Cargando…

Domain topology and domain switching kinetics in a hybrid improper ferroelectric

Charged polar interfaces such as charged ferroelectric walls or heterostructured interfaces of ZnO/(Zn,Mg)O and LaAlO(3)/SrTiO(3), across which the normal component of electric polarization changes suddenly, can host large two-dimensional conduction. Charged ferroelectric walls, which are energetica...

Descripción completa

Detalles Bibliográficos
Autores principales: Huang, F. -T., Xue, F., Gao, B., Wang, L. H., Luo, X., Cai, W., Lu, X. -Z., Rondinelli, J. M., Chen, L. Q., Cheong, S. -W.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2016
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4890185/
https://www.ncbi.nlm.nih.gov/pubmed/27215944
http://dx.doi.org/10.1038/ncomms11602
Descripción
Sumario:Charged polar interfaces such as charged ferroelectric walls or heterostructured interfaces of ZnO/(Zn,Mg)O and LaAlO(3)/SrTiO(3), across which the normal component of electric polarization changes suddenly, can host large two-dimensional conduction. Charged ferroelectric walls, which are energetically unfavourable in general, were found to be mysteriously abundant in hybrid improper ferroelectric (Ca,Sr)(3)Ti(2)O(7) crystals. From the exploration of antiphase boundaries in bilayer-perovskites, here we discover that each of four polarization-direction states is degenerate with two antiphase domains, and these eight structural variants form a Z(4) × Z(2) domain structure with Z(3) vortices and five distinct types of domain walls, whose topology is directly relevant to the presence of abundant charged walls. We also discover a zipper-like nature of antiphase boundaries, which are the reversible creation/annihilation centres of pairs of two types of ferroelectric walls (and also Z(3)-vortex pairs) in 90° and 180° polarization switching. Our results demonstrate the unexpectedly rich nature of hybrid improper ferroelectricity.