Anisotropic field induced phase transitions and negative electrocaloric effect in rhombohedral Mn doped Pb(In1/2Nb1/2)O3-Pb(Mg1/3Nb2/3)O3-PbTiO3 single crystals

2018 ◽  
Vol 44 (8) ◽  
pp. 9045-9052 ◽  
Author(s):  
Yaming Zhou ◽  
Qiang Li ◽  
Fangping Zhuo ◽  
Qingfeng Yan ◽  
Yiling Zhang ◽  
...  
2017 ◽  
Vol 43 (18) ◽  
pp. 16300-16305 ◽  
Author(s):  
Tian-Fu Zhang ◽  
Xin-Gui Tang ◽  
Peng-Zu Ge ◽  
Qiu-Xiang Liu ◽  
Yan-Ping Jiang

2020 ◽  
Vol 4 (8) ◽  
Author(s):  
N. S. Sangeetha ◽  
Santanu Pakhira ◽  
D. H. Ryan ◽  
V. Smetana ◽  
A.-V. Mudring ◽  
...  

2016 ◽  
Vol 89 (7-8) ◽  
pp. 768-776 ◽  
Author(s):  
Irena Jankowska-Sumara ◽  
Min-Seok Jeong ◽  
Jae-Hyeon Ko ◽  
Andrzej Majchrowski ◽  
Józef Żmija

Author(s):  
T. M. Correia ◽  
Q. Zhang

Full-perovskite Pb 0.87 Ba 0.1 La 0.02 (Zr 0.6 Sn 0.33 Ti 0.07 )O 3 (PBLZST) thin films were fabricated by a sol–gel method. These revealed both rhombohedral and tetragonal phases, as opposed to the full-tetragonal phase previously reported in ceramics. The fractions of tetragonal and rhombohedral phases are found to be strongly dependent on film thickness. The fraction of tetragonal grains increases with increasing film thickness, as the substrate constraint throughout the film decreases with film thickness. The maximum of the dielectric constant ( ε m ) and the corresponding temperature ( T m ) are thickness-dependent and dictated by the fraction of rhombohedral and tetragonal phase, with ε m reaching a minimum at 400 nm and T m shifting to higher temperature with increasing thickness. With the thickness increase, the breakdown field decreases, but field-induced antiferroelectric–ferroelectric ( E AFE−FE ) and ferroelectric–antiferroelectric ( E FE−AFE ) switch fields increase. The electrocaloric effect increases with increasing film thickness. This article is part of the themed issue ‘Taking the temperature of phase transitions in cool materials’.


Author(s):  
R.-U. Barz ◽  
F. David ◽  
J. Schneider ◽  
P. Gille

AbstractSingle crystals of Al


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