Strak Pawel, Kempisty Pawel, Sakowski Konrad, Piechota Jacek, Grzegory Izabella, Monroy Eva, Kaminska Agata, Krukowski Stanislaw
Institute of High Pressure Physics, Polish Academy of Sciences, Sokolowska 29/37, 01-142 Warsaw, Poland.
Research Institute for Applied Mechanics, Kyushu University, Fukuoka 816-8580, Japan.
Materials (Basel). 2025 Mar 26;18(7):1489. doi: 10.3390/ma18071489.
In this study, the fundamental properties of spontaneous and piezo polarization and surface polarity were defined. It was demonstrated that the Landau definition of polarization as a dipole density could be used in infinite systems. Differences between bulk polarization and surface polarity were distinguished, thus creating a clear identification of both components. This identification is in agreement with numerous experimental data-red shift presence and absence for wurtzite and zinc blende multiquantum wells (MQWs), respectively. A local model of spontaneous polarization was created and used to calculate spontaneous polarization as electric dipole density. The proposed local model correctly predicted the c-axis spontaneous polarization values of nitride wurtzite semiconductors. In addition, the model's results are in accordance with a polarization equal to zero for the zinc blende lattice. The spontaneous polarization values obtained for all wurtzite III nitrides are in basic agreement with earlier calculations using the Berry phase. Ab initio calculations of wurtzite nitride superlattices in Heyd-Scuseria-Ernzerhof (HSE) approximation were performed to derive polarization-induced fields in coherently strained lattices, showing good agreement with the polarization values. Strained superlattice data were used to determine the piezoelectric parameters of wurtzite nitrides, obtaining values that are in basic agreement with earlier data. Zinc blende superlattices were also modeled using ab initio HSE calculations, showing results that are in agreement with the absence of polarization in all nitrides in zinc blende symmetry.
在本研究中,定义了自发极化、压电极化和表面极性的基本特性。结果表明,朗道将极化定义为偶极密度的方法可用于无限系统。区分了体极化和表面极性之间的差异,从而明确识别了这两个分量。这种识别与大量实验数据一致,纤锌矿和闪锌矿多量子阱(MQW)分别存在和不存在红移。创建了自发极化的局部模型,并用于将自发极化计算为电偶极密度。所提出的局部模型正确地预测了氮化物纤锌矿半导体的c轴自发极化值。此外,该模型的结果与闪锌矿晶格极化等于零的情况一致。所有纤锌矿III族氮化物获得的自发极化值与早期使用贝里相位的计算基本一致。对纤锌矿氮化物超晶格进行了海德-斯库塞里亚-厄恩泽霍夫(HSE)近似下的从头算,以推导相干应变晶格中的极化诱导场,结果与极化值吻合良好。利用应变超晶格数据确定纤锌矿氮化物的压电参数,得到的值与早期数据基本一致。还使用从头算HSE计算对闪锌矿超晶格进行了建模,结果表明与闪锌矿对称性的所有氮化物中不存在极化的情况一致。