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Control of Uniaxial Negative Thermal Expansion in Layered Perovskites by Tuning Layer Thickness

机译:调整层厚控制层状钙钛矿中单轴负热膨胀

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摘要

Uniaxial negative thermal expansion (NTE) is known to occur in low n members of the An+1BnO3n+1 Ruddlesden–Popper (RP) layered perovskite series with a frozen rotation of BO6 octahedra about the layering axis. Previous work has shown that this NTE arises due to the combined effects of a close proximity to a transition to a competing phase, so called “symmetry trapping”, and highly anisotropic elastic compliance specific to the symmetry of the NTE phase. We extend this analysis to the broader RP family (n = 1, 2, 3, 4, …, ∞), demonstrating that by changing the fraction of layer interface in the structure (i.e., the value of 1) one may control the anisotropic compliance that is necessary for the pronounced uniaxial NTE observed in these systems. More detailed analysis of how the components of the compliance matrix develop with 1 allows us to identify different regimes, linking enhancements in compliance between these regimes to the crystallographic degrees of freedom in the structure. We further discuss how the perovskite layer thickness affects the frequencies of soft zone boundary modes with large negative Grüneisen parameters, associated with the aforementioned phase transition, that constitute the thermodynamic driving force for NTE. This new insight complements our previous work—showing that chemical control may be used to switch from positive to negative thermal expansion in these systems—since it makes the layer thickness, n, an additional design parameter that may be used to engineer layered perovskites with tuneable thermal expansion. In these respects, we predict that, with appropriate chemical substitution, the n = 1 phase will be the system in which the most pronounced NTE could be achieved.
机译:已知单轴负热膨胀(NTE)发生在An + 1BnO3n + 1 Ruddlesden-Popper(RP)层钙钛矿系列的低n个成员中,BO6八面体围绕着层轴冻结旋转。先前的工作表明,这种NTE的产生是由于非常接近过渡到竞争相的过渡(所谓的“对称性捕获”)和特定于NTE相的对称性的高度各向异性弹性柔韧性的综合作用。我们将此分析扩展到更广泛的RP系列(n = 1,2,3,4,…,∞),表明通过改变结构中层界面的分数(即值/ n),可以控制这些系统中观察到的明显单轴NTE所必需的各向异性顺应性。对顺应性矩阵的成分如何以1 / n进行更详细的分析,使我们能够确定不同的状态,并将这些状态之间的顺应性增强与结构的晶体自由度联系起来。我们进一步讨论钙钛矿层的厚度如何影响具有较大负Grüneisen参数的软区边界模式的频率,这些参数与上述相变有关,构成NTE的热力学驱动力。这一新见解补充了我们先前的工作-表明化学控制可用于在这些系统中从正热膨胀转换为负热膨胀-因为它使层厚度n(可用于设计可调整层状钙钛矿的附加设计参数)热膨胀。在这些方面,我们预测,通过适当的化学取代,n = 1相将是可以实现最明显NTE的系统。

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