Experimental Investigations of the AC-Conductivity in NaTaO<sub>3</sub> Ceramic Materials Doped with Cu and Al Metal Ions

Two ceramic samples of sodium tantalate (NaTaO<sub>3</sub>), doped with metal ions of copper (Cu; sample S1) or aluminum (Al; sample S2), were obtained by the sol-gel method. Complex impedance measurements in the frequency range (200 Hz–2 MHz) and at temperatures between 30 °C and 90 °C...

وصف كامل

التفاصيل البيبلوغرافية
الحاوية / القاعدة:Metals
المؤلفون الرئيسيون: Iosif Malaescu, Paula Sfirloaga, Catalin Nicolae Marin
التنسيق: مقال
اللغة:الإنجليزية
منشور في: MDPI AG 2024-07-01
الموضوعات:
الوصول للمادة أونلاين:https://www.mdpi.com/2075-4701/14/7/793
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author Iosif Malaescu
Paula Sfirloaga
Catalin Nicolae Marin
author_facet Iosif Malaescu
Paula Sfirloaga
Catalin Nicolae Marin
author_sort Iosif Malaescu
collection DOAJ
container_title Metals
description Two ceramic samples of sodium tantalate (NaTaO<sub>3</sub>), doped with metal ions of copper (Cu; sample S1) or aluminum (Al; sample S2), were obtained by the sol-gel method. Complex impedance measurements in the frequency range (200 Hz–2 MHz) and at temperatures between 30 °C and 90 °C allowed identification of a transition temperature from semiconductor-type behavior to conductor-type behavior for each sample (52 °C for sample S1 and 54 °C for sample S2). In the temperature range with semiconductor behavior, the activation energy of each sample was determined. Based on the Mott’s variable-range hopping (VRH) model, the density of localized states at the Fermi level, N(E<sub>F</sub>), the hopping distance (R) and the hopping energy (W) were determined, for the first time, on NaTaO<sub>3</sub> samples doped with Cu or Al metal ions. The increase in N(E<sub>F</sub>) of sample S2 compared to N(E<sub>F</sub>) of sample S1 was explained by the decrease in the hopping distance of charge carriers in sample S2 compared to that in sample S1. Additionally, using the correlated barrier hopping (CBH) model, the energy band gap (W<sub>m</sub>) and the hopping (crossover) frequency (ω<sub>h</sub>) at various temperatures were determined. Knowledge of these electrical properties is very important for explaining the electrical conduction mechanisms in metal ion-doped compounds, with perovskite structure being of interest for the use of these materials in the conversion of thermoelectric energy, photocatalytic applications, electronics or other applications.
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spelling doaj-art-aa46cb886e7e4dddb04e7c574d9bf0d32025-08-20T00:47:18ZengMDPI AGMetals2075-47012024-07-0114779310.3390/met14070793Experimental Investigations of the AC-Conductivity in NaTaO<sub>3</sub> Ceramic Materials Doped with Cu and Al Metal IonsIosif Malaescu0Paula Sfirloaga1Catalin Nicolae Marin2Faculty of Physics, West University of Timisoara, Bd. V. Parvan No. 4, 300223 Timisoara, RomaniaNational Institute of Research and Development for Electrochemistry and Condensed Matter, 144 Dr. A. P. Podeanu, 300569 Timisoara, RomaniaFaculty of Physics, West University of Timisoara, Bd. V. Parvan No. 4, 300223 Timisoara, RomaniaTwo ceramic samples of sodium tantalate (NaTaO<sub>3</sub>), doped with metal ions of copper (Cu; sample S1) or aluminum (Al; sample S2), were obtained by the sol-gel method. Complex impedance measurements in the frequency range (200 Hz–2 MHz) and at temperatures between 30 °C and 90 °C allowed identification of a transition temperature from semiconductor-type behavior to conductor-type behavior for each sample (52 °C for sample S1 and 54 °C for sample S2). In the temperature range with semiconductor behavior, the activation energy of each sample was determined. Based on the Mott’s variable-range hopping (VRH) model, the density of localized states at the Fermi level, N(E<sub>F</sub>), the hopping distance (R) and the hopping energy (W) were determined, for the first time, on NaTaO<sub>3</sub> samples doped with Cu or Al metal ions. The increase in N(E<sub>F</sub>) of sample S2 compared to N(E<sub>F</sub>) of sample S1 was explained by the decrease in the hopping distance of charge carriers in sample S2 compared to that in sample S1. Additionally, using the correlated barrier hopping (CBH) model, the energy band gap (W<sub>m</sub>) and the hopping (crossover) frequency (ω<sub>h</sub>) at various temperatures were determined. Knowledge of these electrical properties is very important for explaining the electrical conduction mechanisms in metal ion-doped compounds, with perovskite structure being of interest for the use of these materials in the conversion of thermoelectric energy, photocatalytic applications, electronics or other applications.https://www.mdpi.com/2075-4701/14/7/793sodium tantalateperovskitescomplex impedance measurementsDC and AC conductivityVRH and CBH theoretical models
spellingShingle Iosif Malaescu
Paula Sfirloaga
Catalin Nicolae Marin
Experimental Investigations of the AC-Conductivity in NaTaO<sub>3</sub> Ceramic Materials Doped with Cu and Al Metal Ions
sodium tantalate
perovskites
complex impedance measurements
DC and AC conductivity
VRH and CBH theoretical models
title Experimental Investigations of the AC-Conductivity in NaTaO<sub>3</sub> Ceramic Materials Doped with Cu and Al Metal Ions
title_full Experimental Investigations of the AC-Conductivity in NaTaO<sub>3</sub> Ceramic Materials Doped with Cu and Al Metal Ions
title_fullStr Experimental Investigations of the AC-Conductivity in NaTaO<sub>3</sub> Ceramic Materials Doped with Cu and Al Metal Ions
title_full_unstemmed Experimental Investigations of the AC-Conductivity in NaTaO<sub>3</sub> Ceramic Materials Doped with Cu and Al Metal Ions
title_short Experimental Investigations of the AC-Conductivity in NaTaO<sub>3</sub> Ceramic Materials Doped with Cu and Al Metal Ions
title_sort experimental investigations of the ac conductivity in natao sub 3 sub ceramic materials doped with cu and al metal ions
topic sodium tantalate
perovskites
complex impedance measurements
DC and AC conductivity
VRH and CBH theoretical models
url https://www.mdpi.com/2075-4701/14/7/793
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AT paulasfirloaga experimentalinvestigationsoftheacconductivityinnataosub3subceramicmaterialsdopedwithcuandalmetalions
AT catalinnicolaemarin experimentalinvestigationsoftheacconductivityinnataosub3subceramicmaterialsdopedwithcuandalmetalions