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Centrality measures highlight proton traps and access points to proton highways in kinetic Monte Carlo trajectories

机译:集中度度量突出了动力学蒙特卡洛轨迹中的质子陷阱和质子高速公路的访问点

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A centrality measure based on the time of first returns rather than the number of steps is developed and applied to finding proton traps and access points to proton highways in the doped perovskite oxides: AZr(0.87)5D(0.125)O(3), where A is Ba or Sr and the dopant D is Y or Al. The high centrality region near the dopant is wider in the SrZrO3 systems than the BaZrO3 systems. In the aluminum-doped systems, a region of intermediate centrality (secondary region) is found in a plane away from the dopant. Kinetic Monte Carlo (kMC) trajectories show that this secondary region is an entry to fast conduction planes in the aluminum-doped systems in contrast to the highest centrality area near the dopant trap. The yttrium-doped systems do not show this secondary region because the fast conduction routes are in the same plane as the dopant and hence already in the high centrality trapped area. This centrality measure complements kMC by highlighting key areas in trajectories. The limiting activation barriers found via kMC are in very good agreement with experiments and related to the barriers to escape dopant traps. (C) 2015 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution 3.0 Unported License.
机译:开发了基于首次返回时间而不是步骤数的中心度度量,并将其应用于在掺杂的钙钛矿氧化物中寻找质子陷阱和质子公路的入口点:AZr(0.87)5D(0.125)O(3),其中A是Ba或Sr,掺杂物D是Y或Al。在SrZrO3系统中,掺杂剂附近的高中心区域比BaZrO3系统更宽。在铝掺杂系统中,在远离掺杂剂的平面中发现了中间中心区域(次级区域)。动力学蒙特卡洛(kMC)轨迹显示,与掺杂阱附近的最高中心区域相比,该次要区域是铝掺杂系统中快速传导平面的入口。掺钇的系统没有显示该次要区域,因为快速传导路径与掺杂剂在同一平面上,因此已经在高中心俘获区域中。这种中心性度量通过突出轨迹中的关键区域来补充kMC。通过kMC发现的极限激活势垒与实验非常吻合,并且与逃逸掺杂阱的势垒有关。 (C)2015年作者。除另有说明外,所有文章内容均根据知识共享署名3.0未移植许可证进行许可。

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