Effect of spin-orbit interaction on the plasma excitations in a quantum wire

Godfrey Gumbs
Phys. Rev. B 70, 235314 – Published 10 December 2004

Abstract

Incorporating the spin-orbit interaction into the Hamiltonian of a quantum wire, we have calculated the plasma excitation energies. We include both the Rashba term (α coupling) arising from the asymmetry of the heterostructure forming the two-dimensional electron gas, and the β coupling due to the quantum wire confinement which we model with a harmonic potential. The α coupling lifts the degeneracy of the spin states and the β coupling causes the quantized transverse single-particle energy to have negative dispersion. Our model yields several interesting features which may be observed with the use of inelastic light scattering and electron energy loss spectroscopy (EELS). The collective excitations for the quantum wire are determined by the allowed transitions between subbands. The collective plasma excitations split off from each branch of allowed particle-hole modes. The subband structure gives rise to a plasmon mode with a negative group velocity.

  • Figure
  • Figure
  • Figure
  • Figure
  • Received 29 June 2004

DOI:https://doi.org/10.1103/PhysRevB.70.235314

©2004 American Physical Society

Authors & Affiliations

Godfrey Gumbs

  • Department of Physics and Astronomy, Hunter College of the City University of New York, 695 Park Avenue, New York, New York 10021, USA

Comments & Replies

Article Text (Subscription Required)

Click to Expand

References (Subscription Required)

Click to Expand
Issue

Vol. 70, Iss. 23 — 15 December 2004

Reuse & Permissions
Access Options
Author publication services for translation and copyediting assistance advertisement

Authorization Required


×
×

Images

×

Sign up to receive regular email alerts from Physical Review B

Log In

Cancel
×

Search


Article Lookup

Paste a citation or DOI

Enter a citation
×