Large remanent polarization of 100% polar-axis-oriented epitaxial tetragonal Pb(Zr0.35Ti0.65)O3 thin films

2003 ◽  
Vol 82 (26) ◽  
pp. 4761-4763 ◽  
Author(s):  
Hitoshi Morioka ◽  
Gouji Asano ◽  
Takahiro Oikawa ◽  
Hiroshi Funakubo ◽  
Keisuke Saito
2013 ◽  
Vol 42 (2) ◽  
pp. 585-590 ◽  
Author(s):  
Linxing Zhang ◽  
Jun Chen ◽  
Hanqing Zhao ◽  
Longlong Fan ◽  
Yangchun Rong ◽  
...  

2002 ◽  
Vol 92 (3) ◽  
pp. 1518-1521 ◽  
Author(s):  
Takayuki Watanabe ◽  
Takashi Kojima ◽  
Tomohiro Sakai ◽  
Hiroshi Funakubo ◽  
Minoru Osada ◽  
...  

2016 ◽  
Vol 3 (11) ◽  
pp. 1473-1479 ◽  
Author(s):  
Yilin Wang ◽  
Hanqing Zhao ◽  
Linxing Zhang ◽  
Zhanning Liu ◽  
Jun Chen ◽  
...  

Large remanent polarization in PbTiO3–SmFeO3 thin films with distinct a-domains.


2022 ◽  
Vol 120 (2) ◽  
pp. 022903
Author(s):  
Yoshiharu Ito ◽  
Akinori Tateyama ◽  
Rurika Kubota ◽  
Takahisa Shiraishi ◽  
Takao Shimizu ◽  
...  

1998 ◽  
Vol 541 ◽  
Author(s):  
Yu-Jen Chen ◽  
Gwo Jamn ◽  
Kuo-Shung Liu ◽  
I-Nan Lina

AbstractA two-step pulsed laser deposition (PLD) process, including PLD at a substrate temperature lower than 150°C and rapid-thermal-annealing (RTA) at around 550°C (30 s), has been successfully applied for growing (Pb0.97La0.03)(Zr0.66Ti0.034)0.9875O3, PLZT, thin films. Interdiffusion between layers is pronouncedly suppressed due to the presence of the SrRuO3 layer, which markedly improves the electrical properties of PLZT films. The PLZT films thus obtained exhibit large remanent polarization P,=19 µC/cm2 (with coercive force Ec=78 kV/cm), low leakage current density J11≤8 × 1O−6 A/cm2 (up to 400 kV/cm) and fatigue free characteristics.


1991 ◽  
Vol 243 ◽  
Author(s):  
Toshio Ogawa ◽  
Hideo Kidoh ◽  
Hideyuki Yashima ◽  
Akiharu Morimoto ◽  
Tatsuo Shimizu

AbstractLead-zirconate-titanate films were prepared by excimer laser ablation. The coercive field of films deposited on MgO substrates with an electrode was lower than that of films deposited on sapphire substrates. Laser fluence influenced the grain and crystalline size, resulting in a change in the Ec. Film thicknesses were varied over a range from 0.3 to 2.41μm, with the thinnest film showing a large remanent polarization even at an applied effective voltage of 5V.


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