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首页> 外文期刊>The Physics of Metals and Metallography >Penetration of Radiofrequency Electromagnetic Field through Doped Lanthanum Manganites
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Penetration of Radiofrequency Electromagnetic Field through Doped Lanthanum Manganites

机译:掺杂镧锰对射频电磁场的穿透

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摘要

Penetration of a radiofrequency electromagnetic field through plates of lanthanum manganites La_(0.85)Pb_(0.15)MnO_3, La_(0.60)Pb_(0.40)MnO_33, and La_(0.68)Y_(0.07)Ba_(0.25)MnO_3 has been studied in a frequency range of/= 20 kHz-300 MHz and at a frequency of 7.4 GHz under conditions where the thickness of the skin layer is both much greater and much lower than the sample thickness. The measurements have been performed in a temperature range including the magnetic phase transition. It is shown that, in spite of the similarity of static properties, the dynamic properties of the manganites studied differ substantially and that the differences are pronounced more strongly in the frequency range above 1 MHz. In the ferromagnetic region, significant changes in the penetration coefficient occur upon magnetization for all compositions. The initial dynamic magnetic permeability has been estimated. Due to the effect of dispersion, the decrease in the dynamic magnetic permeability in manganites doped with lead begins at frequencies on the order of a few MHz; in the manganites doped with barium and yttrium, substantial changes in the coefficient of penetration of electromagnetic field are observed up to frequencies on the order of 200 MHz. The changes in the penetration coefficient in the ferromagnetic region are primarily due to changes in the dynamic magnetic susceptibility rather than in the magnetoresistance.
机译:已经在一个研究中研究了通过镧锰酸盐La_(0.85)Pb_(0.15)MnO_3,La_(0.60)Pb_(0.40)MnO_33和La_(0.68)Y_(0.07)Ba_(0.25)MnO_3板穿透的射频电磁场。在表皮层的厚度既远大于样品厚度又远小于样品厚度的条件下,频率范围为== 20 kHz-300 MHz,频率为7.4 GHz。测量是在包括磁性相变的温度范围内进行的。结果表明,尽管静态特性相似,但所研究的锰矿的动态特性仍存在很大差异,并且在1 MHz以上的频率范围内,差异更为明显。在铁磁区域中,对于所有组合物,在磁化后渗透系数都会发生显着变化。已经估计了初始动态磁导率。由于色散的影响,掺杂铅的锰矿中动态磁导率的降低始于几兆赫兹的频率。在掺有钡和钇的锰矿中,直到200 MHz左右的频率,电磁场的渗透系数都发生了显着变化。铁磁区域中的渗透系数的变化主要是由于动态磁化率的变化而不是磁阻的变化。

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