Department of Chemistry, Wayne State University , Detroit, Michigan 48202, United States.
ACS Nano. 2014 Jul 22;8(7):6814-21. doi: 10.1021/nn501149s. Epub 2014 Jun 6.
Small changes in the synthesis of MnAs nanoparticles lead to materials with distinct behavior. Samples prepared by slow heating to 523 K (type-A) exhibit the characteristic magnetostructural transition from the ferromagnetic hexagonal (α) to the paramagnetic orthorhombic (β) phase of bulk MnAs at Tp = 312 K, whereas those prepared by rapid nucleation at 603 K (type-B) adopt the β structure at room temperature and exhibit anomalous magnetic properties. The behavior of type-B nanoparticles is due to P-incorporation (up to 3%), attributed to reaction of the solvent (trioctylphosphine oxide). P-incorporation results in a decrease in the unit cell volume (∼1%) and shifts Tp below room temperature. Temperature-dependent X-ray diffraction reveals a large region of phase-coexistence, up to 90 K, which may reflect small differences in Tp from particle-to-particle within the nearly monodisperse sample. The large coexistence range coupled to the thermal hysteresis results in process-dependent phase mixtures. As-prepared type-B samples exhibiting the β structure at room temperature convert to a mixture of α and β after the sample has been cooled to 77 K and rewarmed to room temperature. This change is reflected in the magnetic response, which shows an increased moment and a shift in the temperature hysteresis loop after cooling. The proportion of α present at room temperature can also be augmented by application of an external magnetic field. Both doped (type-B) and undoped (type-A) MnAs nanoparticles show significant thermal hysteresis narrowing relative to their bulk phases, suggesting that formation of nanoparticles may be an effective method to reduce thermal losses in magnetic refrigeration applications.
MnAs 纳米颗粒合成中的微小变化会导致材料表现出截然不同的行为。通过缓慢加热至 523 K(A 型)制备的样品在 Tp = 312 K 时表现出从铁磁六方(α)相到块状 MnAs 的顺磁正交(β)相的特征磁结构转变,而通过在 603 K 快速成核(B 型)制备的样品在室温下采用β结构,并表现出异常的磁性质。B 型纳米颗粒的行为归因于 P 掺入(高达 3%),这归因于溶剂(三辛基氧化磷)的反应。P 掺入导致单位晶胞体积减小(约 1%),并将 Tp 降低至室温以下。温度依赖的 X 射线衍射揭示了高达 90 K 的大相共存区域,这可能反映了近单分散样品中颗粒间 Tp 的微小差异。大的共存范围加上热滞后导致了依赖于过程的相混合物。在室温下呈现β结构的原始制备的 B 型样品在冷却至 77 K 并重新加热至室温后,会转化为α和β的混合物。这种变化反映在磁响应中,在冷却后,磁响应显示出磁矩增加和温度滞后环的移动。通过施加外磁场,也可以增加室温下存在的α相的比例。掺杂(B 型)和未掺杂(A 型)MnAs 纳米颗粒都表现出与体相相比明显的热滞后变窄,这表明纳米颗粒的形成可能是减少磁制冷应用中热损失的有效方法。