Napolitano Simone, Capponi Simona, Vanroy Bram
Laboratory of Polymer and Soft Matter Dynamics, Faculté des Sciences, Université Libre de Bruxelles, Boulevard du Triomphe, Bâtiment NO, 1050, Bruxelles, Belgium.
Eur Phys J E Soft Matter. 2013 Jun;36(6):61. doi: 10.1140/epje/i2013-13061-8. Epub 2013 Jun 24.
The structural dynamics of polymers and simple liquids confined at the nanometer scale has been intensively investigated in the last two decades in order to test the validity of theories on the glass transition predicting a characteristic length scale of a few nanometers. Although this goal has not yet been reached, the anomalous behavior displayed by some systems--e.g. thin films of polystyrene exhibit reductions of Tg exceeding 70 K and a tremendous increase in the elastic modulus--has attracted a broad community of researchers, and provided astonishing advancement of both theoretical and experimental soft matter physics. 1D confinement is achieved in thin films, which are commonly treated as systems at thermodynamic equilibrium where free surfaces and solid interfaces introduce monotonous mobility gradients, extending for several molecular sizes. Limiting the discussion to finite-size and interfacial effects implies that film thickness and surface interactions should be sufficient to univocally determine the deviation from bulk behavior. On the contrary, such an oversimplified picture, although intuitive, cannot explain phenomena like the enhancement of segmental mobility in proximity of an adsorbing interface, or the presence of long-lasting metastable states in the liquid state. Based on our recent work, we propose a new picture on the dynamics of soft matter confined in ultrathin films, focusing on non-equilibrium and on the impact of irreversibly chain adsorption on the structural relaxation. We describe the enhancement of dynamics in terms of the excess in interfacial free volume, originating from packing frustration in the adsorbed layer (Guiselin brush) at t() ≪ 1, where t() is the ratio between the annealing time and the time scale of adsorption. Prolonged annealing at times exceeding the reptation time (usually t(*) ≫ 1 induces densification, and thus reduces the deviation from bulk behavior. In this Colloquium, after reviewing the experimental approaches permitting to investigate the structural relaxation of films with one, two or no free surfaces by means of dielectric spectroscopy, we propose several methods to determine gradients of mobility in thin films, and then discuss on the unexploited potential of analyses based on the time, temperature and thickness dependence of the orientational polarization via the dielectric strength.
在过去二十年中,人们对纳米尺度下受限的聚合物和简单液体的结构动力学进行了深入研究,以检验玻璃化转变理论的有效性,该理论预测了几纳米的特征长度尺度。尽管这一目标尚未实现,但一些系统表现出的异常行为——例如聚苯乙烯薄膜的玻璃化转变温度降低超过70K,弹性模量大幅增加——吸引了众多研究人员,并为理论和实验软物质物理学带来了惊人的进展。在薄膜中实现了一维受限,薄膜通常被视为处于热力学平衡状态的系统,其中自由表面和固体界面会引入单调变化的迁移率梯度,并延伸几个分子尺寸。将讨论局限于有限尺寸和界面效应意味着薄膜厚度和表面相互作用应足以明确确定与本体行为的偏差。相反,这种过于简化的图景虽然直观,但无法解释诸如吸附界面附近链段迁移率增强,或液态中存在长期亚稳态等现象。基于我们最近的工作,我们提出了一种关于超薄膜中受限软物质动力学的新图景,重点关注非平衡态以及不可逆链吸附对结构弛豫的影响。我们用界面自由体积过剩来描述动力学增强,这源于在t()≪1时吸附层(吉斯林刷)中的堆积受挫,其中t()是退火时间与吸附时间尺度的比值。在超过链爬行时间的时间进行长时间退火(通常t(*)≫1)会导致致密化,从而减小与本体行为的偏差。在本次研讨会上,在回顾了通过介电谱研究具有一个、两个或无自由表面的薄膜结构弛豫的实验方法后,我们提出了几种确定薄膜中迁移率梯度的方法,然后讨论了基于取向极化的介电强度对时间、温度和厚度依赖性分析的未开发潜力。