Barium strontium niobate glass ceramics with different additive amount of Sm 2 O 3 were successfully prepared. The effects of different additions of Sm 2 O 3 on the phase composition, dielectric properties, breakdown strength, interfacial polarizations and energy storage properties of glass ceramics
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Barium strontium titanate (BST) glass-ceramics were fabricated via controlled crystallization with different crystallization routes. Effects of the microwave crystallization and microwave
Request PDF | Effect of K:Ba ratio on energy storage properties of strontium barium potassium niobate-glass ceramics | We prepared 15.16SrO–(16.84 − x)BaO–xK2O–32Nb2O5–28B2O3–8P2O5
DOI: 10.1007/s10854-019-02285-x Corpus ID: 204887305; Effect of K:Ba ratio on energy storage properties of strontium barium potassium niobate-glass ceramics @article{Li2019EffectOK,
Optimized energy storage density of approximately 6.0 J/cm3 was achieved for the sample con-taining 0.5% ZnO; the average dielectric constant was 150–180 and the breakdown strength
In this work, the effect of La2O3 content on the phase evolution, microstructure, dielectric properties and energy storage properties of the strontium barium niobate (SBN)
Barium strontium niobate glass ceramics with different additive amount of SmO were successfully prepared. The effects of different additions of SmO on the phase composition, dielectric
behavior of strontium barium niobate system. Although the maximum polar-ization (P max) and remnant polarization (P r) of CSBN-x increase with x, the difference of the two values (P max
down strength of 1400 kV/cm and its energy storage density can reach up to 4.0 J/cm3, which may be a strong candidate for high energy density storage capacitors for portable or pulsed
Many glass-ceramic systems are used for energy storage. In this work, the fixed moderate contents of CaO were added to the traditional SrO-Na 2 O-Nb 2 O 5-SiO 2 system to improve
Two-step crystallization process was employed to improve microstructure and energy-storage density of the strontium barium niobate-based/titanate-based glass-ceramics. By using two-step crystallization
Effect of different Al/Si ratios on the structure and energy storage properties of strontium barium niobate-based glass-ceramics. J. Electron. Mater., 45 (2016), pp. 1017-1022.
The energy storage density of a Ba0.4Sr0.6TiO3 ceramic with the addition of 5–20 vol% glass was investigated. The results show that the improvement of the energy density in glass-added
the capacitors. For energy-storage devices, the energy-storage density is related to the product of dielectric con-stant and breakdown strength (BDS) [4]. Ceramic dielec-trics as a traditional
A glass with composition of B 2 O 3-Bi 2 O 3-SiO 2-CaO-BaO-Al 2 O 3-ZrO 2 (BBSZ) modified Ba x Sr 1-x TiO 3 (BST, x = 0.3 and 0.4) ceramics were prepared by a conventional solid state
In this study, the storage performance of lead-free ceramics was optimized by constructing (1 − x)(Ba 0.8 Sr 0.2)TiO 3 –xBi(Zn 2/3 Ta 1/3)O 3 ceramics using a cooperative optimization strategy. This strategy involved
Barium strontium titanate (BST) glass-ceramics were fabricated via controlled crystallization with different crystallization routes. Effects of the microwave crystallization and
Strontium barium niobate (Ba x Sr 1−x Nb 2 O 6) ceramics, as an essential candidate system for energy storage ceramic capacitors, have received considerable attention because of their extremely high dielectric constant and relatively low dielectric loss [ 15, 16, 17 ].
Strontium barium niobate is the chemical compound Sr x Ba 1−x Nb 2 O 6 for 0.32≤x≤0.82. Strontium barium niobate is a ferroelectric material commonly used in single crystal form in electro-optics, acousto-optics, and photorefractive non-linear optics for its photorefractive properties.
In the relaxor behavior modulation step, the Bi-containing perovskite oxide (Bi0.5 K 0.5)TiO 3 (BKT) is introduced into the SBN ceramic, considering the random distribution of Bi 3+ / K+ and Ti 4+ ions in the SBN ceramic might increase the site disorder and enhance the relaxor behavior [13, 14].
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