A Fully Integrated Ferroelectric Thin‐Film‐Transistor – Influence of Device Scaling on Threshold Voltage Compensation in Displays

材料科学 薄膜晶体管 光电子学 晶体管 阈值电压 无定形固体 AMOLED公司 铁电性 电介质 电压 纳米技术 电气工程 图层(电子) 有源矩阵 工程类 有机化学 化学
作者
David Lehninger,Martin Ellinger,Tarek Ali,Songrui Li,Konstantin Mertens,Maximilian Lederer,Ricardo Olivio,Thomas Kämpfe,Norbert Hanisch,Kati Biedermann,Matthias Rudolph,Varvara Brackmann,Shawn Sanctis,Michael P. M. Jank,Konrad Seidel
出处
期刊:Advanced electronic materials [Wiley]
卷期号:7 (6) 被引量:51
标识
DOI:10.1002/aelm.202100082
摘要

Abstract Thin‐film transistors (TFTs) based on amorphous indium‐gallium‐zinc‐oxide (a‐IGZO) have attracted vast attention for use in organic light‐emitting diode (AMOLED) displays due to their high electron mobility and large current on–off ratio. Although amorphous oxide semiconductors show considerably less threshold voltage ( V th ) variation than poly‐silicon, large‐area processing and degradation effects can impede the characteristic parameters of a‐IGZO TFTs, which manifests in an uneven brightness distribution across the display panel. Such V th variations are usually reduced by additional compensation circuits consisting of TFTs and capacitors. Herein, a new approach to compensate such variabilities is demonstrated: the integration of a programmable ferroelectric (FE) film in the gate stack of the TFT. This simplifies the complexity of the pixel cell and potentially minimizes the need for compensation circuits, which is crucial for transparent displays. To test this new approach, fully integrated FE‐TFTs (i.e., with vias contacting a structured bottom gate electrode from the top) based on a‐IGZO and FE hafnium‐zirconium oxide (HZO) are developed. A single low‐temperature post‐fabrication treatment at 350 °C for 1 h in air is used to simultaneously crystallize the HZO film in the FE phase and to reduce the number of defects in the a‐IGZO channel. The structural and electrical characterizations provide comprehensive guidance for the design of effective FE‐TFT gate stacks and device geometries. An accurate control of the polarization state and linear switching between multiple intermediate states is shown by using programming pulses of various amplitudes and widths. Furthermore, a direct correlation between the channel length and the applied pulse width for programming is observed.
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