首页> 外文期刊>Journal of magnetism and magnetic materials >Surface magnetic interactions between Bi_(0.85)La_(0.15)FeO_3 and BaFe_(12)O_(19) nanomaterials in (1-x)Bi_(0.85)La_(0.15)FeO_3-(x)BaFe_(12)O_(19) nanocomposites
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Surface magnetic interactions between Bi_(0.85)La_(0.15)FeO_3 and BaFe_(12)O_(19) nanomaterials in (1-x)Bi_(0.85)La_(0.15)FeO_3-(x)BaFe_(12)O_(19) nanocomposites

机译:Bi_(0.85)La_(0.15)的表面磁相互作用(0.15)Feo_3和Bafe_(12)O_(19)纳米材料(1-x)Bi_(0.85)La_(0.15)Feo_3-(x)Bafe_(12)O_(19)纳米复合材料

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Two different sets of multiferroic nanocomposites i.e., Bi_(0.85)La_(0.15)FeO_3-(x)BaFe_(12)O_(19) with ⅹ = 0.00, 0.05, 0.10, 0.20, 0.30, 0.40, 0.50 and 1.00 have been synthesized by the solid-state reaction method and high energy planetary ball mill techniques. The peaks in the XRD patterns can be indexed to R3c crystal symmetry of Bi_(0.85)La_(0.15)FeO_3 and P63/mmc crystal symmetry of BaFe_(12)O_(19). It suggests the absence of any major chemical reaction between the two phases. Moreover, it is assumed thatBi_(0.85)La_(0.15)FeO_3 and BaFe_(12)O_(19) crystal symmetries are present in the composite independently. Magnetic properties have been improved significantly due to the incorporation of BaFe_(12)O_(19) in the composites. Vegard's law suggests that the experimentally observed magnetizations are higher than that of theoretically calculated value. The difference between the theoretical and experimental magnetization as well as the anomaly in the magnetic hysteresis have been explained by considering the magnetic interaction correlation length between Bi_(0.85)La_(0.15)FeO_3 and BaFe_(12)O_(19) magnetic phases. The hysteresis loop width (ΔH) versus M plots has been introduced to understand the magnetic interaction (exchange bias) between Bi_(0.85)La_(0.15)FeO_3 and BaFe_(12)O_(19). Magnetocrystalline anisotropy increases with the increase in the percentage of BaFe_(12)O_(19) in the composite.
机译:两组不同的多体纳米复合材料,IE,Bi_(0.85)La_(0.15)FeO_3-(x)Bafe_(12)O_(19)具有ⅹ= 0.00,0.05,0.10,0.20,0.0.30,0.40,0.50和1.00的合成通过固态反应方法和高能行星球磨机技术。 XRD图案中的峰可以索引到BAFE_(12)O_(19)的BI_(0.85)LA_(0.15)FEO_3和P63 / MMC晶体对称的R3C晶体对称。它表明两阶段之间没有任何主要的化学反应。此外,假设具有独立于复合材料中存在于复合材料中的Bi_(0.85)LA_(0.15)FEO_3和BAFE_(12)o_(19)晶体对称。由于复合材料中的BAFE_(12)O_(19)掺入了掺入BAFE_(12)O_(19)而显着提高了磁性。 Vegard的法律表明,实验观察到的磁化高于理论上计算值的磁化。通过考虑Bi_(0.85)La_(0.15)FeO_3和Bafe_(12)O_(12)o_(19)磁相之间的磁相互作用相关长度,解释了理论和实验磁化的差异以及磁滞中的异常。已经引入了滞后回路宽度(ΔH)与M个图来理解Bi_(0.85)LA_(0.15)FEO_3和BAFE_(12)O_(19)之间的磁相互作用(交换偏置)。磁镀晶各向异性随着复合材料中BAFE_(12)O_(19)的百分比增加而增加。

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