期刊文献+

(Ba_(1-x)Sr_x)(Zn_(1/3)Nb_(2/3))O_3固溶体系统第二相的研究 被引量:1

Study on Secondary Phases of the Solid Solution of (Ba_(1-x)Sr_x)(Zn_(1/3)Nb_(2/3))O_3 System
下载PDF
导出
摘要 研究了(Ba1-xSrx)(Zn1/3Nb2/3)O3(BSZN)固溶体系统在烧结中生成的第二相,分析了第二相的分布、形貌、形成规律、机理以及对介电性能的影响。研究表明,系统的主晶相为BSZN,同时生成了大量的第二相——Ba5Nb4O15、(Ba5-xSrx)Nb4O15(x=0~5)、Ba2Nb2O7、BaNb2O6等。第二相的生成是由于ZnO的挥发造成的;烧结温度越高、烧结时间越长,ZnO的挥发越多,第二相的含量也越多。第二相的形貌大部分为长方形的板状,样品的表面部分或完全被第二相所覆盖,且有少量呈粒状散布于晶粒之间。第二相的生成会对系统介质损耗产生不利的影响。 This paper studied secondary phases of (Ba1-xSrx)(Zn1/3 Nb2/3 )O3 solid solutions system and analyzed its distributing, shape, law of form, mechanism and the effect on dielectric properties. The results showed that the main phase of system was BSZN, at the same time, lots of secondary phases: Ba5 Nb4 O15. (Ba5-x Srx)Nb4 O15 (x= 0 ~5).Ba2Nb2O7 .BaNb2O6 et al, have come into being existence. It stats that the formation of secondary phases were caused by volatilization of ZnO. Higher sintering temperature and longer sintering time can cause much more volatilization of ZnO and more formation of secondary phases. The shape of secondary phases is mostly quadrate and the surface of samples is part or full covered with secondary phases, and a small quantity of them distribute in the crystal particles with graininess shape. Secondary phases have disadvantageous effect on the dielectric loss of system.
作者 石锋
出处 《压电与声光》 CAS CSCD 北大核心 2008年第3期311-314,共4页 Piezoelectrics & Acoustooptics
关键词 微波介质陶瓷 固溶体 第二相 机理 介电性能 microwave dielectric ceramics solid solutions secondary phases mechanism dielectric properties
  • 相关文献

参考文献9

  • 1ONODA M, JUN K, KUMIKO K, et al. Ba(Zn1/3 Nb2/3) O3-Sr ( Zn1/3 Nb2/3 ) O3 solid solution ceramics with temperature-stable high dielectric constant and low microwave loss[J]. Jpn J Appl Phys, 1982, 21 (12):1 707-1 710.
  • 2COLLA 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): 3 414-3 418.
  • 3COLLA E L, REANEY I M , SETTER N. The temperature of the relative permittivity of complex perovskites and its relation to structural transformations[J].Ferroelectrics, 1992,133(2) :217-222.
  • 4SREEMOOLANDHAN H, SEBASTIAN M T, MOHANAN P. High permittivity and low ceramics in the BaO-SrO-Nb2O5 system[J]. Mter Res Bull, 1995, 30 (6) :653-658.
  • 5DESU S B, OBRVAN H M. Microwave loss quality of BaZn1/3 Ta2/3 O3 ceramics [J]. J Am Ceram Soc, 1985,68(10) : 546-551.
  • 6HONG K S, KIM I T, KIM C D. Order-disorder phase formation in the complex perovskite compounds Ba (Ni1/3 Nb2/3 )O3 and Ba ( Zn1/3 Nb2/3 ) O3 [J]. J Am Ceram Soc, 1996,79(12):3 218-3 224.
  • 7BARBER D J, MOULDING K M, ZHOU J, et al. Structural order in Ba (Zn1/3 Ta2/3 ) O3, Ba( Zn1/3 Nb2/3 ) O3 and Ba(Mg1/3Ta2/3 )O3 microwave dielectric ceramics[J]. J Mater Sci, 1997, 32(6):1 531-1 544.
  • 8HONG K S, KIM I T, KIM C D. Order-disorder phase formation in the complex perovskite compounds O Ba (Ni1/3Nb2/3)O3 and Ba(Zn1/3 Nb2/3 ) O3 [J]. J Am Ceram Soc, 1996,79(12):3 218-3 224.
  • 9WU H,DAVIES P K. Influence of non-stoichiometry on the structure and properties of Ba (Zn1/3 Nb2/3 )O3 Microwave ielectrics:Ⅱ. Compositional variations in pure BZN[J]. J Am Ceram Soc, 2006,89 (7): 2 250- 2 263.

同被引文献15

  • 1H Lu C, Tsai C C. Reaction Kinetics, Sintering Characteristics and Ordering Behaviour of Ba ( Mg1/3Ta2/3 )O3 [ J ]. J Mater Res, 1996,11 (5) : 1219 - 1227.
  • 2Sun J S, Yu J J, You J C, et al. Microwave dielectric properties of Ba ( SnxZn(1-x)/3 Nb(1-x)2/3) 03 (0 ≤x ≤ 0. 32) ceramics[J]. J Mater Sci, 1993,28(5), 2163 -2168.
  • 3Nomura S,Toyama K, Kaneta K. Dielectric properties of ceramics in the Ba( Zn1/3 Nb2/3 )O3 - Sr( Zn1/3 Nb2/3 ) O3 solid solutions[J]. Jpn Appl Phys, 1983, 22(2) :83 -86.
  • 4Nagai T, Inuzuka T, Sugiyama M, et al. Contribution of dielectric constant to change in temperature coefficient of resonat frequency in compounds[J]. Jpn J Appl Phys, 1992, 31(8) :3132 - 3236.
  • 5Kageyama K. Crystal structure and microwave properties of Ba(Zn1/3 Ta2/3 )O3 - ( Sr, Ba) ( Ga1/2 Ta1/2 ) 03 ceramics [J].J Am Ceram Soc, 1992,75 (3) :1767 - 1771.
  • 6Nagai T, Sugaiyama M, Sando M, et al. Anoumaly in the infrared active phonon modes and its relationship to the dielectric constant of ( Ba1-xSrx ) ( Mg1/3 Ta2/3 ) O3 compound [ J ]. Jpn J Appl Phys, 1996,35:5163 - 5167.
  • 7Sugiyama M, Nagai T. Anomaly of dielectric constant of solid solution and its relation to structural change [ J ]. Jpn J Appl Phys, 1993,32(9) :4360-4364.
  • 8Endo K, F ujimoto K,Murakawa K. Dielectric Properties of Ceramics in Ba( Co1/3 Nb2/3) O3 - Ba( Zn1/3 Nb2/3 ) O3 Solid Solutions [ J ]. Commun Am Ceram Soc, 1987,70 (9), C - 215 - C - 218.
  • 9Setter N, Cross L E. The contribution of structural disorder to diffuse phase transitions in ferroelectrics [ J ]. J Mater Sci, 1980,15(6) :2478 -2483.
  • 10Golla E L, Reany I M, Setter N. Effect of structural changes in complex perovskites on the temperature coefficient of the relative pennittivity[ J]. J Appl Phys, 1993,74 (5) : 3414 - 3425.

引证文献1

二级引证文献1

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部