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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Berg, Fenja
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Topics
Publications (6/6 displayed)
- 2024Strain as a Global Factor in Stabilizing the Ferroelectric Properties of ZrO₂citations
- 2024Strain as a Global Factor in Stabilizing the Ferroelectric Properties of ZrO<sub>2</sub>citations
- 2023Strain as a global factor in stabilizing the ferroelectric properties of ZrO 2citations
- 2023Dual‐Mode Operation of Epitaxial Hf<sub>0.5</sub>Zr<sub>0.5</sub>O<sub>2</sub>: Ferroelectric and Filamentary‐Type Resistive Switchingcitations
- 2023Parameters for ferroelectric phase stabilization of sputtered undoped hafnium oxide thin filmscitations
- 2020Evolution of short-range order in chemically and physically grown thin film bilayer structures for electronic applicationscitations
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article
Dual‐Mode Operation of Epitaxial Hf<sub>0.5</sub>Zr<sub>0.5</sub>O<sub>2</sub>: Ferroelectric and Filamentary‐Type Resistive Switching
Abstract
<jats:p>Since the discovery of its ferroelectricity, hafnium oxide is widely used for applications in ferroelectric field‐effect transistors and ferroelectric tunnel junctions.is especially favored for its robust ferroelectricity and high remanent polarization at low thicknesses. In addition,is well established as amorphous or crystalline oxide layer in resistive switching devices. Herein, ferroelectric switching is found coexisting with high on/off ratio resistive switching in sub‐10 nm epitaxial . The resistive switching shows typical characteristics of a filamentary‐type valence change memory (VCM), clearly contradicting the polarization charges as the origin of different resistance states. In contrast to previous observations, no electroforming step is required to initiate VCM switching. Thebottom electrode enables a RESET to the virgin state, allowing subsequent ferroelectric hysteresis measurements. It is possible to change between both switching schemes repeatedly without impacting the ferroelectric performance. This indicates that ferroelectric switching and oxygen vacancy movement do not interfere with each other, and both switching phenomena can exist independently. This finding opens up ways to unite the different strengths of both switching mechanisms in the same stack. It becomes possible to assign the two operating principles to artificial neural network training and inference according to their respective advantages.</jats:p>