Simultaneously high-energy storage density and responsivity in quasi-hysteresis-free Mn-doped Bi0.5Na0.5TiO3-BaTiO3-(Sr0.7Bi0.2□0.1)TiO3 ergodic relaxor ceramics

Liu, Feng; Zhai, Jiwei; Shen, Bo; Liu, Xing; Zeng, Huarong

doi:10.1080/21663831.2018.1457095

Cited by 188 publications

(48 citation statements)

References 33 publications

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“…at the perovskite lattices due to the oxidation of Mn 2+ to Mn 3+ and/or Mn 4+ . This is consistent with the results of Mn-substituted 0.62Bi 0.5 Na 0.5 TiO 3 -0.06BaTiO 3 -0.32 (Sr 0.7 Bi 0.2 [] 0.1 ) TiO 3 ceramics [23]. For CBNO-0BM, ferroelectric polarization is slightly pinched at around E = 0 kV/cm (Figures 3(a) and S5(a)) and the measured P-E loop after dc poling (150 kV/cm) is strongly asymmetric with the establishment of a large internal bias field (E ib = 35.1 kV/cm) ( Figure S5(b)).…”

Section: Resultssupporting

confidence: 92%

Ultrahigh-temperature piezoelectric polycrystalline ceramics: dramatically enhanced ferroelectricity, piezoelectricity and electrical resistivity in Ca_1−3xBi_2+3xNb_2−xMn_xO₉

Long

Ren

Zheng

et al. 2020

Materials Research Letters

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Among Aurivillius-phase ferroelectric ceramics, CaBi 2 Nb 2 O 9 is considered as the best candidate with potential applications in ultrahigh-temperature piezoelectric devices due to the highest T c ( ∼ 940°C). This paper reports that BiMn co-substitution at A and B sites gives rise to dramatic enchantments in ferroelectricity, piezoelectricity, and electrical resistivity of CaBi 2 Nb 2 O 9 ceramics. The optimum composition (Ca 0.97 Bi 2.03 Nb 1.99 Mn 0.01 O 9 ) with a T c of 953 ± 3°C shows a high ferroelectric remnant polarization (P r ), field-induced strain (S 33 ), piezoelectric activity d 33 and d * 33 with values of ∼ 11.1 µC/cm 2 , 4.9 × 10 −4 , 20.8 and 26.1 pC/N, respectively, which are about two to three times those of CaBi 2 Nb 2 O 9 . IMPACT STATEMENTSignificant ferroelectric remnant polarization (P r = 11.1 µC/cm 2 ), field-induced strain (S 33 = 4.9 × 10 −4 ), and piezoelectric activity (d 33 = 20.8 pC/N, d * 33 = 26.1 pC/N) are simultaneously induced in ultrahigh T c CaBi 2 Nb 2 O 9 piezoceramics by BiMn substitution. ARTICLE HISTORY

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Section: Resultssupporting

confidence: 92%

Ultrahigh-temperature piezoelectric polycrystalline ceramics: dramatically enhanced ferroelectricity, piezoelectricity and electrical resistivity in Ca_1−3xBi_2+3xNb_2−xMn_xO₉

Long

Ren

Zheng

et al. 2020

Materials Research Letters

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“…In this model, the total free energy consists of complementary electrostatic energy per unit volume,

W_{normales} (E, s) = \{\begin{matrix} - {false\int}_{0}^{E_{\max}} \frac{{normalε}_{0} {normalε}_{normalg} (s) E}{{()(, 1 + k E^{2})}^{\frac{1}{3}}} d E & in grain \\ - \frac{{normalε}_{0} {normalε}_{normalgb} (s)}{2} E \cdot E & on grain boundary \end{matrix},

the energy of damage,

W_{normald} (s) = W_{normalc} [1 - f (s)]

, with W c indicating the critical density of the electrostatic energy, and the gradient energy term to regulate the sharp phase boundaries,

W_{normali} (\nabla s) = \frac{normalΓ}{4} \nabla s \cdot \nabla s

. The material parameter Γ is approximately the breakdown energy . Breakdown occurs if such a process decreases the total potential energy of the system

Π [s, ϕ] = \underset{normalΩ}{false\int} [W_{normales} (E, s) + W_{normald} (s) + W_{normali} (\nabla s)] d V .

…”

Section: Modelingmentioning

confidence: 99%

“…The polarization response is one of the essential characteristics that determines the dielectric performance of ferroelectric ceramics such as electric displacement, energy storage density, and efficiency . The apparent polarization response can be easily measured experimentally.…”

Section: Modelingmentioning

confidence: 99%

“…It has been reported that the dielectric breakdown strength dominates the energy performance in ferroelectric materials compared to the dielectric permittivity, especially under an ultrahigh electric field from the experimental aspect . Furthermore, the energy storage efficiency is considered one of the most important indicators of ferroelectric energy storage ceramics, which is why relaxor ferroelectric ceramics are attracting increasingly more attention in applications of energy storage devices . Such energy storage densities can be easily calculated from electric hysteresis loops.…”

Section: Introductionmentioning

confidence: 99%

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Grain‐size–dependent dielectric properties in nanograin ferroelectrics

et al. 2018

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A series of ferroelectric ceramic models with grain and grain‐boundary structures of different sizes are established via Voronoi tessellations. A phase‐field model is introduced to study the dielectric breakdown strength of these ferroelectric ceramics. Afterward, the relation between the electric displacement and electric field and the hysteresis loop are calculated using a finite element method based on a classical and modified hyperbolic tangent model. The results indicate that as the grain size decreases, the dielectric strength is enhanced, but the dielectric permittivity is reduced. The discharge energy density and energy storage efficiency of these ferroelectric ceramics extracted from the as‐calculated hysteresis both increase along with a decrease in their grain size at their breakdown points. However, under the same applied electric field, the ferroelectric ceramic with a smaller grain size possesses a lower discharge energy density but a higher energy storage efficiency. The results suggest that ferroelectric ceramics with smaller grain sizes possess advantages for applications in energy storage devices.

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“…For example, BaTiO 3 -Bi(Mg 2/3 Nb 1/3 )O 3 [13] exhibited a high relative permittivity (~6800). Binary solid solution based on (Bi 0.5 Na 0.5 )TiO 3 -BaTiO 3 was a candidate in hightemperature energy-storage application [14][15][16][17]. BaTiO 3 -BiYO 3 ceramics could meet the X9R criterion [18].…”

Section: Introductionmentioning

confidence: 99%

Phase evolution, microstructure, electric properties of (Ba1-xBi0.67xNa0.33x)(Ti1-xBi0.33xSn0.67x)O3 ceramics

Chen

Zhou

et al. 2019

J Adv Ceram

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Ba 1-x Bi 0.67x Na 0.33x)(Ti 1-x Bi 0.33x Sn 0.67x)O 3 (abbreviated as BBNTBS, 0.02 ≤ x ≤ 0.12) ceramics were fabricated via a traditional solid state reaction method. The phase transition of BBNTBS from tetragonal to pseudo cubic is demonstrated by XRD and Raman spectra. The BBNTBS (x = 0.1) ceramics have decent properties with a high ε r (~2250), small Δε/ε 25°C values of ±15% over a wide temperature range from-58 to 171 ℃, and low tanδ ≤ 0.02 from 10 to 200 ℃. The basic mechanisms of conduction and relaxation processes in the high temperature region were thermal activation, and oxygen vacancies might be the ionic charge transport carriers. Meanwhile, BBNTBS (x = 0.1) exhibited decent energy storage density (J d = 0.58 J/cm 3) and excellent thermal stability (the variation of J d is less than 3% in the temperature range of 25-120 ℃), which could be a potential candidate for high energy density capacitors.

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Simultaneously high-energy storage density and responsivity in quasi-hysteresis-free Mn-doped Bi_0.5Na_0.5TiO₃-BaTiO₃-(Sr_0.7Bi_0.2□_0.1)TiO₃ ergodic relaxor ceramics

Abstract: Zeng (2018) Simultaneously high-energy storage density and responsivity in quasi-hysteresis-free Mn-doped Bi 0.

Cited by 188 publications

References 33 publications

Ultrahigh-temperature piezoelectric polycrystalline ceramics: dramatically enhanced ferroelectricity, piezoelectricity and electrical resistivity in Ca_1−3xBi_2+3xNb_2−xMn_xO₉

Ultrahigh-temperature piezoelectric polycrystalline ceramics: dramatically enhanced ferroelectricity, piezoelectricity and electrical resistivity in Ca_1−3xBi_2+3xNb_2−xMn_xO₉

Grain‐size–dependent dielectric properties in nanograin ferroelectrics

Phase evolution, microstructure, electric properties of (Ba1-xBi0.67xNa0.33x)(Ti1-xBi0.33xSn0.67x)O3 ceramics

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Simultaneously high-energy storage density and responsivity in quasi-hysteresis-free Mn-doped Bi0.5Na0.5TiO3-BaTiO3-(Sr0.7Bi0.2□0.1)TiO3 ergodic relaxor ceramics

Abstract: Zeng (2018) Simultaneously high-energy storage density and responsivity in quasi-hysteresis-free Mn-doped Bi 0.

Cited by 188 publications

References 33 publications

Ultrahigh-temperature piezoelectric polycrystalline ceramics: dramatically enhanced ferroelectricity, piezoelectricity and electrical resistivity in Ca1−3xBi2+3xNb2−xMnxO9

Ultrahigh-temperature piezoelectric polycrystalline ceramics: dramatically enhanced ferroelectricity, piezoelectricity and electrical resistivity in Ca1−3xBi2+3xNb2−xMnxO9

Grain‐size–dependent dielectric properties in nanograin ferroelectrics

Phase evolution, microstructure, electric properties of (Ba1-xBi0.67xNa0.33x)(Ti1-xBi0.33xSn0.67x)O3 ceramics

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Simultaneously high-energy storage density and responsivity in quasi-hysteresis-free Mn-doped Bi_0.5Na_0.5TiO₃-BaTiO₃-(Sr_0.7Bi_0.2□_0.1)TiO₃ ergodic relaxor ceramics

Ultrahigh-temperature piezoelectric polycrystalline ceramics: dramatically enhanced ferroelectricity, piezoelectricity and electrical resistivity in Ca_1−3xBi_2+3xNb_2−xMn_xO₉

Ultrahigh-temperature piezoelectric polycrystalline ceramics: dramatically enhanced ferroelectricity, piezoelectricity and electrical resistivity in Ca_1−3xBi_2+3xNb_2−xMn_xO₉