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최정옥(J.O. Choi),이정중(J.J. Lee),한석희(S.H. Han),김희중(H.J. Kim),강일구(I.K. Kang) 한국자기학회 1993 韓國磁氣學會誌 Vol.3 No.1
Thin films of soft magnetic Fe-Hf-C alloys with nanoscale crystallites were investigated in this study. The films were fabricated by an RF diode magnetron sputtering apparatus and subsequently annealed in vacuum. The soft magnetic properties of the films were observed to differ depending on the different substrates such as Corning 7059, CaTiO₃ and Al₂O₃-TiC with various underlayer(Cr, SiO₂) thickness. This results may be due to the interdiffusion between the substrate and the magnetic layer and / or between the underlayer and the magnetic layer, rather than the microstructural change such as grain size. The Fe-Hf-C films with high permeability up to 4000(at 1 ㎒) and saturation magnetization up to 16 kG were obtained in the vicinity of phase boundary between the crystalline and amorphous state when the size of α-Fe grains is about 5 ㎚. And also the films were found to have thermal stability up to 600 ℃.
초고진공 UBM 스퍼터링으로 제조된 라멜라 구조 TaN 박막의 연구
이기락(G. R. Lee),C. S. Shin,I. Petrov,J. E. Greene,이정중(J. J. Lee) 한국표면공학회 2005 한국표면공학회지 Vol.38 No.2
The effect of crystal orientation and microstructure on the mechanical properties of TaNx was investigated. TaNx films were grown on SiO₂ substrates by ultrahigh vacuum unbalanced magnetron sputter deposition in mixed Ar/N₂ discharges at 20 mTorr (2.67 ㎩) and at 350℃. Unlike the Ti-N system, in which TiN is the terminal phase, a large number of N-rich phases in the Ta-N system could lead to layers which had nano-sized lamella structure of coherent cubic and hexagonal phases, with a correct choice of nitrogen fraction in the sputtering mixture and ion irradiation energy during growth. The preferred orientations and the microstructure of TaNx layers were controlled by varing incident ion energy Ei (=30 eV~50 eV) and nitrogen fractions fN₂ (=0.1~0.15). TaNx layers were grown on (0002)-Ti underlayer as a crystallographic template in order to relieve the stress on the films. The structure of the TaNx film transformed from BI-NaCI δ-TaNx to lamellar structured Bl-NaCI δ-TaNx + hexagonal γ-TaNx or Bl-NaCl δ-TaNx + hexagonal γ-TaNx with increasing the ion energy at the same nitrogen fraction fN₂. The hardness of the films also increased by the structural change. At the nitrogen fraction of 0.1~0.125, the structure of the TaNx films was changed from δ-TaNx + ε-TaNx to δ-TaNx + γ-TaNx with increasing the ion energy. However, at the nitrogen fraction of 0.15, the film structure did not change from δ-TaN, + ε-TaNx over the whole range of the applied ion energy. The hardness increased significantly from 21.1 ㎬ to 45.5 ㎬ with increasing the ion energy.