2020
DOI: 10.1016/j.ssi.2020.115369
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Disagreements between space charge models and grain boundary impedance data in yttrium-substituted barium zirconate

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Cited by 15 publications
(11 citation statements)
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“…The charge imbalance thus emerges as a consequence of excess proton segregation and is neutralized by subsequent depletion of protons across the negatively charged space charge region adjacent to the grain boundary core on both sides as shown in Figure 9. 204 The overall outline presents the significance of microstructure over structural and charge dynamical properties in pure and acceptor-doped PCs. The detailed analysis illustrates a direct correlation between grain and grain boundary dimensions and symmetry over fluctuations in total ionic conductivity among diverse PCs.…”
Section: Microstructural Disorder Over Perturbed Protonmentioning
confidence: 99%
See 1 more Smart Citation
“…The charge imbalance thus emerges as a consequence of excess proton segregation and is neutralized by subsequent depletion of protons across the negatively charged space charge region adjacent to the grain boundary core on both sides as shown in Figure 9. 204 The overall outline presents the significance of microstructure over structural and charge dynamical properties in pure and acceptor-doped PCs. The detailed analysis illustrates a direct correlation between grain and grain boundary dimensions and symmetry over fluctuations in total ionic conductivity among diverse PCs.…”
Section: Microstructural Disorder Over Perturbed Protonmentioning
confidence: 99%
“…The energetically stable protonic site along the grain boundary core imposes trapping centers due to defect segregation. The charge imbalance thus emerges as a consequence of excess proton segregation and is neutralized by subsequent depletion of protons across the negatively charged space charge region adjacent to the grain boundary core on both sides as shown in Figure …”
Section: Impact Of Acceptor Dopant On Perovskite Type Baceo3 Proton C...mentioning
confidence: 99%
“…The potential distribution in one half of the double Schottky barrier can be expressed as 11 φ()x=φ()0()x2λ22xλ+1$$\begin{equation} \varphi \left(x\right)=\varphi \left(0\right)\left(\frac{{x}^{2}}{{\lambda}^{2}}-2\frac{x}{\lambda}+1\right) \end{equation}$$…”
Section: Figurementioning
confidence: 99%
“…However, the assumption concerning the same mobility for charge carriers transporting in the bulk and space charge layer was basically not justified. This argument basically has been pointed out, 11 in which, however, the equation related to the model concerning concentration difference in Ref. [10] was still adopted.…”
mentioning
confidence: 99%
“…weak electrostatic coupling. To address this limitation, a number of more complex one-dimensional models have been proposed that aim to describe space-charge behaviour under non-dilute conditions [10,[14][15][16][17][18]. These models extend the simple model described above by including additional non-ideal local or non-local defect chemical potential terms.…”
mentioning
confidence: 99%