Yang Ziyu, Zhao Tianshan, Huang Xiaoxiao, Chu Xin, Tang Tianyu, Ju Yanmin, Wang Qian, Hou Yanglong, Gao Song
Department of Materials Science and Engineering , College of Engineering , Peking University , Beijing 100871 , China . Email:
Center for Applied Physics and Technology , College of Engineering , Peking University , Beijing 100871 , China.
Chem Sci. 2017 Jan 1;8(1):473-481. doi: 10.1039/c6sc01819j. Epub 2016 Aug 18.
Iron carbide nanoparticles (ICNPs) are considered to have great potential in new energy conversion, nanomagnets and biomedical applications due to their intrinsically peculiar magnetic and catalytic properties. However, the synthetic routes were greatly limited in morphology and phase controlled synthesis. In this article, we present a versatile solution chemistry route towards colloidal ICNPs (FeC-hexagonal and monoclinic syngony, FeC-monoclinic syngony and FeC-orthorhombic syngony) derived from body centered cubic Fe@FeO by introducing heteroatoms to restrain their phase transformation. We found that the phases of FeC NPs could be controlled by direct phase transformation in the drastic thermally driven procedure (defined as thermodynamical manner). Meanwhile, the selective adsorption of Cl ions weakened the bonding between Fe and C atoms, thus interfering with the penetration of C atoms to form lower carbon content FeC and FeC NPs. The kinetic mechanisms were evaluated using density functional theory (DFT) simulations focusing on the bonding energy between Fe-C and Fe-Cl atoms. All the obtained ICNPs exhibited typically soft ferromagnetic properties with the highest saturation magnetization value of 101.2 emu g and the highest Curie temperature of 497.8 K.
碳化铁纳米颗粒(ICNPs)因其固有的特殊磁性和催化性能,在新能源转换、纳米磁体和生物医学应用方面具有巨大潜力。然而,其合成路线在形态和相控合成方面受到极大限制。在本文中,我们提出了一种通用的溶液化学路线,通过引入杂原子来抑制体心立方Fe@FeO的相变,从而制备出胶体ICNPs(FeC-六方和单斜晶系、FeC-单斜晶系和FeC-正交晶系)。我们发现,在剧烈的热驱动过程中(定义为热力学方式),FeC纳米颗粒的相可以通过直接相变来控制。同时,Cl离子的选择性吸附削弱了Fe和C原子之间的键合,从而干扰了C原子的渗透,形成了低碳含量的FeC和FeC纳米颗粒。利用密度泛函理论(DFT)模拟,重点研究了Fe-C和Fe-Cl原子之间的结合能,对动力学机制进行了评估。所有获得的ICNPs都表现出典型的软铁磁性能,最高饱和磁化强度值为101.2 emu g,最高居里温度为497.8 K。