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Interfacial magnetism and exchange coupling in BiFeO_3-CuO nanocomposite

机译:BiFeO_3-CuO纳米复合材料的界面磁性和交换耦合

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摘要

Ferromagnetic BiFeO_3 nanocrystals of average size 9 nm were used to form a composite with antiferromagnetic CuO nanosheets, with the composition (x)BiFeO_3=(100 - x)CuO, x = 0, 20, 40, 50, 60, 80 and 100. The dispersion of BiFeO_3 nanocrystals into the CuO matrix was confirmed by x-ray diffraction and transmission electron microscopy. The ferromagnetic ordering as observed in pure BiFeO_3 occurs mainly due to the reduction in the particle size as compared to the wavelength (62 nm) of the spiral modulated spin structure of the bulk BiFeO_3. Surface spin disorder of BiFeO_3 nanocrystals gives rise to an exponential behavior of magnetization with temperature. Strong magnetic exchange coupling between the BiFeO_3 nanocrystal and the CuO matrix induces an interfacial superparamagnetic phase with a blocking temperature of about 80 K. Zero field and field cooled magnetizations are analyzed by a ferromagnetic core and disordered spin shell model. The temperature dependence of the calculated saturation magnetization exhibits three magnetic contributions in three temperature regimes. The BiFeO_3/CuO nanocomposites reveal an exchange bias effect below 170 K. The maximum exchange bias field HEB is 1841 Oe for x = 50 at 5 K under field cooling of 50 kOe. The exchange bias coupling results in an increase of coercivity of 1934 Oe at 5 K. Blocked spins within an interfacial region give rise to a remarkable exchange bias effect in the nanocomposite due to strong magnetic exchange coupling between the BiFeO_3 nanocrystals and the CuO nanosheets.
机译:使用平均粒径为9 nm的铁磁BiFeO_3纳米晶体形成具有反铁磁CuO纳米片的复合材料,其成分为(x)BiFeO_3 =(100-x)CuO,x = 0、20、40、50、60、80和100。通过X射线衍射和透射电子显微镜确认了BiFeO_3纳米晶体在CuO基体中的分散。在纯BiFeO_3中观察到的铁磁排序主要是由于与块状BiFeO_3的螺旋调制自旋结构的波长(62 nm)相比,粒径减小了。 BiFeO_3纳米晶体的表面自旋无序引起了磁化随温度的指数行为。 BiFeO_3纳米晶体与CuO基质之间的强磁交换耦合诱导了一个界面超顺磁性相,其阻断温度约为80K。通过铁磁核和无序自旋壳模型分析了零磁场和场冷却磁化强度。所计算的饱和磁化强度的温度依赖性在三个温度范围内显示出三个磁贡献。 BiFeO_3 / CuO纳米复合材料显示出低于170 K的交换偏压效应。在50 kOe的磁场冷却下,在5 K下x = 50时,最大交换偏压场HEB为1841 Oe。交换偏置耦合导致在5 K下1934 Oe的矫顽力增加。​​由于BiFeO_3纳米晶体和CuO纳米片之间的强磁性交换耦合,界面区域内受阻的自旋在纳米复合材料中产生了显着的交换偏置效应。

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