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Glass transition of soft colloids

机译:软胶体的玻璃过渡

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摘要

We explore the glassy dynamics of soft colloids using microgels and charged particles interacting by steric and screened Coulomb interactions, respectively. In the supercooled regime, the structural relaxation time τ_α of both systems grows steeply with volume fraction, reminiscent of the behavior of colloidal hard spheres. Computer simulations confirm that the growth of τ_α on approaching the glass transition is independent of particle softness. By contrast, softness becomes relevant at very large packing fractions when the system falls out of equilibrium. In this nonequilibrium regime, τ_α depends surprisingly weakly on packing fraction, and time correlation functions exhibit a compressed exponential decay consistent with stress-driven relaxation. The transition to this novel regime coincides with the onset of an anomalous decrease in local order with increasing density typical of ultrasoft systems. We propose that these peculiar dynamics results from the combination of the nonequilibrium aging dynamics expected in the glassy state and the tendency of colloids interacting through soft potentials to refluidize at high packing fractions.
机译:我们探索使用微凝胶和带电粒子的软胶体的玻璃状动态,分别通过空间和筛选的库仑相互作用相互作用。在超冷度制度中,两个系统的结构弛豫时间τ_α急剧地增长,体积分数急剧地增长,让人联想到胶体硬球的行为。计算机模拟确认接近玻璃转变时的τ_α的生长与颗粒柔软性无关。相比之下,当系统脱离平衡时,柔软在非常大的填充馏分中相关。在这种非QuiliBibimime中,τ_α令人惊讶地缺乏填充部分,并且时间相关函数表现出与应力驱动的松弛一致的压缩指数衰减。向该新颖的制度的转变与局部顺序的异常减少的发作,随着超硬系统的典型密度增加。我们提出这些特殊的动态从玻璃状状态预期的非QuiBibibing动力学的组合以及通过软电位相互作用的胶体在高包装级分中的趋势。

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