Relaxor nature and superior energy storage performance of Sr2Ag0.2Na0.8Nb5O15-based tungsten bronze ceramics through B-site substitution

被引:37
|
作者
Xu, Shudong [1 ]
Shen, Saijiao [2 ]
Hao, Rui [2 ]
Peng, Zhanhui [1 ]
Zhang, Fudong [1 ]
Wu, Di [1 ]
Liang, Pengfei [3 ]
Chao, Xiaolian [1 ]
Wei, Lingling [2 ]
Yang, Zupei [1 ]
机构
[1] Shaanxi Normal Univ, Sch Mat Sci & Engn, Shaanxi Engn Lab Adv Energy Technol, Xian 710062, Shaanxi, Peoples R China
[2] Shaanxi Normal Univ, Sch Chem & Chem Engn, Key Lab Macromol Sci Shaanxi Prov, Xian 710062, Shaanxi, Peoples R China
[3] Shaanxi Normal Univ, Sch Phys & Informat Technol, Xian 710062, Shaanxi, Peoples R China
基金
中国国家自然科学基金;
关键词
Tungsten bronze ceramics; Incommensurate structural modulation; Energy storage; Charging-discharging; LEAD-FREE CERAMICS; HIGH-POWER DENSITY; FERROELECTRIC CERAMICS; ANTIFERROELECTRIC CERAMICS; ELECTRICAL-PROPERTIES; MODULATION; CAPACITORS; EFFICIENCY; PHASE; ND;
D O I
10.1016/j.cej.2021.133812
中图分类号
X [环境科学、安全科学];
学科分类号
08 ; 0830 ;
摘要
A series of Sr2Ag0.2Na0.8Nb5-xSbxO15 (SANNS) tungsten bronze ceramics were synthesized by traditional solidphase methods to investigate the impact of Sb replacement on the structure, relaxor nature, and energy storage properties. The study on the relationship between structure and relaxor behavior revealed two main conclusions: (1) as the Sb5+ content increased, the crystal structure transformed from an orthorhombic Im2a phase to Bbm2, and then to a tetragonal paraelectric P4/mbm phase, accompanied by a decrease in both the cell volume V and the tetragonality of c/a; (2) switching from ferroelectric to relaxor behavior at room temperature was realized through the doping of B-sites, which could be attributed to incommensurate local structural modulations caused by orthogonal distortion of the P4bm structure. Finally, we obtained a superior recoverable energy storage density (2.27 J/cm(3)) and an ultrahigh efficiency (93.3%) in Sr2Na0.8Ag0.2Nb4.7Sb0.3O15. The chargingdischarging performance was also evaluated: a high current density (1166.56 A/cm(2)) and a large powder density (118.54 MW/cm(3)) were achieved simultaneously.
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页数:9
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