2016
DOI: 10.1016/j.jallcom.2016.05.035
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Variation of electrical properties with structural vacancies in ferroelectric niobates (Sr0.53Ba0.47)2.5−0.5Na Nb5O15 ceramics

Abstract: (Sr0.53Ba0.47)2.5-0.5xNaxNb5O15 ceramics (SBNN, 0.0 ≤ x ≤ 2.5) were prepared by the conventional solid-state reaction method. The Na + concentration varied from 0.0 to 2.5 so that the tetragonal tungsten bronze (TTB) crystal structure was designed to transform from 'unfilled' to 'filled' and then to 'stuffed' type. Apart from the change in the structural type, the effects of Na + concentration on the phase structure as well as microstructure, ferroelectric and dielectric properties were also investigated. X-ra… Show more

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Cited by 24 publications
(12 citation statements)
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“…At x = 0.4, the broad peak associated with the low-temperature dielectric anomaly in the 'unfilled' SCNN ceramics showed obvious relaxor behavior: the position of maximum relative permittivity shifted toward higher temperatures as the frequency increases. The relaxor behavior of the low-temperature dielectric anomaly is similar to that observed in (Sr 0.53 Ba 0.47 ) 2.5−0.5x Na x Nb 5 O 15 and Sr 2 NaNb 5 O 15 ceramics[20,21]. In those materials, the relaxor behavior can be attributed to the smeared-out phasetransition state, combined with subtle structure effects[20,21].…”
supporting
confidence: 71%
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“…At x = 0.4, the broad peak associated with the low-temperature dielectric anomaly in the 'unfilled' SCNN ceramics showed obvious relaxor behavior: the position of maximum relative permittivity shifted toward higher temperatures as the frequency increases. The relaxor behavior of the low-temperature dielectric anomaly is similar to that observed in (Sr 0.53 Ba 0.47 ) 2.5−0.5x Na x Nb 5 O 15 and Sr 2 NaNb 5 O 15 ceramics[20,21]. In those materials, the relaxor behavior can be attributed to the smeared-out phasetransition state, combined with subtle structure effects[20,21].…”
supporting
confidence: 71%
“…Correlations among the composition, structure and properties can be studied by modulating the alkali metal ion content in the A-sites of the TB (A1) 2 (A2) 4 Nb 10 O 30 composition to tune the structure (i.e., changing the structure from 'unfilled' to 'filled' type). Previously, we have formed the (Sr 0.53 Ba 0.47 ) 2.5−0.5x Na x Nb 5 O 15 (0.0 ≤ x ≤ 1.0) compounds by introducing the alkali metal Na + into the 'unfilled' Sr 0.53 Ba 0.47 Nb 2 O 6 ceramics [20]. It was found that the low-temperature dielectric anomalies were not observed in 'unfilled' Sr 0.53 Ba 0.47 Nb 2 O 6 ceramics.…”
Section: Introductionmentioning
confidence: 99%
“…The relative permittivity obtained at T s is e s . Rather than the dielectric anomaly corresponding to the smeared-out phasetransition state combined with subtle structure effects observed in (Sr 0.53 Ba 0.47 ) 2.5À0.5x Na x Nb 5 O 15 and Sr 2 NaNb 5 O 15 ceramics, 12,24 this intense low-temperature dielectric anomaly obtained in SCNN:xEu 3+ ceramics is considered as the ferroelastic phase transition related to the orthorhombic (2mm)-tetragonal (4mm) phase. 23,25 With increasing x, the frequency dispersion becomes stronger and the ceramics show obvious relaxor type behavior with a distinct shift of e s to higher temperatures as the frequency increases.…”
Section: Resultsmentioning
confidence: 99%
“…The complete occupation of all above A1, A2, and C sites corresponds to the 'stuffed' TB structure; C site is generally vacant, then the occupation of 6 A sites refers to the 'filled' TB structure; the occupation with only 5 out of 6 A sites refers to the 'unfilled' structure. 5,8,12 In the past decades, luminescent-ferroelectic materials have aroused considerable attention as that they can be developed for future multifunctional optoelectronic devices within a single material. [5][6][7][8][9][10][11] In addition, niobate materials with the 'filled' TB structure usually exhibit much better dielectric and ferroelectric properties compared to those with the 'unfilled' TB structure.…”
Section: Introductionmentioning
confidence: 99%
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