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在高密度纳米粒子系统中从个体磁性向集体磁性的转变:各向异性与偶极相互作用。

Crossover From Individual to Collective Magnetism in Dense Nanoparticle Systems: Local Anisotropy Versus Dipolar Interactions.

机构信息

Instituto Regional de Investigación Científica Aplicada (IRICA) and Departamento de Física Aplicada, Universidad de Castilla-La Mancha, Ciudad Real, 13071, Spain.

Institute of Nanoscience and Nanotechnology NCSR "Demokritos", Agia Paraskevi, 153 10, Greece.

出版信息

Small. 2022 Jul;18(28):e2106762. doi: 10.1002/smll.202106762. Epub 2022 Jun 10.

DOI:10.1002/smll.202106762
PMID:35689307
Abstract

Dense systems of magnetic nanoparticles may exhibit dipolar collective behavior. However, two fundamental questions remain unsolved: i) whether the transition temperature may be affected by the particle anisotropy or it is essentially determined by the intensity of the interparticle dipolar interactions, and ii) what is the minimum ratio of dipole-dipole interaction (E ) to nanoparticle anisotropy (K V, anisotropy⋅volume) energies necessary to crossover from individual to collective behavior. A series of particle assemblies with similarly intense dipolar interactions but widely varying anisotropy is studied. The K  is tuned through different degrees of cobalt-doping in maghemite nanoparticles, resulting in a variation of nearly an order of magnitude. All the bare particle compacts display collective behavior, except the one made with the highest anisotropy particles, which presents "marginal" features. Thus, a threshold of K V/E  ≈ 130 to suppress collective behavior is derived, in good agreement with Monte Carlo simulations. This translates into a crossover value of ≈1.7 for the easily accessible parameter T (interacting)/T (non-interacting) (ratio of the peak temperatures of the zero-field-cooled magnetization curves of interacting and dilute particle systems), which is successfully tested against the literature to predict the individual-like/collective behavior of any given interacting particle assembly comprising relatively uniform particles.

摘要

磁性纳米粒子的密集系统可能表现出偶极集体行为。然而,有两个基本问题尚未解决:i)过渡温度是否会受到粒子各向异性的影响,或者它本质上取决于粒子间偶极相互作用的强度,以及 ii)从单个到集体行为转变所需的偶极-偶极相互作用(E)与纳米粒子各向异性(K V,各向异性⋅体积)能量的最小比值是多少。研究了一系列具有类似强烈偶极相互作用但各向异性差异很大的粒子组装体。通过在磁铁矿纳米粒子中不同程度的钴掺杂来调节 K,导致变化近一个数量级。除了由具有最高各向异性的粒子制成的那个外,所有裸露的粒子压块都显示出集体行为,而后者呈现出“边缘”特征。因此,得出了一个抑制集体行为的 K V/E 阈值约为 130,这与蒙特卡罗模拟结果非常吻合。这转化为易于访问的参数 T(相互作用)/T(非相互作用)的交叉值约为 1.7(相互作用和稀疏散射粒子系统的零场冷却磁化曲线的峰值温度之比),该值成功地通过文献进行了测试,以预测任何给定的相互作用粒子组装体的个体样/集体行为,这些组装体由相对均匀的粒子组成。

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