Sn2+ Doping: A Strategy for Tuning of Fe3O4 Nanoparticles Magnetization Dipping Temperature/Amplitude, Irreversibility, and Curie Point

Doped magnetite (Sn x Fe 3-2/3 x O 4 ) nanoparticles (NPs) (12–50 nm) with different amount of Sn 2+ ions ( x ) were synthesized using co-precipitation method. Sn 2+ doping reduces the anticipated oxidation of Fe 3 O 4 NPs to maghemite (γ-Fe 2 O 3 ), making them attractive in several magnetic applic...

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Published in:Nanoscale research letters Vol. 15; no. 1; p. 192
Main Authors: Al-Kindi, Umaima S. H., Al-Harthi, Salim H., Widatallah, Hisham M., Elzain, Mohamed E., Myint, Myo T. Z., Kyaw, Htet H.
Format: Journal Article
Language:English
Published: New York Springer US 01-10-2020
Springer Nature B.V
SpringerOpen
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Summary:Doped magnetite (Sn x Fe 3-2/3 x O 4 ) nanoparticles (NPs) (12–50 nm) with different amount of Sn 2+ ions ( x ) were synthesized using co-precipitation method. Sn 2+ doping reduces the anticipated oxidation of Fe 3 O 4 NPs to maghemite (γ-Fe 2 O 3 ), making them attractive in several magnetic applications. Detailed characterizations during heating–cooling cycles revealed the possibility of tuning the unusual observed magnetization dipping temperature/amplitude, irreversibility, and Curie point of these NPs. We attribute this dip to the chemical reduction of γ-Fe 2 O 3 at the NPs surfaces. Along with an increase in the dipping temperature, we found that doping with Sn 2+ reduces the dipping amplitude, until it approximately disappears when x = 0.150. Based on the core-shell structure of these NPs, a phenomenological expression that combines both modified Bloch law ( M = M 0 [1 − γ ( T / T C )] β ) and a modified Curie–Weiss law ( M = −  α [1/( T − T C ) δ ]) is developed in order to explain the observed M - T behavior at different applied external magnetic fields and for different Sn 2+ concentrations. By applying high enough magnetic field, the value of the parameters γ and δ ≈ 1 which are the same in modified Bloch and Curie–Weiss laws. They do not change with the magnetic field and depend only on the material structure and size. The power β for high magnetic field was 2.6 which is as expected for this size of nanoparticles with the core dominated magnetization. However, the β value fluctuates between 3 and 10 for small magnetic fields indicating an extra magnetic contribution from the shell structure presented by Curie–Weiss term. The parameter ( α ) has a very small value and it turns to negative values for high magnetic fields.
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ISSN:1556-276X
1931-7573
1556-276X
DOI:10.1186/s11671-020-03423-9