Thickness Dependence of Electronic Structure and Optical Properties of F8BT Thin Films

材料科学 轨道能级差 光致发光 薄膜 带隙 吸收光谱法 吸收(声学) 谱线 辐射传输 光电子学 光学 纳米技术 分子 化学 复合材料 物理 有机化学 天文
作者
Bita Ghasemi,Jakub Ševčík,Vojtěch Nádaždy,Karol Végsö,Peter Šiffalovič,Pavel Urbánek,Ivo Kuřitka
出处
期刊:Polymers [Multidisciplinary Digital Publishing Institute]
卷期号:14 (3): 641-641 被引量:18
标识
DOI:10.3390/polym14030641
摘要

Electronic devices based on polymer thin films have experienced a tremendous increase in their efficiency in the last two decades. One of the critical factors that affects the efficiency of polymer solar cells or light emitting devices is the presence of structural defects that controls non-radiative recombination. The purpose of this report is to demonstrate a non-trivial thickness dependence of optoelectronic properties and structure (dis)order in thin conductive poly(9,9-dioctyfluorene-alt-benzothiadiazole), F8BT, polymer films. The UV-Vis absorption spectra exhibited blue shift and peak broadening; significant changes in 0-0 and 0-1 radiative transition intensity was found in photoluminescence emission spectra. The density of state (DOS) was directly mapped by energy resolved-electrochemical impedance spectroscopy (ER-EIS). Satellite states 0.5 eV below the lowest unoccupied molecular orbital (LUMO) band were revealed for the thinner polymer films. Moreover, the decreasing of the deep states density in the band gap manifested an increment in the material structural ordering with increasing thickness. Changes in the ratio between crystalline phases with face-on and edge-on orientation of F8BT chains were identified in the films by grazing-incidence wide angle X-ray scattering technique. A thickness threshold in all investigated aspects of the films at a thickness of about 100 nm was observed that can be attributed to the development of J-H aggregation in the film structure and mutual interplay between these two modes. Although a specific structure-property relationship thickness threshold value may be expected for thin films prepared from various polymers, solvents and under different process conditions, the value of about 100 nm can be generally considered as the characteristic length scale of this phenomenon.
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