Electronic and hyperbolic dielectric properties of ZrS2/HfS2 heterostructures
In this paper we investigate the electronic and optical dielectric properties of lateral and vertical heterostructures composed of two-dimensional (2D) ZrS2 and HfS2 monolayers based on density-functional theory. First, we show that the bulk and monolayer ZrS2 and HfS2 as well as the vertical (ZrS2)...
Gespeichert in:
Veröffentlicht in: | Physical review. B 2019-10, Vol.100 (16) |
---|---|
Hauptverfasser: | , , , , , , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | In this paper we investigate the electronic and optical dielectric properties of lateral and vertical heterostructures composed of two-dimensional (2D) ZrS2 and HfS2 monolayers based on density-functional theory. First, we show that the bulk and monolayer ZrS2 and HfS2 as well as the vertical (ZrS2)m/(HfS2)n heterostructures are indirect band-gap semiconductors, while the lateral heterostructures exhibit an indirect to direct band-gap transition. Then we demonstrate that the optical properties of the bulk and monolayer HfS2 and ZrS2 are strongly anisotropic; for the bulk HfS2 and ZrS2, the in-plane components of the dielectric function are negative in a certain frequency band, where they can work as naturally hyperbolic metamaterials. Interestingly, the vertical heterostructures also possess a hyperbolic region, whose position and width can be tunable with the thickness ratio of constituents. It is also found that the (ZrS2)/(HfS2) vertical heterostructures can enhance spontaneous emission and about 100-fold improvement of the Purcell factor is obtained. These results prove the feasibility of 2D material heterostructures to realize tunable hyperbolic metamaterials; the heterostructures present a promising opportunity for the practical applications in light-generation technologies. |
---|---|
ISSN: | 2469-9950 2469-9969 |
DOI: | 10.1103/PhysRevB.100.165304 |