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Doping effect and oxygen defects boost room temperature ferromagnetism of Co-doped ZnO nanoparticles: experimental and theoretical studies

机译:掺杂效应和氧缺陷促进Co掺杂ZnO纳米粒子的室温铁磁性:实验和理论研究

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Co-doped ZnO nanoparticles with different dosage concentrations were fabricated by a thermal decomposition method. The nanoparticles show a pure wurtzite structure without the formation of a secondary phase or Co clusters, in which Co ions present as Co ~(2+) and occupy Zn ~(2+) tetrahedral sites within the ZnO matrix. All the samples show ferromagnetic properties at room temperature with nonzero coercivity and remanence magnetization. Besides, the magnetic data is also fitted by the model of bound magnetic polarons (BMP). By increasing the Co ~(2+) doping concentration, the saturation magnetization values of Co-doped ZnO nanoparticles increase first and then decreases, which is related to the variation tendency of oxygen defects on the surface and the number of BMPs. This phenomenon can be ascribed to the formation of defect-induced BMPs, in which ferromagnetic coupling occurs at lower Co ~(2+) concentration and Co ~(2+) –O ~(2?) –Co ~(2+) antiferromagnetic coupling arises at higher Co ~(2+) concentration. Air annealing experiments further demonstrate this result, in which the saturation magnetization of Co-doped ZnO nanoparticles is reduced after annealing in Air. The doping effect and oxygen defects on the magnetic ordering of Co-doped ZnO were calculated using density functional theory. The calculation results reveal that stable long-range magnetic ordering in Co-doped ZnO nanoparticles is mainly attributed to the localized spin moments from 3d electrons of Co ~(2+) ions. Both the experimental and theoretical studies demonstrate that the ferromagnetism in Co-doped ZnO nanoparticles is originated from the combined effects of Co doping and oxygen vacancies. These results provide an experimental and theoretical view to understand the magnetic origination and tune the magnetic properties of diluted magnetic semiconductors, which is of great significance for spintronics.
机译:通过热分解法制备了不同剂量浓度的共掺杂ZnO纳米粒子。纳米粒子显示出纯纤锌矿结构,没有形成第二相或Co团簇,其中Co离子以Co〜(2+)的形式存在,并占据ZnO基体内的Zn〜(2+)四面体位点。所有样品在室温下均显示出铁磁性能,矫顽力和剩磁不为零。此外,束缚极化子(BMP)模型也拟合了磁数据。通过增加Co〜(2+)掺杂浓度,Co掺杂的ZnO纳米粒子的饱和磁化强度先增大然后减小,这与表面氧缺陷的变化趋势和BMP的数量有关。这种现象可归因于缺陷诱导的BMP的形成,其中在较低的Co〜(2+)浓度下发生铁磁耦合,而Co〜(2+)–O〜(2?)–Co〜(2+)反铁磁发生Co〜(2+)浓度较高时会发生偶联。空气退火实验进一步证明了这一结果,其中在空气中退火后,Co掺杂的ZnO纳米颗粒的饱和磁化强度降低了。利用密度泛函理论计算了Co掺杂ZnO的磁有序化过程中的掺杂效应和氧缺陷。计算结果表明,Co掺杂的ZnO纳米颗粒中稳定的远距离磁有序主要归因于Co〜(2+)离子的3d电子的局部自旋矩。实验和理论研究均表明,Co掺杂的ZnO纳米粒子中的铁磁性源自Co掺杂和氧空位的组合效应。这些结果提供了实验和理论观点,以了解磁性起源和调整稀磁半导体的磁性能,这对自旋电子学具有重要意义。

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