Thermal Hysteresis Accompanying the Incommensurate-Commensurate Phase Transitions in Rb2ZnBr4 and Rb2ZnCl4

1981 ◽  
Vol 50 (8) ◽  
pp. 2666-2671 ◽  
Author(s):  
Katsumi Hamano ◽  
Tōru Hishinuma ◽  
Kenji Ema
1980 ◽  
Vol 49 (6) ◽  
pp. 2278-2286 ◽  
Author(s):  
Katsumi Hamano ◽  
Yoshito Ikeda ◽  
Takayuki Fujimoto ◽  
Kenji Ema ◽  
Shunsuke Hirotsu

2006 ◽  
Vol 300 (1) ◽  
pp. e437-e439 ◽  
Author(s):  
A.G. Zhdanov ◽  
T.B. Kosykh ◽  
A.P. Pyatakov ◽  
A.K. Zvezdin ◽  
D. Viehland

2008 ◽  
Vol 42 (1) ◽  
pp. 58-62 ◽  
Author(s):  
R. J. Christie ◽  
P. K. Wu ◽  
P. Photinos ◽  
S. C. Abrahams

Atomic coordinate analysis allows materials with appropriate but previously unrecognized dielectric properties to be predicted as new ferroelectrics if their crystal structure is known. An earlier such prediction that NaSb3F10is ferroelectric is confirmed herein without ambiguity. Its spontaneous polarizationPsis found to exhibit reproducible dielectric hysteresis at room temperature, withPs≃ 60 µC m−2, under the application of a field of 0.3 MV m−1or greater. The pyroelectric coefficient 〈p〉 = 17 (5) µC m−2 K−1at 298 K. NaSb3F10undergoes a phase transition atTC≃ 461 K, on correction for thermal hysteresis, with entropy change ΔS= 5.7 (3) J mol−1 K−1. The colorless crystals melt atTm ≃ 515 K and decompose above ∼600 K. The thermal hysteresis of ∼35 K inTC, on heating and cooling at 5–25 K min−1, is typical of first-order phase transitions. The space group in ferroelectric phase III isP63, and that in phase II is predicted to beP6322, a nonpolar supergroup ofP63; the supergroup expected in the prototypic nonferroic phase I isP63/mmc. The space group of phase III isnota direct subgroup of phase I. The dielectric permittivity ∊′ at 1 kHz increases over an order of magnitude between 300 K and a major inflection atTC, continuing to increase steadily thereafter toTm.


1986 ◽  
Vol 47 (3) ◽  
pp. 483-489 ◽  
Author(s):  
J. Berger ◽  
J.P. Benoit ◽  
C.W. Garland ◽  
P.W. Wallace

2013 ◽  
Vol 756-759 ◽  
pp. 4419-4422
Author(s):  
Jin Song Wang

The irreversibility of ferroelectric phase transitions has been studied by using the irreversible thermodynamics. The thermal hysteresis of first-order ferroelectric phase transitions and the polydomain structure of ferroelectrics can be explained on the basis of the principle of minimum entropy production. A conclusion has been derived that the thermal hysteresis is not an intrinsic property of a system in which a first-order ferroelectric phase transition occurs. The finiteness of the systems surface is connected with the thermal hysteresis.


1968 ◽  
Vol 6 (7) ◽  
pp. 427-429 ◽  
Author(s):  
L.C. Nino ◽  
J.A. Gonzalo

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