Atomic-scale observations of electrical and mechanical manipulation of topological polar flux-closure
arXiv:1911.09822 · doi:10.1073/pnas.2007248117
Abstract
The ability to controllably manipulate the complex topological polar configurations, such as polar flux-closure via external stimuli, enables many applications in electromechanical devices and nanoelectronics including high-density information storage. Here, by using the atomically resolved in situ scanning transmission electron microscopy, we find that a polar flux-closure structure in PbTiO3/SrTiO3 superlattices films can be reversibly switched to ordinary mono ferroelectric c domain or a domain under electric field or stress. Specifically, the electric field initially drives the flux-closure move and breaks them to form intermediate a/c striped domains, while the mechanical stress firstly starts to squeeze the flux-closures to convert into small vortices at the interface and form a continues dipole wave. After the removal of the external stimuli, the flux-closure structure spontaneously returns. Our atomic study provides valuable insights into understanding the lattice-charge interactions and the competing interactions balance in these complex topological structures. Such reversible switching between the flux-closure and ordinary ferroelectric domains also provides the foundation for applications such as memories and sensors.
arXiv comment22 pages, 5figures,
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Cited by in corpus (8)
- Dynamics of Polar Skyrmion Bubbles under Electric Fields
- Ferroelectric Solitons Crafted in Epitaxial Bismuth Ferrite Superlattices
- Local Manipulation of Polar Skyrmions and Topological Phase Transitions
- Order-disorder transitions in a polar vortex lattice
- Electric-field control of the nucleation and motion of isolated three-fold polar vertices
- Manipulation of polar vortex chirality in oxide superlattices
- Topological protection breakdown: a route to frustrated ferroelectricity
- Chemical control of polymorphism and ferroelectricity in PbTiO3 and SrTiO3 monolayers and bilayers