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首页> 外文期刊>Physical review >Space group symmetries of the phases of (Pb_(0.94)Sr_(0.06))(Zr_xTi_(1-x))O_3 across the antiferrodistortive phase transition in the composition range 0.620 approx< x approx< 0.940
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Space group symmetries of the phases of (Pb_(0.94)Sr_(0.06))(Zr_xTi_(1-x))O_3 across the antiferrodistortive phase transition in the composition range 0.620 approx< x approx< 0.940

机译:(Pb_(0.94)Sr_(0.06))(Zr_xTi_(1-x))O_3在反铁畸变相变范围内的相的空间群对称性在0.620左右<x左右<0.940范围内

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摘要

The existing controversies about the space group symmetries of Pb(Zr_xTi_(1-x))O_3 (PZT) above and below the antiferrodistortive (AFD) phase-transition temperature (T_(AFD)) in the Zr~(4+)-rich (0.620 approx< x approx< 0.940) compositions are addressed using the results of dielectric, synchrotron x-ray powder diffraction (SXRPD) and neutron powder diffraction (NPD) studies. These compositions undergo an AFD phase transition above room temperature due to tilting of oxygen octahedra leading to a superlattice phase of PZT. We have substituted 6% Sr~(2+) at a Pb~(2+) site to enhance the tilt angle and thereby the intensity of the superlattice peaks. The real and imaginary parts of the complex dielectric permittivity have been used to locate the paraelectric to ferroelectric and ferroelectric to AFD phase transitions. Rietveld analysis of SXRPD and NPD profiles unambiguously reject the rhombohedral phases in the R3c and R3m space groups below and above T_(AFD), respectively, with or without a coexisting monoclinic phase in the Cm space group and confirm that the true symmetries are monoclinic in the Cc and Cm space groups below and above T_(AFD) respectively. Based on these and previous findings a phase diagram of PSZT for 0.40 ≤ x ≤ 0.90 showing stability fields of monoclinic Cc and monoclinic Cm, tetragonal P4mm, and cubic Pm3m phases has also been presented.
机译:关于富Zr〜(4+)中反铁畸变(AFD)相变温度(T_(AFD))上下Pb(Zr_xTi_(1-x))O_3(PZT)的空间群对称性的现有争论使用介电,同步加速器X射线粉末衍射(SXRPD)和中子粉末衍射(NPD)研究的结果可解决(0.620约<x约<0.940)的成分。由于氧八面体的倾斜导致PZT的超晶格相,这些组合物在室温以上经历AFD相变。我们已经在Pb〜(2+)的位置处替换了6%的Sr〜(2+),以增强倾斜角,从而增强超晶格峰的强度。复介电常数的实部和虚部已用于确定顺电到铁电和铁电到AFD的相变。对SXRPD和NPD轮廓的Rietveld分析明确地拒绝了分别在T_(AFD)之下和之上的R3c和R3m空间组中的菱面体相,在Cm空间组中存在或不存在单斜相,并确认了真实对称性在Cm空间组中是单斜相T_(AFD)之下和之上的Cc和Cm空间组。根据这些和先前的发现,还给出了0.40≤x≤0.90的PSZT的相图,显示了单斜Cc和单斜Cm,四方P4mm和立方Pm3m相的稳定性场。

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  • 来源
    《Physical review 》 |2014年第21期| 214110.1-214110.11| 共11页
  • 作者单位

    School of Materials Science and Technology, Indian Institute of Technology (Banaras Hindu University), Varanasi-221005, India;

    Forschungsneutronenquelle Heinz Maier-Leibnitz (FRM Ⅱ), Technische Universitaet Muenchen, Lichtenbergstrasse 1, D-85747 Garching bei Muenchen, Germany;

    School of Materials Science and Technology, Indian Institute of Technology (Banaras Hindu University), Varanasi-221005, India;

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