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Electronic Material Properties - und Geowissenschaften ...

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Dielectric interface trap engineering by UV irradiation: A novel<br />

method to control OFET charge carrier transport properties<br />

N. Benson, M. Schidleja, C. Melzer, H. von Seggern<br />

For modern day electronics the integration of field effect transistors with complementary<br />

polarity on a single substrate is essential, in order to enhance the logic capability of the<br />

respective circuits. When considering organic electronics, however, this has proven<br />

difficult since most organic semiconductors exhibit either suitable hole (p) or electron (n)<br />

conduction [1]. The development of organic circuitry therefore requires the deposition of<br />

spatially separated p- and n-type organic semiconductors. However, recent publications<br />

[2,3] revealed the importance of the dielectric/semiconductor interface for charge carrier<br />

Drain<br />

Ca<br />

V DS<br />

Pentacene<br />

PMMA<br />

SiO2 ++ p - Si<br />

Gate<br />

Fig. 1: OFET configuration of both p- and n-type<br />

devices.<br />

Ca<br />

Source<br />

transport in the OFET channel, and<br />

demonstrated the feasibility to<br />

determine the OFET charge carrier<br />

transport properties by controlling the<br />

interfacial electrical trap density.<br />

In the current article we demonstrate<br />

that unipolar p- and n-type OFETs can<br />

be realized by employing pentacene<br />

as the organic semiconductor and a<br />

Ca source/drain metallization. The<br />

OFETs simply differ by UV exposure of<br />

the utilized PMMA dielectric layer in<br />

ambient atmosphere prior to the<br />

pentacene deposition. The OFET<br />

substrate is a highly p-doped<br />

1.7x1.7 cm 2 silicon waver, functioning as the gate contact, with a 200 nm thick SiO2 dry<br />

oxide. In the following, an 120 nm thick PMMA dielectric layer was spin coated from a<br />

2% wt THF solution. Subsequently, the PMMA layer of selected substrates was exposed<br />

to UV light for 10 minutes in air, using<br />

wavelengths of 254 and 185 nm with a<br />

respective intensity of 15 mW/cm 2 and<br />

1.5 mW/cm 2 . A 50 nm thick pentacene<br />

layer and 100 nm thick Ca<br />

Drain/Source contacts were then<br />

precipitated by physical vapour<br />

deposition, using a rate of 2 Å/s at a<br />

chamber base pressure

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