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Dielectric and phonon spectroscopy of Nb-doped Pb(Zr1-yTiy)O-3-CoFe2O4 composites

机译:Nb掺杂Pb(Zr1-yTiy)O-3-CoFe2O4复合材料的介电和声子能谱

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摘要

Broad-band dielectric and phonon response of Nb-doped (1-x)Pb(Zr1-yTiy)O(3-)xCoFe(2)O(4) composites with x - 10-30 was investigated between 0.1 MHz and 100 THz. At room temperature, a broad distribution of relaxation times causes a constant dielectric loss below 1 GHz. Above room temperature, a strong Maxwell-Wagner relaxation process dominates below 1 GHz due to the conductivity of CoFe2O4 (CF). Two additional relaxation processes are seen between 1 GHz and 1 THz. The lower-frequency one, coming from domain wall motion, disappears above T-C approximate to 650 K. The higher-frequency component slows down on heating towards TC, because it is the central mode, which drives the ferroelectric phase transition. Time-domain THz transmission and infrared reflectivity spectra reveal a mixture of polar phonons from both ferroelectric Nb-doped Pb(Zr, Ti)O-3 (PZTN) and magnetic CoFe2O4 (CF) components, while the micro-Raman scattering spectra allow to study phonons from both components separately. Similar temperature behavior of phonons as in the pure PZTN and CF was observed. While in CoFe2O4 the Raman-active phonons gradually reduce their intensities on heating due to increasing conductivity and related reduced Raman-scattering volume, some phonons in PZTN disappear above TC due to change of selection rules in the paraelectric phase. Like in the pure Pb(Zr,Ti)O-3, the soft phonon and central modes were also observed. Published by AIP Publishing.
机译:研究了在0.1 MHz和100 THz之间研究了x-10%-30%的Nb掺杂(1-x)Pb(Zr1-yTiy)O(3-)xCoFe(2)O(4)复合材料的宽带介电和声子响应.在室温下,弛豫时间的广泛分布导致介电损耗低于1 GHz。 在室温以上,由于CoFe2O4 (CF)的电导率,强烈的Maxwell-Wagner弛豫过程在1 GHz以下占主导地位。在1 GHz和1 THz之间可以看到两个额外的弛豫过程。来自畴壁运动的低频在T-C上方消失,大约为650 K。高频分量在向 TC 加热时速度减慢,因为它是驱动铁电相变的中心模式。时域太赫兹透射率和红外反射率光谱揭示了来自铁电Nb掺杂Pb(Zr,Ti)O-3(PZTN)和磁性CoFe2O4(CF)组分的极性声子的混合物,而微拉曼散射光谱允许分别研究来自两种组分的声子。观察到声子的温度行为与纯PZTN和CF相似。在CoFe2O4中,由于电导率的增加和拉曼散射体积的减小,拉曼活性声子在加热时的强度逐渐降低,而PZTN中的一些声子由于顺电相选择规则的变化而消失在TC以上。与纯Pb(Zr,Ti)O-3一样,也观察到了软声子和中心模式。由AIP Publishing出版。

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