材料科学
堆积
无定形固体
晶体结构
外延
格子(音乐)
凝聚态物理
带隙
结晶学
宽禁带半导体
工作(物理)
光电子学
Crystal(编程语言)
纳米
电子结构
产量(工程)
化学物理
纳米技术
分子动力学
氮化镓
电子能带结构
作者
Xin Chen,Xin Luo,Duo Wang,Xu Cheng,Peng Cui
摘要
In our recent experimental work [Luo et al., Appl. Phys. Lett. 125, 122109 (2024)], we observed that crystalline Si3N4 cap layers, a few nanometers thick, can form in situ on GaN surfaces. Compared with amorphous SiO2 and Al2O3 caps, these crystalline caps yield cleaner GaN/Si3N4 interfaces with fewer defects and improved device metrics. These observations motivate two questions: why does Si3N4 farther from the interface become amorphous as the cap thickens, and what is the actual crystal structure of the interfacial Si3N4? Prior work proposed a defect-wurtzite (DW) model constructed heuristically from β-Si3N4 and the AlGaN lattice constants, but it is significantly higher in energy than β-Si3N4 and disagrees with experiment in both interlayer spacings and electronic bandgap. Using a systematic structure search approach under in-plane lattice constraints commensurate with AlGaN, we identify a lower-energy configuration, denoted Lam-Si3N4, with quasi-two-dimensional (laminar) stacking normal to the interface. Under AlGaN-matched metrics, Lam-Si3N4 is about 60 meV/atom more stable than DW-Si3N4 and reproduces the experimentally observed interlayer spacings more closely. The substantial lattice mismatch explains amorphization when the crystalline cap grows far from the interface. Upon full relaxation, both DW- and Lam-Si3N4 exhibit wide ∼4 eV bandgaps. Under AlGaN constraints, the DW gap collapses to ∼1.88 eV, whereas Lam-Si3N4 maintains a larger ∼2.70 eV gap (for reference, PBE gaps: GaN 1.73 eV, AlN 4.05 eV). The wider gap and improved structural match of Lam-Si3N4 rationalize the superior capping performance and provide guidance for optimizing AlGaN/GaN device encapsulation.
科研通智能强力驱动
Strongly Powered by AbleSci AI