Zhang Hao, Douglas Jack F
Department of Chemical and Materials Engineering, University of Alberta, AB T6G 2V4 Canada.
Materials Science and Engineering Division, National Institute of Standards and Technology, Gaithersburg, Maryland, 20899 USA.
Soft Matter. 2013 Jan 28;9(4):1254-1265. doi: 10.1039/C2SM26789F.
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 related to the cooperative motion scale. In our initial exploratory study seeking a relationship of this kind, we find 1/ 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 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
大多数凝聚态物质都有很大一部分原子、分子或粒子彼此之间强烈相互作用,同时在任何时刻都以密度相对均匀的“非晶态”进行几何构型。最近,模拟和实验都表明,各种凝聚态非晶材料的动力学一般具有局部迁移率显著的不均匀性,以及在冷却时逐渐增加的集体运动,这种集体运动表现为类似弦的集体粒子重排形式。这种与玻璃形成材料不断增长的弛豫时间直接相关的集体运动的直接实验观测,以及在不同热力学条件下对其进行量化,目前仅限于胶体和驱动颗粒流体。本工作解决了如何确定由分子或原子组成的材料中这种集体运动尺度的基本问题。我们工作的基本前提是,非晶材料中的大规模动态粒子聚集必然会导致粒子迁移率的大幅波动,因此传输性质,尤其是那些与粒子迁移率相关的性质,自然应该表现出与协同运动尺度相关的特征。在我们最初探索这种关系的研究中,我们在镍纳米颗粒(NPs)玻璃态界面层内原子的势能和粒子位移波动中发现了1/f或“有色噪声”。对于一系列NP尺寸、温度以及用其他金属原子(Ag、Au、Pt)对NPs进行表面掺杂以改变Ni NPs表面玻璃态界面层的脆性的情况,观察到了粒子位移(迁移率)噪声指数α与类似弦的集体运动的平均聚合指数之间的直接关系。我们还引入了一个成功的解析模型来理解α与……之间的这种关系