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Structure, phase diagra
m
and
m
agnetic properties of Bi<
su
b>1−
x
su
b>La<
su
b>x
su
b>FeO<
su
b>3
su
b> solid solution
详细信息
查看全文
作者:
Q.R. Yao<
su
p>a
su
p><
su
p>
;
su
p><
su
p>b
su
p><
su
p>
;
su
p><
su
p>c
su
p><
su
p>
;
su
p><
su
p>qingry96@guet.edu.cn" class="auth_
m
ail" title="E-
m
ail the corresponding author
su
p>
;
Y.H. Shen<
su
p>b
su
p>
;
P.C. Yang<
su
p>b
su
p>
;
H.Y. Zhou<
su
p>b
su
p><
su
p>
;
su
p><
su
p>c
su
p>
;
G.H. Rao<
su
p>b
su
p><
su
p>
;
su
p><
su
p>c
su
p>
;
Z.
M
. Wang<
su
p>b
su
p><
su
p>
;
su
p><
su
p>c
su
p>
;
J.Q. Deng<
su
p>b
su
p><
su
p>
;
su
p><
su
p>c
su
p>
关键词:
C.
M
agnetic properties
;
Phase diagra
m
;
Phase transition
;
X-ray diffraction
;
Crystal structure
刊名:Cera
m
ics International
出版年:2016
出版时间:April 2016
年:2016
卷:42
期:5
页码:6100-6106
全文大小:2426 K
文摘
A series of polycrystalline Bi<
su
b>1&
m
inus;
m>x
m>
su
b>La<
su
b>x
su
b>FeO<
su
b>3
su
b> (0≤
m>x
m>≤1.00) solid solution were synthesized by sol–gel
m
ethod. The effects of lanthanu
m
concentration on the phase for
m
ation, phase transition and
m
agnetic properties were studied. The XRD re
su
lts displayed that there is a clear indication of structural
m
odification and sy
mm
etry change brought about by La doping. At roo
m
te
m
perature the crystal structure of the solid solution transfor
m
s fro
m
rho
m
bohedral R3c (
m>x
m>≤0.15) to tetragonal P4
mm
(0.15<
m>x
m><0.40), then to cubic
mmlsi0002" class="
m
ath
m
lsrc">
mathI
m
g" data-
m
athURL="/science?_ob=MathURL&_
m
ethod=retrieve&_eid=1-s2.0-S0272884216000031&_
m
athId=si0002.gif&_user=111111111&_pii=S0272884216000031&_rdoc=1&_issn=02728842&
m
d5=34ed39e41f75ed0c199a5c6d58e8dd4f">
mg class="i
m
gLazyJSB inlineI
m
age" height="15" width="44" alt="View the MathML source" style="
m
argin-top: -5px; vertical-align:
m
iddle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inli
m
geid="1-s2.0-S0272884216000031-si0002.gif">
mg height="15" border="0" style="vertical-align:botto
m
" width="44" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.co
m
/content/i
m
age/1-s2.0-S0272884216000031-si0002.gif">
mathContainer hidden">
mathCode"><
m
ath alti
m
g="si0002.gif" overflow="scroll"><
m
row><
m
i>P
m
i><
m
i>
m
m
i><
m
over accent="true"><
m
n>3
m
n><
m
o>&
m
acr;
m
o>
m
over><
m
i>
m
m
i>
m
row>
m
ath>
(0.40≤
m>x
m><0.50), and finally to orthorho
m
bic Pbn
m
(0.50≤
m>x
m>≤1.00). In situ high te
m
perature X-ray powder diffraction studies reveal that phase transfor
m
ations of the rho
m
bohedral R3c and the cubic
mmlsi0002" class="
m
ath
m
lsrc">
mathI
m
g" data-
m
athURL="/science?_ob=MathURL&_
m
ethod=retrieve&_eid=1-s2.0-S0272884216000031&_
m
athId=si0002.gif&_user=111111111&_pii=S0272884216000031&_rdoc=1&_issn=02728842&
m
d5=34ed39e41f75ed0c199a5c6d58e8dd4f">
mg class="i
m
gLazyJSB inlineI
m
age" height="15" width="44" alt="View the MathML source" style="
m
argin-top: -5px; vertical-align:
m
iddle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inli
m
geid="1-s2.0-S0272884216000031-si0002.gif">
mg height="15" border="0" style="vertical-align:botto
m
" width="44" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.co
m
/content/i
m
age/1-s2.0-S0272884216000031-si0002.gif">
mathContainer hidden">
mathCode"><
m
ath alti
m
g="si0002.gif" overflow="scroll"><
m
row><
m
i>P
m
i><
m
i>
m
m
i><
m
over accent="true"><
m
n>3
m
n><
m
o>&
m
acr;
m
o>
m
over><
m
i>
m
m
i>
m
row>
m
ath>
to the orthorho
m
bic Pbn
m
occur in the te
m
perature regions of 680–730 °C and 300–680 °C,respectively. The phase transfor
m
ations of the tetragonal P4
mm
to the cubic
mmlsi0002" class="
m
ath
m
lsrc">
mathI
m
g" data-
m
athURL="/science?_ob=MathURL&_
m
ethod=retrieve&_eid=1-s2.0-S0272884216000031&_
m
athId=si0002.gif&_user=111111111&_pii=S0272884216000031&_rdoc=1&_issn=02728842&
m
d5=34ed39e41f75ed0c199a5c6d58e8dd4f">
mg class="i
m
gLazyJSB inlineI
m
age" height="15" width="44" alt="View the MathML source" style="
m
argin-top: -5px; vertical-align:
m
iddle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inli
m
geid="1-s2.0-S0272884216000031-si0002.gif">
mg height="15" border="0" style="vertical-align:botto
m
" width="44" alt="View the MathML source" title="View the MathML source" src="http://origin-ars.els-cdn.co
m
/content/i
m
age/1-s2.0-S0272884216000031-si0002.gif">
mathContainer hidden">
mathCode"><
m
ath alti
m
g="si0002.gif" overflow="scroll"><
m
row><
m
i>P
m
i><
m
i>
m
m
i><
m
over accent="true"><
m
n>3
m
n><
m
o>&
m
acr;
m
o>
m
over><
m
i>
m
m
i>
m
row>
m
ath>
occurs in the te
m
perature region of 200–230 °C, whereas the phase structure of orthorho
m
bic Pbn
m
keeps unchanged below 850 °C. Based on careful characterization of crystal structure and phase transition as a function of te
m
perature, the phase diagra
m
of the pseudo-binary BiFeO<
su
b>3
su
b>–LaFeO<
su
b>3
su
b> syste
m
has been constructed. The phase diagra
m
m
anifests that the Bi<
su
b>1&
m
inus;
m>x
m>
su
b>La
m><
su
b>x
su
b>
m>FeO<
su
b>3
su
b> (0≤
m>x
m>≤1.00) solid solution provides
m
ore options to tune the
m
agnetis
m
and
m
ultiferrois
m
, as the crystal structures with polarity feature occur in a wide doping concentration of La (
m>x
m>≤0.30). We then selectively studied the
m
agnetic properties of possible
m
ultiferroic phases, i.e. R3c and P4
mm
phases. The re
su
lts revealed that both the
m
agnetic re
m
anence and the coercive field of Bi<
su
b>1&
m
inus;
m>x
m>
su
b>La
m><
su
b>x
su
b>
m>FeO<
su
b>3
su
b> (0<
m>x
m>≤0.30) increased with the La content.
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