Ferroelectricity and negative piezoelectric coefficient in orthorhombic phase pure ZrO2 thin films
Электронный научный архив УРФУ
Информация об архиве | Просмотр оригинала| Поле | Значение | |
| Заглавие |
Ferroelectricity and negative piezoelectric coefficient in orthorhombic phase pure ZrO2 thin films
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| Автор |
Silva, J. P. B.
Istrate, M. C. Hellenbrand, M. Jan, A. Becker, M. T. Symonowicz, J. Figueiras, F. G. Lenzi, V. Hill, M. O. Ghica, C. Romanyuk, K. N. Gomes, M. J. M. Martino, G. D. Marques, L. MacManus-Driscoll, J. L. |
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| Тематика |
FERROELECTRICITY
ION-BEAM SPUTTERING ORTHORHOMBIC PHASE ZRO2 FILMS PIEZOELECTRICITY CRYSTALLOGRAPHY DENSITY FUNCTIONAL THEORY FERROELECTRIC FILMS FERROELECTRICITY HIGH RESOLUTION TRANSMISSION ELECTRON MICROSCOPY ION BEAMS POLARIZATION SCANNING ELECTRON MICROSCOPY SCANNING PROBE MICROSCOPY SPUTTERING STRONTIUM TITANATES THICK FILMS THIN FILMS TITANIUM COMPOUNDS ZIRCONIA ION-BEAM-SPUTTERING NEW APPROACHES O PHASE ORTHORHOMBIC PHASE ORTHORHOMBIC PHASE ZRO2 FILM PHASE PURE PIEZOELECTRIC COEFFICIENT REMNANT POLARIZATIONS THIN-FILMS ZRO 2 FILMS PIEZOELECTRICITY |
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| Описание |
A new approach for epitaxial stabilisation of ferroelectric orthorhombic (o-) ZrO2 films with negative piezoelectric coefficient in ∼ 8nm thick films grown by ion-beam sputtering is demonstrated. Films on (011)-Nb:SrTiO3 gave the oriented o-phase, as confirmed by transmission electron microscopy and electron backscatter diffraction mapping, grazing incidence x-ray diffraction and Raman spectroscopy. Scanning probe microscopy techniques and macroscopic polarization-electric field hysteresis loops show ferroelectric behavior, with saturation polarization of ∼14.3 µC/cm2, remnant polarization of ∼9.3 µC/cm2 and coercive field ∼1.2 MV/cm. In contrast to the o-films grown on (011)-Nb:SrTiO3, films grown on (001)-Nb:SrTiO3 showed mixed monoclinic (m-) and o-phases causing an inferior remnant polarization of ∼4.8 µC/cm2, over 50% lower than the one observed for the film grown on (011)-Nb:SrTiO3. Density functional theory (DFT) calculations of the SrTiO3/ZrO2 interfaces support the experimental findings of a stable polar o-phase for growth on (011) Nb:SrTiO3, and they also explain the negative piezoelectric coefficient. © 2022 The Author(s)
Corporation for National and Community Service, CNCS; Engineering and Physical Sciences Research Council, EPSRC: 882929, EP/T012218/1; Royal Academy of Engineering, RAENG: CIET1819_24; Fundação para a Ciência e a Tecnologia, FCT: ALT20-03-0246-FEDER-000033, CPCA/A2/4628/2020, CPCA/A2/5649/2020, NECL - NORTE-01-0145-FEDER-022096, POCI-01-0145-FEDER-022217, UID/NAN/50024/2019, UIDB/04650/2020; Isaac Newton Trust: G112877; Unitatea Executiva pentru Finantarea Invatamantului Superior, a Cercetarii, Dezvoltarii si Inovarii, UEFISCDI: 20192055, COFUND-M-ERANET-3-NanOx4Estor, POC 332/390008/29.12.2020-SMIS 109522; Horizon 2020: 958174, M-ERA-NET3/0003/2021 - NanOx4EStor, UIDB/50011/2020; Colegiul Consultativ pentru Cercetare-Dezvoltare şi Inovare, CCCDI; Institute of Information Science, Academia Sinica, IIS This work was supported by: (i) the Portuguese Foundation for Science and Technology (FCT) in the framework of the Strategic Funding Contract UIDB/04650/2020 and (ii) Project NECL - NORTE-01-0145-FEDER-022096 and Project UID/NAN/50024/2019. This work has received funding from the European Union's Horizon 2020 research and innovation programme under grant agreement No 958174 (M-ERA-NET3/0003/2021 - NanOx4EStor). This work was also developed within the scope of the project CICECO-Aveiro Institute of Materials, UIDB/50011/2020 & UIDP/50011/2020, financed by national funds through the Portuguese Foundation for Science and Technology/MCTES. It is also funded by national funds (OE), through FCT – Fundação para a Ciência e a Tecnologia, I.P., in the scope of the framework contract foreseen in the numbers 4, 5 and 6 of the article 23, of the Decree-Law 57/2016, of August 29, changed by Law 57/2017, of July 19. M. C. I. and C. G. acknowledge the financial support by a grant of the Ministry of Research, Innovation and Digitization, CNCS/CCCDI - UEFISCDI, project number COFUND-M-ERANET-3-NanOx4Estor, within PNCDI III and POC 332/390008/29.12.2020-SMIS 109522. The authors acknowledge the CERIC-ERIC Consortium for access to experimental facilities and financial support under proposal 20192055. The authors would also like to thank José Santos (Thin Film Laboratory at CF-UM-UP) and Ming Xiao (Dept. of Materials Science and Metallurgy) for technical support. J.L.M.D. thanks the Royal Academy of Engineering - CIET1819_24 for support. M.H. and J.L.M.D. thank the EPSRC (EP/T012218/1) grant for support. J.L.M.D and M.T.B. also thank EU-H2020-ERC-ADG # 882929 EROS for support. M.O.H. acknowledges support from the Herchel Smith foundation in Cambridge. G.D. acknowledges support from the Winton Programme for the Physics of Sustainability and the Isaac Newton Trust (Grant number G112877 ). This work was supported by: (i) the Portuguese Foundation for Science and Technology (FCT) in the framework of the Strategic Funding Contract UIDB/04650/2020 and (ii) Project NECL - NORTE-01-0145-FEDER-022096 and Project UID/NAN/50024/2019. This work has received funding from the European Union's Horizon 2020 research and innovation programme under grant agreement No 958174 (M-ERA-NET3/0003/2021 - NanOx4EStor). This work was also developed within the scope of the project CICECO-Aveiro Institute of Materials, UIDB/50011/2020 & UIDP/50011/2020, financed by national funds through the Portuguese Foundation for Science and Technology/MCTES. It is also funded by national funds (OE), through FCT – Fundação para a Ciência e a Tecnologia, I.P. in the scope of the framework contract foreseen in the numbers 4, 5 and 6 of the article 23, of the Decree-Law 57/2016, of August 29, changed by Law 57/2017, of July 19. The calculations were carried out at the OBLIVION Supercomputer (based at the High Performance Computing Center - University of Évora) funded by the ENGAGE SKA Research Infrastructure (reference POCI-01-0145-FEDER-022217 - COMPETE 2020 and the Foundation for Science and Technology, Portugal) and by the BigData@UE project (reference ALT20-03-0246-FEDER-000033 - FEDER and the Alentejo 2020 Regional Operational Program). Oblivion resources were accessed through the advanced computing projects CPCA/A2/5649/2020 and CPCA/A2/4628/2020, funded by FCT I.P. The authors gratefully acknowledge the HPC RIVR consortium (www.hpc-rivr.si) and EuroHPC JU (eurohpc-ju.europa.eu) for funding this research by providing computing resources of the HPC system Vega at the Institute of Information Science (www.izum.si), M. C. I. and C. G. acknowledge the financial support by a grant of the Ministry of Research, Innovation and Digitization, CNCS/CCCDI - UEFISCDI, project number COFUND-M-ERANET-3-NanOx4Estor, within PNCDI III and POC 332/390008/29.12.2020-SMIS 109522. The authors acknowledge the CERIC-ERIC Consortium for access to experimental facilities and financial support under proposal 20192055. The authors would also like to thank José Santos (Thin Film Laboratory at CF-UM-UP) and Ming Xiao (Dept. of Materials Science and Metallurgy) for technical support. J.L.M.D. thanks the Royal Academy of Engineering - CIET1819_24 for support. M.H. and J.L.M.D. thank the EPSRC (EP/T012218/1) grant for support. J.L.M.D and M.T.B. also thank EU-H2020-ERC-ADG # 882929 EROS for support. M.O.H. acknowledges support from the Herchel Smith foundation in Cambridge. G.D. acknowledges support from the Winton Programme for the Physics of Sustainability and the Isaac Newton Trust (Grant number G112877). The calculations were carried out at the OBLIVION Supercomputer (based at the High Performance Computing Center - University of Évora) funded by the ENGAGE SKA Research Infrastructure (reference POCI-01-0145-FEDER-022217 - COMPETE 2020 and the Foundation for Science and Technology, Portugal) and by the BigData@UE project (reference ALT20-03-0246-FEDER-000033 - FEDER and the Alentejo 2020 Regional Operational Program). Oblivion resources were accessed through the advanced computing projects CPCA/A2/5649/2020 and CPCA/A2/4628/2020, funded by FCT I.P. The authors gratefully acknowledge the HPC RIVR consortium ( www.hpc-rivr.si ) and EuroHPC JU (eurohpc-ju.europa.eu) for funding this research by providing computing resources of the HPC system Vega at the Institute of Information Science ( www.izum.si ) |
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| Дата |
2024-04-05T16:19:01Z
2024-04-05T16:19:01Z 2023 |
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| Тип |
Article
Journal article (info:eu-repo/semantics/article) |info:eu-repo/semantics/publishedVersion |
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| Идентификатор |
Silva, JPB, Istrate, MC, Hellenbrand, M, Jan, A, Becker, MT, Symonowicz, J, Figueiras, FG, Lenzi, V, Hill, MO, Ghica, C, Romanyuk, KN, Gomes, MJM, Martino, GD, Marques, L & MacManus-Driscoll, JL 2023, 'Ferroelectricity and negative piezoelectric coefficient in orthorhombic phase pure ZrO2 thin films', Applied Materials Today, Том. 30, 101708. https://doi.org/10.1016/j.apmt.2022.101708
Silva, J. P. B., Istrate, M. C., Hellenbrand, M., Jan, A., Becker, M. T., Symonowicz, J., Figueiras, F. G., Lenzi, V., Hill, M. O., Ghica, C., Romanyuk, K. N., Gomes, M. J. M., Martino, G. D., Marques, L., & MacManus-Driscoll, J. L. (2023). Ferroelectricity and negative piezoelectric coefficient in orthorhombic phase pure ZrO2 thin films. Applied Materials Today, 30, [101708]. https://doi.org/10.1016/j.apmt.2022.101708 2352-9407 Final All Open Access, Hybrid Gold, Green https://www.scopus.com/inward/record.uri?eid=2-s2.0-85144067583&doi=10.1016%2fj.apmt.2022.101708&partnerID=40&md5=f30c1a5db42a00f1cff339b7db4ccc05 https://doi.org/10.1016/j.apmt.2022.101708 http://elar.urfu.ru/handle/10995/130370 10.1016/j.apmt.2022.101708 85144067583 000976443200001 |
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| Язык |
en
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| Права |
Open access (info:eu-repo/semantics/openAccess)
cc-by-nc-nd https://creativecommons.org/licenses/by-nc-nd/4.0/ |
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| Формат |
application/pdf
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| Издатель |
Elsevier Ltd
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| Источник |
Applied Materials Today
Applied Materials Today |
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