J. Othmani, S. Hcini, J. Massoudi, M. L. Bouazizi, A. Dhahri, K. Khirouni, E. Dhahri
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引用次数: 0
Abstract
The compound Co0.33Mn0.33Fe2.33O4, synthesized by coprecipitation, crystallizes in a well-defined spinel structure belonging to the Fd \(\overline{3 }\) m space group. Increasing the annealing temperature leads to an improvement in crystallinity, as shown by the increase in average crystallite size from 28 to 32 nm. The study of conductivity in the DC regime reveals a metal–semiconductor transition around 420 K for the sample annealed at 300 °C (Co300). This transition disappears after annealing at 600 °C (Co600), indicating a reduction in active traps at low temperature. This conductivity follows a small polaron hopping mechanism, with a high activation energy increasing from 1.29 to 1.34 eV at high temperature. For the Co600 compound, in the AC regime, the activation energy at high temperature remains comparable to that found in the DC regime, with a strong decrease at low temperature (0.29 → 0.14 eV) as frequency increases, highlighting the role of disorder energy (ED). Frequency analysis reveals that ED decreases with frequency, while the hopping energy (EH) increases, suggesting an increase in the polaron radius. The application of the scaling model combines the conductivity spectra into a master curve, validating the time–temperature superposition principle, although divergences appear at high frequency compared to Summerfield’s theory. Introducing a temperature-dependent scaling parameter significantly improves the coalescence. The high values of the temperature coefficient of resistance (TCR), reaching − 30% (Co300) and − 13.8% (Co600), confirm the bolometric potential of the material. Finally, impedance spectroscopy reveals thermally activated relaxation, with activation energies of 778 meV (Co300), 576 meV (high T), and 103 meV (low T) for Co600. Nyquist diagrams show the contribution of grains, grain boundaries, and electrodes to the overall mechanism. These results open promising perspectives for optimizing the material via dopant introduction, control of iron excess, and thin-film development by spray pyrolysis, aiming at electronic and next-generation sensor applications.
通过共沉淀法合成的化合物Co0.33Mn0.33Fe2.33O4结晶为清晰的尖晶石结构,属于Fd \(\overline{3 }\) m空间群。退火温度的升高导致结晶度的提高,平均晶粒尺寸从28 nm增加到32 nm。研究表明,在300°C (Co300)下退火的样品在420 K左右发生了金属-半导体转变。在600°C (Co600)退火后,这种转变消失,表明在低温下活性陷阱减少。这种电导率遵循一个小的极化子跳变机制,高温下活化能从1.29 eV增加到1.34 eV。对于Co600化合物,在交流环境下,高温活化能与直流环境下的活化能相当,随着频率的增加,低温活化能明显下降(0.29→0.14 eV),突出了无序能(ED)的作用。频率分析表明,极化子半径随频率的增加而增大,而跃迁能随频率的增加而减小。标度模型的应用将电导率谱结合成一条主曲线,验证了时间-温度叠加原理,尽管与Summerfield的理论相比,发散出现在高频。引入温度相关的结垢参数可显著改善结垢效果。电阻温度系数(TCR)偏高,达到−30% (Co300) and − 13.8% (Co600), confirm the bolometric potential of the material. Finally, impedance spectroscopy reveals thermally activated relaxation, with activation energies of 778 meV (Co300), 576 meV (high T), and 103 meV (low T) for Co600. Nyquist diagrams show the contribution of grains, grain boundaries, and electrodes to the overall mechanism. These results open promising perspectives for optimizing the material via dopant introduction, control of iron excess, and thin-film development by spray pyrolysis, aiming at electronic and next-generation sensor applications.
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