Cathodoluminescence imaging and spectroscopy of excited states in InAs self-assembled quantum dots

We have examined state filling and thermal activation of carriers in buried InAs self-assembled quantum dots sSAQDsd with excitation-dependent cathodoluminescence sCLd imaging and spectroscopy. The InAs SAQDs were formed during molecular-beam epitaxial growth of InAs on undoped planar GaAs s001d. The intensities of the groundand excited-state transitions were analyzed as a function of temperature and excitation density to study the thermal activation and reemission of carriers. The thermal activation energies associated with the thermal quenching of the luminescence were measured for groundand excited-state transitions of the SAQDs, as a function of excitation density. By comparing these activation energies with the groundand excited-state transition energies, we have considered various processes that describe the reemission of carriers. Thermal quenching of the intensity of the QD groundand first excited-state transitions at low excitations in the ,230–300-K temperature range is attributed to dissociation of excitons from the QD states into the InAs wetting layer. At high excitations, much lower activation energies of the ground and excited states are obtained, suggesting that thermal reemission of single holes from QD states into the GaAs matrix is responsible for the observed temperature dependence of the QD luminescence in the ,230–300-K temperature range. The dependence of the CL intensity of the ground-and first excited-state transition on excitation density was shown to be linear at all temperatures at low-excitation density. This result can be understood by considering that carriers escape and are recaptured as excitons or correlated electron–hole pairs. At sufficiently high excitations, state-filling and spatial smearing effects are observed together with a sublinear dependence of the CL intensity on excitation. Successive filling of the ground and excited states in adjacent groups of QDs that possess different size distributions is assumed to be the cause of the spatial smearing. © 2005 American Institute of Physics. fDOI: 10.1063/1.1935743g