{"title":"量子准电性中氧同位素效应和铁电跃迁的注解","authors":"E. Matsushita, S. Segawa","doi":"10.1109/ISAF.2007.4393235","DOIUrl":null,"url":null,"abstract":"By extending the soft-phonon theory, a quantum paraelectric(PE)-ferroelectric(FE) transition in SrTi<sup>16</sup>O<sub>3</sub> (ST016) is studied from the viewpoint of the important role of optical phonons in perovskite-oxides. In spite of intrinsic quantum fluctuation of large zero-point vibration induced from light O-atoms, the FE transition due to the O-isotope exchange <sup>16</sup>O<sub>1-x</sub> <sup>18</sup>O<sub>x</sub> is explained in a unified picture by combining with the applied pressure (or uniaxial stress) effect. The calculated T<sub>c</sub> as the function of x is compared with the experimental data in rather good agreement, and the origin of quantum paraelectricity in STO 16 is discussed in comparison with pressure effect in hydrogen-bonded ferroelectrics KH<sub>2</sub>PO<sub>4</sub> (KDP). As the result, it is suggested that quantum PE-FE transition with the critical exponent 1/2 at T<sub>c</sub>=0 where the FE transition will start, must be analyzed by a microscopic theory exceeding soft phonon theory.","PeriodicalId":321007,"journal":{"name":"2007 Sixteenth IEEE International Symposium on the Applications of Ferroelectrics","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2007-05-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Note on Oxygen Isotope Effect and Ferroelectric Transition in Quantum Paraelectrics\",\"authors\":\"E. Matsushita, S. Segawa\",\"doi\":\"10.1109/ISAF.2007.4393235\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"By extending the soft-phonon theory, a quantum paraelectric(PE)-ferroelectric(FE) transition in SrTi<sup>16</sup>O<sub>3</sub> (ST016) is studied from the viewpoint of the important role of optical phonons in perovskite-oxides. In spite of intrinsic quantum fluctuation of large zero-point vibration induced from light O-atoms, the FE transition due to the O-isotope exchange <sup>16</sup>O<sub>1-x</sub> <sup>18</sup>O<sub>x</sub> is explained in a unified picture by combining with the applied pressure (or uniaxial stress) effect. The calculated T<sub>c</sub> as the function of x is compared with the experimental data in rather good agreement, and the origin of quantum paraelectricity in STO 16 is discussed in comparison with pressure effect in hydrogen-bonded ferroelectrics KH<sub>2</sub>PO<sub>4</sub> (KDP). As the result, it is suggested that quantum PE-FE transition with the critical exponent 1/2 at T<sub>c</sub>=0 where the FE transition will start, must be analyzed by a microscopic theory exceeding soft phonon theory.\",\"PeriodicalId\":321007,\"journal\":{\"name\":\"2007 Sixteenth IEEE International Symposium on the Applications of Ferroelectrics\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2007-05-27\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2007 Sixteenth IEEE International Symposium on the Applications of Ferroelectrics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ISAF.2007.4393235\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2007 Sixteenth IEEE International Symposium on the Applications of Ferroelectrics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ISAF.2007.4393235","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Note on Oxygen Isotope Effect and Ferroelectric Transition in Quantum Paraelectrics
By extending the soft-phonon theory, a quantum paraelectric(PE)-ferroelectric(FE) transition in SrTi16O3 (ST016) is studied from the viewpoint of the important role of optical phonons in perovskite-oxides. In spite of intrinsic quantum fluctuation of large zero-point vibration induced from light O-atoms, the FE transition due to the O-isotope exchange 16O1-x18Ox is explained in a unified picture by combining with the applied pressure (or uniaxial stress) effect. The calculated Tc as the function of x is compared with the experimental data in rather good agreement, and the origin of quantum paraelectricity in STO 16 is discussed in comparison with pressure effect in hydrogen-bonded ferroelectrics KH2PO4 (KDP). As the result, it is suggested that quantum PE-FE transition with the critical exponent 1/2 at Tc=0 where the FE transition will start, must be analyzed by a microscopic theory exceeding soft phonon theory.