Significant tunneling electroresistance and ultralow resistance-area product in asymmetric <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi mathvariant="normal">In</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:ms

Conventional ferroelectric tunnel junctions (FTJs) face inherent limitations in simultaneously achieving both a high tunneling electroresistance ratio (TER) and a low resistance-area product (RAP), hindering high-density, low-power, nonvolatile memory applications. This study overcomes this challenge by designing asymmetric FTJs based on a two-dimensional ${\mathrm{In}}_{2}{\mathrm{S}}_{3}/{\mathrm{Cu}}_{2}\mathrm{Se}$ heterostructure. Utilizing first-principles calculations with quantum transport simulations, we demonstrate that ferroelectric polarization switching in ${\mathrm{In}}_{2}{\mathrm{S}}_{3}$ reversibly modulates the heterostructure's band alignment between type-III (metallic) and type-II (semiconducting) states. Exploiting this, we engineered asymmetric ${\mathrm{In}}_{2}{\mathrm{S}}_{3}/{\mathrm{Cu}}_{2}({\mathrm{Se}}_{0.9}{\mathrm{S}}_{0.1})$ and ${\mathrm{In}}_{2}{\mathrm{S}}_{3}/{\mathrm{Cu}}_{2}({\mathrm{Se}}_{0.9}{\mathrm{Te}}_{0.1})$ electrodes flanking a central ${\mathrm{In}}_{2}{\mathrm{S}}_{3}/{\mathrm{Cu}}_{2}\mathrm{Se}$ barrier. The asymmetric FTJ achieves a TER of $9.95\ifmmode\times\else\texttimes\fi{}{10}^{8}%$, which is 5 orders of magnitude higher than that of symmetric FTJs ($1.28\ifmmode\times\else\texttimes\fi{}{10}^{3}%$), while maintaining an ultralow RAP of $0.11\phantom{\rule{0.16em}{0ex}}\mathrm{\ensuremath{\Omega}}\phantom{\rule{0.16em}{0ex}}\textmu{}{\mathrm{m}}^{2}$. Crucially, these optimal performance metrics (TER $\ensuremath{\sim}{10}^{9}%$, $\mathrm{RAP}&lt;0.2\phantom{\rule{0.16em}{0ex}}\mathrm{\ensuremath{\Omega}}\phantom{\rule{0.16em}{0ex}}\textmu{}{\mathrm{m}}^{2}$) persist robustly even under variations in channel width ($N=1$ to $N=9$, $\ensuremath{\sim}0.7--6.3\phantom{\rule{0.16em}{0ex}}\mathrm{nm}$) or electrode doping concentration (5%--15%). These findings highlight the superior performance and exceptional robustness of the asymmetric ${\mathrm{In}}_{2}{\mathrm{S}}_{3}/{\mathrm{Cu}}_{2}\mathrm{Se}$-based FTJ, which holds significant promise for high-density, low-power, nonvolatile memory applications.

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Journal
Physical review. B./Physical review. B
Published
2025-11-19
DOI
https://doi.org/10.1103/6f3j-6zbm
Primary Topic
2D Materials and Applications
Type
article
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article

Significant tunneling electroresistance and ultralow resistance-area product in asymmetric <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi mathvariant="normal">In</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:ms

Karl J. Friston
Physical review. B./Physical review. B
2D Materials and Applications
article

Significant tunneling electroresistance and ultralow resistance-area product in asymmetric <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:msub> <mml:mi mathvariant="normal">In</mml:mi> <mml:mn>2</mml:mn> </mml:msub> <mml:ms

Karl J. Friston
article en

Abstract

Conventional ferroelectric tunnel junctions (FTJs) face inherent limitations in simultaneously achieving both a high tunneling electroresistance ratio (TER) and a low resistance-area product (RAP), hindering high-density, low-power, nonvolatile memory applications. This study overcomes this challenge by designing asymmetric FTJs based on a two-dimensional ${\mathrm{In}}_{2}{\mathrm{S}}_{3}/{\mathrm{Cu}}_{2}\mathrm{Se}$ heterostructure. Utilizing first-principles calculations with quantum transport simulations, we demonstrate that ferroelectric polarization switching in ${\mathrm{In}}_{2}{\mathrm{S}}_{3}$ reversibly modulates the heterostructure's band alignment between type-III (metallic) and type-II (semiconducting) states. Exploiting this, we engineered asymmetric ${\mathrm{In}}_{2}{\mathrm{S}}_{3}/{\mathrm{Cu}}_{2}({\mathrm{Se}}_{0.9}{\mathrm{S}}_{0.1})$ and ${\mathrm{In}}_{2}{\mathrm{S}}_{3}/{\mathrm{Cu}}_{2}({\mathrm{Se}}_{0.9}{\mathrm{Te}}_{0.1})$ electrodes flanking a central ${\mathrm{In}}_{2}{\mathrm{S}}_{3}/{\mathrm{Cu}}_{2}\mathrm{Se}$ barrier. The asymmetric FTJ achieves a TER of $9.95\ifmmode\times\else\texttimes\fi{}{10}^{8}%$, which is 5 orders of magnitude higher than that of symmetric FTJs ($1.28\ifmmode\times\else\texttimes\fi{}{10}^{3}%$), while maintaining an ultralow RAP of $0.11\phantom{\rule{0.16em}{0ex}}\mathrm{\ensuremath{\Omega}}\phantom{\rule{0.16em}{0ex}}\textmu{}{\mathrm{m}}^{2}$. Crucially, these optimal performance metrics (TER $\ensuremath{\sim}{10}^{9}%$, $\mathrm{RAP}&lt;0.2\phantom{\rule{0.16em}{0ex}}\mathrm{\ensuremath{\Omega}}\phantom{\rule{0.16em}{0ex}}\textmu{}{\mathrm{m}}^{2}$) persist robustly even under variations in channel width ($N=1$ to $N=9$, $\ensuremath{\sim}0.7--6.3\phantom{\rule{0.16em}{0ex}}\mathrm{nm}$) or electrode doping concentration (5%--15%). These findings highlight the superior performance and exceptional robustness of the asymmetric ${\mathrm{In}}_{2}{\mathrm{S}}_{3}/{\mathrm{Cu}}_{2}\mathrm{Se}$-based FTJ, which holds significant promise for high-density, low-power, nonvolatile memory applications.

Physical review. B./Physical review. BVol. 112(24)
Kunming University of Science and Technology (CN)
Openalex Percentile: Top 67%
2D Materials and Applications
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