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振动光谱揭示了在以聚合物电解质电介质为栅极的有机薄膜晶体管中的静电和电化学掺杂。

Vibrational spectroscopy reveals electrostatic and electrochemical doping in organic thin film transistors gated with a polymer electrolyte dielectric.

作者信息

Kaake L G, Zou Y, Panzer M J, Frisbie C D, Zhu X-Y

机构信息

Contribution from the Departments of Chemistry and Chemical Engineering and Materials Science, University of Minnesota, Minneapolis, Minnesota 55455, USA.

出版信息

J Am Chem Soc. 2007 Jun 27;129(25):7824-30. doi: 10.1021/ja070615x. Epub 2007 Jun 1.

DOI:10.1021/ja070615x
PMID:17539635
Abstract

We apply attenuated total internal reflection Fourier transform infrared (ATR-FTIR) spectroscopy to directly probe active layers in organic thin film transistors (OTFTs). The OTFT studied uses the n-type organic semiconductor N-N'-dioctyl-3,4,9,10-perylene tetracarboxylic diimide (PTCDI-C8) and a polymer electrolyte gate dielectric made from poly(ethylene oxide) and LiClO4. FTIR spectroscopy of the device shows signatures of anionic PTCDI-C8 species and broad polaron bands when the organic semiconductor layer is doped under positive gate bias (VG). There are two distinctive doping regions: a reversible and electrostatic doping region for VG <or= 2 V and an irreversible and electrochemical doping regime for VG>2 V. On the basis of intensity loss of vibrational peaks attributed to neutral PTCDI-C8, we obtain a charge carrier density of 2.9 x 10(14)/cm2 at VG=2 V; this charge injection density corresponds to the conversion of slightly more than one monolayer of PTCDI-C8 molecules into anions. At higher gate bias voltage, electrochemical doping involving the intercalation of Li+ into the organic semiconductor film can convert all PTCDI-C8 molecules in a 30-nm film into anionic species. For comparison, when a conventional gate dielectric (polystyrene) is used, the maximum charge carrier density achievable at VG=200 V is approximately 4.5 x 10(13)/cm2, which corresponds to the conversion of 18% of a monolayer of PTCDI-C8 molecules into anions.

摘要

我们应用衰减全内反射傅里叶变换红外(ATR - FTIR)光谱法直接探测有机薄膜晶体管(OTFT)中的有源层。所研究的OTFT使用n型有机半导体N - N'-二辛基 - 3,4,9,10 - 苝四羧酸二酰亚胺(PTCDI - C8)以及由聚环氧乙烷和高氯酸锂制成的聚合物电解质栅极电介质。当有机半导体层在正栅极偏压(VG)下被掺杂时,该器件的FTIR光谱显示出阴离子PTCDI - C8物种的特征以及宽极化子带。存在两个不同的掺杂区域:对于VG≤2 V为可逆的静电掺杂区域,对于VG>2 V为不可逆的电化学掺杂区域。基于归因于中性PTCDI - C8的振动峰的强度损失,我们在VG = 2 V时获得了2.9×10¹⁴/cm²的电荷载流子密度;这种电荷注入密度对应于略多于一个单层的PTCDI - C8分子转变为阴离子。在更高的栅极偏压下,涉及Li⁺嵌入有机半导体膜的电化学掺杂可将30 nm薄膜中的所有PTCDI - C8分子转变为阴离子物种。相比之下,当使用传统的栅极电介质(聚苯乙烯)时,在VG = 200 V时可实现的最大电荷载流子密度约为4.5×10¹³/cm²,这对应于18%的单层PTCDI - C8分子转变为阴离子。

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