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Spectroscopic studies of the ferroelectric and magnetic phase transitions in multiferroic Sr1-xBaxMnO3

机译:多铁性Sr1-xBaxMnO3中铁电和磁相变的光谱研究

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Dielectric response of perovskite Sr1-xBaxMnO3 (x = 0.43 and 0.45) ceramics was investigated using microwave, THz and infrared spectroscopic techniques in order to study the ferroelectric and antiferromagnetic phase transitions with critical temperatures T-C approximate to 350 K and T-N approximate to 200 K, respectively. The two lowest-frequency polar phonons are overdamped above T-N and they exhibit pronounced softening on heating towards T-C. Nevertheless, permittivity epsilon' in the THz range shows only a small anomaly at T-C because the phonon contribution to epsilon' is rather small. The phonons are coupled with a central mode which provides the main contribution to the dielectric anomaly at T-C. Thus, the ferroelectric phase transition has characteristics of a crossover from displacive to order-disorder type. At the same time, the intrinsic THz central peak is partially screened by conductivity and related Maxwell-Wagner relaxation, which dominates the microwave and lower-frequency spectra. Below T-N, the ferroelectric distortion markedly decreases, which has an influence on the frequencies of both the central and soft modes. Therefore, epsilon' in the THz range increases at T-N on cooling. In spite of the strong spin-phonon coupling near T-N, surprisingly no magnetodielectric effect was observed in the THz spectra upon applying magnetic field of up to 7 T, which is in contradiction with the theoretically expected huge magnetoelectric coupling. We explain this fact as due to the insensitivity of T-N to magnetic field.
机译:使用微波,太赫兹和红外光谱技术研究了钙钛矿Sr1-xBaxMnO3(x = 0.43和0.45)陶瓷的介电响应,以研究临界温度TC约为350 K和TN约为200 K时的铁电和反铁磁相变,分别。两种最低频率的极性声子在T-N上方过阻尼,在加热到T-C时表现出明显的软化。然而,由于声子对ε'的贡献很小,因此在THz范围内的介电常数ε仅在T-C处显示出很小的异常。声子与中心模式耦合,该中心模式对T-C处的介电异常起主要作用。因此,铁电相变具有从位移型到有序无序型的过渡的特性。同时,固有的太赫兹中心峰部分被电导率和相关的麦克斯韦-瓦格纳弛豫部分屏蔽,而微波和低频频谱占主导地位。在T-N以下,铁电畸变显着降低,这对中心模式和软模式的频率都有影响。因此,在冷却时,THz范围内的THz范围内的ε增加。尽管在T-N附近有很强的自旋声子耦合,但是在施加高达7 T的磁场时,在THz光谱中却没有观察到磁电效应,这与理论上预期的巨大磁电耦合相矛盾。我们解释这一事实是由于T-N对磁场不敏感。

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