TY - JOUR
T1 - Influence of orientation on the electro-optic effect in epitaxial Y-doped HfO2ferroelectric thin films
AU - Kondo, Shinya
AU - Shimura, Reijiro
AU - Teranishi, Takashi
AU - Kishimoto, Akira
AU - Nagasaki, Takanori
AU - Funakubo, Hiroshi
AU - Yamada, Tomoaki
N1 - Funding Information:
This work was partly supported by the Element Strategy Initiative to Form a Core Research Center, Ministry of Education, Culture, Sports, Science, and Technology of Japan (MEXT) (Grant Number JPMXP0112101001) (TY, HF), Foundation of Public Interest of Tatematsu (TY), and Murata Science Foundation (TY).
Publisher Copyright:
© 2021 The Japan Society of Applied Physics.
PY - 2021/11
Y1 - 2021/11
N2 - Recently, we reported linear electro-optic (EO) effects in (100)-epitaxial yttrium-doped hafnium dioxide (Y-HfO2) ferroelectric thin films. In this study, we have investigated the influence of orientation on the EO effect in Y-HfO2 thin-film. (111)-epitaxial undoped HfO2 and Y-HfO2 films were deposited on Sn-doped In2O3/yttria-stabilized zirconia (111) substrates at room temperature through radiofrequency magnetron sputtering. Although the undoped HfO2 film showed typical paraelectric characteristics, ferroelectricity was observed in the (111)-Y-HfO2 film. Remnant polarization in the (111)-Y-HfO2 film was higher than that in the (100)-Y-HfO2 film. The (111)-Y-HfO2 film exhibited a linear EO effect based on ferroelectricity, which is consistent with that of the (100)-Y-HfO2 film. The average EO coefficient r c of the (111)-Y-HfO2 film was 0.67 pm V-1, which is higher than that of the (100)-Y-HfO2 film. This result is reasonable considering the difference in remnant polarization between the (100)-Y-HfO2 and (111)-Y-HfO2 films.
AB - Recently, we reported linear electro-optic (EO) effects in (100)-epitaxial yttrium-doped hafnium dioxide (Y-HfO2) ferroelectric thin films. In this study, we have investigated the influence of orientation on the EO effect in Y-HfO2 thin-film. (111)-epitaxial undoped HfO2 and Y-HfO2 films were deposited on Sn-doped In2O3/yttria-stabilized zirconia (111) substrates at room temperature through radiofrequency magnetron sputtering. Although the undoped HfO2 film showed typical paraelectric characteristics, ferroelectricity was observed in the (111)-Y-HfO2 film. Remnant polarization in the (111)-Y-HfO2 film was higher than that in the (100)-Y-HfO2 film. The (111)-Y-HfO2 film exhibited a linear EO effect based on ferroelectricity, which is consistent with that of the (100)-Y-HfO2 film. The average EO coefficient r c of the (111)-Y-HfO2 film was 0.67 pm V-1, which is higher than that of the (100)-Y-HfO2 film. This result is reasonable considering the difference in remnant polarization between the (100)-Y-HfO2 and (111)-Y-HfO2 films.
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U2 - 10.35848/1347-4065/ac17e0
DO - 10.35848/1347-4065/ac17e0
M3 - Article
AN - SCOPUS:85112863340
SN - 0021-4922
VL - 60
JO - Japanese Journal of Applied Physics, Part 1: Regular Papers & Short Notes
JF - Japanese Journal of Applied Physics, Part 1: Regular Papers & Short Notes
IS - SF
M1 - SFFB13
ER -