The Binding Energies of Shallow Donor Impurities in GaAs–(Ga,Al)As Coaxial Quantum-Well Wires
✍ Scribed by I.D. Mikhailov; R. Escorcia; J. Sierra-Ortega
- Publisher
- John Wiley and Sons
- Year
- 2000
- Tongue
- English
- Weight
- 83 KB
- Volume
- 220
- Category
- Article
- ISSN
- 0370-1972
No coin nor oath required. For personal study only.
✦ Synopsis
Within the effective-mass approximation a simple method to calculate the spectra of a shallowdonor impurity in GaAs±(Ga, Al)As cylindrical quantum-well wires (QWWs) suitable for any confinement potential shape in radial direction is proposed. A trial function is taken as the product of a hydrogenic part with two envelope functions: the ground state wave function of the uncoupled electron in quantum-well wire f k (r), and a variational function j(z) that describes the orbit confinement in axial direction. A Schro È dinger-type equation for j(z) corresponding to the best trial function is deduced. The method is applied to analyze the D 0 ground and first excited states in coaxial cylindrical QWWs. Two peaks in the curve of the 1s-like state binding energy vs. the QWW radius are found.
📜 SIMILAR VOLUMES
The binding energies of shallow hydrogenic donor impurities in GaAs±(Ga,Al)As quantum boxes are calculated as a function of the size of the structure and as a function of the intensity of an applied electric field. The calculations are performed within the effective-mass approximation and using a va
Using a variational approach within the effective mass approximation we calculate the binding energy of the ground and some excited donor impurity states in quantum-well wires with rectangular and cylindrical transversal sections under the action of applied electric fields. We study the binding ener
The binding energy of a donor impurity in a spherical GaAs±(Ga,Al)As quantum dot with parabolic confinement is calculated as a function of the radius of the quantum dot and as a function of the intensity of an applied electric field. Calculations are performed within the effective-mass approximation