TY - JOUR
T1 - Fabrication of M3+-substituted and M3+/V 5+-cosubstituted bismuth titanate thin films [M = lanthanoid] by chemical solution deposition technique
AU - Uchida, Hiroshi
AU - Yoshikawa, Hiroki
AU - Okada, Isao
AU - Matsuda, Hirofumi
AU - Iljima, Takashi
AU - Watanabe, Takayuki
AU - Funakubo, Hiroshi
PY - 2002/11
Y1 - 2002/11
N2 - Lanthanoid (M3+ = La3+, Pr3+", Nd3+ and Sm3+)-consubstituted and lanthanoid/vanadium (V5+)-cosubstituted bismuth titanate thin films were fabricated on (111)Pt/Ti/SiO2/(100)Si substrates by a chemical solution deposition (CSD) technique. All the films consisted of a polycrystalline structure with random crystal orientation. Pe3+, Nd3+ and Sm 3+-substituted BIT films [BPT, BNT and BST] had larger remanent polarization (Pr) values than that of conventional La3+-substituted BIT film [BLT]; furthermore, the Pr value of the BNT film was higher than those of the BPT and BST films. On the other hand, no significant difference in the coercive field (Ec) value was found among those films. Pr and Ec values of the BNT film with y = 0.50 in (Bi4.00-y, Ndy.)Ti3.00O12 were measured to be 32 μC/cm2 and 126kV/cm, respectively. V 5+-substitution varied the Pr value of the lanthanoid-substituted BIT films without changing the in Ec value. The Pr value of the BNT film with y = 0.50 was improved up to 37 μC/cm 2 by V5+-substitution of x = 0.02 in (Bi4.00-y, Ndy) 1-(x/12) (Ti3.00-x, Vx)O 12 [BNTV]. Ferroelectric properties of the Pb-free polycrystalline BNT and BNTV films are comparable to those of conventional Pb-based ferroelectric films such as lead zirconate titanate [PZT] films.
AB - Lanthanoid (M3+ = La3+, Pr3+", Nd3+ and Sm3+)-consubstituted and lanthanoid/vanadium (V5+)-cosubstituted bismuth titanate thin films were fabricated on (111)Pt/Ti/SiO2/(100)Si substrates by a chemical solution deposition (CSD) technique. All the films consisted of a polycrystalline structure with random crystal orientation. Pe3+, Nd3+ and Sm 3+-substituted BIT films [BPT, BNT and BST] had larger remanent polarization (Pr) values than that of conventional La3+-substituted BIT film [BLT]; furthermore, the Pr value of the BNT film was higher than those of the BPT and BST films. On the other hand, no significant difference in the coercive field (Ec) value was found among those films. Pr and Ec values of the BNT film with y = 0.50 in (Bi4.00-y, Ndy.)Ti3.00O12 were measured to be 32 μC/cm2 and 126kV/cm, respectively. V 5+-substitution varied the Pr value of the lanthanoid-substituted BIT films without changing the in Ec value. The Pr value of the BNT film with y = 0.50 was improved up to 37 μC/cm 2 by V5+-substitution of x = 0.02 in (Bi4.00-y, Ndy) 1-(x/12) (Ti3.00-x, Vx)O 12 [BNTV]. Ferroelectric properties of the Pb-free polycrystalline BNT and BNTV films are comparable to those of conventional Pb-based ferroelectric films such as lead zirconate titanate [PZT] films.
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U2 - 10.1143/JJAP.41.6820
DO - 10.1143/JJAP.41.6820
M3 - Article
AN - SCOPUS:1642450387
SN - 0021-4922
VL - 41
SP - 6820
EP - 6824
JO - Japanese Journal of Applied Physics
JF - Japanese Journal of Applied Physics
IS - 11 B
ER -