TY - GEN
T1 - Tantalum vacancy effects on electrical conductivity of La 3Ta0.5Ga5.5O14 and Ba-based P321 crystals
AU - Chung, Chan Yeup
AU - Yaokawa, Ritsuko
AU - Mizuseki, Hiroshi
AU - Kawazoe, Yoshiyuki
PY - 2012
Y1 - 2012
N2 - Single crystalline langatate (La3Ta0.5Ga 5.5O14, LTG) has been widely used in piezoelectric sensors for high temperature applications because of its structural stability at high temperature. However, in the recent experiment, an increase of electrical conductivity has been also observed at the intermediate temperature region ranges from 300 to 700°C. Also, in theoretical calculations, penta-valent Ta vacancy can be easily generated and influence resistivity degradation of the crystal. In this study, to elucidate the Ta vacancy effects on electrical conductivity of LTG and recently proposed Ba-based P321 crystal such as BTGS and BTAS, electrical conductivity of those materials were calculated and compared by utilizing Boltzmann transport theory. The calculated GW band gaps of perfect BTGS and BTAS (5.94 eV and 6.69 eV, respectivily) were much larger than that of LTG (5.36 eV). Also, at intermediate temperature (1000K), the calculated electrical conductivity of LTG with V‴ Ta (in Kröger-Vink notation [13]) was around twelve times higher than the conductivity of BTGS and BTAS with Ta vacancy.
AB - Single crystalline langatate (La3Ta0.5Ga 5.5O14, LTG) has been widely used in piezoelectric sensors for high temperature applications because of its structural stability at high temperature. However, in the recent experiment, an increase of electrical conductivity has been also observed at the intermediate temperature region ranges from 300 to 700°C. Also, in theoretical calculations, penta-valent Ta vacancy can be easily generated and influence resistivity degradation of the crystal. In this study, to elucidate the Ta vacancy effects on electrical conductivity of LTG and recently proposed Ba-based P321 crystal such as BTGS and BTAS, electrical conductivity of those materials were calculated and compared by utilizing Boltzmann transport theory. The calculated GW band gaps of perfect BTGS and BTAS (5.94 eV and 6.69 eV, respectivily) were much larger than that of LTG (5.36 eV). Also, at intermediate temperature (1000K), the calculated electrical conductivity of LTG with V‴ Ta (in Kröger-Vink notation [13]) was around twelve times higher than the conductivity of BTGS and BTAS with Ta vacancy.
KW - Boltzmann transport calculation
KW - Density functional theory
KW - First principles calculation
KW - GW calculation
KW - Langatate
KW - Ta vacancy
UR - http://www.scopus.com/inward/record.url?scp=84859712682&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=84859712682&partnerID=8YFLogxK
U2 - 10.4028/www.scientific.net/KEM.508.325
DO - 10.4028/www.scientific.net/KEM.508.325
M3 - Conference contribution
AN - SCOPUS:84859712682
SN - 9783037853764
T3 - Key Engineering Materials
SP - 325
EP - 330
BT - Materials Integration
PB - Trans Tech Publications Ltd
T2 - Int. Symposium of GCOE: Materials Integration, in Conjunction with the 2nd Int. Symposium on Advanced Synthesis and Processing Technology for Materials, ASPT 2011 and the 8th Materials Science School for Young Scientists, KINKEN-WAKATE 2011
Y2 - 1 December 2011 through 2 December 2011
ER -