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. 2022 Nov 22;7(48):44187-44198.
doi: 10.1021/acsomega.2c05651. eCollection 2022 Dec 6.

Application of Mn x Fe1- x Fe2O4 (x = 0-1) Nanoparticles in Magnetic Fluid Hyperthermia: Correlation with Cation Distribution and Magnetostructural Properties

Affiliations

Application of Mn x Fe1- x Fe2O4 (x = 0-1) Nanoparticles in Magnetic Fluid Hyperthermia: Correlation with Cation Distribution and Magnetostructural Properties

Satish S Phalake et al. ACS Omega. .

Abstract

Optimization of manganese-substituted iron oxide nanoferrites having the composition Mn x Fe1-x Fe2O4 (x = 0-1) has been achieved by the chemical co-precipitation method. The crystallite size and phase purity were analyzed from X-ray diffraction. With increases in Mn2+ concentration, the crystallite size varies from 5.78 to 9.94 nm. Transmission electron microscopy (TEM) analysis depicted particle sizes ranging from 10 ± 0.2 to 13 ± 0.2 nm with increasing Mn2+ substitution. The magnetization (M s) value varies significantly with increasing Mn2+ substitution. The variation in the magnetic properties may be attributed to the substitution of Fe2+ ions by Mn2+ ions inducing a change in the superexchange interaction between the A and B sublattices. The self-heating characteristics of Mn x Fe1-x Fe2O4 (x = 0-1) nanoparticles (NPs) in an AC magnetic field are evaluated by specific absorption rate (SAR) and intrinsic loss power, both of which are presented with varying NP composition, NP concentration, and field amplitudes. Mn0.75Fe0.25Fe2O4 exhibited superior induction heating properties in terms of a SAR of 153.76 W/g. This superior value of SAR with an optimized Mn2+ content is presented in correlation with the cation distribution of Mn2+ in the A or B position in the Fe3O4 structure and enhancement in magnetic saturation. These optimized Mn0.75Fe0.25Fe2O4 NPs can be used as a promising candidate for hyperthermia applications.

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Conflict of interest statement

The authors declare no competing financial interest.

Figures

Figure 1
Figure 1
(a) XRD patterns for MnxFe1–xFe2O4 (x = 0–1) NPs and (b) shift view of the region around the (311) peak at different Mn2+ ions.
Figure 2
Figure 2
Variation of the MnxFe1–xFe2O4 (x = 0–1) NPs with Mn2+ content x in terms of their lattice parameter a (nm), crystallite size Dxrd (nm), and X-ray density dx (g/cm3).
Figure 3
Figure 3
Images of (a–d), (e–h), and (i–l) represent the TEM images, SAED patterns, and histograms of samples MnxFe1–xFe2O4 at x = 0, 0.25, and 0.75, respectively.
Figure 4
Figure 4
Strain graph of MnxFe1–xFe2O4 (x = 0–1) NPs.
Figure 5
Figure 5
FTIR spectra of MnxFe1–xFe2O4 (x = 0–1) NPs.
Figure 6
Figure 6
Magnetization (M) vs field (H) curves of the MnxFe1–xFe2O4 (x = 0–1) NPs.
Figure 7
Figure 7
SAR value of the (x = 0–1) NPs at different concentrations (0.5, 1, 2, 5, and 10 mg/mL) and applied fields, with constant frequency (277 kHz).

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