• Title/Summary/Keyword: (${Ba_{0.66}}{Sr_{0.34}}{TiO_3}$_BST

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Electrical Properties of Ba0.66Sr0.34TiO3 Thin Films Fabricated by a Seed-layer Process (Seed-layer 공정을 이용한 Ba0.66Sr0.34TiO3박막의 제조 및 전기적 특성 연구)

  • 최덕영;박철호;손영국
    • Journal of the Korean Ceramic Society
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    • v.40 no.2
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    • pp.198-205
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    • 2003
  • $Ba_{0.66}Sr_{0.34}TiO_3$ thin films and seed-layers were deposited on $Pt/Ti/SiO_2/Si$substrate by R.F. magnetron sputtering method. Effects of various substrate temperature conditions on electrical properties (such as capacitance and leakage current) of BST thin films were studied. The effect of seed-layer was also studied. When seed-layer was inserted between BST and Pt, the crystallization of the BST thin films was considerably improved and the processing temperature was lowered. Compared to the pure BST thin films, dielectric constant, dielectric loss, and leakage current of BST thin films deposited on the seed-layer were considerably improved. It could be revealed that electrical properties are influenced by the substrate temperatures of BST thin films and are enhanced by the seed-layer.

Structural and Dielectric Properties of the Doped (Ba,Sr)$TiO_3$ Ceramics (불순물이 첨가된 (Ba,Sr) $TiO_3$ 세라믹의 구조 및 유전특성)

  • 임성수;한명수;정민석;김태훈;이금성;한석룡;이성갑
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1998.11a
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    • pp.33-36
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    • 1998
  • BST(66/34) and BSCT(60/30/10) ceramics were prepared by mixed oxide method and studied about the microstructural and dielectric properties with $Y_2$O$_3$, Dy$_2$O$_3$, La$_2$O$_3$, MnCO$_3$. The grain size of undoped BST was 20~30 ${\mu}{\textrm}{m}$, but that of BST, doped content of MnCO$_3$ was 0.1 mol%, was decreased with increasing the contents of $Y_2$O$_3$. As the content of $Y_2$O$_3$ was Increased, Tc was shifted to lower temperature and dielectric constant at Tc was decreased. The dielectric constant of doped BSCT(60/30/10) ceramics ( 0.9 mol% $Y_2$O$_3$. and 0.1 mol% MnCO$_3$) was about 8, 000 at Tc( 22$^{\circ}C$ ).

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