TY - JOUR
T1 - Superconductivity in In2O3-ZnO crystalline films
AU - Shinozaki, B.
AU - Kokubo, N.
AU - Takada, S.
AU - Yamaguti, T.
AU - Yamada, K.
AU - Makise, K.
AU - Yano, K.
AU - Inoue, K.
AU - Nakamura, H.
PY - 2009
Y1 - 2009
N2 - Thin In2O3-ZnO (IZO) films were prepared by DC-magnetron sputtering with changing the weight concentration x of ZnO, 0 ≤ x ≤ 0.07. As-grown amorphous IZO films show the metallic characteristic but do not show superconductivity. We have investigated the T and H dependence of the resistivity ρ and Hall coefficient for annealed films with thickness d 350 nm in air. It is found that the films with 0 ≤ x ≤ 0.03 show superconductivity. Transition temperature Tc and the carrier density n of these films are 2.0 K and 1025 -1026 m-3, respectively. The annealed In2O3-ZnO films were examined by a high resolution transparent electron microscopy. This investigation reveals that films annealed at 300 °C are sufficient crystalline. There is a difference of crystal structures between the superconducting film and normal film. We studied the upper critical magnetic field HC2 (T) for the film with x 0.005. From the slope of dHc2/dT, we obtain the coherent length ζ(0) 100 A at T 0 K and the coefficient of the electronic heat capacity γ 3.2 (J/m3K2) which is small compared with that of other oxide materials.
AB - Thin In2O3-ZnO (IZO) films were prepared by DC-magnetron sputtering with changing the weight concentration x of ZnO, 0 ≤ x ≤ 0.07. As-grown amorphous IZO films show the metallic characteristic but do not show superconductivity. We have investigated the T and H dependence of the resistivity ρ and Hall coefficient for annealed films with thickness d 350 nm in air. It is found that the films with 0 ≤ x ≤ 0.03 show superconductivity. Transition temperature Tc and the carrier density n of these films are 2.0 K and 1025 -1026 m-3, respectively. The annealed In2O3-ZnO films were examined by a high resolution transparent electron microscopy. This investigation reveals that films annealed at 300 °C are sufficient crystalline. There is a difference of crystal structures between the superconducting film and normal film. We studied the upper critical magnetic field HC2 (T) for the film with x 0.005. From the slope of dHc2/dT, we obtain the coherent length ζ(0) 100 A at T 0 K and the coefficient of the electronic heat capacity γ 3.2 (J/m3K2) which is small compared with that of other oxide materials.
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U2 - 10.1088/1742-6596/150/5/052237
DO - 10.1088/1742-6596/150/5/052237
M3 - Article
AN - SCOPUS:77952486382
SN - 1742-6588
VL - 150
JO - Journal of Physics: Conference Series
JF - Journal of Physics: Conference Series
IS - 5
M1 - 052237
ER -