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Overscreening and Underscreening in Solid-Electrolyte Grain Boundary Space-Charge Layers

Jacob Dean, Samuel Coles, William Saunders, Andrew Mccluskey, Matthew Wolf, Alison Walker, Benjamin Morgan

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Abstract

Polycrystalline solids can exhibit material properties that differ significantly from those of equivalent single-crystal samples, in part, because of a spontaneous redistribution of mobile point defects into so-called space-charge regions adjacent to grain boundaries. The general analytical form of these space-charge regions is known only in the dilute limit, where defect-defect correlations can be neglected. Using kinetic Monte Carlo simulations of a three-dimensional Coulomb lattice gas, we show that grain boundary space-charge regions in nondilute solid electrolytes exhibit overscreening—damped oscillatory space-charge profiles—and underscreening—decay lengths that are longer than the corresponding Debye length and that increase with increasing defect-defect interaction strength. Overscreening and underscreening are known phenomena in concentrated liquid electrolytes, and the observation of functionally analogous behavior in solid electrolyte space-charge regions suggests that the same underlying physics drives behavior in both classes of systems. We therefore expect theoretical approaches developed to study nondilute liquid electrolytes to be equally applicable to future studies of solid electrolytes.

Original languageEnglish
Article number135502
JournalPhysical Review Letters
Volume127
Issue number13
Early online date17 Aug 2021
DOIs
Publication statusPublished - 24 Sept 2021

Funding

J. M. D. acknowledges support from the EPSRC (Grant No. 2119790). J. M. D. and B. J. M. acknowledge the support of the Faraday Institution through the Multi-Scale Modeling project (Grant No. FIRG003). S. W. C. and B. J. M. acknowledge the support of the Faraday Institution through the CATMAT project (Grant No. FIRG016). B. J. M. acknowledges support from the Royal Society (UF130329 and URF\R\191006). W. R. S., M. J. W., and A. B. W. acknowledge funding from the European Union’s Horizon 2020 program, via the Energy Oriented Centre of Excellence (EoCoE-II), under grant agreement no. 676629. The authors thank Dr. Ian R. Thompson for useful discussions. We are grateful to the UK Materials and Molecular Modeling Hub for computational resources, which is partially funded by EPSRC (EP/P020194/1). This research made use of the Balena High Performance Computing (HPC) Service at the University of Bath. Engineering and Physical Sciences Research Council Faraday Institution Royal Society Horizon 2020 Framework Programme Engineering and Physical Sciences Research Council University of Bath

FundersFunder number
Energy Oriented Centre of ExcellenceEP/P020194/1, 676629
Engineering and Physical Sciences Research Council Faraday Institution Royal Society Horizon 2020 Framework Programme Engineering and Physical Sciences Research Council University of Bath
The Faraday InstitutionFIRG003, FIRG016
Engineering and Physical Sciences Research Council2119790
Royal SocietyURF\R\191006, UF130329
EU - Horizon 2020

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