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Many competing ceria (110) oxygen vacancy structures: From small to large supercells large supercells

机译:许多竞争的二氧化铈(110)氧空位结构:从小型超级电池到大型超级电池

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We present periodic "DFT+U" studies of single oxygen vacancies on the CeO_2(110) surface using a number of different supercells, finding a range of different local minimum structures for the vacancy and its two accompanying Ce(III) ions.We find three different geometrical structures in combination with a variety of different Ce(III) localization patterns, several of which have not been studied before. The desired trapping of electrons was achieved in a two-stage optimization procedure. We find that the surface oxygen nearest to the vacancy either moves within the plane towards the vacancy, or rises out of the surface into either a symmetric or an unsymmetric bridge structure. Results are shown in seven slab geometry supercells, p(2 × 1), p(2 × 2), p(2 × 3), p(3 × 2), p(2 × 4), p(4 × 2), and p(3 × 3), and indicate that the choice of supercell can affect the results qualitatively and quantitatively. An unsymmetric bridge structure with one nearest and one next-nearest neighbour Ce(III) ion (a combination of localizations not previously found) is the ground state in all (but one) of the supercells studied here, and the relative stability of other structures depends strongly on supercell size. Within any one supercell the formation energies of the different vacancy structures differ by up to 0.5 eV, but the same structure can vary by up to ~1 eV between supercells. Furthermore, finite size scaling suggests that the remaining errors (compared to still larger supercells) can also be ~1 eV for some vacancy structures.
机译:我们使用大量不同的超级电池,对CeO_2(110)表面的单个氧空位进行了定期的“ DFT + U”研究,发现了空位及其两个伴随的Ce(III)离子的一系列不同的局部最小结构。三种不同的几何结构,以及各种不同的Ce(III)定位模式,其中一些以前从未研究过。在两个阶段的优化过程中实现了所需的电子捕获。我们发现最接近空位的表面氧要么在平面内朝空位移动,要么从表面上升到对称或不对称的桥结构中。结果显示在七个平板几何超级单元中,p(2×1),p(2×2),p(2×3),p(3×2),p(2×4),p(4×2) ,和p(3×3),并表明超级单元的选择可以定性和定量地影响结果。具有一个最近和一个最近邻的Ce(III)离子的非对称桥结构(以前未发现过的局部结合)是此处研究的所有(但只有一个)超级电池的基态,以及其他结构的相对稳定性很大程度上取决于超级单元的大小。在任何一个超级电池中,不同空位结构的形成能相差高达0.5 eV,但同一结构在两个超级电池之间可以相差高达〜1 eV。此外,有限尺寸缩放表明,对于某些空位结构,剩余的误差(与更大的超级电池相比)也可以约为1 eV。

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