Threshold Voltage Control in High-Mobility Oxide Thin-Film Transistors Through Thermal Annealing

Thin-film transistors (TFTs) in display circuits require a small and stable threshold voltage (<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub><roman xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">)</roman> for fewer compensation circuits and lower power consumption. Tuning the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> of the oxide TFTs is crucial to match the ideal conditions for display circuits. High-mobility oxide TFTs suffer from negative <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub>. Herein, we studied the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> control in high-mobility amorphous InSnZnO (ITZO)-based TFTs by using temperature-dependent electrical characterization and achieved a small <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> by optimizing annealing process. Consequently, both the postdeposition annealing (PDA) and postmetallization annealing (PMA) led to a similar trend of <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> shifting. The optimized PMA TFT exhibits excellent electrical properties with a <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> of 0.73 ± 0.33 V, a saturation mobility of 32.55 ± 2.05 cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>2</roman></sup>V<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-<roman>1</roman></sup>s<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-<roman>1</roman></sup>, a large on/off current ratio of more than 10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>8</roman></sup>, and a low subthreshold swing (SS) of 0.27 ± 0.02 V/decade, which enables the device can be applied in ultrahigh-definition displays. The resulting good performance of the optimized TFT originates from the modulation of oxygen defects. The <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> shift under gate bias stress is around ±10 V and the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> shows a recovery after the stress is removed. The <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> shift and recovery are attributed to the charge trapping and detrapping, respectively. This work offers a promising high-performance oxide TFT with a small <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> for next-generation electronics.

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Publication Details

Journal
IEEE Transactions on Electron Devices
Published
2025-09-05
DOI
https://doi.org/10.1109/ted.2025.3604779
Citations
4
Primary Topic
Thin-Film Transistor Technologies
Type
article
Field-Weighted Citation Impact
2.92

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article

Threshold Voltage Control in High-Mobility Oxide Thin-Film Transistors Through Thermal Annealing

Yaobin Ma, Jiangmei Su, Xijiao Mu, Wenyue Tan et al.
4 citations
IEEE Transactions on Electron Devices
Thin-Film Transistor Technologies
2.92
article

Threshold Voltage Control in High-Mobility Oxide Thin-Film Transistors Through Thermal Annealing

Yaobin Ma, Jiangmei Su, Xijiao Mu, Wenyue Tan, Xiehong Cao, Xiaodong Yan, Yiyang Xie, Yihong Liu
article en
4 citations

Abstract

Thin-film transistors (TFTs) in display circuits require a small and stable threshold voltage (<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub><roman xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">)</roman> for fewer compensation circuits and lower power consumption. Tuning the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> of the oxide TFTs is crucial to match the ideal conditions for display circuits. High-mobility oxide TFTs suffer from negative <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub>. Herein, we studied the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> control in high-mobility amorphous InSnZnO (ITZO)-based TFTs by using temperature-dependent electrical characterization and achieved a small <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> by optimizing annealing process. Consequently, both the postdeposition annealing (PDA) and postmetallization annealing (PMA) led to a similar trend of <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> shifting. The optimized PMA TFT exhibits excellent electrical properties with a <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> of 0.73 ± 0.33 V, a saturation mobility of 32.55 ± 2.05 cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>2</roman></sup>V<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-<roman>1</roman></sup>s<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-<roman>1</roman></sup>, a large on/off current ratio of more than 10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>8</roman></sup>, and a low subthreshold swing (SS) of 0.27 ± 0.02 V/decade, which enables the device can be applied in ultrahigh-definition displays. The resulting good performance of the optimized TFT originates from the modulation of oxygen defects. The <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> shift under gate bias stress is around ±10 V and the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> shows a recovery after the stress is removed. The <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> shift and recovery are attributed to the charge trapping and detrapping, respectively. This work offers a promising high-performance oxide TFT with a small <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">V</i><sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"><roman>TH</roman></sub> for next-generation electronics.

IEEE Transactions on Electron DevicesVol. 72(11)
Beijing University of Technology (CN), China Electronic Information Industry Development (CN)
Beijing Postdoctoral Science Foundation
Openalex Percentile: Top 8%
Thin-Film Transistor Technologies
2.92
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