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dc.contributor.authorRushchanskii, K. Z.-
dc.contributor.authorBilanych, R. M.-
dc.contributor.authorMolnar, Alexander-
dc.contributor.authorYevych, R. M.-
dc.contributor.authorKohutych, Anton-
dc.contributor.authorPerechinskii, S. I.-
dc.contributor.authorSamulionis, V.-
dc.contributor.authorBanys, J.-
dc.contributor.authorVysochanskii, Yulian-
dc.date.accessioned2024-03-27T12:34:53Z-
dc.date.available2024-03-27T12:34:53Z-
dc.date.issued2016-02-
dc.identifier.citationFerroelectricity in (PbySn1−y)2P2S6 mixed crystals and random field BEG model / K. Z. Rushchanskii, R. M. Bilanych, A. A. Molnar, R. M. Yevych, A. A. Kohutych, S. I. Perechinskii, V. Samulionis, J. Banys, and Y. M. Vysochanskii // Physica Status Solidi B253, - 2016. - No.2, - pp.384–391/ DOI 10.1002/pssb.201552138uk
dc.identifier.otherDOI 10.1002/pssb.201552138-
dc.identifier.urihttps://dspace.uzhnu.edu.ua/jspui/handle/lib/60468-
dc.descriptionIn Sn2P2S6 ferroelectric under compression, the second-order phase transition line is observed down to the tricritical point as the transition temperature decreases to 250 K. A tricriticality at a similar temperature is also revealed in the mixed crystals on S→Se substitution. For the mixed crystals with Sn→Pb substitution, ultrasound, hypersound, and low-frequency dielectric studies also show heterophase features appearing on decrease of the ferroelectric transition temperature below a so-called “waterline temperature” near 250 K. Such behavior agrees with the Blume–Emery–Griffiths (BEG) model appropriate for the ferroelectric system under investigation with a three-well local potential for the order parameter fluctuations. The BEG model modified by the random-field phase diagram in the vicinity of the tricritical point qualitatively explains the influence of the cationic substitution on the (PbySn1−y)2P2S6 ferroelectric properties.uk
dc.description.abstractIn Sn2P2S6 ferroelectric under compression, the second-order phase transition line is observed down to the tricritical point as the transition temperature decreases to 250 K. A tricriticality at a similar temperature is also revealed in the mixed crystals on S→Se substitution. For the mixed crystals with Sn→Pb substitution, ultrasound, hypersound, and low-frequency dielectric studies also show heterophase features appearing on decrease of the ferroelectric transition temperature below a so-called “waterline temperature” near 250 K. Such behavior agrees with the Blume–Emery–Griffiths (BEG) model appropriate for the ferroelectric system under investigation with a three-well local potential for the order parameter fluctuations. The BEG model modified by the random-field phase diagram in the vicinity of the tricritical point qualitatively explains the influence of the cationic substitution on the (PbySn1−y)2P2S6 ferroelectric properties.uk
dc.language.isoenuk
dc.publisherWiley-VCHuk
dc.subjectBlume–Emery–Griffiths modeluk
dc.subjectferroelectricsuk
dc.subjectphase diagramsuk
dc.subjecttricritical pointuk
dc.titleFerroelectricity in (PbySn1−y)2P2S6 mixed crystals and random field BEG modeluk
dc.typeTextuk
dc.pubTypeСтаттяuk
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