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Glassy Interfacial Dynamics of Ni Nanoparticles: Part II Discrete Breathers as an Explanation of Two-Level Energy Fluctuations

机译:镍纳米粒子的玻璃界面动态:第二部分离散呼吸为两级能量波动的一种解释

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摘要

Recent studies of the dynamics of diverse condensed amorphous materials have indicated significant heterogeneity in the local mobility and a progressive increase in collective particle motion upon cooling that takes the form of string-like particle rearrangements. In a previous paper (Part I), we examined the possibility that fluctuations in potential energy E and particle mobility μ associated with this ‘dynamic heterogeneity’ might offer information about the scale of collective motion in glassy materials based on molecular dynamics simulations of the glassy interfacial region of Ni nanoparticles (NPs) at elevated temperatures. We found that the noise exponent associated with fluctuations in the Debye-Waller factor, a mobility related quantity, was directly proportional to the scale of collective motion L under a broad range of conditions, but the noise exponent associated with E(t) fluctuations was seemingly unrelated to L. In the present work, we focus on this unanticipated difference between potential energy and mobility fluctuations by examining these quantities at an atomic scale. We find that the string atoms exhibit a jump-like motion between two well-separated bands of energy states and the rate at which these jumps occur seems to be consistent with the phenomenology of the ‘slow-beta’ relaxation process of glass-forming liquids. Concurrently with these local E(t) jumps, we also find ‘quake-like’ particle displacements having a power-law distribution in magnitude so that particle displacement fluctuations within the strings are strikingly different from local E(t) fluctuations. An analysis of these E(t) fluctuations suggests that we are dealing with ‘discrete breather’ excitations in which large energy fluctuations develop in arrays of non-linear oscillators by virtue of large anharmonicity in the interparticle interactions and discreteness effects associated with particle packing. We quantify string collective motions on a fast caging times scale (picoseconds) and explore the significance of these collective motions for understanding the Boson peak of glass-forming materials.
机译:最近对各种凝聚态无定形材料的动力学研究表明,在局部迁移中存在明显的异质性,冷却后集体颗粒运动以线状颗粒重排的形式逐渐增加。在上一篇论文(第I部分)中,我们基于玻璃态的分子动力学模拟,研究了与这种“动态异质性”相关的势能E和粒子迁移率μ的波动可能提供有关玻璃态材料中集体运动尺度的信息的可能性。 Ni纳米颗粒(NPs)在高温下的界面区域。我们发现,在广泛的条件下,与Debye-Waller因子(与迁移率相关的量)的波动相关的噪声指数与集体运动L的大小成正比,而与E(t)波动相关的噪声指数为似乎与L无关。在当前工作中,我们通过在原子尺度上检查这些量来关注势能和迁移率波动之间的这一意想不到的差异。我们发现,串状原子在两个良好分隔的能态带之间表现出类似跳跃的运动,并且这些跳跃发生的速率似乎与玻璃液体形成的“慢β”弛豫过程的现象学一致。 。与这些局部E(t)跃迁同时,我们还发现了“震级”粒子位移,其大小具有幂律分布,因此琴弦内的粒子位移波动与局部E(t)波动明显不同。对这些E(t)涨落的分析表明,我们正在处理“离散呼吸”激发,其中非线性振动器阵列中的大能量涨落是由于粒子间相互作用中的大不谐和以及与粒子堆积相关的离散效应而产生的。我们以快速的笼形时间尺度(皮秒)量化弦的集体运动,并探索这些集体运动对于理解玻璃形成材料的玻色子峰的重要性。

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  • 期刊名称 other
  • 作者

    Hao Zhang; Jack F. Douglas;

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  • 年(卷),期 -1(9),4
  • 年度 -1
  • 页码 1266–1280
  • 总页数 28
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