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Tunable Negative Differential Resistance Effect in a-SZTO/Dielectric/SZTO Heterostructure TFTs at Room Temperature Tunable Negative Differential Resistance Effect in a-SZTO/Dielectric/SZTO Heterostructure TFTs at Room Temperature AITranslate

Dongguk University-Seoul; Gachon University
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Publisher: ACS
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Abstract AITranslate

We experimentally demonstrate the resonant tunneling and negative differential resistance (NDR) in a-SZTO/dielectric/SZTO heterostructure thin film transistors (TFTs) at room temperature (RT) for the first time. Here, we study the resonant tunneling and the NDR tunability for different middle-layer dielectric and gate biases. The dielectric materials of HfO2, ZrO2, and MgO are used in the a-SZTO/dielectric/SZTO heterostructure devices and are named SHS, SZS, and SMS in this work. The resonant tunneling through an insulator occurs when the energy bands of the two amorphous-SiZnSnO (a-SZTO) are aligned. The previous results of NDR based on resonant tunneling were obtained only using two-dimensional (2D) materials. But we observe the NDR results with a peak-to-valley current ratio (PVCR) of 3 at RT by utilizing the bulk (three-dimensional, 3D) oxide materials for the first time in this work.

KeyWords AITranslate

negative differential resistance resonant tunneling heterostructure peaktovalley current ratio heterostructure TFT aSZTO
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Basic Information:

DOI:https://doi.org/10.1021/acsaelm.3c00178

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Citation Information:

We experimentally demonstrate the resonant tunneling and negative differential resistance (NDR) in a-SZTO/dielectric/SZTO heterostructure thin film transistors (TFTs) at room temperature (RT) for the first time. Here, we study the resonant tunneling and the NDR tunability for different middle-layer dielectric and gate biases. The dielectric materials of HfO2, ZrO2, and MgO are used in the a-SZTO/dielectric/SZTO heterostructure devices and are named SHS, SZS, and SMS in this work. The resonant tunneling through an insulator occurs when the energy bands of the two amorphous-SiZnSnO (a-SZTO) are aligned. The previous results of NDR based on resonant tunneling were obtained only using two-dimensional (2D) materials. But we observe the NDR results with a peak-to-valley current ratio (PVCR) of 3 at RT by utilizing the bulk (three-dimensional, 3D) oxide materials for the first time in this work.

quote

GB/T 7714-2015 [1] Balaji Murugan, Sang Yeol Lee. ACS Applied Electronic Materials, 2023(5). DOI:10.1021/acsaelm.3c00178.
MLA [1] Balaji Murugan, and Sang Yeol Lee. ACS Applied Electronic Materials, no. 5, 2023, https://doi.org/10.1021/acsaelm.3c00178.
APA [1] Balaji Murugan, & Sang Yeol Lee. (2023). ACS Applied Electronic Materials(5). https://doi.org/10.1021/acsaelm.3c00178
IEEE [1] Balaji Murugan and Sang Yeol Lee, ACS Applied Electronic Materials, no. 5, 2023, doi: 10.1021/acsaelm.3c00178. keywords: {negative differential resistance resonant tunneling heterostructure peaktovalley current ratio heterostructure TFT aSZTO}