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Explanation:
The nuclear and magnetic structures and properties of
La
1
−
x
Sr
x
MnO
3
with
0.45
<~
x
<~
1
and
Pr
1
−
y
Sr
y
MnO
3
(
0.58
<~
y
<~
1
)
were investigated using neutron powder diffraction, resistivity and magnetic measurements. In this paper, we present the full magnetic and structural phase diagram for
La
1
−
x
Sr
x
MnO
3
and a partial phase diagram for
Pr
1
−
y
Sr
y
MnO
3
.
At low temperatures, we observe a series of structural phase transitions evolving as a function of increasing x as follows: orthorhombic
Pbn
→
m
rhombohedral
R
3
¯
→
c
orthorhombic
Fmm
→
m
tetragonal
I
4
if/
m
c
→
m
cubic
Pm
3
¯
m
.
At higher temperatures, the orthorhombic Fmmm structural region disappears. We also identify four magnetic states (FM, A, C, and G type) evolving as a function of increasing x. The magnetic and nuclear structural transitions coincide for samples with
0.8
<~
x
<~
0.95.
In the
0.5
<~
x
<~
0.9
region, resistivity and magnetic measurements show a substantial hysteresis near
T
N
.
This hysteresis of a few K is indicative of a first order antiferromagnetic transition in good agreement with the neutron diffraction results. Our data also suggest the existence of a strong competition between the ferromagnetic and A-type states for
Answers & Comments
Answer:
I will show you the answer one's all of you answered.
ok Soo you now the answer ok I will explain all
Explanation:
The nuclear and magnetic structures and properties of
La
1
−
x
Sr
x
MnO
3
with
0.45
<~
x
<~
1
and
Pr
1
−
y
Sr
y
MnO
3
(
0.58
<~
y
<~
1
)
were investigated using neutron powder diffraction, resistivity and magnetic measurements. In this paper, we present the full magnetic and structural phase diagram for
La
1
−
x
Sr
x
MnO
3
and a partial phase diagram for
Pr
1
−
y
Sr
y
MnO
3
.
At low temperatures, we observe a series of structural phase transitions evolving as a function of increasing x as follows: orthorhombic
Pbn
→
m
rhombohedral
R
3
¯
→
c
orthorhombic
Fmm
→
m
tetragonal
I
4
if/
m
c
→
m
cubic
Pm
3
¯
m
.
At higher temperatures, the orthorhombic Fmmm structural region disappears. We also identify four magnetic states (FM, A, C, and G type) evolving as a function of increasing x. The magnetic and nuclear structural transitions coincide for samples with
0.8
<~
x
<~
0.95.
In the
0.5
<~
x
<~
0.9
region, resistivity and magnetic measurements show a substantial hysteresis near
T
N
.
This hysteresis of a few K is indicative of a first order antiferromagnetic transition in good agreement with the neutron diffraction results. Our data also suggest the existence of a strong competition between the ferromagnetic and A-type states for
x
∼
0
.
5
,
and between the C- and G-type states for
x
∼
0.95.
A similar behavior is observed for
Pr
1
−
y
Sr
y
MnO
3
.
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Explanation:
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