TY - JOUR
T1 - Formation mechanism of BaZrO3 nanorods in SmBa 2Cu3Oy thin films
AU - Ozaki, Toshinori
AU - Yoshida, Yutaka
AU - Ichino, Yusuke
AU - Takai, Yoshiaki
AU - Ichinose, Ataru
AU - Matsumoto, Kaname
AU - Horii, Shigeru
AU - Mukaida, Masashi
AU - Takano, Yoshihiko
N1 - Copyright:
Copyright 2010 Elsevier B.V., All rights reserved.
PY - 2010/7
Y1 - 2010/7
N2 - In BaZrO3(BZO) doped REBa2Cu3O y(REBCO) films deposited by pulsed laser deposition, BZO nanorods grow almost parallel to c-axis in REBCO films. In this study, in order to understand the mechanism for the formation of BZO nanorods, we investigated the influence of the substrate temperature of the upper layer (T8 upper) in the low temperature growth (LTG) technique on the growth of BZO nanorods in SmBa2Cu3Oy(SmBCO) films. Furthermore, we discussed the diffusion process on BZO and estimated the activation energy for surface diffusion of constituent atoms in BZO. With decreasing T8upper, the diameter of BZO nanorods was decreased and the number density was increased. In addition, the angle of inclination of BZO nanords with respect to c-axis in SmBCO became larger with decreasing T8upper It is found that the diffusion process could be dominant in the nucleation of BZO. We attributed self-organized growth of BZO nanorods to the diffusion process as well as the strain energy resulting from a lattice mismatch between SmBCO and BZO.
AB - In BaZrO3(BZO) doped REBa2Cu3O y(REBCO) films deposited by pulsed laser deposition, BZO nanorods grow almost parallel to c-axis in REBCO films. In this study, in order to understand the mechanism for the formation of BZO nanorods, we investigated the influence of the substrate temperature of the upper layer (T8 upper) in the low temperature growth (LTG) technique on the growth of BZO nanorods in SmBa2Cu3Oy(SmBCO) films. Furthermore, we discussed the diffusion process on BZO and estimated the activation energy for surface diffusion of constituent atoms in BZO. With decreasing T8upper, the diameter of BZO nanorods was decreased and the number density was increased. In addition, the angle of inclination of BZO nanords with respect to c-axis in SmBCO became larger with decreasing T8upper It is found that the diffusion process could be dominant in the nucleation of BZO. We attributed self-organized growth of BZO nanorods to the diffusion process as well as the strain energy resulting from a lattice mismatch between SmBCO and BZO.
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U2 - 10.2320/jinstmet.74.422
DO - 10.2320/jinstmet.74.422
M3 - Article
AN - SCOPUS:77956164929
SN - 0021-4876
VL - 74
SP - 422
EP - 427
JO - Nippon Kinzoku Gakkaishi/Journal of the Japan Institute of Metals
JF - Nippon Kinzoku Gakkaishi/Journal of the Japan Institute of Metals
IS - 7
ER -