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Non-interacting hard ferromagnetic L10 FePt nanoparticles embedded in a carbon matrix

机译:嵌入碳基质中的非相互作用硬铁磁L10 FePt纳米颗粒

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摘要

Monodispersed ferromagnetic FePt nanoparticles, partially ordered in the L10 phase, were directly prepared without further annealing by high temperature synthesis ( ≈ 300 °C) involving poly(iV-vinyl-2-pyrrolidone) and Triton X-100 as protective agent and reaction solvent respectively. Depending on the synthesis conditions, nanoparticles with average sizes ranging from 5 to 7 nm and coercive fields reaching 0.1 T at 300 K were obtained, but they invariably aggregate by magnetic dipolar interaction. By increasing the solvent viscosity (using PEG 600), 5 nm superparamagnetic nanoparticles are embedded in an amorphous matrix derived from solvent condensation/decomposition, thus avoiding aggregation. Nanoparticles are then completely converted to the hard tetragonal L10 phase, preserving the original size, by annealing in a vacuum at higher temperatures that, at the same time, transform the matrix into amorphous carbon. Annealing at 650 °C for 3 h leads to coercive fields of about 0.25 T at RT and 1.3 T at 5 K (without reaching the saturation magnetization) and to a peculiar squeezing of the hysteresis loops. Subsequent treatments at higher temperatures induce a further shrinking of the loop and a reduction of the coercive field. The possible explanation takes into account that, by raising the annealing temperature, an increasing number of nanoparticles becomes free to rotate inside the matrix, aligning like "nano-compasses" with the applied magnetic field. However a fraction of nanoparticles remains still locked to the matrix, generating a superimposed magnetically hard contribution.
机译:直接制备L10相中部分有序的单分散铁磁FePt纳米颗粒,无需进一步退火即可通过高温合成(≈300°C)进行,其中涉及聚(IV-乙烯基-2-吡咯烷酮)和Triton X-100作为保护剂和反应溶剂分别。取决于合成条件,获得了平均粒径为5至7 nm且在300 K下矫顽场达到0.1 T的纳米粒子,但它们始终通过磁偶极相互作用聚集。通过提高溶剂粘度(使用PEG 600),将5 nm超顺磁性纳米粒子嵌入源自溶剂缩合/分解的无定形基质中,从而避免了聚集。然后,通过在较高温度下在真空中进行退火,将纳米颗粒完全转变为硬四方L10相,从而保留原始尺寸,同时将基质转变为无定形碳。在650°C下退火3 h会导致RT处的矫顽场约为0.25 T,5 K处的矫顽场约为1.3 T(未达到饱和磁化强度),并导致磁滞回线的特殊压缩。在更高温度下的后续处理引起回路的进一步收缩和矫顽场的减小。可能的解释考虑到了,通过提高退火温度,越来越多的纳米粒子可以自由地在基体内旋转,并像“纳米罗盘”一样与所施加的磁场对齐。然而,一小部分纳米颗粒仍然保持锁定在基质上,产生了叠加的硬磁作用。

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