2023
DOI: 10.1016/j.ceramint.2023.01.220
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Achieving high energy storage performance by LaMg0.5Ti0.5O3 modification of multiphase engineered Bi0.5Na0.5TiO3–based ceramics

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Cited by 8 publications
(5 citation statements)
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“…The excellent integrated energy storage performance achieved can be related to the low tan δ , ultra-small P r , large E b , and induced polyphase nanodomains in the superparaelectric state. In comparison with numerous other energy storage ceramics, consisting of BNT-based, BT-based, NN-based, and other-based ceramics, 18–20,37–55,59–65 we can clearly see that at high/low electric fields, the W rec and η values are less than 5.5 J cm −3 and 90%, respectively. Encouragingly, the 0.75BNBT-0.25CTS ceramic simultaneously produces high W rec (= 5.81 J cm −3 ), ultra-high η (= 90.5%) and moderate E b , showing a more comprehensive advantage over the lead-free dielectrics reported so far, as given in Fig.…”
Section: Resultsmentioning
confidence: 76%
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“…The excellent integrated energy storage performance achieved can be related to the low tan δ , ultra-small P r , large E b , and induced polyphase nanodomains in the superparaelectric state. In comparison with numerous other energy storage ceramics, consisting of BNT-based, BT-based, NN-based, and other-based ceramics, 18–20,37–55,59–65 we can clearly see that at high/low electric fields, the W rec and η values are less than 5.5 J cm −3 and 90%, respectively. Encouragingly, the 0.75BNBT-0.25CTS ceramic simultaneously produces high W rec (= 5.81 J cm −3 ), ultra-high η (= 90.5%) and moderate E b , showing a more comprehensive advantage over the lead-free dielectrics reported so far, as given in Fig.…”
Section: Resultsmentioning
confidence: 76%
“…Lin et al prepared (1 − x (0.94Bi 0.5 Na 0.5 TiO 3 -0.06BaTiO 3 )- x LaMg 0.5 Ti 0.5 O 3 ceramics by transforming the ferroelectric phase into an ergodic relaxation phase by adjusting the tetragonal (T, P 4 bm ) and rhombohedral (R, R 3 c ) phase contents to achieve high energy storage performance ( W rec = 3.72 J cm −3 , η = 82.3%) at 270 kV cm −1 . 18 Li et al introduced K 1/2 Bi 1/2 (Zn 1/3 Nb 2/3 )O 3 in BNBT and obtained large W rec = 5.1 J cm −3 and η = 80% at a medium electric field of 290 kV cm −1 by expanding the [AO 12 ] cage and enhancing relaxation. 19 Luo et al achieved a W rec of 4.2 J cm −3 at 280 kV cm −1 by introducing Ca 2+ and Hf 4+ ions in BNBT through enhanced breakdown field strength and refinement of grains, but the η was low at 66.7%.…”
Section: Introductionmentioning
confidence: 99%
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“…12 Deng et al refined grain size through doping La(Mg 0.5 Ti 0.5 )O 3 into Bi 0.47 Na 0.47 Ba 0.06 TiO 3 and realized large W rec (3.72 J/cm 3 ) and η (82.3 %). 13 Wu et al regulated bandgap width through introducing SrHfO 3 into Bi 0.47 Na 0.47 Ba 0.06 TiO 3 ceramics and realized a high W rec (5.83 J/cm 3 ) and η (83.67 %). 14 Wang et al optimized the dielectric behavior through adding KTaO 3 to Bi 0.47 Na 0.47 Ba 0.06 TiO 3 and achieved high W rec (4.89 J/cm 3 ) and η (84 %).…”
Section: Introductionmentioning
confidence: 99%
“…Deng et al. refined grain size through doping La(Mg 0.5 Ti 0.5 )O 3 into Bi 0.47 Na 0.47 Ba 0.06 TiO 3 and realized large W rec (3.72 J/cm 3 ) and η (82.3 %) 13 . Wu et al.…”
Section: Introductionmentioning
confidence: 99%