Peculiarities of ionic transport in LLTO solid electrolytes

The Li3xLa2/3–xTiO3 (LLTO) (x = 0.1 Li+) ionic conductor was investigated by microwave spectrometer set‐up in the 106–109 Hz frequency range and by time‐domain transmission terahertz spectrometer in the 2·1011–3·1012 Hz frequency range. A relaxation dispersion of $ \tilde \sigma $ and $ \tilde \epsi...

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Veröffentlicht in:Physica status solidi. C 2009-12, Vol.6 (12), p.2756-2758
Hauptverfasser: Šalkus, Tomas, Bohnke, Odile, Macutkevic, Jan, Orliukas, Antanas Feliksas, Greičius, Simonas, Kezionis, Algimantas, Krotkus, Arūnas, Suzanovičienė, Rasa, Adomavičius, Ramūnas
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container_title Physica status solidi. C
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creator Šalkus, Tomas
Bohnke, Odile
Macutkevic, Jan
Orliukas, Antanas Feliksas
Greičius, Simonas
Kezionis, Algimantas
Krotkus, Arūnas
Suzanovičienė, Rasa
Adomavičius, Ramūnas
description The Li3xLa2/3–xTiO3 (LLTO) (x = 0.1 Li+) ionic conductor was investigated by microwave spectrometer set‐up in the 106–109 Hz frequency range and by time‐domain transmission terahertz spectrometer in the 2·1011–3·1012 Hz frequency range. A relaxation dispersion of $ \tilde \sigma $ and $ \tilde \epsilon $ of LLTO ceramics was found in the microwave region and was attributed to the Li+ relaxation in bulk. The resonance dispersion of $ \tilde \sigma $ and $ \tilde \epsilon $ was found in the terahertz region with resonance frequency ω0. The value of ω0 correlates well with the value of attempt frequency f0, found from the Arrhenius plot of the relaxation frequency fR. (© 2009 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim)
doi_str_mv 10.1002/pssc.200982527
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source Wiley Online Library Journals Frontfile Complete
subjects 63.20−e
66.30.Dn
77.22.−d
77.84.Dy
81.70.Fy
84.37.+q
Ceramics
Dispersions
Frequency ranges
Microwave spectrometers
Microwaves
Reproduction
Solid electrolytes
Solid state physics
title Peculiarities of ionic transport in LLTO solid electrolytes
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