纤锌矿晶体结构
哈密顿量(控制论)
凝聚态物理
电子能带结构
带隙
密度泛函理论
导带
物理
氮化物
直接和间接带隙
局部密度近似
价带
材料科学
电子结构
量子力学
数学
纳米技术
衍射
图层(电子)
电子
数学优化
作者
Patrick Rinke,M. Winkelnkemper,A. Qteish,D. Bimberg,Jörg Neugebauer,Matthias Scheffler
标识
DOI:10.1103/physrevb.77.075202
摘要
We have derived consistent sets of band parameters (band gaps, crystal field splittings, band-gap deformation potentials, effective masses, and Luttinger and ${E}_{P}$ parameters) for AlN, GaN, and InN in the zinc-blende and wurtzite phases employing many-body perturbation theory in the ${G}_{0}{W}_{0}$ approximation. The ${G}_{0}{W}_{0}$ method has been combined with density-functional theory (DFT) calculations in the exact-exchange optimized effective potential approach to overcome the limitations of local-density or gradient-corrected DFT functionals. The band structures in the vicinity of the $\ensuremath{\Gamma}$ point have been used to directly parametrize a $4\ifmmode\times\else\texttimes\fi{}4$ $\mathbf{k}\ensuremath{\cdot}\mathbf{p}$ Hamiltonian to capture nonparabolicities in the conduction bands and the more complex valence-band structure of the wurtzite phases. We demonstrate that the band parameters derived in this fashion are in very good agreement with the available experimental data and provide reliable predictions for all parameters, which have not been determined experimentally so far.
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