Hybrid improper ferroelectricity in La2Sr (Sc1−xFex)2O7 ceramics with double-layered Ruddlesden–Popper structures
Numerous hybrid improper ferroelectrics have been discovered in bulk oxides with layered perovskite structures. In contrast, the competition between the interlayer rumpling and oxygen octahedral rotation suppresses the ferroelectricity in layered perovskite material with trivalent cation at the B-si...
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description | Numerous hybrid improper ferroelectrics have been discovered in bulk oxides with layered perovskite structures. In contrast, the competition between the interlayer rumpling and oxygen octahedral rotation suppresses the ferroelectricity in layered perovskite material with trivalent cation at the B-site. In the present work, single-phase dense La2Sr(Sc1−xFex)2O7 ceramics with double-layered Ruddlesden–Popper structures have been prepared, and room-temperature ferroelectricity is discovered in the ceramics with x ≤ 0.10. The ferroelectric polarization and coercive field decrease with increasing content of Fe3+ cations, consistent with the decline of oxygen octahedral rotation and tilting angles. Although the linear relationship between the Curie temperature and the tolerance factor for La2Sr(Sc1−xFex)2O7 ceramics is established, the line is far away from that for A2+3B4+2O7 ceramics due to the large interlayer rumpling in the present ceramics. Although no single-phase multiferroic has been discovered in this work, an effective way to introduce magnetism into hybrid improper ferroelectric is provided. |
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In contrast, the competition between the interlayer rumpling and oxygen octahedral rotation suppresses the ferroelectricity in layered perovskite material with trivalent cation at the B-site. In the present work, single-phase dense La2Sr(Sc1−xFex)2O7 ceramics with double-layered Ruddlesden–Popper structures have been prepared, and room-temperature ferroelectricity is discovered in the ceramics with x ≤ 0.10. The ferroelectric polarization and coercive field decrease with increasing content of Fe3+ cations, consistent with the decline of oxygen octahedral rotation and tilting angles. Although the linear relationship between the Curie temperature and the tolerance factor for La2Sr(Sc1−xFex)2O7 ceramics is established, the line is far away from that for A2+3B4+2O7 ceramics due to the large interlayer rumpling in the present ceramics. Although no single-phase multiferroic has been discovered in this work, an effective way to introduce magnetism into hybrid improper ferroelectric is provided.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/5.0220720</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Bulk density ; Cations ; Ceramics ; Coercivity ; Curie temperature ; Ferroelectric materials ; Ferroelectricity ; Interlayers ; Oxygen ; Perovskites ; Room temperature ; Rotation</subject><ispartof>Applied physics letters, 2024-07, Vol.125 (4)</ispartof><rights>Author(s)</rights><rights>2024 Author(s). 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In contrast, the competition between the interlayer rumpling and oxygen octahedral rotation suppresses the ferroelectricity in layered perovskite material with trivalent cation at the B-site. In the present work, single-phase dense La2Sr(Sc1−xFex)2O7 ceramics with double-layered Ruddlesden–Popper structures have been prepared, and room-temperature ferroelectricity is discovered in the ceramics with x ≤ 0.10. The ferroelectric polarization and coercive field decrease with increasing content of Fe3+ cations, consistent with the decline of oxygen octahedral rotation and tilting angles. Although the linear relationship between the Curie temperature and the tolerance factor for La2Sr(Sc1−xFex)2O7 ceramics is established, the line is far away from that for A2+3B4+2O7 ceramics due to the large interlayer rumpling in the present ceramics. Although no single-phase multiferroic has been discovered in this work, an effective way to introduce magnetism into hybrid improper ferroelectric is provided.</description><subject>Bulk density</subject><subject>Cations</subject><subject>Ceramics</subject><subject>Coercivity</subject><subject>Curie temperature</subject><subject>Ferroelectric materials</subject><subject>Ferroelectricity</subject><subject>Interlayers</subject><subject>Oxygen</subject><subject>Perovskites</subject><subject>Room temperature</subject><subject>Rotation</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNp9kM1KAzEUhYMoWKsL3yDgxgpTc5MmU5dSrBUKFdv9kJ87mDLt1GQGOzuXrvUN-yROadeuLgc-zuF-hFwD6wNT4l72Gecs5eyEdIClaSIAhqekwxgTiXqQcE4uYly2UXIhOqSeNCZ4R_1qE8oNBppjCCUWaKvgra8a6td0qvk80Nu5hd33z3aM2x6fpdRi0CtvI_301Tt1ZW0KTArdYEBH32rnCowO17uv39dys6-OVahtVQeMl-Qs10XEq-PtksX4aTGaJNPZ88vocZpYGPIqUcYIp4BZ0E4C16lhCpQcKCvASAQEabnRg4E2TikuDKQD7VKW58bkeii65OZQ2_72UWOssmVZh3W7mAk2FFwKJVVL9Q6UDWWMAfNsE_xKhyYDlu2lZjI7Sm3ZuwMbWze68uX6H_gPzbh5ag</recordid><startdate>20240722</startdate><enddate>20240722</enddate><creator>Guo, Zhe</creator><creator>Zhang, Zheng Duan</creator><creator>Liu, Xiao Qiang</creator><creator>Chen, Xiang Ming</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0001-8028-0644</orcidid><orcidid>https://orcid.org/0009-0005-3760-2077</orcidid><orcidid>https://orcid.org/0000-0001-7029-0662</orcidid></search><sort><creationdate>20240722</creationdate><title>Hybrid improper ferroelectricity in La2Sr (Sc1−xFex)2O7 ceramics with double-layered Ruddlesden–Popper structures</title><author>Guo, Zhe ; Zhang, Zheng Duan ; Liu, Xiao Qiang ; Chen, Xiang Ming</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c182t-6bb3d610c1ad512a7b0616546c31b5e1e15c2ba44abd6623b174ad70ffbbfa83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><topic>Bulk density</topic><topic>Cations</topic><topic>Ceramics</topic><topic>Coercivity</topic><topic>Curie temperature</topic><topic>Ferroelectric materials</topic><topic>Ferroelectricity</topic><topic>Interlayers</topic><topic>Oxygen</topic><topic>Perovskites</topic><topic>Room temperature</topic><topic>Rotation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Guo, Zhe</creatorcontrib><creatorcontrib>Zhang, Zheng Duan</creatorcontrib><creatorcontrib>Liu, Xiao Qiang</creatorcontrib><creatorcontrib>Chen, Xiang Ming</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Guo, Zhe</au><au>Zhang, Zheng Duan</au><au>Liu, Xiao Qiang</au><au>Chen, Xiang Ming</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Hybrid improper ferroelectricity in La2Sr (Sc1−xFex)2O7 ceramics with double-layered Ruddlesden–Popper structures</atitle><jtitle>Applied physics letters</jtitle><date>2024-07-22</date><risdate>2024</risdate><volume>125</volume><issue>4</issue><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>Numerous hybrid improper ferroelectrics have been discovered in bulk oxides with layered perovskite structures. In contrast, the competition between the interlayer rumpling and oxygen octahedral rotation suppresses the ferroelectricity in layered perovskite material with trivalent cation at the B-site. In the present work, single-phase dense La2Sr(Sc1−xFex)2O7 ceramics with double-layered Ruddlesden–Popper structures have been prepared, and room-temperature ferroelectricity is discovered in the ceramics with x ≤ 0.10. The ferroelectric polarization and coercive field decrease with increasing content of Fe3+ cations, consistent with the decline of oxygen octahedral rotation and tilting angles. Although the linear relationship between the Curie temperature and the tolerance factor for La2Sr(Sc1−xFex)2O7 ceramics is established, the line is far away from that for A2+3B4+2O7 ceramics due to the large interlayer rumpling in the present ceramics. Although no single-phase multiferroic has been discovered in this work, an effective way to introduce magnetism into hybrid improper ferroelectric is provided.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0220720</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0001-8028-0644</orcidid><orcidid>https://orcid.org/0009-0005-3760-2077</orcidid><orcidid>https://orcid.org/0000-0001-7029-0662</orcidid></addata></record> |
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subjects | Bulk density Cations Ceramics Coercivity Curie temperature Ferroelectric materials Ferroelectricity Interlayers Oxygen Perovskites Room temperature Rotation |
title | Hybrid improper ferroelectricity in La2Sr (Sc1−xFex)2O7 ceramics with double-layered Ruddlesden–Popper structures |
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