Dimensional control of defect dynamics in perovskite oxide superlattices

Isaac Bredeson, Lipeng Zhang, P. R. C. Kent, Valentino R. Cooper, and Haixuan Xu (徐海譞)
Phys. Rev. Materials 2, 035401 – Published 8 March 2018

Abstract

Point defects play a critical role in the structural, physical, and interfacial properties of perovskite oxide superlattices. However, understanding of the fundamental properties of point defects in superlattices, especially their transport properties, is rather limited. Here, we report predictions of the stability and dynamics of oxygen vacancies in SrTiO3/PbTiO3 oxide superlattices using first-principles calculations in combination with the kinetic Monte Carlo method. By varying the stacking period, i.e., changing of n in nSTO/nPTO, we discover a crossover from three-dimensional diffusion to primarily two-dimensional planar diffusion. Such planar diffusion may lead to novel designs of ionic conductors. We show that the dominant vacancy position may vary in the superlattices, depending on the superlattice structure and stacking period, contradicting the common assumption that point defects reside at interfaces. Moreover, we predict a significant increase in room-temperature ionic conductivity for 3STO/3PTO relative to the bulk phases. Considering the variety of cations that can be accommodated in perovskite superlattices and the potential mismatch of spin, charge, and orbitals at the interfaces, this paper identifies a pathway to control defect dynamics for technological applications.

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  • Received 2 December 2017

DOI:https://doi.org/10.1103/PhysRevMaterials.2.035401

©2018 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Isaac Bredeson1, Lipeng Zhang1, P. R. C. Kent2,3, Valentino R. Cooper4, and Haixuan Xu (徐海譞)1,5,*

  • 1Department of Materials Science and Engineering, The University of Tennessee, Knoxville, Tennessee 37996, USA
  • 2Center for Nanophase Materials Science, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 3Computational Science and Engineering Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 4Materials Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 5Joint Institute for Advanced Materials, The University of Tennessee, Knoxville, Tennessee 37996, USA and Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA

  • *xhx@utk.edu

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Vol. 2, Iss. 3 — March 2018

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