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Review
. 2021 Jan 15;3(4):867-888.
doi: 10.1039/d0na00828a. eCollection 2021 Feb 23.

Hybrid magnetic nanoparticles as efficient nanoheaters in biomedical applications

Affiliations
Review

Hybrid magnetic nanoparticles as efficient nanoheaters in biomedical applications

Gabriel C Lavorato et al. Nanoscale Adv. .

Abstract

Heating at the nanoscale is the basis of several biomedical applications, including magnetic hyperthermia therapies and heat-triggered drug delivery. The combination of multiple inorganic materials in hybrid magnetic nanoparticles provides versatile platforms to achieve an efficient heat delivery upon different external stimuli or to get an optical feedback during the process. However, the successful design and application of these nanomaterials usually require intricate synthesis routes and their magnetic response is still not fully understood. In this review we give an overview of the novel systems reported in the last few years, which have been mostly obtained by organic phase-based synthesis and epitaxial growth processes. Since the heating efficiency of hybrid magnetic nanoparticles often relies on the exchange-interaction between their components, we discuss various interface-phenomena that are responsible for their magnetic properties. Finally, followed by a brief comment on future directions in the field, we outline recent advances on multifunctional nanoparticles that can boost the heating power with light and combine heating and temperature sensing in a single nanomaterial.

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Conflict of interest statement

There are no conflicts to declare.

Figures

Fig. 1
Fig. 1. (A) Design of multigrain Mn3O4 shells grown on Co3O4 nanocubes. The upper panel shows the orientation relationship between the cubic core and the tetragonal shell by mapping the outer (green) and inner (red) spots of the FFT region (indicated by a purple square) obtained from the associated HAADF-STEM image. The lower panel summarizes the grain boundaries between adjacent Mn3O4 grains with a misorientation angle of ∼8.4°. Adapted with permission from Nature, ref. , Copyright 2020 Nature (B) high-resolution TEM and STEM-EELS elemental mapping images confirm a coherent interface between Fe3O4 and CoFe2O4 in core/shell hybrid nanoparticles. Adapted with permission from ref. , Copyright 2020 American Chemical Society (C) evolution from metal Fe to Fe/Fe-oxide core/shell and Fe-oxide hollow nanoparticles and associated TEM images. Adapted with permission from ref. , Copyright 2016 Royal Society of Chemistry (D) TEM image of Janus Fe-oxide-Au nanostars. Adapted with permission from ref. , Copyright 2020 Wiley-VCH (E) TEM image and EDS elemental mapping of Ag/Fe3O4 nanoflowers. Adapted with permission from ref. , Copyright 2016 American Chemical Society.
Fig. 2
Fig. 2. (A) Comparison between DC and AC hysteresis loops for superparamagnetic nanoparticles. The relevant parameters defining the hysteresis losses (Ms, HC, and MR) have been explicitly indicated (B) electron cryotomography image of the chain of magnetosomes of M. gryphiswaldense and experimental and simulated AC hysteresis loops measured at 500 kHz for bacteria dispersed in water (25 °C). Reproduced from ref. and under a Creative Commons (CC BY 3.0) License. (C) 2D schematic representation of the different regions in a FM/FIM core/shell spherical nanoparticle, and SAR of core/shell hybrid nanoparticles with different shapes: spherical (black), cubic (red), octahedral (green), and truncated cuboctahedral (blue), and size distributions: log-normal size distribution (solid lines) and uniform particle size (dotted lines). Adapted from ref. with permission from The Royal Society of Chemistry.
Fig. 3
Fig. 3. (A) Cation-inversion gradient in the shell of a Mn3O4 domain grown on Fe3O4 nanoparticles. Reprinted with permission from ref. , Copyright 2018 American Chemical Society (B) Monte Carlo simulations of the spin configurations for spherical defected (upper panel) and defect-free (lower panel) nanoparticles. From left to right the diagrams indicate the configuration under a positive field and two different reversal fields, while core, surface and defect spins are represented in red, blue and black, respectively. The bottom inset indicates the comparison of the simulated SAR values for both cases. Reprinted from ref. under a Creative Commons Attribution 4.0 International Licence (C) FePt/Fe3O4 core/shell nanocubes: TEM images, 3D-TEM tomography and off-axis electron holography at the remanence state indicating a magnetic vortex magnetic flux configuration. Adapted with permission from ref. , Copyright 2018 Wiley-VCH.
Fig. 4
Fig. 4. (A) HAADF-STEM image and elemental mapping of SiO2-encapsulated Fe-oxide and upconversion NaYF4:Yb3+,Er3+ nanoparticles (scale bars = 50 nm). Temperature dependence of the excitation spectra and temperature change at the surroundings of the hybrid nanoparticles and at the whole medium under the application of an alternating magnetic field. Adapted with permission from ref. , Copyright 2014, American Chemical Society (B) TEM images of Fe-oxide/CuS hybrid nanoflowers and intermediate products (scale bars = 100 nm). Temperature rise (ΔT) as a function of the Fe and Cu concentration for Fe-oxide/CuS hybrid (spiky) nanoflowers at an applied alternating magnetic field (AMF, 471 kHz and 180 Oe), a laser excitation (λ = 1064 nm, 1 W cm−2) or a dual-excitation set-up (AMF + laser). Adapted from ref. under Creative Commons Attribution-NonCommercial 4.0 License.
None
Gabriel C. Lavorato
None
Raja Das
None
Javier Alonso Masa
None
Manh-Huong Phan
None
Hariharan Srikanth

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