Nanosecond Time-Resolved Microscopic Gate-Modulation Imaging of Polycrystalline Organic Thin-Film Transistors

被引:8
|
作者
Matsuoka, Satoshi [1 ,2 ]
Tsutsumi, Jun'ya [2 ]
Matsui, Hiroyuki [3 ]
Kamata, Toshihide [1 ,2 ]
Hasegawa, Tatsuo [2 ,4 ]
机构
[1] Univ Tsukuba, Grad Sch Pure & Appl Sci, 1-1-1 Tennoudai, Tsukuba, Ibaraki 3058571, Japan
[2] Natl Inst Adv Ind Sci & Technol, Tsukuba Cent 5,1-1-1 Higashi, Tsukuba, Ibaraki 3058565, Japan
[3] Yamagata Univ, Grad Sch Organ Mat Sci, Res Ctr Organ Elect ROEL, 4-3-16 Jonan, Yonezawa, Yamagata 9928510, Japan
[4] Univ Tokyo, Dept Appl Phys, Bunkyo Ku, 7-3-1 Hongo, Tokyo 1138656, Japan
来源
PHYSICAL REVIEW APPLIED | 2018年 / 9卷 / 02期
基金
日本科学技术振兴机构; 日本学术振兴会;
关键词
FIELD-EFFECT TRANSISTORS; LARGE-AREA ELECTRONICS; CONTACT RESISTANCE; ARTIFICIAL SKIN; TEMPERATURE; MOBILITY; SILICON; TRANSPORT; VOLTAGE; POLYMER;
D O I
10.1103/PhysRevApplied.9.024025
中图分类号
O59 [应用物理学];
学科分类号
摘要
We develop a time-resolved microscopic gate-modulation (mu GM) imaging technique to investigate the temporal evolution of the channel current and accumulated charges in polycrystalline pentacene thin-film transistors (TFTs). A time resolution of as high as 50 ns is achieved by using a fast image-intensifier system that could amplify a series of instantaneous optical microscopic images acquired at various time intervals after the stepped gate bias is switched on. The differential images obtained by subtracting the gate-off image allows us to acquire a series of temporal mu GM images that clearly show the gradual propagation of both channel charges and leaked gate fields within the polycrystalline channel layers. The frontal positions for the propagations of both channel charges and leaked gate fields coincide at all the time intervals, demonstrating that the layered gate dielectric capacitors are successively transversely charged up along the direction of current propagation. The initial mu GM images also indicate that the electric field effect is originally concentrated around a limited area with a width of a few micrometers bordering the channel-electrode interface, and that the field intensity reaches a maximum after 200 ns and then decays. The time required for charge propagation over the whole channel region with a length of 100 mu m is estimated at about 900 ns, which is consistent with the measured field-effect mobility and the temporal-response model for organic TFTs. The effect of grain boundaries can be also visualized by comparison of the mu GM images for the transient and the steady states, which confirms that the potential barriers at the grain boundaries cause the transient shift in the accumulated charges or the transient accumulation of additional charges around the grain boundaries.
引用
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页数:10
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