Engineering topological phases in triple HgTe/CdTe quantum wells.

Autor: Ferreira GJ; Instituto de Física, Universidade Federal de Uberlândia, Uberlândia, MG, 38400-902, Brazil. gersonjferreira@ufu.br., Candido DR; Department of Physics and Astronomy, University of Iowa, Iowa City, IA, 52242, USA., Hernandez FGG; Instituto de Física, Universidade de São Paulo, São Paulo, SP, 05508-090, Brazil., Gusev GM; Instituto de Física, Universidade de São Paulo, São Paulo, SP, 05508-090, Brazil. gusev@if.usp.br., Olshanetsky EB; Institute of Semiconductor Physics, Novosibirsk, 630090, Russia., Mikhailov NN; Institute of Semiconductor Physics, Novosibirsk, 630090, Russia., Dvoretsky SA; Institute of Semiconductor Physics, Novosibirsk, 630090, Russia.
Jazyk: angličtina
Zdroj: Scientific reports [Sci Rep] 2022 Feb 16; Vol. 12 (1), pp. 2617. Date of Electronic Publication: 2022 Feb 16.
DOI: 10.1038/s41598-022-06431-0
Abstrakt: Quantum wells formed by layers of HgTe between Hg[Formula: see text]Cd[Formula: see text]Te barriers lead to two-dimensional (2D) topological insulators, as predicted by the BHZ model. Here, we theoretically and experimentally investigate the characteristics of triple HgTe quantum wells. We describe such heterostructure with a three dimensional [Formula: see text] Kane model, and use its eigenstates to derive an effective 2D Hamiltonian for the system. From these we obtain a phase diagram as a function of the well and barrier widths and we identify the different topological phases composed by zero, one, two, and three sets of edge states hybridized along the quantum wells. The phase transitions are characterized by a change of the spin Chern numbers and their corresponding band inversions. Complementary, transport measurements are experimentally investigated on a sample close to the transition line between the phases with one and two sets of edges states. Accordingly, for this sample we predict a gapless spectrum with low energy bulk conduction subbands given by one parabolic and one Dirac subband, and with edge states immersed in the bulk valence subbands. Consequently, we show that under these conditions, local and non-local transport measurements are inconclusive to characterize a sole edge state conductivity due to bulk conductivity. On the other hand, Shubnikov-de Haas (SdH) oscillations show an excellent agreement with our theory. Particularly, we show that the measured SdH oscillation frequencies agrees with our model and show clear signatures of the coexistence of a parabolic and Dirac subbands.
(© 2022. The Author(s).)
Databáze: MEDLINE
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