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arXiv 0812.3875cond-mat.mtrl-sci
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室温大极化的磁控

Magnetic control of large room-temperature polarization

Ashok Kumar, G. L. Sharma, R. S. Katiyar R. Pirc, R. Blinc J. F. Scott

摘要:

许多作者将室温下大电极化的强度的磁开关称为磁电学的圣杯,我们使用一种新的物理过程,即磁性和铁电弛豫纳米区之间的耦合,报道了这种长期寻求的效应。在这里,我们报告的正常铁电态和铁电弛豫状态之间的磁切换。这给出了新的室温、单相、多铁性磁电材料PbZr0.46Ti0.34Fe0.13W0.07O3,其极化、损耗(<4%)和电阻率(通常为108 - 109 ohm.cm)等于或优于BiFeO 3,以及新的和非常大的磁电效应:不是在施加H的情况下从+Pr切换到负Pr,而是在施加小于特斯拉的H的情况下从Pr切换到零。这种切换的极化发生不是因为传统的磁感应相变,而是因为动态效应:增加H延长了x500从<200 ns to >100?s,并且它强烈耦合极化弛豫和自旋弛豫。发散极化弛豫时间精确地拟合修改后的Vogel-Fulcher方程,其中冻结温度Tf由0.92正/负0.07特斯拉的临界冻结场Hf代替。该场依赖性和临界场Hc是从球形无规键随机场(SRBRF)模型中解析导出的,该模型没有可调参数和E2 H2耦合。该器件允许三态逻辑(+Pr,0,负Pr)和电容器,其电容具有&gt;5000%的磁场变化。

英文摘要:

Numerous authors have referred to room-temperature magnetic switching of large electric polarizations as The Holy Grail of magnetoelectricity.We report this long-sought effect using a new physical process of coupling between magnetic and ferroelectric relaxor nano-regions. Here we report magnetic switching between the normal ferroelectric state and the ferroelectric relaxor state. This gives both a new room-temperature, single-phase, multiferroic magnetoelectric, PbZr0.46Ti0.34Fe0.13W0.07O3, with polarization, loss (<4%), and resistivity (typically 108 -109 ohm.cm) equal to or superior to BiFeO3, and also a new and very large magnetoelectric effect: switching not from +Pr to negative Pr with applied H, but from Pr to zero with applied H of less than a Tesla. This switching of the polarization occurs not because of a conventional magnetically induced phase transition, but because of dynamic effects: Increasing H lengthens the relaxation time by x500 from <200 ns to >100 ?s, and it couples strongly the polarization relaxation and spin relaxations. The diverging polarization relaxation time accurately fits a modified Vogel-Fulcher Equation in which the freezing temperature Tf is replaced by a critical freezing field Hf that is 0.92 positive/negative 0.07 Tesla. This field dependence and the critical field Hc are derived analytically from the spherical random bond random field (SRBRF) model with no adjustable parameters and an E2H2 coupling. This device permits 3-state logic (+Pr,0,negative Pr) and a condenser with >5000% magnetic field change in its capacitance.

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