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OS are characterized by weak intermolecular bonds of the Van der Baals type, which causes the low energy of their crystal lattice. In this regard, the electronic structure of individual molecules during the formation of a crystal does not change significantly, and the properties of the crystals almost completely preserve the individual features of the molecules in combination with new properties caused by their collective interaction. This determines the main features of optical and electrophysical properties of OS, their energy structure of neutral and ionized states. In this article, it is experimentally confirmed that the planar structure of atoms of molecular crystals, in particular, linear acenes, and therefore the number of π-electrons responsible for exciton absorption in the visible region of the spectrum determines the position of the edge of their own optical absorption. 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引用次数: 0

摘要

近几十年来,有机半导体(OS)薄膜,或它们也被称为有机分子晶体,因其在现代电子功能单元中的应用,以及因此在现代技术设备中的应用而引起了人们的特别关注。同时,OS的光学、电物理和光电性质非常重要,这既由有机分子(即起始材料)的结构决定,也由缩合物的晶体结构(即薄膜生产的技术条件)决定。在这方面,本文介绍了对OS的一些性质的研究结果以及基于它们获得薄膜的技术。OS的特征是范德巴尔斯型的弱分子间键,这导致其晶格的低能量。在这方面,在晶体形成过程中,单个分子的电子结构不会发生显著变化,晶体的性质几乎完全保留了分子的单个特征以及由其集体相互作用引起的新性质。这决定了OS的光学和电物理性质的主要特征,以及它们的中性态和电离态的能量结构。在这篇文章中,实验证实了分子晶体原子的平面结构,特别是线性苊,因此在光谱的可见光区域负责激子吸收的π-电子的数量决定了它们自身光学吸收边缘的位置。还证实,当将重元素(例如铅)的原子引入分子中时,可以观察到酞菁薄膜的光学吸收边缘的长波长偏移。当较轻元素的原子被引入酞菁分子中时,它们的平面性不会受到干扰,并且边缘的长波移要小得多。基于外来原子与相邻分子酞菁环的π-电子系统的相互作用,给出了对这种变化的解释。生产工艺参数,特别是热溅射过程中衬底的温度,对线性聚茂和金属酞菁薄膜的晶体结构和光学性能的重大影响已经得到证明和证实。显示了控制和预先设定分子晶体的薄膜冷凝物的必要性质的可能性。
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Features of obtaining and properties of thin films organic semiconductors
In recent decades, thin films of organic semiconductors (OS), or, as they are also called, organic molecular crystals, have attracted special attention in connection with a number of proposals for their use in functional units of modern electronics, and therefore in modern technological equipment. At the same time, the optical, electrophysical and photoelectric properties of OS are very important, which are determined both by the structure of organic molecules, that is, the starting material, and by the crystal structure of condensates, that is, by the technological conditions of film production. In this regard, this article presents the results of studies of some properties of OS and the technology of obtaining thin films based on them. OS are characterized by weak intermolecular bonds of the Van der Baals type, which causes the low energy of their crystal lattice. In this regard, the electronic structure of individual molecules during the formation of a crystal does not change significantly, and the properties of the crystals almost completely preserve the individual features of the molecules in combination with new properties caused by their collective interaction. This determines the main features of optical and electrophysical properties of OS, their energy structure of neutral and ionized states. In this article, it is experimentally confirmed that the planar structure of atoms of molecular crystals, in particular, linear acenes, and therefore the number of π-electrons responsible for exciton absorption in the visible region of the spectrum determines the position of the edge of their own optical absorption. It was also confirmed that the long-wavelength shift of the optical absorption edge of thin films of phthalocyanines is observed when atoms of heavy elements, for example, lead, are introduced into the molecule. When atoms of lighter elements are introduced into the phthalocyanine molecule, their planarity is not disturbed, and the long-wavelength shift of the edge is much smaller. An explanation of such changes is presented based on the interaction of foreign atoms with the π-electron system of phthalocyanine rings of neighboring molecules. The significant influence of the technological parameters of production, in particular the temperature of the substrate during thermal sputtering, on the crystal structure and optical properties of thin films of linear polyacenes and metallophthalocyanines has been demonstrated and substantiated. The possibility of controlling and presetting the necessary properties of thin-film condensates of molecular crystals is shown.
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