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Coercivity analysis of cubic and tetragonal (Cu,Co) ferrite particles within the global model
We analyzed the coercivity of both cubic and tetragonally distorted Co x Cu 1− x Fe 2 O 4 particles ( x = 0.2 and 0.1, respectively) using the global model. According to magnetic viscosity measurements, the size of the activation volumes v a increases from around 2000 nm 3 ( v a 1/3 ≈ 13 nm) at 10 K...
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Published in: | Journal of physics. D, Applied physics Applied physics, 2021-06, Vol.54 (22), p.224001 |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We analyzed the coercivity of both cubic and tetragonally distorted Co
x
Cu
1−
x
Fe
2
O
4
particles (
x
= 0.2 and 0.1, respectively) using the global model. According to magnetic viscosity measurements, the size of the activation volumes
v
a
increases from around 2000 nm
3
(
v
a
1/3
≈ 13 nm) at 10 K for both samples, to close to 175 000 nm
3
for the cubic sample and 5400 nm
3
for the tetragonally distorted sample at 300 K. The microstructure-related phenomenological parameters obtained from the global model analysis are
α
= 0.29 and
N
eff
= −0.01 and
α
= 0.39 and
N
eff
= −0.24 for the cubic and tetragonal samples, respectively. High-resolution transmission electron microscopy images of the tetragonal sample showed that nanograins are connected through a thin amorphous layer (∼1 nm), which could account for the intergranular exchange interactions indicated by the negative value of
N
eff
as well as values of
M
r
/
M
s
> 0.5 for such isotropic samples. Low temperature discrepancies are tentatively attributed to magnetic reversal being governed by a local heating process following thermal activation. |
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ISSN: | 0022-3727 1361-6463 |
DOI: | 10.1088/1361-6463/abe5e1 |