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多铁性铜氯硼酸盐中的有序-无序、铁弹性及畴壁迁移率

Order-disorder, ferroelasticity and mobility of domain walls in multiferroic Cu-Cl boracite.

作者信息

Fernandez-Posada C M, Cochard C, Gregg J M, Whatmore R W, Carpenter M A

机构信息

Department of Earth Sciences, University of Cambridge, Downing Street, Cambridge CB2 3EQ, United Kingdom.

Centre for Nanostructured Media, School of Mathematics and Physics, Queen's University Belfast, Belfast BT7 1NN, United Kingdom.

出版信息

J Phys Condens Matter. 2021 Mar 3;33(9):095402. doi: 10.1088/1361-648X/abcb0f.

Abstract

Domain walls in Cu-Cl boracite develop as a consequence of an improper ferroelastic, improper ferroelectric transition, and have attracted close interest because some are conductive and all can be mechanically written and repositioned by application of an electric field. The phase transition and its associated dynamical properties have been analysed here from the perspective of strain and elasticity. Determination of spontaneous strains from published lattice parameter data has allowed the equilibrium long-range order parameter for F [Formula: see text]3c → Pca2 to be modelled simply as being close to the order-disorder limit. High acoustic loss in the cubic phase, revealed by resonant ultrasound spectroscopy, is consistent with the presence of dynamical microdomains of the orthorhombic structure with relaxation times in the vicinity of ∼10-10 s. Low acoustic loss in the stability field of the orthorhombic structure signifies, on the other hand, that ferroelastic twin walls which develop as a consequence of the order-disorder process are immobile on this time scale. A Debye loss peak accompanied by ∼1% elastic stiffening at ∼40 K is indicative of some freezing of defects which couple with strain or of some more intrinsic freezing process. The activation energy of ⩾∼0.01-0.02 eV implies a mechanism which could involve strain relaxation clouds around local ferroelectric dipoles or freezing of polarons that determine the conductivity of twin walls.

摘要

Cu-Cl 方硼石中的畴壁是由不当的铁弹性、不当的铁电转变产生的,并且因其具有导电性以及所有畴壁都可通过施加电场进行机械书写和重新定位而备受关注。本文从应变和弹性的角度分析了相变及其相关的动力学性质。根据已发表的晶格参数数据确定自发应变,使得 F [公式:见正文]3c → Pca2 的平衡长程序参量可以简单地建模为接近有序-无序极限。共振超声光谱揭示的立方相中高声学损耗,与具有约 10 - 10 秒弛豫时间的正交结构动态微畴的存在相一致。另一方面,正交结构稳定场中的低声学损耗表明,由有序-无序过程产生的铁弹性孪晶壁在这个时间尺度上是不动的。在约 40 K 时出现的伴有约 1%弹性硬化的德拜损耗峰表明,存在一些与应变耦合的缺陷冻结或一些更内在的冻结过程。⩾约 0.01 - 0.02 eV 的激活能意味着一种机制,该机制可能涉及局部铁电偶极子周围的应变弛豫云或决定孪晶壁电导率的极化子冻结。

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