First Demonstration of Annealing-Free RT-Prepared AlScN Film with Large Polarization ($2 \mathrm{P}_{\mathrm{r}}>300 \mu \mathrm{C} / \text{cm}^{2}$) and Ultra-Sharp $\mathrm{E}_{\mathrm{c}}$ Distribution for 0T1C FeRAM

Selector-free 0T1C FeRAM requires ferroelectric (FE) films with high polarization (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$2 P_{\mathrm{r}}$</tex>) and sharp coercive field (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$E_{\mathrm{c}}$</tex>) distribution. In this work, we present the first demonstration of a 1kb 0T1C FeRAM based on the optimized AlScN FE film, through electrode engineering and interface optimization. An annealing-free room-temperature (RT)-prepared AlScN epitaxial film with high-quality (001) orientation is achieved, resulting in a large <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$2 P_{\mathrm{r}}&gt;300 \mu \mathrm{C} / \text{cm}^{2}$</tex> and an ultra-sharp <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$E_{\mathrm{c}}$</tex> distribution (record <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\alpha$</tex> of 0.045). The sharp <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$E_{\mathrm{c}}$</tex> allows superior disturb immunity under the <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{V}_{\text{dd}} / 2$</tex> read scheme for array operations, even at an elevated 300°C. Furthermore, our circuit model proposes that the optimized AlScN FE film can support much larger array size compared to other ferroelectrics, thanks to its enhanced <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$2 P_{\mathrm{r}}$</tex> and sharper <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$E_{\mathrm{c}}$</tex> distribution. This work underscores the great potential of AlScN-based FE films for high-capacity emerging memory technologies.

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Published
2025-06-08
DOI
https://doi.org/10.23919/vlsitechnologyandcir65189.2025.11074960
Primary Topic
Metal and Thin Film Mechanics
Type
article
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article

First Demonstration of Annealing-Free RT-Prepared AlScN Film with Large Polarization ($2 \mathrm{P}_{\mathrm{r}}>300 \mu \mathrm{C} / \text{cm}^{2}$) and Ultra-Sharp $\mathrm{E}_{\mathrm{c}}$ Distribution for 0T1C FeRAM

Hao Jiang, Xuanyu Zhao, Yingfen Wei, Jie Yu et al.
Metal and Thin Film Mechanics
article

First Demonstration of Annealing-Free RT-Prepared AlScN Film with Large Polarization ($2 \mathrm{P}_{\mathrm{r}}>300 \mu \mathrm{C} / \text{cm}^{2}$) and Ultra-Sharp $\mathrm{E}_{\mathrm{c}}$ Distribution for 0T1C FeRAM

Hao Jiang, Xuanyu Zhao, Yingfen Wei, Jie Yu, Yan Cheng, Yu Li, Ming Liu, Yiwei Wang, Qi Liu, Fuyang Cao
article en

Abstract

Selector-free 0T1C FeRAM requires ferroelectric (FE) films with high polarization (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$2 P_{\mathrm{r}}$</tex>) and sharp coercive field (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$E_{\mathrm{c}}$</tex>) distribution. In this work, we present the first demonstration of a 1kb 0T1C FeRAM based on the optimized AlScN FE film, through electrode engineering and interface optimization. An annealing-free room-temperature (RT)-prepared AlScN epitaxial film with high-quality (001) orientation is achieved, resulting in a large <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$2 P_{\mathrm{r}}&gt;300 \mu \mathrm{C} / \text{cm}^{2}$</tex> and an ultra-sharp <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$E_{\mathrm{c}}$</tex> distribution (record <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\alpha$</tex> of 0.045). The sharp <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$E_{\mathrm{c}}$</tex> allows superior disturb immunity under the <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\mathrm{V}_{\text{dd}} / 2$</tex> read scheme for array operations, even at an elevated 300°C. Furthermore, our circuit model proposes that the optimized AlScN FE film can support much larger array size compared to other ferroelectrics, thanks to its enhanced <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$2 P_{\mathrm{r}}$</tex> and sharper <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$E_{\mathrm{c}}$</tex> distribution. This work underscores the great potential of AlScN-based FE films for high-capacity emerging memory technologies.

Fudan University (CN), East China Normal University (CN)
National Natural Science Foundation of China, National Key Research and Development Program of China
Openalex Percentile: Top 78%
Metal and Thin Film Mechanics
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