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dc.contributor.authorKuo, SYen_US
dc.contributor.authorLi, CTen_US
dc.contributor.authorHsieh, WFen_US
dc.date.accessioned2019-04-03T06:37:29Z-
dc.date.available2019-04-03T06:37:29Z-
dc.date.issued2004-05-01en_US
dc.identifier.issn2469-9950en_US
dc.identifier.urihttp://dx.doi.org/10.1103/PhysRevB.69.184104en_US
dc.identifier.urihttp://hdl.handle.net/11536/26792-
dc.description.abstractInvestigation of the structural and vibrational properties of the PbxCa1-xTiO3 (PCT) system exhibits two phase transitions in the range of x=0-1 by using x-ray powder diffraction and Raman spectroscopy. The first transition occurring at xsimilar to0.65 corresponds to the tetragonal-to-cubic phase and the second one occurs near x=0.35 is attributed to the orthorhombic-to-cubic phase. The absence of the intermediate tetragonal phase between orthorhombic and cubic phases (0<x<0.35) may be mostly attributed to the very restricted region in the PCT system. In addition, a decreasing giant LO-TO splitting behavior similar to that exhibited in PbxSr1-xTiO3 system for lower Pb concentration was also observed, which has been attributed to the highly Pb-O covalent bonding to reduce the long-range Coulomb interaction. Comparison of the change of line shapes of A(1)(1TO) mode among three PbTiO3-based perovskites indicates that the anharmonicity will become more conspicuous due to the larger high-order potential terms of Ba2+ and Ca2+ substitution than Sr2+ substitution for Pb2+.en_US
dc.language.isoen_USen_US
dc.titleLattice dynamics of perovskite PbxCa1-xTiO3en_US
dc.typeArticleen_US
dc.identifier.doi10.1103/PhysRevB.69.184104en_US
dc.identifier.journalPHYSICAL REVIEW Ben_US
dc.citation.volume69en_US
dc.citation.issue18en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department光電工程研究所zh_TW
dc.contributor.departmentInstitute of EO Enginerringen_US
dc.identifier.wosnumberWOS:000222095500025en_US
dc.citation.woscount22en_US
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