Real-Time Microscopy of Reorientation Driven Nucleation and Growth in Pentacene Thin Films on Silicon Dioxide

被引:27
作者
Al-Mahboob, Abdullah [1 ]
Fujikawa, Yasunori [2 ]
Sakurai, Toshio [3 ]
Sadowski, Jerzy T. [1 ]
机构
[1] Brookhaven Natl Lab, Ctr Funct Nanomat, Upton, NY 11973 USA
[2] Tohoku Univ, Inst Mat Res, Aoba Ku, Sendai, Miyagi 9808577, Japan
[3] Tohoku Univ, WPI Adv Inst Mat Res, Aoba Ku, Sendai, Miyagi 9808577, Japan
关键词
monolayers; organic field-effect transistors; self-assembly; thin films; CRYSTAL; DENSITY; TRANSISTORS; EXCHANGE; ACCURATE; MOBILITY; ENERGY;
D O I
10.1002/adfm.201203427
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
The role of molecular reorientation processes in the self-assembly of anisotropic molecules, such as pentacene (Pn) is studied utilizing a unique capability of low-energy electron microscopy (LEEM) for the real-time investigation of the film growth. In Pn film on SiO2, a layer-by-layer growth is observed, albeit different from the expected VolmerWeber growth mode typical for the systems with lower adhesion (weak interfacial interaction). The observed growth mechanism is also different than conventional concept of layer-by-layer, or Frank van der Merwe growth. In the Pn/SiO2 system the nucleation density decreases in each consecutive layer, at least up to four monolayers. This growth mechanism is hereafter named inverse Stranski-Krastanov growth. Furthermore, in this growth system the second layer islands nucleate preferentially at the domain boundaries formed by the interconnections of the bottom (first layer) domains. The top layer overgrows bottom layer with its own, initial in-plane crystal orientation, regardless of the in-plane orientations in underlying Pn domains. The dark-field LEEM imaging allows us to distinguish between Pn domains having different azimuthal direction of molecular tilt. LEEM intensity versus start voltage (LEEM IV) curves taken in the vicinity of mirror potential from the first and second layer Pn islands show that the surface potential of the second layer is higher by about 0.05 eV than that of the first layer, while the surface potentials for the epitaxial and non-epitaxial parts of the second layer island are identical.
引用
收藏
页码:2653 / 2660
页数:8
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