TY - JOUR
T1 - Thermal conductivity of hetero-epitaxial ZnO thin films on c - And r -plane sapphire substrates
T2 - Thickness and grain size effect
AU - Yamashita, Yuichiro
AU - Honda, Kaho
AU - Yagi, Takashi
AU - Jia, Junjun
AU - Taketoshi, Naoyuki
AU - Shigesato, Yuzo
N1 - Funding Information:
A part of this work was supported by JST CREST (Grant No. JPMJCR17I2), Japan. We wish to acknowledge the fruitful discussion with Professor Masahiro Nomura at the University of Tokyo on the phonon scattering effects on thermal conductivity.
Publisher Copyright:
© 2019 Author(s).
PY - 2019/1/21
Y1 - 2019/1/21
N2 - The thermal conductivities of c- and a-axis-oriented zinc oxide (ZnO) thin films with nominal thicknesses of 100, 200, and 300 nm are investigated. The c- and a-axis-oriented ZnO thin films were synthesized by radio frequency magnetron sputtering on the c- and r-plane sapphire substrates, respectively. The epitaxial relationship between the ZnO thin film and the c-plane sapphire substrate is (0001) [1 1 00] || (0001) [11 2 0], and that between the ZnO thin film and the r-plane sapphire substrate is (11 2 0) [1 1 00] || (01 1 2) [11 2 0]. The c-axis-oriented ZnO thin film has a columnar structure, whereas the a-axis-oriented ZnO thin film has a single domain-like structure and a significantly flat surface. The thermal conductivity of the c-axis-oriented ZnO thin film is in the range of 18-24 W m -1 K -1 , whereas for the a-axis-oriented ZnO thin film, it is in the range of 24-29 W m -1 K -1 . For the c-axis-oriented ZnO thin films, the phonon scattering on both the out-of-plane and in-plane grain boundaries affects the thermal conductivity. In contrast, the thermal conductivity of the a-axis-oriented ZnO thin films decreases with the decrease of the film thickness. The distribution of the normalized cumulative thermal conductivity of the a-axis-oriented ZnO thin films suggests that the heat transport carrier mostly consists of phonons with the mean free paths between 100 nm and 1 μm.
AB - The thermal conductivities of c- and a-axis-oriented zinc oxide (ZnO) thin films with nominal thicknesses of 100, 200, and 300 nm are investigated. The c- and a-axis-oriented ZnO thin films were synthesized by radio frequency magnetron sputtering on the c- and r-plane sapphire substrates, respectively. The epitaxial relationship between the ZnO thin film and the c-plane sapphire substrate is (0001) [1 1 00] || (0001) [11 2 0], and that between the ZnO thin film and the r-plane sapphire substrate is (11 2 0) [1 1 00] || (01 1 2) [11 2 0]. The c-axis-oriented ZnO thin film has a columnar structure, whereas the a-axis-oriented ZnO thin film has a single domain-like structure and a significantly flat surface. The thermal conductivity of the c-axis-oriented ZnO thin film is in the range of 18-24 W m -1 K -1 , whereas for the a-axis-oriented ZnO thin film, it is in the range of 24-29 W m -1 K -1 . For the c-axis-oriented ZnO thin films, the phonon scattering on both the out-of-plane and in-plane grain boundaries affects the thermal conductivity. In contrast, the thermal conductivity of the a-axis-oriented ZnO thin films decreases with the decrease of the film thickness. The distribution of the normalized cumulative thermal conductivity of the a-axis-oriented ZnO thin films suggests that the heat transport carrier mostly consists of phonons with the mean free paths between 100 nm and 1 μm.
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U2 - 10.1063/1.5055266
DO - 10.1063/1.5055266
M3 - Article
AN - SCOPUS:85060131085
SN - 0021-8979
VL - 125
JO - Journal of Applied Physics
JF - Journal of Applied Physics
IS - 3
M1 - 035101
ER -