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ZrO2掺杂对Ba(Mg1/3Ta2/3)O3陶瓷结构及介电性能的影响
作者:彭森1 2 吴孟强2 黄同成1 许建明1 周建华1 罗高峰1 张树人2 
单位:1. 邵阳学院信息工程系 湖南 邵阳 422000 2. 电子科技大学能源科学与工程学院 成都 611731 
关键词:微波介质陶瓷 掺杂 晶体结构 介电性能 
分类号:TM277
出版年,卷(期):页码:2016,44(12):0-0
DOI:10.14062/j.issn.0454-5648.2016.12.05
摘要:

采用固相烧结法制备Ba(Mg1/3Ta2/3)O3+x%ZrO2 (BMZT)微波介质陶瓷,研究了ZrO2掺杂对Ba(Mg1/3Ta2/3)O3 (BMT)微波介质陶瓷结构和介电性能的影响。结果表明:陶瓷体系中存在2种相,主晶相Ba(Mg1/3Ta2/3)O3和附加相Ba0.5TaO3。随着x的增大,陶瓷体系的相结构由六方结构逐渐向立方结构转变,同时有序相由1:2有序结构逐渐向1:1有序结构转变。添加适量的ZrO2可以促进液相烧结,当x =8时,陶瓷致密化烧结温度由纯相时的1 650 ℃以上降至1 450 ℃,表观密度ρ =     7.568 g/cm3,相对理论密度达到99.1%,BMZT体系拥有良好的微波介电性能:相对介电常数εr = 25.5,品质因数与谐振频率的乘积Qf = 137 600 GHz (8 GHz),谐振频率温度系数τf = 0.3×10–6/℃。

 

Ba(Mg1/3Ta2/3)O3 (BMT) ceramic with ZrO2 (BMZT) was prepared by a solid-state reaction technique. The structure and microwave dielectric properties were investigated. The results show that there are two phases in the ceramic, i.e., main crystalline phase of Ba(Mg1/3Ta2/3)O3 and secondary phase of Ba0.5TaO3. The crystal structure is transformed from a hexagonal structure to a cubic structure and the ordered phase is transformed from the 1:2 ordered structure to the 1:1 ordered structure when x value increases. It is indicated that the liquid phase sintering can be improved when an appropriate amount of ZrO2 is added. Compared to pure BMT ceramic, when x = 8, the BMZT ceramic shows a lower sintering temperature, its apparent density ρ is 7.568 g/cm3, its relative theoretical density is 99.1% and BMZT possesses superior microwave dielectric properties (i.e., relative dielectric constant εr of 25.5,the quality factor plus resonant frequency Qf  of  137 600 GHz (8 GHz), and the temperature coefficient of resonant frequency value τf  of 0.3×10–6/℃).

基金项目:
湖南省自然科学基金(14JJ7075, 15JJ2130);湖南省教育厅基金(13A091, 14A129); 湖南省高校科技创新团队支持计划资助。
作者简介:
彭 森(1983—),男,硕士,讲师。
参考文献:

[1]MA P P, YI L, LIU X Q, LI L, CHEN X M. Effects of post-densification annealing upon microstructures and microwave dielectric characteristics in Ba((Co0.6–x/2Zn0.4–x/2Mgx)1/3Nb2/3)O3 ceramics[J]. J Am Ceram Soc, 2013, 96(11): 3417–3424.
[2]SHI F, DONG H L. Correlation of phonon characteristics and crystal structures of Ba[Zn1/3(Nb1–xTax)2/3]O3 solid solutions[J]. J Appl Phys, 2012, 111(1): 014111–014115.
[3]HUGHES H, IDDLES D M, REANEY I M. Niobate-based microwave dielectrics suitable for third generation mobile phone base stations[J]. Appl Phys Lett, 2001, 79(18): 2952–2954.
[4]YANG J I, NAHM S, CHOI C H, LEE H J, PARK H M. Microstructure and microwave dielectric properties of Ba(Zn1/3Ta2/3)O3 ceramics with ZrO2 addition[J]. J Am Ceram Soc, 2002, 85(1): 165–168.
[5]SUN T L, CHEN X M. Raman spectra analysis for Ba[(Mg1–xNix)1/3Nb2/3]O3 microwave dielectric ceramics[J]. AIP Adv, 2015, 5(1): 3–26.
[6]ICHINOSE N, SHIMADA T. Effect of grain size and secondary phase on microwave dielectric properties of Ba(Mg1/3Ta2/3)O3 and Ba([Mg, Zn]1/3Ta2/3)O3 systems[J]. J Eur Ceram Soc, 2006, 26(10/11): 1755–1759.
[7]KUZHICHALIL P, SURENDRAN, MAILADIL T, et al. Effect of nonstoichiometry on the structure and microwave dielectric properties of Ba(Mg0.33Ta0.67)O3[J]. Chem Mater, 2004, 17(1): 142–151.
[8]WANG C H, JING X P, et al. XRD and Raman studies on the ordering/disordering of Ba(Mg1/3Ta2/3)O3[J]. J Am Ceram Soc, 2009, 92(7): 1547–1551.
[9]NING P F, LI L X, et al. Raman scattering, electronic structure and microwave dielectric properties of Ba([Mg1–xZnx]1/3Ta2/3)O3 ceramics[J]. Ceram Int, 2012, 38(2): 1391–1398.
[10]KIM B J, KIM M H, NAHM S, et al. Effect of B2O3 on the microstructure and microwave dielectric properties of Ba(Mg1/3Ta2/3)O3 ceramics[J]. J Eur Ceram Soc, 2007, 27(2/3): 1065–1069.
[11]MATSUMOTO K, HIUGA T, TAKADA K, et al. Ba(Mg1/3Ta2/3)O3 ceramics with ultra-low loss at microwave frequencies[C]. IEEE Trans Ultrason Ferroelectr Frequency Control, 1986, 33(6): 118–121.
[12]CHEN X M, SUZUKI Y. Sinterability improvement of Ba(Mg1/3Ta2/3)O3 dielectric ceramics[J]. J Mater Electronics, 1994, 5(6): 244–247.
[13]TIEN L C, CHOU C C, TSAI D S. Microstructure of Ba(Mg1/3Ta2/3)O3-BaSnO3 microwave dielectrics[J]. Ceram Int, 2000, 26(1): 57–62.
[14]SEBASTIAN M T, SURENDRAN K P. Tailoring the microwave dielectric properties of Ba(Mg1/3Ta2/3)O3 ceramics[J]. J Eur Ceram Soc, 2006, 26(10/11): 1791–1799.
[15]SHIMADA T. Far-infrared reflection and microwave properties of Ba([Mg1–xZnx]1/3,Ta2/3)O3 ceramics[J]. J Eur Ceram Soc, 2004, 24(6): 1799–1803.
[16]SINY I G, TAO R, KATIYAR R S, GUO R, BHALLA A S. Raman spectroscopy of Mg–Ta order-disorder in Ba(Mg1/3Ta2/3)O3[J]. J Phys
Chem Solids, 1998, 59(2): 181–195.
[17]KIM Y W, PARK J H, PARK J G. Local cationic ordering behavior in Ba(Mg1/3Nb2/3)O3 ceramic[J]. J Eur Ceram Soc, 2004, 24(6): 1775–1779.
[18]董云飞, 李杨珍, 袁亮亮, 等. Ba1–3x/2Lax(Mg1/3Ta2/3)O3陶瓷的微波介电性能(Eng)[J]. 硅酸盐学报, 2008, 36(6): 739–747.
DONG Yunfei, LI Yangzhen, YUAN Liangliang, et al. J Chin Ceram Soc, 2008, 36(6): 739–747.
[19]SURENDRAN K P, SEBASTIAN M T, et al. The effect of dopants on the microwave dielectric properties of Ba(Mg0.33Ta0.67)O3 ceramics[J]. J Appl Phys, 2005, 98(9): 1–9.
[20]DESU S B, O'BRYAN H M. Microwave loss quality of BZT ceramics[J]. J Am Ceram Soc, 1985, 68(10): 546–551.
[21]陈黎,吴孟强,肖勇,等. Ca–B–Si掺杂对Ba(Zn1/3Ta2/3)O3陶瓷介电性能的影响[J]. 硅酸盐学报, 2011, 39(11): 1787–1791.
CHEN Li, WU Mengqiang, XIAO Yong, et al. J Chin Ceram Soc, 2011, 39(11): 1787–1791.
[22]TANG B, FANG Z X, LI Y X, ZHANG X, ZHANG S R. Microwave dielectric properties of Ba(Co0.56Y0.04Zn0.35)1/3Nb2/3+xO3(x = −0.004 ~ 0.008) ceramics[J]. J Mater Sci: Mater Electron, 2015, 26(9): 6585–6591.
COLLA E L, REANEY I M, SETTER N. Effect of structural changes in complex perovskites on the temperature coefficient of the relative permittivity[J]. J Appl Phys, 1993, 74(5): 3414–3425.

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