2002
DOI: 10.1039/b200122p
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Ionic motion in materials with disordered structures: conductivity spectra and the concept of mismatch and relaxation

Abstract: Ionic transport in 0.2[XNa 2 OÁ(1ÀX)Rb 2 O]Á0.8B 2 O 3 mixed-alkali glasses A ´rpa ´d W. Imre, Stephan Voss and Helmut Mehrer 3225 Diffusion of calcium and barium in alkali alkaline-earth silicate glasses

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Cited by 123 publications
(186 citation statements)
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“…1 [10,18]. In most ion conducting materials with disordered structures, the scaled ionic conductivity, σ S = σ/σ DC , when measured in the impedance regime at different temperatures, is found to be a unique function of scaled angular frequency, ω S = ω/ω O .…”
Section: Introductionmentioning
confidence: 99%
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“…1 [10,18]. In most ion conducting materials with disordered structures, the scaled ionic conductivity, σ S = σ/σ DC , when measured in the impedance regime at different temperatures, is found to be a unique function of scaled angular frequency, ω S = ω/ω O .…”
Section: Introductionmentioning
confidence: 99%
“…As ionic conduction is facilitated by structural disorder, these materials generally belong to level three. The striking difference between ion conductors [10,18]. Here, σ (0) ≡ σ DC .…”
Section: Introductionmentioning
confidence: 99%
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“…As has been documented for many disordered solid electrolytes [11,13,20], experimental data of ionic conductivities due to hopping processes, including their dependence on both frequency and temperature, are generally well reproduced by the MIGRATION concept. This includes in particular the master curve presented in Fig.…”
Section: Separating the Two Universalities From Each Othermentioning
confidence: 57%
“…[13]. [10,11]) is characteristic of many disordered ion conductors which broadly differ in phase, structure and composition. The solid line is obtained from our model, see below .…”
Section: Separating the Two Universalities From Each Othermentioning
confidence: 99%