Ahmad Ashfaq, Strak Pawel, Koronski Kamil, Kempisty Pawel, Sakowski Konrad, Piechota Jacek, Grzegory Izabella, Wierzbicka Aleksandra, Kryvyi Serhii, Monroy Eva, Kaminska Agata, Krukowski Stanislaw
Institute of High Pressure Physics, Polish Academy of Sciences, Sokolowska 29/37, 01-142 Warsaw, Poland.
Institute of Physics, Polish Academy of Sciences, Aleja Lotnikow 32/46, 02-668 Warsaw, Poland.
Materials (Basel). 2021 Aug 30;14(17):4935. doi: 10.3390/ma14174935.
In this paper, ab initio calculations are used to determine polarization difference in zinc blende (ZB), hexagonal (H) and wurtzite (WZ) AlN-GaN and GaN-InN superlattices. It is shown that a polarization difference exists between WZ nitride compounds, while for H and ZB lattices the results are consistent with zero polarization difference. It is therefore proven that the difference in Berry phase spontaneous polarization for bulk nitrides (AlN, GaN and InN) obtained by Bernardini et al. and Dreyer et al. was not caused by the different reference phase. These models provided absolute values of the polarization that differed by more than one order of magnitude for the same material, but they provided similar polarization differences between binary compounds, which agree also with our ab initio calculations. In multi-quantum wells (MQWs), the electric fields are generated by the well-barrier polarization difference; hence, the calculated electric fields are similar for the three models, both for GaN/AlN and InN/GaN structures. Including piezoelectric effect, which can account for 50% of the total polarization difference, these theoretical data are in satisfactory agreement with photoluminescence measurements in GaN/AlN MQWs. Therefore, the three models considered above are equivalent in the treatment of III-nitride MQWs and can be equally used for the description of the electric properties of active layers in nitride-based optoelectronic devices.
在本文中,采用从头算计算来确定闪锌矿(ZB)、六方(H)和纤锌矿(WZ)结构的AlN - GaN以及GaN - InN超晶格中的极化差异。结果表明,WZ氮化物化合物之间存在极化差异,而对于H和ZB晶格,结果与零极化差异一致。因此证明,Bernardini等人和Dreyer等人获得的体氮化物(AlN、GaN和InN)的贝里相位自发极化差异并非由不同的参考相位引起。这些模型给出的同一材料的极化绝对值相差一个多数量级,但它们给出的二元化合物之间的极化差异相似,这也与我们的从头算计算结果相符。在多量子阱(MQW)中,电场由阱 - 势垒极化差异产生;因此,对于GaN/AlN和InN/GaN结构,三种模型计算出的电场相似。考虑到可占总极化差异50%的压电效应,这些理论数据与GaN/AlN MQW中的光致发光测量结果吻合良好。因此,上述三种模型在处理III族氮化物MQW时是等效的,可同等用于描述氮化物基光电器件有源层的电学性质。