| People | Locations | Statistics |
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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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Deleruyelle, Damien
Institut National des Sciences Appliquées de Lyon
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (26/26 displayed)
- 2024Development of ferroelectric and antiferroelectric H1-xZrxO2-based capacitors for non-volatile memories and power supply applications
- 2024Serendipity in materials science: how a simple doping leads to novel and outstanding properties in simple dielectric HfO2 !
- 2024Stabilization of low dimensional ferroelectric HfZrO2 film
- 2023How ALD deposition analysis can help PVD deposition process!
- 2023How ALD deposition analysis can help PVD deposition process!
- 2023Engineering the nano and micro structures of sputtered HfZrO2 thin films
- 2023Engineering the nano and micro structures of sputtered HfZrO2 thin films
- 2023Interplay between Strain and Defects at the Interfaces of Ultra‐Thin Hf 0.5 Zr 0.5 O 2 ‐Based Ferroelectric Capacitorscitations
- 2023Interplay between Strain and Defects at the Interfaces of Ultra‐Thin Hf 0.5 Zr 0.5 O 2 ‐Based Ferroelectric Capacitorscitations
- 2023Interface engineering between HfZrO2 thin films and electrodes for enhanced ferroelectricity
- 2023Interface engineering between HfZrO2 thin films and electrodes for enhanced ferroelectricity
- 2022Fabrication process for sub-8 nm HfZrO2-based ferroelectric tunnel junctions with enhanced properties
- 2022Ferroelectricity Improvement in Ultra-Thin Hf0.5Zr0.5O2 Capacitors by the Insertion of a Ti Interfacial Layercitations
- 2022Ferroelectricity Improvement in Ultra-Thin Hf0.5Zr0.5O2 Capacitors by the Insertion of a Ti Interfacial Layercitations
- 2022A multiscale study of the structure, chemistry and ferroelectric properties of epitaxial sol-gel PbZr0.2Ti0.8O3 films for nanomechanical switching
- 2022A multiscale study of the structure, chemistry and ferroelectric properties of epitaxial sol-gel PbZr0.2Ti0.8O3 films for nanomechanical switching
- 2022How to play on the fabrication process of HfZrO2 ferroelectric thin film to enhance its physical properties
- 2021Electrical Characterisation of HfZrO2 Ferroelectric Tunnel Junctions for Neuromorphic Application
- 2021Bottom electrodes impact on Hf0.5Zr0.5O2 ferroelectric tunnel junctions
- 2021Bottom electrodes impact on Hf0.5Zr0.5O2 ferroelectric tunnel junctions
- 2021Effect of bottom electrodes on HZO thin film properties
- 2021Impact of a dielectric layer at TiN/HfZrO2 interface for ferroelectric tunnel junctions applications
- 2021Impact of a dielectric layer at TiN/HfZrO2 interface for ferroelectric tunnel junctions applications
- 2021Role of ultra-thin Ti and Al interfacial layers in HfZrO2 ferroelectric tunnel junctions
- 2021Role of ultra-thin Ti and Al interfacial layers in HfZrO2 ferroelectric tunnel junctions
- 2014Photo-Cross-Linked Diblock Copolymer Micelles: Quantitative Study of Photochemical Efficiency, Micelles Morphologies and their Thermal Behaviorcitations
Places of action
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document
Engineering the nano and micro structures of sputtered HfZrO2 thin films
Abstract
We focus on (Hf,Zr)O2 thin films deposition for the capacitor of FRAM in the 1T-1C. (Hf,Zr)O2 thin films are studied to either fully understand the stabilization of the ferroelectric phase or to fit with industrial requirements. Changing the pressure in our sputtering chamber during the room temperature deposition lead to the deposition of crystalline or amorphous films. After a Rapid Thermal Annealing, only the amorphous films crystallize in the ferro-phase [1]. Samples are stacks of Si/TiN/Hf0.5Zr0.5O/TiN/Pt. The samples are called NM, and M: NM and M refers to two different architectures, respectively non-mesa and mesa structures [2]. The set-up for electrical measurements have been described in reference [3]. We report the fabrication of two samples deposited by magnetron sputtering with excellent performances, quite similar to samples deposited by ALD. Pr values are among the highest for samples deposited by sputtering. Although the N-sample and NM-samples show very close Pr values, the two samples show completely different electrical behaviors. During cycling, the increase of Pr value for the NM-sample is more than an order of magnitude higher than the M-sample. It is accompanied by a decrease of the endurance which is two order of magnitude higher for the NM-sample than for the M-sample. The origins of the different electrical behaviors come from the micro-crystalline structures of the two samples, according to GIXRD results. The crystallization takes place during the annealing step. It induces different stress states which lead to two different micro-crystalline patterning. The M-sample shows no monoclinic peak, whereas the NM-sample shows many monoclinic orientations. It can explain the huge reduction of the wake-up effect.[1] J. Bouaziz et al. JVST B 37, 021203 (2019).[2] J. Bouaziz et al. ACS Appl. Electron. Mater. 1, 1740 (2019).[3] J. Bouaziz et al. APL Mater. 7, 081109 (2019).