Difference between revisions of "Organic Field Effect Transistor Using Pentacene Single Crystals Grown by a Liquid-Phase Crystallization Process"
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The purpose of this study was to investigate a
The purpose of this study was to investigate a . a . compared to different .
==Soft matter discussion==
==Soft matter discussion==
Revision as of 02:41, 28 October 2009
Original entry: William Bonificio, AP 225, Fall 2009
Organic Field Effect Transistor Using Pentacene Single Crystals Grown by a Liquid-Phase Crystallization Process. Yasuo Kimura, Michio Niwano, Naohiko Ikuma, Kenichi Goushi, Kingo Itaya. Langmuir 2009 25 (9), 4861-4863
Soft matter keywords
Liquid-Phase Crystallization, Pentazene, Organic Field Effect Transistor (OFET), Pentacene, Tricholorbenzene.
The purpose of this study was to investigate a different fabrication technique for creating single crystals of pentacene to be used for organic field effect transistors. The liquid-phase crystallization process creates single crystals by evaporating off a solvent when pentacene is in solution. The pentacene crystals formed by this method then had their semiconducting properties measured and these properties were compared to pentacene crystals grown using different methods.
Soft matter discussion
Future devices may have a need for nanoscale structures, so research in this area is booming even without direct applications in mind. To create these structures, many scientists have already noticed that surfactant molecules can self assemble in unique ways; much research has been done on single tailed, or two tailed surfactants. The people in this study however, have used a trimeric structure, DTAD, pictured left.
The researchers used the critical concentration to create micelles from DTAD, 0.29mM, as a basis for their study. They added concentrations of 0.08, 2, 10, and 20 mM, corresponding to 0.2, 5, 25, and 50 times its cmc, respectively to a mica surface. At the lowest concentration typical islands were observed, then as the CMC was passed, parallel stripes began forming. As the concentration was then increased the islands gave way to longer and thicker parallel stripes. These can be seen in the figure on the right. The dimensions of these structures is about 1um in length, 40-80 nm in width, and 2-4nm in height.
I will refer you to the paper to look into the proposed theory for why this structure arises. It has to do with many different factors, including hydrophobic interactions, lattice matching, and electrostatic binding. A proposed structure is shown in the image to the right.