Duva G, Pithan L, Gerlach A, Janik A, Hinderhofer A, Schreiber F
University of Tübingen, Institute for Applied Physics, Auf der Morgenstelle 10, 72076 Tübingen, Germany.
ESRF - The European Synchrotron, 71, Avenue des Martyrs, 38000 Grenoble, France.
J Phys Condens Matter. 2021 Mar 17;33(11):115003. doi: 10.1088/1361-648X/abd11c.
The evolution of surface roughness in binary mixtures of the two molecular organic semiconductors (OSCs) diindenoperylene (DIP) as electron-donor and 1, 3, 4, 5, 7, 8-hexafluoro-tetracyano naphthoquinodimethane (F6TCNNQ) as electron-acceptor is studied. We co-deposit DIP and F6TCNNQ in vacuum with varying relative molar content while keeping a molar excess of DIP in order to produce phase-heterogeneous mixtures. The excess DIP phase segregates in pristine crystallites, whereas the remaining mixed phase is constituted by DIP:F6TCNNQ co-crystallites. We calculate the surface roughness as function of film thickness by modelling x-ray reflectivity data acquired in situ and in real-time during film growth. To model the experimental data, two distinct approaches, namely the kinematic approximation and the Parratt formalism, are applied. A comparative study of surface roughness evolution as function of DIP:F6TCNNQ mixing ratio is carried out implementing the Trofimov growth model within the kinematic approximation. Depending on the thickness regime, mixing ratio-specific trends are identified and discussed. To explain them, a growth mechanism for binary heterogeneous mixtures of strongly interacting OSCs is proposed.
研究了两种分子有机半导体(OSC)二元混合物表面粗糙度的演变,其中二茚并苝(DIP)作为电子供体,1,3,4,5,7,8 - 六氟 - 四氰基萘并二甲基苯醌(F6TCNNQ)作为电子受体。我们在真空中共沉积DIP和F6TCNNQ,改变相对摩尔含量,同时保持DIP的摩尔过量,以制备相异质混合物。过量的DIP相在原始微晶中分离,而其余的混合相由DIP:F6TCNNQ共微晶组成。我们通过对薄膜生长过程中原位实时采集的X射线反射率数据进行建模,计算表面粗糙度随薄膜厚度的变化。为了对实验数据进行建模,应用了两种不同的方法,即运动学近似和帕拉特形式。在运动学近似范围内实施特罗菲莫夫生长模型,对表面粗糙度随DIP:F6TCNNQ混合比的演变进行了比较研究。根据厚度范围,确定并讨论了混合比特定的趋势。为了解释这些趋势,提出了强相互作用OSC二元异质混合物的生长机制。