• Journal of Semiconductors
  • Vol. 42, Issue 12, 122902 (2021)
Peng Teng1、2、3, Tong Zhou4, Yonghuan Wang2、3, Ke Zhao1, Xiegang Zhu2、3, and Xinchun Lai2
Author Affiliations
  • 1Southwest Jiaotong University, School of Physical Science and Technology, Chengdu 610031, China
  • 2Science and Technology on Surface Physics and Chemistry Laboratory, Jiangyou 621908, China
  • 3Institute of Materials, China Academy of Engineering Physics, Mianyang 621700, China
  • 4Beijing Institute for Advanced Study, National University of Defense Technology, Beijing 100020, China
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    DOI: 10.1088/1674-4926/42/12/122902 Cite this Article
    Peng Teng, Tong Zhou, Yonghuan Wang, Ke Zhao, Xiegang Zhu, Xinchun Lai. Electrical transport properties of cerium doped Bi2Te3 thin films grown by molecular beam epitaxy[J]. Journal of Semiconductors, 2021, 42(12): 122902 Copy Citation Text show less
    (Color online) (a) Schematic crystal structure of Bi2Te3. (b) XRD patterns of (CexBi1–x)2Te3 thin films (x = 0, 0.01, 0.02, 0.03, 0.04, 0.05).
    Fig. 1. (Color online) (a) Schematic crystal structure of Bi2Te3. (b) XRD patterns of (CexBi1–x)2Te3 thin films (x = 0, 0.01, 0.02, 0.03, 0.04, 0.05).
    (Color online) (a) Resistivity of (CexBi1–x)2Te3 samples at different temperatures. Curves have been shifted for better visibility. (b) Normalized resistivity of (CexBi1–x)2Te3 at 3.5–25 K. (Solid lines: fits to Eq. (1).) (c) Magnetoresistance of (CexBi1–x)2Te3 at 4 K. (d) Magnetoresistance of (Ce0.04Bi0.96)2Te3 at 4–14 K.
    Fig. 2. (Color online) (a) Resistivity of (CexBi1–x)2Te3 samples at different temperatures. Curves have been shifted for better visibility. (b) Normalized resistivity of (CexBi1–x)2Te3 at 3.5–25 K. (Solid lines: fits to Eq. (1).) (c) Magnetoresistance of (CexBi1–x)2Te3 at 4 K. (d) Magnetoresistance of (Ce0.04Bi0.96)2Te3 at 4–14 K.
    (Color online) (a) Magnetoconductance of samples with different dopant concentrations under different perpendicular magnetic field at 4 K (solid lines – fits to Eq. (3)). (b) Magnetoconductance of (Ce0.04Bi0.96)2Te3 under different perpendicular magnetic field at different temperatures (solid lines – fits to Eq. (3)). (c) The change of fitting parameters and α with different dopant concentration. (d) The change of fitting parameters and α of (Ce0.04Bi0.96)2Te3 and Bi2Te3 at different temperatures (solid line – fit to Eq. (5)).
    Fig. 3. (Color online) (a) Magnetoconductance of samples with different dopant concentrations under different perpendicular magnetic field at 4 K (solid lines – fits to Eq. (3)). (b) Magnetoconductance of (Ce0.04Bi0.96)2Te3 under different perpendicular magnetic field at different temperatures (solid lines – fits to Eq. (3)). (c) The change of fitting parameters and α with different dopant concentration. (d) The change of fitting parameters and α of (Ce0.04Bi0.96)2Te3 and Bi2Te3 at different temperatures (solid line – fit to Eq. (5)).
    Samplesρ0A (10–5) B (10–3)
    x = 0 0.930310.59
    x = 0.01 0.9459.391.607
    x = 0.02 0.97665.2583.193
    x = 0.03 0.98584.0533.62
    x = 0.04 0.99812.6334.632
    x = 0.05 1.0131.4397.004
    Table 1. Fitting results of the parameters in Eq. (1). All parameters are in corresponding SI units.
    (CexBi1–x)2Te3x = 0 x = 0.01 x = 0.02 x = 0.03 x = 0.04 x = 0.05
    at 4 K (nm) 258.7160.510796.385.373.9
    at 14 K (nm) 117.180.361.956.356.552.0
    at 4 K –1.027–1.079–0.704–0.708–0.709–0.809
    at 14 K –1.266–1.119–0.719–0.708–0.580–0.601
    m–0.633–0.5624–0.415–0.411–0.378–0.306
    Table 2. Parameters extracted by fitting magnetoconductance data with Eqs. (3) and (5). is the phase coherence length, α is the coefficient in HLN formula and m is the power factor in Eq. (5).
    Peng Teng, Tong Zhou, Yonghuan Wang, Ke Zhao, Xiegang Zhu, Xinchun Lai. Electrical transport properties of cerium doped Bi2Te3 thin films grown by molecular beam epitaxy[J]. Journal of Semiconductors, 2021, 42(12): 122902
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