Effects of substitution at the manganese site in RE(Ni,Mn)O 3 perovskites (RE=Y, Eu)
The magnetically ordered states of the YNi x Mn 1− x O 3 and EuNi x Mn 1− x O 3 solid solutions (0.0≤ x≤0.50) have been studied at different temperatures and magnetic fields. The magnetization as a function of temperature M( T) shows features due to canted-antiferromagnetism ( x=0.25 and 0.33) and f...
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Published in | Materials science & engineering. B, Solid-state materials for advanced technology Vol. 104; no. 3; pp. 126 - 130 |
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Main Authors | , , , , , , |
Format | Journal Article |
Language | English |
Published |
Elsevier B.V
15.11.2003
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Subjects | |
Online Access | Get full text |
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Summary: | The magnetically ordered states of the YNi
x
Mn
1−
x
O
3 and EuNi
x
Mn
1−
x
O
3 solid solutions (0.0≤
x≤0.50) have been studied at different temperatures and magnetic fields. The magnetization as a function of temperature
M(
T) shows features due to canted-antiferromagnetism (
x=0.25 and 0.33) and ferromagnetism (
x=0.50), while YNi
0.20Mn
0.80O
3 presents a spin-glass behavior. A large field-dependence of the susceptibility maximum at
T
max is found in the nickel-poor region, except for the spin-glass compound, for which
T
max stays constant at
T
SG∼20 K. For the nickel-rich samples the paramagnetic-to-ferromagnetic transition at
T
c is field-independent, with
T
c∼80 and 150 K, for YNi
0.50Mn
0.50O
3 and EuNi
0.50Mn
0.50O
3, respectively. The coercive field
H
coerc and the high-field data obtained from magnetization loops
M(
H) show a well-defined frontier at
x=
x
crit=1/3, between canted-antiferromagnetism (
x≤
x
crit) and full ferromagnetism (
x>
x
crit). This critical value corresponds to equal amounts of Mn
3+ and Mn
4+, leading to a maximum number of pairs Mn
3+/Mn
4+ and an optimum in the double-exchange interactions. |
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ISSN: | 0921-5107 1873-4944 |
DOI: | 10.1016/S0921-5107(03)00184-3 |