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.ba / Cu Doped Of Lamno <sub> 3 </ Sub> Microwave Absorption And The La <sub> 0.8 </ Sub> Of Ba <sub> 0.2 </ Sub> Of Mno <sub> 3 </ Sub> / Ni Composite System Performance Research

Posted on:2008-06-05Degree:MasterType:Thesis
Country:ChinaCandidate:J J DengFull Text:PDF
GTID:2190360215985701Subject:Condensed matter physics
Abstract/Summary:PDF Full Text Request
The microwave absorbing properties of LaMnO3 system doped byBa at A site, by Cu atB site, by Ba at A site with by Cu at B site andLa0.8Ba0.2MnO3/Ni were studied systematically. The nano-crystallinepowders of LaMnO3 doped system were prepared by sol-gel process andthe La0.8Ba0.2MnO3/Ni composite materials were prepared by physicalmixing. The analysis of DSC-TGA and FT-IR at different heat treatmenttemperature for the dry gelatin showed that the formation ofLa0.8Ba0.2MnO3 nano-crystalline experienced four stages which were theevaporation of leaving water, the decomposition of EDTA, thedecomposition of CH3COO2- and NH3- and the formation of perovskite.La1-xBaxMnO3, LaMn1-yCuyO3 and La1-xBaxMn1-yCuyO3 were perovskitestructure and their lattice parameters changed when doping contents weredifferent from XRD patterns. The shape of above powders was spherical,the size of them was less than 100nm and the diameter of nickel powderwas about 20nm from SEM. In addition, the resistivity of these sampleswas within semiconductor and changed with the doping contents.The complex permittivity and permeability were measured in thefrequency range of 2~18GHz by microwave network analyzer, thereflection coefficient and the loss tangent were calculated based onmeasured data and the absorption mechanism were studied. The resultsshowed that, the following samples had the best microwave absorbingproperties. The effective width of absorption band above 10dB was2.1GHz and the peak was 25dB when x=0.2 and the thickness was 1.6mmfor La1-xBaxMnO3. The effective width of absorption band was 2.6GHzand the peak was 20dB when y=0.1 and the thickness was 1.6mm forLaMn1-yCuyO3. The effective width of absorption band was 3.1GHz andthe peak was 28dB when y=0.1 and the thickness is 1.8mm forLa0.8Ba0.2Mn1-yCuyO3.The effective width of absorption band was 3.4GHzand the peak was 44dB when the mass proportion of La0.8Ba0.2MnO3 was62.5% and the thickness of 1.6mm for La0.8Ba0.2MnO3/Ni.The study of absorption mechanism showed that the dielectric loss of La1-xBaxMnO3 was mainly and the magnetic loss was subordinate. ForLaMn1-yCuyO3 and La0.8Ba0.2Mn1-yCuyO3, there was magnetic loss besidesdielectric loss and the two loss factors had opposite change, so the twolosses competed with each other. It was considered that there wereferromagnetic clusters and anti-ferromagnetic clusters in the materialsbecause of doping Cu and the stability of the two clusters could be linkedwith the value of microwave frequency so that they transformed witheach other. The ferromagnetic clusters resulted in magnetic loss andthe anti-ferromagnetic clusters resulted in dielectric loss. The response ofthem to different frequency gave rise to an alternative effect of dielectricloss and magnetic loss. The absorption mechanism of La0.8Ba0.2MnO3/Nisamples was a common effect of dielectric loss from La0.8Ba0.2MnO3 andmagnetic loss from nickel and the space interracial polar relaxation loss.
Keywords/Search Tags:Ba/Cu doped LaMnO3 system, nano-nickel powders, compound materials, electromagnetic loss, microwave absorption property
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