Abstract
We study collective and single-particle intersubband excitations in a system of quantum wires coupled via weak tunneling. For an isolated wire with parabolic confinement, Kohn’s theorem guarantees that the absorption spectrum represents a single sharp peak centered at the frequency given by the bare confining potential. We show that the effect of weak tunneling between two parabolic quantum wires is twofold: (i) additional peaks corresponding to single-particle excitations appear in the absorption spectrum, and (ii) the main absorption peak acquires a depolarization shift. We also show that the interplay between tunneling and weak perpendicular magnetic field drastically enhances the dispersion of single-particle excitations. The latter leads to a strong damping of the intersubband plasmon for magnetic fields exceeding a critical value. The results are obtained within a random-phase approximation for the total potential and at low electron concentration, where the screening effects are treated perturbatively. © 1996 The American Physical Society.
- Received 4 June 1996
DOI:https://doi.org/10.1103/PhysRevB.54.16749
©1996 American Physical Society