Journal
MATERIALS
Volume 16, Issue 5, Pages -Publisher
MDPI
DOI: 10.3390/ma16052016
Keywords
ammonothermal; gallium nitride; crystal growth; numerical simulation; computational fluid dynamics; natural convection; buoyancy; conjugated heat transfer; solvothermal; hydrothermal
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The ammonothermal method is investigated as a promising technology for scalable production of GaN single crystals. The study focuses on the etch-back and growth conditions, as well as the transition between them. Numerical and experimental analyses show temperature differences and fluctuations during the transition, which affect the deposition of GaN on the crystals. The results provide insights into the crystal growth process and the optimization of production conditions.
With the ammonothermal method, one of the most promising technologies for scalable, cost-effective production of bulk single crystals of the wide bandgap semiconductor GaN is investigated. Specifically, etch-back and growth conditions, as well as the transition from the former to the latter, are studied using a 2D axis symmetrical numerical model. In addition, experimental crystal growth results are analyzed in terms of etch-back and crystal growth rates as a function of vertical seed position. The numerical results of internal process conditions are discussed. Variations along the vertical axis of the autoclave are analyzed using both numerical and experimental data. During the transition from quasi-stable conditions of the dissolution stage (etch-back process) to quasi-stable conditions of the growth stage, significant temperature differences of 20 K to 70 K (depending on vertical position) occur temporarily between the crystals and the surrounding fluid. These lead to maximum rates of seed temperature change of 2.5 K/min to 1.2 K/min depending on vertical position. Based on temperature differences between seeds, fluid, and autoclave wall upon the end of the set temperature inversion process, deposition of GaN is expected to be favored on the bottom seed. The temporarily observed differences between the mean temperature of each crystal and its fluid surrounding diminish about 2 h after reaching constant set temperatures imposed at the outer autoclave wall, whereas approximately quasi-stable conditions are reached about 3 h after reaching constant set temperatures. Short-term fluctuations in temperature are mostly due to fluctuations in velocity magnitude, usually with only minor variations in the flow direction.
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