Abstract
III‐nitride heteroepitaxial thin films and heterostructures suffer from the presence of large densities of structural defects, which are detrimental for the development of efficient devices. These defects result from differences between III‐nitride films and foreign substrates (structure, chemistry, lattice parameters). Transmission electron microscopy (TEM) is the technique of choice for studying such crystalline defects. The understanding of the origin and behavior of structural defects may allow their tailoring and the development of low defect density materials. III‐nitrides are classically grown along the polar c‐direction. In this case, internal electric fields play a major role in the properties of heterostructures. In order to eliminate or at least to reduce the influence of internal electric fields, growth along alternative directions with the c‐direction in the growth plane (nonpolar) or inclined to it (semipolar) have been developed. Heteroepitaxial nonpolar and semipolar films contain large densities of basal plane stacking faults (BSF) and related partial dislocations together with prismatic stacking faults. In this presentation, results of TEM studies of semipolar GaN films deposited on patterned substrates will be presented. Different TEM techniques from diffraction contrast classical imaging, high resolution TEM and scanning TEM to analytical techniques as energy dispersive X‐ray spectroscopy (EDS) have been employed to obtain a complete view of semipolar GaN microstructures. The understanding of the nucleation and propagation of defects allowed us to develop several growth processes resulting in a drastic reduction of the defect density: A 3‐step growth process for (11‐22) GaN deposited on patterned r‐sapphire leads to high quality GaN films with dislocation densities as low as 7x10 7 cm ‐2 and BSF densities below 10 2 cm ‐1 (figure 1) 1,2 . A method based on the introduction of Si at an intermediate stage of the growth (before coalescence of nucleation islands) allows, in the case of (10‐11) GaN on patterned (001) 7° off‐axis Si, blocking the propagation of dislocations (figure 2). A 4nm thick Si‐rich (5% Si from EDS analysis) layer is revealed by HRSTEM (figure 3). This layer has the wurtzite structure of the surrounding GaN and does not introduce significant strain (as revealed by GPA analysis). Selective growth on deeply grooved sapphire substrate results in GaN (11‐22) bands with a dislocation density in the mid 10 6 cm ‐2 on 100µm‐wide regions compatible with the fabrication of laser diodes. Besides presenting results on the improvement of material quality through innovative growth processes, this presentation emphasizes the importance of TEM studies for the developments of heteroepitaxial semiconductors structures.
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