4.7 Article

Modulating Polymer Ultrathin Film Crystalline Fraction and Orientation with Nanoscale Curvature

Journal

POLYMERS
Volume 15, Issue 22, Pages -

Publisher

MDPI
DOI: 10.3390/polym15224453

Keywords

nanostructure; interfacial interactions; nanostructured substrates; strain

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We investigated the effect of nanoscale curvature on the structure of thermally equilibrated P3HT ultrathin films using GIXRD and AFM. The results demonstrate that nanoscale curvature reduces the polymer crystalline fraction and the crystal length, and the crystal anisotropy shows a marked dependence on the substrate curvature.
We investigated the effect of nanoscale curvature on the structure of thermally equilibrated poly-3-hexylthiophene (P3HT) ultrathin films. The curvature-induced effects were investigated with synchrotron grazing incidence X-ray diffraction (GIXRD) and atomic force microscopy (AFM). Our results demonstrate that nanoscale curvature reduces the polymer crystalline fraction and the crystal length. The first effect is strongest for the lowest curvature and results in a decrease in the out-of-plane thickness of the polymer crystals. On the other hand, the crystal in-plane length decreases with the increase in substrate curvature. Finally, the semi-quantitative analysis of crystal anisotropy shows a marked dependence on the substrate curvature characterized by a minimum at curvatures between 0.00851 nm-1 and 0.0140 nm-1. The results are discussed in terms of a curvature-dependent polymer fraction, which fills the interstices between neighboring particles and cannot crystallize due to extreme space confinement. This fraction, whose thickness is highest at the lowest curvatures, inhibits the crystal nucleation and the out-of-plane crystal growth. Moreover, because of the adhesion to the curved portion of the substrates, crystals adopt a random orientation. By increasing the substrate curvature, the amorphous fraction is reduced, leading to polymer films with higher crystallinity. Finally, when the thickness of the film exceeds the particle diameter, the curvature no longer affects the crystal orientation, which, similarly to the flat case, is predominantly edge on.

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