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首页> 外文期刊>Journal of Non-Crystalline Solids: A Journal Devoted to Oxide, Halide, Chalcogenide and Metallic Glasses, Amorphous Semiconductors, Non-Crystalline Films, Glass-Ceramics and Glassy Composites >Fluctuation approach for the estimation of the dynamic heterogeneity in glass-forming liquids from the dispersion in o-Ps lifetimes: Free volume fluctuations in polymers
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Fluctuation approach for the estimation of the dynamic heterogeneity in glass-forming liquids from the dispersion in o-Ps lifetimes: Free volume fluctuations in polymers

机译:根据o-Ps寿命中的分散体估算玻璃成形液中动态异质性的涨落方法:聚合物的自由体积涨落

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Positron annihilation lifetime spectra are analyzed with respect to the mean, tau(3), and mean dispersion, sigma(3), of ortho-positronium lifetimes using the new routine LifeTime, version 9.0, which assumes a log-Gaussian distribution of annihilation rates lambda = 1/tau. From these data the size distribution of subnanometer local free volumes (holes) characterized by their mean, , and mean dispersion, sigma(h) = (1/2), is derived. Pressure-volume-temperature experiments are analyzed employing the Simha-Somcynsky equation of state in order to obtain the fractional, h, and the specific, V-f = hV, hole free volume and its expansivity and compressibility. From comparison of V-f with the specific number of holes N'(h) is estimated. It is assumed that the hole size dispersion mirrors directly the fluctuation in the free volume as long as the relaxation time of structural motion is larger than the ortho-positronium lifetime of a few nanoseconds. The mean fluctuation in the fractional and specific free volume is calculated. Starting from a fluctuation approach the mean size of the smallest subvolume < V-SV > representative for structural relaxations is estimated. This volume is assumed to be closely related to the volume of a cooperatively rearranging region and to mirror the dynamic heterogeneity. Limits of this interpretation and specific features of PALS are discussed. The variation of the subvolume with temperature and pressure is analyzed. A different behavior of and sigma(h) is interpreted in terms of Donth's theory of dynamic glass transition heterogeneity. (c) 2006 Elsevier B.V. All rights reserved.
机译:使用新的例程LifeTime版本9.0,分析正电子寿命的平均值tau(3)和平均弥散度sigma(3),以分析正电子hil没寿命谱,其中假定Time灭率的对数高斯分布lambda = 1 / tau。从这些数据中,亚纳米级局部自由体积(孔)的尺寸分布以其均值和平均色散sigma(h)= (1/2)为特征是派生的。使用Simha-Somcynsky状态方程对压力-体积-温度实验进行分析,以获得分数h和空洞体积V-f = hV的比值,以及它的膨胀性和可压缩性。通过将V-f与进行比较,可以估算出特定的孔数N'(h)。只要结构运动的弛豫时间大于几纳秒的正-正电子寿命,就可以假定孔径分布直接反映了自由体积的波动。计算分数和比自由体积的平均波动。从波动方法开始,估计代表结构松弛的最小子体积的平均大小。假定该体积与协作重排区域的体积紧密相关,并反映了动态异质性。讨论了这种解释的局限性和PALS的特定功能。分析了子体积随温度和压力的变化。顿的动态玻璃化转变异质性理论解释了和sigma(h)的不同行为。 (c)2006 Elsevier B.V.保留所有权利。

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