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dc.contributor.authorElse, Breval
dc.contributor.authorChiping, Wang
dc.contributor.authorJoseph, P. Dougherty
dc.contributor.authorAylin, Yilmazbayhan
dc.contributor.authorKamau, Gachigi
dc.contributor.authorMichael, Stewart
dc.contributor.authorFrank, Duva
dc.contributor.authorAnn, Crespi
dc.date.accessioned2013-08-08T06:47:08Z
dc.date.available2013-08-08T06:47:08Z
dc.date.issued2006
dc.identifier.citationBreval, E., Wang, C., Dougherty, J. P., Yilmazbayhan, A., Gachigi, K. W. A., Stewart, M., Duva, F. and Crespi, A. (2006), PLZT Phases Near Lead Zirconate: 2. Determination by Capacitance and Polarization. Journal of the American Ceramic Society, 89: 3681–3688. doi: 10.1111/j.1551-2916.2006.01320.xen
dc.identifier.urihttp://erepository.uonbi.ac.ke:8080/xmlui/handle/123456789/55372
dc.identifier.urihttp://onlinelibrary.wiley.com/doi/10.1111/j.1551-2916.2006.01320.x/full
dc.description.abstractThe phases of PLZT, (Pb,La)(Zr,Ti)O3, or L/Z/T for L<12 and T<10 were detected via determination of capacitance at varying temperatures at 0 field and via polarization at varying fields at room temperature and at selected elevated temperatures. It was possible to determine two different orthorhombic phases, and three rhombohedral (hexagonal) phases, one of which only exists at elevated temperatures. Two sets of phase diagrams were constructed with the phases as a function of temperature, and electric field, respectively. Temperature/field phase diagrams for 0/100/0, 2.95/5, and 4/95/5 were also constructed. A comparison was made between room-temperature and 0 field PLZT phase diagrams determined via X-ray diffraction, capacitance, and polarization.en
dc.language.isoenen
dc.titlePLZT Phases Near Lead Zirconate: 2. Determination by Capacitance and Polarizationen
dc.typeArticleen
local.publisherMechanical and Manufacturing Engineering, University of Nairobien


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