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首页> 外文期刊>Physical Review, B. Condensed Matter >Electron-energy-loss function of LiTaO3 and LiNbO3 by X-ray photoemission spectroscopy: Theory and experiment
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Electron-energy-loss function of LiTaO3 and LiNbO3 by X-ray photoemission spectroscopy: Theory and experiment

机译:X射线光发射光谱法研究LiTaO3和LiNbO3的电子能量损失函数:理论与实验

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摘要

We report experimental energy-loss structures in x-ray photoemission spectra of single crystalline LiTaO3 and LiNbO3, and then compare these with theoretical electron-energy-loss functions calculated from first principles using the full-potential linearized augmented plane-wave method in the local-density approximation. The energy-loss structure of core electrons can be approximated by a sum of four components: for LiTaO3, the peaks positioned at 8.0, 13.4, 15.8, and 22.6 eV; for LiNbO3, those positioned at 7.0, 12.0, 14.5, and 21.8 eV. The momentum matrix elements between Bloch functions were evaluated to determine the electron energy-loss functions. The theoretical electron-energy-loss functions agreed fairly well with the experimental one. The experimental peaks positioned at 8.0, 13.4, and 15.8 eV for LiTaO3 and those at 7.0, 12.0, and 14.5 eV for LiNbO3 were assigned to the interband transitions from the valence band to the conduction bands. The peaks at 22.6 eV for LiTaO3 and 21.8 eV for LiNbO3 were ascribed to the electron excitation from the O 2s level to the lower conduction band. [References: 17]
机译:我们在单晶LiTaO3和LiNbO3的x射线光发射光谱中报告了实验的能量损失结构,然后将它们与从第一原理使用全电势线性化增强平面波方法在局部计算的理论电子能量损失函数进行比较。 -密度近似。核心电子的能量损失结构可以通过四个分量的总和来近似:对于LiTaO3,峰位于8.0、13.4、15.8和22.6 eV;对于LiTaO3,峰位于8.0、13.4、15.8和22.6 eV。对于LiNbO3,它们位于7.0、12.0、14.5和21.8 eV。评估了Bloch函数之间的动量矩阵元素,以确定电子能量损失函数。理论上的电子-能量损失函数与实验值相当吻合。 LiTaO3位于8.0、13.4和15.8 eV的实验峰以及LiNbO3位于7.0、12.0和14.5 eV的实验峰被指定为从价带到导带的带间跃迁。 LiTaO3的22.6 eV峰和LiNbO3的21.8 eV峰归因于从O 2s能级到较低导带的电子激发。 [参考:17]

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