Identification of charge carriers and quantification of diffusion coefficients in the energy landscape of S53P4 bioglass

Abstract The ionic conduction of S53P4 glass has been investigated by a combination of electric field‐assisted ion exchange and thermal electro‐poling experiments. The dominant charge carrier being mobile in native S53P4 is identified to be the Na + ion. By means of alkali proton substitution and alkali deuteron substitution, the diffusion coefficient, D(Na + ), has been determined as a function of the local Na + concentration. It is found to vary over 2 orders of magnitude due to the distribution of site energies in the potential energy landscape of the glass. The Ca ++ ions appear immobile under the conditions of the alkali‐proton substitution technique and alkali‐deuteron substitution experiments. However, Ca ++ ions become mobile under the conditions of thermal electro‐poling. The diffusion coefficient for Ca ++ ions, D(Ca ++ ), turns out to be five orders of magnitude smaller than D(Na + ) in the bulk.

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Publication Details

Journal
Journal of the American Ceramic Society
Published
2025-09-24
DOI
https://doi.org/10.1111/jace.70257
Primary Topic
Bone Tissue Engineering Materials
Type
article
Field-Weighted Citation Impact
0.00

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article

Identification of charge carriers and quantification of diffusion coefficients in the energy landscape of S53P4 bioglass

Karl‐Michael Weitzel, Kevin Rein, Martin Schäfer, Youssef Elbishbishy
Journal of the American Ceramic Society
Bone Tissue Engineering Materials
article

Identification of charge carriers and quantification of diffusion coefficients in the energy landscape of S53P4 bioglass

Karl‐Michael Weitzel, Kevin Rein, Martin Schäfer, Youssef Elbishbishy
article en

Abstract

Abstract The ionic conduction of S53P4 glass has been investigated by a combination of electric field‐assisted ion exchange and thermal electro‐poling experiments. The dominant charge carrier being mobile in native S53P4 is identified to be the Na + ion. By means of alkali proton substitution and alkali deuteron substitution, the diffusion coefficient, D(Na + ), has been determined as a function of the local Na + concentration. It is found to vary over 2 orders of magnitude due to the distribution of site energies in the potential energy landscape of the glass. The Ca ++ ions appear immobile under the conditions of the alkali‐proton substitution technique and alkali‐deuteron substitution experiments. However, Ca ++ ions become mobile under the conditions of thermal electro‐poling. The diffusion coefficient for Ca ++ ions, D(Ca ++ ), turns out to be five orders of magnitude smaller than D(Na + ) in the bulk.

Journal of the American Ceramic SocietyVol. 109(1)
Philipps University of Marburg (DE)
Deutsche Forschungsgemeinschaft
Openalex Percentile: Top 75%
Bone Tissue Engineering Materials
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