T. Mimura, Reijiro Shimura, Akinori Tateyama, Y. Nakamura, T. Shiraishi, H. Funakubo
{"title":"铁电x%YO1.5 -(100−x%)(Hf1−yZry)O2薄膜的无加热沉积","authors":"T. Mimura, Reijiro Shimura, Akinori Tateyama, Y. Nakamura, T. Shiraishi, H. Funakubo","doi":"10.1002/pssa.202300100","DOIUrl":null,"url":null,"abstract":"The no‐heating deposition of x%YO1.5–(100−x%)(Hf1−yZry)O2 (x = 0−0.09, y = 0, 0.25, 0.50, and 1) is achieved using a radio‐frequency magnetron sputtering method. To investigate the crystal structure and ferroelectric properties, epitaxial films are grown on (111)‐oriented indium tin oxide (ITO)/(111) Y‐stabilized zirconia (YSZ) substrates. The ferroelectric orthorhombic phase is obtained for the 5–7%YO1.5–95–93%HfO2 and 5%YO1.5–95% (Hf0.75Zr0.25)O2 films. The field‐induced phase transition from tetragonal to orthorhombic is confirmed for the 8%YO1.5–92%HfO2 and 5%YO1.5–95%(Hf0.50Zr0.50)O2 films. The remnant polarization (Pr) and coercive field (Ec) are 12–19 μC cm−2 and 2,000–2,500 kV cm−1, respectively. The piezoelectric response of 1 μm thick films is investigated for 6%YO1.5–94% HfO2, 7%YO1.5–93%HfO2, and 5%YO1.5–95%(Hf0.50Zr0.50)O2 films, which have piezoelectric coefficients (d33) of 1.0, 3.3, and 5.0 pm V−1, respectively. These results show no‐heating deposition of x%YO1.5–(100−x%)(Hf1−yZry)O2 films with ferroelectric and piezoelectric properties.","PeriodicalId":87717,"journal":{"name":"Physica status solidi (A): Applied research","volume":"62 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"No‐Heating Deposition of Ferroelectric x%YO1.5–(100−x%)(Hf1−yZry)O2 Films\",\"authors\":\"T. Mimura, Reijiro Shimura, Akinori Tateyama, Y. Nakamura, T. Shiraishi, H. Funakubo\",\"doi\":\"10.1002/pssa.202300100\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The no‐heating deposition of x%YO1.5–(100−x%)(Hf1−yZry)O2 (x = 0−0.09, y = 0, 0.25, 0.50, and 1) is achieved using a radio‐frequency magnetron sputtering method. To investigate the crystal structure and ferroelectric properties, epitaxial films are grown on (111)‐oriented indium tin oxide (ITO)/(111) Y‐stabilized zirconia (YSZ) substrates. The ferroelectric orthorhombic phase is obtained for the 5–7%YO1.5–95–93%HfO2 and 5%YO1.5–95% (Hf0.75Zr0.25)O2 films. The field‐induced phase transition from tetragonal to orthorhombic is confirmed for the 8%YO1.5–92%HfO2 and 5%YO1.5–95%(Hf0.50Zr0.50)O2 films. The remnant polarization (Pr) and coercive field (Ec) are 12–19 μC cm−2 and 2,000–2,500 kV cm−1, respectively. The piezoelectric response of 1 μm thick films is investigated for 6%YO1.5–94% HfO2, 7%YO1.5–93%HfO2, and 5%YO1.5–95%(Hf0.50Zr0.50)O2 films, which have piezoelectric coefficients (d33) of 1.0, 3.3, and 5.0 pm V−1, respectively. These results show no‐heating deposition of x%YO1.5–(100−x%)(Hf1−yZry)O2 films with ferroelectric and piezoelectric properties.\",\"PeriodicalId\":87717,\"journal\":{\"name\":\"Physica status solidi (A): Applied research\",\"volume\":\"62 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physica status solidi (A): Applied research\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1002/pssa.202300100\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physica status solidi (A): Applied research","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1002/pssa.202300100","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
No‐Heating Deposition of Ferroelectric x%YO1.5–(100−x%)(Hf1−yZry)O2 Films
The no‐heating deposition of x%YO1.5–(100−x%)(Hf1−yZry)O2 (x = 0−0.09, y = 0, 0.25, 0.50, and 1) is achieved using a radio‐frequency magnetron sputtering method. To investigate the crystal structure and ferroelectric properties, epitaxial films are grown on (111)‐oriented indium tin oxide (ITO)/(111) Y‐stabilized zirconia (YSZ) substrates. The ferroelectric orthorhombic phase is obtained for the 5–7%YO1.5–95–93%HfO2 and 5%YO1.5–95% (Hf0.75Zr0.25)O2 films. The field‐induced phase transition from tetragonal to orthorhombic is confirmed for the 8%YO1.5–92%HfO2 and 5%YO1.5–95%(Hf0.50Zr0.50)O2 films. The remnant polarization (Pr) and coercive field (Ec) are 12–19 μC cm−2 and 2,000–2,500 kV cm−1, respectively. The piezoelectric response of 1 μm thick films is investigated for 6%YO1.5–94% HfO2, 7%YO1.5–93%HfO2, and 5%YO1.5–95%(Hf0.50Zr0.50)O2 films, which have piezoelectric coefficients (d33) of 1.0, 3.3, and 5.0 pm V−1, respectively. These results show no‐heating deposition of x%YO1.5–(100−x%)(Hf1−yZry)O2 films with ferroelectric and piezoelectric properties.