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Room-temperature paramagnetoelectric effect in magnetoelectric multiferroics Pb(Fe1/2Nb1/2)O3 and its solid solution with PbTiO3

机译:磁电的室温顺磁电效应   多铁性pb(Fe1 / 2Nb1 / 2)O3及其与pbTiO3的固溶体

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摘要

We have observed the magnetoelectric response at room temperature and abovein high-resistive ceramics made of multiferroic Pb(Fe1/2Nb1/2)O3 (PFN) andPFN-based solid solution 0.91PFN-0.09PbTiO3 (PFN-PT). The value of theparamagnetoelectric (PME) coefficient shows a pronounced maximum near theferroelectric-to-paraelectric phase transition temperature, T_C, and thendecreases sharply to zero for T>T_C. The maximal PME coefficient in PFN isabout 4x10(-18) s/A. The theoretical description of the PME effect, within theframework of a Landau theory of phase transitions allowing for realistictemperature dependences of spontaneous polarization, dielectric and magneticsusceptibilities, qualitatively reproduces well the temperature dependence ofthe PME coefficient. In particular, the Landau theory predicts the significantincrease of the PME effect at low temperatures and near the temperature of theparaelectric-to-ferroelectric phase transition, since the PME coefficient isequal to the product of the spontaneous polarization, dielectric permittivity,square of magnetic susceptibility and the coefficient quantifying the strengthof the biquadratic magnetoelectric coupling
机译:我们已经观察到了在室温及以上温度下由多铁性Pb(Fe1 / 2Nb1 / 2)O3(PFN)和PFN基固溶体0.91PFN-0.09PbTiO3(PFN-PT)制成的高阻陶瓷的磁电响应。顺磁电(PME)系数的值在铁电至顺电相变温度T_C附近显示出明显的最大值,然后在T> T_C时急剧下降至零。 PFN中的最大PME系数约为4x10(-18)s / A。在Landau的相变理论框架内,对PME效应的理论描述允许自发极化,介电和磁化率的实际温度相关性,定性地很好地再现了PME系数的温度相关性。尤其是,Landau理论预测,在低温和顺电至铁电相变温度附近,PME效应将显着增加,因为PME系数等于自发极化,介电常数,磁化率平方和量化双二次磁电耦合强度的系数

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