Hybrid Hexagonal Perovskite Ba3Ti0.7Mo1.3O8.3: Integrating High Cationic Disordering with Enhanced Tetrahedral Proportion to Achieve High Oxide Ionic Conductivity

  • Zien Cheng
  • , Liyang Zhang
  • , Yuling An
  • , Ivan da Silva
  • , Joerg C. Neuefeind
  • , Zhengyang Zhou
  • , Congling Yin
  • , Rihong Cong
  • , Tao Yang
  • , Pengfei Jiang

Research output: Contribution to journalArticlepeer-review

Abstract

The advancement of crystalline solid-state oxide-ion conductors is essential for the development of clean energy applications, particularly in the context of solid-oxide fuel cells. Although numerous oxide-ion conducting materials exist, there is a pressing need for electrolyte materials that exhibit high oxide ionic conductivity at intermediate temperatures (300-600 °C). Herein, we report a fast oxide ionic conductor Ba3Ti0.7Mo1.3O8.3, which possesses a hybrid perovskite identified by three-dimensional electron diffraction, neutron powder diffraction, neutron pair distribution functions, and in situ synchrotron X-ray diffraction. Ba3Ti0.7Mo1.3O8.3 exhibits the highest degree of M-site disordering among the Ba3M′M″O8.5 ± δ hexagonal perovskite family while simultaneously maintaining a high proportion of the tetrahedral coordination geometry within the structure. The high level of M-site disordering and the high tetrahedral percentage in Ba3Ti0.7Mo1.3O8.3 facilitate oxide-ion diffusion along the c-axis and ab-plane, respectively, thereby resulting in a high bulk conductivity of 1.4 mS/cm at 500 °C, which is significantly higher than those of the Ba3M′M″O8.5 ± δ family members and other oxide ionic conductors. Our findings demonstrate that achieving a balance between M-site disordering and tetrahedral percentage is an effective strategy for improving the oxide ionic conductivity of Ba3M′M″O8.5 ± δ-type conductors.

Original languageEnglish
Pages (from-to)4629-4638
Number of pages10
JournalChemistry of Materials
Volume37
Issue number13
DOIs
StatePublished - Jul 8 2025
Externally publishedYes

Funding

This work is financially supported by the National Natural Science Foundation of China (nos. 22271030, 22171031, and 22171032) and the Fundamental Research Funds for the Central Universities (project no. 2024CDJXY010). A portion of this research used resources at Spallation Neutron Source, a DOE Office of Science User Facility operated by the Oak Ridge National Laboratory. The beamtime was allocated to NOMAD on Proposal Number IPTS-27837. J.C.N. is supported by contract no. DE-AC05-00OR22725 with the U.S. Department of Energy (DOE). We also acknowledge the support from the sharing fund of large-scale equipment of Chongqing University (202403150085).

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