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首页> 外文期刊>Ultrasonics, Ferroelectrics and Frequency Control, IEEE Transactions on >Lattice Dynamics and Phase Transitions in KNbO3 and K0.5Na0.5NbO3 Ceramics
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Lattice Dynamics and Phase Transitions in KNbO3 and K0.5Na0.5NbO3 Ceramics

机译:KNbO3和K0.5Na0.5NbO3陶瓷的晶格动力学和相变

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摘要

Phonons in both ceramic samples KNbO3 (KN) and K0.5Na0.5NbO3 (KNN-50) were investigated from 10 to 900 K by means of Raman, infrared, and THz spectroscopy. First-order transitions from cubic to tetragonal phases were detected at about 755 K (in KN) and 710 K (in KNN-50), where the first component of the polarization appears. Transitions from the tetragonal to the orthorhombic phases take place around 510 and 475 K, respectively. The last transitions from orthorhombic to rhombohedral phases are strongly firstorder type. TC is shifted from 200 K in KN to about 90 K in KNN-50. All Raman active modes below 200 cm-1. disappear in KN but not in KNN-50. The overdamped soft mode present at high temperatures in the THz range changes its dielectric strength at each phase transition (when the corresponding component jumps to higher frequencies) and abruptly disappears from THz spectra in the rhombohedral phase, because it stiffens up to 200 cm-1. This mode has lower frequency and higher dielectric strength in KNN-50.
机译:陶瓷样品KNbO3(KN)和K0.5Na0.5NbO3(KNN-50)中的声子通过拉曼光谱,红外光谱和太赫兹光谱在10至900 K范围内进行了研究。在大约755 K(在KN中)和710 K(在KNN-50中)检测到从立方相到四方相的一阶跃迁,其中出现了极化的第一分量。从四方相到正​​交晶相的转变分别发生在510 K和475 K附近。从斜方晶相到菱面体相的最后转变是强一阶类型。 TC从KN中的200 K变为KNN-50中的约90K。 200 cm-1以下的所有拉曼活动模式。在KN中消失,但在KNN-50中消失。在THz范围内的高温下存在的过阻尼软模式会在每个相变时改变其介电强度(当相应的分量跳至更高的频率时),并且在菱面体相的THz光谱中突然消失,因为它会变硬至200 cm-1 。在KNN-50中,此模式具有较低的频率和较高的介电强度。

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