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镧系镓酸盐LnGaO中高氧离子电导率的第一性原理预测

First-principles prediction of high oxygen-ion conductivity in trilanthanide gallates LnGaO.

作者信息

Lee Joohwi, Ohba Nobuko, Asahi Ryoji

机构信息

Toyota Central R&D Laboratories, Inc., Nagakute, Japan.

出版信息

Sci Technol Adv Mater. 2019 Feb 6;20(1):144-159. doi: 10.1080/14686996.2019.1578183. eCollection 2019.

DOI:10.1080/14686996.2019.1578183
PMID:30863467
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC6407603/
Abstract

We systematically investigated trilanthanide gallates (LnGaO) with the space group 2 as oxygen-ion conductors using first-principles calculations. Six LnGaO (Ln = Nd, Gd, Tb, Ho, Dy, or Er) are both energetically and dynamically stable among 15 LnGaO compounds, which is consistent with previous experimental studies reporting successful syntheses of single phases. LaGaO and LuGaO may be metastable despite a slightly higher energy than those of competing reference states, as phonon calculations predict them to be dynamically stable. The formation and the migration barrier energies of an oxygen vacancy ( ) suggest that eight LnGaO (Ln = La, Nd, Gd, Tb, Ho, Dy, Er, or Lu) can act as oxygen-ion conductors based on . Ga plays a role of decreasing the distances between the oxygen sites of LnGaO compared with those of LnO so that a migrates easier with a reduced migration barrier energy. Larger oxygen-ion diffusivities and lower migration barrier energies of for the eight LnGaO are obtained for smaller atomic numbers of Ln having larger radii of Ln. Their oxygen-ion conductivities at 1000 K are predicted to have a similar order of magnitude to that of yttria-stabilized zirconia.

摘要

我们使用第一性原理计算系统地研究了空间群为2的三镧系元素镓酸盐(LnGaO)作为氧离子导体的情况。在15种LnGaO化合物中,六种LnGaO(Ln = Nd、Gd、Tb、Ho、Dy或Er)在能量和动力学上都是稳定的,这与之前报道成功合成单相的实验研究一致。尽管LaGaO和LuGaO的能量比竞争参考态略高,但声子计算预测它们是动力学稳定的,因此可能是亚稳的。氧空位( )的形成能和迁移势垒能表明,基于 ,八种LnGaO(Ln = La、Nd、Gd、Tb、Ho、Dy、Er或Lu)可以作为氧离子导体。与LnO相比,Ga起到了减小LnGaO中氧位点之间距离的作用,从而使 迁移更容易,迁移势垒能降低。对于半径较大的Ln原子序数较小的八种LnGaO,获得了更大的氧离子扩散率和更低的 迁移势垒能。预测它们在1000 K时的氧离子电导率与氧化钇稳定的氧化锆具有相似的数量级。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/0f84d5f703b4/TSTA_A_1578183_F0010_OC.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/72a770c501c4/TSTA_A_1578183_F0004_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/ab0084718eff/TSTA_A_1578183_F0005_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/e2e4824a1576/TSTA_A_1578183_F0006_B.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/0169f97480db/TSTA_A_1578183_F0007_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/ac5ac5fa05f1/TSTA_A_1578183_F0008_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/522d2ea6b90e/TSTA_A_1578183_F0009_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/0f84d5f703b4/TSTA_A_1578183_F0010_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/04fac0918e62/TSTA_A_1578183_UF0001_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/999ab56a7ce9/TSTA_A_1578183_F0001_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/a50aa5785746/TSTA_A_1578183_F0002_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/a86de883d8d2/TSTA_A_1578183_F0003_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/72a770c501c4/TSTA_A_1578183_F0004_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/ab0084718eff/TSTA_A_1578183_F0005_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/e2e4824a1576/TSTA_A_1578183_F0006_B.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/0169f97480db/TSTA_A_1578183_F0007_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/ac5ac5fa05f1/TSTA_A_1578183_F0008_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/522d2ea6b90e/TSTA_A_1578183_F0009_OC.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3b80/6407603/0f84d5f703b4/TSTA_A_1578183_F0010_OC.jpg

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