1814.951563.4838.050.273.780.222.290.084.510.14
      MgZrSi2S665.2818.1723.563932.0660.230.285.830.173.760.106.900.12
      MgZrSi2Se655.8915.6320.132879.4351.520.285.080.193.130.095.700.11
      MgZrSi2Te643.5812.3415.621746.9740.090.284.230.232.330.084.380.11
      MgZrGe2S660.6617.3621.653378.0655.690.295.500.176.530.126.530.12
      MgZrGe2Se651.8014.8318.492463.4047.560.294.740.202.900.095.380.12
      MgZrGe2Te640.7611.5014.631529.2637.520.283.870.252.140.084.440.15
      MgHfSi2S673.0420.6826.184907.9867.190.286.420.174.470.127.530.11
      MgHfSi2Se660.6617.5521.553371.1755.580.295.980.113.630.105.540.19
      MgHfSi2Te645.5613.5116.031893.4141.560.304.560.222.520.094.630.11
      MgHfGe2S660.6617.3621.653378.0655.690.296.040.184.090.106.070.10
      MgHfGe2Se651.8014.8318.492463.4047.560.295.140.203.270.095.660.12
      MgHfGe2Te640.7611.5014.631529.2637.520.284.130.232.340.084.490.13
      In2Si2S673.2722.1925.544876.2766.550.304.350.114.170.116.890.14
      In2Si2Se662.4519.0321.713537.5056.650.303.780.113.280.115.810.14
      In2Si2Te50.1614.9917.592291.5945.690.303.050.112.200.094.630.13
      In2Ge2S668.5621.0123.774258.4662.110.314.220.104.020.126.970.15
      In2Ge2Se658.5618.0920.233101.5052.960.313.700.113.170.116.040.15
      In2Ge2Te647.1214.2816.422016.8842.800.303.030.122.100.094.610.14
    • Table 0. Bader charge analysis of MgMX2Y6 and In2X2Y6 MLs.

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      Table 0. Bader charge analysis of MgMX2Y6 and In2X2Y6 MLs.

      MaterialMg/InTi/Zr/HfSi/GeS/Se/TeMaterialMg/InTi/Zr/HfSi/GeS/Se/Te
      MgTiSi2S6+2+1.96+3.00−1.66MgHfSi2S6+2+3.98+2.98−1.99
      MgTiSi2Se6+2+2.04+2.96−1.66MgHfSi2Se6+2+3.76+2.94−1.94
      MgTiSi2Te6+2+1.98+0.65−0.88MgHfSi2Te6+2+2.88+0.74−1.06
      MgTiGe2S6+2+1.98+3.02−1.67MgHfGe2S6+2+3.98+2.98−1.99
      MgTiGe2Se6+2+1.72+2.97−1.61MgHfGe2Se6+2+3.96+2.96−1.98
      MgTiGe2Te6+2+1.58+0.46−0.75MgHfGe2Te6+2+2.88+0.50−0.98
      MgZrSi2S6+2+2.24+2.98−1.70In2Si2S6+3+3.00−2.00
      MgZrSi2Se6+2+2.06+2.95−1.66In2Si2Se6+3+2.97−1.99
      MgZrSi2Te6+2+1.78+0.75−0.88In2Si2Te6+3+0.54−1.18
      MgZrGe2S6+2+2.24+2.98−1.70In2Ge2S6+3+2.97−1.99
      MgZrGe2Se6+2+2.06+2.95−1.66In2Ge2Se6+3+2.97−1.99
      MgZrGe2Te6+2+1.84+0.51−0.81In2Ge2Te6+3+0.48−1.16
    • Table 0. Calculated lattice constant a/b (Å), bond length Mg (In)-Y/M-Y/X-X/X-Y (Å), buckling height d (Å), band gaps at HSE06+SOC ( EgHSE+SOC , eV) levels, the valence band maximum (VBM, eV) and conduce band minimum (CBM, eV) at HSE06+SOC level.

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      Table 0. Calculated lattice constant a/b (Å), bond length Mg (In)-Y/M-Y/X-X/X-Y (Å), buckling height d (Å), band gaps at HSE06+SOC ( EgHSE+SOC , eV) levels, the valence band maximum (VBM, eV) and conduce band minimum (CBM, eV) at HSE06+SOC level.

      Materiala/bMg/In-YM-YX-XX-YdVBMCBMEgHSE+SOC
      MgTiSi2S66.1472.6542.4902.2312.1443.16−6.74−4.961.783
      MgTiSi2Se66.4612.7982.6192.2542.2993.37−6.51−4.821.691
      MgTiSi2Te67.0153.0262.8252.2952.5303.63−5.56−4.551.011
      MgTiGe2S66.2692.6532.4872.3552.2573.15−6.61−4.961.654
      MgTiGe2Se66.5722.7982.6202.3852.4013.37−6.36−4.841.517
      MgTiGe2Te67.1073.0262.8252.4352.6173.64−5.47−4.600.870
      MgZrSi2S66.2502.6812.6072.2332.1493.26−6.83−4.532.307
      MgZrSi2Se66.5562.8202.7392.2612.3023.48−6.71−4.492.225
      MgZrSi2Te67.1023.0452.9472.3032.5303.74−5.69−4.381.314
      MgZrGe2S­66.3722.6782.6082.3542.2613.26−6.78−4.692.084
      MgZrGe2Se66.6622.8182.7402.3882.4023.49−6.48−4.581.905
      MgZrGe2Te67.1873.0422.9462.4402.6163.76−5.52−4.441.074
      MgHfSi2S66.2182.6752.5802.2282.1513.25−6.92−4.422.500
      MgHfSi2Se66.5302.8152.7112.2562.3033.46−6.69−4.302.398
      MgHfSi2Te67.0843.0412.9192.3002.5323.72−5.64−4.181.456
      MgHfGe2S66.3412.6742.5802.3482.2623.25−6.83−4.602.232
      MgHfGe2Se66.6382.8152.7112.3832.4043.46−6.47−4.432.045
      MgHfGe2Te67.1723.0412.9172.4362.6183.73−5.58−4.391.189
      In2Si2S66.2782.7062.2702.1503.41−6.92−4.212.704
      In2Si2Se66.6002.8352.2942.3033.59−6.44−4.252.185
      In2Si2Te67.1533.0442.3292.5333.83−5.54−4.281.261
      In2Ge2S66.3852.7082.3752.2593.43−6.93−4.472.459
      In2Ge2Se66.6962.8362.4092.4013.61−6.44−4.491.952
      In2Ge2Te67.2343.0432.4572.6163.85−5.48−4.261.220
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    Junhui Yuan, Kanhao Xue, Xiangshui Miao, Lei Ye. A family of flexible two-dimensional semiconductors: MgMX2Y6 (M = Ti/Zr/Hf; X = Si/Ge; Y = S/Se/Te)[J]. Journal of Semiconductors, 2023, 44(4): 042101

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    Paper Information

    Category: Articles

    Received: Nov. 1, 2022

    Accepted: --

    Published Online: Apr. 24, 2023

    The Author Email: Xue Kanhao (xkh@hust.edu.cn), Ye Lei (leiye@hust.edu.cn)

    DOI:10.1088/1674-4926/44/4/042101

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