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Dual Ferroelectric Stack of HfZrO₂/Al:HfO₂ With Tunable Coercive Voltage for High-Density Memory Applications

To achieve a multilevel threshold voltage in the configuration of a ferroelectric field-effect transistor for high-density memories, it is crucial to achieve a finely tunable coercive voltage ( {V}_{\text {C}}{)} of the ferroelectric layer (FL). In this study, we demonstrate that the use of dual fe...

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Published in:IEEE transactions on electron devices 2024-06, Vol.71 (6), p.3981-3984
Main Authors: Jeong, Jiae, Park, Hyoungjin, Kim, Nayeon, Kim, Hyun Wook, Hong, Eunryeong, Choi, Hyeonsik, Jeon, Seonuk, Kim, Yunsur, Woo, Jiyong
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container_title IEEE transactions on electron devices
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creator Jeong, Jiae
Park, Hyoungjin
Kim, Nayeon
Kim, Hyun Wook
Hong, Eunryeong
Choi, Hyeonsik
Jeon, Seonuk
Kim, Yunsur
Woo, Jiyong
description To achieve a multilevel threshold voltage in the configuration of a ferroelectric field-effect transistor for high-density memories, it is crucial to achieve a finely tunable coercive voltage ( {V}_{\text {C}}{)} of the ferroelectric layer (FL). In this study, we demonstrate that the use of dual ferroelectric stacks with Zr-doped HfO2 (HZO) and Al-doped HfO2 (HAO) allows the adjustment of {V}_{\text {C}} and remnant polarization ( {P}_{r}{)} over a broad range relative to the ramping voltage. When a single HZO FL is used, a rapid increase in {P}_{r} is observed, reaching approximately 30~\mu \text{C} /cm2 at a specific {V}_{\text {C}} value. In contrast, the HAO FL progresses at a slower rate, achieving a smaller {P}_{r} value approximately equal to 7~\mu \text{C} /cm2 with increasing voltage. In the dual-stack configuration, polarization occurs sequentially through each FL, enabling the incremental adjustment of {V}_{\text {C}} . The stress primarily arises after the deposition of the top electrode during annealing, thus emphasizing the crucial role of the upper FL in the ferroelectric properties of the dual stack. Furthermore, our findings reveal that substituting a dielectric layer (DL)for the HAO FL, rather than the HZO FL, exacerbates polarization, revealing that the synergistic effect originates from two different FLs.
doi_str_mv 10.1109/TED.2024.3387884
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In this study, we demonstrate that the use of dual ferroelectric stacks with Zr-doped HfO2 (HZO) and Al-doped HfO2 (HAO) allows the adjustment of <inline-formula> <tex-math notation="LaTeX">{V}_{\text {C}} </tex-math></inline-formula> and remnant polarization (<inline-formula> <tex-math notation="LaTeX">{P}_{r}{)} </tex-math></inline-formula> over a broad range relative to the ramping voltage. When a single HZO FL is used, a rapid increase in <inline-formula> <tex-math notation="LaTeX">{P}_{r} </tex-math></inline-formula> is observed, reaching approximately <inline-formula> <tex-math notation="LaTeX">30~\mu \text{C} </tex-math></inline-formula>/cm2 at a specific <inline-formula> <tex-math notation="LaTeX">{V}_{\text {C}} </tex-math></inline-formula> value. 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In this study, we demonstrate that the use of dual ferroelectric stacks with Zr-doped HfO2 (HZO) and Al-doped HfO2 (HAO) allows the adjustment of <inline-formula> <tex-math notation="LaTeX">{V}_{\text {C}} </tex-math></inline-formula> and remnant polarization (<inline-formula> <tex-math notation="LaTeX">{P}_{r}{)} </tex-math></inline-formula> over a broad range relative to the ramping voltage. When a single HZO FL is used, a rapid increase in <inline-formula> <tex-math notation="LaTeX">{P}_{r} </tex-math></inline-formula> is observed, reaching approximately <inline-formula> <tex-math notation="LaTeX">30~\mu \text{C} </tex-math></inline-formula>/cm2 at a specific <inline-formula> <tex-math notation="LaTeX">{V}_{\text {C}} </tex-math></inline-formula> value. 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In this study, we demonstrate that the use of dual ferroelectric stacks with Zr-doped HfO2 (HZO) and Al-doped HfO2 (HAO) allows the adjustment of <inline-formula> <tex-math notation="LaTeX">{V}_{\text {C}} </tex-math></inline-formula> and remnant polarization (<inline-formula> <tex-math notation="LaTeX">{P}_{r}{)} </tex-math></inline-formula> over a broad range relative to the ramping voltage. When a single HZO FL is used, a rapid increase in <inline-formula> <tex-math notation="LaTeX">{P}_{r} </tex-math></inline-formula> is observed, reaching approximately <inline-formula> <tex-math notation="LaTeX">30~\mu \text{C} </tex-math></inline-formula>/cm2 at a specific <inline-formula> <tex-math notation="LaTeX">{V}_{\text {C}} </tex-math></inline-formula> value. In contrast, the HAO FL progresses at a slower rate, achieving a smaller <inline-formula> <tex-math notation="LaTeX">{P}_{r} </tex-math></inline-formula> value approximately equal to <inline-formula> <tex-math notation="LaTeX">7~\mu \text{C} </tex-math></inline-formula>/cm2 with increasing voltage. In the dual-stack configuration, polarization occurs sequentially through each FL, enabling the incremental adjustment of <inline-formula> <tex-math notation="LaTeX">{V}_{\text {C}} </tex-math></inline-formula>. The stress primarily arises after the deposition of the top electrode during annealing, thus emphasizing the crucial role of the upper FL in the ferroelectric properties of the dual stack. Furthermore, our findings reveal that substituting a dielectric layer (DL)for the HAO FL, rather than the HZO FL, exacerbates polarization, revealing that the synergistic effect originates from two different FLs.]]></abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TED.2024.3387884</doi><tpages>4</tpages><orcidid>https://orcid.org/0000-0002-4968-6985</orcidid><orcidid>https://orcid.org/0000-0001-9101-1028</orcidid><orcidid>https://orcid.org/0000-0001-6012-3502</orcidid><orcidid>https://orcid.org/0000-0003-4129-4853</orcidid><orcidid>https://orcid.org/0009-0004-9676-9355</orcidid><orcidid>https://orcid.org/0000-0003-3194-9481</orcidid></addata></record>
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source IEEE Electronic Library (IEL) Journals
subjects Al:HFO
Annealing
Coercivity
Configurations
Dielectrics
dual ferroelectric stack
Electrodes
FeFETs
Ferroelectric materials
ferroelectric memory
Ferroelectricity
Field effect transistors
Hafnium oxide
HfZrO
High density
Polarization
Semiconductor devices
Stress
Synergistic effect
Temperature measurement
Threshold voltage
Zirconium
title Dual Ferroelectric Stack of HfZrO₂/Al:HfO₂ With Tunable Coercive Voltage for High-Density Memory Applications
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