AVS 63rd International Symposium & Exhibition | |
Electronic Materials and Photonics | Thursday Sessions |
Session EM-ThP |
Session: | EMPD Poster Session |
Presenter: | Indika Senevirathna, Georgia State University |
Authors: | I. Senevirathna, Georgia State University D. Seidlitz, Georgia State University A. Fali, Georgia State University Y. Abate, Georgia State University N. Dietz, Georgia State University |
Correspondent: | Click to Email |
Fabrication of high quality Indium rich- In1-xGaxN layers is still a challenge due to the immiscibility between the binaries InN and GaN. The lack of lattice-matched substrate is an additional challenge for the growth of In1-xGaxN layers. The lattice mismatch between the substrate template and the In1-xGaxN layer generate residual strains and threading dislocations at the interface that propagate into the In1-xGaxN layers, and consequently, degrade the quality of the In1-xGaxN epilayer. To mitigate these effects, different approaches such as the use of buffer layers (e.g. GaN, InN, AlN) between the In1-xGaxN layers are explored.
In this contribution, we present our findings on the effects of substrate treatments on the structural and optoelectronic properties of In1-xGaxN layers grown by Migration-Enhanced, Plasma-Assisted MOCVD (MEPA-MOCVD). Furthermore, the analysis consist the data for In1-xGaxN layers grown on different nitrided sapphire substrates as well as layers grown on sapphire substrates templates, containing InN, GaN or AlN interlayers.
The optoelectronic properties – e.g. free carrier concentration, the mobility of the carriers, high-frequency dielectric constant ε∞, and layer thickness in the In1-xGaxN layers have been analyzed by simulating the reflectance spectra, obtained via Fourier Transform Infra-red (FTIR) spectroscopy, using a multilayer stack model and a dielectric function based on Lorentz-Drude model. AFM topography has been used to study the surface morphology of the layers. Raman spectroscopy has been utilized to analyze the local crystallinity (E2(high) mode) of the In1-xGaxN layers as well as the composition via the shift of the A1(LO) mode and its broadening with In1-xGaxN target composition.