Band-gap energies, free carrier effects, and phonon modes in strained GaNAs/GaAs and GaNAs/InAs/GaAs superlattice heterostructures measured by spectroscopic ellipsometry

Spectroscopic ellipsometry (SE) is employed to study the optical properties of compressively strained short-period GaAs/InAs/GaNxAs1-x (0% < x < 2.4%) superlattice (SL) heterostructures for photon energies from 0.75 to 1.55 e V (NIR-SE), and for wave numbers from 250 to 700 cm(-1) (IR-SE). The undope d SL structures were grown on top of undoped GaAs buffer layers deposited o n Te-doped (001) GaAs substrates by metalorganic vapor phase epitaxy (MOVPE ). The InAs sequences consist of single monolayers. Structure, composition, layer thicknesses, and parallel and perpendicular lattice mismatch of the samples are studied by high-resolution transmission electron microscopy and high-resolution x-ray diffraction investigations. We employ Adachi's criti cal-point composite model for data analysis in the near-band-gap spectral r egion (NIR-SE). For analysis of the IR-SE data we use the harmonic oscillat or dielectric function model and the Drude model for free-carrier response. We report the direct band-gap energy E-0, and the complex index of refract ion N = n + ik of the (InAs)/GaNxAs1-x sublayers. We observe the well-known strong redshift of E-0 with increase in x, and the strong decrease of the E-0 transition amplitude. The E-0 values obtained for the SL structures are in good agreement with photoluminescence results. We observe no influence of the InAs monolayer on the spectral position of the fundamental GaNxAs1-x band-to-band transition E-0. We detect the transverse-optic (TO) lattice r esonance mode of the GaN sublattice at 470 cm(-1) within the (InAs)/GaNxAs1 -x SL sublayers. The polar strength of the GaN TO mode increases linearly w ith x. The same techniques were used previously to study tensile strained G aAs/GaNxAs1-x (0% < x < 3.3%) SL heterostructures grown by MOVPE. The depen dencies of n and k and E-0 [Appl. Phys. Lett. 76, 2859 (2000)], and the amp litude of the GaN TO modes [MRS Internet J. Nitride Semicond. Res. 5, 3 (20 00)] on the nitrogen concentration x for tensile strained GaAs/GaNxAs1-x SL s are compared to the results for compressively strained GaAs/InAs/GaNxAs1- x SLs obtained here. We find similar redshift and bowing parameters for E-0 , but different slopes for the amplitudes of the GaN TO mode. The different slopes are due to the different strain states. From there we calculate the strength of the GaN TO amplitude versus x for strain-compensated InAs/GaNx As1-x SLs, and the GaN TO mode amplitude can be used to monitor strain or c oncentration. We further obtain that the InAs monolayer effectively suppres ses the effects of free carriers in the GaNxAs1-x sublayers. Absorption by free carriers was observed previously within the tensile strained GaNxAs1-x /GaAs SL heterostructures. This can be explained by the predicted electroni c properties of the InAs monolayer, which can effectively bind free holes a nd free electrons due to folding of the InAs bands along the growth directi on [R. C. Iotti, L. C. Andreani, and M. Di Ventra, Phys. Rev. B 57, R15072 (1998)]. The improvement of the morphology of InAs/GaNxAs1-x sublayers is r eflected by the decrease of all broadening parameters within both NIR and I R dielectric function models used here, as well as by the occurrence of roo m-temperature photoluminescence emission. We also discuss IR resonance feat ures due to transverse-magnetic interface modes observed between the Te-dop ed GaAs and the undoped GaAs buffer layer. We find that these TM interface modes are extremely sensitive to the existe nce of free carriers within the SL structures. (C) 2001 American Institute of Physics.