Abstract

Solid-state ferrimagnetic MFe $_{2}$ O $_{4}$ (M = Mg, Ni, Co; mean diameter size $d$ = 30–35 nm) and superparamagnetic MFe $_{2}$ O $_{4}$ (M = Mg, Ni, Mn $_{0.5}$ Zn $_{0.5}$ ; $d$ = 6–8 nm) nanoparticles [ferromagnetic nanoparticles (FMNPs) and superparamagnetic nanoparticles (SPNPs)] were used to explore the physical mechanisms of ac magnetically induced heating and identify what physical parameters would be the most critical to enhance the ac magnetically induced heating power for local in vivo hyperthermia agent applications. It was experimentally confirmed that “dc (minor) hysteresis loss power” generated by the magnetization reversal process, and “Neel relaxation loss power” generated by fluctuation of the magnetic moment dominantly contribute to the ac heat generation of FMNPs and SPNPs, respectively. In addition, all the experimentally and physically analyzed results demonstrated that the improvement of in-phase magnetic susceptibility $\chi^\prime _m$ is directly relevant to the “dc (minor) hysteresis loss power” as well as the dc magnetic softness, and the out-of-phase magnetic susceptibility $\chi^{\prime \prime} _m$ is directly relevant to the “Neel relaxation loss power (or ac magnetic hysteresis loss power, A )” as well as the ac magnetic softness are the most crucial physical parameters responsible for enhancing the ac magnetically induced heating power of solid-state FMNPs and SPNPs, respectively. Particularly, some technical and engineering approaches, which can improve the $\chi^\prime _m$ of FMNPs and the $\chi^{\prime \prime} _m$ of SPNPs, were proposed and introduced in this study to provide crucial information how to effectively design and develop a new promising hyperthermia agent in nanomedicine.

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