April 22 - 26, 2024
Seattle, Washington
May 7 - 9, 2024 (Virtual)
Symposium Supporters
2024 MRS Spring Meeting & Exhibit
EL07.01.01

Emergent Dipolar Textures and Properties in All-Ferroelectric Superlattices

When and Where

Apr 23, 2024
10:30am - 11:00am
Room 342, Level 3, Summit

Presenter(s)

Lane Martin, University of California, Berkeley

Co-Author(s)

Lane Martin1

Rice University1

Abstract

Lane Martin1

Rice University1
Emergent topological dipolar textures including vortices, dipolar waves, skyrmions, merons, hopfions, and more have generated considerable interest in the ferroelectrics and wider condensed-matter physics communities. The delicate balance of electric, elastic, and gradient energies of ferroelectrics can be tailored in low-dimensional forms and nanostructures to manipulate the order parameters. Exotic functional properties (<i>e.g.</i>, coexistence of phases, chirality, negative capacitance, and emergent ultrafast dynamical responses) make them interesting candidates for devices. Ferroelectric-dielectric superlattices such as (PbTiO<sub>3</sub>)<i><sub>n</sub></i>/(SrTiO<sub>3</sub>)<i><sub>n</sub></i> have been widely studied as a model system in part due to the high depolarizing field boundary condition provided by the SrTiO<sub>3 </sub>layer. Such layers, however, limit the incorporation of such heterostructures into devices that could use the electronic characteristics of these polar topologies.<br/><br/>Looking to expand upon this rich design space, we ask a simple question: can similar emergent dipolar textures be produced in all-ferroelectric (and other) heterostructures while providing additional tunability based on the susceptibilities of the constituent layers? Here, we demonstrate the formation of polar vortices in all-ferroelectric Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3</sub>/PbTiO<sub>3</sub>/Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3 </sub>trilayer and (Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3</sub>)<i><sub>n</sub></i>/(PbTiO<sub>3</sub>)<i><sub>n</sub></i> superlattice structures wherein 0.5 &lt; x &lt; 1 grown on DyScO<sub>3</sub> (110) substrates. Unlike their counterparts with SrTiO<sub>3</sub>, the Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3</sub> layers exhibit robust, in-plane ferroelectric polarization and domain structures, but still provide the appropriate boundary condition for the formation of polar vortices in the PbTiO<sub>3</sub> layers. We describe the manifestation of complex polar order in these structures that combines traditional ferroelectric order with emergent dipolar textures. Reciprocal space mapping studies reveal that the strontium content in the Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3 </sub>provides a fine control knob over the vortex periodicity; as supported by molecular-dynamics simulations. Furthermore, while recent studies on in-plane ferroelectric switching of polar vortices showed classical bistable switching, here, the in-plane polarization component of the vortices in the PbTiO<sub>3</sub> layers and the ferroelectric domains in the Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3 </sub>layers exhibit strong elastic and dipolar coupling, leading to a coercivity enhancement of the trilayer stack upon decreasing the strontium content of the Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3</sub>. Phase-field simulations further explain the polarization arrangement in the trilayer and the system’s subsequent collective switching pathway of the two order parameters. Formation of such in-plane domains in the Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3 </sub>leads to the formation of a labyrinthine vortex arrangement, unlike the highly unidirectional vortices observed in (PbTiO<sub>3</sub>)<i><sub>n</sub></i>/(SrTiO<sub>3</sub>)<i><sub>n</sub></i> superlattices. Further, we have explored the coupling between different emergent dipolar heterostructures of the from Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3</sub>/PbTiO<sub>3</sub>/Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3</sub>/SrTiO<sub>3</sub>/PbTiO<sub>3</sub>/SrTiO<sub>3</sub>. Therein, the thickness of the SrTiO<sub>3 </sub>layer separating the two vortex structures controls the strength of the elastic and electric fields that extend between layers, affecting the sequence in which each trilayer would switch and the number of switching events. The result is an ability to produce low-field multi-state, four-step switching with robust retention and fatigue performance. Finally, in (Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3</sub>)<i><sub>n</sub></i>/(PbTiO<sub>3</sub>)<i><sub>n</sub></i> superlattices we have explored the dielectric tunability and out-of-plane switching and find improved tunability as a function of the chemistry of the Pb<sub>1-x</sub>Sr<sub>x</sub>TiO<sub>3 </sub>layer, antiferroelectric-like switching due to an unraveling of the vortex phase upon application of the electric-field, and strong back switching on releasing the same leading to improvements in the low-field energy storage as compared to (PbTiO<sub>3</sub>)<i><sub>n</sub></i>/(SrTiO<sub>3</sub>)<i><sub>n</sub></i>.

Keywords

ferroelectricity | thin film

Symposium Organizers

John Heron, University of Michigan
Morgan Trassin, ETH Zurich
Ruijuan Xu, North Carolina State University
Di Yi, Tsinghua University

Symposium Support

Gold
ADNANOTEK CORP.

Bronze
Arrayed Materials (China) Co., Ltd.
NBM Design, Inc.

Session Chairs

Ruijuan Xu
Pu Yu

In this Session