Apr 9, 2025
5:00pm - 7:00pm
Summit, Level 2, Flex Hall C
Steve Park1,Yuxing Liang1,Jingyu Tang1,Abhishek Pathak1,Lisa Porter1,Jonathan Malen1
Carnegie Mellon Unversity1
Steve Park1,Yuxing Liang1,Jingyu Tang1,Abhishek Pathak1,Lisa Porter1,Jonathan Malen1
Carnegie Mellon Unversity1
β-Ga
2O
3 is a promising ultra-wide bandgap semiconductor with the potential to provide significant improvements in the performance and the manufacturing cost of power electronic devices. An unexpected γ-phase inclusion as a defect has been reported when β-Ga
2O
3 was doped or alloyed. Because thermal transport in γ-Ga
2O
3 has not been studied, the effect of the γ-phase inclusion on the thermal conductivity of β-Ga
2O
3 is still in question. γ-Ga
2O
3 also has a potential to be used as an efficient catalyst due to its porous structure and high surface area, and thermal conductivity of the catalyst is an important attribute for an effective thermal management. The thermal conductivities of (100) γ-Ga
2O
3 films deposited on (100) MgAl
2O
4 substrates with various thicknesses were measured using frequency-domain thermoreflectance (FDTR). A multi-fit iteration algorithm was implemented to simultaneously extract thermal conductivities and thermal boundary conductances from these measurements. Measured thermal conductivities of γ-Ga
2O
3 are comparable to thermal conductivity of (-201) β-Ga
2O
3, which suggests that the γ-phase inclusion in the doped or alloyed β-phase will not adversely affect its thermal conductivity. The thermal conductivity of γ-Ga
2O
3 increases from 2.3 (+0.9, −0.5) W/mK to 3.5 ± 0.7 W/mK over films from 75 nm to 404 nm in thickness, which demonstrates a prominent size effect on thermal conductivity. The thermal conductivity of γ-Ga
2O
3 also shows a slight increase as temperature increases from 293 K to 400 K. This increasing trend in thermal conductivity can occur due to defect scattering dominating Umklapp scattering in this temperature range. γ-Ga
2O
3 has a cation-defective spinel structure with at least two gallium vacancies in every unit cell, which causes defect scattering to dominate Umklapp scattering at these temperatures.