Sequential Phase Transitions in Sm Substituted BiFeO3
The compositional and thermal evolution of the crystal structure of the solid solution Bi 1-x Sm x FeO 3 synthesized at a high pressure of 4 GPa was investigated. It was found that Bi 1-x Sm x FeO 3 with $x = 0.10$ and 0.15 had an antipolar PbZrO 3 -type structure with a $\sqrt{2}a\times 2\sqrt{2}a\...
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Veröffentlicht in: | Jpn J Appl Phys 2011-09, Vol.50 (9), p.09NE08-09NE08-4 |
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container_title | Jpn J Appl Phys |
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creator | Kubota, Makoto Oka, Kengo Nakamura, Yoshitaka Yabuta, Hisato Miura, Kaoru Shimakawa, Yuichi Azuma, Masaki |
description | The compositional and thermal evolution of the crystal structure of the solid solution Bi 1-x Sm x FeO 3 synthesized at a high pressure of 4 GPa was investigated. It was found that Bi 1-x Sm x FeO 3 with $x = 0.10$ and 0.15 had an antipolar PbZrO 3 -type structure with a $\sqrt{2}a\times 2\sqrt{2}a\times 4a$ perovskite superstructure at room temperature, while that with $x = 0.05$ had the same structure as the parent BiFeO 3 ($x = 0$). The $x = 0.10$ sample transforms from an antipolar PbZrO 3 -type orthorhombic structure to a polar BiFeO 3 -type rhombohedral structure and eventually to a nonpolar GdFeO 3 -type structure on heating as Zr-rich PZT. |
doi_str_mv | 10.1143/JJAP.50.09NE08 |
format | Article |
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It was found that Bi 1-x Sm x FeO 3 with $x = 0.10$ and 0.15 had an antipolar PbZrO 3 -type structure with a $\sqrt{2}a\times 2\sqrt{2}a\times 4a$ perovskite superstructure at room temperature, while that with $x = 0.05$ had the same structure as the parent BiFeO 3 ($x = 0$). The $x = 0.10$ sample transforms from an antipolar PbZrO 3 -type orthorhombic structure to a polar BiFeO 3 -type rhombohedral structure and eventually to a nonpolar GdFeO 3 -type structure on heating as Zr-rich PZT.</description><identifier>ISSN: 0021-4922</identifier><identifier>EISSN: 1347-4065</identifier><identifier>DOI: 10.1143/JJAP.50.09NE08</identifier><language>eng</language><publisher>The Japan Society of Applied Physics</publisher><ispartof>Jpn J Appl Phys, 2011-09, Vol.50 (9), p.09NE08-09NE08-4</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27923,27924</link.rule.ids></links><search><creatorcontrib>Kubota, Makoto</creatorcontrib><creatorcontrib>Oka, Kengo</creatorcontrib><creatorcontrib>Nakamura, Yoshitaka</creatorcontrib><creatorcontrib>Yabuta, Hisato</creatorcontrib><creatorcontrib>Miura, Kaoru</creatorcontrib><creatorcontrib>Shimakawa, Yuichi</creatorcontrib><creatorcontrib>Azuma, Masaki</creatorcontrib><title>Sequential Phase Transitions in Sm Substituted BiFeO3</title><title>Jpn J Appl Phys</title><description>The compositional and thermal evolution of the crystal structure of the solid solution Bi 1-x Sm x FeO 3 synthesized at a high pressure of 4 GPa was investigated. 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It was found that Bi 1-x Sm x FeO 3 with $x = 0.10$ and 0.15 had an antipolar PbZrO 3 -type structure with a $\sqrt{2}a\times 2\sqrt{2}a\times 4a$ perovskite superstructure at room temperature, while that with $x = 0.05$ had the same structure as the parent BiFeO 3 ($x = 0$). The $x = 0.10$ sample transforms from an antipolar PbZrO 3 -type orthorhombic structure to a polar BiFeO 3 -type rhombohedral structure and eventually to a nonpolar GdFeO 3 -type structure on heating as Zr-rich PZT.</abstract><pub>The Japan Society of Applied Physics</pub><doi>10.1143/JJAP.50.09NE08</doi></addata></record> |
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title | Sequential Phase Transitions in Sm Substituted BiFeO3 |
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