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Effects of the intercalation time on the dielectric properties of Na2xMn1?xPS3
Authors:L Silipigni  L Schirò  L Monsù Scolaro  G De Luca  G Salvato
Affiliation:1. Analiza, Inc., 3516 Superior Ave., Suite 4407B, Cleveland, OH 44114, USA;2. Department of Molecular Medicine, University of South Florida, Tampa, FL 33612, USA;3. Institute for Biological Instrumentation, Russian Academy of Sciences, 142290 Pushchino, Moscow Regions, Russia;1. Key Laboratory of Mineralogy and Metallogeny/Key Lab of Guangdong Province for Mineral Physics and Materials, Guangzhou Institute of Geochemistry, Chinese Academy of Sciences, 511 Kehua Street, Guangzhou 510640, China;2. University of Chinese Academy of Sciences, 19 Yuquan Road, Beijing 100049, China;3. School of Material Science and Engineering, Jingdezhen Ceramic Institute, Taoyang Road, Jingdezhen 333001, China;4. School of Chemistry, Physics and Mechanical Engineering, Science and Engineering Faculty, Queensland University of Technology, 2 George Street, Brisbane, QLD 4000, Australia
Abstract:Manganese thiophosphate powders have been intercalated with sodium ions at two different intercalation times (150 min and 180 min) in order to evaluate the influence of this parameter on the dielectric properties of the obtained compounds labeled like Na2xMn1?xPS3. In particular, dielectric permittivity measures have been carried out as a function of temperature (80 K–350 K) and frequency (20 Hz to 1 MHz) and compared with each other and with those of the pure matrix and of the Na2xMn1?xPS3 compound corresponding to a 120 min intercalation time. Both investigated compounds show a dielectric response characterized by a loss peak at low temperatures, by a strong dispersion at low frequency and at not very high temperatures and by a crossover frequency showing an Arrhenius temperature dependence in agreement with what already observed in Na2xMn1?xPS3 (120 min). The results have been also discussed in terms of ac conductivity, Maxwell–Wagner–Sillar (MWS) polarization, electrode polarization and dc conductivity and all the above cited features have been attributed to the Na+ ions which are, by their nature, hopping charge carriers that behave like jumping dipoles in their alternate motions and simultaneously show conducting characteristics resulting from their extended hopping over many sites. This attribution allows us to classify the analyzed sodium compounds like hopping charge carrier systems in which a greater Na intercalation time translates into a decrease in the loss peak intensity and an increase in the activation energy associated to the crossover frequency.
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