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Journal of Advanced Dielectrics
Contents
2021
Volume: 11 Issue 2
6 Article(s)
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Research Articles
Dielectric properties of amorphous Bi–Ti–O thin films
R. Sun, W. Xu, and R. B. van Dover
We report the unexpectedly excellent dielectric properties of amorphous thin films with compositions in the Bi–Ti–O system. Films were deposited by RF magnetron reactive co-sputtering. In the composition range of 0.5 x Bi1−xTixOy exhibits excellent dielectric properties, with a high dielectric constant, 𝜀r∼ 53,
We report the unexpectedly excellent dielectric properties of amorphous thin films with compositions in the Bi–Ti–O system. Films were deposited by RF magnetron reactive co-sputtering. In the composition range of 0.5 <
x
< 0.7, amorphous
Bi
1
−
x
Ti
x
O
y
exhibits excellent dielectric properties, with a high dielectric constant,
𝜀
r
∼
53, and a dissipation factor as low as tan
δ
= 0.007. The corresponding maximum breakdown field reaches
∼
1.6 MV/cm, yielding a maximum stored charge per unit area of up to 8
μ
C/cm
2
. This work demonstrates the potential of amorphous Bi–Ti–O as a high-performance thin-film dielectric material that is compatible with high-performance integrated circuits.We report the unexpectedly excellent dielectric properties of amorphous thin films with compositions in the Bi–Ti–O system. Films were deposited by RF magnetron reactive co-sputtering. In the composition range of 0.5 <
x
< 0.7, amorphous
Bi
1
−
x
Ti
x
O
y
exhibits excellent dielectric properties, with a high dielectric constant,
𝜀
r
∼
53, and a dissipation factor as low as tan
δ
= 0.007. The corresponding maximum breakdown field reaches
∼
1.6 MV/cm, yielding a maximum stored charge per unit area of up to 8
μ
C/cm
2
. This work demonstrates the potential of amorphous Bi–Ti–O as a high-performance thin-film dielectric material that is compatible with high-performance integrated circuits..
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Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 11, Issue 2, 2150009 (2021)
Get PDF
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Lead-free 0–3-type composites: From piezoelectric sensitivity to modified figures of merit
Ashura N. Isaeva, and Vitaly Yu. Topolov
Effective piezoelectric properties, electromechanical coupling factors (ECF) and figures of merit (FOM) are studied in lead-free 0–3-type composites based on novel ferroelectric 0.965(K0.48Na0.52)(Nb0.96Sb0.04)O3–0.035Bi0.5Na0.5Zr0.15Hf0.75O3 ceramic. Systems of prolate ceramic inclusions are surrounded by a large poly
Effective piezoelectric properties, electromechanical coupling factors (ECF) and figures of merit (FOM) are studied in lead-free 0–3-type composites based on novel ferroelectric 0.965(
K
0
.
4
8
Na
0
.
5
2
)
(
Nb
0
.
9
6
Sb
0
.
0
4
)
O
3
–0.035
Bi
0
.
5
Na
0
.
5
Zr
0
.
1
5
Hf
0
.
7
5
O
3
ceramic. Systems of prolate ceramic inclusions are surrounded by a large polymer matrix that can be either monolithic (in the 0–3 composite) or porous (in the 0–3–0 composite). Non-monotonic volume-fraction dependences of the effective piezoelectric coefficients
g
3
j
∗
, ECF
k
3
j
∗
, squared FOM
d
3
j
∗
g
3
j
∗
and their modified analogs for stress-driven systems are analysed, and examples of the high longitudinal piezoelectric sensitivity (
g
3
3
∗
>
100 mV ⋅m/N) are considered. A role of microgeometrical factors, that promote the large effective parameters and anisotropy of properties in the 0–3-type composites, is highlighted. New “aspect ratio — volume fraction” diagrams are first built to describe conditions for high piezoelectric sensitivity, large modified FOM and their anisotropy in the studied composites. These advanced materials can be of value for piezoelectric sensor, energy-harvesting and related applications.Effective piezoelectric properties, electromechanical coupling factors (ECF) and figures of merit (FOM) are studied in lead-free 0–3-type composites based on novel ferroelectric 0.965(
K
0
.
4
8
Na
0
.
5
2
)
(
Nb
0
.
9
6
Sb
0
.
0
4
)
O
3
–0.035
Bi
0
.
5
Na
0
.
5
Zr
0
.
1
5
Hf
0
.
7
5
O
3
ceramic. Systems of prolate ceramic inclusions are surrounded by a large polymer matrix that can be either monolithic (in the 0–3 composite) or porous (in the 0–3–0 composite). Non-monotonic volume-fraction dependences of the effective piezoelectric coefficients
g
3
j
∗
, ECF
k
3
j
∗
, squared FOM
d
3
j
∗
g
3
j
∗
and their modified analogs for stress-driven systems are analysed, and examples of the high longitudinal piezoelectric sensitivity (
g
3
3
∗
>
100 mV ⋅m/N) are considered. A role of microgeometrical factors, that promote the large effective parameters and anisotropy of properties in the 0–3-type composites, is highlighted. New “aspect ratio — volume fraction” diagrams are first built to describe conditions for high piezoelectric sensitivity, large modified FOM and their anisotropy in the studied composites. These advanced materials can be of value for piezoelectric sensor, energy-harvesting and related applications..
showLess
Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 11, Issue 2, 2150010 (2021)
Get PDF
View fulltext
Dielectric spectroscopy and structural characterization of nano-filler-loaded epoxy resin
S. G. Thakor, V. A. Rana, H. P. Vankar, and T. R. Pandit
This work outlines the characterization of epoxy resin [Bisphenol A-(epichlorhydrin): epoxy] and hardener [N(3-dimethylaminopropyl)-1,3-propylenediamine] with various inorganic nano-fillers. Dielectric characterizations of epoxy, hardener, neat epoxy (epoxy + hardener) and nano-epoxy (nano-filler + neat epoxy) composit
This work outlines the characterization of epoxy resin [Bisphenol A-(epichlorhydrin): epoxy] and hardener [
N
(3-dimethylaminopropyl)-1,3-propylenediamine] with various inorganic nano-fillers. Dielectric characterizations of epoxy, hardener, neat epoxy (epoxy + hardener) and nano-epoxy (nano-filler + neat epoxy) composites loaded with 1 wt.% of inorganic nano-fillers (SiO
2
, Al
2
O
3
, TiO
2
and ZnO) were carried out using precision LCR meter, over the frequency range of 1 kHz–2 MHz at a constant temperature of 300.15 K. The structural information of nano-fillers, neat epoxy and nano-epoxy composites was understood by Fourier transform infrared spectroscopy and by XRD. Moreover, hardness and shear strength (shear punch) were also determined in order to gain additional information about the mechanical properties of epoxy composite. Influence of inorganic nano-fillers on the dielectric properties, structural chemistry and mechanical properties of neat epoxy composite is discussed thoroughly in this study.This work outlines the characterization of epoxy resin [Bisphenol A-(epichlorhydrin): epoxy] and hardener [
N
(3-dimethylaminopropyl)-1,3-propylenediamine] with various inorganic nano-fillers. Dielectric characterizations of epoxy, hardener, neat epoxy (epoxy + hardener) and nano-epoxy (nano-filler + neat epoxy) composites loaded with 1 wt.% of inorganic nano-fillers (SiO
2
, Al
2
O
3
, TiO
2
and ZnO) were carried out using precision LCR meter, over the frequency range of 1 kHz–2 MHz at a constant temperature of 300.15 K. The structural information of nano-fillers, neat epoxy and nano-epoxy composites was understood by Fourier transform infrared spectroscopy and by XRD. Moreover, hardness and shear strength (shear punch) were also determined in order to gain additional information about the mechanical properties of epoxy composite. Influence of inorganic nano-fillers on the dielectric properties, structural chemistry and mechanical properties of neat epoxy composite is discussed thoroughly in this study..
showLess
Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 11, Issue 2, 2150011 (2021)
Get PDF
View fulltext
Improved ferroelectric and piezoelectric properties of (
Na
0
.
5
K
0
.
5
)
NbO
3
ceramics via sintering in low oxygen partial pressure atmosphere and adding LiF
Bing-Yu Li, Xiao-Ming Chen, Mei-Dan Liu, Zi-De Yu, Han-Li Lian, and Jian-Ping Zhou
Dense (Na0.5K0.5)NbO3 lead-free ceramics with the simple composition were prepared via sintering in low oxygen partial pressure (pO2, ∼10−12 atm) atmosphere and adding LiF. All the ceramics have pure orthorhombic structure. Compared to the LiF-added (Na0.5K0.5)NbO3 ceramics sintered in air and the low pO2-sintered pure
Dense (
Na
0
.
5
K
0
.
5
)
NbO
3
lead-free ceramics with the simple composition were prepared via sintering in low oxygen partial pressure (pO
2
,
∼
10
−
1
2
atm) atmosphere and adding LiF. All the ceramics have pure orthorhombic structure. Compared to the LiF-added (
Na
0
.
5
K
0
.
5
)
NbO
3
ceramics sintered in air and the low pO
2
-sintered pure (
Na
0
.
5
K
0
.
5
)
NbO
3
ceramics without LiF addition, the present ceramics exhibit improved piezoelectric and ferroelectric properties. The piezoelectric constant
d
3
3
is 125 pC/N, and the converse piezoelectric constant
d
3
3
* is 186 pm/V. The dielectric constant and dielectric loss of the ceramics at room temperature and 1 kHz are 451 and 0.03, respectively. Under the measured electric field of 70 kV/cm, the remanent polarization is 25.9
μ
C/cm
2
and the coercive field is 13.9 kV/cm. Furthermore, if the base metals such as Cu and Ni powders were mixed into the green pellets and sintered in the low pO
2
atmosphere, the base metals cannot be oxidized, suggesting possibility of using base metals as electrodes.Dense (
Na
0
.
5
K
0
.
5
)
NbO
3
lead-free ceramics with the simple composition were prepared via sintering in low oxygen partial pressure (pO
2
,
∼
10
−
1
2
atm) atmosphere and adding LiF. All the ceramics have pure orthorhombic structure. Compared to the LiF-added (
Na
0
.
5
K
0
.
5
)
NbO
3
ceramics sintered in air and the low pO
2
-sintered pure (
Na
0
.
5
K
0
.
5
)
NbO
3
ceramics without LiF addition, the present ceramics exhibit improved piezoelectric and ferroelectric properties. The piezoelectric constant
d
3
3
is 125 pC/N, and the converse piezoelectric constant
d
3
3
* is 186 pm/V. The dielectric constant and dielectric loss of the ceramics at room temperature and 1 kHz are 451 and 0.03, respectively. Under the measured electric field of 70 kV/cm, the remanent polarization is 25.9
μ
C/cm
2
and the coercive field is 13.9 kV/cm. Furthermore, if the base metals such as Cu and Ni powders were mixed into the green pellets and sintered in the low pO
2
atmosphere, the base metals cannot be oxidized, suggesting possibility of using base metals as electrodes..
showLess
Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 11, Issue 2, 2150012 (2021)
Get PDF
View fulltext
Impedance and modulus studies of
Na
0
.
9
Ba
0
.
1
Nb
0
.
9
(
Sn
0
.
5
Ti
0
.
5
)
0
.
1
O
3
ceramic
A. Oueslati, and A. Aydi
Polycrystalline Na0.9Ba0.1Nb0.9(Sn0.5Ti0.5)0.1O3 is prepared by the solid-state reaction technique. The formation of single-phase material was confirmed by an X-ray diffraction study and it was found to be a tetragonal phase at room temperature. Nyquist plots (Z′′ versus Z′) show that the conductivity behavior is accur
Polycrystalline
Na
0
.
9
Ba
0
.
1
Nb
0
.
9
(
Sn
0
.
5
Ti
0
.
5
)
0
.
1
O
3
is prepared by the solid-state reaction technique. The formation of single-phase material was confirmed by an X-ray diffraction study and it was found to be a tetragonal phase at room temperature. Nyquist plots (
Z
′
′
versus
Z
′
)
show that the conductivity behavior is accurately represented by an equivalent circuit model which consists of a parallel combination of bulk resistance and constant phase elements (CPE). The frequency dependence of the conductivity is interpreted in terms of Jonscher’s law. The conductivity
σ
d
c
follows the Arrhenius relation. The modulus plots can be characterized by the empirical Kohlrausch–Williams–Watts (KWW),
φ
(
t
)
= exp(
−
(
t
/
τ
)
β
)
function and the value of the stretched exponent (
β
)
is found to be almost independent of temperature. The near value of activation energies obtained from the analyses of modulus and conductivity data confirms that the transport is through an ion hopping mechanism dominated by the motion of the (
O
2
−
)
ions in the structure of the investigated material.Polycrystalline
Na
0
.
9
Ba
0
.
1
Nb
0
.
9
(
Sn
0
.
5
Ti
0
.
5
)
0
.
1
O
3
is prepared by the solid-state reaction technique. The formation of single-phase material was confirmed by an X-ray diffraction study and it was found to be a tetragonal phase at room temperature. Nyquist plots (
Z
′
′
versus
Z
′
)
show that the conductivity behavior is accurately represented by an equivalent circuit model which consists of a parallel combination of bulk resistance and constant phase elements (CPE). The frequency dependence of the conductivity is interpreted in terms of Jonscher’s law. The conductivity
σ
d
c
follows the Arrhenius relation. The modulus plots can be characterized by the empirical Kohlrausch–Williams–Watts (KWW),
φ
(
t
)
= exp(
−
(
t
/
τ
)
β
)
function and the value of the stretched exponent (
β
)
is found to be almost independent of temperature. The near value of activation energies obtained from the analyses of modulus and conductivity data confirms that the transport is through an ion hopping mechanism dominated by the motion of the (
O
2
−
)
ions in the structure of the investigated material..
showLess
Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 11, Issue 2, 2150013 (2021)
Get PDF
View fulltext
Influence of sintering behavior on the microstructure and electrical properties of BaTiO
3
lead-free ceramics from hydrothermal synthesized precursor nanoparticles
Do Viet On, Le Dai Vuong, Truong Van Chuong, Dao Anh Quang, Ho Van Tuyen, and Vo Thanh Tung
BaTiO3 nanoparticles were synthesized by hydrothermal method using amorphous phase TiO2 precursor as the Ti-source. The microstructure and phase structure were determined using XRD, SEM and Raman spectroscopy analysis results. The results showed that BaTiO3 nanoparticles have tetragonal structure, average size of about
BaTiO
3
nanoparticles were synthesized by hydrothermal method using amorphous phase TiO
2
precursor as the Ti-source. The microstructure and phase structure were determined using XRD, SEM and Raman spectroscopy analysis results. The results showed that BaTiO
3
nanoparticles have tetragonal structure, average size of about 100 nm was obtained at Ba/Ti ratio of 1.5, synthesis temperature of 200
∘
C and reaction time of 12 h. The components of the BaTiO
3
lead-free ceramic system are fabricated by conventional solid-phase reaction from the average size BaTiO
3
particles about 100 nm obtained by hydrothermal process. The effects of sintering behavior on dielectric, ferroelectric and piezoelectric properties of BT high-density ceramic were studied. The BaTiO
3
ceramic composition sintered at 1300
∘
C has a relative density of 97%, the value of the electromechanical coefficient
k
p
= 0.40,
k
3
3
= 0.42, the large piezoelectric coefficient
d
3
3
= 300 pC/N,
d
3
1
=
−
125 pC/N.BaTiO
3
nanoparticles were synthesized by hydrothermal method using amorphous phase TiO
2
precursor as the Ti-source. The microstructure and phase structure were determined using XRD, SEM and Raman spectroscopy analysis results. The results showed that BaTiO
3
nanoparticles have tetragonal structure, average size of about 100 nm was obtained at Ba/Ti ratio of 1.5, synthesis temperature of 200
∘
C and reaction time of 12 h. The components of the BaTiO
3
lead-free ceramic system are fabricated by conventional solid-phase reaction from the average size BaTiO
3
particles about 100 nm obtained by hydrothermal process. The effects of sintering behavior on dielectric, ferroelectric and piezoelectric properties of BT high-density ceramic were studied. The BaTiO
3
ceramic composition sintered at 1300
∘
C has a relative density of 97%, the value of the electromechanical coefficient
k
p
= 0.40,
k
3
3
= 0.42, the large piezoelectric coefficient
d
3
3
= 300 pC/N,
d
3
1
=
−
125 pC/N..
showLess
Journal of Advanced Dielectrics
Publication Date: Jan. 01, 1900
Vol. 11, Issue 2, 2150014 (2021)
Get PDF
View fulltext
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