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Piezoelectric polar nanoregions and relaxation-coupled resonances in relaxor ferroelectrics

机译:LAXERONERECRECTRICS中压电极性纳米导致和弛豫耦合共振

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摘要

indent It is a generally accepted fact that the unique dielectric propertiesof relaxor ferroelectrics are related to the formation of polar nanoregion(PNRs). Less well recognized is the corollary that, because they are polar andtherefore lack inversion symmetry, PNRs are also piezoelectric at the nanoscaleand can therefore behave as nanoresonators. Using the particular relaxorferroelectric K$_{t1-x}$Li$_{t x}$TaO$_{t 3}$ (KLT), we show that, whenelectrically excited into oscillation, these piezoelectric nanoresonators candrive macroscopic electro-mechanical resonances. Unexpectedly however, pairs ofcoupled resonances are observed, with one of the two exhibiting acharacteristic Fano-like lineshape. The complex resonance spectra can bedescribed equally well by two alternative but complementary models bothinvolving two resonances coupled through a relaxation: a purely classical onebased on two coupled damped harmonic oscillators and a semi-classical based ontwo discrete excitations coupled to each other through a continuum. Together,they provide complementary perspectives on the underlying physics of thesystem. Both reproduce the rapid evolution of the resonance spectrum acrossthree wide temperature ranges, including a phase transition range. In the hightemperature range, the coupling between modes is due to the collective $pi$relaxation of the lithium ions within PNRs and in the phase transition range to"heterophase relaxation" of the surrounding lattice between its hightemperature cubic and low temperature tetragonal phases. The coupling issuppressed in the intermediate range of the collective $pi/2$ relaxation ofthe lithium ions. Incidentally, the measured dielectric spectra are shown tobear a surprising but justifiable resemblance to the optical spectra of certainatomic vapors that exhibit electromagnetically induced transparency.
机译:缩进是普遍认为的,即松弛器铁电器的独特电介质特性与极性纳米引格(PNR)的形成有关。不太公认的是必然性,因为它们是极性的,因此缺乏反转对称性,PNR也是纳米型在纳米粒子的压电中,因此可以表现为纳米腔。使用特定的松弛剂k $ _ { tt1-x} $ ri $ _ { tt x} $ tao $ _ { tt x} $(klt),我们表明,当电促进到振荡时,这些压电纳米响应器糖化宏观电力谐振。然而,意外地,观察到耦合的共振,其中两个展示了富有的Fano的线φ之一。复杂的共振光谱可以通过两种替代但互补模型同样地涂布两种耦合通过弛豫的两个共振的互补模型:在两个耦合的阻尼谐波振荡器上纯粹的典型,通过连续函数彼此耦合到彼此的半古典基于离散激励。它们共同提供了对体系的潜在物理学的互补视角。两者都再现共振谱宽度温度范围的快速发展,包括相变范围。在高温范围内,模式之间的耦合是由于PNR中的锂离子和相转变范围内的集体$ PI $弛豫,以在其高温立方和低温四方相之间的周围晶格中的“异相体弛豫”。耦合在锂离子的集体$ Pi / 2 $弛豫的中间范围内发出。顺便提及,测量的介电光谱显示出令人惊讶的但是与具有电磁诱导的透明度的定语蒸汽的光谱的令人惊讶但合理的相似之处。

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