单层和叠层聚合物薄膜的玻璃化转变和老化动力学

K. Fukao, Takehide Terasawa, Yuto Oda, Kenji Nakamura, Daisuke Tahara
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摘要

采用差示扫描量热法和介电弛豫光谱对聚苯乙烯(PS)和聚苯乙烯(2-氯苯乙烯)(P2CS)叠合薄膜进行了研究。与叠薄膜的玻璃化转变温度T g PS有很强的抑郁的大部分样品。然而,在高于T g的高温下退火后,堆叠薄膜在几乎等于体体系T g的温度下表现出玻璃化转变。在等温退火过程中,叠置P2CS薄膜α-过程的动力学表现出从单一薄膜样动力学到块状动力学的时间演化过程。α-过程的弛豫速率随退火时间的增加而减小。退火过程中α-动力学演化的时间尺度较重复动力学演化的时间尺度长。同时,随着退火时间的增加,α-过程弛豫时间的温度依赖关系由Arrhenius-like转变为Vogel-Fulcher-Tammann依赖性。利用介电弛豫光谱研究了厚度小于10 nm的P2CS薄膜的老化动力学。厚度为3.7 nm的P2CS薄膜的介电磁化率ε”随等温老化时间的延长而增大,而厚度大于9.0 nm的P2CS薄膜的介电磁化率ε”随等温老化时间的延长而增大。超薄膜中ε”的异常增加与薄膜内可移动的类液体层的存在密切相关。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Glass Transition and Aging Dynamics in Single and Stacked Thin Polymer Films
stacked thin films of polystyrene (PS) and poly(2-chlorostyrene) (P2CS) were investigated using differential scanning calorimetry and dielectric relaxation spectroscopy. The glass transition temperature T g of as-stacked thin films of PS has a strong depression from that of the bulk samples. However, after annealing at high temperatures above T g , the stacked thin films exhibit glass transition at a temperature almost equal to the T g of the bulk system. The dynamics of the α-process of stacked P2CS thin films show a time evolution from single thin film-like dynamics to bulk-like dynamics during the isothermal annealing process. The relaxation rate of the α-process becomes smaller with increase in the annealing time. The time scale for the evolution of the α-dynamics during the annealing process is very long compared with that for the reptation dynamics. At the same time, the temperature dependence of the relaxation time for the α-process changes from Arrhenius-like to Vogel-Fulcher-Tammann dependence with increase of the annealing time. The aging dynamics of P2CS thin films with thickness less than 10 nm were also investigated using dielectric relaxation spectroscopy. The imaginary part of the dielectric susceptibility ε " for P2CS thin films with a thickness of 3.7 nm increased with an increase in isothermal aging time, while this was not the case for P2CS thin films thicker than 9.0 nm. This anomalous increase in ε " for the ultrathin films is strongly correlated with the presence of a mobile liquid-like layer within the thin films.
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