Abstract:
The band structure of mercury telluride (HgTe) nanoplatelets in the two-monolayer (2ML) limit was studied taking into account spin-orbit coupling and using various density functional theory (DFT) types. Single-layer (1ML) and two-layer (2ML) HgTe nanoplatelets in the sphalerite phase, as well as bulk HgTe, were considered. It was demonstrated that strong spin-orbit coupling, combined with two-dimensional quantum confinement, lead to significant changes in the electronic band structure of ultrathin two-dimensional (2D) HgTe nanoplatelets and the ordering of their boundary bands compared to a three-dimensional material. Calculations of band structure of 2D-nanoplatelets in ultrathin limit revealed a number of specific features: (i) the nature of band structure of 1ML HgTe (inverted/non-inverted band order) depends on the type of density functional used; (ii) the regular band structure of 1ML-HgTe has a non-inverted (normal) band order, and the nanoplate itself is a direct-gap semiconductor at the à point; (iii) the band structure of 2ML-HgTe has no forbidden band and has an inverted band order; (iv) the band structure of 2ML-HgTe near the Fermi level exhibits behavior characteristic of a type-II Weyl semimetal.
Keywords:mercury telluride, 2D-nanoplatelets, inverted band structure, type-II weyl semimetal.