Photomodulated reflectance of InxGa1-xAs/GaAs/AlAs microcavity vertical-cavity surface emitting laser structures: Monitoring higher-order quantum well transitions

Citation
Pj. Klar et al., Photomodulated reflectance of InxGa1-xAs/GaAs/AlAs microcavity vertical-cavity surface emitting laser structures: Monitoring higher-order quantum well transitions, PHYS REV B, 59(4), 1999, pp. 2902-2909
Citations number
22
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
PHYSICAL REVIEW B-CONDENSED MATTER
ISSN journal
01631829 → ACNP
Volume
59
Issue
4
Year of publication
1999
Pages
2902 - 2909
Database
ISI
SICI code
0163-1829(19990115)59:4<2902:PROIMV>2.0.ZU;2-E
Abstract
In the previous paper, a Line shape model was developed to describe photomo dulated reflectance (PR) spectra of vertical-cavity surface emitting laser (VCSEL) structures in the vicinity of the resonance between the cavity mode and ground-state quantum well (QW) exciton, in the weak cavity exciton cou pling regime. Here, this model is extended to cavity mode resonances with h igher-order QW transitions, both allowed and forbidden. In addition, the mo del's validity is further confirmed by demonstrating a way of obtaining "ps eudo-PR" spectra of the QW ground-state and higher-order transitions. These spectra are derived by monitoring changes in PR line shape, as the cavity mode energy is tuned through the QW transitions. These spectra are virtuall y free of VCSEL cavity effects, and represent plots of the energy dependenc e of the imaginary part of the modulated QW dielectric function, Delta epsi lon(2) The Delta epsilon(2) spectra can be fitted using conventional excito nic PR line shapes to extract the energies and linewidths of the ground-sta te and higher-order QW transitions. Examples are given for two LnGaAs/GaAs/ AlAs VCSEL structures. The results of this technique are confirmed by compa ring with those obtained in two other experimental approaches: (i) measurin g sets of complete PR spectra, at different positions on the sample, of the resonances between the cavity mode and various QW excitons, and fitting th ese with the new lint: shape model; (ii) measuring the PR spectrum of the e xposed QW after removal of the top Bragg stack by etching, and fitting in t he conventional way. All the results are found to be in good agreement both with each other and with the ground-state and higher-order QW transition e nergies calculated using a three-band k(.)p model. [S0163-1829(99)02004-4].