30-band k·p model of electron and hole states in silicon quantum wells

Nemanja A. Čukarić, Milan Ž. Tadić, Bart Partoens, and F. M. Peeters
Phys. Rev. B 88, 205306 – Published 19 November 2013

Abstract

We modeled the electron and hole states in Si/SiO2 quantum wells within a basis of standing waves using the 30-band k·p theory. The hard-wall confinement potential is assumed, and the influence of the peculiar band structure of bulk silicon on the quantum-well sub-bands is explored. Numerous spurious solutions in the conduction-band and valence-band energy spectra are found and are identified to be of two types: (1) spurious states which have large contributions of the bulk solutions with large wave vectors (the high-k spurious solutions) and (2) states which originate mainly from the spurious valley outside the Brillouin zone (the extravalley spurious solutions). An algorithm to remove all those nonphysical solutions from the electron and hole energy spectra is proposed. Furthermore, slow and oscillatory convergence of the hole energy levels with the number of basis functions is found and is explained by the peculiar band mixing and the confinement in the considered quantum well. We discovered that assuming the hard-wall potential leads to numerical instability of the hole states computation. Nonetheless, allowing the envelope functions to exponentially decay in a barrier of finite height is found to improve the accuracy of the computed hole states.

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  • Received 13 May 2013

DOI:https://doi.org/10.1103/PhysRevB.88.205306

©2013 American Physical Society

Authors & Affiliations

Nemanja A. Čukarić1,2,*, Milan Ž. Tadić1,†, Bart Partoens2,‡, and F. M. Peeters2,§

  • 1School of Electrical Engineering, University of Belgrade, P.O. Box 35-54, 11120 Belgrade, Serbia
  • 2Department of Physics, University of Antwerp, Groenenborgerlaan 171, B-2020 Antwerp, Belgium

  • *nemanja.cukaric@etf.bg.ac.rs
  • milan.tadic@etf.bg.ac.rs
  • bart.partoens@ua.ac.be
  • §francois.peeters@ua.ac.be

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Vol. 88, Iss. 20 — 15 November 2013

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