Quantum Oscillations of Magnetoresistance in HgCdTe/HgTe/HgCdTe Heterostructures with Inverted Band Spectrum

The effects observed in the Shubnikov–de Haas oscillation regime in the HgCdTe/HgTe/HgCdTe heterostructure with a wide (20.3 nm) HgTe quantum well with an inverted band structure are discussed. In a topologically trivial 2D system, a π-shift of magnetooscillation phase is found. A thorough experimen...

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Published in:Physics of the solid state Vol. 64; no. 3; pp. 107 - 117
Main Authors: Bogoliubskii, A. S., Gudina, S. V., Neverov, V. N., Turutkin, K. V., Podgornykh, S. M., Shelushinina, N. G., Yakunin, M. V., Mikhailov, N. N., Dvoretsky, S. A.
Format: Journal Article
Language:English
Published: Moscow Pleiades Publishing 01-03-2022
Springer
Springer Nature B.V
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Summary:The effects observed in the Shubnikov–de Haas oscillation regime in the HgCdTe/HgTe/HgCdTe heterostructure with a wide (20.3 nm) HgTe quantum well with an inverted band structure are discussed. In a topologically trivial 2D system, a π-shift of magnetooscillation phase is found. A thorough experimental study and theoretical analysis of the data is presented to understand the physical causes of this anomalous phase shift. The effective electron mass m c / m 0 = (0.022 ± 0.002) obtained from the region of doubly degenerate magnetoresistance peaks is approximately half the theoretical estimates. In the region of stronger magnetic fields, for non-degenerate magnetoresistance peaks, we have m c / m 0 = (0.034 ± 0.003), which is in good agreement with both theoretical predictions and experimental results obtained from the analysis of activation conductivity in the quantum Hall effect regime. The reasons for this discrepancy are discussed.
ISSN:1063-7834
1090-6460
DOI:10.1134/S1063783422030027