Poperechny I S
Institute of Continuous Media Mechanics, Russian Academy of Sciences, Ural Branch, Perm 614018, Russia and Perm State National Research University, Perm 614068, Russia.
Phys Rev E. 2024 Apr;109(4-1):044601. doi: 10.1103/PhysRevE.109.044601.
Within a kinetic theory, the linear magnetic response of uniaxial single-domain particles suspended in a fluid is analyzed. The main qualitatively different types of frequency dependence of the longitudinal dynamic magnetic susceptibility of such particles are described. It is shown that superparamagnetic (related to orientation thermal fluctuations of the magnetic moment inside a particle) peculiarities of the response of a particle to a probing magnetic field are not fully determined by the ratio of anisotropy energy to thermal energy when a stationary bias field is applied. For a case where the indicated ratio is much greater than one, a simple approximate expression for the dynamic magnetic susceptibility of a particle is proposed. The developed approach is extended to polydisperse suspensions of noninteracting uniaxial nanoparticles. It is shown that polydispersity does not vanish away specific superparamagnetic features in the dynamic magnetic response of such systems. Quantitative estimates of the corresponding effects are performed in different frequency ranges of the applied field. It is demonstrated that under certain restrictions on the disperse composition of a suspension, the internal diffusion of the magnetic moment can lead to a splitting of the absorption spectrum of the system. The significant role of the bias field is revealed. In particular, it can cause an additional absorption maximum provided the particle-size distribution meets the outlined condition. Also, it enables one to assess how important it is to take into account superparamagnetism of particles: the effect of the biasing is stronger for particles with smaller anisotropy and thereby more pronounced superparamagnetic properties. A qualitative agreement of some of the inferences with the experimental data is briefly discussed.
在动力学理论框架内,分析了悬浮在流体中的单轴单畴颗粒的线性磁响应。描述了此类颗粒纵向动态磁化率频率依赖性的主要定性不同类型。结果表明,当施加静态偏置场时,颗粒对探测磁场响应的超顺磁性(与颗粒内部磁矩的取向热涨落有关)特性并非完全由各向异性能量与热能之比决定。对于该比值远大于1的情况,提出了颗粒动态磁化率的一个简单近似表达式。所发展的方法扩展到了非相互作用单轴纳米颗粒的多分散悬浮液。结果表明,多分散性并不会消除此类系统动态磁响应中特定的超顺磁特征。在施加场的不同频率范围内对相应效应进行了定量估计。结果表明,在对悬浮液分散组成的某些限制条件下,磁矩的内部扩散会导致系统吸收光谱的分裂。揭示了偏置场的重要作用。特别是,如果颗粒尺寸分布满足所述条件,它会导致额外的吸收峰。此外,它还能让人评估考虑颗粒超顺磁性的重要程度:对于各向异性较小从而超顺磁特性更明显的颗粒,偏置效应更强。简要讨论了一些推断与实验数据的定性一致性。