Mechanism and Kinetics of Na+ Ion Depletion under the Anode during Electro-thermal Poling of a Bioactive Glass

TL;DR

This study investigates the formation and kinetics of Na+ ion depletion layers in bioactive glass during electro-thermal poling, revealing a linear relation between layer thickness and voltage and highlighting the role of electronic mobility in charge compensation.

Contribution

It provides new insights into the depletion layer formation, showing a linear thickness-voltage relation and the significance of electronic mobility increase during poling, contrasting with standard theories.

Findings

Depletion layer thickness is linearly related to applied voltage.

Electric field in the layer is near dielectric breakdown and independent of voltage.

Depletion occurs on a shorter timescale than resistance change.

Abstract

Electro-thermal poling experiments were carried out on a bioactive glass, and the kinetics of the Na+ ion depletion layer formation under the anode was studied in-situ by means of ac impedance spectroscopy. One important finding is a linear relation between the depletion layer thickness and the applied voltage, which is in contrast to the predictions of standard space charge theory. The average electric field in the layer is independent of the voltage and is close to the dielectric breakdown field of alkali ion conducting glasses. Furthermore, we observe that the thickness of the depletion layer is established on a much shorter time scale than the resistance. We explain these results by assuming that the huge electric fields created under the anode during Na+ ion depletion lead to a strong increase of the electronic mobility in the layer and to charge compensation via extraction of electrons. It is shown that in the initial stages of the depletion process, a relative Na+ ion depletion of only 400 ppm is sufficient to generate electric fields of the order of the dielectric breakdown field.