铣削时间对锰掺杂钴铁氧体纳米颗粒结构和电磁性能的影响

Md. Ziaul Ahsan, M. F. A. Khan, M. Islam
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引用次数: 4

摘要

本文报道了采用行星球磨技术,通过固相反应途径,在不同的研磨时间(8h和12h)下合成的锰掺杂钴铁氧体纳米颗粒的电磁性能,以调整材料在高频和微波器件中的应用。XRD分析表明材料具有立方尖晶石结构。随着磨矿时间的延长,颗粒的晶格常数和其他相关结构参数增加,但颗粒尺寸减小。对于铣削时间为8h的试样,渗透率实部正值随频率的增加而增大。但对于铣削时间为12h的样品,在2 kHz以下观察到其负值,之后变为正值。实部的负值是低频区抗磁性行为的标志,这被认为是由于Mn2+离子在B位上的反铁磁效应占主导地位。抗磁性可以使这种材料适合用于电磁抑制或屏蔽装置。在2 kHz和0.1 MHz频率下,当铣削时间为8h和12h时,样品的介电常数实部e′表现出正常的行为。铣削时间为8h的样品的虚部色散在8MHz处的峰值和铣削时间为12h的样品在1MHz处的峰值表明了各自样品在较高频率区域的共振情况,假设这是由于B位的Fe2+和Fe3+之间电子的快速希望引起的。在低频区,铣削时间为8h和12h的样品,交流电阻率随频率的增加几乎呈指数下降,分别在10 kHz和1 kHz时达到一定的最小值,之后几乎与频率无关。用cole - cole图分析了结构相关性,其中单不完全半圆对应12h磨矿样品的晶界电阻,双不完全半圆对应8h磨矿样品的晶界和晶粒电阻。在铣削时间为12h的样品中,特性阻抗几乎恒定,磁导率和介电常数相等,且涡流损耗接近于零,适合用于微带贴片天线的设计。而在铣削时间为8h时,样品的特性阻抗随频率呈线性变化,说明存在多层电容的调谐效应,可以将该样品与微带/贴片天线集成为调谐器。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Influence of Milling Time on Structural and Electromagnetic Properties of Manganese Doped Cobalt Ferrite Nanoparticles
This paper reports on the electromagnetic properties of manganese doped cobalt ferrite nanoparticles, synthesized via solid state reaction route using the planetary ball milling technique at different milling time (8h and 12h)in order to tune the material for applications in high frequency as well as microwave devices. The XRD patterns show the cubic spinel structure of the material. The lattice constant along with other associated structural parameters are found to increase but the particle size to decrease with the milling time. The positive value of real part of permeability is found to increase with the increase of frequency for the sample of milling time 8h. But for the sample of milling time 12h, its negative value is observed below 2 kHz and after onwards it becomes positive. This negative value of real part is the signature of diamagnetic behavior at the low frequency regime, which is assumed to originate due to the dominance of antiferromagnetic effect of Mn2+ ions on the B site. The diamagnetic behavior may make this material suitable to be used in electromagnetic suppression or shielding devices. The real part e' of permittivity demonstrates the normal behavior for both the sample of milling time 8h and 12h below 2 kHz and 0.1 MHz respectively. The peaks at 8MHz for the sample of milling time 8h and at 1MHz for the sample of milling time 12h in the dispersion of its imaginary part e'' indicate the resonance condition for the respective sample at the higher frequency regime, which is assumed to be originated from the faster hoping of electrons between Fe2+ and Fe3+ in the B site. At the low frequency regime, the a.c resistivity decreases almost exponentially with the increase of frequency to a certain minimum value at 10 kHz and 1 kHz for the samples of milling time 8h and 12h respectively and after onwards it becomes almost independent of frequency. The structural correlation is analyzed with the Col-Cole plot where the single incomplete semicircle corresponds to the grain boundary resistance for 12h milled sample and double incomplete semicircles to both the grain boundary and grain resistances for 8h milled sample. Almost constant characteristic impedance implies that both the permeability and permittivity are of equal value for the sample of milling time 12h and its nearer-to-zero value of eddy current loss may make this material suitable to be used in the design of microstrip/patch antenna. However the linear variation of characteristic impedance with the frequency for the sample of milling time 8h implies the tuning effect of multilayer capacitance, which may make this sample to be integrated as tuner with the microstrip/patch antenna.
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