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- W4385192287 abstract "HZO/ZrO <inf xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>2</inf> (HZZ) nanolaminates have attracted attention as a promising strategy for obtaining ultra-low equivalent oxide thickness (EOT) [1]. HZZ nanolaminates have a structure of alternate thin layers of HZO and ZrO <inf xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>2</inf> with o- (ferroelectric or FE) and t-phase (anti-FE or AFE), respectively (Fig. 1a) [2]. HZZ displays an intermediate polarization-voltage (P-V) characteristic of FE and AFE, referred to as a broken loop. Atomic-scale sub-lattice model of HZO attributes this effect to morphotropic phase boundary (MPB) formation (Fig. 1b) [3]. However, the device-scale model with multi-phase co-existence is yet to be explored. In this work, we propose a phase-field model based on sub-lattices to explain the unique characteristics of HZZ nanolaminates. We investigate the underlying polarization switching mechanisms for HZZ and compare them to those in HZO and ZrO <inf xmlns:mml=http://www.w3.org/1998/Math/MathML xmlns:xlink=http://www.w3.org/1999/xlink>2</inf> ." @default.
- W4385192287 created "2023-07-25" @default.
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- W4385192287 date "2023-06-25" @default.
- W4385192287 modified "2023-09-23" @default.
- W4385192287 title "Analysis of Polarization Switching in HZO/ZrO<sub>2</sub> (HZZ) Nanolaminates based on Sub-lattice Phase-field Model" @default.
- W4385192287 doi "https://doi.org/10.1109/drc58590.2023.10186928" @default.
- W4385192287 hasPublicationYear "2023" @default.
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