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Polar nanoregions of Ca0.28Ba0.72Nb2O6 probed by second harmonic generation and Raman spectroscopy at high pressure

机译:Ca0.28Ba0.72Nb2O6的极性纳米区域在高压下通过二次谐波产生和拉曼光谱探测

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摘要

The pressure-induced ferroelectric phase transition of calcium barium niobate Ca0.28Ba0.72Nb2O6 is studied by second harmonic generation (SHG) and Raman spectroscopy. We observe the ferroelectric to paraelectric phase transition at Pc = 4 GPa and evidence for two additional local changes at 8.5 and 11.5 GPa that are interpreted as the characteristic intermediate P* and the Burns pressure PB of a relaxor phase. The pressure dependence of the SHG intensity has a Landau critical exponent of γ = 1.3 between 4 and 8.5 GPa, indicating the presence of static polar nanoregions. At higher pressures, from 8.5 to 11.5 GPa, these nanoregions become dynamic, with γ = 2.4, and disappear at 11.5 GPa. The polar nanoregions appear when only one of the two non-equivalent octahedral positions of Nb is centrosymmetric. A Landau exponent of γ = 1 above 11.5 GPa together with a change in the compression mechanism indicates that the system completes a phase transformation to a centrosymmetric space group and the polar nanoregions vanish.
机译:通过二次谐波(SHG)和拉曼光谱研究了压力诱导的铌酸钡钙Ca0.28Ba0.72Nb2O6的铁电相变。我们在Pc = 4 GPa处观察到铁电到顺电相变,并在8.5和11.5 GPa处发现了另外两个局部变化的证据,这些变化被解释为弛豫相的特征中间P * 和Burns压力PB 。 SHG强度的压力依赖性在4至8.5 GPa之间具有γ= 1.3的Landau临界指数,表明存在静态极性纳米区域。在8.5至11.5 GPa的较高压力下,这些纳米区域变成动态的,γ= 2.4,并在11.5 GPa时消失。当Nb的两个非等价八面体位置中只有一个是中心对称时,就会出现极性纳米区域。 γ= 1高于11.5 GPa的Landau指数以及压缩机制的变化表明,该系统完成了向中心对称空间群的相变,并且极性纳米区域消失了。

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  • 来源
    《Applied Physics Letters》 |2014年第26期|1-5|共5页
  • 作者单位

    Geowissenschaften, Goethe-Universität, Altenhöferallee 1, 60438 Frankfurt am Main, Germany|c|;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
  • 原文格式 PDF
  • 正文语种 eng
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  • 入库时间 2022-08-17 13:10:12

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