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弱相互作用和强相互作用钴铁氧体基纳米颗粒的阻塞和剩磁特性

Blocking and remanence properties of weakly and highly interactive cobalt ferrite based nanoparticles.

作者信息

Vieira C A M, Gomes R Cabreira, Silva F G, Dias A L, Aquino R, Campos A F C, Depeyrot J

机构信息

Complex Fluids Group, Instituto de Física, Universidade de Brasília, Caixa Postal 04455, 70919-970, Brasília (DF), Brazil.

出版信息

J Phys Condens Matter. 2019 May 1;31(17):175801. doi: 10.1088/1361-648X/ab0353. Epub 2019 Jan 30.

Abstract

We compare both magnetic blocking properties and remanence curves for dilute ferrofluid and powder samples of ferrite magnetic nanoparticles. Low field DC magnetization, AC susceptibility, isothermal remanent magnetization and DC demagnetization techniques are employed to investigate the role of interparticle magnetic interactions on the superparamagnetic relaxation, the magnetic anisotropy and on the super-spin-glass state in closely packed particles. The samples used herein are 3 nm sized spinel-type nanocrystals made of a cobalt ferrite core covered by a layer of maghemite on its outermost surface and can be obtained as aqueous colloidal dispersions thanks to this core-shell strategy. They show large anisotropy attributed to an enhanced surface contribution and the blocking temperature is shifted towards higher values as interparticle distance decreases. For all investigated diluted liquids and powder samples the frequency dependency of the peak temperature is well accounted by a Vogel-Fulcher law, with the insertion of a phenomenological temperature associated to the magnitude of interparticle dipolar interactions. The fractional change of the peak temperature per decade of frequency enlights the presence of interactions between particles in dilute liquids and of a spin-glass-like state in powder samples. The remanence curves always show global demagnetizing behavior, attributed to the combination of both spin surface disorder and interparticle dipolar interactions, the former being predominant in isolated nanoparticles and the latter in powder samples. However, in the most compacted powder, exchange interaction between surface ions of different particles becomes more pronounced and promotes an additive magnetizing effect.

摘要

我们比较了稀磁流体和铁氧体磁性纳米颗粒粉末样品的磁阻塞特性和剩磁曲线。采用低场直流磁化、交流磁化率、等温剩磁磁化和直流退磁技术,研究了颗粒间磁相互作用对超顺磁弛豫、磁各向异性以及紧密堆积颗粒中超自旋玻璃态的作用。本文使用的样品是尺寸为3纳米的尖晶石型纳米晶体,由钴铁氧体核组成,其最外层表面覆盖有一层磁赤铁矿,由于这种核壳策略,可以制成水性胶体分散体。它们表现出较大的各向异性,这归因于表面贡献的增强,并且随着颗粒间距离的减小,阻塞温度向更高值移动。对于所有研究的稀释液体和粉末样品,峰值温度的频率依赖性可以很好地用Vogel-Fulcher定律来解释,并引入了一个与颗粒间偶极相互作用大小相关的唯象温度。每十倍频率下峰值温度的分数变化揭示了稀释液体中颗粒间相互作用的存在以及粉末样品中类似自旋玻璃态的存在。剩磁曲线总是呈现出整体退磁行为,这归因于自旋表面无序和颗粒间偶极相互作用的共同作用,前者在孤立的纳米颗粒中占主导,后者在粉末样品中占主导。然而,在最致密的粉末中,不同颗粒表面离子之间的交换相互作用变得更加明显,并促进了附加磁化效应。

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