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Electrical Transport of Mn-Zn-Ti Ferrite with Fe-Poor Composition

机译:Mn-Zn-Ti铁氧体的电气传输与Fe差的组成

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The real parts of the complex permittivity and complex impedance spectra of Mn-Zn-Ti ferrite with Fe-poor composition (FPF:Fe_2O_3 less than 50 mol percent) were measured. The relaxation time was estimated by numerical fitting of the permittivity spectra data. The relaxation time of FPF was about 10~(-5)-10~(-6) s, because dielectric relaxation occurred below 1 MHz. The resistance of the grains is separated from that of the grain boundary in the complex impedance spectra. As a result, it was found that the relaxation time is proportional to the resistance of the grains. It is reasonable to suppose that the relaxation time is related to the electrical mobility. The temperature dependences of the real parts of the complex permittivity and the complex impedance spectra of the same sample were measured. The activation energy of the resistances of the grains was a little larger than that of the relaxation times.
机译:测量Mn-Zn-Ti铁素体的复杂介电常数和复杂阻抗光谱的实际部分测量(FPF:Fe_2O_3小于50摩尔%)。 通过介电常数谱数据的数值拟合来估计松弛时间。 FPF的弛豫时间约为10〜(-5)-10〜(-6)S,因为介电松弛发生在1 MHz以下。 晶粒的电阻与复杂阻抗光谱中的晶界的电阻分离。 结果,发现松弛时间与晶粒的电阻成比例。 假设弛豫时间与电动机有关是合理的。 测量复杂介电常数的实际部分的温度依赖性和相同样品的复杂阻抗光谱。 晶粒电阻的激活能量大于松弛时间的电阻。

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