Electrical Characterization and Microstructures of Bi3.3Tb0.6Ti3O12 and Bi3.3Tb0.6Ti2.97V0.03O12 Thin Films

2013 ◽  
Vol 537 ◽  
pp. 126-129
Author(s):  
Rui Fang Liu ◽  
M.B. Sun ◽  
W.P. Ding ◽  
X.A. Mei

Bi3.3Tb0.6Ti3O12(BTT), Bi3.3Tb0.6Ti2.97V0.03O12(BTTV), and pure Bi4Ti3O12 (BIT) thin films with random orientation were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well developed rod-like grains with random orientation. The experimental results indicated that Tb doping into BIT also result in a remarkable improvement in ferroelectric property. The remanent polarization (Pr) and coercive field (Ec) of the BTT film were 25 μC/cm2 and 85 kV/cm, respectively. Furthermore, V substitution improves the Pr value of the BTVT film up to 35 μC/cm2, which is much larger than that of the BTT film.

2012 ◽  
Vol 624 ◽  
pp. 178-181
Author(s):  
C.Q. Huang ◽  
J.G. Liu ◽  
X.A. Mei ◽  
J. Liu

Bi3.25Er0.75Ti3O12(BET) and Bi3.25Er0.75Ti2.97V0.03O12(BETV) thin films with random orientation were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well developed rod-like grains with random orientation. The experimental results indicated that Er doping into Bi4Ti3O12 (BIT) also result in a remarkable improvement in ferroelectric property. The remanent polarization (Pr) and coercive field (Ec) of the BET film were 17 μC/cm2 and 80 kV/cm, respectively. Furthermore, V substitution improves the Er value of the BETV films up to 28 μC/cm2, which is much larger than that of the BET film.


2013 ◽  
Vol 537 ◽  
pp. 122-125
Author(s):  
Min Chen ◽  
X.A. Mei ◽  
Rui Fang Liu ◽  
C.Q. Huang ◽  
J. Liu

Bi2.9Pr0.9Ti3O12(BPT) and Bi2.9Pr0.9Ti2.97V0.03O12(BPTV) thin films with random orientation were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well developed rod-like grains with random orientation. The experimental results indicated that Pr doping into Bi4Ti3O12 (BIT) result in a remarkable improvement in ferroelectric property. The remanent polarization (Pr) and coercive field (Ec) of the BPT film were 28 μC/cm2 and 80 kV/cm, respectively. Furthermore, V substitution improves the Pr value of the BTVT film up to 43 μC/cm2, which is much larger than that of the BPT film.


2013 ◽  
Vol 833 ◽  
pp. 41-44
Author(s):  
Bei Li ◽  
X.H. Yuan ◽  
M. Chen ◽  
X.A. Mei

Tm2O3-doped bismuth titanate (Bi4-xTmxTi3O12, BTT) and pure Bi4Ti3O12 (BIT) thin films with random orientation were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well developed rod-like grains with random orientation. The experimental results indicated that Tm doping into BIT results in remarkable improvement in ferroelectric properties. The Pr and the Ec values of the BTT film with x=0.75 were 28 μC/cm2 and 80 kV/cm, respectively.


2013 ◽  
Vol 591 ◽  
pp. 208-211
Author(s):  
Min Chen ◽  
J. Liu ◽  
X.A. Mei

Y2O3-doped bismuth titanate (Bi4-xYxTi3O12: BYT) and pure Bi4Ti3O12 (BIT) thin films with random orientation were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well developed rod-like grains with random orientation. Y-doping into BIT caused a large shift of the Curie temperature ( TC ) from 675 °C to lower temperature and a improvement in dielectric property. The experimental results indicated that Y doping into BIT also result in a remarkable improvement in ferroelectric property. The Pr and the Ec values of the BYT film with x=0.75 were 28 μC/cm2 and 65 kV/cm, respectively.


2011 ◽  
Vol 492 ◽  
pp. 222-225
Author(s):  
J. Liu ◽  
M. Chen ◽  
X.A. Mei ◽  
Y.H. Sun ◽  
Chong Qing Huang

Tb-doped bismuth titanate (Bi4-xCexTi3O12: BCT) and pure Bi4Ti3O12 (BIT) thin films with random orientation were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well developed rod-like grains with random orientation. Ce-doping into BIT caused a large shift of the Curie temperature (TC) from 675°C to lower temperature and a improvement in dielectric property. The experimental results indicated that Ce doping into BIT also result in a remarkable improvement in ferroelectric property. The Pr and the Ec values of the BCT film with x = 0.75 were 23 μC/cm2 and 80 kV/cm, respectively.


2008 ◽  
Vol 368-372 ◽  
pp. 82-84
Author(s):  
Y.H. Sun ◽  
Min Chen ◽  
W.K. An ◽  
A.H. Cai ◽  
J. Liu ◽  
...  

Tb-doped bismuth titanate (BixTbyTi3O12: BTT) and pure Bi4Ti3O12 (BIT) thin films with random orientation were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well-developed rod-like grains with random orientation. Tb doping into BIT caused a large shift of the Curie temperature (TC) from 675°C to lower temperature. The experimental results indicated that Tb doping into BIT result in a remarkable improvement in dielectric property.


2014 ◽  
Vol 633 ◽  
pp. 257-260
Author(s):  
Min Chen ◽  
X.A. Mei ◽  
J. Liu

Gd2O3-doped bismuth titanate (Bi4-xGdxTi3O12: BGT) and pure Bi4Ti3O12 (BIT) thin films with random orientation were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well developed rod-like grains with random orientation. Gd-doping into BIT caused a large shift of the Curie temperature ( TC ) from 675 °C to lower temperature and a improvement in dielectric property. The experimental results indicated that Gd doping into BIT also result in a remarkable improvement in ferroelectric property. The Pr and the Ec values of the BGT film with x=0.75 were 28 μC/cm2 and 65 kV/cm, respectively.


2007 ◽  
Vol 336-338 ◽  
pp. 152-154
Author(s):  
K.L. Su ◽  
Y.H. Sun ◽  
Min Chen ◽  
Z.M. Wan ◽  
Z.H. Hou

Nd-doped bismuth titanate and random oriented Bi4-xNdxTi3O12 (BNT) thin films were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well developed rod-like grains with random orientation. The remanent polarization (Pr) and coercive field (Ec) of the BNT film with x = 0.5 were above 19 μC/cm2 and 50 KV/cm, respectively. Nd doping into BIT caused a shift of the Curie temperature (TC) of the BIT from 675°C to 660, 520, 410 and 256oC for the films with x = 0.25, 0.5, 0.75 and 1.0, respectively. The experimental results indicated that Nd doping into BIT result in a remarkable improvement in ferroelectric and dielectric properties.


2013 ◽  
Vol 591 ◽  
pp. 200-203 ◽  
Author(s):  
X.A. Mei ◽  
Min Chen ◽  
J. Liu ◽  
R.F. Liu

Ce-doped bismuth titanate (Bi4-xCexTi3O12: BCT) and pure Bi4Ti3O12 (BIT) thin films with random orientation were fabricated on Pt/Ti/SiO2/Si substrates by pulsed laser deposition technique. These samples had polycrystalline Bi-layered perovskite structure without preferred orientation, and consisted of well developed rod-like grains with random orientation. The experimental results indicated that Ce doping into BIT result in a remarkable improvement in ferroelectric propertis. The Pr and the Ec values of the BCT film with x=0.75 were 23 μC/cm2 and 80 kV/cm, respectively.


2010 ◽  
Vol 105-106 ◽  
pp. 259-262 ◽  
Author(s):  
X.A. Mei ◽  
Min Chen ◽  
A.H. Cai ◽  
K.L. Su ◽  
Chong Qing Huang ◽  
...  

Tb4O7-doped bismuth titanate (BixTbyTi3O12 BTT) thin films were fabricated on Pt/Ti/SiO2/Si substrates by rf magnetron sputtering technique, and the microstructures and ferroelectric properties of the films were investigated. Microstructure studies indicate that all of BTT films with well-developed rod-like grains consist of single phase of a bismuth-layered structure without preferred orientation. The experimental results indicate that Tb doping into Bi4Ti3O12 results in a remarkable improvement in ferroelectric properties. The remanent polarization (Pr) and coercive field (Ec) of the BTT film with y=0.6 were 22 μC/cm2 and 85 kV/cm, respectively.


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