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 |
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Main Authors: | , , , , , |
Format: | Journal Article |
Language: | English |
Published: |
New York
Springer US
01-10-2020
Springer Nature B.V SpringerOpen |
Subjects: | |
Online Access: | Get full text |
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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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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 1556-276X 1931-7573 1556-276X |
DOI: | 10.1186/s11671-020-03423-9 |