Stress effects on shallow-donor impurity states in symmetrical GaAs/AlxGa1_xAs double quantum wells

ABSTRACT: The effects of the compressive stress on the binding energy and the density of shallow-donor impurity states in symmetrical GaAs/AlxGa12xAs double quantum wells are calculated using a variational procedure within the effective-mass approximation. Results are for different well and barrier...

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Autores:
Raigoza Bohórquez, Nicolás Fernando
Morales Aramburo, Álvaro Luis
Montes Barahona, Augusto León
Porras Montenegro, Nelson
Duque Echeverri, Carlos Alberto
Tipo de recurso:
Article of investigation
Fecha de publicación:
2004
Institución:
Universidad de Antioquia
Repositorio:
Repositorio UdeA
Idioma:
eng
OAI Identifier:
oai:bibliotecadigital.udea.edu.co:10495/8387
Acceso en línea:
http://hdl.handle.net/10495/8387
Palabra clave:
Efectos de estrés
Estados de impurezas
Pozos cuánticos
Rights
openAccess
License
Atribución-NoComercial-SinDerivadas 2.5 Colombia
Description
Summary:ABSTRACT: The effects of the compressive stress on the binding energy and the density of shallow-donor impurity states in symmetrical GaAs/AlxGa12xAs double quantum wells are calculated using a variational procedure within the effective-mass approximation. Results are for different well and barrier widths, shallow-donor impurity position, and compressive stress along the growth direction of the structure. We have found that independently of the well and barrier widths, for stress values up to 13.5 kbar ~in the direct-gap regime! the binding energy increases linearly with the stress. For stress values greater than 13.5 kbar ~indirect gap regime! and for impurities at the center of the wells, the binding energy increases up to a maximum and then decreases. For all impurity positions the binding energy shows a nonlinear behavior in the indirect gap regime due to the G-X crossing effect. The density of impurity states is calculated for a homogeneous distribution of donor impurities within the barriers and the wells of the low-dimensional heterostructures. We have found that there are three special structures in the density of impurity states: one associated with on-center-barrier-, the second one associated with on-center-well-, and the third one corresponding to on-external-edge-well-impurity positions. The three structures in the density of impurity states must be observed in valence–to–donor-related absorption and conduction–to–donor-related photoluminescence spectra, and consequently these peaks can be tuned at specific energies and convert the system in a stress detector.