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arXiv 2302.03150cond-mat.mtrl-sci
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β-LiGaO₂中改进的准粒子自洽电子能带结构与激子

Improved quasiparticle self-consistent electronic band structure and excitons in $β$-LiGaO$_2$

Niloufar Dadkhah, Walter R. L. Lambrecht, Dimitar Pashov, Mark van Schilfgaarde

AI总结:

采用含电子-空穴梯形图的QSĜŴ方法改进计算β-LiGaO₂能带,获得约7.0 eV带隙及约6.0 eV激子带隙,并揭示各向异性修正的类里德伯激子态。

摘要:

本文采用准粒子自洽QSĜŴ方法计算了β-LiGaO₂的能带结构,其中屏蔽库仑相互作用Ŵ在计算时包含电子-空穴相互作用梯形图,而G为单电子格林函数。与以往计算相比,收敛性的改善使带隙显著增大至约7.0 eV。然而,研究发现激子结合能较大;若再计入约−0.4 eV的零点运动修正,则激子带隙约为6.0 eV。这些结果与近期关于吸收起始点的实验结果高度吻合。除迄今已观测到的激子外,计算还表明存在类里德伯系列的激子激发态;但由于材料的各向异性以及Bethe-Salpeter方程所导致的激子中Bloch态更复杂的混合,该系列不同于经典的Wannier激子模型。本文还以多种方式对激子精细结构和激子波函数进行了可视化与分析。

英文摘要:

The band structure of $β$-LiGaO$_2$ is calculated using the quasiparticle self-consistent QS$G\hat W$ method where the screened Coulomb interaction $\hat W$ is evaluated including electron-hole interaction ladder diagrams and $G$ is the one-electron Green's function. Improved convergence compared to previous calculations leads to a significantly larger band gap of about 7.0 eV. However, exciton binding energies are found to be large and lead to an exciton gap of about 6.0 eV if also a zero-point-motion correction of about $-0.4$ eV is included. These results are in excellent agreement with recent experimental results on the onset of absorption. Besides the excitons observed thus far, the calculations indicate the existence of a Rydberg-like series of exciton excited states, which is however modified from the classical Wannier exciton model by the anisotropies of the material and the more complex mixing of Bloch states in the excitons resulting from the Bethe-Salpeter equation. The exciton fine structure and the exciton wave functions are visualized and analyzed in various ways.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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