Low-energy effective Hamiltonian and end states of an inverted HgTe nanowire

Fuente: arXiv
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Autor principal: Li, Rui
Formato: Preprint
Publicado: 2025
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author Li, Rui
author_facet Li, Rui
contents The band inversion transition in a cylindrical HgTe nanowire is inducible via varying the nanowire radius. Here we derive the low-energy effective Hamiltonian describing the band structure of the HgTe nanowire close to the fundamental band gap. Because both the $E_{1}$ and $H_{1}$ subbands have quadratic dependence on $k_{z}$ when the gap closes, we need to consider at least three subbands, i.e., the $E_{1}$, $H_{1}$, and $H_{2}$ subbands, in building the effective Hamiltonian. The resulting effective Hamiltonian is block diagonal and each block is a $3\times3$ matrix. End states are found in the inverted regime when we solve the effective Hamiltonian with open boundary condition.
format Preprint
id arxiv_https___arxiv_org_abs_2505_07478
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Low-energy effective Hamiltonian and end states of an inverted HgTe nanowire
Li, Rui
Mesoscale and Nanoscale Physics
The band inversion transition in a cylindrical HgTe nanowire is inducible via varying the nanowire radius. Here we derive the low-energy effective Hamiltonian describing the band structure of the HgTe nanowire close to the fundamental band gap. Because both the $E_{1}$ and $H_{1}$ subbands have quadratic dependence on $k_{z}$ when the gap closes, we need to consider at least three subbands, i.e., the $E_{1}$, $H_{1}$, and $H_{2}$ subbands, in building the effective Hamiltonian. The resulting effective Hamiltonian is block diagonal and each block is a $3\times3$ matrix. End states are found in the inverted regime when we solve the effective Hamiltonian with open boundary condition.
title Low-energy effective Hamiltonian and end states of an inverted HgTe nanowire
topic Mesoscale and Nanoscale Physics
url https://arxiv.org/abs/2505.07478