闭锁温度以上 Fe3O4 纳米粒子磁化数据建模

Navneet Kaur
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摘要

采用简单的共沉淀法制备了纳米 Fe3O4 粒子。使用 X 射线衍射仪、透射电子显微镜和振动样品磁力计对样品进行了表征。样品的 X 射线衍射图样清楚地表明它是单相磁铁矿。透射电子显微镜照片显示,样品的粒度分布较窄,平均粒度为 9.9 纳米。SAED 图样只显示了与磁铁矿相对应的衍射平面,没有检测到其他相杂质。由于粒度减小,磁性无序壳的计算厚度为 1.7 nm。样品的磁化测量是温度和外加磁场的函数。在 250 Oe 的外加磁场下测量了样品的零场冷却曲线和场冷却曲线,两条曲线都在 170 K 分叉。零场曲线中的峰值表明样品的阻挡温度约为 100 K。这些磁化数据用于拟合分析 Fe3O4 纳米粒子的磁性行为。.纳米粒子系统的磁化受多种因素影响,如粒度分布、无序表面、磁晶各向异性、磁矩分布和磁相互作用。在分析磁化数据时,如果忽略了这些因素,就会导致结果出现偏差。表面效应对颗粒尺寸的减小很敏感,导致表面自旋受挫,形成磁性无序层,从而影响纳米颗粒的磁性行为。这项研究用适当的磁化表达式分析了磁化数据,其中考虑到了磁矩分布的影响。磁矩分布对磁化分析有重大影响,并受磁性无序表面的影响,这说明粒子表面存在磁各向异性和磁相互作用。本文详细讨论了研究结果和观察结果。
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Modelling the magnetization data of Fe3O4 nanoparticles above blocking temperature
Nanoparticles of Fe3O4 are prepared by simple co-precipitation method. The sample is characterized using an x-ray diffractometer, transmission electron microscope, and vibrating sample magnetometer. The x-ray diffraction pattern of the sample clearly shows that it is a single-phase magnetite. The transmission electron micrograph shows that the sample has a narrow distribution in particle size with average particle size of 9.9 nm. The SAED pattern only shows the diffraction planes correspond to magnetite and no other phase impurity is detected. The calculated thickness of the magnetic disordered shell due to the reduction in particle size is found to be 1.7 nm. The magnetization of the sample is measured as a function of temperature and applied magnetic field. The zero-field cooled and field cooled curves of the sample are measured in the presence of 250 Oe applied magnetic field and both the curves bifurcate at 170 K. The peak in the zero-field curve indicates that the sample has a blocking temperature of around 100 K. The magnetization as a function of applied magnetic field data at 200, 225, 250, 275 and 300 K are measured (up to ±20 kOe). These magnetization data are used for the fitting to analyze the magnetic behavior of Fe3O4 nanoparticles. . The magnetization of nanoparticles systems is influenced by several factors such as particle size distribution, disordered surface, magnetocrystalline anisotropy, magnetic moment distribution and magnetic interactions. The ignorance of such factors while analyzing the magnetization data leads to discrepancies in the results. The surface effects are sensitive to the reduction in particle size leading to the spin frustrations on the surface suggesting a magnetic disordered layer which affect the magnetic behavior of nanoparticles. This work presents the analysis of the magnetization data in an appropriate magnetization expression which takes into consideration the effect of magnetic moment distribution. This distribution in the magnetic moment is found to be significantly influenced the magnetization analysis and affected by the magnetic disordered surface which accounts for the presence of magnetic anisotropy and magnetic interactions on the particles surface. The results and observations are discussed in detail.
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