CsH 3 (SeO 3)的相变

Y. Makita
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引用次数: 24

摘要

研究了csh3 (SeO 3) 2的介电、热释电、热学、光学和晶体学性质。各种热释电试验表明,在居里点(-128°C)以下基本上没有净自发极化。相应的,没有出现铁电磁滞回线;D与E曲线是线性的,除了一个令人印象深刻的形式,在一个垂直于(100)的交流电场下,临界场E c在居里点T c以下的狭窄温度范围内。临界场随温度的降低而增大,可以用表达式给出;E c =2.3×10 4 (T c - T) 1/ 2v /cm。介电常数e⊥(100)在居里点处显示出一个峰值,在施加偏置直流场时,居里点会向较低的温度移动。这些介电结果可以很好地解释为场诱导的从反铁电态到准电态的过渡现象。比热作为温度函数的测量结果为δ S =0.81卡/摩尔·度。…
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Phase Transition in CsH 3 (SeO 3 ) 2
Dielectric, pyroelectric, thermal, optical and crystallographic properties of CsH 3 (SeO 3 ) 2 were studied. Various pyroelectric tests indicate essentially no net spontaneous polarization below the Curie point, -128°C. Correspondingly, no ferroelectric hysteresis loop appears; D vs E curves are linear except for an impressive form having the critical field, E c , in a narrow temperature range just below the Curie point, T c , under an applied ac field perpendicular to (100). The critical field increases with decreasing temperature and is given with sufficient approximation by an expression; E c =2.3×10 4 ( T c - T ) 1/2 V/cm. The dielectric constant, e ⊥(100) , shows a peak at the Curie point, which shifts, to lower temperature on application of a biasing dc field. These dielectric results may well be interpreted as a field-induced transition phenomenon from an antiferroelectric state to a paraelectric one. The measurement of specific heat as a function of temperature yields δ S =0.81 cal/mole·deg . The ...
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