首页> 外文期刊>Journal of magnetism and magnetic materials >Exchange-coupling of hard and soft magnetic sublattices and magnetic anomalies in mixed spinel NiFe_(0.75)Cr_(1.25)O_4 nanoparticles
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Exchange-coupling of hard and soft magnetic sublattices and magnetic anomalies in mixed spinel NiFe_(0.75)Cr_(1.25)O_4 nanoparticles

机译:NiFe_(0.75)Cr_(1.25)O_4混合尖晶石中硬磁和软磁亚晶格的交换耦合和磁异常

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摘要

A set of single-crystalline nanoparticles (NPs) of nickel-chromium ferrite NiFe0.75Cr1.25O4with a cubic spinel structure were synthesized and investigated. The NPs size can be varied from about 5 to 50 nm by the final annealing of the precursor at different temperatures. The distribution of cations over the tetrahedral (A) and the octahedral [B] sites (Fe0.75Ni0.25) [Ni0.75Cr1.25] O4was established from the magnetic and Mössbauer measurements. In large NPs, the magnetic structure at low temperatures is close to the collinear antiferromagnetic (AFM) structure of the Neel type; and the total magnetic momentMtotof the ferrite coincides with the direction of the B-sublattice moment. Several size-dependent magnetic anomalies were revealed. Three types of magnetic ions present in the A- and B- sublattices cause the competition of AFM and FM exchange interactions resulting in the highly frustrated magnetic ordering and the occurrence of canted magnetic structure in the octahedral B-sublattice. The frustrated structure is very flexible and significantly subjected to temperature and applied field. It results in several magnetic anomalies observed, including the occurrence of magnetic compensation, abnormal behavior of ZFC and FC magnetization curves and hysteresis loops. It was shown that magnetic anomalies can be explained in terms of exchange coupling of “soft” and “hard” magnetic B- and A-sublattices. This effect in the (Fe0.75Ni0.25) [Ni0.75Cr1.25] O4NPs can be considered as anatomic-scale analogof a similar effect observed in two-phase exchange-coupled alloys developed for permanent magnets and for the perpendicular recoding media.
机译:合成并研究了一组具有立方尖晶石结构的镍铬铁氧体NiFe0.75Cr1.25O4的单晶纳米颗粒。通过在不同温度下对前驱体进行最终退火,NP尺寸可在约5至50 nm之间变化。通过磁性和穆斯堡尔测量法确定了阳离子在四面体(A)和八面体[B](Fe0.75Ni0.25)[Ni0.75Cr1.25] O4上的分布。在大型NP中,低温下的磁性结构接近Neel型的共线反铁磁性(AFM)结构。铁氧体的总磁矩Mtotof与B亚晶格矩的方向一致。揭示了几个尺寸相关的磁异常。存在于A-和B-亚晶格中的三种类型的磁离子引起AFM和FM交换相互作用的竞争,从而导致高度受挫的磁序和八面体B-亚晶格中倾斜的磁性结构的出现。挫折的结构非常柔软,并且显着经受温度和施加的电场的影响。它导致观察到多个磁异常,包括磁补偿的发生,ZFC和FC磁化曲线的异常行为以及磁滞回线。结果表明,磁异常可以用“软”和“硬”磁B和A子晶格的交换耦合来解释。 (Fe0.75Ni0.25)[Ni0.75Cr1.25] O4NPs中的这种作用可被视为解剖学尺度的类似物,类似于在为永磁体和垂直记录介质开发的两相交换耦合合金中观察到的类似作用。

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