2019
DOI: 10.1016/j.jeurceramsoc.2019.03.030
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A new family of sodium niobate-based dielectrics for electrical energy storage applications

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Cited by 153 publications
(42 citation statements)
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“…(5) When the amounts of CuO additives are high than 1 mol%, the P r values are contrary decreased with increasing the amounts of CuO additives shown in Figure 6b because of the less densification as mentioned in Section 3.2 and the more pinning effect by the pairs of Cu 2+ ions and oxygen vacancies [5,6,20,21]. In conclusion, the maximum remnant polarization P r = 18.93 µC/cm 2 and minimum coercive electric field E C = 8.75 kV/cm are obtained with a good piezoelectricity at 1 mol% CuO additives since there are the largest spontaneous polarizations and easily rotated under poling processing [36,37]. Figure 7 shows the piezoelectric properties (kp, Qm, d33 and g33) of the NKLNTS-ST-xCuO ceramics.…”
Section: Piezoelectric Propertiesmentioning
confidence: 72%
“…(5) When the amounts of CuO additives are high than 1 mol%, the P r values are contrary decreased with increasing the amounts of CuO additives shown in Figure 6b because of the less densification as mentioned in Section 3.2 and the more pinning effect by the pairs of Cu 2+ ions and oxygen vacancies [5,6,20,21]. In conclusion, the maximum remnant polarization P r = 18.93 µC/cm 2 and minimum coercive electric field E C = 8.75 kV/cm are obtained with a good piezoelectricity at 1 mol% CuO additives since there are the largest spontaneous polarizations and easily rotated under poling processing [36,37]. Figure 7 shows the piezoelectric properties (kp, Qm, d33 and g33) of the NKLNTS-ST-xCuO ceramics.…”
Section: Piezoelectric Propertiesmentioning
confidence: 72%
“…To further verify the relaxor behavior, the Curie–Weiss law, 40 as shown in eqn (7), was employed to calculate the diffuseness degree ( γ ), which varies from 1 (normal ferroelectric) to 2 (typical relaxor ferroelectric). 41 The γ values for BF-BT- x NT capacitors at x = 0.05 and 0.08, as shown in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…This phenomenon demonstrates that more and more long-range polar FE orders are disrupted into fragmented short-range polar states with the increase in BST content, which might be due to the local random field generated by the ion random distribution and charge imbalances. [43,56] Figure 3c reveals the unipolar P-E loops of the (1-x)NN-xBST ceramics and Figure 3d exhibits the variations of W rec and η with different BST contents under 120 kV cm À1 . As can be seen, the W rec increases from 0.47 J cm À3 for x ¼ 0.10 to 0.90 J cm À3 for x ¼ 0.20 and then decreases to 0.65 J cm À3 for x ¼ 0.40, while the corresponding η increases from 57.75% to 94.16% and then decreases to 85.70%.…”
Section: Resultsmentioning
confidence: 99%
“…[42] Yang et al reported a high W rec % 1.50 J cm À3 and a η % 68.2% in the BaTiO 3 -modified NaNbO 3 -based ceramics. [43] Especially, remarkable W rec % 12.2 J cm À3 with moderate η % 69% was achieved in the 0.76NaNbO 3 -0.24(Bi 0.5 Na 0.5 )TiO 3 AFE relaxor ceramic by Qi et al [44] However, it seems difficult to obtain giant recoverable energy storage density and high efficiency by these procedures concurrently.…”
Section: Introductionmentioning
confidence: 99%