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Journal of Advanced Dielectrics
Contents
2023
Volume: 13 Issue 3
8 Article(s)
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Research Articles
Stable large-area monodomain in as-grown bulk ferroelectric single crystal Sn
2
P
2
S
6
Yingzhuo Lun, Jiaqian Kang, Wenfu Zhu, Jianming Deng, Xingan Jiang, Cheng Zhu, Qi Ren, Xian Zi, Ziyan Gao, Tianlong Xia, Zishuo Yao, Xueyun Wang, and Jiawang Hong
Driven by the minimization of total energy, the multi-domain morphology is preferred in as-grown ferroelectrics to reduce the depolarization and strain energy during the paraelectric to ferroelectric phase transition. However, the complicated multi-domain is not desirable for certain high-performance ferroelectric elec
Driven by the minimization of total energy, the multi-domain morphology is preferred in as-grown ferroelectrics to reduce the depolarization and strain energy during the paraelectric to ferroelectric phase transition. However, the complicated multi-domain is not desirable for certain high-performance ferroelectric electro-optic devices. In this work, we achieve a reproducible and stable large-area monodomain in as-grown bulk ferroelectric single crystal
Sn
2
P
2
S
6
. The monodomain dominates the entire single crystal, which is attributed to the internal charge carriers from the photoexcited disproportionation reaction of Sn ions. The charge carriers effectively screen the depolarization field and therefore decrease the depolarization energy and facilitate the formation of monodomain. This work offers a potential approach for engineering bulk ferroelectrics with a stable monodomain, which is desirable for the high-performance ferroelectric electro-optic devices..
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Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 13, Issue 3, 2243001 (2023)
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Ferroelastic and
90
∘
ferroelectric domains in
Bi
2
WO
6
single crystals
Xianghan Xu, Fei-Ting Huang, and Sang-Wook Cheong
High-quality single crystals of Bi2WO6 are grown using a flux method. With different flux growth recipes, we aim to control the crystallization temperature to be lower and higher than the ferroelectric transition temperature, resulting in mono-domain and multi-domain Bi2WO6 crystals, respectively. Abundant ferroelastic
High-quality single crystals of
Bi
2
WO
6
are grown using a flux method. With different flux growth recipes, we aim to control the crystallization temperature to be lower and higher than the ferroelectric transition temperature, resulting in mono-domain and multi-domain
Bi
2
WO
6
crystals, respectively. Abundant ferroelastic orthorhombic twin domains are observed in the multi-domain crystals under an optical microscope. PFM studies unveil the 90
∘
polarization change across those ferroelastic domain walls, as well as the absence of 180
∘
ferroelectric domains in the as-grown multi-domain crystals, indicating a high energy cost of 180
∘
ferroelectric domains. Moreover, a 45
∘
tilt of the 90
∘
ferroelectric domain walls is discovered, and this tilt creates a new type of charged 90
∘
ferroelectric walls, which have not been observed in other bulk ferroelectrics..
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Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 13, Issue 3, 2243002 (2023)
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Domain wall state diagram for SrTiO
3
/BaTiO
3
superlattice structures
Yimei You, Fengjuan Yang, and Pingping Wu
The domain wall structure of ferroelectric/ paraelectric superlattices can be much more complex due to the influence of the superlattice stacking structure, the in-plane strain induced by the substrate and environmental temperature. In this study, we employed a phase field model to investigate the domain wall state of
The domain wall structure of ferroelectric/ paraelectric superlattices can be much more complex due to the influence of the superlattice stacking structure, the in-plane strain induced by the substrate and environmental temperature. In this study, we employed a phase field model to investigate the domain wall state of the SrTi
O
3
/BaTi
O
3
superlattice structure. The domain wall thickness for the SrTi
O
3
/BaTi
O
3
layer was measured using a hyperbolic function. Based on the simulation results, here, we show a domain wall state diagram to distinguish the hard and soft domain states. The polarization profiles across hard/ soft domain walls were illustrated and analyzed. Our simulation results offer a useful concept for the control of the domain wall state in the ferroelectric superlattice..
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Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 13, Issue 3, 2243003 (2023)
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Insulator-to-metal transition in RCoO
3
(R = Pr, Nd)
Sujoy Saha, Sadhan Chanda, Alo Dutta, and T. P. Sinha
We report a straightforward tool to investigate insulator-metal transition in RCoO3 (R = Pr, and Nd) nanoparticles prepared by a sol–gel technique. Thermogravimetric analysis (TGA) of the as-prepared gel is performed to get the lowest possible calcination temperature of RCoO3 nanoparticles. The Rietveld refinement of t
We report a straightforward tool to investigate insulator-metal transition in RCo
O
3
(
R
= Pr, and Nd) nanoparticles prepared by a sol–gel technique. Thermogravimetric analysis (TGA) of the as-prepared gel is performed to get the lowest possible calcination temperature of RCo
O
3
nanoparticles. The Rietveld refinement of the powder X-ray diffraction (XRD) patterns for both samples shows that the samples crystallize in the orthorhombic (
Pnma
) phase at room temperature. The particle size of the sample is determined by scanning electron microscopy. Ac conductivity of the materials is analyzed in the temperature range from 303 K to 673 K and in the frequency range from 42 Hz to 1.1 MHz. The insulator-to-metal transition of PrCo
O
3
and NdCo
O
3
is analyzed by ac impedance spectroscopy. DC resistivity measurement is also done to cross check the insulator-metal transition in RCo
O
3
system..
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Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 13, Issue 3, 2350003 (2023)
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Effects of Mn-doping on the structure and electrical properties of Sm-PMN-PT piezoceramics
Chaofeng Wu, Wen Gong, Jinfeng Geng, Jianye Cui, Lipeng Mi, Jingkai Nie, Qiang He, Jiajiu Li, and Fang-Zhou Yao
MnO2-modified Pb0.9625Sm0.025(Mg1/3Nb2/3)0.71Ti0.29O3 ceramics were prepared via a solid-state reaction approach. Results of detailed characterizations revealed that the addition of MnO2 has influence on the grain size, and all samples exhibit a pure perovskite structure. As the content of manganese increases, the volu
Mn
O
2
-modified
Pb
0
.
9
6
2
5
Sm
0
.
0
2
5
(
Mg
1
/
3
Nb
2
/
3
)
0
.
7
1
Ti
0
.
2
9
O
3
ceramics were prepared via a solid-state reaction approach. Results of detailed characterizations revealed that the addition of Mn
O
2
has influence on the grain size, and all samples exhibit a pure perovskite structure. As the content of manganese increases, the volume of tetragonal phase increases. The ceramics with 1.5 mol.% Mn
O
2
show a high electro-strain of 0.151% at 2 kV/mm. Therefore, this study provides a new insight into the role of Mn
O
2
addition in tailoring the electrical properties of the Sm-PMN-PT ceramics by acceptor doping..
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Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 13, Issue 3, 2350004 (2023)
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High recoverable energy storage density of Na
0.5
Bi
0.5
TiO
3
lead-free ceramics modified by Bi(Mg
0.5
Hf
0.5
)O
3
Kaiyuan Wang, Wenhua Li, Xingui Tang, Siyuan Zhang, Yansong Zhang, Jia Hu, Zhihao Shen, Yanping Jiang, and Xiaobin Guo
Enhancing the availability and reliability of dielectric ceramic energy storage devices is of great importance. In this work, (1-x)Na0.5Bi0.5TiO3–xBi(Mg0.5Hf0.5)O3 (NBT–xBMH) lead-free ceramics were created utilizing a solid-state reaction technique. All NBT–xBMH ceramics have a single perovskite structure. With increa
Enhancing the availability and reliability of dielectric ceramic energy storage devices is of great importance. In this work, (1-
x
)
Na
0
.
5
Bi
0
.
5
TiO
3
–
x
Bi(
Mg
0
.
5
Hf
0
.
5
)
O
3
(NBT–
x
BMH) lead-free ceramics were created utilizing a solid-state reaction technique. All NBT–
x
BMH ceramics have a single perovskite structure. With increasing BMH doping, the grain size shrinks drastically, which greatly enhances the breakdown electric field (310 kV/cm at
x
= 0.25). Additionally, the relaxation behaviors of NBT–
x
BMH ceramics with high BMH content are more remarkable. Among all designed components, the NBT–0.25BMH ceramic exhibits the best energy storage performance with a high
W
rec
of 4.63 J/
cm
3
and an
η
of 75.1% at 310 kV/cm. The NBT–0.25BMH ceramic has exceptional resistance to fluctuations in both frequency (5–500 Hz) and temperature (30–100
∘
C). Charge–discharge test shows that the NBT–0.25BMH ceramic has a quick discharge rate (
t
0
.
9
<
110 ns). With these properties, the NBT–0.25BMH ceramic may have applications in microdevices as well as in ultra-high power electronic systems..
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Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 13, Issue 3, 2350008 (2023)
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Ferroelectric and piezoelectric properties of lead-free Li
0.06
(K
0.5
Na
0.5
)
0.94
NbO
3
thin films
Xinyu Bu, Changhong Yang, Mengjia Fan, Wenxuan Wang, Xiujuan Lin, and Shifeng Huang
Lead-free (K0.5Na0.5)NbO3 (KNN) and Li0.06(K0.5Na0.5)0.94NbO3 (LKNN) thin films were fabricated by a sol-gel method. The effects of Li substitution on crystal structure, microstructure and electrical properties of KNN film were systematically studied. Li doping can enhance the ferroelectric and piezoelectric properties
Lead-free (
K
0
.
5
Na
0
.
5
)NbO
3
(KNN) and
Li
0
.
0
6
(
K
0
.
5
Na
0
.
5
)
0
.
9
4
NbO
3
(LKNN) thin films were fabricated by a sol-gel method. The effects of Li substitution on crystal structure, microstructure and electrical properties of KNN film were systematically studied. Li doping can enhance the ferroelectric and piezoelectric properties of KNN film. Compared with pure KNN film, the LKNN film possesses larger remanent polarization (
P
r
∼
9.3
μ
C/
cm
2
) and saturated polarization (
P
s
∼
41.2
μ
C/
cm
2
) and lower leakage current density (
∼
1
0
−
5
A/
cm
2
at 200 kV/cm). Meanwhile, a typical butterfly shaped piezoelectric response curve is obtained in the LKNN film with a high piezoelectric coefficient (
d
3
3
∼
105 pm/V). Excellent fatigue resistance (
∼
1
0
9
switching cycles) and aging resistance (
∼
180 days) demonstrate the long-term working stability of LKNN film. These findings indicate that KNN-based lead-free piezoelectric films have a broad application prospect in microelectromechanical systems (MEMS)..
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Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 13, Issue 3, 2350009 (2023)
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Microstructure, domain structure, ferroelectric and piezoelectric properties of textured bismuth-containing ceramics
E. I. Sitalo, O. A. Bunina, V. G. Smotrakov, N. V. Malomyzheva, and N. A. Boldyrev
In this report, the processes of texture formation in grain-oriented ferroelectric ceramics based on layer-structured ferroelectric Bi4Ti3O2 (LSBT) prepared by hot forging method are considered. The microstructural and X-ray methods revealed the axial textured formation in ferroelectric ceramic that are used to estimat
In this report, the processes of texture formation in grain-oriented ferroelectric ceramics based on layer-structured ferroelectric Bi
4
Ti
3
O
2
(LSBT) prepared by hot forging method are considered. The microstructural and X-ray methods revealed the axial textured formation in ferroelectric ceramic that are used to estimate the orientation factor of ceramics. For the first time, the domain structure changes when poling the anisotropic ferroelectric ceramics are investigated. The anisotropy of electromechanical, piezoelectric and ferroelectric properties of ferroelectric ceramics due to the crystal texture existence in it is studied. The aim of this study is to study the processes of crystalline texture formation in polycrystalline BLSF and to establish the dependence of the electrophysical properties of ceramics on the degree of texturing. Ceramics were textured using the hot stamping (HS) method developed at the Research Institute of Physics. The mechanism of the method is that the workpiece is subjected to uniaxial pressure and free radial deformation occurs due to the plastic flow of the material until the workpiece fills the free volume of the mold, which is created by placing the workpiece in the mold with a gap. The study of the microstructure of ceramics showed that an increase in the firing temperature in the range 950–1050
∘
C causes a sharp decrease in porosity and increases the density to 7.95 g/
cm
3
, which is 98% of theoretical. An X-ray analysis was performed and microstructural studies were carried out, which revealed the formation of an axial texture in ceramics. The features of the switching processes of textured ceramics are revealed. The characteristics of the polarization switching of ceramics in the directions parallel and perpendicular (
⊥
) of the pressure axis during hot processing were obtained from the dielectric hysteresis
P
(
E
) loops, i.e., axis axial texture. The
⊥
-cut ceramics are characterized by a more complete polarization switching, which is associated with the additional orientation of the (001) crystallographic planes in the textured material, as well as the presence of a threshold switching field. In the temperature range from -196 to + 600
∘
C, the anisotropy of the electro physical properties of ceramics due to the presence of a crystalline texture in it was studied. The dielectric constant, electrical conductivity, piezoelectric and elastic coefficients were measured for sections of ceramics of different orientations relative to the axis of the texture. The anisotropy of the dielectric constant and electrical conductivity manifests itself weakly at room temperature and increases sharply when approaching the Curie temperature. In the temperature range +20–400
∘
C, the high thermal stability of the piezoelectric module
d
3
3
, measured by the quasistatic method, was established..
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Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 13, Issue 3, 2350011 (2023)
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