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Ferroelectric-Antiferroelectric Transition of Hf(1–x)Zr(x)O(2) on Indium Arsenide with Enhanced Ferroelectric Characteristics for Hf(0.2)Zr(0.8)O(2)

[Image: see text] The ferroelectric (FE)–antiferroelectric (AFE) transition in Hf(1–x)Zr(x)O(2) (HZO) is for the first time shown in a metal–ferroelectric–semiconductor (MFS) stack based on the III-V material InAs. As InAs displays excellent electron mobility and a narrow band gap, the integration o...

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Detalles Bibliográficos
Autores principales: Dahlberg, Hannes, Persson, Anton E. O., Athle, Robin, Wernersson, Lars-Erik
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2022
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9798826/
https://www.ncbi.nlm.nih.gov/pubmed/36588621
http://dx.doi.org/10.1021/acsaelm.2c01483
Descripción
Sumario:[Image: see text] The ferroelectric (FE)–antiferroelectric (AFE) transition in Hf(1–x)Zr(x)O(2) (HZO) is for the first time shown in a metal–ferroelectric–semiconductor (MFS) stack based on the III-V material InAs. As InAs displays excellent electron mobility and a narrow band gap, the integration of ferroelectric thin films for nonvolatile operations is highly relevant for future electronic devices and motivates further research on ferroelectric integration. When increasing the Zr fraction x from 0.5 to 1, the stack permittivity increases as expected, and the transition from FE to AFE-like behavior is observed by polarization and current–voltage characteristics. At x = 0.8 the polarization of the InAs-based stacks shows a larger FE-contribution as a more open hysteresis compared to both literature and reference metal–ferroelectric–metal (MFM) devices. By field-cycling the devices, the switching domains are studied as a function of the cycle number, showing that the difference in FE–AFE contributions for MFM and MFS devices is stable over switching and not an effect of wake-up. The FE contribution of the switching can be accessed by successively lowering the bias voltage in a proposed pulse train. The possibility of enhanced nonvolatility in Zr-rich HZO is relevant for device stacks that would benefit from an increase in permittivity and a lower operating voltage. Additionally, an interfacial layer (IL) is introduced between the HZO film and the InAs substrate. The interfacial quality is investigated as frequency-dependent capacitive dispersion, showing little change for varying ZrO(2) concentrations and with or without included IL. This suggests material processing that is independently limiting the interfacial quality. Improved endurance of the InAs-Hf(1–x)Zr(x)O(2) devices with x = 0.8 was also observed compared to x = 0.5, with further improvement with the additional IL for Zr-rich HZO on InAs.