TY - JOUR
T1 - Incorporation of protons and hydroxide species in BaZrO3 and BaCeO3
AU - Rowberg, Andrew J.E.
AU - Li, Meng
AU - Ogitsu, Tadashi
AU - Varley, Joel B.
N1 - Funding Information:
The authors acknowledge support from the HydroGEN Advanced Water Splitting Materials Consortium, established as part of the Energy Materials Network under the U.S. Department of Energy (DOE), the Office of Energy Efficiency and Renewable Energy (EERE), the Hydrogen and Fuel Cell Technologies Office (HFTO). Part of this work was performed under the auspices of the DOE by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344. M. Li additionally acknowledges support from the DOE Idaho Operations Office under contract no. DE-AC07-05ID14517. The research was performed using computational resources sponsored by the DOE's EERE and located at the National Renewable Energy Laboratory.
Publisher Copyright:
© 2023 RSC.
PY - 2023/10/18
Y1 - 2023/10/18
N2 - Barium zirconate (BaZrO3 or BZO) and barium cerate (BaCeO3 or BCO) are among the best-performing proton-conducting oxides used as electrolytes in all-solid-state fuel and/or electrolysis cells. During synthesis, they are seeded with oxygen vacancies (V2+O), which charge-compensate with acceptor dopants such as yttrium (Y−Zr) and, upon exposure to water vapor, are replaced by interstitial protons (H+i). Here, we investigate this and alternative processes for protonation by calculating defect formation energies, concentrations, and migration barriers for several relevant species, including H+i, V2+O, interstitial oxygen (O2−i), and interstitial hydroxide (OH−i), using density functional theory. We confirm that V2+O are favorable under typical operating conditions, although at lower partial pressures of H2 gas and wet conditions, H+i becomes the dominant donor species. Higher H+i concentrations in BCO than in BZO under comparable conditions help to explain the higher conductivity measured in BCO. OH−i species are present in low concentrations in the bulk (particularly in BZO; they may incorporate in BCO under wet conditions), and their migration is slow; however, they may form at surfaces and help seed materials with H+i. Alloying BZO and BCO improves ionic conduction in general, although the presence of native defects tends to impede kinetics. Our results show that high ionic conductivity can be achieved through optimizing synthesis conditions to maximize the concentrations of H+i, as well as reducing defect-rich regions such as grain boundaries.
AB - Barium zirconate (BaZrO3 or BZO) and barium cerate (BaCeO3 or BCO) are among the best-performing proton-conducting oxides used as electrolytes in all-solid-state fuel and/or electrolysis cells. During synthesis, they are seeded with oxygen vacancies (V2+O), which charge-compensate with acceptor dopants such as yttrium (Y−Zr) and, upon exposure to water vapor, are replaced by interstitial protons (H+i). Here, we investigate this and alternative processes for protonation by calculating defect formation energies, concentrations, and migration barriers for several relevant species, including H+i, V2+O, interstitial oxygen (O2−i), and interstitial hydroxide (OH−i), using density functional theory. We confirm that V2+O are favorable under typical operating conditions, although at lower partial pressures of H2 gas and wet conditions, H+i becomes the dominant donor species. Higher H+i concentrations in BCO than in BZO under comparable conditions help to explain the higher conductivity measured in BCO. OH−i species are present in low concentrations in the bulk (particularly in BZO; they may incorporate in BCO under wet conditions), and their migration is slow; however, they may form at surfaces and help seed materials with H+i. Alloying BZO and BCO improves ionic conduction in general, although the presence of native defects tends to impede kinetics. Our results show that high ionic conductivity can be achieved through optimizing synthesis conditions to maximize the concentrations of H+i, as well as reducing defect-rich regions such as grain boundaries.
UR - https://www.scopus.com/pages/publications/85175192533
U2 - 10.1039/d3ma00308f
DO - 10.1039/d3ma00308f
M3 - Article
AN - SCOPUS:85175192533
SN - 2633-5409
VL - 4
SP - 6233
EP - 6243
JO - Materials Advances
JF - Materials Advances
IS - 23
ER -