Selective Nucleation of Organic Single Crystals from Vapor Phase on Nanoscopically Rough Surfaces

材料科学 橡胶 成核 并五苯 有机半导体 四烯 微电子 纳米技术 光电子学 晶体管 单晶 Crystal(编程语言) 微接触印刷 半导体 化学物理 薄膜晶体管 结晶学 化学 有机化学 分子 物理 图层(电子) 量子力学 电压 计算机科学 程序设计语言
作者
Stefan C. B. Mannsfeld,Alejandro L. Briseño,Shuhan Liu,Colin Reese,Mark E. Roberts,Zhenan Bao
出处
期刊:Advanced Functional Materials [Wiley]
卷期号:17 (17): 3545-3553 被引量:65
标识
DOI:10.1002/adfm.200700330
摘要

Abstract Organic field‐effect transistors (OFETs) are attractive for microelectronic applications such as sensor arrays or flexible displays, due to their adequate performance and relatively low production costs. Organic single‐crystal transistors have emerged as benchmark devices for studying the intrinsic charge‐transport properties in organic semiconductor materials. Conventional approaches for growing organic single crystals result in uncontrollable dimensions and the formation of extremely fragile crystals. In addition, the hand‐selection and placement of individual crystals on a device structure represents a severe limitation for producing arrays of single‐crystal transistors with high density and reasonable throughput. As a result, the application of organic single‐crystal transistors has been restricted to fundamental charge transport studies, with their commercial application not yet realizable. We recently reported a materials‐general method of fabricating large‐area arrays of patterned organic single crystals. Microcontact‐printed octadecyltriethoxysilane (OTS) film domains on smooth, inert substrates were found to act as preferential nucleation sites for single crystals for a broad range of organic semiconductor materials, such as pentacene, tetracene, rubrene and C 60 . In order to understand the underlying mechanism of preferential nucleation, the stamped OTS domains and the contact plane between the OTS domains and the organic crystals were inspected by atomic force microscopy (AFM) and optical microscopy. Our analysis suggests that crystals nucleate at the base of tall OTS pillars that form the significantly rough surface in the stamped domains. The selective nucleation inside the rough surface regions is discussed by means of a rate‐equation model of the growth process.

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