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首页> 外文期刊>Solid state ionics >High activation energy for proton migration at Σ 3 111 / 1 1 ? 0 tilt grain boundary in barium zirconate
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High activation energy for proton migration at Σ 3 111 / 1 1 ? 0 tilt grain boundary in barium zirconate

机译:质子迁移的活化能高,为Σ3 111/1 1?锆酸钡中的0倾斜晶界

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摘要

The behavior of a proton at a Σ3111/11?0 tilt grain boundary in barium zirconate was investigated in order to explain proton migration at grain boundaries by using density functional theory. The space charge layer model and the structural disorder model have been proposed in the literature to explain the high activation energies for proton migration at grain boundaries as compared with those at the bulk. The space charge layer model was evaluated by calculating the segregation of an oxygen vacancy at the grain boundary core. The segregation of the oxygen vacancy at the grain boundary core developed a Schottky barrier height and generated a space charge layer at both sides of the core by expelling positively charged mobile protons. Since the activation energy for proton migration was affected by the decreased proton concentration in the space charge layer, the formation energy of the proton was considered in explaining the high activation energy at grain boundaries. The structural disorder model was evaluated by calculating the energy barriers for proton migration at the grain boundary core. High energy barriers for proton migration, in the range of 0.61 ~ 0.64 eV, were required at the grain boundary core, while relatively low energy barriers, in the range of 0.18 ~ 0.24 eV, were required near it. This high energy barrier for proton migration due to the structural disorder at the grain boundary core can also explain the high activation energy. Therefore, both the effect of the Schottky barrier height and the structural disorder at the grain boundary core should be considered in explaining the high activation energy for proton migration at the grain boundary in barium zirconate.
机译:研究了质子在锆酸钡中Σ3111/ 11?0倾斜晶界处的行为,以利用密度泛函理论解释质子在晶界处的迁移。文献中已经提出了空间电荷层模型和结构无序模型,以解释质子迁移与块体迁移相比具有较高的活化能。通过计算晶界核心处的氧空位的偏析来评估空间电荷层模型。晶界核心处的氧空位偏析形成了肖特基势垒高度,并通过排出带正电的移动质子在核心的两侧生成了空间电荷层。由于质子迁移的活化能受到空间电荷层中质子浓度降低的影响,因此在解释晶界处的高活化能时考虑了质子的形成能。通过计算晶界核心处质子迁移的能垒来评估结构无序模型。在晶界核心处要求高的质子迁移能垒在0.61〜0.64 eV的范围内,而在其附近需要较低的能垒在0.18〜0.24 eV的范围内。由于晶界核心处的结构紊乱,质子迁移的这种高能垒也可以解释高活化能。因此,在解释锆酸钡中质子迁移的高活化能时,应考虑肖特基势垒高度的影响和晶界核心处的结构紊乱。

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