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Giant isotope effect and spin state transition induced by oxygen isotope exchange in (
P
r
1
β
x
S
m
x
)
0.7
C
a
0.3
C
o
O
3
Pr_{1-x}Sm_x)_{0.7}Ca_{0.3}CoO_3
P
r
1
β
x
β
S
m
x
β
)
0.7
β
C
a
0.3
β
C
o
O
3
β
Authors
C. H. Wang
G. M. Zhao
+6Β more
G. Wu
G. Y. Wang
I. B. Bersuker
T. Wu
X. G. Luo
X. H. Chen
Publication date
30 April 2006
Publisher
'American Physical Society (APS)'
Doi
Cite
View
on
arXiv
Abstract
We systematically investigate effect of oxygen isotope in
(
P
r
1
β
x
S
m
x
)
0.7
C
a
0.3
C
o
O
3
(Pr_{1-x}Sm_x)_{0.7}Ca_{0.3}CoO_3
(
P
r
1
β
x
β
S
m
x
β
)
0.7
β
C
a
0.3
β
C
o
O
3
β
which shows a crossover with x from ferromagnetic metal to the insulator with spin-state transition. A striking feature is that effect of oxygen isotope on the ferromagnetic transition is negligible in the metallic phase, while replacing
16
O
^{16}O
16
O
with
18
O
^{18}O
18
O
leads to a giant up-shift of the spin-state transition temperature (
T
s
T_s
T
s
β
) in the insulating phase, especially
T
s
T_s
T
s
β
shifts from 36 to 54 K with isotope component
Ξ±
S
=
β
4.7
\alpha_S=-4.7
Ξ±
S
β
=
β
4.7
for the sample with x=0.175. A metal-insulator transition is induced by oxygen isotope exchange in the sample x=0.172 being close to the insulating phase. The contrasting behaviors observed in the two phases can be well explained by occurrence of static Jahn-Teller distortions in the insulating phase, while absence of them in the metallic phase.Comment: 4 pages, 5 figure
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Last time updated on 02/01/2020