Home > Publications database > Ferroelectricity in (PbySn1−y)2P2S6 mixed crystals and random field BEG model > print |
001 | 279906 | ||
005 | 20210129221155.0 | ||
024 | 7 | _ | |a 10.1002/pssb.201552138 |2 doi |
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024 | 7 | _ | |a 0370-1972 |2 ISSN |
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100 | 1 | _ | |a Rushchanskii, Konstantin |0 P:(DE-Juel1)130926 |b 0 |e Corresponding author |u fzj |
245 | _ | _ | |a Ferroelectricity in (PbySn1−y)2P2S6 mixed crystals and random field BEG model |
260 | _ | _ | |a Weinheim |c 2016 |b Wiley-VCH70889 |
264 | _ | 1 | |3 online |2 Crossref |b Wiley |c 2015-10-19 |
264 | _ | 1 | |3 print |2 Crossref |b Wiley |c 2016-02-01 |
264 | _ | 1 | |3 print |2 Crossref |b Wiley |c 2016-02-01 |
336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1456146862_16631 |2 PUB:(DE-HGF) |
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520 | _ | _ | |a In Sninline imagePinline imageSinline image 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 Sinline imageSe substitution. For the mixed crystals with Sninline imagePb 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 (Pbinline imageSninline image)inline imagePinline imageSinline image ferroelectric properties. |
536 | _ | _ | |a 142 - Controlling Spin-Based Phenomena (POF3-142) |0 G:(DE-HGF)POF3-142 |c POF3-142 |f POF III |x 0 |
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700 | 1 | _ | |a Bilanych, R. M. |0 P:(DE-HGF)0 |b 1 |
700 | 1 | _ | |a Molnar, A. A. |0 P:(DE-HGF)0 |b 2 |
700 | 1 | _ | |a Yevych, R. M. |0 P:(DE-HGF)0 |b 3 |
700 | 1 | _ | |a Kohutych, A. A. |0 P:(DE-HGF)0 |b 4 |
700 | 1 | _ | |a Perechinskii, S. I. |0 P:(DE-HGF)0 |b 5 |
700 | 1 | _ | |a Samulionis, V. |0 P:(DE-HGF)0 |b 6 |
700 | 1 | _ | |a Banys, J. |0 P:(DE-HGF)0 |b 7 |
700 | 1 | _ | |a Vysochanskii, Y. M. |0 P:(DE-HGF)0 |b 8 |
773 | 1 | 8 | |a 10.1002/pssb.201552138 |b : Wiley, 2015-10-19 |n 2 |p 384-391 |3 journal-article |2 Crossref |t physica status solidi (b) |v 253 |y 2015 |x 0370-1972 |
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