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Low-temperature dynamics of magnetic colloids studied by time-resolved small-angle neutron scattering

机译:时间分辨小角中子散射研究磁性胶体的低温动力学

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The dynamics of ordering and relaxation processes in magnetic colloids has been studied by means of stroboscopic small angle neutron scattering techniques in an oscillating magnetic field. Surfactant stabilized ferrofluids (FFs) of Fe_3O_4 and Co nanoparticles have been investigated as a function of temperature and frequency and compared to a solid Cu alloy with 0.8 vol % Co precipitates. This technique allowed elucidating the dynamical nature of the locally ordered domains in both ferrofluids as "living objects" becoming arrested below the freezing temperature of the solvent. The time-dependent intensities have been analyzed in terms of Langevin statistics including dynamical interparticle structure factors, which scale with the square of the Langevin function. The local ordering is mainly determined by the effective dipole-dipole interaction, which is enhanced by the partial alignment of the particle moments in an external magnetic field. Starting from the frozen state, the amount of freely rotating particle moments increases continuously with increasing temperature. The dynamical structure factors describing the hexagonal (Fe_3O_4-FF) or chainlike (Co-FF) ordering reach a maximum around the melting temperature. The alignment of particle moments along the applied field is governed by the fast Brownian rotation of individual nanoparticles and small aggregates, while the magnetic relaxation of longer dipolar chains and local hexagonal domains is much slower. In contrast, no field-induced interparticle correlations occur in the diluted solid CuCo alloy where the moment relaxation is purely of fast Neel type, which-due to a low anisotropy constant-follows the oscillating field at all temperatures.
机译:利用频闪小角度中子散射技术在振荡磁场中研究了磁性胶体中有序和弛豫过程的动力学。已经研究了Fe_3O_4和Co纳米颗粒的表面活性剂稳定的铁磁流体(FFs)作为温度和频率的函数,并将其与具有0.8 vol%Co沉淀的固态Cu合金进行了比较。该技术可以阐明两种铁磁流体中的局部有序域的动力学性质,因为“活体”在溶剂的冷冻温度以下被捕。随时间变化的强度已根据Langevin统计数据进行了分析,包括动态粒子间结构因子,这些因子与Langevin函数的平方成比例。局部有序主要由有效的偶极-偶极相互作用确定,该相互作用通过外部磁场中粒子矩的局部对准而增强。从冻结状态开始,自由旋转的颗粒力矩随温度升高而连续增加。描述六角形(Fe_3O_4-FF)或链状(Co-FF)有序的动力学结构因子在熔化温度附近达到最大值。粒子力矩沿外加磁场的排列方式受单个纳米粒子和小聚集体快速布朗旋转的支配,而较长的偶极链和局部六角形畴的磁弛豫要慢得多。相比之下,在稀疏的固态CuCo合金中,没有矩引起的粒子间相关性,在矩型弛豫纯粹是快速Neel型的情况下,由于各向异性常数低,因此在所有温度下都遵循振荡场。

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