INTERFACE ROUGHNESS AND HOMOGENEOUS LINEWIDTHS IN QUANTUM-WELLS AND SUPERLATTICES STUDIED BY RESONANT ACOUSTIC-PHONON RAMAN-SCATTERING

Citation
T. Ruf et al., INTERFACE ROUGHNESS AND HOMOGENEOUS LINEWIDTHS IN QUANTUM-WELLS AND SUPERLATTICES STUDIED BY RESONANT ACOUSTIC-PHONON RAMAN-SCATTERING, Physical review. B, Condensed matter, 50(3), 1994, pp. 1792-1806
Citations number
46
Categorie Soggetti
Physics, Condensed Matter
ISSN journal
01631829
Volume
50
Issue
3
Year of publication
1994
Pages
1792 - 1806
Database
ISI
SICI code
0163-1829(1994)50:3<1792:IRAHLI>2.0.ZU;2-Q
Abstract
Acoustic-phonon Raman spectra of GaAs/AlAs superlattices show two char acteristic features: Sharp lines originate in crystal-momentum conserv ing backscattering by folded superlattice phonons. A continuous emissi on background with superimposed peaks and dips is observed due to diso rder-induced scattering from modes of the whole folded acoustic-phonon dispersion. In this case, neither the crystal-momentum component q(z) along q(parallel-to) nor perpendicular to the growth direction is con served. Even in high-quality samples the amount of disorder is such th at both effects appear at the same time. These phenomena allow us to o btain information on growth-related and intrinsic parameters of semico nductor superlattices and multiple quantum wells. Gaps of the folded-p honon dispersion cause intensity anomalies in the background emission. From the ratio of such features at mini-Brillouin-zone boundary gaps, for which only q(z) is not conserved, to those at internal gaps, wher e both q(z) and q(parallel-to) can take arbitrary values, the degree o f interface roughness and the lateral extent of growth islands are ded uced. The resonance behavior of the continuous emission and relative c hanges of wave-vector conserving folded-phonon to background scatterin g intensities are analyzed in terms of homogeneous and inhomogeneous b roadenings of interband critical points. Changes of the homogeneous li newidth with energy and temperature, as well as electron-phonon intera ction constants, are determined.