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通过溶液法制备离散的、可分散的 MnAs 纳米晶:纳米尺度上的相控制和磁学后果。

Discrete, dispersible MnAs nanocrystals from solution methods: phase control on the nanoscale and magnetic consequences.

机构信息

Department of Chemistry, Wayne State University, Detroit, Michigan 48202, USA.

出版信息

ACS Nano. 2009 May 26;3(5):1129-38. doi: 10.1021/nn900194f.

Abstract

Nanocrystals of thermodynamically stable alpha-MnAs (hexagonal NiAs-type) and metastable beta-MnAs (orthorhombic MnP-type) have been synthesized by the reaction of triphenylarsine oxide (Ph(3)AsO) and dimanganesedecacarbonyl (Mn(2)CO(10)) at temperatures ranging from 250 to 330 degrees C in the presence of the coordinating solvent trioctylphosphine oxide (TOPO). Morphologically, both alpha- and beta-MnAs nanoparticles adopt a core-shell type structure with a crystalline core and low-contrast noncrystalline shell. In contrast to prior studies on MnAs particles, disks, and films, the present bottom-up synthesis yields discrete, dispersible MnAs nanoparticles without a structural support. Even in the absence of epitaxial strain, the lattice parameters of the nanocrystals are decreased relative to bulk MnAs, resulting in a volume decrease of 0.35% in alpha-MnAs and 0.38% in beta-MnAs nanoparticles. In contrast to bulk MnAs, where the ferromagnetic phase transition upon warming through 313-317 K is concomitant with a structure change from ferromagnetic alpha- to paramagnetic beta-MnAs, powder X-ray diffraction studies suggest there is no conversion of alpha-MnAs to beta over the temperature range 298-343 K. Moreover, magnetic measurements suggest that both alpha- and beta-MnAs are ferromagnetic with T(C) approximately 315 K. Partial phase transformation of beta-MnAs nanoparticles into thermodynamically stable alpha-MnAs occurs slowly over time (i.e., months) at room temperature. However, there is no associated change in magnetization, suggesting the ferromagnetism observed in beta-MnAs is intrinsic and cannot be attributed to alpha-MnAs impurities.

摘要

热力学稳定的α-MnAs(六方 NiAs 型)和亚稳β-MnAs(正交 MnP 型)纳米晶已通过三苯基氧化膦(Ph(3)AsO)和二茂铁十二羰基(Mn(2)CO(10))之间的反应合成,反应温度范围为 250 至 330°C,在配位溶剂三辛基氧化膦(TOPO)的存在下。形态上,α-和β-MnAs 纳米颗粒均采用核壳结构,具有结晶核和低对比度非晶壳。与先前关于 MnAs 颗粒、盘和薄膜的研究相比,本底向上合成产生了离散的、可分散的 MnAs 纳米颗粒,而无需结构支撑。即使没有外延应变,纳米晶的晶格参数也相对于块状 MnAs 减小,导致α-MnAs 纳米晶的体积减小 0.35%,β-MnAs 纳米晶的体积减小 0.38%。与块状 MnAs 不同,在通过 313-317 K 升温时的铁磁相变伴随着从铁磁α-MnAs 到顺磁β-MnAs 的结构变化,粉末 X 射线衍射研究表明,在 298-343 K 的温度范围内,α-MnAs 没有转化为β-MnAs。此外,磁性测量表明,α-MnAs 和β-MnAs 均为铁磁体,T(C)约为 315 K。β-MnAs 纳米颗粒的部分相转变为热力学稳定的α-MnAs 会在室温下随着时间的推移(即数月)缓慢发生。然而,磁化强度没有变化,这表明在β-MnAs 中观察到的铁磁性是本征的,不能归因于α-MnAs 杂质。

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