Possible realization of hyperbolic plasmons in a few-layered rhenium disulfide
arXiv:2301.06521 · doi:10.3390/condmat10030040
Abstract
The in-plane structural anisotropy in low-symmetric layered compound rhenium disulfide () makes it a candidate to host and tune electromagnetic phenomena specific for anisotropic media. In particular, optical anisotropy may lead to the appearance of hyperbolic plasmons, a highly desired property in optoelectronics. The necessary condition is a strong anisotropy of the principal components of the dielectric function, such that at some frequency range, one component is negative and the other is positive, i.e., one component is metallic, and the other one is dielectric. Here, we study the effect of anisotropy in and show that it can be a natural material to host hyperbolic plasmons in the ultraviolet frequency range. The operating frequency range of the hyperbolic plasmons can be tuned with the number of layers.
7 pages, 15 figures
References in corpus (10)
- Infrared hyperbolic metasurface based on nanostructured van der Waals materials
- Hybrid waves localized at hyperbolic metasurfaces
- Van der Waals thin films of WTe2 for natural hyperbolic plasmonic surfaces
- QS: Quasiparticle Self consistent with ladder diagrams in
- Excitons in Bulk and Layered Chromium Tri-Halides: From Frenkel to the Wannier-Mott Limit
- Electronic Structure of Chromium Trihalides beyond Density Functional Theory
- Two-dimensional plasmonic polarons in n-doped monolayer MoS2
- Finite-temperature plasmons, damping and collective behavior for model
- Infrared Plasmons Propagate through a Hyperbolic Nodal Metal
- ZnPSe as ultrabright indirect bandgap system with microsecond excitonic lifetimes