Abstract

Understanding magnetic interparticle interactions within a single hydrodynamic volume of polydispersed magnetic nanoparticles and the resulting nonlinear magnetization properties is critical for their implementation in magnetic theranostics. However, in general, the field-dependent static and dynamic magnetization measurements may only highlight polydispersity effects including magnetic moment and size distributions. Therefore, as a complement to such typical analysis of hysteretic magnetization curves, we spectroscopically examined the complex magnetization harmonics of magnetic nanoclusters either dispersed in a liquid medium or immobilized by a hydrocolloid polymer, later to emphasize the harmonic characteristics for different core sizes. In the case of superparamagnetic nanoclusters with a 4-nm primary size, particularly, we correlated the negative quadrature components of the third-harmonic susceptibility with an insignificant cluster rotation induced by the oscillatory field. Moreover, the field-dependent in-phase components appear to be frequency-independent, suggesting a weak damping effect on the moment dynamics. The characteristic of the Néel time constant further supports this argument by showing a smaller dependence on the applied dc bias field, in comparison to that of larger cores. These findings show that the complex harmonic components of the magnetization are important attributes to the interacting cores of a magnetic nanocluster.

Highlights

  • Superparamagnetism of magnetic nanostructures has been one of the main concepts underlining recent theranostic applications [1,2]

  • We confirm that the immobilized carboxymethyl-diethylaminoethyl dextran (CMEAD)-γFe2O3 nanoclusters have similar dynamic magnetization curves to those dispersed in water

  • Magnetic interparticle interactions contribute to changing the nonlinear properties of the dynamic magnetization and highlight the field-induced particle rotation of polydispersive magnetic nanoclusters as one of the crucial factors

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Summary

Introduction

Superparamagnetism of magnetic nanostructures has been one of the main concepts underlining recent theranostic applications [1,2] This property is well understood as a physical manifestation of the dynamic behavior of a macrospin system above its blocking temperature, which results in a non-hysteretic magnetization curve against a periodically ramped magnetic field at extremely low frequencies [3,4]. The resulting heat dissipation and magnetic signals are promising for magnetic hyperthermia, particle imaging, and biosensing [9,10,11]. These applications substantially demand a good understanding of colloidal magnetic nanostructures and their nonlinear magnetization dynamics to acquire high hyperthermic efficiency and nonlinear magnetization at low-field regimes

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