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研究了温度、等静压力对PbLa(Zr,Sn,Ti)O3陶瓷相变、介电常数(εr)及损耗(tanδ)的影响.结果表明:在温度场下,随着温度的升高,PbLa(Zr,Sn,Ti)O3陶瓷从四方反铁电相(AFET)转变为立方顺电相(PEc),在低温段出现频率弥散现象;在压力场下,随着等静压力的增加极化过的AFE陶瓷发生FE/AFE相变,同时伴随突然的释放电荷过程;在.一定的等静压力下,经极化后变为铁电体的PbLa(Zr,Sn,Ti)O3陶瓷在温度的诱导下会转变为反铁电相,最后转变为顺电相;随着等静压力的增加,铁电/反铁电转变温度降低,反铁电/顺电转变温度上升.

参考文献

[1] Blue C T;Hicks J C .[J].Applied Physics Letters,1996,68(21):2942.
[2] Newnham R E;Ruschau G R .[J].American Ceramic Society Bulletin,1996,75(10):51.
[3] Dai Xunhu;DiGiovanni A;Dwight Viehland .[J].Journal of Applied Physics,1993,74(05):3399.
[4] Berlincourt D;Jaffe H;Krueger H H A et al.[J].Applied Physics Letters,1963,3:90.
[5] Jaffe B;Cooke W R;Jaffee H.Piezoelrctric Ceramics[M].London:Academic Press,1971:231.
[6] Shebanov L;Kusnetsov M;Sternberg A .[J].Journal of Applied Physics,1994,76(07):4301.
[7] Pan W;Zhang Q;Bhalla A et al.[J].Journal of the American Ceramic Society,1989,72:571.
[8] Pan W Y;Pan C Q;Zhang Q M et al.[J].Journal of Applied Physics,1989,66(12):6014.
[9] Gordon A;Dorfman S .[J].Physical Review B,1994,50(18):13132.
[10] Essig O;Wang P;Hartweg M et al.[J].Journal of the European Ceramic Society,1999,19:1223.
[11] Berlincourt D.IEEE Trans Sonics Ultrason[M].New York:Springer-Verlag,1966:116.
[12] Smolensky GA .[J].JPhys SocJpn,1970,28:26.
[13] Chen IW. .Structural origin of relaxer ferroelectrics - revisited[J].The journal of physics and chemistry of solids,2000(2):197-208.
[14] Kittel C .[J].Physical Review,1951,82:729.
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