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中国物理学会期刊

(Pb0.97La0.02)(Zr0.65Sn0.35-xTi x)O3反铁电陶瓷的热膨胀性质

CSTR: 32037.14.aps.52.2315

Thermal expansion property of (Pb0.97La0.02)(Zr0.65Sn0.35-xTix)O3 ceramics

CSTR: 32037.14.aps.52.2315
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  • 在-100—200℃温度范围内,测量了(Pb0.97La0.02)(Zr0.65Sn0.35-xTix)O3(PZST,0.1≤x≤0.14)反铁电陶 瓷的热膨胀性质.实验结果表明,组分在0.1 ≤x≤0.12的试样室温下为反铁电(AFEt)四方相,热膨胀系数(α)在低温段发生 “弯曲” ,而变温x射线衍射谱(XRD)显示材料保持四方相结构;当Ti含量在0.125≤x≤0.14时,室温 下是铁电三方相(FER),温度升高时FER→AFEt相变体 积收缩,AFEt→立方顺电(PE c)相变体积增大;变温XRD谱证明了材料相结构随温度的转变过程.用多元复杂 化合物存在 纳米线度组分非均匀的观点解释了热膨胀性质随Ti含量演化的物理机理,并得到了该系统的 温度-Ti(x)含量相图.

     

    The phase transformation and thermal expansion behaviour of (Pb0.97La 0.02(Zr0.65Sn0.35-xTix)O3 (PZST,0.1≤x≤0.14)antiferroelectric ceramics (AFEt)have been investigated as functions of temperature and Ti conte nt x.It was found that for the specimens with 0.1≤x≤0.12,the thermal expansion coefficient (α) curve showed an unusual “bending” at the temperature of T,wh ile the specimens remained a tetragonal phase.For 0.125≤x≤0.14,the specimens s howed a ferroelectric rhombohedral phase (FER) at room temperature.Wh en heated ,the FER phase was changed to an antiferroelectric tetragonal phase ( AFEt) a nd pareoelectroic cubic phase (PEc) at temperatures of TFA and Tc,resp ectively.In addition,T and TFA increased with the increase of Ti cont ent x , while Tc was decreased.The phases were detected by the XRD pattern at differ ent temperatures.The temperature-Ti content (x) phase diagram of (Pb0.97La 0.02)(Zr0.65Sn0.35-xTix)O3 was finally established.The the rmal expansion behaviour of (Pb0.97La0.02)(Zr0.65Sn0.35-xTix)O3 (0.1≤x≤0.14) have been expla ined based upon the nano-size phase s eparation of the PZST complex pervoskite compounds.

     

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