Abstract
Theoretical calculations of the electronic properties of n-type HgTe/CdTe superlattices (SLs) have provided an agreement with the experimental data on the magneto-transport behaviour. We have measured the conductivity, Hall mobility, Seebeck and Shubnikov-de Haas effects and angular dependence of the magneto-resistance. Our sample, grown by MBE, had a period d=d 1+d 2 (124 layers) of \(d_{1}=8.6~\mathrm{nm}~\mathrm{(HgTe)} /d_{2}=3.2~\mathrm{nm}~\mathrm{(CdTe)}\). Calculations of the spectras of energy E(d 2), E(k z ) and E(k p ), respectively, in the direction of growth and in plane of the superlattice; were performed in the envelope function formalism. The energy E(d 2,Γ,4.2 K), shown that when d 2 increase the gap E g decrease to zero at the transition semiconductor to semimetal conductivity behaviour and become negative accusing a semimetallic conduction. At 4.2 K, the sample exhibits n type conductivity, confirmed by Hall and Seebeck effects, with a Hall mobility of \(2.5 \times 10^{5}~\mathrm{cm}^{2}/ \mathrm{V\,s}\). This allowed us to observe the Shubnikov-de Haas effect with n=3.20×1012 cm−2. Using the calculated effective mass (\(m^{*}_{E1}(E_{F}) = 0.05 m_{0}\)) of the degenerated electrons gas, the Fermi energy (2D) was E F =88 meV in agreement with 91 meV of thermoelectric power α. In intrinsic regime, α∼T −3/2 and R H T 3/2 indicates a gap E g =E 1−HH 1=101 meV in agreement with calculated E g (Γ,300 K)=105 meV. The formalism used here predicts that the system is semiconductor for d 1/d 2=2.69 and d 2<100 nm. Here, d 2=3.2 nm and E g (Γ,4.2 K)=48 meV so this sample is a two-dimensional modulated nano-semiconductor and far-infrared detector (12 μm<λ c <28 μm).
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Braigue, M., Nafidi, A., Idbaha, A. et al. Correlation Between Band Structure and Magneto- Transport Properties in HgTe/CdTe Two-Dimensional Far-Infrared Detector Superlattice. J Low Temp Phys 171, 808–817 (2013). https://doi.org/10.1007/s10909-012-0818-x
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DOI: https://doi.org/10.1007/s10909-012-0818-x