Please use this identifier to cite or link to this item: https://ir.swu.ac.th/jspui/handle/123456789/15073
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dc.contributor.authorSvitelskiy O.
dc.contributor.authorLa-Orauttapong D.
dc.contributor.authorToulouse J.
dc.contributor.authorChen W.
dc.contributor.authorYe Z.-G.
dc.date.accessioned2021-04-05T04:32:29Z-
dc.date.available2021-04-05T04:32:29Z-
dc.date.issued2005
dc.identifier.issn10980121
dc.identifier.other2-s2.0-29544437557
dc.identifier.urihttps://ir.swu.ac.th/jspui/handle/123456789/15073-
dc.identifier.urihttps://www.scopus.com/inward/record.uri?eid=2-s2.0-29544437557&doi=10.1103%2fPhysRevB.72.172106&partnerID=40&md5=bdb0ca27a49fe04055318509a2a62248
dc.description.abstractWe present the results of the Raman study of lattice dynamics and development of mesoscopic range order in a relaxor ferroelectric Pb(Zn13Nb23)O3 crystal containing 4.5% of PbTiO3 as it is cooling down from 1000to100K. As in the other relaxors, the relaxor state develops in four stages separated by three temperatures: Burns temperature TB∼800K, intermediate temperature Td∼550K, and freezing temperature Tf∼370K. However, the mixed crystal shows significant differences compared to the nominally pure one. First, there is a dramatic decrease of the scattered intensity above TB; second, a significant asymmetry of the polarizability tensor occurs near the Td reflected by polarization properties of the central peak; third, a softening of line B (∼780cm-1) is found in the neigborhood of Td; fourth, essentially different in each case is the splitting of the broad band E (∼560cm-1), and its value can serve as an indicator of the order parameter in the system. © 2005 The American Physical Society.
dc.titlePbTiO3 addition and internal dynamics in Pb(Zn13Nb23)O3 crystal studied by Raman spectroscopy
dc.typeArticle
dc.rights.holderScopus
dc.identifier.bibliograpycitationPhysical Review B - Condensed Matter and Materials Physics. Vol 72, No.17 (2005), p.-
dc.identifier.doi10.1103/PhysRevB.72.172106
Appears in Collections:Scopus 1983-2021

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