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Aging and non-linear glassy dynamics in a mean field model

机译:平均场模型中的老化和非线性玻璃态动力学

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The mean field approach of glassy dynamics successfully describes systems which are out-of-equilibrium in their low temperature phase. In some cases an aging behaviour is found, with no stationary regime ever reached. In the presence of dissipative forces however, the dynamics is indeed stationary, but still out-of-equilibrium, as inferred by a significant violation of the fluctuation dissipation theorem. The mean field dynamics of a particle in a random but short-range correlated environment, offers the opportunity of observing both the aging and driven stationary regimes. Using a geometrical approach previously introduced by the author, we study here the relation between these two situations, in the pure relaxational limit, i.e. the zero temperature case. In the stationary regime, the velocity (v)-force (F) characteristics is a power law v ~ F~4, while the characteristic times scale like powers of v, in agreement with an early proposal by Horner. The cross-over between the aging, linear-response regime and the non-linear stationary regime is smooth, and we propose a parametrization of the correlation functions valid in both cases, by means of an "effective time". We conclude that aging and non-linear response are dual manifestations of a single out-of-equilibrium state, which might be a generic situation.
机译:玻璃态动力学的平均场方法成功地描述了在低温阶段不平衡的系统。在某些情况下,发现老化行为,从未达到静止状态。但是,在存在耗散力的情况下,动力学确实是固定的,但仍然不平衡,这是由明显违反波动耗散定理得出的。在随机但短程相关的环境中,粒子的平均场动力学提供了观察老化和驱动稳态的机会。使用作者先前介绍的几何方法,我们在纯松弛极限(即零温度情况)下研究这两种情况之间的关系。在平稳状态下,速度(v)-力(F)的特征是幂律v〜F〜4,而特征时间像v的幂一样按比例缩放,这与Horner的早期建议一致。老化,线性响应状态和非线性平稳状态之间的过渡是平滑的,我们通过“有效时间”提出了在两种情况下均有效的相关函数的参数化。我们得出结论,老化和非线性响应是单个失衡状态的双重表现,这可能是一种普遍情况。

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