https://doi.org/10.1140/epjb/e2002-00250-6
Electron energy state spin-splitting in 3D cylindrical semiconductor quantum dots
1
National Nano Device Laboratories, Hsinchu 300, Taiwan
2
Microelectronics and Information Systems Research Center, National Chiao Tung University, Hsinchu 300, Taiwan
3
Institute of Electronics, National Chiao Tung University, Hsinchu
300, Taiwan
4
Kiev Taras Shevchenko University, 01033, Kiev, Ukraine
Corresponding author: a ymli@cc.nctu.edu.tw
Received:
15
May
2001
Revised:
14
May
2002
Published online:
13
August
2002
In this article we study the impact of the spin-orbit interaction on the electron quantum confinement for narrow gap semiconductor quantum dots. The model formulation includes: (1) the effective one-band Hamiltonian approximation; (2) the position- and energy-dependent quasi-particle effective mass approximation; (3) the finite hard wall confinement potential; and (4) the spin-dependent Ben Daniel-Duke boundary conditions. The Hartree-Fock approximation is also utilized for evaluating the characteristics of a two-electron quantum dot system. In our calculation, we describe the spin-orbit interaction which comes from both the spin-dependent boundary conditions and the Rashba term (for two-electron quantum dot system). It can significantly modify the electron energy spectrum for InAs semiconductor quantum dots built in the GaAs matrix. The energy state spin-splitting is strongly dependent on the dot size and reaches an experimentally measurable magnitude for relatively small dots. In addition, we have found the Coulomb interaction and the spin-splitting are suppressed in quantum dots with small height.
PACS: 71.70.Ej – Spin-orbit coupling, Zeeman and Stark splitting, Jahn-Teller effect / 73.21.La – Quantum dots / 78.20.Bh – Theory, models, and numerical simulation / 85.35.Be – Quantum well devices (quantum dots, quantum wires, etc.)
© EDP Sciences, Società Italiana di Fisica, Springer-Verlag, 2002