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Moderately and strongly supercooled liquids: A temperature-derivative study of the primary relaxation time scale

机译:中度和高度过冷液体:一次弛豫时间尺度的温度导数研究

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The primary. relaxation time scale tau(T) derived from the. glass forming supercooled liquids (SCLs) is discussed within ergodic-cluster Gaussian statistics; theoretically justified near and above the glass-transformation temperature T-g. An analysis is given for the temperature-derivative data by Stickel. et al. on the steepness and the curvature of tau(T). Near the mode-coupling-theory (MCT) crossover T-c, these derivatives separate by a kink and a jump, respectively, the moderately and strongly SCL states. After accounting for the kink and the jump, the steepness remains a piecewise conitnuous function, a material-independent equation for the three fundamental characteristic temperatures, T-g, T-c, and the Vogel-Fulcher-Tamman (VFF) T-0, is found. Both states are described within the heterostructured model of solidlike clusters parametrized in a self-consistent manner by a minimum set of observable parameters: the fragility index, the MCT slowing-down exponent, and the chemical excess potential of Adam and Gibbs model (AGM). Below the Arrhenius temperature, the dynamically and thermodynamically stabilized clusters emerge with a size of around of seven to nine and two to three molecules above and close to T-g and T-c, respectively. On cooling, the main transformation of the moderately into the strongly supercooled state is due to rebuilding of the cluster structure, and is attributed to its rigidity, introduced through the cluster compressibility. It is shown that the validity of the dynamic AGM (dynamically,equivalent to the standard VFT form) is limited by the strongly supercooled state (T-g < T < T-c) where the superrigid cooperative rearranging regions,are shown to be well-chosen parametrized solidlike clusters. Extension of the basic parameter set by the observable kinetic and diffusive exponents results in prediction of a subdiffusion relaxation regime in SCLs that is distinct from that established for amorphous polymers. (c) 2005 American Institute of Physics.
机译:首要的。弛豫时间标度tau(T)从中得出。在遍历群集高斯统计中讨论了玻璃形成的过冷液体(SCL);从理论上讲,在玻璃转化温度T-g附近和之上是合理的。 Stickel对温度导数数据进行了分析。等。关于tau(T)的陡度和曲率。在模式耦合理论(MCT)交叉T-c附近,这些导数分别通过扭折和跳跃分别分离为中度和强度SCL状态。在考虑了扭结和跳动之后,陡度仍然是分段的连续函数,对于三个基本特征温度T-g,T-c和Vogel-Fulcher-Tamman(VFF)T-0,找到了与材料无关的方程。两种状态均在固体簇的异质结构模型中描述,该模型以最小的一组可观察参数以自洽的方式进行参数化:脆性指数,MCT减慢指数以及亚当和吉布斯模型(AGM)的化学过量势能。在阿伦尼乌斯温度以下,动态和热力学稳定的团簇出现,其大小分别在T-g和T-c上方并接近T-g和T-c约7至9个和2至3个分子。在冷却时,中度转变为强度过冷状态的主要转变是由于团簇结构的重建,并归因于团簇可压缩性带来的刚性。结果表明,动态AGM的有效性(在动力学上,等同于标准VFT形式)受到强过冷状态(Tg

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