Bagchi Kushal, Deng Chuting, Bishop Camille, Li Yuhui, Jackson Nicholas E, Yu Lian, Toney M F, de Pablo J J, Ediger M D
Department of Chemistry, University of Wisconsin-Madison, Madison, Wisconsin 53706, United States.
Pritzker School of Molecular Engineering, University of Chicago, Chicago, Illinois 60637, United States.
ACS Appl Mater Interfaces. 2020 Jun 10;12(23):26717-26726. doi: 10.1021/acsami.0c06428. Epub 2020 May 27.
While the bulk structure of vapor-deposited glasses has been extensively studied, structure at buried interfaces has received little attention, despite being important for organic electronic applications. To learn about glass structure at buried interfaces, we study the structure of vapor-deposited glasses of the organic semiconductor DSA-Ph (1,4-di-[4-(,-diphenyl)amino]styrylbenzene) as a function of film thickness; the structure is probed with grazing incidence X-ray scattering. We deposit on silicon and gold substrates and span a film thickness range of 10-600 nm. Our experiments demonstrate that interfacial molecular packing in vapor-deposited glasses of DSA-Ph is more disordered compared to the bulk. At a deposition temperature near room temperature, we estimate ∼8 nm near the substrate can have modified molecular packing. Molecular dynamics simulations of a coarse-grained representation of DSA-Ph reveal a similar length scale. In both the simulations and the experiments, deposition temperature controls glass structure beyond this interfacial layer of a few nanometers.
虽然气相沉积玻璃的整体结构已得到广泛研究,但埋入界面处的结构却很少受到关注,尽管其对有机电子应用很重要。为了了解埋入界面处的玻璃结构,我们研究了有机半导体DSA-Ph(1,4-二-[4-(α,α-二苯基)氨基]苯乙烯基苯)气相沉积玻璃的结构随膜厚的变化;用掠入射X射线散射探测该结构。我们将其沉积在硅和金基板上,膜厚范围为10 - 600纳米。我们的实验表明,与本体相比,DSA-Ph气相沉积玻璃中的界面分子堆积更无序。在接近室温的沉积温度下,我们估计基板附近约8纳米的区域分子堆积会发生改变。对DSA-Ph的粗粒度表示进行的分子动力学模拟揭示了类似的长度尺度。在模拟和实验中,沉积温度都控制着超出这几纳米界面层的玻璃结构。