Multi-domain electromagnetic absorption of triangular quantum rings

TL;DR

This theoretical study explores how the geometric shape of triangular quantum rings influences their electronic spectra, localization, and optical absorption, revealing tunable properties for potential electromagnetic applications.

Contribution

It provides a detailed analysis of the dependence of energy levels and localization on geometric parameters and external magnetic fields in triangular quantum rings.

Findings

Energy levels form a shell localized at corners

Energy gap varies non-monotonically with thickness

Optical transitions can be tuned from THz to infrared

Abstract

We present a theoretical study of the unielectronic energy spectra, electron localization, and optical absorption of triangular core-shell quantum rings. We show how these properties depend on geometric details of the triangle, such as side thickness or corners' symmetry. For equilateral triangles, the lowest six energy states (including spin) are grouped in an energy shell, are localized only around corner areas, and are separated by a large energy gap from the states with higher energy which are localized on the sides of the triangle. The energy levels strongly depend on the aspect ratio of the triangle sides, i.e., thickness/length ratio, in such a way that the energy differences are not monotonous functions of this ratio. In particular, the energy gap between the group of states localized in corners and the states localized on the sides strongly decreases with increasing the side thickness, and then slightly increases for thicker samples. With increasing the thickness the low-energy shell remains distinct but the spatial distribution of these states spreads. The behavior of the energy levels and localization leads to a thickness dependent absorption spectrum where one transition may be tuned in the THz domain and a second transition can be tuned from THz to the infrared range of electromagnetic spectrum. We show how these features may be further controlled with an external magnetic field. In this work the electron-electron Coulomb repulsion is neglected.