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Glassy Interfacial Dynamics of Ni Nanoparticles: Part I Colored Noise Dynamic Heterogeneity and Collective Atomic Motion

机译:镍纳米粒子的玻璃界面动态:第一部分有色噪声动态异质性和集体原子运动

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摘要

Most condensed materials exhibit a significant fraction of atoms, molecules or particles that are strongly interacting with each other, while being configured geometrically at any instant of time in an ‘amorphous’ state having a relatively uniform density. Recently, both simulations and experiments have revealed that the dynamics of diverse condensed amorphous materials is generally characterized by significant heterogeneity in the local mobility and by progressively increasing collective motion upon cooling that takes the form of string-like collective particle rearrangements. The direct experimental observation of this type of collective motion, which has been directly linked to the growing relaxation times of glass-forming materials, and its quantification under different thermodynamic conditions, has so far been restricted to colloidal and driven granular fluids. The present work addresses the fundamental problem of how to determine the scale of this type of collective motion in materials composed of molecules or atoms. The basic premise of our work is that large scale dynamic particle clustering in amorphous materials must give rise to large fluctuations in particle mobility so that transport properties, especially those related to particle mobility, should naturally exhibit noise related to the cooperative motion scale. In our initial exploratory study seeking a relationship of this kind, we find 1/fα or ‘colored noise’, in both potential energy and particle displacements fluctuations of the atoms within the glassy interfacial layer of Ni nanoparticles (NPs). A direct relation between the particle displacement (mobility) noise exponent α and the average polymerization index of the string-like collective motion L is observed for a range of NP sizes, temperatures and for surface doping of the NPs with other metal atoms (Ag, Au, Pt) to change of fragility of the glassy interfacial layer at the surface of the Ni NPs. We also introduce a successful analytic model to understand this relationship between α and L
机译:大多数凝聚态材料都表现出很大一部分原子,分子或粒子彼此强烈相互作用,同时在任何时刻以几何形状配置为密度相对均匀的“非晶”状态。最近,模拟和实验均表明,各种凝聚态无定形材料的动力学特征通常是局部迁移率具有明显的异质性,并且在冷却时以串状集体颗粒重排的形式逐渐增加集体运动。对这种集体运动的直接实验观察,与玻璃形成材料的弛豫时间的增长直接相关,并且在不同的热力学条件下对其进行定量分析,迄今为止仅限于胶体和驱动颗粒流体。本工作解决了一个基本问题,即如何确定由分子或原子组成的材料中这种集体运动的规模。我们工作的基本前提是,非晶态材料中的大规模动态粒子团簇必须引起粒子迁移率的大波动,以便传输特性(尤其是那些与粒子迁移率有关的特性)自然会表现出与协同运动尺度有关的噪声。在我们寻求这种关系的初步探索性研究中,我们发现1 / f α或“彩色噪声”,位于镍纳米粒子的玻璃状界面层内原子的势能和粒子位移波动中(NP)。对于一定范围的NP尺寸,温度以及NP与其他金属原子(Ag的表面掺杂)观察到了颗粒位移(迁移率)噪声指数α与弦状集体运动L的平均聚合指数之间的直接关系Au,Pt)改变Ni NPs表面玻璃状界面层的脆性。我们还介绍了一个成功的分析模型,以了解α和L之间的这种关系。

著录项

  • 期刊名称 other
  • 作者

    Hao Zhang; Jack F. Douglas;

  • 作者单位
  • 年(卷),期 -1(9),4
  • 年度 -1
  • 页码 1254–1265
  • 总页数 24
  • 原文格式 PDF
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