Journal of Alloys and Compounds 509 (2011) 7742–7748
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Journal of Alloys and Compounds
j our na l ho me p ag e: www.elsevier.com/locate/jallcom
Bismuth ferrite bilayered thin films of different constituent layer thicknesses
Jiagang Wu
a,b,∗
, John Wang
b
, Dingquan Xiao
a
, Jianguo Zhu
a
a
Department of Materials Science, Sichuan University, Chengdu 610064, PR China
b
Department of Materials Science and Engineering, National University of Singapore, Singapore 117574, Singapore
a r t i c l e i n f o
Article history:
Received 25 March 2011
Received in revised form 27 April 2011
Accepted 29 April 2011
Available online 10 May 2011
Keywords:
Bismuth ferrite
Bilayer structure
Multiferroic behavior
Fatigue behavior
a b s t r a c t
Bilayered thin films consisting of (Bi
0.90
La
0.10
)(Fe
0.85
Zn
0.15
)O
3
and (Bi
0.90
La
0.10
)(Fe
0.90
Zn
0.10
)O
3
layers have
been fabricated by radio frequency sputtering. Both multiferroic layers are well retained in these bilayers.
Their leakage current, multiferroic properties, and fatigue behavior are largely dependent on the thick-
nesses of (Bi
0.90
La
0.10
)(Fe
0.85
Zn
0.15
)O
3
. With an increase of the thickness in the (Bi
0.90
La
0.10
)(Fe
0.85
Zn
0.15
)O
3
layer, the leakage current density of bilayers is degraded due to different grain growth modes and an
increase in oxygen vacancies, the dielectric constant (ε
r
) becomes larger due to the introduction of
(Bi
0.90
La
0.10
)(Fe
0.85
Zn
0.15
)O
3
with a high ε
r
value, and their magnetic properties are deteriorated with
increasing the thickness ratios of (Bi
0.90
La
0.10
)(Fe
0.85
Zn
0.15
)O
3
with a weaker magnetization. All bilayers
exhibit a good ferroelectric behavior regardless of varying thicknesses of the (Bi
0.90
La
0.10
)(Fe
0.85
Zn
0.15
)O
3
layer, while their coercive field decreases with increasing the thickness of the (Bi
0.90
La
0.10
)(Fe
0.85
Zn
0.15
)O
3
layer. An anomalous enhancement in switchable polarization is demonstrated by these bilayers, owing
to the involvement of space charges accumulated at the interfaces between two constituent layers.
© 2011 Elsevier B.V. All rights reserved.
1. Introduction
Multilayered ferroelectric thin films differing in their structures
or/and compositions exhibit novel magnetics [1,2], an improved
polarization [3–5], a high dielectric constant [6,7], a new structural
phase [8], and other new functional properties [9,10] owing to the
epitaxial strain and the interface coupling and interactions among
these constituent interfacial layers.
Multiferroic materials have recently attracted much attention
[11–24]. Among those, multiferroic BiFeO
3
(BFO) material with a
rhombohedrally distorted perovskite structure has recently been
given to considerable attention due to its giant remanent polariza-
tion, a high Curie temperature, and the existence of ferroelectric
and ferromagnetic properties at and above room temperature
[13–26], and the material shows promise for practical applications
in high density ferroelectric random access memories, spintron-
ics, and sensors and actuators, and so on [11–26]. In contrast, a
very high leakage current density at room temperature seriously
degrades the electrical behavior of BFO material, and thus hin-
ders its practical applications [11–26]. Although some methods
have been used to decrease the leakage current density of BFO thin
films, their electrical behavior is still not ideal [2,5,27,28]. Among
these promising methods, the bilayered structure consisting of
∗
Corresponding author at: Department of Materials Science, Sichuan University,
Chengdu 610064, PR China. Tel.: +86 28 85412202; fax: +86 28 85412202.
E-mail addresses: wujiagang0208@163.com, msewujg@scu.edu.cn (J. Wu).
BFO and other ferroelectrics may be a more promising method for
decreasing the leakage current density and improving the elec-
trical properties of BFO, owing to the advantage of the bilayered
structure. In the past, the bilayered thin films consisting of BFO
and other ferroelectric layer have been reported [2,5,28], such as
Bi
1/2
Na
1/2
TiO
3
, Pb(Zr, Ti)O
3
. Some interesting results have been
demonstrated by such a bilayered structure, such as the reduction
in leakage current density, the improvement in phase purity, and
the enhancement in fatigue behavior [2,5,26], but their polarization
value is much lower as compared with the intrinsic polarization one
of BFO thin films [2,5,28].
In the present work, the bilayered thin films con-
sisting of (Bi
0.90
La
0.10
)(Fe
0.85
Zn
0.15
)O
3
(BLFZO15) and
(Bi
0.90
La
0.10
)(Fe
0.90
Zn
0.10
)O
3
(BLFZO10) layers were grown in situ
on Pt/TiO
2
/SiO
2
/Si(1 0 0) substrates without any buffer layers by
radio frequency (rf) sputtering, where the thickness of the BLFZO10
layer is fixed, and the thickness of the BLFZO15 layer is changed
from 20 nm to 180 nm. The thicknesses of the BLFZO15 layer seri-
ously affect the leakage current density, dielectric properties, and
multiferroic and fatigue behavior of BLFZO15/BLFZO10 bilayered
thin films, and the underlying physics mechanisms were clearly
addressed.
2. Experimental procedure
The two-inch BLFZO10 and BLFZO15 ceramic targets with an excess of 10%
Bi have been synthesized via a solid state reaction of constituent oxides, namely
Bi2O3 (99.9%), Fe2O3 (99.9%), La2O3 (99.99%), and ZnO (99.9%). The powder mix-
tures of appropriate compositions of these oxides were calcined at ∼700
◦
C in
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doi:10.1016/j.jallcom.2011.04.140